SCIENTIFIC ABSTRACT VERKHUNOV, V.M. - VERKLOV, B.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001859510017-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 1, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

I. Lobaohevskiy and Mechanics SOV/55-58-6-11/31
(8, T. 11 PP158-159)- Several similar quotations from this
work are given. He was the first to define space by the real
properties of physical bodies, and he connected time with
motion in space. He wrote: "The duration of the motion of a
body in space is called time". The causes of motion, the
"forces", are identical with present-day "impulses". Aboat
the attraction and repulsion of bodies be wrote, "when two
bodies approach each other, they at the same time attract
and repulse each other". In his lecturos, he dealt in detail
with the addition of forces. An outline of what he said in
this respect is given. In his work on "The Projection Theory
of Vectors" he raised the question as to whether the simple
way of dealing with the problem with the parallelograms of
forces in Euclidian space is sufficient In order to be able
to describe the addition of forces and motions. There are
24 references, 10 of which are Soviet.
ASSOCIATIONt Kafedra obshchey fiziki (chair for General Physics)
SUBMITTEDs February 26, 1958
Card 2/2

vrammHOVI-VOM.
N#1. Lobachevok-ii and mechanics. Vest.Mook.un.Seromateguakho,amtron.,
fiz.,khim. 13 no.6:77-89 158. (Kln 12:4)
1, lafedra obshchey fisiki Moskovskogo goeudarstvennogo universiteta.
(Lobachevskii, Nikolai Ivanovich, 1793-1856)
(Mechanics)

_~YXRKH(~JSHK ~1 ~~QkApe2ye h; SHIMOT, T.A., red.; BRUMMM. A.I..
!vicb
red.itd-va; XMS(ff, I.K., tekhn.red,
[Technical norms for manufacturing metalware) Tekhnichaskoe
normirovanie metiznogo proinvodstva. Moskva. Goe.usuchno-tekhn.
izd-vo lit-ry po chernoi i tovetnoi metallurgil, ig6o. 141 p.
(miRA :L4:3)
(Ketalwork)

- - - -- SEM, N=KAYAj - - E.-- N. - - and VIMKWXINA., A
"Age-Linked Changes in the Functional Mobility (Lability) of the Vizual
Analyser."
Problemy Fiziologicheskoi optiki 7: 34-38, 1949.
Trans: OR

VERKII0111INA" A. 1. Cand. Blolog. Sei.
DisBertation: "The Electrical Sensitivity of the Lye and Variations in it
Due to Age, Time of Day and Certain Other iectors." Inst of' Neurology,
Acad Med Sci USSR, 14 9eb 47.
SO: Vechernypya Moskva, Feb, 1947 (Project #17836)

lj~c T, 'I ~, , A. _i .
.il-4.j~j-.. .. -
24302 A. 1. aon-ast-rr.,-~ iomcncrdya -f~mkt!:].onallnoy polvi zhl 35ti
(Labillnostli) analLzatora. Frob!3:-~- flzzlol. , T, ~~Ii,
Y)40xf S. '* 'S. - Eilbllio.-r: 7
~ ---
SO: Dotoids, 1,o- 32, 1949.

8(6), 14(6) SOV/143-56-11-10/16
AUTHORS: Gokhsteyn, D.P., Doctor of Technical Sciences, P~rofes-
sor, Verkhivker, G.P., Engineer, Gorode-tskiy, A.E.,
Engine--er-
TITLE: The Problem of Expanding Existing Power Plants
PERIODICAL: Izvestiya vys3hikh uchebnykh zavedeniy, Energetika,
1958, Nr 11, pp 71-78 (USSR)
ABSTRACT: The rapid increase of installed capacities in thermal
power plants during the sixth Five-Year Plan and during
the following years necessitates an expansion of the
existing high and medium pressure power plants. In
addition the construction of new power plants with in-
creased and super-high steam pressures ia required.
Steam superimposing (parovaya nadstroyka) and gas tur-
bine extension (gazoturbinnaya pristro-ka) may be used
for expanding existing thermal power plants. Under
"steam superimposing" the authors understand an addi-
tional cycle connected to the basic operation cycle
of a thermal power plant. The waste heat of this ad-
Card 1/6 ditional cycle is used for obtaining superheated, or,

The Problem of Expanding Existing Power Plants
Card 2/6
SOV/143-58-11-10/16
dry, saturated steam. It is assumed that the super-
heating of steam for the installation to be superim-
posed is achieved by the heat of the fuel. The "gas
turbine extension" means the connection of an addition-
al cycle during which a considerable amount of the
heat, used for obtaining dry, saturated steam, and the
heat, required for superheatingp are provided by the
fuel. Figures 1 to 3 are graphic representations of
these additional cycles. These diagraxis show that any
steam superimposing leads to an efficiency increase
which is also confirmed by three equations which are
used for determiningT 'f. The power limitation of gas
turbine will create some difficulties when combining
the latter with steam turbines. The authors then in-
vestigate in somewhat more detail various possible
power plant reconstruction. systems taking into con-
sideration locally available fuel. In case only solid
fuels are available, steam superimposing or gas tur-
bine extension with a closed cycle may be used. The
authors consider the reconstruction of two turbine

