SCIENTIFIC ABSTRACT KHOLOMONOV, I.A. -

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R002201320003-8
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 9, 2001
• Sequence Number: 3
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT


U PROCESSING DATE--13NOV70
ICLASSIFIED
T L TL E~-A DU I T I V EFOR AN INTERNAL COMBUST I UN: ENGINE fUEL.!_U-
AUTHOR- -(05)-SANtNt P. I.. tARABYANt S*'G., SHER, V.V.V~ KHoLo,40NOV, I.A.,
'GORDASHr YU.T.,
44TP 1,NFO--US59
-CCU Y. OF
SOURCE--U.S*SvR9 266t457
~REFEREN .CE--OTKR IYTIYAj I Z08PET. PR CM. 00RAZTSYt TOVARNY~ MAKI L970)
D.AT, E-PUS L I S HE D-- 1 7M Arl 7 0
SUBJ EC T AREAS--PROPULSION AND FUELS
-10PM TAGS--CHEMICAL-PATENTs CARBOXYLIC ACID# ESTER# KETONEv ACETYLENE,
-M I N E RA LOIL, FUEL ADUITIVEr INTERNAL COMBUSTION ENG I NE OR,;ANDALUMINUM
'CO.
C.IINTROL- _-4AKKING--NO RESTRICTIONS;.
CLASS--UNCLASSIFIED
--UR/Oevl32/Tl)/00(3/000/0000/0000
PROXY~REEL/FRAPIE-3005/0879 STEP NO
CIRC ACCESSION NO--AA0
132969
'FIED
NCLASSI
Ull
mg I Ing

bSSR UDC: 5 3a. 72
MALYUS011, V. A. , MAVOROTTROV, N. 14.
BABAK, V. If., KKQL? NOV. L.-F.,
"Steady-State Mass Exchange in a Liquid-Gas System Under Conditions of
Laminar Opposed bbtion of the Phases"..
Teor osno-vv kh--'m. tekhnol. (Th6breticai- P.Irinciples of Chemi cal Technology)
.1971, 5 179-186 rom RZh-Melkhanika No 7,~Jul 71, Abstract No
No 2, pp
7B832)
Translation: This paper deals; vith the problem of redistribution of
matter between'the gas and liquid phases in the case. of laininar film
run-off of a liquid along the valls of vertical platez under counterflow
conditions. The eauations of diffusion. in the liqui (I and gas phixen re-
rm .
--upectively are vritten in the fo
134 C31cr
Dx dgi p, Dr -j.-I
'The boundary conditlons are set up in 'the following vinniner: C.=kc,
D.dc.My=D,4rddy on the phase interface, dc,jIf)y=0. on, tbc- axis of the cbannel
1/2

BABAK, V. V. et al., Teor. csnovy khim. tekhnol., 1971, 5, No 2, PP 179-186
formed by the vertical plates &.1dy-o on the surface o-,r' the plates. ETrans-
lator's note: the subscripts m and r in these expressions stand for
liquid and gas respectivelyJ. The concentration of transferred matter in
the gas phase at the time of gas input into the system is co, while the
concentration of transferred matter in the liquid 1~hese at the time of
liquid Snput into the system is zero. For different values of the dimen-
sionless parameters c and 02, assuming a flat velocity profile in tilie
liquid and gas phases, viz. where V-,, u,- axe the average ve-
locities of the gas and liquid phases respecti-iely, formulas are derived
for the average concentrations of liquid band gas at the output. It is
shown that when the inequalities rP21 are simulteaie-ously satisfied, the
problem can be solved onlyin the gas.phase, assuming that the concentration
is'equal to zero on the phase interfaced_ -Authors' abstract.
2/2
- 70-

USSR UDO 621.376.234
KIREYEV, P.S., %agau"61. KOL'TSOV, G.I., YUHTANOV, YE.D.
"On.The Nature Of The Quick Action Of Cadmium Tellurido Detaotoron
Radiotakhnika i elektronika, Vol XVII, No 3, Mar 1972, pp 60-608
Abstract: The cadmium telluride p-n junction detootoro used In this study had
a working area of 0.1 cm2, a thicknean of 200 miaromet-ar, a capacitance mnasur-
ed at 600 kH-- of 5 pf with a back bias of 220 v, and a back current with this
voltage of 0.1 microamp. The thickness or the region oLf the space charge,
aosessed from the voltfarad characteristic, had a magnitude of approximately
10 micrometer. The output signal won taken from a load recintance of 75 ohm,
With the use
and -the time constant of the oircuit did not excond 0.6 nanoijec.
of an amplifiarp the time constant increased to 4.6 naiiosec. The complex
structure of the output signal is interpreted as the r4mult of a collection of
charges from the space charge rogiong giving a current pulse with a duration of
approximately 10 nanaBoc, and from the bano with a pulme duration of 150-100
68nosece The drift collection of ohurgoa~from the baso Is aoijured an a result
of- redistribution off the field with a sufficiently high level of genorEition of
the charge carriers. 2 fig. 9 ref. Received by editors, 4 Dec: 1970-

NOW"
Instriunents: and easurements~~
USSR UDC: 621.382.001.S:621.376
KOL'TSOV, G. I., KIREYEV, P. S.
ItPulse Characteristic of a Detector With a PIN Silicon Struc-
ture"
Moscow, Radiotekhnika i Elektronika, Vol 17, No 1, Jan 72,
pp 132-137
Abstract: The authors calculate the pulse characteristic of
a silicTn structure with PIN structure uniformly excited with
respect to volume. The detector is made by a method briefly
described by P. S. Kireyev and others in Pribory i 2'Jkhnika eke-
0111
*menta, 1968, No 5, p 63. A pulse x-ray tube was used as
P
the SoUrce of emission, giving an x-ray pulso with an average
on of several
energy of the quanta of about 60 keV and a durati
nanoseconds. This enables comparison of the theoretical And
experimental pulse characteristic. The results of the study
show that silicon detectors with PIN structure can be suc-
cessfully used to register x-ray pulses in the nanosecond
range. Utilization of a simple model of the process of col-
lection of charge carriers enables investigation of the pulse
shape and the processes determining it. Fig. 4, bibl. 6.

