>JH. „ , ^ .sbA

^ecUnlcciL ^^ote 92o. 20^

CALCULATIONS OF THE FIELD NEAR THE

APEX OF A WEDGE SURFACE

lAMES R. WAIT AND CAROLEN M. JACKSON

U. S. DEPARTMENT OF COMMERCE

NATIONAL BUREAU OF STANDARDS
U. S. DEPARTMENT OF COMMERCE

Luther H. Hodges, Secretary

NATIONAL BUREAU OF STANDARDS

A, V. Astin, Director

THE NATIONAL BUREAU OF STANDARDS

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Printing Office, Washington, D.C, 20402.
NATIONAL BUREAU OF STANDARDS

technical *^ote 204

Issued November 21, 1963

CALCULATIONS OF THE FIELD NEAR THE

APEX OF A WEDGE SURFACE

James R. Wait and Carolen M. Jackson

Central Radio Propagation Laboratory

National Bureau of Standards

Boulder, Colorado

NBS Technical Notes are designed to supplement the Bureau's regular publications program. They provide a means for making available scientific data that are of transient or limited interest. Technical Notes may be

listed or referred to in the open literature.

For sale by the Superintendent of Documents, U. S. Government Printing Office Washington, D.C. 20402 ONCE 4 5 CETtrS

J.
Lx
C ONTENTS Pag(

1. Introdviction 1

2. Graphical Presentation - Case 1 5

3. Graphical Presentation - Case II 6

4. Graphical Presentation - Case III 6

5. Remarks Concerning Phase 7

6. Effective Surface Impedance 7

7. Concluding Remarks 10

8. References 10

Figures 12

Appendix 25

CALCULATIONS OF THE FIELD NEAR THE APEX OF A

WEDGE SURFACE

James R. Wait and Carolen M. Jackson

Using the exact series solution for diffraction by a

perfectly conducting wedge, numerical results are presented for the structure of the field in the apex region.

This provides insight to the nature of electromagnetic

fields near a surface discontinuity. Furthermore, the

results provide some justification for the use of approximate boundary conditions which have been used previously

in studying radio propagation over terrain features.

1. Introduction

In the bulk of theoretical radio propagation studies, the earth' s surface is assumed to be smooth. Unfortunately, it is known from

experience that the roughness plays an important role in determining the characteristics of the field. A general mathematical treatment of general unevenness of the surface does not seem to be possible

because of the difficulty of rigorously satisfying the boundary conditions.

However, if the surface is gently sloping and/or at long wavelengths,

some simplifying approximations may be made. It is the principal

purpose of the present paper to investigate the validity of these

simplifications.

Considerable success has been achieved by Feinberg [1946] in his

introduction of approximate boundary conditions for solving rough

Surface problems. His idea is to transfer the exact boundary conditions

on the actual surface to a plane reference surface which may or may

not be the mean surface. An example of such a problem would be the

calculation of the field in the neighborhood of a sloping beach at a coast

line. While the land and the sea may often be idealized as flat horizontal surfaces, the transition region will tend to distort the electric

field lines with a subsequent modification of the transmitted wave.

Furthermore, a reflected wave will be produced which may be significant in the operation of radio navigational systems.
In order to establish the validity of the approximate boundary

conditions which have been used for sloping surfaces, it is desirable

to adopt a very simple model which has an exact solution. The wedge

is such a model. It consists of two intersecting plane surfaces which

are semi-infinite in extent. A wedge in the limiting case where the

open angle is 2 tt is often called a knife edge. The exact solution

for the diffracted field in this case may be expressed conveniently

in terms of Fresnel integrals. The knife edge model has been used

extensively in the study of diffraction by mountainous obstacles and

other pronounced relief features. However, in the case of coastal

relief and other low lying features, the knife edge is an inadequate

model and instead the general wedge is more meaningful. For example, a beach with a linear slope can be regarded as the superposition of two wedges.

The model is illustrated in figure 1. The wedge of assumed

perfect conductivity is defined by the surfaces 0=0 and (/) = i[/ with reference to a cylindrical coordinate system (p, 0, z). A plane

wave is incident from the direction = as indicated in figure 1. The field is to be observed at P(p, 0, z) where is in the range

to ijj . For simplicity, the direction of propagation is taken to be

perpendicular to the wedge apex. Also, the incident wave of unit

strength is polarized so that the magnetic field has only a z component. The exact expression for the resultant magnetic field, which

also has only a z component, is given by [Wait, 1959],

00 H=—- )g COSV0 cos V exp (i v n/2) J (k p ) , (1)

Z l]j /_ ITl O V

m = 0, 1, 2, . . .

i

-2-
where v = mTj/\\i, e = I, e =2 for m :^ 0. In this formula,

o m

J (k p ) is the Bessel function of order v and argument kp where

V

k = 2 TT/wavelength.

Series formulas of the kind given by (1) are often

considered to be unuseable because of poor convergence. For this

reason^they are often replaced by asymptotic forms which are

particularly useful when kp is a large parameter and vJj is somewhat greater than 180 . When i]j = 180 or when \\j is any submultiple of n > the series formula given above may be transformed

into a summation from a finite number of image waves. This matter

has been discussed in some detail in a previous publication [Wait, 1959]

In the present situation, the wedge is taken to have an angle near

180 , corresponding to a small change of slope of the surface. Also,

we are interested in the behavior of the field at all distances from

the apex and, consequently, the parameter kp may be either small

or large compared with unity. For these reasons, it was considered

worthwhile to program the infinite series solution despite its poor

convergence and other complexities.

The expression for the H field [denoted HZ] is normalized

so that H = exp(+ikp) if = 0=0 while H = exp ( - i k p ) Z O 2

if =0 and = 180 ' This would follow from the identity o

00

/ ^^^^P i^T^"^/^) ^ (kp) = exp(ikp) , (2)

m = 0, 1, 2, .. .

which involves only integral-order Bessel functions.

-3
For the present problem, the electric field has both a p and an

(j) component. From Maxwell's equations

E = : j^ and E . = - .—^

, (3)

p ieoL)p?^9 9 leojP^p

o o

-12

where e =8. 854 x 10 is the dielectric constant of free space,

o Thus,

00 i G 00 E

,

^

EO = - : ^ = -— ) e ^ cos V cos v exp (i v n/Z) J' (k p ) , k V Z- o V

m = 0, 1, 2, . . . (4)

where J' (Z) = -^ J (Z) , V d Z V

EP = -^ B

i e GO E^ ^ J (kp

)

= —r- / 2 V sin v cos v exp (i v n/2) —r; ^— . ^ L o (kp)

m =1, 2, 3, . . . (5)

The letter symbols HZ, EO, and EP are used to designate

the quantities H , -i E,/ri , and i E /n , respectively, where

z 0o po

r\ = £ oo/k = 120 TT . Also, in the subsequent numerical listings,

the dimensionless parameter kp is designated by X.

For the numerical work, three cases (designated I, II, III)

are considered. They are:

I = 0, =

o n = 0, = 180 , o m = 0, = iij . o

-4-
_3

In all these cases, X(orkp) ranges frora 10 to 50. In case I and case III, i|j - 180 takes the values 0, ± 5 , ± 10 , + ZO , ±30 ,

In case II, ij; - 180 takes only the positive values 0, + 5 , + 10 , + 20 , +30 , because the plane = 180 is inaccessible if 4^ < 180 .

The totality of the numerical results are listed in the appendix

where both Cartesian and polar representations are given. As an

interesting check, the infinite series was used in cases I and II for

ijj =180 . As indicated in the tabulated results, the magnitude of the

normalized fields is unity to better than four-digit accuracy. The

phase is also equal to ±kp +2qn, where q is an integer, to within

the same accuracy. To achieve this accuracy at the large values of

k p (or X), approximately 200 terms in the series were required.

2. Graphical Presentation, Case I. To illustrate the behavior of the reflected fields in the vicinity

of the wedge, the amplitude of H and E , /v, is plotted as a function of k p in figures 2a, 2b, 2c, and 2d for values of ip ranging from 150 to 210 and = = . It is evident that a standing wave pattern is formed which has a characteristic period of

TT radians or \/2. wavelength. As is evident from figures 2b and 2d,

the |h I and the |e, /r| j fields have almost an identical pattern

except within 1/^ radian (or l/6 wavelength) from the apex. Within

the immediate neighborhood of the apex, the characteristics of the

magnetic and electric fields are quite different, as illustrated in

figures 2a and 2c. In particular, the |H | field is finite at kp =0.

In fact, as may be ascertained from the series solution, H = (^/|j) z as kp tends to zero. On the other hand, the E , field for 4> > 180

has a singular behavior as kp tends to zero. In fact, E, varies
i-1

according to (k p ) as k p -* 0. If i|/ > 180 , the field rises

quite sharply right at the apex. This is analogous to an electrostatic

fringing effect which occurs in potential fields near sharp edges. On

the other hand, if ifj < 180 , the E , field vanishes at the edge.

Another interesting feature of the curves in figures 2a, 2b, 2c,

and 2d is the non-symmetry of the fields about \\j = 180 . For example, in figure 2b, it is seen that the reflected wave for ij^ =150

is somewhat greater than the case for ^ =210 . For small departure

of ijj from 180 , this non- symmetry disappears. In fact, the curve

for ijj = 175 is almiost symmetrical with the curve for ijj = 185 .

3. Graphical Presentation, Case II

In figures 3a, 3b, 3c, 3d, 3e, and 3f, the amplitude of the field

components H , E , , and E is plotted for the plane =180

for ijj = 180°, 185°, 190°, 200°, and 210°. As before, = 0°. o Here the observer is above the wedge surface at = i); . As may

be seen from figures 3a and 3b, the | H j field diminishes with

z distance from the apex. The decrease is more pronounced for the

large values of 4^. Actually, the asymiptotic limit of all these curves

(for ijj > 180 and kp — °o) is 0. 5. The curves for |e , /ri | in

figures 3c and 3d show a very similar behavior; the only major

difference is the expected singular behavior near the apex. The

singular effect is evident in the curves for E /ri given in figures

p o 3e and 3f.

4. Graphical Presentation, Case III

In figures 4a, 4b, 4c, and 4d, the amplitude of the fields H

z and E , are plotted for the plane = if; for ifj from 150 to 210 . Here, as in case I, the field E is identically zero. These curves

P

• 6-
for the case ijj > 180 clearly show the shadowing effect of the

wedge. On the other hand, if i]; < 180 , the fields are raagnified

somewhat because of the upward tilt of the surface = tj/ . For all

values of 4" > the H field is finite at the apex where the E, field

has the expected singular behavior.

5. . Remarks Concerning Phase

The phase of the field for the three cases is available from the

tabulated data in the appendix. It should be noted that phase is given

in radians and is always listed in the range to 2 tt . Generally,

the phase is rapidly varying because a rapidly varying factor of the

type exp (±ikp ) is included. In order to understand the behavior

of the phase, one should subtract the rapidly varying portion. For

example, in case I, a meaningful quantity is the phase increment of

H defined by

z (phase H ) - kp , z

o. Thus, if there were no reflection from the apex (e.g. , i{^ =180 ),

the field H at = would be equal to exp (ikp). Phase results

which are normalized as indicated are illustrated in figures 5a, 5b,

5c, and 5d for (j) =0 and (j) = 0. As expected, the phase of H at o z the apex is zero, but for larger values of kp , an oscillatory pattern

i s evident. The phase curves for E , are quite sinnilar except

that the phase is finite at the apex.

6. Effective Surface Impedance

In approximate theoretical treatments of wave propagation over

undulating surfaces, the boundary conditions are often applied to

some reference plane just above the actual surface. In this context,

-7-
it is of interest to plot the exact value of the wave impedance normal

to the surface =180 when 4^ > 180 . Thus, in figures 6a and 6b,

the normalized impedance E /n H is plotted as a function of

p o z k p . Clearly, in the limiting case, \\j =180 , the impedance must be

zero as indicated. However, as \\j is increased beyond 180 , it is

evident that the impedance is finite and is approximately proportional

to 180 - ijj . The simplified boundary condition proposed by Feinberg

[1946] and applied by Wait and Jackson [1963] is equivalent to using

•^p

i|j - 180°

o z 57. 3

For example, if t|j = 190 , the normalized impedance is 0.174,

which is in fair agreement with the curves in figure 6a, except very

near the apex, if kp < 3. If i|j = 185 , the agreement is somewhat

better and the upper limit of kp stretches out to about 6.

Although the simple approximate boundary condition is not

valid for the large values of kp , it may be used for certain approximate field calculations. An illustrative example is shown in figures

7a and 7b where the reflected field at = is shown as calculated

by both exact and approximate methods. The approximate method

would assume that. the boundary condition given by the equation holds

on = 180 for all values of kp . Using a method discussed in a previous paper [Wait and Jackson, 1963], the reflected field would

be given by

_(r) 1 /^l|j-180% , ^ ^ ,

and

g(x) =xe-'^[H[^'>(x) + iH<''(x)] - ie-'^'H^^^W "

L

-8-
(2) (2)

In this expression, H and H, are the Hankel functions of the

o 1 second kind of order zero and one, respectively. The corresponding

(r)

exact expression for E , , on the plane 0=0, is obtained by subtracting the incident field r] exp (ikp) from the expression for

the total field given by (4). In this way, we may write

(r) 1 ^iL-180" E'"' = t(^^^) 8^W '°^ +>18°° • ''' - ~ 57.3

and

= --2-(^ ^^g(x)for ^<180 _(r) 1 ^180^^^jj_-^ -, , ^ , .,^^0 ^ "57,3

where g (x) and g (x) are derived from the exa^t series expressions.

The comparative results of g(x) and g (x) are shown in figures

7a, 7b, 7c, and 7d in an Argand-type plot for 4; =185°, 190°, 175°

o and 170 , respectively. It is evident that despite the violation of the

assumed boundary conditions in the approximate approach, g(x) is

reasonably close to the exact results obtained from g (x). Physically,

this may be attributed to the importance of the region of the reference

boundary near the apex. Contributions from the reference boundary

far from the apex must tend to cancel one another. It is noted that

o o the curves for ^ = 185 and 175 show a very close similarity

between the approximate and exact forms. As the departures of ifj o from 180 become greater, the dissimilaritiei

approximate results become quite noticeable.

o from 180 become greater, the dissimilarities between exact and

-9-
7. Concluding Remarks

This detailed numerical study gives some justification for the

use of approximate conditions for gently sloping surfaces. In

addition, the detailed description of the field near the apex of a

wedge has now been made available. The stated purpose of the

paper has thus been accomplished.

8. References

Feinberg, E. (1946). On the propagation of radio waves along an

imperfect surface, J. Phys. USSR 10^ 410-440.

Wait, J. R. (1959). Electromagnetic radiation from cylindrical

structures (Pergamon Press, Oxford).

Wait, J.R. , and C. M. Jackson (Nov. -Dec. 1963). The oblique

propagation of ground waves across a coast line - Part II, J. Res. NBS 67D (in press).

L

-10-
Figure Captions

Figure 1 Illustrating incident plane wave on perfectly conducting wedge.

Amplitude of H and E , fields as a function of

radian distance kp from apex showing interference

pattern between incident and reflected w^aves.

Amplitude of H and E , fields as a function of

radian distance kp fronn apex showing shadowing

effect of wedge.

Amplitude of H and E , fields as a function of

radian distance kp for observer on wedge face

Normalized phase ^ of H and E , fields as a

z function of radian distance kp from apex showing

interference pattern between incident and reflected

wave.

Normalized wave impedance on surface = TT .

Argand plot of the reflected field, for various

distances kp , as obtained from exact and approximate methods.

Figures 2a

2b

2c

2d

Figures 3a

3b

3c

3d

3e

3f

Figures 4a

4b

4c

4d

Figures 5a

5b

5c

5d

Figures 6a

6b

Figures 7a

7b

7c

7d

-11-
H

U

U\

PiW

OhO

W

^ Q

W W

%^

Q. ^

w

p

l-H o

H

<

w

u

H

U

P

o

u

-12-
2.0 22 2.4

FIGURES 2a AND 2b - AMPLITUDE OF H FIELD AS A FUNCTION OF RADIAN DISTANCE

z k p FROM APEX SHOWING INTERFERENCE PATTERN BETWEEN INCIDENT AND REFLECTED

WAVES

-13-
FIGURES 2c AND 2d - AMPLITUDE OF E, FIELD AS A FUNCTION OF RADIAN DISTANCE

kp FROM APEX SHOWING INTERFERENCE PATTERN BETWEEN INCIDENT AND REFLECTED

WAVES

-14.
1.0

_0.9

fsj ^

0.8

0.7-

1 I I —[—1—p—^

\—

_

<f> = 180°^——-^^

1 1 1 1 1 1 1 1

-1

\—\—\—r-'

"] 1—

[

r

I V 1

' 1 ^v//=l80°

'I

IQDo

1

— ?nno

""" — 210<>

1 1 1 1 1 1 1 1 1 , 1 1 1

0.2 0.4 Q6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2 24

1.0

( b

^' 1

1 1

1 1 lyi ' 1

1

1

1

1

1

1

1

1 (^ = 180°

1

0.9 C^^-„^^ t;l85°____ <fe=o° —

N 0.8 X

\N.\^^^_^0_^—..^ —

0,7 — ^^^...^^ *-- ^^200^^^__^ —

- ^^'"^—

^__210;______^

' 06

1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 ,.,

I 2 5. 6 7 8 9 10

FIGURES 3a AND 3b - AMPLITUDE OF H FIELD AS A FUNCTION OF RADIAN DISTANCE kp

FROM APEX SHOWING SHADOWING EFFECT OF WEDGE

-15-
I.t 1 1

1 1

1

1

1

1

1

1

1

1

1 11

1

1

1

1 1

' 1

'

1.3

. —

1 <p = ISO*' -

1.2 ^

^0=0*^ —

I.I a\

o V^k

^ 1.0 LU

~^^i^^^ i// =180*'

\V''''^:=::r irf>°

\. ^"^v,^,^ ——- 1900

0.9 ^xT^"^"""----^^ —

^'^""^^^""

""^^^-^-....aop*

-

0.8 - ^*^---.-,^ -— —

^""""•"—-..^2/0° =

0.7

1 1 1 1 1 1 1 1 1 1 1 1 1 1 , 1 1 1 1 1 ~i 1 1 ^

0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2 2.4

1.2

1.0

p-0.9

LjJ

0.8

0.7 -

0.6-

1

1 '

1

1

1 1

(^ = 180°

I

1

I

1 1 1 {

1

1

' 1

'

I

<^o = 0^

i//=l80°

- % -—«___I85^

:\ ^-^>^_J90° —

-^--—-...200° —

-

..->_2]02____^ —

1

1 1 1 1 1 1

1 1 1 1 1 1 I 1 1 1 1 1

10

k/=

FIGURES 3c AND 3d - AMPLITUDE OF E^. FIELD AS A FUNCTION OF RADLAN DISTANCE

k p FROM APEX SHOWING SHADOWING EFFECT OF WEDGE

-16-
0.7

- r--\ 1

1 1 1 > 1 I1

>

1 1 1

1

1 '1

1 1

'

1

1

0.6 <^ =180° —

0.5 — \ —

^0.4

^"o.3

0.2

" 200'' —

190*'

0.1 =^ 185'' —

(\

xj/ = 180**--^

1 1 1 1 1 1 1 1 1 1 1 1 ^1,1,1,1 , 1 , Q2 0.4 0.6 as .0 1.2 14 1.6 1.8 2.0 2.2 24

FIGURES 3e AND 3f AMPLITUDE OF E^ FIELD AS A FUNCTION OF RADIAN DISTANCE

kp FROM APEX.SHOWING SHADOWING EFFECT OF WEDGE

•17.
2.2 2.4

b

2.0

1

1

4>

1

1

1

1

1 1

1 I

1 11

I

1 ^^1 _

1.8 1 ^0

--0°

J,

^ ^^ 1.6 - ^^!^^^^ —

1.4 - y

jo^

'-.

^ 1.2 ^^^-'^ -

175°

180°

1.0 ^—-. 185° _

0.8 -

^ 190° -

- ^^\ »_200°

-

0.6 — —

..,210° =

0.4

1 1 1 1 1 1 1 1

, 1 1 1 1 1 <

1 1 1 1

I 2 3 4 5 6 7 8 9 10

FIGURES 4a AND 4b - AMPLITUDE OF H FIELD AS A FUNCTION OF RADL^N DISTANCE kp FOR OBSERVER ON WEDGE FACE <f = if

\

.18-
o

-e- ijj

1.6

1

1

1

1

1 1

1

1

1

1

1

1

'

1

' 1' 1

v// = l50°—^^.^

' 1

1

1

1 1

4>

- ^ 160°—-^-..^^^X-

1.4 1 *o

= 0° l70°--.,.^^\ \

1.2

1.0 ^^^.-^ii^^^^^^^J.

0.8 —

v// = l85°-^

0.6 190° -

200°- —

0.4 ,1,1 1 1

210°-

,1,1, 1,1,1,1 ,1,1,

0.2 0.4 0.6 1.2 1.4 1.6 1.8 2.0 2.2 2.4

2.0

1.8

1.6

1.4

o^ 1.2 6-

UJ

1.0

0.8

06

1

1

' 1' 1 1

' 1' 1' , i — ^^ 4> --^ ^^i^^"""^

—

- ^^""^^^^ _ - ^^^^"^"^ -

- ^

—— '-

i

-— 175° — h

180°

\R^o _

(j — (901_____ -

I

^^-—^_2oo:__________

[

""""^^^^ -—.^_2I0^_____^^ :

1 1 1 1 1 1 1 1 . 2 3 5 6 7 9 10

\

FIGURES 4c and 4d - AMPLITUDE OF E^ FIELD AS A FUNCTION OF RADIAN DISTANCE

Vp FOR OBSERVER ON WEDGE FACE ^ - if

19-
-0,2

0.2 0.4 0.6 J L0.8 1.0 1.2 1.4 1.6 li 2.0 11 2.4

150°

-0.2 12 3 4 5 6 7 8 9

FIGURES 5a AND 5b - NORMALIZED PHASE OF H^ FIELD AS A FUNCTION OF RADIAN

DISTANCE kp FROM APEX SHOWING INTERFERENCE PATTERN BETWEEN INCIDENT

AND REFLECTED WAVES

.20.
I I I I \ \ L -0.3 I L

0.2 0.4 0.6 0.8

_L J L

1—^ r

1.0 1.2 1.4 1.6 J L

2.0 22 2.4

lij

FIGURES 5c AND 5d - NORMALIZED PHASE OF E. FIELD AS A FUNCTION OF RADIAN

DISTANCE kp FROM APEX SHOWING INTERFERENCE PATTERN BETWEEN INCIDENT

AND REFT.F.r.TED WAVES

.21-
1

\—

r

LU

M

f?0.4

0.2

-\ r

cp = 180*

190*

185° 180"

J \ L

1 I I 02 04 0.e 0.8 1.0 1.2 1.4 1.6 1.8 2j0 2.2 2.4

ISJ Q> X

III o

p^

0.8

0.6

0.4

0.2

1

1

1

I

1

I

1 1

1

1

'

1

1

1

1 1

'

1

1 L (^ = 180°

V *o=0°

^"---it^a^ — _^^

190°

-

185° -

1 1 1 i'89°-~K ,1,1 1,1, 12 3 5 6 7 8 9 10

FIGURES 6a AND 6b - NORMALIZED WAVE IMPEDANCE ON SURFACE = n

1

.22-
E

U.4

1

'

1 '

1

1

1 2.0

1

' 1

1 1 ' 1

'

1

1 1

^ =0°

1 1 1 1 1

07 // ^'° ^> *o = 0° — ^^ V i|/ =185° %nT= -

// '^•'^-///fi

'^ IV l2,7 // I % '0 507M // ^oAmj3^^7^'°

1.04 '0 ^^^^ c\^{t\

0.2 _ \ .0.9 ^rT'^^-^^ ^-o 0-9U 7.0 ^5f=^3.4

g (x) —

\\o.8

0.8\\

0.4 \\0.7 ~ 0.7\\

\\o.6 -

-nfi "^

0.5\\0.4 vC

0.4>^^j^0.3

" *^jN^

-08 — '^^>~^ ~o^ —

-

0.15^ ——ii! -

-1.0 2£!____ 0.04 , =0.02 1,1, 1 1 1

1 , 1 1 1 1 1 . 1 1 1 , 1,1, 0.4 -0.2 0.2 0.4 0.6 0.8 1.0 1.2 REAL g*(x) OR g(x)

2.0

-0.2 0.2 0.4 0.6 0.8 1.0 REAL g*(x) OR g (x) n

FIGURES 7a .AND 7b - .A.RGAND PLOT OF THE REFLECTED FIELD, FOR VARIOUS DISTANCES kp

OBTAINED FROM EXACT AND APPROXIMATE METHODS

AS

-23-
0.4 "^—

r

T 1 r 1

r

2.0

i> --0° 00=0°

1^ =175°

g"(x)

g (x)

Q06 0.04

X =0.02

J L

0.4 0.6 0.8 1.0 1.2 REAL g'(x) OR g (x)

2S

0.4

0.2

-0.2

en -0.4 E

-0.6

-0.8 -

I'll .o' ' ' '

1 1

'

1

' 1 1 1 ' 11 I'll

/^^ S^:^ <^ =0°

~ - 1 V/^5 BOy^^=0^ x"

*o=0° ^ = 170° -

1 ^^rfff ^3-

-

- 1 «-&^Mo" n" t-i\ - ~

\

\o.9 ^•°'^^

Q9\ \ 3.5 ;--^;/ —

3.4 \ \°'® -

osX \ \ v

0.7\\ \ y06 - \ \ _ 0.6\\ 0.5 \ \

1

K>^ ^^ 0.3

- — 0.4 ^*^..^"*»^ ^"^^f.^;-!^^ 0.2 X:0.02

1 . 1 1 , 1 , 1

=fcXfai,ai5

, 1 1

0-OS ^

1 , 1 1 1 1 1 1 1 1 1 . -0.4 -0.2 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 REAL g"(x) OR g (x) FIGURES 7c AND 7d - ARGAND PLOT OF THE REFLECTED FIELD, FOR VARIOUS DISTANCES kp

OBTAINED FROM EXACT AND APPROXIMATE METHODS

.8 Za

AS

-24-

I
CASE I

(^ = o' i|j = 150

X R6{HZ) IM(HZ) HZ(AMP) PHASE(HZ)