SOV/143-58-11-10/16
The Problem of Expanding Existing Power Plants
types: VK-100-2 (90oatmospheres, 480 0C) and AK-50
(29 atmospheres, 400 C). By comparison and thermo-
dynamic analysis the authors arrive at the conclusion
that an initial steam pressure increase above 300-350
atmospheres will not provide a noticeable fuel saving.
In this connection, the upper steam superimposing
parameters are indicated with 300 atmospheres and 6500
C, corresponding to the initial parameters of the
SKK-300 turbine. Considerable results are achieved
when superimposing the 29 atmosphere unit, since here,
intermediate superheSting and a feed water temperature
increases to 280-300 0 may be used. The gas turbine
extension is justified only in case the cost per in-
stalled kilowatt is lower than that of steam superim-
posing, i.e. when the excess in fuel consunption is
justified by lower amortization costs. The authors
then consider power plants at which gas and coal are
available as fuels. In this case, beside the steam
superimposing an open-cycle gas turbine may be used,
Card 3/6 using the arrangement shown in figure 7. Such a gas

SOV/143-58-11-.10/16
The Problem of Expanding Existing Power Plants
turbine cycle was suggested b Professor- Ya.I. Shnee
D
and Engineer A.A. K"atkin ~R_Yef 17. With this system,
u
it is possible using solid uel in the Eiteam boiler.
The efficiency of such a combine unit with a VK-100-2
turbine is 36.7% at a superimposing power of 58,000
kilowatts. For reducing the heater surface and in-
creasing the possible unit power of the gas turbine,
a semi-closed cycle may be suggested, as shown in
figure 8. The power of such unit will exiount to
40,700 kilowatts, having a somewhat lower efficiency
(35.6%) than the aforementioned unit. Eowever, the
regenerator and water-gas heater surfaces are reduced
by 30-40%. The gas turbine 11ant consists of one
main turbine and auxiliary gas turbines, driving axial
compressors and electric generators. Finally, the
authors consider power plants using only liquid or
gaseous fuels. In this case the open cycle gas tur-
bine unit may be used which will be more economical
when using a VK-100-2 turbine than the steam super-
Card 4/6 imposing with steam parameters of 300 atmospheres and

The Problem of Expanding Existing Power Plants
SOV/143-58-11-10/16
6500C. The efficiency of such a system, working on
natura; gas (8533 Cal) with tin initial gas temperature
of 700 C, is 38.3% with the IM-100-2 turbine and -34.8%
with the AK-50 turbine. The authors compared the
various pcssible superimposing and eytension systems.
This comparison is shown in -table 1. The authors ar-
rive at the following conclusions: 1) From the thermo-
dynamic viewpoint, only such a gas turbine extension
will be more effective at which the in'ernal ret~,enera-
tion of the gas cycle is highly developed. 2) In a
number of cases, a gas turbine extension aill be more
profitable than steam superimposing of eXiSting pov;er
plants, provided liquid or gaseous fuel is available.
This pecularity is especially obvious vihen superim-
posing power plants wish initial steam parameters of
90 atmospheres and 480 C. 7') The lower the parameters
of the steam section of the existing power plant, the
relatively higher the superimposing of such power
plants aill be. The efficiE!ncy of superi:,-iposed po,.,ier
Card 5/6 plants having lo,;,,er steam parameters will exceed in

The Problem of Expanding Existing Power Plants
SOV/143-58-11-10/16
some cases also by absolute values the efficiency of
superimposed plants with higher steam parameters.
4) Using semi-closed gas turbine cycles for superim-
posing facilitates a considerable reduction of the
heater surfaces and dimensiona of units with a small
reduction of the profitableness. There are 2 dia-
grams, 6 graphs, 1 table and 2 Soviet references.
ASSOCIATION: Ode3skiy tekhnologicheskiy institut imeni I.V. Stalina
(Odessa Institute of Technology imeni I.V. Stalin)
Kafedra obshchey teplotekhniki (Chair of General Heat
Engineering)
SUBMITTED: June 24, 1958
Card 6/6

VIRKIN, A.
I--------
Withet respect of persons. Okh.trudA i nots.strakh. no-1:35-36
ja 6o. (MIRA 13:5)
1. Starshiy inzhener po takhnike bezopasmosti zavoda elektro-
schetchikov, gjillnyus.
(Works councils)

L 6
ACC Nib AP5025259 1JP 0 J1)/WH OURCE DE.:---
,WOJO/6~/dWlc~/oiM/0189 11 ---
CO
~e
'5A
AMMON Clickin
V. V.; RoMarray, V. P.; Verkdn, 13. 3okov, V. A.-
MG: Plwsicotechnical Institute of Low TeMpe atures, Acaderzv of Sciences llkrSSR~,t, I
(1;4_ziko-tekhnicheskiy ins
titut nizkikh temperature Aimd,!mi. rnmma 55
-Tl!rLE*,* Change in the.probability of the Mossbauer effect 6d -_-. n"9 Impurity nuclei in
the fer-roelectric phase transibion Inp
SOIAE: Zhurnal eksperimentallnoy i teoretic'heskoy fiziki. Pis1ma v redak-tolyu
(Pzilozhenive)p v. 2. no. 4, 1~65., l86-189
TOMC TAGS: Mossbauer effect, ferroelectric effect, phase transition, barium titanate
Awpurity- center,, -tin containing &U
AR3TRACT: This ~s Ocontinuation of earlier vork (FTT v. T, 1886, 1.965), where it was
assumed that the phase transition in solid solutions of the Ba(TIO.EiGnO.2)03 SYsteM isl
considerably spread out. In the preaent study, the authors have imestigated the pro- I
ba:bility of the Mossbauer effect on Sn'19 Impurity nuclei in the L
'a(TiO.99Sn0-01)03
system near the ferroelectric phase- transit ion temperature. The introducticn of so
smill an amount of tin impurity into barium tAanate dces not chango its ferroelectric;
properties noticeably, but at the same time maker. it pcssible to measure the resonance~_
absorption of 23.8-kev y quanta by the SnI29 impurity ruclei. The trampler, were pre-
pared by standard ceraMic technology, using tin oxide enriched with Sn'19 to 65.14?2.
The measurements were made with a setup In which the atsorber was cb-iven at constant
Card- V3

