SCIENTIFIC ABSTRACT YAKIMENKO. L.M. - YAKOBSON, G.E.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R002203610016-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 1, 2001
• Sequence Number: 16
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

2/2 olq UNC L A I FIl E' d PROCESSING DATE--11SEP70
,1-.CTRC ACCESSION, NO--AP0104206
~,~:..ABSTRACT/EXTRACT~--(,Ul GP-0- ABSTRACT. THE ELECTRO CHEM. AND CORROSION
BEHAVIOR'OF, A JT %ASE: COVEPED BY PT WAS STUDIED 4,T -PH 0-14 AND
80,DEGREES. TO W KINDS OF TI ELECTRODES WERE USEO, ONE OF WHICH WAS EMERY
CLEANED, DF-GRE-ASEO, TREATED FOR 20 MIN IN H SU92'SO SUB4 AT 800EGREESt
RINSED IN WATEk, DRIED ON FILTER PAPERw AND KEPTIN THE AIR FOR 24 HR
BEFORE USE.- TjJiIS ELECTRODE WAS.CALLED AtR OXIDIZED. THE OTHER
ELECTRODES ~(ERE,NOT REMOVEL) 'FROMJHE SCLN. FOLLOW-ING ANIDDIC POLARIZATION
AMO THESE- WEAE~-~REFERRED TO AS ANODICALLY OXIDJZED~. A~STUDY OF THE
STATIONAR. '-POTf_NTIAL SHOWED THAT AN INCR-FASE,~ IN THE PH 'OF- THE ANOLY'TE
LOWERED THE,TASSIViTY OF TI WHICH WAS~ATJTS 9TRON'GEST AT PH 13-14. THE
STATIONARYPOTENTIAL OF PT COATED,T-I,ANODES AT PH~0-13 WERE VERY MUCH
-ALIKE:AND INDEPENDENT OF~THE THICKNESS ~OF:THE Pr COATING. THE EFFECT OF
THE, rt BASE '~OR., COATED EL' PH
jH PT ECTRODE,APPEARED ONLY AT 14
ANd THIN PT
tOATINGS,. Q.1-1:.0 MU. IN A STUDY.Or-ANDOIC POLARIZATION OF TI 4NO PT
COATED~ TI# THE;,:_ T IIN ALK* AND CARBONATE SOLN'S"o PARTICIPA.TED IN THE
ANODIC PROCEW
PORES IN-THE:PT COATINGi. AT THE SAME C.D. THE
-CURRENT~ORAIN THROUGH THE TI O.F.PT CCATED',AN66ES~WAS APPRECIABLY HyrHTER
AT P14:1 UNL'IKE, AT ~ PH 9. 5 ~A'ND 14 ,p THE
3 THAN AT PH 9.5 OR 149
~PULARIZATION-CURVFS AT PH li ANV11.6 ON TI A0 PTICOATED TI WERE
-ANALO60USv_8UTVTHE- CURRENT DRAIN THROUGH TI ROSE.~~ITHE:,EXPTL. RESULTS
-LEAD TO: THE, CONCLUS I ON THAT OXT ON. , OF TI. IS THP MAIN REAsoN FOR THE
-'DESTRUCTI.QN PF,:,THE PT COATING IN ALK. AND,'CAROONAITC- SOLNS.
UNCLASSIFIgO..,

111 11 kdi; `11:1 11
N
USSR UDC 62D.193*1801t669.29
TISMIKOV, V. V., DAMILKIN, V. A., YA"MM&j. M. , DALKINA, R. I., and
MUMHUNA, YE. P.
_.'Iiydr~ogenation of Titanium and Platinized Titanium With Cathode Polarization in
~an_ Alkaline Medium"
Moscow, Zashchita Metallov, No 4, 1972 pp446-448.
Abstract: The authors studied the influence of platinum, galvanically deposited
on the surface of titanium, the duration of cathodepolari2atiOn, current densitv,
the presenceof potassium bichromate in the solution ion the quantity of hydrogen
absorbed during cathode polarization. The electrolyte consisted of potassium
carbonate and potassium hydroxide.- The Tesults indicated that hydrogenation of
platinized titanium increases with time according to ~a PaTabolic curve. The
influence of the platinum layer decreases with the passage of time. The presence
of bichromate in the solution decreased the~hydragenation of titanium, with and
without the platintun layer. The bichromate:probably reacts with the hydrogen on
the surface of the electrodej without separation of chromium. When platinized
titanium is stored in air, orparticularl in the carbonate-alkaline solution
y
being studied, hydrogen content drops -rather sharplywith the current off.

USSR uDc 6iz.74j
Yo. -Ya., ani YAIIK21-LEQIJ.KO~ X. A., Lfi.'Iboratory or General
Physiology, institute of. Fhysialogy , 'S, or a aneft Z`Zty. Acadei*r 0~ Sciences
USSR,,and Laboratory of Thornoregulation, ;a~stitute of Phy~iolo4y imeni 1. P.
Pavlov. Itovosibirsk-Leningrad
"The Te=perature Effect of Muscular Contractions After Adaptation to Cold"
I Vol 56*V INO 10, Out 7! PP 11
Leningrad. Fizio."Logichaskiy Zhurnal _SSSR L~,14,
ADstract.; ~7he effect of tae crgani~:mls adaptation to cold on the an LLit of' heat
ff
oneratel by DI-ascular contraction was qtudi~d, -no irath"I usea~ was based on com-
9
'vity.: :Ls dop;LcLf~d in
parison of the index of' bioelac-,,rical musouLar ;Lctl
peaks on the electromqogram iniuced bj coli.tremors and val'onta"-y coaLraction,
with the value of the increase in muscular tempera tu.t-e. Alb~.nu nale rats 20f)-300
grams in woight kept at tot araturea of 2 to 4~~I* in '04,ht. i.r4iv.Wui1 cages 'pe, -
i, rIp k
'ttL CoLtparioun purno-les,
a ng normal posture but limiting L4obility) were
control rats in a vivariiua 'were kept at a constant tempez-atura of& Z0"t_"0C. Tempera-
ture measia-ement was accozplished with tile 1101P. Of Q1(Y;tr(;dE!:3 RLtAUhQd 1,0 ITIUSMIIIIS
tibialis anterior and z-asculus trapeziu The investiza-ions bstabiished that
-,normally higher temperatures in the muscles. am. the resui~,.of muscular contractions.

L' - i LILL.
tpaEho lo.g~
USSR
Kokand Trachoma Dispen Sary, Fergana Oblast, Uzbek SSR
Tye Diseases Associated With Leptosp-liosis"
Tashkent, Meditsinskiy Zhurnal Uzbekiqtana,,No 11, 1971, pp 69-70
Abstract: The author examined and treated 12 persons (11 age 8 to 21 and 1
age 40) Who came for treatment of eye disorders , that developed 15 days to 8
months after suffering from leptospirosis in the course of an epidemic in
1967-1968 in the Fergana Oblast of the Uzbek' SSR. The- main eye diseases were
serous cyclitis complicated in two cases by-toxic neuritis of tile optic
nerve, exudative iridocyclitis, and.acute neuritis of the optic nerve. Tile
leptospiral etiology of these diseases was confirmed serologically. They
were differentiated from similar diseases on the basis of anamnesis, symptoms,
and laboratory and evideniological data. Treatment was syiiiptomatic and
included antibiotics and fractional blood transfusions. The results were
good In all-cases.

:i H: 11 -1 141:'] 1, ~: I 1 1 3

t3NOV70
PROCESSING DATE
uNciLASS1r,
Z/5
-_C,IKC ACCESSION- NO-AP010960fn
GP-0- ABSTRACT. THE FLIGHT OFITHE SCjYUZ 9
D
-IS NOW IN ITS EIGHTH DAYi EACH DAY 0 F YHE COSMONAUTS I S
~SPACECRAFT
~F_ILLED WITH SCIENTIFIC TECH141CAL EXPERIMENTS, WHICH:MAKF A CGNTR[bUTION
RSTAN NIVERSE -AND THE DEVELOI,*MENT OF-
TO THE UNDEt )DING OF THE U,
ccstooNAUTICS. VARIED IN NATURE, iHi-=y DEMAND 01-VER51. OYNAMIC OPERATION'S
-WITH THE SPACECRAFT. OBSERVATION OF CERTAI,N ST.ARS,,:pHor,*:)GRAPHING OF THE
'EARTH'S SURFACE, REGISTRATION OF SOLAR RADIATION, CORREcrIONS,
ORIENTATION ON THE SUN FOR THE GENERATIGN-OF ELECTRICITY BY THE SOLAR
BATTERIES, FOR INSTANCE, ALL THIS REQUIRES'CERTAIN filANEUVERING OF THE
YPE POSSESS VERYBIG POSS
SQYUZ T
SHIP* ..SHIPS OF THE FOR
-EVOLUTIONS DURING SPACE FLIGHT, THIS .13EING, WENTLY PROVE-0 BY THE
~CURRENT FLIGHT.,10RBIT CORRECTIONS,WERE.:MADE ON THE 5rH AND .17TH ORBITS
-OF qlScyUz 911.1 SUCH OPERATIONS ARE CC-NNECTE.D. FIRST; OF ALL W ITH
INCREASING THE HEIGHT OF FLIGHT SO:THAT ;THE SHIP WOULD PIASS OVER PRE SET
AREAS AT A DEFINITE TIME. THIS IS ALSOINEGESSARY IN TRYING OUT AND
SYSTEMS ENSURING ORBIT CORRECTION AND IN GIVING COSMONAUTS
~..~EXPERIENCE IN PILOTING THE SHIP. BUT BEFORE AN, ORBIT IS COPIRECYED THE
~SHIP HAS TO BE ORIENTED, THAT [Sw MUST OCCUPY A STRICTLY DEFINITE
POSITION IN SPACE. THESE OPERATIONS CAN.BE~ACCOMPLISHED BOTH
AUTCMATICALLY AND MANUALLY* THE CREW OF "SIOYUZ. 911, TWICE ACCOMPLISHED
THESE COMPLEX MANEUVERS WHILE PILOTING THE SHIP BY PlEAN.5 OF mANUAL
CIONTROLS. USING MANUAL CONTROLS, THE SPACESHIP.IS COMMANDER ANDRIAN
IKOLAYEV IGNITED THE CORRESPONDING~ JET 'MICRO E.NGINIIS A,,,,,D TURNED THE
N
A WAY.THAT THE IMAGE OF THE EARYH:!OCCUPTED THE CENTRAL'
SPACESHIP IN SUCH
PART OF THE SCREEN OF A SPECIAL SIGHT.
UNCLASS 1)
I N7-1-11