10.00006--03 1.1988E 00 3. 58846-03 1.19886 CO 2.99336-03

2.0000E--02 1.19726 00 8.23956-03 1.19726 00 6.88226-03

4.0000E--02 1.19336 00 1.89046-02 1.19356 00 1.58416-02

6.0000E--02 1.18886 00 3.07046-02 1.18926 00 2.58236-02

l.OOOOE--01 1.17806 00 5.64726-02 1.1794E 00 4.79006-02

2.0000E--01 1.1432E 00 1.28216-01 1.15046 00 1.11696-01

3.0000E--01 1.0981E 00 2.05406-01 1.11726 00 1.84916-01

4.000CE--01 1.04366 00 2.84746-01 1.08176 00 2.66366-01

5.0000E--01 9.80256-01 3.64116-01 1.04576 00 3.55656-01

6.0000E--01 9.08716-01 4.41896-01 1.01056 CO 4. 52626-01

7.0000E--01 8.29626-01 5. 16746-01 9.77386--01 5.57066-01

8.0000E--01 7.43666-01 5.87476-01 9.47716--01 6.68606-01

9.0000E--01 6. 51606-01 6.53076-01 9.22546--01 7.86526-01

l.OOOOE OG 5.5427E-01 7.12636-01 9.0280E--01 9.09756-01

1.4000E 00 1.3019E-01 8.76266-01 8.8588E--01 1.42336 00

2.0000E 00 -5.0216E-01 8.54786-01 9.91366--01 -1.03966 00

2.4000t 00 -8.31126-01 6.62396-01 1.0628E 00 -6.72906-01

3.0000E 00 -1.06596 00 1.81706-01 1.0813E 00 -1.68846-01

3.A0OOE 00 -I.0171E 00 -1.91406-01 1.0350E 00 1.86016-01

4.0000E 00 -6.57236-01 -6.81136-01 9.4651E--01 8.03256-01

4.4C00E 00 -2.81636-01 -8.83796-01 9.27586--01 1.26236 00

5.0000E 00 3.40196-01 -9.20546-01 9.81396--01 -1.21686 00

6.0000E oc 1.01756 00 -3.04916-01 1.06226 00 -2.91166-01

7.0000F 00 7.62096-01 5.99346-01 9.69536--01 6.66426-01

e.oooot OG -1.8713E-01 9.54076-01 9.72256--01 -1.37716 00

9.0000E 00 -9.6031E-01 4.27546-01 1.05126 00 -4-18866-01

l.OOOOE 01 -8.5174E-01 -4.9674E-01 9.86016--01 5.27986-01

1.30006 01 9.2387E-01 3.8041E-01 9.99126--01 3.90606-01

1.50006 01 -7.99726-01 6.5201E-01 1.03186 00 -6.84006-01

1.8000E 01 6.9676E-01 -7.4760E-01 1.02196 00 -8.20586-01

2.00006 01 3.96546-01 8.80196-01 9.65396--01 1.14756 00

2.30006 01 -5.2638E-01 -8.14476-01 9.69766--01 9.97046-01

2.50006 01 1.01636 00 -1.50726-01 1.02746 00 -1.47236-01

2.8000E 01 -9. 88506-01 2.84816-01 1.02876 00 -2.80526-01

3.00006 01 1.76876-01 -9.70916-01 9.86896--01 -1.39066 00

3.30006 01 -3.23556-02 9.80746-01 9.8127E--01 -1.53786 00

3.50006 01 -9. 12916-01 -4.0356E-01 9.9813E--01 4.16236-01

4.00006 01 -6.91476-01 7.4345E-01 1.0153E CO -8.21616-01

4.50006 01 5.20266-01 8,28296-01 9.78136--01 I.OIOOE 00

5.00006 01 9.84186-01 -2.73126-01 1.02146 00 -2.70706-01

-25-
CASE I

'= i}j = 150

X RE{EO) IM(EO) EC(AMP) PHASE(EO)

lO.OOOOE--03 -1.4643E-01 4.3043E-01 4.5466E--01 -1.2429E 00

2.0000E--02 -1.7400E-01 4.9388E-01 5.2363E--01 -1.2321E 00

4.0000E--02 -2.1185E-01 5.6577E-01 6.0413E--01 -1.2125E 00

6.0000E--02 -2.4179E-01 6.1156E-01 6.5762E--01 -1.1943E 00

l.OOOOE--01 -2.9275E-01 6.7205E-01 7.3304E--01 -1.1600E 00

2.0000E--01 -4.0143E-01 7.5184E-01 8.5230E--01 -1.0804E 00

3.0000E--01 -4.9918E-01 7.8675E-01 9.3175E--01 -1.00'54E 00

4.0000E--01 -5.9028E-01 7.9656E-01 9.9144E--01 -9.3306E-01

5.0000E--01 -6.7540E-01 7.8822E-01 1.0380E 00 -8.6233E-01

6.0000E--01 -7.5431E-01 7.6521E-01 1.0745E 00 -7.9258E-01

7.0000E--01 -8.2649E-01 7.2969E-01 1.1025E 00 -7.2327E-01

8.0000E--01 -8.9138E-01 6.832bb-01 1.1231E 00 -6.5399E-01

9.0000E--01 -9.4836E-01 6.2719E-01 1.1370E 00 -5.8431E-01

l.OOOOE 00 -9.9688E-01 5.6267E-01 1.1447E 00 -5.1385E-01

1.4000E CO -.1.0977E 00 2.4153E-01 1.1240E 00 -2.1658E-01

2.0000E 00 -9.5105E-01 -3.1301E-01 1.0012E 00 3.1796E-01

2.4000E 00 -6.7321E-01 -6.3600E-01 9.2612E--01 7.5698E-01

3.0000E 00 -8.7890E-O2 -9.1677E-01 9.2097E--01 1.4752E 00

3.A00OE 00 3.2842E-01 -9.2316E-01 9.7984E--01 -1.22«)0E 00

4.0000t ou 8.3486E-01 -6.5860E-01 1.0634E 00 -6.6792E-01

4.4000E 00 1.0182E 00 -3.4073E-01 1.0737E 00 -3.22'^2E-01

5.0000E oc 9.9270E-01 2.2252E-01 1.0173E 00 2.2061E-01

6.0000E 00 2.4905E-01 9.04iaE-01 g.37R6E--01 1.3020E 00

7.0000E 00 -7.1576E-01 7.4962E-01 1.0365E 00 -8.085CE-01

'8.0000E 00 -1.0224E 00 -1.0140E-01 1.0274E 00 9.8854E-02

9.0000E 00 -3.9395E-01 -8.6249E-01 9.4820E--01 1.1423E 00

l.OOOOE 01 5.9216E-01 -8.2868E-01 1.0185E 00 -9.5035E-01

1.3000E 01 -4.6066E-01 8.9250E-01 1.0044E 00 -1.0943E CO

1.5000E 01 -6.4726E-01 -7.1962E-01 9.6788E--01 8.3829E-01

1.8000E 01 7.^340E-01 6.2372E-01 9.7808E--01 6.9I51E-01

2.0000E 01 -9.4546E-01 4.2G47E-01 1.0347E 00 -4.1846E-01

2.3000E 01 8.7787E-01 -5.4000E-01 1.0307E 00 5.5147E-01

2.5000E 01 1.1349E-01 9.6647E-01 9.7311E--01 1.4539E 00

2.8000E 01

' -2.5656E-01 -9.3696E-01 9.7145E--01 1.3035E 00

3.0000E 01 1-0048E CO 1.3131E-01 1.0134E 00 1.2995E-01

3.3000E 01 -1.0188E 00 6.1218E-03 1.0188E 00 -6.0086E-03

3.5000E 01 4.5294E-01 -8.9485E-01 1.0029E 00 -1.1022E 00

4.0000E 01 -7.4650E-01 -6.4238E-01 9.8434E--01 7.1057E-01

4.5000E 01 -8.7348E-01 5.3067E-01 1.0220E 00 -5.4594E-01

5.0000E 01 2.5147E-01 9.4588E-01 9.7874E--01 1.3109E 00

-26.

I
CASE I

= i\i = 160

X RE (HZ) IN(HZ) HZ{AMP) PHASE(HZ)

lO.OOOOE--03 1.1239E 00 5.3682E-03 1.1239E 00 A.7763E-03

2.0000F--02 1.1225E 00 1.1702E-02 1.1226E 00 1.0424E-02

4.0000E--02 1.1193E 00 2.5A90E-02 1.1196E 00 2.2769E-02

6.0000E--02 1.1157E 00 A.0167E-02 1.1164E 00 3.5987E-02

l.OOOOE--01 1.1070E 00 7.1126E-02 1.1093E 00 6.4162E-02

2.0000E--01 1.0783E 00 1.5349E-01 1.0892E 00 1.4139E-01

3.0000E--01 1.0402E 00 2.3887E-01 I.0673E 00 2.2573E-01

4.0000E--01 9.9298E-01 3.2A57E-01 1.0447E 00 3.1591E-01

5.0000E--01 9.3709E-01 A.0880E-01 1.0224E 00 4.1135E-01

6.0000E--01 8.7299E-01 4.9017E-01 1.0012E 00 5.1161E-01

7.0000E--01 8.0123E-01 5.6748E-01 9.8184E--01 6.1625E-01

8.0000E--01 7.2242E-01 6.3971E-01 9.64g4E--01 7.2476E-01

9.0000E--01 t).3726E-01 7.0593E-01 9.5i:.2E--01 8.3648E-01

l.OOOOE 00 5.4653E-01 7.6534E-01 9.A0A5E--01 9.5067E-01

1.4000E CO 1.4513E-01 9.2211E-01 9.33A6E--01 1.41A7E 00

2.0000E 00 -4.6686E-01 8.7865E-01 9.9498E--01 -1.0824E 00

2.A000E 00 -7.9192E-01 6.6894E-01 1.0366E 00 -7.0141E-01

3.0000E oc -1.0335E 00 1.6536E-01 1.0467E 00 -1.5865E-01

3.A000E 00 -9.9528E-01 -2.1802E-01 1.0189E 00 2.1564E-01

4.0000E 00 -6.5509E-01 -7.1311E-0I 9.6833E--01 8.2778E-01

4.4000E 00 -2.9199E-01 -9.1270E-01 9.5827E--01 1.2612E 00

5.0000E OG 3.1650E-01 -9.3721E-01 9.8921E--01 -1.2451E 00

6.0000E 00 9.9298E-01 -2.9443E-01 1.0357E 00 -2.8825E-01

7.0000E oc 7.5831E-01 6.2379E-01 9.819ie--01 6.8837E-01

8.0000E 00 -1.6960E-01 9.6927E-01 9.84rOE--01 -1.3976fc 00

9.0000E 00 -9.3933E-C1 4.2119E-01 1.0294E 00 -4.2152E-01

l.OOOOE 01 -8.4617E-01 -5. 1681E-01 9.91S1E--01 5.4829E-01

1.3000E 01 9.1677E-01 3.9728E-01 9.9915E--01 4.0892E-01

1.5000E 01 -7.3268E-01 6.5139E-01 1.0183E 00 -6.9410E-01

1.8000E 01 6.8125E-01 -7.4912E-01 1.0126E CO -8.3282E-01

2.0000E 01 4.0140E-01 8.9A16E-01 9.8013E--01 1.1489E 00

7-3000E 01 -5.2y08E-01 -8.2801E-01 9.8261E--01 1.0022E 00

2.5000E 01 1.0056E 00 -1.4294E-01 1.0157E 00 -1.4120E-01

2.8000E 01 -9.77A5E-01 2.7893E-01 1.0165E 00 -2.7797E-01

3.0000E 01 1.6726E-01 -9.782AE-01 9.9244E--01 -1.4015E 00

3.3000E 01 -2.4189E-02 9.88g7E-01 9.8926E--01 -1.5463E 00

3.5000E 01 -9.0896E-01 -4.1A04E-01 9.9882E--01 4.2742E-01

4.n000E 01 -6.81C2E-01 7.4419E-01 1.0088E 00 -8.2969E-01

4.5000E 01 5.2241E-01 8.3793E-01 9.87A4E--01 1.0133E GO

5.0000E 01 9.7599E-01 -2.6856E-01 1.0123E 00 -2.6852E-01

-27-
CASE I 0=0 4; = 160

X RE(EO) IM(EO) EO(AMP) PHASE(EO)

lO.OOOCE--03 -1.2702E-01 6.0365E-01 6.1687E--01 -1.3634E 00

2.0000b--02 -1.4518E-01 6.5757E-01 6.7341E--01 -1.3535E 00

4.0000E--02 -1.7221E-01 7.1523E-01 7.3567E--01 -1.3345E 00

6.0000E--02 -1.9530E-01 7.5014E-01 7.7515E--01 -1.3I6IE GO

l.OOOOE--01 -2.3740E-01 7.9382E-01 8.2856E--01 -1.2802E CO

2.0000E--01 -3.3478E-01 8.4458E-01 9.0851E--01 -1.1934E 00

3.0000E--01 -4.2741E-01 8.5881E-01 9.5929E--01 -1.1090E 00

4.0000E--01 -5.1624E-01 8.5221E-01 9.9637E--01 -1.0261E 00

5-OOOOE--01 -6.0079E-01 8.3013E-01 1.0247E 00 -9.4432E-01

6.0000E--01 -6.8031E-01 7.9527E-01 1.0466E 00 -8.6315E-01

7.0000E--01 -7.5398E-01 7.4935E-01 1.0630E 00 -7.8232E-01

8.0G00E--0 1 -8.2104E-01 6.9369E-01 1.0749E 00 -7.0162E-0i

9.0000E--01 -8.8076E-01 6.2939E-01 1.0825E 00 -6.2046E-01

l.OOOOE 00 -9.3248E-01 5.5750E-01 1-0864E 00 -5.3885E-01

l.AOOOE 00 -1 -0495E 00 2.1418E-01 1.071IE 00 -2.0132E-01

2.0000E CO -9.3176E-01 -3.5563E-01 9.9732E--01 3.6461b-01

2.4000E 00 -6.7266E-01 -6.7878E-01 9.5562E--01 7.89Q3E-01

3.0000E 00 -1.0951E-01 -9.4840E-01 9.5470E--01 1.4558E 00

3.A000E 00 2.9802E-01 -9.4246E-01 9.8845E--01 -1.2645E 00

A.OOOOE 00 8.0169E-01 -6.5724E-01 1.0367E 00 -6.8671E-01

4.4000E 00 9.B965E-01 -3.2713E-01 1.0423E 00 -3.1925E-01

5.0000E 00 9.7788E-01 2.4824E-01 1.0089E 00 2.48e>0E-01

6.0000E 00 2.6160E-01 9.2819E-01 9.6435E--01 1.2961E 00

7.0000E 00 -6.9078E-01 7.5178E-01 1.0209E 00 -8.2766E-01

8.0000E 00 -1.0081E 00 -1.2001E-01 1.0152E 00 I.1848E-01

9.0000E 00 -4.0148E-01 -a.8328E-01 9.7024E--01 1.1442E 00

l.OOOOE 01 5.7170E-01 -8.3330E-01 1.0106E 00 -9.6948E-01

1.3000E 01 -4.4346E-01 8.9899E-01 1.0024E 00 -1.1125E 00

1.5000E 01 -6.4845E-01 -7.3670E-01 9.8143E--01 8.4902E-01

1.8000E 01 7.5230E-01 6.3930E-01 9.8725E--01 7.0438E-01

2.0000E 01 -9.3159E-C1 4.1526E-Q1 1.02C0E 00 -4.1932E-01

2.3G00E 01 8.6437E-01 -5.3701E-01 1.0176E 00 -5.5591E-01

2.5000E 01' 1.2149E-01 9.7704E-01 9.8457E--01 1.4471E 00

2.8000E 01 -2.6264E-01 -9.4791E-01 9.8362E--01 1.3005E 00

3.0000E 01 9.9764E-01 1.4106E-01 1.0076F 00 1.4047E-01

3.3000E 01 -1.0107E 00 -2.0828E-03 1.0107E 00 2.0607fc-03

3.5000E 01 4,4240E-01 -8.9865E-01 1.0016E 00 -1.1133E 00

4.0000E 01 -7.A589E-01 -6.5284E-01 9.9124E--01 7.1897E-01

4.5000E 01 -8.63B6F-01 5.2842E-01 1.0127E 00 -5.4897E-01

5.0000E 01 2.5611E-01 9.5402E-01 9.8780E--01 1.3085E 00

I

.28.
CASE I

(/> = o' i|j = 170

X RE (HZ) IM(HZ) HZ(AMP) PHASE(HZ

lO.OOOOE--03 1.0581E 00 7.5196E-03 1.0581E 00 7.1066E-03

2.0000E--02 1.0572E 00 1.5659E-02 1.0573E 00 1.4811E-02

4.0000E--02 1.0551E 00 3.2593E-02 1.0556E 00 3.0880E-02

6.0000E--02 1.0527E 00 5.0019E-02 1.0539E 00 4.7480E-02

l.OOOOE--01 1.0466E 00 8.57.00E-02 1.0501E 00 8.1704E-02

2.0000E--ni 1.0247E 00 1.7706E-01 1.0399E 00 1.7110E-01

3.0000E--01 9.9343E-01 2.688gE-01 1.0292E 00 2.6433E-01

4.0000E--01 9.5302E-01 3.5930E-01 i.oiasE 00 3.6054E-01

5.0000E--01 9.0375E-01 4.4694E-01 1.0082E 00 4.5927E-01

6-noooE--01 8.4605E-01 5.3064E-01 9.9869E--01 5.6018E-01

7.0000E--01 7.8043E-01 6.0941E-01 9.9018E--01 6.6296E-01

8.0000E--01 7.0749E-01 6.8233E-01 9.8291E--01 7.6730E-01

9.0000E--01 6.2789E-01 7.4857E-01 9.7704E--01 8.7285E-01

l.OOOOE oc 5.A240E-01 8.0743E-01 9.7269E--01 9.7928E-01

1.4000E 00 1.5842E-01 9.5752E-01 9.7053E--01 1.4068E 00

2.0000E 00 -4.3879E-01 8.9609E-01 9.9776E--01 -1.1154E 00

2.4000E 00 -7.6151E-01 6.7293E-01 1.0162E 00 -7.2372E-01

3.0000E 00 -1.0091E 00 1.5204E-01 1.0204E 00 -1.^955£-01

3.4000E 00 -9.7915E-01 -2.3888E-01 1.0079E 00 2.3929E-01

4.0000E 00 -6.5409E-01 -7.3758E-01 9.85R3E--01 8.4532b-01

4.4000E 00 -3.0043E-01 -9.3456E-01 9.8167E--01 1.2598E 00

5.0000E 00 2.9817E-01 -9.4951E-01 9.9522E--01 -1.2665E 00

6.0000E 00 9.7454E-01 -2.8612E-01 1.0157E 00 -2.8557E-01

7.0000F 00 7.5575E-01 6.4240E-01 9.9189E--01 7.0450E-01

8.0000E 00 -1.5612E-01 9.8060E-01 9.9295E--01 -1.4129E 00

9.0000E 00 -9.2349E-01 4.1616E-01 1.0129E 00 -4.2339E-01

l.OOOOE 01 -8.4214E-01 -5.3207E-01 9.9614E--01 5.6348E-01

1.3000E 01 9.1150E-01 4.1011E-01 9.9952E--01 4.2280E-01

1.5000E 01 -7.6977E-01 6.5081E-01 1.0080E 00 -7.0185E-01

1 .8000E 01 6.6950E-01 -7.5020E-01 1.0055E 00 -8.4218E-01

2.0000E 01 4.0514E-01 9.0472E-01 9.9129E--01 1.1498E 00

2-3000E 01 -5.3118E-01 -8.3824E-01 9.9237E--01 1.0060E 00

2.5000E 01 9.9750E-U1 -1.3701E-01 1.0069E 00 -1.3650E-01

2.8000E 01 -9.6911E-01 2.7444E-01 1.0072E 00 -2.7596E-01

3.0000E 01 1.5996E-01 -9.8375E-01 y.9667E--01 -1.4096E 00

3.3000E 01 -1.8088E-02 9.9511E-01 9.9528E--01 -1.5526E 00

3.5000E 01 -9.0600E-01 -4.2198E-01 9.9945E--01 4.3588E-01

4.0000E 01 -6.7311E-01 7.4A72E-01 1.0038E 00 -8.3586E-01

4.5000E 01 5.2405E-01 8.4522E-01 9.9450E--01 1.0158E 00

5.0000E 01 9.6980E-01 -2.6510E-01 1.0054E 00 -2.6684E-01

.29-
CASE I

^ = i|j = 170

lO.OOOOE-03

2.00005-02

4.0000E-02

6.0000E-02

l.OOOOE-01

2.0000E-01

3.0000E-01

4.0000E-01

5.0000E-01

6-OOOOE-Ol

7.0000E-01

8.0000E-01

9.0000E-01

l.OOOOE OC

1.4000E 00

2.0000E 00

2.A000E 00

3.0000E 00

3.4000E 00

4.0000E 00

4.4000E 00

5.0000E 00

6.0000E 00

7.0000E 00

8.0000E 00

9.0000E 00

l.OOOOE 01

1.3000E 01

1.5000E 01

1.8000E 01

2.0000E 01

2.3000E 01

2.5000E 01

2.8000E 01

3.0000E 01

3.3000E 01

3.5000E 01

4.0000E 01

4.5000E 01

5.0000E 01

RE(EO)

-8.1732E-02

-9.3177E-02

-1.1361E-01

-1.3316E-01

-1.7150E-01

-2.6599E-01

-3.5881E-01

-4.4902E-01

-5.3558E-01

-6.1751E-01

-6.9390E-01

-7.6391E-01

-8.2677E-01

-8.8181E-01

-1.0133E 00

-9. 1864E-01

-6.7376E-01

-1.2695E-01

2.7435E-01

7.7650E-01

9.6821E-01

9.6710E-01

2.7150E-01

-6.7181E-01

-9.9753E-01

-4.0739E-01

5.5617E-01

-4.3039E-01

-6.4945E-01

7.5154E-01

-9.2111E-01

8.5418E-01

1.2758E-01

-2.6728E-01

9.9224E-01

-1.0047E 00

4.3442E-01

-7.4546E-01

-8.5658E-01

2.5963E-01

IM{EO)

7.9592E-01

8.2838E-01

8.6122E-01

8.7999E-01

9.0167E-01

9. 1983E-01

9.1376E-01

8.9230E-01

8.5849E-01

8.1397E-01

7.5985E-01

6.9711E-01

6.2665E-01

5.4935E-01

1.9035E-01

-3.8924E-01

-7.11616-01

-9.7192E-01

-9.5635E-01

-6.5545E-01

-3.1620E-01

2.6804E-01

9.4620E-01

7.5307E-01

-1.3427E-01

-8.9894E-01

-8.3660E-01

9.0378E-01

-7.4961E-01

6.5110E-01

4.1126E-01

-5.3469E-01

9.8501E-01

-9.5617E-01

1.4846E-01

-8.3709E-03

-9.0150E-01

-6.6076E-01

5.2669E-01

9.6018E-01

EO(AMP) PHASE(EO

8.0011E--01 -1.4685E 00

8.3361E--01 -I.4588E 00

8.6868E--01 -1.4396E 00

8.9001E--01 -1.4206E 00

9.1784E--01 -1.3828E 00

9.5752E--01 -1.2893E 00

9.8168E--01 -1.1966E 00

9.9891E--01 -1.1046E 00

1.0119E 00 -1.0130E 00

1.0217E 00 -9.2178E--01

1.0290E 00 -8.3073E--01

1.0342E 00 -7.3971E--01

1.0374E 00 -6.4857E--01

1.0389E 00 -5.5715E--01

1.0310E 00 -1.8569E--01

9.9770E--01 4.0078E--01

9.7997E--01 8.1271E--01

9.-8017E--01 1.4409E 00

9.9493E--01 -1.2914E 00

1.0162E 00 -7.0107E--01

1.0185E 00 -3.1566E--01

1.0036E 00 2.7037E--01

9.8438E--01 1.2914E 00

1.0092E 00 -8.4236E--01

1.0065E 00 1.3380E--01

9.8695E--01 1.1453E 00

1.0046E 00 -9.8409E--01

i.OOlOE 00 -1.1264E 00

9.9182E--01 8.5686E--01

9.9436E--01 7.1391E--01

1.0088E 00 -4.1992E--01

1.0077E 00 -5.5929E--01

9.9324E--01 1.4420E 00

9.9282E--01 1.2982E 00

1.0033E 00 1.4852E--01

1.0047E 00 8.3319E--03

1.0007E 00 -1.1217E 00

9.9615E--01 7.2524E--01

1.0056E 00 -5.5129E--01

9.9466E--01 1.3067E 00

-30
CASE I

(/) = ijj = 175

lO.OOOOE-03

2.0000E-02

4.0000E-02

6.0000E-02

l.OOOOE-01

2.0000E-01

3.0000E-01

4.0000E-01

5.0000E-01

6.0000E-01

7.0000E-01

8.0000E-01

9.0000E-01

l.OOOOE 00

1.4000E 00

2.0000E 00

2.4000E 00

3.0000E 00

3.4000E 00

4.0000E 00

4.4000E 00

5.0000E 00

6.0000E 00

7.0000E 00

8.0000E 00

9.0000E 00

l.OOOOE 01

1.3000F 01

1.5000E 01

1.8000E 01

2.0000E 01

2.3000E 01

2.5000E 01

2.8000E ni

3.G000E 01

3.3000E 01

3.5000E 01

4.0000F 01

4.5000E 01

5.0000E 01

RE(HZ)

1.0281E GO

1.0276E 00

1.0262E 00

0245E 00

.0198E 00

0014E 00

7343E-01

3617E-01

8.8990E-01

8.3504E-01

7.7210E-01

7.0168E-01

6.2445E-01

5.4116E-01

1.6441E-01

-4.2688E-01

-7.4878E-01

-9.9896E-01

-9.7259E-01

-6.5382E-01

-3.0406E-01

2.9051E-01

9.6693E-01

7.5476E-01

-1.5051E-01

9.1695E-01

8.4G51E-01

9.0936E-01

-7.6443E-01

6.6A64E-01

4.067GE-01

5.3206E-01

9.9417E-01

-9.6567E-01

1.5693E-01

-1.5538E-02

-9.0479E-01

-6.6984E-01

5.2473E-01

9.6725E-01

IM(HZ)

8.7218E-03

1.7788E-02

3.6267E-02

5.4996E-02

9.2839E-02

1.8811E-01

2.8261E-01

3.7490E-01

4.6383E-01

5.4838E-01

6.2761E-01

7.0068E-01

7.6681E-01

8.2532E-01

9.7227E-01

9.0313E-01

6.7433E-01

1.4631E-01

-2.4766E-01

-7.4774E-01

-9.4359E-01

-9.5451E-01

-2.8259E-01

6.5011E-01

9.8525E-01

4. 1404E-01

-5.3839E-01

4. 1543E-01

6.5054E-01

-7.5063E-01

9.0908E-01

-8.4246E-01

-1.3455E-01

2.7258E-01

-9.8603E-01

9.9766E-01

-4.2526E-01

7.4494E-01

8.4823E-01

-2.6367E-01

HKAMP) PHASE(HZ)

1.0282E CO 8.4829E--03

1.0277E 00 1.7309E--02

1.0269E 00 3.5326E--02

1.0259E 00 5.3631E--02

i.0240E 00 9.0788E--02

1.0189E 00 1.8569E--01

1.0136E 00 2.8256E--01

1.0084E 00 3.8091E--01

1.0035E 00 4.8047E--01

9.99C1E--01 5.8107E--01

9.9500E--01 6.8253E--01

9.9162E--01 7.8469E--01

9.8891E--01 8.8737E--01

9.8692E--01 9.9043E--01

9.8608E--01 1.4033E 00

9.9893E--01 -1.1293E 00

l.'0077E 00 -7.3313E--01

1.0096E 00 -1.4543E--01

1.0036E 00 2.4934E--01

9.9328E--01 8.5231E--01

9.9136E--01 1.2591E 00

9.9774E--01 -1.2753E 00

1.0074E 00 -2.8434E--01

9.9615E--01 7.1105E--01

9.9668E--01 -I.4192E GO

1.0061E 00 -4.2413E--01

9.9816E--01 5.6970E--01

9.9975E--01 4.2853E--01

1.0038E 00 -7.0508E--01

1.0026E 00 -8.4608E--01

9.9590E--01 1.1501E GO

9.9641E--01 1.0075E GO

1.0032E 00 -1.3452E--01

1.0034E 00 -2.7511E--01

9.9844E--01 -1.4130E GO

9.9778E--01 -1.5552e GO

9.9974E--01 4.3937E--01

1.0018E 00 -8.3843E--01

9.9741E--01 1.0168E GO

1.0G25E 00 -2.6613E--01

31-
CASE I 0=0 4j = 175<

io.noooE-03

2.0000E-02

4.0000E-02

6.0000E-02

l.OOOOE-01

2.0000E-01

3.0000E-01

4.0000E-01

5.0000E-01

6.0000E-01

7.0000E-01

8.0000E-01

9.0000E-01

l.OOOOE 00

1.4000E 00

2.0000E 00

2.A000E 00

3.0000E 00

3.4000E 00

4.0000E 00

4.4000E 00

5.0000E 00

6.0000E 00

7.0000E 00

8.0000E OC

9.0000h 00

l.OOOOE 01

1.3000E 01

1.5000E 01

1.8000E 01

2.0a00E 01

2.3000E Oi

2.5000E 01

2.8000E 01

3.0000E 01

3.3000E 01

3-5000E 01

4.0000E 01

4.5000E 01

5.0000E 01

KE(EO)

4.9124E-02

-5.9052E-02

-7.8418t-02

9.7666E-02

-1.3613E-01

-2.3199E-01

-3.2643E-01

-4.1826E-01

•5.0642E-01

5.8993E-01

6.6789E-01

•7.3946E-01

8.0389E-01

-8.6052E-01

9.9850E-01

•9.1360E-01

•6.7458E-01

-1.3440E-01

2.6443E-01

7.6607E-01

9.5941E-01

9.6275E-01

2.7567E-01

•6.6397E-01

-9.9320E-01

-4.09B9E-01

5.4974E-01

4.2498E-01

•6.4990E-01

7.5125E-01

9.1679E-01

8.4997E-01

1.3011E-01

•2.6920E-01

9.9002E-01

1.0022E 00

4.3112E-01

-7.4528E-01

8.5358E-01

2.6109E-01

IM(£0)