USSR
BELUMNBLIT) M. B..V VVEDBIOKAYA, if. D., WDUAVICHUS, I., KOV,41 EV, S. A., FOMIM,
S. V.J* KGOLOPOVI A. V.,, and MAYLAYaCYAN., L. 14. Institutki-'6f P~;61616u-,s-oe Information
Trans~ TssiE, ca e0y of Sciences USSR, Moscow and Moscow State University imeni,
M. V. Lomonosov
"Study of Propagation of Excitation in Purkinje Fibers of the Heart Studied in a
MathematicU 14odel!'
Moscow, Biofizika, Vol 15, No 3, 11AY/Jun 70, PP 521-527
Abstract: Propagation of the action potential in a uniform Purkinje fiber w--s modeled
on a computer using 116ble and McAlister models. The velocity of impulse propagation
in the Noble model is shown to be five times lover, and in the McAlister model two
times lower,, than that rRasured experimentally.. This discrepancy can be explained
by the underestimated value of the rate of grovt1i of thetorward front. of the action
otential in the models used, since the calculations shovc-d that the velocity of
p
the impulse propagation to a first approxitration, linearly depends upon the growth
of velocity of the fox-ward front. The action potential in the regrioLl of fEber expan-
sion waa modeled on the Foble Model. It passen throwh larger expanalons than the
i1apulse in the Hodgkin-Huxley model, apparently because Gf the more extended time
of the heart impulse. It in aloo ahaim that geometric nonuniformity can provide a
1/2

USSR
BERMIBLIT, 1141. B., et al., Biofizlka, Vol 15, 1NO 3, May/Jull 70) PP 521-527
temporary delay in impiLlse propagation, which comprises a consicLv~rable rart oC
atrioventricul.-x delay. It is sug&eBt4-,d that the experimentally observed "hollow"
and "hunip" on the background of the plateau of cardiac action potentials are caused
by the electrotonic reflection" of the potential from geonetric. non)iorriogeneities,,
since the potentials of such a shape are reproduced in model calculationo.
2/2

USSR
BERIKII~O-LIT, Y1. B., DUDZYAVIC-TiYUS, 1., KOVALEV, S. A., FOMIN, S. V., IQIOLOPOV,
- - Tl-.. s-
A. V., zind CMiLAFMAN, L. M., Institute of Problems df_InY~r atfon ran'-
mission, Academy of Sciences USSR, Moscow
"Study of the Formation of a Local Response in a Nonuniform Membrane Cor-
responding to the Hodgkin-Huxley Model"'
Moscow, Biofizika, Vol 15, No 5, Sep/Oct 70, pp 873-880
Abstract: The electric response of a model which cons:ULS of two membranes
regions (otie active and the other shunting) connected in parallel is con-
sidered. This model imitates biological objects containing membrane regions
with a different threshold (c. g., neurons), as viell aa conditions of non-
uniform membrane polarization.. The transition is gradual in actual mem-
branes, however. Shif ts in the amplitude and duration of the reaction that
develops, in the stimulation threshold, and in ionic ciLTrents as a result
of shifts in the ratio of the excitable to nonexcitable area of the membrane
are discussed. On the basis of the model, it is shown that the nonuniformity
of the membrane considerably increases the range of strengths of the stimu-
~lating current at which a local response develops. The relations obtained
1/2
:,[I'll F..'JAJ W IIJ. ION: I t.~, I AI 17~

USSR
BERKINBLIT, M. B., et al, Biofizika, Vol 15, No 5, Sep/Oct 70, pp 873-880
explain some characteristics of the electric reactions of smooth muscles and
of myocardial tissue.
2/2
3

PROCESSING DATE-- 30CT7
1/2 020 UNCLASSIFIED 2 0
MEMBRANE UNDER
TITLE--COMPUTER MODELING OF THE BEHAVIOR OF NERVE FIBER
RHYTHMIC STIMULATION -U-
AUTHOR-(05)-BERKINBLIT# 14*8*1 DUOZEVICUSp I.r KOVALEV* S.A., FOMIN, S.V.,
KHOLOPOVI
1970r 15(1)t 147-55
DATE PUBLISHED ------- 70
---BIOLOGICAL AND MEDICAL SCIENCES
-SUBJECT AREAS
TOPIC TAGS--NERVE TISSUE-y CELL MEMBRANEv MATHE14ATIC MODEL
CONTROL MARKING--NO RESTRICTIONS
DOCUMENT CLASS--tUNCLASSIFIED
PROXY REEL/FRAME--1988/0017 STEP NO--UR/0217/70/015/001/0147/0155
C I RC ACC ES-S ION __N_0--AP0 10 5117
tj I'll, et. L AS-co If-IE0__----ZL

. .. . . . . . . . .
2/2 020 UNCLASSIFIED PROCESSING DATE--230CT70
CTRG ACCESSION ND--AP0105117
ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. THE BEHAVIOR OF EXCITABLE MEMBRANE
UNDER RHYTHMIC STIMULATION WAS STUDIED USING THE MATH MODEL OF HODGKIN
AND HUXLEY. SUMMATION OF SUBTHRESHOLD STIMULI WAS REPRODUCED ON THE
MODEL. THIS PROCESS WAS MAINLY DETO, BY THE TIME CONST, OF THE RESTING
MEMBRANE. THE- PERIODIC FALL OF IMPUI.SES AND THE CHARACTER OF IONIC
PROCESSES RESPONSIBLE FOR THIS PHENOMENON WERE STUDIED IN DETAIL.
EXISTENCE OF MAX. FREQUENCIES WAS SHOWN; THESE WERE REPRODUCED BY THE
MEMBRANE UNDER HIGH FReOUENCY.STtMULATIONP IN THE RANGE.OF 140-170
RESPONSES-SEC. THE CHANGE OF FIBER IONIC GRADIENTS'MAY BE THE CAUSE OF
FATIGUE AND OF GRADUAL TRANSITION FROM LONG CYCLES TO THE SHORTER ONES
IN THE PROCESS OF PROLONGED RHYTHMIC STIMULATION, FACILITY:
INST. PROBL. INFORM. TRANSM., MOSCOW# USSR*
Immimm

