SCIENTIFIC ABSTRACT GOVORKOV, B.B. - GOVOROV, A.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000516420019-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 13, 2001
• Sequence Number: 19
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

P A tI C, V o r k ov
T e r'." I j P -1c) t op r tAuc t i OT -j ipul
Y_-Iderniya fizika, v. 1, no. 1, 1965, 9Z-95
ne-~ r ra I p I on prodtic t I an , P I nn rill t i on e I ec t r ica I d I Po I e
phoLoproductLon, near chreshoid pion productiun
~,.777RA-- The correct dateT-mination c-f the phy-;tcai pgranu-trrg of low-ener-3y
r~-_I, !riper !a I importarw_ e i n r onner t i on w t r n no avDcthes-Is cancerning
-m--5on (A. M , Baidin Nuovo Cint. ibli 1 17 A M . 58 L L i, .
R - i 2 2 , 3 6 1 . 19 5 8 ; A K . Ba 1 d i t A . A - Ki F_- a r z I z. t o v. or. Hi-gh
Phy, i
r qIcs at CERN, 1962, p. 657) Exper, Lment a I data on the r+ P-- p
have been analyz,-d in the vivinity of -,he -hreshold so a6 to deter-mine
ci,~ tiectrkcal dipole amplitude E for x~-weson ~tiotoprooljct ion. Twu, metho-is of
determining E lead to dIfferent valuei for this quantity, The authors remark in
,c~ Added in proof or 19 December [964 that in vIEv of tho paper by Yu. D.
Prokoghkin submitted to the 12th Inte--national -Ionference on High Energy Physics
Card
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ASSOCTATION: FizicheskLy institut im. P. N. Lebedeva Akademii r-auk SSSR (Phyaics
Institute of the Academy of Sciences, SSSR)
SU-Pn=D: ZOJ4164
hV UP SOV: 006
ENCL: 03 SUB CODE: te
OTHER..
Card 2/2

ACC NR: AP60314220 -SOURCE CODE: UR/0120/66/000/005/0060/0066
AUVHOR: Capotchenko, A. G. ; G2o~vo~~; Denisov, S. P.; Kotf?l Inikov, Ys. G.;
Stoyanova, D. A.
ORG: Physics Institute of the AcadenV of Sciences ISSSR, Moscow (Fizicheskiy
institut AN SSSR, Moskva)
TITLE: A spark chamber as a detector of hidi-energy electron and photo showers
SOURCE: Pribory i teklinika eksperimenta, no. 5, 1966, 60-66
TOPIC TAGS: spark camera, spark chamber, electron energy, DF-rPCr-"'7')
ABSTRACT: Characteristics of a multi-plate spark chamber used as a detector of
y-quanta and electron showers whose energies range between 50 and 200 Yev are studied.1
The total number of sparks formed in the camera while it is registering showers is I
proportional to the energy of primary particles; the average number of sparks is
linearly related to the primary particle enerr&r. Fluctuations in the total nunfoer of
sparks varies according to Poisson's law. A formula relating the thickness of the
chanber electrodes with the camera resolution is derived. Data on spark distri -
bution along the shower axis and on the effectiveness of the camera in registering
y-quanta are given. Orig. art. has- 8 figures.
SUB CODE: 20, 14/.SUBM DAM: 09Nov65/ ORIG PEF: 003/ OUR REF! oo6
Card 1 /1 UDC:- 539-1.071-

GOVORKOV, E.
Sorevnovanie za snizhenie sebestoi-
inosti (Competition for reducing costs). Moskva,
Profizdat, 1952. 87 p.
SO: Monthly List of Russian Accessions, Vol. 6, No. 1, April 1953

ACC NRi AP70056o8 SOURCE; CODE: uR/o4l3/67/OOO/OO2/oo48/oo48
INVENTOR: fuifilov, Ye. A.; Govorkov. I I.; Gurevich,iR. V.; Zhuchkin, I. A.;
uznetsovi V. D.; Olifin, L.
ORG: None
TITLE: A cophased antennh array with electrical scanning. Class 21, No. 19o433
ISOURCE: Izobreteniya, promyshlennyye obraztsy, tovarnyye znaki, no. 2, 1967, 48
C TAGS: dipole antenna, antenna array, antenna d*ectivity
MRACT: This Author's Certificate introduces a cophased antenna array with electri-
scanning. The installation is made in the form of center-fed dipoles arranged
groups and equipped with an aperiodic or -tuned reflector. In order to reduce the
,el of side lobes of the directional pattern in the horizontal plane, the lower
mp of dipoles is shifted horizontally with respect to the upper group in the plane
the array by one-half the distance between the adjacent dipoles in the group.
UDC: 621-396.677-32

ACC Nib Ap7oo%W
L"center-fed dipoles;* 2--lower group of dipoles; 3-upper group
UB CODE: 091,' SUBM DATEt 27AUS65
0

MCOM, A.G., kandidat takhnichookilch nauk; GOVORKOV$ N.A. inshener,
retsenzent; TARIM3190, M.Ts. inzhene., P.To.,
inzhener, redaktor; MOWV, 3.0., tekhnichaskiy redaktor
[Electric equipment for hoisting and transporting machinery] Blektro-
oborudovante pod"emno-tran P,Drtnykh mashin. Koodkva, Goo. n&uchno-
tekhn. izd-vo mashinostroitellnoi lit-ry, 1954. 372 P. (ML8A 8:4)
(Electric machinery) (Hoisting machinery)