8.9691E-01

9.1437E-01

9.3142E-01

9.4066E-01

9.5013E-01

9.5166E-01

9.3601E-01

9.0787E-01

8.6899E-01

8.2038E-01

7.6287E-01

6.9725E-01

6.2431E-01

5.4486E-01

1.7975E-01

-4.0342E-01

-7.2524E-01

-9.8151E-01

-9.6193E-01

-6.5454E-01

-3.1154E-01

2.7629E-01

9.5361E-01

7.5353E-01

-1.4020E-01

-9.0540E-01

-8.3792E-01

9.0573E-01

-7.5494E-01

6.5598E-01

4.0959E-01

-5.3371E-01

9.8829E-01

-9.5958E-01

1.5152E-01

-1.0960E-02

-9.0267E-01

-6.6403E-01

5.2598E-01

9.6272E-01

EO(AMP)

8.9825E-01

9.1628E-01

9.3471E-01

9.4571E-01

9.5983E-01

9.7953E-01

9.9129E-01

9.99I59E-01

1.0058E 00

1.0105E 00

1.0139E 00

1.0163E 00

1.0178E 00

1.0185E 00

1.0145E 00

9.9870E-01

9.9047E-01

9.9067E-01

9.9761E-01

1.0076E 00

1.0087E 00

1.0016E 00

9.9265E-01

1.0043E 00

1.0030E 00

9.9386E-01

1.0022E 00

1.0005E 00

9.9614E-01

9.9734E-01

1.0041E 00

1.0036E 00

9.9682E-01

9.9663E-01

1.0015E 00

1.0022E 00

1.0003E 00

9.9819E-01

1.0026E 00

9.9749E-01

PHASE(E01

-1.5161E 00

-1.5063E 00

-1.4868b 00

-1.4673E 00

1.4285E 00

-1.3317E 00

1.2352E 00

1.1391E 00

-1.0431E 00

-9.4737E-01

-8.5169E-01

-7.5603E-01

-6.6031E-01

-5.6445E-01

-1.7811E-01

4.1582E-01

8.2158E-01

1.4347E 00

-1.3025E 00

-7.0705E-01

-3.1398E-01

2.7947E-01

1.2894E 00

-8.4850E-01

1.4023E-01

1.1457E 00

-9.90I6E-01

-1.1321E 00

8.6004E-01

7.1780E-01

-4.2016E-01

-5.6070E-0I

1.4399t 00

1.2973E 00

1.5187E-01

1.0936E-02

-1.1252E 00

7.2781fc-01

5.5225E-01

1.3060E 00

I

-32.
CASE I

0=0° v|j = 180

X RE(HZ)

O.OOOOE--03 9.9995E--01

2.0000E--02 9.9980E--01

4.0000E--02 9.9920E--01

6.0000E--02 9.9820E--01

l.OOOOE--01 9.9500E--01

2.0000E--01 9.8007E--01

3.0000E--01 9.b534E--01

4.0000E--01 9.2106E--01

5.0000E--01 8.7758E--01

6.0000E--01 8.2534E--01

7.0000E--01 7.6485E--01

8.0C00E--01 6.9672E--01

9.0000E--01 6.2163E--01

l.OOOOE 00 5.A030E--01

l.AOOOE 00 1.6997E--01

2.0000E OC -4.1619E--01

2.4C00E 00 -7.3739E--01

3.0000E 00 -9.9000E--01

3.4000E 00 -9.6680E--01

4-OOOOE 00 -6.5366E--01

4.4000E 00 -3.0737E--01

5.0000F 00 2.8366E--01

6.0000E 00 9.6017E--01

7.0000E 00 7.5389E--01

8.0000E 00 -1.45A9E--01

9.0000E 00 -9.1114E--01

l.OGOOE 01 -8.391CE--01

1.3000E 01 9.0744E--01

1.5000E 01 -7.5966E--01

1.8000E 01 6.6033E--01

2.0000E 01 4.0806E--01

2-3000E 01 -5.3286E--01

2.5000E 01 9.9121E--01

2.8000E 01 -9.6260E--01

3.0000E 01 1.5422E--01

3.3000E 01 -1.3203E--02

3.5000E 01 -9.0369E--01

4.0000E 01 -6.6689E--01

4.5000E 01 5.2b30E--01

5.0000E 01 9.6497E--01

IM(HZ)

9.9998E-03

1.9999E-02

3.9989E-02

5.9964E-02

9.9833E-02

1.9867E-01

2.9552E-01

3.8942E-01

4.7943E-01

5.6464E-01

6.4422E-01

7.1736E-01

7.8333E-01

8.4147E-01

9.8545E-01

9.0930E-01

6.7547E-01

1.4112E-01

2.5554E-01

7.5681E-01

9.5161E-01

9.5893E-01

2.7942E-01

6.5698E-01

9.8937E-01

4. 1213E-01

•5.4403E-01

4.2016E-01

6.5031E-01

7.5099E-01

9. 1294E-01

8.4623E-01

•1.3236£-01

2.7092E-01

•9.8805E-01

9.99g5E-01

4.2817E-01

7.4515E-01

8.5089E-01

•2.6239E-01

HZ(AMP)

l.OOCOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOCOE 00

l.OOOOE 00

l.OOOOE CO

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOCOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE 00

l.OOOOE CO

l.OOOOE 00

9.9999E-G1

l.OOCOE 00

l.OOOOE CO

l.OOOOE 00

9.9999E-G1

9.9999E-01

l.OOCOE 00

9.9999E-01

l.OOOOE 00

l.OOOOE CO

lO.OOOOE-01

l.OOCOE 00

l.OOCOE 00

lO.OOOOE-01

9.9999E-01

9.9998E-01

l.OOOOE 00

PHASE(HZ)

lO.OOOOE-03

2.0000E-02

4.0000E-02

6.0000E-02

lO.OOOOE-02

2.0000E-01

3.0000E-01

4.0000E-01

5.0000E-01

6.0000E-01

7.0000E-01

7.9999E-01

8.9998E-01

lO.OOOOE-01

1.4000E 00

-1.1416E 00

-7.4160E-01

-1.4160E-01

2.5840E-01

8.5840E-01

1.2584E 00

-1.2832E 00

-2.8319E-01

7.1682E-01

-1.4248E 00

-4.2478E-01

5.7521t-01

A.3363t-01

-7.0800E-01

-8.4955E-01

1.1505E 00

1.0088E 00

-1.3275E-01

-2.7435t-01

-1.4160E 00

-1.5576E 00

4.4247E-01

-8.4077E-01

1.0177E 00

-2.6550E-01

•33-
CA

= 0°

SE I ^ = 180°

X RE(EO) I»1(E0) EfJ{AMP) PHASECEO

O.OOOOE--03 -9.9965E-03 9.9995E-01 lO.OOOOE--01 -1.5608E 00

2.0000E--02 -1.9995E-02 9.9980E-01 lO.OOOOE--01 -1.5508E 00

4.0000E--02 -3.9986E-02 9.9920E-01 IC.OOOOE--01 -1.5308E 00

6.0000E--02 -5.9961E-02 9.9820E-01 lO.OOOOE--01 -1.5108E 00

l.OOOOE--01 -9.9830E-02 9.9500E-01 lO.OOOOE--01 -1.4708E 00

2.00C0E--01 -1.9867E-01 9.8007E-01 lO.OOOOE--01 -1.3708E 00

3.0000E--01 -2.9552E-01 9.5534E-01 lO.OOOOE--01 -1.2708E 00

4.0000E--01 -3.8941E-01 9.2106E-01 lO.OOOOt--01 -1.1708E 00

5.0000E--01 -4.7941E-01 8.7758E-01 lO.OOOOE--01 -1.0708E 00

6.0000E--01 -5.6462E-01 8.2534E-01 9.9999E--01 -9.7082E--01

7.0000E--01 -6.4417E-01 7.6485E-01 9.9997E--01 -8.7083E--01

8.0000E--01 -7.1727E-01 6.9671E-01 9.9994E--01 -7.7086E--01

9.0000E--01 -7.8318E-01 6,2162E-01 9.9989E--01 -6.7090E--01

l.OOOOE 00 -8.4147E-01 5.4030E-01 l.OOOOE 00 -5.7080E--01

1.4000E 00 -9.8547E-01 1.6997E-01 l.OOOOE 00 -1.7079E--01

2.0000E 00 -9.0947E-01 -4.1617E-01 1,0002E 00 4.2915E--01

2.4000E 00 -6.7546E-01 -7.3739E-01 9i9999F--01 8.2921E--01

3.0000E 00 -1.4113E-01 -9.9000E-01 l.OOOOE 00 1.4292E 00

3.4000E 00 2.5553E-01 -9.6680E-01 l.OOOOE 00 -1.3124E 00

4.0000E 00 7.5677E-01 -6.5365E-01 9.9998E--01 -7.1242E--01

4.4000E 00 9.5151E-01 -3.0736E-01 9.9992E--01 -3.1244E--01

5.0000E oc 9.5894E-01 2.8366E-01 l.OOOOE 00 2.87616--01

6.0000E 00 2.7942E-01 9.6017E-01 1.0000"E CO 1-2876E 00

7.0000E 00 -6.5703E-01 7.5390E-01 l.OOOOE 00 -8.5395E--01

8-OCOOE 00 -9.a935E-01 -1.4549E-01 9.9999E--01 1.4601E--01

9.0000E 00 -4.1213E-01 -9.1113E-01 l.OOOOE 00 1.1460E 00

l.OOOOE 01 5.4398E-01 -8.3909E-01 9.9999E--01 -9.9562E--01

1.3000E 01 -4.2019E-01 9.0745e-01 l.OOOOE 00 -1.1371E GO

1.5000E 01 -6.5C26E-01 -7.5968E-01 9.9997E--01 8.6285E--01

1.8000E 01 7.5102E-01 6.6032E-01 l.OOOOE 00 7.2122E--01

2.0000E 01 -9.1298E--01 4.0808E-01 l.OOOOE 00 -4.2033E--01

2.3000E 01 8.4620E-01 -5.3285E-01 lO.OOOOE--01 -5.6197E--01

2.5000E 01 1.3236E-01 9.9121E-01 l.OOOOE 00 1.4380E 00

2.8000E 01 ' -2.7090E-01 -9.6261E-01 l.OOOOE 00 1.2965E 00

3.0000E 01 9.8802E-01 1.5424E-01 9.9999E--01 1.5486E--01

3.30UUE 01 -9.9986E-01 -1.3240e-02 g.9995E--01 1.3241E--02

3.5000E 01 4.2819E-01 -9.0370E-01 l.OOOOE 00 -1.1283E 00

4.0000E 01 -7.4508E-01 -6.6692E-01 9.9996E--01 7.3010E--01

4.5000E 01 -8.5094E-01 5.2532E-01 l.OOOOE 00 -5.5308E--01

5.0000E 01 2.6239E-01 9.6497E-01 l.OOOOE 00 1.3053E 00

-34-
CASE I 0=0 v|; = 185

X RE(HZ) IM(HZ) HZ(AMP) PHASE(HZ)

lO.OOOOE--03 9.7340E-01 1.1346E-02 9.7346E--01 1.1656E-02

2.0000E--02 9.7369E-01 2.2276E-02 9.7395E--01 2.2874E-02

4.0000E--02 9.7394E-01 4.3737E-02 9.7492E--01 4.4877B-02

6.0000E--02 9.737AE-01 6.4897E-02 9.7590E--01 6.6549E-02

l.OOOOE--01 9.7207E-01 1.0666E-01 9.7790E--01 1.0928E-01

2.0000E--01 9.6057E-01 2.0872E-01 9.8299E--01 2.1396E-01

3.0000E--01 9.3893E-01 3.0764E-01 9.8804E--01 3.1663E-01

4.0000E--01 9.0746E-01 4.0292E-01 9.9289E--01 4.1786E-01

5.0000E--01 8.6658E-01 4.9383E-01 9.9741E--01 5.1796E-01

6.0000E--01 8.1674E-01 5.7959E-01 1.0015E 00 6.1716E-01

7.0000E--01 7.5849E-01 6.5941E-01 1.0050E 00 7.1563E-01

8.0000E--01 6.9243E-01 7.3255E-01 1.0080E 00 8.1354E-01

9.0000E--01 6.1926E-01 7.9832E-01 1.0103E 00 9.1105E-01

l.OOOOE 00 5.397AE-01 8.5609E-01 1.0120E 00 1.0083E 00

1.4000E 00 1.7513E-01 9.9727E-01 1.0125E 00 1.3970E 00

2.0000E 00 -4.0644E-01 9.1475E-01 I.OOIOE 00 -1.1527E 00

2.4000E GO -7.2715E-01 6.7639E-01 9.9311E--01 -7.4925E-01

3.0000E 00 -9.8199E-01 1.3640E-01 9.9142E--01 -1.3802E-01

3.4000E 00 -9.6166E-01 -2.6264E-01 .9.9688E--01 2.6661E-01

4.0000E 00 -6.535AE-01 -7.6493E-01 1.0061E 00 8.6376E-01

4.4000E 00 -3.1032E-01 -9.5877E-01 1.0077E 00 1.2578E 00

5.0000E DO 2.7750E-01 -9.6286E-01 1.0020E 00 -1.2902E 00

6.0000E 00 9.5413E-01 -2.7655E-01 9.9341E--01 -2.8212E-01

7.0000F 00 7.5317E-01 6.6314E-01 1.0035E 00 7.2192E-01

8.0000E oc -1.4100E-01 9.9303E-01 1.0030E 00 -1.4298E 00

9.0000E 00 -9.0593E-01 4.1040E-01 9.9456E--01 -4.2535E-01

l.OOOOE 01 -8.3781E-01 -5.4906E-01 1.00I7E 00 5.8013E-01

1.3000E 01 9.0576E-01 4.2441E-01 1.0003E 00 4.3818E-01

1.5000E 01 -7.5544E-01 6.5007E-01 9.9664E--01 -7.1057E-01

1.8000E 01 6.5645E-01 -7.5133E-01 9.9770E--01 -8.5269E-01

2.0000E 01 4.0935E-01 9. 1641E-01 1.0037E 00 1.1507E 00

2.3000E 01 -5.3355E-01 -8.4959E-01 1.0032E 00 I.OIOOE 00

2.5000E 01 9.8856E-01 -1.3040E-01 9.9713E--01 -1.3115E-01

2.8000E 01 -9.5988E-01 2.6943E-01 9.9697E--01 -2.7365E-01

3.0000E 01 1.5183E-01 -9.8985E-01 1.0014t 00 -1.4186E 00

3.3000E 01 -1.1232E-02 1.0019E 00 1.0020E CO -1.5596E 00

3.5000E 01 -9.0274E-01 -4.3079E-01 1.0003E 00 4.4524E-01

4.0000E 01 -6.6434E-01 7.4530E-01 9.9840E--01 -8.4277E-01

4.5000E 01 5.2589E-01 8.5330E-01 1.0023E 00 l.0185t 00

5.0000E 01 9.6294E-01 -2.6125E-01 9.9775E--01 -2.6492E-01

35.
CASE I

lO.OOOOE-03

2.0000E-02

4.0000E-02

6.0000E-02

l.OOOOE-01

2.0000E-01

3.0000E-01

4.0000E-01

5.0000E-01

6.0000E-01

7.0000E-01

b.OOOOE-01

9.0000E-01

l.OOOOE 00

1.4000E 00

2.0000E 00

2.4000E 00

3.0000E 00

3.4000E 00

4.0000E 00

4,400QE 00

5.0000E 00

6.0000E 00

7.0000E 00

8.0000E 00

9.0000E 00

l.OOOOE 01

1.3000E 01

1.5000E 01

1.8000E 01

2.0000E 01

2.3000E 01

2.5000E 01

2.8000E 01

3.0000E 01

3.3000E 01

3.5000E 01

4.0000E 01

4.5000E 01

5.0000E 01

0=0^

KE(EO)

3.5422E-02

2.356AE-02

1.1679E-03

-2.0548E-02

-6.3034E-02

-1.6626b-Ul

-2.661AE-01

-3.6243E-01

-4.5445E-01

-5.4144E-01

-6.2265E-01

-6.9733E-01

-7.6478E-01

-8.2436E-01

-9.7388E-01

-9.0560E-01

-6.7639E-01

-1.4722E-01

2.4754E-01

7.4851E-01

9.4464E-01

9.5554E-01

2.8281E-01

-6.5073b-01

-9.8595E-01

-4.1415E-01

5.3889E-01

-4.1585E-01

-6.5067E-01

7.5078E-01

-9.0951E-01

8.4287E-01

1.3438E-01

-2.7246E-01

9.8628E-0I

-9.9793E-01

4.2555E-01

-7.4499E-01

-8.4852E-01

2.6355E-01

4; = 185

IM(EO)

1.1042E 00

1.0841E 00

1.0643E 00

1.0525E 00

1.0364E 00

1.0054E 00

9.7213E-01

9.3223E-01

8.8462E-01

8.2914E-01

7.6602E-01

6.9568E-01

6.1871E-01

5.3579E-01

1.6096E-01

-4.2762E-01

-7.4828E-01

-9.97t)4E-01

-9.7110E-01

-6.5279E-01

-3.0353E-01

2.9028E-01

9.6604E-01

7.5422E-01

-1.5025E-01

-g.l626E-01

-8.4010E-01

9.0899E-01

-7.6393E-01

O.6420E-01

4.0675E-01

-5.3206E-01

9.9382E-01

-9.6532E-01

1.5668E-01

-1.5331E-02

-9.0463E-01

-6.6954E-01

5.2477E-01

g.6700E-01

EO(AMP)

1.1048E 00

1.0843E 00

1.0643E 00

1.0527E 00

1.0383E 00

1.0190E 00

1.0079E 00

1.00C2E 00

g.9452E-01

9.9027E-01

9.8716E-01

9.8501E-01

9.8371E-01

9.8317E-01

g.8709E-01

1.0015E 00

1.0087E 00

1.0083E 00

1.0022E 00

9.9318E-01

g.9221E-0l

g.9866E-01

1.0066E 00

9.9615E-01

9.9733E-01

1.0055E 00

9.98Q9E-01

9.9959E-01

1.0035E 00

1.0024E 00

9.9632E-01

9.9676E-01

1.0029E 00

1.0030E 00

9.9865E-01

9.9805E-01

9.9973E-01

1.0016E 00

9.9768E-01

1.0023E 00

PHASECEQJ

1.5387E 00

1.5491E 00

1.5697E 00

-1.5513E 00

-1.5101E 00

-1.4069E 00

-1.3036E 00

-1.2000E 00

-1.0962E 00

-9.9230E-01

-8.8827E-01

-7.8421E-01

-6.8020E-01

-5.7634E-01

-1.6379E-01

4.4116E-01

8.3581E-01

1.4243E 00

-1.3212E 00

-7.1720E-01

-3.1090E-01

2.9492E-01

1.2860E 00

-8.5892E-01

1.5122E-01

1.1463E 00

-1.0004E 00

-1.1417E 00

8.6530E-01

7.2429E-01

-4.2054E-01

-5.6308E-01

1.4364E 00

1.2957E 00

1.5755E-01

1.5362E-02

-1.1311E 00

7.3211E-01

-5.5388E-01

1.3047E 00

I

.36.
CASE I 0=0 i|; = 190

X RE(HZ) IM{HZ)

LO.OOOOE--C3 9.4836t-01 1.2754E-02

2.0000E--02 9.491AE-01 2.46C7E-02

^.OOOGE--02 9.5029E-01 A.7489E-02

6.0000E--02 9.5094E-01 6.9773E-02

l.OOOOE--01 9.5081E-01 1.1329E-01

2.0000E--01 9.4270E-01 2.1828E-01

3.0000E--01 9.2400E-01 3.1902E-01

4.0000E--0-1 8.9519E-01 4.1549E-01

5.0000E--01 8.5672E-01 5.0715E-01

6.0000E--01 8.0910E-01 5.9333E-01

7.0000E--01 7.5289E-01 6.7332E-01

8.0000E--01 6.8872E-01 7.4642E-01

9.0000E--01 6.1730E-01 8.1197E-01

l.OOOOE oc 5.3939E-01 8.6936E-01

1.4000E GO 1.7992E-01 1.0079E 00

2.0000E 00 -3.9763E-01 9.1960E-01

2.4000E 00 -7.1791E-01 6.7716E-01

3.0000E oc -9.7A80E-01 1.3210E-01

3.4000E 00 -9.57076-01 -2.6907E-01

4.000CE 00 -6.5349E-01 -7.7225E-01

4.4000E 00 -3.130AE-01 -9.6522E-01

5.0000E 00 2.719AE-01 -9.6637E-01

6.0000E oc 9.A871E-01 -2.7395E-01

7.0000E oc 7.5253E-01 6.6868E-01

8.0000E 00 -1.369AE-01 9.9632E-01

9.0000E oc -9.0126E-01 4.08a3E-01

l.OOOOE 01 -8.3668E-01 -5.5360E-01

1.3000E 01 9.0A25E-01 4.2H22E-01

1.5000E 01 -7.5162E-01 6.4986E-01

1.8000E 01 6.5297E-01 -7.5161E-01

2.0000E 01 4.1048E-01 9.19536-01

2.3000E 01 -5.3419E-01 -8. 52616-01

2.5000fc 01 9.8618E-01 -1.28636-01

2.8000E 01 -9.5742E-01 2.6809E-01

3.00C0E 01 1.4967E-01 -9.9147E-01

3.3000E 01 -9.A020E-03 1.0038E 00

3.5000E 01 -9.0188E-C1 -4.3314E-01

4.0000t 01 -6.6200E-01 7.45A5E-01

4.5000E 01 5.2638E-01 8.55A6E-01

5.0000E 01 9.6112E-01 -2.6C22E-01

HZ(AMP) PHASe(HZ)

9.48A4E--01 1.34486--02

9.49A6E--01 2.5919b--02

9.51486--01 4.9931E--02

9.5350E--01 7.3242E--02

9.5754E--01 1.1859E--01

9.6764E--01 2.27536--01

9.7753E--01 3.3245E--01

9.8691E--01 4.34556--01

9.9557E--01 5.3449E--01

1.0033E 00 6.32746--01

1.01006 00 7.29676--01

1.C156E 00 8.25586--01

1.C200E 00 9.20776--01

1.0231E 00 1.0155E 00

1.02396 00 1.39426 00

1.00196 00 -1.16276 00

9.86886--01 -7.56206--01

9.83716--01 -1.34696--01

g.9417E--01 2.74076--01

1.01166 00 8.68506--01

1.01476 00 1.2572E 00

1.00396 00 -1.2965E ou 9.87476--01 -2.31126--01

1.00676 00 7.26476--01

1.00576 00 -1.4342,6 00

9.89656--01 -4.25866--01

1.00336 00 5.8453b--01

1.00056 00 4.42286--01

9.93616--01 -7.12916--01

9.95636--01 -8.55526--01

1.00706 00 1.15096 00

1.00616 GO 1.01116 00

9.94546--01 -1.297U6--01

9.94246--01 -2.73026--01

1.00276 CO -1.42106 00

1.00386 00 -1.56146 00

1.00C56 00 4.47746--01

9.96966--01 -8.44626--01

1.00446 00 1.01926 00

9.95726--01 -2.64416--01

-37-
CASE I

(j) = 4; = 190

X KECEO) IMCEO)

lO.OOOOE--03 8.6821E-02 1.20g0E 00

2.0000E--02 7.1165E-02 1. 1667E 00

4.0000E--02 4.4551E-02 1.1264E 00

6.0000E--C2 2.0114E-02 1.1036E 00

l.OOOOE--01 -2.6100E-02 1.0745E 00

2.0000E--01 -1.3491E-01 1.0279E 00

3.0000E--01 -2.3832E-01 9.8673E--01

4.0000E--01 -3.3722E-01 9.4170E--01

5.0000E--01 -4.3135E-01 8.9038E--01

6.0000E--01 -5.2016E-01 8.3203E--01

7.0000E--01 -6.0298E-01 7.6657E--01

8.0000E--01 -6.7915E-01 6.9430E--01

9.0000E--01 -7.4800E-01 6.1569E--01

l.OOOOE oc -8.0893E-01 5.3137E--01

l.AOOOE 00 -9.6356E-01 1.5265E--01

2.0000E 00 -9.0239E-01 -4.3800E--01

2.4000E 00 -6.7732E-01 -7.5807E--01

3.0000E 00 -1.5277E-01 -1.0043E 00

3.4000E 00 2.4032E-01 -9.7492E--01

4.0000E 00 7.4105E-01 -6.5'l98E--01

4.A000E 00 9.3839E-01 -3.0006E--01

5.0000E 00 9.5253E-01 2.9624E--01

6.0000E 00 2.8587E-01 9.7130E--01

7.0000E 00 -6.4511E-01 7.5448E--01

8.0000E 00 -9.8290E-01 -1.5453E--01

9.0000E 00 -4.1598E-01 -9.2087E--01

l.OOOOE 01 5.3428E-01 -8.4101E--01

1.3000E 01 -4.1197E-01 9.1036E--01

1.5000E 01 -6.5100E-01 -7.6775E--01

1.8000E 01 7.5059E-01 6.6769E--01

2.0000E 01 -9.0642E-01 4.0554E--01

2.3000E 01 8.3986E-01 -'5.3136E--01

7.5000E 01 1.3620E-01 9.9617E--01

2.8000E 01 -2.7384E-01 -9.6776E--01

3.0000F 01 9.8469E-01 1.5888E--01

3.3000E 01 -9.9614E-01 -1.7190E--02

^.5000E 01 4.2318E-01 -9.0547E--01

4.0000E 01 -7.4487E-01 -6.7188E--01

4,5000E 01 -8.4637E-01 5.2425E--01

5.0000E 01 2.6460E-01 9.6881E--01

EO(AMP)

1.2121E 00

1.1689E 00

i.l273E 00

1.1038E 00

1.07^8E 00

1.0367E 00

I.0151E 00

1.0003E 00

9.8936E-01

9.8124E-01

9.7531E-01

9.7124E-01

9.6881E-01

9.6784E-01

9.7557E-01

1.0031E 00

1.0166E 00

1.0158E 00

1.0041E 00

9.8703E-01

9.8520E-01

9.9753E-01

1.0125E 00

9.9268E-01

9.9497E-01

1.0105E 00

9.9637E-01

9.9924E-01

1.0066E 00

1.0046E 00

9.9301E-01

9.9383E-01

1.0054E 00

1.0058E 00

9.9743E-01

9.9628E-01

9.9948E-01

1.0031E 00

9.9558E-01

1.0043E 00

PHASE(Ea)

1.4991E 00

1.5099E 00

1.5313E 00

1.5526t 00

-1.5465E 00

-1.4403E 00

-1.3338E 00

-1.2269E 00

-1.1197E 00

-1.C121E 00

-9.0428E-01

-7.9643E-01

-6.8868E-01

-5.8119E-01

-1.5711E-01

4.5188E-01

8.4159E-01

I.4198E 00

-1.3291E 00

-7.2155E-01

-3.D949E-01

3.0152E-01

1.2846E 00

-8.6338E-01

1.5594E-01

1.1465E 00

-1.0048E 00

-1.1458E 00

8.6750E-01

7.2702E-01

-4.2070E-01

-5.6410E-01

1.4349E 00

1.2950E 00

1.5997E-01

1.7255E-02

-1.1336E 00

7.3392E-01

-5.5457E-01

1.3042E 00

.38-
CASE I

<l> = 0° ijj = 200°

X RE{HZ) IM(HZ) HZ(AMP) PHASECHZ)