Al LASSIHF13~~:~ PROCESSING DATE--090CI'fO
--T~ ESS AND STRUCTURE OF THE SEDIMENTARY COYER IN T~JE INDIAN
TI Yl E lICKNE
'bCtAN, ITHICKNESS AND STRUCTURE OF SEDIMENTARY LAYER IN INDIAN OLEAN)
YU.P.f KHULCPOV# i3.V.
-USSR, INDIAN OCEAN
COU,NTRY OF INFO
UACE-hOSCOd, DGKLADY AKADEM11 NAUK SS SR. VOL. 191, NO. 1, 1970s PP.
DATE- PUBLISHED
~7:.oijJECT AREAS-EARTH SCIENCES ANU OCEANOGRAPHY
71JOPIC TAGs-OCEAN, SEDIMENTARY ROCK LAYERt SEISMIC VELUCITYP SEISMIC
REFLECTION,~SEISMIC SOUNDING
CONTR'OL MARKING-NO RESTRICTIONS
CLASS-UNCLASSIFIED
-PROXY REEL/FRAML-1993/1876 STLP NO--UR/0020/70/191/001/0183/018b
CIRC ACCESSIGN NO--AroII4325
Ul 11C LASIS IF IED

Z/A 009 UNCLASSI FltD PAOCESSING DATE-09OCT70
_~CLRC ACCESSION NQ--AT011-4325
AgSTRACT/EXTRACT--(U) GP-0- A35TRACT. SINCE 1960 rriE INSTITUTE OF
UCEANG-L0&;Y HAS 6EEN CONOUCTING SEI.SMIC STUDIES OF CRUSTAL STRUCTURE IN
-CFED WAVES
THE INDIAN OCEAN BY THE DEEP SEISMIC SOUNDING AND AEFLL
A4ETHODS. F[GUkE 1 IN THE TEXT S.'qGWS EXACTLY WHEkE THIS WUKK HAS bEEN
DONE-AND BY WHAT IRESEARCH VESSELS, THIS ARTICLE 15 DEVOTED EXCLUSIVELY
.,.TG WHAT HAS bcEN LEARNED CONCERNING THE THICKNESSES OF rHE SEDIMENTARY
N
LAYER INN THE INDIAN OCEAN A1~ 0 FIGURE 2 IS A MAP S!"IMARIZING OATA FROM
-:ALL SUCH RESEARCH. THE THILKNESS OF SEDIMENTS ON.THE 141L) OCEAN RE-oGES
IS SMALL ANO VERY VARIABLE. THE SLOPES OF RIFT CANYONS ARS USUALLY
r4lTHOUT A SEDIMENTARY COVER. IN THE ARABIAN SEA AND 711f: SAY OF BENGAL
THICKNESSES WERE RECKONED FROM THE SURFACE OF TifFlAYER WITH A VEL3CITY
OF 6.5 KM-SEC. FOR OTHER REGIUNS THICKNESS Of SEOPIEWS WAS RECKONED TO
THE SURFACE Of T-HE LAYER Wl'TH A~VELOC'ITY-Of' 4a.5_5.5~ KA-'.51EC, THAT IS', IN
SUME AREAS PR06ABLY APPLIES ONLY TO UNCUMPACTLD SEDIMENTS RAfHER THAN
TH-E ENTIRE SEDIMENTARY LAYER. MAXIMUM SEDIMENT THICKNESS (MORE THAN I-Z
THE NORTHEviN REGIONS OF THE OCEAN WHERE
KM) ARE CONCENTRATED IN
ACCUMULATIVE PLAINS ARE PKESENro IN'THE JAVA TRENCH AND NLAR THE SHORES
'Ir-A. IN EXTENSIVE REGIONS OCCUPIED BY OCEAN 13ASINS AND
OF AFR A
OCEANIC kIDGES THE THICKNESS OF THE UN' f H
COMPACTED SEDIMENTS IS L SS T AN
-5 KM AND VARIES GREATLYs PARTICULARLY~ON THE RI&GES. THE TOTAL
THICKNESS OF THE SEDIREUTS I.-Ni. THE OCEANIC 8ASINS ANO ON THE RIDGES WILL
~REMAIN.OPEN UNTIL THERE IS A FULL UNDERSTANDING OF THE NATURE OF THE
LAYER WITH A VELOCITY OF 4.5-5.5 KM-SE~.

UNCLASSIFIED'
--W3 009 PROCESSING DATE--090CT70
-,CIR- ACCESSION NO--AT0114325
_!-:A6.STkACTlEXTRACT-IT US ENTIRELY PROBABLE THA TIN MANY REGIONS AS A RESULT
INTENSE VOLCANIC ACfJVITY THE LOWER PART OF THE 5EDIMENTS HAS 6ELN
COMPACTED AND MIXED WITH VOLCANIC MATERIAL. FACILITY: INSTITUTE
OCEANJLOGY.
UNC LASS I F IE 0
69

UNCL ASS I FED*:7'
009 PROCESSING DAtE--090C'I*fO
AND STRUCrURE OF THE SEDIMENTARY CC]VER IN THE INDIAN
LAY R I I [AN OC AN)
OCEAN (THICKNESS AND STRUCTURE OF SEDIlli~NTARY i~ N No E
.,AUrfiOR-(02)-NEPR0CHfqUVr YU*P.t KH'J
ULOPOV, 13.V*
~'.CGUNTRY OF INFO--USSRf INDIAN OCEAN
saU'AcE--7-m(jsccjN* DQKLADY AKADEM11 NAUK S,SSR.. VOL. 1144, NO. Is 19703 pp.
a4iE PU13L I SHED---70
-~WiJECT AREAS-EARTH SCIENCES AND OCEANOGRAPHY
~J(JP'IC TAGS-OCEAtl, SEDIMENTARY RUCK LAYER, :SEISMIC VELUCITY, SEISMIC
REFLECTION9 SEISMIC SOUNIDING
~.~CCNTROL. MARKINU-NO RESTRICTIONS
-,,.,:-DOCUMENT CLASS-UNCLASSIFIED
;,PROXY kEEL/FRAAE--1993/1876 STEP NO--UR/0020/70/19LI00110183/01-ib
CIRC ACCESS16N Nu--Af0I.143Z5
UNCLASSIFIED

