SCIENTIFIC ABSTRACT YAROSHENKO, YU.G. - YAROSHEVA, A.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001962210007-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 1, 2001
• Sequence Number: 7
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

YAROSHEM&,, Yu.G.,; LAZAREV, B.L.; OVCHINNIKGV., Yu.H.
Comipletion of heat t"fer procesoes in blast furnaces. Izv.
uckeb, zav.; chern. nk. 6 no.3:185-188 163. (KOU 16:570
1. Urallskiy politekhnicheskiy institut.
kBlast furnaces) (Heat-Tranamiosion)

M(1)/EWP(q)/EW(m)/BDS---AFFTC/ASDZ.-WH
L 11219-63
AC.CESSION IM; AP3000024 ..910131163100010051019910206
1-7
AMOR: Budr In, D. V.; _Suchkov, V. D.; Yaroshenko, Yu. G.
TIM: Rapid c~termination of the co t; and heat diffusivity in refrac-
tory material
BMCE., Ogneupory, no. 5p 1963, 199-2o6
TCPIC TAGS: refractories, thermal conductivity, heat diffusivity, magnesite, fire
clay, thermocouple
ABBITMACT: The authors propose a method,of using limiting conditions of a third
kind, more general than previously employed, in solving a differential Fourier
equation as a means of determining thermal properties. The technique for deter-
mining measured values,requires no observation of special conditions in setting up
the tests ' except the maintenance of uniformly symmetrical heating (and cooling) of
samples in an environment of constant temperature. Cylinders of magnesite, fire
clay, and foamy fireclay were used in the.experinnnts, and measurements were made
by reeans of Chromel-Alumel thermocouples with thermoelectrodes 0.2 mm in diameter,
connen.ted to an EPP-09 electronic potenticAneter. Errors in measured temperatures
did not exceed 2%. The method is simple and needs no special heating device. It
can be used in any plant laboratory and permits determination of tbnrmal properties
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lWF 7~~7i~f
-F kAt

BRATCHIKOV, S.G.; BAZILEVIGH, S.V.; YAROSHENKO, Yu.G.; MAYZELI, G.M.
Analysis of heat-exchanging processes during sintering by the
filtration method. Izv. vys. ucheb. zav.; chern. met. 6 no.6:
18-26 .163. (KRA 16: 8)
1. Ural'skiy politekhnicheskiy i'nstitut.
(Sintering) (ifeat-TranBmission)

BRATCHIKOV, S.G.; DAZILEVICII, S.V.; YAROSIIENKO, Yu.G.; MAYZELI, G.M.
Calculating temperatures during the sinte-ring pro-cess. Izv.
vys. ucheb. zav,; chern. met. 6 no.8:47-53 163. (MIRA 16:11)
1. Ural'skiy politekhnicheskiy institut.

Y k I K I L~ Y F, IBI L A Z, A TCE VPL 11 ~114 0
Stah-12izirxg hea'l'- txriditiona of a blast fuxma~e b~,, inJecting
ths fuel through the tuyar,,,~sd Izv,VY5.-ucheb.zav.~ chern.met. 8
r1j.6227-32 165- (MIRA 18:8)
1. Urallakly poiltekhaicheskiLy ipntitut.

KITAYFV B. I.; YAROSIIENKO Yu r.- LAZAREV, fu.; SUKHANOV, Ye.L.
Quantitative eat'-mate of heat conditions at a blast furnace
top. Izv. vys. ucheb. zav.; chern. met. 8 no.1001-305 '65-
(ICRA 1839)
I. Urallskiy politekhnicheskiy instit-a'".

I 8~65c~
13,,; 7ilO 5/520/59/000/022/019/021
-2 / 2,0 E073/E535
AUTHORS-, Vdovin, Yu. A and Yaroshenko, Yu.N.
TITLE& On the Sheet by S~eet Nnuniformity of the Magnetic
Properties of Cold Rolled Electrical Steel
PERIODICALt Akademiya nauk SSSR. Urallskiy filial, Sverdlovsk.
Institut fizikl metallov~ Trudy, no.22, 1959,PP-137-142
TEXTa Experimental results are available on the sheet by
sheet nonuniformities of the magnetic properties of hot rolled
dynamo and transformer sheet. However, such data are not available
on cold rolled sheet. This paper contAins some data on the variation
of these properties in cold rolled 0.35 mill thick and 0.50 mm thick
transformer sheeis. The data were obtaLned by means of Epstein
apparatus. For detailed study of the nonuniformity of the
induction of cold rolled transformer steel, sheets 1500 x 240 x
Oo35 mm were investigated by means of simple apparatus, the basic
circuit of which is shown in Fig.l. It consists of plywood frames:-
placed on top of each other, 1400 mm long with windows of
20 x. 260 mm. A metering coil of 600 turns is mounted on the
central part (3/5ths of the length) of each frame. The magnetiza-
tion winding surrounds both frames and has 522 turns, which are
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S/520/59/000/022/019/021
E073/E535
on the Sheet by Sheet Nonuniformity of the Magnetic Properties of
Cold Rolled Electrical steel
distributed longitudinally as followS3
Number of 89 44 4-5 41 42 42 41 45 44 89 Total
turns 522
Length of 14 14 14 14 14 14 14 14 14 14 Total
the sectian 140
(cm)
The resulting longitudinal distribution of the induction in a pair
of equal sheets placed into the solenoid is plotted in Fig.2.
The indicating instrument is a magnetoelectric one, which is series
connected with a half-wave controlled bridge rectifier made up of
equal cuprous-oxide elements. The instrument is shunted with a
smoothing condenser and with a resistance for the purpose of
adjusting the sensitivity. The indicator coils are connected in a
differential circuits The control voltage is obtained from a
supplementary win ding with 80 turns, which are wound on a central
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E073/E535
I.On the Sheet by Sheet Nonuniformity of the Magnetic Properties of
Cold Rolled Electri*cal Steel
ipart.of the solenoid; the control voltage is several times the
value of the e.m.f. difference in the metering windings, as a
result of which the rectifier circuit is piactically blocked for a
half-cycle of the control voltage, whilst during the other half-
cycle it shows only a low resistance to the current flow in the
:metering coils, regardless of the direction of the current (this
lis necessary for ensuring an unequivocal relation between the
-;readings of the measuring instrument and the difference in the
amplitudes of the induction in the "standard" and the tested sheet
'The instrument Is fed from'a.c. mains via an autotransformer. The
J
Imagnetization winding is fed with a voltage of 45 V, thus obtaining,
:a field amplitude of 15 Oe, which corresponds to a point on the
~magnetization curve beyond the bend, on a relatively "flat" section:
Iso that fluctuations in the mains supply voltage will not seriously.-
~influence the relation between the induction amplitudes in the
'tested sheet and in the sheet used as a standard. By means of
this instrument two batches of cold rolled-steel were sorted out
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E073/E535
:On the Sheet by Sheet Nonuniformity of the Magnetic Properties of
Rolled Electrical Steel
;which, as regards induction, were.rejects from ordinary tests.
~The results obtained by the Epstein method for 0-35 mm sheet before
after sorting on the basis of induction values were*as follows:
Table 4.
Batch Type of specimen P P B B
10 15 25 30
1 Shop specimen o.81 2.07 16620 176oo
Specimen after scrapping 0.74 1,76 1721b 18130
2 Shop specimen o.82 1.84 1694o 17850
Specimen after scrapping 0.83 1.95 17180 18010
..Specimen from the better
sheets 0,-7 1.52 18920 19500
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89656
S/520/59/000/022/019/021
E073/E535
On the Sheet by Sheet Nonuniformity of the Magnetic Properties of
Cold Rolled Electrical Steel
The distribution of the 0.35 mm sheets of individual batches sor ed
on the basis of the B values was as followsa 11
25 Table_5
Batch Grade, % Satisfactory,% Rejects,%
~~330 4320 )310
(E330) (E320) (E310)
1 12 14 35 61 39
2 39 35. 15 ~89 11
Thus, it was found that the nonuniformity within individual batches
of cold rolled transformer sheet is very considerable and, therefore,..
the properties of standard specimens chosen arbitrarily may deviate
considerably from the average properties of the batch. A real
increase in the testing accuracy can be achieved only by increasing
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On the Sheet by Sheet Nonuniformity of tile Magnetic Properties of
Cold Rolled Electx*.cal Steel
.very considerably the number of sheets tested within each batch.
It is recommended that this can be done by means of the instrument
described in this paper-, using as a criterion the induction Blpy or
B2~ since the quantity of sheets scrapped due to unsatisfhcto
lo s values is only a fraction of that scrapped due to unsatisfactory
induction. It would be advisable to combine the system of
preliminary sorting of sheets on the basis of induction with
subsequent more accurate evaluation of each batch by means of
apparatus which permits obtaining absolute values. The work
described in tile paper was directed by R,, I., Yanus, There are
3 figures, 5 tables and 4 reforences2 2 Soviet and 2 non-Soviet.
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~ EWVE535

!On the Sheet by Sheet Nonuniformity of the Magnetic Properties of
!Cold Rolled'Electrical Steel
Fig.1 Fig.'2

MAO"