Fig. 1. Temperature dependence of the
relative Mosabauer effect probability
(1), dielectric constant (2), and
dielectric loss tangent for the system
Pal(Ti 0.99 Sn 0.01 )0 3*
fr IfTC
IC
4-- Z
273 -JZ I j7j r,- 4ZI
L Card

~-.-ACC-NM -AP5025259
--speed by meAnd of a mechanical cam drive. Me y-quantum -source-wax -rognealtm stannide
,qB mg1crx, Ahick, -14easarements'-iiere made of the temperature deperdence of the rela-
*,~i;ie Mossbauer- effect probability (1). of the dielectric constant (2). euid of the di-
electric loss tangent (3) for the system Ba(Tio.99Sno,oj)03 (Fig. 1). 7he relative
probability of the effect was determined from the ratlo of the areas of the absorption
cpectre. at the given temperature to the area of the spectrum at thk! Curie tempersture,l
the value of which (Tc - 390K) was chosen to correspond to the maxirwm of the dielec-
tric constant. It is seen from the figure that the relative Mossbauer-effect pro-
bability decreases quite sharply on approaching the Curie point from the paraelectric
region, passes through a minimum,and then begins to grow with decrease In temperature
in the usual manner. This singuleriV can be attributed to the temperature dependence
of the frequency of the anomaloua optical branch. A extparlson of the results with
earlier measurements (Bokov, Rcmanov, and Chekin, M *r. T, 1886, 1965) confirms the
previously advanced hypothesis that the phase transition In solid solutions of the
Be.( S system is considerab3i "smeared." Authors thank ProfessOr G. A.
SM1=;"5 ntinuou
1 s interest in the worky Candidate of Technical Sciences I. E.
N~ I I nikoiUl eparing the samples, and L. 1. Mzakev-lch for help idth the measure-
meats. Orig. art. has: I figure. T77
SM CODE: SS/ SUEH DATE: 21am65/ OHIG REF: 00,5/ OM MFj 002
AW

B. 1.
I,. C
kive like tvwmad! metals at frequencies sinaller thita 100
L yries th m I trun.). It was presuffievi that a min. qtukntum
ruff" with Pon,. m lot' cycles is necessary to excite the
"Vetal and that In light reflected or transmitted through a
thin film of a sulverrooductor a secand line sboult! toppew
liesitles the original line and displaced by a% - 0.7 klrm,
cut. l6fanocrystals opt Ifg and So we. grown hi jUss
tubes with flat %IA" windows. After rtinoval of the
Window good specuburly reflecting wdsces ovem obulned.
fly pladrit; the samples at I.M. between the poloo of an
eketymmstiet they coWd be made -perconotactive.
eith" the frequency as rutaturvol with a pabry-p4rot in.
N
I
1"fernmetef nor tbe izteft-~tv of the telloorit'l fir trans.
thittewl light sho"I any morlibcation during the transition
It-M "M Oate into the other. S. pakswror

PA 173T98
11~~16z Lov TO ,*eratUred- 21 -D-e-C -49 -------- ----- I-
"Magnetic PropertieB of Tin at Lov Tempera-
tures," B. 1. Verkin, B. 0. Lazarev, N. S.
Rudenko, Physicotech Inst, Acad Sci USSR, Kharkov
"Dok Ak Nauk sssR* vol Lxix, No 6, P.P 773-77
Subject studies at temp of liquid hydrogen and
helim show presence in tin of strongly ex-
pressed DeHaas-Van Alphen effects, studied by
measuring force-couple of crystal inwagnetic
field up to 12,000 oersteds. Submitted 31 Oct
49 by S. I. Vavilwr.
173T98

..b
d"awsm" 41 thA
=0 mmplm*
a I vFkW
MIZ-4kiij
and IN. IL Ro
$.Sj(.. Kkv). Zkor. Eksli.
cf. C-4. 41S. WIM.- 164 SAIMACIlk"46
11.4a* aski The de Haas-vam Alpbm dlects tZift 10 MnY
"WIJ& 011wr than IN, fly "zr*Aure%vbmio* of ow rmj,4~
m4l"S 4-H d VVrmAI Wnwskled in a Ismanelic firld. The Or
liass-vwn Alpbou elln't wAs lowid to In 4t I*id-11, tmp,,
AlldillSO. PNW;c vatialloaof the meartle maropff .blilly
witk the -enetic &M wits hirther ofmrvtd in Ik at 2).4,.
and much nWe strmWy at 16"Id-Ife temp.; in J"P
I Mf-4r4., thr owillation Perkwl nt the- suoreptRAIM" dd-
frfrjj(,e Altlim INI nersteds, and M) in a
deld. In Mg. the effect is obwryabit at 4.2 K. and I"-
"re'le'
with halber decremsing truip.; the *ocillatim
torriml, in lf;,Ofxl. and 14,000-o"Amd IkWo, is IW and AN),
U ilb In, the effort becocues obwrv" at abmt
7.,KPI' '" 1:1.14" Orr%tCdC With Cd, at 2'K- tk* OWRIAlin"
perkk I iii 12.0" 1 3nd 14,(X9 1 oersteds is 23 aml 40. rq,.
N. Thmi

