SCIENTIFIC ABSTRACT KHODOV, M. P. - KHODSKIY, L. G.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000722120017-9
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 17, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

4/100/60/000/003/002/003
All-Purpose Self-Propelled Tower-Boom Cranes A053Ao26
carrying out from beginning to.end the'entire complex assembly work, starting with
the heavy.elements on low and medium heights and finishing with the comparatively
lighter elements at great heights. They are also easier to be transported and
assembled than tower cranes. Cranes of the class SKG are transported on trailers
in three sections. (Fig. 6) The.tower-boom 6ranes have a Diesel-electric power
equipment with',the possibility of' taking power frouroutside sources. It can be
anticipated that tower-boom craneis will meet with a great demand in-Mture. There
are 6 figures and two tables.
Figure 6: Transportation and assembly of Crane'SK-300,
A) crane in position for RR transportation
al UMM C#W-4*
j!) intermediate platform
with crane
I T n- - - -
Card 3/5

41/_100/60/000/003/002/003
All-Purpose Self-Propelled Tower-Boom Craner, A053/AO26
Figure 6:
C) assembly of crane on supportinsi 0) lifting up of crane by means of
cribs along track tackle blacks
C
'IN
Mom
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All-Purpose Self-Propelled Tower-Boom Cranes A053A026
FiEre 6:
D) crane'in working position with D
40 m boom and 28.9 m beak,
TnK liptia CK-300
a.- xpall a Tva"COOPTOOM no-
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BOLOBAN,, Nikolay Alaknandroirichp kwA. tokbn. nauk,- KHODOV, M.P.v inzh.
red#
[Toohnical obaracterlation cf WWlsie'~W aesembly oranoo of the
U.M.R.] Takhnichoolde kharaktoriatiki otroitel'vo-m=t&sbnykh
kranor SM. Hoakrai"Goa.izd-vo lit-ry po atroit*# arkhit. i stroit.
materialamp 1961. 4~ pe (KIRA 14:6)
1. Akademi-ya otroitellstra i Arkbitektury SWR. Ipatitut organiza-
tbiiq mekhanizataii i takhnicheakcry pmoohohi ot~oitollptvu. E~uro
takhniohaskoy inforaktoU. 2. ,Starshiy nauchnyy sotrudnik Fauchno-
isaledovatellskogo hibtituta arganizatoli, makhanizataii i tekbni-
shchi atobitellotvu Akademii stroitellotva i arkhitak-
'0:~9SPRm(:Oror Boloboin).
t
(Craniont derickat stoo)

SnUSHKOO A.1a.0 inzh.; Enyl-m-d--i
NeV SKG-50 assexUimg crane, Mont. i opets. rab. v strcl. 23
no. 2 s 7-n F l6i, (mu 14 11)
11 QlavGUlfkowt4ndrWdva i Proyektnyy imtitut Prowteal-
komstr4tviya*
(11,ramnp Derrickst Etc,)

SOKOLOVA, Anna Dmitriyevna,, kand. tekhn. naukj KOROBOV, Vikior
Mikhaylovich, inzh.; ~-F4trOVichj,,,inzh-;
Prinimal uchasti7e SIVITSM, Ye.S... inzh.
(Lifting# conveying and tackling equipment for assembling
structural elementsi Pod"emno-transportnoe i takelazhnoe
obDrudovanie dlia montazha stroitellrorkh konstruktsii.
3o izd,, perero Moskvap Stroiizdat) 1964. 326 p.
(11 IRA 18: 3)

OKOHOKOVr A,A., utv. red.; 141ARKIN, A.M.,, otv. red.;
BEILEZOVSaY, V.I.0 x!ed.; DOLGUSHIII, II.I.p red.;
KIRILLOV, L'Ye., red~.j MIKILMM'i MI., red.;
NEVZOROV, L.A.0 red,~; NIKOLAYEVSKIY, G.H., red.;
ROZHDESTVENSKIY, red.; USHAKOV, P.N.p red.;
KIiODOV,_.M.P,.,, red.;-,SHARQNOV, 14.5,) red.
(Regulations for this design and safo operation of load-
lifting cranes) PrPiUla ustroiutya i bezopasnoi ekspluata-
ts1i gruzopod"emnykh, kranov. Moskva, Nedra$ 1965. 127 p.
WIRA 18:7)
1. Russia (1917.- R,;iS.F.S.R.) Gosudarstvennyy koritet po
nadzoru za bezopasMrm 7edeniyem rabot v promyshlennosti i
gornomu, nadzoru.

.MM=r4h+vi POIYASHCIIUKO L.A.
The SM-0 cravler-t)Ve diesal-eloctric crane. Stroi. i dor. masb#
10 no.10:9-11 0 165, (MLRA .18tlo)

L 8220-66 EWVM MA (d)jtWP(j,~jEW0(x AWP(b) WW/JDAM
M0
ACC Nits ~AP5025597 SOURCE CODE:- UR/0129/65AK10/010/0035/006
AUTHOR:. Khodov V.~ V.
TTI-7-)
ORG: none
TITM Hnt_&J]~ 01minizinjuaf V667 alloy
Yqr 5!r'
~heskaya obrabotka metallov, no. 10, 1965, 35-36,
SOURCE: i4et.allovedeniye i termil,
and bottom half of insert facing~p. 24
TOPIC TAGS: high alloy steel, steelp aluminizing, waluminum plating, aluminized
steel, steel-oxidation resistanci.6/EI 867'steel
d%
ABSTRACT: The conditions of hot: dip.aluminizing of VI867 steel have been studied.
After degreasing and oxidizing- ~Oeel specimens werF11_=ersed into a flux bath for
10 min, withdrawn, immersedinto A 7GDC -bot aluminum bath for 30 sec, and, withdrami at
different rates of speed. A ratit! of 50 cm/min yielded the best results and wasused
in the rest of the test. Alumin~lzed specimens were then diffusion annealed at 850 to
1200C. The t6tal thickness of the hluminized layer after diffusion annealing varied
from 150 to 250 V depending on the temperature and the duration of annealing. Surface
porosity was observed in specimens annealed at 850C or 950C, but no porosity was found
in specimens annealed at 1050C O.'r' 1200C. Annealing at 850-950C for 2 hr produced the
highest hardness, 850-930 HV. The most oxidation-resistant part of the aluminized
layer is located at a depth of 75-125 U. Orig. art. has: 3 figures Emd 2 tables.
[NDI
Co-d 1 i=i- 621,785,53:669a4mt~.45

KHODOVP Yelml
Davice for aut=atic alAutronic adjustmeni. of precAaicn pairs.
Priborcutroenie nn..'Allt].8-20 N 164. (MTRk 18~:!)

KHODOVj_T!~,g.,j_inzh#
Technological relationship between the automation of part
macnining and of the assembly of precision units. Vest.
mashinostr. 45 no.8:47-50 Ag 165,
(MIRA 18t12)

a m, p p a A

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124--58-6-6403
Translation from: Referativniry zhurnal, Mekhanika, 1958, Nr 6, p 16 (USSR)
AUTHORS: Polotskiy, 1. G. Khodov, Z. L.
TITLE: Ultrasonic -wave, Propagation Velocity in Some Binary Fluid
Systems and Their Compressibility (Skorost' ul'trazvuka v
nekotorykh dvoynykh zhidkikh sistemakh i ikh szhimayemost')
PERIODICAL: Sb. nauchn. rabot labor. metallofiziki AN UkrSSR, 1954,
Nr 5, pp 34-44
ABSTRACT: Measurements were made of the velocity of sound with an
ultrasonic interferometer at temperatures of 20-500C ~(in the
range of concentration fror.-i 0 to 100%0), and the compressibility
was calculated for a number of binary fluid systems in which
reactions between like molecules differed from those between
unlike molecules. Investigated were the following four systems:
1) a benzene -toluene system in which the forces of reaction be-
tween like molecules were approximately identical with those
of reactions between unlike molecules; 2) an allyl-mustard-oil/
piperidine systera in which the components reacted chemically
amongst themielves; 3) a chloroform/ethyl-ether system in
Card 1 /Z which the forces of reaction between unlike molecules greatly

124-58-6-6403
Ultrasonic-wave Propagation 'Velocity in Some: Binary Fluid (cont. )
exceeded those of reactions between like molecules; 4) a benzene -~ nitrobenzene
system in which the associated component dissociated. In the benzene-toluene
system the compressibility isotherms had a weakly expressed maximum. It
is assumed that this is related to the fact that the reactions between. unlike
molecules were somewhat less vigorous than those between like molecules,
In the berizene -nit robenzene system the speed of sound was a litlear function
of the concentration. , In the chloroform/ethyl- ether system the dependence
on concentration of the speed of sound was likewise nearly linear. The
compressibility isotherms of the allyl-mustard-oil/piperidine system had a
clearly identifiable minimum at temperatures of 25 and 500. The presence of
the minimum was an indication of a powerful reaction between the system
components. The point is made that the study of the Lidiabatic compressibility
of binary fluid systems has made it possible to arrive at certain conclusions
concerning the nature of the interaction between the molecules. Bibliography:
23 references.
1. Ultrasonic radiat,ion--Velocity I. G. Mikhaylov
2. Ultrasonic radiation--Propagation
3. Liquids--Ultrasortic properties. 4. Liquids--Physical properties
Card Z/2

KHODDV, Z.L.; 13NIYBU, T.Ya.
Determination of the opecific electric resistance of the 11262,
RYI aul St.5 steel vewieties in the process of heatin and cooling.
Trudy Inst.chern.mat., vol.8:84-88 154. U% 7:12)
(Steel alloys-Blectric properties) (Ilectric resistance)

. XRODOV, Z. L., PO=KIY.. 1. 0.
"Ultrasonic.Interfer,ometer for Ybasur a at High Temperatures"
VA
an article in the bcok "Questions on the Aysics of Metals and Metal
Science") AB Ukr. SSR, Kiev, 1955, 151 PP-
So: Sum, Do. 1102, 3.9 Oct 56

KHODOV, Z. L. and POLOTSKIv-, I. G.
"Investigation of the Velocity of Ultrasound and Adiabatic Compressibility
for Certain Liquids With Various Characters of the Bond", a paper presented at
the second conference on the Liquid State of Matter., Kiev,, 30 May to 3 June 1955.,
Usp. Fiz. Nauk, April 1955
6

---------- MCIDGIT,
"Ultrasound Velocity in Binary Liquid Alloys. Bi-Cd and BIFb.
paper presentea at the 4th All-Union Conf. on Acomitics, Moscov, 26 IMay Jun 58.