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S/133/60/000/008/011/013
AUTHORS. Belyakov, A. 1. and Yaroshenko, Yu. N.
TITLEt Relation Between the Magnetic Induction of Cold-Rolled
Transformer Steel and the Conditions of Final Annealing
~6
PERIODICAL: Stall, 19609 No. 8, PP- 750-752
_a~ali~n'of cold-rolled transformer
TEXT: The effect of final anne i
steel in vacuum on magnetic induction in weak and medium fields is not
sufficiently clear. Many steels with high induction capacity in strong
fields display relatively low induction in weak and medium fields. In
order to investigate this problem, tests were carried out with three
kinds of steelsz 6260 (SiO-16%), 6247 (Si:3.23%) and 6230 (SiO-10%)-
Until a 0-35 mm thickness of the sheet was obtained the technological
process took place according to the conventional methods. Final anneal-
ing was carried out in vacuum electric furnaces up oto 1,1500C for 30
hours. The.metal was cooled by the furnace to 600 C, after removing the
hood cooling was continued to 2500C under a muffle in a protecting gas
medium. Test specimens (0.35 x 30 x 250 mm; 1 kg) were made of all
three types of steel, the magnetic properties were determined by the
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S/133/60/000/008/011/013
Relation Between the Magnetic Induction of Cold-Rolled Transformer Steel
and the Conditions of Final Annealing
Epshteyn ballistic method before and after the additional annealing which
was the main feature of the new process. Type 6260 was cooled by the
furnace between 6000C and 4500C to.various degrees and the types 6247
and 6230 were tested in 6 charges, three of which were cooled by the furnace
to 6000C and three to 4500C- The results obtained with the 6260 type
specimens showed that in proportion to the decrease of the temperature,
at which the hood is removed, the magnetic properties in weak and medium
fields improve; magnetic induction B 0 M increases from 1.25 to 1.62
gauss, B0.008 from 10.11 to 25.10 gau;s Fig. 1A) and B Ifrom 12,680 to
14,650 gauss; the coercive force H increases from 0.18 to 0.13 oersted,
maximum magnetic permeability/.z., from 18,280 to 36,380 gs/oersted
max
Fig. 2),q the plasticity of the metal increases from 2.7 to 18 bendings.
This change in the magnetic and plastic properties can be explained by
a more thorough distribution of the internal stresses upon the removal
of the hood at a lower temperature with a corresponding re-distribution
of the admixtiires (Ref. ~). With additional annealing of the specimens
at 7500C, in order to eliminate work hardening due to cutting, the
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Relation Between the Magnetic Induction of Cold-Rolled Transformer Steel
and the Conditions of Final.Annealing
improvement of magnetic properties can be maintained. The results obtained
with specimens of 6247 and 6230 type steels agree with the results of the
6260 type specimens. Generally, it was found that after the additional
annealing of specimens to eliminate the work hardening due to cutting,
the yield of products complying with F'OCT (GOST) 802-58 increased from
40% (in the conventional cooling by furnace to 6000C) to 80%, when cooling
with the furnace to 4500C. There are 2 figures, 2 tables and 2 Soviet
references.
ASSOCIATION:. Novosibirskiy metallurgicheskiy zavod (Novosibirsk Metallur-
gical Plant)
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S/1 10/61/000/001/012/0-2-3---l
E073/E455
AUTHORS: Vdovin, Yu.A., Engineer and Yaroshenko, Yu.N., Engineerl
TITLE, ___oT ~-Rolle
Experience Gained in Sorting d f~Llectrical io
Steels According to Their Magnetic Properties
PERIODICAL: Vestnik elektropromyshlennosti, 1961P-No.1, pp.38-4i
TEXT: For a detailed study of the nonuniformities of magnetic
induction in cold-rolled transformer sheets of 1500 x 240 x 0.35 mm,
the authors used tho circuit shown in Fig.l. Two 1400 mm frames
1 with windows of 20 x 260 mm are placed on top of each other*
A 600-iturn metering coils, El and 't2 are differentially series-
connecte'd and feed into the indicator loop consisting of a
capacitance-shunted microammeter and a phase-controlled'half-wave 20
rectifier system. The driving voltage for.the loop is fed to the
rectifiers from an 80-turn winding L2 which surrounds both frames~ .
The magnetization winding Ll has 522 turns and is distributed
nonuniformly along the length of the solenoid for the purpose of
obtaining a more uniform magnetization (variance below 10%). One
of the frames carri#a a standard specimen, and.the other carries
J.the sheets to be tested. The system is fed from the maiiis
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'455
E073/E
Experience Gained in Sorting Cold-Rolled Electrical Steel#
%jAccording to Their Magnetic Properties.
throughan autotransformer giving 45V on the magnetiz'a'tion kiinding.
The maximum field strength is about 15 oersteds. 'Thus it is
lbeyond.the bend point and on the flat section of the-magnetization
curve, where even the highest voltage fluctuations cannot change
igreatly the maximum induction. The indications of the metering
~instrumenta are proportional to the differences in the maximum
iinductions of the reference specimen and the tested sheets. By
means of this apparatus, several batches of cold-rolled steel were
..,tested. The average B values corresponding to the B25 and the
~mean square of the variance 02 as'well as the integral
idistribution function WB = NBIN were determined for each batch
(N = total number of sheets and NB = number of sheets for which
B25 is lower than B). The distribution function WB proved near!
:to the Gauss distribution law. Sorting results are given,for
.,.a number of batches. Fig.3 given the normal distribution of the
IB2!; values for batches of cold rolled steel; the circles denote
I I
Ameasured values, the curve is-the calculated Gauss distribution
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Experience Gained in Sorting Cold-Rolled Electrical Steels
According to Their Magnetic Properties
curve, It was found that the properties varied considerably inside,
the individual cold-rolled batches. It was also apparent that
tests by the Epstein square give only very approximate indications
of the properties of the batch. Even in scrapped batches, the
number of sheets that eventually proved satisfactory was over 50%.
It is necessary to increase very appreciably the number of sheets
tested. However, it in sufficient to limit a test to measuring a
.single quantity, for instance B25 The following conclusions area
arrived at: 1) Individual 'sheets of cold-rolled electrical steel
differ considerably in their magnetic properties. no
2) The induction B25 is one of 'the most reliable guides of the
quality of cold-rolled electrical steel. Therefore, it should be
used as a basis for quality control in mass production.
3)
~quare,_there
Before testing on the Epstein
should be a
preliminary sorting into several groups on the basis of results
obtained on whole sheets'with the author's instrument. The
proportion to be tested on the Epstein square is thereby reduced,
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E073/9455
Experience Gained in Sorting Cold-Rolled Electrical Steels
According to Their Magnetic Properties

so that more gener ous sample s may be taken, thus giving closer
supervision of the magnetic properties inside each'batch. There
are 3 figures and 4 tables.
SUBMITTED: June 21, 1960
J~' 0

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Y

31058.
5/126/bl/012/004/020/021
0 E073/E535
AUTHOWI: Ounayev, F.N. and Yaraslienko-, Yu.N.
,rrru,; volume magnetoAtriction in iron-si
con alloys
PKI? 101) ICAL: Fizika inetallov I metal lovedenlye, V.12, no.4, l.9.61,
620-b22
TEXT: According to the theory of It. Becker (Ref.1i 'Zo.Phys.,
1.933, 87, 5147) volume magnetortriction in the sum total of thre
different phenomena: 1) the inflijence of the demagnetizing effe:t
of the ends of a Verromagnetic on its volume; 2) a change In,
volume 'occurring during turning of the magnetization v*ector in
the crystal Inttice; 3) a change in volijme caused by the magnetiza-
tion. I.nvestigation of volume magnetostriction ii% like.ly to yield
useful information on the magnetic and the volume interactions in
ferromagnetics. The authors of thla paper investigated'the
volume magnetostriction on iron-silicon specimens in the form of
rotation elli-psoids. Four specimenq were tined, the chemical
compositions and the geometrical cliaracteristics of which are
gJven. The silicon content in these alloys varied between 1-05
and 4. IW4. The iapproximate nhape of the ellipsoid was:
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31058
Volume isiagnet.ostriction ... s/1'26/6J/012/004/020/021
E073/E535
3
major axis, a = 150 mm, minor axis, b -t 9. '35 mm, volume = 2280 mm
ALI the apecimens were heat-treated in vacutirli at 10000C for two
hours and, followitig that, cooled at a rate of' 100"C/hour. The
change in the volume magnetostriction wits by tile dilatometrIc
met-hod. The mpecimen was sealed int-o a- container with a capillary
which was filled with distilled water From which the air bubbles
were removed hy boiling Vor a long time. 'fo ensure isothermal
conditions, th"e container was placed in a (fewar vessel which in
turn was placed inl.o a magnetizing iolenoid capithle of producing
fteldn of up to 6000 Oe, the unirormity of' which-was maintained
throxighout the specifffen with an accuracy of tip to 2%. Th e
displacement of tile meniscus in the capillary was measured by
mersoog a microscope. The sensitivity of the equipment was
4. -1 - and the relative error or mcasurement of' -the volume
magnetostriction was'about T"'. The results, which are plotted in
the pap~er, show that I**rom a field z4t-renith of 1000 Oe onwards up
to 5700 Oe the dependence of W . on ~H is linear, i.e. tho
volume mngnetostri ct ion in this t -t~, t tPi L ields I m due to the Para-
process. The inclinat ion of' tile sLraighl. I ine .9ection.-4 of tile
curveA increases with increasing content of silicon in the alloy:
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3L 058
Volume magnetostriction ... s/j26/61/012/004/020/021
E073/EI35
dw/dH increases from 7.3-10- 10 for a silicon content of 1.05% to
9.8-10- 10 for a silicon content of 1#..10*)(. The results also show
that the initial section of the curves,..vhich is usually
attributed to the form effect, differs considerably for alloys
with various silicon contents Ailihqigh blfetipitlmona-.are*i~-
of the name shape. With increasing silicon content
curves at the initial range of field strengths are lower and for
specimens with 3-40 and 4.M, silicon the volume magnetostriction
has negative values in the field range 0 to 500 Oe. This phenome-
non cannot be expl.nined solely by sAturation magnetization and
elasticity moduli and apparently the voltime magnetostriction tn
this range of fields is due to a considerAblG extent to processes
of technical magnetization. 'there are I figiore, I table and
11 references% 6 Soviet-bloc and 5 non-Soviet-bloc. Tho English-
language references r1ead as followst llef.l: Gersdorf It. J.Appl.
Phys., 1959, 30, 2018; Ref.4t Gersdorf It. Physics,1960, 26, .5531
Ref."51 Stausis H.J!". J.Appl.Phyx., i9!;9, 30, 098.
ASSOCIATION: Ural'skiy gosudarstvennyy univeraltet im.A.M.Gor1kogo
(Ural State University imeni A.M.Gorlkly)
SUBMITTED: April 21, 1961
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.......... .........
NEFEDOV, A.A.; BELYAKOV,, A.I.; YAROBHENKO, Yu,No; DUKHNOVA, Z.I.
High-alloy., cold rolled, electrical steel with low anisotropy.
Stall 22 no./+:349-351 AP 162. OMIRA 15:5)
I* TSentra Inyy naachno-isaledovateliskiy institut chernoy
metallurgii i Novosibirskiy metallurgicheskiy zavod.
(Sheet steel) (Anisotropy)

NEFEDOV, A.A.,, inzh.; BELYAKOV,, A.I., inzh.; YAROSHENKO Yu.N.4 inzh.;
DUKHNPVA, Z.I., Inzh,
Cold-rolled 1 m. thick electrical steel. Elektrichestvo
no.ls75-77 A 163. (NIRA l6t2)
(Steel-Electric properties)

NEFEDOV, A.A., inoh.; BELYAKOV, A.I., inzh.;_XMOPHENK,O,,. Yu..,11., inzh,;
DUKHHOVAI M., inzh.
Cold-rolled o.35 mm thick generator steel. Elektrichestvo no.8;
70-72 Ag 163. (KRA 16:10)
1. TSentralInyy nauchno-issledovatellskiy institut chernoy
metallurgii (for Nefedov). 2. Novosibirskiy metallurgicheskiy
zavod (for all except Nefedov).