O.OOOOE--03 9.0239E-C1 1.5723E-02 9.0253E--01 1.7422E-02

2.0000E--02 9.0429E-01 2.9377E-02 9.0477E--01 3,2475£-02

4.0000E--02 9.0740E-01 5.4939E-02 9.0906E--01 6.0471E-02

6.0000E--02 9.0979E-01 7.9281E-02 9.1324E--01 8.6923E-02

l.OOOOE--01 9.1278E-01 1.2593E-01 9.2142E--01 1.3710E-01

2.0000E--01 9.1120E-G1 2.3595E-01 9.4125E--01 2.5338E-01

3.0000E--01 8.9798E-01 3.3971E-01 9.6009E--01 3.6166E-01

4.0000E--01 8.7398E-01 4.3808E-01 9.7763E--01 4.6464E-01

5.0000E--01 8.3983E-01 5.3089E-01 9.9356E--01 5.6372E-01

6.0000E--01 7.9614E-01 6.1768E-01 1.0076E 00 6.5983E-01

7.0000E--01 7.4352E-01 6.9783E-01 1.0197E 00 7.5371E-01

8.0000E--01 6.8266E-01 7.7075E-01 1.0296E 00 8.4593E-01

9.0000E--Gl 6.1427E-01 8.3583E-01 1.0373E 00 9.3701E-01

l.OOOOE 00 5.3914E-C1 8.9250E-01 1.0427E 00 1.0274fc GO

1.4000E 00 1.8848E-01 1.0263E 00 1.0435E 00 1.3892E 00

2.0000E 00 -3.8228E-01 9.2782E-01 1.0035E 00 -1.1800E 00

2.4000E 00 -7.0191E-01 6.7833E-01 9.7612E--01 -7.6831E-01

3.0000E 00 -9.6245E-01 1.2456E-01 9.7047E--01 -1.2871E-01

3.4000E 00 -9.4922E-01 -2.8024E-01 9.8972E--01 2.8707E-01

4.0000E 00 -6.5347E-01 -7.8487E-01 1.0213E 00 8.7650E-01

4.4000E 00 -3.1779E-01 -9.7630E-01 1.0267E 00 1.2561E 00

5.0000E 00 2.6232E-01 -9.7237E-01 1.0071E 00 -1.3073E 00

6.0000E oc 9.3938E-01 -2.6942E-01 9.7725E--01 -2.7931E-01

7.0000E oc 7.5145E-01 6.7824E-01 1.0123E 00 7.3424E-01

8.0000E 00 -1.2992E-01 1.0020E 00 1.0104E 00 -1.4418E 00

9.0000E oc -8.9321E-01 4.0611E-01 9.8120E--01 -4.2672E-01

l.OGOOE 01 -8. 3476E-01 -5.6143E-01 1.0060E 00 5.9208E-01

1.3000E 01 9.0165E-01 4.3481E-01 I.OOIOE 00 4.4933E-01

1.5000E 01 -7.4505E-01 6.4949E-01 9.8840E--01 -7.1698E-01

1.8000E 01 6.4697E-01 -7.5210E-01 9.9208E--01 -8.6040E-01

2.0000E 01 4. 1243E-01 9.2489E-01 1.0127t 00 1.1513E 00

2.3000E 01 -5.3530E-01 -8.5782E-01 I.OIUE 00 1.0129E 00

2.5000E 01 9.8209E-01 -1.2558E-01 9.9008E--01 -1.2718E-01

2.8000E 01 -9.'.318E-01 2.6577E-01 9.8954E--01 -2.7192E-01

3.0000E 01 1.4593E-01 -9.9425E-01 1.0049E 00 -1.4251E 00

3.3000E 01 -6.1781E-03 1.0069E 00 1.0069E CO -1.5647E 00

3.5000E 01 -9.0039E-01 -4.3720E-01 1.0009E 00 4.5203fc-01

4.0000E 01 -6.5797E-01 7.4570E-01 9.9448E--01 -8.4782E-01

4.5000E 01 5.2723E-01 8.5917E-01 1.0080E 00 1.0204E 00

5.0000E 01 9.'5797E-01 -2.5844E-01 9.9222E--01 -2.6351E-01

39-
CASE I

= 0° i|j = 200°

X RE{EO) IM(EO) EO(AMP) PHASE(EO)

O.OOOOE--03 2.0600E-01 1.4172E 00 1.4321E 00 1.4264E 00

2.0000E--02 1.7659E-01 1.3254E 00 1.3371E 00 1.4383E 00

4.0000E--02 1.3619E-01 1.2416E 00 1.2491E 00 1.4615E 00

6.0000E--02 1.0360E-01 1.1961E 00 1.2006E 00 1.4844E 00

l.OOOOE--01 4. 7036E-02 1.1415E 00 1.14256 00 1.5296E 00

2.0000E--01 -7.5793E-02 1.0658E 00 1.0685E CO -1.4998E 00

3.0000E--01 -1.8724E-01 1.0105E 00 1.0277E 00 -1.38766 00

4.0000E--01 -2.yi75E-01 9.5655E-01 I.OOOIE 00 -1.27486 00

5.0000E--01 -3.9022E-01 8.9891E-01 9.7996E--01 -1.1612E 00

6.0000E--01 -4.8261E-01 8.3573E-01 9.65076--01 -1.0471E 00

7.0000F--01 -5.6855E-01 7.6641E-01 9.5427E--01 -9.3254E--01

8.0000E--01 -6.4751E-01 6.9093E-01 9.4692E--01 -8.1783E--01

9.noooE--01 -7.1896E-01 6.0962E-01 9.4262E--01 -7.0329E--01

l.OOOOE 00 -7.8233E-01 5.2299E-01 9.41046--01 -5.89276--01

1.4000E 00 -9.4598E-01 1.3790E-01 9.5598E--01 -1.44766--01

2.0000E 00 -8.9710E-01 -4.5600E-01 1.0063E 00 4.70276--01

2.4000F no -6.7912E-01 -7.7495E-01 1.0304E 00 8.5120E--01

3.0000E 00 -1.6244E-01 -1.0158E 00 1.0287E 00 1.41226 00

3.4000E 00 2.2781E-01 -9.8140E-01 1.0075E 00 -1.3427E 00

4.0000E 00 7.2820E-01 -6.5048E-01 9.76426--01 -7.2908E--01

4.4000E 00 9.2767E-01 -2.9403E-01 9.73156--01 -3.0694E--01

5.0000E oc 9.4739E-01 3.0656E-01 9.95756--01 3.1295E--01

6.0000E 00 2.9120E-01 9.8034E-01 1.02276 00 1.282IE 00

7.0000E 00 -6.3542E-01 7.5489E-01 9.86726--01 -8.7112E--01

8.0000E 00 -9.7766E-01 -1.6192E-01 9.9098E--01 1.64146--01

9.0000E 00 -4.1915E-01 -9.2879E-01 1.01906 00 1.14696 00

l.OOOOE 01 5.2633E-01 -8.425SE-01 9.93446--01 -1.0124E 00

1.3000E 01 -4.0527E-01 9.1271E-01 9.98646--01 -1.1529E 00

1.5000E 01 -6.5160E-01 -7.7433E-01 1.01206 00 8.71266--01

1.8000E 01 7.5026E-01 6.7371E-01 1.00846 00 7.3169E--01

2.0000E 01 -9.0110E-01 4.0345E-01 9.8730E--01 -4.20976--01

2.3000E 01 8.3467E-01 -5.3013E-01 9.8880E--01 -5.6586E--01

2.5000E 01 ' 1.3933E-01 1.0002E 00 1.0099E 00 1.4324E 00

2.8000E 01 -2.76236-01 -9.7196E-01 1.01046 00 1.2939E 00

3.0000E 01 9.8197E-01 1.6267E-01 9.95356--01 1.64166--01

3.3000E 01 -9.9299E-01 -2.0374E-02 9.93196--01 2.0515E--02

3.5000b 01 4.1911E-01 -9.0690E-01 9.99066--01 -1.1.3796 00

4.0000E 01 -7.4467E-01 -6.7592E-01 1.00576 00 7.37046--01

4.5000E 01 -8.4267E-01 5.2336E-01 9.91966--01 -5.55776--01

5.0000E 01 2.6641E-01 9.7194E-01 1.00786 00 1.3033E 00

-40-
CASE I 0=0' i|j = 210

X RE (HZ) IM(HZ) HZ(AMP) PHASE(HZ)

lO.OOOOE--03 8.6130E-01 1.8848E-02 8.6150E--01 2.1879E-02

2.0000E--02 8.6A46E-01 3.4218E-02 8.6513E--01 3.9562E-02

4.0000E--02 8.6965E-01 6.2223E-02 8.7187E--01 7.1428E-02

6.0000E--02 8.7383E-01 8.8378E-02 8.7829E--01 1.0080E-01

l.OOOOE--01 e.7989E-01 1.3770E-01 8.9060E--01 1.5524E-01

2.0000E--01 8.8445E-01 2.5181E-01 9.1960E--01 2.7737E-01

3.0000E--01 8.7616E-01 3.5792E-01 9.4645E--01 3.8782E-01

4.0000E--01 8.5639E-01 4.5770E-01 9.71G3E--01 4.9083E-01

5.0000E--01 8.2597E-01 5.5132E-01 9.9307E--01 5.8857E-01

6.0000E--01 7.8563E-01 6.3847E-01 1.0124E 00 6.8243E-01

7.0000E--01 7.3605E-01 7.1865E-01 1.0287E 00 7.7344E-01

8.0000E--01 6.7796E-01 7.9132E-01 1.0420E 00 8.6240E-01

9.0000E--01 6.1210E-01 8.5591E-01 1.0523E 00 9.4998E-01

l.OOOOE 00 5.3927E-01 9.1190E-01 1.0594E 00 1.0367E GO

l.AOOOE 00 1.9586E-0L 1.0415E 00 1.0598E 00 1.3849E 00

2.0000E 00 -3.69A2E-01 9.3451E-01 1.0049E 00 -1.1943E 00

2.4000E 00 -6.8859E-G1 6.7916E-01 9.6717E--01 -7.7850E-01

3.000nE 00 -9.5223E-01 1.1821E-01 9.5954E--01 -1.2351E-01

3.4000E 00 -9.4277E-01 -2.8956E-01 9.8623E--01 2.9799E-01

4.0000E 00 -6.535AE-01 -7.9536E-01 1.0294E 00 8.8297E-G1

4.4000E 00 -3.2180E-01 -9.8548E-01 1.0367E 00 1.2552E 00

5.0000E 00 2.5A31E-01 -9.7731E-01 1.0099E 00 -1.3162E 00

6.0000E 00 9.3165E-01 -2.6563E-01 9.6878E--01 -2.7775E-01

7.0000E 00 7.5059E-01 6.8617E-01 1.0170E 00 7.4G59E-01

8.0000E oc -1.2409E-01 1.0066E 00 1.0142E 00 -1.4481E 00

Q.OOOOE 00 -8.8655E-01 4.0382E-01 9.7419E--01 -4.2742E-01

l.OOOOE 01 -8.3318E-01 -5.6793E-01 1.0083E 00 5.9830E-01

1.3000F ni 8.9951E-01 4.4027E-01 1.0015E 00 4.5518E-01

1.5000E 01 -7.3959E-01 6.4917E-01 9.8408E--01 -7.2038E-01

1 .8000E 01 6.4199E-01 -7.5250E-01 9.8915E--01 -8.6448E-01

2.0000E 01 4.1406E-01 9.2934E-01 1.0174E 00 1.1517E 00

7.3000E 01 -5.3623E-01 -8.6213E-01 1.0153E 00 1.0144E 00

2.5000E 01 9.7869E-01 -1.2304E-01 9.8640E--01 -1.2507E-01

7.8000E 01 -9.4967F-01 2.6385E-01 9.8564E--01 -2.7100E-0I

3.0000E 01 1.4283E-01 -9.9656E-01 1.0067E 00 -1.4284E 00

3.3000E 01 -3.6263E-03 1.0095E 00 1.0095E 00 -1.5672E 00

3.5000E 01 -8.9916E-01 -4.4056E-01 1.0013E 00 4.5559E-01

4.0000E 01 -6.5462E-01 7.4591E-01 9.9243E--01 -8.5049E-01

4.5000E 01 5.2794E-01 8.6225E-01 l.OllOE 00 1.0214E 00

5.0000E 01 9.5536E-01 -2.5697E-01 9.8932E--01 -2.6276E-01

«41-
CASE I

ijj = 210

X KE(EO) IM{EO) EO(AMP) PHASEiEO)

lO.OOOOE--03 3.4405E-01 1.6200E 00 1.6562E 00 1.3615E 00

2.0000E--02 2.9254E-01 1.4737E 00 1.5024E 00 1.3748E 00

4.0000E--02 2.3167E-01 1.3445E 00 1.3643E 00 1.4002E 00

6.0000E--02 1.8781E-01 1.2765E 00 1.2902E 00 1.4247E 00

l.OOOOE--01 1.1781E-01 1.1976E 00 1.2034b 00 1.4727E 00

2.0000E--01 -2.1689E-02 1.0959E 00 1.0961E 00 -1.5510E 00

3.0000E--01 -1.4192E-01 1.0285E 00 1.0382E 00 -1.4337E 00

4.0000E--01 -2.5221E-01 9.6728E-01 9.9962E--01 -1.3157E 00

5.0000E--01 -3.5496E-01 9.0456E-01 9.7171E--01 -1.1968E 00

6.0000E--01 -4.5076E-01 8.3754E-01 9.5113E--01 -l.a771E 00

7.0000E--01 -5.3957E-01 7*6517E-01 9.3628E--01 -9.5661E-01

8.0000E--01 -6.2106E-01 6.8718E-01 9.2625E--01 -8.3590E-01

9.0000E--01 -6.9479E-01 6.0375E-01 9.2046E--01 -7.1540E-01

l.OOOOE 00 -7.6030E-01 5.1532E-01 9.1848E--01 -5.9566E-01

1.4000E 00 -9.3162E-01 1.2530E-01 9.4001E--01 -1.3370E-01

2.0000E 00 -8.9295E-01 -4.7102E-01 1.0096E 00 4.8539E-0/1

2.4000E 00 -6.8083E-01 -7.8893E-01 1.0421E 00 8.5882E-01

3.0000E 00 -1.7056E-01 -1.0253E 00 1-0394E 00 1.4060E 00

3.4000E 00 2.1739E-01 -9.8667E-01 1.0103E 00 -1.3539E 00

4.0000E 00 7.1756E-01 -6.4915E-01 9.6762E--01 -7.3539E-01

4.4000E 00 9.1881E-01 -2.8896E-01 9.6318E--01 -3.0470E-01

5.0000E 00 9.4319E-01 3.1513E-01 9.9444E--01 3.2245E-01

6.0000E 00 2.9565E-01 9.8781E-01 1.0311E 00 ~ 1.2800E 00

7.0000E 00 -6.2739E-01 7.5520E-01 9.8180E--01 -8.7758E-01

8.0000E 00 -9.7334E-01 -1.6807E-01 9.8774E--01 1.7099E-01

9.0000E 00 -4.2181E-01 -9.3535E-01 1.0261E 00 1.1471E 00

l.OOOOE 01 5.1974E-01 -8.4381E-01 9.9103E--01 -1.0187E 00

1.3000e 01 -3.9971E-01 9.1464E-01 9.9817E--01 -1.1588E 00

1.5000E 01 -6.5210E-01 -7.7978E-01 1.0165E 00 8.7433E-01

1.8000E 01 7.5000E-01 6.7870E-01 1.0115E 00 7.3553E-01

2.0000E 01 -8.9669E-01 4..0171E-01 9.8257E--01 -4.2118E-01

2.3000E 01 8.3038E-01 -5.2911E-01 9.8462E--01 -5.6732E-01

2.5000E 01 ' 1.4193E-01 1.0035E 00 1.0135E 00 1.4303E 00

2.8000E 01 -2.7822E-01 -9.7543E-01 1.0143E 00 1.2930E 00

3.0000E 01 9.7971E-01 1.6581E-01 9.9364E--01 1.6765E-01

3.3000E 01 -9.9050E-01 -2.3054E-02 9.9076E--01 2.3271E-02

3.5000E 01 4.1573E-01 -9.0808E-01 9.9872E--01 -1.1415E 00

4.0000E 01 -7.4450E-01 -6.7926E-01 1.0078E 00 7.3961E-01

4.5000E 01 -8.3960E-01 5.2261E-01 9.8896E--01 -5.5677E-01

5.0000E 01 2.6791E-01 9.7454E-01 1.0107E 00 1.3025E 00

-42.
CASE n

^ = 180° ^ = 185°

X RF(H7 ) IM(HZ)

.O.OOOOE--03 9.7244E-01 -1. 13006-02

2-.0000E--02 9.7181E-01 -2.21736-02

4.0000E--02 9.7025E-01 -4.34936-02

6.0000t--0? 9.6827E-01 -6. 44766-02

l.OOOOE--01 9.6310E-G1 -1.05776-01

2.0000E--01 9.4320E-01 -2.0604E-01

3.0000E--01 9.1362E-01 -3.0234E-01

4.00006--01 8.7477E-01 -3-9423E-01

5.0000E--0 1 8.2715E-01 -4.8104E-01

6.0000E--01 7.7130E-01 -5. 62076-01

7.0000E--01 7.0786E-01 -6.36636-01

8.0000E--01 6.3750E-01 -7.04076-m

9.0000E--01 5.6099E-01 -7.63796-01

l.OOOOE 00 4.7913E-01 -8.15276-01

1.4000E 00 1.1585E-01 -9.31036-01

2.0000E 00 -4.33126-01 -8.2149E-01

2.4000E 00 -7.1740E-01 -5.8084E-01

3.0000E 00 -9.12g5E-01 -6.77a5E-02

3. 4000

E

00 r^8.6177E-01 2.9488E-01

4.0000E 00 -5.3718E-01 7. 27576-01

4.4000E 00 -2.0780E-01 8.7608E-01

5.0000E GO 3.2469E-01 a.3377E-01

6.0000E 00 8.6969E-01 1.7016E-01

7.0000E 00 6.0426E-G1 -6. 37546-01

B.OOOOE 00 -2.1231E-01 -8.4501E-01

9.0000E 00 -8.20696-01 -2.7232E-01

l.OOOOE 01 -6.6572E-01 5.4214E-01

1.3000fc 01 7.1744E-01 -4.4123E-01

1.5000E 01 -6.9428E-01 -4.59906-01

l.BOOOE 01 6.16456-01 5.4G92E-01

2.0000E 01 2.3034E-01 -7.7918E-01

2.3000E 01 -3.30306-01 7.30956-01

2.5000E 01 7.95736-01 -5.9057E-03

2.8000E 01 -7.80226-01 -1.02606-01

3.0000E 01 2.31276-01 7.46476-01

3.3000E ni -1.2A39E-01 -7.63776-01

3.5000E 01 -6.38126-01 4.2925E-01

4.00006 01 -5.85706-01 -4.81316-01

4.5000E 01 2.89906-01 -6.8986E-01

5.0000E 01 7.35136-01 7.9969E-02

HZ(AMP) PHASE(HZ)

9.72516-01 -1.1619E-02

9.7207E-01 -2.28126-02

9.7122E-01 -4.4797E-02

9.7042E-01 -6.6490E-02

9.6889E-01 -1.09386-01

9.65446-01 -2.1507E-01

9.6234E-01 -3.1958E-01

9.59506-01 -4.23406-01

9.5685E-01 -5.26756-01

9.54376-01 -6.29756-01

9.52036-01 -7.3247E-01

9.49806-01 -8.34986-01

9.47676-01 -9.37306-01

9.45636-01 -1.0395E 00

9.3821E-01 -1.4470E 00

9.28676-01 1.08566 DC

9.23066-01 6.80606-01

9.15466-01 7.41136-02

9.10826-01 -3.29706-01

9.04396-01 -9.34826-01

9.00396-01 -1.33796 00

8.94766-01 1.19946 00

8.8618E-01 1.9321E-01

8.7840E-01 -8.1219E-01

8.7128E-01 1.3246E 00

8.6469E-01 3.2039E-01

8.5855E-01 -6.83446-01

8.42266-01 -5.51396-01

8.32786-01 5.85066-01

8.20126-01 7.20236-01

8.12516-01 -1.28346 00

8.02126-01 -1.1464E 00

7. 95766-01 -7.4215E-03

7.86946-01 1.30756-01

7.81486-01 1.27046 00

7.7383E-01 1.40946 Ou

7.69066-01 -5.9216E-01

7.5809E-01 6.87876-01

7. 48306-01 -1.17306 00

7.39466-01 1.08366-01

-43-
CASE n

</> 180 i\j = 185

X R£(EO)

10.0000b--03 -5.3069E--02

2.0000E--02 -6.aC78E--02

4.0000E--02 -8.a505E--02

6.0000t--02 -1.0892E--01

1.0000&--01 -1.4939E--01

2.0000E--01 -2.4a08E--01

3.0000E--01 -3.4288E--01

4.0000E--01 -4.3320E--01

5.0000E--01 -'3.1833E--01

6.0000E--01 -5.9757E--01

7.0000E--01 -6.7022E--01

8.0000E--01 -7.3564E--01

9.0000E--01 -7.9324E--01

l.OOOOE oc -e.4252E--01

1.4000E 00 -9.4897E--01

2.0000E 00 -8.2560E--01

2.A000E 00 -5.7722E--01

3.0000E 00 -5.6513E--02

3.4C00E 00 3.0818E--01

4.0000E 00 7.3951E--01

4.4000E 00 8.3486E--01

5.0000E oc 8.3609E--01

6.0G00E 00 1.631AE--01

7.0000E 00 -6.4588E--01

a.OOGOfc 00 -8.4714E--01

9.0000E 00 -2.6739E--01

l.OOOOE 01 5.4872E--01

1.3000E 01 -4.4671E--01

I.5000E 01 -4.5724E--01

1.8000E 01 5.3898E--01

2.0000E 01 -7.8153E--01

2.3000E 01 7.3333E--01

2.5000E 01 -8.9910E--03

2.8000E 01 -9.9920E--02

3.0000E 01 7.4639E--01

3.3000E 01 -7.6399E--01

3.5000E 01 4.3149E--01

4.0000E 01 -4.7998E--01

4.5000E 01 -6.9087E--01

5.0000E 01 7.8 32 3E--02

IM(EO)

1.0991E

•1.0780E

1.0563E

1.0427E

1.0229E

9.8321E00

00

00

00

00

•01

9.4191E-01

8.9463E-01

8.4039E-01

-7.7909E-01

-7.1104E-01

•6.3673E-01

5.5681E-01

-4.7200E-01

1.0063E-01

4.5189E-01

7.3427E-01

9.22g4E-0l

8.6597E-01

5.3323E-01

1.9987E-01

-3.3531E-01

•8.7623E-01

•6.0193E-01

2.1990E-01

8.2599E-01

6.6440E-01

•7.1683E-01

6.9842E-01

6.2024E-01

2.2722E-01

3.2777E-01

7.9670E-01

7.8140E-01

•2.3402E-01

1.2690E-01

6.3728E-01

5.8734E-01

2.8831E-01

•7.3555E-01

£0(AMP)

1.1006E 00

1.0802E 00

1.0600E 00

1.0483E 00

1.0338E 00

1.0140E 00

1.0024E 00

9.9400E-01

9.8738E-01

9.8187E-01

9.7712E-01

9.7293E-01

9.6916E-01

9.6573E-01

9.5429E-01

9.4117E-01

9.3399E-01

9.2467E-01

9.1917E-01

9.1171E-01

9.0715E-01

9.0082E-CI

3.9133E-01

8.8288E-01

8.7522E-01

8.6819E-G1

8.6169E-01

8.4462E-01

8.3478E-01

8.2171E-01

8.1389E-01

8.0324E-01

7.9675E-01

7.8777E-01

7.8222E-01

7.7445E-01

7.6961E-01

7.5851E-01

7.4862E-01

7.3970E-01

PHASE

,^180E

,5077E

,4872E

,4667E

1.4258E

1.3236E

1.2217E

1.1199E

1.0181E

1650E

1494E

1346E

1203E

1066E

,0565E

-5.0080E

-9.0458E

-1.5096E

1.2289E

6.2472E

2.2215E

-3.8141E

1.3867E

7.5019E

2.5398E

-1.2577E

8.8047E

1.0135E

-9.9114E

-8.5538E

2.8294E

4.2033E

1.5595E

-1.4436E

3.0383E

1.6460E

9.7561t

-8.8565E

3.9535E

1.4647E

(EO)

00

00

00

00

00

00

00

00

00

-01

-01

-01

-01

-01

-01

-01

-01

00

00

-01

-01

-01

00

-01

-01

00

-01

00

-01

-01

-01

-01

00

00

-01

-01

-01

-01

-01

00

-44-
CASE U

</) = 180° 4i = 185°

X RE(EP) IM(EP) EP(AMP) PHASE(EH)

O.OOOOE--03 5.0882E-03 9.3475E-02 9.3613E-02 1.5164E 00

2.0000E--02 6.0A51E-03 9.l633t-02 9.1833E-02 1.5049E 00

4.000CE--02 7.9537E-03 8.9694E-02 9.0046E-02 1.4824E 00

6.0000E--U2 9.8312E-03 8.8441E-02 8.8985E-02 1.4601E 00

l.OOOOE--01 1.3500E-02 8.6n69E-02 8.7615E-02 1.4161E 00

2.0000E--01 2.2265E-02 8.2699E-02 8.^643E-02 1.3078fc 00

3.0000E--01 3.0513E-n2 7.8683E-02 8.4392E-G2 1.2009E oc 4.0000E--01 3.8240E-02 7.4162E-02 8.3440E-02 1.0947E 00

5.0000E--01 A.5409E-02 6.9066E-02 8.2657E-02 9.8918c--01

6.0000E--01 5.1977E-02 6.3399E-02 8.1982E-02 8.8408t--01

T.OOOOE^-01 5.7R95E-02 5.7197E-02 8.1384E-02 7.7933E--01

8.0000E--01 6.3122E-02 5.0511E-02 8.0843E-02 6.7487E--01

9.0000E--01 6.7617E-02 4.3403E-02 8.0348E-02 5.7066E--01

l.OOOOE 00 7.13A7E-02 3.5942E-02 7.9889E-02 4.6665E--01

1.4000E 00 7.8P0AE-02 4.0928E-03 7.8311E-C2 5.2287E--02

2.0000E oc 6.A517E-02 -4.0974E-02 7.6428E-C2 -5,6582E--01

2.4000E 00 4.2212E-02 -6.2440E-02 7.5369E-02 -9.7633E--01

3.0000E 00 -1.A531E-03 -7.3962E-02 7. 39766-02 l. 5512b 00

3.4000E oc -3.0371E-02 -6.6541E-02 7.3144E-02 1.1426E 00

A.OOOOE 00 -6.2098E-02 -3.6454E-02 7.20C8E-02 5.3083E--ul

4.400nE 00 -7.0766E-02 -6.787bE-03 7.1310E-02 1.2354E--01

5.0000E oc -6.2170E-02 3.2R96E-02 7.0337E-02 -4.8668E--01

6,0000E 00 -4.7236E-03 6.8710E-02 6.8873E-02 -1.5022E OJ

7.0000E 00 5.4771E-02 3.9558E-02 6.7562E-02 6.255CE--01

B.OOOOE oc 6.1A59E-02 -2.5063E-02 6.6373E-02 -3.8721E--01

9.0000E oc 1.1166E-02 -6.4318E-02 6.5280E-02 -1.3989E 00

l.OOOOE 01 -4.7813E-n2 -4.2947E-02 6.4269E-02 7.3183E--01

1.3000E 01 4.0900E-02 4.6G73E-02 6.1608E-02 8.448ie--01

1.5000E 01 2.33A2E-02 -5.5353E-02 6.0073E-02 -1.1717E 00

1.8000E 01 -2.8768E-02 5.0400E-02 5.8032E-02 -1.0521E 00

2.000nE 01 5.6646E-02 4.332jE-03 •i.6811E-02 7.6326E--02

2.3000E 01 -5.4048E-02 -1.0957E-02 5.5147E-02 2.0002E--01

2.5000E 01 1.2872E-n2 5.2579E-02 5.4131E-C2 1.3307E 00

2.8000E 01 -5.9762E-C3 -5.23a5E-02 5.2723E-02 1.4572E 00

3.0000E 01 -4.4149E-02 2.7197E-02 5.1854E-02 -5.5212E--01

3.3000E 01 4.6162E-02 -2.0811E-02 5.0636E-02 -4.2354E--01

3.5000E 01 -3.7826E-02 -3.2508E-02 4.9875E-02 7.0994E--0 1 4.0000E 01 1.8908E-02 -4.4258E-02 4.8128E-02 -1.1671t 00

4.5000E 01 4.6333E-02 4;6289E-03 4.6564E-02 q.9573E--02

5.0000E 01 9.1002E-03 4.4226E-02 4.5152E-02 1.3679E 00

.45-
CASE n

(/) = 180 i|j = 190

lO.OOOOE-03

2.0000E-02

4.0000£-02

6-OO00E-02

i.ooooe-01

2.000GE-01

3.0000E-01

4.0000E-0I

5.0000E-01

6.0000E-01

7.0000E-01

8.0000E-01

9.0000E-0I

l.OOOCE 00

1.4000E 00

2.0000E 00

2.4000E 00

3.0000E 00

3.4000E 00

4„0000E 00

4.4000E 00

5.0000E 00

6.0000E 00

7.0000E 00

8.0000E 00

9.0000E 00

l.OOOOE 01

1.30nnE 01

1.5000E 01

1 -BOOOE 01

2.0000E 01

2. 3000 E 1 2.5000E 01

2.800nE 01

3.0000E 01

3.3000E 01

3.5000E 01

4.0000E 01

4.5000E 01

5.0000E 01

RE(HZ)