PROCiESStNG DATE -13NOV70
61 UNCLASSI Ft
,~.-CILRC ACCESSICN NO-AP0109602
.,A-&.sJRACT/EXTRACT--AT THE SAME T 18F THE b IRECT ION OF,JHE EARTHIS MOVEMENT
BECAME PARALLEL TO THE SHIP#S LONGITUDINAL AMS) THAT IS, THE &,HlP WAS
~.ARIENTED. THIS POSI TIOi WIAS- MAINT AINED BY 14EANS OF MICRO ENGINES THAT
ARE swircHED ON FOR CERTAIN PERIODS OF, TIME, BY COMMANOS FROM GYROSCOPES
THAT "REMEMBERED'' THE SHIPIS IfqtTIA .L G.RIEN TATION. ': WASH IN'G TO* MOVE TO A
-NEW OR81T, THE COSIMIL;NAUT PRESSES A,' BUTTOV-SWITCHINA.G OPJ~THE ENGINE.
1::_: lvS0YUZll SPACECRAFT CAN MAKE MANEUVERS TO AN ALTITUOE OF 1.0300
-KILOMETEPS. jr
WAS NOTED BY SPECIALISTS AT THE MA14NED FLIGHT CONTROL
N S E -WSOYUL-91! DURING THE ORBIT
,:CENTER THAT ALL ACT[Os OF THE CR Iq 01:
:.-:.GOR,RECTlCr4 WERE EXC~7PTIGNALLY PRECISEs-_/'-THE INEW OR ,ilr IS VEPY CLOSE To
THE PLANNED ONE. ANOTHER TYPE OF: MANEUVE."l, WAS CAR ON THE THIRG
RIED GIUT
DAY OF FLIGHT WHFN EXPERUMIENTS WEkE :MAPE INVOL VING:30RIENTATION BY STARS
:FOR THE AUTijN0,110US NAVIGATION OF 'THE S"IP~ WITHOUll"THE P,ARLrICIPATfON OF
FACILITIES. THIS MAIN(OEUVRE IS BASED ON THE~PRINCIPLE THAT IF ONE
.-OF THE AXES OF THC~HIP IS DIRECTEOP SAYt AT THE SUN AND THE OTHER AT
SOME CELESTIAL BOOY, THE SHIP WILL OCCUPY A DEFINITE: POSITE&N IN SPACE.
FLIGHT E14GINEER virALY SEVASTYNOV ~S ELECTED A BR[Gtif, SrAR, THE VEGAs ON
THE NIGHr SKY, STARTED THE ORIENTATION
ENGINES AND ORIENITED THE
SPACESHIP BY AN OPTICAL DIEVICE. OF GREAT INTEREST ARE EXPERIMENTS TO
DETERMINE THE LOCATION OF THE SHIP V AUTONOMOUS MEAr4S,;,WHtCH WERE
-C-01-JEUCTED ON, JUNE FIFTH AND EIGHTH. RF50RTIP.4G_'TO 1,111E MAiNU4L SYSTEM, THE
_SIHIP WAS 0RlEiNfATE0 CN THE EARTHiBEFOPE!ITHE.FLIGHT ENGINEER MADE THE
NECESSARY MEASUREMENTS AND COMPUTED 'THF:PARAMEI'ERS OF THE ORBIT.
UNCLASSIFIED
---- - ----- --------------

415 061'-, UNCLASSIFIED-.: PROCE S S I NG DATE-13NOV70
IRC ACCESSION NQ--AP0109602
.,-"'ABSTRACT/EXTRACT--CCMPARISON OF THE RESULTS OF THE COMPUTATION WITH THE
DATA OBTAINED BY SURFACE FACILITIES BROUGHT OUT THU IR CGINI~ IDENCE.
OPERATI DNS MAKE IT POSSIbLE TO TEST T RE METHODS Or- SPACE
NAVIGATIONr ASSESS THE PRECISIUIN Or- INSTRUMEWS AND THEIR PERFECTIOrl OF
THP SHIR AROUND
OES I Gm. ANOTHER DYNAMIC MANOEUVRE IS THE n Tlyl I S T I NG CF
ANY OF ITS AXES, FOR IINSTANCE, WITH RFGARD :TO THE SUN. I-HIS OPERATION
IS, MADE BY SWITCHING GN T14E SMALL THRUST, ENCOINE: FOR TIME. GEFORE
THE, BEGINNING OF THE rivi.ST T14E -SHIP IS ORIENITATED IN SOCH A WAY THAT THE
AXIS PERPENDICULAR TO THE SURFACE OF ITS :SOLAR 134TTERIE.'i COINCIDES WITH
~-THE DIkECTICN TOWARDS THE SUN. IN THiS CASE THE SOLAR, 13-ATTERIES RECEIVE
A.~MAXIMUM.FLOW OF FLIGHT AND, HENCE ENOUGH ELECTRICITY IS GENERATED FOR
CHARGING TF-E BUFFER CHEMICAL BATTERIES~. MUCH FUEL WOULD BE NEEDE0 TO
-MAINTAIN THE SHIP IN SUCH A POSIT16N FOR A: LONG' ENOUGH T11PIE. THAT IS
WHY AT IS BE LNG KEVOLVF0 AROUND THE. SHIP ;:SUN AXIS AT A SPEED OF SEVERAL
DEGREES PEP SECOND. THANKS TO THE HYDROSCOMCAL EFFECTt: THE SET
-POSITION IS MAIINTAINED FOR A PROLONGED TIME% IN THC:
COURSE OF FLIGHT ON
6 AN "OBLIQUE TWIST" OF THE SHIP WAS ALSO CARR(ED OUT. AS
.-DIFFERENT FROM THE ONE JUST DESCRIBED, IN T.HIS ~PART:KULAR CASE THE AXIS
OF TdIST-IS PEPPENDICULAR TO THE PLANE OF THE PANEL:5 OF SOLAR BATTERIES
AND Fr-;RAS A CERTAIN ANGLE WITH THE,I)IRECTION TO THE.SUN. USING THE
.-::...mANUAL ORIENTATION SYSTEMP A COSMONAUT CAN CHANGE YHIS ANGLE AND SELECT
TH E N E C E 51SARY CONUITIONS FOR THE REC,IFAROING: OF T14E OIJFF~R, CHEMCAL
~BATTERIE

-1 . I . I ; . , . ~. : ~ : I . i, i
~~- 5 - - ~061 -1 - UNCLASSIFIE6. ~*~ , k!
OtES81NG UAT&-~-BNOV70
COSMONAUTS
WORK OF THE

(0104957
'lllic" Nr. Ref. Code: .2 _,3
--:AUTHOR-- SCIENCE~COMMENTATOR
TITLE-- MANEUVERING IN THE ORBIT
-.NEWSPAPER-- SOVETSKIY PATRIOT, JUNE 100 1970, P:1. COLS 5-71
ABSTRACT-- IN EVALUATING THE CAPABILITIES OF THE,WSOYUZ-9
YAK114ENKO STATES-- *THE SOYU2-TYPE SHIPS HAVE VERY EXTENS14
CAPABILITIES FOR BRINGING ABOUT -AN EVOLUTION OF SPACE FLIGHT". HE
CLAIMS THAT SOYUZ-TYPE SRIPS ARE CAPABLE OF PERFORMING -
.-MANEUVERS AT ALTITUDES UP TO 1,300 KILOMETERS, THE AUTHOR PLACES A
SPECIAL',EMPHASIS ON THE ABILITY OF ASTRONAUTS OF THE SOYUZ-g TO
_.:~:~,MANEUVER AND TO ORIENT,THEIR SHIP INDEPENDENTLY Of GROUND CONTROL.
REEL/MME
1987:1840

,-::LIZ 021
UNCLASSIFIED PROCESSING DATE--IISEPTO
'-TtTLE-CALCULATION AND STUDY OF THE INFRARED ABSORPTION SPECTRUM OF
HI0HY0ANTOIN -U-
0-R -8 -R.P., YUKHIMEYSt V-N-9 YAKIM---NKO# V.I.
L EEDEVI R.S., CHUMAKOVA#
H
-INFO--USSR
COUNT Y.Op
29-33
-13( 1) t
_s6bRcE__jZV. VYSSH. UCHE8. ZAVED.t'FIZ. 19,709
------- 70
_DATE
":~SUBJECT AREAS-CHEMISTRY
"'T IMIDAZOLEj. FREQUENCY:~VIBRATIONI HYDP.OGP.14 BONDING,
0Pl,,C:,'lTAGS- IR. -SPECTRUM,
~:'~-MELECTRIC CONST
ANT, ORGANIC SULFUR CIOMPOUNFO
"~fCONTROL MARKING--NO RESTRICTIONS
IMENT CLASS- UNCLASSIFIED
,~J)OCU
PROXY REEL/FRAME--1988/01*T2 STEP ~10--UR/0139/701013/001/0)2Q/0033
CIRC ACCESSION NO--AT0105248
UNCLASSIFIED

2/2 021 UNCL ASSI FI~D PROCESSINS DATE--11SEP70
Cl R CACCESSION ND--AT0105248
.,,ABSTRAGI/EXTRACT--(U) GP-0- ABSTRACT. THE XR SPECTRUM (400-3500 CM PRIME
FwTH10HYDANTOIN (1) WAS MEASURED; THE FREQUENCIES OF NIQRMAL
NEGATIVEI) 0 L
VIBRATIONS WERE CALCO. ON T14E BASIS OF A 11ECH. )A00FL (SYM. A
WITH REG RD
TO T14E RING PLANE, GIVING 18 SYM. A PRIME:AND 9 ANTISYM. A DOUBLE 0qlmC-
VIRRATIONS) AND COMPARED WITH THE EXPTL. ONES. Tx,4E FREQUENCIES AND
ASSIGNMENTS TOGETHER WITH THE KINEMATIC COEFFS. OF I ARE TABULATED. THE
FREOUENCIES OF ALL INTENSE LINES IN JHE SPECTRum nF- I ARE COMPA.CZABLE
CALCO. ONES. TH5 6ANDS AT 3231 AND,3118,CM PRIME NEGATIVEI
(WHICK 'WERE -.N!3T. CALCO.. I HERE '' ASSIGNEDJO THE INTRA OR INTERMOL.
INTERACTIONS,. THE' FXT~TENCE OF AN INTERMOL. 14' BOf'0 INCPEASES IN THE
SERIES It-RHODANTNE# AND HYDANTOIN. ON THE BASIS'OP A COMPARISON OF THE
_OIELEC. CONSTS. EPSILON AND THE FREQUENCIES 00 CWSUB2 SCISSORING
-,VIBRATIONS OF, I (EPSILON EOUALS 3N RHODANINE:(EPSILON'EQUALS 3.06)v AND
21THI012~1 4t-OXAZOLIGINEDInNE (EPSILON EOUALS 3.28)'.t THF BA-40 AT 1412 CM
:.PRIME NEGATLVEI~ WAS ASSIGNED TO THE- CH~ S002 SYM. EFOR, ATION VIBR TI NS.
D
R
-THE JR,SPECTRU4 nF I CAN BE !NTERP EFTED By cnNSTRERIKIC, A C SUOS
..-SYMMETRY t-OGETHER WITH A SLIGHT -TkF W14LILP- AND'.AN .4;PPROT. C SUB2V
SYMMETRY T04ETHER WITH A SLIGHT EFFECr OF :5
D SU85H YMMETkY FOR THE RING.
UNCLASSIFIED

uDc. 621.374.5
USSR
I., IVANOV, V. I., RUSAKI Yu. M.
'A De~rice for Delaying Radio Pulse Sip4ls"
-ytiya, Izobreteniya, Promyshlennyye Obraz e Znaki
Moscow, Otkx tsy, Tovarnyj
-hor's Certificate No 319060, Divisicn H, filed 5 Feb 70,
No:32, Nov 71, Aut
published 28 Oct 71, p 173
Translation-. This Author's Certificate introduces a device for delaying
radio pulses., 'rhe unit contains a contro.1 signal oscillator, a controlling
signal pickup and a multistage delay channel'where eabb stage consists of
a delay line with uniformly distributed taps a tap col~trriutator, a memoi7
unit and multichannel analyzer controller..'As a distinguishing feature
of the patent, the precision and stability of delay are-improved by con-
necting the inputs of the analyzers for all stages of the clicannel through
switches gated by the controlling signal pickup to the corresponding inputs
ofthe tap commutators, the inputs of the~reference channels being con-
nected through a switch garted by the controlling signal picku-P to the con-
signal oscillator. The outputs of the: Punalyzer ch-ailnels are connected
112,

- 7 5 -

Vitrogen Compounds
USSR UDC 632-95
MM I MOV, 11. N. , TMASKIN, B. A. , VORCLIKOVA, V. V., YAKDOMO, Ye. F., and
~SABLIUA, I. V.
"Thermal Stability of Quaternary Salts of 4,41-Dipyridyln
V:zb. Xhim. sredstva zashchity rast. (Chemical Protectionof Plants
works) No 2, Moscow, 1972, p . 306-311 (from. FLZh-Khimiya, No 22,
~.Collection of p
~25 Nov 73, Abstract No 22N572 by V. A4 Kozlov)
Translation: A study was made of the thermal stability of~compoLlpds -with the
general formula (I) ZX_ = I, MeOSO
31 (14eo)2F021 and (MeO)MeS)-PO,4 and II by
paper electrophoresis. acamples. (1) 15 ml ~of HeI is added to 0.02 mole of
4,41-dipyridyl (III). The mixturo is sealed in an ampul-and allowed to stand
at 2(P for 24 hours when -the crystals are filtered off ard washed with ether
to obtain I (X = i), yield 72%, melting point 240o (alcohol containing vater
3:7)4 (~eo)(MeS) F02) (10 isobtained in a sirdlar manner by heating
JI
-to 500 for 12 hours. Purification is carried.out by repre6ipitat).on, adding
an acetonitryl solution of I a drop at a time to acetone~at -50 to -700 to
obtain la, yWd 34%, melting point 59-61.5c'. (2). A mixtUre of 0.03 mole of
("'L-0)3'PO and 10 ml:df water -is heated.to
IN, 0.04 tole o 90-1.001 for 5
1 3

