SCIENTIFIC ABSTRACT SOLSKAYA, L.L. - SOMIN, V.I.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R002203120011-9
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 1, 2001
• Sequence Number: 11
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

_SSING DATE-
UNCLASSI FIED P R 0 C E -27NOV70
CIRC. ACCESSION NO-- AT 0 1287919
ABSTRACT/EXTRACT-0J) GP-0- A3STRACT. THE FLOTATMN GJF GALENA, PY-'~ITE,
J.,
11TE OF -1E C 0 i"11C OF MCj'110 AiND
AND ANTI MON WAS STUDIED AS A FUNCTION T,
01THIOPHOSPHORIC AND PHOSPHIORGUS ACLOS I THE EFF,ECT '!F.Pri ON THE
FLOTATABILITY OF GALEP14A BY DIETHYL THJ~PHOS-HfIINAiTE, DIETHYL
THOPHOSPHATEt AND DIPHEP,4YL DrTHIOPHO5PHlNATli*.: OF DIFFERENT Co~jrNIS. Wj~c*
,ALSO DET0. FACILITY: INST. KH1111. OUSHAWBE, USSR.
U,'14C LA S SI f7 [ED

USSR
S-OLIS-1 and ROZGOlft M. L., Bi chemical Depaa-Went of the Central
%=oen*;O%* AaKch laboratory of the 1asokent rKedical Institute
"An investigation on tha Collulax Doval. of the Fo=atlon of Antibodler. to
Salm. Typhimurium in Hice of Various Ages"
Tashkwrt, Meditsinzkly Zhurnal Uzbekistara, Ho 10, 1,971, PP 48-52
Abstracti To elucidate the effect of age on imnunoloTica-1 reactions, 270 mice
aged I &-y to 120 days were given intraperitoneally an 1=unlzing dose (150
raillion bac-teria r,!3r 16-20 g mouse) of Sall typhimurlini containing the 0-
antigen. The anUals were sacrificed en the 4th day tdter vaceiratian, and
their spleen, cecura, and mosenteric lyTaph nodes as w3U. as ~.ierurz antibodies
were investigateCl. in the spleent the number of cellit, (per 100 karyoc~tcs)
producing, anit-libodlen to 0-itntigen did not Inmroase in 4-day old mice, Just
began to increase in 6-day old mice, ard was iAgwif iatintly Increased in III-day
old mice, resulting in a mozwumble Increane in the 4--oxum tttur of SPOO111C
antibodies. The swelfic binunologic.,J reaotion ween Ivss pronounced in
the cecun arA --esenteric lymph nodes of, young zlo~. izowever, these struc-
tures developed a Lix-ger number of calls producing arrLibodies to sheep
erythroty-tes. The nature of this cross reaction rezairw unclear.

Da 621.38~.292/52
U85R W
it, n; A.I., LEPILIN, V.A.,
ALEYSANTROV, I.R., DUXArzV;,XAYA,' N.V., KL
-0V, V.I.
"Use Clf' Silicon Kaltivlier Elements In Fhotoelectron Devices"
Elektron. tekhnika. ~'muchnc-tekhn. rib. Elei:tronnoluch. J. fotcele'itr. rriborv
TEloctron4cs chnical Collectlons. Electron Beum And Photo-
Tiee-nology. Ecientific-Te
electric Dev4ces), 1970, Iasue 1(15), pp '58-61 (from M-Elektro-exika I veye
.11 .1,
prim-eneniye, N'o 2, February 1971, Abstract No 2A~4~)
led of cathode amilif-calion in silicon
Transla-lion; 71~e Dhenomonon is inves4i'ca'.
-n structures developed for hybrid photomultipliers. 'fae phenomenon con3ists of
p
the fact that durin- bombardment of a crystal with a shallow lying p-n junction by
an alectrcr, stream -dith a uower U Is, in the circuit of a backward-biased junc-
tion.,the current I = aIa 6 appears. The diffusion u-n structures with the
ence < 1 micrometer is investigated, as well as junct'ons obtained
depth of occur
by the method of ion implantation which are characterized by better reproducibility

USSR
et al, Elektron. telchnllca. Na-uchno--~-ekbm. sb.
:Eli6ktronnoluch. i fotoelerc-sr. Pribory, 1WO, Issue 1(15),
of results. The deDendences obtained for a(U.) are -presented. Lt a rramber of dif-
fusion junctions the anomalous effect is detected of cathode amplification with the
coefficient a considerably exceeding the limit which is determined by the theory
f impact ionization. (Js~ng as. an example models of a photomultiplier with silicon
o
A-
photomultiplier elements,the use or this phenomenom, in phatoelt~ctron devices is
shown. 6 ill. 8 ref. N.S.
212

USSR UDC 53.07/.08+53.001.5
MOV, U. B., ALEKSANDROV, 1. ~R., DUNAYEVSKAYA, N. V., KLIMIN, A. 1.
,�qLTAI
LEPILIN, V. A., SMIRNOV, V. I.
"The Use of Silicon Multiplying Elements in Photoelectron Devices. (Brief Note)II
Elektron. tekhnika. Nauchno-tekbn. sb. Elektronnoluch. I fotoelektr. pribory
(Electronic Engineering. Scientific-Technical Collecti4n. El'sctron Ray and
Photoelectric Devices), 1970, No 1(15), pp, 58-61 (from.'RZh-Fizika, No 1, Jan 71,
Abstract No W60)
Translation: The phenomenon ef cathode amplification In oflfxon pn-atructure-'j io
investigated. The uac of thlij phenomenon in photoeleaLr()n devices was shown in
mackups of photomultipliers with silicon multiplying elements. Authors abstract.

Now
USSR UDC 519.1
ZAMBITSKIY, D. K., Sa6T.AN...P,. S.
"Finding the Class of ~-Connectedness of a Graph"
V sb. Prikl. matem. i programmir. (Applie'd Mathematicfj and Progriuning
Collection of Works), No 1, Kishinev, Academy of Sciences Moldavian SSR, 1969,
pp 61-67 (from RZh-Matematika, No IOP Oct 70, Abstract No 10V227)
Translation: The authors solve the problem of findin$ the minimum cut in a
plane, connected, weighted graph G: i.e., sets of ar--a with minimum sum of the
weights, separation of which breaks down the connectedness of the graph. I'he
problem is essentially that of,finding.'the cycle of~minimum length in a double
graph G*; an algorithm isgiven for solving the latter. Generalizations of the
initial problem are also discussed. Ye. Dinits.
26

Acc. Nr: Re'i. Cod
AP0047766-
PRMARY SOURCEZ. Izvesclya Ak-ademii Nauk Turk-menskoy SSR, Seriya
Liologicheskikh Nauk, 1970, Nr pp ql-qS
A. Soltanoy
EFFICIENCY OF OXYGENOTIIEI~APY UNDER HYALOID TURBIDITY
Subconjunctive intraducimr, ~11` oxygen midor. variaws hyaloiO turbidities effect
,good resolving. H3v;ln(,,- recelved the fir5t course of treatmeatt resolvira of hvaloid
turbidity . and vision acuty improvement. have been ~Pb3erycd in 29 cases of 40.
The repeated course of oxyg-enotitzrapy is oflilttc effickricy. Thl-, improVement, a( yi-
sion acuty has been observed in 3 cases. of S.
"ZLIFRAME
19791387
A

Ulu UNCLASSIFIED 1~~PROCESSING DATE--30OCT70
.~TITLE-SPECTROPHOTOMETRIC METHOGFOR THE QUANTITATIVE DETERMINATION OF
FURAN ALDEHYDES AND THEIR CONVERSION PRUDUCTS IN REACTION MIXTURES -U-
AUTHOR-(03)-KULNEVICHt V.G.t SOLTOVETS*-,,G*N.t ZELtKMANP Z.I*
COUNTRY OF INF0--USSR
.~_SGURCE--KHIM* GETEROTSIKL* SOEDIN- 19701 12)v 183-4
,--.DATE PUBL ISHED ------- 70
AREAS--CHEMISTRY
.TOPIC TAGS--SPECTROPHOTOMETRIC ANALYSISt FURANr ALDEHYDEj ALCOHOL, ACETAL
~:CCNTROL t4ARKING--NO RESTRICTIONS
DOCUMENT CLASS--UNCLASSIFIEO
REEL/FRAME-1997/0747 STEP NO-, -UR/0409/701000/0OZ/0283/0284
CIRC ACCESSION NO--AP0119654
UINCLASSIFIE0

PRO'CESSING DATE--30OCT70
V2 010 UNCLASSIFIED
CIRC ACCESSION NG--AP0119654 FURAN ALDEHYDES
''ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. THE UV SPECrRA OF
PEC 'OT 01M, E TIR I C
-Mv ALCS. ill) AND ACETALS (111) WERE STUDIED. A
IT. DETN. 10F Ip Ill AriD Ill SEPARATELY OR IN THE
-14ETHOD FOP, THE QUAN
XT. POLITEKH.
-REACTION MI, WAS DEVELOPED. F.ACILITY*' KRASNODAR.
INST.~, KRASNODAR, USSR.
UNCLASSIFIED

008 WNC L AS S I F I Ef) PROCESSING DATE--- 233 OCT70
"'i TITLE--~URFURYL 41-COHOLS F~~OM TiE COP R[~'10,11101 l,"G ALOEHYDES -U'-
AUTHOR-(04)-SMIPNOV, V.A., KULNEVICHt V.G., 5OLTOVETS, G.tl.r SEMCHEN;Kct
D.P.
':COUNTRY OF INFO--USSR
SOURC GER GFFEN. lit303#373
--14MAY70
DATE PUBLISHED
-.-,..,SUBJECT AREAS--CHEMISTRY
'-~TOPIC TAGS--CHEMICAL PATENT, FURFURYL ALCOHOLv ALDEHYDEr ORGANIC
SYNTHESIS, PENTOSE, HFXOSE
CONTROL WARKING--NO RESTRICTIONS
00CUMEINT
CLASS--UNCLASSfFIED
,-,-,.PROXY REEL/FRAME-1997/1422 STEP NO--GY/0000/70/0",)0/00~J/00~)0/0000
CIRC ACCESST0,10 NO--AA0120210
UNCLASS IF IED

212 008 UNCLASSIFIED PROCESSING 0ATE-230CT70
-CIRC ACCESSION NO--AA0120210
AaSTIRACT/EXTRACT-W) GP-0- ABSTRACT. FURFURYL ALC~, ( It R EQUALS 11, 04
SUB2 0H, ?4F, RR, Ok CL) WERE PREPD, IN 90-IMPERCENT t YI ELI) tl'~ TR~ATING
THE CORRESPONDING ALDEHYDES ( I I ) W['Tli NA AMALGAik~ AtL) PASSING CO S'J32.
AQ. SOL'NS., AQ. ALC. SOUNS., OR SOLNS. oBrAINED, F-R(.;?,r THE HYDROLYSIS OF
PE-',,lT0SX?l5 OR -DEHYDRATED HEXOSE WERE, USED~AS S(]Ltq!;. OF 11. THUS, A
3.34PERCENT AQ. SOLN. OF 6.99 G I (R EQUALS. CHO) WAS ADDEO TO 0.1 L.
2.35N NA AMALGAM AT A RATE DF 16 ML-4tlN AT 18DE131REES AND GO SUBZ WAS
BLOMiN THROUGH AT 45 L.-HR TO GIVEN 6,,3- IG I tR EQUALS CH SU!52 0H).
FACILITY: OROLHONIKIOZE# S.t POLYTECHNIC INST17UTE iNOVOCHERKASSK AND
KRASNODAR POLYTECHNIC INSTITUTE.
UNCLASSIFIED