9.4626E-01

9.4511E-01

9.4253E-01

9.3957F-01

9.3247t-01

9.0800E-01

b.7428E-01

8.3184E-01

7.8124E-01

7.2312E-01

6.5816E-01

5.8709e-01

5.1070E-01

4.2980E-01

7.8606E-02

4.3253E-01

•6.8578E-01

-8.4174E-C1

•7.7703E-01

•4.5948E-01

1.5285E-01

3.2715E-01

7.8671E-01

5.1322E-01

2.2118E-01

-7.3481E-01

•5.6553E-01

6.1048E-01

6.1531E-01

5.4491E-01

1.8038E-C1

2.6934E-01

6.8006E-01

-6.6678E-01

2.0443E-01

•1.1086E-01

•5.4099E-01

4.9777E-01

2.4983E-01

6,2474E-01

IM(HZ)

-1.2566E-02

-2.4217E-02

-4.6642E-02

-6.8392E-02

-1.1C62E-01

-2.1116E-01

-3.0586E-01

-3.9488E-01

-4.7786E-01

-5.5431E-G1

-6.2372E-01

-6.8560E-01

-7.3950E-01

-7.8502E-01

-8.7805E-01

-7.4877E-01

-5.1067E-01

-2.6594E-02

3.0421E-01

6.8394E-01

8.0312E-01

7.3950E-01

1.1733E-01

-5.9238E-01

-7.4110E-01

-2.0937E-01

5.0105E-01

'4.0756E-01

-3.7803E-01

^.5054E-01

-6.7467E-01

6.3198E-01

-1.7679E-02

-7.8008E-02

6.3382E-01

-6.4931E-01

3.6802E-01

-4.0948E-01

-5.8519E-01

7.4463E-02

H7 (AMP)

9.4634E-0i

9.4542E-01

9.4368E-01

9.4205E-01

9.3901E-01

9.3223E-01

9.2624E-C1

9.2080F-C1

9.1579E-01

9 1113E-U1

9.0675E-Ui

9.0262E-01

8.9870E-01

8.9497E-01

8.8156E-01

8.6472E-01

8.5503E-01

8.4216E-01

8.3445E-01

8.2395E-01

8.1753E-01

8.0864E-01

7.9541E-01

7.8378E-01

7.7340E-01

7.6406E-01

7.5556E-01

7.3403E-01

7.2216E-01

7.0704E-01

6.9837E-01

6.8698E-01

6.8029E-01

6.7133E-01

6.6597E-01

6.5870E-01

6.5430E-01

6.4456E-01

6.3629E-01

6.2917E-01

PHASE(HZ)

1 .3279E--02

2 .5618E--02

4 .9445E--02

7 .2663E--02

1 .1808E--01

2 .2849t--01

3 .3654E--01

4 .4321E--01

5 .4895E--01

6 .5401E--01

7 .5854E--01

8 .6265E--01

9 .6641E--01

1 .n699E GO

1 .4815E 00

1 .0470E 00

6 .4008E--01

3 .1583E--02

3 .7316E--0 1 9 .7923E--01

1 .3827E 00

1 .1543E 00

1 .4805E--01

8 .5688E--01

1,.2808E 00

2 .7758E--01

7 .2502E--01

5 .8865fc--01

5..5092E--01

6..9088E--01

1 .3095E 00

1 .1679E 00

2..5991E--02

1..1646E--01

1 .2588E 00

1..4017E 00

5..9737E--01

6,.8839E--01

1 .1673E 00

1..1863E--01

I

-46-
CASE n

(/> = 180° Hi = 190°

X RE(EO) IM(EO) EO{AMP) PHASE (EO)

lO.OOOOE--03 -1.1147E-01 -1.1897E 00 1.1949E 00 I.-4774E 00

2.0000E--02 -1.1955E-0I -I.1457E 00 1.1519E 00 1.4668E 00

4.0000E--02 -1.3834E-ai -1.1016E 00 1.1I03E 00 1.4459E 00

6.0000E--02 -1.5783E-01 -1.0750E 00 i.oaesE 00 1.4250E 00

I.OOOOE--01 -1.9688E-01 -1.0386E 00 1.0571E 00 1 .3835E 00

2.0000E--01 -2.9179E-01 -9.7bl9E-0l 1.0179E 00 I.2801E 00

3.0000E--01 -3.8175E-01 -9.1897E-01 9.951IE-C1 1.1771E 00

4.0000E--01 -4.6623E-01 -8.6C72E-01 9.7888E-01 1.C744E 00

5-COOOE--01 -5.4469E-ni -7.9801E-01 9.6618E-01 9.7187E-01

6.0000E--01 -6.1659E-01 -7.3C19E-01 9.5570E-01 8.6955E-01

7.0000b--01 -6.8140E-01 -6.5726E-01 9.4673E-01 7.6737E-01

8.0000E--01 -7.3863E-01 -5.7957E-01 9.3887E-01 6.6532E-0I

9.000uE--0 1 -7.8784E-01 -4.9766E-01 9.3185E-01 5.6338E-01

l.OOOOE 00 -8.2866E-01 -4. 1216E-01 9.2550E-0I 4.6155)h-0l

I.4000E CO -9.0326E-01 -4.9769E-02 9.0463E-01 5.5044E-02

2.0000E 00 -7.5005E-01 4.6279E-01 8.8133E-G1 -5.5284E-01

2.4000E 00 -5.0031E-01 7. 1037E-01 8.6887E-01 -9.5719E-01

3.000CE 00 -6.8870E-03 8.5304E-01 8.53r6E-01 -1.5627E 00

3.4000E 00 3.2481E-01 7.7890E-01 8.4392E-01 1.1757E 00

4.0000E 00 6.9951E-01 4.4996E-01 8.3173E-01 5.7161E-01

4.4000E 00 8.1265E-01 1.3885E-01 8.2443E-01 1.6923E-01

S.OOOOfc 00 7.3898E-01 -3.4241-E-Ol 8.1445E-01 -4.3391E-01

6-OOOOE 00 1.0575E-01 -7.9287E-01 7.9989E-01 -1.4382E 00

7.0000E GO -6.0215E-01 -5.0719E-01 7.8729E-01 7.0000E-01

8.0000E 00 -7.409IE-01 2.3137E-01 7.7620E-01 -3.0269E-01

9.0000E 00 -2.0142E-01 7.3936E-01 7.6630E-01 -1.3048E 00

l.OOOOE 01 5.0829E-01 5.6147E-01 7.5737E-01 8.3507E-01

1.3000t 01 -4.1337E-01 -6.0771E-01 7.3498E-01 9.7348E-01

1.5000E 01 -3.7361E-01 6.1fi70E-01 7.2275E-01 -1.0275E 00

1.8000E 01 4.4715E-01 -5.4a01E-01 7.07?9E-01 -8.8640E-01

2.0000E 1 -6.7580E-01 -1.7644E-01 6.9846E-01 2.5538E-01

2.3000E i: 1 6.3329E-01 2.6608E-01 6.8691E-01 3.9776t-01

2.5000F 01 -2.0866E-02 -6.7982E-01 6.8014F-01 1.5401E 00

2.8000E 01 -7.5207E-02 6.6683E-01 6.7111E-01 -1.4585E 00

3.0000E 01 6.3278E-01 -2.0679E-01 6.6571E-G1 -3.1586E-01

3.3000fc 01 -6.4862E-01 1.1307E-01 6.5840E-01 -1.7258E-01

3.5000E 01 3.6960E-01 5.3953E-01 6.5398E-01 9.7018fc-01

4.0000E 01 -4.0788E-01 4.9864E-01 6.4422E-01 -8.8518E-01

4.5000E 01 -5.8347E-01 -2.4fi28E-0I 6.3594E-01 ^.0108E-01

5. 0000

E

01 7.3105E-C2 -6.2456E-01 6.2882E-01 -1.4543E 00

-47-
CASE II

= 180 v|j = 190

X KE(EP) IM{EP)

lO.OGOaE--03 1.9228E-02 1.9829E-01

2.0000E:--02 2.0999E-02 1.9073E-01

4.0000E--02 2.4801E-C2 1.8297E-01

6.0000t--02 2.8587E-02 1.7012E-01

l.OOOOE--01 3.5933E-02 1.7125E-01

2.0000E--01 5.3030E-02 1.5867E-01

3.0000E--01 6.d552E-02 1.4734E-01

4.0000t--01 8.2615E-02 1.3574E-01

5.0000E--01 9.5236E-02 1.2351E-01

6.0000E--01 1.0639E-01 1.1059E-01

7.0000E--01 1.1605E-01 9.7004E-02

S.OOOOh--01 1.2418E-01 8.2843E-02

9.0000E--01 1.3075E-01 6.8217E-02

l.OOOOE oc 1.3575E-01 5.3256E-02

1.4000E 00 1.4004E-01 -7.1428E-03

2.0G00t oc 1.0384E-01 -8.4219E-02

2. 4000

E

00 5.9166E-02 -1.1589E-01

3.0U00E 00 -1.8838E-02 -1.2400E-01

3.4000E 00 -6.5660t-02 -1.0376E-01

4.0n00h oc -1.1029E-01 -4.5117E-02

4.4000E JO -1.1693E-01 2.6676E-03

5.00U0E Oc -9.1521E-02 6.7881E-02

6.0000t 00 9.3527E-03 I.0907E-01

r.ooout uo 9.4626E-02 4.6980E-02

8.0000E oc 8.6780E-02 -5.4C23E-02

9.0000E 00 -1.8478E-04 -g.9148E-02

l.OOOOE 01 -B.1920E-02 -5.0743E-02

1.3000E 01 7.0557E-02 5.4753E-02

1.5000E 01 1.7879E-02 -8.3527E-02

1.8000E 01 -2.5861E-02 7.6180E-02

2.0000E 01 7.7061E-02 -9.0052E-03

2.30006 01 -7.3805E-02 -4.7509E-04

2.5000E 01 ' 3.0083E-02 6.4942E-02

2.8000E 01 -2.0713b-02 -6.5359E-02

3.0000E 01 -4.9075E-02 4.5248E-02

3.3000E 01 5.2498E-02 -3.7091E-02

3.5000E 01 -5.4494E-02 -3.1155E-02

4.0000E 01 1.2737E-02 -5.8029E-02

4.500 0E 01 5.6322E-02 -4.7835E-03

S.OOOOt 01 2.0213E-02 5.0085E-02

EP(AMP) PHASE(EP)

1.9922E-01 1.4741E 00

1.9188E-01 1.4611E GO

1.8464E-01 1.4361E 00

1.8040E-01 1.4117E 00

1.7498E-01 1.3640E GO

1.6730t-0i 1.2483t 00

L.6250E-01 1.1353E 00

1.5890b-01 l.')240E 03

1..5596E-01 9.1394E--01

1.5346E-01 8.0473E--01

1.5125E-01 6.9623E--Gl

1.4928E-01 5.8831E--01

1.4748E-01 4.8087E--01

1.4582E-01 3.7385E--01

1.4022E-01 -5.09626--02

1.3370E-01 -6.8145E--01

1.3012E-01 -1.0987E 00

1.2550E-01 I.4201E GO

1.2279E-01 1.0066E GO

1.1916E-01 3.8832E--01

1.1696E-01 -2.2810E--02

1.1395E-01 -6.3817E--01

1.0951E-01 1.48076 00

1.0565E-01 4.6083E--01

1.0222E-01 -5.5682E--01

9.9148E-02 1.5689E 00

9.6362E-02 5.54586--01

8.9310E-02 6.5994E--01

8.5419E-02 -1.3599E 00

8.0450E-02 -1.2435E 00

7.75R5E-02 -1.1633E--01

7.3807E-02 6.4371E--03

7.1571E-02 1.1370E 00

6.8563E-02 1.2639E GO

6.6751E-02 -7.4486E--Gl

6.4279E-02 -6.1510E--01

6.2772E-02 5.I936E--01

5.9411E-02 -1..3547E GO

5.6525E-02 -8.4729E--02

5.4010E-02 1.1872E 00

-48-
CASE n

= 180° \\> = 200°

X R£(HZ) TM(HZ) HZ(AMP) PHASE(HZ)

o.ooooe--03 8.9755E-01 -1.4912E-02 8.9768E-01 -1.6612E-02

2.0000E--02 8.9529E-01 -2.7793E-02 8.9572E-01 -3.1034E-02

4.0000E--02 8.9069E-01 -5.1743E-02 8.9219E-01 -5.8026E-02

6.0000E--02 8.8584E-01 -7.4353E-02 8.8896E-01 -8.3738E-02

l.OOOOE--01 8.7527E-01 -1.1716E-01 8.8308E-01 -1.3306E-01

2.0000E--01 8.433AE-01 -2.1548E-01 3.7044t-01 -2.50156-01

3.00006--01 8.0374E-0I -3.0497E-01 8.5965E-01 -3.6265E-01

4.0000E--01 7.5695E-01 -3.8694E-01 8.501 lE-01 -4.7256E-01

5.COO0E--01 7.0355E-01 -4.6169E-01 8.4151E-01 -5.80746-01

6.0000E--01 (S.4418E-01 -5.2916E-01 8.3365E-01 -6.87686-01

7.0000E--CI 5.7949E-01 -5.8916E-01 8.2639E-0L -7.9367E-01

8.0000E--01 5.1020E-0I -6.415aE-01 8.1965E-01 -8.9891E-0I

9.0000E--01 4.3703E-01 -6.8596E-01 8.1335E-01 -1.0035E 00

l.OOOOE 00 3.6073E-01 -7.2241E-01 8.0747E-01 -1 .1077E DC

1.4000E 00 3.9569E-02 -7.8591E-01 7.8691E-0I -1.5205E 00

2.0000E 00 -4.3632E-01 -6.4526E-01 7.6253E-01 1.UQ88E 00

2.4000E 00 -6.1691E-01 -4.25I4E-01 7.4921E-01 6. 03406-01

3. 0000

E

00 -7.3234E-01 1.6116E-03 7.3234E-01 -2.2006E-03

3.4000E 00 -6.6428E-01 2.8458E-01 7.2267E-01 -4.0475E-01

4.0000E 00 -3.7921E-01 6.0025E-01 7.0999E-01 -1.0074E 00

4.4000E 00 -1.1353E-01 6.9330E-01 7.0254E-01 -1.4085E 00

5.0000fc 00 2.9418E-01 6.2696t-01 6.9255E-01 1.1321E 00

6.0000E 00 6.7258E-0I 8.9031E-02 6.7844E-01 1.3161E-01

T.OOOOt Ow 4.3102E-01 -5.0P69E-01 6.6674E-01 -8.6786E-01

a.oooot DC -1.9155E-01 -6.2030E-0I 6.5685E-01 1.2749E 00

9.0000E 00 -6.2374E-01 -1.7693E-01 ft.4835E-Cl 2.7640F-01

l.OOOOE 01 -4.8109E-01 4.2353E-01 6.4096E-01 -7.2185E-01

1.3000E 01 5.2347E-ni -3.3B82E-01 6.2355E-01 -5-7445E-01

1.5000E 01 -5.1717E-0I -3.3228E-01 6.1472E-01 5.7109E-01

1.8000E 01 4.S489E-01 3.9763E-01 6.0418t-01 7.1833E-0I

2.0000t 01 1.7264E-01 -5.7302E-01 5.9847E-01 -1.2782E 00

2.3000E 01 -2.!>14aE-01 5.3522E-01 5.9132E-01 -1.1317E 00

2.5000E 01 5.8723E-01 7.6022E-03 5.8728E-01 I.2945E-02

2.8000E 01 -5.7475E-01 -9. 1989E-02 5.8206E-01 1 .5870E-01

3.0000E 01 1.5329E-01 5.5843E-01 5.7908E-01 1.3029E 00

3.3000E 01 -7.0405E-02 -5.7071E-01 5.7'i03E-01 1.448IE 00

3.5000E 01 -4.8829E-01 2.9919E-01 5.7266E-01 -5.497^6-01

4.0000E 01 -4.1971E-0I -3.8206E-01 5.6756E-01 7.^R47e-01

4.5000E 01 2.4770E-01 -5.0600E-01 5.6337E-01 -1.11566 00

5.0000E 01 5.5162E-01 9.5547E-02 5.5984E-01 1.7151E-01

-49-
CASE U

(j> = 180 4; = 200

X RE(EO) IMCtO) EO{AMP) PHASE(EO)

lO.OOOOE--C3 -2.2804E-01 -1.3403E 00 1.3595E GO 1.402 36 OC

2.0000t--02 -2.2617E-01 -1.24 74E 00 1.2678E 00 1.39146 00

4.0000E--02 -2.3547E-01 -1.1581E 00 1.1818E 00 1.37026 00

6.0000fc--02 -2.4918E-01 -1.1063E 00 1.1340E 00 1.34926 00

l.OOOOE--01 -2.7987E-01 -1.0391E 00 i.0761E 00 1.30776 00

2.0G00E--01 -3.5834E-01 -9.3517E-01 1.0015E 00 1.2049E 00

3.0000E--01 -4.3291E-01 -8.5638E-01 9.59586-01 1.1027E 00

4.0000E--01 -5.0196E-01 -7.8354E-01 9.30546-01 I.OOIOE 00

5.00006--01 -5.6493E-01 -7.1130E-0I 9.0a35E-Gl 8.9959E-01

6.0000E--01 -6.2141E-01 -6.3771E-01 8.90416-01 7.9834E-01

7.0000E--01 -6.7105E-01 -5.6209E-01 8.7536E-01 6.9726E-01

8.0000E--01 -7.1357E-01 -4.8431E-01 8.62416-01 5.9630E-01

9.0000E--01 -7.4872E-01 -4.0460E-01 8.51056-01 4.9543E-01

l.OOOOE 00 -7.7620E-01 -3.2356E-01 8. 40946-01 3.9495E-01

1.4C00E 00 -8.0887E-0] 5.6345E-03 8.08896-01 -6.9658E-03

2.0000E 00 -6.3637t-0] 4.4303E-01 7.7540E-01 -6.0B16E-01

2.4000E 00 -4.0455E-01 6.4163E-01 7.58526-01 -1.0082E OC

3.0000E 00 2.7214E-02 7.3769E-01 7.3819E-01 I.5339E 00

3.40nOE 00 3.0713E-01 6.5891E-01 7.2697E-Ci 1.I346E 00

4.000Ut oc 6.1271E-01 3.6395E-01 7.12656-01 5.3599E-01

4.4000E GO 6.9779E-01 9.6242E-02 7.0440E-01 1.3706E-01

5.0000E oc 6.2108t-01 -3.0863E-0I 6.9353E-01 -4.6119E-01

6.0000E 00 7.6348E-02 -6.74iaE-0l 6.7848E-01 -1.4580E 00

7.0000E 00 -5.1516E-01 -4.2246E-01 6.6624E-01 6.8685E-01

8.0000E oc -6.2477E-0I 2.0003E-01 6.5601E-01 -3.0985E-01

9.0000E -1.6904E-01 6.2486E-01 6.4732E-01 -1.3066E 00

l.OOOOE 01 4.2794E-01 4.7365E-01 6.3982E-01 8.3814E-01

1.3000E 01 -3.4224E-01 -5.1979E-01 6.2234E-01 9.8853E-01

1.5000E 01 -3.2827E-C1 5.1833E-0I 6.I354E-01 -1.0062E 00

1.8000E 01 3.9458E-01 -4.5610E-0I 6.G309E-01 -8.5759E-01

2.0000E 01 -5.7281E-01 -1-.6982E-01 5.9746E-01 2.8821E-01

2.3G0OE 01 5.3530E-01 2.4907E-01 5. 90406-01 4.3549E-01

2.5000E 01 - 5.6951E-03 -5.8640E-0I 5.8643E-01 -1.5611E 00

2.8000E 01 -9.0296E-02 5.7424E-01 5.8130E-01 -1.4148E 00

3.0000E 01 5.5731E-01 -1.5443E-01 5.78316-01 -2.7032E-01

3.3000E 01 -5.6990E-01 7.1556E-02 5.7438E-01 -1.2490E-01

3.5000E 1 2.9984E-01 4.8717E-01 5.7205E-01 1.0191E 00

4.0000E 01 -3.8102E-01 4.1994E-01 5.6703E-01 -8.3395E-01

4.5000E 01 -5.0591E-01 -2.4682E-01 5.6291E-01 4.539CE-01

5.0000E 01 9.4835E-02 -5.5133E-01 5.5943E-01 -1.4005E 00

50.
CASE II

= 180° i|; = 200°

X RE(EP) IM(EP) EP(AMP) PHASE(EP)

lO.ooonE--03 7.6924E-02 4.3405E-01 4.40aiE-0I 1.3954E 00

2.0000E--02 7.8005E-02 4.0280E-01 4.1029E-01 1.3795E 00

4.0000E--02 8.3530E-02 3.7132E-01 3.8109E-01 1.3498E 00

6.0000E--0 2 8.9881E-02 3.5316E-01 3.6442E-01 1.3216E 00

l.OOOOF--01 1.0260E-01 3.2790E-01 3.4357t-0I 1.2675E 00

2.0000E--01 1.3159E-01 2.8619E-01 3.1499E-01 1.1398E 00

3.000CE--01 1.5639E-01 2.5336E-01 2.9774E-01 1.0178E 00

4.0000E--01 1.7742E-01 2.231RE-01 2.8511E-01 8.9913E-01

5.0000E--01 1.9498E-01 1.9398E-01 2.7504E-01 7.8282E-01

6.0000E--01 2.0925E-01 1.6521E-01 2.6661E-01 6.6635E-01

7.0000E--01 2.2034E-01 1.3673E-01 2.5931E-01 5.5338E-01

8.0000E--01 2.2836E-01 1.0855E-01 2.5284E-01 4.4374E-01

g.oooot--01 2.3340E-01 8.0B13E-C2 2.4700F-01 3.3332t-01

l.ooonE 00 2.3601E-01 5.2937E-02 2.4187E-01 2.2065E-01

1.4000E 00 2.1949E-01 -4.8020E-02 2.2468E-01 -2.1539E-01

2.0000E 00 1.3466E-01 -1.5555E-01 2.0574E-01 -8.5724E-01

2.4000E oc 5.6179E-02 -l,8759E-01 1.95a2E-01 -1.2798E 00

3.0000E 00 -6.0756E-02 -1.7320E-01 1.8354E-01 1.2334E 00

3.A000E 00 -1.2085E-01 -1.2880E-01 1.7662E-01 8.1727E-01

4.0000E 00 -1.6440E-01 -3.2675E-02 1.6762E-01 1.9619E-01

4.4000E 00 -1.5857E-01 3.4821E-02 1.6235E-01 -2.1616E-01

5.0000E 00 -1.0451E-01 1.14R9E-01 1.5532E-01 -8.3267E-01

6.0000E 00 4.0877E-02 1.3953E-01 1.4540E-01 1.2858E 00

7.0000E 00 1.3230E-01 3.6152E-02 1.3715E-01 2.6674E-01

a.oooot 00 9.'D291fc-02 -8.8645E-02 i.3015E-Cl -7.4928E-01

9.0000E 00 -2.3700E-02 -1.2181E-01 1.2410E-01 1.3786E 00

l.OOOOE 01 -1.1090E-01 -4.2609E-02 1.1880E-01 3.6683E-01

1.3000E 01 9.4127E-02 4.9062E-02 1.0615E-01 4.8049E-01

l.50nOE 01 3.B006E-03 -9.9^47E-02 9.9619E-02 -1.5326E 00

1.8000E 01 -1.4955E-02 g.0471E-02 9.1699E-02 -1.4070E 00

2.0000E 01 8.4059E-02 -2.3629E-02 8.7317E-02 -2.7403E-01

2.3000E 01 -8.0973E-02 1.1629E-02 8.1804E-02 -1.4264E-01

2.5000E 01 4.;'q36E-02 6.5e83E-02 7.8638E-02 9.9323fc-01

2.8000E 01 -3.1960E-02 -6.7270E-02 7.4477E-C2 I.1273E OC

3.0000E 01 -4.6171E-02 5.5617E-02 7.2284E-02 -8.7793E-01

3.3000E 01 5.0817t-02 -4.6429E-02 6.8833E-02 -7.4031fc-01

3.5000E 01 -6. 16'53E-02 -2.5935E-02 6.6886E-02 3.9ai8E-01

4.0000E 01 6.5099t-03 -6.2347E-02 6.2686E-02 -1.4668E 00

4.5000E 01 5.ai38E-n2 -1.1165E-02 5.9201E-O2 -1.8974E-01

5.0000E 01 2.5969E-02 4.9B23E-02 5.6185E-02 1.0903E 00

51-
CASE n

= 180 4/ = 210

X RE(HZ ) IM{HZ)

lO.OOOOt--03 a.^319E-01 -1.6&99E-02

2.0000E--02 8.4983E-01 -3.0561E-02

4.60OOE--02 8.4337E-01 -5.5185E-02

6.0000E--02 8.3693E-01 -7.7879E-02

l.OOOOE--01 8.2 36 3E-01 -1.1992E-01

2.0000E--01 7.8679E-01 -2.1362E-01

3.0000E--01 7.4433E-01 -2.9666E-01

4.0000E--01

-01

6.9638E-01

6.4335E-01

-3.7137E-01

5.0000E- -4.3854E-01

6.0000E--01 5.8571E-01 -4.9846E-01

7.0000E--01 5.2398E-01 -5.5119E-01

s.oooot--01 4.5873E-01 -5.9670E-01

9.0000E--01 3.9055E-01 -6.3493E-01

l.OOOOE 00 3.2006E-01

2.7796E-02

-6.6582E-01

1.4000E 00 -7.1573E-01

2.0000E 00 -3.7171E-0] -5.8268E-01

2.4G00E 00 -^.5925E-01 -3.8350E-01

3.0000E oc -6.6228E-01 -2.427SE-04

3.4000E 00 -6.0216E-01 2.5407E-01

4.0000E oc -3.4824E-01

-1.1013E-01

5.3994E-01

4.A000E 00 6.2658E-01

5.0000E oc 2.')834E-01 5.7236E-01

6.0000E 00 6.0978E-01 9.2494E-02

7.0000E 00 4.0314E-01 -4.5489E-01

8.0000E CO -1.6081E-01 -5.7857E-01

9.0C0PE .00 -5.6727E-01 -1.7750E-01

l.OOOOE 61 -4.5315E-01 3.7658E-01

1.3000b 01 4.y435E-01 -2.9828E-01

1.5000E 01 -4.7052E-01 -3.2448E-01

1.8000E 01 4.1256E-01 3.8570E-01

2.0000E 01 1.7986E-01 -5.3156E-01

.2,3000E 01. -2.5347E-01

5.?S358E-01

4.9563E-01

2.5000e 01 ' 2.5699E-0?.

