IMPROVED SCREEN FOR REAR PROJECTION VIEWERS

• Document Type: CREST
• Collection: NGA Records (Formerly NIMA)
• Document Number (FOIA) /ESDN (CREST): CIA-RDP79B00873A002000010081-3
• Release Decision: RIPPUB
• Original Classification: C
• Document Page Count: 43
• Document Creation Date: December 28, 2016
• Document Release Date: November 8, 2012
• Sequence Number: 81
• Publication Date: August 24, 1966
• Content Type: REPORT

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MEP "Mr
Cad
'k J-44-c' CORNIN%96LASS WORKS LPLUAt rnunuLinfts:
REV. 2/63
CORNING
CORNING. NEW YORK
RESEARCH AND DEVELOPMENT LABORATORY
TECHNICAL STAFFS DIVISION
TITLE: IMPROVED SCREEN FOR REAR PROJECTION VIEWERS
Technical Report No. 12
REPORT NO. P-19-12
PRINT NOS.
PROJECT NO. 89050
NO. OF PGS. 39
NO. OF FIGS. 5
DATE August 24,
V
ABSTRACT:
This report summarizes the light scattering properties of some
Corning Glass Works' materials along with those of some commercial
rear projection screens. These data are discussed with reference
to our theoretical studies of light scattering.
We have found good agreement between the experimental and theoretical
data on the fraction of incident energy scattered into the forward
hemisphere by volume scattering materials as a function of axial
gain. The predicted wavelength dependence of the scattering cross-
section has been observed and possesses some problems, which are
discussed.
Three of the samples of Corning Glass Works' materials that were
measured meet the necessary optical requirements for application
in rear projection screens.
KEY WORDS: Light Scattering, Rear Projection Screens, Glass-Ceramics
25X1
Data Bk.
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?0.
tLe L"'
CORNING GLASS WORKS
ELECTRO-OPTICS LABORATORY
RALEIGH, NORTH CAROLINA
IMPROVED SCREEN FOR REAR PROJECTION VIEWERS
Technical Report No. - 12
Date - August 24, 1966
Period Covered - July 11, 1966
to
August 24, 1966
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umFMtiii Nih Eic)
ABSTRACT
This report summarizes the light scattering properties of
some Corning Glass Works' Materials along with those of
some commercial rear projection screens. These data are
discussed with reference to our theoretical studies of light
scattering.
We have found good agreement between the experimental and
theoretical data on the fraction of incident energy scattered
into the forward hemisphere by volume scattering materials as
a function of axial gain. The predicted wavelength dependence
of the scattering cross-section has been observed and possesses
some problems, which are discussed.
Three of the samples of Corning Glass Works' materials that
were measured meet the necessary optical requirements for
application in rear projection screens.
CC FRIE T
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1U1u ukiLv u
TECHNICAL REPORT #12
A. Materials
This report summarizes the light scattering properties of
some Corning Glass Works' materials together with those of
some commercial rear projection' screens. Although we do
not as yet have the physical data on particle size and den-
sity of the Corning materials measured, we can make some
inferences as to approximate particle size, and correlate
some of the experimental data with theoretical predictions.
Light scattering data have been obtained on 34 different
samples of Corning Glass Works' materials and on 23 com-
mercial rear projection screen materials. These data include
the angular gain function, axial gain, diffuse transmittance,
specular transmittance, spectral properties of the specularly
transmitted component, and the fraction of power within a
viewing angle of ?45?.
The angular gain function, Gain (0), is defined as the ratio
of the brightness of any material to that of an isotropic
scatterer as a function of the angle (0), assuming the same
amount of incident energy
Gain (0) = 471(0)
(1)
where 1(0) is the scattered intensity as a function of the
angle B. One may define the gain function as the ratio of
the intensity at any angle to the average intensity,
47 I(0)
Gain' (e) -
(2)
f2TI(8)- sin 0 de d?
0 0
However, the one difference between these two expressions
is that Equation (2) assumes no absorption, and for rear
projection screens this is generally not true. In fact,
the difference between Equations (1) and (2) provides a
EGE7157;',11Mill
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enEEETIVARMITO
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measure of of the fraction of the power absorbed, A,
27 r
A = 1 - y? y i(0). sin 8 de do .
