NUREG/IA--0134

CAMP005

International

Agreement Report

Assessment of RELAP5/MOD3.1 for

Gravity-Driven Injection Experiment

in the Core Makeup Tank of the

CARR Passive Reactor (CP-1300)

Prepared by

Sang I1 Lee, Hee Cheon No, KAIST

Young Seok Bang, Hho Jung Kim, KINS

Korea Advanced Institute of Science and Technology

Nuclear Engineering Department

373-1, Gusung-Dong

Yusung, Taejon

305-701 Korea

Korea Institute of Nuclear Safety

Advanced Reactor Dept.

P.O. Box 114

Yusung, Taejon

305-600 Korea

Office of Nuclear Regulatory Research

U.S. Nuclear Regulatory Commision

Washington, DC 20555-0001

October 1996

Prepared as part of

The Agreement on Research Participation and Technical Exchange

under the International Thermal-Hydraulic Code Assessment

and Maintenance Program (CAMP)

Published by

U.S. Nuclear Regulatory Commission
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NUREG/IA-0134

CAMP005

International

Agreement Report

Assessment of RELAP5/MOD3.1 for

Gravity-Driven Injection Experiment

in the Core Makeup Tank of the

CARR Passive Reactor (CP-1300)

Prepared by

Sang H Lee, Hee Cheon No, KAIST

Young Seok Bang, -ho Jung Kim, KINS

Korea Advanced Institute of Science and Technology

Nuclear Engineering Department

373-1, Gusung-Dong

Yusung, "liejon

305-701 Korea

Korea Institute of Nuclear Safety

Advanced Reactor Dept.

P.O. Box 114

Yusung, Thejon

305-600 Korea

Office of Nuclear Regulatory Research

U.S. Nuclear Regulatory Commision

Washington, DC 20555-0001

October 1996

Prepared as part of

The Agreement on Research Participation and TIchnical Exchange

under the International Thermal-Hydraulic Code Assessment

and Maintenance Program (CAMP)

Published by

U.S. Nuclear Regulatory Commission
NUREGIIA-013C has b~een" oero due

from the: best avail able coy............. .... .
Assessment of RELAP5/MOD3.1 for Gravity-Driven Injection

Experiment in the Core Makeup Tank of the CARR Next Generation

Reactor

Abstract

The objective of the present work is to improve the analysis capability of RELAP5/MOD3.1 on the direct contact condensation in the core makeup tank(CMT)

of passive high-pressure injection system(PHPIS) in the CARR Passvie Reactor(CP1300). The gravity-driven injection experiment is conducted by using a small scale

test facility to identify the parameters having significant effects on the gravitydriven injection and the major condensation modes. It turns out that the larger

the water subcooling is, the more the initiation of injection is delayed, and the

sparger and the natural circulation of the hot water from the steam generator

accelerate the gravity-driven injection. The condensation modes are divided into

three modes: sonic jet, subsonic jet, and steam cavity. RELAP5/MOD3.1 is chosen to evaluate the code predictability on the direct contact condensation in the

CMT. It is found that the predictions of MOD3.1 are in better agreement with

the experimental data than those of MOD3.0. From the nodalization study of

the test section, the 1- node model shows better agreement with the experimental

data than the multi- node models. RELAP5/MOD3.1 identifies the flow regime

of the test section as vertical stratification. However, the flow regime observed

in the experiment is the subsonic jet with the bubble having the vertical cone

shape. To accurately predict the direct contact condensation in the CMT with

RELAP5/MOD3.1, it is essential that a new set of the interfacial heat transfer

coefficients and a new flow regime map for direct contact condensation in the

CMT be developed.

iii

Contents

Abstract

Table of Contents

List of Tables

List of Figures

Executive Summary

Acknowledgment

1 Introduction

1.1 Background ....... ..............................

1.2 Objectives and report organization .....................

2 Gravity-Driven Injection Experiment

2.1 Experimental setup and instrumentation ..................

2.2 Test procedure ...... ............. ............... .

2.3 Experimental results ...... .........................

2.3.1 Effects of water subcooling on gravity-driven injection

2.3.2 Effects of natural circulation on gravity-driven injection

iii

V

vii

viii

xi

xv

1

1

3

6

6

9

10

10

11

v
2.3.3 Effects of the sparger on gravity-driven injection ..... .. 12

2.3.4 Effects of the pressure on gravity-driven injection ..... .. 13

2.3.5 Identification of condensation modes ................ 13

3 Assessment of RELAP5/MOD3.1 35

3.1 Description of code and modeling ........................ 35

3.2 Analysis results and discussion .......................... 36

3.2.1 Base case ........ ........................... 36

3.2.2 Sensitivity study ....... ....................... 38

3.2.3 Nodalization study ....... ...................... 39

3.2.4 Run statistics ....... ......................... 40

4 Conclusions 61

Bibliography 63

Appendices: Input Decks and Experimental data 65

vi
List of Tables

1.1 Summary of condensation regime map .................... 4

2.1 Tag list for the KARD-I instrument ...... ................ 16

2.2 Test matrix ........ .............................. 17

2.3 Transition time between subsonic jet and steam cavity, and injection time ......... ............................... 18

3.1 Grind time ....................................... 42

vii
List of Figures

1.1 A schematic diagram of CARR Next Generation Reactor ....... 5

2.1 A systematic diagram of test facility ...... ................ 19

2.2 A systematic diagram of test section ...................... 20

2.3 The pressure trend for test G1021 ...... .................. 21

2.4 The effect of water subcooling on the injection flow rate for test

G1021, G1022, and G1023 ............................. 22

2.5 The temperature distribution of test section for test G1021 . . .. 23

2.6 The effect of the natural circulation on the injection flow rate for

test G1021 and GN021 ....... ........................ 24

2.7 The comparison of the natural ciculation flow with the injection

flow rate for test GN021 ............ .................. 25

2.8 The temperature distribution of test section for test GN021 . . .. 26

2.9 The effect of the sparger on the injection flow rate for test G1021

and GS021 ........ ............................... 27

2.10 The temperature distribution of test section for test GS021 . . .. 28

2.11 The effect of the high pressure on the injection flow rate for test

G1021 and PI021 ........ ........................... 29

2.12 The pressure trend for test PI041 ...... .................. 30

2.13 The injection flow rate at 4bar for test P1041, PN041, and PS041 31

2.14 Sonic jet ......... ............................... 32

viii
2.15 Subsonic jet ........ .............................. 33

2.16 Steam cavity ........ ............................. 34

3.1 A systematic diagram of RELAP5 nodalization .............. 43

3.2 Comparison of the steam generator pressure between experiments

and calculation ........ ............................ 44

3.3 Comparison of the test section pressure between experiments and

calculation ........ ............................... 45

3.4 Comparison of the pool water temperature between experiments

and calculation ........ ............................ 46

3.5 Comparison of the steam flow rate between experiments and calculation ......... ................................ 47

3.6 Comparison of the injection flow rate between experiments and

calculation ........ ............................... 48

3.7 Comparison of the water level between experiments and calculation 49

3.8 Comparison of the pressure of the steam generator and the test

section between test G1021 and calculation(MOD3.0 vs MOD3.1) 50

3.9 Comparison of the pool water temperature between test G1021 and

calculation(MOD3.0 vs MOD3.1) ...... .................. 51

3.10 Comparison of the steam flow rate between test G1021 and calculation(MOD3.0 vs MOD3.1) ........................... 52

3.11 Comparison of the injection flow rate between test G1021 and calculation(MOD3.0 vs MOD3.1) .......................... 53

3.12 Comparison of the water level between test G1021 and calculation(MOD3.0 vs MOD3.1) ....... ...................... 54

3.13 Comparison of the pressure of the steam generator and the test

section between test G1021 and calculation(Nodalization study) 55

ix
3.14 Comparison of the pool water temperature between test G1021 and

calculation(Nodalization study) ...... ................... 56

3.15 Comparison of the steam flow rate between test G1021 and calculation(Nodalization study) ....... ...................... 57

3.16 Comparison of the injection flow rate between test G1021 and calculation(Nodalization study) ........................... 58

3.17 Comparison of the water level between test G1021 and calculation(Nodalization study) ....... ....................... 59

3.18 CPU time and time step size ........................... 60

x
Executive Summary

At Center for Advanced Reactor Research(CARR) in Korea a passive PWR

concept named CARR Passive Reactor(CP-1300) has been developed by adopting

a passive engineered-safety-feature-system. The CP-1300 passive safety injection

system consists of passive high-pressure injection system(PHPIS), accumulator

, and in-containment refueling water storage tank(IRWST), which are used to

supply emergency core cooling water at high, intermediate, and low pressure,

respectively. The PHPIS consists of the core makeup tanks(CMTs) with a sparger

and the pressurizer-pressure balancing line. The PHPIS can provide cold water at

any RCS pressure by gravity force because the pressure of the CMT is equilibrated

with the RCS through lines connecting the inlet of the CMT to the pressurizer.

RELAP5 code has been developed as one of the best-estimate codes. The code

is based on a non-homogeneous and non-equilibrium model for one dimensional,

two-phase flow. Recently, RELAP5 code development program has been initiated

to develop a code version suitable for the safety analysis of passive advanced

reactors like the CP-1300. However, there is no model in RELAP5 that can deal

with the direct contact condensation of steam in the pool like the CMT of the

PHPIS.

The objective of the present work is to improve the analysis capability of

the RELAP5/MOD3.1 on the direct contact condensation in the CMT of the

PHPIS. The gravity-driven injection experiment is conducted by using a small

scale test facility to identify the parameter governing the gravity-driven injection

xi
and the major phenomena. To evaluate the code predictability on the direct

contact condensation in the CMT, the base case studies are performed on the

experiments. Also, a sensitivity study is performed on two code versions (MOD3.0

vs MOD3.1). Finally, the effect of the node number of the test section on the

gravity driven injection is investigated. From the present study, the following

conclusions axe obtained:

* The experimental results show that the lower the water temperature is, the

longer the initiation time of injection is delayed, and the sparger and the

natural circulation from the hot water in the steam generator accelerate

the gravity-driven injection. The condensation modes identified through

the experiments are divided into three modes: sonic jet, subsonic jet, and

steam cavity. The steam cavity is the unique mode of downward injection

with a solid surface directly connected to the pipe exit not seen in other

experiments.

* RELAP5/MOD3.1 better predicts the experiment data of the water level at

4 bar than that at 1.5 bar. However, the calculated results are not in good

agreement with the other measurement parameters, such as the pressures

of the steam generator and the test section, the pool temperature, the flow

rate of steam and injection, the test section water level.

* The overall prediction capabilities of RELAP5/MOD3.0 and MOD3.1 are

poor. However, the predictions of RELAP5/MOD3.1 are in better agreement with the experimental data than those of RELAP5/MOD3.0. MOD3.0

and MOD3.1 identify the flow regime of the test section as vertical stratification, and they have the same heat transfer correlation of the vertical

stratification. It is not clear the reason why MOD3.1 better predicts the

experimental data than MOD3.0.

xii
* From the nodalization study of RELAP5/MOD3.1, the 1-node model shows

better agreement with the experimental data than multi-node models. However, considering the penetration depth of the jetting, the proper node number of the CMT must be determined.

9 To accurately predict the direct contact condensation in the CMT by the

RELAP5/MOD3.1, it is necessary that a new set of the interfacial heat

transfer coefficients and a new flow regime map for the direct contact condensation in the CMT be developed. The new set of the interfacial heat

transfer coefficients and the flow regime map should capture the physical

process of the direct contact condensation in the CMT.

xiii

Acknowledgment

This report was performed under the sponsorship of Korea Science and Engineering Foundation(KOSEF). Authors appreciate the KOSEF for the financial

support.

xv

Chapter 1

Introduction

1.1 Background

At Center for Advanced Reactor Research(CARR) in Korea, a passive PWR

concept named CARR Next Generation Reactor(CP-1300) has been developed

by adopting a passive engineered-safety-feature-system as shown in Figure 1.1

The CP-1300 is a large passive PWR with the power of 1300MWe because of

limitations on plant site size and a decrease of construction costs per power.

The CP-1300 adopts the core of Korea Standard Nuclear Power Plant(KSNPP)

such as YGN units 3 and 4 PWRs and Ulchin units 3 and 4 PWRs. However, the

number of fuel assembly is increased to reduce power density. The RCS of the CP1300 consists of 2 hot legs and 4 cold legs (2 loop), which is the same as those of

KSNPP and System 80+. Instead of canned motor pumps used in AP600, sealed

pumps are used. A natural circulation loop is installed in the secondary side of

each S/G to achieve passive residual heat removal system(PRHRS). In addition,

2 natural circulation loops serve as passive containment cooling system(PCCS).

The CP-1300 passive safety injection system consists of Passive High-Pressure

Injection System(PHPIS), accumulators, and In-Containment Refueling Water

Storage Tank(IRWST), which are used to supply emergency core cooling water

1
at high, intermediate, and low pressure, respectively. In order to provide RCS

with IRWST water at low pressure, automatic depressurization system(ADS) is

installed.

The PHPIS consists of the core makeup tanks(CMTs) with a sparger and

the pressurizer balancing line. The PHPIS can provide cold water at any RCS

pressure by gravity force because the pressure of the CMT is equilibrated with

the reactor coolant system through lines connecting the inlet of the CMT to the

pressurizer. The major merit of the PHPIS is that it is considered to have a potential to establish a more reliable means to replenish the reactor coolant inventory

without operator's intervention. Despite such a potential of the gravity-driven

injection system, there are few published experimental data showing its thermalhydraulic characteristics, especially the direct contact condensation phenomena

of steam in the CMT. A rigorous study of the effect of direct contact condensation

on the injection of the CMT is required for the design of passive safety injection

system.

RELAP5/MOD3.1 [1] developed at Idaho National Engineering Laboratory (IN

-EL) is a highly generic code to calculate the behavior of a reactor coolant system

during a transient. The application of this code includes analysis required to support licensing audit calculation, evaluation of accident mitigation strategies, and

experiment planning and analysis. However, there is no model in RELAP5 that

can deal with the direct contact condensation of steam in the pool like the CMT.

To simulate the licensing accidents of Passive Advanced Reactors like the CP1300 by using RELAP5, it is essential to develop the condensation regime map

and the model for the interfacial heat transfer coefficients of the direct contact

condensation of steam in the pool. Since the interfacial heat transfer coefficient

for direct contact condensation in the pool is strongly dependent on flow regime,

if the regime can not be identified correctly, it is unlikely that we will produce

2
correct predictions for the associated heat transfer rate. Table 1.1 shows the summary of the condensation regime map related in this study. There is no existing

experimental data concerning the transition criteria between the condensation

regimes when steam is condensed out of the steam pipe exit in the CMT. Unlike

the vent pipe in the BWR suppression pool, the steam pipe is connected to the

CMT, and there is a solid boundary directly connected to the pipe exit which

inhibits the steam bubble moving upwardly along the tubes.

1.2 Objectives and report organization

The present study aims at assessing and improving the analysis capability of the

RELAP5/MOD3.1 on the direct contact condensation in the CMT of the PHPIS.

For this purpose, first the gravity-driven injection experiment is conducted by using a small scale test facility named KARD-I(KAIST Experiments for Advanced

Reactor Development-I) to investigate the effect of the direct contact condensation on the gravity-driven injection and the major condensation modes.

Secondly, the gravity injection experiment is simulated by RELAP5/MOD3.1

to evaluate whether or not it can describe the direct contact condensation occurring in the top of the test section.

The following material is contained in this report. Chapter 2 includes a description of experimental facility and conditions and results. In Chapter 3, a

code description and modeling of the test facility axe described. The calculated

results of base cases are discussed in detail with the experimental data. Also,

the calculated results of sensitivity studies , nodalization study and run statistics

are described in this chapter. Chapter 4 summarizes the conclusions through the

present study. Finally, the RELAP5 input deck and the experimental data are

attached as a Appendix A and B, respectively.

3
Table 1.1: Summary of condensation regime map

author steam pipe water steam mass flux direction regime

diameter(mm) temp.(C) (Kg/sec m2 ) pipe exit shape

Fukuda 8 25-90 0- 350 downward type A chugging

[5] 16.1 vent type B transition

27.6 pipe type C : subsonic jet

type D : osillatory bubble

type E : sonic jet

Chan 51 40- 90 1 - 175 downward chugging

Lee vent oscillatory bubble

[6] pipe ellipsoidal oscillatory bubble

ellipsoidal jet

oscillatory cone jet

I. Aya 9 - 38 0 -100 40 downward chugging

H. Nariai vent condensation oscillation

[71 pipe bubbling

Liang 19.1 50-100 0-50 upward chugging

[8] 10.9 rectangular bubbling

channel subsonic jet

soinc jet

4
External

Water

RCP

Figure 1.1: A schematic diagram of CARR Next Generation Reactor

5
Chapter 2

Gravity-Driven Injection

Experiment

One of the safety concerns is the prevention of the gravity-driven injection because

of a large pressure drop in the top of the CMT resulting from the direct contact

condensation. The direct contact condensation in the top of the CMT is mainly

governed by condensation modes. The objectives of the present experiment axe

to identify the condensation modes to answer which phenomena axe dominant,

and investigate the major parameters governing the gravity-driven injection. To

these ends, a small scale test facility named KARD-I(KAIST Experiments for

Advanced Reactor Development-I) has been constructed, and the experimental

work is in progress.

2.1 Experimental setup and instrumentation

A diagram of the KARD-I is shown in Figure 2.1. It consists of three major parts:

test section simulating the CMT, steam generator simulating the pressurizer, and

the measuring system.

The test section includes a heater, a heater controller controlling the water

6
temperature, front and back visual windows, and drain line as shown in Figure

2.2. The test section is a tank with 85cm height and 65cm diameter. The scaling

ratios of the test section relative to the CMT of AP600 are 1(height ratio) and

'(area ratio), respectively. The visual windows are reinforced glass with 30cm

diameter. Through the visual windows, the phenomena occurring at the exit of

the steam pipe can be observed and recorded by using a high speed camera. To

investigate the vertical temperature distribution of the test section, ten RTDs are

installed along the wall of the tank. The heater has a heating capacity of 8 KW

to control the test condition of water temperature. Filtered water is used as the

working liquid.

The steam generator which functions as a pressurizer is 2 m high, 1 m dia.,

10 mm thick cylindrical stainless steel pipe which is connected to the 12-mm-thick

stainless steel hemisphere. The total volume is 1.332 m3 . The capacity of the

heater is 108 KW. It is located in the lower part of the steam generator in the

horizontal direction to prevent uncovery of the heater. Filtered water is supplied

to the steam generator and the test section by a pump.

The associated piping lines are the steam feed line and the natural circulation

line for hot water from the steam generator. The diameters of these piping lines

are 0.015 m and 0.032 m, respectively. The steam feed line is insulated by an

asbestos to minimize the heat loss. The injection line from the bottom of the test

section has a check valve to prevent air ingress due to a rapid pressure drop.

To measure the chugging boundary, beyond which subcooled water in the

tank rushes periodically into the steam path, a thermocouple is installed at the

exit of the steam feed line. Ten resistance temperature detectors(RTD) are used

for measurement of the vertical distribution of water in the test section. Three

vortex flowmeters made by Omega Co. are used to measure the steam flow rates

from the steam generator, the drain water flow rate from the bottom of the test

7
section, and the natural circulation flow of the hot water from the steam generator. The measurement ranges of the flowmeters are 10- 90kg/mrsec, 0 - 8GPM,

0- 25GPM, respectively. The pressure of the steam generator is measured by the

pressure transducer made by Foxboro Co. The pressure of the test section is measured by two types of pressure transducers made by Foxboro Co. and Omega Co.

The PX176 pressure transducer made by Omega Co. has a frequency response of

10KHz, which is sufficient to measure the pressure oscillation of the test section.

The water level of the test section can be measured by visual observation because

there is a scale on the visual window.

A high speed camera system is used to record the process of the direct contact

condensation in the top of the test section, and after the experiment, it can be

used to analyze the recorded data.

The data acquisition system consists of HP3852A control unit, 10 channel I-V

converter, 8 channel power supply, GPIB card, IBM-PC/AT. The three vortex

flowmeters and the three pressure transducers generate DC current signals which

vary from 4 to 20mA. The DC current signals are changed into the voltage signals

by the I-V converter with 1-5VDC output. The voltage signals from 3 pressure

transducers, 1 thermocouple, 3 vortex flowmeter are read by the HP3852A control

unit through HP44708H multiplexer. The 10 RTDs are read by the HP3852A

control unit through HP44711A high speed multiplexer. Through the GPIB

interface card, these readings are transferred to a IBM-PC/AT and displayed

on the monitor screen dynamically, and restored in the hard disk.

Table 2.1 shows the tag list for the KARD-I instrumentation. This tag list

includes the model number, the measurement range, and the uncertainties of

measuring parts(RTDs, pressure transducers, flowmeters). The uncertainties of

the data acquisition system and I-V converter is 0.1% and 0.1% respectively.

These valves are negligible compared with those of the measuring parts.

8
2.2 Test procedure

The test matrix is listed in Table 2.2. In the first part, three tests(G1021, G1022,

G1023) are conducted to determine the condensation regimes and the effect of

water subcooling on the gravity-driven injection. The forth and fifth tests(GN021, I

GS021) investigated the effects of natural circulation of the hot water from the

steam generator on the gravity-driven injection and the effects of the sparger on

gravity-driven injection, respectively. In the second part, three tests investigated

the effects of the high pressure on the gravity injection.

The test procedure is as follows:

Stepl: The filtered water is filled up to valve V3 .

Step2: The air in the system is initially driven out by the steam generated in

the steam generator. Then valves V1, V2 , V4 are opened, while valve V3 remains

closed(Figure 2.1). To ensure the total purging of the air in the system, this

process is normally continued for two hours. Then the steam generator remains

at atmospheric pressure.

Step3: Valve V4 is closed, and valve V3 is opened. Opening valve V3 allows the

test section and the steam generator to be the same pressure. The water in the

test section is heated to the desired temperature, and simultaneously the steam

generator heater is turned on until the steam generator temperature reaches the

desired value.

Step4: After the test conditions reach the desired point, the data acquisition

system and the high speed camera are started to record the data and the interface

motion at the pipe exit. After 10 sec, valve V6 is opened within a second. During

the test, the power of the steam generator remains at 8KW to compensate the

heat loss of the overall system.

Step5: When the water level drops below the visual windows, the experiment is

9
terminated.

2.3 Experimental results

2.3.1 Effects of water subcooling on gravity-driven injection

Figure 2.3 shows the pressure trend of the top of the test section for test G1021.

As soon as the valve V6 is opened, the pressure of the test section suddenly drops

below atmospheric pressure because the condensation rate is much larger than

the steam supply rate.

Figure 2.4 shows the effects of water subcooling on injection flow rates. At T" =

31CC and T. = 61°C, the test section begins to drain at 1400sec and 2250sec,

respectively. At T, = 91°C, after the valve V6 is open, the injection begins

immediately due to the fast recovery of the pressure drop between the test section

and the steam generator caused by the high water temperature. The result shows

that the lower the water temperature is, the more the initiation of injection is

delayed.

Figure 2.5 shows a transient of the temperature distribution of the test section for

test G1021. As the condensation proceeds, thermal stratification begins to occur

at 1250sec. In the early stage of test G1021, the water temperature measured

at all RTDs increases. After 1250sec, the temperatures of the upper four RTDs

begin to increase, and the rest of RTDs are the constant temperature. It is

observed that before 1250sec, the size of the steam bubble is smaller than 2 cm,

and the pressure oscillation is vigorous. However, after 1250sec, the transition of

the condensation mode begins to occur. At this time,'the size of the steam bubble

is larger than 4 cm, and the pressure oscillation disappears. It can be therefore

stated that the momentum of the steam jet induces circulatinn of the cold water,

10
and as a result, the interaction between the cold water and the steam bubble

promotes the condensation resulting in the pressure drop as shown in Figure 2.3.

When the water begins to inject, the temperatures of the upper four RTDs are

about 80°C. It is certain that the thermal stratification exists between 4th RTD

and 5th RTD because the temperature difference between 4th RTD and 5th RTD

is approximately 300C.

2.3.2 Effects of natural circulation on gravity-driven injection

Recently, the AP600 integral system tests were conducted by using SPES-2 in

Italy [10]. In those experiments, the valves in the CMT balancing line and the

CMT injection line were simultaneously opened after the S-signal. The results

show that the CMT begins to drain, changing from natural circulation operation

to steam displacement. This result also shows that there may be a means to

enhance the CMT injection performance.

To understand the mechanism of natural circulation in the CMT, the experiment(GN021) was conducted. In this experiment, at the same time of Step 4,

valve V5 is opened, which allows a flow between the top of the test section and

the midpart of the steam generator, i.e. natural circulation between two tanks.

Figure 2.6 shows the effects of natural circulation on the injection flow rate.

The result shows that the natural circulation of the hot water from the steam

generator accelerates the injection of the test section.

Figure 2.7 shows a comparison between the natural circulation flow rate and the

injection flow rate. It is observed that the hot water from the steam generator

is jetted into the test section. This is why the trend of natural circulation flow

is oscillatory. Until 650s, the water level does not decrease and the injected

water is compensated by the natural circulation flow from the steam generator.

11
After 650s, the water level of the test section begins to decrease, which means a

transition from natural circulation to steam displacement.

Figure 2.8 shows the temperature distribution in the test section for test GN021.

Thermal stratification does not occur because of the mixing of the hot water.

This result shows that the mixing process of the hot water inhibits the thermal

stratification and promotes the gravity-driven injection.

2.3.3 Effects of the sparger on gravity-driven injection

To investigate the effect of the sparger on the gravity-driven injection, as shown

in Figure 2.2, the sparger is installed 3 cm beneath the exit of the steam feed

line. The sparger is the circular disk with 5 mm thickness and 15 mm diameter.

Figure 2.9 shows the effects of the sparger on the injection flow rate. This result

shows that the sparger promotes the injection of the water in the test section.

Figure 2.10 shows the temperature distributions in the test section for test GS021.

It is observed that the thermal stratification occurs between 80cm and 76cm, and

the momentum of the steam bubble does not reach the region below 76cm because

the sparger changes the vertical direction of the momentum of the steam jet to

the horizontal direction. As a result, all the energy of the steam is transferred to

the upper hot water layer. Thus, the sparger tends to prohibit the energy of the I

steam jet from being transfered to the water below the sparger.

The mechanism of the gravity-driven injection with the sparger is different

from that from the natural circulation. The former is that the sparger reduces

the region affected by the momentum of the steam jet, and all the steam injected

into the tank is used to increase the temperature of the upper hot water layer.

When the temperature of the upper hot layer is about 800C, the water begins to

inject.The hot water from the steam generator tends to promote circulation of all

of water in the test section, and the energy of the hot water and the steam jet

12
is used to increase the temperature of the bulk water in the test section because

the large amount of the hot water from the steam generator is supplied by the

pressure difference.

2.3.4 Effects of the pressure on gravity-driven injection

To investigate the effects of the high pressure on the gravity-driven injection,

experiments(PI041, PN041, PS041) were conducted at 4 bar. Figure 2.11 shows

the effects of the high pressure on the gravity-driven injection. The results show

that the gravity-driven injection at 4 bar is initiated much earlier than that at

1.5 bar because the pressure difference between the test section and the steam

generator at 4 bar is much larger than at 1.5 bar as shown in Figures 2.3 and

2.12. This causes the large steam flow rate and the high increase of the pool

water temperature at 4 bar.

Figure 2.13 shows the effects of the sparger and the natural circulation on the

gravity-driven injection at 4 bar. In the case of the natural circulation, before

500sec, the water level in the test section does not drop because the hot water

from the steam generator compensates the injection flow rate. After 500sec, the

water level begins to drop because the natural circulation flow rate begins to

decrease.