112 0 14 'lJN,,,CLASSl FTFO PROdrM Mr. lls!TE--11SFPT0
T'%TLE--DlFFR4CTlCN ~__'F A TWO 91MENSIONAL ELECTROMAGNETIC WAVE UN DIELE-1-IT-kic
CYLINDER WITH AN ARRITRARY SHAPE, OF THE: TPANISVERSE SfCTION _V.-
AUTHOR-02 I- _lL -V V.V., VASTLYEV, Y~a*N*
lul"i-yid-1
~-EOMUY OF INFO--USSR
~_SOURCE-ZHUKNAL TEKHNICHESK01 FIZI'Kls VOL, 40,s JAI44 lq70j P 47-53
~D 4TE PUBL ISHED ------- 70
S.UBJ EC TAREAS-PHYS Ics
"TORIC TAr~S-ELECTROMAGNETIC i4 -AV EDIFFRACTION, ELECTK)MAGNETIC ooAVF
-PHEK~MENON
`C01tTAr'L PFST~ICTI`0
0 d.C UA F NT C L A S 5 - - U N C L A S S I F 1 E 0
-:PROXY STEP N(j--UR/00.5?/70/-,:4j 09471 D,_ 53
CIRC ACCESSIIN NU--AP0047940
UNCLASSIFIED

UP-11C L A S S I FI E 1) PRIMESSI~1"~
CIPC
AF3ST;:AC.T/=-XT~4.ACT--0)f ABSTPACT. SqLUTIGN CT THa P; C~3L E M
D F P~ A C T 10 % OF A T -w 01 M E,%, S I ON AA L FL EC T R 0!,, 4G NIE T I C - ,,.i A vE- r)N. A
DIELECTRIC CYLINOER WITH. AN ARBM~ARY SqAVE USING A SYSTEM '7V
a E;~UATIOCNS WITH !RESPECT TC THE ElUIVALENT CURREINT-S ON VH71: CYLINDRICAL
SURFACE. THIS EQUATION SYSTEM IS SOLVED USING A 01GITAL tOMPUTER.
EXAM-PLES ARE-PRESENTED FOR ILLUSTRATING THE METHGO USEDt A-140 A
COMPARISON WITH THE RESULTS OBTAINED BY OTHER MET1400S 15 PRESENTED.
UNCLASSIFIED

USSR LU)C 612.858-76
ces Ukrainian SSR, Kiev
WILKFA, B. V., Institute of Zoology, Academy of Scion
"Soun(i Location by Naz Under Water"
Moscow, Doklady Akademli Nauk SSSR, Vol 213, lio Iv J973, pp 246-246
Translationt To assess the possibility of man's locating sound sources under
water, it waa necessary to perform a succeasion of experiments to studyl (1)
the rechanism of reception of sound oscillationsl (2~~ location of a single sound
source' (3) location of a si&Aal. source during interferttmce.
With a piezoelectria emitter pressed against thil) skini, acoustic oscil-
lations vere excited in the tissues of the hewli and the thretsholds of percep-
tion were deter,-ined. Harronic signals at,frequencies of I alid I ],_9z wore
'0
studied. The thipsholds were lowest when tho mastoid p=cess, tOMDOral and
submaxillary regiona, and lateral surface of the neck we~~a stimulated.

USSR
ITO 1973, pp 246-248
SOLIUKHA, B. V., Doi-lady Akademii Ilauk SSSHt Vol 213t
v
b
6
t
Fig. 1. Distribution of areas with the lowest
threshold of excitation upon tactile atimulation,
which correspond to the pattern of,,rece4ion of
P
sound oscillations under ittLterp a, b, dt zones
which differ in tbreshold,~,by 3.db. 1) t~Lctiljt
stimulation at a frequoneyof I hHZI 2) '4A 30 Ift.
2/8

USSR
SOLUKHA, B. V., Doklady Akademii Nauk SSSR# Vol 213# Ho 1, 19731 PP 246-248
The thresholds for remote stimulation in water and tactile stimulation in air
coincided. Deatherage /-4 7 6howed that persons submorged In water and ex-posed
to an ultrasonic f ield behaved as though they sensed rotimniil%sttion by bone con-
duction. In our experiments, the thresl.lQlds correspoilding -to etimulaticn of
bone structures and soft tissues differed only slightly.
Thust it is fair to say that round is cDnductOd in water by tiazue
structures, which are a distributed receiver with a charactoristics size of
about 0.2 m.
Then using threshold mathols we determined radiation patterns of tl-~c
so=d system for harmonic slEnals of 0.25, Is 10, 15, and 110 k1fz. The results
were averaged for the number of subjects, and numter o 'I exporlmorits with each
subject. The pattern showed an industinot =iximura oZzily at frequencies of
15 and 30 kJiz duo to diff raction. The absence of directivity at the rvinainin'T
frequencies is in agreenont with the conclusions of lfo2lien an-ft Rothman fg.-
However# the differentiation of signals from sources lod(Ltad to the left or
right of the sub.-Jecta was qUlte DVNIOILYI,~-od for suprallml-11al ilgnals at both
audio and ultrasonic frequencies.
The ability to locate nound Bources under vater auggoul:3 the prenence
in man of psychoacouctic phenomena doscribod in 1-17 uith algorithtua similar
3/8

USSR
SOLUKHA, B. V., Doklady Akadexii Nauk SSSR# Vol 213, No 1, 1973, pp 245-248
to those mentioned in ff. To check thia assumptioni. we parTormed art experi-
jaent in water to detect a signal against a backr~round of intorference uith
some differences in the spatial location of the signal sources and Interference,
but with an equal Bignal-to-interference level xatio. A zilxlure of and
noise was supplied to two spherica emitters. The siGnal was harmonic or
pulsed with harmonic filling, The interfference was a thezril noise ranging from
50 to 20,000 Hz,-or almost an order higherthan the width of -the critical
frequency band 27.
no
)IN" Pig
-1 rg
4/8
PSIC"
2
2

USSR
SOLUKHA, B. V., Doklady Akademii Mauk SSSH., Vol 213, Ica 1, 11073, pp 246-248
Fig. 2. Directivity patterns for hm= threshold signals in
the water. Zero de6raes corresponds to the 1xisitian when the
subject Is looking directly at the radiator; the nunber repre-
sent frequency In kHz.
Fi 3 Relationship between frequency (f) and the probability
(P~Oof'differentlatlng sources of audible and ultraaania
oscillations from sosrces located at the left tind right of a
subject (900 and 270
We determined the probability of detecting the signal amvinst P, noise Iac"t-
ground durine the e~.ission of the total signal and noi*3 components by each of
the two emitters, With ar., harzonic signal at a frequency of 10 kft, 'Che pro-
bability of detection was 0.84 but with a mdJo
1~ pul$,e siTnal at a freq-uency of
10 PYz lasting I mse,~- ~md a repetition froquency of 10 Fizz, the probability
was 0.75. Then the sii7nal alone Waz supplied to one of the eml-Cltters and the
noise alon-e to tlae Other emitter (the probability of detection for the harmonic
emd radio pulse signals was 0.95 and 0.94, respectively).

USSR
SOLWA, B. V., Doklady Akademii Naulc 55SRi Vol 213, 1vo t, 1973, pp 246-248
The noise level and signal-to-noise ratio In the 2:onD of reception was
set the same way as in the D1,0ceding case. If the acoustic system does not have
the capacity for space and tire analysis (i.e., if it is Incapable of taking
into account the relative coordinates of ~the signLl source ;md interferenct
source and only the energy characteristics of the sigyiaA wid interference are
inforrational), the probability of detecting the signal against the noise
background must remain as before because the ratio did not
change. However, the probability of detection increas,9d.; tile difference was
much greater than the possible accidental deviations. It ia interesting to nete
that when the signal and noise were supplied to the receivers at the same t1jre.
the subjects detected the sip,-nal from the Increase in noUe lovell but Ath
spatial depa=tion of the signal and noise# they xvadily diatijiguishad tile
sigma and could avon differentiate somewhat the filling frequency.
Thus, man's acoustic systen under water possesn6s tho capacity for
spatial and temporal, anutlysio of acou*tic information, I.e., reFardle-'so of the
location of the oitpial ao~~o4 information is uoed about the welative coordi-
nat0s of the slejlal atd- interference zources,
6/8
3

USSR
.SOLUKHAO B. V. , -Doklady Akademii Vauk SSSR, Vol 213, -No ia 1973, pp 246-248
The experimentally detartained rolationship bwti(een the possibility of
man's detecting a signal in water against a noise background and the relative
coordinates of the signal and noise sources is analagous to the "cocktail
party" effect known in psychlacousties F17 but for a1r. Otir experiment raerely
demonstrated the existence of this effectduring hearii-ir, in water. Further
carefull nsearch is needed to determine the capacity of the acoustic system
for solving the problem of locating a signal source against a background of
interference sources.
This effect can be mathezatically modeled on this basis of a slight
elaboration of Licklider's hypothesis /-~7- If there are efforent Impulses
from the neurons that detect coincidences, inpulne;;~ rt~cronsible for Inhibition
in -the group of neurons that reflect the position of ths Inte-rference source
in space, the curves showing the relationship betiteen ti-Pe probability of
detecting a signal against a noise background and the c~ltordinates of the sierml
and noise sources will reflect the effects of spatial and tenporal analysis,
These curves were obtained, but there is as yet too little ex-perimental data to
be able to compare then with the oxparimea*tal xesultse
7/8

U33R.
SOLUKM# B. V., Doklady Akaderdi wauk SSSR, Vol 213, Ifa If 1973, pp 246-24-8
1 Al'tmano Ya. A. and N. A. Dubrovskiy# "Spatial HeiLringj" in the books
Fiziologiya. sensornykh sistem (Physiology of the Sensory Systems), pt, 2,
Leningrad, 1972,
2. Dubrovskly, N. A., L. 14. Timarkina, and A. A. Freydin, DMI (Reports of the
Academy of Sciences)# 170t No 1, 1966. 1
3. Samoylemko, Yu. I. and V. L. Volkovicht Pro3tra-nstv(?nno~-rasp--edelennyye
priye=ye i. upravlyayushchlye sistemy ($patlully Mstributed Receiving and
Control Systems), Kiev, 1968.
4, Deatheragel B. H., L. A.$ Jeffres, and H. C. Blodgatt, J, Acoust, Soc. Am.#
No. 26, 1954.
.5. Hollien, H. and H. Rothman# Government Reports Announcemuntt 71, No 12l
1971.
6. Licklidert J. C., Intern, AudioL, 1, Is 1, 1962.