USSRAbysics Viscosity Jun 50
Nitrogen
"Temperature Dependence of Viscosity of Liquefied
Nitrogen and Argon for Constant Density," B. I *
'Verkin, N. S. Rudenko, Physicotech Inst, Acad Sci
Ukrainian SSR
"Zhur Eksper i Teoret Fiz" Vol XX, No 6, PP 523-526
Visco.simeter for measurin~g viscosity of liquids and
gases,at constant density for wide range of tem;pera-
tures has been developed and constructed. Measures
viscositj~ of N2 and A between aoli=14c'ation point
163T90
4OW
USSR/Physics Viscosity (Contd) Jun 50
I-and 3000 K. Establishes complex relation between
their viscosities and temperature for constant*-den-
sity. Submitted 26 Dec 49.
im
163T-90

UM/Physics - Lov Temperatures Nov 50
*Magnetic Properties of Metals at Low Tem~era-
tures: I. The Periodic Variation of Cd, Be, Xg,,
Sn in Monocrystals' Magnetic Susceptibility in
Dependence Upon the Magnetic Field Strength,"
D. I. Verkino B. G. Lazarev, N. S. Rudento,
Physicotech Inst, Acad Sci Ukrainian SSR
"Ehur Eksper i Teoret Fiz" Vol XX, No 11,
PT 995-1010
Susceptibility varies periodically with field
strength at law temperatures, differing for
MW
169=2
USSR/Physics - Low Temperatures Nov 50
(Contd)
,different subject metals. This effect can be
characterized by definite parameters, differing
for varioua metals, which correspond to peculiar-
ities of crystallic structure. Submitted
30 Mar 50.
16W102

USSR/Physics - Crystals 1 Jul 50
Magnetic Properties
*Crystallographic knisotropy of the de Haas-van.
Alphen Effect)" B. I.Verkin, B. G.' Lazarev,
N. S. Rudenko, Physicotech Inst, Acad Sci U',:rain-
ian SSR, KharIkov
*Dok Ak Wauk SSSR" Vol T II, No ; PP 59-62
Studied anisotropy of magnetic properties in
Use plane of Zn and Be monocrystals at low
temperatures cf liquid H and He in field of
3,000 to 14,500 oersteds. Establisbed new
9;roperties of de Haas-van Alphen. Effect in
tbese metals. Graphs show couple acting on
VW 166T98
USSR/Physics - Crystals (Corxtd) 1 Jill 50
monocrystal versus angle between field vector
and one of binary axes of crystal. Submitted
3 May 50 by Acad S. I. Valrilov
166T9G

Roe"
Tech. 1n!4. Acwt. M. Ukr. $3,R.. KWhoys. Asp.
Lkjpd. Mwol. F"- It. cf. C.A. 45, 031M.-
In singiv rrymals of 8b. w,,lienlied wltb the 3rd-l, and further multiple zone ctystalliz&tion
guarantees a more effective removal of the impurities of this kind re-
maining in the ingot. The use of fractionized multiple zone crystalliza-
tion for the purification of chemically pure tin with initial value o~,,
F ~~ (1.4 4 1.6) x 10-3 has made it possible to obtain is metal with 6'=
2.7 x 10 A pubsequent 10-bour heating of this metal at 1DO(P and a
pressure o 10-0 mm mercury reduced the residual resistance to (2.0
2.1) x 10-k
Card : 1/1

VBBRI 11hysical Chadstry Liquids aud amorphous bodies# Cases B-6
Abs Jour : Referat 2hur Xhimiya: No h, 1957, 11069
Author : Bagrov N.N.., Verkin B.I. Dolgopoloy D.G.
Title : Determi=tion-6_fD_i?Mio'n Coefficient in Liquid by the Method of
Saturation from Gaseous Phase
Orig Pub : Zh. fiz. khimii, 1956, 30, No 2. 476-478
Abstract : Description of the method of determining diffusion coefficient in liquid by
saturating it with vapor of another-substance. There are proposed the forma-
las:
-,V- ~Y-77A X -t Ae )_7
2
'4 R/P - -ye, /M) f 11r (V rr ~Dt. /Z) 5":~ -1~4 (4 "Imeg-tE- I W/257 03
vherein 4. Q/4 is the relative increase in. weight of the liquid as a result
of diffusion, D --diffusion coefficieat., c --concentration of the saturated
solution of vapor in liquid, 1 --depth of the liquid layer, X sad a --mass
of the &tons of,solvent &M solute., t --time. Formula (1) related to the
instance 79-J2r>,Z-~ (long duration of experizient, or shallov depth of li-
quid layer), formula (2) to the instance The method consists
in plotting the experimental curve.4 Q/Q = f(111), deternining the tangent
Card 1/2

VERKIN, Boris Jyeremlyf~vich (Physioal-Tech Irl-St, Ass 11k.93R) w,arded
f
sci det.,ree of Doc Physic al-Miath Sci for 21 Jun 57 defense of disser-
C
tation: "Magnetic properties of vietals at low temperatures and the
problem of the energy spectrwra, of electrons in metals" at the Council,
Kharlkov State Univ imeni. Gortki; Prot No qP, 1" Feb 58.
(Bldvop 6-58120)