POLOTSKIY, I.G.: BMUYIVA, T.Ya.1 KHODOV, Z.L.
.. I
Effect of alloy elements on the temperature relation of elaoticity
modulus in nickel and nicbrome alloys. Isel. po zharopr. splay,
3:310-324 1 58, (MIR& 11111)
Olickel alloys-Testing) (Elasticity)
(Metals, Effect of temperature on)

_A~
VA-
AUTHORSs Polotskiy, I.G., and Khodov, I.L. 46-4-2-.11/20
TITLSS Ultrasound Velocity*in Liquid Tin-Bismuth AllOY3 and Their
Compressibility kSlcorostl ulltrazvulm v zhIdkIkh splavakh,
olovo-vismut I ikh szhimayemost')
PERIODIG&L; -Akusticheakiy Zhur;ial, 1958, Vol IV, Wr 2, pp 184-186 (USSR)
ABSTR&CT-. Dependence of the ultrasound velocity and adiabatic compressibility
on concentration "to measured In sub-4utectic and trans-autectic
liquid tin-bismuth, alloys at temperatures of 10-1500 above the
malting point. Tho ultrasound velocity and adiabatic cmipressibiliV
were obtained also at 3000C. The adiabatic compressibility was
calculated from th4) ultrasound velocity and the litarature data
on tin-bismuth and-tiheir liquid alioyal.densitiss kReA 6,17). For
certain compositioi%%Saity was calculated by interpolation- The
ultrasound volocitir -vas measured by a pulse method. The t*ethod
used (developed at the Institute of Metal Physics of the Academy
of Sciences of the Ukrainian S.S.R.) differs from that deiscribed
in Refs 2-4 in that the measurements were made by displacement of
the reflector and determination ok the time necessary to travel
Card 1/3
46-4-2.-11/20
.Ultfasound Velocity in Liquid Tia-Bismath Alloys and Their Compressibility
the additional path. To avoid oxidation of the liquid alloys
studied their surface was covered by a layer of paraffin wax.
To improve the contact between the'rod transmitting the ultrasonic
pulses and the 1~q4id alloys, the rod was covered by a thin layer
of paraffin vex. A table on p. .185 gives the measured vulues of
the ultrasound velocity (4, in m/sec, third column of t'ho table)
and adiabatic compressibility ( in 10-12cm2/din, f ourth column)
The firat col-n of the table ge;es the sition in atc~c
per cant of bismuth and the last two columns give pt and )s at 3000C -
A figure on p. 186 shove the ultrasound velocity (two straight lines)
and the compressibility (two slightly convex curves) of 8a-Bi alloys
as a fanction.of composition expressed In atomic per cent of Bi.
With increase of BI content the ultrasound velocity decreages
~linearly and the adiabatio'compressibility increases. For each of
these two quantities a distinct break occurs at the eutectic point,
near 40% Bi. The presence of these breaks indicates structural
changes-in the liquid alloy on transition to the eutectic composition.
At this composition a claasi-eatectic structure -was reported to exist
In liquid phase (Ref 9). Since on Increase of temperature from
3" 3000G the ultrasound velocity and the adiabatic compressibility
the autectic composition alloy do not change, the authoM conclude
Card 2/3 of

POWTSKIT, I.G. Relotalkyip I.H.J; IMODDV, Z.L.;-LXVIN# L-Levin~-H.-
Iffect of oxygen Iopurities and alloying additions an the elastic
properties and Internal friction of chromium Lwith sum=-.r In Englishi.
Ukr. fiz..zhur. 4 no.ltll,6-121 Ja-Y 159. (MIRA MO
19'Institut metalofiziki AN USSR.
. -- (Chromium alloys) (Oxygen)

bOV/46-5-2-12/,34
AUTHORS: Polotskiy, I.G., Taborov, V.P. and Khodov, Z.L.
TITLE#- Apparatus for Measurement of Ultrasound Velocity in Liquid
Metals (Ustanovka dlya izmereni-ya skorosti ul'trazvuka v.
zhidkikh metallakh)
PEUIODICAL: Akusticheskiy zhurnal, 1959, Vol 5, Nr 2, pp 202-205
(USSR)
ABSTRACT: The paper describes a now method of measurement of ultrasound
velocity in liquid metals and alloys. The method is based on
measurement of the time of travel of a short ultrasonic pulse
between a source and a reflector which can be moved about in
the liquid metal. In this way sound velocity can be measured
with an accuracy of 0.3%. The metal was placed in a 30 mm
diameter, 50 mm high heated quartz tube (Pig.1). The
tube was closed from below by a transmitting rod 2 (40 mm
diameter, 110 mn high). A polished hollow quartz reflector
4 was placed in the metal and Its motion was controlled to
within 0.005 mm by a micrometer 5. The molten metal was
covered by a layer of paraffin to prevent oxidation. Good
Card 1/3 contact between the rod 2 and the metal was achieved by

BOV/46-5-2-12/34
Apparatus for Measurement of Ultrasound Velooity in Liquid Motals
placing a thin layor of wax on top of the rod. The rod 2
was excited by a plezo-quartz plate (I No/s workIng frequency)
kopt at a constant tempurature*by means of a wator-cooled
jacket. Pulses reflected from the upper end of the transinit-
ting rod (pulse 2 In F18;3) and from the reflector (pulse
.3 in Fig*3) were displayed on a c.r.o* screen, The
oscillator circuit supplying the quartz plate was based,on a
thyratron TO 0.1/L3 (Fig.5). ~ The apparatus was checked
by measuring sound velocity in water: the value obtained
agreed with 91khaylov's value (Ref.6) to within 0.1%.
Than.the apparatus'was used to measure sound velocities in
liquid tin, bismuth, cadmium and lead at 10 - 150C above
their respective malting_points. The values found were.,
Sn 2454,1/sao at 24700; BI 1663,J./Bec at
28goce ~Gd, e w 2215Atllsea at 33600?, Pb, 0. -- 1634/Y/800
at 34000. The results for Bi, Cd and Pb agree With those
reported by other workers (Refs.1-3). Sound velocity
in Sn differs from the values reported earlier. There
are 5 figures, 1 table and 6 references, of which 2 are
Soviet, 3 English and I translation from English into
Card 2/3 Russian.

SOV/46-5-2-12/34
Ipparatus for Measurement of Ultrasound Velocity in Liquid Metals
ASSOCIATION: Institut metallcifiziki AN USSR Kiyev (Institute of
Metal Physics,, Ac. Sao Ukr.SSR, Kiyev)
SUBMITTED: Ootober 25, 1957
Card 3/3

24(6)9 18(6)
AUTHORS: Polotskiy, I. G. and Khodov, Z. L. SOV/126-7-2-17/39
TITLE: Temperature Dependen'c_e__o_f_tHe--MDftlus of Shear and
Internal Friction of a Few Nickel-Base Alloys
(Temperaturnaya zavisimost' modulya sdviga i
vnutrennego treitiya nekotorykh splavov na nikelevoy
osnove)
PERIODICAL: Fizika Metallov i Metallovedeniye, 1959, Vol 7, Nr 2,'
pp 274-277 (USSIO
ABSTRACT: Within the lafst few years a series of papers has
appeared which is devoted to the study of the modulus
of shear and internal friction of mqtals and_al.loys.
The investigations carried out by 1W (Refs 1 5),
uovic (Refs 6 and 7), Finkel'shteyn (Refs 8 and 9) and
:Fos-unikov (Refs'10 and 11) are of great interest. The
authors of this'paper have investigated the temperature
dependence of the modulus of shear and internal friction,
of nickel-molybdenilm alloys, as well as nicrome with
additions of titanium and aluminium. In this work the
torsional oscillation method has been used. The
Card 1/5 difference betwoen.the method used by the authors and

SOV/126-7-2-17/39
Temperature Dependence of the Modulus of Shear and Interna-l-Priction
of a,Few Nickel-Base Alloys
that described by other investigators (Refs 8-10),consists
in the application of an electronic..measuring device for
he defer
V mination of the period of tortional oscillation.
U
The measurements viere carried out as follows (see Fig 1):-
a beam of light passing through a narrow slit falls on a
mirror, which reflects it onto a screen behind which there
is a photoelectric cell. As the rays pass through the
slit in the screen, a stress impulse forms at the entrance
to the starter me-Dhanism, which is, so~arranged that its
time of action is equal to four periods of tor-sional.
oscillation. During this time the electronic measuring
device counts the number of oscillations of a quartz
generator working at a frequency of 2.5 kilocycles. This
enables the period of torsional oscillation to be
determined with an accuracy of up to a tenth of a. milli-
second. For the determination of the absolute value of the
modulus of shear, the periods of oscillation of-the system
were measured at two different magnitudes of moment of
inertia, corresponding to two different.positions of the
Card 2/5 load on the tortion rod.. The-modulus for nickel alloys at