2.3.5 Identification of condensation modes

The condensation identified through the experiments are divided into three modes:

sonic jet, subsonic jet, steam cavity. The sonic jet can be observed at early stage

of G1021 and G1022. Figure 2.14 is the sonic jet having the shape of the inverted

cone. If the water temperature increases and the steam velocity decreases, the

interface of the sonic jet will start to oscillate and collapse at the tip of the cone.

After that, as shown in Figure 2.15, the condensation mode is the subsonic jet in

13
which the bubble grows, is broken into two parts and collapes.

In test G1021, after 1380s, the cylindrical bubble attached to the exit of the

steam feed line as shown in Figure 2.16. This bubble does not collapse but

oscillate vertically. After this mode, the water level begins to decrease. To the

author's knowledge, there has been no research performed to investigate this

mode of condensation. Based on the regime map presented by Chan and Lee [61,

the ranges of the water temperature and steam flow rate including this mode

correspond to oscillatory bubble regime. The characteristics of oscillatory bubble

are that the steam region has expanded to encapsulate part of the pipe and

detachment occurs above the vent exit. The geometry of present experiment has

the solid boundary to inhibit the steam bubble separating from the steam nozzle.

It is believed that this mode may result from the effect of this geometry. This

mode is called steam cavity here.

Table 3 shows the time of the initiation of the water injection and the transition between subsonic jet and steam cavity. When the water injection begins, the

major regime is the steam cavity. When the water in the test section is injected,

the steam cavity mode persists. In the steam cavity mode, the steam injection

rate is larger than the condensation rate through the interface because of the high

water temperature. Then the pressure in the test section builds up to the steam

generator pressure, and after that, the steam begins to displace the water in the

test section during the water injection period. With respect to the condensation

mode, the sparger and the natural circulation cause the reduction of the initiation

time of the steam cavity by 1000sec and 600sec at 1.5bar and 4 bar, respectively.

In these experiments, the chugging mode is not observed. The chugging mode is

known to be observed at low steam mass flux and low water temperature.

14
Before the condensation mode enters the chugging mode, the water temperature

increases beyond the chugging boundary.

15
Table 2.1: Tag list for the KARD-I instrument

Experiment Model no. Measurement Units Instrument Calculated

parameters ranges uncertainty parameters

S/G pressure Foxboro 0- 230 PSIS 1% P-100100000

EllAH

T/S pressure OMEGA 0 - 100 PSIS 1% P-160010000

PX176-10OS5V

Steam flow OMEGA 10 - 90 kg/rn2 sec 5% mflowj-131000000

rate FV-505G

Injection flow OMEGA 0 - 8 GPM 3.6% mflowj-161000000

rate FV-505L

Natural circulation OMEGA 0 - 25 GPM 3.6% mflowj-325000000

flow rate FL-505L

T/S temperature Type 92 -200 - 500 0 1% tempf-160100000

RTD

Water level 1 70 - 85 cm 6% cntrlvav 130

16
Table 2.2: Test matrix

test no Pg(bar) T.(°C) Ti(OC) AT(°C) parameter effect

subcooling effect

GI021 1.5 111.4 31 80

G1022 1.5 111.4 61 50

G1023 1.5 111.4 91 20

GN021 1.5 111.4 31 80 natural circulation

GS021 1.5 111.4 31 80 sparger

high pressure effect

P1041 4.0 144 31 113

PN041 4.0 144 31 113 natural circulation

PS041 4.0 144 31 113 sparger

17
Table 2.3: Transition time between subsonic jet and steam cavity, and injection

time

Transition time (sec) Injection time (sec)

G1021 1380 2250

G1022 432 1400

G1023 15 40

N1021 285 600

SP021 134 750

PI041 1064 1300

PN041 300 470

PS041 240 600

18
Natural circulation line

Figure 2.1: A systematic diagram of test facility

19
Natural circulation line

850 ""

100

200

650

Injection line Heater

controller

Figure 2.2: A systematic diagram of test section

20
1.6

1.5

I

i

---- P1: steam generator

- P3: test section

1.4 1 I.I

1.3

aa1.2 L.

1.1

1.0

0.9

0.8

0.7 A I | i | i • i i 

= | 

= I i I | •

0 500 1000 1500

Time (second)

2000 2500 3000

Figure 2.3: The pressure trend for test G1021
0.5

0.4

Tw=31oC

Tw=61°C

-o-Tw=910 C

0)

M,

2b

0.3 1-

0.2 1

0.1 1-

r

J

0.0 II I ! I I I I i i I i i I I I

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 2.4: The effect of water subcooling on the injection flow rate for test

G1021, G1022, and G1023

22
100 -0- KIu3 Lc) .kIO

-- RTD 4(70cm)

-- RTD 5(60cm) 0

* 80 -o- -+--RTD RTD 6(50cm) 5(0m 01C(

O -x- ~RTD 6(0m

0)C 60-~-RTD 

5(68Cf

80 

T 40 m 20D 

6 5 )

0 60 100 150 200 200 30

Tim (sec))

Fiur 25:Th tmertue isriuio o tstsetonfo7tst(42

23
W

C13

0)

0.40

0.35

0.30

0.25

0.20

0.15

0.10

0.05

0.00

-- W2: no natural circulation(GI021)

-o--W2: natural circulation(GN021)

IrI

--- I

I I

0 500 1000 1500

Time (second)

2000 2500 3000

Figure 2.6: The effect of the natural circulation on the injection flow rate for test

G1021 and GN021

24
0.40

--o--W2: Injection flow rate(GN021)

0.35 in W&: Natural circulation rate(GN021)

0.30

' 0.25

0.20

• 0.15

0

C 0.10

0.05

0.00

I . I ! ,

0 200 400 600 800 1000

Time (second)

Figure 2.7: The comparison of the natural ciculation flow with the injection flow

rate for test GN021

25
RTD 1(84cm)

--- RTD 2(80cm)

-. o- RTD 3(76cm)

--- RTD 4(70cm)

-v- RTD 5(60cm)

--- RTD 6(50cm)

-- +-- RTO 7(40cm)

-x- RTD 8(30cm)

-x- RTD 9(20cm)

100 .

0

0,

1~

(UI....

0)

0.

E

0)

I801-

60 k

40 .

20 . . I . I

0 200 400 600 800 1000

Time (sec)

Figure 2.8: The temperature distribution of test section for test GN021

26
I

0)

M4

(U

0.35

0.30

0.25

0.20

0.15

0.10

0.05

0.00

mom

W2: Without sparger(G1021) I

--a-W'2: With sparger(GS021)

I . I . . I . I

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 2.9: The effect of the sparger on the injection flow rate for test G1021 and

GS021

27
120

100

(D

CD

CL.

E

CD

80

60

40

20

0 200 400 600 800 1000

Time (sec)

Figure 2.10: The temperature distribution of test section for test GS021

28
0.5

0.4

0.3

,- 0 0.2

11

IC 0.1

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 2.11: The effect of the high pressure on the injection flow rate for test

G1021 and PI021

29
!D

IL

4.5

4.0

3.5

3.0

2.5

2.0

1.5

1.0

0.5

--- PI: Steam generator

- P3: Test section

-- I

I I I

0 500 1000

Time (second)

1500

Figure 2.12: The pressure trend for test PI041

30
1.00

0.75 0

SI 0

• a 0)0

0.50

(D

00

00

, 0.25

0.00 ........

0 500 1000 1500

Time (second)

Figure 2.13: The injection flow rate at 4bar for test P1041, PN041, and PS041

31
ffrf

-t

Figure 2.14: Sonic jet

32
.4'

Figure 2.15: Subsonic jet

33
F 2v

Figure 2.16: Steam cavity

34
Chapter 3

Assessment of RELAP5/MOD3.1

3.1 Description of code and modeling

The RELAP5 code has been developed as one of the best-estimate codes. The

code is based on a non-homogeneous and non-equilibrium model for one dimensional, two-phase system that is solved by the semi-implicit numerical scheme

to permit efficient evaluation of system transients. Recently, RELAP5/MOD3.1

code development program has been initiated to develop a code version suitable for the analysis of new safety system of passive advanced reactors like the

CMT in the CNGR. However, there is no model in RELAP5/MOD3.1 that can

deal with the direct contact condensation of steam in the pool like the CMT.

To simulate the accidents of passive advanced reactors like the CNGR using RELAP5/MOD3.1 , it is essential to develop the condensation regime and the model

for the interfacial heat transfer coefficients of the direct contact condensation of

steam in the pool. In this code assessment, RELAP5/MOD3.1 is mainly used,

and standard RELAP5/MOD3.0 without any modification is used to compare

with the results of the released version of RELAP5/MOD3.1.

RELAP5 nodalization used to simulate the graVity-driven injection experiment is represented in Figure 3.1. The model is based on 43 volumes connected

35
by 43 junctions and 3 heat structures for the electric heater. For other volumes

except the electric heater, the heat structure are not installed because the power

of the steam generator remains at 8KW to compensate the heat loss of the whole

system during the test. The steam generator is modeled by pipe component

(100) having 10 volumes. The heaters in the steam generator are modeled by

heat structure having the power of 100 kw. The steam feed line between the test

section and the steam generator is modeled as a single volume component (101),

pipe components (110,120,130). The natural circulation line between the test

section and the hot water of the steam generator is modeled as a branch component (310), pipe components (320, 330, 340). The injection valve is modeled

as a servo valve component (161). At 10 sec, this valve is opened within 1 sec.

The water injection line is modeled by pipe components (170,180). When the

injection valve is opened, the water drains to the atmosphere which is model as a

time dependent volume(200). If the large pressure drop occurs in the test section,

there exists the possibility for air to enter the test section through the injection

line. To prevent this, We installed a very large backward form loss coefficient as

check valve in SJ171.

3.2 Analysis results and discussion

3.2.1 Base case

For base case calculations, tests G1021, GN021, PI041 and PN041 are simulated

by RELAP5/MOD3.1 to determine whether or not it can describe the direct

contact condensation occurring in the top of the test section. In addition, the

results simulated by RELAP5 show different trends for different nodalization.

The results show that the 1-node model of the test section predicts better the

experimental data than the multi-node models [3]. In the base case calculations,

36
the 1-node model of the test section is used. The transient was initiated at 10 sec

by opening the valve V101. The results of the simulation are compared with the

experimental data in Figures 3.2 through 3.7. The following main characteristics

are found:

* The calculated steam generator pressure is lower than that of the experimental data as shown in Figure 3.2. However, the code predicts the steam

generator pressure transient for natural circulation(GN021 and PN041) relatively better than those for no natural circulation test(G1021 and P1021).

These results show the code better represents the depressurization due to

the steam condensation with natural circulation than that without natural

circulation.

* As shown in Figure 3.3, in the case of no natural circulation(test G1021

and P1021), the calculated test section pressures overpredict the experimental data. However, the code underpredicts the experimental data of

the natural circulation(test GN021 and PN021). Those results show that

RELAP5/MOD3.1 overpredicts the pressure variations without natural circulation but underpredicts the pressure variation with natural circulation.

* As shown in Figure 3.4, the water temperature of the test section is overpredicted for the experiment with no natural circulation(G1021 and P1021).However,

for the experiments with natural circulation, an underprediction is found.

These results show that in the case of no natural circulation, RELAP5/MOD3.1

overpredicts the amount of the steam condensation without the hot water

mixing, and in the case of natural circulation, it underpredicts the amount

of the steam condensation with the hot water mixing. It is consistent with

the results of the steam generator pressure.

37
" RELAP5/MOD3.1 underpredicts the experimental data of the steam flow

rates due to the underpredictions of pressure difference between the steam

generator and the test section. In the case of natural circulation(GN021)

as shown in Figure 3.5, after 600sec the experimental steam flow rapidly

decreases, but the predictions smoothly decrease because an increase of the

water temperature due to the steam condensation and the hot water mixing

make the pressure of the test section increase.

" As shown in Figure 3.6, RELAP5/MOD3.1 well predicts the time of the

injection initiation, but it does not well predict the amount of the injection

flow. In the case of test GN021, RELAP5/MOD3.1 shows high oscillation

in the injection flow rate because the predictions of the test section pressure

and the natural circulation flow rate show highly oscillatory behavior.

" The comparison of the water level between the experimental data and the

calculated results shows that at 4 bar the code better predicts the experimental data than those at 1.5 bar as shown in Figure 3.7.

3.2.2 Sensitivity study

Sensitivity studies were performed with two RELAP5 code versions (MOD3.0 vs

MOD3.1). The results of the sensitivity studies are compared with the experimental data as shown in Figures 3.8 through 3.12. The following main characteristics

are found:

* As shown in Figure 3.8, MOD3.1 better predicts the experimental pressure

than does MOD3. Figure 3.8(b) shows that MOD3.0 don't predict the pressure drop in the test section at all. Since the pressure difference between the

steam generator and the test section predicted'by MOD3.0 is smaller than

that of MOD3.1, the steam flow rate and the test section water temperature

38
of MOD3.0 are lower than those of MOD3.1. These results show that the

amount of the condensation in the test section predicted by MOD3.0 is less

than that of MOD3.1.

o The comparison of the water level between the experimental data and the

calculated results shows that although the predictions are in poor agreement

with experimental data, MOD3.1 better predicts the experimental data

than does MOD3.0. Both MOD3.0 and MOD3.1 predict the flow regime of

the test section as vertical stratification. Both codes use the same interfacial

heat transfer correlation for the vertical stratification regime. The reason

MOD3.1 shows better agreement with the experimental data than does

MOD3.0 is currently unknown. The flow regime observed in the experiment

is the subsonic jet having the vertical cone shape. This is why the results

of RELAP5/MOD3.1 is in poor agreement with the experimental date. For

better prediction of the direct contact condensation in the CMT , it is

essential that a new correlation for the interfacial heat transfer coefficient

be developed.

3.2.3 Nodalization study

A nodalization study was performed to investigate the effect of the number of

nodes in the test section(1 node, 2 nodes, 3 nodes). The results from the nodalization study are compared with the experimental data in Figures 3.13 through

3.17. The following main characteristics are found:

a The calculated pressures of the steam generator and the test section are in

poor agreement with the experimental data for all nodalization schemes.

These results show that the current models of RELAP5 can not produce

sufficiently accurate predictions for the pressures of the steam generator

39
and the test section. The basic reason for such an inaccuracy is considered to results from the poor predictions of the amount of condensation by

RELAP5/MOD3.1.

9 As shown in Figure 3.14, the results of the 1-node model well agree with the

experimental data until 1500sec. After 1500sec, the experimental tank temperature increases because of a decrease in the water level. It is shown that

the larger the number of nodes, the higher the water temperature. Since

RELAP5/MOD3.1 calculates the node average temperature, the component having the small volume reaches the saturation temperature faster

than that of the large volume. In the 1-node model, a higher amount of

condensation is predicted than in other models.

* The comparisons of the steam flow rate and the injection flow rate between

the experimental data and the calculated results show that all the models

underpredict the steam flow rate, but the 1-node and 2-node models have

trends similar to the experimental data.

* Figure 3.17 shows the comparison of the water level between the different

models and the experimental data. The results show that 1-node and 2-node

models have trend similar to the experimental data. In the nodalization

study, the results of the 1-node model are in better agreement with the

experimental data than those of the other models.

3.2.4 Run statistics

The primary computer used in the calculation is a SUN SPARC 10 with SunOS

4.1.3-KL operating system. The random access memory is 32 Mbyte. The calculation speed is 86.1 MIPS. The clock speed of CPU is 36 MHz.

40
Figures 3.18 shows the required CPU time and time step size with respect to

the real transient time for the base case run. As shown in the figure, the slope

of the CPU time become steep as the injection valve is opened, and the time

step size is reduced down to 0.00075. Table 3.1 shows the grind time of each

calculation. The grind time of G1021-MOD3.0 has the lowest value because the

transient is mild due to a decrease in the interaction between steam and water

resulting from a rapid decrease in the water level of the test section. The grind

times of natural circulation experiments, such as GN021 and PN041, have larger

values than the other calculations because of the oscillatory natural circulation

flow and the coexistence of steam, cold water, and hot water. In the cases of

G1021-3-node, G1021-MOD3.0 and GN021, the transients are terminated by the

generation of thermodynamic property error.- This error is an inherent weakness

of RELAP5 which occurs when the steam exists in the subcooled water at the

low pressure. In the case of test G1021, the grind time is as follow:

CPU time = 58333.9 sec

Number of time steps- = 914360

Number of volumes = 28

Grind time = 2.2785

41
Table 3.1: Grind time

test Real time CPU time Number of Number of Grind time Termination

(second) (second) time step volume stutus

G1021-1node 2600 58333.9 914360 28 2.2785 time control card

G1021-2node 2600 60692.2 908476 29 2.3037 time control card

G1021-3node 1950 56751.6 779543 30 2.4267. failure

G1021-MOD3.0 458.6 3402.32 72822 28 1.6686 failure

GN021 753 46887.7 449086 43 2.428 failure

PI041 1600 121665 2002225 28 2.1702 time control card

PN041 660 87906.9 847921 43 2.411 time control card

42
SJ131 -Geneator

04

03

160

Test 0 33-1 1

Section

Natural Circulation line

V161

170

01 S11 Water Draining Line

Figure 3.1: A systematic diagram of kELAP5 nodalization

43
150000

(a) G1021 140000

-. 130000 CO

. 120000

- 110000

(/AU)

0)100000

90000

80000

(b) GN021 145000

140000

CC 135000 0..

130000

C 125000

120000

115000

(c) P1041 400000

350000

CL 300000

. 250000

200000

C, 150000

I

- RELAPSIMOD3.1: p-100100000

- Experimental data: P1

Ii

0 500 1000 1500 2000 2500 30( time(sec)

0.5w0'e 1..

0 250 5'00 750 101

)0

00

1UUUUU I I

0 500 1000 1500

(d) PN0414 °

0

000

M 360000 0.

' 320000

S280000 (L•

240000

0 250 500 750

Figure 3.2: Comparison of the steam generator pressure between experiments

and calculation

44
(a) GI021

SI..

160000

120000

80000

40000

0

(b) GN021 160000

a. 120000

80000 U)

U)

S.. 4O0

CL 40000

(c) P1041 400000

300000 tu

0~

200000 5) 

100000

0

500000

(d) PNO41 400000

0Q. 300000

200000 In

CL 100000

0

-RELAPS/MOI3.1: p-160010000

E~erkimental data: P3

0 500 1000 1500 2000 2500 3000

Time (second)

r I

o 250 500 750 1000

0 500 1000 1500

a 250 500 750

Figure 3.3: Comparison of the test section pressure between experiments and

calculation

45
(a) G1021

cc

E

(b) GN021CL

E)

E

I--

I - RELAP5=MOO3.1: temf-160010000

.. Experimental data

320

300 ,

0 500 1000 1500 2000 2500 3000

Time(second)

400

(c) P1041

380

360

L.340

0. E

E 320

300

0 500 1000 1500

(d) PN041 4'0

380

360

: 340

CCX

E 320

300:=,t

0 250 500 750

Figure 3.4: Comparison of the pool water temperature between experiments and

calculation

46
IJ.uo

(a) G1021 RELAPSh¶OD3.1: mftowj-131000000

Expethnental data: WI

0.06 -

W

0)U)

0.04 1

0.02 1

0.00 L

A Ai' #

0 500 1000 1500 2000

Time (second)

2500 3000

(b) GNO21

C)

Figure 3.5: Comparison of the steam flow rate be'tween experiments and calculation

47
(a) G1021

0

0

U)

(b) GN021_

0

C4

(b) p1041

0

&n

oA

0)l

0.2

0.1

0.0

-0.1

-0.2

- ~Tr~!I4 ~

I RELAPS/M003.1: mflowj-161000000

.. Experimental data: W2 I

0 500 1000 1500 2000 2500 3000

Time (second)

0.4

0.3

0.2

0.1

0.0

-0.1

0 250 500 750 10(

0.6

0.4 ......

0.2 - .

0.0 "

-0.2

-0.4,

O0

0 500 1000 1500

(d) B PN041

1.0

0.8

0.4 . ............................-.........

0.2

0.0

U) u) -0.2

CU -0.4

0 250 500 750

Figure 3.6: Comparison of the injection flow rate between experiments and calculation

48
(a) GI021

E

(b) GN021

E,

0.86

0.84

0.82

0.80

0.78

0.76

0.85

0.80

0.75

0.70

0.65

Exeimna daa wae level 1 =

0 500 1000 15oo 2000 2500 300

Time (second)

0 250 500 750 1000

0 500 1000 1500

a0

(c) P1041 0.o

0.85

0.80

0.75

0.70

0.65

(d) PNO41

E

0.90

0.85

0.80

0.75

0.70

0 250 500 750

Figure 3.7: Comparison of the water level between experiments and calculation

49
(a) steam generator 150000.

CL

140000

130000

120000

110000

100000

RELAPS/M003.1

90000

98000000

160000

140000

120000

o 100000

( 80000

U) 60000

n. 40000

0 500 1000 1500 2000 2500 3000

Time (second)

(b) test section

-V

20000

0

I I i i I i I I g I I

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 3.8: Comparison of the pressure of the steam generator and the test section

between test G1021 and calculation(MOD3.0 vs MOD3.1)

50
3501- RELAP5/MOD3.0

-RELAP5/MOD3.1

........ Experimental data

I

I AI-./ 3401-

0)

I-

.4-

L.

U,

E

U) I3301-

3201-

310 1

300 2 I I I

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 3.9: Comparison of the pool water temperature between test G1021 and

calculation(MOD3.0 vs MOD3.1)

51
0.05

0.04

--- RELAP5/MOD3.0

-RELAP5iMOD3.1

- - Experimental data

(0

0.03 I

0.02 .

0.01 1.

0.00

-0.01 I I I = I a I a I I I I

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 3.10: Comparison of the steam flow rate between test G1021 and calculation(MOD3.0 vs MOD3.1)

52
0.5

0.4

RELAP5/MOD3.0

R ELAP5/MOD3.1

I xExperimental d ataI

Ca

M4-

0.3 I

0.2

0.1 I

0.01-

-0.1

-0.2

-0.3 I i |

0I 0 ,, 1 00 500 1000 I . . P

1500 2000 2500 3000

Time (second)

Figure 3.11: Comparison of the injection flow rate between test G1021 and calculation(MOD3.0 vs MOD3.1)

53
0.9

0.8 .

0.71-

E.

CU

.0:

0.6 .

0.5 1

0.4 1

--- RELAP5/MOD3.0 I -RELAP5IMOD3.1

........ Experimental data

0.3 I

ll]ll -

0.2

- . I ~

500 1000 1500 2000 2500 3000

Time (second)

Figure 3.12: Comparison of the water

tion(MOD3.0 vs MOD3.1)

level between test G1021 and calcula54
150000

140000

130000

. 120000

I.-

110000

. 100000

90000

80000

160000

140000

120000

' 100000

U) i a) 60000

Time (second)

ýWvvv

20000

0

I I I I I B I I • I

0 500 1000 1500

Time (second)

=

2000 2500 3000

Figure 3.13: Comparison of the pressure of the steam generator and the test

section between test G1021 and calculation(Nodalization study)

55
360 - IUUW II iUU,

2 node model

350.3 node model

350 - o Experimental data

340

vI

a)

330 ,

CL

I-- 320

310

300 , 0 500 1000 1500 2000 2500 3000

Time(sec)

Figure 3.14: Comparison of the pool water temperature between test G1021 and

calculation(Nodalization study)

56
0.08

0.06

0.04 I'

-4 0.02

.• 0.00

o -0.02 -

M -0.D4 - -I node

---- 2 node

...-- 3 node -0.06 a Experimental data

-0.08 • . ... . - , • , •

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 3.15: Comparison of the steam flow rate between test G1021 and catculation(Nodalization study)

57
0.3

0.2

0

'S

0)

C13

43;

0.1

0.0

-0.1

-0.2

-0.3

0 500 1000 1500 2000 2500 3000

Time (second)

Figure 3.16: Comparison of the injection flow rate between test G1021 and calculation(Nodalization study)

58
0.90

0.85

0.80

E 0.75

a 0.70

0.65

0.60

0.55

0 500 1000

Tin

Figure 3.17: Comparison of the

tion(Nodalizationstudy)

1500 2000 2500 3000

ne (second)

water level between itest G1021. and'calcula59
80000

E

CD

60000

40000

20000

0 0 I , I I 24 

0 500 1000 1500 20

Time(second)

00 2500 3000

0.12

0.10 L

(A

S0.08

(D

E 0.06

P.O.00

£0.o

.E 0.02

I1-

U.UU.

0 500 1000 1500 2000 2500 3000

Time(second)

0

0)

(D

E.

0.10

0.08

0.06

0.04

0.02

0.00

a

0

a

0

9 . . . . S

0 0.00 0.02 0.04 0.06 0.08 0.10

User specified maximum time step(second)

Figure 3.18: CPU time, time step size versus transient time and code determined

time step versus user specified maximum time step

60
Chapter 4

Conclusions

The RELAP5/MOD3.1 was assessed using the small scale gravity injection experiment simulating direct contact condensation in the CMT of the PHPIS. For

this assessment, a gravity injection experiment was conducted in the small scale

test facility, KARD-I to identify the parameters governing the gravity injection

and the major phenomena. To evaluate the code predictability of the direct contact condensation in the CMT, the calculated results were assessed and compared

with the experimental data. From the present study, the following conclusions

were obtained:

* The lower the water temperature, the longer the initiation time of injection

is delayed. The results show that the sparger and the natural circulation

from the hot water in the steam generator accelerate the injection of the

test section. The condensation modes identified through the experiments

are divided into three modes: sonic jet, subsonic jet, and steam cavity. The

steam cavity is a unique mode of downward injection with a solid surface

directly connected to the pipe exit not seen in other experiments.

e In the base case study, RELAP5/MOD3.1 predicts better the experimental

water level at 4 bar than those at 1.5 bar. However, the calculated results

61
are not in good agreement with other experimental data, such as the pressures of the steam generator and the test section, the pool temperature, the

flow rate of steam and injection, the test section water level.

" Sensitivity studies were performed with two RELAP5 code versions(MOD3.0

and MOD3.1). Although both codes do not predict precisely the experimental data, the results from RELAP5/MOD3.1 are in better agreement with

the experimental data than those of RELAP5/MOD3.0. Both MOD3.0 and

MOD3.1 identify the flow regime of the test section as vertical stratification, whereas the experimental flow regimes were sonic jet or subsoinc jet

according to steam flow.

" From a nodalization study of RELAP5/MOD3.1, the 1-node model shows

better agreement with the experimental data than other multi-node models. However, considering the penetration depth of the jetting, the proper

number of nodes of the CMT still remains to be determined.

" To reproduce direct contact condensation in the CMT with RELAP5/MOD3.1, I

it is necessary that new correlations for the interfacial heat transfer coefficients be developed. They should have a capability to capture the physical

process of the direct contact condensation in the CMT.

62
Bibliography

[1) C. D. Flether, et al, RELAP5/MOD3 Code Manual, NUREG/CR-5535,

EGG-2596, August, 1991.

[2] T. Yonomoto, et al, Passive Safety Injection Experiment at the ROSA-V

Large Scale Test Facility, NURETH-5, 1992.

[3] Lee, Gyu Cheon, Effects of a Steam Jetting Mode on the Safety Injection of

the Core Makeup Tank, KAIST, MS Thesis, 1994.

[4] Y. Murao, et al, Outline of Emergency Coolant Injection System and Preliminary Test for Core Makeup Tank of JPSR, J. Atomic Energy Soc. Japan(in

Japanese) Vol.24, No.5, 1982.

[5] S. Fukuda, Pressure variation due to vapor condensation in liquid (II), J.

AESJ, Vol.24, No.6, 1982.

[6] C. K. Chan, et al, A Regime map for direct contact condensation, Int. J.

Multiphase Flow Vol.8, No.d, pp.11-20, 1982.