AUTHOR: VERKIN,B.I. PA - 2077
TITLE: On the Temperature Dependence of the Magnetic Susceptibility of
Elements. (K voprosu temperaturnoj zavisimosti magnitnoj bos-
priimevivosti elementov, Russian).
PERIODICAL: Zhurnal ENerimentaltnoi i Teoret.Fiziki, 1957, Vol 32, Nr 1,
pp 156-157 ~U-S-S-R-)
Receivedt 3 / 1957 Reviewed: 4 / 1957
ABSTRACT: The experimentally investigated magnetization of a substance is
composed of the diamagnetism and the paramagnetism of the atomic
trunk as well as of the paramagnetism of free charge carriers
(e.g. of the conductivity electrons in the case of metals). For
the following formula then applies:
the susceptibility of elements
-
+
+
+ ~
+ I
Y F
on
electr
exp ion
i alectr. Here - and +
denote the contributions made by diamagnetism and paramagnetism
respectively to the measured susceptibility.
The classification of magnetics, hitherto accepted is based on the
consideration of the signs of the susceptibility experimentally
measured. On the strength of the experimental data obtained for
the temperature dependence of the susceptibility of elements
another classification of magnetica can be suggested which is
based on consideration of the character of the temperature de-
pendence of susceptibility in weak magnetic fields. Four groups
Card 1/3

PA - 2077
On the Temperature Dependence of the Magnetic Susceptibility
of Elements.
of elements are here concerned: 1) A paramagnetism which is prac-
tically temperature-dependent (alkali and alkaline earth metals),
2) A temperature-dependent paramagnetism (rare earths,, transition
elements), 3) A temperature-dependent diamagnetism (Be,Mg,Zn,Cd,
Hg, Al,Ga,In,T1,C,Sn,Pb,A9,Sb IBi~, 4) A diamagnetism independent
of temperature (noble gases etc. . Mostly the character of the
temperature dependence of suoeptibility in each group is deter-
mined by the predominance of one of the components in the formu-
la given above. Thus e.g. the practically temperature-indepen-
dent paramagnetism is characterized by the predominance of the
paramagnetic contribution made by conductivity electrons.
Special attention has to be paid to the fact that the elements
of the aforementioned 4 groups take up a line in the so-called
long periodical system of elements. In all metals of the third
group the HAAS-VAN ALPVEN effect was observed at low tempera-
tures. At T > T 0 the existing theory describes
qualitatively the character of the temperature dependence of the
metals of the third group. Here T 0 denotes the degenAration
Card 2/3 temperature of a group with small amount (of electrons?).

PA - 2077
On the Temperature Dependence of the Magnetic Susceptibility
of Elements.
A systematical investigation of the temperature dependence of
the magnetic susceptibility of the metals of the third group
offers a further experimental possibility for -the study of the
energy spectrum of electrons in metals.
ASSOCIATION: Physical-Teohnical Institute of the Academy of Sciences of
the Ukrainian SSR
PRESENTED BY:
SUBMITTED:
AVAILABLE: Library of Congress
Card 3/3

AUTHOR
TITLE
PERIODICAL
DMITRE11KOt I.M., VERKIX~ B.I., LAZAREV, B.G. 56-7-53/66
The Influence Exe_rc1`-9-eCYyFrressure from all sides
upon the 11agnetic Properties of a Zinc Monocrystal at
low Temperatures.
(VliAte vaeatoronnego uzhatiya na magnitMye 3vcystva
monokristallov tsinka prinizkikh temperaturakh)-l
Zhurnal Eks erim. i Teoret..Fiziki 1957, Vol 33, Nr 7.
pp 287-289 MSR)
ABSTRACT At a temperature T - 4,20K of a magnetic fiwld H a 840003
a self made zinc monoogyatal was once exposed to a pres-
sure of P ^, 1500 kg/cm' which pressure was then lifted.
Taese conditions prevailing the our-yes fob the angular
denenden-le of the moment L which acts upon the crystal,
and the dependencie
for e 20 and 800 are given.
(With 2 Illustrai~
,ions and 5 Slavic references)
ASSOCIATION: Physical-Technical Institute of the Ukrainian Academy of
Sciencese (Fiziko-tekhnioheekiy inetitut Akademii nauk
Ukrainakdy SSR.)
PRESENTED BY:
SUBMITTED:
AVAILABLE: Library of Congress.
Card 1/1

SOV/137-59-12-26631
Translation from: Referativriyy zhurnal, Metallurgiya, 1959, Nr 12, p 124 (USSR)
AUTHORS: Aleksandrov, B.N., Verkin, B.I., Lazarev, B.G.
TITLE: Preparation of Pure Metals by the Method of Multiple Zonal-~ec
tion and the Use of Radigactive Tsotope ho Investigato the Mechanism of
Purifying the Metal From Admixtures by the Indicated Method
PERIODICAL: Tr. Sessii AS UkrSSR po mirn. ispollzovaniyu atomn. enorgii, Kiyev, AS
UkrSSR, 1958, PP 119 - 137
ABSTRACT: The authors analyze the methods of metal purifying by recrystallization,
and the equipment for multiple zonal melting developed at FTI of AS
UkrSSR; they discuss results obtained by investigating the mechanism
of the process (distribution of the admixture over the zone, non-
stability of the process, and deviations from the e ullib i with the
use of radioactive isotopes (snll3, zn65, AgIlO, FeY9 , TnIll It was
established that the design of an Instaalation with a ring-shaped crucible,
divided by a partition, proved convenient. In this installation the motion
of the ingot is performed by the continuous rotation at a required speed
Card 1/2 of a horizontal disk and the crucible. The authors describe a variant of
V/