SOV/126-7-2-17/39
Temperature Dependence of the Modulus of Shear and Intornal Friction
of a Few Nickel-Base Alloys
various temperatures has been wo-vi out. Experimental
nickel-molybdenilm alloys, as well$ nichrome-aluminium
and nichrome-titanium alloys, were made in a high
frequency furnace in an argon atmosphere. The purity of
the raw materials was: nickel - 99.99%, molybdenum - 99.93%5
aluminium 99.95%, titanium - 99.C~6 and chromium - 98.%, .
From each alloy a 500 g ingot was cast. The ingots were
forged into rods of 8 mm diameter, after which they were
drawn into wire of'O.8 mm diameter. The chemical
composition of the nickel alloys investigated is shown
in the Table, p 275. In order to determine the modulus
of shear and internal friction, wire specimens, 0.8 mm
diameter and 330 mm long, were made. All measurements
were taken in vacuum. The alloys were investigated in
the annealed condition. For heat treatment the specimens
P
were sealed in a quartz tilbe, from which air was pumped
out until a vacuum of 10-2 mm Hg col. was attained. The
nickel-molybdenum alloys were given the follow:ing 0
Card 3/5 annealing treatment: the specimens were heated to 1200 0

sov/126-?-2-17/39
Temperature Dependence of -the Modulus of Shear and Internal Friction
of a Few Nickel-Base Alloys
and soaked at this temperature for 48 hours. Alloys of
nichrome containing additions of titanium or alinainium
were heated to 900 C. held there for 5 hours, and cooled
in air. The modulus of shear and internal friction of
each of the investigated alloys were determined using two
specimens, and the period of torsional.oscillation of the
system was measured five times in the temperature range
under investigation. In Fig 2 the temperature dependence
of the modulus of shear and internal friction of nickel-
molybdenum alloys, is shown. In Fig 3 the temperature
dependence of the modulus of slip, internal friction and
Poisson coefficient',of alloys of nichrome and aluminium
or titanium is shown'; 1-'- nichrome + 2.2 at.% Al;
2 - nichrome + 1. 5% a6t Ti;-9- modulus of shear, -- modulus
of internal friction; ---- Poisson coefficient. As a
result of the above experiments, the authors have
arrived at the following conclusions:
1. For the investigated nickel alloyst a deviation of
the temperature dependence of the modulus of shear from
Card 4/5 linearity, and a sharp increase in internal friction,

SOV/126-7-2-17/'39
Temperature Dependence of the Modulus of Shear and Internz-0. Friction
of a Few Nickel-Base Alloys
occur in the same temperature range and are probably due
to elastic imperfections and, more Important, to plastic
s'ip along the grain boundaries.
-L
2. The Poisson coofficient for nichrome con8aining 2.5% Ti
,begins to increase noticeably at 400 to 500 0, which may
be associated with a considerable increase in plasticity
of this alloy.
There are 3 figures, I table and 12 references, 6 of which
are Soviet, 6 English.
ASSOCIATION: Institut metal,lofiziki AN Ukr.SSR (Institute of Metal
Physics, Ac. Sc., Ukr. SSR)
SUBMITTED: April 16, 1957
Card 5/5

25576
ILI I S/18SJ60/005/002/01:L/022
D274/D304
AUTHORS: Khodovq Z.L* and 111chenko, V.I.
-----------
TITLE: Temperature dependence of Young's modulus ani of
the damping idecrement~of Nichrome alloys with
tungsten and molybdenum admixtures
PERIODICAL: Ukrayinslkyy fizychnyy.zhurnal, v. 5, no. 2, 1960,
235-239
TEXT: The influence of tungsten and molybdenum admixtures on
Young's modulus and the internal friction of Nichrome alloys is
studied, as well as their temperature dependence. For determining
Young's modulus and the damping decrement, a device was used (de-
signed at the Institute of Metalphysics) which permits determining
very accurately the frequency of.the natural oscillations of the
specimen and the number of oscillations for which the amplitude is
reduced by half; the elasticity modulus and the danping decrement
were calculated on this basis. Graphs are given where the obtained
time-dependences are plotted. For Ni-Cr-W alloys, an increase in
Card 1/3

Temperature dependence...
2q 6
S/18X5D, 60/AR~002/011/022
D274 D304
tungsten content from 0.6 to 2.86 at A leads to an increase of the
elasticity modulus over a temperature range of 20 to 8000C. The
damping decrements for these alloys vary little from room tempera-
ture to 500-5500C, but a further increase in temperature leads to
a sharp rise in the damping decrement. For Ni-Cr-Mo alloys, con-
taining 0.97 and 3.25 at A Mo, the elasticity modulus has nearly
the sane value; the alloy with 6.44 at A Mo has the smallest modu-
lus. The relationships for the damping decrement of these alloys
are similar to those for Ni-Cr-W. The observed sharp rise in the
damping decrement is apparently due to viscous slip along the grain
boundaries. From the obtained temperature dependences of the elas-
ticity modulus, the temperature coefficients-were computed graphic-
ally; the temperature coefficients differ very little from each
other for all the investigated alloys at the same temperature. It
is noted that the alloycontaining 15.94 at A Cr and 3.25 at A ho
has an elasticity modulus nearly equal (for the entire interval) to
the modulus of the alloy containing 16.48 at A tungsten; this value
of the elasticity modulus is the largest of all the investigated
values. The relationships obtained between the modulus and the
Card 2/3

25576
S/185J60/003/002/011/022
Temperature dependence... D274/D304
molybdenum and (respectively),tungeten content lesd to the conclu-
sion that these admixtures have a similar effect on Ni-Cr alloys,
(at any rate for small admixtures of the third element, up to
3 at A). There are 5 figures, 2 tables and 4 Soviet-bloc refer-
ences,
ASSOCIATION: Instytut metalofizyky AN USSR (Institute of Metal-
physics AS UkrSSR)
SUBMITTED: July 8, 1959
Card 3/3

27957
S/185Z60/005/004/019/021
D274/D306
AUTHOR: Khodov, Z.L.
TITLE: Ultrasound velocity in binary metal-alloy systems
of eutectic. type and their elastic properties
PERIODICAL: Ukrayins1kyy fizychnyy zhurnal, v. 5, no. 4, 1960,
574-576
TMM The results are given of an experimental study of the depen-
dence of ultrasound velocity on concentration in binary, liquid,
metal-systems of eutectic type. The following alloy systems were
measured: bismuth-lead, bismuth-tin, bismuth-cadmium, lead-tin, lead-
cadmium and tin-cadmium. The velocity of ultrasound was measured by
a special pulse-apparatus. From the velocity and from density data
(taken from literature), the factor of adiabatic compressibility and
the reciprocal magnitudes - the bulk moduli, were determined, It
was established that for the systems bismuth-tin and bismuth--lead,
Card 1/4

Ultrasound velocity...
27957
S/185/60/005/004/019/021
D274/D306
the bulk modulus is a linear function of the concentration. For the
system bismuth-cadmium, the factor of adiabatic compressibility is
a linear function of the concentration. The isotherms of the bulk
modulus, as well as those 'of the factor of adiabatic compressibility
are nearly linear for the system lead-tin and cadmium-lead. In the
ideal case, the velocity of ultrasound in an alloy is expres.,3ed by
MI 2 M2 2
a2 = Cl ~ al + C2 7- a2
M
(2)
where a and a are the velocities of ultrasound in the components:
M, and A2 are Le atomic weights; cl and C2 are the concentrations.
For the velocity of ultrasound in an emulsion one obtains:
a2 (E101 " '~2k) 1(-"IF1 + F-2f2y
where P, and P2 are.the factors of adiabatic compressibility of
the components, P 1 and 2 are the densities, and E 1 and F-2 are
the bulk concentrations. The obtained experimental results were
Card 2/4
27957
S/18 60/005/004/019/021
Ultrasound velocity... D274YD306
compared xrith the theoretical curves obtAnc,d from ~01'!IliuIlc.!" .(Z,) arC
(3). For all the systems, with the exception of bismut'll-cadmiur"
the experimental data agree with the.values obtained from formula
(2). For the system bismuth-cadmium, the experitaental values agree
with those obtained from formula (3). If small volume chaR,~Cs
accompany the formation of the alloys, it follows from Eq. 6) that
the bulk modulus depends linearly on the bulk concentration, whereas
formula (3) was obtained on the assumption of lincar dependence of
factor of adiabatic compressibility on bulk concentration. It can
be assumed that the presence of a high degree of short-range order
affects~the changes in elal;tic properties of liquid alloys, render-
ing them (in this respect) similar to emulsions. If this assumption Y
is accepted, the obtained result cap. be explained by the fact that V,
the system bismuth-cadmium,should have,' in the liquid state, a high
degree of short-range order. Evident ly, this high degree of short-
range order is preserved over a wide temperature range. This was
confirmed by A.k. Regell and F. Gabdullayev (Ref- 11: ZWE', 19-57,
27t 9, 1956). Since the solubility of lead and of tin in bismuth is
Card 3/4

85970
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2 Q. b I JWW W62 1-IN-7 E032/E414
AUTHOR: Khodov, Z,L.
'~~~%sonic Waves in Melts of Binary
TITLEi Velocity of Ultr
Metallic Systems,of the Eutectic Type and Their Elastic
Properties
--- 49
PERIODICAL: Fizika metallov i metallovedeniye, 1960, Vol.10, No,5,
pp-772-779
TEXT: The aim of the present work was to investigate the
concentration dependence of the velocity of ultrasonic waves in
binary liquid metal systems of the eutectic type. For some of
the systems the concentration dependence of the coefficient of
adiabatic compressibility was also determined. Measurements were
carried out on the following binary alloys: tin-lead, tin.-bismuth,
tin-cadmium,,lead-bismuth, lead-cadmium. and bismuth-cadmium.
The present work is a development of previous investigations
reported by the present author in Ref.5 and 6. The velocity of
the ultrasonic waves was measured with the pulse apparatus
described in Ref.11 and built at the Institute of Physics of Metals,
AS UkrSSR.' The velocity of' ultrasonic waves in tfie four basic --
metals used in this investigation is given in the following tablei
Card 1/5

