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TECHNICAL TRANSLATION 



MSA TT F-13,892 



SOME RESULTS OF SPECTROPHOTOMETRIC MEASUREMENTS OF THE EARTH 
FROM THE "SOYUZ-7" SPACECRAFT 

K. Ya. Kondrat'yev, A. A. Buznikov, B. B. Vinogradov, 
V. I. Volkov, V. V. Gorgatko, 0. I. Smoktly and V. M. Orlov 



Translation of: "Nekotoryye rezul'taty 
spektrofotometrirova niya zemli s kos micheskogo 
korablya 'Soyuz-7' ".{Akademii 5lauklpokladyl SSSR 
Vol. 195 (5), 1970, pp I08U-IO8V 



^72-U36 8 



Unci as 
1173 7 



IffCTHopHOTOHETlt^ ^°"^ RESULTS op 

CSCi. 




MTIOML AEROMUTICS MD SPACE ADMINISTRATIOK 
WASHINGTOW, D.C. 205^+6 NOVEMBER I97I 



Reproduced by 

NATIONAL TECHNICAL 
INFORMATION SERVICE 

Springfield, Va. ,22151 



SOME RESULTS OF SPECTROPHOTOMETRIC MEASUREMENTS OF THE EAR'iH 
FROM THE "SOYUZ-7" SPACECRAFT 

K. Ya Kondrat'yev , A. A. Buznikov, B. V. Vinogradov, V. I. Volkov, 
V. V. Gorbatko, 0. I. Smoktiy, and V. M. Orlov* 

ABSTRACT. It is found that spectrophotometric measurements 
from "Soyuz 7" made it possible to compare data on reflectivity, 
radiation temperature, and other reflective and radiative 
characteristics of the Earth's surface. 

The first experiments on spectrophotometric measurements of the twilight /1084 
halo of the Earth from space were made in January, 1969, during the flight o f tpre 
"Soyu2-5" spacecraft. The basic results of this experiment were discussed irK 
the papers [1-4]. With the combined flight of the spacecrafts "Soyuz-6,7,8", 
the program of complex optical experiments was broadened to include the solu- 
tion of the following basic problems: 

1. Spectrophotometric measurements of the sun and the twilight halo of 
the Earth's atmosphere under various observation conditions, solar radiation, 
and the position of the observer in space in order to study the brightness 
and colors of the halo, and to determine the vertical. distribution of various 
atmospheric components . 

2. Spectrophotometric measurements of various natural formations with the 
goal of determining the feasibility of identifying them from spectral reflec- 
ting characteristics, measured from space. 



** 



* 
Associate member of the Academy of Sciences. 

Numbers in the margin indicate pagination in the original foreign text. 



3. Synchronous execution of a complex program of earthbound and airborne 
optical investigations of the atmosphere and of various types of underlying 
surfaces in the region under the satellite for obtaining data which would 
characterize the spectral transmission function of the atmosphere, spectra, 
and spectral contrasts of natural formations as a function of the basic optical 
parameters . 

]> .^- Spectrophotometric measurements of the twilight atmosphere and the 
underlying surfaces were made from the "Soyuz-7" spacecraft by means of ^ 
modified manual RSS-2 spectrograph(v^[5] . The input telescope objective simul- 
taneously focused the image of the distant object at the input slit of the 
spectrograph (spectrograph channel) and directly on the photographic film 
(photographic channel). The focal distance was f — 135 ram; the relative 
opening was D/f = 1:4. For this model of the spectrograph, the linear dis- 
persion was 166 A/mm, the spectral width of the slit was 50 A, and the spectral 
range for measurements was 430 to 690 my. The limiting angular resolution of 
the spectrographic channel was 2 minutes of arc; that of the photographic 
channel was 4 minutes. The spectra were reduced using the method described in 
[4]. 

This experiment [1] did not evaluate the effect of the spectral transmis- 
sion of the solar radiation through the spacecraft illuminator. Evaluation of 
this quantity ahead of the spectrograph objective was carried out by installing 
a light-scattering filter with known optical characteristics. Then the appa- 
ratus was pointed at the Sun. 

Photographic film in the spectrograph was exposed to a standard source 
and the Sun using the light-scattering filter. The darkening densities of 
the photographic films from the two sources were compared. The comparison 
made it possible to find the spectral illumination of a unit area, which gave 
the solar illumination transmitted through the spacecraft illuminator. 



During the group flight of the "Soyuz-6,7,8" satellites, spectrophotometric 
measurements of the twilight halo were taken on the 87*^ revolution of "Soyuz- 
7". at 21A7 hrs Moscow time as the sun set. The geographic coordinates of the /1085 
spacecraft were 23.18" north latitude and 23.39° east longitude (in the region 
of northeast Africa) . The altitude of the orbit at the moment of the experi- 
ment was approximately 218 km. 