SOV1137-59-12-26631
preparation of Pure Meta.1s by the Method of Multiple Zonal Recryatallization and the
Use of Radioactive Isotopes to Investigate the Mechanism of Purifying the Metal From
Admixtures by the Indicated Method
the installation for smelting easily-melted and low-malting substances (the latter
with a refrigerator) and of high-melting metals. An Installation for zonal melting
.by electronic bombardment is described. Information is also given on the posijible
preparation of an ingot with a constant concentration,.of the admixture aver the
length, on account of the circulation through the liquid zone of a metal with an
initial content of the admixture.
Yu.Sh.
Card 2/2

BOV/126-6-1-22/33
AUTHORS: Aleksandrov, B. N.I.Verkin, B. 1.1 Lifshits5 1, M, azd
Stepanova, G. I.
TITLE: On the Possible Causes of the Non-uniform Distribution
of Admixturce in a Crystallising Casting (K voprosu o
vozmozhnykh prichinakh neodnorodnop raspredeleniy_-
primesey v kristallizuyemom sl~tke)
PERIODICAL: Fizika Metallov i Metallovedoniye, 1958, Vol 6... lir 1.
pp 167-168 (USSR)
ABSTRACT: In a paper published in 1956 by the authors (Ref.1) the
mechanism was investigated of purifIcation. of metals
from admixtures by means of zonal recrystallisation,
There it was assumed that in front of the cryst-allisation
front the conditions are such that solidification of the
melt does not take place; in this paper the possible
consequences are mathematically analysed of the non-
validity of this assumption. Numerical evaluation for
the system lead-tin (about 1% tin) indicates that for
this system a periodic "blocking up" of admixtures in
the solid phase can be anticiiated. In
P _jj~d, exposures
obtained by contact radiograp."Ity of Pb-Sn castings
Card 1/2 showed a. large number of transverse bands corresponding

SOV/126-6-1-22/33
On the Possible Causes of the Non.-uniform Distribution of
Admixtures in a Crystallising Casting
to excess Sn admixture in these spots (Ref.1).
There is one Soviet reference.
AMOCIATION: Fiziko-tekhnicheskiy institut AN Ukr. SSR
(Institute for-Physics &nd T6chnblqV,&c.Sc. Ukr.,Ic',SR)
SUEMITTED: January 7, 195?
1. Metals--Purification 2. Metals--Crystallization
Card 2/2 3. Mathematics--Applications

AUTHORS: -.lc-kzardrov, 2. 'T., Vsr'-in,
T !T LE
.,~;th 057777 --- 37775-n E; 4. nn
'I'ha :-:LLe Patjj T,,
(D11na cvobodno.-o Prolbe-n olektronov v nlrve
PE'RIODICAL: Zhurnal eksne7irientallnoy i tec.r~:tich~~-c'---oj
Vol- 34, ITr 6, p~I. 1655-,.6,r--j (rszi)
ABSTRACT: The purification of t,--- tin admi~:(;uren control!,2d
: /P, of z7-ec--*.-
by measurin;_- the rcrianent ro~:i~:t-ncr-, !I?
roo-M
-,
mens ti.ken from vr.-ri6us re,-,ion~7 off n heito,! .:,d
bar. 7,
denot,,~s the r---.-iFitance of tho --pr-cin,~.,n at 4,2 K
412
- its resistance at room tci-.perature. A liagrar.
a nd R
room
shows the dependence of 6 on the diameter of' cylindric ~7ires
-
.10-5. - second diagr-m zihowc the de-
for tin with 6
= 1,8
CO
for p - 0, a denotes the conductivity of
pondence of a/cf
OD
- the conductivity of the massive metal,
the specimen, a
00
and p - the probLbility that the electron in --cattered elacti-
Card 1/2 cully. The best consistency between the experimental and theo-

The Free Path Length of Electrons in Tin of 1!ig~j 7urity SOV/56-34-6-47/51
retical data may be obtained fc)r the free path length
X = 0,65 mm- A table compares the dr-ta of thic pap2r -,--th
thooe of other authors. All t-P-2e data complately correspond
with the results obtained by investigating, t*ae anomalous skin
effect of tin. There are 2 tables and 11 references, 4 of
which are Soviet.
ASSOCIATION: Fiziko-tekhniche3kiy institut Akademii niAuk TTkrtlinskoy SSIR
(Physico-Technical Institute of thp A4UkrSSR)
SUBMITTED: March 26, 1958
Card 2/2

AUTHORS: Verkin, B. I., Dmitrenko, I.
----------
TITLE: The Influence of Uniaxial Elastic Deformationo on the tla'-rneti~~
Properties of Zink Crystals at Low Temperatures (V14.yP-n-Lye
odnoosnykh uprugikh deformatsiy na magnitnyye svoyotva
kristallov tsinka pri nizkikh temperaturakh)
PERIODICAL: Zhurnal eksperi-entallnoy i teoreticheskoy fiziLci, 1956,
Vol. 35, 1Tr 1.9 pp. 291 - 293 (USSR)
ABSTRACT: It was of great interest to investij:ate the influence of
the uniaxial elistic deformations of a lattice on the
Haas (Gaaz) - Van Alfv'en (van AlIfen) effect in zink
crystals in order to obtain a relation between the varLation.
of the number of the charJes in a group with an anomalou3ly
low number, and the sign of the change of c/a. c/a denotes
the ratio of the crystal axes. A figure shows the apparatl;s
for the elastic uniaxial compression or expansion of zink
orystalu. First the aniooti,opy of the tri--q~netic
of a non-3train~d zinl, cryatal wau Invantli-ate(l. ThiL; rv~-
isotropy wa3 then measured for uniaxially expanded arid
uniaxially compressed crystals. Two diagrams demonstrate
Card 113 the results of the measurerients, i.e. the periods T of