0 0 0
(3)
By definition the diffuse transmittance, Td, is the ratio
of the sum of the scattered light, Is, and the specularly
transmitted light 'spec' to the incident light-,10,
27 7/2
1(0- e de d?
Td
s + Ispeco jo spec . (4)
Io Io Io
The specular component represents the fraction of light
directly transmitted through a material, i.e., not scattered,
and where I(e) denotes only the intensity of the scattered
light. For convenience we shall denote I s /I by Ts and the
o
specular transmittance by Tspec. Thus, by measuring Ts in
addition to ve), the angular gain function can be obtained,
4r Ts 1(0)
Gain (e) = 2irs7/21(0). sin 0 de 0
0 0
(5)
This can be simplified somewhat by performing the integration
over 0, which gives
Gain (0) -
2 Ts 1(0
7/2
'(e) ?
'0
sin 0 de
(6)
Besides Ts' it is important to know the fraction of power
scattered inside ?45? since the primary viewing angles lie
within ?45? of the optical axis. The fraction of the power
inside 45?, T45, is
T45 -
7/4
27 j I(0)- sin e de
0
o
which after reduction becomes
ammo
(7)
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U
7/4
Td 1(e). sin 0 de
0
T45 -
7/2
f 1(0)- sin e de
0
(8)
The function 1(e) is measured directly with our goniophoto-
meter, and the diffuse transmittance is measured by a scheme
shown in Figure 1.
Pinhole
Aperture
Collimated
Light
Sample
V-
Phototube
Figure 1. The Measurement of Ts
Collimated light passing through the pinhole is scattered
by the sample, which is physically so close to the photo-
tube that all of the light scattered through the material
is detected along with the specular component. All of the
backscattered light is absorbed by a dull black coating on
the pinhole aperture. Thus, the ratio of the phototube
signals, with and without the sample, gives the diffuse
transmittance. To obtain only the scattered component Ts,
we must measure Tspec and subtract this from Td. To measure
Tspec we use the arrangement shown in Figure 2.
The relatively large distance between the sample and the
succeeding lens ensures that only the specularly transmitted
component is intercepted by the lens and focused through the
ECTir-kroli_th
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60111aU riff
Light
Source
Pinhole
Scattered
Light
Pinhole
Aperture
Collimator
Sample
Figure 2. The Measurement of Tspec
Phototube
pinhole aperture onto the detector. Having Ts, we can
compute Gain (0) and T45 using Equations (6) and (8)
respectively. A computer program which computes Gain (0)
and T45 from values of 1(e) and Ts has been written, and
is being used regularly to summarize the light scattering
properties of the materials measured. These summaries,
along with angular gain curves of the different materials
measured, constitute Appendices A and B. For brevity,
TSP and ABS represent the specular transmittance and the
fraction of energy absorbed, respectively. Absorption, not
yet measured, has been left blank.
Tables I and II summarize the viewing properties of the
Corning Glass Works' materials and the commercial rear
projection screen materials, respectively. The manufacturer
and his designation of the commercial materials is given
in Table III. Included among the Corning materials is the
first set of samples made to have the desired physical
properties as determined by our previous theoretical inves-
tigations. These samples have the Prefix "AF".
Cink7-757 r
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Table I
Summary of the Optical Properties of Some
Corning Glass Works' Materials
Sample
Code
Ts
T45
TsRec
Axial
Gain
Half Gain
Point (c))
Thickness
mm
AC-1A
37.
15.
36.
1.2
75.
.534
AC-1B
40.
17.
19.
1.3
75.
.915
AC-3A
64.
?25.
10.
8.3
5.8
.483
AC-3B
60.
26.
4.8
2.4
70.
.787
AC-10A
69.
27.
4.8
1.9
77.
.534
AC-10B
55.
23.
7.2
1.6
74.
1.287
AC-11A
25.
16.
57.
11.
5.6
.368
AC-11B
79.
39,
19.
17.
2.8
.825
AC-12A
38.
14.