2.8000E 01 -5.403SE-01 -1.0503E-01

3.0000E 01 1.2792E-01 5.339BE-01

3.3000E 01 -4.9368E-02 -5.4440E-01

3.5000E 01 -4.7372E-01 2.6983E-01

4.0000E 01 -3.8932E-01

2.5174E-01

-3.7718E-01

4.5000E 01 -4.7717E-01

5.0000E 01 5.2654E-01 1.0722E-01

HZ

8.533

8.503

8.451

8.405

8.323

8.152

8.012

7.892

7.786

7.691

7.605

7.526

7.454

7.387

7.162

6.911

6.781

6.622

6.535

6.425

6.361

6.279

6.167

6.078

6.005

5.943

5.892

5.773

5.715

5.647

5.611

5.566

5.541

5.509

5.490

5.466

5.451

5.420

5.395

5.373

(AMP)

5E-01

8E-0I

7E-01

4E-01

lE-01

8E-01

7E-01

2E-01

OE-01

OE-01

OE-01'

5E-01

3E-01

5E-01

7E-01

4E-01

lE-01

8E-01

6E-01

OE-01

9E-01

6E-01

5E-01

2E-01

OE-01

9E-01

OE-01

7E-01

6E-01

8E-01

6E-01

8E-01

8E-01

5E-G1

9E-01

3E-01

8E-01

6E-01

OE-01

5E-01

PHASE(HZ)

1..9804E--02

3..5945E--02

6..5340E--02

9..2786E--02

1..4458E--01

2 .6512E--01

3..7927E--01

4..8992E--01

5..9831E--01

7 .0510E--01

8..1070E--01

9..1539E--01

1 .3193E 00

1 .1227E 00

1..5320E 00

1..0030E 00

6..0109E--01

3 .6657E--04

3,.9927E--01

9..9798E--01

1 .3968E 00

1.. 1468E 00

1..5054E--01

8..4564E--01

1,.2997E 00

3 .0326E--01

6..9338E--01

5..4290E--01

6.,0372E--01

7 .5177E--01

1..2445E 00

1..0981E 00

4..6391E--02

1..9180E--01

•1..3357E 00

1,.4804E 00

5..1777E--01

7..6956E--01

I..C853E 00

2..0089E--01

.52-
CASE n

= 180° ij; = 210°

X RE(EO) IM(EO) EO{AMP) PHASE(EO)

lO.OOOOE-03 -3.4753E-01 -1.4455E 00 1.4867E 00 I.3349E 00

2.0000E-02 -3.2819E-01 -I.3048E 00 1.3454E 00 1.3244E 00

4.0000E-02 -3.2082E-01 -1.1740E 00 1.2L70E nn 1.3040E 00

6.0000E-G2 -3.2455E-01 -1.I006E 00 1.1475E 00 1.284CE 00

l.OOOOE-OI -3.4145E-01 -1.0090E 00 1.0652E 00 1,2445E 00

2.0000E-01 -3.9639E-01 -8.7739E-01 9.6277E-01 1.1463E 00

3.000nE-01 -4.5258E-0I -7.8671E-01 9.0760E-01 1.0488E 00

4.0000E-01 -5.0561E-01 -7.0867E-01 8.7055E-01 9.5109E-01

5.0000E-01 -5.5423E-01 -6.3523E-01 8.43G2E-C1 8.5339E-0I

6.0000E-01 -5.9779E-01 -5.6322E-01 8.2I32E-01 7.5562E-01

7.0000E-01 -6.3587E-01 -4.9I26E-01 8-0353E-C1 6.5780E-01

8.0000E-01 -6.6814E-0I -4.1879E-01 7.8854E-01 5.5990E-01

9.0000E-OL -6.9435E-01 -3.4569E-01 7.7564E-01 4.6194E-01

L.OOOOE 00 -7.1431E-0i -2.7206E-01 7.6437E-01 3.6391E-01

1.4G00E 00 -7.7976E-01 2.0982E-02 7.3006E-01 -2.8744E-02

2.0000E 00 -5.6734E-01 4.0427E-01 6.9664E-01 -6.1911E-01

2.4000E 00 -3.6010E-01 5.7774E-01 6.8078E-01 -1.0134E 00

3.0000E 00 2.3174E-02 6.62I4E-01 6.6254E-01 1.5358E 00

3.4000E 00 2.7240E-01 5.9336E-01 6.5290E-01 I.1404F 00

4.0000E OC 5.4757E-0I 3.3324E-01 6.4100E-01 5.4669E-01

4.4000E 00 6.2719E-01 9.5126E-02 6.3436E-01 l-5n52E-01

5.0000E 00 5.6511E-01 -2.6895E-01 6.2585E-01 -4.4420E-01

6.0000E 00 8.2316E-02 -6.089AE-01 /S.1447E-01 -1.^364E 00

7.0000E 00 -4.5849E-01 -3.9559E-01 6.0556E-01 7.1188E-01

8.0000E 00 -5.7467E-01 1.6664E-01 5.9834E-01 -2.8223E-01

9.0000E OC -1.7153E-01 5.6698E-01 5.9236E-0I -1.2770E 00

l.OOOOE ni 3.7905E-01 4.4860E-01 5.R729E-01 8.6923E-01

1.3000E 01 -3.0025E-01 -4.9135E-01 5.7583E-01 I. 0223b 00

1.5000E 01 -3.2157E-01 4.7089E-01 5.7022E-C1 -9.7164E-01

1.8000E 01 3.8351E-01 -4.1309E-01 5.6367E-01 -8.2251E-01

2.0000E 01 -5-3116E-01 -1.7797E-01 5.6018E-01 3.2330E-01

2.3000E 01 4.9550E-01 2.5190E-01 5.55P5E-01 4.7033E-01

2.5000E 01 2.4490E-02 -5.5288E-01 5.5342E-01 -l.'3265E 00

2.8000E 01 -1.0394E-'01 5.4039E-01 5.5030E-01 -1.3808E 00

3.0000E 01 5.3319E-01 -1.2863E-01 5.4849E-01 -2.3673E-01

3.3000E 01 -5.4380E-01 5.0076E-02 5.4610E-01 -9.182/E-02

3-5000E 01 2.7019E-01 4.7295E-01 5.4469E-C1 1.0518E 00

4.0000E 01 -3.7649E-01 3.8941E-01 5.4165E-01 -8.0228E-01

4-5000E 01 -4.7707E-01 -2.5117E-01 5.3915E-01 4.8460E-01

5.0000E 01 1.0678E-01 -5.2632E-01 5.3705E-01 -1.3706E 00

-53.
CASE n

= 180° ^ = 210°

X RE(EP) IM(EP) EP(AMP) PHASE(EP)

lO.OOOOE--03 1.7449E-01 6.9159E-01 7.1327E-01 1.3236E 00

2.0000E--02 1.6891E-01 6.2081E-01 6.4338E-01 1.3051E 00

4.0000E--02 1.7054E-01 5.5277E-01 5.7848E-01 1.2715E 00

6.0000E--02 1.7601E-01 5.1295E-01 5.4231E-01 1.2402E 00

l.OOOOE--01 1.8907E-01 4.6079E-01 4.9807E-01 1.18146 00

2.0000E--01 2.2031E-01 3.8011E-01 4.39346-01 1.0455E 00

3.0000E--01 2.4609E-01 3.2181E-01 4.0512E-01 9.1795E-01

^.OOOOE--01 2.6657E-01 2.7183E-01 3.8072E-01 7.9517E-01

5.0000E--0 1 2.a223E-01 2.2620E-01 3.6169E-01 6.7564E-01

6.0000E--01 2.9347E-01 1.8338E-01 3.4605E-01 5.5851E-01

7.0000E--01 3.0062E-01 1.4272E-01 3.3278E-01 4.4324E-01

8.0000E--01 3.0397E-01 1.0394E-01 3.2125E-01 3.2947E-01 J 9.0000E--0 1 3.0377E-01 6.6950E-02 3.1106E-01 2.1693E-01 1 l.OOOOE 00 3.0026E-01 3.1775E-02 3.0194E-01 1.0543E-01

1.4000E 00 2.5788E-01 -8.9114E-02 2.7284E-01 -3.3272E-01 J

-9.7453E-01 1

-1.3959E 00

2.0000E 00 1.3610E-01 -2.0C54E-01 2.4236E-01

2. 4000

E

00 3.9509E-02 -2.2362E-01 2.2708E-01

3.0000E CO -9.0987E-02 -1.8795E-01 2.0881E-01 1.1199E 00

3.4000E 00 -1.5131E-01 -1.2-897E-01 1.9882E-01 7.0589E-01

4.0000E 00 -1.8545E-01 -1.6401E-02 1.8617E-01 8.8213E-02

4.4000E 00 -1.6976E-01 5.6595E-02 1.7895E-01 -3.2179E-01

5.0000E oc -1.0069E-01 1.3635E-01 1.6950E-01 -9.3473E-01

6.0000fc 00 5.8262E-02 1.4531E-01 1.5656E-01 1.1895E 00

7.0000E 00 1.4388E-01 2.5565E-02 1.4613E-01 1.7585E-01

8.0000E oc 9.2277E-02 -1.0194E-01 1.3750E-01 -8.3510E-01

9.0000t 00 -3.5144E-02 -1.2538E-01 I.3021E-01 1.2975E 00

l.OOOOE 01 -1.1877E-01 -3.5441E-02 1.2394t-01 2.9000E-01

1.3000E 01 1.0012E-01 4.4118E-02 1.0941E-01 4.1507E-01

1.5000E 01 -2.2339E-03 -1.0209E-0I 1.0211E-01 1.5489E 00

1.8000E 01 -1.0355E-02 9.2868E-02 9.3444E-02 -1.4598E 00

2.000GE 01 8.4169E-02 -2.8137E-02 8.8747E-02 -3.2261E-01

2.3000E 01 -8.1422E-02 1.5349E-02 8.2856E-02 -1.8632E-01

2.5000E 01 4.6099E-02 6.4793E-02 7.9519E-02 9.5240E-01

2.8000E 01 -3.4745E-02 -6.6678E-02 7.51886-02 1.09046 00

3.0000E 01 -4.4507E-02 5.7437E-02 7.2663E-02 -9.1156E-01

3.3000E 01 4.9636E-02 -4.8374E-02 6.9309E-02 -7.7253E-01

3.5000E 01 -6.2817E-02 -2.4191E-02 6.7314E-02 3.6760E-01

4.0000E 01 4.8432E-03 -6.2805E-02 6. 29926-02 -1.49386 00

4.5000E 01 5,8063E-02 -1.2560E-02 5.9406E-02 -2.1304E-01

5.0000E 01 2.7151E-02 4.9399E-02 5. 63696-02 1.0682E 00

-54.
CASE ni

tjt ^ 150° i|j = 150°

X RE (HZ) IM{HZ) HZ(AMP) PHASECHZ)

lO.OOOOE--03 1.2015E 00 -3.5912E-03 1.2011E 00 -2.9899E-03

2-OOOOE--02 1.2025E 00 -8.2545E-03 1.2026E 00 -6.8640E-03

4.0000E--02 1.2056E 00 -1.8983E-02 1.2058E 00 -1.5745E-02

6.0000E--02 1.2088E 00 -3.0914E-02 1.2092E 00 -2.5569E-02

l.OOOOE--01 1.2150E 00 -5.7185E-02 1.2163E 00 -4.7032E-02

2.0000E--01 1.2277E 00 -1.3197E-01 1.2348E 00 -1.0708E-01

3.0000E--01 1.2346E 00 -2.1530E-01 1.2532E 00 -1.7266E-01

4.0000E--01 1.2343E 00 -3.0437E-01 1.2713E 00 -2.4176E-01

5.0000E--01 1.2262E 00 -3.9739E-01 1.2890E 00 -3.1341E-01

6.0000E--01 1.2096E 00 -4.9297E-01 1.3062E 00 -3.8699E-01

7.0000E--01 1.1843E 00 -5.8987E-01 1.3230E 00 -4.6212E-01

8.0000E--01 1.1499E 00 -6.8694E-01 1.3394E 00 -5.3852E-01

9.0000E--01 1.1063E 00 -7.8309E-01 1.3554E 00 -6.1597E-01

l.OOOOE 00 1.0536E 00 -8.7729E-01 1.3711E 00 -6.9432E-01

l.AOOOE 00 7. 55186--01 -1.2147E 00 1.4303E 00 -1.0146E 00

2.0000E 00 9.3784E--02 -1.5083E 00 1.5112E 00 -1.5087E 00

2.4000E 00 -4.2118E--01 -1.5030E 00 1.5609E 00 1.2976E 00

3.0000E 00 -1.1^90E 00 -1.1566E 00 1.6303E 00 7.8869E-01

3.4000E 00 -1.5095E 00 -7.2260E-01 1.6736E 00 4.4646E-01

4.0000E 00 -1.7303E 00 1.2169E-01 1.7346E 00 -7.0209E-02

4.4000E 00 -1.6214E CO 7.17iaE-01 1.7730E 00 -4.1644E-01

5.0000E 00 -1.0808E 00 1.4734E 00 1.8273E 00 -9.3791E-01

6.0000E 00 4.5526E--01 1.8550E 00 1.9101E 00 1.3301E 00

7.0000E 00 1.7843E 00 8.67A1E-01 1.98A0E 00 4.5249E-01

8.0000E 00 1.8647E 00 -8.5094E-01 2.0496E 00 -4.2812E-01

9.0000E 00 5.4153E--01 -2.0368E 00 2.1076E 00 -1.3109E 00

l.OOOOE 01 -1.2619E 00 -1.7507E 00 2.1581E 00 9.4623E-0I

1.3000E 01 3.2083E--01 2.24A9E 00 2.2677E 00 1.4288E 00

1.5000E 01 2.1716E 00 -7.82C7E-01 2.3081E 00 -3.4567E-01

1.8000E 01 -2.3029E 00 -3.1432E-01 2.32A2E 00 1.3565E-0I

2.0000E 01 1.4761E--01 2.3036E 00 2.3084E 00 1.5068E 00

2.3000E 01 9.3808E--01 -2.0464E 00 2.2512E 00 -1.1410E 00

2.5000E 01 -2.1312E 00 -5.2725E-01 2.1955E 00 2.4253E-01

2.8000E 01 1.5174E 00 1.4443E 00 2.0949E 00 7.6071E-01

3.0000fc 01 1.1310E 00 -1.6772E 00 2.0229E 00 -9.7751E-01

3.3000b 01 -1.7483E 00 7.9223E-01 1.9194E 00 -4.2546E-01

3.5000t 01 1.0029E 00 1.5671E 00 I.8605E 00 1.0015E 00

4.0000E 01 -1.7667E 00 2.0006E-01 1.7780E 00 -1.1276E-01

4.5000E 01 6.2I13E--01 -1.6975E 00 1.8076t 00 -1.2200E 00

5.0000E 01 1.3683E 00 1.3479E 00 1.9207E 00 7.7786E-01

-55.
(CASE ni

(/) = 150° i|j = 150°

X RE{EO) IM(EO) EO(AMP) PHASE(EO)

G.OOOOE--03 1.3349E--01 -4.3111E-01 4.5131E--01 -1.2705E 00

2.0000E--02 1.4752E--01 -4.9568E-01 5.1717E--01 -1.2815E 00

4.0000E--02 1.5733E--01 -5.7051E-01 5.918IE--01 -1.3017E 00

6.0000E--02 1.5830E--01 -6.1993E-01 6.3982E--01 -1.3208E GO

I.OOOOE--01 1.4936E--01 -6.8915E-01 7.0515E--01 -1.3574E 00

2.0G00E--01 1.0074E--01 -7.9679E-01 8.0313E--01 -1.4450E 00

3.0000E--01 3.4792E--02 -8.6545E-01 8.6615E--01 -1.5306E 00

4.0G00E--01 -4.0795E--02 -9.1304E-01 9.1395E--01 1.5261E 00

5.0000E--01 -1.2279E--01 -9.4520E-01 9.5314E--01 1.4416E 00

6.0000E--01 -2.0921E--01 -9.6434E-01 9.8677E--01 1.3572E 00

7.0000E--01 -2.9857E--01 -9.7167E-01 I.G165E GO 1.2727E 00

8.0000E--01 -3.8959E--01 -9.6789E-01 1.0434E 00 1.1881E 00

9.0000E--01 -4.B113E--01 -9.5345E-01 1.G680E GO 1.1035E 00

l.OOOOE 00 -5.7213E--01 -9.2873E-01 1.0908E GO 1.0187E GO

l.AOOOE OG -9.1095E--01 -7.3385E-G1 1.1698E GO 6.7814E--01

2.0000E 00 -1.2490E 00 -2.0600E-01 1.2659E 00 1.6346E--01

2.4000E 00 -1.2992E 00 2.3890E-01 1.3210E 00 -1.8185E--01

3.0000E OG -1.0647E 00 9.0127E-01 1.39A9E 00 -7.0246E--01

3.4000E 00 -7.1516E--01 1.2496E 00 1.4398E 00 -I.G510E 00

4.0000E GO 7.2226E--03 1.5018E 00 1.5G18E 00 I.5660E 00

4.A000E 00 5.3618E--01 1.4439E 00 1.5402E 00 1.2152E 00

5.0000E 00 1.2315E 00 1.0119E GO 1.594GE 00 6.8782E--01

6.0000E on 1.6433E 00 -3.2278E-G1 1.6747E 00 -I.9395E--01

7.0000E 00 8.2537E--01 -1.5384E GO 1.7459E 00 -1.0784E 00

8.0000E 00 -6.9423E--01 -1.6699E 00 1.8G85E 00 1.1768E GO

9.0000E 00 -1.7860E 00 -5.3089E-G1 1.8632E GO 2.8893E--01

l.OOOOE 01 -1.5769E 00 1.G789E 00 1.9106E 00 -6.0002E--01

1.3000E 01 1.9953E 00 -2.5835E-01 2.0119E GO -1.2877E--01

1.5000E 01 -6.8068E--01 -1.9315E GO 2.G479E GO 1.2320E 00

1.8000E 01 -2.7561E--01 2.0407E GO 2.0593E 00 -1.4366E 00

2.0000E 01 2.0364E 00 -1.4325E-01 2.0414E GO -7.G231E--02

2.3000E 01 -1.8125E 00 -8.0357E-G1 1.9826E 00 4.1732E--01

2.5000E 01 -4.3285E--01 I.8772E 00 1.9264E 00 -1.3442E 00

2.8000E 01 1.2327E 00 -1.3468E GO 1.8258E 00 -8.2957E--01

3.0000E 01 -1.4739E 00 -9.5048E-01 1.7538E GO 5.7276E--01

3.3000E 01 7.1018E--01 1.4896E 00 1.6502E 00 1.1259E 00

3.5000E 01 1.3258E 00 -8.7986E-G1 1.5912E 00 -5.8591E--01

4.0000E 01 1.7511E--01 1.4989E 00 1.5091E 00 1.4545E GO

4.5000E 01 -1.4415E 00 -5.4458E-GI 1.5409E GO 3.6122E--01

5.0000E 01 1.1811E 00 -1.1607E 00 1.6560E GO -7;7671t--01

I

-56-
CASE m

(/> = 160 i|j = 160

X RE(HZ) IM(HZ) HZ(AMP) PHASE(HZ)

lO.OOOOE--03 1.1260E 00 -5.3727E--03 1.1260E 00 -4.7713E-03

z.oooot--02 1.1272E 00 -1.1723E--02 1.1273E 00 -1.0400E-02

4.0000E--02 1.1295E 00 -2.5592E--02 1.1298E 00 -2.2654E-02

6.0000E--02 1.1317E 00 -4.0420E--02 1.1324E 00 -3.5701E-02

I.OOOOE--01 1.1354E 00 -7.1923E--02 1.1377E 00 -6.3259E-02

2.0000E--01 1.1401E 00 -1.5728E--01 1.1509E 00 -1.3709E-01

3.0000E--01 1.1368E 00 -2.4825E--01 1.1636E 00 -2.1500E-01

4.0000E--01 1.I249E 00 -3.4237E--01 1.1758E 00 -2.9546E-01

5.0000E--01 1.1039E 00 -4.3796E--01 1.1876E 00 -3.7770E-01

6.0000F--01 1.0736E 00 -5.3366E--01 1.1990E 00 -4.6129E-01

7.0G00E--01 1.0340E 00 -6.2624E--01 1.2099E 00 -5.4595E-01

8.0000E--01 9.8520E--01 -7.2056E--01 1.2206fc 00 -6.3148E-0I

9.0000E--01 9.2725E--01 -8.0955E--01 1.2309E 00 -7.I773E-01

l.OOOOE 00 8-6049E--01 -8.9418E--01 1.2410E 00 -8.0460E-01

1.4000E 00 5.1451E--01 -1.1707E 00 1.27fi8E 00 -1.1567E 00

2.0000E 00 -1.6382E--01 -1.3199E 00 1.33C0E 00 1.4473E 00

2.4000E 00 -6.3580E--01 -1.2039E 00 1.3615E 00 1.0849fc 00

3.0000b 00 -1.2075E 00 -7.1919E--01 1.4055E 00 5.3717e-0l

3.4000E 00 -1.4125E 00 -2.4237E--01 1.4331E 00 1.6994E-01

4.0000E 00 -1.3656E 00 5.5066E--01 1.4725E 00 -3.8329E-01

4.4000E 00 -1.0922E 00 1.0245E 00 1.4975E 00 -7.5340E-01

5.0000E 00 -3.9521E--01 1.4817E 00 1.5335E 00 -1.3101E 00

6.0000E .00 9.8804E--01 1.2456E 00 1.5899E 00 9.0021E-01

7.0G00E 00 1.6A16E 00 -5.6293E--02 1.6425E 00 -3.4279E-02

8.0000E 00 9.5471E--01 -1.3969E 00 1.6920E 00 -9.7126E-01

q.OOOOE 00 -5.7886E--01 -1.6394E 00 1.7386E 00 1.2314E 00

l.OOOOE 01 -1.7078E 00 -5.1112E--ul 1.7827E 00 2.9079E-01

1-3000E 01 1.5658F 00 1.0792E 00 1.9017E 00 6.0345E-01

1.5000E 01 5.'i223E--01 -1.8923E 00 1.9713E 00 -I.2869E 00

1.8000E 01 -1.1398t 00 1.7188E 00 2.0624E 00 -9.8522E-01

2.0000E 01 2.0436E 00 5.4591E--01 2.1152E 00 2.6104E-01

2.3000E 01 -1.8524E 00 -1.15^5E 00 2. 1827E 00 5.5732E-01

2.5000E 01 -5.0664E--01 2.1618E 00 2.22C4E 00 -1.3406E 00

2.8nnnF ni 1.1338E 00 -I.9623t 00 2.2663E 00 -1.0469E 00

3.0000E 01 -2.2464E 00 -4.4554E--01 2.29G1E 00 1.9580E-01

3.3000E 01 2.0447E 00 1.0876E 00 2.3160E 00 4.8885E-01

3.5000E 01 3.7237E--01 -2.2970E 00 2.3270E 00 -1.4101E 00

A.OOOOE 01 2.3149E 00 2.9604E--01 2.3337E 00 1.272GE-01

4.5000E 01 -2.2453E--01 2.3026E 00 2.3135E 00 -1.4736E 00

5.0000E 01 -2.2641E 00 -1.6466E--01 2.2701E 00 7.2'i99t-02

-57-
CASE UI

<f) = 160 4i = 160

X RE(EO)

.O.OOOOE--03 1.1333E--01

2.0000E--02 1.1688E--01

4.oonoE--02 1.1343E--01

6.0000E--02 1.0493E--01

i.ooooe--01 8.1724E--02

2.0000E--01 8.3752E--03

3.0000E--01 -7.5173E--02

4.0000E--01 -1.6406E--01

5.0000E--01 -2.5594E--01

6.0000E--01 -3.4917E--01

7.0000E--01 -4.4239E--01

8.0000E--01 -5.3440E--01

9.0000E--01 -6.2409E--01

l.OOOOE 00 -7.1041E--01

1.4000E 00 -1.0031E 00

2.0000E 00 -1.2013E 00

2.4000E 00 -1.1301E 00

3.0000E 00 -7.1973E--01

3.4000E 00 -2.8957E--01

4.0000E 00 4.4976E--01

4.4000E 00 9.0422E--01

5.0000E 00 1.3618E 00

6.0000E 00 1.1960E 00

7.0000E 00 -1.7511E--03

8.0000E oc -1.2833E 00

9.0000E 00 -1.5558E 00

l.OOOOE 01 -5.2221E--01

1.3000E 01 1.0494E 00

I.5000E 01 -1.7806F 00

1.8000E 01 1.6131E 00

2.0000E 01 5.4148E--01

2.3000E 01 -1.1126E 00

2.5000E 01 2.0479E 00

2.8000E 01 -1.8564E 00

.3.0000E 01 -4.3342E--01

3.3000E 01 1.0385E 00

3.5000E 01 -2.1801E 00

4.0000E 01 2.7946E--01

4.5000E 01 2.1835E 00

5.0000E 01 -1.4522E--01

IM(EO)

-6.0466E-01

6.5997E-01

7.2095E-01

-7.5962E-01

-8.1176E-01

8.8702E-01

-9.2865E-01

•9.5102E-01

-9.5859E-01

9.5333E-01

-9.3633E-01

-9.082HE-01

•8.6977E-01

•8.2133E-01

-5.3957E-01

6.7497E-02

5.1057E-01

1.0702E 00

1.2B78E 00

1.2858E 00

1.0539E 00

4.2383E-01

8.7923E-01

1.5380E 00

•9.3517E-01

5.0130E-01

1.5953E 00

-1.4580E 00

5.5397E-01

1.1032E 00

1.9310E 00

1.7468E 00

4.97B1E-01

•1.0880E 00

2.1309E 00

-1.9383E 00

•3.5774E-01

•2.1967E 00

2.0639E-01

2.1443E 00

EO(AMP)

6..1519E--01

6..7024E--01

7..2981E--01

7,.6684E--01

8..1587E--01

8, 8706E--01

9..3169E--01

9. 6507E--01

9..9217E--01

.0153E 00

.0356E 00

,0538E 00

.07C5E 00

0859E 00

.1390E 00

,2032E 00

,240 IE 00

2897E 00

.3199E 00

,3622E 00

3887E 00

,4263E 00

.4844E 00

,5380E 00

.5879E 00

.6346E 00

,6786E 00

.7964E 00

,8648E 00

9542E 00

2, 0054E 00

2. 0710E 00

2. 1075E 00

2. 1517E 00

Z. 174bE 00

2. 1990E 00

2. 2093E 00

2. 2144E 00

2. 1932E 00

2, 1492E 00

PHASE(EO)