The Influenne of Uniaxial Elastic Deformations on the SO'1/a6-3c--! 47/59
Magnetic Properties of Zink Crystals at Low Temperatures
the oscillations of the susceptibility (which are caused
by the "low-number group of the charges" (malochislennaya
gruppa. zaryadov) and the influence exercised by the uni-
axial elastic coAipression of the zink crystals on the form
of the curves The second diagram demonstrates
also the straight lines n(l/H) which determine the period
of the oscillations of the susceptibility Gf free and
compressed crystals. The uniaxial compression of zink
crystals in the interval 04~ 300 increases the period
of the susceptibility oscillation bY 4 - 51'fo. 0 aenotes
the angle between the field vector 2 and the principal
axis of the crystal. If 0 increases, the increase of the
oscillation period becomes slower. At 0 - 700 thin period
is not changed, and at 0 = 80* the oscillation period
decreases slightly (4W/T" 1~o). A uniaxial expansion of
zink crystals in the interval Q~~z 300 reduces the period
of the susceptibility oscillations by 2 - 'J~2. The amulitude
of the susceptibility oscillations is diminished several
times by a uniaxial elastic deformation of the cr.7stal. A
Card 2/3 decrease (increase) of C/a causes an increase (decrease)

The influence of Ela~;tic Dr&fcr.-.ations on
Magnetic Prop~rties of Zink Crystaln -~T AL :~w Ti-mperr-tUr;~S
ASSOCIATION:
SUBMITTED:
of the numbers of the char,~ez in the anom-ALwi.l. e
are 2 figures, 1 table, and 2 referencu- In r e:
Sovi e t
Fiziko-tekhnicheckty in2tittit Aj,~,-,de:nii n~ iiV Ilk v:i in E;?,.oy SSI~
(pjjysico-Technical lw~;tillute of the IS
Aprill 4, 1958
Card 3/3

o fthe ie I d Intensit yThe I o I I owin r r ca u 1t swere obtifnoA, ITU.
Ar

r)er~ J,
ter-i
C,r
nR

24 (2), 24 (3)
~'AUTHORS: Dmitrenko, 1. Y,.,, Verkin, B, I,, Sov/c6--35-2-4/60
Lazarev, B. G~
TITLE: The Magnetic Properties of Metals at Low
Temperatures IV (Idagnitnyye sv,Dyutva metallov pri
nizkikh temperaturakh IV), The Influence of Pressure
Brought to Bear From All Sides Upon the de Haas-van
Alphen Effect in Zinc Crystals (Vliyaniye vaestoronnego
szhatiya na effekt de Gaaza-van Allfemu kristallov tsinka)
PLRIODICAL: Zhurnal eksperimentallnoy 1 teoretilcheskoy fiziki, 1958,
Vol 35, TIr 2, PP 328-339 (USSR)
ABSTRACT: The present paper aims at contributing towards facilitating
research work concernin& the anisotropy of the magnetic
properties of crystals at low temperatures. Homogeneous
compression of samples (from all sides) was brought about
by applying the method developed by Lazarev et al. (Ref 10).
i. e~ by allowing water to freeze in a bomb. The bomb
consisted of pure beryllium bronze (made by I. Bolgov)-
Experimental ccnditions; Pressure P 1700 kg/cm2
Card 1 Magnetic field H 20 000 Oa

The Magnetic Properties of Metals at Low SOV/56-35-2-4/60
Temperatures IV. The Influence of Pressure Brought to
Bear From All Sides Upon the do Haas-van Alphen Effect in Zinc Crystals
Temperature Interval 1~6 - 4,2oK
The samples investigated consisted of spectrally pure zinc
supplied by the firm of Khillger, which was subjected to
different kinds of treatment;
Zn-.l: prepared according to reference 12. 7 times
recrystallized Xhillger-zinc.
Zn-2., Zn-3, Zn-4: (round) prepared in quartz shell
according to Obreimov-Shubnikov; velocity of growths
10, 15, 50 mm/hour,
Zn-7 (hexagonal) prepared by the method developed by Kapitsa,
growth; 5 mmlhourl
Pirst the de-Haas-van Alphen-effect in the free zinc crystals
is dealt with. The results obtained are shown by diagrams
(Figs 2 - 6) (Angle-dependence of oscillation periods of
magnetic susceptibility for the numerically smallest group
of mobile charZes for two different orientations of the
crystall de Haas-van Alphen-fine-Btructure effect for 3
different orientations; dependence of the oscillation
Card 2/4 moment Lz/H2 on orientation and temperature).. The foliowinC