[7] 1. Aya and H. Nariai, Boundaries between regimes of pressure oscillation

induced by steam condensation in pressure suppression containment, Nucl.

Eng. Des, Vol.99, pp.31-40, 1981.

63
[8] Kuo-Shing Liang, et al, Experimental and Analytical Study of Direct Contact Condensation of Steam in Water, Nucl. Eng. Des, Vo1.147, pp.425-435,

1994.

[9] Frank, R. Cheslak, et al, Cavities formed in liquid surfaces by impinging

gaseous jets, J. Fluid Mech, vol.36, pp.55-63, 1969.

[10] M. Bocchiai, et al, SPES-2 AP600 integral system test inadvertent ADS

opening and cold leg break transient, European Two-Phase Flow Meeting,

1994.

[11] M. E. Simpson, et al, Hydrodynamics of a subsonic vapor jet in subcooled

liquid, J. of Heat transfer, Vol.104, pp.271-278, 1982.

64
Appendix A : Input Decks

1) G1021-1 node model

=RELAP5/MOD3.1 CMT 1 Nodes

*test G1021 simulation

*CMT node : 1 node

*water valve: 10sec. opened

*job cards

100 new transnt

101 run

110 air

*time step cards

201 10.0 1.0e-12 0.1

202 20.0 1.0e-12 0.005

203 1950. 1.0e-12 0.1

204 2000. 1.0e-12 0.01

205 2600. 1.0e-12 0.1

*minor editor cards

3 10 100 100

3 200 1000 1000

3 10 2500 2500

3 100 5000 5000

3 10 2500 2500

335 mflowj

336 mflowj

355 vapgen

358 vapgen

359 vapgen

360 vapgen

361 vapgen

362 vapgen

363 vapgen

364 floreg

365 floreg

366 floreg

367 floreg

368 floreg

369 floreg

372 floreg

373 floreg

374 tempg

377 tempg

378 tempg

379 tempg

380 tempg

383 satterp

386 sattemp

387 sattemp

388 sattemp

389 sattemp

160010000

170010000

180010000

110010000

120010000

130010000

130020000

110010000

120010000

120020000

130010000

130020000

160010000

170010000

180010000

160010000

100100000

110010000

120010000

130010000

160010000

100100000

110010000

120010000

130010000

171000000

181000000

* CMT - node I

301 tempf

311 p

312 p

313 p

314 tempf

315 tempf

316 tempf

317 tempf

318 tempf

319 voidg

322 voidg

323 voidg

324 voidg

325 voidg

326 voidg

327 voidg

328 mflow*

329 mflowj

330 mflowj

331 mflowj

332 mflowj

334 mflowj

160010000

100100000

130050000

160010000

* CMT - node I

130020000

120010000

120020000

100050000

100010000

160010000

130010000

130020000

120010000

110010000

100100000

100050000

130040000

111000000

121000000

131000000

161000000

170010000

392 cntrlvar 130 * condensate level, frac.

* CMT - node 1

20800001

20800002

20800003

20800004

20800005

20800006

20800007

2OOOO

hif

hif

hif

hif

hif

hif

hif

160010000

170010000

180010000

110010000

120010000

.130010000

130020000

* CMT - node 1

20800008 hig

1

20800009 hig

20800010 hig

20800011 big

20800012 big

20800013 big

160010000 * CMT - node

170010000

180010000

110010000

120010000

130010000

65
20800014 hig 130020000

*condensate levelfraction

20513000 con-lvl sum 1.0

20513001 0.0 0.85 voidf

0.0 1

160010000

*** ******* *** ** *** *** ***   ** **   ** *** *

*hydrodynamic data

*component 100 : pipe ( steam generator )

1100102 0.00049 3

*1100201 0.00049 2

1100301 0.22 1

1100302 0.90 3

1100401 0.0 3

1100601 0.0 3

1100801 0.000046 0.0 3

1100901 0.30469 0.30469 2

1101001 00000 3

1101101 000100 1

1101102 000000 2

1101201 002 1.4300e5 1.0

1101300 1

1101301 0.0 0.0 0.0 2

*junction 111 : single junction

*

0.0 0.0 0.0 3

1000000 sgtank

1000001 10

1000101 0.0

1000102 0.78540

1000103 0.0

1000301 0.205

1000401 0.02197

1000402 0.0

1000403 0.02197

1000601 90.0

1000801 0.00004E

1001001 00000

1001101 000000

1001201 002 1

1001202 002 1

1001203 002 1

1001300 1

1001301 0.0 0.

pipe

1

9

10

10

1

9

10

10

0.0

10

9

.430e5

.430e5

.430e5

1110000 vortexm sngljun

1110101 110030002 120010001 0.0

000100

1110201 1 0.0 0.0 0.0

0.75 0.75

*component 120 : pipe (horizontal pipe above SG)

10

0.0

0.5

1.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

4

5

10

0 0.0 9

*branch 101 : branch (from S/G to horizontal pipe)

1200000 horzp2 pipe

1200001 3

1200101 0.00015 3

1200301 0.17 1

1200302 0.84 3

*1200501 90.0 1

*1200502 0.0 3

1200601 0.0 3

1200801 0.000046 0.0

1200901 0.75 0.75 1

1200902 0.0 0.0 2

1201001 00000 3

1201101 000000 2

1201201 002 1.4300e5

1201300 1

1201301 0.0 0.0 0.0

3

1010000 sgjup branch

1010001 2 1

1010101 0.00126 0.34

1010102 0.0 00000

1010200 002 1.4300e5

1011101 100100002

0.49920 000100

1011201 0.0 0.0 0.0

1012101 101010002 11

000100

1012201 0.0 0.0 0.0

1C

0. 0. 90. 0.34 0.000046

1.0

01010001 0.00126 0.49920

)010001 0.00126 0.57 0.57

1.0 0.0 0.0 0.0 3

2

*junction 121 single junction

1210000 pipl snglun

1210101 120030002 130010001 0.00015

000000

1210201 1 0.0 0.0 0.0

*component 110 : pipe (horizontal pipe above SG)

1100000 horzpl pipe

1100001 3

1100101 0.00126 1

0.75 0.75

*component 130 : pipe (vertical pipe above CMT)

66
1300000 vertpip pipe

1300001 5

1300101 0.00015 5

1300301 0.204 5

1300401 0.0 5

1300601 -90.0 5

1300801 0.000046 0.0

1301001 00000 5

1301101 000000 4

1301201 003 1.4300e5

5

*junction 161 : valve junction (valve below CMT)

1610000 dowvv valve

1610101 160010002 170(

1.75 000100

1610201 1 0.0 0.0 0.0

1610300 srvvlv

1610301 120

010001 0.00071 1.75

5

304.0 0.0 0.0 0.0

*component 170 : vertical pipe below CMT

*1301202 002 1.4300e5 0.66

4

*1301203 003 1.4300e5 304.

0.0 0.0 0.0

0.0 0.0 0.0

5

1301300 1

1301301 0.0 0.0 0.0 4 *

*junction 131 : junction from vertical pipe to the

cmt

1700000 belopipl pipe

1700001 2

1700101 0.00071 1

1700102 0.00015 2

1700301 0.30 1

1700302 0.12 2

1700401 0.0 2

1700601 -90.0 2

1700801 0.000046 0.0

1700901 0.3750 0.3750

1701001 00000 2

1701101 000100 1

1701201 003 1.013e5

1701202 003 1.013e5

1701300 1

1701301 0.0 0.0 0.0

1310000 cmtjun sngljun

1310101 130050002 160010001

0.99945

1310102 000100

1310201 1 0.0 0.0 0.0

*volume 160 : single volume

1600000 cmt snglvol

1600101 0.32170 0.85 0.0

0.000046

1600102 0.0 00000

1600200 003 1.4300e5 304.27

*component 160 : pipe (cmt)

0.00015 0.99945

293. 0.0 0.0 0.0

293. 0.0 0.0 0.0

1

2

*junction 171 : junction between vertical and

0.0 -90. -0.85 horizontal pipes

1710000 beljun sngljun

1710101 170020002 1I

1000.75

1710102 000100

1710201 1 0.0 0.0

80010001 0.00015 0.75

0.0

*1600000 cmttank pipe

*1600001 2

*1600101 0.32170 2

*1600301 0.425 1

*1600302 0.425 2

*1600401 0.0 2

*1600601 -90.0 2

*1600801 0.000046 0.0

*1601001 00000 2

*1601101 000000 1

*1601201 003 1.4300e5

*1601300 1

*1601301 0.0 0.0 0.0

*component 180 : horizontal pipe below CMT

1800000 belopip2 pipe

1800001 2

1800101 0.00015 2

1800301 1.0 2

1800401 0.0 2

1800601 0.0 2

1800801 0.000046 0.0 2

1801001 00000 2

1801101 000000 1

304.0 0.0 0.0 0.0 2

67
1801201 004 1.013e5 293. 0.0 0.0 0.0 1

1801202 004 1.013e5 293. 0.0 0.0 0.0 2

1801300 1

1801301 0.0 0.0 0.0 1

*junction 181 : junction to atmosphere

*11600100

*11600101

*11600201

*11600301

*11600400

**11600401

*11600501

*11600601

1

*11600701

*11600801

1.0 1

*11600901

1.0 1

0 2

0.0225 2

5 2

0.0 2

0

288.0 3

160010000

0

1 1 0 0.32170 1

0 0 1 0.32170

1810000 atmjun sngljun

1810101 180020002 200000000

1.75

1810102 000100

1810201 1 0.0 0.0 0.0

*

*component 200 : atmosphere

0.00015 1.75 0

0.0

0.0 0.0 0.0 1

10.0 10.0 10.0 10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

* cmt (1160-1)

2000000 air

2000101 0.0

2000102 0.0

2000200 004

2000201 0.0

tmdpvol

100.0 1000.0 0.0 0. 0.

0.0 00

1.013e5 293.0 0.0

*11601000

*11601100

*11601101

*11601201

*11601301

**11601400

*11601401

*11601501

*11601601

*11601701

*11601801

1.0 10

*11601901

1.0 10

10 3 2 1 0.32

0 2

0.0025 2

5 2

0.0 2

0

288.0 3

160010000 10000 1 1

0 0 0 1

0 0.0 0.0

0.0 10.0 10.0 10.0

*valve control

0.085 10

0.085 10

0.0 10

10.0 0.0 0.0

20512000 vlvarea function 1.0 0.0 0

20512001 time 0 003 0.0 10.0 10.0 10.0 10.0 0.0 0.0

* SG (1100)

*valve table

20200300 normarea

20200301 0.0 0.0

20200302 10. 0.0

20200303 10.01 1.0

20200306 10000. 1.0

* heat structure input

*11000000

*11000100

*11000101

*11000201

*11000301

*11000400

**11000401

*11000501

*11000601

*11000701

*11000801

1.0 10

*11000901

1.0 10 *

10 3 2 1 0.5

0 2

0.006 2

5 2

0.0 2

0

373.14 3

100010000 10000 1 1 0.205 10

0 0 0 1 0.205 10

0 0.0 0.0 0.0 10

0.0 10.0 10.0 10.0 10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

* cmt (1160)

*11600000 1 3 1 1 0.0 *

68
***   ** * **** **** *•*******   ** ** **

* heat structure input for electric heater

11005000 3 4 2 1 0.0

11005100 0 2

11005101 0.0015 2 0.001 3

11005201 11 2 5 3

11005301 1.0 2 0.0 3

11005400 0

11005401 384.4 4

11005501 0 0 0 1 36.0 3

11005601 100010000 10000 1 1 36.0 3

11005701 10212 1.0 0.0 0.0 3

11005901 0.0 10.0 10.0 10.0 10.0 0.0 0.0 1.0

3

* power table

20100552

20100553

20100554

20100555

20100556

20100557

20100558

20100559

20100560

20100561

(w/m.k)

20100501

20100502

20100503

20100504

20100505

20100506

20100507

20100508

20100509

20100610

20100511

20100512

.3109278e+03

.3664834e+03

.4220389e+03

.4775945e+03

.5331500e+03

.5887056e+03

.6442611e+03

.8109278e+03

.9220389e+03

1.9220389e+03

.3831330e+07

.3985580e+07

.4105300e+07

A224090e+07

.4308800e+07

.4359790e+07

.4410320e+07

.4561910e+07

.4625250e+07

.4625250e+07 *

temp (k) thermal conductivity

*20221200

*20221201

*20221202

*20221203

*20221204

power 501

-1. 0.0

0. 1.0

100. 1.0

1000. 1.0

1. 100000.0

.2732611e+03

.2942611e+03

.3109278e+03

.3664834e+03

A220389e+03

.4775945e+03

.5331500e+03

.5887056e+03

.6442611e+03

.8109278e+03

.9220389e+03

1.9220389e+03

.1489124e+02

.1489124e+02

.1505739e+02

.1609584e+02

.1696813e+02

.1800657e+02

.1885809e+02

.1956423e+02

.2041575e+02

.2297030e+02

.2423029e+02

.2423029e+02

20100500 tbl/fctn 1 1 * s - steel

20101100 tbt/fctn 1 1* PZR heater (MgO)

* MgO (011)

****** *** ***•* **** ** ****** ****** *** ***

*

* heater control

(jl/r3.k)

20101151

20101152

20101153

20101154

20101155

temp (k) volumetric heat capacity

0.293e+03

0.450e+03

0.800e+03

1.120e+03

1.922038e+03

.26000000e+07

.28350000e+07

.34020000e+07

.37260000e+07

.37260000e+07

20521200 heater constant 0.0

end of file

temp (k) thermal conductivity (w/m.k)

20101101

20101102

20101102

0.29320e+03

1.27320e+03

1.9220389e+03

81.40

100.47

100.47 *

* stainless steel (005) 18cr-8ni

(/:m3.k)

20100551

*20100551

temp (k) volumetric heat capacity

.2742611e+03

.2942611e+03

.3831330e+07

.3831330e+07

69
2) G1021- 2 node model modification

*component 160 : pipe (cmt)

1600000 cmttank pipe

1600001 2

1600101 0.32170 2

1600301 0.425 1

1600302 0.425 2

1600401 0.0 2

1600601 -90.0 2

1600801 0.000046 0.0

1601001 00000 2

1601101 000000 1

1601201 003 1.4300e5

1601300 1

1601301 0.0 0.0 0.0

1600101 0.32170 3

1600301 0.2833 1

1600302 0.2833 2

1600303 0.2833 3

1600401 0.0 3

1600601 -90.0 3

1600801 0.000046 0.0 3

1601001 00000 3

1601101 000000 2

1601201 003 IA300e5 304.27 0.0 0.0 0.0 3

1601300 1

1601301 0.0 0.0 0.0 2

304.27 0.0 0.0 0.0 2

3) G1021- 3 node model modification

*component 160 : pipe (cmt)

*

1600000 cmttank pipe

1600001 3

70
4) GN021

=RELAP5/MOD3.1 CMT 1 Nodes

* GN021 simulation

* CMT node : 1 node

* water valve: 10sec. opened

* natural circulation line v/v : 10sec. opened

*job cards

100 new transnt

101 run

110 air

*time step cards

201 10.0 1.Oe-12 0.1

202 20.0 1.Oe-12 0.005

203 40.0 1.Oe-12 0.1

204 60.0 1.Oe-12 0.005

205 1000.0 1.0e-12 0.1

*minor editor cards

3

3

3

3

3

10

100

10

100

10

100

500

100

500

2500

100

500

100

500

2500

301 tempi

311 p

312 p

313 p

314 tempf

315 tempf

316 tempf

317 tempf

318 tempf

319 tempf

320 voidg

321 voidg

322 voidg

323 voidg

324 voidg

325 voidg

326 voidg

328 mflowj

329 mflowj

330 mflowj

331 mflowj

332 mflowj

334 mflowj

160010000

100100000

130050000

160010000

130020000

120010000

120020000

100050000

100010000

320010000

160010000

130010000

130020000

120010000

110010000

100100000

100050000

130040000

111000000

121000000

131000000

161000000

170010000

* CMT - node 1

335 mflowj

336 mflowj

337 mflowj

338 mflowj

339 mflowj

355 vapgen

358 vapgen

359 vapgen

360 vapgen

361 vapgen

362 vapgen

363 vapgen

364 floreg

365 floreg

366 floreg

367 floreg

368 floreg

369 floreg

372 floreg

373 floreg

373 floreg

374 tempg

377 tempg

378 tempg

379 tempg

380 tempg

383 sattemp

386 sattemp

387 sattemp

388 sattemp

389 sattemp

392 cntrlvar

20800001 hif

20800002 hif

20800003 hif

20800004 hif

20800005 hif

20800006 hif

2080O007 hif

20800008 big

20800009 big

20800010 big

171000000

181000000

310020000

325000000

345000000

160010000

170010000

180010000

110010000

120010000

130010000

130020000

110010000

120010000

120020000

130010000

130020000

160010000

170010000

180010000

330030000

160010000

100100000

110010000

120010000

130010000

160010000

100100000

110010000

120010000

130010000

130 * condensate level, fr-ac.

160010000

.170010000

180010000

110010000

120010000

130010000

130020000

160010000

170010000

180010000

* CMT - node 1

71
20800011 hig

20800012 big

20800013 hig

20800014 big

110010000

120010000

130010000

130020000

*condensate levelfraction

20513000 con-lvl sum

20513001 0.0 0.85

1.0 0.0 1

voidf 160010000

* hydrodynamic data

*component 100 : pipe ( steam generator )

1100000 horzpl pipe

1100001 3

1100101 0.00126 1

1100102 0.00049 3

*1100201 0.00049 2

1100301 0.22 1

1100302 0.90 3

1100401 0.0 3

1100601 0.0 3

1100801 0.000046 0.0 3

1100901 0.43 0.43 1

1100902 0.0 0.0 2

1101001 00000 3

1101101 000100 1

1101102 000000 2

1101201 002 1.4300e5 1.0 0.0 0.0 0.0 3

*1102001 boron concentration should be considered

in future job

1101300 1

1101301 0.0 0.0 0.0 2

*junction 111 : single junction

1000000 sgtank pipe

1000001 10

1000101 0.0 1

1000102 0.78540 9

1000103 0.0 10

1000301 0.205 10

1000401 0.02197 1

1000402 0.0 9

1000403 0.02197 10

1000601 90.0 10

1000801 0.000046 0.0 10

1001001 00000 10

1001101 000000 9

1001201 002 1.430e5 0.0

1001202 002 1.430e5 0.8

1001203 002 1.430e5 1.0

1001300 1

1001301 0.0 0.0 0.0 9

1110000 vortexm sngljun

1110101 110030002 120010001 0.0

000100

1110201 1 0.0 0.0 0.0

1.26 1.26

*component 120 : pipe (horizontal pipe above SG)

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

.0.0

6

7

10

*branch 101 : branch (from S/G to horizontal pipe)

1010000 sg.up branch

1010001 2 1

1010101 0.00126 0.34 0. 0. 90. 0.34 0.000046

1010102 0.0 00000

1010200 002 1.4300e5 1.0

1011101 100100002 101010001 0.00126 0.5 0.5

000100

1011201 0.0 0.0 0.0

1012101 101010002 110010001 0.00126 0.63 0.63

000100

1012201 0.0 0.0 0.0

*component 110 : pipe (horizontal pipe above SG)

1200000 horzp2 pipe

1200001 3

1200101 0.00015 3

1200301 0.17 1

1200302 0.84 3

* 1200501 90.0 1

*1200502 0.0 3

1200601 0.0 3

1200801 0.000046 0.0

1200901 0.81 0.81 1

1200902 0.0 0.0 2

1201001 00000 3

1201101 000000 2

1201201 002 I.4300e5

1201300 1

1201301 0.0 0.0 0.0

1.0 0.0 0.0 0.0 3

*junction 121 : single junction

1210000 pipl sngljun

72
1210101 120030002 130010001 0.00015 1.62 1.62

000000

1210201 1 0.0 0.0 0.0

*component 130 : pipe (vertical pipe above CMT)

*1601001 00000 2

*1601101 000000 1

*1601201 003 1.4300e5 304.0 0.0 0.0 0.0 2

*1601300 1

*1601301 0.0 0.0 0.0 1

1300000 vertpip pipe *junction 161 : valve junction (valve below CMT)

1300001 5

1300101 0.00015 5

1300301 0.204 5

1300401 0.0 5

1300601 -90.0 5

1300801 0.000046 0.0

1300901 0.0 0.0 1

1300902 0.54 0.54 2

1300903 0.0 0.0 4

1301001 00000 5

1301101 000000 4

1301201 003 1.4300e5

5

1301300 1

1301301 0.0 0.0 0.0

1610000 dowvv valve

1610101 160010002

1.75 000100

1610201 1 0.0 0.0

1610300 srvvlv

1610301 120

170010001 0.00071 1.75

5

304.0 0.0 0.0 0.0

4*

*component 170 : vertical pipe below CMT

*junction 131 : junction from vertical pipe to the

cmt

1700000 belopipl pipe

1700001 2

1700101 0.00071 1

1700102 0.00015 2

1700301 0.30 1

1700302 0.12 2

1700401 0.0 2

1700601 -90.0 2

1700801 0.000046 0.0 2

1700901 0.394 0.394 1

1701001 00000 2

1701101 000100 1

1701201 003 1.013e5 293. 0.0

1701202 003 1.013e5 293. 0.0

1701300 1

1701301 0.0 0.0 0.0 1 *#

1310000 cmtjun sngljun

1310101 130050002 160010001

1.0

1310102 000100

1310201 1 0.0 0.0 0.0

*volume 160 : single volume

1600000 cmt snglvol

1600101 0.32170 0.85 0.0

0.000046

1600102 0.0 00000

1600200 003 1.4300e5 304.27

*component 160 : pipe (cmt)

*1600000 cmttank pipe

*1600001 2

*1600101 0.32170 2

*1600301 0.425 1

*1600302 0.425 2

*1600401 0.0 2

*1600601 -90.0 2

*1600801 0.000046 0.0 2

0.00015 1.0

0.0

0.0

0.0

0.0

1

2

0.0 -90. -0.85

*junction 171 : junction between

horizontal pipes

1710000 beljun sngljun

1710101 170020002 180010001

1000.75

1710102 000100

1710201 1 0.0 0.0 0.0

vertical and

0.00015 0.5

*component 180 : horizontal pipe below CMT

1800000

1800001

1800101

1800301

1800401

belopip2

2

0.00015

1.0

0.0

pipe

2

2

2

73
1800601 0.0 2

1800801 0.000046 0.0

1801001 00000 2

1801101 000000 1

1801201 004 1.013e5

1801202 004 1.013e5

1801300 1

1801301 0.0 0.0 0.0

2

293. 0.0

293. 0.0

0.0

0.0

0.0

0.0

1

2

3200401

3200601

3200602

3200801

3200901

3200902

3201001

3201101

3201201

3201300

3201301

0.0 6

-90.0 1

0.0 6

0.000046 0.0

0.81 0.81 1

0.0 0.0 5

00000 6

000000 5

003 1.4300e5

1

*junction 181 : junction to atmosphere

300. 0.0 0.0 0.0 6

1

0.0 0.0 0.0 5

1810000 atmjun sngljun

1810101 180020002 200000000

1.75

1810102 000100

1810201 1 0.0 0.0 0.0

*component 200: atmosphere

0.00015 1.75 *junction 325

3250000 hp-junl sngljun

3250101 320060002 330010001

0.739

3250102 000100

3250201 1 0.0 0.0 0.0

0.00015 0.739

2000000 air

2000101 0.0

2000102 0.0

2000200 004

2000201 0.0

tmdpvol

100.0 1000.0

0.0 00

0.0 0. 0. *component 330 : natural circulation line

1.013e5 293.0 0.0

* Natural circulation line

*branch 310 : branch (from S/G to circulation line

inlet)

*

3300000 nc.hp2 pipe

3300001 4

3300101 0.00126 4

3300301 0.14 1

3300302 0.23 3

3300303 0.4225 4

3300401 0.0 4

3300601 0.0 1

3300602 90.0 4

3300801 0.000046 0.0

3300901 0.63 0.63 1

3300902 0.0 0.0 3

3301001 00000 4

3301101 000000 3

3301201 003 1.4300e5

3301300 1

3301301 0.0 0.0 0.0

3100000 ncjn branch

3100001 2 1

3100101 0.00049 0.11

3100102 0.0 00000

3100200 003 1.4300e5

3101101 100040004

000120

3101201 0.0 0.0 0.0

3102101 310010002 3

000100

3102201 0.0 0.0 0.0

7 0. 0.