GRIGORIYEVA, V.I., prof.; KRAYCHIK, V.R.; SHULITS~ V.A.; YAROSHETSKAYA, B.S.
Outpatient service to glaucoma patients. Trudy LPMI 31 no.2:40-47 163.
(MIRA 17:10)
1. 17, kafedry- glaznykh bolezney Leningradskogo pediatricbeskogc medfm.
Awln#b"o tnatituta i glaznogo otdolenlya Ob"yedinennoy bollnitst-Imeni
-;~;:.eva, Leningrad.

YAROSHETSKAYA N.A.
Clinical observations cn the treatmont of syphilis with
bicillin-4. Vest. derm-1 ven. no.l.*62-65 '65.
(MIRA 18ilO)
1. Kozhnaya klinika (;,av.- prof. A.A. Akovbyan) Tashkenlu-skogo
maditsin"kogo institute.

8(6), 14(6) SOVI 112-59 -4-6726
Translation from: Referativnyy zhurnal. Elektrotekhnika, 1959, Nr 4, p 47 (USSR)
AUTHOR: jaL2,hey,, I. F.
TITLE: Joining the Earth Dam of the Pavlovsk* Hydroelectric Station With Itc-
Foundation
PERIODICAL: Tr. N.--;. sektora Mosk. fil. in-ta "Orgenergostro7," 1957, Nr 1,
pp 7-Z4
ABSTRACT: The blueprint of the hydraulic -fill -and - core dam of the Pavlov3k*
hydroelectric station envisages a counter-seepage system in the foundation.
The system con3ists of a concrete wedge, that cuts through the latest alluvium
and the upper disintegrated limestone layer, and a deep cement curtain wall.
Extensive actual exploratiors of the permeability of the dam-foundation rock
have corroborated the selected version of seepage-resilstive protection for the
given geological conditions.
*Translator's note: It is not clear from the Russian original whether Pavlovsk,
Voronezh oblast, or Pavlovo, GoAiy oblast, is the site.
A. A. S.
Card I / I

YAROSHETSKAU, N.A.
HIstopathological cLangos in secondary syphilids of the skin
following treatment with bacillin-1 and 3. Vest. derm. i van.
36 no.10946-49 0162 (MMA 16:11)
1. Iz kafedry kozbn-ykh i. venericheskikh bolezney ( zav, - prof.
A.A.AkoVbyan i kafedxy gistologii (zav. - dotsent K.Td. Usmancv;
nauchnyy rukovoditell - dotsen't L.A.Ellkind) Tashkentakogo me-
ditsinskogo instituta.
It

T~.
I - I ~~ Ir7".f. ~~
A F ,-, -
M.

USSR/Electronics - Secondary emission FD-569
Card 1/1 : Pub. 153-9/28
Author : Shullman, A. R., and Yaroshetskiy, I. D.
Title Secondary electronic emission of thorium oxide
Periodical Zhur. tekh. fiz. 24, 845-854, May 1954
Abstract Investigates the dependence of the coefficient of secondary electronic
emission upon the energy of the primary electrons and upon the tem-
perature of the target. Concludes that the transition of theorium
oxide from the inactivated state to the activiated slate is accompanied
by a decrease in the coefficient of secondary emission, which fact
does not substmitiate the conclusion of Arizumi and Esaki (J. Phys.
30c. Jap. o' 11.5, 1951). Thanks Acad. P. I. Lukirskiy, in whose
laboratory the work was done.
Institution
Submitted December 10, 1953

49,4-.77oo
AUTHORS:
TITLE:
PERIODICAL:
S/181 60w#/04/02/034
B002 Bo63
YB
Konopleva, 2. F., Ryvkin, S. M., YaroshetskiY,_1__4),.
The Problem of theThgoing Cross Section of Holes in
Germahium by Defects Formed by Gamma Irradiation Ig
Fizika tverdogo tela, 19609 Vol. 2, No- 4, PP. 566-56a
TEXT: The trapping cross section of holes by defects formed by neutron
bombardment vas found to be - lo-15 cm2 (Refs. 1-3). The trapping cross
section for gamma irradi&tion was 4 .10-16om2. The present paper shows
that this difference is due to a false assumption: A defect formed by
gamma irradiation has not two but four acceptor levels in the forbidden
band. The dependence of the lifetime on the irradiation with gamma
quanta was determined on 11 specimens, wherefrom the trapping cross
section of the holes was calculated (Table). A Cobo preparation with an
activity of 400 gram-equivalent Ra was used as gamma source. The authors
used the photomagnetic method, the method of photodiffusion, and the
examination of the relaxation curves of photoconductivity to measure the
lifetime. The mean value of the trapping cross section was found to be
3.8-10- 15cm 2. This is close to the value obtained for the neutron
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819W4
The Problem of the Trapping Cross Section 5/181J60/002/04/02/034
of Holes in Germanium by Defects Formed B002/Bo63
by Gamma Irradiation
bombardment (3-10-15cm2 in Ref. 1). Ther a are 1 table and 7 references:
4 Soviet, I American, and 2 British.
ASSOCIATION: Leningradskiy fiziko-tekhniobeskiy institut AN SSSR
(Leningrad Physicotechnical Institute of the AS USSR)
SUBMITTED: October 14, 1959

830222
S/161 60/002/008/041/045
.4p.*j 11DO Boo6YBo63
AUTHORSs gyvkin, S. M., Yaroshetskiy, I. D.
TITLE: The Influence of Adhesion Levels on the Relaxation of Non-
equilibrium Conductivity in Germanium Irradiated With Gamma
Rays 7\
PERIODICAL: Fizika tverdogo tela, 1960, Vol. 2, No. 8, pp. 1966 - 1977
TEXTt In order to stixdy the mechanism of recombination processes of
defects, the authors made a number of experiments which are described
here and whose results are discussed in detail. The main purpose of the
experiments was to determine the effect of 7-induced defects on the
,temperature dependence of the relaxation time of the conductivity of
n-type germanium. First, the method and the experimental arrangement are
3
discussed.-n-type Ge single crystals of 5 - 5 - 15 mm , etched with
CF-4 (SR'4) to reduce the rate of surface recombination, served as
,samples. They were exposed to ?,-rays of 120 r/sec (Co 6o ) at 200C. The
concentration of the resulting structural defects was determined from
Card 1/4
--- - -------

1 83022
The Influence of Adhesion Levels on the S/181/60/002/008/041/045
Relaxation of Non-equilibrium Conductivity in B006/BO63
Germanium Irradiated With Gamma Rays
formula Nt M '6N.J, where 0 ist the V-f lux per am2of the sample surface,
NGe the concentration of the germanium atoms, and a the cross section of
defect formation which was assumed to be 6 - 4-3-10-27cm2 according to
Ref. 6. The experimental arrangement is schematically shown in Fig. 1.
The sample is placed in a cryostat between the poles of an electromagnet
which can generate a field of up to 4,000 oersteds. This cryostat permits
a change in temperature from room temperature to that of liquid nitrogen.
Fig. 2 shows the temperature dependence of the relaxation time, T', of
non-equilibrium conductivity as the function Inil - f(I/T). The six
13 -3
curves refer to six Jifferent Nt-values between zero and 1.0-10 am
With inoroaning Irradiation, a dropping slope of the curves having a
minimum could be obt,erved. After passing through this minimum, they
steeply rose again. Thus, the relaxation time first decreased with
dropping temperature and again increased with further dropping tempera-
ture. Fig. 3 again shows lnT' - f(l/T) for the same sample, however, for
Card'2/4

83022
The Influence of Adhesion Levels on the S/181/60/002/008/041/045
Relaxation of Non-equilibrium Conductivity in Boo6/Bo63
Germanium Irradiated'With Gamma Rays
Nt - 1.5-10130M-3 in a wide temperature range. The curve starts in the
minimum, riBes-linearly and quickly, and after having passed through a
peak, it slowly drops. Yext, the results-are discussed in detail and
compared with theory. The curves In'll - fO/T) may be well represented in
thr,-)~_characteristic parts (I - drop, II - rise, III - almost saturation)
(cf. Fig. 5). The posit'mon bBS of the recombination levels of these
31'~_ induced defects in the forbidden band are determined (Fig. 4) from the
slope of the curves (part I, Fig. 2). The authors found that AES - 0.2 ev
(distance of the S-level from the conduction band). The hole trapping
cross section on the S-level at room temperature was determined to be VX
3.5-10-15cm2. The position of the second level (M) is determined by its
distance from the valency band AEM; it was1found.that AEM - 0.24 ev. The
values found for the second sample deviate but little from those of the
first sample; the second sample had a somewhat lower resistivity. The
numerical values are compiled in a table (P- 1976). The S-levels are
Card 3/4
--- - ------

83022
The Influence of Adhesion Levels on the B/181/60/002/008/041/045
Relaxation of Non-equilibrium Conductivity in B006/BO63
Germanium Irradiated With Gamma Rays
recombination levels, while the M-levels play the part of adhesion levels
under certain conditionsl as may be seen from a comparison with results
of other authors. At low temperatures, the adhesion -levels become
recombination'.1eveli. Finally, the authors thank E. Borutayta for
assistance in the measurements. There are 5 figures, 1 tabIT,.and
20 referencesi 9 Soviet, 3 US, 2 German, and I Dutch.
ASSOCIATION& Fiziko-tekhnicheskiy institut AN SSSR Leningrad (Institute
of Physics and Technology of the AS 6SSR, Leningrad)
SUBMITTED: February 20, 1960
Card 4/4

