NBS SPECIAL PUBLICATION 260-34

U.S. \RTMENT

OF

Immerce

National

«<r7

Standard Reference Materials:

THERMOELECTRIC VOLTAGE OF

SILVER-28 ATOMIC PERCENT GOLD

THERMOCOUPLE WIRE, SRM 733,

VERSUS COMMON THERMOCOUPLE MATERIALS

(BETWEEN LIQUID HELIUM AND

ICE FIXED POINTSj
NATIONAL BUREAU OF STANDARDS

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Bureau of Standards JN 2 7 1972 r^^ occ

'^0 Standard Reference Materials:

n

i^O'Z'-i Thermoelectric Voltage of Silver-28 Atomic Percent Gold Thermocouple Wire, SRM 733, Versus Common Thermocouple Materials (Between Liquid Helium and Ice Fixed Points)

L. L. Sparks and J. G. Hust

Institute for Basic Standards

National Bureau of Standards

Boulder, Colorado 80302

U.S. DEPARTMENT OF COMMERCE, Peter G. Peterson, Secretary NATIONAL BUREAU OF STANDARDS, Lewis M. Branseomb, D/recfor, Issued April 1972
Library of Congress Catalog Number: 72-600029

National Bureau of Standards Special Publication 260-34

Nat. Bur. Stand. (U.S.), Spec. Publ. 260-34, 34 pages (Apr. 1972) CODEN: XNBSAV

Issued April 1972

For Bale by the Superintendent of Documents, U.S. Government Printing Office Washintgon, D.C. 20402 (Order by SD Catalog No. C 13.10:260-34). Price 40 cents.
PREFACE

Standard Reference Materials (SRM's) as defined by the

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Inquiries concerning the technical content of this

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vii
Table of Contents

1 . Introduction 2

2. Material Characterization and Specimen Preparation .... 4

3. Thermocouple Comparator 8

4. Data Analysis 9

5. Results and Discussion 11

6. Acknowledgements 12

7. References and Footnotes 13

List of Figures

Figure 1. Thermoelectric voltage of Ag - 25 at % Au versus Ag - X at % Au between 4 and 76 K. Error bars

represent ±2'^ values 16 Figure 2. Electrical residual resistivity of Ag - X at % Au

alloys 17 Figure 3. Electrical residual resistivity ratio of the ends

of the five spools of SRM 733. The standard

deviation of these measurements is 0.0014 18 Figure 4. Thermoelectric comparisons of Ag - 28 at % Au

wires, annealed at various currents, to an SRM

733 wire (Ag - 28 at % Au annealed with 3.5 A).

The comparisons were made between 4 and 273. 15 K

and the error bars represent ± 2 a values 19 Figure 5. Thermoelectric intercomparisons of SRM 733 wire

from each of the five stock spools. Intercomparisons were made with respect to a SRM 733 comparator between 4 and 273. 15 K and a Pt-67 comparator between 76 and 273. 1 5 K. The Pt-67 versus SRM 733 values have been normalized to show only the spool-to- spool variations. The

error bars represent ± 2 a values 20

viii

I
Figure 6a. Typical Thermocouple Arrangement 21 Figure 6b. Comparator Circuit for Calibration of Standard

Reference Thermocouple Wires 21 Figure 7a. Details of comparator construction (pictorial

view) 22 Figure 7b. Details of comparator construction (junction

terminal blocks ) 23 Figure 7c. Details of comparator construction (wiring

diagram) 24 Figure 8. Intercomparison of three SRM 733 thermocouple

comparators via a common thermocouple wire.

The error bars represent ± 2 a values 25 List of Tables

Table 1. Chemical Composition of SRM 733 14 Table 2. Thermoelectric voltage for SRM 733 versus commonly used thermocouple wire between liquid

helium and ice fixed points 15

ix

THERMOELECTRIC VOLTAGE OF SILVER - 28 ATOMIC PERCENT GOLD THERMOCOUPLE WIRE, SRM 733,

VERSUS COMMON THERMOCOUPLE MATERIALS

(Between Liquid Helium and Ice Fixed Points )''~

L. L. Sparks and J. G. Hust

Institute for Basic Standards

National Bureau of Standards

Boulder, Colorado 80302

Industry wide standardization of thermocouple wire depends, in part, on the ability to thermoelectrically compare commercial wires