PART 111. ;ffVR0At0=ICS
Z,
HYD)WLOCATION CAPACITY OF DOLPH INS 7.Z1
(Article b~
_AjjdW.v, 6QAO-ud rliev; Kiev,
Itionika. Russian,.No 5, 197 a 7TFlaukova Duaka .pp 52-561
Much attention In now being, devoted to the acholocation
of dolphin* because the scouitlic ~a'y3tan of a dolphin is exceed-
Ingly well- developed and many of it2 components can be used in
engineering.
The ranging s7utem.of a dolphin ecnaists of two psirta:
transmitting Q~ayatom 4f z11V bladders.' IFIX"JnXi fatty Ions.
rafle*bor (skull,bonas), and receiving system -- organs of
hearing, mechanorecoptors.in tho_ftead, upper and lower jaws.
Transmitting part of dolphin ranging mystem. I,-'ong the
nabal passage there are threb pairs of sacs or blAdders (pro-
maxillitry, tubular and vestibular). ~10 will szoullin that sound
generation occurs duving pas-nage of air from a aite Into the
nanal passage. The air bleddars are jurrounded by it systen ot
fine, wall-differentiated muscles regulating the A&P flow. In
accordance 6dth the nature of the sounds utiared hy the dol-
phin and the complexity of the sound-forming eynton, one can
postulato presunce or a complex somantio-InformQt ion procaus
in the articulation of the sounds used In intercoarao and navi-
hation. The tubular and promsxillar7 sites evidently particl-
pate in formation of the directional diagram, sinan the ves-
tibular seen protrude from the frontal part or the nkulIx
playing the principal role in focusing of soundsto,y
. ri~ Thn
eyatom of air sacs, without taking Into account lue
of the altull and lerts, should have a directional characterLs-
tic different from circular.
Shifting of the directional charpotoriatic Is neces-
Bury r r a totml ocar-Ung of space. rt in evidently possible
to bring about some displacement of the ray. by, changing the

USSR UDG 535.343.1
-5-OLMIN, R. I., YaKOBI, Yu. A.j and KOMIN, A. V., Institute of Theoretical and
A~P 10_966a~lbs) Siberian Branch of the Academy of Sciences of the USSR
"Total Radiation from Hydrogen at Temperatures Below 10,000 Degrees"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy) Novosibirsk, "Naukall (Siberian
Branch), 1973, pp 29-33
Abstract: Calculating the radiational characteristies'of gases at relatively
low temperatures requires primarily consideration of molecular radiation.
Detailed calculations for this were made by Olfe in 10,61. For a thin layer of
plasma In which self-absorption can be ignored, radiation from rotational transi-
tions predominates up to 10000; thLt from oscJ1.1lation-rotational transitions
betwoen 1000 and 50000. At higher temperatures negative hydrogen ions and posi-
ti:v,e molecular ions appear, the former more significant by an order of =Cnitude
from 30C10 to 10,000'3K. It higher temperatures linear radiation becomes signifi-
cant. 'When the plasma is of significant density and thickness, the results must
be adjusted to account for the var7ing degrees of absorption at different fre-
quencies and by different mechanisms.
50
-- ------ --

USSR UDC 535.343-1
_NWKhrIzI R. .-I. I YaKOBI, Yu. A., and KOMIN, A. V., institute of Theoretical and
Applied Mechanics, Siberian branch of the Academy, of $cIences of the USSR
"Discussion of Some Results of the Calculations"
Onticheskiye Kharakteristiki Vodorodnoy PIP-zmy, Novosibirsk, "Ifaukall (Siberian
Branch), 1973, pp 40 - 48
Abstract: The special characteristics obtained are based on modern theoretical
concepts and do not require extensive commentary. A few interesting results may
be noted. At a temperature of 0,6 electron volts the Doppler mechanism begins to
predominate for the la and L5 resonance lines at I atmos.phere and for the !a lines
at 10 atmospheres because of the low electron density at this temperature and the
deep locations of the levels corresponding to these lines. At 10 and 20 atmos-
Pheres. the lines are clearly visible against the backgrroundl at high temperatures
they become narrower again because of the reduced electron density.
Although much energy is in the Lymm lines and continuum, self-absorption
reduces radiation in these regions quite strongly, particularly at low tempera-
tures.
The ~.ines of the Balmer and Lyman ceries tend to fuse even at relatively
low quantilm, numbers. There is some question about the boundary between discrete.,
113

USSR
SOLUMN, R. I., et al., Opticheskiye Kharakterist-4ki Vodorodnoy Plazmy, 1973,
.pp~40-48
continuous spectra and the relative displacement of this boundary due to Coulomb
interactions and the smearing of lines as a result of transitions from high energy
levels. The authors' calculations show that the spectral lines begin to fuse
significantly earlier than the Coulomb "trimming" of the discrete spectrntzi.
In addition to the spectral curves, the authoro calculated integral
energy losses for hydrogen plasma over the range of parameters used. Special
calculations were made to relate their work to that of D. B. 01fe, reported in
J. Q=t. Spec. Rad. Trans. 1,104, 1961, and satisfactory agreenent was foiLnd.
The use of lasers to probe plasma requires quantitative infornation
about the relationship between transparency and plasma temperature and density.
These calculations vere performed in two ways, assuming, constant pressure and
at a given initial particle density. The first procedure is necessary becauge
t1hie plasma has significant absorption only at relatively high pressures, yielding,
a condition without significant prossare gradients, but isith Ugh temperature
and density gradients as the plasma is forced against the walls. Although there
is. an overall tendency to-vard absorption at longer wrave lengths, there are
anomalies due to the existence of strong ab%)rption lines which are more or less
active, depending on pressure and temperature. The secotid form of calculition
213
77

USSR
-SOLUIWN, R. I., et al., Opticheskiye Kharakteristiki Arodorodnoy Plazmy, 1973,
pp 40-48
is more appropriate when the laser beam is directed along the long axis of the
plasm chamber, as well as in evaluating the transparency of a plasma under
laser heating.
313

UM 5,$5.343.1
I., YaKOBI, Yu.. A., and KOMIN, A. V., Institute of Theoretical and
XPP:Liea Sibeirian Brant-
h of the Academy of Science-s of the USSR
"The Continuum"
Opticheskiye Kharakteristiki Vodorodnoy Plazzmy, Novosibirsk, "Nauka"
(Siberian Branch), 1973, PP 23 - 29
Abstract: Continuous SDectra are generated by transitions to, from, or within the
unbound ("free,,) state. At temperatures below 5000 de. ees these represent
r, r
free atoms (the total continuous radiation is small) while at 'higher temperatut-es
free electrons are a prirAry radiation mechanism. At electron temperatures much
less than 500 ev a semiclassical- treatment is approprimto:,,, yielding the so-called
Kramer's foxviulas with tile Gaunt fp-ctor ar. a quantum me,-,hanlcal corrective. .4
formula for recombination radiation can be obtained by mpplyinp, Kirchhoff's law
for local thermal equilibrium to the formulas for photc~ionization ab:~orption.
This radiation is characterized by significant intensity close to the line series
and an exponential decay in the direction of short waves. Bremsstrahlun~3 extends
indefinitely in the direction of long waves. The ratio of these two effects can be
calculated for a ;riven tez-,peratuxe and frequency. Another factor is so-called
multi-quantum recombination occurring as a.. result of triple recombination, In a
nonequilibrium plasma this can. substantially influence t~",e distribution of electrons
in levels and the number of free electrons, but in an equllibAum plasma a
1/2

ueli'a
SOLUMIN, R. I. et al, Opticheskiye Kharakteristiki V10dorodnoy Plazmy, Novosibirsk,
IfNauka- (Siberian Branch), 19?3, pp 23 29
Boltzmann distribution in the levels is established, uniquely determined by
temperature equilibrium. At fairly high pressures and temperatures below 10,000 0K
a significant role is played by the formation of neg.ative hydrogen ions,
accompanied by radiation, At still lower temperatures continuous molecular
spectra appea::. There is also the so-called quasi-molwular continuum, which is
due to the transition of a hydroggen molecule from an,initia-1 unstable state
.(occurring as the result of a collision between atoms with paTallel spins) to a
stable state.
In addition to the true ccn-Iinuum, there are quasi-continua, resulting from
the overlap-)ing of large numbers of broadened lines. These occur as various
bands. At temperatures below 1000 K. induced rotatlona1tran*ritions are signifi-
cantl although the radiation of gazes at low temperatures is very low, the
coefficient of absorption is quite significant.
51+

USSR,
OC 535-343.1
SOLMD!,-R.-I., YaKOBI,.Yu. A,., and KOMIN, A. V., Institute of Theoretical and
-Xp-p-~f-ed Mechanics, Siberian Branch of the Academy of Scitt,,nces of the USSR
"Spectral Lines"
Opticheskiye Khaxakteristiki Vodorodnoy Plazmy, Novosibirsk, "Haukall
.(Siberian Branch), 1973, pp, 16 - 23
A
bstract: Three factors determine the nature of spectral lines: population,
~transition probabilityand form of the line. Although many processes contribute
to population distribution, collision with electrons and spontaneous radiation are
usuallv dominant. At low plasma densities secondary collisions can be Ignored and
radiative transitions are dominant, while in dense plasmas nonradiative de-excitation
predominates. When the electron density becomes sufficiently high, radiation
intensity becomes independent of Itl the plasma becomes a Boltzmann radiator.
Spectral lines fron a. plasma are all broadened as a result of interaction with
fluctuating internal microfields. The extension can,be cansidered in terms of two
components,*, one described as the result of a linear Stark effect, due to the inter-
action of ions with other, relatively slow ions, and the other due to collision
broadening (also with a Stark effect component) from interActions with faster-movin~r,
electrons. The electron effect is most si~-gnificant at the center of the broadened
line; the statistical effectat its edges. The center Is vlr~-o somewhat displaced
1/2

USSR
SOLUM-ilN, R. I., et al., Opticheskiye Khai-akteristiki Vodorodnoy Plaz~V, Novisibirsk,
"Nauka," (Siberian Branch), 1973, pp 16 - 23
from what would be obtained from an Isolated atom. Although theoretical calculations
for the edges of the broadened line show good agreement Ath experiments, computations
for the central portion are considerably less satisfactor
y. In this area the
authors base their work on a theory developed by Sobellman, extended to cover also
broadening due to collisions with other particles.
When the concentration of charged particle* 4S JOW, Doppler broadening becomes
significant. The Interral expression for combined Doppler and dispersion broadening
is not in finite form, so that calculation by approximation method Is required.