S/089/60/009/005/010/020
Boo6/B07O
.25 0.~,
AUTHORS: Konovalenko, 3. Ryvki S. 14.) )~aroshetskiy, !o Des
Bogomazov, L. P.
T#L-E: An*Ap~paratus for Studying the Effect of Gamma Radiation
on Semiconductor Materials Vr
PERIOD;CAL: Atomna*ya.energiya, 1960, Vol. 9, No- 5, PP. 408 - 409
TEXT: jin the present "Letter to the Editor", a cobalt apparatus for
th4d itudy of the effect of gamma radiation on 'the electrical proper-
ties of semiconductors is described. The apparatus was developed in
1956 by,the Fiziko-tekhnicheskiy institut AN SSSR (Insti ute ;f Physics
and Tec nQlogy of the AS USSR). The principal use of the apparatus is
in the !production of defects that'are constant in time. To obtain
enough,defects, fluxes of 1011 cm-2sec-1 are required. Fig.1 gives a
schematl~c representation of the apparatus; FiG.2 shows'the experimental;
chamber. Both are described in detail. The dose rate was measured at
differeInt points of.the chamber, and some of the results are Given in
U-he center of
a Table The highest dose rate of 128 r/sec was found at
I
Card .1

85566
An App ratus for Studying the Effect of SIOB91601009100510101020
G:amma radiation on Semiconductor Boo6/BO70
Materials
the ch mber flo6r; 10 mm, above the floor it was only 72 r/sec; 20 mm
abovei 43 r/sec,'and 40 mm above, 22 r/sec (all values refer to the
centerlof,the chamber). There were no disturbances during the experi-
ment, ~he work was satisfactory in all respects. L. V. Maslova is
thanked for help in measuring the field of 6amma radiation. There are
2 figu4es, 1 table, and 2 Soviet references.
F; .4
SUBMITIED: April 6, 1960
Legend.1to Figl: Scheme of the
4
apparaius: 1 - C660 standard
sourcei activity: 400 &-equ..Ra;
2 '- ir tank, 2.9 m high, filled
comple ly with water. 2
5 x 0.6 M21 wall,thio%neas,
5 mm; f- coppel, tube 125 mm wide
on the)inside; 5 chamber with the sample.
Card .273

85566
~S/089/60/009/005/010/020
2 Boo6/BO70
21
3
3
Legend to Fig.2:
Scheme of the sample chamber. 1 measuring
vessel; 2 - cover; 3 - rubber ring;
4 - hermetically closable opening through
which a cable
.(8) is introduced for the
moasurement of the electrical parameters of
the irradiated samples; 5 - two supports;
6 --holder for the sample (7) made of
7 asbestos cement; 9 conical insert;
7
10 f;uide box.
Fig.. 2
Card
7_
71

89297
3/181/61/003/001/036/042
77 B102/B204
AUTHORS: Ryvkin, S. M., Paritskiy, L..G., Khansevarov, Ro Yus, and
Yaroshetskiy, I. D.
TITLE: Investigation of the kinetics of impurity photoconductivity
for the purpose of determining the parameters of local
levels
PERIODICAL: Fizika tverdogo tela, V. 3, no. 1, 1961, 252-266
TEXT: An investigation of impurity photoconductivity is not only of
interest in principle, but is also of practical importance for studying
the local electron states in the forbidden band and especially of its
interaction with exciting radiation. Apart from an earlier paper by the
authorst relaxation processes of impurity photoconductivity have hithert
not been investigated in detail; this was, however, the aim of the present
voluminous paper. The authors set themselves the task of investigating
theoretically the most important cases of photocurrent relaxation during
excitation in the impurity region. The rules governing the kinetics of
impurity photoconductivity have certain peculiar features as is shown
Card 1/6

IS11811611003100110361042
Investigation of the kinetics of.*. B102[B204
here, due to which impurity photoconductivity relaxation differs
essentially from that of intrinsic photoconductivity. An exact analysis
of these rules shows that an experimental investigation of the kinetics
of impurity photoconductivity may serve the purpose of determining
various parameters of impurity centers as, e.g., the photon capture cross
section, the trapping cross section for free carriers, as well as the
energy position of the impurity level in the forbidden band, the
concentration of centers and the degree of their completion. In part 1
of this paper, the most important rules of the kinetics of impurity
photoconductivity in the excitation of carriers for one type of local
centers are dealt with. This is done on the basis of an example of a
semiconductor, in whose forbidden band there is a sort of local level
with concentration M; these levels are assumed to be in the upper half of
the band, so that they are in heat exchange with the conduction band.
This semiconductor is irradiated with monochromatic light of such a
wavelength that only electrons pass from the local levels onto the
conduction band, and that monopolar impurity photoconductivity occurs.
The equation of motion (13) d &n/dt (m a- an)qJ y,8n(N am +M-M 0+n0+ on)
Card 2/8

S11811611003100110361042
Invoutigation.of the kinetics of**$
.13102/B204
(2.13)
_I:~ VXn )q AJ-r For I-
O.'o-ni n -4- rtj
t H ~_M-L4 :- , " , `N'
0 nis IM
TMO -
is obtained. In part 3 of this paper,' th6 effeo.t.of constant exposure
Within the region of intrinsic absorption upon the relaxation of impurity
"Photoconductivity is investfgated., This is done on the basis of a simple
example of ".absolute adhesion levels" (levels for which the trappi
ng cross
sections for carriers of one kind vanish) for short-wave exposure of
Anten ity~Ip.which conveys-electrone from the valence band into the
I .,..conduction' ba'ndj electron-hole recombination was carried out over the
level S. Here,the most simple case of monopolar electronic intrinsic
photoconductivity in linear1recombination of free electrons,is.
'investi atdd.
9 The kinetics of the electron tranbitione is described by
the, system
an
Pkj 7- (M m) -t-.jtn1Vx -t- qinj-.-a (3.1)
=7nW M) mMm qmj, (3.2)
7
Caid 618-.,
:A.
-7- 7e--_

-7 r-71

ov~
Lm~
2206h
S/101/61/003/004/030/030
- (16 Tr, 11443 10r-459J B102/B209
0 :1
AUTHORSt Dobregop V. P.p Rogachev, A. A.t Ryvkin, S. M.p and
Yaroshetskiy, I. D.
Low-temperature breakdown in germanium in connection with
TITLEt
radiative defects
PERIODICAL: Fizika tverdogo tela, v. 3, no. 4, 1961, 1298-1300
TEM In germanium doped with elements of the third or fifth group, the
current may suddenly rise at helium temperatures when the field applied
exceeds a certain critical value. This effect is known as low-temperature
breakdown. The following is the mechanism of this effect; At these tempera-
turesp the majority of carriers causing impurity conduction is localized at
impurity centers, and resistivity is high. When a field is appliedf the free
carriers are accelerated and, at a certain field strength, their energy is
high enough to cause impact ionization of the filled impurity centers, The
low-temperature breakdown in Ge or Si due to donor or acceptor impurities
has been investigated repeatedly. The present paper is a report on studies
of this effect which is caused by radiative defects; such defects have been
,---Card 1/4

22064
S/18 61/003/004/030/030
A. B102 209
Low-veinporature ... YB
produced by irradiating the semiconductor with gamma quanta or fast neutrons.
First, the energy levels of the radiative defects are discussed; Fig. 1
shows the level scheme for gamma-irradiated (a) and faat-neatron irradDateft
(b) germanium. The two shallow levels of the radiative defects axe only
0.02 and 0.01 ev, respectively, off the valency bandl at helium temporatur,r"',
they are occupied by electrons only partly or not at all. In neutron-iv-
radiated Go specimens, the 0.01-ev level was found to be free from clectrcais
at helium temperatures. In chemically impure specimens, the presence of
donor centers offered a certain compensation, and the level wa8 partly oc-
oupied by electrons. Volt-ampere characteristics of such specimens were
taken by means of a "characteriograph.11 They were analogous to those ob-
tained by B. Vul, E. Zavaritskayal and V. Chuyenkov for the low-temperature
breakdown due to impurity centers. Altogether; three specimens were examin-
ed; gamma-irradiated 1-,r had a concentration of shallow radiation levels of
Na - 7-jol3cm-3 and a hole concentration on them of p a = i.iol3cm-3; 1-n and
2-n were n-type specimens having a resistivity of 2 ohm-cm; after neutron
irradiation they were p-type. n-type and p-type specimens having a resistiv-
itY Of 3 and 12 ohm-cm, respectively, were measured for comparison. The
Card 2/4

S/18 611003100410301030
Lo"w;temperature ... B102YJ3209
values of the critical field strength (1) and of the bre~2kdown field
strength (2) for these two,specimens are listed in columns (3) and (4) of
'th6,table. The authori thank T. V.Mashovets and N. A. Vitovskiy for having
prepared the gamma-irradiated specimens, as well as S. R. Novikov and R. F.
Konoplevaya for the neutron-irradiated specimens. There are 2 figures, 1
table,and 11 references: 5 Soviet-bloc and 6 non-Soviet-bloc. The most
recent reference to an English-language publication reads as follows:
McWhorterf R. Rediker, Proc. IREt 471 1207f 1959.
ASSOCIATIONt 'Fiziko-tekhnichesk
iy inatitut im. akad. A. F. Ioffe AN SSSR
Leningrad (Institute of Physics and Technology imeni
Academician A. F..Ioffe AS USSR Leningrad)
SUBMITTEDs December 2 1960
:QKTVOAb- :OXTPGAb-
E.P" N/Cu 110 12 9.5 7.5
14'.
As, x1cW 44 110 ~'15 10.2 9
Card 3/4