with a Standard Reference Material (SRM). The alloy Ag - 28 at % Au,

SRM 733, meets the requirements of a thermoelectric reference

material, particularly in the temperature range of liquid helium and

liquid hydrogen where Pt-67 is not adequate. Thermoelectric voltage

comparisons are reported for SRM 733 versus common thermocouple

materials between liquid helium and ice fixed points. Detailed stan- dard reference data based on these common materials are given in NBS Monograph 124. The comparisons were made in a thermocouple

comparator which was designed to be a permanent holder of three SRM

733 wires; the comparator allows tests to be made without handling the standard wires . Details of the construction, testing, and analysis of the comparators are givexi.

Key words: Cryogenics; Seebeck voltage; silver - gold alloy; standard

reference material; thermocouple.

* This work was carried out at the National Bureau of Standards,

Boulder, Colorado, under the sponsorship of the National Bureau of Standards, Office of Standard Reference Materials (NBS-OSRM),

Washington, D. C.

1
IJ Introd action

The ability to standardize thermocouple wires depends, in part, on the availability of a reliable StcUidard Reference Material (SRM). In addition, thermocouple materials must be well characterized if excessive manufacturer-to-manufacturer, batch-to-batch, or spool-to-spool

variations are to be avoided. Because of the difficulty of accurately

characterizing thermocouple wires in terms of composition or other

commonly used parameters, they must be controlled primarily by direct thermoelectric measurements. If these direct thermoelectric measurements are made with respect to an SRM which, in turn, is compared to standard reference data, then industry-wide uniformity is possible. The

first step of this program, to establish such standard reference data

for commonly used thermocouples at cryogenic temperatures, has been

completed by Sparks, et al., [1] at the National Bureau of Standards,

Boulder, Colorado. The next step, to establish an SRM, is the subject of this paper. The general requirements for a thermoelectric SRM are that the material:

(1) be insensitive in thermoelectric power to small changes in composition,

(2) be readily fabricated into the desired form and quantity at reasonable cost, and

2
(3) be easy to use in practice, i. , be flexible, ductile, and

chemically compatible with the measurement system.

In some instances it is also important to have a material with low thermal conductivity and a thermoelectric power near the median of the thermoelectric power of commonly used thermocouple materials. Tests made earlier in this laboratory by Powell, et al. , [z] on a series of silver -gold alloys (20 to 40 atomic percent gold) indicated

that silver with approximately 25 to 30 at % gold met the above require- ments. Since that time, more extensive tests have been performed

on six silver -gold alloys (25, 26, 27, 28, 29, and 30 at % gold).

These tests were conducted with experimental arrangements described

in a later section. The results of these measurements, figure 1, show

that the systematic emf variation among these wires (from 4 to 76 K)

is small (approximately 0. 1 |jV/at % Au). Based on the previous

measurements by Powell, et al., [z] and these later measurements,

silver - 28 at % gold was selected as a suitable low temperature

thermoelectric SRM. This report describes the research performed

to establish and maintain this silver -gold alloy as an SRM.

Traditionally, platinum is used by thermocouple wire manufacturers for production control. At temperatures above approximately 50 K platinum is a suitable SRM; however, below 50 K the thermoelectric power of platinum becomes sensitive to physical

imperfections and trace chemical impurities, notably iron. This

low-temperature sensitivity to imperfections i? typical for pure

materials. In view of past use, applicability at higher temperatures,

extensive characterization, and availability in the form of homogeneous wire, platinum will also be maintained as a low

temperature thermoelectric SRM. A report on platinum dS such a

3
stcindard will be a subsequent publication in this series. It is to be 1 remembered that at lower temperatures (~ 4 K) spurious emfs

generated by inhomogeneities in platinum may be as much as ten times

greater than the spurious emfs found with the silver -28 at % gold alloy.

Thus, platinum is recommended for measurements at temperatures as low as liquid nitrogen (76 K) and the silver -gold alloy is recommended

for measurements below 76 K.