The results of the experiment were compared with similar data taken during 
the flight of "Soyuz-5". The comparison showed that the qualitative behavior 
of the monochromatic curves of the halo brightness was the same for both 
experiments. However, the absolute values of the brightness in the first 
experiment [1] were 2 to 3 times smaller (A = 650 my). The monochromatic 
', brightness curves of both the previous experiment and the current experiment 
'; showed an absence of noticeable depressions^ caused by aerosol layers, locali_zed . . ^^ 
j at various levels in the atmosphere. 

-^ This communication also presents data on the spectra of various natural 
^urfaces,/ which were obtained on October 13, 1969 from "Soyuz-7" on the tra- 
jectory from the Arabian peninsula to the Aral Sea. Spectrophotometric measure- 
ments of various parts of the Earth's surface were made in a short period of 
time from 1319 hrs to 1329 hrs, Moscow time, for a solar height of 35-50°. 

During the flight of "Soyuz-7" spectra were obtained on the following 
identified types of natural surfaces: 1) thick clouds, 2) thin clouds, 
3) rocky wilderness, and 4) cloud shadows (Figure la). Continuous and dense 
cumulus and stratocumulus clouds are characterized by a maximum brightness in 
the range of 0.20 to 0.24 watt/m -mysteradian in a wavelength range of 440 
to 580 my (Curve 1, Figure la). The brightness significantly decreases to 
0.14 to 0.14 watt/m^ 'mysteradian in the orange-red part of the spectrum 
for X = 580 to 690 my. Thin clouds of the high-altitude stratus and strato- 
cumulus types at various levels give an integral image for a cloud layer and 
for shaded surface. This type of surface has little effect on the spectral 
distribution of the brightness, but its absolute brightness is lowered to 



2,11 



1.0 

4 

■0.1 



2,i 



J/}) — 'm HI ko mm ; "^0 Ifo no m oiOK^ 
}, — _. r f. — 





Figure 1. Curves of Spectral Brightness B (watt/m • 
mysteradian) for ten natural surfaces obtained on 
October 13, 1969 during the flight of the "Soyuz-7" 
spacecraft, a - from the spacecraft: 1 - dense 
clouds; 2, 3 - thin clouds; 4 - surface of the desert 
in the northern part of the Arabian peninsula; 5 - O 
surface of the desert on the Ust Urt plateau at the 
eastern bank of the Caspian Sea; b - from an air- 
craft: 1 - thick clouds, 2 - thin clouds, 3 - sand, 
4 - salt marsh, 5 - rocky wilderness, crossed by 
dirt roads, 6,7- rocky wilderness. 

0.12 to 0.14 watt/m -mu'steradian in the interval \ - 440 to 480 my, and to 

9 

0.07 to 0.1 watt/m -mysteradian in the interval X = 580 to 690 my (Curves 
2 and 3, Figure la). 

The rocky wilderness of the Ust-Urt plateau is composed of limestone 
and is covered with a rough gray loamy stoney soil. In places there is takyr 
soil and thin dusty-sandy deposits. The plant covering is sparse, and has little 
effect on the spectrum of the landscape. Underlying surfaces of this type 
yield spectral brightness curves with very weak spectral intensity changes 
in the range 0.05 to 0.07 watt/m 'mysteradian (Curves 4 and 5 in Figure la). 



Finally, it is interesting to analyze the darkest, spectrophotometrically 
analyzed surfaces — regions of ilight shadows from clouds. Since the 



shadows were discontinuous, their brightness was much lower than was the rocky 

2 
wilderness (0.04 to 0.05 watt/m •mysteradian) . The differences were signif- 
icantly less in the blue-green region of the spectrum than in the red-orange 
region. 

The spectral contrasts were calculated from data given above on 
spectral brightness in all possible combinations of natural surfaces (Figure 
2a). 