29702
811811611003101010321036
B125/B102
l'UTHORSt Ryvkin, 8, 1.9 Khansevarovg R. Yu., and Yaroshetskiy, I. D.
TITLEs Impurity photoconductivity with gamma-irradiated germanium
PERIODICILi Fizika tverdogo tela, V. 3, no. 10, 1961, 3211 - 3219
TEXTs gamma irradiation of n-type germanium gives rise to an appreciable
impurity photoconductivity which exceeds that in nonirradiated germanium
by some orders of magnitude. 'It was examined in n-type germanium
specimens (Q - 20 - 30 ohm-cm irradiated with Co 80 quanta. Since
irradiation took place at .INC, the radiation defel were stable at
room temperature. The experimental setup is shown in Fig. 1. The
specimen was placed in a cryostat with Or- indow. All measurements wero
made at N1000K. Parasitic light was eliminated by a set of filters. The
gamma-induced defects in n-type Ge form four levels in the forbidden band
which are 0.02, 0.11 and 0.*26-ev above the edge of the valence band and
0.2 ey below the bottom of the conduction band. The Fermi level was con-
siderably above the level at 0.2 ev throughout the temperature range in-
volved. The typical dependence of this photoconductivity on the energy
Card I

29qO2
5/181/61/003/010/032/036
Impurity photoconductivity... B125/B102
of incident quanta is presented in Fig. 3. The relaxation of unipolar
impurity photoconductivity was also examined. In these experiments, the
light frequency was chosen such that electron transitions occurred only
from the 0.2-ey level. Growth and decay curves of photoconductivity, when,
respectively, switching the light on and off, are "asymmetric" and do not
obey the exponential law. The experimental results may be explained by
calculations of S. M. Ryvkin et al. (FTT9 III, no. 1, 1961). quenching
was obseryed in all n-type specimens when irradiating simultaneously by
light corresponding to the self-absorption band and the impurity band.
Fig. 5 presents typical curves of quenching spectra. The complicated
characterl the great variety of relaxation curves, and of spectral proper-
ties of querohing are due to the superposition of two concurring processes,
namely, of quenching and of the impurity photoelectric effect. The shape
of the spectral distribution curve, while depending on the ratio between
the two light intensities depends on the experimental conditions and is
not characteristic of the examined material. Conclusionst The radiation
defeats forming as a result of gamma irradiation of germanium gives rise
to an impurity photoconductivity reaching as far as 6 microns. The posi-
tion of the two independent radiation defeat levels agrees with results
Card 2X 7

29
S/1 8715 1/003/010/032/036
Impurity photoconductivity... B125/B102
earlier found from the-measurement of the Hall constant and from the
Icinetics of intrinsic photoconduction. Quenching resulting from the com-
bined action of light corresponding to the self-absorption and impurity
bands results in the trapping of minority carriers. There are-7 figures,
1 table, and 16 referenoeas 8 Sovie 't and 8non-Soviet. The three most
recent references to English-language publications read as followst
R. Newman, W. W. Tyler, Sol. State Phys. Acad. Press. 1 19591
Z. Johnson a.,H. Levinstein. Phys. Rev., 117, no. 5, ;Igi,, 196o,
R. Newman, H. H. Woodbury a. W. W. Tyler. This. Rev., 102, 613, 1956.
ISSOCIATIONj Fiziko-tekhnicheskiy inetitut im. A. F. Ioffe AN SSSR
Leningrad (Phyeiootechnical Institute imeni A. F. Ioffe
AS USSR, Leningrad)
SUBMITTEDt xarch-6, 1961 (initially),
June 13t 1961 (after revision)
Card '~Y

29
702
003/010/032/0316
Impurity photoconductivity... B125/B102
Fig. 1. Experimental arrangement.
Logendi 0 - sample, 31 2,3 - mirrorsq set of filters, S 1 - Nernst
light source, S - whit: light source, G filter for varying light
2
intensity, JqTM-2 (UIPP-2) d-o amplifier, M electromagnetic shutter,
NO-1 (ENO-1) oscilloscope, CD synchronous detection, ~M-09 (EPP-09)
recorder, K - calibrator..
Fig. 3. Spootral.distribution of impurity photoconductivity. Curves were
taken for,an equal number of incident quanta. The daahed section of the
curve of Fig- 3a is reproduced in Fig- 36' on alarger scale.
Fig. 5. Spectral distribution of quenching. Curves were'taken for an
equal number of incident quanta. IMII(2) NO).
Card 4/ 6

34228
S/18 62/004/002/011/051
B102YB138
AUTHORS: Konovalenko, B. M., Ryvkin, S. M., and Yaroshetakiy7 I, D.,
TITLE; Radiation defects caused by fast electrons in n-type
germanium
PERIODICAL: Fizika tverdogo tela, v- 4, no. 2, 1962, 379-382
TEXT: The concentration M of radiation defects, the number 1 of the
defect levels and their energies were determined for n-type Ge
(" I ohm-cm, n =2-10 15 cm-3) which was irradiated by 2,541ev electrons,
The electron current density was - 5 j-a/cm 2, pulse duration was - 2tAsec
and repetition frequency was .50 see- 1. The samples (8,1.1 Mm 3) wer~-
-water-cooled. The electron energy behind the specimens was -1.5 Mev, so
-that for calculations the electron energy in the specimen was taken to be
-/2 Mev. Carrier concentration was determined by measuring the [fall
constant between 770K and room temperature, M and 1 were determined using
the relations: n 2 = Nd Ml1 and n4 ~ N d- M(1-1); n2 is the electron
Card

3h228
4/002/0,,/054)
S/16 62100
Radiation defects caused by fast- B102XB138
.~~onct,ntratioIn in tho conduction band at low temperatures, when all defect,
!e7els are filled up and all donor levels are completely ionized (section I
in Fig. 1)~ At high temperatures, when the upper defect levels ate
completely ionized, n 4 is the electron concentration (section II in - V~
Fig~ 1). M was also determined from the activation energy of the upper
levels and the carrier concentration of the linear part of II, using the
relation n-n,, = ff- ---xp(-AE-./2kT). No was calculated for the effeat-1,.e
c __hI
Mass M' = 0.25 mo~ For several different specimens, the following results
n -1015 cm-3 , hIl was 0 6c~ - 2 ~ 03)-,015 _'3'
were obtained: 11, was (2.08 -2~26) cm
d 14 3
M was (4.25 - 5.2)-10 cm- , 1 was 3.9 - 4.2, AEM 0,20 0.23 ev, and
the radiation defect formation cross section was 1~45-1-55 barn; it was
calculated from a = M11N Ge' electron flux density, N Ge - number of Ge
3~ t h
atoms per cm Electrons with j25 Mev were found to produce defect:, wi.
the following levels: E -0.24 ev, Er-0-36 ev, E +0.25 ev and E +0.11 ev,
c v v
There are 3 figures, 2 tables, and 7 references: 3 Soviet and 4 non-
Soviet. The three references to English-language publications read as
Card 2/3
7_7
-7K

342ePi
F, 1 //0'21/CC4/002/01 1 /05 1
Radiat.1un duf(;Cts
-Follows: J. Ciel&nd i-I. Rtav- 7-2, iq~-6; L. Brown
et al. Ph-s. c,:"
2
Procress in Semiconc-acia,
ASSOCIATION: inst4-'ut 4m. A. F. o"e A"' ~---SR
Lenin,,~rad ~cc i~~c..nicai institute A. F. loffe
AS USSR, Lenin-rad)
SUBLUTTED: Aiigust 8, 1961
Ig n
14.9-
2 3 4 5 6 7
d
.Car 3
ITIM

RYVKIN S.M.; DOBPEGO, V.P.; XONOVALENKO, B.M.; YAROSHETSKIY, I.D6
Induced impurity breakdown in compensated germanium and-,.
current oscillations related to it. Fiz.tver.tela 4 no.71
1911-1914 JI 162. (MIRA 16:6)
1. Flziko-tekhnicheskly institut Imeni A.F.1offe AH SSSR,
Leningrad.
(Breakdown, Electrid) (Germanium-Electric properties),
~si
T

(.q)/EWt(m)/ S WTG /ASD
L 13869-63 EWP
ACMSIOU IM: 03MOT8 8/0181/63/005/007/1833/1841
AVMOR: VitOvGMZj H. Aj Kmovalenko,, B. H.;- Hashavete, Te Vo; IV*vldn, so Mt.
-jaroshetskiy, I,
TMM Gamna-ray- 69
generated dafacts in go
ISOURCEs Fizik% tverdogo tela,,'.V* 50 no* 7s 1963,,.1833-1841
T'OPI"
TAM.- Xs=a-m semiconductor irroAiation
radiation defeat monopolar
i=ealin~, bipolar annealing, germaniUM irradiation, gennaniun defeat, germpnim
iABSMWT; In the latest stage o,- research on the subject,, dating back to 1959,
:a large nudber of n- and y type specimens was investigated. 11-type
germanium
;was doned with antimony and had a donor ecracentrati-cm between 2-1012 to 8.1015
cm 5; p-type geifilanium was doped with Gallim and'had an acceptor concentration
ibetveen 1012 to 1015 an-13. The source van Co6o at, a dosage of 2010U jrr1,:jj2*seO
and temperature of IOC. The work was aimed at clarifying the saturation of ir-
radiated specimens which occurs after polarity reversal, whereby further exposure
to radiation, however, prolonged, no longer affects the slope'of the themal de-
Pendence of carrier concentration. The latter remains equal to the activation
wenergy. while the saturation process is evident up to very high concentrati
:Card 1/2

16

KONOVALENKO, B.M.; RYVKINj S.M.; YAROSHET9UY, I.D.
Radiation defects in getmanium caused by fast 28 Her. electrons.
Fiz. twer. tela, 5 no.8t2O75-2086 Ag 163. (MIRA 16:9)
1. Fiziko-tekhnicheskiy institut im. A.F.Ioffe AN SSSR, Leningrad.
(Germanium crystals-Defects) (Electrons)

GERASIMV, A.B.; RYVKIN, S.M.; YAROSHETSKIYP I.D.
impurity photoconductivity in germanium irradiated bf fast electrons.
Fiz. tver. tela 6 no.3:695-705 Mr t64. OaRA 17:4)
1. Fiiiko--tekhnlcheskiy institut imeni A.F.1offe AN SSSR, Leningrad.
I-IMN
N,