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SA 64
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"621-318.2.042.1
V. A. Govorkov. Elektricheatyo (No. 4) 47-56
3364
Degian o Lg=p.
.
.
.
1950)_ i1m. 7
In
Russ
(April
x.
If the wquat ono of the magnetic circuit a~e so expressed as to conWn

wh
'd funation of-the speqific energy W(B) -j HdB.* ich may be unambigu
determined from the maEpetizi~qotj curve of the material, a number of
problems in the practical. 01cuiation of vapetio oircuits can be solved.
An-important example is the calc~latiqn of laminated cores~,with overlap
'
of the..individusil sheets.- The method-le
based on COG ma Izations

abut its results are suitable for,-allbernating magnstizat
Well
provided the fi-equency is not too high The approximation tormiulas derived
a broken linear curve substituted for the actuai ma'Setization
are based on

B, F. KRAUS
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JI-

GOVORKOV, V. A.
"Electric and Magnetic Fields," 339 P., State Publishing House Pertaining to Lit.
on Communications and Radio,. Moscow 1!~51.

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w-kTOFIN-OV, V.
Solvin.- problems in the electric and magnetic fields by using potential screen ~grids.
Tr, from the Russian. p. 42. (StrojnoplektrotechInicky C--~z5o,,A5. '71ratislava. '101.
3, no. ?, 1952)
M: Mont'hly L st of Fast European Accessions, Lr,, Val, 4, Nol -6,
June 1955, Unci.

r,ov()RKOV,
Calculating electric and magnetic fields in polar coordinates 10~y US4ng
potential screen grids. Tr. fromthe Rus,-4an. P- 53 (rjtro.,jnoel~-ktrotechnIcJ-y
Ca5opis. 9ratislava. V01. 3, no. 2, 1932)
SO: Monthly List of East Nropean Accessions, (ML), M, Vol. h, iio- 6,
June 1955, Unel.

GUVORKCVJ V.A.
03novy tekhniki avtomatichaskoi telefonii. fBasic principles of automatic telephonz7-
Moskva, Sviazl-izdat, 1937, v. 1-2
SO: Soviet Iransportation and Comrunications, A Bibliographj , Library of Congress,
Reference uepartment, Washington, 1~52, Unclassified.

WVORIKOV, V. A.
"Works of Acad. M. V. Shuleykin on :,2ectrical Machines," Elektrichestvo, No. 5, 1952.

1. GOVORKOV, V. A.
2. USSR (600)
- 4. Physics and Mathematics
7. Electrical and Magnetic Fields. V. A.Covorkov. (1408cowp Communications Press, 1951).
Reviewed by A. A. Semenov. Sov. Kniga, No. 5, 1952.
9. FDD Report U-3081, 16 Jan. 1953, Uncla&sified.

GOVMWV,, A
WoulatIng UAW IMA nonliam eilsetric networks 'by the tabu-
lar method. Blektrosviss' 10 noolo:63-73 0 156. wa 9: 11)
(Ilectric networks) 1,

PHASE I BOOK EXPLOITATION SOV/1175
Govorkov, Vladimir AlekBandrovich and Kupalyan, Stepan Davydovich
Teoriya 61ektromagnitnogo polya v uprazhneniyakh i zadachakh (Elec-
tromagnetic Field qbeory in Exeroises and Problems) Moscowo Izd-
vo "Sovetskoye radio," 1957. 339 p. No. of copies printed not
given.
Ed.; Masharova, V.G.; Teoh. Ed.: Koruzev, N.N.
PURPOSE: This book Is intended fo:? students of vuzes studying the
electromagnetic field theory anti for specialists conducting calcu-
lations on electric and magnetic, fields.
COVERAGE: The book comprises over 400 exercises, problems and tests
on electromagnetic field theory at the level studied in radio engi-
neering vuzes. The authors claim that some exercises are published
for the first time, namely the exercises on:.approximate calculation
of fields, application of the relaxation method and the method of'
constructing the field pattern for calculating stationary and al-
ternating fields. The authora have paid special attention to graphi-
Card 1A

Electromagnetic Field Theory (Cont.) SOV/1175
cal construction of electric and magnetic field patterns. Chap-
tera 1 through 6 were written by S.D. Kupalyan, and Chapters 7
through 9 by V.A. Govorkov. The authors thank Docent M.R. Shebes
for his help. There are 15 referenoes, of which 9 are Soviet and
6 English.
TABLE OF CONTENTS:
Foreword
Lists of Symbols
Ch. 1. Vector Analysis
Ch. 2. Electrostatic Field
Ch. 3. Electric Field in a Conduoting Medium
Ch. 4. Magnetic Field From Direat Currents
Card 2/4
5
7
9
22
48
53
A

Eleotromagnetic Field Theory (Cont.) SOV/1175
'Ch. 5. Electromagnetic Waves in a Dieliectric 76
Ch. 6. Electromagnetic Waves in a Conducting Medium 93
Ch. 7. Directional Electromagnetic Waves 1o6
1, Reflection of electromagnetic waves from a conducting
surface 106
2. Electromagnetic waves between parallel conducting surfaces
( y-0 and y~-b ) ill
3. Electromagnetic-waves in a rectangular wavegaide with cum-
section ab 136
4. Electromagnetic waves in a parallelepiped cavity resonator
with edges
doaob 157
5. .
Electromagnetic waves in a cylindrical waveguide 169
Ch. 8. Special Methods of Calculating Electric and Magnetic Plaza 180
1. Principle of super position 18o
2, linage method 215
3. Method of average potentials 229
4.. Method of conformal mapping 234
Card 3/4