85970
S/126/60/010/005/022/030-
E032/9414
Velocity of Ultrasonic Waves in Melts of Binary Metallic Systems
of the Eutectic Type and Their Elastic Properties
Metal: TemlI~erature, *C Velocity of the
ultrasonic waves,
m/sec.-
Sn 243 2466
-FG- .,,I
344 1826
331 2223
Bi 289 1666
The values obtained are in.good agreement with measurements
carried out by other authors,& The variation of the velocity of
ultrasonic waves with temperature was found to be 0.2 m/sec dog
for tin and 0.3 m/sec deg for lead. No noticeable change in the
velocity of ultrasonic waves in bismuth with temperature was found
in the region 289 to 356%. The velocity of U~trasonic waires in
alloys was'measured at temperatures close to the liquidus
temperature and also at higher temperatures. Fig.1 to 6 show the
Card 2/5

85970
S/126/60/010/005/022/030
E032/E414
Velocity of Ultrasonic Waves in Melts of Binary Metallic. Syiste ms
of the Rutectic Type and Their Elastic Properties
isotherms of the velocity of ultrasonic waves in.the above ioystems.
These curves were then used to calculate the coefficient of
adiabatic compressibility using the-well known formula
a2p
where a is the velocity of' ultrasonic waves and is the
density of the alloy. Fig.7 to 10 show the isotherms of the
adiabatic compressibility (0) and the bulk modulus W. It was
found that the velocity of ultrasonic waves in the majority of
these alloys can be represented by the following formula.:
a2 = c MI a2 + c M2 a2 (3)
1 2 2
Card 3/5

85970
S/126/6o/olO/005/022/030
'Velocity of Ultrasonic Waves in Melts of Binary Metallic Syistems of
the Butectic Type and Their Blastic.Properties
where al and a2 are the velocities of ultrasonic waves in the
two components respectivelyl Ml and M2 are the atomic weights
of the components and el. and C2 are the atomic concentrations.
R in given by R = ClMl + 02M2. The bulk modulus on the other
hand depends linearly on tho concentration. InIthe case of.a high
degree of short-range order (the' Di-Cd system), the velocity of
ultrasonic waves Is given by
a2 = - 1 .1 1 (4)
('IP1 " '2P2) ('-1p1 :+ 2P2
where P and P2 are the densities of the components,
P d ~2 are their adiabatic compressibilities and e1 and E2
taeira~jlvolume concentrations. In such cases the adiabatic
compressibility in a linear function of the volume concentration.
Card

85970
5/126/6o/oio/oo5/O22/030
9032/9414
Velocity of Ultrasonic Waves in Melts of Binary Metallic Systems.of
the Eutectic Type and Their Elastic Properties
If the elastic properties of the tiro components are not very
different, then the velocity of ultrasonic waves can be calculated
from either of the above two formulae. Themp are 10 figures,
I table and 27 referencest ILB Soviot and 94ye-Soviet (one of w Ihich
is translated into Russian),$
ASSOCIATION: Institut metalJLofizik:L AN USSR
(Institute of Physics of Metals AS UkrSSR)
SUBMITTED: March 8, 196o
Card 5/5

20268
5/180/61/000/002/008/012
h1b, 9071/035
AUTHORSs Polotskiy, I.Q., Beniyeva, T.Ta., Khadov, 42.L. and
TITLEt The Influence of AllvoyinS an Some.Physical
Characteristics of Chromium and Nickel-Chromium Alloys
PBRIODICAL: Izvestiya Ak&dsmil. nauk SSSR, Otdoleniye tekhnicheskikh
nauk, Metallurgiya, i toplivo, 19611 No.2, pp.108-114
TEXTs The relations govering changes in the elastic properties
of alloys were studied in ordq,r to investigate the influence of
some factors on the strength cof interatomic bonds. The,influence
of the composition, teMperature and plastic deformation on the
elastic properties of siolid evolutions of transition elements was
investigated. In addition, non-alastic properties for nickel-
based Alloys wore.also'studied. The influence of tungsten and iron
on the elastic properties of Chromium, as well as of tungsten and
nely~odenun on the elastic and,non-slantic properties of nichrome,
and the influence of plastic deformation on the elastic propertiox
of nichrome were investigated, Determination of the elastic
Card 1/14

20268
B/180/61/000/002/008/012
.'.The Influence of 9071/9435
properties of chromium and its alloys was carried out on
ultrasonic impulse apparatus described by I,G.Polotakiy and
T.Ye.Stefanovich (Ref.1) and the Young modulus and the damping
decrement at elevated t I*mporatures on an apparatus doseribed by
I.G.Polotakiy and V,F,7'aborov (Ref.2). Cbromium-based alloys,
containing up to 13-05% of turkgoten and up to 3.11% of iron, were
used for the investigations. Chromium and its alloys were
prepared from electrolytic chromium by smelting and casting in a
high vacuo. The cast chromium was about 99.9% purity.
Experimental chromium-tungeteu alloys were smelted in a high-
frequency furnace in an argon atmosphere. Nickel-based alloys
Ni-Al, Ni-Cr-Mos Ni-Cr--W wore smelted in a high-frequency furnace
in a vacuo. The purity of the starting materials was as follows.*
Cr - 99.9%, Nil- 99.99%. W -- 99495% and Mo- 99.9%. The
chemical composition oir the alloys investigated in g1ven in wt.%
in the table ( OCT - robot). The Toung modulus 'and the damping
decrement were measured on polished specimens in the form of rods
7 mm in diameter and 2,00 mm long. During heat treatment the
specimens were sealed in a quartz tube from which air had been
evacuated (10-4 mm Hg). Chromium and Cr-Fe, Cr-W alloys were
Card 2114

s/i8o/61/000/002/oo8/012
The Influence of ... 9071/E435
heated to 1100% and retained at this temperature for 3 hours.
Determination of the temperaturo dependence of the Young modulus
was carried out in vacuo., In iorder to preserve approximately the
same grain size of nickel alloyis, the following heat tretatment was
useds nichrome alloys with various additions of tungston in the
form of 12 mm semis were heated to 9000C for 4 hours and, after
producing the specimen, akt 900'4'. for I hour; nichrome alloys with
molybdenum additions in the forn of 12 mm semis were annealed at
900% for 2 hours and tho sp*cinens made from these were
annealed at 900% for I hour,, After polishing, the specimens were
ann*aied at 800*C in vacuo for 40 minutes. Coolingafter
annealing was dono with the furnace. Determination of the velocity
of propagation of longitudinal and transverse sonic waves in
chromium (99.9%) enabled calculating the Young modulus, the shear
modulus, Poisson's coefficient sind the modulus compression from all
sides for specimens of electrolytic chromium (Z = 27540 kg/mm2,
6 or 11150 kg/MM2, p w 0.24 and K w 17100 kg/mm2)'. The
experimental results are given in graphs as followst concentration
and temperature dependence of the elastic modulus for chromium
Card 3/14

20268
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The Influence of ... Z071/E435
alloys (Fig.l)l temperature dopendonce of the Young Imodulus for
Ni-Al alloys (Fig.2)1 temperature dependence of the Young modulus
(continuous lines) and the damping decrement (broken lines) for
nichrome with various additions of tungsten (a) and molybdenum,(b)
(Fig.3). Since changes in the elastic properties of metals and
alloys after cold plastic defornation have been little studied,
the authors investigated this influence on Ni-Cr alloys
(Ni + lo.48 &t.% Cr, Ni + 23.46 at.% Cr and Ni + 28.13 at.% Cr).
In order to establish general relationships, copper of 99.9% purity
was studied first. Determination of the elastic characteristic
was done on the basis of changes in the velocity of propagation of
longitudinal and transverse sound traves in the initial and deformed.
states in the direction or deforming stresses and perpendicular to
this direction. . The accuracy of the moaaurenients was about 0.1%,
All specimens were investigated in the annealed state. Ni-Cr
alloys were deformed in a,60 ton press by uniaxial compression,
The degree of deformation var*ed from 0 to 60%. The experimental
results for copper are shown in Fig.4. The magnitude of' the
elasticity modulus of copper chai-,iges depending on the direction and
Card 4/14

~20268
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The Influence of 3071/E435
degree of plastic deformation. In the direction of applied
stresses for up to 9% of plastio deformation the Young modulus
decreasesj then remains oonstant to up to about 12% and-with
further increase of plastic deformation it decreases linearly,
The elasticity modulus intho direction perpendicular to the
direction of applied stresses decreases more sharply up to about
9% of the plastic deformation, then remains practically unchanged
up to 20% of deformation and reaches a constant value on increasing
the degree of deformation to 57%, At a deformation above 10%
the differenca in the value of the elasticity modulus in two
perpendicular directions in probably related to a steady formation
of the texture which is characteristic for this form of
deformation. The influence of a low temperature annealing (100,
200t 3000 400 and 500%) on the elastic proportion of copper
submitted to plastic deformation of 25 to 57% wag; also studied.
The results (Fig.3) indicite that the temperature of the beginning
of recrystallization is l*w*r at higher degrees of deformation,
e.g. for a 57% deformed copper specimen an increase in tbe
elasticity modulus was observed already at 200% while for less
deformed specimens no change in the Young modulus was- observed at
Card 5,A4