USSR UDO 5j5.343.1
-.S=Kh,IN - -R-~--I-. .-YaKOBI Yu. A. , and X01MIN, A. V. , Institute of Theoretical and
Applied mechanics, Siberian Branch of the Acadeqr of Sciencen of the USSR
"Method of Performing the Calculations"
Orpticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka." (Siberian
:~Branch), 19?3. pp 33 - 39
Abstraett Five mechanisms vere considered in the computer programs used:
C'
1) bound-bound electron transitions (linear radiation from atons); 2) free-free
and free-bound electron transitions in the field of protons (the H continuum);
free-free and free-bound electron transitions in the field of atoms(H-continuum);
4) ~ frpe-free and free~bound proton transitions in the field af atoms (-the H+
2
continuum)i 5) continuous radiation of quasi-molecular hydmren
~.quasi
continuum). Previous studies have lumped line spectra in two or three
groups.. The present work considers all transitions betreen ditcrete levels in the
hydrogen atom that realistically exist in the plasma. Within the limits of the
parameters chosen, -this rurber varies from less than 10 to several tens of levels,
the number of snectral lines is proportional to the square of this numb-or. Each
line is considered in its broadened form, The results axe presented on a -wrave zcale,
Variable step sizes are used to keep the calculation err-or approximately const,"t
Ov the entire spectrum. Stop sizen wore based on relative values of she derivative
2

ASR
SOLUKhIN, R. I., et al., Opticheskiye Kharakteristiki*Vodorodfloy Plazmy, Novosibirsk,
"Nauka" (Siberian Branch), 1973, P-P 33 - 39
of spectral intensity, OXCeDt where the contribution of the maxinium line was less
than 1/10 the background radiation, where the step size was based on the continuum.
In each ste -D the calculation of step size was based on the line making the
strongest contribution, rather than the line with the neaxest center.
The program was written in ALPHA, a modification,of ALGOL. Calculations
were performed at the computer center of the Siberian Branch, Academy of Sciences
of the USSR.
r2 -

USSR UDC 535.343.i
SOI Tlf.~R. I., YaK6BI, Yu, A., and KOMIN, A. V., Inslitute of Theoretical and
-Xp_~jhed M'e_C-1ii6ff6s, Siberian Branch of the Academy of Sciences of the USSR
"Energy Structure of the Hydrol-:,en Molecule"
Opticheskiye Yharakteristiki Yodorodnoy Plazmy, Novosl'bix-sk, "Nauka"
ISiberian Branch), 1973, pp 12 14
Abstract: Quantum mechanical analysis shows that the ~Iatomlc hydrogen mole'cule
is not stable unless the ends of the tuo.electrons are in an antiparallel
orientation. Alt-hou!zh the two electrons of the molecule can be in various
enerry states, they are within an axially symmetric field whose axis of syrr%netry
is the line connecting the two nuclei. In this case what is significant is not
the absolute value of the orbital moment. but its projertion on the axis
where 41 is Planck's constant and I is a quantum number similar to the
magnetic quantum number m In atoms,
In addition to the electron degrees of freedom, the molecule has oscillatory
and rotationp-1 de--
rees of freedom. For each characterlittic electron state, there
a set of discrete oscillatory states, which can be ol)-tained as the solution
of Schroedinger's equation for a harmonic oscillator. Consid-eration of non-
h rmonic oscillations leads to a more complex expression. Rotation is also
122

USSR
SOLMIN, R. I., et al.. Onticheskiye Kharakteristiki Vodorodnoy PlazMY'
Novosibirsk, *,.;auk& (Siberian Branch), 19?3, PP 12
characterized by a discrete selection of energy states, describable in terms of
the rotational quantum number, the,molecular cont;tant,and a coefficient which
characterizes the relationship of rotation to oscillation (nonrltjdity of the
rotator). Since the hydrogen molecule does not have a constant dipol6 moment,
it cannot in isolation have oscillatoi-I and rotational transitions, but in a
nduced electric dipole moments
real gas this prohibition is removed becausq.of L
occurring in collisions. Althowh any transition can occur, transitions of :t 1
are most common, For electron-oscillatory spectra, the relative probability of
various transitions is determined by the Frmick-Condon principle.
2/2
51

USSR UDC 535-343-1
,aQ~WbIN,.R. I., YaKOBI, Yu. A., and KOIffN. A. V., institute of Theoretical
and Applied Mechanics, Siberien Branch'of ihe Academy:of Sciencea of the USSR
"Diergy Structure of the Hydrogen Atom"
Opticheskiye. Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka",
(Siberian Branch), 1973, pp 9-12
Abst-ract: Schroedinger's equation yields solutions ofi-ly for negative values of
E for which
2jr2me4
E21 2 2
h n n
where n is a whole number and R is the Rydberg constant. m must be replaced
by MM
M+M
where m is the mass of the electron and M is the masz of the nucleus, to account
for wve--x-nt cf the nuclear mass. Relativistic Egeneralization of schroedin-
ger#s equation requires that azimut al a antum =-abers be considered in addi-
th lu
tion to the primzqry number n. In the presence of an external field, the
1/2
-gaff W-7

TISSR
SOLUKhTII, 11. 1., et al., Opticheskiye Kharakteristlk- Vodorcdnoy Fllazmy,
1973, PP 9-112'
magnetic quantum number must also be considered (Zerrian effect). Hourever,
not all transitions described by this scheme are foun& in spectroscopic oll-ser-
vetion. According to quantum mechanics, the follouring types of optical dipole
transitions are possible: change in azimuthal quantum~wjmber + 1; chance in
magnetic. quantum number = 0 + 1; change in m 0; change in. internal quantum
number azimuthal + m'I 0 + 1.

USSR UDC 535-343.1
YaKOBI, Yu. A., and KOMIN, A. V., Institute of Theoretical
and Applied Mechanics, Siberian Branch of the Acade--O- of Sciences of the USSR
"The Composition of Hydrogen Plasma"
Opticheskiye Kharakteristiki Vodorodnoy Plasmy, Novosibirsk, "Nauka"
(Siberian Branch), 1973, pp 5-9
Abstract: A plasma of pure hydrogen can contain ten different kinds of
particles -- H2 and 'f3 molacules, positive and negative ionts of these. molecules,
atons, positive and negative ions of the atoms, and frep, electrons. Diagrams
are given to show the relative contribution of each of these particles 85 a
function of temperature and pressure. The law of masg action gives the rela-
tive amounts of large particles and their breakdown products as functions of
the degrees of freedom of each such component. There tire four types of freedom:
electron, oscillatory, rotational, and translational. -The product of the first
three is the statistical sum of internal degrees of freedom, called the statis-
tical weight of the particle. There are formulas for finding each of these as
the sum of a series in terms of energy of excitation, electron level, natural
oscillation frequency, oscillatory quantum number, and other factors. Trans-
lational freedom can also be expressed in terms of maiss and relative volume.
1/2

USSR
SOLUY%hIN, R. I., et all., Opticheskiya Kharakteristiki Vodorodnoy Plasny,
pp 5-9
Since dissociation and ionization ordinarily begin at temperatures
significantly below the corresponding binding energy, becauee of the high
statistical sum of the free state, in the majority of cases only the basic
electron term need be considered and the unharronic nature of hydrogen molecule
oscillations can be ignored. Several studies have determdned ionization
energy in a plasma and its reduction due to the total electric field of charged
particles around the atom, particularly Eaker and Kroell (1963). The thermo-
dynamic calculations of plasmic composition made in the present work yielded
results close to those obtained by Patch in 1969.
2/2

USSR UDC 535-343.1
SOJAWIT, R. I., YaKOBI, Yu. A., and KOMIN, A. V., Inst -I-tute of Theoretical
and Yfechanics~ Siberian Branch of the Academy of Sciences of the USSR
','Gas Dynamic Properties and Elements of Radiation Gas Dynamics"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Naukall (Siberian
Branch), 1973, pp 61-69
Abstract: In many cases, gas dynamic properties of plasmas must be considered
along with radiative properties. The authors arbitrarily distinguish tvo
thermodynamic regions: a ) temperature less than 10 electron volts and pressure
less than I atmosphere -- radiation is not blocked and the pressure of the
photon gas may be,ignored; b) a "black" plasma at high tomperatures and der,
sities -- radiation energy and pressure must be considered. There are also
such cases as the propagation of shock waves-vith high rpOiation flow,in -.4hich
'At is necessary to consider changes in the thermodynamic properties of the gas
ahead of the front due to absorption of the flow of advaiice radiation froln the
hot gas behind the front. Knowledge of some thermodynemte and ga8 dynamie
properties of low-temperature bydrOgOIL plasma is therefore also necessary.
Where there is overall flow of matter in an opticaliy thin plaloma, the
usual hydrodynardle equations raust be supplemented by a rttdiant energy factor
ut.Uch reprevents a volume energy source. For an optically thick body in which
the radimit heat transfer approximation holds, the -state bf tht3 matter is
d termined solely by its optical properties. In other calses, ,~s in the problem
Y
72

USSR
SOLIMM11, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazmy,
19731 pp 61-69
without material flow, a complete system of equations must ba solved.
The equilibrium concepts used by the authors are applicable to quasi-
equilibrium processes, since the time to establish equilibriv'm between radiation
and matter is of the same order as the lifetime of the photon, which is
usually very much less than the characteristic,times of hydrodynamics, vhich
are equal to or less than the therrmal velocities of the molecules. Of course,
the usual conditions of quasi-equilibriwa must be supplemented by a condition
that the radiation absorbed by matter in the time interval of interest does not
chanee the state of the matter.
2/2

USSR UDC 535-343.1
jpxhix,_R~ 1., YaKOBI, Yu, A., and KOMIN, A. V., Institute of Theoretical and
Applied Mechanics, Siberian Branch of the Academy of Sviences of the U533R
"lAser Heating of a Plasma"
Opticheskiye Yharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka" (Siberian
Branch), 1973, pp 69 72
Abstract: Iaser heating is one of the proposed methods of attaining a controlled
thermonuclear reaction. The necessary conditions are the opposite of those~
necessary for optical analysis witnout perturbation. There axe varyim-7, difficulties
process. At low temperatures, there are mpny enerr- - b-sorbing transitions
imthis y a
to be,passed through, and radiation losses bagln to be significant as the plasma
is heated. At hi-her temper9tures, effective heAtin!T is also reduced by the
increase in transparency of the plasma. The heatim-, mus--'- be rapid to prevent loss
of-heat to the walls and the development of instabilities. Use of a solid or
liquid target, although it requires additional energy for melting and evanoration,
makes attainment of the Laxeson criterion easier because of the high initial plasma
density; if evaporation takes place from all sides simultaneously, a significant
compression factor c-::.n lee added
.At thermonuclear temperatures, only inverse bremsstrahlung is elffective for
I ~ -3),
ual 40 1019cm
heating. For plasmas of moderate density (less than or e 11
1/2

- ---------
us
SR
SOLUKUN, R. 1.) et al. j OPticheskiye Kharakteristjj~i Vodorodnoy Flazziny,
1973, pp 69-72
infra-red lasers are significantly more effectivep but .9hort-Urave lasers are
most effective for heating solid targets. The decrease in the coefficient of
absorption at very high temperatures may be compensated by the inverse cy lotron
effect.. Heat absorption may also be increa I - C
linearitiea that have recently be sed-by several new types of non-
en reported.
2/2

USSR UDC 535-343.1
YaKOBI, Yu. A., and KOMI, J,- V., Institute of Theoretical
and Applied Mechanics, Siberian Branch of the Academy cf Sciences of the USSR
"Radiation of a Nonisothermic Plasma. Transfer Coefficients"
Opticheskiye Kharakteristiki Vodorodnoy~Plazmy, Novosibirsk, "Naukall, (Siberian
Bianch)., 1973, Op 55-58
Abstract: In the presence of a substantially nonisotherrAc plasre, radiation
transfer is described with the aid of special coefficients, calculated, in turn,
from the spectral characteristics of isothermal plasmns. In an optically thin
layer,,the divergence of radiation flow can be described by using modified Planck
coefficients, while an optically dense plasma is described by Rosseland's equa-
tion. In the general case of arbitrary optical density, the radiation transfer
is computed by using the so-called modified endosion capacity. Although the
Calculations are simpler for extremely thin plasmas in which lines predominate
or extremely thick plasmas in Vnich the continuum is dominant, real situations
usually require dealirg with the more complex calculatlann, of intermediate cases.