I 'LZ20L_A-._ BVT(I)/EWri(k)/SqT(m)/EPF(c)/FPF(n)-2/EFC(t FWP(b)/ENP(t) Pz-,6/
P-r-4/Pli-i IJP(C)/AS(mp)-'/AFrIL/SSD/ASD(a~~ 1Z
4 .-5/--T3D/ESD(gs )/ ESDf tJ'Dlri,-/~' TI
ACCESSION NR: AP4046643 S/0181/64/006/010/3166/3158
AUTHOR.: Gerasimov, A. B.; Konovalenko, B. M.;Yaroshets!ii
Barkalaya, A. A.
TITLEo Impurity otoconductivity produced in gormanium by gamma-----_
ray irradiation
SOURCE: Fizika tverdoqo tela, v. 6, no. 10, 1964, 3166-3168
TOPIC TAGS: gamma irradiation, photoconductivity, germanium, for-
bidden band, line up3ctrum, carrier density, impurity conductivity
ABSTRACT: This is a continuation of earlier research in which one
of the authors participated (S. M. Ry*vkin, R. Yu. Khansevarov, 1. D.
Yaroshetakiy, FTT v. 3, 211, 1961), using a larger y-ray flux in
order to observe a more extensive line spectrum in the forbidden band
In this case n- and p-type germanium with initial carrier densities n
= (2--6) x 1013 and p. = (0.6--2) x 1013 cm-3 were used. The sampleR
Cord 1/4

maw
-o-s o-y-ray rdtn---Co_ at-a~Aose_-_ rat"- 0;;;'-~~s9O-
e exp ed t s
tallation d ribed- 61sewhere (13' alenko, S. H.
an, ins esc -M., Konov
Ry*v' kin, I. D. Yaroshetskiy, and L. P. BcK
jomazo Atomnwya energiya
v. 9, 408, 1960). The results are illustrated in Fig. I of the
enclosure. The spectral curves disclose a large number of bends and
ledges, pointing to a complicated spectrum of the local levels in
the forbidden band. Measurements of all the investigated samples
indicate the presence of the following energy levels: Ev + 0.52,
Ev + 0.48, EV + 0.43, Ev + 0.41, Ev + 0.37, E V + 0.33, Ev + 0.31,
and Ev + 0.27. This spectrum coincides fully with the spectrum of
the local levels produced in the central part of the forbidden band
when germanium is irradiated with fast neutrons, to which the levels
with, energies Ev + 0.31 and Ev + 0.43 eV, which are symmetrical re-
lative to the center of the forbidden band, are added. It is fur-
ther concluded that the various levels introduced by impur-
ities in the central part of the forbidden band are not due to any
clustering of the point defects with the atoms of the doping impur-
Card 2/4
~E

L 120016-65
...,ACCESSION NR: AP4046643
"The-Authors are deeply* grateful to-..q H n for a discus-
sion of the results." Orig. art. has: 1 figure.
:ASSOCIATIONs Fiziko-tekhnicheakiy inatitut im. A. F. loffo AN SSSR
(Physicotechnical InatitutepAll SSSR)
,SUBMITTED: 18May64 ATD PRF.SSI 3120 ENCL: 01
~SUB CODE: ic, NP No REF SOV: 003 OTHER: 000

L 12006-65
NRt AP4046643
ENCIDSM: 01
rig, 1. PhotoccndWtivity gpectra
of Ge irradiated with ga= rays
from co~o.
I - Sanple with initial cmductiv-
ity n-type and Nd 5.5-1013 cm-?
after irradiaticn - E + 0.27 ev
(T = 85K) . 2 - swpie v -ith in-
itial cmdwtivity p-byW and 11
6.5-1012 cur3i after irradiatica
00-18 -ov. (T
Cord 4/4

19M MDR
=11-M-1- =F-MY-1
-002_'~a~ T- k)
ACC NR. 6030009 IJP(c) WG/JD/1,~W/&// SOURCE, CODE: UR/0020/66/169/005/1041/1043
JG/D1/VJ1 .71-7
i-qWOR: Ashkinadze. B. M.; Vladimirov, V. I.; Likhachev, V. A.; RyvKin, S. 14.; -7
S1.1lmanov0_- M.;-Yaroshetskiy, I. D.; Konstantinov, B. P. (Academician)
ORG: Physicotechnical institute im. 1. F. Ioffe, Acadeny of Sciences SSSR (Fiziko-
tekhnicheskiy institut Akademii nauk SS,SR)
TITLE: Laser induced damage in transEarent dielectrics
SOURCE: AN SSSR. Doklady, v., 169, no. 5, 1966, lo4l-lOh3
erwam GF162dimm
TOPIC TAGS: laser garglass, dielectric, alkali halide,
cr7st&l
duced I an ant-pulse lasers in a broad class
ABSTRACT: Demagq4n ,by standard
materials (alkaliv-4alid6Phingle crystalsl~lgi
polymers, glasses) was inveetl;:,--;~a
'experimentally., Pla-ne eVacko were observed in'.
V 4 0 poly.(methyl methacrylarA.A(PIM) Under
t standard-pulse radiation Za a 5 angle with respect to the laser beam axis and at
ra4dom with respect to th crack rotation plane around the same axis. A large
nuAer of isolated 'cracks\ as observed at superthreshold energies, A,20-j beam
fociieed at f a 6 cm caused tail-end dwwge in glasses, The same pulse caused total
de0ruction along the cleavage-planes in alkali-halide crystals at energies slightly
ab~re threshold. In each instance, damage was observed when a giant-pulse beam was
foopsed oti the inside of specimens. In single crystals the damage occuj~red along
1-CON I/Z; ROL

.,-,stimulated
L 4.3025-66
ACq. NRs AP6030009
all three cleavage planes; In the case of PMW it had the form of an extended cone
codsisting of small individual cracks (of the order of 0.1-0.5 mm); 1h, glasses,
filiform, damage appear'ed sharply with the thickening at the focus.
To explain the damage mechanism and kinetics, the effects of pulse energy, focus
position, temperature, and the focal length on the nature and extent of the damaged
region were investigated. The experimental dataindicate a strong dependence of
'the nature' and extent of damage on the test material and the operating (peak or
total energy) eonditions. The damage in each spot occurred independently and was
caused by beams of a small critical density. Die most probable damage mechanism.
is thought to be the coherent hypersonic phonons generated as the result of
Brillouin scattering. The.thermal explosion accompanying damage due to
hypersonicphmorij in the 'case of strong optical dbsorption is suggestea as a
secondary mechanism.
The experiments showed that the thermal explosion occurred I
basically near therfocus and that its role varied with materials and energy density.
Crack formation occurred during a period not exceeding the pulse auration (for
11 giant pulse laser 10.9sec), Abe damage taking place first at the focus and traveling
backwar&3. Damage Induced by powerful laser beams can be used as a method of
tcomparing the bulk and surface-AIXIn.&W of a material, Orig. art. has: 2 figures
and 1'formula. [YK1
01
SUB CODE: 20/--suBmTATE.-24Yft65/ ORMREF: 002/ ftl Rkif-6W11A
2

,4T
1-312634-66 F L-11).IFAP(-)/PliT(m)/EE~C(k)-?/T/EyiP(k) -IJP(c
WEI WG/WH 1101i~61 -
ACC NR: SOURCE CODE: ' UP/00b/ 050/VJ5/
A116018797
AUIMOR: Ashkinadze, B. M.; Vladimiray, V. I.; Likhachey, V. A. Eakin, S. Me.
Salmanov, V. M.; Yaroshetskiyy
ORG: Filysicotechnical Institute im.,A. F. loffg,_Academy of %cienr_es_SSSR_(Fiziko-
tekhnicheskly institut Akademil nauk SSSR)
TITLE: Breakdown of transparent dielectrics by intense laser rAdiation
SOURCE: Zh eksper I teor fiz, v. 50, no- 5, 1966P 1187-191
TOPIC TAGS: dielectric breakdown, laser effect, laser radiation, phonon interaction
ABSTRACT: The transparent dielegtricu investigated were alkali-halide single crys-
tals (LiF, NaCl, CsI, KBr KI tand others), polymers (poiymet~yl methacrylatelani
pol 6 - e), and glasses'ianilicate glasc-and fused quartzi? RLbM5and
y tyren neodymi
lasers generating 1-79 and 1.1t ev photonsreopectivelywere used at first, but when
it was found that the breakdown was qualitatively the same for polarized (ruby) and
unpolarized (neodymium) radiation, only the latter was used, since it could operate
in both the ordinary (20 J) and giant-pulse (2 J) modes. The diagram of the experi-
ment is given in Fig. I The samples were parallelepipeds with polished faces of
varying lengths and cross sections. The character of the breakdown was examined
under a microscope and its size measured with a horizontal comparator. The laser-
induced breakdown begins in locations exposed to high light-flux intensity and spreadi
to lower-intensity regions. In the case of focused beams, no destruction occurs be-
hind the focal point. The bre&~Aown occurs in Yory short time Intervals, shorter that-
_J

ACC NR, AP6018797
Fig. 1. Diagram of experiment. 1
Totally reflecting mirror or rotating
prism, 2 - ruby or neodymium rod, 3
partially reflecting mirror or plane-
a. 13104- 5-..
parallel plate, 4 - light filter, 5 - .. 1 2 34 /a 12 14 Is
plane parallel-plate, 6,10,14 - neutral H 13
filters, 12 - tested sample, 7,11,13
lenses, 8,15 -photodiodes, 9,16 - oscilloscopes.
the length of the light pulse, and develops independently at various points of the
solid. Estimates of stresses caused by the hypersonic wave due to the laner,beam in-
dicate that local effects play a substantial role in the breakdown process. In the
case of an ordinary laser pulse, the breakdown mechanism is governed by the peak
power, whereas in the case of a giant pulse the decisive factor is the total energy.
The cause of the breakdown is shown to be connected with the action of coherent
acoustic pbonons generated in the course of a stimulated Brillouin scattering,
thermal effects being secondary. Study of the breakdown makes possible compari.
son of volume and surface strengths of the material and can be used to evaluate the
time of phonon coherence loss, which Is found to be of the order of 6 Rsec for poly-
methyl methacrylate. The authors thank B. P. Konstantinov for continuous interest
and valuable disdussions, and A. M. Prokboroy, P. P. Pashinin, A. V. Prokhindeyev,_L._
N. Filimonova, G. V. Vladimirova, G. M. Malyshev F. F. Vitman, Vs P. Pukh. -a=. At.
j_fAly&in for help'with the experiments and for discussions. Orl-g. art. has: 10 fig-
ures and 11 formulas. 102]
ard 2/2 SUB COM.- 207 SUBM DATE: 3ONov56/ QRIG'RSF.' 004/ OTH REP: 004/- ATD PP
A