Electromagnetic Field ~%eory (Cont,) SOV 175
A
Ch. 9. Approximate Calculation of Electric and Magnetic Fields
1. Graphical construction of field pattern
2. Relaxation method (finite differences) applied to station-
ary ahd"qaasi-stationary fields
30 Relqxatlcffr method applied to alternating electromagnetic
fields in a conducting medium
4. Relaxation method applied to alternating electromagnetic
fields in an ideal dielectric
5. Determination of critical wave-length in wdveguides and
' cavity reponators by the relaxation method
60. Application of the-expected stream-paith method
Answers
Appendixes
Bibliography
AVAILABLE: Library of Congress
irlsfm
2-24-59
Card 4/4
251
?51
259
275
287
292
307
~14
338
340

V. m I
16(0)s 28(2) M%fz I rox IMAMTral SOY/3365
Aladaimlys, monk Azorbarulacckr am
lbaloy daklMor So"mbdAnlys yo -ryehislitel'opy matematiza, t prixonvatyu
amdqtv vychUlttaL-wy tkbnLtl (Outlines of Nmorto of tbo Conference On
C-Plutionel ihtboM%t.v al the Use of Camputor Tvc)=lq-s) b-J-, 190.
63 p. 4M "too printed.
A&LItlemal Opme"s ASencimot U14autp nook SM. Trahlolitel'UTY 14matz,
ond Ak.&mt.- -uk MU. I..Utt ,U-%LU t tol-Ab-M.
On dootritutm mentioned.
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..at-" mod &et*.tLft6 -~irk*ra, ~Wmm, ~k Involves c*Met.Uft and the MAND
of dlglt-I ond auslog 914atruclo , term.
COMM IM. book contains wavattoa of reports umbdo at t1w CoeNrecom, ca
COMPmtAtIonal tkt)wlnttce wA Uw AVVIlo4Um of Computer Tt~MlVwo.
The book to dLvtdod into two imila, parts. Ito first par% to drow to
computational matbamatlem and contains 19 rumovarlso of reports. In togma&
.tion to 4-otod to -Tttad Mhlquma -4 contains 20 -.rise erf
rts. So parowalittee arm mwsU*cw4. No xiforenc4a an Alves.
=
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With woestic (Serrita) lit"wate With &arv Central Co. Stereo )2
low, Ms. ON as solution, of D"lep"olsion Ffvblom = sicefts
54
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levels Of Its Tm"ftf 10 IIIM Nut is Us lint Approx1jualtoce 31
Call 5/t

C" Vu /Z-, V
lo5-58-4-3/37
AUTHOR: Gov orkov, V. A.,Docent, Candidate of Technical Sciences
TITLE: Calculating Electromat,inetic Wave by tile Lattice
Method(Raschet rasprostraneniya ele!-.tromagnitny1:h voln
metodom setki)
PERIODICAL: Elektrichestvo, 1950, 1Tr 4, PP. 16 - 22 (Ussm)
ABSTRACT: In this paper a method of the approximated nuiierical solution
of the calculation of the propa~;ation of electroma,-enetic
waves is given. It is assumed that the dielectric flillinE
of the hollow s~.)ace of the wave juide or of the resonator
is ideal, i.e.exhibits no conductivity (y = 0) and the vialis
of the wave guide or resonator concist of an ideal crnductor
y=oo). At first the electric tranf;verse waves (TE-or H-waves)
are investi,-ated. The distribution of the lonf:-itudinal com-
ponent of the maL.-netic field strenZth 11Xon the transverse
plane uz(the X---Xis coinciding -aith the direction of the
Cz~-~(- 1/5 wave propagation) follows the tvo-dimensional wave equation (1)

105-50-4-3/37
Calculating Blectromapetic Wave Propagation by the Lattice Method
2 ~-2
H + k Hx - 0, on which occasion 12 - - + 7
~Yz x 2
42 yz y 2 z
denotes the two-dimennional scalar Laplace operator in the
transverse plane yz. h denotes the ei,~;envalue which in the
wave guide i,-- equal to the critical ph---.ne factor and in
the resonator to the phaze factor of the ei~;cnoscillations
of the lowest frequency. The derivative of c"u-Aion (1)
as aell as of (3) Ymo carried out for tile special case of
a direct travellinj wave in the wave ~;Llide in reference 1.
These equations c-an be P-Pplied also in the wave guide in
which the electroma~nctic ota--din- is the result of
a superposition of the direct and the reflected wave. Follo,,-Iin,"-
the equations(3) and(4) by neans of widich the tranaverac
components of the r3a~netic and eloct-ric field are deter!.-:i:1cd
froin the lonoitudinal component, arc z,2itten down. In th.--
case of the wave -uide the equations are rcduced to(5) or
(6), The lon---itudinal co;,.iponent of the field 11- can be re-
card 2/5 -arded as the funda-:iantal charactcristica of t'lle elcctro-

105-58-4-3/37
Calculating Electromagnetic Wave Propajation by the Lattice Method
magnetic process if all other field components can be
obtained from it according to the equations (3)-(6). The
nu-merical calculation of the distribution of H. can be
carried out by means of (2) according to the lattic me-
thod at any form of the boundary lines. The boundary con-
dition is the following:llormal components of the magnetic
field and the taGential components of the electric field
at the wave guide or resonator walls equal zero. The inte-
gration of equation(l) is a typical Neumann(Heyman) prob-
lem. Following, the magnetic transverse waves (TIT-or E-
waves) are investiEated. The equations (9) and (10) for
the transverse components of the electric and magnetic
field are written down. in the case of a wave guide they
are reduced to(11) and(12).The limit condition is the follow-
ing;the longitudinal component of the field E x at the
boundaries of the cross section of the wave guide or the
resonator is zero. The integration of (7) represents a
Card 3/5 Dirichlet problem. The calculation is rendered difficult
_41