3.6
0.98
81.
.610
AC-12B
39.
15.
4.8
1.0
81.
.623
AC-15B
53.
21.
14.
1.5
79.
.991
AC-16A
59.
24.
24.
1.8
77.
.376
AC-16C
52.
20.
7.2
1.4
80.
.864
AC-17A
46.
17.
14.
1.2
80.
.534
AC-17B
35.
13.
12.
0.88
83.
.929
AC-18A
61.
23.
3.6
1.6
80.
.864/
AC-18B
76.
30.
2.4
2.5
77.
.356V
AC-19A
59.
22.
4.8
1.5
81.
.850
AC-19B
73.
27.
3.6
1.9
82.
.330
AC-20A
52.
20.
3.6
1.4
80.
.623
AC-20B
48.
20.
2.4
1.4
75.
.864
AC-21A
55.
21.
26.
1.5
80.
.457
AC=21B
56.
21..
19.
1.6
80.
.965
AC-24A
46.
18.
29.
1.5
77.
.521
AC-24B
53.
20.
12.
1.4
80.
.940v/
AC-26B
67.
27.
7.2
2.1
77.
.864v/
AF-1A
28.
11.
43.
1.1
66.
.534
AF-1B
41.
15.
24.
1.3
80.
.991
AF-2A
46.
22.
19.
1.9
63.
.521
AF-2B
36.
12.
4.8
0.93
85.
.965
AF-3A
42.
20.
14.
1.9
56.
.534
AF-3B
40.
14.
4.7
1.1
84.
.991
AF-4A
37.
20.
4.7
1.9
53.
.534
AF-4B
27.
10.
2.4
0.8
82.
.991
ITYTWEJT,F,,p,
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Table II
Summary of the Optical Properties of Some
Commercial Rear Projection Screen Materials
Sample
Code
Ts
T45
Axial
Gain
Half Gain
Point (degrees)
DA-TEX
o.
53.
34.
8.2
15.
SN-2148
64.
62.
65.
7.
SN-214914-
43.
17.
1.2
77.
HITRANS
78.
44.
25.
8.
S5OR
70.
31.
3.7
35.
LS 40FM
48.
30.
5.8
20.
OC 50FM
83.
51.
10.
18.
LS 60FM
59.
33.
4.9
26.
LS 60BFM
68.
42.
11.
14.
LS 60G
38.
25.
3.8-
26.
LS 6ONG
48.
34.
5.5
25.
LS 60PL
55.
40.
6.0
26.
LS 60STG
35.
27.
5.8
18.
LS 60VR
59.
43.
8.8
20.
LS 75G
61.
52.
29.
10.
LS 85PL
75.
67.
77.
6.
LUX-50
54.
39.
10.
16.
LUX-70
60.
37.
6.2
22.
RAVEN
56.
33.
5.0
25.
TR-50PL
60.
27.
2.4
60.
TYPE 1
82.
70.
23.
14.
TYPE 4
tf
28.
24.
6.7
15.
VCA 3606
78.
37.
37.
4.
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c)
Table III
Identification of Materials Codes with the Respective
Manufacturers of Commercial Rear Projection Screens
Sample
Code
Manufacturer
Manufacturers' Codes
DA-TEX
Da-Lite Screen Company, Inc.
SN-2148* Edmund Scientific Company
SN-21494 Edmund Scientific Company
LS-40FM Polacoat Incorporated
LS-60BFM
LS-60FM
LS-60G
LS-6ONG
LS-60PL
LS 60STG
LS-60VR
LS-75G
LS-85PL
OC-50FM
TR-50PL
RAVEN Raven Screen Corporation
HITRANS Trans-Lux News-Sign Corp.
S-50R
LUX-50
LUX-70
TYPE 1_
_
Kodak Corporation.
TYPE 4 . Kodak Corporation
VCA 3606* Union Carbide Corporation
Plastics Division-Films Dept.
*These materials are not sold as Rear projection screens.