1 .3855e 00

1..3955E 00

1..4147E 00

1 .4335E 00

1 .4705E 00

1..5614E 00

1 .4900E 00

1 .400GE 00

1 .3099E 00

1 .2197E 00

1 .1294E 00

1 .0390E 00

9 .4840E--01

8 .5768E--01

4 .9350E--01

5 .6125E--02

4 .2434E--01

9 .7875E--01

1 .3496E 00

1 .2343E 00

8 .6170E--01

3..0172E--01

6 .3392E--01

I .5697E 00

6 .2975E--01

3..1170t--01

1 .2544E 00

9 .4695E--01

3 .0162E--01

5..9986E--01

1..2974E 00

1..0037E 00

2 .3846E--01

5 .3010E--01

1,.3701E 00

1..0789E 00

1 .6264E--01

1.4443E 00

9..4244E--02

1 .5032E 00

I

.58-
CASE m

(/> = 170° i|j = 170°

X RE(HZ) IM(HZ) HZ(AMP) PHAS6(HZ)

lO.OOOOE--03 1.0595E 00 -7.5242E-03 1.0595E 00 -7.10176-03

2.0000E--02 1.0601E 00 -1.5679E-02 1.0602E CO -1.47896-02

4.0000E--02 1.0612E 00 -3.2681E-02 1.06176 00 -3. 07876-02

6.0000E--C2 1.C620E 00 -5.0226E-02 1.0631E 00 -4.72616-02

l.OOCOE--01 1.0625E 00 -8.6312E-02 1.0660E 00 -8.10566-02

2.0000E--01 1.0577E 00 -1.7970E-01 1.07286 00 -1.68296-01

3.0000E--01 1.0436E 00 -2.7509E-01 1.07926 00 -2.57746-01

4.n000E--01 1.0200E 00 -3.7063E-01 1.08536 00 -3.48526-01

5.0000E--01 9.8700E--01 -A.6493E-01 1.09106 00 -4.40226-01

6.000nE--01 9.4461E--01 -5.5679E-01 1.09656 00 -5.32626-01

7.0000E--01 8.9312E--01 -6.4514E-01 1.10186 00 -6.25566-01

8.0000E--01 8.3287E--01 -7.2893E-01 1.10686 00 -7.1895E-01

9.0000E--01 7.6433E--01 -8.0724E-01 1.1117E 00 -8.12706-01

l.OOOOE 00 6.8804E--01 -8.79176-01 1.11646 00 -9.06766-01

1.4000E 00 3+1931E--01 -1.0881E 00 1.13406 00 -1.28526 00

2.0000E 00 -3.2782E--01 -l.llOOE 00 1.15746 00 1.28366 00

2.4000E oc -7.2845E--01 -9.1766E-01 1.17166 00 B. 89846-01

3.0000E 00 -1.1302E 00 -3.7710E-01 1.19146 00 3.22056-01

3.A000E 00 -1.2012E 00 7.7238E-02 1.20386 00 -6.42076-02

A^OOOOE 00 -9+7611E--01 7+3410E-01 1.22126 00 -6.4482E-01

4.4000E 00 -6.3179E--01 1.C582E 00 1.23256 00 -1.03266 00

5.0000E 00 5.5200E--02 1.2473E 00 1.24856 00 1.52666 00

6.0000E oc 1.0831E 00 6.7007E-01 1.27366 00 5.54046-01

7.0000E 00 1. 18A3E 00 -5.2919E-01 1.29716 00 -4.20236-01

8.0000E 00 2.2961E--01 -1.2992E 00 1.31946 00 -1.39596 00

9.0000E 00 -9.6335E--01 -9.3221E-01 1.34056 00 7.68986-01

l.OOOOE 01 -1.3313E 00 2.8193E-01 1.36086 00 -2.0869fc-01

1.3000F 01 1.4173E 00 -6.13086-03 1.41736 00 -4.32556-03

1.5000fc 01 -5.5798E--01 -1.3407E 00 1.4522E 00 1.1764E 00

1.8000E 01 2.9389E--01 1.4721E 00 1.5011E 00 1.3737E 00

2.0000E 01 1.2723E 00 -8.5314E-01 1.5319E 00 -5.90686-01

2.3000E 01 -1.4528E 00 6.1014E-01 1.5758E 00 -3.9759E-01

2.5000E 01 1.1A31E 00 1.12476 00 1.6037E 00 7. 77276-01

2.800OE 01 -9.3264E--01 -1.3535E 00 1.64376 00 9.67466-01

3.0000E 01 -9.0070E--01 1.4055E 00 1.6694E 00 -1.00096 00

3.3000E 01 1.1731E 00 -1.2392E 00 1.7064E 00 -8. 12816-01

3.5000E 01 -1.6197E 00 -6.0819E-01 1.73016 00 3.59216-01

A.OOOOE 01 2.5986E--01 -1.7676E 00 1.78666 00 -1.42486 00

A.5000E 01 1.83A9E 00 -1.2735E-01 1.83936 00 -6.92916-02

5.0000E 01 5.3312E--01 1.8118E 00 1.88866 00 1.28466 00

•59'
<l> = 170°

CASE ni

l^ = 170°

X RE(EO) IMCEO) EO(AMP) PHASt(EO)

lO.OOOOE--03 6.5858E-02 -7.9691E-01 7.9962E--01 -1.4883E 00

2.0000E--02 6.0531E-02 -8.3053E-01 8.3273E--01 -1.4980E 00

4.G000E--02 4.6385E-02 -8.6587E-01 8.6711E--01 -1.5173E 00

6.0000b--02 3.0520E-02 -8.8730E-01 8.8783E--01 -1.5364E 00

l.OOOOE--01 -3.4428E-03 -9.1460E-01 9.1461E--01 1.5670E 00

2.0000t--01 -9.4040t-02 -9.4772E-01 9.5237E--01 1.4719e 00

3.0000E--01 -1.8808E-01 -9.5717E-01 9.7547E--01 1.3768E 00

4.0000E--01 -2.8306E-01 -9.5128E-01 9.9251E--01 1.2816b 00

5.0000E--01 -3.7743E-01 -9.3272E-01 1.0062E 00 1.1863E 00

6.0000E--01 -4.6992E-01 -9.0278E-01 1.0178E 00 1.0909E 00

T.OOOOt--01 -5.59386-01 -8.6233E-01 1.0279E 00 9.9535E-01

8.0000E--01 -6.4477E-01 -8.1205E-01 1.0369E 00 3.9972E-01

9.0000E--01 -7.2513E-01 -7.5262E-01 1.0451E 00 8.0400E-01

l.OOOOE 00 -7.9955E-01 -6.8471E-01 1.0527E 00 7.0818E-01

1.4000E 00 -1.0223E 00 -3.4343E-01 1.0784E 00 3.2410E-01

2.0000E oc -1.0735E 00 2.7868E-01 1.1091E 00 -2.5398E-01

2.A0OOE 00 -9.0333E-01 6.7312E-01 1.1265E 00 -6.4039E-01

3.0000E 00 -3.9383E-01 1.0802E 00 1.1498E 00 -1.2212E 00

3.4000E 00 4.4518E-02 1.1631E 00 I.1639E 00 1.5325E 00

4.0000E 00 6.8b^yE-01 9.6267E-01 1.1835E 00 9.4995E-01

4.4000E 00 1.Q124E 00 6.3630E-01 1.1958E 00 5.6110E-0I

5.0000E 00 1.2129E 00 -2.7619E-02 1.2132E 00 -2.2768E-02

6.0000E 00 6.7293E-01 -1.0416E 00 1.2401E 00 -9.9720E-01

7.0000E 00 -4.9511E-01 -1.1640E 00 I.2649E 00 1.1686E 00

8.0000E 00 -1.2646E 00 -2.4551E-01 1.2882E 00 1.9176E-01

9.0000E 00 -9.2587E-01 9.2701E-01 1.3102E 00 -7.8601E-01

l.OOOOE 01 2.5630E-01 1.3062E 00 1.3311E 00 1.3770E OC

1.3000E 01 1.1916E-02 -1.3890E 00 1.3891E 00 -1.5622E 00

1.5000E 01 -1.3215E 00 5.3167E-01 I.4245E 00 -3.8250E-01

1.8000E 01 1.4485t 00 -2.7314E-01 1.4741E 00 -1.8638E-01

2.0000E 01 -8.2568E-01 -1.2584E 00 I.5051E 00 9.9013E-01

2.3000E 01 5.8677E-01 1.4339E 00 1.5493E 00 1.1824E 00

2.5000E 01 1.1160E 00 -1.1147E 00 1.5773E 00 -7.8484E-01

2.8000E 01 , -1.3393E 00 9.0702E-01 1.6175E 00 -5.9528E-01

3.0000E 01 1.3767E 00 8.9720E-01 1.6432E 00 5.7758E-01

3.3000& 01 -1.2119E 00 -1.1638E 00 1.6803E 00 7.6516E-01

3.5000E 01 -6.0996E-01 1.5911E 00 1.7040E 00 -1.2047E 00

4.0000E 01 -1.7401E 00 -2.6684E-01 1.7604E 00 1.5216E-01

4.5000E 01 -1.1536E-01 -1.8094E 00 1.8131E 00 1.5071E 00

5.0000E 01 1.7891E 00 -5.1651E-01 I.8622E 00 -2.8105E-01

60.
CASE in

(/. = 175° i|j = 175°

X RE(HZ) IMCHZ) HZ(AMP) PHASE(HZ)

lO.OOOOE--03 1.0289E 00 -8.725nE-03 1.0290E 00 -8.4796E-03

2.0000F--02 1.0292E 00 -1.7802E-02 1.0293E 00 -1.7295E-02

4.0000E--02 1.0295E 00 -3.6323E-02 1.0301E 00 -3.5268E-02

6.0000E--02 1.0294E 00 -5.5124E-02 1.0309E 00 -5.3499E-02

l.OOOOE--01 1.0281E 00 -9.3207E-02 1.0323E 00 -9.0410E-02

2.0000b--01 1.0183E 00 -1.8964E-01 1.0358E 00 -1.8412E-01

3.0000E--01 9.9882E--01 -2.8611E-01 1.0390E 00 -2.7898£-01

4.0000E--01 9.6975E--01 -3.8116E-01 1.0420E 00 -3.7450E-01

5.0000E--01 9.3125E--01 -4.7363E-01 1.0448E 00 -4.7050E-01

6.0000E--01 8.8362E--01 -5.6246E-01 1.0474E 00 -5.6685E-01

7.0000E--01 8.2725E--01 -6.4665E-01 1.0500E 00 -6.6347E-01

8.0000E--01 7.6262E--01 -7.2529E-01 1.0524E 00 -7.6032E-01

9.0000E--01 6.9031E--01 -7.9753E-01 1.0548E 00 -8.5734E-01

l.OOOOE 00 6.1098E--01 -8.6260E-01 1.0571E 00 -9.5452E-01

1.4000E 00 2.3913E--01 -1.03H3E 00 1.0654E 00 -1.3444E 00

2.0000E 00 -3.8009E--01 -1.0072E 00 1.0765E 00 1.2099E 00

2.4000E 00 -7.4101E--01 -7.9009E-01 1.0832E 00 8.1744E-01

3.0000t 00 -1.0643E 00 -2.4653E-01 1.0924E 00 2.2763E-01

3.4000E 00 -1.0831E 00 1.8158E-01 1.0982E 00 -1.6611E-01

4-noooE -8.CJ390E--01 7.6000E-01 1.1063E 00 -7.5734E-01

A.4000E oc -^.5213E--01 1.0153E 00 1.1114E 00 -1.1518E 00

5.0000E 00 1.9279E--01 1.1020E 00 1.1187E 00 1.3976E 00

6.0000E 00 1.0366E 00 A.5(j26E-01 1.1302E 00 4.0977E-01

7-OOOOE 00 y.5A92E--01 -6.2419E-01 1.14n8e 00 -5.7894E-01

8.0000E oc 2.8118E--03 -1.1509E 00 1.1509E 00 -1.5684E 00

Q.OOOOfc 00 -9.6852E--01 -6.3907E-01 1.1604E 00 5.8326E-01

l.OOOOE 01 -1.0738E 00 A.6313E-01 1.1694E 00 -4.0718E-01

l.^nnoE 01 1.1606E 00 -2.8294E-01 1.1946E 00 -2.3913E-01

1.5000E 01 -7.3430t--01 -9.6174E-01 1.2100E 00 9.1871E-01

l.BOOOE 01 5.7714fc--01 1.0880E 00 1.2316E 00 1.0831E 00

2.0000E 01 7.7156E--01 -9.7738E-01 1.2452E 00 -9.0254E-01

2,3000E 01 -9.3351E--01 8.5310E-01 1.2646E 00 -7.4042E-01

2.5000E 01 1.1689E 00 5. 1403E-01 1.2770E 00 4.1429E-01

2.8000E 01 -1.0866E 00 -7.0396E-01 1.2947E 00 5.7485b-01

3.0000E 01 -2.0535E--01 1.2-899E 00 1.3062E 00 -1.4129E 00

3.30OOF 01 4.1265E--01 -1.2568E 00 1.3228E 00 -1.2535E 00

3.5000fc 01 -1.3268E 00 1.3367E-01 1.3335E 00 -1.0041E-01

4.0000F 01 -4.7902E--01 -1.2721E 00 1.3593E 00 1.2107E 00

4.5000E 01 1.1254E 00 -8.0522E-01 1.3838E 00 -6.2106E-01

5.0000E 01 1.0873E on 8.93A0E-01 1.4072E 00 6.8783E-01

-61-
CASE m

= 175 x\j = 175 ^

X RE(EO) IM(EO) EO(AMP) PHASE(EO)

lO.OOOOE--03 3 1459E-02 -8.9757E-01 8.9812E--01 -1.5358E 00

2.0000E--02 2.3127E-02 -9.1575E-01 9.1605E--01 -1.5455E 00

4.0000E--02 5.3404E-03 -9.3429E-01 9.3431E--01 -1.5651E 00

6.0000E--02 -1.3040E-02 -9.4507E-01 9.4516E--01 1.5570t 00

l.OOOOE--01 -5.0617E-02 -9.5769E-01 9.5903E--01 1.5180E 00

2.0C00E--01 -1.46blE-01 -9.6728E-01 9.7831E--01 1.4205E 00

3.0000E--01 -2.4291E-01 -9.5971E-01 9.8998E--01 1.3229E 00

4.0000E--01 -3.3821E-01 -9.3949E-01 9.9851E--01 1.2252E 00

5.0000E--01 -4.3118E-01 -9.0817E-01 1.0053E 00 1.1275E 00

6.0000E--01 -5.2075E-01 -8.6665E-01 I.OIUE 00 1.0297E 00

7-nOOOF--01 -A.0592E-01 -8.1563E-01 1.0161E 00 9.3187E-01

8.0000E--01 -6.8574E-01 -7.5578E-01 1.0205E 00 8.3395E-01

9.0000E--01 -7.5937b-01 -6.8778E-01 1.0245E 00 7.3597E-01

l.OOOUE GO -8.2601E-01 -6.1237E-01 1.0282E 00 6.3795E-01

1.4000E 00 -1.0096E 00 -2.5286E-01 1.0408E 00 2.4541E-01

2.0000E 00 -9.9357E-01 3.5644E-01 1.0556E 00 -3.4444E-01

2.4000E 00 -7.8693E-01 7.1596E-01 1.0639E 00 -7.3821E-01

3.0000E 00 -2.5690E-01 1.0438E 00 1.0749E 00 -1.3295E 00

3.4000E 00 1.6503E-01 1.G689E 00 i.0816E 00 1.4176E 00

4.0000E 00 7.3981E-01 8.0155E-01 1.0908E 00 8.2544E-01

4.^nooE 00 9.9650E-01 A.5751E-01 1.0965E 00 4.3041E-01

5.0000E 00 1.0901E 00 -1.7862E-01 1.1046E 00 -1.6242E-01

6.0000E 00 4.5510E-01 -1.0201E 00 1.1170e 00 -1.1512E 00

7.0000E 00 -6.0874E-01 -9.5015E-01 1.1284E 00 I.OOIOE 00

R.OOOOE 00 -1.1390E 00 -1.2537E-02 1.1391E 00 1.1006E-02

9.0000E oc -6.4057E-01 9.539AE-01 I 1491E 00 -9.7946E-01

l.OOOOE 01 4.5065E-01 1.0673E 00 1 1585E 00 1.1713E 00

1.3000E 01 -2.7285E-01 -1.1528E 00 1.1846E 00 1.3384E 00

1.5000E 01 -9.5870E-01 7.2255E-01 1.2005E 00 -6.4585fc-01

1.8000E 01 1.0833E 00 -5.6677E-01 1.2226E 00 -4.8202E-01

2.0000E 01 -9.6639E-01 -7.7135E-01 1.2365E 00 6.7363E-01

2.3000E 01 8.4277E-01 9.3153E-01 1.2562E 00 8.3538E-01

2.5000E 01 5.1627E-01 -1.1589E 00 1.2687E 00 -1.1517E 00

2.8000E 01 -9.9144E-01 ' -7.0447E-01 1.0768E 00 1.2867E 00

3.0000E 01 1.2813E 00 2.0968E-01 1.2983E 00 1.6221E-01

3.3000fc 01 -1.2477E 00 -4.1540E-01 1.3151E 00 3.2138E-01

3.5000E 01 1.2763E-01 1.3197E 00 1.3259E 00 1.4744E 00

4.0000E 01 -1.2669E 00 4.7171E-01 1.3519E 00 -3.5643E-01

4.5000E 01 -7.971ie-01 -1.1223E 00 1.3766E 00 9.5321E-01

5.0G00E 01 8.9243E-01 -1.0788E 00 1.4001E 00 -8.7968E-01

(

-62.
(CASE ni

= 180° ^ = 180°

X RE{HZ) IM{HZ) HZ(AMP) PHASE(HZ)

lO.OOOOE--03 9.9995E-01 -9.9998E-03 lO.OOCOE-Cl -lO.OOOOE-03

2.0000t--02 9.9980E-01 -1.9999E-02 lO.OOCOE-Ol -2.0000E-02

4.0000E--02 9.9920E-01 -3.9989E-02 lO.OOOOE-01 -4.0000E-02

6.0000E--02 9.9a20E-01 -5.9964E-02 lO.OOOOE-01 -6.0COOE-02

l.OOOOE--01 9.95C0E-01 -9.9833E-02 lO.OOOOE-Ol -l.COOGE-01

2.0000E--01 9.8007E-01 -1.9867E-01 lO.OOOOE-01 -2.0000E-01

3.0000E--01 9.5534E-01 -2.9552E-01 lO.OOOOE-01 -3.D000E-01

4.0000E--01 9.2106E-01 -3.8942E-01 lO.OOOOE-01 -4.0000E-01

5.0000E--01 3.7758E-01 -4.7g43E-01 lO.OOCOE-Ol -5.000CE-01

6.0000E--Ul 8.2534E-01 -5.6464E-01 lO.OOOOE-Ol -6.0000E-01

7.0000E--01 7.6485E-01 -6.4422E-01 l.OOOOE 00 -7.0000E-01

8.0000F--0 1 6.9672E-01 -7. 1736E-01 I.OOCOE 00 -7.9999E-01

9.0000E--01 6.2163E-01 -7.8333E-01 l.OOOOE 00 -8.9998E-01

l.OOOOE 00 5.4030E-C1 -8.4147E-01 10.00006-01 -l.OOOOE 00

1.4C00E 00 1.6996E-01 -9.8545E-01 lO.OOOOE-01 -1.4000E 00

2-OOOOE 00 -4.1619E-01 -9.0929E-01 l.OOOOE 00 1.14156 00

2.4000E 00 -7.3739E-01 -6.7546E-01 lO.OOCOE-01 7.4159E-01

3.0000E 00 -9.8999E-01 -I.4112E-01 lO.OOOOE-Cl 1.4159E-01

3.A000E 00 -9.6680E-01 2.5554E-0I lO.OOOOE-01 -2.5841E-01

4-OOOOE OL -^.5365E-0I 7.5680E-01 l.OOOOt 00 -8.5840E-01

4.4000E 00 -3.0736E-01 9.5161E-01 l.OOOOE 00 -1.2584E 90

s.noooE 00 2.8367E-01 9.5892E-01 lO.OOOOE-Ol 1.2832E 00

6.0000E 00 9.6016E-0I 2.7941E-01 9.9999E-01 2.8318E-01

7.0000E 00 7.5387E-01 -6.5698E-01 9.99976-01 -7.1683E-01

8.0000t 00 -1.4550E-01 -9.8935E-01 9.9999E-01 1.4248E 00

9.0000E 00 -9.1113E-01 -4.1211E-01 lO.OOOOE-01 4.2477E-01

l.OOOOE Jl -8.3908E-01 5.4403E-01 l.OOOOE 00 -5.7522E-01

1.3000E 01 9.0742E-0I -4.2017E-01 9.99986-01 -4.3364E-01

1.5000E 01 -7.5966E-01 -6.5029E-01 9.99936-01 7.37986-01

1.8000E () 1 6.6034E-01 7.5097E-01 10.00006-01 8.4953E-01

2.0000E 01 4.0804E-01 -9. 1293E-01 9.9997E-01 -1.1505E 00

2-3000E 1 -5.3284E-01 8.4622E-01 l.OOOOE 00 -1.00886 00

2.5000E 01 9.9119E-01 1.3234E-0I 9.9999E-01 1.32736-01

2.8000E 01 -9.6259E-01 -2.7090E-01 9.99986-01 2.74336-01

3. 0000

E

01 1.5424E-01 9.8b03E-01 9.9999E-C1 1.41596 Ou

3.30nOE 01 -1.3225E-02 -9.9993E-0I l.OOOOE CO 1.55766 00

3.5000E 01 -9.0366E-01 4.2818E-01 9.99976-01 -4.42496-01

4.0000E 01 -6.6689E-01 -7.4512E-01 9.9997E-01 8.^0756-01

4.5000E 01 5.2527E-01 -8.5088E-01 9.9996E-01 -1.0177E 00

5.00006 1 9.6495E-01 2.6236E-01 9.9998E-01 2.65476-01

-63-
= 180°

CASE m

ijj = 180°

X RE(EO) I^^(EO) EC(AMP) PHASE(E(J)

ICOOCOh--03 -1.J003E-02 -9.9995E-01 lO.OOOOt-Ol 1.5608t 00

2.0000t--02 -2.0002E-02 -9.9980E-01 lO.OOOOt-01 1.5508t 00

4.0000b--02 -3.9993t-02 -9.992?E-01 lO.OOCOE-01 1 .530eE 00

6.0U00E--02 -5.9967E-02 -9.9820E-01 io.nocoE-01 l.bl08£ 00

l.OOOOE--01 -9.9037E-02 -9.9500E-0L lO.OOOOE-Cl 1.470&t 00

z.ooooe--01 -1.9867E-01 -9.8007E-01 lO.OOCOE-Ol 1.3708E 00

3.0C0':^E--CI -2.9552fc-01 -9.5b34E-01 lO.OOGOE-Cl 1.2708E 00

4.0000E--01 -3.8942E-01 -9.2106E-01 lO.GOOOE-01 1.1708E 00

5.0000E--01 -4.7942E-01 -8.7758E-01 lO.OOOOE-01 1.0708E 00

6.00006--01 -5.6463E-01 -8.2533E-01 9.9999E-01 9.7081b--01

7.0000E--01 -6.4418E-01 -7.6484E-01 9.9997E-01 8.7083G--01

8.0000E--Ul -7.1728E-01 -6.9671E-01 9.9994E-01 7.7085E--01

9.0000E--01 -7.8318E-01 -6.2162E-01 9.9989E-0I 6.7089E--01

l.OOOOE oc -8.4147E-01 -5.4030E-01 I.OOOOE 00 5.7079E--01

1.4C00E GO -9.8546E-01 -1.6996E-01 I.OOOOE 00 1.7079t--01

2.0000E oc -9.0946E-01 4.1617E-01 1.0002E 00 -4.2916E--01

2.4000E 00 -6.7545E-01 7.3739E-01 9.9999E-01 -8. 2921b--01

3.000Ub -1.4112E-Ui 9.8999E-01 lO.OOOOE-01 -1.4292b 00

3.400GE 00 2.b554E-01 9.6679E-01 lO.QOOOE-ol 1.3124E 00

4.UULifjt OL 7.5677E-01 6.5364E-01 9.9997E-01 7.1241E--01

4.4000E 00 9.5151E-01 3.0735E-01 9.9992E-01 3.1243b--01

5.0000E 00 9.5893E-01 -2.8367E-0I I.OOOOE 00 -2.8761b--01

6. 0000

F

00 2.7940E-01 -9.6C17E-01 9.9999E-L)1 -1 .2876E 00

7.0000E 00 -6.5703E-01 -7.5388E-01 I.OOOOE 00 8.5393E--01

s.oooot 00 -9.8933E-01 i.4550E-01 9.9998E-01 -1.4602t--01

9.0000E 00 -4.i212E-01 9.1I13E-01 lO.OOOOE-01 -1.1460E 00

I.OOOOE 01 5.4399E-01 8.3907E-01 9.9998E-01 9.956GE--01

i.BOOOE CI -4.2020E-01 -9.0743E-01 lO.OOOOE-Ol 1.1371E 00

1.5000E 01 -6.5024E-01 7.5967E-01 9.9996E-01 -8.6286E--01

1.8000E 01 7.5100E-01 -6.6033E-01 I.OOOOE 00 -7.2124E--01

2.0000E 01 -9.1298E-01 -4.0806E-01 I.OOOOE 00 4.2032E--01

2.3000t 01 8.4620E-01 5.3283E-01 9.9998E-01 5.6195E--01

2.5000E 01 ^ 1.3234E-01 -9.9119E-01 9.9999E-01 -1.4381E 00

2.8000E 01 -2.7088E-01 9.6259E-01 9.9998E-01 -1.2965E 00

3.0000E 01 9-8800E-01 -1.5425E-01 9.9997E-01 -1.5488E--01

3.3000E 01 -9.9984E-01 1.3261E-02 9.9993E-01 -1.3263E--02

3.5000E 01 4.2820E-0I 9.0367E-01 9.9999E-01 1.1283E 00

4.0000E 01 -7.4505E-01 6.6692E-01 9.9994E-01 -7.3012E--01

4.5000E 01 -8.5093E-01 -5.2529E-0I I.OOOOE uO 5.5305E--01

5.0000E 01 2.6235E-01 -9.6495E-0I 9.9998E-01 -1.3053E 00

-64-
CASE m

= 185'- i|j = iss'^

X RE(HZ) IMtHZ) HZ(AMP) PHASEIHZ)

lO.OOOOE--03 9.7243E-01 -1.1341E-02 9.7250E-01 -1.1662E-02

2.0000E--02 9.7180E-01 -2.2254E-02 9,7205E-01 -2.2896E-02

4.0000E--02 9.7022E-01 -4.3651E-02 9.7121E-01 -4.4960E-02

6.0000E--02 9.6824E-01 -6.4709E-02 9.7040E-01 -6.6732E-02

l.OOOOE--01 9.6304E-01 -1.0615E-01 9.6887E-01 -1.0978E-&1

2.0000E--01 9.4300E-01 -2.0677E-01 9.6540E-01 -2.1585E-01

3.0000E--01 9.1321E-01 -3.0337E-01 9.6228E-01 -3.2074E-01

4.0000E--01 8.7409E-01 -3.9552E-01 9.5941E-01 -4.2493E-01

5.0000E--Oi 8.2614E-01 -4.8254E-01 9.5674E-01 -5.2864E-01

6.0000E--01 7.6992E-01 -5.6372E-01 9.5424E-01 -6.3200E-01

7.0000E--CI 7.0607E-01 -6.3837E-01 9.5187E-01 -7.3509E-01

8.0000E--01 6.3528E-01 -7.0582E-01 9.4961E-01 -8.3795E-01

9.0000E--01 5.5831E-01 -7.6548E-01 9.4746E-01 -9.4064E-01

l.OOOOE 00 4.7600E-01 -8.1682E-01 9.4539E-01 -1.0432E 00

l.AOOOE oc 1.1105E-01 -9.3126E-01 9.3786E-01 -1.4521E 00

2.0000E 00 -4.3874E-CJ1 -8.1787E-01 9.2812E-01 1.0784E 00

2.4000E 00 -7.2179E-01 -5.7426E-01 9.2236E-01 6.7206E-01

3.0000E 00 -9.1268E-01 -5.8085E-02 9.1453E-01 6.3557E-02

3.4000E 00 -8.5717E-01 3.0474E-01 9.0973E-01 -3.4158E-01

4.0000E CO -5.2626E-01 7.3385E-01 9.0304E-01 -9.4867E-01

4.4000E 00 -1.9418E-01 8.7764E-01 8.9887E-01 -1.3531E 00

5.0000E CO 3.3819E-01 8.2644E-01 8.9296E-01 1.1824E 00

6.0000E 00 8.7071E-01 1.5214E-01 8.8390E-01 1.7298E-01

7.0000E 00 5.8736E-01 -6.4940E-0I 8.7562E-01 -8.3552E-01

8.0000E GO -2.3364E-01 -8.3594E-01 8.6797E-01 1.2983E 00

9.0000E 00 -8.2465E-01 -2.4699E-01 8.6084E-01 2.9101E-01

l.OOOOE 01 -6.4453E-01 5.6049E-01 8.5415E-01 -7.1577E-01

1.3000E 01 6.9368E-01 -4.6679E-01 8.3611E-01 -5.9232E-01

1.5000E 01 -7.0858E-01 -4.2337E-01 8.2542E-01 5.3857E-01

1.8000E 01 6.3776E-01 5.0C79E-01 8.1088E-U1 6.6568E-01

2.0000E 01 1.810CE-01 -7.8130E-01 8.0199E-01 -1.3431E 00

2.3000E 01 -2.7596E-01 7.3985E-01 7.8964E-01 -1.2138E 00

2.5000E 01 7.7947E-01 -6.2314E-02 7.8196E-01 -7.9775E-02

2.8000E 01 -7.7013E-01 -3.9433E-02 7.7114E-01 5.1158E-02

3.0000E 01 2.8686E-01 7.0G46E-01 7.6433E-01 1.1861E 00

3.3000E 01 -1.8863E-01 -7.3071E-01 7.5467E-01 1.3182E 00

3.5000E 01 -5.7833E-01 4.7522E-01 7.4854E-01 -6.8784E-01

4.0000E 01 -6.1359E-01 -4.0315E-01 7.3418E-C1 5.8131E-01

4.5000E 01 1.9983E-01 -6.9276E-01 7.2100E-01 -1.2900E 00

5.0000E 01 7.0868E-01 -1.3215E-02 7,0880E-01 -1.8645E-02

-65-
(/) = 185°

CASE ni

^\l = 185°

X RE{EO) IM{EO) En(AMP) PHASE{EO)

lO.OOOOE--03 -5.8347E-02 -1.1031E 00 1.1046E 00 1.518GE 00

2.0000E--02 -6.8440E-02 -1.0819E 00 1.0841E 00 1.5076E 00

4.0000E--02 -8.9032E-02 -1.0601E 00 1.0638E 00 1.4870E 00 , 6.0000E--02 -1.0961E-01 -I.0464E 00 1.0521E 00 1.4664E 00 1 l.OOOOE--01 -1.5039E-01 -1.0265E 00 1.0375E 00 1.4253E 00