USSR
MINIKOV, N. N., et al., Khim. aredstva zashchity rast, No 2, 1972,
pp-J06-311
hours in the presence of 0.1 g of alkaline activated cm-bon (A brand). The
carbon is filtered off, the filtrate evaporated in~a vacuum, the residue kept
in a vacuum (40-5&/0.2 mm) and treated with methyl ethyl ke'Llone. The mass
el7stallizes and purification is carried out by repreci itation to obtain I
P-1
ZX = WeOY027(Ib), yield 90%, melting point-117- 1200- 0.03 mole of III is
added to 0.06 mole of (MeO) 3-Po at 6o-65%, heated for 2 hoursAo 7-800, left
to,stand for 7 days at 200 after.,which the, crystals gormed are washed with
dimethyl formamide~ dissolved in MeCN, and pc~,,jred a drop at a time into AcOA
chilled bydry ice to obtain II ZX = MCOY-022i yield,P%, melting point 95-
I is kept at 90, 120, 150, and 2000. '~(X = 11 ReOS03) wben heated for
4 hours to 2000 forms a monoquaternary salt and when heated to over 2000 it
forms the original III. 1b at 901 forms on an'electrophoregram the spot of a
cation of a monoquaternary salt within 3 hours and at 120 and 1500 within 20
to 10 min, respectively. Under these conditions the cation of N-methyl-
pyridinium is formed within 40 and 10 min, re pectively., la is even less
s
stable at 90, 120, and 1500; the monoquaternary salt is Parmed1within 20 and
5-6 min, respectively, and at 120-1500 the cation of N-methylpyrldini= is
formed within 30 min. 11 is not broken down at 900 but:at 120'and 1500 forms
2/3,
19

~- ~. ~ ". - - 4 - . -, ; - .. . 11 i- -'. I
1 ~. 1-1-1- it " 11- J-J ;

USSR UDC 616.28--001.34-091.
'N
PROW* L.. S., Y.0-RETSOV, N. I., YAKDETSVI. 1.~ M., JOROZ.011. V. U., Candidates
of.Hedical Sciences, BUGROV, V. 0. C-ididates of
Technical Sciences
rAftex Single Exposure to
"Pathomorphology of Trauma of the Auditory,Analyso
Pulsed Noise"
Lk Otorinolaringologii, No 1, Jan/Feb 72, pp 37-43
Moscow, Vestni
Ahstrp~ct: After a single I-second exposure to hi gh intemsitv (155-173 db)
sm-id' ir;-V-Ase~s of a sinusoidal form and a frequency of 10-20CO 112, guinea pi.,gs
r'uffar partlal or rc~k- lete 10S~5 of hearLag, 4up- to mechwAcal dastruction or
nrecrosis of the organ, of Corti. Pathological procasseS terminate With-in 3
da~.s. Welve days aiter expoiz;-ure to tha "Less traumatic lev-frtcluency waves,
-j..r4=0'j j=t:jo Medi, reziencv, scundz,
a E=- to th= &7~4~za_l 9 2nd high freg- 'acy sounds izdace
-(-Ie ees-tructian of- the gan- f Carti.i -_~Ueldle ear injury is
or a
jad =-611cal t"ME"ers of lh~ug. re=zin Intact.;

621.373.521.1
USSR UDG
V
MOVI 11
fect of Flicker Interference of Power
Supplies an the~Stability of Tran-
sistor Generators
Uch. zap. Gorkovsk. un-t (Scientific,~Iotes of Gorkiy University), 1970, vyp.
pp 58-62 (from RZli-Radiotekhnilka, No 9, Sep 70, Abst-ract No 9D2'4)
Translation: The flicker voltage fluctuations.of the power supplies of
transistor generators affect the stability of the generators. The present
paper is devoted to an analysis of the effect of flicker'fluctuations of the
bias of the collector and emitter junctions on the:fluctuations of the ampli-,
cude and frequency of the transistorized autogenerator oo cl. 11at ions. There
is one illustration anda five-entry bibliography..~

Nr* Abstracting Service: Ref. Code:
Acc
.
Cy.,Ej,1jCt__L :ABST.

r' 712631Y SIr t fiitrAte~0(1411 --meal uitoatt-W'Uer vy%om.
,
'V~1 Z,~Ddr
A, E. V X'IaLsov- B.'P, (1158R).
Zh.
- -
771 i Wifties "t
E
M
item, I i at 2W and in
HID and nd V11,
'
resp.) at '15 -and 35c ar~ zivem -System I
llas Oh~et soly'. iso-
fherms corropopoiag tc);.,9r (N(WaA146, Sr(,NQ,)';' i~nd
'
and aalv
In systeins 11 and 11 ouly 5r(1N _0 foim~ ~t
x

am-
Sr(N04'2 forms at:36. ln"thes~ ~Y'ae;~% the Col !or ith'c
t
Dent increasex, Wit Increasing COD
pla h t~e At

This Mnd:111 ari-I its
prove-i compkx-forintion hi~ ms 11
absence In system 1. HmsR 'J

REEL/ FRAME

_77-
USSR UDC.155.3+599.88.019.941
NEYSTRUKH, M. N. and YAKI (Reviewers)
MOVL-V. P
Pamyat' u Antropoidov. Fiziologicheskiy Analiz: (Memory in Anthropoids,
A-Physiological Analysis), by Firsov, L. A., Leningrad, 1972, 231 pp
Leningrad,~Fiziologicheskiy Zhurnal SSSR imeni I. M. Sechenov, Vol 59,
No 9, Sep 73, pp 1452-1453
Abstract: As a result of many years of investigation Firsov has concluded
that the chimpanzee demonstrates a fuller use of:subsOiquent reactions than
other animals. He also maintains that subsequent conditioned reflexes are
connected to long-term memory, while.delayed reactions are a manifestation
of operative, short-term memory.. Firsov observes the power of elementary
abstraction in chimpanzees, such as generalization a-no representation.
This.monograph is considered in important contribution.to physiology and
primatology-by the reviewers.

UDC
-K-
a

rig 0-1p
LuLe) j.~)i
No 7, J-Ll T Vrj-trflc-~ i"o Tv, 2'
Trans !a' ion - A on - p 1
_i n t r at J on th~L .rmj7,Cej wl ne-miconduv~c-,., i1j. c-c -`.L
tha on~

-2
in the econc~~;U"- ~V'ld fl"o- the std;-,
fo!-
IT
A
is d-sc- 'fOC"~ C W',-!s. iJJ.u-f"-La t i I 1:i. f~ ;')-n
Optimum ve r s 10 %, of ",L r;~-Wft with an overall ltrrol of i
lc

p to 30 wnd I structed ns nai. tyanp- f d-vnlo~iai-
w COOT IS CC]
-rs
ry fo, vall~~visir-n ree
grated circuit eivc On e
S.

USSR UDC 532.5
'osc
'OV, Yu. L: 1, 0177
BONDARENICO L. A.*, and YAKr
"The Force Acting From the Side of the Fluid Flow on a Garved
Thin Body of Circular Cross Section!'
Yloscow, Izvestiya IU-,ademii Nauk USSR, Melchanika Zhid-kosti i Gaza,
-No 1, Jan-Feb 73, pp 9-12
Abstract: Res-alts of classical hydrom-echanics. caid -oreviously ob-
tained results by one of t-he authors (.Yu. L. Yal~:J_Mov, Ibid.*-
19701 No 2), concerning the stre,-m--Iining o -Lo a. cylinder by an aar-
L 'low ure generalized for the case o-.':' the motion of
bitrary ~Iu i d f - .:) -
a curved thin body of circulav cross soction:An an arbitra.ry throc-
-dimenoional potential floq of an; ideal non-oom%-M,~if-.AbIv, fluid.
The solut-ion. of the problem Iro found- by flotermining sin.~~ilarj_ties
on the curved axis of the body,undier.the ascumption that the -.Eunc-
tions chara2terizing the distribution of singulaxities on a len,-.-tl
1 -of the anp-Jyred section of the bbely depend slightly on the ch-1-Int-
&- 1: ncll~. ractor of" the variable along the: axi:~ of tlne body. 1-11 e~x-
Pression. is derived in vi-hich the first three ricmb~_-,rs charact-crize
them force acting on an arbitrary contour of' =- all. diriension-s m
U
five bibl o7,-., hic
a -Dlane -ootential fjovj. Seventeen formulaq i " nwo re
ferences.

USSR UDC 616.72-001-008.822-12-073.6
ROXITYANSXIY, V. 1. Kam' Pedagogical Institute and
Kazan' Institute of =uazaAo Zog3hr 'aE+Ahopedica
"Proton ReLwmtion in Joint Tissues After: Trauma; Study Based on Nuclear
Magnetio.Resonance Data"
Moscow, Ortopedlya, Travmatologiya i Protezirovaniyap ]to 9* 1971P pp 35-41
Abstract# The time of proton relaxation In the joint tissues of rats mas
investigated by the nuclear aagnetic~resonance spin echo method during the
month following the inflicting of a trauma, The tissues of the intact knee
joint of.white rats have I to 2 gram of.waterperlgram~of dxy substance. They
are characterized by absolute values of:spin-4ttice re.laxation (T and
spin-spin reUxation (T2) which are much smaller than those: for pure
waterl the TI tT2 ratio is about 10. The first 3 day's aftor the trauma
were marked by a considerable longer t1mie, of proton relaxation (T and T
2)
and little change in the T IiT. ratioe There was.a statistically Insignifi-
cant increase in water per gTan of dry substance and Z substantial decrease
iii'structural water. Ton days after the trauvA there was a moderate decrease

USSR UDC 534.
NAGAYEV, R. F., r OVA, K. S.
"Impact Interaction Between a 2-Mass Elastic System and a Nonmovina Plane"
Mekhanika Tverdogo Tela, No 6, 1971, pp 1.4-24.
ABSTRAM. The process of interaction of a nonmoving plane with a free system
consisting of two bodies connected by a linear spring (2-mass system) is
studied. It is demonstrated that in the process of the interaction, the
number of impacts of one of the bodies of the system,with the plane is deter-
-mined exclusively by the ratios of masses of the body and the velocity re-
storation factor upon impact R. Using methods dcveloped in an earlier work,
the area of change of these dimensionless param. Ieters of the problem within
which the number of impacts is infinite and, therefore, quasiplastic impact
occurs is determined. Statements are~made concerning the correspondence
between initial and final dynamic.states of the system and, related to this,
the effective velocity restoration fELCtOr upon impact. The results of the
Mork can be used in the investigtion s- of a number of vibration-
dynamic
Of
..impact mechanisms.