DA-TEX (Da-Lite
Translucent Fabric)
SN-2148 Ground
Glass - Satin Finish
SN-2149 Opal Glass
LS
LS
LS
LS
LS
LS
LS
LS
LS
LS
OC
TR
40FM
60BFM (Blue)
60FM
60G 1/8"
6ONG 1/8"
60PL 1/16"
60STG 1/8"
60VR 025
75G 1/8"
85PL 1/16"
50FM (white)
50PL 1/16"
Lenscreen-Rear Projection
HI-TRANS
S-50R
Luxchrome "50"
Luxchrome "70"
Day-View Screen
White Type 1
Day-View Screen
Black Type 4
VCA-3606 White
CORTEEITA,
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n r_77, r7.7
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The fraction of incident energy scattered into the forward
hemisphere, i.e., the efficiencylis plotted against axial
gain in Figure 3. The theoretical curve in the figure is
based on single volume scattering. The data from the
Corning Glass Works' materials behaved as predicted: they
showed a rapid increase in efficiency with increasing gain*.
The commercial materials showed little correlation between
efficiency and gain, indicating that they have less than
optimum viewing properties. Many of the commercial
materials have some neutral density, which in part is
responsible for their lower than optimum efficiency.
In the theoretical summary, some calculations were made
showing the effects of variations in the scattering cross-
section with wavelength for particles of different relative
refractive indices. This work indicated that for refractive
indices near unity, i.e., .8 n 1.2, there would be large
differences between the scattering coefficients for red and
blue light. As more of the blue light would be scattered
than the red, a red colored specular component would be
transmitted through the screen. Although the relative
refractive indices of the particles in the samples measured
are not exactly known, they are believed to be near unity,
and the size parameter m, (a = 7D/:where D is the particle
diameter), to be less than 5.
Experimentally we have measured the spectral characteristics
of the specular component of many CGW samples. As predicted,
many of these have a strong excess of red, Figure 4. Because
different samples have different physical properties, no two
samples have the same light scattering characteristics or
the same spectral properties of the specularly transmitted
component.
There is little doubt that the variations in scattering with
wavelength are produced by particles about the same size as
the incident wavelength, not by very small particles. This
Report No. P-19-9, "Improved Screen for
Rear Projection Viewers", Phase II. Theoretical Studies,
April 26, 1966.
en'Arml Fri 177,, nrmrrn rA
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25X1
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50
40
30
20 /
15
5
Figure 4. Spectral Properties of the
Specularly Transmitted Component
for Some Corning Glass Works'
Materials
AC11A,
AC26A
373 .40 .45 .50 .55 .60 .65 .70
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is shown in Figure 5 by the large differences between these
data, and a curve of 1/x4 which represents Rayleigh
scattering produced by very small particles. Such curves
are a good measure of the approximate size of the particles
producing the scattering. Here the size parameter a is
thought to lie between .5 and 5, and probably between .9
and 2.. The absolute values are not as important as the
relative shapes of the curves. If any absorption occurs,
it is relatively independent of wavelength, only lowering
the curves given and having no effect on their shape. The
presence of the colored spectral component in almost all
of the glass-ceramic materials measured suggests we should
consider only systems where large relative refractive indices
can be obtained. No specular transmission can be tolerated,
not only because of efficiency considerations, but because one
would be able to see the projector through the screen. This
analysis implies we should also seriously consider materials
containing metallic particles, which for the most part
would circumvent this problem at some loss of efficiency.
The three best Corning Glass Workt! materials thus far
measured are AC18A, AC18B, and AC19B, Figure 3. These
materials are considered best because they are more efficient,
have higher gains, show little or no specular transmission,
and give the necessary uniformity of screen brightness.
B. Instrumentation
The contrast computer for the modulation transfer function
analyzer is progressing on schedule. Construction is over
90 percent complete and initial checkout has started;
completion is expected by the first of September.
We have made six sine-wave masks which are to be used with
the modulation transfer function analyzer. Some difficulties
in making these have been encountered; however, we will be
able to use the masks we have, and expect to make more when
the present difficulty has been corrected. These difficulties
are due to minute variations of the film transport speed and
produce slight variations in the density of the mask pattern.