:213 bog UNCLASSIFIED PROCESSING DATE-09OCT701
ClqC ACCESSICA NQ--AT0Ill,3Z5
ABSrRACT/EXTRA%'.T--(U) GP-0- ABSTRACT. S I NCL 1960 ]Ht: INSTITUTE OF
UCEANGLGUY HAS 96EN CUNOUCTING SEISMIC STUDIES Of C4USTAL SIRUCTURE iN
THE INDIAN UCEAN BY THE DEEP SEISMIC SOUNJING AND REFLECrED WAVES
METHODS. FIGURE I IN THE TEXT SHOWS EXACTLY 61-iEkii THIS WL-iiK HAS BEEN
DONE AND BY WHAT RESEARCH VESSELS. THIS ARTILLE IS DEVOTE0 EXCLUSIVELY
EEN LEARNED CONCERNING THE THICKNESSES UF rHE SEDIMENTARY
TO WHAT HAS ijc
LAYER IN THE IINDIAN OCEAN AND FIGURE 2 IS A MAP SIUMMARIZIN 13 DATA FROM
ALL SUCH RESEARCH. THE THICKNESS OF SEDIMENTS ON THE MID OCEAN REOGES
IS SMALL AND VERY VARIABLE. THE SLOPES OF RIFT CANYONS ARS USUALLY
WITHOUT A SEDIMENTARY COVER. IN THC ARABIAN SEA AND THE.' 8AY OF BENGAL
THICKNESSES WERE RECKONED FROM THE SURFACE OF.TllE LAYER WITH A VEL:)CITY
~.OF 6.5 KR-SEC. FOR OTHER REGIUNS THICKNESS OF SE01MENTS WAS RECKONED TO
THE SURFACE OF THE LAYER WITH' A'V'EL0Cl:T'Y'0fl 4.5-5~5 KM~-SEC, THAT IS, IN
SOME AREAS PR06ABLY APPLIES ONLY TQ UNCOMPACTED SEDIMENTS RATHER THAN
THE ENTIRE SEDIMENTARY LAYER. 14AXIMUM SEDIMENT FHICKN~SS (MORE THAN 1-2
-K,14) ARE CUNCENTRATED IN rHE NORTHERN REGION'S OF THE OCEAN WHERE
ACCUMULATIVE PLAINS ARE PkESENrt IN THE JAVA TRENCH AND NEAR THE SHORES
IN EXTENSIVE REGIONS OCCUPIED BY OCEAAl BASINS AND MID
OF AFRICA.
OCEANIC-RI DGES THE THICKNESS OF THE.UNLUMPACTED SE01MENTS IS LESS THAN
0.51 KH AND VARIES GREATLY, PARTICULARLY ON THE RIDGES.. THE TOTAL
THICKNESS OF THE SEDIMENTS IN THU. OCEANIC 13ASINS A.1,11) 0,11 THE RIOGF.S wILL
REMAIN OPEN UNTIL THERE IS A FULL UNDERSTANIJI14G OF THE NAIURE OF THE
LAYER,WITH A VELOCITY OF 4.5-5.5 KM-SECIO
UNIC L A S S I F I E 0

313 009 UNCLASSIFIED' PAUCE'SSING OAT.E--090CT70
CIRC~--ICGESSION NO-AT0114325
:ABSTRACT/EXTRACT-IT IS ENTIRELY PROUBLE THAT IN MANY REGIONS AS A RESULT
S I- -N
Of INTENSE VOLCANIC ACTIVfTY THE LOWER PART OF THE --04MENTS HAS dEL
AND MIXED WITH VOLCANIC MATERIAL. f AC I L I TY: INSTITUTE
.OF GCEA4)LOGY.
89
UNC LASS I f I E 0

1/2-. 022 UNCLASSIFIED PROCESSING DATE--30OCT70
...TITLE-SCATTERING OF X RAYS NEAR. THE MACNETIC ORDERENG POINT -U-
,..:-AUT)JOR-t02)-NA8UTOVSKIY, V.M., KHOLOPOV, YE.V.
_,._.tCUNT,RY OF INFO-USSR
~~-,SQURCE-FIZ. TVERD. TELA 1970t 12(2)t 619-21
"DATE P UBL I SHE 0--- 7 0
-,~SUSJECT AREAS-PHYSICS
,TGPIC TAGS--X RAY SCATTERING, CRYSTAL LATTICE STRUCTUREY MAGNETIC
SPIN LATTICE RELAXATION, CURIE. POINT, -MAGNETIC TRANSFORmATIoN,
JEMPERATURE DEPENDENCE
.,--CNTROL MARKING-NO RESTRICTIONS
-l_-00CUMENT CLASS-UNCLASSIFIED
Pf(GXY REEL/FRAME--1987/1971 STEP NO~-UR/018117C)/012/002/0619,(062t
:.CIRC ACCr:SSI1N NO--AP0105045
UNCLASSIFIED