1 ~, .- . . . . ., -... a
-, - - .4 !;;~--.-~!jlll;-Fj-,
. ... .... li;411: -1 -.1 1 1 1 -1. -

I Fl PR'0CESSING DATE OCT70
-:06 UNCL SS E. 23
~7 C IRC ACCESSION NO--AP0125112
4BST,RACT/EXTRACT--(U) GP-0- ABSTRACT. STATISTICAL ESTIMATION OF A
-;POSSIBLE EMUSSION EXCESS OVER EQUILIBRIUM DURING A MAXIMUM BRIGHTNESS
'PERIOD OF CLASSICAL CEPHEIDS OF THE GALAXYp TAKING, INTO ACCOUNT THE
'PHASE SHIFT BETWEEN THE MOMENT OF MAXIMUM RADIATION jr4l-p4SrTY AND rHF:
MOMENT OF MAXIMUM CONTRACTION OF A STARp.-A COMPARlSON OF PHOTOMETRIC
~-:AND GE04ETRICAL RADIAL AMPLITUDES FOR A TOTAL OF 5,0 VARIABLES SUGGESTS
THE PRESENCE OF'AN EMISSION EXCESS. CONVECTION IS.BELIEVED TO BE A
_.POSSIBLE~CAUSE OF EXCESS EMISSION DURING A BRIGHTNESS MAXIMUM.
-MOSKOVSKII GOSUDARSTVENNYI UNIVERSITETt; MOSCOW, USSR.
p
Uri, C- L A S-5-1 F I E D

USSR UDC 47.26.118
FRIDWTDI S. V. 3 L aak and K1,14A G. n. ceased), Deua-~m~en-c
de
of T-echnology of Basic OrTanic and Petrochemical'Synthl sis, Kazan Institute
of Chej-dcal,Technolo,:;y imemni 5. M. Kirov
"Study of the Reaction between Phosrhoras Tricholorde and. o-Allyl--p-Cresol"
Ivanovo, izvestiya Ilysshildl Uchebnvkh Zavedeniy, Khiriiye. i TTimicheska-ya
nol=iya, vol. 13
Tekh. no. 12, 70, VP 1:76-0-1:161
Abstract: Tbe reaction of o-allyl-73-cri-:!sol ~with phosphor~as trichlorL ?. has
been studed. Fractionation of the reaction rass, yiplcl'~etllin, anal,ituically re
--id 11)
f ox-r-, two fnactlions -- diaci'd chlormie of
and the acid ch-loride of di(o-allyi-p-cresyl) phosphoro-as ac--'-- (II). T'. f. e
reaction was conducted in cquimolar ratios ai.d the famation of product 11 may
be c=Loined af; tiv, reactiom of nuclcoplii lie sm il; ~0 Ututi-on of' tho secord
chlorii-e- atom a-, well as 1--v coneurrent ~-he Dbtair!C-d aci-I
W--
chloridec, L-, colorlp.,r,
all -Odor to !"cift tic'I'd
alcollol in diethyl in t1le -oresence of triet-h-i-irOic for cembinim- th--
liberated hydrofen chloride. This reaction, as we] I e.91 all other op--ratimis
-L/P

Device~
7T, UDC 631.327
Douov-Lsov, -.q. S., mwavs A. 1-1. 9 KOTOVf V. 11. L BK Vi-A.I., A., NE.STERIKIIIN,
--RMqllll:-V, K. F., TOKAR-EV, A. S. MMIMM A. Novos
_YU. YE. 01;'- Pi ibirsk
"Prolilema of Constructing Devices for Operative Interaction of Ilan wiLh a Cori-
puter"
Novosibirsk,. N a 2, 1.9 7 2, pp ~5-39
-to bas
Abstract: Two tvpas of devices corresponding to d cic requirements for
ryatems, for opc-~rovivc- inveractimi of man with, a computer -- a computer operating
in the timic ~Afmn vocie and poripberal dcviccS tiumberimt, I to 1,000 ---
have boert at LT*.u iv;U'vilto. of Auwmal-ion au& lectronutry U" Lhu
Siberian of 'C'le USSR ACCILICTIV Of SCR_'1CV5. Olle Of thC-IC deVICCS --
the Ekrz~n ~iscufscd previously tr).~ S_ blolgovesovi et ~J, Avtonctriya,
No 4, 1971; B. S. Do"govesov, et al., Avtometriva, No 410 1971; A. 11. Kovalev,
et al., Avtcnctriya, 4. 19711. Tho other - the Simbol -- is investj.gd~ted
iT, t-ne irosent --rcicle. bitach diagram oi;.-' the Si:-,bol alplhanui,.ieric system is
for the Vjriot~'V o-Oratin T-:1j~IeG of the Syste:1
-Ill. vot* -; of nv:~ cNecu-zed, by -,loans
are
I 1 0 j:
of a C------ v C!,*cvc. thr. fastest
cyck of the control
a Lc; W.C LIJ! riTi!-,1(', jAlk,-! iWE-Lyuctions

71,
R
OLGOUSOV, B. S., et al. , kirtometriya, :o 2, 1972, pp 35-39
are processed sir-ultancously; a very high cycle frequency is !,Llected 2.5
millihertz. The operating logic of the device. can be chanfed. One of the basic
parameters o-f the cy)erative interaction device. alon- with. broad futictional
possibilitic-s is the inforiuatioa capacity. Thus, much attention was given to
the high spced of individual unitsi in particulari the sipeed of the ssyribol
ptor. The prograrimed segmient nethod;wasq. used as the basis Alor constructin(g,
Senora
~tha -Symbol g-c-nerator which provi6es I,W4~ symbols- with ,,in ii:m-e regeneration
frequency of 50 hertz. An ex~miple image p4otograph fro~m the Sirfbol screen is

:,-:-DOCUMENT CLASS-UNCLASSIFIE0
PROXY- REEL/FRAME-2000/1328 STEP NO--UR/0198/fO/000/006/0093/0096
C IRC ACCESSION NO--AP01249'78
--UNCLJ"_R_fF-l&D-

"MiMMUHMn 'AgVIONIN ,inilISNI 1.ANa13i1O'dIS319vsbN.-
I INSA3VIOMNI , ~.,Al 1-1 10VA *T10H ~H_L :40 300-3 AHi IV
N01IVW1N3JN0D SS31JJ_S 3HI 141 3SV3HDNI 31OV3011ON V A01411M (9NINGH-LEM9141S
-1v i.Ldvc4, :io qvilv ~3mi m.um) oamTd 30 NVO IN911313
~11-11 :10 B19191i Im twistei : iv i x j rqn 'M1*)N31'd3dX3 M-ld V '80:f IMI-1
_11WIS S-_)V1U3,IvW
NMOHS si 11 *3106 Ellii :jo IvmI! Wolij 91'JI'dg-J-410 ONIV 01 MV
FIN' I KI-711 11 e,)N3VIS Z10J OjUMJ~Qd B*dV RSV') ~f_31IVI 3HI ~Md sNouvino-1VO
*IMOINOO 51.1 30 ~SIIA'dl (3IJS0dd0) 0141 IV 03N31-119N3blS k11V)1'dI3Wh',ks
-31DH V M ONV 1:110 ',)NO-IV 03NNIONI~Jl~ DICH V (T) MDJ SW3-_)UQ'dd
14011V',~IN30NOD SSDOIS: OHJ. j-o l4olin-toS. ativ %lonvimdDA _~Hl Di ~Inrjik'H:)~)_L
r,)1\f1HJ.0C4,.*S ~jnoINOD T -40 ND1IVD11ddV 10 V ~f I S 0*,kl -0-c19 (n)--I:MiJX9/I3V'd.Ls9V
R161;ZT0dV--0N
N01533)OV
0LA0f,jL2--31V0 9N1SS9:)0',xd, 031JISSVIONn 13z0 Z/2-

0-
USSR UDC~536.45
SF2IL'RAYN, E. E., YAKIMOITM-. K.; A.,. and]TSITSIARKIN, F.
"Investigation of Boron Oxide Density.at-_.Hith Tempera'iur,~s by the Hydro-
dynamic Weighing Method"
1*cov, Teplofizika Vysokikh Temperatur;.Ak
adcmiya Nauk SSS)k, Vol 9, NQ 1,
Jan-Feb 1971, pp 67-73
Abstract: The hydrodynamic weighing metho& onsists of immersing a molibdenum
c
sph suspended by a thin.wire.from a b-i-lhnce into liquid boron oxide; the
ere
sphere moves up or down depending on the~.pull of . the balance; the movement
is slcrj due to the high viscosity of boron-oxide, The velocity of this motion
'tio
is plotted.versus the balance pull.' The equilibrium.condi n corresponds to
zero velocity, it is used to calculate the.-density of the boron oxide.
The.density obtained by this method in the,,temperature: range from 850 to
2600% is presented. The relative eirot iswithin 0,25%.

'008- r-ESSING DATE-18SEP
UNCLA~Sf- 70
Mir.-TTLF-ISOMERIZATION OF ALPHA-IN-(-gF-TA"CYANOETH'YL)At4l~-40):KETONES TO
AMINE,
LUNITROL MARKING-NO RESTRICTIONS
CLASS:-UNCLASSIFIED
.-.-PROXY REEL/FRAME-"1937/1108 STEP NO--VR/O4O9t7O/OOO/OO2/0260/0281
CIRC ACCESSION NO-APOL04506
-UNCLASSIF[FD-

Hi..
.. A !11'!.;!.!;;!; ~": : ~ !,:.

2/2 020 UNCLASSI FIFO PROCEi SING DATE--04DECT(,
CIRC ACCESSION NO--AP0140527
.ABSTRACTIEXTRACT--(Ul GP-C- ABSTRACT. A NEW METHOD IS SUGCESTED FOR
LOC:ALIZATION OF A FALSE MACULA- WHICH INCLUDES THEi STUDY OF FIXATION
CHARACTER ON A CAMPIMETER. THE ~TRI AL-1 OF THE METHOD SHOWED 1T TO BE
SIMPLE'AND ACCESSIBLE FOR ITS CLINICAL USE.
-A CLIINICAL TRIAL OF THE
CAMPIMETRIC METHOD OF LOCALIZATION OF,FALSE MACUL14 WAS PERFORMED ON A
NEW DEVICE PLEOPTOCAMPIMETEk. A CO~
MPARATIVE:EiALUATIC'.'N OF THESE
:CAMPIMETRIC AND OPHTHALMOSCOPIC HETHODS USED;FOR 1HE GETERMINATIOt4 OF
FIXATION c
CHARACTER WAS PERFORNE0.11111 5S.PATIENTS Will) SL4FFERED i::ilom
AMBLYOPIA. FOVEAL AND PARAFOVEAL FIXATION IS R.EY.EAL1-0 MORE FREQUENTLY
WHEN STUDIED WITH THE CAPIMFTRIC. MUH00RATHER THAN WITH THE
OPHTHALMOMETRIC ONE* THIS. 15 CONNECTED WITH THE~ BREAK OF NON STAbLE
FOVEAL'OR PARAFOVEAL FIXATION DUE TO A:BRIGHT LIGHT FROM A BIG
OPHTHALMOSCOPE WHICH BLINDS THE EYE. THE CAMPIMETRIC JMETHOD FOR
OF FIXATION CHARACTER IS CONSIDERED:UNDER MORE EXPRESSED
PHYSIOLOGIC CONDITIONS TO ALLOW REVEALING'.LOCALI.IATION OF FIXATION IN AN
~AMBLYQPIC EYE. THE DETERMINA71ON OF FIXATIOU PERIFORMED, IN GRADES 14AKES
-11: POSSIBLE TO REGISTER THE. FINDINGS, OF-,-THE INVESTIGATION AND TO OBSERVE
OF THE TREATMENT APPL.IEO+;. FA`61,11'Y' V. P. FILATOV
~OOESSA RES. INST. EYE DIS..TISSUE. THER i:0 DESSA,~ -VSSR&
-tED
----- - UNC LASS I I

w i
, I i ;l ; ": l": I 1 1111. , .11! 11 ; P1:1 1. 1.1 , I .:. . i.,

DATE. -30OCT70
ARE PREPD.
AT
---, P-!E,- - ---- - - - - - - - - - --- - - - -- -- - -
u 1-q -k- t A-s-s-, -, -- -

USSR UDC 621.396.61.621.396.2(088.8)
YAMOVIC
1, V. I.
"Device for Suppression of Higher Harmonics"
USSR Author's Certificate No 248782, Filed 15 Feb, 6 7, Published 7 Jan 70
(from RZh-Radiotekhnika, No 9., Sep 70b Abstract No 9D220,P)
Translation: This author's certificate introduces a device zor suppression
of higher harmonics in ultrashortwave and decimetric wave radio transmitters
executed on the basis of utilization of band-eliiatnation filters. In order
to improve the stability of the active input impedance in harmonics with
simultaneous insurance of a high value of the travelina~wave coefficient in
the operating frequency range, the output load was connected to the radio
transmitter via a balanced two-conductor bridge executed in the form of two
'plane buses with geometric length equal to one-fourth tlie average wavelength
of the transmitter. Absorbing resistors are connected to the terminals of
the second diagonal of the mentioned,,bridge.via band-elimination filters or
high-frequency filters.