2. Material Characterization and Specimen Preparation

A specially prepared lot of Ag -28 at % Au alloy was fabricated as wire for further testing and to establish and maintain a thermoelectric

standard. The metal was alloyed and cast in 2. 5 cm diameter billets. The billets were swaged to 0. 6 cm diameter, drawn to 0. 06 cm with

carbide dies, ajid finally drawn to 0. 020 cm (0. 008 inch) wire with

diamond dies. Drawing was accomplished without lubricant and

without annealing or etching between passes. The wire was supplied

uninsulated to facilitate later annealing. Annealing is necessary

to eliminate physical damage introduced by normal handling, e. g. , winding cind unwinding from the spools. The chemical composition

of the wire is given in table 1. The Ag-Au standard wire was supplied on five spools.

Specimens were cut from both ends of each spool for characterization

measurements. The residual resistivity ratios (RRR = P1s73k/P4K> where p = electrical resistivity) of these 10 specimens were determined

after annealing at 400''C for one hour. Variation in the residual resistivity ratio of annealed specimens indicates variation in composition. The composition variation can be determined from RRR variation

if one knows the specific resistivity, bp^/'bC (p^ = residual resistivity and

C = relative composition in atomic units). BlattLs] has compiled values

of specific

4
resistivity for many elements and lists 0. 4 cm/at % Au in Ag. We

have performed RRR measurements on Ag - 13. 5 at % Au as well as the Ag -28 at % Au alloy. From an approximate (±3%) resistivity measure- ment and by the application of Matthiessen' s rule, we obtain values of versus composition as shown in figure 2. Blatt's [3] specific resistivity,

3P^/BC, is in reasonable agreement with the slope of our curve in figure

2 at low Au concentration. If we assume the form of the residual resistivity — composition relation suggested by Nordheim [4], = 0!C{1 - C), and evaluate the best estimate of a, we obtain 0. 35 p,^cm/at % Au as compared to 0. 40 |j,ji.cm/at % Au listed by Blatt [3]. Using Nordheim' s rule, we have shown that the change in atomic

percent composition, AC, is related to change in residual resistivity ratio,

ARRR, as follows:

Ar - ARRR C(l - C)

^ (RRR - 1) (1 - 2C) • ^ ' The determination of RRR instead of p eliminates the need to determine

o the form factor (cross-sectional area/length) of the specimen; therefore,

the results are both more precise and accurate. The range of RRR variation, ARRR, measured for the ten specimens from the ends of the five spools is 0. 0044, as shown in figure 3. This variation in RRR corresponds

to about 0. 7 atomic percent variation in gold concentration and apparently

is random over the five spools. The thermoelectric variation caused by

a 0. 7 atomic percent composition variation is undetectable, as shown in figure 1. Thus, specimens from the five spools of material should be

thermoelectrically indistinguishable.

5
Specimen preparation is important in obtaining uniform standard

reference thermocouple specimens. The wire must be cleanedj aruiealed,

and subsequently handled with care to avoid chemical contamination or physical damage, either of which can affect thermoelectric power.

Several preanneal cleaning and etching procedures were considered

in order to prevent diffusion of impurities into the wire during the anneal. It was determined that cleaning with a degreasing agent

followed by rinsing in distilled water was adequate. Etching the surface did not make a detectable difference in thermoelectric properties.

Several cuinealing procedures were also investigated. As a first attempt,

the wire was degreased, washed in distilled water, and wrapped on a fused quartz spool. This wire was annealed in an air furnace for one hour at 400°C. This procedure proved unsatisfactory because there was a tendency for the wire to adhere to the spool after annealing; re- moving the wire from the spool undoubtedly introduced some strain. Resistance annealing, i. e. , self heating caused by an electric current through the wire^ resulted in wires which were thermoelectrically more

reproducible. This procedure is convenient and can be done with less chance of chemical contamination or physical strain. The effect of different annealing currents is shown in figure 4. Based on this, an

annealing current of 3. 5 A through the 0. 020 cm diameter wire was

selected as optimum. This current produced a dull red glow (hardly

visible in a darkened room) and resulted in a well-annealed wire. We

found that the Ag-Au wire is weakened and will break with very low

stress after a 4^ 3 A anneal. This may be caused by grain growth

across the wire during the anneal and subsequent hydrogen diffusion

into the grain boundary. These 0. 020 cm diameter wires melt at currents slightly above 4. 3 A. The recommended wire preparation

procedure is:

6
1. Degrease and rinse in distilled water.