22 022 UNCLASSIFlio PROCESSING DATE-30OCT70
~-CIRC ACCESSION NO--AP0105045
'ABSTP.ACTIEXTRACT--(U) GP-0- ABSTRACT. THE SCATTERING OF X RAYS ON
FLUCTUATIONS OF D. IN MAGNETS WAS CGNSIDERED. Ut4DER THE EFFECT OF
EXCHANGE INTERACTION OF SPINSt THE LATTICE IS DEFORMED RANOOMLYs LEADING
TO ADONL. BACKGROUND. ON THE OTHER HAND, ANCMALKES AkE PRODUCEO IN THE
PHk)NCN SPECTRUM. BY STUDYING THC TEMP. AND ANGULAR OEPENDENCES OF THE
BACKGROUND ANG INTENSITIES OF BRAGG PEAKS, IT IS POSSIBLE TO DET* THE
TYPE OF THE CORRELATOR ENERGY ANO THE,DEPENDENCE UF THE RELAXA910N TIME
OF THE SPIN SYSTEM ON TEMP. CLOSE TO THE CURIE TEMP. A CUBIC LATTICE
WAS CGNSIDERED WITH I ATOM IN THE UNIT CELL. THE FORCES ACTING AT THE
LATTICE POINTS ARE ASSUMED TO BE CENTRAL, AND THE APPROXiN. OF NEAREST
NEIGHbORS ONLY.IS CONSIDERED. THERMAL~AND EXCHANGE FLUCTUATIONS ARE
CONSIC6RED AS STATISTICALLY INDEPENDENT. FOR DIFFERENT MAGNETS,
-,-DIFFERENT MACHANISMS OF ANOMALIES. CAN PREVAIL~ 'FACILITY: INST.
-NEORG KHIM., NOVOSIBIRSK, USSR.

USSR UOC:621.791.16.052:621.7.011
KHOLOPOV, Yu. V., All-Union Scientific Research Institute of Electric
Welding Equipment
"Treatment of Welded Metal Joints with Ultrasound in Order to Relieve
Residual Stresses"
Moscow, Svarochnoye Proizvodstvo, No 12, Dec 73, pp 20-21
Abstract: The laboratory of ultrasonic welding of the author's institute
has studied the basic energetic characteristics of the process of stress
relief in.welded joints by ultrasonic treatment and the possibility of
using powerful mechanical oscillating systems. Butt joints in several
titanium alloys, produced by argon-are.welding, were studied. Reliable
50-80% reductions3in residual stresses were produced with energy densities
of 1000-1400 j/cm . Energy density seems to be the main factor deter-
mining the reduction in residual stress. At lower densities, for example
700 j/cm3, slight reductions (5-15%) were 'achieved. Oscillating intensi-
ties of up to 10-15 w/mm2 surface area can be used, producing an oscil-
-lating stress of around I kg/mm2. Materials can be processed at at least
20 m/hr.
1/1

USSR uDe 621.?qi.i6,66q.24
YdiOLOPOY YU V.
BERIIH, B. V., Candidate of Technical Sciences, and All-
Union Scientific Research Institute of Electric IdelaTq Equipment
"Selection of a Welding Nozzle Eaterial for the Ultrasonic Welding of Nickel"
Moscow, Byarochnoye Proizvodstvo, ho 8, Aug ?3, pp 26-27
Abstracti Various materials were tested for use as uieldinE nozzles in the
ultrasonic weldina of JvK02 nickel.- The materials tested were EA925 surfacing
alloyt recormendecL for welding copper; 0311, for welding altuijinuir; stellite,
normally used for providing high erosion stability at elevated tem-peratures;
TsN12 surfacing alioy, rec~mmendod for Calling operations a elevated tempera-
turesl nolybdenwa rods(TsF2A alloy), R61.3 high-speed cutting alloy, and E1572
and E1787 heat-resistant Fe-base alloys, and EI89,3 andl DIC26 Ni-base alloys.
Two nozzles made from each material were tested and the performance was evaluated
by the number of spot welds that could be done before cleaning. I-Any off the
materials were rejected for reasons of crack development, low mechanical strength
at higher temperatures, etc. It was ascertained that the strength of a
material in ultrasonic welding depends on its yield strength at the welding
temperature, impact strength, and surface condition. In the weldins of nickel
1/2

USSR
IERIIN# B. V., et al., Svarochnoye Proizvodstvol No 8, Aug ?3, pp 26-27
it waz established that the best nozzle material was the nickel-base heat-
resistant alloys. Three figures, six bibliographic references.
69

..............
Welding' -
USSR UDC: 6'21.791.16
MOLOPOV, Yu. V.
"Ultrasonic Welding"
Ultrazxrukovaya svarka (English version above], Leningrad, Mashinostroyeniye
Press, 1972, IS2 pp.
T
ranslation of Foreword: Powerful ultrasonic oscillations are broadly used
in various branches of the national vconomy. At the present time, industry
uses ultrasonic cleaning and degreasing of vaxious products. Ultrasound is
used to produce highly dispersed emulsions, to disperse solids in fluids,
coagulate aerosols and hydrosols, degas liquids and melts. It has been
established that powerful ultrasonic oscillations influence the structure and
mechanical properties of a crystallizing melt.
Ultrasonic oscillations can relieve the residual stresses in welded scams
produced by arc welding. Ultrasound has been found to influence the intensity
of polymerization of adhesives quite effectively. The ultrasonic treatment of
hard and superhard materials has been broadly introduced-to industry.
One interesting and promising industrial application of ul.LTasound is
ultrasonic welding (USW). This method of welding has vory valuable techno-
logical properties, it is possible to join. metals vdthaut removing surface

USSR UDC: 621.791.16
ishinostroyeniye Press,
Kholopov, Yu. V., Ultrazvukovaya svarka, Leningrad, M,
1972, 152 pp.
films or melting, excellent weldability,is achieved for pure and superpure
s and ceramic
aluminum, copper and silver; thin metal.foil can be welded zo glas
substrates.
Ultrasound is used to weld over half of all known thermoplastic polymers.
Ultrasonic welding of plastics is particularly valuable, since for many
polymers it is the only possible reliable method of joining. Polystyrene, one
of the polymers most commonly used for the manufacture of various mass-
produced products, is best welded by ultrasound.
The possibility pf using USII for tile production of' micxoalceLrojiic pro-
ducts has particularly drawn the attention of researchers.
Presently, equipment and technology,for USIV of metals and plastics have
been developed in the USSR and are being successfully lised in industry.
Abroad (USA, England, FRG, Japan' a number of large firms are involved in the
development of equipment and technology for USIC Series production of USIV
machines for welding of thin metal films, plastics, etc, has been undertaken.
2/6