Polym6rs:'-and'~Po-1j,iiei7i:za'ti:bn
USSR UDC 678.742-13
KURYLENKO, A. I., and YAKIMTSOV,.V. P., Belorussian State University Imeni
I.- Lenin
"Inhibited Radiation Grafting P-Aymerization of Acrylonitrile in Poly-
ethylene Films"
Minsk, Doklady Akademii Nauk BSSRj Vol 16, No 10, Oct 72, pp 901-904
Abstract: The effect of hydroquinone on graft polymerization of acryloni-
trile in polyethylene films was studied. It was shown that addition of such
an inhibitor does not lower the effectiveness of the influence of graft
polymer on the properties of the materials, that it does counteract the
formation of homopolymer and acids in regulating the distribution of the
graft polymer throughout the entire material. This polymerization in-
hibition method may be used with various initiators.. The Inhibitor makes
it possible to select optimal chain length,of the graft materials as -.Tell
as,gradients of the polymerization rates in microregions differing by their
densities and properties.

US SR UDC: 621'.~96.69:621.319.4088.8)
WAWYAIN, G. S., Y-AMRILIN R. V SIMMOV31 A. !., Leningrad Production
Union "Radiodetall""7
A Fixed Capacitor of the Mansbridge T~Ypell
USSR Author's Certificate No 266071 filed 17 Feb 66, 3n,:Dlished 6 Jul 70
Afrom PM-Radioteklmika, No 1, Jan., 7' Abstract 110 lv3O'L P-)
Translation.- This Author's Certificate introducesacanacitor equipped
vith a rectangular r-etall housing and iusulating p~ckiag'gasketts loca-ced
be-Ween the inner we-Ils of the housing-mid the outer su~-face of the ca-
-oacitor sectica. As a distinguishing feature of the patent, the assembly
process is sirwlified by maJzing the insulation gaakets Jn the fom of two
holl6v sections of ather-m-oplastic material such as polytithylene with
e4es which fit iinto each other amd side valls -fitted vith l6np-,.udinally
arranged extrusions, the protruding elements, of these 0.,trusioris being
directed partly toward the inside* of. -the ovscti6n,! and riartly to,,rard
holl e
t7he- outside.
30

C dLP-td
aR C1
VDCi 6164U~MtWi.fi
ImIN DIREMOKU OF 1.14--vemi ION OF DISAMLITY

(ArtLcla by rhair of Social
hygiene ani Public Haalth. (hOAUT-VrTrMWFn~7-A 0 V).
WL,
-
Mad.-col J.notitto Jisa.,j F.,d Ir=, VrA,intidar ~ )bccow. :!OVoLqUaVT%TAvM.
o0hirtavenive. guiltsioulo No 9. 1111, submitt" 16 robv.aty 1971, pp
TI-mr-Ignifftint Lo4v~ tjk%, ?,"Ith of the Population nod national
c&;zad by disabIlIty U th;t roaAon for the urgency of imprcivtng UIC
jaocloliy~14atc tiethoda of fnv~~tiAotinr, thim prnfolom, Itich tins hitort done by A. F.
1rc-,'7&kov. A.Ya. Ayarbakh, Va.Z% Shibeol, H.Yv. MiqAtril -tth rttapptt to
4--lopinj epthcklologtcal app:aftahea in tho at-;!y of 4inability. particularly
1.~ th. latt. decade. -On. of the T,:?pul ar iiortods In elynamic deramtnation
or
'
;==ry dizzbility status on the ba4t$ at VrFX J?Wdieal Coft.466100 r6r~Deter-
minstion of MoubilitYl. . In Krasnaddr, the JAridices of primarl realAtuition.
!due to d!azb--1it7:droppa4i 51~4 per 10.000 vorkerti to 44W3 froo-1964
it. 1970. anJ the fi&urea- for inatvicLaals of amplbyable mile 4ropps4l from 47.4
Ita 40.9, rtspactively,
i lhv ags and &4)1 ~u',Orfftlent* or disability statue prozrizen vith all*,
hith for =en ~;id womtriq and risaah a. isuMiauvt in the decade preceding ratiramant
~&sa: &Q yaarr- ror men ond SS -fears for woeicss (Table 1).
10 Indicez aim -him in-thr.
=-.a
Sm-up from 0 to 25, -,cnr;. tcc.-vi;c of the XTvarnr numter of Invalt4r, since
c.-Iildhood -hn became entleled to ~ pension in 1967. In the age groups up to
19 yi-.;;rs, the. Ind(ceFs jiro much lflpher for men than women. and In the next two
-M.73 ~40-49 and !i0-:i4-yczrri tricy ara or,
C- th. tho disabilityAndicts r=f.r;LC to t=plcy=blr =Fr KTCU-,n C=-
.-I;uted 45.1 for rpn And 3.6.7 for wc-~eri per 10,006 workers.
'11*6 r-ethod we hdve p=opostt, by unalegy to mortalit:7 tiblon, of tozpil-
ing ditiabilfty tablets to it~aluatc the lines caused by disability in3icate 11 that
h
T7,
even wit
Telatively low ditiabil[ty indicui in 19676 the period of gainful
e:~;loymcnlt (44 yezis for mcn and Ij y,,art, for women) will be threo years
shorter.
Tht most
I izaportant cauacc of dirability azrnF man are circulatory
~lt..a&ea (26.9%). acc4dtats, poitioning ~d tr-.a (17_5%), ci~npla.;.;F~ (12.5Z),

- 20

USSR UDC 542.65 546.212
KIRGUMEV, A. N., and S)WiINSXIY, B.
X., Institute of
'Inorganic Chemistry, Siberian branch of ;,the,. AcAdemy of.Sciences.USSR
"Dixected CTystallization of '~Sea!' Waterl~l
Moscow, Izvestiya Akademii 1,
Yauk SSSR, Seriya Xhimicheskaya, No 10, Oct 71,
-2320
pp 2318
~kbstractt Distribution of the main components of "sea" water in solid phase
was studied during directed crystallization of a solution with following
Conposition: NaCl -- 2. Vo; Me-SO4 -- 0.331%; Cacl 2:-- 0.11%. Distribution
of these co Donents in solid phase is determined by total concentration and
not by the concentration of asingle.componant. All the components have
practically identical coefficients of distribution rega�cuess of the con-
centration. The coefficient of distribution is practically constant in the
range of the crystallization rate - from: 0. 4 -to 8 ~=/hr. ~. In this range
atirxing has very little effect.on'the cooffiaent, of distribution.
79 -

2 Z 018
NCLASSI F I EO PROCES51ING DATE--~V,IGV70
TO
S S I F-
I E D~

U S.S'R UDC 535-343-1
SOLMIN, R. I., YaKOBI, Yu. A., and KOMRT, A. V., Institute of Theoretical and
Applied Mechaniczr;7-Sibi~Ain~ c-h-of the Academy of Sciences of the USSR
"Discussion of Some Results of the Calculations"
Omticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka,# (Siberian
-Bravich). 1973, PD 40 48
tract:, The sDecial characteristics obtained are based on modern theoretical
A
b:s
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 LO resonance lines at 1 atmosphere and for the la lines
at 10 atmospheres because of the low electron density at %,his temperature and the
deep locations of the levels corresponding to these lines.. At 10 and 20 atmos-
pheres. the lines axe clearly visible against the ba6kground; at high temperatures
they become narrower again because of the reducedt,electron' density.
Although much energy is in the Lyman lines and contihiiw-n, self-absorption
reduces radiation in these regions quite strongly, particularly at low tempera-
tures.
The lines of the Balmer and Lymmi series tend to fuse even at relatively
low quantum numbers. There is some question about the bounda:ry between discrete,
113

USSR
SOLUMN, R. I., et al., Opticheskiye KharakteriBtiki Vc,darodnoy 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 showthat the spectral lines begin to fuse
-significantly earlier than the Coulomb "trimming" of the discrete spec.trum.
In addition to the spectralcurves) the.authors calculated integral
energy losses for hydrogen plasma over the~range of-parameters used. Special
calculations were made to relate their woA tolthat of D.,L B. 01fe, reported in
J. Quant. Spec. Rad. TranG. 1,101,., 1961, and satisfactory agreement was found.
The,use of lasers to probe plasma requires,quantitative information
about the relationship between transparency and plasma temperature and density.
These calculations were performed.in two ways, assuming constant prensure and
at a given initial particle density. The first procfdure is necessary because
the plasma has significant absorption only at relatively lilgh pressures, yielding
a condition without significant pressure gradientss-but with high temperature
And density gradients as the plasma is forced against the walls. ilathough there
is an overall tendency to-wrard absorption.at, longer wave lengths, there are
anomalies due to the existence of strong absorption lines sthich are more or less
~active, depending on pressure and temperature. The second form of calculation
2/.3

USSR UW 535.343-1
SOLUKhIN, R 1.),,YaKOBI, Yu., A., and KOMPT, A. V., Institute of Theoretical and
Applied Mechanics,-Siberian Braich,of the Academy of Sciences of the USSR
"The Continuum"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy- Novosibirsk, IsNaulcall
(Siberian Branch), 1973, PP 23 - 29
Abstract; Continuous spectra are generated by transitiom to, from, or within 1;he
unbound ("free-) state.' At temperatures below 5000 dogreas these represent
free atoms (the total continuous radiation is small).while at higher temperatures
free electrons axe a primary radiation mechanism. At electron temperatures much
less than 500 ev a semiclassical treatment is appropriate,,yielding, the so-called
Kramer,s formulas with the Gaunt factor asa quantum mechanical corrective. A
formula for recombination radiation can be obtained by app3Zrinc, Kirchhoff's law
for Ideal thermal equilibrium to the formulas for photo-ioifl.zatlon absorption.
This radiation is characterized by significant intensity close to the line series
and an exponential decay in the direction of short waves. Lremnstrahlumq extends
Indefinitely in the direction of long- waves. The ratio of.these two effects can be
calculated for a given temperature and frequency. Anothez- factor is so-called
multi-quantum recombination occurring, as aresult of trinle recombination. In a
nonequilibrium plasma this can substantially.influence Ithe d3stribution of electrons
in levels and the number of free electrons, but in an equilibrium plasma a
1/2

IJSSR
SOLUKUN, R. I. et al, Opticheskiye KharaRteristiki, Vodorodnoy Plazmy, Novosibir-sk,
"Nauka" (Siberian Branch), 19?3. PP 23 29
Boltzmann distribution in the levels Is established, uniquely determined by 0
temperature equilibrium. At fairly:high pressures and temperatures below 10,000 K
a significant role is played by the formation of negative bydrogen ions,
accompanied by radiation. At still lower temperatures continuous molecular
spectra appear. There Is also the so-called quasi-molecular continuun which is
due to the transition of a hydrogen molecule:from an initial unstable*state
(occurring as the result of a collision between atoms with~parallel spins) to a
stable state.
In addition to the true continuum, there. are quasi-coatinua, resulting from
the overlapoing- of large numbers of broadened lines. These occur as various
0
bands. At temperatures below 1000 K, induced'.rotational transitions are signift-
cant
1 although 'he radiation of gases at lov,~temparatures is very low, the
coefficient of absorption ic quite significant.-
~2/2
5 4

I I S UDC 335-343.1
Yu Institute of Theoretical and
SOLUKhM, R. UOI ..A and XOMIN, A. V. L
Ihanics Sheka_~ _Ij~7~~ch of ',th&;Aca46zy,; of s c ien c e s' of the USSR
ti
Opticheskiye Kharakteristiki Vodorodnoy Plazmy , Novosibirsk, "Naulta"
ASiberian Branch), 1973, pp !6 - 23
Abstracti Three factors determine the nature of spectral liness population,
transition probabilityand form of the line. Although many processes contribute
to population distribution, collision with electrons and spontaneous radiation are
usually dominant. At low plasma densities secondary collisions can be ignored and
radiative:transitions are dominant, while.in dentso pla.,qmas nonradiative de-excitation
predominates. When the electron density becomes sufficiently high, radiation
intensity becomes independent of it; the plasmat becomes a Boltzmann radiator.
Spectral lines from a plasma are all brGadened as a result of interaction with
fluctuating internal microfields. The extensioft can be considered in terms of two
components: one described as the result of a linear Stark effect. due to the inter-
action of ions vith other, relatively slow ions, snd the other due to collision
broadening (also with a Stark effect component) from interactions with fa-ster-moving
electrons. The electrort effect is most si.onificant at the center of the broadened
ms,
li e; the statistical effect,,at Its edges. 7he center is also so. ihat displaced
172