2. Suspend wire in air and connect to a current source.

3. Continuously increase current to obtain proper annealing

temperature (3. 5 A for the 0. 020 cm diameter wire).

4. Maintain this temperature for about 30 seconds.

5. Gradually decrease current to zero over about 15 seconds.

6. Handle with care: avoid unnecessary mechanical stresses

of the wire prior to use. Specimen wires from each of the five spools of the Ag - Au alloy were thermoelectric ally intercompared after being prepared as above.

The results, shown in figure 5, show that statistically no difference in thermoelectric power exists among the wires from the five spools.

These comparisons were made with respect to a SRM 733 comparator

for temperatures from 4 to 273. 15 K and a Pt-67 comparator for temperatures from 76 to 273. 15 K. The results from the Pt-67 comparator

have been normalized so as to show only the spool-to-spool variation. These thermoelectric intercomparisons are in accord with the previously mentioned resistivity results. The preceding results, in some instajices, were obtained with

thermocouple comparators. The design and construction of the comparators are described in the next section.

7
I 3. Thermocouple Comparator 1 The basic measurement arrangement for a thermocouple calibra-

| tion measurement is shown in figure 6a. This arrangement is used to determine the difference in thermoelectric emfs, - of wires A i A B

and B between temperatures T^ and Tg. The average thermopower, S, of the thermocouple is defined by (E^ - Eg)/(T2 r T^). Errors are \ introduced into this measurement by (1) the presence of spurious thermal ' emfs caused principally by wire inhomogeneity in regions of high temperature gradient, and (2) improper thermal anchoring to each of the baths.

It is possible to reduce the systematic effect of spurious voltages by taking

readings at different immersion depths and by measuring with respect to more than one reference wire.

The thermal anchoring problem is solved by reducing the thermal

resistance between the wires and the constant temperature baths. This is accomplished by intimate contact between the wires and the liquid over a

sufficient length leading up to the thermocouple junctions. This problem

has been examined carefully both experimentally and theoretically [ 5] . No detectable error due to inadequate thermal anchoring is believed

present in the thermoelectric emfs reported here. The thermocouple

comparator is shown schematically in figure 6b. The selector switch

allows one to measure the thermoelectric emf of the test wire with respect

to each of the reference wires as well as to inter compare each of the reference wires. Inter comparison of the reference wires is done

to detect possible deterioration of these wires or other comparator components. The construction details of the comparator are shown in figures

7a, 7b, and 7c.

8
4. Data Analysis

The experimental data, depicted in figure 6b, are designated

as E^j, E^2' ^T3' "^12' ^23' ^13' subscript T indicates the

test wire while 1, 2, and 3 refer to the three standard reference wires

permanently installed in the comparator. A set of six voltages is obtained for each immersion depth in the forward (T^ to T^) direction as well as in the reverse (T^ to T ^) direction. The values obtained in the forward direction, averaged over the various depths, will be designated by

E. .(F), while the reverse readings are designated E. .(R). The sets of six voltages are illustrated in the following measurement graph.

T

In this figure the vertices represent the wires illustrated and defined in figure 6b, while the lines represent the emfs of the associated thermocouple pairs. For convenience, the vertical position of the vertices

designate the relative position of each wire in the electromotive series,

e. g. , the most theirmoelectrically positive wire is denoted by the upper- most vertex. The most probable (weighted averages) values E^^, E^^'

E^2» -^12' "^13' ^23 obtained from the redundant but independent

equations based on the various paths which can be used to define each E_.

There are four such independent paths which can be used to obtain four estimates of each measured voltage. As an example, the four independent

paths used to estimate E yield the following four equations:

9
(6) = ^Tl

(3) F - ^Tl -'- ^T2 -^12 t

(3) E -

= ^T3 -^13

(2) F - ^Tl -= ^T3 -^12-^23-

The relative weighting, as suming the same variance for each measured

voltage, is shown in parenthesis before each equation. The average

value,

J

, is then

Values of E.. are obtained with such equations for the forward and re- verse directions for each immersion depth. These values are then

averaged to obtain the final value of E_. The values E^^, E^^' ^-^^ E^^ are further averaged to obtain the best estimate of the emf of the

test wire with respect to the SRM.