300.0

310010001

20010001

0. 0.0 0.000046

4

300. 0.0 0.0 0.0 4

3

0.00049 0.5

0.00015 1.12

0.5

1.12

*junction 335 : natural circulation valve junction

*component 320 : natural circulation line

3200000 nc..hpl pipe

3200001 6

3200101 0.00015 6

3200301 0.13 1

3200302 0.436 6

3350000 dowvv valve

3350101 330040002

1.75 000100

3350201 1 0.0 0.0

3350300 srvvlv

3350301 120

340010001 0.00126 1.75

0.0

*component 340 : natural circulation line

74
3400000 nc-hp3 pipe

3400001 4

3400101 0.00126 4

3400301 0.223 3

3400302 0.1 4

3400401 0.0 4

3400601 0.0 3

3400602 -90.0 4

3400801 0.000046 0.0

3400901 0.0 0.0 1

3400902 0.63 0.63 3

3401001 00000 4

3401101 000000 3

3401201 003 1A300e5

3401300 1

3401301 0.0 0.0 0.0

* cmt (1160)

*11600000

*11600100

*11600101

*11600201

*11600301

*11600400

**11600401

*11600501

*11600601

1

1 3 1 1 0.0

0 2

0.0225 2

5 2

0.0 2

0

288.0 3

160010000 1 1 0 0.32170 1

0 0 0 1 0.32170

4

300. 0.0 0.0 0.0 4

3

*11600701

*11600801

1.0 1

*11600901

1.0 1

0

0.0

0.0 0.0 0.0 1

10.0 10.0 10.0 10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

*junction 345 : junction from natural circulation

* pipe to the ant

* cmt (1160-1)

3450000 cmtjun sngljun

3450101 340040002 16()010001 0.00126 0.1

0.1

3450102 000100

3450201 1 0.0 0.0 0.0

***** ********************************

*valve control

*******************

*11601000

*11601100

*11601101

*11601201

*11601301

**11601400

*11601401

*11601501

*11601601

*11601701

*11601801

1.0 10

*11601901

1.0 10

10 3 2 1 0.32

0 2

0.0025 2

5 2

0.0 2

0

288.0 3

160010000 10000

0 0

0 0.0

0.0 10.0 10.0 1

1

0 1

0.0

0.0

1 0.085 10

0.085 10

0.0 10

10.0 0.0 0.0

20512000 vlvarea

20512001 time

function 1.0 0.0 0

0 003 0.0 10.0 10.0 10.0 10.0 0.0 0.0

* SG (1100)

*valve table

20200300 normarea

20200301 0.0 0.0

20200302 10. 0.0

20200303 10.01 1.0

20200306 10000. 1.0

* heat structure input

*******************

*11000000

*11000100

*11000101

*11000201

*11000301

*11000400

**11000401

*11000501

*11000601

*11000701

*11000801

1.0 10

*11000901

1.0 10

10 3 2 1 0.5

0 2

0.006 2

5 2

0.0 2

0

373.14 3

100010000

0

0

0.0 10.0

10000 1

0 0

0.0 0.0

10.0 10.0

1 0.205 10

1 0.205 10

0.0 10

10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

75
*

. heat structure input for electric heater

110050003 4 2 1 0.0

11005100 0 2

11005101 0.0015 2 0.001 3

11005201 11 2 5 3

11005301 1.0 2 0.0 3

11005400 0

11005401 384.4 4

11005501 0 0 0 1 36.0 3

11005601 100010000 10000 1 1 36.0 3

11005701 10212 1.0 0.0 0.0 3

11005901 0.0 10.0 10.0 10.0 10.0 0.0 0.0 1.0

3

U

* power table

*

*20221200 power 501 1. 100000.0

*20221201 -1. 0.0

*20221202 0. 1.0

*20221203 100. 1.0

*20221204 1000. 1.0

U

20100500 tbl/fctn 1 1 * s - steel

20101100 tbl/fctn I 1 * PZR

heater (MgO) U*UUU** ** U***U**U*UU*** * *** *UUUUU**UUUU***U

* MgO(011)

* temp (k) volumetric heat capacity

U

20100551

*20100551

20100552

20100553

20100554

20100555

20100556

20100557

20100558

20100559

20100560

20100561

*

*

(w/nmk)

20100501

20100502

20100503

20100504

20100505

20100506

20100507

20100508

20100509

20100510

20100511

20100512

*

temp (k) volumetric heat capacity

Q/m3.k)

.2742611e+03 .3831330e+07

.2942611e+03 .3831330e+07

.3109278e+03 .3831330e+07

.3664834e+03 .3985580e+07

.4220389e+03 .4105300e+07

.4775945e+03 .4224090e+07

.5331500e+03 .4308800e+07

.5887056e+03 .4359790e+07

.6442611e+03 .4410320e+07

.8109278e+03 .4561910e+07

.9220389e+03 .4625250e+07

1.9220389e+03 .4625250e+07 *

temp (k) thermal conductivity

.2732611e+03

.2942611e+03

.3109278e+03

.3664834e+03

.4220389e+03

.4775945e+03

.5331500ee+03

.5887056e+03

.6442611e+03

.8109278e+03

.9220389e+03

1.9220389e+03

.1489124e+02

.1489124e+02

.1505739e+02

.1609584e+02

.1696813e+02

.1800657e+02

.1885809e+02

.1956423e+02

.2041575e+02

.2297030e+02

.2423029e+02

.2423029e+02

* heater control

20101151

20101152

20101153

20101154

20101155

*

2

20101101

20101102

20101102

*

(j/m3.k)

0.293e+03 .26000000e+07

0.450e+03 .28350000e+07

0.800e+03 .34020000e+07

1.120e+03 .37260000e+07

1.922038e+03 .37260000e+07

temp (k) thermal conductivity

(w/m.k)

U

20521200 heater constant 0.0

e

•end of file

0.29320e+03

1.27320e+03

1.9220389e+03

81.40

100.47

100.47 *

* stainless steel (005) 18cr-8ni

76
5) P1041

=RELAPS/MOD3.1 CMT 1 Nodes

*PI041 simulation

*CMT node : 1 node

*water valve: 10sec. opened

*job cards

100 new transnt

101 run

110 air

*time step cards

201 10.0 1.0e-12 0.1

*202 20.0 1.Oe-12 0.005

202 20.0 1.Oe-12 0.005

203 1600. 1.Oe-12 0.1

*205 2600. 1.Oe-12 0.1

*minor editor cards

3

3

3

3

3

10 100 100

I00 500

200 1000

10 2500 2

10 2500

500

1000

5OO

2500

355 vapgen

358 vapgen

359 vapgen

360 vapgen

361 vapgen

362 vapgen

363 vapgen

364 floreg

365 floreg

366 floreg

367 floreg

368 floreg

369 floreg

372 floreg

373 floreg

374 tempg

377 tempg

378 tempg

379 tempg

380 tempg

383 sattemp

386 sattemp

387 sattemp

388 sattemp

389 sattemp

160010000

170010000

180010000

110010000

120010000

130010000

130020000

110010000

120010000

120020000

130010000

130020000

160010000

170010000

180010000

160010000

100100000

110010000

120010000

130010000

160010000

100100000

110010000

120010000

130010000

* CMT - node 1

301 tempf

311 p

312 p

313 p

314 tempf

315 tempf

316 tempf

317 tempf

318 tempf $

319 voidg

322 voidg

323 voidg

324 voidg

325 voidg

326 voidg

327 voidg

328 mflowj

329 mflowj

330 mflowj

331 mflowj

332 mflowj

334 mflowj

335 mflowj

336 mflowj

160010000

100100000

130060000

160010000

* CMT - node 1

130020000

120010000

120020000

100060000

100010000

160010000

130010000

130020000

120010000

110010000

100100000

100050000

130040000

111000000

121000000

131000000

161000000

170010000

171000000

181000000

* CMT - node 1

392 cntrivar 130 *

20800001 hif 160010000

20800002 hif 170010000

20800003 hif 180010000

20800004 hif 110010000

20800005 hif 120010000

20800006 hif 130010000

20800007 hif 130020000

condensate level, frac.

* CMT - node 1

20800008 big

20800009 hig

20800010 big

20800011 hig

20800012 hig

20800013 big

20800014 big

160010000

170010000

180010000

110010000

120010000

130010000

130020000

* CMT - node 1

*condensate level,fraction

77
20513000 con-lvI sum 1.0 0.0 1

20513001 0.0 0.85 voidf 160010000

* hydrodynamic data

***** ****** *** *** *** ****** *****************

*component 100 : pipe ( steam generator )

1100401 0.0 3

1100601 0.0 3

1100801 0.000046 0.0 3

1100901 0.43 0.43 1

1100902 0.0 0.0 2

1101001 00000 3

1101101 000100 1

1101102 000000 2

1101201 002 4.0e5 1.0

1101300 1

1101301 0.0 0.0 0.0 2

0.0 0.0 0.0 3

1000000 sgtank pipe

1000001 10

1000101 0.0 1

1000102 0.78540 9

1000103 0.0 10

1000301 0.205 10

1000401 0.02197 1

1000402 0.0 9

1000403 0.02197 10

1000601 90.0 10

1000801 0.000046 0.0 10

1001001 00000 10

1001101 000000 9

1001201 002 4.0e5 0.0

1001202 002 4.0e5 0.5

1001203 002 4.0e5 1.0

1001300 1

1001301 0.0 0.0 0.0 9

*junction 111 : single junction

1110000 vortexrm sngljun

1110101 110030002 120010001 0.0

000100

1110201 1 0.0 0.0 0.0

1.26 1.26

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

4

5

10

*branch 101 : branch (from S/G to horizontal pipe)

1010000 sg.up branch

1010001 2 1

1010101 0.00126 0.34 0. 0.

1010102 0.0 00000

1010200 002 4.00e5 1.0

1011101 100100002 101010001

000100

1011201 0.0 0.0 0.0

1012101 101010002 110010001

000100

1012201 0.0 0.0 0.0

90. 0.34 0.000046

0.00126 0.5 0.5

*component 120 : pipe (horizontal pipe above SG)

1200000 horzp2 pipe

1200001 3

1200101 0.00015 3

1200301 0.17 1

1200302 0.84 3

*1200501 90.0 1

*1200502 0.0 3

1200601 0.0 3

1200801 0.000046 0.0 3

1200901 0.81 0.81 1

1200902 0.0 0.0 2

1201001 00000 3

1201101 000000 2

1201201 002 4.0e5 1.0 0.0 0.0 0.0 3

1201300 1

1201301 0.0 0.0 0.0 2

*junction 121 : single junction

1210000 pip1 sngljun

1210101 120030002 130010001 0.00015 1.62 1.62

000000

1210201 1 0.0 0.0 0.0

*component 130 : pipe (vertical pipe above CMT)

0.00126 0.63 0.63

*component 110 : pipe (horizontal pipe above SG)

1100000 horzpl

1100001 3

1100101 0.00126 1

1100102 0.00049 3

*1100201 0.00049 2

1100301 0.22 1

1100302 0.90

pipe

!

3

1300000 vertpip

1300001 5

1300101 0.00015

pipe

5

78
1300301

1300401

1300601

1300801

1300901

1300902

1300903

1301001

1301101

1301201

1301300

1301301

0.204 5

0.0 5

-90.0 5

0.000046 0.0 5

0.0 0.0 1

0.54 0.54 2

0.0 0.0 4

00000 5

000000 4

003 4.00e5 304.0

1610101 160010002 170010001 0.00071

1.75 000100

1610201 1 0.0 0.0 0.0

1610300 srvvlv

1610301 120

*component 170 : vertical pipe below CMT

1.75

0.0 0.0 0.0 5

1

0.0 0.0 0.0 4 *

*junction 131 : junction from vertical pipe to the

test section

1310000 testse sngljun

1310101 130050002 160010001 0.00015 1.0

1.0

1310102 000100

1310201 1 0.0 0.0 0.0

*volume 160 : single volume

1600000 ant snglvol

1600101 0.32170 0.85 0.0 0.0 -90. -0.85

0.000046

1600102 0.0 00000

1600200 003 1.4300e5 304.1

*component 160 : pipe (cmt)

1700000 belopipl pipe

1700001 2

1700101 0.00071 1

1700102 0.00015 2

1700301 0.30 1

1700302 0.12 2

1700401 0.0 2

1700601 -90.0 2

1700801 0.000046 0.0 2

1700901 0.3750 0.3750 1

1701001 00000 2

1701101 000100 1

1701201 003 1.013e5 293.

1701202 003 1.013e5 293.

1701300 1

1701301 0.0 0.0 0.0 1

0.0

0.0

0.0

0.0

0.0

0.0

1

2

*

*junction 171 : junction between

horizontal pipes

1710000 beljun sngljun

1710101 170020002 180010001

1000.75

1710102 000100

1710201 1 0.0 0.0 0.0

vertical and

0.00015 0.5

*1600000 cmttank pipe

*1600001 2

*1600101 0.32170 2

*1600301 0.425 1

*1600302 0.425 2

*1600401 0.0 2

*1600601 -90.0 2

*1600801 0.000046 0.0 2

*1601001 00000 2

*1601101 000000 1

*1601201 003 1.4300e5

*1601300 1

*1601301 0.0 0.0 0.0 1

*

*component 180 : horizontal pipe below CMT

D4.0 0.0 0.0 0.0 2

nction (valve below test

1800000 belopip2 pipe

1800001 2

1800101 0.00015 2

1800301 1.0 2

1800401 0.0 2

1800601 0.0 2

1800801 0.000046 0.0 2

1801001 00000 2

1801101 000000 1

1801201 004 1.013e5 293.

1801202 004 1.013e5 293.

1801300 1

1801301 0.0 0.0 0.0 1

*junction 161 : valve

section)

ju 0.0

0.0

0.0

0.0

0.0

0.0

1

2

1610000 dowvv valve

79
*junction 181 : junction to atmosphere

1810000 atmjun sngljun

1810101 180020002 200000000

1.75

1810102 000100

1810201 1 0.0 0.0 0.0

*component 200 : atmosphere

*11600400

**11600401

*11600501

.*11600601

1

*11600701

*11600801

1.0 1

*11600901

1.0 1

0

288.0 3

160010000

0

1 1 0 0.32170 1

0 0 1 0.32170

0.00015 1.75 0

0.0

0.0 0.0 0.0 1

10.0 10.0 10.0 10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

* cmt (1160-1)

2000000 air

2000101 0.0

2000102 0.0

2000200 004

2000201 0.0

tmdpvol

100.0 1000.0

0.0 00

0.0 0. 0.

1.013e5 293.0 0.0

*va* *********************************** * *

*valve control

*11601000

*11601100

*11601101

*11601201

*11601301

**11601400

*11601401

*11601501

*11601601

*11601701

*11601801

1.0 10

*11601901

1.0 10

10 3 2

0 2

0.0025 2

5 2

0.0 2

0

288.0 3

160010000

0

0

0.0 10.0

1 0.32

10000

0

0.0

10.0

1

0

0.0

10.0

1 0.085 10

1 0.085 10

0.0 10

10.0 0.0 0.0

20512000 vlvarea

20512001 time

function 1.0 0.0 0

0 003 0.0 10.0 10.0 10.0 10.0 0.0 0.0

* SG (1100)

*valve table

20200300 normarea

20200301 0.0 0.0

20200302 10. 0.0

20200303 10.01 1.0

20200306 10000. 1.0

*11000000

*11000100

*11000101

*11000201

*11000301

*11000400

**11000401

*11000501

*11000601

*11000701

*11000801

1.0 10

*11000901

1.0 10

10 3 2

0 2

0.006 2

5 2

0.0 2

0

373.14 3

100010000

0

0

0.0 10.0

1 0.5

10000

0

0.0

10.0

1

0

0.0

10.0

1 0.205 10

1 0.205 10

0.0 10

10.0 0.0 0.0

* heat structure input

* cmt (1160)

0.0 10.0 10.0 10.0 10.0 0.0 0.0

*11600000

*11600100

*11600101

*11600201

*11600301

1 3 1 1 0.0

0 2

0.0225 2

5 2

0.0 2

*$***$***** ** *$****** **  $**  ******* ** *** *** **

* heat structure input for electric heater

110050003 4 2 1 0.0

80
11005100 0 2

11005101 0.0015 2 0.001 3

11005201 11 2 5 3

11005301 1.0 2 0.0 3

11005400 0

11005401 384.4 4

11005501 0 0 0 1 36.0 3

11005601 100010000 10000 1 1 36.0 3

11005701 10212 1.0 0.0 0.0 3

11005901 0.0 10.0 10.0 10.0 10.0 0.0 0.0

3

* power table

1.0

20100554

20100555

20100556

20100557

20100558

20100559

20100560

20100561

20100501

20100502

20100503

20100504

20100504 20100605

20100506

20100507

20100508

20100509

20100510

20100511

20100512

.4220389e+03

.4775945e+03

.5331500e+03

.5887056e+03

.6442611e+03

.8109278e+03

.9220389e+03

1.9220389e+03

.4105300e+07

.4224090e+07

.4308800e+07

.4359790e+07

.4410320e+07

.4561910e+07

.4625250e+07

.4625250e+07 *

temp (k) thermal conductivity

*20221200

*20221201

*20221202

*20221203

*20221204

power 501

-1. 0.0

0. 1.0

100. 1.0

1000. M.C

1. 100000.0

.2732611e+03

.2942611e+03

.3109278e+03

.3664834e+03

.4220389e+03

A775945e+03

.5331500e+03

.5887056e+03

.6442611e+03

.8109278e+03

.9220389e+03

1.9220389e+03

(w/m.k)

.1489124e+02

.1489124e+02

.1505739e+02

.1609584e+02

.1696813e+02

.1800657e+02

.1885809e+02

.1956423e+02

.2041575e+02

.2297030e+02

.2423029e+02

.2423029e+02

20100500 tbh/fctn 1

20101100 tbhfctn 1

1

1

* s - steel

* PZR heater (MgO) *

*MgQ (011)

20101151

20101152

20101153

20101154

20101155

(w/m.k)

0101101

20101102

20101102

temp (k) volumetric heat capacity

(j/m3.k)

0.293e+03 .26000000e+07

0.450e+03 .28350000e+07

0.800e+03 .34020000e+07

1.120e+03 .37260000e+07

1.922038e+03 .37260000e+07

temp (k) thermal conductivity

**** ****************************************

* heater control

20521200 heater constant 0.0

end of file

0.29320e+03

1.27320e+03

1.9220389e+03

81.40

100.47

100.47 *

* stainless steel (005) 18cr-8ni

* temp (k) volumetric heat capacity

(j/m3.k)

20100551

*20100551

20100552

20100553

.2742611e+03

.2942611e+03

.3109278e+03

3664834e+03

.3831330e+07

.3831330e+07

.3831330e+07

.3985580e+07

81
6) PNO41

=RELAP5/MOD3.1 CMT 1 Nodes

* PNO41 simulation

* CMT node : 1 node

* water valve: 10sec. opened

* natural circulation line v/v : 10sec. opened

*job cards

100 new transnt

101 run

110 air

*time step cards

201 10.0 1.0e-12 0.1

202 20.0 " .Oe-12 0.005

203 40.0 l.Oe-12 0.1

204 60.0 1.0e-12 0.005

205 1000.0 1.0e-12 0.1

*minor editor cards

3 10 100 100

3 100 500 500

3 10 100 100

3 100 500 500

3 10 2500 2500

336 mflowj

337 mflowj

338 mflowj

339 mflowj

355 vapgen

358 vapgen

359 vapgen

360 vapgen

361 vapgen

362 vapgen

363 vapgen

364 floreg

365 floreg

366 floreg

367 floreg

368 floreg

369 floreg

372 floreg

373 floreg

373 floreg

374 tempg

377 tempg

378 tempg

379 tempg

380 tempg

383 sattemp

386 sattemp

387 sattemp

388 sattemp

389 sattemp

160010000

170010000

180010000

110010000

120010000

130010000

130020000

301 tempf

311 p

312 p

313 p

314 tempf

315 tempf

316 tempf

317 tempf

318 tempf

319 tempf

320 voidg

321 voidg

322 voidg

323 voidg

324 voidg

325 voidg

326 voidg

328 mflowj

329 mflowj

330 mflowj

331 mflowj

332 mflowj

334 mflowj

335 mflowj

181000000

310020000

325000000

345000000

* CMT - node 1

160010000

100100000

130050000

160010000

* CMT - node 1

110010000

120010000

120020000

130010000

130020000

160010000

170010000

180010000

330030000

160010000

100100000

110010000

120010000

130010000

160010000

100100000

110010000

120010000

130010000

130020000

120010000

120020000

100050000

100010000

320010000

160010000

130010000

130020000

120010000

110010000

100100000

100050000

130040000

111000000

121000000

131000000

161000000

170010000

171000000

* CMT - node 1

392 cntrlvar 130

20800001 hif

20800002 hif

20800002 hif

20800004 hif

20800005 hif

20800006 hif

20800007 hif

20800008 big

20800009 hig

20800010 big

20800011 hig

20800012 hig

20800013 hig

* condensate level, frac.

160010000

170010000

180010000

110010000

-.120010000

130010000

130020000

* CMT - node 1

160010000

170010000

180010000

110010000

120010000

130010000

82
20800014 hig 130020000

*condensate level,fraction

20513000 con-lvl sum 1.0 0.0 1

20513001 0.0 0.85 voidf 160010000

* hydrodynamic data

*******m ** *** ** ***** ***** ********************

*component 100 :pipe ( steam generator

1100102 0.00049 3

*1100201 0.00049 2

1100301 0.22 1

1100302 0.90 3

1100401 0.0 3

1100601 0.0 3

1100801 0.000046 0.0 3

1100901 0.43 0.43 1

1100902 0.0 0.0 2

1101001 00000 3

1101101 000100 1

1101102 000000 2

1101201 002 4.0e5 1.0

1101300 1

1101301 0.0 0.0 0.0 2

0.0 0.0 0.0 3

1000000 sgtank

1000001 10

1000101 0.0

1000102 0.78540

1000103 0.0

1000301 0.205

1000401 0.02197

1000402 0.0

1000403 0.02197

1000601 90.0

1000801 0.000046

1001001 00000

1001101 000000

1001201 002 4.(

1001202 002 4.(

1001203 002 4.(

1001300 1

1001301 0.0 0.0

pipe

1

9

10

10

1

9

10

10

0.0 10

10

9

)e5 0.0

)e5 0.8

)e5 1.0

0.0 9

*junction 111 : single junction

1110000 vortexm sngljun

1110101 110030002 120010001 0.0

000100

1110201 1 0.0 0.0 0.0

1.26 1.26

*component 120 : pipe (horizontal pipe above SG)

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

6

7

10

1200000 horzp2

1200001 3

1200101 0.00015

1200301 0.17

1200302 0.84

*1200501 90.0

*1200502 0.0

pipe

3

1

3

1

3

*branch 101 : branch (from S/G to horizontal pipe) 1200601 0.0 3

1200801 0.000046 0.0 3

1010000

1010001

1010101

1010102

1010200

1011101

000100

1011201

1012101

000100

1012201

sg.up branch

2 1

0.00126 0.34 0. 0.

0.0 00000

002 4.0e5 1.0

100100002 101010001

0.0 0.0 0.0

101010002 110010001

90. 0.34 0.000046

0.00126 0.5 0.5

0.00126 0.63 0.63

1200901 0.

1200902 0.

1201001 OX

1201101 OX

1201201 0(

1201300 1

1201301 0.

81 0.81 1

0 0.0 2

)000 3

)0000 2

4.0e5 1.0

0 0.0 0.0 2

0.0 0.0 0.0 3

0.0 0.0 0.0

*junction 121 : single junction

1210000 pipl sngljun

1210101 120030002 130010001 0.00015

000000

1210201 1 0.0 0.0 0.0

*component 110 : pipe (horizontal pipe above SG) 1.62 1.62

1100000 horzpl

1100001 3

1100101 0.00126 1

pipe

*component 130 : pipe (vertical pipe above CMT)

83
1300000 vertpip pipe

1300001 5

1300101 0.00015 5

1300301 0.204 5

1300401 0.0 5

1300601 -90.0 5

1300801 0.000046 0.0 5

1300901 0.0 0.0 1

1300902 0.54 0.54 2

1300903 0.0 0.0 4

1301001 00000 5

1301101 000000 4

1301201 003 4.Oe5 304.0

1301300 1

1301301 0.0 0.0 0.0 4 *

*

*junction 131 : junction from

cmt

*junction 161 : valve junction (valve below CMT)

1610000 dowvv valve

1610101 160010002 170

1.75 000100

1610201 1 0.0 0.0 0.0

1610300 srvvlv

1610301 120

010001 0.00071 1.75

*component 170 : vertical pipe below CMT

0.0 0.0 0.0 5

vertical pipe to the

1700000 belopipl pipe

1700001 2

1700101 0.00071 1

1700102 0.00015 2

1700301 0.30 1

1700302 0.12 2

1700401 0.0 2

1700601 -90.0 2

1700801 0.000046 0.0 2

1700901 0.394 0.394 1

1701001 00000 2

1701101 000100 1

1701201 003 1.013e5 293.

1701202 003 1.013e5 293.

1701300 1

1701301 0.0 0.0 0.0 1

1310000 cmtjun s

1310101 130050002

1.0

1310102 000100

1310201 1 0.0 C

ngljun

160010001 0.00015 1.0

0.0

0.0

0.0

0.0

0.0

0.0

1

).0 0.0 2

*volume 160 : single volume

1600000 cmt snglvol

1600101 0.32170 0.85

0.000046

1600102 0.0 00000

1600200 003 4.0e5 304.3

*junction 171 : junction between vertical

horizontal pipes

and

0.0 0.0 -90. -0.85

*component 160 : pipe (cmt)

1710000 beljun sngljun

1710101 170020002 180010001

1000.75

1710102 000100

1710201 1 0.0 0.0 0.0

0.00015 0.5

*1600000 cmttank pipe

*1600001 2

*1600101 0.32170 2

*1600301 0.425 1

*1600302 0.425 2

*1600401 0.0 2

*1600601 -90.0 2

*1600801 0.000046 0.0

*1601001 00000 2

*1601101 000000 1

*1601201 003 1.4300e5

*1601300 1

*1601301 0.0 0.0 0.0

*

*

*component 180 : horizontal pipe below CMT

*

1800000 belopip2 pipe

1800001 2

1800101 0.00015 2

1800301 1.0 2

1800401 0.0 2

1800601 0.0 2

1800801 0.000046 0.0

1801001 00000 2

1801101 000000 1

1801201 004 1.013e5

1801202 004 1.013e5

2

304.0 0.0 0.0 0.0 2

293. 0.0

293. 0.0

0.0

0.0

0.0

0.0

1

2

84
1801300 1

1801301 0.0 0.0 0.0 1

*junction 181 : junction to atmosphere

3201001 00000 6

3201101 000000 5

3201201 003 4.0e5 300. 0.0

3201300 1

3201301 0.0 0.0 0.0 5

*junction 325

0.0 0.0 6

1810000 atmjun sngljun

1810101 180020002 200000000

1.75

1810102 000100

1810201 1 0.0 0.0 0.0

*component 200 : atmosphere

*k

0.00015 1.75

3250000 hpjunl

3250101 320060002

0.739

3250102 000100

3250201 1 0.0

sngljun

330010001 0.00015 0.739

0.0 0.0

2000000 air

2000101 0.0

2000102 0.0

2000200 004

2000201 0.0

tmdpvol

100.0 1000.0

0.0 00

0.0 0.0. *component 330 : natural circulation line

1.013e5 293.0 0.0

* Natural circulation line

*branch 310 : branch (from

inlet)

S/G to circulation line

3300000 nc.hp2 pipe

3300001 4

3300101 0.00126 4

3300301 0.14 1

3300302 0.23 3

3300303 0.4225 4

3300401 0.0 4

3300601 0.0 1

3300602 90.0 4

3300801 0.000046 0.0 4

3300901 0.63 0.63 1

3300902 0.0 0.0 3

3301001 00000 4

3301101 000000 3

3301201 003 4.0e5 300.

3301300 1

3301301 0.0 0.0 0.0 3

3100000 ncin branch

3100001 2 1

3100101 0.00049 0.17 0. 0.