105-58-4-3/37
Calculating Electromagnetic Wave Propagation by the Lattice Method
by the fact that Ilk" is contained in the equation. There-
fore some provisional values of the number k 1 must be
assumed and the calculation must be carried out in all
points according to(2) and(B). A complete liquidation
0
of all "rests" is riot possible on this occasion. All or
at least the majority of the rests should be brought to
the same sign. In order to carry out the problem more
quickly first a calculation should he carried out accor-
ding to a rougl(network. with few nodal points. If, in the
course of the calculation none of the rests has an abso-
lute value greater than trio random units, the more pre-
cise calculation on a finer network can be carried out.
An increased accuracy can be achieved 1) by multiplying
all values obtained and the rests by 10 and a subsequent
liquidation of these rests on which occasion this process
can be continued until the desired accuracy,2)by applying
Card 4/5 a still finer network, and 3) by passing to more precise
3

lo5-5s-4-3/37
Calculating Electromagnetic Wave Propag-ation by the Lattice Method
calculation equations. In the supplement 3 examplea are
calculated numerically and the derivatives of tfib'formulae
are given.There are 5 figures, 1 table, and 5 So*iet
references.
ASSOCIATION: flockovakiy eluktrotel-chnicheskiy institut svyazi(Moscow
Electrotechnical Institute for Telecommunications)
SUBMITTED: February 19,1957
AVAILABLE: Library of Congress
E1sctrMBPGtiC waves-PropegAtion-ThO017 Lattices-AppUcatjow
Card 5/5

PHASE I BOOK EXPLOITATION
Govorka;r, Vladimir Aleksandrovich SOV/3T24
Elektricheskiye I ma$nitnyye po3jys (Electric and Magnetic Fields) 2d ed.,
completely rev. and enl. Moscow, Gosenergoizdat, 196o. 4Q p. Errata
sUp inserted. 15,000'copies printed.
Edo~. D,V. Bychkov; Tech.: N.I. Borunov.
PURPOSE: This book is intended for students and aspirants of institutes and
divisions.of electrical and ratio engineering, as wen as for engineers deal-
ing with problems based on the theory of electrTaguetic fields.
COVERAGE:. The theory of electrcn&gnetic fields is presented with a view to its
practical application In calculations of. statioh~ 'and alternating fields ea-
countered in radio engineerinop, comunications, electrical power engineering,
and in. automation and telemecbsni es equipment. Stress is therefore Wd on
simple: methods of calculation, such as relaxation methods, which use very
simple instruments and tables of calculation. ReMirs desiring more extensive
-information on the theory of electre-agoetic fields are refwmd to Soviet text-
books by,L.R. Neyman and T.L. Kalantarov., A.V. Netushil, and K.M. Polivanov,
card 1/18

Zlectrieg! and Magnetic Fields SOV/3724
and to the works of I.Ye. Tam, V. K. Arkad'.yev, L.D. GoI'(3Ehte-,n,
N.V. Zernov, and L.A. Vaynshteyn. The book " Tor.riy~i elektromagnitnoco
polya v uprazhnenyakh i zadaebalch" by V. A. Govorkov
and S.D.-Kupalyaa is repeatedly reterred.to in the text of the monograph.
There are 53 references& 50 Soviet. and 3 Engiish.
TABLE OF CONTEM:
Foreword 3
Ch. 1. Introduction 13
1. Basic definitions 13
2. Scalar and vector qualities in electrical engineering 1-8
Ch. fI. Conceipt of Vec~or Analysis 18
1. Addition of vectors 18
2o Scalar product of vectors 19
3- Vector product of vectors
' 19
4. bizit ;mcto'r
s
' 20
5. Scilar'ijd
vector -prolucts expiessed thr6ugh their ccopments 22
-6. Product:of thrve vectors 23
7- Gradient of scalar p6tential 24
8. bifferential operator 26
Card 2/18

GOVORKOVp V2adimir Aleksandrovich; DOIENKO, L.N... red.
(A.c. networks with ferromagnetic cores] Uepi peremeh-
n6go toka a ferromagnitromi serdechnikami; tichebrLos -po-
sobie. Moskvap Moak, elektrotekhn. in-t av-iazij' .1,962. 78 p.
(MIRA '17'2'5).

GOVORKOV Vjgdimir Aleksandrovich; KUPAIYAN, Stepan Davidovich;
:~~~~WA, G.Ye.,, red.; GOROKHOVAO S.S., tekhn. red.
(Islectromagnetic field theor-y in exercises and problems)
Teoriia elektromagnitnogo polia v uprazhteniiakh i zada-
chakh. Izd.2.0 perer. i dop. Moskva, Vysshaia shkolap
1963. 370 p. (MIRA 17:4)

GOTOREDT, T.G.; PARTOV, TOY*
fine Interval Indicator :for cinematography. Trudy Inst.krist.
no.11:243-246 955. (MIRA 9:6)
(Cinematography)