2.0000E--01 -2.4981E-01 -9.8649E-01 1.0176E 00 1.3228E 00

3.0000E--01 -3.4528E-01 -9.4479E-01 1.0059E 00 1.2204E 00

4.0000E--01 -4.3619E-01 -8.9702E-01 9.9745E-01 1.1182E 00 % 5.0000E- 1.0161E 00 \ -01 -5.2183E-01 -8.4221E-01 9.9077E-01

6.0000E--01 -6.0149E-01 -7.8028E-01 9.8520E-01 9.1408E-01

7.0000E--01 -6.7446E-01 -7.1154E-01 9.8040E-01 8.1214E-01 J

7.1028E-01 1 6.0849E-01

8.0000E--01 -7.4010E-01 -6.3650E-01 9.7615E-GI

9.0000E--0] -7.9781E-01 -5.5581E-01 9.7233E-01

l.OOOOE 00 -8.4709E-01 -4.7022E-01 9.6885E-01 5.0675E-01

l.AOOOE 00 -9.5240E-01 -9.5827E-02 9.5721E-01 1.0028E-01

2.0000E 00 -8.2447E-01 4.5934E-01 9.4380E-01 -5.0831E-01

2.4000E 00 -5.7214E-01 7.4129E-01 9.3641E-0i -9.1348E-01

3.0000E 00 -4.6505E-02 9.2562E-01 9.2679E-01 -1.5206E 00

3.4000E oc 3.1947E-01 8.6390E-01 9.2108E-01 1.2166E 00

A.OOOOt uo 7.4836E-01 5.2350E-01 9.1329E-01 6.1041E-01

4.4000E 00 8.8921E-01 1.8630E-01 9.0852E-01 2.0653E-01

5.0000E 00 8.3102E-01 -3.5036E-01 9.0186E-01 -3.9899E-01

6-OOOOE 00 1.4498E-01 -8.7995E-01 8.9181E-G1 -1.4075E 00

7.0000E 00 -6.6001E-01 -5.8625E-01 8.8278E-01 7.2628E-01

8.0000E 00 -8.4023E-01 2.4249E-01 8.7452E-01 -2.8097E-01

9.0000E 00 -2.4211E-01 8.3240E-01 8.6689E-01 -1.2877E 00

l.OOOOE 01 5.6907E-01 6.4450E-01 8.5978E-01 8.4747E-01

1.3000E 01 -4.7404E-01 -6.9444E-01 8.4081E-01 9.7183E-01

1.5000E 01 -4.2113E-01 7.1483E-01 8.2966E-01 -1.0384E 00

1.8000E 01 4.9946E-01 -6.4350E-01 8.1459E-01 -9.1076E-01

2.0000E 01 -7.8560E-01 -L.7758E-01 8.0542E-01 2.2230E-01

2.3000E 01 7.4411E-01 2.7334E-01 7.9272E-01 3.5204E-01

2. 5000

E

01 ' -6.6274E-02 -7.8205E-01 7.8485E-01 1.4863E 00

2.8000E 01 -3.6094E-02 7.7294E-01 7.7378E-01 -l.'3241E 00

3.0000E 01 7.0953E-01 -2.9089E-01 7.66e4E-01 -3.8907E-01

3.3000E 01 -7.3217E-01 1.9223E-01 7.5698E-01 -2.5676E-01

3.5000E 01 4.7894F-01 5.7813E-01 7.5075E-01 8.7895E-01

4.0000E 01 -4.0194E-01 6.1675E-01 7.3616E-01 -9.9322E-01

4.5000h 01 -6.9517E-01 -1.9789E-01 7.2279E-01 2.7733E-01

5.0000E 01 -1.5597E-02 -7.1026E-01 7.1043E-01 1.5488E 00

.66-
CASE ni

</) = 190° i|i = 190

X RE(HZ) IM(HZ) HZ{AMP) PHASE (HZ)

lO.OOOOE--03 9.4624E-01 -1.2739E-02 9.4633E-01 -1.3462E-02

2.0000E--02 9.4507E-01 -2.4551E-02 9.4539E-01 -2.5972E-02

4.0000E--02 9.4244E-01 -4.7282E-02 9.4363E-01 -5.0127E-02

6.0000E--02 Q.3942E-01 -6.9327E-02 9.4197E-01 -7.3664E-02

l.OOOOE--01 9.3216E-01 -I.1212E-01 9.3888E-01 -1.1970E-01

2.0000E--01 9.0707E-01 -2.1393E-01 9.3196E-01 -2.3162E-01

3.0000E--01 8.72A7E-01 -3.0973E-01 9.2582E-01 -3.4112E-01

4.0000E--0 1 8,2893£-01 -3.9962E-01 9.2023E-01 -4.4922E-01

s.ooooe--01 7.7705E-01 -4.8324E-01 9.1506E-01 -5.5636E-01

6.0000E--01 7.1751E-01 -5.6009E-01 9.1023E-01 -6.6280E-01

7.0000E--01 6.'>102E-01 -6.2962E-01 9.0568E-01 -7.6869E-01

8.0000E--01 5.7837E-01 -6.9134E-01 9.0137E-01 -8.7414E-01

9.0000E--01 5.0038E-01 -7.4479E-01 8.9727E-01 -9.7923E-01

l.OOOOE 00 4.1790E-01 -7.8958E-01 8.9335E-01 -1.0840E 00

1.4000E 00 6.1489E-02 -8.7700E-01 8.7916E-0] -1.5008E 00

2.G000E 00 -4.5045E-01 -7.3381E-01 8.6103E-01 1.0203E 00

2.4000E 00 -6.9775E-01 -4.8619E-01 8.5044E-01 6.0857E-01

3-OOOOE 00 -8.3613E-01 5.7550E-03 8.3615E-01 -6.8827E-03

3.4000E 00 -7.5686E-01 3.3449E-01 8.2748E-01 -4.1614E-01

4.0000E 00 -4.2065E-01 6.9861E-01 8.1547E-01 -1.0288E OU

4.4000E 00 -1.0811E-01 8.0077E-01 8.0804E-01 -1.4366E 00

5.0000E 00 3.6b94E-01 7.0868E-01 7.9759E-01 1.0941E 00

6.0000E 00 7.7936E-01 6.0753E-02 7.8173E-01 7.7795E-02

7.0000E 00 4.5458E-01 -6.1829E-01 7.6741E-01 -9.3682E-01

8.0000E 00 -2.7930E-01 -7.0073E-01 7.5434E-01 1.1915E 00

9.0000E 00 -7.3037E-01 -1.3241E-01 7.4228E-01 1.7934E-01

l.OOOOE 01 -4.9235E-01 5.4042E-01 7.3107E-G1 -8.3191E-01

1.3000E 01 5.2741E-01 -4.6244E-01 7.0144E-01 -7.1985E-01

1.5000E 01 -6.2897E-01 -2.6945E-01 6.8425E-G1 4.0474E-01

I.8000E 01 5. 7?67E-01 3.3079E-01 6.6134E-01 5.2381E-01

2.0000E 01 5.2507E-02 -6.4547E-01 6.4760E-01 -1.4896E 00

2.3000E 01 -1.2770E-01 6.1574E-01 6.2884E-01 -1.3663E 00

2.5000E 01 6.0028E-01 -1.4425E-01 6.1737E-01 -2.3584E-01

2.8000E 01 -5.9785E-01 6.5792E-02 6.0146E-C1 -1.0961E-01

3.0000E 01 3.0836E-01 5.0489E-01 5.9161E-01 1.0225E 00

3.3000E 01 -2.3557E-01 -5.2761E-01 5.7781E-01 I.1509fc 00

3.5000E 01 -3.7250E-01 4.3038E-01 5.6919E-01 -8.5737E-01

4.0000E 01 -5.0450F-01 -2.1744E-01 5.4936E-01 4.0695E-01

4.5000E 01 5.4426E-02 -5.2882E-01 5.3161E-01 -1.4682E 00

5.0000E 01 5.0527E-01 -1.0249E-01 5.1556E-01 -2.0013E-01

.67.
CASE ni

= 190° ^\^ = 190°

X RE(EO) IM(60) 60(AMP) PHAS6{60)

lO.OOOOE--03 -1.1330E-01 -1.20616 00 1.21146 00 1.47716 00

2.00QUE--02 -i.2172E-01 -1.16146 00 1.16786 00 1.46646 00

4.0000E--02 -1.4119E-01 -1.11666 00 1.12556 00 1.44506 00

6.00006--02 -1.6133E-01 -1.08956 00 1.10146 00 1.42386 00

l.OOOOE--01 -2.0162E-01 -1.05236 00 1.07146 00 1.38156 00

2.0000E--01 -2.99356-01 -9.87036-01 1.03146 00 1.2764E 00

3.0000E--01 -3.9167E-01 -9.28846-01 1.00806 00 1 17176 00

^.OOOOE--01 -4.7817E-01 -8.68366-01 9.91326-01 1.0674E 00

5.0000E--01 -5.5827E-01 -8.03226-01 9.78186-01 9.63416-01

6.0U0QE--01 -6.3140E-01 -7.32786-01 9.67296-01 8.59586-01

7.0000E--01 -6.9703E-01 -6.57106-01 9.5793E-01 7.55926-01

8.0000E--01 -7.5464E-01 -5.7657E-01 9.4969E-01 6.52426-01

9.0000E--01 -8.0381E-01 -4.9178E-01 9.42316-01 5.49066-01

l.OOOOE 00 -8.44166-01 -4.0342E-01 9.35606-01 4.45816-01

1.4000E 00 -9.1283E-01 -3.0908E-02 9.13366-01 3.38476-02

2.0000E 00 -7.41956-01 4.8805E-01 8.88086-01 -5.81836-01

2.40006 00 -4.7888E-01 7.31516-01 8.74326-01 -9.91166-01

3.00CV0E 00 2.8352E-02 8.56116-01 8.5658E-01 1.53776 00

3.4000E 00 3.6111E-01 7.65236-01 8.46156-01 1.12996 00

4.0000E 00 7.2249E-01 4.12726-01 8.32066-01 5.19016-01

A.4000E 00 8.1831E-01 9.22286-02 8. 23496-01 1.12236-01

5.0000E 00 7.1330E-01 -3. 87216-01 8.1162E-01 -4. 97336-01

6.0000E 00 4.6710E-02 -7.92546-01 7.9391E-01 -1.5119E 00

7.0000E 00 -6.3496E-01 -4.49906-01 7.78196-01 6.16436-01

S.OOOOE 00 -7.0497E-01 2.94496-01 7.6401E-01 -3.95706-01

9.0000E oe -1.2253E-01 7.40986-01 7.51C4E-01 -1.40696 00

l.OOOOE 01 5.5357E-01 4.89696-01 7.3908E-01 7.24246-01

1.3000E 01 -4.7339E-01 -5.26186-01 7.07796-01 8.3816E-01

1.5000E 01 -2.6411E-01 6.3725E-01 6. 89826-01 -1.1779E 00

1.8000E 01 3.26926-01 -5.80266-01 6.66016-01 -1.05776 00

2.0000E 01 -6.5017E-01 -4.62636-02 6.51816-01 7.10356-02

2.3000E 01 6.2048E-01 1.22636-01 6.32496-01 1.95126-01

2.5000E 01 -1.5042E-01 -6.02206-01 6. 20716-01 1.32606 00

2.8000E 01 , 7.1149E-02 6.00226-01 6.04426-01 1.45286 00

3.0000E 01 5.04726-01 -3.13876-01 5.94356-01 -5.56346-01

3.3000E 01 -5.28046-01 2.4060E-01 5.80276-01 -4.27546-01

3.5000E 01 4.34866-01 3.7081E-01 5.71496-01 7.0607E-01

4.0000E 01 -2.14786-01 5.0777E-01 5.5133E-01 -1.1706E 00

4.5000E 01 -5.30846-01 -5. 12476-02 5.33316-01 9.62416-02

s.oooot 01 -1.05786-01 -5.06116-01 5.17056-01 1.36486 00

-68-
CASE ni

<l> = 200° ijj = 200

X REfHZ) IM{HZ) HZ(AMP) PHASE(HZ)

lO.OOOOE--03 8.9742E-01 -1.5675E-02 8.9755E-01 -1.7466E-02

2.0000E--02 8.9501E-01 -2.9211E-02 8.9549E-01 -3.2625E-02

4.0000E--02 8.9009E-01 -5.4359E-02 8.9175E-01 -6.0995E-02

6.0000E--02 8.8A89E-01 -7.8078E-02 8.8832E-C1 -8.8007E-02

l.OOOOE--01 8.7344E-01 -1.2292E-01 8.82G5E-01 -1.3981E-01

2.00GOE--01 8.3865E-01 -2.2551E-01 8.6844E-01 -2.6268E-01

3.0000E--01 7.9536E-01 -3.1823E-01 8.5667E-01 -3.8060E-01

4.0000E--01 7.4428E-01 -4.0245E-01 8.4613E-01 -4.9569E-01

5.0000E--01 6.8618E-01 -4.7843E-01 8.3650E-01 -6.0888E-01

6.0000E--01 6.2184E-01 -5.4612E-01 8.2761E-01 -7.2066E-01

7.0000E--01 5.5211E-01 -6.0535E-01 8.1931E-01 -8.3136E-01

8.0000E--01 4.7784E-01 -6.5592E-01 8.1152E-01 -9.4119E-01

9.0000E--01 3.9991E-01 -6.9767E-01 8.0416E-01 -1.0503E 00

l.OOCJOE 00 3.1921E-01 -7.3048E-01 7.9717E-01 -1.1588E 00

1.4000E 00 -1.3b28E-02 -7.7212E-01 7.7224E-01 1.5533E 00

2.0000E 00 -4.5018E-01 -5.8887E-01 7.4124E-01 9.1808E-01

2.4C00E 00 -6.3546E-01 -3.4593E-01 7.2351E-01 4.9352E-01

3.0000E 00 -6.9446E-01 8.8566E-02 7.0008E-01 -1.2685E-01

3.4000E 00 -5.8787E-01 3.5379E-01 6.8611E-01 -5.4175E-01

4.0000E 00 -2.6530E-01 6.1208E-01 6.6711E-UI -1.1618E 00

A.4000E 00 2.J389E-03 6.5551E-01 6.5552E-01 1.5677E 00

5.0000E 00 3.7142F-01 5.2055E-01 6.3947E-01 9.5106E-01

6.0000E 00 6.1399E-01 -4.5126E-02 6.1565E-01 -7.3365E-02

T.OOOOfc 00 2.7261E-01 -5.2854E-01 5.9470E-01 -1.0946E 00

8.0000E 00 -2.9741E-01 -4.9370E-01 5.7602E-01 1.0282t 00

9.0000t 00 -5.5913E-01 -6.4081E-03 5.5917E-01 1.1460E-02

l.OOOOE 01 -2.9215E-01 4.5871E-01 5.4384E-01 -1.0037E 00

1.3000E 01 3 1373E-01 -3.9549E-01 5.0481E-01 -9.0017E-01

1.5000E 01 -4.7146E-01 -1.0574E-01 4.8317E-01 2.2063E-01

1.8000E 01 4.2997E-01 1.5014E-01 4.5543E-01 3.3594E-01

2.0000E 01 -4.7476E-02 -4.3682E-01 4.3940E-01 I.4625E 00

2.3000E 01 -5.7601E-03 4.1817E-01 4.1821E-01 -1.5570E 00

2.5000E 01 3.6925E-01 -1.6795E-01 4.0565E-01 -4.2687E-01

2.8000E 01 -3.7131E-01 I.15G7E-01 3.8873E-01 -3.0052E-01

3.0000E 01 2.5490E-01 2.7984E-01 3.7853E-01 8.3201E-01

3.3000E 01 -2.0870E-01 -2.9895E-01 3.6459E-01 9.6l3e)E-01

3.5000E 01 -1.7841E-01 3.0818E-01 3.5609E-01 -1.0460e GO

4.0000E 01 -3.2893E-01 -7.3880E-02 3.3712E-01 2.2094E-01

4.5000E 01 -2.5730E-02 -3.1978E-01 3.2081E-01 1.4905E GO

5.0000E 01 2.847RE-01 -1.1358E-01 3.0659E-01 -3.7951E-G1

-69-
CASE III

(t> = 200° ^ = 200°

X RE(EO) IM(EO) EO(AMP) PHASE(EO)

lO.OOOOE--03 -2.4152E-01 -1.4086E 00 1.4291E 00 1.4010E 00

2.0000E--U2 -2.4075E-01 -1.3104E 00 1.3324E 00 1.3891E 00

4.00C0E--02 -2.5252E-01 -1.2155E 00 1.2415E 00 1.3660E 00

6.0000E--C2 -2.6864E-01 -1.1600E 00 1.1907E 00 1.3432E 00

l.OOOOE--01 -3.0376E-01 -1.0874E 00 1.1290E 00 1.2984E 00

2.0000E--01 -3.9144E-01 -9.7260E-01 1.0484E 00 1.1882E GO

3.0000t--CI -4.7305E-01 -8.8379E-01 1.0024E 00 1.0793E 00

4.00CCt--01 -5.4725E-01 -8.0093E-01 9.7004E-01 9.7139E-01

5.0000E--01 -6.1358E-01 -7.1858E-01 9.4490E-01 8.6405E-01

6.0000E--01 -6.7174E-01 -6.3488E-01 9.2429E-01 7.5720E-01

7.0000E--01 -7.2144E-01 -5.4929E-01 9.0675E-01 6.5074E-0I

8.0000E--01 -7.6247E-01 -4.6185E-01 8.9144E-01 5.4462E-01

9.0000E--01 -7.9467E-01 -3.7294E-01 8.77a3E-0l 4.3879E-01

l.OOOOE 00 -8.1794E-01 -2.8311E-01 8.6555E-01 3.3322E-01

1.4000E 00 -8.2239E-01 7.1721E-02 8.2552E-01 -8.6990E-02

2.0000E 00 -5.9114E-01 5.1090E-01 7.8133E-01 -7.1272E-01

2.4000E 00 -3.2497E-01 6.8470E-01 7.5790E-01 -1.1277E 00

3.0000E CO 1.2815E-0I 7.1697E-01 7.2834E-01 I.3939E 00

3.4000E 00 3.9509E-01 5.9150E-01 7.1131E-01 9.8191E-01

4.0000E 00 6.4324E-01 2.4613E-01 6.8873E-01 3.6546E-01

4.4000E 00 6.7455E-01 -3.0122E-02 6.7522E-01 -4.4625E-02

5.0000E 00 5.1943E-01 -4.0199E-01 6.5682E-01 -6.5863E-01

6.0000E 00 -6.8353E-02 -6.2628E-01 6.3000E-01 li4621£ 00

7.0000E 00 -5.4810E-01 -2.6050E-01 6.0685E-01 4.4368E-01

8.0000E 00 -4.9289E-01 3 1784E-01 5.8648E-01 -5.7275E-01

9.0000E 00 9.5340E-03 5.6821E-01 5.6829E-01 1.5540E 00

l.OOOOE 01 4.7320E-01 2.8400E-01 5.5188E-01 5.4054E-01

1.30O0E 01 -4.0711E-01 -3.0817E-01 5.1059E-01 6.4794E-01

1.5000E 01 -9.68846-02 4.7823E-01 4.8794E-0I -1.3709E 00

1.800UE 01 1.4334E-01 -4.36iaE-01 4.5913E-0I -1.2533E 00

2.0Q00E 01 -4.3909E-01 5.5369E-02 4.4257E-01 -1.2544E-01

2.3000E 01 4.2077E-01 -7.7185E-04 4.2077E-01 -1.8344E-03

2.5000E 01 -1.7433E-01 -3.6877E-01 4.0790E-01 1.1292E 00

2.8000E 01 1.2068E-0I 3.7150E-01 3.9061E-01 1.2567& 00

3.0000E 01' 2.7775E-01 -2.5963E-01 3.8020E-01 -7.5170E-01

3.3000E 01 -2.9758E-01 2.1311E-01 3.6602E-01 -6.2147E-01

3.5000E 01 3.1133E-01 1.7548E-01 3.5738E-01 5.1327E-01

4.0000E 01 -7.0678E-02 3.3067E-01 3.3814E-01 -1.3602E 00

4.5000E 01 -3.2034E-01 2.8822E-02 3.2163E-01 -8.9732E-02

5.0000E 01 -1.1630E-01 -2.8440E-01 3.0726E-01 1.1826E 00

-70-
CASE ni

<f> = 210° 4i = 210

X RE(HZ) IM(HZ) HZ(AMP) PHASE(HZ)

lO.OOOOE--03 8.5272E-01 -1.874GE-02 8.5293E-01 -2.1973E-02

2.0G00E--02 8.4892E-G1 -3.3863E-02 8.4960E-01 -3.9868E-02

4.0000t--02 8.4153E-01 -6.1G59E-G2 8.4374E-G1 -7.2431E-02

6.0000E--02 8.34G7E-01 -8.6G47E-02 8.3850E-01 -1.028GE-01

l.OOOOfc--01 8.185GE-01 -1.3212E-G1 8.2909E-G1 -1.6G03E-01

2,0000E--01 7.7478E-G1 -2.3359E-G1 8.G923E-01 -2.9283E-01

3.0000E--01 7.2421E-01 -3.2177E-G1 7.9247E-01 -4.1811E-01

4.0000E--01 6.6740E-C1 -3.9928E-01 7.7771E-01 -5.3914E-01

5.0000E--ui 6.0513E-G1 -4.6706E-01 7.6441E-G1 -6.5733E-01

6.0000E--01 5.3823E-01 -5.2553E-01 7.5225E-01 -7.7346E-01

7.0000E--01 4.6756E-G1 -5.7488E-01 7.4101E-G1 -8.8799E-01

8.0000E--01 3..y395E-01 -6.1522E-01 7.3054E-01 -1.0G12E 00

9.0000E--01 3.1825E-01 -6.4666E-01 7.2G73E-01 -1.1135E GO

l.OOOOE 00 2.413GE-01 -6.6931E-01 7.1148E-G1 -1.2248E GO

l.AOOOE 00 -6.2842Er02 -6.7607E-01 6.7899E-01 1.4781E 00

2.0000E 00 -4.3G20E-G1 -4.7336E-G1 6.3964E-01 8.3312E-G1

2.'^000t 00 -5.6680E-01 -2.4548E-01 6.1767E-01 4.0871E-01

3.0000E GO -5.7471E-G1 1.2990E-01 5.8921E-01 -2.2229E-01

3.A000E 00 -4.5920E-01 3.4199E-G1 5.7255E-01 -6.4013E-G1

4.0Gi)_0E oc -1.6635E-G1 5.2452E-01 5.5027E-GI -1.2637E GO

4.400Ut 00 5.7267E-02 5.3383E-G1 5.3689E-01 1.4639E GO

5.0000E GO 3.4422E-01 3 8795E-01 5.1865E-01 8.^5G6E-G1

6.0000E 00 4.84G1E-01 -8.9060E-02 4.9213E-01 -1.8197E-01

7.0000E GO 1.6800E-G1 -4.3831E-01 ^.694GE-G1 -1.2G48E GO

8.0000E 00 -2.7335E-01 -3.5693E-01 4.4958E-01 9.1723E-01

9.0000F GO -4.2992E-GI 4.3069E-02 4.3207E-G1 -9.9848E-02

l.OOOOE 01 -1.8335E-01 3.7390E-01 4.1644E-01 -1.1149E GO

l.3000h 01 2.0118E-G1 -3.1995E-01 3.7795E-01 -1.0095E GO

1.5000E 01 -3.551GE-G1 -4.0421E-02 3.5740E-01 1.1334E-01

1.8000E 01 3.2296E-01 7.6387E-02 3.3187E-01 2.3225E-G1

2.0000E 01 -6.5990E-02 -3.1059E-G1 3.1752E-01 1 3614E GO

2.3000E 01 2.A89gE-02 2.97g7E-Gl 2.99C1E-01 1.4874E GO

2.50OOE 01 2.4997E-01 -1.4359E-01 2.8828E-01 -5.2140E-G1

2.8000E 01 -2.5338E-ni 1.G451E-01 2.7408t-Gl -3.9119E-G1

3.0000fc 01 1.9551E-G1 1.7989E-01 2.6568E-01 7.4381E-G1

3.3000E 01 -1.6271E-G1 -1.9552E-G1 2.5436E-01 8.7673E-G1

3.5000E 01 -1.0599E-01 2.2372E-01 2.4756E-01 -1.1284E GO

4.0000E 01 -2.3022E-G1 -3.3371E-02 2.3262E-G1 1.4395E-GI

4.5000E 01 -3.3416E-G2 -2.1750E-G1 2.2GC5E-G1 1.4183fc GO

5.0000E 01 1.8869E-01 -9.G519E-02 2.0928E-01 -4.4730E-01

-71-
= 210

CASE m

i|j = 210

X RE(EO) IM(EO) EO(AMP) PHASECeO)

lO.OOOOE--03 -3.9112E-01 -1.6015E 00 1.64P.6E 00 1.3313E 00

2.000GE--02 -3.7284E-01 -1.4433E 00 1.4906E 00 1.3180E 00

4.0000E--02 -3.6953E-01 -1.2946E 00 1.3463E 00 1.2928t 00

6.00006--02 -3.7750E-01 -1.2099E 00 1 2674E 00 1.2684E 00

I.OOOOE--01 -4.0219E-01 -1.1021E 00 1.1732E 00 1.2209E 00

2.0000E--01 -4.7217E-01 -9.4117E-01 1.0530E 00 1.1058E 00

3.0000E--01 -5.3818E-01 -8.2607E-01 9.8591E-01 9.9337E-01

4.0000E--01 -5.9677E-01 -7.2551E-01 9.3941E-01 8.8246E-01

5.0000E--Gl -6.4721E-01 -6.3C84E-01 9.0380E-01 7.7259E-01

6.0000E--01 -6.8927E-01 -5.3885E-01 8.7490E-01 6.6352E-01

7.0000E--01 -7.2286E-01 -4.4827E-01 8.5057E-01 5.5509E-01

8.0000E--01 -7.4795E-01 -3.5871E-U1 8.29'53E-01 4.47196-01

9.0000E--01 -7.6462E-01 -2.7025E-01 8.1097E-01 3.3974E-01

l.OOOOt 00 -7.7296E-01 -1.8317E-01 7.9437E-01 2.3269E-01

1.4000E 00 -7.2747E-01 1.4174E-01 7.4115E-01 -1.9242E-01

2.0000E 00 -4.6506E-01 5.0182E-01 6.8419E-01 -8.2340E-01

2.4000E 00 -2.1209E-01 6.1948E-01 6.5478E-01 -1.2409E 00

3.0000E 00 1.7867E-01 5.9215E-01 6.1852E-01 1.2778E 00

3.4000E 00 3.8826E-01 4.5490E-01 5.9807E-01 8.6427E-01

4.0000E 00 5.5420E-01 1.3925E-01 5.71^3E-01 2.4616E-01

A.4000E 00 5.4825E-01 -9.1139E-02 5.5577E-01 -1.6473E-01

5.0000E CO 3.8033E-01 -3.7595E-01 5.3478E-01 -7.7960E-01

6.0000E 00 -1.1531E-01 -4.9154E-01 5.0489E-01 1.3404E 00

7.0000E 00 -4.5511E-01 -1.5178E-01 4.7975E-01 3.2190E-01

8.0000E 00 -3.5214E-01 2.9309E-01 4.5815E-01 -6.9414E-01

9.0000E 00 6.0184E-02 4.3514E-01 4.3929E-01 1.4334E 00

l.OOOOE 01 3.8572E-01 1.7265E-01 4.2259E-01 4.2086E-01

1.3000E 01 -3.29186-01 -1.9381E-01 3.8200E-01 5.3212E-01

1.5000E 01 -3.1349E-02 3.5921E-01 3.6058E-01 -1 4837E 00

1.8000E 01 6.9453E-02 -3.2688E-01 3.3417E-01 -1.3614E 00

2.0000E m -3.1098E-01 7.2955E-02 3.1942E-01 -2.3043E-01

2.3000E 01 2.9890E-01 -3.G655E-02 3.0047E-01 -1.0220E-01

2.5000E 01 -1.4860E-01 -2.4847E-01 2.8951E-01 1.0318E 00

2.8000E 01

' 1.0894E-01 2.5258E-01 2.7507E-01 1.1636E 00

3.0000E 01 1 .7749E-01 -1. 988^4 E-01 2.6654E-01 -8.4206E-01

3.3000E 01 -1.9378E-01 1.6586E-Ui 2.5507E-01 -7.0794E-01

3.5000E 01 2.2566E-01 1.0329E-01 2.4818E-01 4.2925E-01

4.0000E 01 -3.0735E-02 2.3106E-01 2.3309E-01 -1.4386E 00

4.5000E 01 -2.1749E-01 3.5761E-02 2.2041E-01 -1.6297E-01

5.0000E 01 -9.2444E-02 -1.8807E-01 2,0957E-0I 1,1139E 00

.72-

GPO 837-446
THE NATIONAL BUREAU OF STANDARDS

The scope of activities of the National Bureau of Standards at its major laboratories in Washington, D.C.and

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