USSR TJDC 535-343.1
SOLW~j1j,_R.,1.j,_YaKOBI, Yu. A., and KOMIN, A. V., Institute of Theoretical
ffd-Xpplied Muchanics, Siberian Branch of the tcademy of Sciences of the USSR
"Radiation of a Quasi-Equilibrium Hydrogen Plasma, Considering Conductive
Thermal Conductivity"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosib rsk, "Naukall (Siberiem
Branch), 1973, pp 59-61
In
Abstract: Only conductive and radiant heat transfer are considered 4 this
book, although convective transfer is important in a number of cases, because
convective heat transfer has not been adequately studied, either theoretically
or experimentally. There are, however, many-caEes in which convective transfer
does not occur.
The relative contributions of radiant and convective heat transfer for A
plasm without interior directed velocities can be determined from the differ-
ential equation of radiation transport and the law cf energay conservation. If
the absorbed energy is much less than the radiated energy, the system of d3s-
criptive equations can be reduced to two equations; art expression for heat trans-
fer which determines t~o state of matter throughout the entire volLoro, and nn
expression of radiation transfer which can bo iased to fin(l thn iipoctral der..~Ify
of radiation. Tbla occurs In an optically thin. systurri witliout rrcternal
41

..... .. .......
USSR
SOLMIN, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plaziny,
1973, pp 59-61
radiation flows. A similar separation can be obtained if the absorbed ener.gy
is greater than the radiated energy, but the total absorption of the radiation
flow throughout the entire volume is less than the'flvir of energy related to
heat transfer and is thus incapable of changing the temperature distributicn.
Truly radiative transfer states also exists described by th3 so-called diffusion
or radiant heat transfer approximations.~ Although the assu;Tption that radiant
heat trwisfer exceeds conductive transfer is correct in. the overwhelming major-
ity of cases, there is a region in which.this is not true.
2/2
_IE Sir
Ing
Pum

USSR UDG 535-343.1
SOLUKKII, R. I., YaKOBI, Yu. A., and KOM!, A. V.0, Instituto of Theoretical
giTd'-Xp-PI!ed--Y4chanics, Siberian Branch of the Academy of Sciences of the U3SR
"The Role of Hydrogen Plasma Radiation in the Problem of Thermonuclear Fusion"
Opticheskiye Kharakteristiki Vodorodnoy Flazmy, Novosibirsk, "I'lauka" (Siberian
1973, pp 73-76
Abstract: In the majority of thermonuclear installations radiation is the
Primary source of heat loss, since the times involved are too short for con-
vection losses (particularly when viscosity is increased by n Magnetic field),
and conductive heat loss can ho ignored when the plaomn. is or dis-
tant-fi-om the walls. For a douteriu;n-tritium plasma the nece,3_~.:Iry conditions
can be achieved at tarnperature5 over 5 kev, while for pure deuteriun they
cannot be achieved at all unless the magnetic field is u,-ed only for thermal
insulation, not retention of the plan=, or measures are taken to reduce
radiation loss (use of an optivilly thick plasrm oz- radlation-ruflecting
walls).
m malke
Quantitative information about radiation capacity of the plas, a - s
it possible to deternine the mirimum. power of a steady-Bt.-atue reactor and the
zainimm temperature of it's center in the general case of combined heat transfer

USSR
SOLMIN, H. I., et al., Opticheskiye Khar.-azteristikl Vodorodnoy Flazmy, 1973,
pp 73-7b
and radiation losses. Assuming the plasma is not sepoxated from the wall and
its lifetime is not limited by instabilities, the zone of maxim=- brightness
will be a hallow cylinder at a temperature of several electron volts. Cal-
culations indicate a minimal temperature of about 7 kev at the center of a
-reactor without magnetic field, using a,50% deuterium-f-ritium mixture. The
dimensions of such a reactor must be on the order of severall kilometers and
the heat loads on its walls must greatly exceed the capacity of modern ma-ter-
ials.
Calculations show that an equilibrium reactor with a magnetic field
would not produce energi at the center sufficient to c~3mpensate losses at the
exterior due to the poor heat transfer properties ofthe magnetized plasma
and that reflecting shells would be difficult to obtain, since most of the
radiation is in the form of x-rays.
Since continuous operation is apparently impossible, attention is
currently focused on various short-term processes. One main line of re.1carch
involves tbo use of relatively long, laser pulses for sup lemvntary heating of
plasma in various magnetic containment devIces, uttile a. recond Hne is
directed toward the use of very short-powerful laser pulses to bring targets
213

USSR
SOLUKh121, R. I., et al., Opticheskiye KharakteristjJci Vodarodnoy Plazmy,
1973, pp 73-76
to the threshold of useful fusion without auxiliary containment. Unfortunately
laser efficiencies at the wave length needed for this second process are very
low. There is also work being done on combined fusion-fission mechanisms,
using the fusion to produce additional neutrons for improved fission output.
31:3
40
MW
W
M~

USSR UDC 535.343.1
A. V., Institute of Theoretical and
SOLMIN, R. I., YaKOBI, Yu. A. and KOIMIN,
-Apprfie-d--M6chanics, Siberian Branch of the Academy of Sciences of the USSR
00ptical Diagnostics of Plasma"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Wovosibirsk, "Naukall
(Siberian Branch), 1973, pp 48-55
Abstract: Plasma characteristics (primarily the concentration and temperature of
various components) are determined from active and passive optical analysis.
Passive methods, in which the plasma is illuminated by external sources, have
the advantage of causing less perturbation to the plasma than other sampling
techniques, although nonlinearities must be considered when such strong light
sources as lasers are used.
The most developed methods are based on measurement of radiative and
absorptive properties, although measurements of the index of refraction are also
used. Due to the complexity of optical procnsses in a plasnki, the most widely
used method is to begin with rough measurements based on one of the basic
radiation mechanisms and proceed to more detailed analy4zis. AlthouEh in some
particularly clear situations this method is expedient, t(here are many cases
in which the preliminary determination of the prirmry mechanism is quite.
113

USSR
SCLUKhRI, R. I., et al., Opticheskiye Kharak-Leristiki Vodorodnoy Plazmy,
Novosibirsk, 1973, pp 48-55
difficult or even meaningless. in addition, the overwhelminLl Mjority of
these methods assume an optically rare plasma; when self-absorption must be
considered, this analytical approach leads to very complex expressions. A
more general approach, ignoring only those components- vhase contribution is
obviously unimportant, is clearly necessary. he use cS cemputer calculations
over a broad range of parameters provides this more general approach, serving
as a "mathematical experiment" to relate the results of different studies and
serve as a guide for future research.
The index of refraction is the foundation of another group of methods,
primarily interferometry and Schlieren methods. These methods can determine
the density and density gradient of a single type of particle when this type
has primairy influence on the effects of refraction. The relative sensitivity
of these tvo methods depends on the effective radlus ofAhe plasma formation,
the diameter of the focal point, the focal length of the lenses used in the
Schlieren method, and the wave length of light employed.
Primary attention is, currently on the use of infra-red and x-ray-probe
wave lengths. Infra-red is particularly sensitive to the charged particle
components, including the electron continuum. Passive x-ray diagnosis can be
used in determining parameters of a high-temperature plasma along the discharge
213

USSR
SOLMIN, R. I., et al., Opticheskiye Kharakteristik-i Vodorodnoy Plazmy,
Novosibirsk, 10/73, PP 48-55
axis.
As a rule, the diagnostic methods produce information about the plasma
in a given element of the volume at a specific moment in tine. Local discrim-
ination is achieved usually by using the Abel transform and assuming axial sym-
metry of the plasma formation. Time discrimination is achieved by using various
types of time scanning. Optical analysis of hydrogerr plasma, is characterized by
four specific factors: 1) absence of a constant dipole iwment; 2) relatively
high availability of electrons, so that the continuum in the initial stages of
ionization is determined primarily by radiation related to negative ions;
3) the Stark effect as a primaxy deiuerminant of the spectral 11-ine broadening;
4) complete ionization at high plasma temperatures.
43

-USSR UDC 535-343.1
'zOLUKhIN., R.
Yu. A., and KOM, A. V., Institute of Theoretical
and Applied 31echanics, Siberian.Branch of the Academy of Sc iences of the US'SR
Opticheskiye Kharakteristiki Vodorodnoy PlazrV (Optic-0 Characteristics of
Hydrogen Plasma), Novosibirsk, "Nauka" (Siberian Branch), 1973, 82 pp
Abstract: Results are given from detailed calculations of the special char-
acteristics of hydrogen plasma over a wide range of parameters, considering
all significant radiation mechanisms. The material on the comutation is pre-
ceded by a brief systematic sum;l-~- of information about the hydroeen atom
and molecule and the composition and thermodynamic and g
.,as dynamic properties
of the hydrogen plasma. Radiation processes are covered in detail, including
radiation from n6isothermic plasma, u-1hich requires similtaneous consideration
of radiation and thermal conduction. In this connection, the results of the
calculations are discussed, recommendations for their practical use are made,
and some questions of the diagnostics of hydrogen plasma are ex,=ined.
Thin material will be useful, to a broad group of engineer-physicists
and graduate students and students in senior courses speclalizilig in spectro-
scopy, plasma physics, a::trophysics, and physical gas dymtmics.
1/3

*USSR
SOLUKUN, R. I., et al., Opticheskiye Kharakter-stiki Vodarodnoy Plazmy, 1973,
.82 pp
CONTa7S La=
Introduction 3
1. The Composition of Hydrogen Plasma 5
2. biergy Structure of the.Eydrogen Atom 9
3. Energy Structure of the Hydrogen Molecule 12
4. On the Thermodynamics of Radiation 14
5. SpectralLines 16
6. The Continuum 23
7. Total Radiation from Hydrogen at Temperatures Beloit 10,000 Degrees 29

S.
Method of Performing the Calculations 33
9. Discussion of Some Results of the Calculations 40
10. Optical Diagnostics of Plasm-, 48
11. Radiation of a Nonisothermic Plasma. Tran6fer Goeffieients 55
12. Radiation of a Quasi-Equilibrium Hydrogen Plasma, Considering
Conductive Thermal Conductivity 59
13. Gas Dynamic Froperties and Elements of Radiation Gas 74namicz 61
14. Laser Heating of a Plasma 69

44

USSR
SOLUKUN, R. I., et al., Opticheskiye Kharakteristiki ~Icdorodnoy Plazr:y,
1973, 82 pp
15. The Role of Hydrogen Plasma Radiation in the Problem of
Thermonuclear FVsion 73
Appendix 79