I SOV/70-3-1-10/26
AUTHORS: Regel', V.R. and Govorkov, V.G.
TITLE The Dependence of-t_he__UF17_ti0a1'Splitting Stress of
Single Crystals of Zinc on Temperature and Rate of
Deformation (Zavisimost1,kAticheskog0 Bkalyvayushchego
napryazheniya, monokristallov tsinka ot temperatury
i skorosti deformirovaniya)
PERIODICAL: KriBtallografiya, 1958, Vol 3, Nr 1, pp 64 - 70 (USSR)
ABSTRACT: Studies have already been reported by Schmidt and Boas
("Plasticity of Crystals") on the behaviour of Cd at
different temperatures and at different rates of defor-
mation. In view of the similarity of its structure Zn
has now been studied. Crystals of Zn were prepared from
99.98% Zn by the method of Obreimov and Shubnikov; they
were withdrawn from the stove at a constant rate of
1.8 cm/h and had a length of about 150 mm. Each rod was
cut into 3-4 spegimens. The orientation was determined
optically to 0-5 by identification of the 0001.(cleavage)
plane. The angle between the normal to this plane and
the axis of the rod was kept between 25 and 700 for the
Cardl/4 crystals used. Extension experiments were carried out

SOV/70-3-1-10/26
The Dependence of the Critical Splitting Stress of Single Crystals
of Zinc on Temperature and Rate of Deformation
on a Polyani-typB machine and the temperature was
stabilised to 1 C. Experiments were made in the range
20 - 416 0C at extension speeds of 2,3 X 10-1 NTA X 10-4
and 3.3 x 10-5 mm/sec. These gave the limit of flow s t
from which the critical splitting stress t cr was
obtained by t cr ~ st Bin X0 Cos X0 where X 0 is the
angle between 0001 and the specimen axis and Xo is the
angle between the specimen axis and the direction of slip.
Certain connections between the form of the extension
curves and the external shape of the deformed specimens
could be observed. Photographs of the extended specimens
are reproduced. The tabulated values of t cr determined.
under identical conditions on specimens cut from different
crystals agree moderately well considering that the
crystal orientation is not under control. The curves
Card2/4 for t cr as a function of T (temperature) for Zn are

SOV/70-3-1-10/26
The Dependence of the Critical Splitting Stress of Single Crystals
of Zinc on Temperature and Rate of Deformation
ASSOCIATION: Institut kristallografii AN SSSR (Institute of
SUBMITTED:
Crystallography of the Ac.Sc.USSR)
Januar7 5, 1957
Card 4/4

SOV/70-3-1-10/26
The Dependence of the Critical Splitting Stress of Single Crystals
of Zinc on TempErature and Rate of Deformation
sigqficantly different to those for Cd. For Cd above
500 C t or is independent of T but for Zn at the
higher temperatures t cr decreases faster and faster.
Bi shows the same type of behaviour as Cd. The influence
of the superficial oxide layer and sur4ace irregularities
on the yield stress of the specimens of the low-melting-
point metals studied by Schmidt and Boas, which were only
1 mm. in diameter, may be considerable. Bot only the limit
of flow of these specimens may be influenced but also there
may be some retardation on the formation of slip planes.
All these effects can be reduced by using large-diameter
specimens. Differences between the behaviour of the Zn and
Cd may be due to oxide films and supplementary experiments
are necessary to clarify the situation. The dependence
of t cr on velocity of deformation is substantially the
same f or Zn and Cd. There are 5 f igures, 3 tablea, and
Card3/4 3.references,-2 of which are Soviet-and 1 English.

HIGILI, VOR.; GOVORM DOBRZFIANSKIT, G.F.
Iffeet of the temperature and the rate of deformation on the
parameters of tension curves for silver chloride single crystals.
Opt.-mekh. promo 25 no*6:28-32 Je '58. (MMA 11:10)
(Crystallography) (Silver chloride)

AUTHORS:Regell, T. R Govorkc 4mulaw
TITLE: A Raster tecorUing Mic"rometer
SOV/120759-4-32/50
PERIODICAL: Fribory i tekhaika eksperimenta, 1959, Nr 41 PP 133-136
(USSR)
ABSTRACT: The authors describe a raster recording micrometer which
can be used to measuro displacements of up to 10 mm with a
precision of 0.1 IL. The action of a raster micrometer is
based on photoelectric measurement of a light beam passing
through a system of two rasters which can be moved with
respect to one another. The instrument is shown schemati-
4ally in Fig 1. A light beam from a small incandescent
lamp 1 passes through a condenser lens 2 , an optical
grey wedge 3 and falls on an inclined glass plate 4
This glass plate acts as a beam splitter. Some of the
light passes through -two rasters 5 and 6 and reaches
a measuring photo-element 7 . The rest of the light
passes through a second grey wedge 8 and reaches a compen-
sation photo-element 9 . By displacement of the wedge 3
it is possible to altez the initial light intensity Io of
the beam reaching the plat-e 4 . The compensation part of
the system, which consists of the wedge 8 and the photo-
Card 1/6 element 9 is used to establish the zero position of the

SOV/120-59-4-32/50
A Raster Recording Micrometer
galvanometer r' when the rasters are exactly aligned. Each
of the rasters is rigidly connected to one of the two points.
whose mutual displacement is to be measured. Fig 1 shows
the instrument when it is used to measure deformation of a
sample in creep tests. One of the rasters 5 is rigidly
connected to the upper part of the sample 10 , and the
second raster 6 is attached to the lower part of the sample.,
Fig 2 is a photograph of the raster micrometer as used in
micro-mechanical experiments (Fig 2a shows the micrometer
as a whole and Fig 26 shows the niarometer without the opt-
ical system). The rasters should be as light as possible,
especially when they are attached directly to a sample. This
is particularly important in measurements of deformation of
comparative4 weak, brittle or plastic --riaterials. The ras-
ters were prepared by V. F. Parvov in A. V. Shubnikov's
laboratory by photographing a system of white and black
bands (the latter were painted with Indian ink). The bands
were recorded either on a photographic plate or on a photo-
graphic film; the rasters made of films are lighter and more
Card 2/6
77777"IPI