The values E^^. E,^, and E^^j similarly determined, are used to detect possible systematic changes among the reference wires. Control

charts of E^^' -^13' ^23 ^^^^ ^® maintained to detect such changes in the comparators. To further reduce the possibility of undetected changes

in reference wires, three comparators have been built. The first or working standard will be used for routine testing; the second or primary

standard will be used occassionalLy for comparison to the working comparator. The third comparator will be considered as a replacement for either of the others. Occassional intercomparisons will be made among

all three comparators. Figure 8 illustrates the present intercomparisons

of these three comparators.

10
The determination of the emf of a test wire with respect to the standard reference thermocouple wire is summarized below:

(1) Record the six emfs illustrated in the previous measure- ment graph.

(2) Repeat step 1 for three immersion depths to randomize

spurious emfs.

(3) Repeat (1) and (2) with comparator reversed in the baths.

(4) Compute the most probable values of the six sets of six voltages using all of the redundancy in the data, both for the forward

and reverse directions.

(5) Compute the average emf for the test wire with respect to the reference standard

^TR = [(^Tl + ^TZ + Et3)fWd/^ +(=T1 + ^T2 + ^TsXey/']

and the variance of this emf. This variance is based upon the random

scatter indicated by the redundancy of these measurements.

5. Results and Discussion

SRM 733 is intended for use as a standard reference thermocouple wire at low temperatures. In order for this wire to be useful, one must know the emf generated by this wire with respect to commonly used thermocouple materials. The temperature interval

chosen for standardization of these wires with respect to SRM 733 is 4 to 273. 15 K. The data are based on the extensive measurements of Sparks, et al., [l] and more recent measurements as explained in table 2c The emf of SRM 733 with respect to commonly used wires

over the range 4 to 273. 15 K are presented in table 2.

11
standardization measurements have been made at several

1 intra-spool locations to insure that the variability of SRM 733 does ! not exceed that reported here. As pointed out earlier, this possibility

j is remote because the emf of SRM 733 is insensitive to composition ' change.

Consideration has been given to extending the calibration range

of SRM 733 to higher temperatures. The upper limit of usefulness

would be dictated by the temperature produced by the optimum anneal

described in this paper. This temperature is approximately 500 °C. At the present time the demand for this extension does not justify the additional effort, especially since Pt-67 can be used in this range. SRM 733, issued as 32 AWG wire, 3 meters long, may be ordered from the Office of Standard Reference Materials, Room 3314,

Chemistry Building, National Bureau of Standards, Washington, D.C.

20234. (Longer continuous lengths in multiples of 3 meters can be

obtained by special order to the OSRM).

6. Acknowledgements

We wish to thank the thermocouple manufacturers, especially

Sigmxand-Cohn Corp. , Cominco American, Inc. , and Engelhard

Industries, Inc. , for their cooperation in this program. This program

was initiated and directed in its early stages by R. L. Powell; we

also thank him for his many suggestions throughout the program.

12
7. References and Footnotes

[l] Sparks, L. L. , Powell, R. L. , and Hall, W. J., Reference

Tables for Low-Temperature Thermocouples, NBS (U. S. )» Monogr. 124.

[2] Powell, R. L. , Caywood, L. P., Jr., and Bunch, M. D. , Low Temperature Thermocouples, Temperature -Its Measurement and Control in Science and Industry 3, part 2, 65 (1962).

[3] Blatt, F. J., Physics of Elect ronic Conduction in Solids,

McGraw-Hill Book Co. , N. Y. , p. 199 (1968).

[4] Ziman, J. M. , Electrons ajid Phonons, Oxford at the Clarendon Press, p. 337 (I960).

[5] Hust, J. G. , Thermal Anchoring of Wires in Cryogenic

Apparatus, Rev. Sci. Instr. 41, 622-624 (1970).

[6] Trademark - Wilbur B. Driver Co.

[7] Trademark - Driver-Harris Co.

[S] Trademark - Kanthal Corp.

[9] Trademark - Hoskins Manufacturing Co.