USSR UDC 535-343.1
SOLUKhIN,_.,R_J-., YaKOBI, Yu. A., and KOM, A. V., Institute of Theoretical
ara-Wip'-p-lded Machanics, Siberian Branch of the Academy of Sciences of the USSR
"On the Thermodynamics of Radiation"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Naukall
(Siberian Branch), 1973, pp 14-16
Abstract: The primary obstacle to establishing equilibrium in a system includ-
ing radiation is the loss of energy by radiation otitside.the sy-,tem.. In
excited particle can lose energy either through a dmmping collision or by
spontaneous radiation. If there is any significant ionIttation, the majority
ot collisions are with electrons.. Thus, given the damping colAlsion crons-
section of the particle and its radiational lifetime (considering also stimil-
lated emission), the relative probabilities of damping and radiation can be
calcalated. If damping is more probable, local th~rmodynanic equilibrium may
be established. Overall equilibrium will depend on the voltzme. absorption
coefficient and the relatille probability of damping, The calculaticns for
absorption must consider re-radilation, so that Pabsomtioall Implies a sufficient
number of collisions to make the probability of dampin'g high. if this total
path length is much greater than ihe dimensions of the volume, the result is
113
- 45

USSR
SOLUKUN, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazzy,
1973, pp 14-16
-libri rad'ation
volume radiation; if it is much less, surface radiation. Fpu Um
of a surface plasma radiator is equi-alent to that of an absolute black body
and is referred to as Planck radiation. Volume equilibrium in the sense of
local thermodynamic equilibrium yields so-called BcIttmaiLn, radiation, since the
nature, of the radiation is determined by the Boltzmann distribution of electrons
in levels. While a special form of Kirchhoff'S laur applies to the latter case
and the black body radiation is determined from Flanck's foraula, nonequilibrium
radiation can be analyzed only by solving an enormous system of kinetic equa-
tiona, since nature depends on the probqbilities of a large number of elementary
processes,
-In a moderately dense plasma local thermodynairdc equilibr-Luil is the
most probable state;-it is sufficient for the probability of collision processes
to exceed the probability of radiation processes by an order of magnitude. In
fact4 the rigidity of this condition for a resonance traosition with imixinium
probability of spontaneous radiation can be significantly reduced in the
majority of real cases by the trapping of radiation in the optically dence
plasma. Since most expc-rimtental installations produce a pl.asms for a short
time, it is necessary to verify that the time to establish equilibriiLm is brief
i comparison with the time to establish a quasi-stable state. This can be
2

...........,
USSR
SOLUKhIN, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazwor, lG73,
PP 14-16
done by considering the slowest process, the relaxation of the resonance level.
Under experimental conditions, radiation scattering (primarily Thomson
scattering) is ignored, since the mean free path is very, long; under actual
physical conditions, this factor may be important.
313
40

USSR UDC 617-001.34-r)7:616-009.939.6
V.
MOLCHANOV, V. V. and SOL Saratov Medical Institute
"Changes in Blood Protein Metabolism in Vibration Disease"
Moscow, Gigiyena Truda i Professional'nyye Zabolevani-ya, No 10, 1971, pp
43-45
Abstract: Total proteins and changes in the blood ptotein fractions were
studied in 94 persons who had been expQsed to local vibration for varying
lengths of tine, 34 still using vibrating tools at the time of the exandinn-
tion and 60 no longer doing so because SYMPMMS of -vibration sickness had
been detected. Both groups showed changes in pro tein~ metabolisa, -- decrease
in albumins, hyperglobulinemia (increase in the a2, a2, and y fractions),
and decrease in the albumin- globulin ratio, These changes were more prc-
nounced in the first group, especially among the female workers. Dyspro-
teinemia intensified with length of time on the job, being particularly
severe in those with 16 to 20 years of experience. Ptoteiz metabolism ex-
hibited a tendencv to return to normal in those rio longer exposed to
vibration.
2/2
- 42

USSR UDC 5$0.12:b31.18+538.3
ZAYTSEV, G. A., SOLUNIN, A. M.
"On the Problem of the External Invariance of Maxwell Equations in a Space
With a Medium"
V sb. Nekotor. differents. uravneniya mat. fiz. i teorii,xolebaniy (Certain
Differential Equations of Hatbpmatical Physics and the Theory of Oscillations
Collection of Works), Ivanovo, 1970 pp 91-97 (from RZh -rizikai, No 1, Jan 71,
Abstract No 1B137)
j-. Translation-, The general Maxwell equations in the presemce of electric and
fictitious magnetic charges aro described in the algebralc fw1m:
In the above expression V e at where e are generatinjil, algebras of the 16th
order A, related by the relationships;
1/2

USSR
ZAYTSEV, G. A. SCLUNIN, A. III. , Nekotor. differents. izravneniya mat.- f Iz. i
teorill kolebaniy, ivanovo, 1970, pp 91-97
The elements 0 and j from thg algebra A are expressed in terms of the- electroinag-
netic field tensor F 1/2F e e and in terms of the 14-vector and 4-pseudovector
a 8
jEt
electric and magnetic currents and Va e by the formulas:
je, elfa imag mag CE
(D~p+F, p~P%4?+ptj, jni~e2ele,t
72
-41T/c(jei _ijma~ VP + ii
'The Maxwell equations in for% (1) are invariant relative to external transforma-
tions under which the coordinates of X a do not change and P and j are multiplied
on the right by the inverse elements from algebra A which are llnear ccmbinations
of the products of an even iiumber c& generatrices e . ror a space with a medium,
a
it is proposed that the bound electric charges and currents be replaced by fic-
titious bound magnetic charges and currents leading to.the same macroscopic
character.`Lst-ics of;~ the me,i=. . As a result, it becomes possible by an external
transformatioz to give a new physical sense: namely, they c-anvert free and
bound electric charges and currents amon&.themselves. G. A. Zaytsev.
2/2

L12 OC9 UNCLASSIFIED PROCESSING DATE--090CT70
TITLE--DETERMINATION OF THE MON-ETHYL ADIPIC ACID CHLORIDE -U-
AUTHOR-104)-SOLUNINAw I.A., PARFENOVA, V.V.t DEVYATNINY V.A., KUZNETSOVA,
T.N.
~tGUNTRY OF INFO--USSR
SQURCE--KHLM. FARM 1H. 1970#.412),, 46-8
-.DATE PUBL ISHED--70
'*SIJBJECT~ AREAS--BIOLOGICAL AND MEDICAL SCIENCESt CHENISTRY
-TUPIC TAGS-CHEMICAL ANALYSISt ADIPIC ACID, CARBOXYLIC ACLO CHLORIDE,
'HYDROLY 5 1 S
.CONTROL MARKING-NO RESTRICTIONS
,00CUMENT CLASS-UNCLASSIFIED
,;PAGXY:REEL/1-RA~IL--1993./0538 STEP NO--UR/0450/70YO04/002/0046/'0048
'-CI,RC ACCESSION NO--AP0113429
NC I
U
-ASSIFIED

".-.-2/2 009 UNCLASSIFIED PROCESSING DATE--090CT70
.CIRC ACCESSION 140--AP0113429
''AtiSTRACT/EXTRACT-(U) 6P-0- A3SfRACT. A PROCEDURE WAS DEVELUPEO FOR
Dr-TG. THE TITLE COMPD. (11 1,14 THE PRESENCE OF MONG ET ADIPATE t1l) AND
HCL. THE PROCEDURE WAS 8ASE0 ON EfHANOLYSIS OF f WITH:A13S. ET0H TO FORM
DI ET AOIPAfE AND liCL, AND ON HYDROLYSIS OF I,TJ FORM 11 AND HCL. A
TITRIMETRIC DETN. Of- THE ACIDS FORMED BOTH REACTIONS PERMITS THE I
-LONTENT TO BE ASSESSED FROM THE I)IFFERENCE. THE HCL CGNTENT WAS DETD.
BY THE VOLHARD METHOD. THE PROCEDURE IS AS FULLUivS., DISSJLVE A SAl-lPEL
(SIM',LAR.TkJ 0.1.5 G) IN 5 ML ABS. ETOH,:ADO SEVERAL DROPS OF BROMOTHYMOL
BLUE AND,TITRATE WITH O.L N NAUH. THEN.ADO 10 ML L6PER(;ENT-HNO SUB31 20
14L 0.1 N AGNO SUB3, AND BACK TITRATE THE AGNO SUB3 WITH 0.1 N NH SU84
SCN IN THE PRESENCE OF NH SU64 FEISO -SU84) SU82. DISSOLVE ANOTHER
SAMPLE IIN 5 ML DIOXANEw ADO 20 ML H SUB2 Or AND TITRATE WITH 0.1 N NAOH
USING THE SAME IND-lCATOR AS IN -THE IST TITRN;. ~ CALC-. THE CUINTENT, OF
1,11s, AND HCL FROM THE GIVEN FORMULAS. THE RELATIVE ERRORS OF THE DETN.
.~Uf- Ii IIt,ANU HCL BY THIS PROCEDURE WERE 5.51 ltv AND 15.OPERCENT,
kl~sp. FACILITY: VSES. NAUCH. USSLED. VITAMIN. INST-i MOSCOWt
'USSR.
UNCLASSIFIED

777777
112 019 UNCL AS S I P I ED PRnCESSING DATr--160CT70
JITLE--CERTAIN UNSTEADY PROBLEMS OF THE 'mEoRy OF H;,4m AMPLITUDE WAVES
WSSIPATIVE ME01-A -U-
O.V., SOLUYAN, S.I*
.:-COUNTRY OF INFO--USSP
-~SOURCE-AKADEMIIA NAUK SSSRv DOKLADY, VOL.. L970, P. 815-181
~-DATE' PUBLISHED ------- 70
UBJEC-T~AREAS-PHYSI.CS
~j-OPIC TAGS--PARTIAL DIFFERENTIAL EQUATION, CYLINDRIC, WAVE, WAVE
....-PROPAGATION, ORDINARY DIFFERENTIAL EQUATION
~;t'ONTROL MARKING--NO RESTRICTIONS
"DOCUMENT CLASS--UNCLASSIFIED
.-PROXY REEL/FRAME--198410267 STEP
:ClIRC ACCESSION NO--A)"0055063
UNCLASSIFIED
---- ----------------

771"
019 UNC L ASS IF IE D PROGESSINIG DArE-161OCT70
ACCESSION NO-AT0055063
GP-0- ABSTRACT. STUDY Of: CERTA.IN UNSTEADY PR'13LE,'-lS
REGAPDING wAVE PROPAGATION liN DiSSIPATIVE, SPATIALLY SYAMETRICAL MEDIA.
IT IS SHOt-4i%' THAT, IN CEkTAIN IMPORTANT PAkTICULAA CASES, THE, NONLINEAR
PARTIAL DIFFEREIN'TiAL EQ'UATIGNS DESCRHING PLANE ANJ CYLIINDkICALLY
SYMMETRICAL WAVES CAN, BE REDUCED TO GROINAkY DIFFc"RENTIAL EQUAllUi,\45.
EXACT SOLUTIONS 4! of suporlattLce pea", and an the basis of analyaLs of the extinguishing law,
be proposed. an Nb 03 mod*" The. experimental and theorarIcal values of the
intensity were not compared in (5). Accordingly, the purpose of this oxporl-
must was more precisely I to define the lattice of NbO3 mod study its
possible varlation with a rise to temperature by soma of vrautron diffractloo
tha moat.rellabl* method of localAzing the light stow In the presence, of
;
;a"
36 -