SOV/120-59-4,-32/50
A Raster Recording Micrometer
suitable for micro-mechanical experiments. The raster dim-
ensions were 1.5 x 15 mm and the widths of the white and
black bands were the same (d = 0.1 mm). The sensitivity, (p
of a raster micrometer is j~iven by the number of the galva-
nometer scale divisions n per unit displacement of the
rasters; (P = dn/dx . For ideal rasters the relationship
between their mutual displacement and the photocurrent as
recorded by the galvanometer should be linear for displace-
ments smaller than the raster bandwidth d . Such a linear
dependence of n on x: for ideal rasters is shown in Fig 3a.
In this case the micrometer sensitivity is constant and equal
to (P =. CIO/d 9 i.e. the sensitivity is proportional to Io I
the intensity of the light bewa incident on the plate 4 and
it is inversely proportional to the raster bandwidth d .
The coefficient of proportionality c depends on the sensi-
tivity of the photo-elaments and the galvanometer. In the
micrometer constructed by the authors selenium photo-elements
SF-10 of ,v 500 ItA/lumen sensitivity were used. The p4oto-
current was recorded by means of a galvanometer of 10-'J A/mm
per metre sensitivity. To record the photocurrent the authors
used the appropriate part of a MiCrODhotometer MF-4 (there
Card 3/6

SOV/120-59-4-32/50
A Raster Recording Micrometer
were 1000 divisions on the scale of the galvanometer used in
MP-4). The sensitivity of the micrometer was then
(p = nmax/d =11000 divisions/mm, i.e. one scale division
corresponded to a displacement of 0.1 ~L . This figure refers
to the rasters in the fully open position (exact alignment)
and the conditions when a 2W lamp was used and the grey wedge
3 was only partly inserted. Higher sensitivity could be
obtained by removing the grey wedge 3 altogether. Still
higher sensitivity could be obtained by replacing the photo-
elements by photomulti,pliers and using d.c. amplifiers. The
above discussion of the micrometer sensitivity assumed that
the rasters are ideal. For real rasters the relationship be-
tween the photocurrent r- and the raster displacement x is
not linear. Fig 36 shows schematically the dependence of n
on x for real rasters. For real rasters we have a linear
portion AB , where (dn/dx) AB ~ const . The value of
(dn/dx) AB for a real caster io higher than for an ideal
Card 4/6
_2

'30V/120-59-4-32/50
A Raster Recording M4 crometer
0 _L
raster, i.e. the sensitivity of a micrometer with real raE;-
ters is higher in the AB. region than that of a micrometer
with ideal rasters. On the other hand, the sensitivity is
much lower in the regiOrLS from 0 to A and from B to
E where dn/dx is not constant. The interval A between
3 and E in Fig 39 is exaggerated. Fig 4 shows the depen-
dence of the photo-current on the raster displacement for a
real micrometer shown in Fig 2; the graph was obtained by
recording the photo-current by means of the appropriate part
of a micro-photometer Mr-4. Fig 4 shows that for this micro-
meter the value of & is r-.10.2d. The raster micrometer of
Fig 2 was tested in sevoral experiments. Fig 4a shows the
record of motion of the upper plunger of the micrometer dis-
placed at a uniform rate with respect to the lower plunger.
When the upper plunger was stopped the instrument recorded
a straight line parallel to the abscissa axis (Fig LIZ*) which
indicates that temperature variations in the room where the
experiment was carried out do not produce unstable displace-
ment of the rasters during periods of, say, 15 min. Fig 5
shows the re-ord of creep of plasticized polymethylmethaerylate.
Card 5/6

SOV/120-59-4-32/50
A Raster Recording Micrometer
Fig 6 shows the record of creep of the same material but
under the action of a smaller force. Acknowledgments are
made to A. V. Shubnikov who suggested the subject and ad-
vised on it, and to V. F. Parvov for preparation of the
rasters. There are 6 figures and 4 Soviet references.
ASSOCIATION: Institut kristallografii AN SSSR (Crystallography
institute, Academy of Sciences, USSR)
SUBMITTED: JulY l?, 1958.
Card 6/6

REGELIO V.R.; GOVOftMV, V.G.
Plastic deformation of zine utonocryotals under conditions
'forbidding baaai Plane BUppage. Part 1: Deformation curves.
Kristallograftia 4 no.6:8?EI-886 N-D 159. (MIRA 14:5)
1, Inatitut kristallograffl. AN WM.
(Zinc cryotaloo

24.7100 77112
sov/7o-4-6-i3/31
AUTHORS: Regell) V. R., Govorkov, V. G.
TITLE: Concerning Plastic Deformation of Zinc Monocrystals
With Orientations Eliminating Basal Slip. 1. Deforma-
tion Curves
PERIODICAL: Kri8tallograflya, 1959, Vol 4, Nr 6, pp 8,(8-886 (USSR)
ABSTRAM Variation of parameters of compression curves with the
change of temperature T and velocity of deformation
v was studied in crystals in which the axis is either
parallel to the basal plane ( )( = the angle formed
by the crystal axis with the bAdal plane- ~~ 00) or
perpendicular to It ( >, = the angle between the
crystal axis and direction of slip 1Z,,900). shearing
stress in the basal plane T for both orientations
equals zero (since -c = a' sin X cos >, , where 6
applied normal stress). Compression c~:,rves of the
crystals, grown by the method of Obreimov-Shubnikov (in
glass tubes, covered by a thin layer of carbon black)
Card 1/9 and prepared from pure Zn (99.98%) or from Zn + 0.1% Cd