The spectral contrasts of the cloud density and the partially shadowed 
surface of the rocky wilderness reached maximum values of k = 0.77 for X = 630 
my. This contrast was somewhat lower in the blue-green region, where k = 0.62. 
The spectral contrasts of the dense cloudlines and of the rocky wilderness 
also gave high absolute values of k between 0.6 - 0.7. The changes in the 
contrasts were the same over the entire curve or decreased in the short-wave- 
length part of the spectrum (Curves 1 and 2 in Figure la) . The spectral 
contrasts for the thin clouds and the rocky wilderness had an analogous 
brightness pattern. However, the absolute values of the contrast decreased /1087 
to about 0.4 (Curves 3 and 5, Figure 2a). Moderate contrast values arose 
from thick and thin clouds (Curve 4 in Figure 2a). The shape of the curve was 
monotonic, with variations of k in the range of 0.40 to 0.45. The spectral 
contrast of the illuminated and shadowed rocky wilderness was also rather 
small (k ^ 0.3). Here the contrast was significantly decreased in the short- 
wavelength region of the spectrum, and increased in the long-wavelength region 
(Curve 6, Figure 2a). The contrasts between distant parts of the rocky wild- 
erness were the least, k = 0.05 to 0.15 (Curve 7, Figure 2a). The contrast 
was higher in the green-blue region of the spectrum for X = 520 my, as well 
as in the red region for X = 660 my. 

These results were compared with simultaneous measurements of the 
brightness and the contrasts, which were made with analogous equipment (RSS-2) 
in an airplane flying over the Ust-Urt plateau at the "meeting point" of the 




^'^X^.^^^f^s^ 






0,tl 



3 V 




0.5 

0,6 

"0,1 

0.2 

0.1 



-0.1 




A 

7 0!,'^^., 



"o , « ; ..«' I''..-- 



filr^JOO 600 *fji '700 



Figure 2. Spectral contrast (K) curves for natural 
surfaces. These curves were obtained from spec- 
trophotometric data from the flight of the manned 
spacecraft "Soyuz-7" on October 13, 1969. a - 
from the spacecraft: 1 - dense clouds over the 
Arabian desert, 2 - thick clouds over the Ust-Urt 
desert, 3 - thin clouds over Ust-Urt, 4 - thick 
clouds and thin clouds , 5 - thin clouds over the 
Arabian desert, 6 - illuminated Arabian desert, 
7 - illuminated desert, partially shadowed (Ust- 

. Urt) . b - from an aircraft: 1,2 - thick clouds 
over a rocky wilderness, 3 - thick clouds over 
loamy rocky wilderness, crossed by roads, 4 - 
thick clouds over a loamy-stoney wilderness, 

.5,6 - loamy-rocky wilderness, crossed by roads 
— rocky wilderness, crossed by roads, 7 - loamy- 
stoney wilderness loamy-stoney wilderness, . 

crossed by roads, 8 - loamy-stoney wilderness — 
rocky wilderness, 9 - two sections of the rocky 
wilderness on the Ust-Urt plateau. 



spacecraft and the scientific-research, airplane. Spectrophotometric measure- 
ments were made from the satellite at an altitude of 220 km, and from the 
airplane at about 2.7 km. Comparison of the satellite results (Figures la 
and 2a) and the airplane results (Figures. lb and 2b) for the measured spec- 
tral brightness and contrasts of the same types of underlying surfaces show 
that the effect of the haze on the optical characteristics was small as ' 
compared with the measurements made at 2.7 km. The haze effect is more 



important in the short-wavelength region of the spectrum, as should be 
expected. In the long-wavelength region, the solar radiation scattered by 
the atmosphere above 2.7 km only slightly affects the absolute brightness 
values of natural surfaces. 

In conclusion, it should be noted that the shape of the spectral 
brightness curves of natural surfaces makes it possible to differentiate 
several types of natural formations from their spectra, which are measured 
from spacecraft. It should also be emphasized that the atmosphere distorts 
the shape of the spectral brightness curves and lowers the spectral contrasts. 
However, the optical density of the Earth's atmosphere is not very large, in 
the absence of clouds. Thus it is possible to compare data on reflectivity, 
radiation temperature, and a combination of other reflective and radiative 
characteristics of underlying surfaces. These comparisons give a rather 
precise differentiation of natural formations based on their spectra. 



REFERENCES 



1. Kondrat'yev, K. Ya. , B. V. Volyhov, et al. Doklady Akademii Nauk 

(DAN), Vol. 190, No. 2, 1970. 

2. Kondrat'yev, K. Ya. , A. P. Gal'tsev, et al. DAN, Vol. 191, No. 4, 

1970. 

3. Kondrat'yev, K. Ya. , A. P. Gal'tsev, et al. DAN, Vol. 191, No. 5, 

1970. 

4. Kondrat'yev, K. Ya. , B. V. Volypov, et al. Izvestiya Akademii Nauk, 

SSSR; Seriya, Fizika Atmosfery i Okeana, Vol. 6, No. 4, 1970. 

5. Gal'tsev, A. P., V. V. Mikhaylov, et al. Problemy Fiziki Atmosfery, 

No. 7, 1969. 



Translated for Goddard Space Flight Center under contract No. NASw 2035, by 
SCITRAN, P. 0. Box 5456, Santa Barbara, California 93108.