20268
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The Influence of ... 9071/9435
this temperature. The vlue ofithe Young modulus of nickel
alloys (Fig.6) also chang:s depending on the direction of applied
stresses and the degree of deformation, whereupon a larger
decrease of elastic properties was observed for alloys than for
copper. It is pointed oxxt thatin nickel alloys, the influence
of.plastic deformation on the deiDrease of the modulus of
elasticity increases with increasing concentration of chromium.
The latter is possibly caused by-the fact that in Ni-Cr alloys
in addition to the formatton of texture widecrease of elasticity
takes place due to the deAitruction of the K-state, formed during
the thermal treatment of alloys. The following conclusions are
arrived at. 1) An increase in the elasticity moduli on
additions of tungsten to chromium and a decrease in the Young
modulus for Cr-Fe alloys within a, wide range or temperatures
indicates that tungsten in, binary, Cr-W alloys slightly strengthens
interatomic bonds, while an addition of iron to.chromium Leads to
weakening of the latter. 2) The temperature dependence of the
Young modulus for nickel alloy& containing 1.1 to 5-0 atAt of
aluminium in the ferromagnetic temperature range is .of the same
character as for pure nickel but with increasing concentration of
Card 6/14

20268
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The Influence of ...
E071/E435
aluminium the curves of the temperature dependence begin to
flatten out. Additions of aluminium have a slowing effect on the
decrease in the Young modulus at elevated temperatures (.1500 to 800*C)
and thus aluminium counteracts the weakening of'Ni-Al alloys.
3) With increasing concentration of tungstenlin nichrome (from
o.6o to 2.86 at.% w) the absolute value of the Young modulus-for
Ni-Cr-W alloys increases and its higher value is retained for
alloys with a higher concentration of tungsten in.the whole
temperature range investigated (20 to 700*C)- With increasing
concentration of molybdenum from 0.97 to 6.44 at.%, the elasticity
modulus for Ni-Cr-Mo alloys changes little. Therefore, the above
alloys can be Onssified into a'single group, as their Young
moduli are basically determined by.the elasticity moduli of
nichrome. 4) The curves of the,temperature dependence of the
damping decrement for nichrome with various concentrations of
tungsten and molybdenum have the same character but for ailloys with
a lower concentration of'the above elements a sharp increase in the
damping decrement was observed at lower temperatures, The latter
isapparently caused by elastic.imperfections and in the first
instance by viscous slipping along the grain boundaries. There
Card 7/14

0 N H
w
m'. Cr N1
0.04 0.04 O.M.11 OCT.*
0.04 O,ml '1.02 OCT.
0.04 0.04 0.0(9-1 3.11 om
2.08 om
13.05 om
Ocr. 90.99
0.5D OCT.
2.37 OCT.,
- 0 t0 1.6 HAS VCT.
0: 50 5.3 14. t0 ou.
0. t5 0.3 14.63 oer.,
1.90 - 12 So OCT.
5.00 - 14:00 OCT.
8.60 -14.01 0~7.
20268
S/180/61/000/002/008/012
The Influence of E071/E435
are 6 figures, 1 table and 16 r~ ef6rences: 12 Soviet and
4 non-Soviet.
SUBMITTED: June 1, 1960
Table

20268
S/180/61/000/002/008-/012
The Influence of E071/E435
Fig-1. Concentration (a,6 And temperature (B),dependences of
elasticity.moduli of chromium alloys. 2 1
Fig.la - Young modulus of Cr-W alloys, E x 10-3 kg/mm Vs Wat.%;
Fig.16 - shear modulus of Cr-W al:Lo'ys, G x 10-3 kg/mm2 vs W,at.%;
Fig.1B - the influence of the temj)erature on the Young modulus of
the alloys, E x 1o-3 kg/mm!2. va t,'C. I - Cr + 0.13 at.% 0;
2 Cr 1.0 at.% Fe; 3'- Cr 2.9 at.% Fe.
I., IN, 4"1 Up 40C
Card.9/14.

20268
S/180/61/000/002/008/012
The Influence of ... E071/E435
Fig.2. Temperature dependence of the Young modulus for Ni-Al
alloys. E x 10-3 kg/mmA'l vs t,,Oc
I Ni; 2 Ni + 1.1 at ~P-Vv Al;3 Ni -P 5 at.% Al.

20268
s/lBo/61/000/002/008/012.
The Influence of,,O,,, E071/E435
Fig.3 Temperature'd opend'ence of the Young modulus,(continuous
linesi and damping de crement (brolken lines) for nichrome with
various.additions of tungsten Qig.,3a) and molybdenum (Fig-36)
1 - 0.6 at.% Wj 2 - 1.152 at.%'W; 3 2.86 at.% w;
4 - 0,,97 at.% Mol 5 3.25 at.% Mol 6 6.44 at.% Mo.

- 1
S4 -1
~

20 -

11 '41
0
614
1.
let? 48it 600 9.0c
P UO IWO 690 Oc
Card 11/14 OHr. 3.

20268
s/18061/000/002/008/012
The Influence of ... E071/E435
Fig.4. Influence of the degree of plastic deformation Of
copper on the velocity of propagation of ultrasonic vibrations (a)$
on.the change of the Young modulus and Poissonicoef;icient, in
fit It
the direction of the application of stress (V,,VVI~ 0I and in
the perpendicular direction (
V* V� E-L, II.L)
AT wV04 ION
OL

20268
s/i8o/61/000/002/oo8/m
The Influence of ... E07l/B435
Fir,.5. Influence of the~annealing temperature on changes'in
the Young modulus of copper subjected to deformation
25.6%; 2, 40-3%; .~3 57.0%
w log Joe 400 t. -C
Card 13/14

20268
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The... Influence of ... E071/E435
FiS.6. The influence of the degiree of plastic deformation,
of Ni-Cr alloys on the velocity of propagation of supersonic
vibrations (Fig.6a and B)~;and changes of the Young modulus
(Fig. 6 49 in the d1rection of stress (V" vt% Et') and in the
x yl
direct perpendicular to the'direction of.ap;lication of stresal
(v-xLv-L,E-L) Fis.6a,B NJ. + 10. 48 a t Cr; Fig. Ni + 28.13 at.%
y
Cr
JJ
St
$
U. 7r~~
Joex 11 10,
%
Card.1

L 36111-66 SWT(l)/8WT(M)/EWPtk)_AAWPA) RTY T.IPIC) WJH
ACC NRi A?6017306 (_/V SWILL CODI~: ' UR/0126/66/02176-63/072776731
j,.UT!:O-.-',.S: Polots G.; Ovsiyonko, D. Yo.- Khodov Z. L.; Sosnina) Ye. I.;
kiy4 I
Ba-.olyuk, G. Ya.; Kush9r, V. T*_
0"!(;: Institute of Matal Physics AN UkrSSII (InacituL inatallofiziki UkrSWi)
TITLE: Influence of ultrasound 'on -the degroo of perfection of singlo cryuLals of
Alum-inum, pgrown from the melt IVA
SUURGE:;Lika mutallov i motallovudoniyo, v, 21, no, 5. 1966, 727-731
TOKC TAGS: aluminum, metal crystal, metal crystallization, ultrasonic effect#
ultrasonic Irradiation, single crystal
IOSTIULCT: The effect of an ultraVnic field tin the degree of perfection of aluminum
cr%ysGals grown from the melt was studied. 1.'he study supplcmonts the results of
3. Laneenecker (Phys. Rev. Letters, 1965, 111) 221). The eyperimontal procedure
conrAsted of subjecting a crystallizing alw.31.nuin i,,iult 6o the action of an ultrasonic
icIa (sco Fig. 1). The 'structure of singlo crystala of aluminum derived from the
cdt- alth and without the action of the ultrasorde field was studied by means of
(,ollblc x-ray reflection (Yo, 1. Sosp~ina L. I. 'MoloshIcu, and D. Ye. Ovsiyen~oe
lsvledovaniye nesovershonstv Icristallichosko-o strayoniya, Kiyov, izd. Nauchnaya
1965, str. 1.22) and bor round abs .orption and etching techniques. The. oxperimen
Lal romiIL3 are presontErd graphically (suo Fig, 2). Thu' application of an ultrasonic
UDC: 669.172:621-7892:516.621

A& NR.
S
8%-
APW1730~ in b

Fig. lo Apparatus for growLtk
of single crystals~ in an
ultrasonic field. 1 - graphite
~ ave
crucible, 2 - metal stock,
- single crystalline smIj
3 4000 -

- tube furnace., quarlz SM
tube, 6 - vibrator, 7 - concentrator, IM -
B - inner thermocouple., 9 .. outer
thermocoupla, 10 molten autectic
Bi Cd, 62 a A
an Q9 min I
91
'3 FiC. 2. Curves for double
A refloction from a single
crystal of aluminum. a- -
to diffujilon
to di before ultrasonic truat-

-*
FlM ment; b - after ultra-
-
tp q1tra- sordo treatment in the
tp
.9
.sonialgenerator solid phaise,
t
field to -i grairing aluminum crystal causen a considerable disorientation of the
subgrains in the lattero It is suWouted thRt the disorientation off oct is caused
%the2ttZIe0nssanCS6&tkI the ultrttsonic fiold in the growing crystals, Orig, art,
FB I ARE: 19Jtul65/ IgrORM REF: 004/ OTH REPt 002
ks SU 1'

PANKOVA, R.A.; VQPQX&A ~D.N.; GORYUSHXINA, I.A.
Study an the survival, of dysentery microbes in dryed feces In
transportation under the condAtions of Northern Caucasus. Zhur.
mikrobiol.; epid. i iimmn. 41:no*6,.133-134 Je 164.
(MIU 18-1)
1. Dorozhnaya sanitarno-epideiaiologicheskaya stantsiya Severo-
Kavkazskoy zheleznoy dorogi.