Concerning Plastic Deformation of Zinc
Monocrystals With Orientations Eliminat-
ing Basal Slip. I. Deformation Curves
Card 2/9
77112
sov/7o-4-6-13/3i
and Zn + 0.5% Cd mixtures were obtained using apparatus
and methods described earlier C.Dubov, 0. A., Regell,
V R. Kristallografiya, 2, 6, 746-755, 1957; Regell,
V: R:, Berezhkova G. V Dubov, G. A., Zavodskaya Lab.,
1, 101-105, 1959 Y_. Re;hts for the crystals with
orientation X -60 are illustrated in Figs. 1, 2, 3,
and 5. Figures 3 and 5 show fmIl agreement of compre8-
sion data obtained by the authors with the empirical
equation derived from the results of tensile tests by
Gilman CGilman, J. J. Plastic Anisotropy of Zinc Mono-
crystals, J. Metals, 6, 10, 1326-1336, 1956] for crystals
with X -,, o0 -(at the temperature above 2500 C). The
value'for the activation energy Q (^,45 kcal/mole for
Zn + 0.1% Od) found by the authors compares favorably
with 46 kcal/mole found by Gilman and stay constant
for Zn-Cd mixtures up to Cd content of 0,5;. Qompres-
sion of crystals of the second series ( A -~ go') (see
Fig. 6) does not follow Gilman's equation even in the
narrow temperature range (300-11000 C) indicatIng

Concerning Plastic Deformation of Zinc
Monocrystals With Orientations Eliminat-
ing Basal Slip.7. Deformation Curves
IDA
7~
Au.S.
4 Oc

Lj
zoo'
400' ~
77112
sov/7o-4-6-i3/3i
0 2 1, 6 8 10 IZ E.%
Fig. 1. Compression curves for Zn + 0.1% Cd monocryptals
at various temperatures X ~~ 00): 6- stress, kg/mm!2;
Card 3/9 4F , compression,%.

77112, sov/7o-4-6-13/31
Card 4/9
0 4 a rz 166,%
Fig. 2. Compression curves for Zn + 0.1% Cd monocrystals
at vaFlous velocities of deformation cr, stress,
kg/mm ; ec compression, %; v ..' 4.5; 1. 12; v3
3.65-10-1 ; v 41 11.25-10-2 ; v6 2.2-10-~ v 8. 2.2-lo-3
mm/min.

Concerning Plastic Deformation of Zinc
Monocrystals With Orientations Eliminat-
ing Basal Slip. 1. Deformation Curves
196,
r
0~
77112
Soil/70-4-6-13/31
'a ZO ZZ Z4 26 M 30 32 34 36 Tb
Card 5/9
Fig. 3. Variation of yield limit with temperature
for Zn monocrystals. 6, Zn + 0.1% Cd; 0, Zn + 0.5% Cd
( )(~~ 00).

77112, SOV/70-4-6-i3/,2i
01

-3 -3
-4L
Fig. 5. Variation of log V T(With 1/T for Zn monocrystals
(&- t; 1) pure Zn, from the data cf
a~&) at constan
(reference is given in thetext belo4, (2) zn +
+ 0.1% Gd, from the data of Gilman; (3) Zn + 0.1% Cd;
Card 6/9- (4) Zn + 0.5% Cd.

77112, sov/7o-4-6-13/31
Card 7/9
9 Z 4 6 8 10 M 14 16 E.1Z
Fig. 6. Compression curves for Zn monocrystals at
various temperatures ( X -900): c , stress, kg/mm2;
v , compression, %.
a-, k*

Concerning Plastic Deformation of Zinc 77112
Monocrystals With Orientations Eliminat- SOV/70-4-6-13/31
ing Basal Slip. I. Deformation Curves
Card 8/9
nonconstancy of Q (at the same time, the value of Q
above 3500 C for Zn~crystals with X _-900 is much
higher than for the crystals withs~ -- 00). The
greater value of deformation resi ance found for
crystals with ~, -_ 900 at room temperature is explained
by the fact that orientation A z 900 eliminates not
only basal slip but also slip in the prism plane, which
takes place in crystals with X ~~O 0, and that deforma-
tIon In the former takes place by twinning and faulting
(slip in some other plane, e.g., pyramid plane, is also
possible). The authors point out that there exists a
a relationship between the mechanism of deformation and
the form of deformation curves (and the appearance of
deformed sample). The zigza s on the deformation
curves (below 3000) in Fig. 9, for example, indicate
reorientation of individual regions of the crystal
during twinning or faulting. However, detailed informa-
tion of the deformation mechanism can be obtained unly
by metallographic study of dislocations (already started