USSR
~SOUJKhIH, R. 1., et al., Opticheskiye Kharakteristlki Vodoro4noy Plazmy, Novisibirsk,
WWI .(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 with experiments, computations
-for the central portion axe considerably less satisfactory. In this area the
authors base their.work on a theory developed.by Sobellman, extended to cover also
s
broadening due to collisions with.other particle
When the concentration of charged particles is low, Doppler broadening becomes
significant. The integral expression for combined.Do~ppler and dispersion broadening
,-is not in finite form, so that calculation by approximation Method is required.
2/2

7-
UDC 535.343.1
SOLUKhIN, R. I., YaYOBI1 Yu. A., and YONIN, A. V*, Institute of Theoretical and
Applied: ~lechant-eg;-SilYdi~i-dft~'Branch of the Academy of Sciences of the USSR
"Method of Performing the Calculations"
.073tic heskiye Kharakteristiki Yodorodnoy PW,.my,, Novosibirski "Nauka" (Silberian
Branch):, -1973, pp 33 - 39
Abstraett Five mechanisms vere considered in the computer progrrams used:
j
-bound electron transitions (linear radiation --atoms); 2) free-free
1) bound from
and free-bound electron transitions in the field of protons'(the H continuum)i
3~ free-free and free-bound electron transitions in the field of atoms(H-coTitinuum);
4) free-free and free-bound protontransitions inthei,fiel& of ELtoms (the H+ 2
co&tinuum)l 5) continuous radiation of quasi-molecular hyqro.-en
--quasi
2 continuum), Previous studies have lumped line spectxa in two or three
groups., The present work considers all transitions between discrete levels in the
hydrogen atom that realistically exist in the~plasma. Within the:limits of the
parameters chosen, this number varies from less than 1.0 to several tens of levels,
the number of s-)ectral lines is proportional to the square of this number. Each
-line is considered in its broadened form.1 The results are pt-estnted on a wave scale.
Variable step sizes are used to keep the calculation error approximately constant
over the entire spectrum. Step BiZ85 were based on rel ative values of the derivative
112

USSA
SOLUKUN, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plumy, NovosibiTsk,
"Nauka" (Siberian. Branch). 1973. pt) 33 - 39
of spectral intensity, except where the contribution of the maximum line was less
tha
n 1/10 -he bacjv-round radiation# where the step size was based on the continuum.
In each sten the calculation of step size was based on the.1ine making the
strongest
contribution, rather than the line with;the:nearest center.
-7.
The program was uTitten in ALPHA, a modification of:ALGOL. Calculations
were performed at the computer center of.the Siberian Branch, Academy of Sciences
__ofAhe,USSR.
92

-USSR
UDG 535.343.1
SOLUDIN, R. I., and KOMIN, A. :V., Institute of Theoretical and
Applied Mechanics, Siberian Branch,of the Acadekv of Sciences of the USSR
"Energy Structure of the Hydrogen Molecule"
Opticheskiye Kharakteristiki Vodorodnoy Plamy, Novosibirsk, "Naukall
(Siberian Branch)o 1973, p-D 12 - 14
Abstract: Quantum mechanical analysis shows that the diatomic hydrogen molecule
is not stable unless the ends of the two electrons are in.an antiparallel
orientation. Althoun:h the two electrons of the molecule.'can be in various
enerr metry
gy states, they are within an axially symmetric field whose axis of sym;
4s the line connectin- the two nuclei, Inthis case what is significant is not
the absolute value of the orbital moment, but its projection on the axis
where 41 Is Planckts constant and X is a~ quantum number' similzar to the
magnetic quantum number m In atoms.
in addition to the electron degrees of freedom, the.molecule has oscillaAory
and rotational degrees of freedom.. For each characteristic electron state, there
is a set of discrete oscillatory states,-which can be obtained as the solution
of Schroedinger's equation for a harmonic oscillator. Consideration of non-
h
_qrmonic oscillations leads to a more complex expression. Rotation is also

SOIDKhIN, R. I.i et al., O~3ticheskiye Kharakteristiki Vodorodnoy Plazmy,
Novosibirsk, .".qauka (Siberian Branch),: 1973,, -typ 12 14
characterized by a discrete selection of energy states, describable in terms of
the rotational quantum number, the molecular constant,and,a coefficient which
characterizes the relationship of rotation to oscillation (nonrigidity of the
xotator).. Since the hydrogen molecule does:not have a constant dipole moment,
it cannot in isolation have oscillatory and rotational transitions, but in a
real gas this prohibition is removed because of induced electric dipole moments
~occurring in collisions. Although any transition can occur, transitions of I
are,most common. For electron-oscillatory,.spectra, the relative probability of
is determined by ~the Franck-Condon ptiheiple.

USSR UDC 535.343.1
SOLUXhIll, R. I., YaKQBI,,,._.Yu,.A*,,--and KOMIN) A,V.p Institute of Theoretical and
-792'.ber
Applied Mlechani-cs, ian Branch of the AcadenW of Sciences of the USSR
"Total Radiation from Hydrogen at Temperatures Below 10,000 Degrees"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "ITauka" (Siberian
.,Branch) , 1973j pp 29-33
Abstract: Calculating the radiational characteristics.of gases at relatively
low temperatures requires primarily consideration of molecular radiation.
Detailed calculations for this were made by Olfe in 196L For a thin layer of
plasm in which self-absorption can be ignored, radiation from rotational transi-
tions predominates up to 10000; that from oacillatim-rotational transitions
between 1000 and 50000. At higher tom eraturos, nagative:hydroron ions and posi-
.p
tive molecular ions appear, the former more significant by an order of rmgnitude
from.3000-to 10,OOOOK. At higher temperatureslinear radiation becomes signifi-
cant..,~hen the plasma is of significant density and thictmess, the results must
be adjusted to account for the varying,.degrees~of absorption at different fre-
quencies and by different mechanisms,
1A

USSR UDC 535-343.1
R. I. _YaK I ~titute of Theoretical
SOLUM117 Yu. A. and KOMIN, A. V.,. inr
-Sib"' ' Branch of the lcademy:af Sciences of the USSR
and Applied Mechanics, erian
"Energy Structure of the Hydrogen. Atom"
icheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, 1111auka",
Stiberian,Branch), 1973, pp 9-12-1
~
Abstract: Schroedingerts equation yields solutions only for negative values of
E for which
)(2m 4
2 1 e! ~R
E
n 2 2- n~7
h n
vhere n is a whole number and R is the Rydberg constant. m must be replaced
by.
1M+M
where m is the mass of the electron and M is the mass of the nucleus, to account
for novement, of the nuclear mass. Relativistic generalization of Sch-rced-in-
ger's equation requires that azimuthal qu.-mtum numbTrs be considered in addi-
tion to the primary number n. In the presence of an external field, the
1/2

J161, 0rU;q
USSR
SOLUXhVI, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazmy,
1973, pp 9-12
magnetic quantum number must also, be considered (Zerman~effect). Howevcr,
not all.transitions described by this-schbme~aro found in spectroscopic obser-
vation. According to quantum mechanics, the following types of optical dipole
transitions are possible: change in~azimuthal quantum number = + 1; 6hange in
magretic quantum number = 0 + 1; change in m 0; change in internal quantum
number azimuthal + msI G + 1.
2/2

UDC 535-343.1
SOLUKHN, R. I., YaKOPT,ju. A., and KOMIN, A. V., Institute of Theoretical
and_Applied 14ech-a'n'ies, Siberian Branch ofth~ Academy 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 H3 m0led"es, positive and negative ions of these molecules,
atoms, positive and negative ions of the atoms, and free electrons. Diagrams
are given to.show the relative contribution of each of these particies as a
function of temperature and pressure. The law of mass action gives the rela-
tive amounts of large particles and their breakdown products as functions of
the degrees of freedom of each such component.. Thers are 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 fix1ding each of these as
the sum of a series in terms of energy of e*xcitation, clectron~levcl, natural
oscillation frequency, oscillatory qi4antum~number, and A,her factors. Trans-
lational freedom can also be expressed in torwof mos and, rel ativo volitmo.
1P

USSR
SOLUKhIN, R. I., et al., Opticheskiya Kharakteristiki Vodorodnoy Plasmy,
1973 pp 5-9
Since dissociation and ionization ordinarily begin at temperatures
significantly below the corresponding binding energy, because of the high
statistical sum of the free state, in the majority.of cases only the basic
electron teria need be considered and the unharmonic nature-of-hydrogen MolecuIe
oscil],ations can be ignored. Several studies have determined.ionization
energy in a plasma and its reduction due to the total'el
A.
patric field of charged
particles around the atom, particularly Ecker~and Kroell:(1963). The thermo-
dynamic calculations of plasmic COMDosition.made in the.present work yielded
I'atch in~,1969.
results close to those obtained by
2/2
14.7

I lit,
jjD);~l 11A'D r,
'USSR UDIC 535-343.1
SOLUKhIN, R. I., and KOMIN, A. V.~ Institute,of Theoretical
and Applied Mechanics, Siberian Branch of~the Academy of Sciences of the USSR
"On the Thermodynamics of Radiation't
Opticheskiye Kharakteristiki Vodorodnoy Plazmy Novosibirsk, "Nauka"
(Siberian Branch), 1973, pp 14-16
ilibrium in a sy3te.. includ
Abstract: The primary obstacle to establishing equ
ing radiation is the loss of energy by radiation outside the system. An
excited particle can lose energy either through a damping collision or by
spontaneousrad-4ation. If there is any significant ionivation, the 1Mjority
of collisions are with electrons. Thus given~the damping collision cross-
feti,
section of the particle and its radiational li no (Considering also stizwj-
lated emission), the relative probabilities of damping arid radiation can be
calculated. If damping is more probable, local thermodynamic equilibrium may
be established. Overall equilibrium will depend on the volume absorption
-coefficient and the relative probability of damping. The calculations for
absorption must consider re-radiation, so,that."absorptic.-i" implies a sufficiei)t
number of collisions to make theprobability of damping high. If this total
path length is much greater than the dimensions.of the volume, the result is
1/3
45
WE IF14T M-M

USSR
SOLUKhINj R. L, et al., Opticheskiye Kharakteristiki Vodorodnoy Plazmy,
1973, pp 14-16
volume radiation; if it is much less, surface radiation. Equilibrium radiation
of a surface plasma radiator is equivalent to that of an absolute black body
and is,referred to as Planck. radiation. Nolume.equilibri-um in the sense of
local thermodynamic equilibrium yields so-called Boltzmann radiation, since the
nature of theradiation is deterair-ed by the Boltzmann,distribution of electrons
in levels. VWle a special form of.Kirchhoff's law applies to the latter case
and the black body radiation is determined from Planck's formula, nonequilibrium,
radiation can be analyzed only by solving an enormous system cf kinetic equa-
tions, since nature depends on the probabilities of a large number of elementary
processes.
In a moderately dense plasma locallthermodynamic equilibrium is the
most probable state; it is sufficient for the probability of collision prccesses
to exceed the probability of radiation processes by an order of =gnitude. In
facti the rigidity of thio condition for a rosonancs trawiitlort with traximum
probability of apontanoouv rrdiation~czm be significantly%reduced in the
majority of real canes by the trapping of radiation in the optically dense
plasma. Since most experimental installations produce a plasma for a short
time, it is necessary to verify that thetimie to est'ablish equilibrium is brief
in comparison with the time to establish a qqasi-stable.state. This can be

VSSR
UDC 535-343.1
SOLUKhM, R. I. VaKGBI Yu. 4.1 and KOMIN, A. V., Institute of Theoretical
SSR
and Applied Y-lechanics Siberian Branch of:the Academy of Sciences of the US
Opticheskiye Kharakteristiki Vodorodnoy Plazmy (Optical,Characteristies 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 computation is pre-
ceded by a brief systematic summary of information aboutt the hydrogen atom
and molecule and the composition and thermodynamic and gas dynamic properties
of the hydrogen plasma. Radiation processes are covered in detail, including
radiation from nonisothermic plasma, which.requires simultaneous consideration
of radiation and thermal condjetior.. In this.connection, the results of the
calculations are discussed, recom;%endations for their peacticp-1 use are made,
and some questions of the diagnostics of hydrogen plasma are examined.
This material will be useful to a broad group of engineer
-physicists
and
graduate students and students in senior,courses spt-cializing in spectro-
scopy, plasma physics, astrophysics, and physicall gas dynamics.