The Magnetic Froperties of Metals at Low SOV/56~35-2-4/60
Temperatures IV.. The Influc-;_nce of Pressure Brought to
Bear From All Sides Upon the de 11aas--van Alphen Effect in Zinc Crystals
investigations were carried out under pressure-. The
dependence of the period and of the amplitude of the
oscillations for the smallest group of mobile charges in
the case of different orientation of the crystal. Por all
0 - values (angle between H and the main aXis of the
crystal) the periods of these oscillations increase by
40 - 48 '/L Homogeneow compreasion (from all sides) further
causes a considerable decrease of the oscillation amDl-.'tude
as well as a modification of its temperature-dependence
Experimental results are compared with the phenomenological
theory of the effects of oscillations in mezals- The author
thanks A. M, Kosevi:ih for discussing results, There are
7 figures, 3 tables, and 22 references, 15 of which are
Soviet,
ASSOCIATION: Fiziko-tekhnicheskiy institut Akademii nauk Ukrainskoy SSR
(Physico-Technical Institute )AS Ukrainskaya SSR)
Card 3/4

5 (0
AUTHORS: Manzheliy, V. G., Verkinj',B.,j.,., sov/76-33-8-13/39
TITLE: Investigation of the Diffusion Phenomena in Liquefied Gases
PERIODICAL: Zhurnal fizicheskoy khimii, 1959, Vol 33, Nr 8, PP 1758 - 1761
(USSR)
ABSTRACT: An investigation method, as well as the corresponding apparatus~
for the study of diffusion pheaomena in liquefied gases at low
temperatures were developed. The advantage of the method of the
gaseous phase applied (Refs 1-.~) in contrast with the capillary
method (Ref 5) lies in the fact that the former permits the
checking of the ocaurrence of a convection as well as the con-
tinuous recording of the diffusion coefficient as a function of
the concentration. The system methane (I)-propylene(II) was in-
vestigatedy since it possesses relatively simple molecules. The
test arrangement (Fig 1) contains a copper flask (250 cm3) in
which the pressure can be measured by means of a manometer and
read by means of a cathetometer. The flask is contained in a
Dewar vessel. The dependence of the diffusion coefficient of M
and on the concentration in the range of 0 - 27-5 mol4, at
II
)
9
as examined, and the results obtained were indicated
w
90.2
K
Card 1/2 (Table). The aggregate error in the determinations is given as

Investigation of the Diffusion Phenomena in Liquefied SOV/76-33-8-13/33
Gases
amounting to 61i4o at most. The authors thank V. A. PikovetB,
Ye. A. Seniko, and G. L. Shatrovskiy. There are 2 figures,
1 table, and 5 references, 4 of which are Soviet.
ASSOCIATION: Kharlkovskiy gosudarstvennyy universitet im. A. M. Gorlkogo
(Kharfkov State University imeni A. M. Gorll:iy)
SUBMITTED: January 17, 1958
Card 2/2

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24(2)924(3)
AUTHORS: Verkin, B. I., Dmitrenko, 1. M. SOY/20-124-3-17/0'7
,r__
TITLE: The Dependence of the Main Characteristics of the Effect of
Pres 'Zavisi-
de Haas-van Alphen, in Crystals of Zinc ou sure k
most' dsnovnykh kharakteristik effekta de Khaaza-van AlIfena u
kristallov tainka ot davleniya)
PERIODICAL: Doklady Akademii nauk SSSR, 1959, Vol 124, 11r 3, PP 557-558
(USSR)
ABSTRACT: The present paper discusses the experimental investigation of
the magnetic properties of zinc crystals at low temperatures
in a constant field and at various pressure values. The method
of investigating the anisotropy of the magnetic properties of
zinc crystals consisted as before in measuring the pair of
forces acting upon this crystal. In this case the crystal
was mounted in a high-pressure bomb which was magnetically iso-
tropic and which was suspended on a thin thread within a
homogeneous magnetic field. The magnetic properties of the
zinc crystals were investigated at the temperatures of 4.2,
14 and 200 K in the pressure interval 0 --- P 4 1,750 kg/CM2 and
Card I at field strengths H (. 20,000 oersted. The maximum pressure
J

The Dependence of the Main
Characteristics of the SOV/20-124-3-17/67
'
Effect of de Haas-van Al-phea in Crystals of Zinc m, Pressure
in the bombwas attained by means of frozen water at a constant
volume; for lower pressures aqueous solutions of ethyl alcohol
were used. The results obtained by the investigations are
shown in form of a diaGram. The dependence of the period of
the oscillations of susceptibility of pressure has a very
complicated periodic character, and the course taken by the
curves and also the relative pressure dependence of the
period in the case of the two values of e are practically
equal, Nere 9 denotes the angles between the crystallographical
axis of the zinc crystals in the bomb and the field vector. As
expected. the anisotropy of the magnetic properties of zinc-
crystals o.,cillates with pressure. at H - const, but this
effect is --endered very complicated by the geriodic dependence
of the period on pressure. However, not only the period, but
also the amplitude of oscillations depends non-monotonously
on pressure. These and other data given here lead to the dis-
covery of
two new characteristic features of the de Haas-
'
van A:Iphen effect: 1) The period of the oscillations of zinc
susceptibility depends periodically on presoure. 2) Whereas
Card 2 the period in the case of free zinc crystals at T < 20-40 K

The Dependence of the Main Characteristics of the SOV/20-124-7-17/67
Effect of de Haas-van AlPheil in Crystals of Zinc ca Pressure
does not depend on temperature, the period of the oscillations
of susceptibility of a crystal subjected to a pressure of
1,000 kg/CM2 increases considerably with rising temperature
(within the same temperature interval). These two particular
features cannot be explained by the present theory on the
de Haas-van Alfven effect. The experimental data determined by
the present paper may perhaps be explained by the attenuation
of the inequations kT