3100102 0.0 00000

3100200 003 4.0e5 300.0

3101101 100040004 310010001

000120

3101201 0.0 0.0 0.0

3102101 310010002 320010001

000100

3102201 0.0 0.0 0.0

0. 0.0 0.000046

0.00049 0.5 0.5

0.0 0.0 0.0 4

0.00015 1.12 1.12

*junction 335 : natural circulation valve junction

*component 320 : natural circulation line

3350000 dowvv valve

3350101 330040002

1.75 000100

3350201 1 0.0 0.0

3350300 srvvlv

3350301 120

340010001 0.00126 1.75

3200000 ncjhpl pipe 0.0

3200001 6

3200101 0.00015 6

3200301 0.13 1

3200302 0.436 6

3200401 0.0 6

3200601 -90.0 1

3200602 0.0 6

3200801 0.000046 0.0

3200901 0.81 0.81 1

3200902 0.0 0.0 5

*component 340 : natural circulation line

3400000 ncjhp3 pipe

3400001 4

3400101 0.00126 4

3400301 0.223 3

3400302 0.1 4

6

85
3400401 0.0 4

3400601 0.0 3

3400602 -90.0 4

3400801 0.000046 0.0 4

3400901 0.0 0.0 1

3400902 0.63 0.63 3

3401001 00000 4

3401101 000000 3

3401201 003 4.Oe5 300. 0.0 0.0 0.0 4

3401300 1

3401301 0.0 0.0 0.0 3

*junction 345 : junction from natural circulation

*11600301

*11600400

**11600401

*11600501

*11600601

1

*11600701

*11600801

1.0 1

*11600901

1.0 1

0.0 2

0

288.0 3

160010000 1 1 0 0.32170 1

0 0 0 1 0.32170

0 0.0 0.0 0.0 1

0.0 10.0 10.0 10.0 10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

* cmt (1160-1)

*

*

pipe to the cmt

3450000 cmtjun sngljun

3450101 340040002 16()O10001 0.00126 1.0

1.0

3450102 000100

3450201 1 0.0 0.0 0.0

** *** ***   ** ****** ***   **  *** ****** ***** *

*valve control

20512000 vlvarea function 1.0 0.0 0

20512001 time 0 003

*11601000

*11601100

*11601101

*11601201

*11601301

**11601400

*11601401

*11601501

*11601601

*11601701

*11601801

1.0 10

*11601901

1.0 10

10 3 2 1 0.32

0 2

0.0025 2

5 2

0.0 2

0

288.0 3

160010000 10000 1 1 0.085 10

0 0 0 1 0.085 10

0 0.0 0.0 0.0 10

0.0 10.0 10.0 10.0 10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

* SG (1100)

*valve table

20200300 normarea

20200301 0.0 0.0

20200302 10. 0.0

20200303 10.01 1.0

20200306 10000. 1.0

*11000000

*11000100

*11000101

*11000201

*11000301

*11000400

**11000401

*11000501

*11000601

*11000701

*11000801

1.0 10

*11000901

1.0 10

10 3 2 1 0.5

0 2

0.006 2

5 2

0.0 2

0

373.14 3

100010000 10000 1 1 0.205 10

0 0 0 1 0.205 10

0 0.0 0.0 0.0 10

0.0 10.0 10.0 10.0 10.0 0.0 0.0

0.0 10.0 10.0 10.0 10.0 0.0 0.0

* heat structure input

* cmt (1160)

*11600000 1 3 1 1 0.0

*11600100 0 2

*11600101 0.0225 2

*11600201 5 2

* heat structure input for electric heater

86
110050003 4 2 1 0.0

11005100 0 2

11005101 0.0015 2 0.001 3

11005201 11 2 5 3

11005301 1.0 2 0.0 3

11005400 0

11005401 384.4 4

11005501 0 0 0 1 36.0 3

11005601 100010000 10000 1 1 36.0 3

11005701 10212 1.0 0.0 0.0 3

11005901 0.0 10.0 10.0 10.0 10.0 0.0 0.0 1.0

3

. power table

*20221200 power 501 1. 100000.0

*20221201 -1. 0.0

*20221202 0. 1.0

*20221203 100. 1.0

*20221204 1000. 1.0

20100500 tbVfctn 1 1 s- steel

20101100 tbl/fctn 1 1 * PZR

heater (MgO)

* MgO (011)

20100552

20100553

20100554

20100555

20100556

20100557

20100558

20100559

20100560

20100561

20100501

20100502

20100503

20100504

20100505

20100506

20100507

20100508

20100509

20100510

20100511

20100512

.3109278e+03

.3664834e+03

.4220389e+03

.4775945e+03

.5331500e+03

.5887056e+03

.6442611e+03

.8109278e+03

.9220389e+03

1.9220389e+03

.3831330e+07

.3985580e+07

.4105300e+07

.4224090e+07

.4308800e+07

.4359790e+07

.4410320e+07

.4561910e+07

.4625250e+07

.4625250e+07 *

temp (k) thermal conductivity

(w/m.k)

.2732611e+03 .1489124e+02

.2942611e+03 .1489124e+02

.3109278e+03 .1505739e+02

.3664834e+03 .1609584e+02

.4220389e+03 .1696813e+02

.4775945e+03 .1800657e+02

.5331500e+03 .1885809e+02

.5887056e+03 .1956423e+02

.6442611e+03 .2041575e+02

.8109278e+03 .2297030e+02

.9220389e+03 .2423029e+02

1.9220389e+03 .2423029e+02 *

20101151

20101152

20101153

20101154

20101155

(w/m.k)

20101101

20101102

20101102

temp (k) volumetric heat capacity

(j/m3.k)

0.293e+03 .26000000e+07

O.ASOe+03 .28350000e+07

0.800e+03 .34020000e+07

1.120e+03 .37260000e+07

1.922038e+03 .37260000e+07

temp (k) thermal conductivity

* heater control

20521200 heater constant 0.0

end of file

0.29320e*03

1.27320e+03

1.9220389e+03

81.40

100.47

100.47 *

* stainless steel (005) 18cr-8ni

lm/3.k)

20100551

*20100551

temp (k) volumetric heat capacity

.2742611e+03

.2942611e+03

.3831330e+07

M.331330e+07

87
Appendix B : Experimental

Data

1) GI021

Psg Pressure at steam generator(bar or

Pa)

Pts Pressure at test section(bar or Pa)

Tts Temperature at test section(c)

Ws steam flow rate(kg/sec)

Winj injection flow rate(kg/sec)

What natural circulation flow(kg/sec)

Time Tts Psg(bar)

1.4300 31.01 1.43000

2.6410 31.47 1.43000

3.7890 31.42 1.43000

4.9380 31.36 1.43000

6.3200 31.42 1.43000

7.5230 31.25 1.43000

8.7340 31.40 1.43000

10.0470 31.44 1.43000

11.2580 31.33 1.43000

12.4690 31.36 1.42000

13.6800 31.55 1.41000

14.9920 31.51 1.41000

16.1480 31.69 1.41000

17.2970 31.80 1.41000

18.6720 32.02 1.41000

19.8830 32.31 1.41000

21.0940 32.33 1.41000

22.4140 32.57 1.41000

23.5630 32.66 1.41000

24.8280 32.79 1.41000

25.9840 32.92 1.41000

27.3520 33.05 1.40000

28.5080 32.99 1.40000

29.6640 33.06 1.40000

31.0310 33.19 1.40000

32.2420 33.12 1.40000

33.4530 33.12 1.40000

34.7730 33.25 1.39000

35.9840 33.34 1.39000

37.1800 33.25 1.39000

38.3440 33.32 1.40000

39.6640 33.27 1.40000

40.8590 33.19 1.40000

42.0700 33.32 1.40000

43. 4530 33.21 1.40000

44.6020 33.21 1.39000

45.8130 33.25 1.39000

46.9610 33.23 1.39000

48.3280 33.30 1.39000

49.4920 33.21 1.39000

50.6410 33.36 1.39000

52.0080 33.29 1.39000

53.2190 33.30 1.39000

54.3830 33.34 1.39000

55.6880 33.18 1.39000

56.8520 33.27 1.39000

Pts(bar) Is

1.51000

1. 51000

1.51000

1.51000

1.51000

1. 51000

1.51000

1.51000

1.23000

1.15000

1.04000

0.94000

0.85000

0.80000

0.80000

0.81000

0.81000

0.79000

0.81000

0.81000

0.80000

0.80000

0.81000

0.81000

0.80000

0.81000

0.82000

0.81000

0.81000

0.81000

0.79000

0.81000

0.81000

0.81000

0.80000

0.81000

0.80000

0.80000

0.80000

0.80000

0.81000

0.80000

0.81000

0.81000

0.80000

0.79000

0.00082

0.00082

0.00082

0.00082

0.00082

0.00082

0.00082

0.OOD82

0.00084

0.00104

0. 00143

0. 00131

0. 00133

0. 00170

0.00264

0. 00318

0.00410

0.00528

0.00621

0.00706

0.00775

0.00838

0.00884

0.00920

0.00951

0.00968

0.00981

0.00990

0.00999

0. 01012

0.01023

0.01039

0.01051

0. 010N1

0.01073

0.01076

0.01082

0. 01081

0.01080

0.01083

0.01085

0.01089

0. 01087

0. 01092

0. 01096

0.01099

wini

0.00694

0.00694

0.00694

0.00694

0.00694

0.00694

0.00694

0.00694

0.06476

0. 14034

0.18740

0.20267

0. 19573

0.15192

0.10745

0.07974

O.05912

0.04484

0.03509

0.02786

0.02354

0.02061

0.03103

0.03450

O.02872

0.02570

0.02201

0.02285

0.02M36

0.03461

0.04464

0.03871

0.03945

0.04098

0. 03790

0.03306

0.02875

0. 04347

0.04296

0.04504

0.04765

0.10350

0.11621

0. 08745

0.07002

0.06912

58.0000 33.27 1.39000

59.2110 33.34 1.39000

60.5310 33.30 1.39000

61.7420 33.29 1.39000

62.8910 33.38 1.39000

64.2110 33.29 1.39000

65.3590 33.36 1.39000

66.5700 33.34 1.38000

67.8910 33.21 1.39000

69.1020 33.32 1.39000

70.2970 33.36 1.39000

71.4610 33.23 1.38000

72.7810 33.30 1.39000

74.0390 33.36 1.39000

75.1880 33.25 1.39000

76.5700 33.29 1.38000

77.7190 33.32 1.38000

78.8670 33.32 1.38000

80.0780 33.45 1.38000

81.4530 33.38 1.38000

82.6640 33.38 1.38000

83.8200 33.34 1.38000

85.1880 33.54 1.38000

86.3440 33.54 1.38000

87.5470 33.52 1.38000

88.8670 33.43 1.38000

90.0780 33.50 1.38000

91.2340 33.49 1.38000

92.4380 33.56 1.38000

93.7580 33.61 1.38000

95.0230 33.65 1.38000

96.1720 33.92 1.38000

97.5470 33.67 1.38000

98.7030 33.74 1.38000

99.9610 33.76 1.38000

101.2810 33.78 1.38000

102.4920 33.78 1.38000

103.6410 33.85 1.38000

104. 9140 33.92 1.38000

106.1720 33.96 1.38000

107.3830 33.92 1.38000

108.5940 33.87 1.38000

109.9610 33.96 1.38000

111.1090 33.94 1.38000

112.3200 33.98 1.37000

113.6410 33.89 1.37000

114.7890 33.96 1.37000

116.0000 33.91 1.37000

117.1640 33.91 1.37000

118.5310 33.91 1.37000

119.6800 33.96 1.37000

120.8910 33.85 1.37000

122.2110 33.91 1.37000

123.4220 33.96 1 *.37000

124.6170 33.87 1.37000

125.7810 33.94 1.37000

127.1020 33.98 1.37000

128.2500 34.02 1.37000

129.4610 34.14 1.37000

130.7810 33.96 1.37000

131.9840 34.09 1.37000

133.1410 34.16 1.37000

134.4610 34.05 1.37000

135.6090 34.11 1.37000

138.8200 34.18 1.37000

137.9690 34.27 1.36000

0.80000

0.80000

0.80000

0.80000

0.81000

0.80000

0.81000

0.80000

0.81000

0.79000

0.81000

0. 80000

0. 81000

0.81000

0.81000

0. 78000

0.80000

0.80000

0.80000

0.79000

0. 81000

0. 82000

0. 80000

0.79000

0.:82000

0. 82000

0.81000

0.81000

0.81000

0.80000

0.80000

0.81000

0.82000

0.81000

0.81000

0. 81000

0.81000

0.81000

0.80000

0.80000

0.79000

0.81000

0.79000

0.82000

0. 81000

0.80000

0.80000

0.78000

0.79000

0.78000

0.81000

0.82000

0.82000

0.80000

0.79000

0.80000

0.81000

0.80000

0.80000

0.80000

0.81000

0.82000

0.80000

0.78000

0.80000

0.81000

0.01100

0.01098

0.01097

0.01098

0.01100

0. 01 098

0.01099

0.01099

0.01097

0.01096

0.01100

0.01104

0.01101

0.01103

0.01105

0.01108

0.01108

0.01110

0.01109

0. 01109

0. 01108

0. 01109

0. 01106

0.01109

0. 01107

0.01108

0.01109

0.01107

0.01107

0. 01112

0.01109

0. 01110

0.01109

0.01110

0.01110

0.01111

0.01109

0.01108

0. 01104

0.01102

0. 01104

0.01104

0. 01101

0.01105

0.01106

0.01105

0.01107

0.01105

0.01106

0.01108

0.01108

0.01106

0.01100

0.01100

0.01103

0.01104

0. 01098

0.01095

0.01095

0. 01096

0. 01095

0. 01091

0. 01093

0. 01095

0. 01095

0.01092

0. 06410

0. 06481

0.06268

0.05418

0.05622

0. 05417

0.06521

0. 06988

0. 05807

0.05829

0.05204

0.05830

0.05599

0.05507

0.05618

0.05312

0.05556

0.05853

0.05328

0. 05079

0. 04872

0. 04711

0.04338

0. 03853

0. 03355

0.03536

0.04057

0.04188

0.03675

0.04119

0. 04012

0. 04422

0.04408

0.04237

0.04067

0.03714

0. 03288

0. 03960

0.04199

0.04753

0.04497

0. 03942

0. 03812

0.03759

0.03292

0. 03123

0.03730

0.04037

0.03857

0.03349

0.03496

0.03841

0. 04400

0.04118

0. 03841

0.03247

0.03477

0. 04123

0.03883

0.04101

0. 03932

0. 03652

0.03628

0.03891

0.03362

0.03792

88
139.2890 34.27 1.37000

140.5000 34.34 1.36000

141.6480 34.33 1.37000

143.0230 34.27 1.37000

144.1800 34.27 1.37000

145. 3910 34.42 1.37000

146.7030 34.40 1.37000

147.9140 34.40 1.37000

149.0700 34.51 1.36000

150.2190 34.40 1.36000

151.5940 34.58 1.36000

152.7500 34.56 1.36000

153.9610 34.53 1.36000

155.2730 34.53 1.36000

156.4840 34.67 1.36000

157.6410 34.73 1.36000

158.8440 34.76 1.36000

160.1640 34.58 1.36000

161.3670 34.71 1.36000

162.5230 34.87 1.36000

163.8440 34.82 1.36000

165.0470 34.80 1.36000

166.2580 34.89 1.35000

167.5780 34.82 1.35000

168.7810 34.87 1.35000

169.9380 34.95 1.35000

171.1480 35.02 1.36000

172.4610 34.87 1.35000

173.6170 34.98 1.36000

174.8280 35.07 1.36000

176.1480 35.00 1.35000

177.3520 35.07 1.35000

178.5080 35.04 1.35000

179.8280 35.00 1.35000

181.0310 35.02 1.35000

182.1880 37.08 1.35000

183.3980 34.95 1.35000

184.7110 35.20 1.35000

185.9220 35.02 1.35000

187.0780 35.04 1.35000

188.4530 35.15 1.35000

189.6640 35.02 1.35000

190.8130 34.98 1.35000

192.1800 35.04 1.35000

193.3440 35.20 1.35000

194.5470 35.13 1.35000

195.7030 35.20 1.35000

197.0700 35.24 1.35000

198.2810 35.22 1.35000

199.4300 35.35 1.35000

200.8130 35.31 1.35000

201.9610 35.35 1.35000

203.1720 35.44 1.35000

204.3200 35.44 1.35000

205.6880 35.38 1.35000

206.8520 35.48 1.35000

208.0000 35.44 1.34000

209.3670 35.40 1.34000

210.5310 35.33 1.34000

211.7420 35.40 1.35000

213.0470 35.38 1.34000

214.2580 35.49 1.34000

215.4220 35.51 1.34000

216.6330 35.51 1.34000

217.8910 35.66 1.34000

219.1020 35.35 1.34000

0.81000 0.01093

0.81000 0.01095

0.8M000 0.01097

0.8100 m 0.01094

0.80000

0.79000

0.79000

0.81000

0.81000

0.80000

0.78000

0.81000

0.79000

0.81000

0.81000

0.79000

0.80000

0.80000

0.82000

0.81000

0.81000

0.81000

0.79000

0.80000

0.79000

0.82000

0.81000

0.81000

0.78000

0.80000

0. 82000

0.80000

0.80000

0.82000

0.79000

0.79000

0.80000

0.81000

0.79000

0.82000

0.79000

0.81000

0.80000

0.79000

0.79000

0.81000

0.80000

0.79000

0.81000

0.81000

0.80000

0. 79000

0.81000

0. 79O0

0.80000

0.80000

0.80000

0.80000

0.81000

0.80000

0.81000

0.80000

0.80000

0.80000

O.82000

0.79000

0. 01099

0. 01097

0.01100

0.01101

0.01097

0.01096

0. 01087

0.01088

0. 01093

0.01095

0.01095

0.01090

0.01090

0.01090

0. 01085

0.01083

0.01085

0.01088

0.01085

0.01082

0. 01081

0.01083

0.01081

0.01080

0. 01079

0.01080

0. 01081

0.01084

0.01080

0.01080

0.01080

0. 01079

0. 01081

0.01081

0.01078

0.01077

0,01077

0.01074

0.01071

0.01068

0.01071

0.01075

0.01077

0.01077

0.01074

0.01075

0.01076

0.01076

0. 01076

0. 01076

0.01069

0.01069

0.01073

0.01072

0.01072

0. 01071

0.01073

0. 01074

0.01074

0.01068

0.01066

0. 01067

0.03917

0.03639

0. 03407

0. 03516

0.03172

0.03280

0.03485

0.03422

0.03740

0.03378

0. 04344

0. 04451

0.03642

0. 03157

0.03204

0.03573

0.03432

o. 03672

0.04689

0. 04819

0.04463

0.05026

0.05546

O. 0812

0.05401

0. 05324

0.05422

0.04968

0. 04518

.04765

0.05554

0.05837

0.05392

0.04298

0.03998

0.04040

0.03593

0.03217

0.03210

0.03126

0.03055

0.03482

0.03770

0.03924

0.03703

0.03216

0.04369

0.03942

0.04635

0.04754

0.04672

0.04511

0.04538

0.04556

0.04587

0.04833

0.05179

0.04740

0.05154

0.05014

0. 04755

0.04144

0.03617

0.04202

0.03540

0.03092

220.2500 35.79 1.34000

221.5700 35.64 1.34000

222.7810 35.73 1.34000

223.9300 35.73 1.34000

225.2970 35.71 1.34000

226.4610 35.77 1.34000

227.6720 35.91 1.34000

228.8200 35.75 1.34000

230.1410 35.91 1.34000

231.2890 35.91 1.34000

232.4380 35.97 1.34000

233.8200 36.00 1.34000

234.9690 36.04 1.34000

236.1800 35.93 1.34000

237.3910 36.04 1.34000

238.7580 35.93 1.34000

239.9140 36.04 1.34000

241.1170 36.08 1.34000

242.4380 36.15 1.33000

243.5940 36.11 1.33000

244.7970 36.13 1.33000

246.1800 36.17 1.33000

247.3280 36.11 1.33000

248.5390 36.17 1.33000

249.7500 36.19 1.33000

251.1170 36.15 1.33000

252.2730 36.24 1.33000

253.4840 36.15 1.33000

254.7970 36.97 1.33000

256.0080 36.04 1.33000

257.1640 38.19 1.33000

258.5310 36.35 1.33000

259.6880 36.26 1.33000

260.8980 36.13 1.33000

262.0470 36.33 1.33000

263.4220 36.48 1.33000

264.5780 36.48 1.33000

265.7810 36.48 1.33000

267.1020 36.52 1.33000

268.3130 36.50 1.33000

269.5230 36.57 1.33000

270.8440 36.52 1.33000

272.0390 36.57 1.33000

273.2500 36.57 1.33000

274.4140 36.52 1.33000

275.7190 36.53 1.33000

276.9300 36.61 1.33000

278.1410 36.64 1.33000

279.4610 36.59 1.33000

280.6090 36.68 1.33000

281.8830 37.14 1.33000

283.0310 36.66 1.33000

284.3520 36.88 1.33000

285.5630 36.86 1."33000

286.7580 36.90 1.32000

288.1880 36X83 1.32000

289.3520 36.90 1.32000

290.5470 36.81 1.32000

291.8670 36.90 1.32000

293.0310 36.99 1.32000

294.2340 36.99 1.32000

295.4380 37.01 1.32000

296.7110 36.97 1.32000

297.9140 37.06 1.32000

299.0700 37.06 1.32000

300.3910 37.10 1.32000

0.81000

0. 82000

0.80000

0.81000

0. 80000

0.80000

0. 8000

0.80000

0.80000

0.81000

0.82000

0.82000

O.8m000

0.81000

0.78000

0.79000

0.81000

0.81000

0. 81000

0.80000

0.80000

0.79000

0.80000

0.79000

0.80000

0.79000

0. 81000

0.81000

0.79000

0.80000

0.81000

0.78000

0.80000

0.79000

0.80000

0.81000

0. 81000

0.79000

0.81000

0.82000

0.79000

0.79000

0.80000

0.81000

0.81000

0.81000

0.81000

0.82000

0.80000

0.79000

0.81000

0.81000

0.81000

0.80000

0.80000

0.80000

0.81000

0.80000

0.81000

0.80000

0.81000

0.80000

0.82000

0. 81000

0.81000

0.81000

0.01066

0.01065

0.01063

0.01063

0. 01067

0.01071

0.01066

0.01066

0.01069

0. 01069

0.01064

0.01065

0.01065

0.01066

0.01062

0.01057

0. 01054

0.01056

0.01057

0.01057

0. 01 059

0.01058

0. 01061

0.01057

0. 01054

0.01054

0. 01057

0.01055

0.01056

0. 01061

0.01056

0.01050

0. 01050

0.01050

0.01051

0. 01051

0. 01053

0. 01052

0. 01052

0. 01051

0. 01051

0.01051

0. 01048

0. 01047

0.01048

0.01047

0. 01048

0.01044

0.01047

0.01050

0. 01052

0.01050

0. 01048

0.01052

0. 01055

0. 01054

0.01053

0. 01048

0. 01048

0. 01044

0. 01043

0. 01047

0.01050

0. 01047

0. 01051

0.01050

0.02680

0.02686

0. 02716

0.02388

0. 02441

0.02174

0.02923

0. 03092

0. 04086

0. 03759

0.04438

0. 04717

0. 05036

0.05395

0.05105

0. 04837

0. 04881

0.04351

0. 04451

0. 04107

0. 03434

0.02977

0.02661

0.03184

0. 03706

0.03152

0.03005

0.02938

0. 02444

0. 02424

0. 02496

0.02529

0.02256

0.02874

0.02628

0. 02453

0.02115

0.02354

0.02165

0. 02258

0. 02670

0.02945

0. 03672

0. 03597

0. 03944

0.03804

0. 03471

0.03555

0.03161

0.03043

0.02894

0. 02729

0.02224

0. 01867

0.02275

0.01873

0. 01626

0. 01958

0.01988

0.01967

0.02006

0. 01984

0.02697

0.03171

0.02565

0. 02079

89
301.5940 37.19 1.32000

302.7500 37.10 1.32000

304.1170 37.21 1.32000

305.2730 37.10 1.32000

306.4840 37.30 1.32000

307.6410 37.26 1.32000

309.0080 37.32 1.32000

310.2190 37.28 1.32000

311.4300 37.23 1.32000

312.7970 37.34 1.31000

313.9530 37.28 1.31000

315.1640 37.26 1.31000

316.3670 37.43 1.31000

317.7420 37.39 1.31000

318.9530 37.48 1.31000

320.1020 37.12 1.31000

321. 4220 37.43 1.32000

322.6330 37.54 1.31000

323. 8440 37.48 1.31000

325.1640 37.56 1.31000

326.3130 37.48 1.31000

327.5230 37.56 1.31000

328.7340 37.63 1.31000

330.0470 37.63 1.31000

331.2500 37.74 1.31000

332.4610 37.67 1.31000

333.7810 37.74 1.31000

334.9920 37.67 1.31000

336.1410 37.74 1.31000

337.4610 38.21 1.31000

338.6720 37.76 1.31000

339.8200 37.85 1.31000

341.0940 37.94 1.31000

342.3980 37.76 1.31000

343.6090 37.85 1.31000

344.7730 37.85 1.31000

346.0780 37.92 1.31000

347.2420 37.90 1.30000

348.3910 37.90 1.30000

349.7580 37.90 1.30000

350.9220 38.03 1.30000

352.1800 38.01 1.30000

353.3280 37.96 1.30000

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355.8590 38.07 1.30000

357.1170 37.99 1.30000

358.4380 38.01 1.30000

359.6480 38.21 1.31000

360.7970 38.07 1.30000

361.9610 38.14 1.30000

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364.5390 38.23 1.30000

365.7500 38.18 1.30000

367.0700 38.23 1.30000

368.2190 38.05 1.30000

369.4300 38.21 1.30000

370.75W0 38.21 1.30000

371.8980 38.32 1.30000

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374.3200 38.63 1.30000

375.6880 38.27 1.30000

376.8440 38.32 1.30000

378.1090 38.34 1.30000

379.4220 38.29 1.30000

380.6330 38.30 1.30000

381.7890 38.45 1.30000

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383.1640 38.45

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387.9920 34.87

389.2030 38.52

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392.9380 38.60

394.0940 38.65

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400.3520 38.69

401.5000 38.78

402.7730 38.71

404.0940 38.80

405.2890 38.83

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407.7110 38.80

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410.1800 38.76

411.3440 38.91

412.7110 38.83

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415.0230 38.91

416.3280 39.00

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418.7030 39.05

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423.5310 39.09

424.8520 39.07

426.0630 36.38

427.2110 39.14

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450.6640 39.42

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458.0780 39.53

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460.4380 39.75

461.7580 40.29

462.9690 39.67

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90
464.1170 39.58 1.28000

465.3280 39.18 1.28000

466.6480 39.82 1.28000

467.8520 39.80 1.28000

469.0080 39.89 1.28000

470.3280 39.80 1.28000

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472.6880 39.84 1.27000

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480.0470 40.02 1.27000

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492. 4140 40.13 1.27000

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499.8200 40.24 1.26000

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545.5230 40.82 1.26000

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547.8830 40.P6 4.26000

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625.2730 41.92 1.24000

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91
626.4220 42.19 1.24000

627.7970 42.10 1.24000

629.0080 42.17 1.24000

630.1640 42.10 1.24000

631.3670 42.17 1.24000

632.6880 42.30 1.24000

633.8910 42.19 1.24000

635.0470 42.21 1.24000

636.4220 42.21 1.24000

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638.7810 42.25 1.24000

640.1640 42.23 1.23000

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643.7340 42.30 1.24000

645.1020 42.39 1.23000

646.2500 42.32 1.23000

647.4140 42.30 1.23000

648.7190 42.34 1.23000

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99
1924.2581 61.35 1.02000

1925.4139 61.41 1.02000

1926.5699 61.48 1.02000

1927.8831 61.59 1.02000

1929.0389 61.53 1.02000

1930.2500 61.57 1.02000

1931.5630 61.50 1.02000

1932.7729 61.46 1.02000

1933.9840 61.35 1.02000

1935.1880 61.55 1.02000

1936.5081 61.50 1.02000

1937.7190 61.53 1.02000

1938. 9220 61.46 1.02000

1940.2419 61.13 1.02000

1941.3979 61.57 1.02000

1942.5470 61.59 1.02000

1943.9220 61.64 1.02000

1945.0780 61.53 1.02000

1946.2810 61.46 1.02000

1947.4380 61.48 1.02000

1948.8130 63.14 1.02000

1950.0229 62.26 1.02000

1951.2810 61.64 1.02000

1952.5470 61.62 1.02000

1953.7500 61.62 1.02000

1954.9611 61.31 1.02000

1956.3440 61.68 1.02000

1957.4919 61.71 1.02000

1958.7030 61.77 1.02000

1959.9139 61.73 1.02000

1961.2190 61.71 1.01000

1962.4301 61.64 1.02000

1963.6410 61.93 1.02000

1964.9611 61.73 1.02000

1966.1720 61.75 1.02000

1967.3199 61.42 1.02000

1968.5310 61.79 1.02000

1969.8521 61.73 1.02000

1971.0630 61.84 1.02000

1972. 2581 61.73 1.02000

1973.5780 61.86 1.02000

1974.7889 61.79 1.02000

1976.0000 61.82 1.01000

1977.3199 61.82 1.02000

1978. 5310 61.79 1.02000

1979.6801 61.82 1.01000

1980.8910 61.80 1.01000

1982.2111 61.75 1.01000

1983.4139 61.66 1.01000

1984.5699 60.44 1.01000

1985.9380 61.88 1.01000

1987.0940 61.91 1.01000

1988.2500 61.88 1.01000

1989.6169 61.93 1.01000

1990. 7729 61.88 1.01000

1991.9840 61.88 1.01000

1993.1410 61.95 1.01000

1994.5081 61.88 1.01000

1995.7190 61.95 1.01000

1996.8669 61.93 1.01000

1998.2419 61.86 1.01000

1999.3979 61.73 1.01000

2000.6090 61.91 1.01000

2001. 9220 61.84 1.01000

2003.1331 61.95 1.01000

2004.2889 62.00 1.01000

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O.OO730

0.00721

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0.00722

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0.00710

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2006.8130 62.15 1.01000

2007.9690 62.62 1.02000

2009.1169 62.15 1.01000

2010.4380 62.13 1.01000

2011.6479 62.13 1.01000

2012.7970 62.15 1.01000

2014.0081 62.15 1.01000

2015.3280 62.15 1.01000

2016.5310 62.11 1.01000

2017.7419 62.20 1.01000

2019.0630 62.29 1.01000

2020.2111 62.15 1.01000

2021.3669 62.29 1.01000

2022.7419 62.24 1.01000

2023.8910 62.46 1.01000

2025.1021 62.35 1.01000

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2031.3130 62.27 1.01000

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2035.0389 62.40 1.01000

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2567.9299 75.52 0.97000

2569.0779 75.54 0.97000

2570.4609 75.57 0.97000

2571.608 75.68 0.97000

2572.8201 75.77 0.97000

0.90000

0.90000

0.90000

0.90000

0.90000

0.90000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.91000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.92000