USSR
SOLUKhDT, R. I., et al., Opticheskiye Kharakter--stiki Vodorodnoy Plazmy, 1973,
82-pp
CONTENT5 Pape
Introduction 3

,The Composition of Hydrogen Plasma 5
2. Energy~Structure of the Hydrogen Atom
9
-3.: Energy.Structure of the Hydrogen Molecule
12
4. On-the-Thermodynamics of Radiation; 14
5. Spectral Lines 16
6. The.Continuum 23
Total Radiation from Hydrogen at Temperatures Below 10,000 Degrees 29
-8# Method of Performing the Calculations 33
~9_ Discussion of Some Results of the Calculations 40
10. Optical Diagnostics of Plasma:' a 48

11, a Nonis
Radiatio, of a I othermic Plasma Transfer Coefficients
55
12. Radiation of a Quasi-Equilibrium Hydrogen Plasma, Considering
Conductive Therral Conductivity. 59
Gas.Dynamic Properties and KLements ofRadiation Gas'Dynardcs 61
14. Laser Heating of a Plasma 69
213

M
i - I . . 1 . - 1 1 .1 11 .

7", '77-
-USSR UDC 535-343.1
SOLUJz7hD1, R. I., and KONIN, A. V. Institute of Theoretical and
Applied Mechanics, Siberian Branch of~the;Academy of Sciences of the USSR
Diagnostics of Plasma"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka"
(Siberian Branch), 1973, pp 48-55
Abstract: Plasma characteristics (prims
-11y,the concentration and temperature of
various components) are determined from active and passive optical analysis.
Passive methods, in which the plasma is illuminated by ~bxternal 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 processes in a plasma, the most widely
used method is to begin with rough measurements based-on one of the basic
radiation mechanisms and proceed to more4etailed analysis. Although in some
particularly clear situations this method is~expedient 'thers-, are many cases
in which the preliminary determination ofthe primary r-,--:!chanism is quite
1/3

USSR
SOLUKUN, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazmy,
-Novosibirsk, 1973, pp 48-55
difficult or even meaningless. In addition, the overwhelming majority of
when self-absorption must be
these methods assume an optically rare plasma,
considered, this analytical approach leads to very complex expressions. A
more general approach, ignoring only those Icomponents whose contribution is
obviously unimportant, is clearly necessary. The use of computer calculations
over a broad range of parameters providesthis,more general approach, serving
as'a "mathematical experiment" to relate the results of different stud-Les 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 vhen this type
has primary influence on the effects of refraction. The relative sensitivity
of these two methods depends on the effective radius of the 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 in currently on the use of inira-red and x-ray-probe
wave lengths. Infra-red is particularly acn.9itive to th.,q charged particle
components, including the electron continuum. hisvive x-ray diagnosis can be
used in determining parameters of a high-tamperature plasma along the discharge
2/3

USSR
SOLUIMIN, R. I., et al., Opticheskiye.Kharakteristiki Vodorodnoy Plawy,
Novosibirsk, 1973, 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 i~ time. Local discrim-
ination is achieved usually by using the Abel,transform:and agouming axial sym-
metry of the plasma formation. Titv, discrimination is achieved by using various
-ized by
types of time scanning. Optical analysis:of,hydrogen plasma is charactei
four specific factors: 1) absence of a constant dipole moment; 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 primary determinant.of the speAral line broadening;
4)'complete ionization at high plasma:temp;eratures.
313

UDC 535-343.1
SO=bIN R I YAKOBI, Yu. 'A. of Theoretical
and KOWN A.~~V*;.Institute
d--A -Branch of tl,,~ Academy of'Scie ces of the USSR
an Appl~ied Wchanics;-Siberian n
"The Role of Hydrogen Plasma Radiation in the Problem of Thermonuclear Rasion"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, 1111auk-all (Siberian
Branch), 1973, pp 73-76
Abstract; In the majority of thermonuclear installations radiation is the
primary sol.=e of heat loss, since the times involved are too short for con-
vection losses (particularly when viscosity is increased by a magnetic field),
and conductive heat loss can be ignored when the plasma isseparated or dis-
tant-from the walls. For a deuterium-tritium plasma the necessary conditions
can be achieved at temperatures over 5 kevi while for pure deuterium they
cannot be achieved at all unless the magnetic field is used only for thermal
insulation, not retention of the plasma, or measures are taken to reduce
racUation loss (use of an optically thick plasma or radiarlion-reflecting
walls).
Quantitative inf,-rmtion about radiation capacity of the plasma makes
it possible to determine the minimumpower of a steady-state reactor and the
minimum temperature of its center in the general case of combined heat transfer
113

USSR
SOLMIN, R. I., et al., Opticheskiye Kharakteristiki,.Vodorodnoy Plazmy, 1973,
pp,73~76
and radiation losses. Assurung the plasma is.not separated from the wall and
its lifetime is not limited by instabilities, the zone of ra-aximum brightness
will be a hollow cylinder at a temparature of.several electron volts. Cal-
eulations indicate a minimal temperature of about 7 kev,at the center of.a.
reactor without magnetic field, using a 50% deuterium-tritium mixture. The
dimensions of such a reactor must be on the order of several kilometers and
A-he heat loads on its walls must greatly eycedd the capacity of modern mater-
e
ials.
Calculations show that an equilibrium reactor vith a magnetic field
would not produce energy at the center sufficient to compensate losses at the
exterior due to.the poor heat transfer properties of the magnetized plasma
and that- reflecting~shells would be difficul
t 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 research
involves the itse of relatively longlaser pulses for supplementary heating of
plasma in various magnetic containment devices.1 uhile a second line is
directed toward the use of very short-powerful laser pulses to bring targets
2/3

USSR
- -I- - 40 -7---

USSR UDC 535-343.1
SOLMIN, R. L, YaKOBI, Yu..,- A. , and KOMIN:, A. V., Institute of Theoretical
and Applied Wd-hdfii&s, Siberian Branch of the Academy of~~Sciences of the USSR
"Radiation.of a Quasi-Equilibrium Hydrogen Plasm, Considering Conductive
Thermal Conductivity"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy,, Novosibirsk, "Naukall (Siberian
'Branch), 1973, pp 59-61
Abstract: Only conductive and radiant heat transfer are corsidered in this
book; although convective transfer is important in a number of.cases, because
convective beat transfer has not been adequately studied,,aither theoretically
or experimentally. There are, however, many cases in which convective transfer
does not occur.
'The relative contributions of radiant,and convecti-Ve heat transfer for.a
plasm without interior directed velocities~can. be determtned from the differ-
ential equation of radiation transportL and the law of energy conservation. If
the absorbed energy is much less than the radiated energy, the system of des-
criptive equations can be reduced to two equations; an expression -Por heat trans-
Xer which determines the state of matter throughout the entire volume, aiQ3 an
expression of radiation transfer which can b 'e used to find the spectral density
of radiation. This occurs in an optically thin system without external
I.; WHIMAR, ~W~

USSR
T
SOLUKhINI R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazmy,
1973P pp 59-61
radiation- flows. A similar separation can be obtained if the absorbed energy
is.greater than the radiated energy, but the total,absorption of the radiation
flow throughout the entire volume is less~than ,;he flow~,of energy related to
beat transfer and is thus incapable of changing the temperature distribution.
Truly radiative transfer states also exist,- described byithe so-called diffusion
or radiant heat transfer approximations. Although the a~ssumption that radiant
heat transfer exceeds conductive transfer is correct in the overwhelrnlng major-
ity of cases, there is a region in which this is not true.

USSR UDC 535-343.1
SOLMIN, R. I., YaKOB1,-Yu-A.., and KOMIN, A. V., Institute of Theoretical
and Applied Mechanics, Siberian Branch of the Academy of Sciences of the USSR
"Radiation of a Nonisothermic Plasma. Transfer Coefficients"
Opticheskiye narakteristiki Vodorodnoy FlazMY, Novosibirsk, "Nauka", (Siberian
Branch), 1973, pp 55-58
Abstract: In the presence of a substantially nonisothermic plasma. radiation
transfer is described with the aid of special coefficients, calculated, in turn,
from the spectral characteristics of isothermal plasmas.~ In an optically thin
layer, the divergence of radiation flow can be desaribed,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 tho so-called modified emission ca-pe-city. Although the
calculations-are simpler for extremely thin'plasmas in which lines predominate
or extremely thick plasmas in which,the continuum is dominant, real situations
usually require dealing with the more complex calculations of intermediate cases.

JSSR UDC 535-343.1
SOUMIN, R. I., YaKOBI,__Tp_,,_A,, and KOMLINA V,, Institute of Theoretical and
Applied Mecha~nica-,-Slii~Aan Viinch of the Academy of Sciences of the USSR
"Laser Heating of a Plasma"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka" (Siberian
Branch), 1973, pp 69 - 72
Abstracti laser heating is one of the proposed methods*of attaining a controlled
thermonuclear reaction. The necessary conditions axe the opposite of thaw
axe varying difficulties
necessary for optical analysis without perturbation. There
in:this process. At low temperatures, there are many energy-absorbing transitions
to be passed throuc,-h, and radiation losses b".1n to:be significant as the plasma
is heated. At hi~Ther temperaturest effective. heatir4g, is Uso reduced by the
increase in transparency of the plasma. The heating must be rapid to prevent loss
of heat to the valls and the development of Instabilities, Use of a. solid or
liquid target, Plth=~h it requirm additional energy for,melting and evanoration,
makes attainment of the Lavson criterion easier because of the high initial plasma
densityl if evaporation takes place from all sides simultrineouslyt a significant
compression factor can be ;added
effective for
..-At thermonuclear temperatures$ only inverse bremsstrahlung i_ -3)$
heating, For plasmas of moderate density,(leas than or equal to 1019cm
1/2

USSR UDC 535-343.1
SOLMIN, R, I., IL,._-Yu.-A.-j and KOIMIN, A. V., Institute of Theoretical
and Applied Mechanics, Siberian Branch of1the Academy of Sciences of the USSR
"Gas Dynamic Properties and Elements of Ra iation Gas Dynamics"
d
Opticheskiye Kharakteristiki Vcdorodnoy Plazmy' Novosibi~rsk, "Naukall (Siberian
Branch), 197-3, pp 61-69
Abstract. In many cases, gas dynamic properties of plasmas must be considered
along,vrith radiative properties. The authors arbitrarily distinguish two
thermodynamic regions-, a ) temperature leso than 10.electron volts and pressure
'less than 1 atmosphere -- radiation is not blocked and the pressure of the
photon gas.may be ignored; b) a "black" plasna'at high temperatures and den-
sities --.radiation energy and pressure must belconsidered, There are also
such cases as the propagation of shock waves with high radiation flow,in which
it is necessary to consider changes in the thermodynamic properties of the gas
ahead of the front due to absorption of the flow of advance radiation from the
m0
hot gas behind the front. Knowledge of some ther dynamic and gas dynamic
properties of low-temperature hydrogen plasma is therefore also necessary.
Where there is overall flow of matter in an optically thin-plasma, the
usual hydrodynamic equations must be supplemented by a radiant energy factor
which represents a volume energy source. For an opticrilly*.thick body in which
the~radiant heat transfer approximation holds, the state of the matter Is
d tormined colely by its optical properties, In other cason, as in the problem

USSR
SOLMINI.R. I., et al., Opticheskiye Kharaktoristiki Vddoroduoy"Plazmy,
1973i pp 61-69
without material flow, a complete system of equations must be solved.
The equilibrium concepts used by the authors are applicable to quasi-
eqailibrium. processes, since the time to establish equilibrium 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, which
are equal to or less than the thermal velocities of the molecules. Of course,
the usual conditions of quasi-equilibrium must be supplemented by a condition
Ahat the radiation absorbed by matter-in-the time interval of interest does not
change the state of the matter.
2/2
7~