Uri C L a S S ft J' AkbC ESS I NIG OAT c- 2 10
OF MWNGANESE VAINADIUM AlLnYS -LOSE JO
T ITLE
COMPOS-ITION, I-N RELATION TO T14E blAGNET-IC PROK.-RTIE, -tJ-
AUTHOR-(03)-KUCHlNt V.M.t SOMENKOV, V.A.,~ SHILSHTEYN~ S.Sll.
COUNTRY OF IMF0--USSR
.-:.-SOURCE--FIZIKA ,,tETALLOV I tMETALLOVEDENIEv FEB. 197oq 1 29, 42), t04-406
DATE Ptin I SHCD ------- 7 0
SUBJECT AREAS--MATEPIALS
TAGS--ALLOY s,rRUCTURE, MANGANESc_ ALLOY, VAMADIU.M ALLOY, NIEUTRO,"I
MAGNETIC MOMENT, ALUMINWIll 'MER.;:f) ALLOY,
DIFFRACTIOM, CONTAINING' ALLGY Or
MAGNETIC PROPERTY
CONTROL tMAPKING--NO RESTRICTIHNNS
DOCUMENT CLASS--til"JUA15 :;H~ [Ell)
-PROXY PEFL/FRAME-3100 V0349 's T;:_ P
C!Rc,

2/2 022 UNCLASSIFIED PQAjCES!,'INC, f)ATE---27N0V*7C
CIRC ACCESSION NG--AP0129581
ABSTRACT/EXTIRACT-(U) ABSTRACT. THE STRUCTUKE OF ~-'N~V AN-D
DIFFRACTION AND THE RizsUl.
ALLOYS ~)AS STUDIED 3Y N1 TS wFRE
INTERPRETE0 liN TEPMS OF THE PECULfAR MAGNETIC PROP:;:RTH.S~ OF THESF
MATERLALS. SUPERSTRUCTURAL F,EFLc"CTf,-),14S APPEAR.E0 ON TH',~: -N'C-UfR0,N
-1 -11 J,j 01 T ~ I ER M A. L1
OIFFRACTION PATTERNS OF MN9V ALLOYS PREPARED Filij,' ~Ai~'U,'
PRESUMABLE AS A RESULT OF TRACES OF AL. Tii~ ADOITjOiN OF SIMILAR TO
5PERCENT AL TO MNtV ALLOYS LED TO THE FORMATION OF~ AN ORDERFD STRUCTURE
WITH A SPONTANEOUS MAGNETIC MOMENT, THE AL. APPARENTLY STABILIZING THE
MAGNETIC PHASE.
i~ s i F If)

pqoCESSIM, DATE--IISEP.70
'112 013 UNCLASSIFIE
,TITLE--STRUCTURE OF TA SUB2 D -U-
~AUTHOR-PETRUNINt V.F.# SOMENKOVr,V.A., SHILSHTEYN,.$.SH.,_C)4ERKOV, &.A.
.-C--CUNTRY OF INFO--USSR
~S-OURCE-KqISTALLOGRAFIYA, 1970, 15(l) 171-:3
~~ATE PUBLISHED ------- 70
~--SUSJECT AREAS--CHEMISTRY
T-OPIC TAGS--DEUTERIUM COMPOUIND, TANTALU4 COMPOUND, NEUTRO'l OlPFRACTIC-N
.,i-"!lTR0_L.MAF_KING--N0 RESTRICTIONS
:.DOCUMENT CLASS--UNCLASSIFIED
RFEL/FRAME--1936/0015 STr-P ll
CIRC ACCIESSION NO--AP0102115

2/2 013 U~,,rt. ASS IF [ED PROCESSING, DATE-11SEP'70
C. IRC ACCESSION NO-AP0102115
~~.ABSTRACT/EXTRACT-fp) GP-0- A,5STRACT, BY MEANS OF A Hl(';,I-i l.,4TEENIS~TY, ~41~H
RESOLUTION NEUTRON DIFFRACT04ETER, POLycrysr. rAD SfJr_,0 53 !,,AS
STUDIED AT -S11-400DEGRFESK. ON THE NFUTInN OIFFRACTIrN P!,TTERNNS, IN
A',30N. TO THF JQIFF_RACrr0N PEAKs naSo. PREVIOUSLY BY WALLACc (CA 95:
1?396G), SEVERAL WEAK REFLECTIONS ALSO WERE OBSO, ALL l'i-V: qE:~-LECT[ONS
MAY BE INOEXED IN A UNIT CIELL 'WITH PARAMETERS A APOROXIMATELY C-(.'!JkL TP r1
APPP-13XI14ATELY EQUAL TO A SU30 ROOT BAP 2 AND C APP'-'.f")(.lm.,lTr-LY E-J"JaL To
STRUC T AL
SUBO (A SUBC IS THE TA LATTICE PERIOD)o. THE WEAK HYPERFT4;
REFLECTIONS-ARE DES-CRA-BE0 BY TH&RELAfION.K PLUS L~EoUaLc 2i'A. TAn, SuB,)
TIMES 53 BELONGS Td THE SPACE GROUP 1) PRIME6 OVER 2 MINUS A222; 4 TA
ATOMS ARE IN POSITION 4K AND 2 D IN 2A:POSITION. THIS MoDEL Is
-.:..C4.ARACTERIZED BY I PARAMETER X FOR METAL ATOMS; ITS VALUE OBTAINED BY
--MINIMAL IZATION. OF DIVERGENCE FACTOR FOR HYPERFINE OEFLECTIONS AT ROOM
TEMP.~ I-S -X EJUALS 0.012- (0.01? FOR THE ~TEMP. OF Lld. '41. r-R9'l THE REP~trlD
2A~OF TRE,ORTHORHOMBIC DEUTERIDE LATTICE.:
I A,
U; 4 U L 14

1/2 024 UNCLASSIFIED PROCESSING DATE--IISEP70
S BASED ON GAMMA MANGANESE -U--'
..,TITLE--ANTIFERROMAGNETISM OF SOME ALLOY
-SOMENKOV9 V.A.v KUCHINY V.m.
.~..AUTHOR
.,"'COUNTRY OF fNFO--USSR
~..~,,.SOURCE-FIZ. METAL. METALLOVED. 19T0, 20(l) 207-9
-.`DATE PUBLISHED ------- 70
AREAS--MATERIALS
TOPIC.TAGS--MA.NGANESE ALLOYv ANTIFERROMAGNETIC MATERIALt NICKEL ALLOY,
--INDUCTION FURNNCE, NEUTRO-4 DIFFRACTIONI RRILLOUIN EFFECT, HELIUM, ZINC
;-::..-.CCNTAININ,G ALLOY# MAGNETIC STRUCTURE
,:rUNTROL MARKING--NO RESTRICTIONS
CL.ASS--UNCLASSIFIED
~PROXV REEL/FRAME--1988/0628 STEP NO--UR/0126/7t.11029/001/02071')20'~I
C IRC -ACCESSION 401-7-AP-910560-7

2/2 024 UNCLASSIFIED PRCCESSING DATC--11SEP70
ClRC ACCESSInN~N0--AP0105607
..A8STRACT/EXTRACT--fp) GP-0- ABSTRACT. THE STUDY OF THE MAGNETIC
STRUCTURE OF ANTIr-EPROMAGN;:TTC ALLOYS OF TRANSITIGNS -3 ETALS Nl;iKES IT
POSSIBLE-TO DET. THE CONDITIONS UNDER WHICH LOCALIZED 1AGNETIC MOME-NTS
CAN EXIST IN;;THE CRYSTALS. NEUTqON DIFFRACTION OF-BINARY ALLOYS OF 0
METALS BASED.-ON GAMMA MN WAS USED TO BRING OUT THF EFFECT OF THE
IMPURITIES-OF T14E 2ND COMPONENT ON THE PROPERTIES OF THE METALLIC
-ANTIFERROMAGNET. MN ALLOYS CONTG. 10, 15# 20y 25v AND 140 AT. PERCENT
Nl* AS WELL AS MN ALLOYS CONTG. 3.5 AND.5.6PERCENT AT, ZN AND 409 509
56i AND 60-~AT.- PERCENT FlEv WERE USED. , THE ALLOYS' WERE MELTED IN AN
INDUCTION FURNACE IN A He ATM. AND QUENCHED IN WATER TO STABILIZE THE
GAM4A'PHASE. NEUTRON DIFFRACTION SHOWED THAT ALL THE ALLOYS STUDIED
WERE AT. DISORDERED SYSTEMS WITH GIVE4 MAGNETIC ORDERING. THE PRESENCE
OF DIFFUSION PEAKS ON THE NEUTRO14 DIFFRACTION PATTERNS [S ASSOCD. WITH
THE AT, SHORT RANGE ORDER, WHtCH INCREASES WITH I~JCREASTNGV CONTENT OF
THE no comPONENT. THE TE4P. DEPENDENCE UP T14E INTENSITY OF THE
MAGNETIC SUPERSTRUCTURE PEAK IS SATISFACTORILY DESCRIREO PRY A t3RtLLOUIN
TYPE FUNCTIn4. INASMUCH AS THESE ALL:OYS CONSIST nF RELATIVELY SIMILAR
-IMS, THE SPIN SYSTEM CAN
(.WITH REGARb TO THE STRUCTURE OF THE 3D BAND) ATL
APPAREN-TLY__,9EcnME ORDERED INDEPENDENTLY OF THE EXACT CONFIGUR4TION OF
-N'THE-LATTICE OF THE ALLOY. THE OETG,,~R~ILE IN THESE
THE-ATOMS I
~ANTIFERROMAGNCETIC ALLOYS IS PLAYED BY THE INTERACTION OF THE D ELECTRONS
AND NOT.-THE S AND THE D ELECTRONS.