'OORYUSHKINA, I.A.; KHODOVA, D.N.,
Some simplification of the Uthodology for determining the
nanvitIvIty of microbem to oulfanllamides. Iab. delo no.32
178-179''165. (MIRA 18:~)
1. laboratoriya d9rozhnoy sanitarno-epidemiologicheakoy stantaii
Sev-erp-Kavkamakoy zheloznoy dorogi (nachallnik V.S. Krivtsov).

XBOPOVAO Noy prepodavatell
Vftdor-the motto *Love-bhe beauUful.0 Obehobeety. pit. no.3338
Mr 163. (KMA 16s 6)
I* Ivanoveldy tekbh1han obobbbestvennogo pitaniya,
-(Rootaurante,p luncbrcow,, *to.-Vocational
guidance)

XIAODOVA 0
V&W Neftelm - Mosquitoes Urd Nests mey/Jun 49
ONA I t4l" W""Dg or,wds for HOVIto" (Mobotows) 'A P4 J4 F9tr$ahchmj,
T. Tt Oubalo A.,, T~ Toyloebal)wvi 14 %~ 02*kboi*qpa# K* N Solmloyao Oj U xh5dovav
A~ Bit GazParm Div of Famaltol aid Ikd Zoali lost of Zp1damlol and HicrobtAg
AW Y*d Sol pp
WAOCII zhuro So 3
zov utig" n3 nestaliof nine upeolem of bWsi OM IWW 0AY tUbt vmW120A
avld of mosquitoenj ra these eUbb nests I'qml alzbt Urn# 25 Ma# a zea 136
~Awaa indliating that nests wv not cr~.ke of aoj*, Crequently used brooding pliAC634
Dlr WV of Parealtol and Sod Z-xav Mad To. A~ ~P&Iviovakly~ Dirt UBt ~Of
Womai am ml~ftbiaa rrof Y. D. TIMov.,

ANMSOV, Y.Z.; KARAVASMVA, A.I.; LAPIDUS, S.S*; MIDDOVA, O.Ta._
Control of flies in i1tock pavilions at the All-Union Agri-
oultgral fthibition. Vaterinarfla 32 no,5t?2 RY 155.'
(FLI193)(DISIMOTIONIND DISIMOTANTS) (Km 8:7)

ZKONA,
Infinitesimal clavelfication of second order curves in L:ibachavskil's
piano* uche gap, ],van* goo* pod, inste 10:45-34 156. (XLRL 10: 4)
(Game-try. Non-Duclidean)

10SHXIN, XoLe, prof. IDLINA, A.G., kandemed.naukv ROTTMAN, T.A., IMODOVA, 14t.
DUDCKWO, I.I.
Effect of BUY-16 lulps on children of kindergarten age (with
summAry in Ingliehh, Pedintrits 36 no.6t67-73 Jo 158 (HDU 11t6)
1. Is kafedry obehihey gigiYonY Khar1kovskogo meditsinskoigo
instituta I Kharlkov,skogo oblastnogo doma robenka No.l.
(UIMVIOIRT RATS, off,
Indirect, on Mild developm (Run))
(ANTIS]CPTSIS AND ASEPSIS,
ultramiolet iTradiation in prov. of serogenic infect.
In schools (Rixe))
(AIR, microbiology,,
ultrayiolet prev, of aerogenic infect. in schools (RUB))

YAMPOLISKIY,, S.M. lAmpollalkyi* S.M.).p prof.; VENGEROVSKIY, Ye 0. NenherovalkAo
IE.O.],, vrach; ABER, S.Ya., dotsentj SHELUDIKO, Ye.i. [SheludIko., IE.Ij,
vrach; YJIODOVAO R.Z.9 vrach
----------------
In memory of O.M.Fedotova. Pod., akush. i gin. 23 no.6:34 161.
(MIFUL 15:4)
(FEDOTOVA, OLENA lffKUILIVNA, 1884-196o)

ALIKOV,, Stanislav Petrovich; LUBSONj Mark'Genrikhovich,- 92PY-ETst-
--kavel loag?jt0; SAV3 NA, Z.A.p vedushchiy red.1 POLOSINAp
AeSo-j-ii-kbnorede
(Increasing oil recovoryj S~"alin oil vorkers' practice]
Intensifikateiia dobychi. raefti; opyt eakhalinskikh neftianikov.
Moskvaj Gos*naucbno-Ukhnizd-dro nefto I gorno-+,oplivnoi lit-ryp
1961. 71 P. (MIU 24t6)
(Sakhalin-Oil fields-Production methods)

43409
s/o5l/62/013/005/015/017
E039/E420
iAUTHORS: Aleksandrov, Yo.B., Khodovoy, V.A.
TITLE;, The detection of the IKP-iiotope by means of the
optical orientation of atoms
PERIODICAL: Optika i spekt:roskopi,)ra,'v.l3,,no-5, 1962, 751-752
TEXT: In this method the paramagnetic resonance is detected by
a change in optical absorption in the medium. It has betan used
previotaly in the case of alkali metali at vapour pressures of
'~- 10- mat Hg and less. The detection of Knu in the natural
isotopic mixture of potassium by means of paramagnetic resonance
between Zeeman components of the hyperfine structure of the basic
state in the Earth's field, was shown to lae impossible. Thitowas
because of the signal to noise ratio and the faft that.the K
is orientated only by collision with atoms,of Vl and K394
An increase in the X40 content by raising the temperature of the
.resonance vessel In precluded as the vapour then becomes opaque
to resonanc radiation. This dIfficulty is overcome by
allowing th: K40 Atoms to make collisions with optically
orientated atoms of sodiuca'vapour. In this case the resonance
Card.1/2 4

S/051/62/013/005/015/017
The detection of the K40 isotope E039/E420
vessel contains potassium with a Na admixture and argon as a
buffer gas. In order to increase the relaxation time the walls
of the resonance vessel are coated, with sicosane. At 1800C the
optimum pressure of Na vapour is attained (.r-10-5 mm fig), Th
~potassium vapour pressure to then - 10-2- inm lig and hence the K90
vapour pressure is - 1016,:mm fig. As a result of collisions with
the Na.atoms the K atomea6quire some orientation and as the
number of Na atoms transmitting their orientation to K atoms
increases the tranamission,of the vapour with respect to sodium V~
light decreases. The arrangement of the apparatus is similar to
that of H. G. Dehmelt W. Phy3. raci., 19, 1958, 866). In a
magnetic field of 0.34 gauss, three resonance signals were
obseryed: the first at 238 Uc/8 corresponds to the resonance for
Na, 01, K39 and probably R07 with a signal td noise ratio I
S = 4 x 103; the second at~ 158 Kc/s corresponds to Rb85 present
as an impurity and the third at 107 Kc/s is the K40 resonance with
Sf'v5. The possibilities,of thisi method for the detection and
determination of small concentrations of one alkali metal or an
isotope in another are not'exhausted. Abstractor's note:
SUBMITTED: May 14, 1962 [Abridged translationj
-Card 2/2

/014/OD6/0823
2714 3/0051/63 JM3
Iso; Bilj'-'~ Inhod %.-A.,
AUTROM Aleksandrovi
TIM: P.Wwrding the D"Oui 2iorilaiint
J-1
SOURCE; Optika i spOktrosko'Oa 823
ins At- mo. 6,1963 j,
ThPiDd TAM: para~xagnetic rieIaI6bande, totical* 0 tation, spin relaxation,
optical pumping
)mTnCT:- -H, G. Dahmelt (Fnyi~
x 10,50, 14870 1957) carried out an experimient
on deternining tbe,relaxationAime,of, Wita, atom in-the cess ofloptical
, I- .0 Ant pro ,
--orientation* -The-presemt attbora .~uiAivn Dqbmeltfs erpretation and analysis
of his experimental results.-',.Dehmelt 'Utribuled the appearance of the absorption
signal to inversion of the kminetic Mold; the Whors assert that the absorption,
is determined by tho_pro)>abi3Aties-for..opt*oal-transi+,ions-that do not depend on
.."Ahe--energy -of the atom in field. -- Accordingly the absorption
Ashould not change with field i~iersiontl -The authors repeated the Delmelt experic,
ment with particular attentiontto the il6lation between the residual field and the
rate of reversal of the main field. , Stray. fields were thoroughly compensatede
The-orientation was realized- 14- rubidium -vapor.- No_, ~h ange intranspaxency-of the- -
-Card 1/1
2
V; 1114;ck-
--- - ------

ALEKSANDROV, Ye.B.; BONCH-MUYEVICII, A.M.; KHODOVOYP V.A.
SPin exchange. Izv. AN SSSR. Ser. fiz. 27 no.8sl070-1077 Ag
163. k-'MIRA, 16:10)

T
ACCESSION Nki 4P3007069
326, 1 A was d a t 0 r- t e d b y ''a h 6 t tou 11 tl I i e r'4 7T h a rf'magnetiti:fteld
030 k c), we a establish d'b 11119poid surroundin the'vessel" wi tb.,,
additlonal--vo tion.4 :high volt' e a ii
%uclad'- byl -4 3 0-ovp.6 ag
i ch we s us e d as. . the _bias C--vol tij`~ f or- ~,the -a yn ch ronou a -- do t e- c t o r 9
-The- constant magnetic f ie id il ed by~ a system of Helmholtz
was mpos
rings4 This f i Ield was _slouly-varl6d :to. obtain the rve
resonance vu
The excited state of the-C ..Yapor,,vas split into a Zeeman tr iplet,
f and the. intensity of sc~at~i re 1 Et -was, modul.ated b- the. frequency
~ _;;o 1-1-1 - ~!. y
i th e rf Uleld and~into n y. :The ex-
0 'les_oU that freque
gr 1 i,iiu e
tent~of *modulati n nd tb6l!'
0 a men )teniity.of lumines.cente i;howed
r :e~ of theJrequencies of a-com-
resonant maxima when-the f, e
ponents was an integral multiple of the rf modulation frequency.
A possible combination of-the effects-ofiresonance scatterlIng of
modulated light and paramatric re:ionance:was indicated. When the
modulation frequencies of the field 'and the light do not coincide
the intensity of scattered :'light %U~l Contain combinetion harmonleg.,
Orig.,art. has- 5 fitures"fand-22 tfb
ASSOCIATION: Opticheskiy 'institut; 1n. -S' I Vavilova (Insi1tute of
SUBMTTTED: Ac
-680otO df
Q
RV 001 05
LV