USSR UDC: 621.791.16
Kholopov, Yu. V., Ultrazvukovaya svarka, Leningrad, Mashinostroyeniye Press,
1972, 352 pp.
However, the process of ultrasonic welding of metals and plastics ;ias
not been sufficiently studied. Recommendations published earlier for the
development of equipment and selection of the most important technological
parameters of the welding mode have been incomplete and partially contradic-
tory. The machines developed in the earl), 1960's failed to meet the
requirements of industry in a number of areas of design and technology.
Furthermore, the opinion developed that USW had an inexplicably unstable
nature, manifested in a wide variation in the strengths of the joints pro-
duced, disappearance of the welding effect and general unreliability of this
welding method.
The necessity therefore arose of analyzing published materials, summar-
izing the results of research and development work Performed at the All-Union
Scientific Research, Planning-Design and Technological Institute for
Electric Welding Equipment (VNIIESO), the Acoustical Institute (AKIN), the
Moscow Higher Technical School imeni Bauman (W7U) and other organi zat ions.
C,
This book Presents a brief description of existing concepts coiicerning
the physical principles of the welding process. The general., most important
316

USSR UDC:.621.791.16
Kholopov, Yu. V., Ultrazvukovaya svarka, Leningrad, blishinostroyeniye Press,
1972, 152 pp.
problems of technology and equipment are studied, typical machines for US111
and specific examples of their utilization in industry are described.
Considering the similarity of the technological equipment used for welding
of metals and plastics, reinforcement of plastics with metals, and also
polymerization of adhesives and relief of residual stresse5 in seams Produced
by fusion welding, we hope that this work will be useful to a broad range of
specialists involved in the utilization of powerful ultrasonic oscillations.
~Table of Contents
Foreword 3
Chapter I. Physical Principles of Ultrasonic Welding
1. General Characteris ties of a Nechanical Oscillating System
2. Characteristics of Loads 40 9
3- Connection of the Load to an Oscillating System 11
4. Basic Parameters Determining the Process of V'elding
and Their Interrelationships 16
5. Mechanism of Formation of the Welded Joint 27
/6---- - 91

USSR UDC: 621.791.16
Kholopov, Yu. V., Ultrazvukovaya svarka, Leningrad, Mashinostroyeniye Press,
1972, 152 pp.
Chapter II. Ultrasonic Welding Technology 39
6. Peculiarities of USW Technology -
7. Zone of Access to Welding Tip 41
8. Influence of Form and Materials of Welding Tip on Welding 45
9. Influence of Surface Condition of Metals Welded on Welding 51
10. Basic Parameters of Welding Mode 53
11... Quality Control of Welded Joints 61
12. Analysis of the Stability bf.the.Mechanical Strength of
Welded Joints 65
Chapter III. Principal Units of Machines for USW of Metals and
Plastics 67
13. Electromechanical Converters
Wave Guides 78
15. Converter Power Supplies 97
Chapter IV. Methods and Apparatus for Measurement and Stabilization
of Parameters of a Ifechanical Oscillating.Systo.m 105
16. Methods and Apparatus for Measurement of Parameters of a
Mechanical Oscillating System
5/6

USSR UDC: 621.791.16
Kholopov, Yu. V., Ultrazvukovaya svarka, Leningrad, Mashinostroyeniye Press,
1972, 152 pp.
Methods of Stabilization of Output Parameters of a Mechanical
Oscillating System and Power Supply 115
Chapter V.- Equipment for USW of Metals and its Application to Industry 125
18. Classification and Principal Technical Requirdments for
Equipment
19. Equipment for Welding of Metals 127
20. Use of USiV of Metals in Industry 137
21. Equipment of USIV of Plastics 143
Bibliography 149

USSR UDC 621-791.16.037
Y-U2W..Y.Y.~ (Cand. of Techn. Sciences), SMIRNOV, A. S., MIPKIN,
R.i USHCHEYEVA, L. P., IGNAVYEV, A. S.,and ERLIN31, M. G. (Engineers)
"HTU-0,4-4 Ultrasonic Welder for Plastics and Metals"
Moscow, Svarochnoye proizvodstvo, No 5, May 72, pp 47-48
,pe of the IITU-0.4-3
Abstract: The New MTO-0,4-4 welder is a prototy
machine. with a redesigned welding headJurnished with'two types of
mechanical oscillatory systems, The new unit is suited for we'-ding
plastic components in the radio engineering and electronics industry
including micromotors, condensers, batteries, filters, cells, etc.
The machine will join plastics with metals by pressing them into
polymers,and will weld copper, aluminum,and nickel. ;The KTU~0,4-3
-model has been successfully operated f9r.-several years at radio
engiueering plants and has shown yearly savings ranging from 5000
to 10,000 rubles. The technical specifications for,the new ultra-
sonIc model are cited. The serial production project has been
assigned to the Kaliningrad Plant of Electrical Equipment. (I
14ustration)

USSR UDC 621.791.89
POVSTYAN, V. 1. , OLLO YU. V.
ItHethod of Stabilizing the Rechanical Strength of Joints in the Case of Ultra-
sonic Welding of Metals"
Kiev, Avtomaticheskava Svarka, No 7, 1971, pp 75-76
Abstract: A method of stabilizing the mechanical strength of joints during
ultrasonic welding of metals and experimental work performed at the All.-Union
Scientific Research Institute of Electric Welding Equipment confirming the
principles on which the method is based are discussed.: The.riechanical power of
an oscillatory system is equal to the product of the force times the velocity
mech ' Fv (where F and v are the oscillatory force and the system velocity).
The required Pi4ech can be obtained by varying these parlqneters of the oscilla-
tory system, Decreasing the amplification coefficient K with a given power of
the oscillatory systen essentially increases its equivalent force, and this
permits stabilization of the amplitude in the welding pToce5s (Kholopov, Zlek
tronnaya te'khnika, Series 10, ANo 7, 1967]. From the. nature of the deviation of
the mechanical power during oscillation of the networL voltage, the following
conclusions are drawn: first, it is most efficient to use oscillatory systems
with small K, in individual cases K < 1; secondly, stabilization of E (the
1/2 'weld
,Wunwn ~.,n