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1111111111111111111111111111811!!!!!!!"111111111111111111
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111110111111111111111111111"10101
ICREFEIDEN11
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
CflWhEriDAL 'EP
APPENDIX A
SUMMARY OF LIGHT SCATTERING DATA OF
CORNING GLASS WORKS' MATERIALS
CONFIDENTIAL
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Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
? A-1 Cr)
E E. Ti
SUMMARY OF ANGULAR GAIN FUNCTIONS.
ANGLE
' SAMPLE
CODES
K
AC...1A
AC.....18
AC-3A
AC-38
AC.....10A
AC......105
0
1.245
1.320
8.302
2.368
1.934
1,587
5
1.220
1.240
5.977
1.902
1.896
1.746
10
1.164
1.207
1.826
1.860
1.876
19746
15
1.164
1.201
1.652
1,839
1.876
1,667
20
1.133
1.188
1.635
1,807
1.867
1.587
25
1.071
1.161
1.627
1.797
1.838
1.572
30
1.009
1.135
1.618
1.786
1.828
1.572
35
.971
1.108
1.602
1,765
1.809
1.564
40
.934
1,089
1.585
1.754
1,780
1.548
45
.909
1.069
1.569
1.733
1.760
1,540
50
.884
1.049
1.544
1.680
1.731
1.524
55
.853
1.016
/o502
1.638
1.712
1,476
60
.822
.983
1.461
1.564
1,654
1.429
65
.784
o924
1.403
. 1.448
1.547
1,341
70
.716
.844
1.303
1.226
1.451
1.143
75
.629
0666
1.162
.655
1.267
o698
80
.498
0277
0880
.031
.832
.063
85
.199
.013
.132
.010
.038
.007
90
.000
.000
.000
.000
.000
.000
TS
.372
.403
c640
.599
o687
.546
T45
.149
.166
.253
.261
0266
0232
TSP
.363
.186
.095
0048
0048
.072
ABS
numt FalTIPAL
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
-
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
cip) A-2
CONFIDENTIAL
ANGLE
.
SUMMARY
OF ANGULAR GAIN FUNCTIONS
SAMPLE CODES
AC-12A
AC-128
AC..'./.513
AC....16A
0
11.040
170462
0984
1,025
1.492
1,798
5
6.127
6.984
1,033
1,025
4.462
1.816
10
2.870
4.755
.984
1.015
1.462
1.906
15
1.913
3.715
.969
10015
1,455
1.942
20
1.352
30120
m964
1.025 .
1.440
. 1.879
25
1.002
2.675
o964
1,025
1,432
1.762
30
.772
2.377
0934
1.000
1.410
1.690
35
.634
2.154
.934
.984
1,402
1.582
40
0542
1.932
o934
.984
1,380
1.510
45
6469
1.783
.915
0974
1.358
1,438
50
.404
/0709
.915
0943
1.335
1,366
55
.377
1,560
.885
.933
1,298
1,303
60
0349
1.486
0846
.902
1.253
1.222
65
.322
1,367
.826
0871?
1.193
10150
70
.290
1.263
.782
.810
1,104
1006/
75
0248.
1.070
0688
0707
0955
0935
80
.187
.817
0580
0574
.701
.755
85
.018
.445
41236
-.256
.119
8449
90
.000
.000
0000
0000
0000
0000
TS
.252
0790
0376
.394
0534
0586
145
.160
0387
.138
0146
0206
.244
TSP
0572
0190
0036
.048
0143
.238
ABS
CONFIDECIAL
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
ANGLE
K
AC.-.1.6C
SUMMARY
ACI7A
OF ANGULAR GAIN FUNCTIONS
SAMPLE CODES
AC17B AC-18A
AC.....188
AC-19A
0
1.388
1.224
0883
1.585
2.462
10505
5
.1.388
1.224
.883
1,585
2.425
1.520
10
1.402
1.224
0892
1.585
2,339
1,520
,
15
1.388
1.218
0883
1.577
2.277
1.513
20
1.374
1.212
0874
1.577
2,216
1.513
25
1.374
1.193 ?