ACCESSXON NR% AP4012561 6/0056/64/046/00l/033l/M8
AMOR: 1%R_dRY0_Y_t V. A.
TITLEs "Parametric resonance" in luminescence as a many-photon pro-
cess
SOURCE: Zhurnal ekspei. i teoret. fiz., v. 46, no. 1, 1964., 331-338
TOPIC TAGS: luminescence, parametric resonance, many photon pro-
cesses, modulation of atom luminescencee optical photon, radio fre-
quency photon, atomic level spacing,
ABSTRACTt It is shown that t1he prccess defined as parametric reso-
nance in luminescence and described by Ye. B. Aleksandrov et al_
MEW., v. 415, 503, 1963) can, be regarded as a process in wirj=h one
optical and seversl radio-fr,equo,ncy.phqtone,participate simultane-.
.ously. A qualitative analysis shows that the many-photon transi-
tions can lead to a constant phase difference between excited states,
and that the various processes occurring in parametric resonance can
Card 1/2

ACCESSION NRt AP4012561
be described in terms of the~absorption and emission of fixecl num-
bers of photons. An appr-oxidate thitoretical analysis of the pheno
menon is also presented. Th(q similarity between many-photon process-
es in radiation and-frequenc~r modulation of~'the radiation of an atom
with the aid of the Stark and.zeeman effects is also pointed out. "I
am grat4=:Wr the opportunitj ',,to -thank Ye. B. Alelcsandrov for con-
tinuous aid, and also 0. V. 116notantinov and V. 1. Perell for useful
discussions." Orig. art. haof 3 figures and 15 formulas...
ASSOCIATION: None
SUMITTEDs 24Jun63 DATE ACov 26Peb64 ENCLi 00
SUB CODEt PH'~ 110. UP VOV,# 003 OTIM& 0013
cord 2/2'

AUMWU=p YO*B#lt, Nffp ~.A~
lbtte" to the edito". Opto i spektr. 19 no#6tM .& 165.
(MIFA 18832)

~7 F 'i
A_W(AtOANK
AP6001660 SOURCE CODE: UR/OD51/65/019/006/0982/0984
qq
AMOR: Aleksandrovs Ye. -E-;A~onch-Bru vich,-A.-M.; Kostin N. W A.
I
ORG., none
TITLE: Stimulated Raman sca'ttiliring in 4 selective resonator
SOURCE: Optika I spektroskopiy~a, v. 194 'no. 6, 1965, 982-984
..TOPIC TAGS: laser,.Xaman scatt ,Orfng, 910,~zulated emission, loser cavity, Raman
laser
ABSTRACT: The stimulated, Ravahl' -WAO-Invea -at- -axel tation-po4er.-
-three A tigat -ed - air-
__above t e
-the-follo ing
t reshold using - Ifferent setups: 1) A Raman
cell In the resonator of a lasers; 2)-a longitudinal selective resonator (the term-
used by the authors for the casia when tfie Raman- laser ator is in the direction,
of the ruby laser resonator); ai 3)a trani0verse selectil -onator (the term used for
the case when the/Raman laser r4! .zsonatorls rotated 90* from the direction-of the
axis of the rubyMasei, i.e., a'~;90* off-4xis Raman laser resonator). In the first
setup the. gl7an-Evulses were.prouced by:.a' ruby crystal. Using two vatiable-trans-
mission-coef f teient f Ilters (tri.ansmissien' coefficient 30-50% at X -.694 mv) the
effe~:tive intensity of the 30-100 neec-,4uration pulses in the resonator reached
100 Mwt1/cM7- The maximum energ: ~ per pulse was 3-4 J. Two dielectric mirrors with
a transmission coefficient of 044% at X w~694 up, 0.8% at A 745 mo (the fundamental
2

:-L 107
~7
_~ACC
'~CC
SRS line in benzene) 40% at mpi (f irst harmonic) and 70% at A~- 875 m
SRS
'e a
(second harmonic).w6re.,used in~~!'the xp ~~1mpnts. The SRS in benzene had thresholds
for a specified length of the n,celt (1) and the loser Input power. No SRS
Itama
was observed at I < 2; however~ SRS was;6table or 5 < I < 60 cm. The threshold
ppv;er dec-ressed almost-linear with. incl'keasing 1- At 1 -60 cm the efficiency of
e _convvrsio:~~- reacbed.1OZ-4of-the-powe r Ln---the-cavi -was
Mergy A -- - - - xy_-~=It~ -observed that
--i lltii~ ___ - -
-ast - 8 t ~"isebJi~ 1- 5 -2 fi A6
667 Incre .~the i p owthi ruby mes ve the
tbreshold-res*Ulted in a three--~irderlndt~ase In SRS* In tN,-longitudinal selective
setup the'additional reflector',~I_etweenihe ruby rod and the Raman cell had a trans-
mission coefficient Of 902 atJ"al 694 m0 10% at A'- 745 v, and 1% at:) - 805 and
875-mij. ln.tilkig mode of, .operatlon thelo;ficiency of energy conversion was at least
as high as that in the previoum case. 'rIii* higher harmonies at A - 745 and 805 mp
which reached saturation at ul(IZ of the'Input power were observed. Results similar
to those.of the longibAlnbi, setur. were ai,;Meved with a transverse selectlvesetup. tbwever,
SRS was achieved Ina Raman cell the le2gth of which along the laser beam was only
I cm. Stimulated Brillouin sce1tering ~Ln benzene was also observed in this setup.
-art----ha __TCST
r-Ig4
SUMM DATV I Ap If. 0TH REF: 004/ ATD PRESSt,~
CODE: 20 5
CWd
2122f

J.- 102424 6 -FWAWr IMEWPWA ; WT.(m )LEE &aA (h) .1 T
e(04LT&_qP(k)ja_A(m)-2 -7P(
Acc N14 AP6=197 MA)II --,souRacoDE.- UR/0056/65/0119)1005/1435/1444
-AUMOR.- Aleksandrov*s B* Ik~nch r #Mich
Ye. A. M.. Xost1n. N. Modovoy, V.- A.
OHO: none
TITLE: Investigation of Stimulated: Dam h and Brillouin scattering in.selective
resonators
SOURCE: Zhurnal eksperimentall6by 1-tedreticheakoy fiziki, v. h9, no. 5, 1965,
1435-14h4
A -
TOPIC TAGS: -laser, second, barTonic nontinear optics, RWM'scatterinEo,
scattering, AxAah#,-;+a4_ -
01
AWTHACTot The'stimulated Hamm: scatterlDig was investigated at an excitation power
just above the threshold using $he _ follc4on'g three different setups: - l1) a Raman
cell In-tbe resonator of a laser,, 2) a lOngitudinal s ive resonator (the term
used-by the.. t ors ~for the ca&6 when t1jo Raman jasex--wonator is in the direction
of the ru Cl'eqr resonator); aj6d 3) a i,iransverne selective resonator [the term used
for the case when the Raman laser resong&,or Is rotated 90* from the direction of the.
axis of the ruby laser, i.e., 4,*900 off-iWo Raman laser resonator] (see Fig. 1).
In the first setup (Fig. Is) th~, 'giant pAlses were produced by a ruby crystal 10 to
12 ca-long and 12-16 mm in dift~eter. VRth two vartable-tranaminsion.-coefl'icient
filters (transmission coefficient 10-8(6 at A 6943 1) the effective intensity of
1/4

I ALMON Rdz%n .1
j_jQL4Z-66
CC Nat
Ap6ooo197
2
the 20-200 neec-4uratlon puloi~s In thCresonator renched 100 M/cm Thm maximum
energy,per pulse was 5-4 J. 'Two dlele6~.ric mirrors 01 and 02 with a~ transmivs1on
coefficient or O.h% at A = 694 :'~Mjj, o..8%~~at A.= 745 mij (the fundamental SPS line In
benzene), and,40% at A 805 mO (the ffiot.barmontc) were used in the experiments.
The.sensitivity of the detectoj~ro was suificient to regiater 10 -11 or the energy of the
laser pulse. The setup shown i,n Fig. iwwas used to investigate SRS in benzene. 11.
was observed that an increase in the-enirgy of,the pulses from the ruby laser 1.5-2
a': three
times above the threshold resulted in -order increase in SRS at the funda- -
mental frequency. Saturatioh*VLa -s r eacht .d when the intensity of SRS w6n about 100. of
rgy Input, at t6 sec;'~ ~ a h
the ene which 0*a armonic whose energy output quickly----
~V -_ - a-f-44t-urati6h -appeared.
----reached -the-1,6vel of-SHS-at-th*-fund=6~_'t f
-1- ..47 req ency
sity -of
When-, the second harmonic reachod- saturatlon- the- duration and -the inte'n -the
laaer-pulues decreased itharply ~"6e to'tlt~vi, reverse effect of SRS on thi% ruby laser
When the length of the~]R an 6.
pulses. am ~ ciltdi (1) was increased, the threshold power
and the pulse energy required't6 achievt~~SRS decreased. Also, the larger the cell,
the smaller the energy above th6 thresh(~~ld at whichsecond harmonics vere generated.
The SRS was stable when 1.vaa-*'~tvee~- 5114nd 60 cm . :In the longitudinal selective
s
UP-(Fig. 10 reflector 02.reolacedAil'and ent Of-03
et the transmission doeffic!l was
very hAgb at x 694 mij and was; at a miziirm at A = 745 mp. The gain.of SRS at,
I = 5, 20, and 60 cm was at iealis't as b4l, as in.the previous case, although the pump
power and the pulse energy required,werticonsiderably smaller. For example, when the
output of a ruby laser pulse of~ 0 nsecl,~Auration van hO-Mv (I = 20 cm) -three 10 Mw
3
SRS pulses of-20 nsec duration 4ere obsiij.4ved in the ]Raman laser cell. Similar re-.
Card -3/4