VSSR
POVSTYMT, V. 1. et al., Avtomaticheskaya Svarka, No 71 1971, op 75-76
oscillatory displacement amplitude) can be increased appreciably under the
conditions of some Dower reserve of the power supply when the required anplitude
of the mechanical oscillations is reached by. increasing the power in t1he conver-
ter instead of by varying the amplification coefficient. Ulnen using this system
to weld various materials (aluminLux,copper and gold conductors with nickel,
copper, gold and aluminum Jfflm~circuits an metalP, glass and.silicon), joints are
obtained with high stability of the mechanical strength.
2/2

VSSR UDC 621.791.06
NEFEDOV, V. V., and jpiOLOPOV, Yu. V., M-Union Scientific Research Institute
of -Electrowelding
"Ultrasonic Foil Seam Welding"
Kiev, Avtomaticheskaya Svarka, No 12, Dec 70, pp 58-59
Abstract: A process developed by the All-Union Scier-tific Research Institute
of Electrowelding Equipment for a continuous transverse system with 1.5 kW
of power for ultrasonic seam welding of metal foils is described. Features
of the process are its low sensitivity to loading and the br*ad zone of ap-
proach to the welding roller. Experiments on using tbo process for aluminum
welding are described. The energy for the device is supplied by an UZM-1,5
ultrasonic generator whose output parameters are controlled.by a T-141 thermal
volt-ampere meter. The amplitude of the welding roller oscillations J.s mea-
sured by an UBV-2 vibrometer and its frequency by Lissajou figures using the
51-1 electronic oscillator and the CZ-34 sonic oscillator. A drai-wing and a
description of the welding head,are given as well as curves showing the
strength of the weld seam as a function:of the oscillation frequency of the
welding head and the welding rate. Ultrasonic seam welding:is seeA as a
highly productive method for Joining aluminum, coppert uickel, and other foils.
mop w.

DATE-11DEC70
1/2 0 le, UNCLASSIFIL-0
T.1 TLE--VTU 0 ei- FOR ULTi,~ASuNIC :AETAL WELJING -U-
T (C5) KiiC. -YU. V. LAYTSEV9 M.P., S,14IW-.0Vj A.S., SC.'JATENKOVI
,-~.V*A. s- tl(L M*Gt
LU;,iT P Y CF f;jFL--USSRs U'41TED KINGOGA, UNITt-D STATES
.SGURC E-~,35C6 W SVAR0CHNGYE PK(jIZVUUSTVC, NO, 51 1970, Pll 47-43
,-i, )AtE PuliL fSHEC------70
�.UBJ E C T AREAS-MECH.t IN0.9 CIVIL.-AND YA,RINE ENGR
'TOPIC TAGS--PATENTv ~ELUING EQUIPMENT, FOREIGN' TECHNICAL kEL"TIONt
WELDING, MAChINERY MANUFACTURING PLAIlr~(U)AIU04 3 UfRASON[C
-WELDER
:.CCt4:tPCL PA~KI&G-410 RESTRICTIONS
-0 CCUMENT CLA~`S--UNCLASSIFIED
~PRJXY FICHE STEP
CI - RC- ACC ESSIUI NG--APOIA2720

212 018 UNCtASS[FIED
CIRC ACCLESSIGN NO--A PO 142 72 0
A --(U) (;P-0- Ab S TRA C T ~CHINE FOR k; L T 1; S Cs;, i IN
dSTRACTIEXfRA(;T THE H!, "Ic ~!E
N COUSTICAL SECTION, USIN6 .4 1 ICALLY
OF METALS CCNSISTS OF A. A
OSCILLATURY SYSTEM, ThE ~4ELOIING HEAC-p FIXED T13 A fABLEv A WRLZONTAL
SEFVU FOR THE ACOUSTICAL SECTICN, A CON-TACT PRESSLIkE SEt~vur
CLNTRC;L EQUIPMENT FOR THE EiNEkGY FEE[) SOURCE, At.11) CtINTRDL t-IEDALS. Tli E
E
ACOUSTICAL SELTION HAS A MAGNETosr.R[CTIVE TRAINSOUCER, ~A KNiFE
EXPCNENTIAL WNCENTRATUk, AND A RESON41ING ROD OP!-_'kATJ'N(,' 1`4 THE 61__N0!N('-
Ai 'E I
QSGILLATICii il"WE. A PH..,jr,'JGRAVH -OF THE MACHINE IS GIVE To(- HER VITf(
'EIAILS OF ITS CONSTRUMON, ANG A CRGS5 SECT t AL OIA RAM Of
FURTHER I, A G
THE ACOUSTICAL SECTION IS PRESENTED. OPERATION Of THE MIACHINE W40ER
PLANT. CCNDITICtNS HAS SHOirioN TAHT IT IS :SIMPLE ANU RELIABLE N OPPRATION,
% _F ADE !3~
--EXPEPIMENTS 6EkE CONGUCTLf~ ON THE. MECHANICAL STA3~LITY (j 4ELDS 'A
ThE MACHME IN THE CGURSE OF FILM TRANSFORMER ANU ELECT!'-!lc.%L cApAC[Tf-jR
MANUFACTUkE; THE RESULTS OF THOSE EXPERIMENTS Ak:E.,(;IVCb; IN TABULAR FURtit
THE MTU~0.:4-3 PACHINE HAS BEEN dK(;',ANIZE0
ASSEYbLY. LINE. MANUFACTURE Uf
THE "E:LEKTROSVARKA" PLANT IN KALININGRAD. PATC-NTS HAVE BEEN 013TA N
iN I cl)
FOR' THE MACHINE IN GREAT ERLTAlk AND THE, UNITEO ESTATES.
A:LiLITY.-' VNIIESO.
F
c-T
- ~ I , f I lj