.874
1,569
2.142
1.505
30
1.354
1.181
.870
10569
2.056
1,505
35
1.340
1.175
.865
1.561
1.994
1.498
40
1.333
1.175
0856
1,553
1.920
1.490
45
1.306
10175
.847
1,537
1.846
1.483
50
1,292
1.151
0843
1,521
1.797
10475
55
1,264
1,126
0829
1,497
1.723
1.430
60
1,209
1.095
0784
1.458
1,662
1,385
65
1,161
1.065
.757
1,394
1.600
1.324
70
1.072
0998
07/2
1.299
1,480
1,234
75
0934
.881
0631
1.141
1.305
1,084
80
0673
.600
.541
.824
.985
*767
85
0192
.036
.351
.158
.443
0180
90
0000
0000
.000
.000
0000
0000
TS
0519
0460
o352
.611
.756
0585
T45
.198
0174
0127
.228
0302
.219
TSP
0072
.143
0/19
.036
.024
.048
ABS
tsf..
CO HOME 1.
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Co)
CONNIE-FON,
ANGLE
K
AC-198
SUMMARY
AC,...20A '
OF ANGULAR GAIN FUNCTIONS
SAMPLE CODES
AC....208 AC...'21A
AC...218
AC-24A
1.897
. 1.431
1.447
1.508
1.578
1.467
5
1.887
1.416
1.447
1.390
1.499
1.248
10
1.887
1.416
1,433
1.404
1.484
1.241
15
1.878
1.402
1.418
1.412
1.477
1,241
20
1.868
1.388
1,404
1.419
10460
1.234
25
1.849
1.388
1.389
1.419
1.460
1.227
30
1,840
1.345
1,375
1.419
1.436
1.220
35
1.821
1.330
1.346
1.419
1.436
1,220
40
1.811
1,316
1.332
1.412
1.421
1,200
45
1.792
1.330
1.317
1.397
1.405
1.193
50
1,754
1.288
1.303
1.375
1.373
1.172
55
'1.716
1.273
1,245
1.345
1.357
1o131
60
1.659
1.202
1,187
1.301
1.326
1.083
65
1.582
1.166
1.129
1.249
1.255
1,028
79.
1.487
1.059
6999
1.168
1.184
.925
75
1.334
.930
.709
1.027
1.026
.795
80
1.087
.744
.159
.739
.773
0603
85
.533
.214
m000
0088
.157
m192
90
.000
.000
.000
.000
.000
.000
TS
.729
6523
.476
.548
.559
.464
T45
0268
0198
.200
.206
.211
6178
TSP
.036
.036
.024
.206
.186
6286
ABS
ECKFIE-H71811,
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08 : CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Ca) A-5 Cm)
E HEIDENTIAL
SUMMARY 01- ANGULAR GAIN FUNCTIONS
ANGLE
K
AC-24t3
AC-268
SAMPLE
AF'-1A
CODES
AF-1B
AF 2A
AF-2B
0
1.402
2.140
1.134
1,260
1.901
0925
5
1.388
2.119
.954
1.118
1.799
.883
10
1.374
2.087
0850
1.089
/0735
0879
15
1.367
2.034
.831
1.071
1o679
.869
20
1.381
1.971
.803.