Concerning Plastic Deformation of Zinc 77112
Monocrystals With Orientations Eliminat- SOV/70-4-6-13/31
ing Basal Slip. 1. Deformation Curves
for the samples investigated in this work [Urusovskaya,
A. A., Stepanova, V . M., Kristallographiya (in the
-)] ). M. V Klassen-Neklyudova
process of printing,
articipated in discussions on this study. There are
figures; 2 tables; and 10 references, 9 Soviet, 1
U.S. The U.S. reference is: Gilman, J. J., J. Metals,
8, lo, 1326-1336, 1956.
ASSOCIATION: Institute of Crystallography qf the Academy of Sciences,
USSR (Institut Kristallografil AN SSSR)
SUBMITTED., June 6, 1959
Card 9/9

s/12o/Wooo/oi/o44/051
Elk
AUMORSi -Govorkov, V.G,, Zakatov, A.F. a a/Riffil, V.R.
TITLE: A Recording quipment for the Photographic Measurement
of Low Currentsill
PERIODICAL: Pribory i tekhbika eksperimenta, 1960, Nr 1,
PP 138 - 139 (USSR)
ABSTRACT: The recording equippent, type ZU-1, for the measurement
of currents in the ranze 10-9 to 10-6 A was developed
and constructed at the Institute of Crystallography of
the Ac.Sc., USSR. The operation of ZU-1 is based on the
6r'inciple of photo-electric measurement of the light
reflected from the mirror of a galvanometer. The optical
system of the device is illustrated in Figure 3; this
consists of: 1- a light source; 2 - a condenser lens;
3 - a calibrated scalel 4 - an objective lens;
5 - a galvanometer mirror; 6 - a prism; 7 a
photographic plate; 8 - a 'correcting lens; 9 a
mirror; 10 - a screen; 11 - a slot; 12 - a
diaphragm; 13 - a cylindrical lens. The intensity o
Cardl/2 the light falling onto the photo-sensitive layer is

S/l2o/6o/ooo/oi/o44/o5i
flqA/2~82
A Recording Equipment for the Photograph c ea urement of Low Currents
controlled'either by changing the diaphragm or by means
of an auto-transformer. The equipment is used for the
recording of the photo-currents produced by double
refraction (Ref 2), photo-electric-optical dynamometer
(Refs 1, 4) and other purposes. The authors thank
I.N. Zhokho_v and I.N. Tsigler for participation in the
development of the oquipment.
There are 3 figures and 4 Soviet references.
ASSOCIATION: Institut kristallografii AN SSSR (Institute of
Crystallography of the Ac.Sc., USSR)
SUBMITTEDt January 8, 1959
Card 2/2

REGILI, V.R.; GOVORKOV, V.G.; ZAKATOV, A.?.
Apparatus for mechanical tests of refractory materials. Zav.lab.
26 no.2:243-245 16o. (MIRA 13:5)
1. Institut kristallografit Akademli nauk SSSR.
(Refractory materials-Testine)

zJU98
S/181/61/003/005/003/042
B101/B214
AUTHORS; Govorkov, V. G. and Regal', V. R.
TITLE: Dependence of the parameters of the compression curves of
single crystals of gartcan:ium on temperature and rate of deforma-
tion
PERIODICAL: Fizika tverdogo tela, v. 3, no- 5~ 1961 , 1324-1330
TEXT: Up to now the plasticity of germanium has been tested predominantly
for shearing and stresa. The object of the present work was to supplement
these data by testing for compression at different temperatures and ratos of
deformation -,r. Samples of the form of parallelepiped 5A 2 x2 mm. are out out
from single crystals of gezmanium with principal axes along -..111>, ,
and -100>. The experimental apparatus i ,q described in Ref. 15: V- R-
Regell, V. G. Govorkov, A. F. Zakatuvy Zav. lab., 26, no. 2, 243-245, 1960.
Before the experiment the samples were heated for Thr at the temperature of
the experiment. The tests were made in oxygen-free dry argon at 2000000.
The rate v of relative deformation was varied between 10-1-2.4-10- sec-1.
Fig. 2 gives the results for Y 6.3.1()-4 sec-1. Below 4000C trittle
Card 1/7

23098
B/18 61/003/005/003/042
Dependence of the parameters B1 OIX214
destruction Get in without prior deformation. Between 400-7000C the curves
show a "peak of fluidity"., Thu rtoults depend only slightly on the orienta-
tion of the samples, The following experiments were, therefore, carried out
only with samples oriented towarde and at temperatures 500, 600, an&
7000C (Fig. 4). Reaulte ftra found which differ considerably from those of
V. R. Patel, B. H. Alexander (Acta Metallurg., A, no, 4, 385-395, 1956).
These authors found no "peak of fluidity". Graphioal determination of the
functions 1n v . f(c); In v - rf(lna)j In v - P(1/T) ahowed that the following
equation holds for the experimental data; v - Ban exp(-Q/Ty' (2). The
activation energy (Q - 47 kcal/mole) calculated by this formula agrees with
the values found from the ahearing. As is shown by Fig. 6, the peak of
fluidity is not reproduoible If the cumpression is repeated after release,
or if new loading is dono at. lower temparature. The peak is explained as
due to the aggravation of the deformation whose origin remains still obscure.
The irreversibility of the effect could be caused by small diffusion coef-
ficients and low concentration of the impurities, M. V. Klassen-Reklyudov
is thanked for advice and discussion. There are 6 figures, I table, anti
16 references: 2 Soviet-bloc and 14 non-Soviet-bloc. The 2 most important
references to English-language publications read as follows: J. Hornatra,
Card 2/7

23098
S/181~/61/COVOC5/003/042
Dependence of the.parameters ... BIOI/B2114
J. Phys..a. Chem. Sol., 5,.no. 1/2; 128-141, 1958; D. Dew-Hughea, G. E.
Brock, J. Appl. Phys., 30, no. 121 2020-2021, 1959.
ASSOCIATION: Institut kristallografii AN SSSR, Yoskva (Institute of
Crystallography AS USSR, Moscow)
SUBMITTED: November 25, 1960
Fig. 2: Compression curve of single crystals of germanium at different
temperatures with relative rate of deformation.v 6-3-10-4 cm-1.
Legend: a) orientat ion -.::.l 1 i.->