US3R L D-,' 02 11 16 u-7
'"an-J"date o~ i" e ch r.-; c -a I-oicrices, ZAY-3EV,
K
40
of lec-Ini DIV, A 3 E n;,, -1. n e e r ,SQIDA~-i L-, i , vA er,
ca L Scionces, ngL,,
a kid EIR L-Tili1G E n i i i e o r VIN SO (All-Union Sciontific iesearcii LristiLiute of
*IIE
Electric V.,'elding Equipment)
"The A,-iTU-0.4-) Machine for the Ultrasonic Welding of lHotal-l"
Froizvodstvo, No 1, I-Ilay 70, pp 47-1,-.-)'
Xoscow, 3varocanoye J
Abstract: A description JL3 given of the IrIU-0.4-3 nacid.ine -Car the, u-Ii.trasonic
weldinc- of metals. 'E,,mloitation of the maciiine under ~mdustrial conditicas si-.ows
that it is simple and reliable in its operation. . ;-lear-resistazat welding Lips
may produce up to 81,000 spot welds before servicing, Atma" up to 250,C,60 b~-~fora
being replaced. The use of. the machine in The productioa of K-110-6 and K50-7
aluminum electrolytic condenser5 resulted in a 14.5'f mduction of rojecLs, and
in increased. welding reliability, greater service life of tie article, and a
39;~ increase in labor productivity. Specifications of the machino are as follows:
rcrwer in k.; 0.4
Omrational frequency in kc 22t7 5-'
1/2

USSR
MOIDPOV, YU. V., et al, Svarochnoye Froizvodstvo, No 5, MaY 70, pp 47-48
Contact prossure in kg 8-6o
Thickness of welded articles
in mm 0.01-0.2
Productivity 15-90 spots per min.
Welding tip feeding in mm 120 x 47 or 120 x 74
Gap.be-tween tips in O-n
Dimensions in mm ~1300 x 600 x 1235

USSR UDC:669.018.95:537.311
DYADENIKO, N. S., LUINIKO, A. I, and KHOLOPTSEVA, T, V,, "Radiopribor"
Plant, Kiev
"Electrical Resistance of Copper-Graphite Powder Compositions"-
Kiev, Poroshkovaya Metallurgiya, No 12, Dec 73, pp 62-66
Abstract: This article studies the change in electrical resistance
during the process of pressing of copper-graphite powder compositions
with "open" graphite and graphite covered.with copper. For comparison,
experiments were also performed with pure copper. Furthermore, the
evenness of distribution of the components in presshigs p7-odoced at the
greatest pressures was determined. The change in resistivity of copper-
graphite compositions during the process.of their pressing shows that
a sharp reduction in resistivity of all compositions studied is observed
at pressing pressures of 1.2-1.6 t/cm2, while resistivity decreases more
smoothly above this pressure. Compositions containing graphite granules
clad with copper have significantly lower resistivity than compositions
with "open" graphite, as a result of the formation of a solid copper
framework-in the first case, and a graphite frame in the second.
1/1

USSR UDC: None
G., VOYEVODIN, Yu. M., VERKLOV, B. A., and ZAVGO
RODNIY, Ye. IM.
"Safety Valve for Hydraulic Systems"
Moscow, Otlgrytiya, izobreteniya, U'romyshlemyye abraztsy, tovarny.Ve
znaki, No 27, 1971, p 124, No (11)351027
Abstract: The body of the valve contains a load spring in a gate
made of a hollowed cavity containing a two-Piston differential
plunger. There is also an added cavity with a two-piston plun-
ger containing a stepped bore -into which the first cavity fits,
thus lending the device compactness and a better structure. The
valve is made by cutting slits In the body into which the plungers
are inserted. A diagram of the device in cross section is given.
1/1

USSR UDC 537.29
KOMNILOV, E. N., KHOLP-0
10V, L. P..and PUPKOV, Ye. I., Tula
"Effect of Electrolyte Composition and Temperature on the Anodic Dissolution
of VT-14 Titanium Alloy"
Moscow, Fizika i Khimiya Obrabotki Materialov, No 5, Sep-Oct 72, pp 130-133
Abstract: Experimental data are presented on an investigation of the anodic
polarization of VT14 titanium alloy in different electrolytes and oil a de-
termination of the limiting stage of the anode process during electrochemical
treatment. It was sho,4n that the dissolution rate and anodic polarization of
the alloy depends primarily on anion composition and temperature of the
electrolyte and that the limiting stage of VT14 dissolution is electrochemical
for the electrolytes used: 15%. KBr (pff 8.2), 15% NaQ + U NaF (pit 8.3),
15% NaCl (pit 7.5) and 14% KF (pit 9.2).~ Of these ele,_~,trolytes, the bromide
and chloride-bromide electrolytes had the greatest electrovi-ienical activity,
allows them to be recommended for~the.electrocbemical treatment of
which,
VT14. 3 figures, I table, 7 b-bliogra'hic refe'rencesl.
P
83

USSR UDC 532.516
KHOLPANOV, L. P. , SHKADOV, V. Ya., MALYUSOV I V. A., 71-14AVORONKOV, 11. 1/1
"A
Theoretical Study of Gravitational Runoff of Thin Laye_rs of Liquid Under
Wave Formation"
V sb. Teplo- i massoperenos. T. I Ofeat and Hass Transfer. I'Tol. I -- Col-
lection of Works), Minsk, 1972, pp 186-197 (from RM-Mekhanika, No 8, Aug 72,
Abstract No BB741)
Translation: The problem of the flai of a thin liquid --film over a vertical.
plane. in the absence of gas flow and the analogous proUen of a film In the
1wesence of a gas flow washing, the film are solved in t*.~e nonlinear
approximation. To solve the first problem the flo4 function and the
variable thickness of the fibi are expanded in series in terms of harmonIcs.
Equations -for the expansion coefficients obtained after substituting expan-
sions into the Navier-Stokes equations and the boundary conditions are
solved by ccmDuters. Figures are given shoeing the lines of flaa and
ratio of the surface velocity to the average (with respect to the film
thickness) for t-wo values of the Galilean number G = gh3/v2. It is uointed
1/2

MOM
1