1.059
1.642
.865
25
1.374
1.907
0779
1,036
1.587
0851
30
1.360
1.865
.765
1.012
1,513
0846
35
1,318
1.801
.746
1.006
1,449
.832
40
1.346
1,748
0727
.989
1.393
o823
45
1o325
1.695
0699
.971
1.329
.814
50
1,297
1,642
.680
.959
1o236
0805
55
1.262
1o579
.652
.930
1.144
.795
60
1.206
1.515
.614
.900
1.070
.791
65
10164
1.420
0576
.871
.904
.786
70
1.052
1.314
.524
.818
.710
.763
75
0925
1.144
0453
.741
.452
.740
80
o715
.847
.340
0618
.184
0675
85
.378
.254
.170
.441
.005
.462
90
m000
0000
0000
0000
0000
0000
IS
0528
.0673
6278
0409
0457
.364
145
0198
.272
.112
o149
0221
.123
TSP
.119
.072
6428
0238
6190
0048
ABS
ENIREITIITAL
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
A-6
C NFIDENTi
SUMMARY OF; ANGULAR GAIN FUNCTIONS
ANGLE
K
AF-3A
1.898
i0403B
1.053
SAMPLE
AF-4A
1.878
CODES
AF-?4S1
.678
.000
0000
5
1.788
1.001
1.803
.678
0000
0000
10
1.659
.990
1.737
.678
o000
.000
15
1.548
o969
1.615
0678
o000
.000
20
1.465
0969
1.568
0671
.000
0000
25
/0391
0937
1.474
.678
.000
.000
30
1.308
0927
1.399
.674
0000
.000
35
1.262
.927
1.286
0657
0000
.000
40
1.179
0916
1,183
0671
m000
0060
45
1.124
.906
1,089
.644
0000
0000
50
1,041
o895
0995
0650
0000
0000
55
0958
0874
.901
0630
o000
0000
60
0884
0858
0751
.623
0000
.000
65
0746
0843
0563
.589
0000
0000
70
0663
0821
0460
0545
0000
0000
75
0534
0769
0216
0494
0000
m000
80
0368
.679
0037
.393
0000
.000
85
o184
*495
.018
.250
0000
.000
90
0000
0000
0000
0000
.000
.000
TS
*418
.395
.365
.270
0000
0000
145
.195
0137
0201
0097
0000
0000
TSP
.142
.047
0047
.024
ABS
? CONFEDEFilt.
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
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Declassified in Part - Sanitized Copy Approved for Release 2012/11/08 CIA-RDP79B00873A002000010081-3
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Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
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Declassified in Part - Sanitized Copy Approved for Release 2012/11/08 : CIA-RDP79B00873A002000010081-3
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Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
"SA/Ara ak ? rim rm. mei MI Ili
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79800873A002000010081-3
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s, Declassified in Part - Sanitized Copy Approved for Releasie 2012/11/08: CIA-RDP79800873A002000010081-3
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Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
E NF1 all I
APPENDIX B
SUMMARY OF LIGHT SCATTERING DATA ON
COMMERCIAL REAR PROJECTION SCREENS
CONFIDENTIAL
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
B-1 Co?
CONFIDEITIAL
SUMMARY OF ANGULAR GAIN FUNCTIONS
ANGLE
K-
DA...?TEX
SN-.^2.148
SAMPLE
SN....2149
CODES
HITRANS
S...50R
LS..-40FM
0
8.220
640451
1.209
25.059
3.696
5.789
5
6.740
47.049
1.185
17,416
3.548
5.123
10
5.507
22.557
1.197
10,274
'30142
4.382
15
4,192
10.312
1.185.
5.638
2.809
3,473
20
3,164
4,511
1.179
3,508
2.476
2.865
25
2,507
1.933
1.148
2,505
2.236
2,258
30
1.972
.966
1,160
1.854
2,033
1.852
35
1,602
0644
1,148
1.503
1,848
1,459
40
1.315
.322
1.124
1,303
/0681
1.215
45
1.068
0257
1,118
1,227
1.552
1.013
50
0904
6193
1.112
1,052
1.423
.839
55
.739
.128
1,076
1.027
1,330
o694
60
.657
.064
1,027
1,002
1,256
.607
65
6534
.000
.991
1,002
1.182
0521
70
.493
0000.