0.00317

0.00315

0.00312

0.00311

0.00309

0.00307

0.00306

0.00304

0. 00303

0. 00301

0.00299

0. 00298

0.00296

0.00295

0.00294

0.00293

0.00290

0.00289

0.O288

0.00286

0.00285

0.00284

0.00283

0.00282

0. 00281

0.00280

0. 00278

0.00278

0.00277

0.00277

0. 00276

0. 00275

0.00274

0.00272

0.00271

0.00271

0.00270

0.00269

0.00271

0.00271

0. 00270

0. 00270

0.00269

0.00269

0.00269

0.00268

0.00267

0.00267

0.00267

0.00266

0.00265

0.00262

0.00259

0.002,57

0.00256

0.00254

0.00253

0. 00253

0.00253

0.00253

0.00255

0.00255

0.00255

0.00255

0.00254

0.00252

0. 16876

0.16892

0.16905

0. 16907

0.16893

0.16964

0.16986

0.17036

0.17128

0. 17127

o. 17234

0.17216

0.17238

0.17309

0.17345

0. 17425

0.17456

0.17474

0.17521

0.17452

0.17462

0.17534

0.17541

0. 17559

0. 17609

0.17617

0.17680

0.17736

0.17709

0. 17685

0.17697

0. 17766

0. 17785

0. 17831

0. 17852

0.17896

0.17888

0.17881

0. 17887

0.17918

0. 17951

0. 17993

0. 18020

0.18095

0.18069

0.18079

0.18156

0.18124

0.18147

0. 18152

0.18132

0. 18160

0.18129

0.18105

0.18143

0. 1t893

0.18074

0.18048

0. 18012

0. 17988

0.18037

0. 18033

0. 18040

0.18105

0. 18107

0.18068

103
2574.1411 75.79 0.97000 0.92000 0.00251 0.18023

2575.3521 75.74 0.97000 0.92000 0.00250 0.18014

2576.5000 75.86 0.97000 0. 92000 0.00250 0.16521

2577.6479 76.10 0.97000 0.92000 0.00247 0.12215

2579.0310 75.88 0.97000 0.92000 0. 00244 0.08717

2580.1799 76.13 0.97000 0.92000 0.00242 0.06537

2581.3911 76.06 0.97000 0.92000 0.00238 0.04998

2582. 6479 76.01 0.97000 0. 920 0.00232 0.03758

2583. 8589 76.03 0. 97000 0. 92000 0. 00228 0.02967

2585.0081 76.15 0.97000 0.92000 0.00224 0.02376

104
2) GN021

Time

1.5900

What

0.04125

2.8520

0.04125

4.1210

0.04125

5.3790

0.04125

6.8590

0. 04125

8.1210

0.04125

9.3910

0.04125

10.8200

0.10125

12.1290

0.16500

13.3980

0.21375

14.6090

0.24750

16.0310

0.22875

17.3520

0.19500

18.6210

0.17250

20.0390

0. 15750

21.3090

0. 14250

22.6290

0.13875

24.0510

0. 13500

25.3710

0.13500

26.6910

0.13125

27. 9490

0. 12750

29.3280

0.12750

30.5900

0.12750

31.9100

0.12750

33.3910

0. 13125

34.6480

0.13500

35.8590

0.13500

37.2890

0.13500

38.5510

0.13500

39.8710

0.13500

41.1410

Tts

29.88

Psg(Pa) Pts(Pa) Ws

143000.0 140579.0 0.00083

29.93 143000.0

29.93 143000.0

29.86 143000.0

29.86 143000.0

29.88 143000.0

29.86 143000.0

29.91 143000.0

29.84 142000.0

29.84 143000.0

29.93 143000.0

30.06 142000.0

30.04 142000.0

30.17 142000.0

30.35 142000.0

30.41 142000.0

30.72 142000.0

31.16 142000.0

31.51 141000.0

140579.0

140579.0

140579.0

140579.0

140579.0

140579.0

125246.0

123852.0

121065.0

119671.0

118277.0

116883.0

116883.0

116883.0

118277.0

122458.0

118277.0

119671.0

118277.0

118277.0

111307.0

111307.0

108520.0

104338.0

102944.0

102944.0

101550.0

101550.0

98763.0

101550.0

0.00083

0.00083

0.00083

0.00083

0.00083

0.00083

0.00089

0.00094

0.00099

0.00101

0.00102

0.00105

0.00112

0. 00142

0.00247

0.00337

0.00414

0.00465

0.00502

0.00531

0.00572

0.00613

0.00662

0.00713

0.00754

0.00786

0.00812

0.00844

0.00863

0.00886

Winj

0. 00710

0.00710

0.00710

0.00710

0.00710

0. 00710

0.01580

0.14470

0. 21520

0.26100

0. 28M0

0.30910

0. 31990

0.32800

0.33630

0.34160

0.34650

0.35010

0.35260

0.35390

0.35540

0.35140

0. 34330

0.33120

0. 31590

0.30350

0.29480

0.28360

0.27620

0. 27180

0.26530

0.13500

42.5590

0.13500

43.8280

0.13125

45.0900

0.13125

46. 5700

0.12750

47. 8400

0. 13125

49.1020

0.13125

50.5310

0.13500

51.8520

0.13500

53.1090

0. 13875

54.4300

0.13500

55. 9100

0.13500

57.2300

0. 13875

58.5510

0.13875

59.9690

0.14250

61.2380

0.13500

62.5000

0.13500

63.9800

0.13875

65.2500

0.13500

66.5120

0. 13125

67.7190

0. 13125

69.1480

0. 13125

70.4690

0.12750

71.7300

0.12750

73.1600

0.12750

74.4220

0.12750

75.7380

0. 13125

77.1720

0.12750

78. 4300

0. 12750

79.6910

0. 13125

81. 0120

0.13125

82.4880

0. 13125

83. 8090

0.12750

35.64

35.73

35.93

36.13

36.20

36.33

36.55

36.73

36.77

36.75

36.97

37.22

37.44

37.70

37.75

37.88

37.90

37.93

37.97

37.99

38.04

38.15

38.39

38.50

38.77

38.85

39.12

39.36

39.63

39.63

140000.0

140000.0

140000.0

141000.0

140000.0

140000.0

141000.0

140000.0

140000.0

140000.0

141000.0

141000.0

141000.0

141000.0

141000.0

141000.0

141000.0

140000.0

140000.0

140000.0

140000.0

140000.0

140000.0

141000.0

140000.0

140000.0

140000.0

140000.0

140000.0

140000.0

109914.0

105732.0

100157.0

109914.0

100157.0

109914.0

112701.0

114095.0

119671.0

116883.0

112701.0

119671.0

118277.0

118277.0

116883.0

119671.0

121065.0

121065.0

121065.0

116883.0

122458.0

123852.0

118277.0

128034.0

129428.0

132216.0

126640.0

128034.0

130822.0

135003.0

0.00909

0.00918

0.00934

0.00955

0.00974

0.00974

0.00975

0. 00974

0.00970

0.00974

0.00991

0.00993

0.00990

0.00987

0.00984

0.00982

0.00976

0.00966

0.00968

0.00972

0.00972

0.00974

0.00981

0.00976

0.00971

0.00964

0.00969

0.00969

0.00963

0.00967

0.00969

0.25980

0.25670

0.25340

0. 25160

0.25060

0.25140

0. 24950

0.24900

0.24810

0.24680

0.24730

0. 24820

0.24880

0.24820

0. 24770

0.24920

0.25070

0.25120

0.25300

0.25390

0.25420

0.25430

0.25220

0. 25170

0.25350

0.25280

0.25330

0. 25790

0.25580

0.25550

0.25560

0.25330

0.25410

32.20

32.86

33.39

34.03

34.35

34.48

34.63

34.81

35.14

35.23

35.16

35.54

141000.0

141000.0

141000.0

141000.0

141000.0

141000.0

140000.0

140000.0

141000.0

141000.0

141000.0

141000.0

39.87 140000.0 129428.0

39.94 140000.0 129428.0 0.00971

85.1290 40.25 139000.0 135003.0 0.00964

105
0.12750

86.5590

0. 12750

87.8200

0. 12750

89.1410

0. 12750

90.6210

0. 13125

91.8280

0. 13125

93.1480

0.13500

94.4690

0.13125

95.8980

0.13500

97.1600

0. 13125

98.4220

0.13125

99.8010

0.13125

101.1090

0.13125

102.4300

0.13125

103.8590

0.13875

105.1210

0.13875

106.4410

0. 14250

107.6990

0.13500

109.1290

0.13500

110. 4490

0.13875

111.7110

0. 14250

113.1410

0. 14250

114.4100

0. 14250

115.7190

0.14625

117.0390

0. 14250

118.4220

0.14250

119.7890

0. 14250

121.1090

0.13875

122.5310

0.13875

123.8010

0.13875

125.1210

0.13875

126.5390

0.13500

127.8090

0.13500

129.0700

40.49 139000.0

40.49 139000.0

40.67 139000.0

40.78 140000.0

41.09 140000.0

41.35 139000.0

41.48 140000.0

41.62 139000.0

41.64 139000.0

41.62 139000.0

41.84 139000.0

41.93 139000.0

42.01 139000.0

42.12 139000.0

42.21 139000.0

125246.0

129428.0

130822.0

128034.0

130822.0

129428.0

147548.0

133609.0

135003.0

129428.0

129428.0

136397.0

128034.0

130822.0

130822.0

0. 00963

0.00964

0.25380

0.25290

0.00963 0.25150

0.00974 0.25230

0.00978

0.00977

0. 00976

0.00973

0.00975

0.00979

0.00985

0.00986

0.00979

0.00995

0.00999

0.01004

0.00996

0.00990

0.00985

0.00984

0.00987

0.00989

0.00999

0.01002

0.00999

0.00985

42.50 139000.0 130822.0

42.68 139000.0 133609.0

42.99 139000.0 132216.0

42.92 139000.0 137791.0

42.92 139000.0 133609.0

42.90 139000.0 130822.0

43.03 139000.0 126640.0

43.08 139000.0 130822.0

43.21 139000.0 130822.0

43.36 139000.0 132216.0

43.50 139000.0 136397.0

0.25050

0. 25010

0.24970

0.24810

0.24770

0. 24850

0.24970

0. 24730

0. 24720

0. 24440

0.24360

0.24360

0. 24430

0.24490

0.24490

0.24670

0. 24640

0.24640

0.24510

0.24360

0. 24450

0. 24310

0.24500

0. 24450

0.24390

0.24360

0.24530

0.24630

0. 24430

0.13875

130.3280

0.13875

131.8200

0.13875

133.0780

0.12750

134.3980

0.12750

135.8280

0.12750

137.0900

0. 12750

138.3520

0. 12750

139.7810

0.12375

140.9880

0. 13125

142.3090

0.12750

143.6290

0.12750

145. 0510

0.12375

146.3200

0. 12750

147.5310

0. 12750

148.9490

0.12750

150.1600

0.12750

151.4800

0. 13125

152.9100

0.12750

154.2300

0.12750

155.4880

0.12750

156.7500

0. 12375

158.2380

0.12375

159.5510

0. 12375

160.8200

0.12375

162.2500

0.12375

163.5120

0.12375

164.8280

0.12375

166.2620

0.12375

167.5700

0. 12750

168.8400

0.12750

170.1600

0.12750

171. 5310

0.12750

44.74 138000.0

44.96 138000.0

136397.0

130822.0

45.29

45.29

45.44

45.69

45.93

46.26

46.24

46.44

46.39

46.55

46.64

46.75

46.75

46.97

46.79

46.79

46.81

46.88

46.97

46.99

47.08

47.28

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000. 0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

138000.0

130822.0

130822.0

128034.0

130822.0

129428.0

129428.0

129428.0

129428.0

130822.0

129428.0

129428.0

129428.0

130822.0

128034.0

128034.0

129428.0

129428.0

129428.0

129428.0

128034.0

132216.0

125246.0

45.05 138000.0 128034.0

45.24 138000.0 132216.0

0.00988 0.24330

0.00988 0. 24450

0.00987 0.24510

0.00995 0.24240

O.00996 0.24060

0.00994 0.23900

0. 00995 0.24090

0.00995 0. 24310

0.00994 0.24110

0.00995 0.24150

0.01001 0.24200

0.00994 0.24080

0.00994 0.24070

0.00997 0.24000

0.01004 0.24040

0.01002 0.24210

0.01004 0.24170

0.01009 0.24070

0. 01012 0. 24040

0. 01010 0.23960

0.01009 0.24090

0.01005 0.24090

0.01006 0.23960

0.01004 0.23980

0.01006 0.24170

0.01005 0. 24240

43.56 139000.0 132216.0 0.00974

43.65 139000. 0 132216.0 0.00981

43.67 139000.0 135003.0 0.00983

43.98 138000.0 129428.0 0.00987

44.27 138000.0 126640.0 0.00989

44.40 138000.0 132216.0 0.00991

44.62 138000.0 132216.0 0.00993

47.32 138000.0 126640.0 0.00999

47.41 138000.0 126640.0 0.01002

47.39 137000.0 125246.0 0.01003

0.24220

0.24180

0. 24270

0. 24420

0.24360

0.24250

0. 24040

47.48

47.37

47.52

137000.0

137000.0

137000.0

125246.0

130822.0

126640.0

0. 01007

0.00993

0.00984

172.8520 47.59 137000.0 125246.0 0. 00986

106
0.12750 0.14250

174.1090 47.68 137000.0 126640.0 0.00990 0.24190 217.7190 49.58 136000.0 122458.0 0.01010 0.23950

0.12750 0.14250

175.5390 47.70 137000.0 128034.0 0.00999 0.24000 219.1990 49.63 '137000.0 122458.0 0.01015 0.23710

0.13125 0.14625

176.8590 47.74 137000.0 126640.0 0.01001 0.23990 220.4100 49.80 137000.0 123852.0 0.01018 0.23620

0.12750 0.15000

178.0590 47.85 137000.0 128034.0 0.01002 0.23910 221.7300 49.87 136000.0 123852.0 0.01017 0.23620

0.12375 0.15000

179.5510 47.96 137000.0 125246.0 0.01007 0.23860 223.0510 50.00 136000.0 122458.0 0.01015 0.23620

0.13125 0.15000

180.8090 48.10 137000.0 125246.0 0.01009 0.23970 224.4800 50.18 136000.0 122458.0 0.01016 0.23670

0.13125 0.14625

182.0700 48.12 137000.0 126640.0 0.01007 0.24110 225.7380 50.36 136000.0 123852.0 0.01007 0.23750

0.12750 0.14250

183.2810 48.19 137000.0 128034.0 0.01004 0.24140 227.0590 50.49 136000.0 125246.0 0.01008 0.23720

0.13125 0.14625

184.7110 48.28 137000.0 128034.0 0.01006 0.24090 228.4880 50.76 136000.0 123852.0 0.01013 0.23730

0.13500 0.14625

185.9690 48.56 137000.0 126640.0 0.01010 0.23990 229.8010 50.92 136000.0 122458.0 0.01015 0.23760

0.13875 0.14250

187.2380 48.72 138000.0 128034.0 0.01015 0.23960 231.1210 51.05 137000.0 121065.0 0.01017 0.23690

0.14250 0.14625

188.7190 48.92 137000.0 126640.0 0.01017 0.24030 232.4410 51.14 136000.0 123852.0 0.01018 0.23810

0.13875 0.15000

189.9800 49.16 137000.0 126640.0 0.01015 0.24080 233.9220 51.27 137000.0 123852.0 0.01016 0.23780

0.13875 0. 14625

191.3010 49.21 137000.0 123852.0 0.01018 0.23980 235.1910 51.47 136000.0 121065.0 0.01016 0.23860

0.14250 0.14250

192.6720 49.34 137000.0 123852.0 0.01016 0.24060 236.5120 51.63 136000.0 121065.0 0.01013 0.24020

0.14250 0.15000

193.9880 49.32 137000.0 126640.0 0.01015 0.23990 237.9880 51.67 136000.0 121065.0 0.01012 0.23960

0.13875 0.15000

195.2620 49.29 137000.0 126640.0 0.01013 0.24170 239.2500 51.83 136000.0 123852.0 0.01006 0.24010

0.13500 0.15000

196.5200 49.23 137000.0 126640.0 0.01010 0.24220 240.4610 51.94 136000.0 121065.0 0.00998 0.24130

0.13125 0.14250

197.8910 49.12 137000.0 125246.0 0.01009 0.24270 241.8910 52.00 136000.0 121065.0 0.00997 0.24170

0.13125 0.14250

199.2110 49.14 137000.0 125246.0 0.01010 0.24240 243.1480 52.27 136000.0 122458.0 0.00994 0.24160

0. 13500 0. 13875

200.5310 49.09 137000.0 123852.0 0.01003 0.24250 244.4100 52.38 136000.0 122458.0 0.00996 0.24130

0.13875 0. 13875

201.9610 49.09 137000.0 126640.0 0.01003 0.24250 245.7300 52.40 138000.0 122458.0 0.01000 0.23950

0.13875 0.13500

203.1 720 49.01 137000.0 125246.0 O.01000 0.24200 247.1600 52.51 135000.0 122458.0 O.00998 0.23870

0.13875 0.13500

204.4300 49.10 137000.0 126640.0 0.01003 0.24120 248.4800 52.71 135000.0 122458.0 0.00994 0.23950

0.14250 0.13125

205.8010 49.18 137000.0 123852.0 0.01005 0.24070 249.8010 52.78 135000.0 119671.0 0.00992 0.24030

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843.4880

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864.6910

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93.88 119000.0

93.79 119000.0

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94.04 .119000.0

118277.0 0.00376

94.00

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94.20

94.13

94.13

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94.22

94.31

94.35

94.33

94.40

94.40

94.47

94.56

94.51

94.58

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94.67

94.58

94.67

94.76

94.65

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94.76

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883.4690 95.23 118000.0 119671.0 0.00319

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884.7890 95.43 118000.0 119671.0 0.00317

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886.0510 95.37 118000.0 119671.0 0.00315

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887.4300 95.41 118000.0 119671.0 0.00312

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888.7500 95.48 118000.0 119671.0 0.00310

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900.9410 95.77 117000.0 119671.0 0.00292

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912.7500 96.09 117000.0 119671.0 0.00278

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918.0780 96.09 117000.0 118277.0 0.00271

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924.9410 96.35 117000.0 118277.0 0.00266 0.31290

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115
3) P1041 78.3320 35.22 376000.0 34000.0 0.01025 0.15597

79.5430 35.53 376000.0 84000.0 0.01025 0.17569

80.6910 35.42 375000.0 84000.0 0.01026 0.18748

Time Tts Psg(Pa) Pts(Pa) Ws WinJ 81.9490 35.48 375000.0 34000.0 0.01026 0.19270

1.4920 30.83 395000.0 408000.0 0.00082 0.00694 83.1600 3S.51 374000.0 84000.0 0.01028 0.18355

2.7500 30.81 395000.0 408000.0 0.00082 0.00694 84.3200 36.02 375000.0 84000.0 0.01027 0.19782

4.0120 29.88 395000.0 408000.0 0.00082 0.00686 85.6330 35.77 374000.0 84000.0 0.01027 0.19159

5.2810 30.94 395000.0 408000.0 0.00082 0.00694 86.7930 36.28 374000.0 84000.0 0.01027 0.21334

6.6520 30.68 395000.0 408000.0 0.00082 0.00694 88.0000 36.17 374000.0 84000.0 0.01027 0.21525

7.9100 30.90 395000.0 408000.0 0.00082 0.00694 89.3130 36.15 374000.0 840o0.0 0.01028 0.19719

9.1800 31.12 395000.0 408000.0 0.00082 0.00694 90.5200 34.89 374000.0 84000.0 0.01028 0.21246

10.5000 31.01 395000.0 315000.0 0.00084 0.05149 91.7300 35.91 374000.0 84000.0 0.01029 0.24915

11.6990 31.01 390000.0 151000.0 0.00135 0.24878 92.9410 36.39 373000.0 84000.0 0.01029 0.28049

12.9730 30.96 389000.0 98000.0 0.00147 0.28331 94.3130 36.44 373000.0 84000.0 0.01030 0.29058

14.2930 31.29 390000.0 83000.0 0.00186 0.29070 95.5200 36.17 373000.0 84000.0 0.01030 0.26237

15.6600 31.14 389000.0 81000.0 0.00216 0.22539 96.6720 36.42 373000.0 84000.0 0.01031 0.23556

16.8130 31.95 389000.0 82000.0 0.00250 0.18784 97.9920 36.59 372000.0 84000.0 0.01031 0.20585

18.0200 31.80 389000.0 82000.0 0.00284 0.17999 99.1990 36.35 372000.0 84000.0 0.01032 0.20734

19.3400 32.28 388000.0 82000.0 0.00351 0.24783 100.3010 36.13 371000.0 84000.0 0.01032 0.23284

20.5510 32.66 388000.0 82000.0 0.00378 0.29481 101.6720 36.64 371000.0 84000.0 0.01032 0.29258

21.7620 32.15 387000.0 82000.0 0.00411 0.33220 102.8830 36.90 371000.0 34000.0 0.01033 0.28678

23.1330 32.30 387000.0 82000.0 0.00456 0.31012 104.0900 36.81 371000.0 85000.0 0.01033 0.26805

24.3910 32.57 388000.0 82000.0 0.00594 0.28859 105.3010 36.81 371000.0 84000.0 0.01034 0.24311

25.5430 32.46 387000.0 82000.0 0.00718 0.25482 106.6090 37.03 370000.0 84000.0 0.01036 0.22539

26.6990 32.65 386000.0 82000.0 0.00818 0.21187 107.8200 38.70 370000.0 84000.0 0.01036 0.21872

28.0200 32.48 386000.0 81000.0 0.00906 0.17231 109.0310 38.94 370000.0 84000.0 0.01038 0.20894

29.1720 32.52 385000.0 82000.0 0.00960 0.16668 110.2930 36.94 370000.0 84000.0 0.01038 0.23198

30.3830 33.01 385000.0 83000.0 0.01000 0.15039 111.5000 34.61 370000.0 34000.0 0.01038 0.21606

31.6990 32.99 385000.0 83000.0 0.01026 0.13587 112.6020 37.06 370000.0 84000.0 0.01039 0.24122

32.8520 33.10 384000.0 84000.0 0.01038 0.10789 113.9730 37.32 370000.0 84000.0 0.01039 0.25959

34.0630 34.60 386000.0 84000.0 0.01044 0.15183 115.1800 37.14 369000.0 84000.0 0.01040 0.25901

35.3830 33.23 385000.0 84000.0 0.01043 0.11644 116.3910 37.28 369000.0 84000.0 0.01041 0.26815

36.5820 32.75 384000.0 84000.0 0.01041 0.12982 117.5510 37.12 368000.0 84000.0 0.01042 0.25741

37.7420 33.32 384000.0 84000.0 0.01037 0.14459 118.8590 37.54 368000.0 84000.0 0.01043 0.26049

38.9490 33.25 384000.0 84000.0 0.01034 0.11529 120.0200 37.21 368000.0 84000.0 0.01044 0.26757

40.2620 33.43 382000.0 84000.0 0.01032 0.12715 121.2300 37.90 368000.0 84000.0 0.01044 0.30353

41.4730 33.54 383000.0 84000.0 0.01030 0.17097 122.5430 37.63 368000.0 84000.0 0.01045 0.33691

42.6330 33.47 383000.0 84000.0 0.01030 0.17192 123.7500 37.41 367000.0 84000.0 0.01045 0.37312

44.0000 33.76 382000.0 84000.0 0.01029 0.15334 124.9100 37.70 367000.0 84000.0 0.01045 0.35563

45.2110 33.54 383000.0 84000.0 0.01029 0.21171 128.1090 37.54 367000.0 84000.0 0.01046 0.33823

46.3590 34.56 382000.0 84000.0 0.01029 0.17737 127.4300 37.70 367000.0 84000.0 0.01047 0.34698

47.5700 34.00 382000.0 84000.0 0.01028 0.17760 128.6410 37.59 367000.0 84000.0 0.01048 0.36658

48.8910 33.91 382000.0 84000.0 0.01027 0.18026 129.7930 37.50 366000.0 84000.0 0.01049 0.38809

50.1020 34.11 381000.0 84000.0 0.01026 0.16272 131.1090 37.76 366000.0 84000.0 0.01050 0.41679

51. 2500 34.03 381000.0 84000.0 0.01025 0.12846 132.2700 37.72 366000.0 84000.0 0.01051 0.41842

52.5700 34.25 380000.0 84000.0 0.01026 0.11974 133.5310 37.94 366000.0 84000.0 0.01051 0.40481

53.8320 34.16 382000.0 84000.0 0.01026 0.10617 134.8520 38.14 366000.0 84000.0 0.01053 0.40801

54.9800 34.25 381000.0 84000.0 0.01025 0.10480 136.0630 38.14 365000.0 84000.0 0.01054 0.37713

56.3010 34.16 380000.0 84000.0 0.01024 0.13253 137.2620 38.12 365000.0 84000.0 0.01055 0.34329

57.4610 34.62 380000.0 84000.0 0. 01025 0.10837 138.5310 72.47 365000.0 84000.0 0.01055 0.31988

58.6090 34.58 380000.0 84000.0 0.01025 0.09919 139.9020 38.60 365000.0 84000.0 0.01056 0.30511

59.8200 34.71 379000.0 84000.0 0.01025 0. 07938 141.1090 38.05 364000.0 85000.0 0.01057 0.28850

61.1410 34.82 379000.0 84000.0 0.01025 0.05851 142.3710 38.36 364000.0 84000.0 0.01058 0.31274

62.3520 34.62 379000.0 84000.0 0.01025 0.04529 143.8010 38.58 364000.0 84000.0 0.01059 0.32069

63.5000 34.87 379000.0 84000.0 0.01025 0.03847 145.0120 38.43 363000.0 84000.0 0.01059 0.31959

64.8200 35.00 379000.0 84000.0 0.01025 0.04319 146.2700 38.47 363000.0 84000.0 0.01060 0.31414

65.9730 35.07 378000.0 84000.0 0.01024 0.04598 147.6410 38.76 363000.0 84000.0 0.01061 0.30159

67.2300 34.89 378000.0 84000.0 0.01024 0.07890 148.8520 38.80 363000.0 84000.0 0.01062 0.29540

68.5510 35.18 378000.0 84000.0 0.01024 0.13509 150.0120 38.71 363000.0 85000. 0 0.01063 0.29943

69.7620 35.33 377000.0 84000.0 0.01024 0.14756 151.2110 39.02 363000.0 85000.0 0.01064 0.28935

70.9100 35.09 377000.0 84000.0 0.01024 0.13434 152.5900 39.00 363000.0 84000.0 0.01064 0.28984

72.1800 35.13 377000.0 84000.0 0.01024 0.12504 153.8520 39.14 362000.0 84000.0 0.01065 0.30192

73.4410 35.42 377000.0 84000.0 0.01024 0.12020 155.0000 39.22 363000.0 84000.0 0.01065 0.27892

74.6520 35.40 376000.0 84000.0 0.01025 0.13083 156.3830 39.47 362000.0 84000.0 0.01066 0.25571

75.8010 34.98 376000.0 84000.0 0.01026 0.13792 157.5900 39.62 362000.0 84000.0 0.01067 0.26242