1/3 0;A I UNCL A',i S I F I ED V11-9 C E S11%
3
fLrLE---SY,h,'Th,:' IS OF I Z-:ETHYLPV'i,.AlGLE ANO,
I L Ti I i VL Z~ i,YR A Z G L I N E A L J L HY 0 ~E S
I r
r
ANU THEIR ACL-TALS -IJ-
UA 4
'T
SomliNs I.N.
A
_TCLUNTRY CF INF"--JJSSR
kJ CPO
.L
S CURIZ E -K F; 124 GETEPCT-"'AKL. SUEVIN. 19709 3) it 404-6~
S CU"
DATE PUBL I SHEP--7 0
_~.S,UBJECT ARCAS--CHEMISTRY
:-.TCPIC TAGS--ORGAINIC SYNITHESIS, PYRA
ZQ L E ALGEHYDEP ACET4, IR SPECTRUM
-.,CCMTR0L INARKINC-NO RESTRICTIONS
-MUMENT LLASS--UNCLA.SSIFlE0,
I --UP 76/000 0,5
PROXY REEL/FKAkE--3CQI/G2L2 STEP NO /040'),' ,1003/0404/0
CIRC ACCESSICN hkG--AP0126003
J,

Rim
2/3 022 UINCLASSIFIED PROCESS ING DArE--20NOV70
~--'CJRC ACCESS ICN NO--AP0126003
-ABSTRACTYEXTRACT-M GP-0- ABSTRACT. TO SOLN. OF 2.135 G MENHNH SUB2
'ED 5.23 G '-H SU32-CliLGL:HlEJET)5Uf32 AND THE MIXT.
JU ~20 .41L- H SU32 0 WAS ADU
12 HR -WITH ETHEk TO YIELD 78PERCENT I (,( ElUALS tGETJSUi32) (M , B
~''SUB 895-7DEGREES, N PWIE20 SUBD 1.4540. A S13I.N. DF '1.33 G 11 IN 18 ML
-.~.A:HCL '"'AS KEPT 3 HC AND :AA,E TO YI.F-LD 631PE-~CE,~'T I iX EQUALS 01 v B
SUB3 70-3t;EGREES, N Pklikic-210 SU1.10 1.5410.; OXIV* HCL ,
m. 162-30EGREES MJS,
ETU h) * S11,11LARLY iiAS o6TIAINED 64PLulGENT III iX L~JUALS Wt:T)SU82) I IV)v
6 SUB18 95-EGEGREES, N Piml~ME20 S06ZI IV.-,'-IEI* iMa L20-10EGREES
114. ZELENIN 41963) 1--
REARkANGE0 ACCORDING TO b. V. 1()FFI-:: AND K GA V E
98PERCENT ME SUB2 INCHICH SUB2 CN)CHMM.E)SUB2 B SUBli. 86DEGREES, 14 PRIME20
.3 ( tj p
SUBD 1.4430. 11 (5.5 IN 30 ML AtNHYD. C Silb~~ H SUB T EATEO STE Pwf SE
WITh STIRRING WITH P13 (CAC)SUB4 GAVE AFTER Z.5 HR 7bPERCENT 4j-c DEHYDRO
ANALOG (V) rk--F III B SU33 101-4DEGREESi. N PRIMEZO Sllpi~D 1.(t645.
HYDRCLYSIS OF V GAVE 75PERCENT 4,5 GEHYOR0 ANALOG t;)1- I (X EQUALS 0), B
SUB2 72-tiLEGREES, IN JIKINt20 SUBD 1.5132. A SOLN. OF 6.6 G I
CLE I" 4tO 1,1 A,~'iHYO. ETHER. WAS TREATED AT ;MiNUS 100EGREES W[Tfi
MET~-,YLPY~,AZL; Vv
5.8 G BULI fN 40 ML P-ErriCLEUM ETHER, THE SUSPENS.1ohl STIKlkFD 1.5 lik AT
-Rfjcj~l TEMP. 1 8.03 6 OMF 1N IC.,",L ANHYD. ETHER ADOFI)il AND" THE WHOL.,
'R f- 4C i)E ~j D 0 t
I ~iR p THE K EP f oVEi,.t-.o'IG8f i TO Y I ELD 43 PERCEN T f v5 Y R AL4ALCG
(Vt I OF I I I X EQUAi S ~-'J) SUB-4 50-311EGRCE .5 , N 11JI11VIE20 S060 I . 5Q I
L
11.1 61 Ald) 1.6 G C1110ET)SUB-1
OXI ME Hr-L,, 'I V I
IN 5 ML ANHY6. FIGH, TRLATED WITH A F~-'W ORCPS 30POiCENT
KL ET0H GAVE
-TEP 4#5 01-HYUR0 ANALOG (Vil) OF 111 CX EQUALS
l , `0 hk 71PERCFNT
A
tOETISUB2), 5 SUBI 86-90DEGREES, Pi PRIME20 SUBD 1.#+690,#
A C&~
-1. L U

--313 GZ2 UNCLASSIFIED POUICESS ING G AT F- 2 0 NO ti 7 0
-CIRC,ACCESSICN NO-AP lei I 26CO3
o'3STK,hCT/EXT-'Af.T--THE REACTIUN C-F Mr- SUB2 CH i CH SU1132 C~OCMC'i~T)SIJ162 AND
MENHN-h SU62.H SU62 SO SUolt 00~ERCENT. EXCESS) GAV.F-, 81-ill:tKENJ 'MIAT.v 8
'OF ANO~ll
-SUBl 92-3~;L-C-&~LES, K Prli~',E-20 SUBD 1.4661,1 Vll~ 5619E IR DATA ARE
.GIVEN.
A'SF;

1/2 010 UNCLASSIFIED PROCESSING DATE--16OCT70
..,TlTLE--AMlNO ACIDS COMPOSITION OF DIFFERENT RYE VAKLETIES PREVALENT IN THE
USSR- -U-
~~AUTHOR-SOMIN, V.I.
_'COUNTRY OF INFO--USSR
"'.."SOURCE--VOPROSY PITANIYAr 1970s, NR 31 PP 48-54
_~:~DATE PUBLISHED ------- 70
.1 _SUBJECT _AREAS--AGR.1 CULTURE, BLULOGICAL AND-MEDICAL S,G I EN/; C- S
TOP I CTAGS-C~2EAL CROP, AMINO ACID, CHEMICAt ANALYSIS, JW4 EXCHitNGE
CHROMATOGRAPHY, PROTEIN
CbNTROL MARKING--NO RESTRICTIONS
'DOCUMENT CLASS--UNCLASSIFIED
024,(- 70 0 00/00 3/00!f /00 5~
:,--P.ROXY REr'_L/.FRAME--1998/0005 STEP NO--UR/
ACCESSION NO--AP0120705
LINCLAS S I F I E D

2/2 010 UNCLASSI FI~D PROCESSING DATE--160CT7C
CIRC ACCESSION NO--AP0120705
~~ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. THE AMINO ACIDS --P~IPDSITlf~N OF
SUMMARY PROTEING IN 15 SPECIMENS OF RYE BELONGING T-3 10 SOVIET y~i~rETI~s
CULTIVATCO IN OfFFE-KEN'T ARE4S CF THE USSR WAS STUC)IED i3'( :JS 'N
EXCHANGE RESIMS PAI)JI'rION CHROMATOGRAPHY. NO SIGNIFICANT OISTINCTL:'~4
CORROBORATED STATISUCALLY WERE UISCLOSEL)t THIS AIJESTING TO rH.1S
A.BSENCE OF ANN' MARKE0 EFFeCT OF ME RYE VARIETIES:AND CONDITIONS
ATTENDING THEIR CULTIYATION ON THE AMINO ACIDS COMPUSITION THEREIN'.
SMALL (LYING WITHIN THE ERROR OF THE METHOD) FLUCTUATIONS IN THE AMIND
ACIDS COMPOSITION OF SUMMARY PROTEINS IN7HF RYE OF DIFFERENT VARIETIES
AND IN SPECIMENS OF A SINGLE VARIETY CULTIVATED IN OISSIMILAR CLIMATIC
U 0
-AND SOIL CONDITIONS C4~, APPARENTLY, TAKE PLACE OUE T THE C MBINEL)
EFFECT OF SUCH FACTORS AS A SHARP VARIATION IN THE CONTENT OF SUMMARY
PROTEINS IN THE GRAIN (IN THIS PARTICULAR CASE FRIPI 5.6 TO Itt.4PERCENT)
ANO DIVERGENCES I~N TH-E CORRELATION OF DIVERSE TYPI:S OF PROTEP-45
CONTAINED IN THE RYE (GLO13Ut.INS# ALBUMINSt GLUTELINESt ETC), WHICH, AS
IS KNOWNI HAVE DIFFERENT AMINU ACIDS COMPOSITIUN.~, FACILITY:
GRUPPA KHIMII PISHCHEVYKii PRODUKTOV INSTITUTA PtTA,,im, AMN SSSRv MOSCOW.
--c C
I

010 UNCLASSIFIED PROCESSING DATE--230CT70
T.ITLE--FREE AMINO ACIDS CONTENT IN SPRING WHEAT GkAIN ~U-
AUTHOR-(02)-YEKIMOVSKIY, A.P., SOMIN, V,s I
":Z.
COUNTRY OF INFO--USSR
:'SCURCE--VOPROSY PITANTYA, 1970t Nk 39 PP 58-62
~.:DATE PUBL.ISHED------7:D
S GJ E CT AREAS--BIOLOGICAL AND.-MEDICAL SCIENCES
-~-~TOPIC TAGS--WHEATt AMINO ACIDt CHROMATOGRAPHIC ANALYSIS
CONTROL MARKING-NO RESTRICTIONS.
-DOCUMENT CLASS--UNCLASSIFIFO
~,PROXY REEL/FRAME--1997/2054 STE P NO--Ulk/0244/'tO/ODO/003/0058/0062
'CESSION NO
C IRC A C
UNCLASSIFIED

2/2 010 UNCLASSIFIED PROCE$SING DATE--230CT7(
CIRC ACCESSION NO--AP0120697
ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT, AMINJ ACIDS COMPOSITION WAS
STUDICD WITH THE AID PARTITION lCOLUtAN) CHRO11ATOGRAPHY WITH SULFOINATED
PLOYSTERENE-CATION EXCHANGE RESINSt AND TOTAL FrEE A141NO ACIDS WERE
DETERMINED IN THREE SPEC114ENS OF HOME GROWN SPRING WHEAT (VARIETIES:
.11MINSKAYA", "KHARKOVSKAYA 46111 "GORKOVSKAYA 20!'l WITH A VIEW TO
CLARIFYING THE SIGNIFICANCE,OF FREE AMINO ACIDS IN THE TOTAL AMINO ACID
BALANCE OF RIPE WHEAT GRAIN. FREE AMINO AC.10S WERE EXTRACTED WITH
80PERCENT ETHYL ALCOHOL, FOLLOWED BY k3 FOLD CHLOROFORM PRECIPITATION
OF PROTEINS. FREE AMINO ACIDS WERE FOUND TO COMPRISE ALTOGETHER AROUND
0.03PERCEN OF AMIND ACIDS-CONTAINE04WTHE WHEAT GRAIN PROTEINS.
FACILITY: INSTITUT PITANIYA.AMN SSSRt MOSCOW.-
a I L L

112 011 UNCLASSIFIED PROCESSING DATE--23OCT70
OF AMMONIA FROIM A CITRATE: BUFFER -U-
AUTHOR-- SJM 1,4.; V.I.
.-.COUNTRY OF INFO--USSR
DELO 1970, (2), 116-17
-:'DATE.PUBL.ISHED ------- 70
:SUBJECT AREAS--CHEMISTRY
TOPIC TAGS--AMMONIA* CITRIC ACIDi ION EXCHANGE CHROMATOGRAPHY
,~_,CGKTROL -4ARFtNG--N0 RESTRICTIONS
DOCUMENT CLASS--UNCLASSIFIED
.-W-OXY REEL/FRAME--1997/0332 STEP ~10--Uq/9099/70/0001')02/0116/0117
ACCESSION NO--AP0119309
UN C L A S S-1 F I-E