[10] The use of tradenames of specific products is essential to the proper understanding of the work presented here. Their use

in no way implies approval, endorsement, or recommendation

by NBS.

13
Table 1. Chemical Composition of SRM 733

Element ppm, by

Al 0. 5 Ca 0. 5 Cu 0. 3 Fe 2. 0 Pb 0. 3 M 0. 5 Ni 0. 2

Si 2. 0 Au 28 at %

Ag balance

14
Table 2. Thermoelectric voltage for SRM 733 versus commonly used

thermocouple wire between liquid helium and ice fixed points,

^ + Thermocouple EMF, ^V

Pt vs SRM 733 541 ± 3 KP or EP** vs SRM 733 4098. 3 ± 0. 8 TP** vs SRM 733 521. 8 ± 0. 8 5735.2 ± 0. 8 2358. 7 ± 0. 8

These data are calculated from reference data by Sparks, et al.,[l]

and more recent comparisons of the emf of SRM 733 (resistance

annealed at 3.5 A) to the Ag-28 at % Au wire used in [l] which was

oven annealed at 400°C for 1 hour. The Pt-67 wire used here was

resistance annealed at 10 95°C for 1 minute.

t The uncertainties given are twice the estimated standard deviations.

The larger uncertainty for Pt reflects the sensitivity of this pure

material to trace impurities at liquid helium temperature. The

effect of these impurities is strongly dependent on the temperature

distribution along the wire. For dip tests, where the temperature

gradient along the wire is extremely localized, a range of thermal

voltages as large as 15 \j.V has been observed.

EN or TN A copper-nickel alloy, constantan, Cupron [6], Advance [7], Thermo Kanthal JN [8]. KP or EP A nickel-chromium alloy, Chromel [9], Tophel [6], T-1 L7j, Thermo Kanthal KP [8]. KN A nickel

aluminum alloy, Alumel [9], Nial [6], T-2 L7j, Thermo Kanthal [8]. TP Copper, usually electrolytic tough pitch.

The use of trade names does not constitute axi endorsement of any

manufacturer's products. Materials manufactured in compliance with

established standards are equally suitable.

15
0 #

-0.2

>

25 26 27 28 29 30

X,at % Au in Ag

Figure 1. Thermoelectric voltage of Ag-25 at % Au versus Ag-X at % Au

between 4 amd 76 K. Error bars represent ± 2a values.

16
\

<

O

c

1—1 o

o ^

CD C>

o

CVJ <

<

o 00 to oj o

uJi)U^ *AllAllSIS3d ivnais3d

17
CD Oi oo

a.

</> oo

cx OO

Q.

O, m UJ

18
I

0,1 2 3 4

CURRENT, A

Figure 4. Thermoelectric comparisons of Ajg-28 at % Au wires, annealed

at various currents, to an SRM 733 wire ( Ag -28 at % Au

einnealed with 3. 5 A). The comparisons were made between

4 and 273. 15 K and the error bars represent ± 2a values. 19
1.0 I

>^ 0

E Spool

Number

1.0 i SRM733ComparGtor (4 to 273.15 K range) ^ Pt 67 Comparator (76 to 273.15 K range)

Figure 5. Thermoelectric intercomparisons of SRM 733 wire from each

of the five stock spools. Intercomparisons were made with respect to a SRM 733 comparator between 4 and 273. 15 K and

a Pt-67 comparator between 76 and 273. 15 K. The Pt-67

versus SRM 733 values have been normalized to show only the spool-to-spool variations. The error bars represent ± 2a values.

20
Thermal Anchor

I Temperature = Ti

I ^^J Temperature ~ '^Zj

Copper

Wires

FIGURE 6a - TYPICAL THERMOCOUPLE ARRANGEMENT

T = Test Wire

Reference Wire #1

jJTemperature = T |

[

Potentiometer and

Null Detector

Temperature = T FIGURE 6b- COMPARATOR CIRCUIT for CALIBRATION of STANDARD REFERENCE THERMOCOUPLE WIRES

21
Figure 7a. Details of comparator construction (pictorial view).

22
^10-32 NF

Channel for tube carrying

test wire. Cut with hand

grinder after piacennent on

rod. Cut into rod as req'd.

Hand grind notches

for wires after placement on rod.