~--A~~~-~AP6 0 3 0 ~97 1'
~q)
AUTHOR: Ashkinadze, B. M.; Likhachev,_V. A.; kak-ing S._M.; Salmanov, V. M.;
Tomashevskiy. E. Ye.; laroshetskiy. I. D.
ORG: Physicotechnical Institute im. A. F. Ioffe AN SSSR, Leningirad (Fiziko-
tekhnicheakiy institut AN SSSR) -,X,.
J~ the effect of laser
TITLE: Occurrence of par agnetic centers*in p lymers under
radiation
SOURCE: Fizika tverdogo tela, V. 8, no. 9, 1966, 2735-2737
OPIC TAGS: laser radiation, laser effect, laser r and d, polymethylmethacrylate,
polystyrene, electron paramagnetic resonance
ABSTRACT: The authors report observation of paramagnetic centers in polymethyl-
methacrylate (FMMA) and polystXrenel(PS) under the influence of radia-t-To-n from pulold
ruby. and' n dymium lasers (0.69. and 1.08 p, respectively) and also i
under the ' influence of a giant-pulse , neody-mium laser. The samples (20 ma
long, 7 mm dia) were investigated in a standard radiospectrometer, using a procedure
described earlier (ZbETF v. 50, 1187 (1966). In both materials, clearly pronounced
electron parampgnetic resonance (EFR) was observed above a certain threshold radi-
I ' '" f
stion. The EPH sped
Card 1/2

ACC NN AP6030971
lines characterized by g factors close to 2.002 and small-width (1-and 3 Oe between
t~
for
fied
~
maximum-slope points for PMMA and PS, respectively). The Curie law is satisfied for
the EPR signals from PMMA, but not PS. The observed paramagnetic centers have a con-
cm;-. difference was seen
centration estimated at. -. 4 X 1,015 4 and are. quite Vkt!Pjg.,,, t,,,V9
between the effect of the ruby0and neodymium laver, 'or_ ~qtyeeg 'Qri - ana giant
Unary
pulaeo. The paramagnetic centera appeared only,in the pregence of cracks produced.-in.-wi,w
the material by the laser radiation. In view of some unusual.-featurea of the ob-
served paramagnetic centers (absence of macroradicals and absence of hy-perfine struc-
ture), it is difficult to draw definite conclusions concerning their nature, but it
is suggested that they may be the results of the decomposition of the polymers under
the influence of the laser beam. The differences between the centers-of PMMA and PS
may be caused either by differences in the centers themselves, or by differences in
their local concentration. Orig. art. has: .3 figures. (02]
SUB CODE: 20/ SUBM DATE: 28Feb66/ ORIG REF: 004/ ATD Prins: 5085
2/2
Cord
i MR.
"A

IT
AP603o966 SOURCE CODE: UR/0181/66/006/009/2668/2671'
AUTHOR: Volkova, N. V.; Likhachev, V. A.; Hyykin,-S. M.; Salmanov, V. M.;
Yaroshetikiy, I. D.
ORG: Physicotechnical Institute im. A. F. loffe AN SSSR, Leningrad (Fiziko-
tekhnicheskiy institut AN SSSR)
TITLE: Deatruction of LiF (single crystals b~ iaser radiation
SOURCE: Fizika tverdogo tell, V. 8, no. 9, 1966, 2668-2671
TOPIC TAGS: lithium fluoride, laser radiation, laser effect, crystal defect, crystal'
dislocation phenomenon, laser r and d
ABSTRACT: This is a continuation of earlier studies of damage to transparent die-
lectrics by laser radiation (ZhETF V. 50, 1187, 1966), where principal attention was
paid to amorphous substances. The present article deals with the effect of the ener-
gy contained in the laser pulse on the general evolution of damage to aingle-crystai
LiF and describes the dislocation structure in the cleavage surfaces. The experi-
mental procedure is similar to that described In the earlier paper. A pulsed
neoOymium glass laser was used, with the light beam directed always along
the (001) crystal axis. Dal3age occurred at pulsed energy density exceeding 100 J/cp2.
corresponding to 1-, 0.2 x 100 Wcm2. At this threshold value, damage usually started
Card 1/2

L 45783-66
ACC NRs AP603o966
with a single crack e (001) plane, perpendicular to the beam direction. With...
in th
increasing energy, additional cracks appeared and their character and pattern varied
with the energy. The evolution of the damage is explained from the point of view o~ -
the existence of a hypersonic damage mechanism, wherein the crack is produced first's'
by a hypersonic waved and absorption of heat in the crack leads to further disinte-,
gration. The peculiar dislocation pattern observed on the cleavage surface (concen'-!-,~-,.',,,
tric circles or ellipses) is attributed't*6 the initermitte'ni dh&ia~cier' of propaghtiolt,
,of the crack front, due in turn to spiking, Orig. art. has: 3 figures. '[4
SUB CODE: 20/ SUBM DATE: 3lJan66/ ORIG REF: 003/ OTH REF: 001/ ATD PRESS-
5085
CQ,d 2/2 pb

.ACC NRt IAE6037017 CAIN) SOURCE-CODE:' _6R/03131/66/W;/011/~)~32/3~34
AUTHOR: Likhachev, V. A.; Ryvkin, S.- M.; Salmanov, v.. M. ; yaroshetskiy, 1. D.
ORG.- physicotechnical Institute im. A. F. Joffe, AN SSSR;-T1i6h-1n'grad_0iziko-
~tekhnicheskiy institut AN SSSR)
TITLE: Fatigue under optical damage to transparent dielectrics
SOURCE: Fizika tverdogo tela, V. 8, no. 11, 1966, 3432-3434
TOPIC TAGS: fatigue strength, dielectric material, polymethylmethacrylate, poly-
styrene, laser effect, irradiation damage, crack propagation
ABSTRACT: This is a continuation of earlier work (ZhETF v. 50, 2735, 1966), and con-1
tains more detailed information on the fatigue produced during optical destruction
of transparent bodies in polymers (polymetbylmethaerylate and polystyrene). Tibe ex-
perimental procedure was the same as in the earlier investigation. 71he radiation
source was a neodymium laser operating in the ordinary-pulse mode. The tests con-
sisted.of determining the influence of energy on the number of irradiations necessary!
for the first visible crack in the material to appear, or the change in the dimensioW
of the damaged region with changing number of pulses. Comparison of the results of
the two tests has shown that the true threshold of optical strength is approximately
one-third as high as expected from an analysis of results of damage produced by
single irradiation. An investigation was made of the nature of the irreversible
changes due to the fatigue occurring at pulse energies lower than critical (necess
ary.
Card

ACC NRt AP6037017
-to start visibledamage by a single pul-se), and also the Influence of such factors.
.as,,-the temperature and the healing time between successive pulses. Experiment has
.-,,shown that,neither the temperature (from 20 to 100C) nor an increase in the pause
'A~iyeen I aditions (from 3 to 70 minutes) exert any influence whatever on the damaged
rr
aken as '.vidence that the changes introduced in the material
hreshold. This is t e
'4t-energies below critical are microscopic cracks which gradually grow 'upon repeated
'4*12*xradiation to sizes visible with the unaided eye:' Favoring this deduction are the
,-absence of healing of visible cracks in polymetbylmethaerylate up to the temperature
of complete softening, and the increase in the visible cracks upon repeated irradia-
tion. It is thus concluded that fatigue effects must be taken into account in stu-
dies of damage to transparent materials by laser beams. The authors thank I. A.-
Kodaneva for help withthe experiments. Orig. art. has: 2 figures and 1 table.
SUB CODE: 20/ SUEM DATE:~ lLxn66/ ORIG REF: 001
Ccrd 2/2

ACC NR; AW005V19 SOURCE CODE: UR/6i81/66/oo8/O12/3595/36o1
AUT11OR: Volkova) 11. V. Likhachev, V. A. ; Salmanov, V. M.; Yaroshetsk-11y, 1. D.
ORG: Physicotechnical Institute im. A. F. Ioffe, AN SSSR, Teningrad (Fiziko-
tekhnicheskiy institut AN SSSR)
TITLE: Kinetics of formation and healing of damage produced in lithium-fluoride
single crystals by a laser beam
SOURCE: Fizika tverdogo tela, v. 8, no. 12, 1966, 3595-3601
TOPIC TAGS: laser effect, 8emiconductor laser, semiconductor single crystal, crystal
lattice dislocation, ar=ing 0ee.,90.4 rqA-
ABSTRACT: This is a continuation of earlier work (ZhETF v. 50, 1187, 1966 and else-
where), where it was shown that a laser beam produces cracks in alkall-halide crys-
tals. although no detailed description was giVen of the nature of the cracks). To de-
termine this structure and to explain the mechanism whereby the damage is initiated,
the authors investigated LiF single crystals measuring 20 x 20 x 20 mm cleaved alon.-
the cleavage planes. A neodymium laser operating in the spiked modewas used. The
beam focusing procedure iias the same as in the earlier work, the damage was - exarained
under'a microscope, and the dlslo~ation slWucturawas revealed by selective etching.
Besides confirming the earlier results,, the present tests - demonstrated that the
damage produced by the laser pulse consist; of a main crack in the cleavage plane
(001) normal to the beam., and dislocetion slip along directions forming a rosette-like
1/2
Card UDC: none

'-ACC NO:- A'F7605849--
pattern, the occurrence of which can be interpreted by assuaing a suitable cc-.birP--
tion of thermal and elastic stresses produced in the crystal by the passage of the
laser beam and hypersonic oscillations accompanying it. Annealing the crystal after
the damage) either in air or in the oven, led to'healing of the cracks characterized
by a unique structure of the front of the annealed rosette. "lile the causes of this
healina are not clear, they definitely can be ascribed to transport of matter via the
gas pha-se, as proposed in a number of papers. The authors thank S. M..Ivvkin for
continuing interest and a discussion of the results. Orig. art. has: 5 figures.[021
SUB CODE: 201 Sum nA-.E: 27Yay66/ ORIG,W:, 007/ OTH REF: 003
ATD PPXSS: 5117
Card 2/2