77.1720 35.44 375000.0 84000.0 0.01026 0.14434 158.7930 39.29 361000.0 84000.0 0.01068 0.25693

116
160.0000 39.20 361000.0

161. 3830 39.31 361000.0

162.5820 39.31 360000.0

163.8520 40.99 360000.0

165.2230 39.36 360000.0

166.4800 39.42 360000.0

167.6910 39.60 360000.0

169.0700 39.69 360000.0

170.2700 39.80 359000.0

171.4300 39.78 359000.0

172.6910 39.73 358000.0

173.9490 39.71 358000.0

175.1600 40.06 358000.0

176.3710 40.00 358000.0

177.7420 39.96 358000.0

178.9020 40.18 357000.0

180.1090 40.26 357000.0

181.4220 40.17 357000.0

182.6330 40.44 357000.0

183.7930 40.11 357000.0

184.9920 40.29 357000.0

186.3130 40.71 356000.0

187.5200 40.55 356000.0

188.6720 40.49 356000.0

190.0510 40.53 356000.0

191.2620 41.06 356000.0

192. 4610 40.77 355000.0

193.7810 40.73 355000.0

194. 9410 40.97 355000.0

196.1410 40.99 354000.0

197.3010 40.68 355000.0

198.6720 41.30 354000.0

199.8830 41.06 354000.0

201.0900 41.08 354000.0

202.4100 41.10 353000.0

203.6090 41.15 354000.0

204.7700 41.06 353000.0

205.9800 40.97 353000.0

207.3520. 41.26 353000.0

208.5630 41.57 352000.0

209.7700 41.39 352000.0

211.1910 41.37 352000.0

212.3520 41.30 352000.0

213.5510 41.48 351000.0

214.8710 41.39 351000.0

216.0820 41.86 351000.0

217.2930 41.88 351000.0

218.4410 41.81 351000.0

219.8200 41.90 350000.0

221.0200 41.66 350000.0

222.2300 42. 14 349000.0

223.6600 41.88 350000.0

224.8710 41.92 349000.0

226.1330 42.17 349000.0

227.5120 42.25 350000.0

228.6600 42.19 349000.0

229.8130 42.50 349000.0

231.0200 42.45 348000.0

232.3400 42.37 348000.0

233.5510 42.61 347000.0

234.6990 42.74 347000.0

236.0200 42.43 347000.0

237.1720 42.48 347000.0

238.3830 42.76 347000.0

239.5310 42.85 347000.0

240.8520 42.79 347000.0

84000.0 0. 01069

84000.0 0.01070

84000.0 0.01071

84000.0 0.01072

0.0o 0.01072

85000.0 0. 01073

84000.0 0.01074

84000.0 0.01075

84000.0 0.01076

84000.0 0.01077

84000.0 0. 01078

84000.0 0.01078

84000.0 0.01079

84000.0 0.01081

84000.0 0.01081

85000.0 0.01082

84000.0 0.01083

84000.0 0.01083

84000.0 0.01085

84000.0 0.01086

84000.0 0.01087

84000.0 0.01088

84000.0 0.01089

84000.0 0.01089

84000.0 0.01091

84000.0 0.01091

84000.0 0.01092

83000.0 0.01093

84000.0 0.01094

84000.0 0.01094

84000.0 0.01095

84000.0 0.01095

84000.0 0.01096

84000.0 0.01097

84000.0 0.01098

84000.0 0.01099

84000.0 0.01099

84000.0 0.01100

84000.0 0.01101

84000.0 0.01101

84000.0 0.01101

85000.0 0.01101

84000.0 0. 01101

84000.0 0.01102

84000.0 0.01103

85000.0 0.01103

84000.0 0.01103

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84000.0 0.01104

84000.0 0.01104

84000.0 0.01104

84000.0 0.01105

84000.0 0.01106

84000.0 0.01106

83000.0 0.01106

84000.0 0.01106

84000.0 0.01106

84000.0 0.01106

84000.0 0.01107

84000.0 0.01107

84000.0 0.01107

83000.0 0.01107

83000.0 0.01109

83000.0 0.01109

83000.0 0.01110

83000.0 0.01110

0.27050

0.30385

0.30525

0.31233

0.28914

0.29950

0.29238

0.28863

0.32104

0. 34570

0. 34302

0.32683

0.33666

0.33860

0.33556

0. 34029

0.35871

0.37441

0.37209

0. 36717

0. 34493

0.34357

0.33939

0. 32729

0.28303

0.29639

0.32344

0. 34514

0. 34678

0. 34731

0. 33959

0. 31201

0.32165

0.33413

0. 33882

0.35238

0.36307

0.33598

0. 31770

0.30897

0.30622

0. 31901

0.33865

0.35466

0. 35166

0.34492

0.32341

0.32659

0.32577

0. 34045

0. 34025

0.31998

0. 31639

0. 31830

0.32060

0. 33389

0.33812

0. 33751

0.34120

0.33796

0. 34132

0.34781

0.35062

0.35843

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0.37897

242.0120 42.76 347000.0

243.1600 43.14 346000.0

244.5310 42.94 346000.0

245.7420 42.92 .346000.0

246.8910 43.01 ý$34500o.0

248.2110 42.99 345000.0

249.4220 43.05 346000.0

250.5700 43.16 345000.0

251.7810 42.87 344000.0

253.1020 43.14 344000.0

254.3130 43.32 344000.0

255.4610 43.29 344000.0

256.8400 43.76 344000.0

257.9920 43.54 343000.0

259.1410 43.23 343000.0

260.5200 43.60 343000.0

261.7230 43.45 343000.0

262.9920 44.80 343000.0

264.1990 43.63 342000.0

265.6210 43.56 342000.0

266.7810 44.18 342000.0

267.9920 43.74 343000.0

269.3010 43.87 342000.0

270.4610 44.07 342000.0

271.6720 43.87 342000.0

273.0430 44.07 341000.0

274.2500 44.42 341000.0

275.4610 44.00 341000.0

276.6600 42.98 342000.0

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119
648.4490 57.99 287000. 0

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120
810.5430 60.66 267000.0

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1292.7930 77.48 221000.0

1294.0980 78.17 221000.0

1295.2620 77.44 221000.0

1296.4730 79.54 221000.0

83000.0 0.01201

82000.0 0.01201

83000.0 0.01202

83000.0 0. 01202

83000.0 0.01201

82000.0 0. 01200

82000.0 0.01200

82000.0 0.01200

82000.0 0.01200

83000.0 0.01202

82000.0 0. 01201

82000.0 0. 01201

83000.0 0.01201

83000.0 0.01201

2000. 0 0. 01201

830O. 0 0.01202

82000.0 0.01202

82000.0 0.01201

82000.0 0.01201

83000.0 0.01201

82000.0 0.01202

83000.0 0.01202

83O00.0 0.01201

84000.0 0.01201

83000.0 0.01201

83000.0 0.01200

83000.0 0. 01201

83000.0 0.01200

83000.0 0.01201

83000.0 0.01202

82000.0 0. 01202

82000.0 0.01203

83000.0 0. 01203

81000.0 0.01202

83000.0 0.01202

83000.0 0.01202

84000.0 0. 01201

83000.0 0.01201

83000.0 0.01201

84000.0 0.01201

83000.0 0. 01201

82000.0 0. 01201

83000.0 0.01202

83000.0 0.01202

83000. 0 0. 01202

83000.0 0.01202

83000.0 0.01201

83000. 0 0.01202

83000.0 0.01203

83000.0 0.01202

83000.0 0.01202

83000.0 0.01201

83000.0 0.01201

83000.0 0.01201

83000.0 0.01201

84000.0 0.01201

83000.0 0.01201

85000. 0 0.01201

83000.0 0.01201

85O00. 0 0.01201

83000.0 0.01200

83000.0 0.01201

84000.0 0. 01201

84000.0 0.01201

84000.0 0.01201

84000.0 0. 01200

0.00703

0. 00703

0. 00703

0. 00703

0.00704

0.00694

0.00699

0.00698

0.00699

0.00702

0. 00701

0.00703

0.00698

0. 00701

0. 00702

0.00697

0.00703

0. 00701

0. 00701

0.00692

0. 00701

0. 00701

0. 00702

0. 00702

0. 00701

0.00692

0. 00701

0. 00701

0.00693

0. 00701

0. 00701

0.00701

0. 00701

0. 00702

0.00698

0. 00701

0.00700

0.00700

0. 00700

0. 00700

0. 00690

0.00702

0.00694

0. 00702

0.00698

0. 00700

0. 00701

0. 00697

0. 00700

0.00695

0. 00702

0. 00700

0. 00701

0.00695

0.00700

0.00698

0. 00731

0.00817

0.01003

0.01153

0.01160

0. 01033

0.00965

0. 01045

0.01967

0.02358

123
1297.6210 79.45 221000.0 84000.0 0.01200 0.02456 1378.8480 83.50 214000.0 97000.0 0.01183 0.24657

1298.9880 83.53 221000.0 84000.0 0.01200 0.03159 1380.0120 83.88 214000.0 99000.0 0.01182 0.24891

1300.1520 79.92 220000.0 84000.0 0.01201 0.04824 1381.3320 82.16 214000.0 100000.0 0.01180 0.25414

1301.3010 80.47 221000.0 84000.0 0.01200 0.04922 1382.5270 82.02 214000.0 100000.0 0.01178 0.25880

1302.6680 78.22 220000.0 84000.0 0.01200 0.04172 1383.8010 83.19 214000.0 101000.0 0.01176 0.26330

1303.8320 78.73 220000.0 84000.0 0.01201 0.03926 1385.0590 82.12 213000.0 100000.0 0.01174 0.26636

1305.0270 79.78 220000.0 85000.0 0.01202 0.04792 1386.3790 80.91 213000.0 100000.0 0.01174 0.26795

1306.1910 80.68 220000.0 84000.0 0.01201 0.05912 1387.6450 84.28 213000.0 101000.0 0.01174 0.26942

1307.5590 80.32 220000.0 85000.0 0.01202 0.07524 1388.9100 84.20 213000.0 102000.0 0.01172 0.27200

1308.7150 79.83 220000.0 84000.0 0.01201 0.08035 1390.2770 82.70 213000.0 103000.0 0.01171 0.27593

1309.9180 78.29 220000.0 84000.0 0.01200 0. 06398 1391.5430 83.95 213000.0 101000.0 0.01169 0.27778

1311.2380 80.81 220000.0 85000.0 0.01200 0.07474 1392.7540 84.51 213000.0 102000.0 0.01169 0.27790

1312.4490 80.52 219000.0 85000.0 0.01201 0.07537 1394.1210 83.75 212000.0 103000.0 0.01167 0.28163

1313.5980 80.03 219000.0 85000.0 0.01201 0.07892 1395.3320 84.35 213000.0 103000.0 0.01167 0.28404

1314.9180 78.09 219000.0 86000.0 0.01201 0.09296 1396.5430 83.12 213000.0 103000.0 0.01165 0.28514

1316.1290 79.80 220000.0 86000.0 0.01201 0.08845 1397.7540 82.61 213000.0 103000.0 0.01164 0.28708

1317.3400 80.57 219000.0 85000.0 0.01201 0.08890 1399.1210 83.86 213000.0 104000.0 0.01163 0.28948

1318.5510 79.58 220000.0 85000.0 0.01201 0.09002 1400.3320 85.45 213000.0 104000.0 0.01161 0.29127

1319.9180 81.28 219000.0 85000.0 0.01200 0.10184 1401.6520 83.39 213000.0 105000.0 0.01160 0.29448

1321.0740 80.88 218000.0 85000. 0 0.01200 0.10708 1402.9730 85.40 212000.0 105000. 0 O.01158 0.29774

1322.2770 80.43 219000.0 85000.0 0.01199 0.10545 1404.2300 73.78 212000.0 105000.0 O.O1157 0.30047

1323.5980 80.39 219000.0 85000.0 0.01199 0.09628 1405.4410 84.34 211000.0 106000.0 0.01154 0.30287

1324.8090 83.11 220000.0 86000.0 0.01199 0.09253 1406.8710 83.84 212000.0 106000.0 0.01151 0.30538

1325.9650 78.69 219000.0 85000.0 0. 01200 0.09786 1408.1290 85.09 212000.0 106000.0 0.01150 0.30691

1327.2770 80.10 220000.0 86000.0 0.01199 0.09781 1409.3400 85.41 212000.0 107000.0 0.01149 0.30919

1328.4340 80.88 220000.0 87000.0 0.01200 0.10575 1410.5980 83.57 211000.0 107000.0 0.01146 0.31153

1329.5900 81.53 218000.0 86000.0 0.01200 0.11849 1411.9180 83.46 211000.0 107000.0 0.01145 0.31398

1330.7930 81.33 219000.0 87000.0 0.01200 0.12333 1413.0740 83.66 212000.0 108000.0 0.01142 0.31487

1332.1680 81.19 218000.0 86000.0 0.01199 0.13032 1414.2770 86.02 211000.0 108000.0 0.01141 0.31662

1333.3240 81.46 217000.0 86000.0 0.01199 0.12960 1415.5980 84.22 211000.0 108000.0 0.01140 0.31900

1334.5270 79.65 218000.0 88000.0 0.01200 0.13290 1416.8090 84.56 211000.0 109000.0 0.01138 0.32059

1335.8480 81.19 219000.0 86000.0 0.01200 0.13441 1417.9650 87.27 211000.0 109000.0 0.01137 0.32275

1337.1130 80.75 217000.0 88000.0 0.01199 0.13592 1419.2770 84.43 212000.0 109000.0 0.01136 0.32436

1338.3240 80.72 218000.0 86000.0 0.01198 0.14072 1420.4880 87.11 211000.0 109000.0 0.01134 0.32619

1339.6450 78.83 217000.0 88000.0 0.01198 0.14293 1421.6990 87.16 211000.0 109000.0 0.01133 0.32649

1340.8480 80.03 217000.0 87000.0 0.01198 0.14851 1422.9020 85.88 211000.0 109000.0 0.01132 0.32704

1342.0040 79.27 217000.0 87000.0 0.01197 0.15099 1424.2770 86.89 211000.0 109000.0 0.01131 0.32754

1343.2150 79.54 217000.0 89000.0 0.01198 0.15618 1425.4340 87.43 211000.0 109000.0 0.01130 0.32899

1344.5270 79.69 216000.0 89000.0 0.01197 0.16381 1426.6450 84.74 211000.0 109000.0 0.01129 0.32996

1345.7300 80.37 216000.0 90000.0 0.01198 0.16520 1427.9650 86.69 211000.0 110000.0 0.01127 0.33002

1346.8950 81.73 216000.0 90000.0 0.01197 0.16735 1429.1130 85.91 210000.0 110000.0 0.01126 0.33141

1348.2150 79.67 216000.0 89000. 0 0.01198 0.17123 1430.3240 85.55 210000.0 110000.0 0.01126 0.33302

1349.4100 82.51 216000.0 88000.0 0.01198 0.17006 1431.4730 86.55 210000.0 110000.0 0.01125 0.33342

1350.5740 79.97 216000.0 90000.0 0.01197 0.16997 1432.8480 85.21 210000.0 111000.0 0.01124 0.33437

1351.7770 81.51 216000.0 92000.0 0.01197 0.17647 1434.0040 87.99 211000.0 111000.0 0.01123 0.33499

1353.0900 79.61 216000.0 91000.0 0.01196 0.18239 1435.2620 86.35 210000.0 111000.0 0.01121 0.33557

1354.2540 82.18 216000.0 91000.0 0.01196 0.18700 1436.5820 87.05 211000.0 111000.0 0.01120 0.33618

1355.4650 79.74 216000.0 91000.0 0.01195 0.18767 1437.7930 87.83 210000.0 111000.0 0.01119 0.33693

1356.7700 82.51 215000.0 92000.0 0.01195 0.19077 1438.9410 86.06 210000.0 111000.0 0.01118 0.33820

1358.0430 79.84 216000.0 92000.0 0.01195 0.19313 1440.2620 83.47 210000.0 112000.0 0.01118 0.33968

1359.1910 79.79 216000.0 93000.0 0.01194 0.19893 1441.4730 88.29 210000.0 112000.0 0.01117 0.34082

1360.5120 80.15 215000.0 92000.0 0.01193 0.20285 1442.6210 87.12 210000.0 112000.0 0.01116 0.34246

1361.7230 80.26 215000.0 92000.0 0.01193 0.20281 1443.8320 87.83 210000.0 112000.0 0.01115 0.34440

1362.8710 82.85 215000.0 92000.0 0.01193 0.20320 1445.1520 88.13 209000.0 112000.0 0.01114 0.34524

1364.0820 82.81 215000.0 92000.0 0.01193 0.20560 1446.3630 88.93 209000.0 112000.0 0.01112 0.34483

1365.4020 80.01 215000.0 93000.0 0.01193 0.20622 1447.5740 87.14 208000.0 112000.0 0.01110 0.34577

1366.5510 84.78 215000.0 95000.0 0.01192 0.21048 1448.8790 88.76 209000.0 113000.0 0.01108 0.34551

1367.6990 80.91 215000.0 94000.0 0.01191 0.21472 1450.0430 88.26 209000.0 113000.0 0.01108 0.34672

1369.0820 83.03 215000.0 94000.0 0.01191 0.21834 1451.3010 89.39 208000.0 113000.0 0.01107 0. 34726

1370.2300 85.31 215000.0 94000.0 0.01191 0.21860 1452.5590 88.58 209000.0 114000.0 0.01104 0.34808

1371.4410 81.06 215000.0 94000.0 0.01192 0.21723 1453.7700 87.60 208000.0 114000.0 0.01103 0.34938

1372.7620 83.01 215000.0 95000.0 0.01190 0.22111 1454.9340 86.92 209000.0 114000.0 0.01101 0.35091

1373.9100 83.57 215000.0 98000.0 0.01189 0.22705 1456.0820 87.23 209000.0 114000.0 0.01099 0.35200

1375.1210 81.51 215000.0 97000.0 0.01186 0.23596 1457.4490 87.61 208000.0 114000.0 0.01098 0.35286

1376.3320 79.73 215000.0 98000.0 0.01185 0.23962 1458.6130 87.30 208000.0 114000.0 0.01096 0.35466

1377.6520 80.97 214000.0 96000.0 0.01184 0.24320 1459.8090 89.90 209000.0 115000.0 0.01095 0.35635

124
p:'j 4.

I ~-

1461.1290 82.94

1462.2930 89.90

1463.4880 89.61

1464.6520 90.06

1465.9730 87.75

1467.1680 89.27

1468.3790 88.29

1469.6990 89.75

1470.9100 87.99

1472.0590. 88.31

1473.3790 89.52

1474.5900 88.50

1475.8010 88.76

1477.0120 88.47

1478.3240 90.53

1479.4800 89.68

1480.6910 91.84

1482.0040 91.61

1483.1600 91.63

1485.6840 90.53

1486.8950 91.45

1488.0510 90.11

1489.1990 92.51

1490.5740 89.50

1491.7770 92.02

1492. 9880 93.21

1494.3090 91.27

1495.5200 93.27

1496.6680 93.61

1499.1450 91.68

1500.2930 93.68

1501.5040 91.91

1502.8240 92.58

1503.9730 93.52

1505.1290 91.32

1506.5040 95.05

1507.6520 94.80

1508.8630 94.33

1510.0200 93.29

1511.3950 94.26

1512.5430 95.23

1513.6990 95.05

1515.0740 94.80

1516.2770 93.45

1517. 4880 95. 07

1518. 8010 93.07

1520.0120 95.38

1521.1680 93.23

1522.3710 92.78

1523.6910 92.98

1524.9650 94.80

1526.1600 94.65

1527.5430 95.36

1528.6910 95.86

1529.9020 96.15

1531.2230 94.98

1532.4340 96.17

1533.5200 94.51

1534.6840 95.47

1536.0510 95.38

1537.1990 95.92

1538.4100 96.15

1539.6840 93.68

1540.8320 92.55

1542.0430 94.36

1543.3630 96.38

208000.0

208000.0

208000.0

208000.0

208000.0

207000.0

207000.0

207000.0

207000.0

208000.0

207000.0

207000.0

207000.0

207000.0

207000.0

207000.0

206000.0

206000.0

206000.0

206000.0

207000.0

206000.0

206000.0

206000.0

206000.0

207000.0

206000.0

206000.0

206000.0

206000.0

206000.0

205000.0

206000.0

206000.0

205000. 0

207000.0

205000.0

205000.0

204000.0

204000.0

205000.0

205000.0

204000.0

205000.0

204000.0

204000.0

204000.0

205000.0

203000.0

204000.0

204000.0

203000.0

203000.0

203000.0

203000.0

203000.0

204000.0

203000.0

204000.0

203000.0

203000.0

204000.0

203000.0

203000.0

203000.0

203000.0

115000.0

115000.0

115000.0

115000.0

116000.0

115000.0

116000.0

116000.0

117000.0

117000.0

117000.0

117000.0

118000.0

119000.0

119000.0

119000.0

119000.0

120000.0

120000.0

121000.0

121000.0

121000.0

121000.0

122000.0

122000.0

123000.0

122000.0

123000.0

123000.0

124000.0

124000.0

124000.0

125000.0

125000.0

125000.0

126000.0

126000.0

126000.0

127000.0

127000.0

127000.0

128000.0

128000.0

128000.0

128000.0

12900. 0

129000.0

129000.0

129000.0

129000.0

129000.0

129000.0

130000.0

130000.0

130000.0

130000.0

130000.0

130000.0

129000.0

130000.0

129000.0

130000.0

130000.0

130000.0

130000.0

130000.0

0.01093

0. 01092,,

0.01091

0.01089

0. 01087

0.01085

0. 01084

0. 01082

0.01080

0.01078

0. 01075

0.01073

0. 01071

0.01069

0.01066

0.01065

0.01063

0.01059

0.01056

0. 01052

0. 01050

0.01048

0. 01046

0. 01044

0. 01042

0. 01039

0. 01036

0. 01034

0. 01032

0.01027

0.01025

0.01022

0. 01020

0.01017

0.01014

0.01011

0.01008

0.01004

0. 01001

0.00997

0.00995

0.00992

0.00989

0.00987

0.00984

0.00982

0.00979

0.00977

0.00975

0.00973

0.00972

0.00970

0.00968

0.00966

0.00964

0.00963

0.00963

0.00963

0.00963

0.00962

0.00961

0.00961

0.00900

0.00959

0.00957

0.00956

0.35916

0.35953

0.36023

0.36071

0. 36103

0.36217

0.36354

0.36564

0.36644

0. 36742

0. 36937

0. 37073

0. 37266

0.37422

0. 37542

0.37725

0.37817

0. 37946

0.38426

0.38502

0.38733

0.38807

0.38962

0.39132

0.39303

0.39418

0.39555

0.39724

0.39935

0. 40130

0.40276

0.40284

0.40368

0.40536

0.40679

0.40933

0.41101

0.41254

0. 41472

0.41518

0.41722

0.41792

0.41954

0. 42107

0.42267

0.42381

0.42439

0.42600

0.42597

0. 42546

0.42610

0.42634

0.42748

0.42751

0.42817

0.42821

0.42831

0.42815

0.42822

0.42833

0. 42882

0.42854

0. 42957

0.42992

0.43009

1544.5590

;1545.7230

1546.9340

1548.2380

1549.4490

1550.6600

1552.0270

1553.1910

1554.4020

1555.5510

1556.8710

1558.0820

1559.2770

1560.6600

1561. 8090

1563.0200

1564.3400

1565.4880

1566.6990

1567.8480

1569.2300

1570.3790

1571.6450

1572.9100

1574.1130

1575.3240

1576.6990

1577.9020

1579.1130

1580.3790

1581.7540

94.20 203000.0

96.22 202000.0

93.99 202000.0

96.26 202000.0

94.58 202000.0

96.29 202000.0

94.37 ý202000. 0

94.96 I202000.0

94.62 202000.0

97.14 202000.0

97.05 201000.0

95.14 201000.0

95.52 202000.0

97.61 201000.0

95.34 201000.0

98.06 201000.0

98.00 201000.0

96.44 201000.0

96.04 201000.0

96.71 201000.0

98.04 201000.0

96.67 201000.0

97.88 200000.0

96.89 201000.0

96.98 202000.0

99.45 203000.0

98.62 203000.0

98.71 203000.0

98.26 202000.0

98.71 203000.0

97.47 203000.0

130000.0

130000.0

130000.0

131000.0

131000.0

131000.0

131000.0

131000.0

131000.0

131000.0

132000.0

132000.0

132000.0

133000.0

133000.0

133000.0

133000.0

134000.0

134000.0

134000.0

134000.0

135000.0

135000.0

135000.0

127000.0

125000.0

123000.0

122000.0

121000.0

120000.0

118000.0

0.00955

0.00953

0.00953

0.00951

0. 00950

0.00948

0. 00947

0.00945

0.00943

0. 00941

0. 00938

0.00935

0.00933

0.00930

0.00927

0. 00925

0.00922

0.00920

0.00917

0.00916

0.00913

0. 00911

0. 00908

0.00867

0. 00572

0.00419

0. 00321

0. 00265

0. 00225

0. 00195

0. 00171

0. 43031

0.43080

0. 43103

0.43131

0.43228

0.43235

0. 43311

0. 43443

0.43546

0.43605

0.43614

0.43609

0.43621

0.43673

0. 43677

0.43753

0.43848

0.43973

0.44156

0.44270

0. 44353

0. 44540

0. 44671

0.44784

0.44307

0.43239

0.42186

0.41246

0. 40455

0.39670

0. 38987

125
4) PN041

Time Tts Psg(Pa) Pts(Pa) Ws

1. 5390 31.36 398000.0 409000.0 0.00082

Wmat

0.03500

2.8590 32.59 398000.0 409000.0 0.00082

0.03460

4.2300 31.36 398000.0 409000.0 0.00082

0.03470

5.4880 31.42 398000. 0 409000.0 0. 00082

0.03470

6.9800 31.31 398000.0 409000.0 0.00082

0.03470

8.3010 31.33 398000.0 409000.0 0.00082

0.03480

9.6090 31.38 398000.0 409000.0 0.00082

0.03490

11.1020 31.40 398000.0 409000.0 0.00082

0.03500

12.4690 31.33 398000.0 409000.0 0.00082

0.03490

13.7300 31.42 398000.0 409000.0 0.00082

0.03500

15.2700 31.38 398000.0 403000.0 0.00083

0.03780

16.5900 31.49 395000.0 332000.0 0.00095

0.20700

17.9100 31.42 393000.0 302000.0 0.00105

0.28320

19.1680 31.31 393000.0 299000.0 0.00116

0.24470

20.5390 31.71 393000.0 290000.0 0.00131

0.22270

21.8090 32.15 393000.0 295000.0 0.00146

0.21600

23.1290 32.92 392000.0 253000.0 0.00179

0.21250

24.6090 33.87 391000.0 203000.0 0.00269

0.20230

25.8710 34.65 391000.0 184000.0 0.00333

0.19940

27.1290 35.16 391000.0 172000.0 0.00383

0.19090

28.6210 35.66 391000.0 165000.0 0.00531

0.18610

29.9410 36.04 390000.0 163000.0 0.00698

0. 19060

31.2500 36.35 390000.0 161000.0 0.00843

0.19430

32.6800 36.55 390000.0 159000.0 0.00977

0.19370

34.0000 39.45 389000.0 158000.0 0.01068

0.19080

35.3200 38.66 389000.0 157000.0 0.01136

0.19550

36.5780 36.72 389000.0 158000.0 0.01185

0. 19980

38.0080 36.79 388000.0 158000.0 0.01226

0.20870

39.3280 36.94 388000.0 157000.0 0.01250

0.20700

40.6990 37.39 388000.0 158000.0 0.01267

0.21520

42.1290 37.72 387000.0 156000.0 0.01282

Wini

0.00690

0.00690

0.00690

0.00690

0.00690

0.00690

0.00690

0.00690

0.00690

0.00690

0.00770

0.27790

0.46170

0.57720

0.66670

0. 71900

0. 74670

0.72930

0.69530

0.66040

0.62460

0.59760

0.57580

0.55830

0.54640

O.53610

0.52940

0.52350

0.52140

0.51880

0.51660

0.21360

43.3910 37.92 387000.0 157000.0 0.01291

0.21990

44.6600 38.34 387000.0 156000.0 0.01299

0.21940

46.1410 38.76 386000.0 156000.0 0.01304

0.21690

47.4610 39.00 386000.0 156000.0 0.01307

0.22410

48.6680 39.18 386000.0 156000.0 0.01311

0. 22480

49.9800 39.47 385000.0 157000.0 0.01313

0. 22440

51.4100 39.69 385000.0 155000.0 0.01314

0.23910

52.7300 39.82 385000.0 155000.0 0.01315

0.23560

53.9880 40.11 385000.0 155000.0 0.01316

0.24390

55.4800 40.33 384000.0 155000.0 0.01318

0.24470

56.7890 40.48 384000.0 154000.0 0.01318

0. 25160

58.1090 40.73 384000.0 154000.0 0.01319

0.25870

59.6020 40.97 383000.0 155000.0 0.01320

0.25760

60.9100 41.24 383000.0 155000.0 0.01320

0.26080

62.2300 41.41 382000.0 153000.0 0.01320

0.26260

63.6600 41.66 382000.0 153000.0 0.01322

0.27460

64.9180 41.79 382000.0 153000.0 0.01324

0.27970

66.2380 42.14 382000.0 153000.0 0.01323

0.27990

67.5590 42.43 382000.0 153000.0 0.01325

0.27530

68.9880 42.76 382000. 0 152000.0 0.01326

0.27190

70.3090 43.12 381000.0 153000.0 0.01328

0.27110

71.5700 43.29 381000.0 152000.0 0.01329

0.27270

73.0510 43.63 380000.0 15100.0 O0.01330

0.27780

74.3200 43. 69 380000.0 152000.0 0.01331

0.28050

75.6290 43.89 380000.0 152000.0 0.01332

0.28070

77.1210 44.31 380000.0 153000.0 0.01333

0.28380

78.3790 44.42 380000.0 152000.0 0.01335

0.27810

79.6990 44.64 380000.0 151000.0 0.01336

0.28830

80.9610 44.91 379000.0 152000.0 0.01337

0.29440

82.4410 45.28 379000.0 152000.0 0.01337

0.28400

83.7580 45.37 379000.0 152000.0 0.01338

0.29190

85.0780 45.66 378000.0 153000.0 0.01340

0.28900

86.5590 46.01 378000.0 152000.0 0.01341

0.51350

0.51180

0.50960

0.50970

0.50910

0.50920

0.50750

0.50690

0. 50670

0.50680

0.50590

0.50500

0.50560

0.50500

0.50370

0.50330

0. 50160

0.49950

0.49900

0. 49940

0.49870

0.49850

0. 49880

0. 49760

0.49580

0.49710

0.49740

0. 49770

0.49810

0. 49850

0.49900

0.49850

0. 49790

126
46.32 377000.0 152000.0 0.01342' 0.49790'