10-32 NF

Hand grind clearance

slot for 0-80 NF

set screw, (one req'd.)

*56 Drill, thru. 4 Places as shown. DETAIL 'A' DETAIL 'B'

^^-^p"! ^ Hand grind clearance

Slot for A .AJ slot for 0 - 80 N F

insulated ^HVtJ^ set screw, (one req'd.) junctions. "^Se Drill, thru. 2 Places as shown. DETAIL 'C' Figure 7b. Details of comparator construction (junction terminal blocks ^.

23
Electrical connector

Expansion

loop Reference wires {Separate Tubes)- 6 Long , 32 AW6 copper Instrumentation wires

in one flexible tube.

Test wire (Separate Tube)

All wires in separate tubes. Reference wires Wound on nylon

collar (one layer)— Swires wound on nylon collar in separate

layers with teflon tape between layers. I

^ ....

Wires soldered into brass ( Details BSC)

with Wood's metal, (after assembly is complete). Junctions soldered, placed in slot (Detail 'C' and insulated from each other and brass by

layers of Teflon [10] tape secured by wire bands.

^Low melting - <- point solder (both ends)

Details of comparator construction (wiring diagram). 24
WORKING PRIMARY RESERVE

STANDARD STANDARD STANDARD

Figure 8. Intercomparison of three SRM 733 thermocouple comparators

via a common thermocouple wire. The error bars represent

± 2ct values.

U. S. GOVERNMENT PRINTING OFFICE : 1972—481-332/206 25
FORM NBS-114A (1-71) U.S. DEPT. OF COMM. 1. PUBLICATION OR REPORT NO. 12, Gov't Accession BIBLIOGRAPHIC DATA NBS SP 260-34 1 SHEET

3. Recipient's Accession No.

4. TITLE AND SUBTITLE Thermoelectric Voltage of Silver - 28 Atomic Percent Gold Thermocouple Wire, SRM 733, Versus Common Thermocoupl^

Materials (Between Liquid Helium and Ice Fixed Points)

5. Publication Date March 1972

'6. Performing Organization Code

7. AUTHOR(S) L. L. Sparks and J. G. Hust

8. Performing Organization

9. PERFORMING ORGANIZATION NAME AND ADDRESS NATIONAL BUREAU OF STANDARDS DEPARTMENT OF COMMERCE Boulder, Colorado 80302

10. Project/Task/Work Unit No. Project 2752759

11. Contract/Grant No. NBS-OSRM

12. Sponsoring Organization Name and Address National Bureau of Standards

r^ff\i-e^ rif <^f a r\ r\ a r r\ R f»f r f^n f AAatf^rialQ ^ TM R c; _ Oc; R A/T ^ Washington, D. C

13. Type of Report & Period CoveredFinal

14. Sponsoring Agency Code

15. SUPPLEMENTARY NOTES

16. ABSTRACT (A 200-'word or less factual summary of most significant information. If document includes a significant bibliography or literature survey, mention it here.) Industry wide standardization of thermocouple wire depends, in part, on

the ability to thermoelectrically compare commercial wires with a Standard Reference Material (SRM). The alloy Ag - 28 at % Au, SRM 733, meets the requirements of a thermoelectric reference material, particularly in the temperature range of liquid helium and liquid hydrogen where Pt-67 is not adequate. Thermoelectric voltage comparisons are reported for SRM 733 versus common

thermocouple materials between liquid helium and ice fixed points. Detailed standard reference data based on these common materials are given in NBS

Monograph 124. The comparisons were made in a thermocouple comparator

which was designed to be a permanent holder of three SRM 733 wires; the comparator allows tests to be made without handling the standard wires. Details

of the construction, testing, and analysis of the comparators are given.

17. KEY WORDS (Alphabetical order, separated by semicolons) Cryogenics; Seebeck voltage; silver-gold

alloy; standard reference material; thermocouple.

18. AVAILABILITY STATEMENT

[xH UNLIMITED. FOR OFFICIAL DISTRIBUTION. DO NOT RELEASE

TO NTIS.

19. SECURITY CLASS

(THIS REPORT) UNCL ASSIFIED

20. SECURITY CLASS

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34

22. Price

USCOMM-DC 66244. P71
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