6919
/0002
1,127
0463
75
.411
.000
o76/
1,002
1,072
.347
80
.328
0000
.362
.977
1.035
o318
85
.287
.000
0024
.952
.961
.289
90
0000
.000
000,0
.000
0000
6000
IS
0528
o637
.426
.775
.700
.475
145
o344
.619
.168
.439
0308
.302
TSP
.000
.000
0000
.000,
0000
.000
ABS
CONFIDENTIM
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized. Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
B-2
SUMMARY OF
FCTIONS
ANGLE
K
OC??-50FM
LS?==60FM
SAMPLE
LS6OBFM
CODES
LS?==.606
LS....60NG
LS..60PL
0
10.340
4.873
10.596
3.823
5.491
6.026
5
8.685
4.532
9.166
3.670
5.656
5.935
10
7,445
4.020
6.993
3.364
5.162
5.544
15
5.945
3.435
5.192
2.867
4.366
4.700
20
4.756
2.924
3.963
2.408
3.459
3.856
25
3.722
2.534
3.020
1.949
2.636
3,103
30
3.060
2.144
2.384
1.605
2.086
2.470
35
2.481
1.754
1.907
1.280
1.537
1?928
40
2.026
1.540
1.536
1.032
1.208
1.506
45
1.706
1.315
1.292
.841
o961
1,205
50
1.447
1.169
1.102
.688
.768
.934
55
1.240
.999
0964
.573
.604
.705
60
1.075
.877
.858
.458
.466
*542
65
.982
.779
*794
.305
.356
.397
70
.827
.682
.688
.248
.302
0301
75
.620
.609
.635
.229
.247
.271
80
.620
*536
.529
.229
.192
.241
85
.723
.487
0413
.152
.164
.210
90
.000
.000
.000
.000
.000
o000
TS
.825
0588
.675
0375
.475
.550
T45
.508
.331
.424
.252
.342
.395
TSP
.000
.000
0000
.000
.000
.000
ABS
CARMEN
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
fts.) B-3
commnrarm
SUMMARY OF ANGULAR GAIN FUNCTIONS
ANGLE
K
LS6OSTG
LS*60VR
SAMPLE
LS-75G
CODES
LS*85PL
LUX-50
LUX-70
0
5.803
8.769
29.135
760821
100374
6.186
5
5.223
8.418
21.559
43.020
9,544
5.691
10
4,642
70366
14.276
2105/0
7.366
5.103
15
3,540
5.814
8.157
,90218
5.446
4.206
20
2.698
4.472
4.661
4,993
30942
3.371
25
2.060
3.358
2,913
3.072
2080/
2,814
30
1.508
2.455
10893-
1,920
2,074
2.289
35
1.102
1.771
1.340
1.152
1,452
1.825
40
0812
1.359
1.019
.921
1.141
1.515
45
.620
1.0052
0699
0768
.881
1.237
50
.487
0833
0640
0614
0726
1.082
55
.377
.631
.582
.384
0601
0897
60
03/3
.526
0437
0307
0497
0804
65
o237
0420
0291
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.414
0711
70
.203
0350
0174
0153
.394
0649
75
.145
0333
0087
0076
0363
0606
80
0116
.263
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.076
0331
0556
-
85
0087
0245
0000
0000
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90
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0266
0434
0529
0670
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0000
0000
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ABS
EMMET:MR
, Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
C DENTPAk
SUMMARY OF ANGULAR GAIN FUNCTIONS
ANGLE
:I(
,
RAVEN
TYPE 1
SAMPLE
TYPE-4
CODES
VCA3606
TR....50PL
0
4.965
23.094
6.730
36,758
2.412.
.000
5
4.320
19,399
5.922
16,357
2.412
.000
10
30972
14,780
4.643
6.432
2.340
.000
15
- 3.376
10.392
3,365
3.675
2,219
o000
20
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7.043
2.355
2.462
2.087
0000
25
2,507
4.849
1,749
2.021
1.978
.000
30
2.085
3.348
1.211
1.837
1.833
.000
35
1,787
2.309
0874
1.543
1.713
.000
40
10489
1.732
0639
1.470
1.592
.000
45
1.29/
1.270
.47/
1.396
1,483
0000
50
1.092
1,039
.403
1.360
1.387
.000
55
.918
0808
0269
1.323
1.278
.000
60
.819
.577
.201
1.286
1,201
G000
65
.720
.461
.134
1.249
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.000
70
0645
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.000
1.213
1.025
.000
75
.571
'c000
0000
1.176
1.013
0000
80
.496
0000
0000
1.102
.880
.000
85
.347
.000
.000
1.102
0048
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90
.000
.000
.000
0000
.000
.000
IS
.563
.820
0280
.775
.600
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145
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0236
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.270
0000
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ABS
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,? Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
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Declassified in Part - Sanitized Copy Approved for Release 2012/11/08: CIA-RDP79B00873A002000010081-3
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