M
TERM71OV, A.A.,inzh; SEULINp N*As,lnzh; CHUHISMY, P.L., lnzh.,- OMMLE. Yu.M.i
j4USATOV,'.T.P., 662h.; YZD636T, A.A., )Wad,tekhn#nauk;.
iizhS;'ZA00Nq' N.k,, In'zh.; SHOMiIN- B.M., inzh.
Improving planning of industrial power suppl7. Prom. energ. 13 tOG7'-
18-29 A .'58- (14in 11:105
lN'Tvazhprvmelektroproyekt. (for Yermilov). 2.Zhemproyektasg-g**Kauna9
ifor Chep?le).Denbassonergo (f6r Musatov),.; 4 KOBkovskly efibrgbtichenki
notitut for Yedorov.). 5.Uzgiprovodkhoz. it lashkent Uor YaroshetskiiT.
6.Proyaktny7 institut Ministerstva strotte atya USSR.,Odessa Ver
Golldenblat). 7031ektroproyekt. goKuyb7shev (for Rudryai3hov).
Mouradioelektronika, (for Zakharov).-9. Iltdroproyekt.g. Kuyb7shev (for
Shchukin).
Ollectric Power)

YAROSHE TSKIY, L.M.
Automation and remote cor trol of hydraulic and land-Improving
structures in the Golodnaya Steppe. Mat. po proizv. sil.
Uzb. no.15:332-336 160. (MIRA 34:8)
1. Institut, "Uzgiprovodkho-,?'#
(Go-lodnaya SUp e-Irrigation)
(Remote contro,3
a 2 ~&fflmm=a

YARWHEV,, A.~-', (K,~,Yov)
Effect of I'actnrs m the re-ul.:~ of a
quAlif,7 nortrol nf the ax~arna'L layers of machine parts by
mean-9 oi' the eddy eurrimit mothod, !-,JkI. mak-h. I no.4397-
100 165. (IMj. 18; 6)
IS Ins"Atul, mek-haniki AN Uki-315P.

7--F-r~ V (A -I i7 if I I rv I
ITTTW-YTI-T-~0
YASIL'Y3V, A.A., lm=eat Stalinskoy premil, inzboner, redaktor; BORO-
DACHW, I.P., kandidat tekhntcheskik~ nauk; PRUSSAK,B.N.
inzbener; URUSOV, H.M., Inzhener; WSMOBT, A.T., Inzbener;
YAMSMU" , kaadidat tekhnicheakikh nauk; NWIROVSKIT, B.I.
Inzbener, retsenzent; PETROV, G.I., inzbener, redaktor;
PISTIUAKOV, A.I., inzhener, redaktor; POPOVA, S.M., tekhnicheskiy
redaktor.
[Road bulldlW machinery,] Doroshnostroitel'rW~ mashiiW; Bpravoch-
n1k. 2~-oe perer. i dop.izd. Moskva, Gos.nauchno-tekhn.izd-vo
maahinostroit.lit-ry, 1955. 8~2 P. (MLRA 8:10)
(Road machinery)

SOVALOV,I.G., kandidat tekhnicheskikh nmuk; YAROSHEV,D.H., kandidat
tekhnicheskikh
.4
New specifications for construction and building erection. Strul.
prom. 33 no.8:22-25 Ag'55. (MLRA 8:11)
(Building)

ly.
PHASE I BOOK EXPLOITATION 1010
Yaroshev, D.M., Candidate of Technical Sciences
Problemy kcmpleksnoy mekhanizatsii i energeticheskiy metod (Problems in Complex
Mechanization and The Power Method) Moscow., Gosstroyizdat, 195;8. 119 p.
7,000 copies printed.
Scientific Ed.: Voynik, O.M., 2ngineer; Edo. of Publishing House: Begak, B.A.
and Udod, V.Ya.; Tech. Eds.: Guseva, S.S. and Borovnev., N.K.
PURPOSE: The book is intended for engineers and technicians working in the
building industry.
COVERAGE: The book describes the fundamentals and practical applications of
a:nev method of studying mechanized processes in the building Indu try.
The author explains how the power indices of individual machines are reduced
to indices common to the whole machine group. He shows how laws governing
construction processes are determined and gives solutions for various practical
problems in complex mechanization. The author states that this nev method has
'been employed repeatedly and successfully in practice by Profeesor V.A. Kirpichev.,
Card 1/5
ME

Pr&lems in Complex Mechanization (Coat.) 1010
Academician N.I. Gersevanov., and others. The present vork is based on an
analysis of teohnico-econamic indices of constr-action machines as published
by VNICMS.Thexe are 5 Soviet references.
TABLE OF CONTENTS:
Introduction 3
Ch. 1. Theoretical Principles of Complex Mechanization in Construction
Work 5
1. Power method of analyzing mechanized construction processes 5
2. Consmption of energy by building materials (minimum energy
required to process unit weight of material)
3. Efficiency of energy sources 7
4. Interrelation of basic techn-Scal indices of mechanized
processes
5- Nomograms for mechanized construction processes 10
6. Productive capacity of ma-hines in mechanized processes 11
7- Ormanization of mechanized constractiaa processes and
tneir power indices 15
03rd 2/ 5

Problems in Complex Mechaalzation (coat.) 1010
Ch. 2. Methods of Determining Power Indices 19
1. Diagrams of the interaction between the working menber of
the machine and the material being processed 19
2. Interaction between grader blade and soil 20
3- Interaction between roller and compacted material 21
4. Power indices of machines 26
Ch- 3- Complex Mechanization of Individual Types of Work 31
1. Complex mechanization of earth work 31
2. Complex mechanization of building the road bed 39
30 Ccmplex mechanization of transport and handlin
, operations 53
4. Complex mechanization of other types of construction work 69
Ch. 4. Examples of Applying the Power Method 83
Card 3/5

ProblIems in Ccmplex Mechanization (Cont.) 1010
1. Selection of machine groups 83
2. Analysis.of mechanized processes 85
3- Power analysis of production data 88
4. knelysis of design changes in maebinery 90
5- Productive capacity of machine groups during erection
of various structures 91
6. Establishing efficient, use of 1"a-bines and machine groups 92
7- Establishing values for various technical indices 94
8. Canparative evaluation of machines 95
Ch- 5- Solution of Problem of Ccaplex Mechanization in
Individual Cycles of Construction Processes 101
1. Equation of the process 101
2. Energy consumption by stone as a function of its
initial and final dimensions 106
3. Laws govering the perfazmance of transport machinery 107
card V5

Problems in Complex Mecbmnization (Cont.)
4. Vacwn treatment of concrete
5- Pile driving
Conclusion
AVAnOLE: Llbr=7 of Congress
Card 5/5
1010
1-30i59
109
112
112

BARANOV, L.A.; GCMTOV, V.I.; YEWINOV, D.V.; YMIMOV, Ye.I.;
PITER OT, N.I.; RILITSEV, A.M.; RYAXANTSHV K.G.; TORCPOV, A.S.;
TSMLIM, G.I.; TAROSH97,D.R.; TOBIN, T.'A.: glavu;yy red.;
30SHIN, A.Y., za ".- AqWo'je-i~d.; RAKITIN, G.A., red.; GRINWICH.
G.B., red.; YEPIFANOV, :�.P., red.; ONMIYEV,'I.A., red.; KHOKHLOV,
B.A., red.;, tIMIM. P.A., red.; TABUNINA, K.A., red,izd-va;
OS = 0, L,M., tekhn.red,
(Kanual on accident prevention and industrial sanitation during
construction and repair operational Spravochnoo posobie po tekhnike
bezopasnosti i promeanitarli pri proizvodstva stroitelluo-montazh-
rifth rabot. Pod red. G.A.Rakitins. Koskva. Goo.izd-vo lit-ry po
stroit., arkhit. i stroit.materielam, 1961. 359 p
jHnU 14:4)
1. Akademiya stroitel'stva i arkhitektury SSSR. Institut organi-
zateii, mekbanizatail i takhnichookoy pomoshchi atroitelletvu.
(Construction industry--Hygienio aspects)

YAROSHEV, Dmitriy Mikhaylovich,, kand. tekhr, naukj RYAZANTSEVA,
O~
[Problems in overall mechanization and the power method]
ProbleW kompleksnoi mekhanizatsii i energeticheskii me-
tod. Izd.2., perer. i dop. Moskvap Stroiizdat, 1964.
185 p. (MIRA 17:5)

AINDROSOV, A.A., inzhener; YAROSHN, D.M., redaktor; GUROVA, O.A.
toikhnicbeekiy redakttr, -4 Mgt&
[Machines for building and maintaining city streets] Mashiny
dlia postroiki i sodermhantia gorodakikh dorog. Moskva, Izd-vo
Ministerstva. kommunallnogo khoziatstva RSFSR, 1948 148
(Road machinery) (Ou 8:83*
A'.

VA-"l--v, 1 4
41 4L 6
"CLami.-es in Qi2 Atorta
4,
I.o 1, Janu r~-11",-!briuar,
the Val-i-isl and ~~Ioro!~,Ury
1)51.., k*; i6mp-~r), Losco*.l.

M
YAROSHIVA, A.A..kandid&t maditainakikh nauk.
Fatal hemorrhages from the aorta and large vessels in cases of
foreign bodies in the esophagus. Vast. oto-rin. 18 no.1:55-57 J&-F
156. OLRA 9:6)
1. Is kafe(try patologichaskoy anatooli (sav.-prof. SM. Krinitakiv)
Rostovskogo-na-Donu maditsinakogo inatitut&.
(ZSOPHAGUS, foreign bodies
c&us ing fatal hemorrh. from aorta & large vessels)
(ACRTA, hemorrh.
caused by foreign bodies of esophagus)
aorta 8~ large vessels. caused by foreign body of esophagus)
(YMBIGN BODIES
esophagus. causing fatal hemorrh. from aorta & large vessels)