0. 28270

87.8280

0.28680

89.1480

0.30010

90.6290

0.30840

91.9490

0.31360

93.2700

0.31130

94.6910

0.30950

96.0080

0.31510

97.3280

0. 31400

98.6480

0.32190

100.1290

0.32200

101.3910

0.32020

102.7110

0. 32440

104.1990

0.31890

105.5080

0.32270

106.8280

0.32400

108.2580

0.33150

109.5780

0.32880

110.8980

0.32860

112.1600

0.33310

113.6410

0.33060

114.9610

0.32970

116.2810

0.33080

117.7580

0.33300

119.0780

0.33310

120.3980

0.33200

121.8790

0.33290

123.1410

0.33090

124.4610

0.32060

125.8910

0.32600

127.2110

0. 32710

128.5310

0.32110

129.8520

0.32760

131.3280

51.04

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47.30 376000.0

47.70 376000.0

47.96 376000.0

48.25 375000.0

48.54 375000.0

48.74 375000.0

48.78 375000.0

49.05 375000.0

49.40 374000.0

49.62 374000.0

54.03 374000.0

50.15 373000.0

50.48 373000.0

50.79 373000.0

50.99 372000.0

51.12 372000.0

51.43 372000.0

51.70 372000.0

51.81 372000.0

52.08 371000.0

52.28 371000.0

52.61 370000.0

52.74 370000.0

53.01 370000.0

53.06 369000.0

53.30 369000.0

53.45 369000.0

53.66 368000.0

53.92 368000.0

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0. 49780

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132.5900

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133.9100

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135.3910

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136.6600

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137.9180

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139.3980

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140.7810

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142.0900

0.28410

143. 4100

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144.8980

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147.5310

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148.9610

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150. 2810

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151.6020

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153.0200

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154.3400

0. 29510

155.6600

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157.0900

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158.4100

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159.6680

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161.0390

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162.5310

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163.8400

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165.1600

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166.6480

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169.2300

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170.7110

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172. 0310

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173. 2890

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174.6090

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55.94 366000.0 152000.0

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57.37 366000.0 152000.0

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57.72 365oo0.0 152OO0.0

57.86 365000.0 151000.0

57.97 365000.0 154000.0

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58.26 364000.0 149000.0

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59.26 36M000.0

59.44 363000.0

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60.06 362000.0

60.51 361000.0

60.57. 361000.0

148000.0

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177.4100 61.97 359000.0 148000.0 O.01396

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178.7300 62.22 359000.0 150000.0 0.01397

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180.1600 62.35 359000.0 147000.0 0.01398

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181.4800 62.53 35M00. 0 150000.0 0.01399

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182.7890 62.64 358000.0 150000.0 0.01399

0.31080

184.2190 63.00 358000.0 148000.0 0.01399

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185.4300 63.27 357000.0 148000.0 0.01399

0. 30740

186.7500 63.47 358000.0 151000.0 0.01400

0.32020

188.2300 63.82 357000.0 148000.0 0.01400

0.32240

189.5510 63.84 357000.0 151000.0 0.01401

0. 31980

190.8710 64.18 356000.0 154000.0 0.01402

0.32790

192.1910 64.38 356000.0 151000.0 0.01402

0.32440

193.6680 64.53 356000.0 149000.0 0.01402

0. 31780

195.0390 64.91 356000.0 148000.0 0.01404

0.31650

196.3090 65.18 355000.0 150000.0 0.01405

0. 31210

197.7890 65.45 355000.0 148000.0 0.01404

0.31330

199.0510 65.34 355000.0 147000.0 0.01404

0.31600

200.3710 65.83 355000. 0 148000.0 0.01404

0.31480

201.8520 66.05 354000.0 147000.0 0.01404

0. 32430

203.1210 66.25 354000.0 149000.0 0.01405

0.33020

204.4300 66.76 354000.0 149000.0 0.01405

0.32470

205.8590 66.50 354000.0 146000.0 0.01406

0.31950

207.1800 66.83 353000.0 150000.0 0.01406

0. 31790

208.5000 67.03 353000.0 151000.0 0.01406

0. 31030

209.8200 67.16 353000.0 149000.0 0.01407

0.31230

211.3010 67.39 352000.0 149000.0 0.01406

0. 31210

212.5590 67.56 352000.0 149000.0 0.01407

0.31050

213.8790 67.83 352000.0 148000.0 0.01407

0.31370

215.3590 67.99 351000.0 148000.0 0.01406

0.32110

216.6290 68.14 351000.0 146000.0 0.01407

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217.8910 68.39 351000.0 149000.0 0.01407

0. 31710

219.3710 68.63 351000.0 14900. 0 0.01409

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220.6910 68.76 350000.0 148000.0 0.01410

0.48030

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0.47720

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0. 47840

0. 47780

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0. 32410

222.0080 69.01 350000.0 148000.0 0.01410

0.32270

223.3280 69.41 350000.0 149000.0 0.01411

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224.8090 69.52 350000.0 150000.0 0.01412

0. 32130

226.1290 69.63 349000.0 151000.0 0.01411

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227.4490 69.94 349000.0 149000.0 0.01411

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228.9300 70.19 349000.0 149000.0 0.01410

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230.1910 70.50 348000.0 151000.0 0.01410

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231.5080 70.79 348000.0 147000.0 0.01413

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233.0000 70.94 348000.0 151000.0 0.01413

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234.2580 71.12 348000.0 149000.0 0.01412

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235.5780 71.30 348000.0 152000.0 0.01411

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237.0590 71.50 347000.0 150000.0 0.01413

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238.3790 71.68 347000.0 149000.0 0.01415

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239.7500 71.90 347000.0 149000.0 0.01415

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241. 0080 72.02 347000.0 150000.0 0.01416

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242.4410 72.13 346000.0 151000.0 0.01416

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243.7580 72.37 346000.0 149000.0 0.01414

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245.0780 71.77 345000.0 148000.0 0.01414

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246.5080 72.68 345000.0 149000.0 0.01414

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247.8280 72.93 345000.0 148000.0 0.01414

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249.1410 73.15 345000.0 147000.0 0.01415

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250.5700 73.29 344000.0 147000.0 0.01415

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251.8910 73.40 344000.0 147000.0 0.01417

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253.2110 73.49 344000.0 147000.0 0.01417

0.32500

254.5310 73.60 344000.0 149000.0 0.01418

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256.0080 74.02 343000.0 147000.0 0.01417

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257.3280 73.93 343000.0 149000.0 0.01418

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258.6480 74.00 343000.0 147000.0 0.01417

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260.0700 74.11 343000.0 147000.0 0.01417

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261.3910 74.31 342000.0 145000.0 0.01416

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262.7110 74.54 342000.0 144000.0 0.01417

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264.1410 72.15 342000.0 147000.0 0.01417

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265.4610 74.67 342000.0 146000.0 0.01417

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266.7190

0.33370

268.1480

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269.4100

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270.7300

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272.0510

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273.4800

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276.0000

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277.4880

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278.8590

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280.1210

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281.6020

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282.8710

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286.9880

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288.2500

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289.5700

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291.0510

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295.1680

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307.1990

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308.6290

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309.9490

74.76 342000.0

74.92 341000.0

75.07 341000.0

75.43 340000.0

75.52 340000.0

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75.81 340000.0

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76.17 339000.0

76.15 339000.0

76.42 339000.0

76.53 339000.0

76.62 338000.0

76.84 338000.0

76.86 338000.0

77.18 337000.0

77.40 337000.0

77.60 337000.0

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¶6.4660•

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314.0700

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315.3280

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316.6990

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318.1290

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324.8280

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326.3090

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327.5780

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328.8980

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330.3200

0. 32170

331.6410

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332.9610

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334.2810

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338.3400

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351.8520

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79.84 332000.0

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80.16 332000.0

80.34 331000.0

80.41 331000.0

80.50 331000.0

80.65 330000.0

80.79 330000.0

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81.14 329000.0

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82.11 328000.0

82.22 328000.0

82.69 327000.0

85.09 327000.0

82.64 327000.0

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0.01421

0.01422

0. 01422

0. 01422

0.01420

0.01421

0.01421

0. 01420

0. 01420

0. 01420

0.01421

0.01420

0.01420

0. 01420

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0.01421

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0.01421

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0. 45700

0.45870

0.45740

0.45720

0.45780

0.45710

0. 45670

0. 45700

0. 45760

0.45780

0.45840

0.45780

0.45740

0.45790

0.45680

0.45710

0.45740

0.45630

0.45610

0.45620

77.85 336000.0 141000.0 0.01419

77.85 336000.0 142000.0 0.01420

77.98 335000.0 153000.0 0.01420

78.16 335000.0 150000.0 0.01420

78.30 334000.0 150000.0 0.01421

78.41 334000.0 146000.0 0.01421

78.63 334000.0 148000.0 0.01419

78.77 334000.0 145000.0 0.01420

78.97 333000.0 147000.0 0.01421

79.08 333000.0 143000.0 0.01421

79.24 333000.0 142000.0 0.01421

79.49 332000.0 144000.0 0.01420

79.60 332000.0 146000.0 0.01420

147000.0 0.01422 0.45460

143000.0

143000.0

139000.0

146000.0

152000.0

143000.0

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0.01421

0.01420

0.01420

0. 01420

0. 01420

0.01421

0.01421

0.01421

0.01421

0.01419

0.01419

0.01419

0. 45430

0.45320

0.45370

0.45240

0. 45180

0.45310

0.45380

0. 45430

0. 45430

0. 45780

0. 45850

0.45940

129
0.33230

355.9690

0.33040

357.3980

0.32710

358.7190

0.32400

360.0390

0.32340

361.4690

0.31230

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364.0510

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365.3710

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366.7890

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368.1090

0.31550

369.4300

0. 31730

370.9100

0.31360

372.2300

0.32330

373.5510

0. 32500

374.9800

0.32380

376.3010

0.32790

377.6090

0.32550

379.0390

0.32570

380.3590

0.31960

381. 6800

0. 31780

382.9410

0.32050

384.4300

0.31320

385.7380

0.31920

387.0590

0.32030

38.5390

0.32620

389.8090

0.32520

391.1290

0. 31910

392.6090

0.32090

393.9300

0. 31950

395. 2500

0.32010

396.5080

0. 3218O

397.9880

0.33180

399.3090

84.84

84.82

85.02

85.04

85.40

85.36

85.67

85.38

323000.0

323000.0

323000.0

323000.0

322000.0

322000.0

322000.0

321000.0

321000.0

321000.0

152000.0

147000.0

143000.0

145000.0

140000.0

148000.0

0.01419

0.01418

0.01419

0.01418

0.01419

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85.96

86.05

86.34 321000.0

86.70 320000.0

87.01 320000.0

87.26 320000.0

87.51 320000.0

87.66 319000.0

87.84 319000.0

88.13 319000.0

88.33 318000.0

88.65 318000.0

88.81 318000.0

88.94 318000.0

89.05 318000.0

89.05 317000.0

89.34 317000.0

89.43 317000.0

90.06 316000.0

89.54 316000.0

89.61 316000.0

89.63 316000.0

89.68 315000.0

89.77 315000.0

89.88 315000.0

150000.0 0.01418

141000.0 0.01420

144000.0 0.01419

149000.0 0.01419

141000.0 0.01420

145000.0 0.01419

138000.0 0.01420

142000.0 0.01420

140000.0 0.01419

140000.0 0.01419

139000.0 0.01418

137000.0 0.01419

139000.0 0.01419

143000.0 0.01419

143000.0 0.01418

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143000.0 0.01419

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140000.0 0.01418

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0.45700

0.45640

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0. 45450

0.45270

0. 45460

0.45390

0.45300

0.45390

0. 45370

0.45540

0. 45670

0.45490

0.45350

0.45370

0.45210

0.45260

0. 45180

0. 45150

0. 45280

0.45080

0.44820

0.44710

0. 44900

0. 44980

0.44710

0.44500

0.44660

0. 44510

0. 44490

0.44510

0.44730

0. 44840

0. 33460

400.6290

0. 34100

402.1090

0.34340

403.4300

0. 33220

404.7500

0.33630

406.1800

0.33310

407.4880

0.33260

408.8090

0.33560

410.2380

0. 33430

411.5590

0.34590

412.8200

0.33860

414.1910

0.33530

415.6210

0.32690

417.0000

0.33410

418.3090

0.32960

419.7380

0.33250

421.0590

0.33460

422.3200

0.33810

423.8090

0.33720

425.0700

0. 33480

426.3910

0.32820

427.6480

0.32840

429.1290

0. 33120

430.4490

0.32380

431.7190

0. 32760

433.0900

0. 33130

434.4100

0.32390

435.7300

0. 31840

437.1480

0. 31590

438.4690

0.31640

439.7890

0. 32400

441.2190

0.32510

442.4800

0.32770

443.7380

90.75 314000.0

90.87 313000.0

91.20 313000.0

91.36 313000.0

91.60 313000.0

91.92 312000.0

92.01 312000.0

92.26 312000.0

92.30 311000.0

92.48 311000.0

92.66 311000.0

93.00 311000.0

93.13 311000.0

93.24 310000.0

93.40 310000.0

93.47 310000.0

93.56 310000.0

93.67 309000.0

93.71 309000.0

93.83 309000.0

93.92 308000.0

93.98 3O8000.0

94.10 308000.0

94.28 308000.0

94.30 308000.0

94.41 307000.0

94.26 307000.0

94.48 307000.0

147000.0

140000.0

142000.0

143000.0

146000.0

138000.0

143000.0

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146000. 0

140000.0

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145000.0

144000.0

143000.0

142000.0

143000.0

139000.0

138000.0

143000.0

141000.0

139000.0

141000.0

143000.0

142000.0

137000.0

0.01418

0.01418

0.01418

0.01417

0.01416

0.01415

0.01417

0.01416

0.01416

0.01415

0.01415

0.01414

0.01414

0.01414

0.01414

0.01415

0.01415

0.01416

0.01414

0.01413

0.01413

0.01412

0.01412

0.01414

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89.90

86.22

90.19

90.28

315000.0 146000.0 0.01418

314000.0 142000.0 0.01418

314000.0 141000.0 0.01417

314000.0 140000.0 0.01418

90.57 314000.0 142000.0 0.01419

0.44700

0. 44620

0. 44680

0.44540

0. 44270

0.44640

0.44620

0.44760

0.44870

0.44940

0. 44920

0. 44700

0. 44850

0.45060

0.45060

0.45080

0. 45050

0.45040

0. 45090

0.45040

0.44890

0. 44930

0.44850

0.44720

0. 44740

0.44910

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0.45020

0. 45110

0. 45030

0.44970

0.45170

0. 45420

143000.0 0.01413

145000.0 0.01411

140000.0 0.01410

130
0.32550

445.0590

0.32890

446.5510

0.32930

447.8090

0.33180

449.1290

0.33440

450.5590

0.33580

451.8710

0.34010

453.1910

0.33470

454.6210

0.34540

455.9410

0.35250

457.2580

0,35670

458.5200

0.36740

460.0000

0.38080

461. 3200

0.38170

462.6410

0.38190

464.1210

0.38580

465.3910

0.39310

466.6480

0.40310

468.1290

0. 41310

469.3910

0.41700

470.7110

0. 42030

472.1990

0.42920

473.5060

0. 44300

474.8280

0.44080

476.1480

0.44600

477.6290

0.46030

478.8980

0.45730

480.1600

0.44760

481. 6410

0.44090

482.9610

0.45150

484.2810

0.43810

485.7580

0. 46180

487.0310

0. 45780

488.3400

94.46 307000.0 145000.0 0,01411

94.59 306000.0 144000.0 0.0141

94.66 306000.0 138000.0 0.01412

94.61 305000.0 138000.0 0.01412

94.57 304000.0 149000.0 0.01411

94.84 303000.0 138000.0 0.01410

94.90 302000.0 147000.0 0.01409

94.95 302000.0 136000.0 0.01409

95.02 301000.0 139000.0 0.01407

95.10 300000.0 141000.0 0.01405

95.22

95.33

95.47

95.44

95.51

95.69

95.80

95.94

96.12

96.21

300000.0

300000.0

300000.0

299000.0

299000.0

298000.0

298000.0

298000.0

297000.0

297000.0

140000.0

148000.0

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134000.0

136000.0

143000.0

144000.0

133000.0

133000.0

136000.0

0.01407

0.01407

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0.01408

0. 01409

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0.01408

0.01408

0.01408

0.45420

2 0.45330

0.45300

0.45370

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0.45480

0.45480

0.45330

0.45440

0.45370

0.45180

0.45030

0.45080

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0.44520

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0.44240

0.44060

0.43980

0.44030

0.43760

0.43620

0.43830

0.44100

0.44750

0.45630

0.46390

0.47040

0.46460

489.6600 97.20

0. 45160

491.1480 97.16

0.44630

492.4610 97.22

0.44730

493.7300 97.36

0.44440

495.2110 97.47

0.43520

496.5310 97.52

0. 43940

497.8520 97.63

0.43590

499.3280 97.81

0.44110

500.5900 97.90

0.43240

501.9100 97.85

0. 43440

503.3400 98.08

0. 42430

504.6600 98.17

0.42500

505.9800 98.26

0.41680

507.2380 98.26

0.41190

508.6680 98.56

0.40120

509.9800 98.76

0.40340

511.2500 98.91

0.40510

512.6800 99.05

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513.9880 99.37

0.40740

515.3090 99.50

0.40290

516.7380 99.61

0. 40120

518.0000 99.73

0.39480

519.3200 100.09

0.38330

520.6990 100.38

0.37990

522.1800 100.58

0.37760

523.4410 100.74

0. 37810

524.6990 100.97

0.36820

526.1910 101.28

0. 36180

527.4490 101.39

0.35580

528.7700 101.55

0.35180

530.2500 101.94

0.35050

531.5700 102.12

0. 34010

532.8910 102.32

292000.0

292000.0

291000.0

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157000.0

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0.01380

0.01372

0.01363

0.01354

291000.0 160000.0 0.01345

291000.0 167000.0 0.01331

290000.0 166000.0 0.01318

290000.0 168000.0 0.01304

290000.0 168000. 0 0.01295

289000.0 172000.0 0.01282

289000.0 176000.0 0.01266

289000.0 175000.0 0.01252

96.37 297000.0 136000.0 0.01408

288000.0

288000.0

287000.0

288000.0

287000.0

286000.0

287000.0

286000.0

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283000.0

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205000.0

206000.0

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96.55 296000.0

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97.06 294000.0

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133000.0

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135000.0

137000.0

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0.01068

0.01047

0. 01034

0. 01021

0. 01005

0.00985

0.00967

0.00949

0.47630

0.48250

0. 48870

0.49550

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0.51110

0.51860

0.52570

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0.58480

0.59040

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0.63020

0.63520

0.63900

0.64550

0.65010

0.65470

282000.0 211000.0 0. 00933 0.66090

282000.0 213000.0 0.00916 0.66550

131
0.33270

534.3200 102.70

0.32920

535.6290 103.02

0.32830

536.9490 103.27

0.32600

538.2700 103.56

0.31980

539.7500 103.74

0.31160

541.0700 104.01

0.30270

542.3910 104.26

0.30410

543.8200 104.60

0.28770

545.1410 104.78

0.27940

546.4610 105.03

0. 27460

547.8790 105.28

0. 26960

549.1990 105.44

0.26410

550.5200 105.64

0.25970

551.9490 105.93

0.25700

553.2700 106.07

0. 24710

554.5780 106.36

0.23710

555.8980 106.66

0.22300

557.3910. 106.95

0.21690

558.6480 107.18

0.21440

559.9690 107.42

0.20400

561.3980 107.63

0.20530

562.6600 107.92

0.20270

563.9800 108.08

0.20160

565.4610 108.40

0.19230

566.7190 108.71

0.18160

568.0390 108.81

0.18140

569.3590 109.03

0.17300

570.7890 109.21

0.16000

572.1090 109.39

0.15280

573.4180 109.71

0.15170

281000.0

281000.0

281000.0

280000. 0

280000.0

279000.0

279000.0

279000.0

279000.0

278000. 0

214000.0

216000.0

217000.0

219000.0

221000.0

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225000.0

229000.0

231000.0

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0.00894

0.00877

0.00860

0.00841

0.00820

0.00801

0.00784

0.00764

0.00744

0.00722

278000.0 234000.0 0.00704

277000.0 236000.0 0.00686

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278000.0 238000.0 0.00655

277000.0 240000.0 O.00640

277000.0 243000.0 0.00624

276000.0 245000.0 0.00605

277000.0 246000.0 0.00586

276000.0 248000.0 0.00571

276000.0 249000.0 0.00557

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275000.0 251000.0 0.00531

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275000.0 253000.0 0.00506

275000.0 254000.0 0.00494

274000.0 255000.0 0.00485

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274000.0 257000.0 0.00462

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273000.0 258000.0 0.00441

0. 67110

0. 67430

0.67910

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0.79270

132
NRC FORM 335 U.S. NUCLEAR REGULATORY COMMISSION 1. REPORT NUMBER

(2-9) (Aassge by NRC. Add VoL., Sipp., Rev, NRCM 1102. BIBOGRAPHIC DATA SHEET .)

3201. 3202 NUREG/IA-0134

2. TITLE AND SUBTITLE

Assessment of RELAPS/MOD3.1 for Gravity-Driven Injection Experiment in the

Core Makeup Tank of the CARR Passive Reactor (CP-1300) 3. DATE REPORT PUBISHEY

October 1996

4. FIN OR GRANT NUMBER

W6238

S. AUTHOR(S) 6. TYPE OF REPORT

Sang II Lee, Hee Cheon NoJKAIST Technical

Young Seok Bang, Hho Jung Kim/KINS

7. PERIOD COVERED pou.siw DO•s•)

B. PERFORMINGORGANIZATION - NAME AND ADDRESS (FNRC, provieavisi Oft& Regior U.S. MJCIWrRegQ 'yCOITarl3sion. and meigddross, Iamhcknr

provide name and wafini addess.)

Korea Advanced Institute of Science and Technology Korea Institute of Nuclear Safety

Nuclear Engineering Department Advanced Reactor Dept.

373-1, Gusung-Dong P.O. Box 114

Yusung, Taejon 305-701 Korea Yusung, Taejon 305-600 Korea

9. SPONSORING ORGANIZATION - NAME AND ADDRESS (WNRC, Inve 'Sme as above', Wori , proid N Dmi, Office orRgi U.S. Mucker ftubbr, Cvmfiown

and waIng addss.)

Office of Nuclear Regulatory Research

U.S. Nuclear Regulatory Commission

Washington, DC 20555-0001

10. SUPPLEMENTARY NOTES

S. Smith, NRC Project Manager

11. ABSTRACT (OX wors cra,)

The objective of the present work is to improve the analysis capability of RELAP5IMOD3., on the direct

contact condensation in the core makeup tank (CMT) of passive high-pressure injection system (PHIS) in

the CARR Passive Reactor (CP-1300). The gravity-driven injection experiment is conducted by using a

small scale test facility to identify the parameters having significant effects on the gravity-driven injection

and the major condensation modes. The condensation modes are divided into three modes: sonic jet,

subsonic jet, and steam cavity. RELAP5/MOD3.I is chosen to evaluate the code predictability on the

direct contact condensation in the CMT. It is found that the predictions of MOD3.1 are in better

agreement with the experimental data than those of MOD3.0. From the nodalization study of the test

section, the 1-node model shows better agreement with the experimental data than the multi-node

models. RELAPSIMOD3.1 identifies the flow regime of the test section as vertical stratification.

However, the flow regime observed in the experiment is the subsonic jet with the bubble having the

vertical cone shape. To accurately predict the direct contact condensation in the CMT with

RELAP5/MOD3.1, it is essential that a new set of the interfacial heat transfer coefficients and a new flow

regime map for direct contact in the CMI" be developed.

12. KEY WORDS/DESCRIPTORS A mwodsn crws a gi heta iassist msarcher in a g she oWa0.J 13. AVALABLITY STATEMENT

CAMP unlimited

RELAP5/MOD3 14. SEcURIT•YCLA.SS1AcKON

unclassified

Thas AepAo0

unclassified

15. NUMBER OF PAGES

16. PRICE

NR FR I3 l Inh Ir IoaaIy wse rdue by ll t eea Fm.bc

NRC FORM 335 (2419) This form vas electronically produced by Eke• Federal Famm. Ir_


Federal Recycling Program

UNITED STATES

NUCLEAR REGULATORY COMMISSION

WASHINGTON, DC 20555-0001

SPECIAL STANDARD MAIL

POSTAGE AND FEES PAID

USNRC

PERMIT NO. G-67

OFFICIAL BUSINESS

PENALTY FOR PRIVATE USE. $300