USSR UDC: 533.9-15
SOLOtVAHIN, R. I.. YAKOBI, Yu. A.
"Methods of Infrared Diagnosis and Laser Interferometry in Gas Dynamics"
"ovosibirsk, Aerofiz. issledovaniya--sbornik (Aerophysical Research--col-lection
N
of works), 1972, pp 27-32 (from RZh-Fizika;, No .6, Sun 7~,, abstract No 6G128
by V. Ch.)
Translation: Optical methods were used to study a pulse discharge plasma in
shock,tubes. Laser interferometry and schlieren photography were used. A
diagram is given of the experimental equipment, which enables rapid conversion
from one research method to another or a combination of different methods.
The principal components are a carbon dioxide laser and a Michelson interfero-
meter. The authors give the radial distributions of electron density in the
forward pulse discharge, as well as EL schlieren signal os-.illogram which shows
a series of sequential radial perturbations,. Rxperiments-for measuring absorp-
tion in a pulsed discharge of molecular hydrogen emission an a wavelength of
10.6
4m are briefly described. Detailed calculations of the absorption
coefficient of the plaoma were made for interpretation of theselmeasurements.
Thu following are obtained and presented for the sho6k tube: an oscillogram of
tile phase advance, the profile of the electron concentration behind the zhock
wave front, and the variation of maximum electron concentratioivwith temperature.
NINE

USSR UDG 621.375.9
SKOVORODKO, P. A., YAKOBI, Yu. A., Novosibirsk
"Inverse Population and Emission: Density in.a Q-Switched C02 Laser"
Moscow, Zhurnal Prikladnoy Mekhaniki i Tekhnicheskoy Fiziki, No 6, Nov/Dec
72, pp 18-23
Abstract: Processes which take place in a C02 laser vith Q-switching are
numerically analyzed on the basis of a system of kinetic equations for laser
level populations and the deas3.ty of radiant energy in the cavity. It is
shown that the process of laser Q-switching is oscillatory., The time of
relaxation of emission density to the steady state depends on the differpnee
between losses in the terminal and initial states and varies for a C02 laser
.over: a. range of 0.1-1 ms; this corresponds in order of, magnitude to the.
rel.nxation time of the upper laser ,level. The ailthors; thank R. I. Soloukhin
1or constant. interest and assistance with the' work.

oi_
us SR uDc: 62-1.373,029.7-001.5
A,-
6 Relations in a Michelson Laser Interferometer"
Moscow, Radiotekhnika i Elektronika, Vol 17, No 4, Apr 72, pp 787-793
Abstract: The author studies the phase relations between the nodulating
signal, the radiation density in the cavity and the emission power of a
Michelson C02 laser interferometer. The optical system of the installation
is shown in the figure. The unit,is supported by a massive stand and all
mirrors are flat. A rock salt beam splitter in the form of a.two-degree
wedge is used to ensure interference on only one face. The interferometer
is sharply asy=etric since the intensities.of;theIradiant fluxes going
from rdrror 2 to mirrors 3 and 4 amount to 99 and r,~ respectively as shown
by'Fresnel's formulas. The beam splitter acts :as a pover.deco'upler. A
chahge in the optical length of one of the~legB of the Michelson inter-
ferometer changes the phase shift.betv-een the radiant fluxes reflected from
mirrors 3 and 4, which results in Ya~riation.of the outputpower. Thus only
the energy coupled out of the ca*Aty is notiulated rather 'than all the energy
stored in the laser. This increases tbe,width of the modulation band. The
1/2
Nil

. . - 1 .; I - 1: i i :: ~: J1,; I 1 *11 IF ! *111 1.11; 1 ~1:1 i:i ~ 1 !- H i- I !"
! I . ` L i ~l : I . I : . . _
i . . . I

'i 7, 'g _7~,7
USSR YJD C621.384.66
PAPADICHEV,V. A., and YAKOBI, Yu. A. (Novosibirsk)
11M ment of Magnetic Field in Charged-Particle Adceler ators by Paired Coil
Leasure
'Method"
Novosibirsk, Avtometriya., No 3, May-Jun 70, p.76-80
p
Abstract: In the variable magnetic field in the vacuum chamber of a charged-
particle accelerator.the field gradient can:be measured by means of two induc-
tion coils whose axes are parallel and directed along the Z-axis. The article
describes methods which assure the required: ac cu racy even In tb,;i case of com-
paratively rough adjustment of the coil sensitivites and p;irallelism. These
methods also permit the elimination of errors due to interference from the
One of the methods (the:turn method) compensates for
magnetic field source.
~,=easurement errors by turning the sensor 180*. about the Z-aXis. The second
or co,
method (the "effective distance" method) provides er]. by replac
coils) with the
ing the quant:Lty,&,, (the distance between the. axes ;of thi
ParameterA!Nzeff. The latter is determined 1rom:zeasurentent of :.the "median
lane" separately. for each coil.
p
69

CP
a T-thINZIir
FUR Ux; IrUJY UF P,W:~Lzlti OP
r4rltal-y by ujut-Irlant 101anil 1% :;hL.1
rvico, 140 3 a ghon,
lil)v~w,,r jwn~pij -,52f.
?or r.(.m orrn~,tLvj stAy by *t,,iL)nt!l Of problorai or
tontrol, or. the conll~lona of' lonor or poraonnoLof ru,lnp-etti-
tions and V)Stlrle ul.),14vul 6f jimlistion by thom we divelop-
ad a prograz-_,nd iralner (Piparj"31).
,APR-.
iq
Pirure'l. generil Vim* of Trainer
140
7'., p"

USSR
UDO: 620.179.15
YAKOBSON A. X LEGNOV, B. I., IMMER, B, M., and.KOPEELIOVICH,
-"Comparative Exnerimental 'E~'stimate:of Various Visual X-Ray Tntro-
scopic Systems Using Electronic Devices"
Sverdlovsk, Defektoskopiya, .7Lqo. 4,11970, P-P 137-139
Abstract: The authors of this brief communication, trembers of the
Scientific Research Institute of introscopy, discuss zhe labora-
tory model of the RIUS Ui-.-Q,2 Introscope, and offer -indic-es by
'Which this instrument can be compared with th-.~-l JZTI, an x-ray
television in-16-roscope with a monocrystalline screen, described in
an earlier article ;by the firat-namea author in collaboration with,
K. X. Dzhgalyan (Zavodskalra lp'Lorator' ci). The HUS
19622 e !~o.
U1-1-92 described in the present, artiqle,..is i~lso an x-ray introscope
with a'monocrystallirie screen, and.uses an.clectron-optical IiSht
amplifier of the LTU-92 type. A sinple diagram~of the instrument
given in this article shows. that the radiation from an. x-ray source
isprojected through the 5paciMen under examination onto the mono-
crystalline screen, the x-rayed' image being,conyterted to a lir,-ht
image by the screen and then put througii the light arwolifier and
a telescope to the observer's eye. kthird instrwnent containing
1/2
88

USSR uDc 616.936-V34.4(47o.4i)
CHUYEVA. S. V., and-YAKMQN.,,__4, Republic Sanitary pidendological Station
of the Tartar ASSR, Kazan'
"Organization of Yalaria Control, Eradication of Malaria., and. Prophylaxis of
this Disease in the Tartar ASSR"
No 61
Mosco-VI ~Ieditsinskaya Parazitologiya i.Parazit.arny~de Bolezni, Vol 41,
flov/Dec 72, pp 747-750
two significant
Abstract: During 1920-70 there were rise;a in the incidence of
tralaria in the Tartar ASSR, one in 1923 and.another in 1935. in 1936-43 the
incidence of malaria steadily decreased, There -was a slight increase in 103-44
i4-
as a result of cond "ions due to World Warill, but the increaze brought about
by the war iras insignificnnt, because ireanares for the control oV this disease,
were not interrupted. In 1951 nalaria im s el:Uidnated as it mass disease in the
Tartar ASSR. In 1962 there was only a single case of nalaria there that
originated locally. In 1966-70 there were individ"I caBt~n of.pvtlaria wiiong
itwi un E;
USSR citizens who had returned from 69sigrar-en'tel, in Afr and Arian co trie
and Imd beco= infected there. L. 1Q,62 there. were 3,~~ antimalarla. stationo,
n
.~which in 1955 *were incorporated in the sanitary epid~~rnioiciigical- stations. Mass
-examination of the population for the presence of malaria was carried. out; in
the period after World War II, up to 600-'800 thousand persons per year were

USSR
CRTff.VA, S. V. and YAKOBSON, B. L.) Meditsinskaya ParaIzitologiya i Parazitarnyye
Bolezni, Vol 41, No 6, i1ov/Dec 72, 7
pp W-750
examined. In 1954, the number of persons examined hwl ~been increased to 910
thousand to establish reliably that malaria as a mass;(Lirleasea had been actually
eradicated, In regions in which the cha4ces of infection with malaria vere
great, chemoprophylaxis was carried out on,aa extensive~scale. Dusting against
mosquitoes and draining of areas covered with',stagnant imter vere applied.
the danger. of the develop,,-.ent of new -foci of
While malaria has been eliminated
infection still exists. In connection with the construction of the Volga Reser-
voir. imeni V. 1. Lenin and its fining starting with 1955t shalloy flooding
develbped in areas at Kazan', Chistopoll,.and IZelenodollok as well as in 13
rayons with the result that favorable conditions foi, the ~. breeding of Anapheles
mosquitoes were created. However I because~of,the effective measures taken,
malaria did not appear in the regions. in question. Great attention is being
paid to the prevention of malaria at ~ the site of the construction of the Kama
Automobile Plant at Nabrezhnyye Chelny, which will be located in an area in
which malaria ray develop, and in the 3 km zone of populated localities down-
stream from there, Vnich will be affected by the construdtion ofthe dam of the
Lower Mpa Hydroelectric Station*
12

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026 UNCLASSIFIED: PROCESSING DATE--18SEP70
C-I ACC.ESSION,NO-AP0102309
..'~."AgSTRACT/EkTRACT-W) GP-0- ABSTRACT., T.HE INFLUENCE OF REACTION
~...CONDTTIGNS (TIME.(S MIN,5 HR), CONCN. OF.MONOMER AND TICL SUB3, MACRO
~CHAINS IN POLYMN4 OF PROPYLENE (11) (MI.XED.WITII PROPANE) CATALYZED BY
4:1 ET SU82 ALCL AND TICL SUB3 MIXTS. WAS'STUDIED MOL. WTS.p CALCD.
FROM POLYMFR~INTRINSIC VISCOSITY DETNSe IN DECALI~t INCREASED ABRUPTLY
WITH REACTION TIME AND TEMP.- WHETHER.MONUMER CONCN* WAS DECREASING OR
CONST. INCREASING TICL SUB3 CONCN, (0o4 TO 3,5 TIMES 10 PRIME NEGATIVE2
MOLE-1.) DJD--NOT INFLUENCE CHAIN VIABIL-ITYv~ BUT DECREASED INTRINSIC
VISCOSITYt.-PROBABLY DUE TO INCREASED NOS. OF-ACTIVE.CENTERS. THE LINEAR
DERENDENCE.OF POLYMER YIELD ON HOL. WT.~ AT:,DIFFERENT REACTION TIMES AND
TICL:SU83 CONCNS., EXCLUDING INITIAL.NON ST:EAOY STATE REGIONS, INDICATED
FREEDO-kt FROM- MOL. C-HAIN TER.MINAlON_AND..A.FFlRMED THE EXIS.TENCE OF LIVING
MACROMOLS..-IN THE SYSTEM. SUCCtSSIVE POLYMN. OF 11, WITH ETHYLENE (0.13
JO 1PERCENT)i ISOBUTYLENE (III) (4.TO 4,,~SPERCENT)i VINYLCYCLOHEXANEq AND
STYRENE J 1.-. TO 1. 2PERCENT) AND I I I ( 3' TO. ~4.'I:PERCENT 1~ GAVE BLOCK
ZOPOLYMPERS-HAVING RESISTANCE TO F RE E Z I NG... IMPACT StRENGTH 2 TO 4 AND 2
TfJ '3 T IME-St. RESPO, GREATER THAN: THOSE 6ft

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