TITLEt Multiphoton proceenes
'iuk:- :v 5, not
-SOURCE: '-Uspeklii-- fizicheskikh-MA, 4 1965s 3-6h
qiinntuz
-pr
laser effect, nonlinear procets, frec.,tency conversion. harm.-~n_c ;7-n-
eration, Raman scattering, parametric resonance
4 sections. Th,E! f i rs t
T"encen--are Soviet. Th-e --reVi-ev- 147~_ diviliflis &At6 - 3 -
section is devoted to the bas,; e theoi*v of reultiphoton procec-9 -9
to a general re,riev of experiiiento poy-formed in this f--e~ -
second section demls with mul-;iphoton processes not requiri.---
sideration of the interferenco effec';i-_ Afi!iannlysis Is
multiphoton tranultinno betve..-n Zeeraioi sublevels of 9,)diu-
in a rotating f'Leld and,in a rield applied in any arnitrary
.An anal7ais is iande of txo-photon abnorption in C&F, doped w;
2,
A
&
'a 14 k"M 0006.~ PM41, 'RA-Z WN Vrr
Usk M MM --y'R ~5 WN
- Mal

SW
.4
2721.8 6 (3) 1~1?(a G_G_1w
7-
AkTjM 8 1',Wwx CODE: uW6,10616610031c) 2 29
T~,
Bonch-BEWevicb, At Koatini. ~41. W. Xb?qgrM,,L# A.
AMORI:
none
Aesonawt birefr ence tbi eUttriio*field of a light wave-
LIN
ISOURCE i Zhurnal eksper i'teoriltichesk4 fizW. Platma Y redaktiliyu.
_~.Pjrllozheniye., Y. 3,, no. n, 1966j~ .42
TOPIC TAGS: potassium~ dofole r on -application, resonance absorptionp
laser
~Ligbt absorptioil
ABSTRACT: -The authors observed tbo. ocour~ence -of. birefringence: in potassium vapor
--under the-influenc7e-of -the' eieAilc field~of, ruby laseremission by passing simul-
teneously light from a potftssium~~ft'and~ from. a ru* laser through a vessel con-
taining saturated potassium vapo6i at ioC,i, At this temperature., the *19or absorbi~d
approximately %)%.of the resonant,! light ft,'om the 1smp. When the laser piase was'
applied (20 nsee duration) a cl"
.0,, ear-cut aJ.Lgml was observedjs indicating an increase
in the resonant radiation from the lw* pimsing through the vessel. At a laser
emission power density of the ord br of 5 blw/crf the amplitude of the sl(;nal corres.
ponded-to transmission of aevera1,'_,t1ipes_t~'pa_,per-- cent ot--the-intenBity-oJ!---tbe--light----
sie igni'll -was _&avrved -Vben 4he - lamp- radiatiori- and --laser
miss-16-n--e-lentl7ric fields Vere at lk 45$ wvlee' There was no signal vhen this angle
was 0 or 90** There van likewise~,no signal vhen the potass~vm vapor in the vessel
Card 1/2

L 27
ACC NR, AP6
OIT698
was frozen out., when the potass wao.turned off., or when the filters used to
larize the Ught were removed. -,Ihe,latter, together with the de enderice of the
P
0 ~P
signal on the angle between the electric 4ictorsj,4roves that the observed effect
is.due to bireftingence indtu~d lt~~ the la,66r. pulse because the shift of the ab'sorp-
tion. line in the laser--emiss-ion electric fLeld has different values when. the elec;-
tric'vector of.the light ls'para3jel and.p"arpeinlicular to thevector of the laser,
The value of this line shift is c4culated:and,the wavelength dependence.of the
laser emission intensity required 'to obtain a signal of prescribed magnitude is mea-
sured and found to be linear in.the ,vavelej~b 'difference between the reeonant transi-4
7b il
'tion and the laser emission. i ~ av"s irith the theoretical calculationa& The
authors thwik-,V. M. Zakharova emd.W. A.: V~).Obs;L of IGU for the opportimity to
the
measure the line contour wit the yparalun, am Ye. B. Aleksandrov for help and
a discussion. Orle. arta. has: 3 figures sad 1 formus,
-SUB-CODE6.----2D/ K61 (M RzFt--- 1~31 OTH-WO. W1
T-C M
Q4

L_ !21967-66 EWT(1) 132(c)
WCC NRIAP6002883 SOURCE CODE: UR/0286/65/000/0'- 4/0041/0041
2
INVENTOR: Aleksandrov., Ye. B.; Bonch-Bruyevich, A, M.; Yhodqvoy., V.A.;
ORG: none
TITLE; Method of measuring the modulus ahd direction of the vector
of force of weak magnetic fields Class 21,, Mo. 176976
SOURCE: Byulleten' izobre .t~,~Y:l movarnylch znakov,, no. 24, 1965, 41
TOPIC TAGS: magnetic field measuriamentj vector, weak magnetic field,
magnetic field intens paramagnetism.. measurement
ABSTRACT: The method otAmeasuring the modulus 'and direction of the
vector of force of weak Magnetic flLelds based on the optic orien-
tation of atoms, i i-rizedUy tri fact that the effect of the
.action of 'he measured magnetic field and of the known light intensity'i
on the paramagnetic atoms is compared and the magnetic field strength
is determined by the intensity of the orienting light. The0e charac -
teristics are incorporated in order to widen the measurement rang e of
weak magnetic fields,.-.
SUB CODE: 20/ SuBm I)ATE: 1 .*~Apr64 A;

SOUROB
ACC NRI AP70076811 UR/0386/66/M/06/0*/60i~i
AUTHORS Aleksan V, as 0 Bonch-Bryevich, As M.;! Kostin, No No; Khodov V&-- A.
.ORG: State "Order of Lenin" Institute of Optics im. So I. Vavilov (Gosularstvennyy
OHena Lenina Opticheskiy institut.)
TMEt. Freq-aency shift of optical transition in theifield of a light wwre
41" 1 1 i
SOURCE., Zhurnal kaperimentalln6y:J teoreticheokoy fiziki. Fis1ma v redaktsiyu, v. 3P
no. 2o 1966, 854;
TOPIC TAGS: optid transition.- rub~i laserp photomultiplier, optic filter resonance
line, laser pulsatlon., niagnetia field intenitity., light absorption/FS-7 filter., KS-19
bl-eaching filter
ABSTRAM The a4hors experimentally investigated the frequency shift of' the optical
resonant transitiqn 4S, 01/2 3,/2 of potassium (principal doublet). It can be
~P,shown that, theexpec6ed frequen*cy shiA of this transition is connected principallyl
wMi.virtual tran4ition induced bythe lasw pulse from the ground level (01/2
Q1?2,3/~) and the excited level (4P3/2 /Ao The first pair of transitions is
sti l,sufficiently far from the resonances 11W transition wavelengths are 766~ and
7699 A, that of thIe lasqr is 6943 A)- The 4P3/? - 651/2 transition is much closer
to resonance OL - ~939 A)- In spite of thiop all these transitions make comparable
contributions to the~sought frequency shift of the investigated transitionp owlng-to~l
the difference in the oscillator strengths. It is inportant that the ground and
UDC: none
Lclr4-11-L

ACC NR1 AP7007681 1'
excited,levels are shifted here byAhe rubjr-laser light in opposite directions.
In the. e,xperiment ilight from potassium lamp 1 was seed through vessel 2 with
P?4"i= vapor 'saiturated at 100*0, (see tho figurer. At the selected temperature,
the-,v~apor absorbed about 80% of the lampts resonant radiation. Transmission of
light by vessel 2 was expected to increase during the action of the pulse from laser
3,, -provided the resultant transition frecpxincy shift is conuensurate with the line
width of the lamp hdiation (it was assumed that this line was broader than the
absorption line 0 he vapor), The transmission of the resonant light was recorded
with a hotomat or whose output was fed to a pulsed oscilloscope (4 glass
ip~
filters
1 ~4
c
4 AMP,, ter
A r..-A 2 IL

Acic -NRI AP70D?681.
s
~The scattered la r light in the registrationchanhel-waa reliably cut out with FS-7
~
als
fIlters. ., F~elimi airy experiments.have shown, however, that the laser pule -eo is
5c
-accompanied by 5c tered radiation with spectral components lying inthe region of
.the registered assium line. 7be authorB used a special method of filtoring the
it
resonant line wit the aid of the Taraday taffect to tombat ihe mechanism of radiation,
te
occurrence. Aft pasAng through vesseI2, the light beam of the potassium lamp
5
was made to pass hrough an*auxiliary cuvette 6 filled with potassium vapor and place
between crossed P) aro a 5. A local magnotic field of approximately 2 We was
4pplied to cuvett) 6. The magnetic field produced, besides splitting of the absorp-
tion line, strong radiation of the,plane or polarization of the light, but only in
the nearest iicinLty of optical reisonance. By magnetic field intensity selection,
the-system was maoe to transmit alrost all the resonant line, and to absorb the
extraneous light -The entire appW-,atus behaves like a high-transmission optical
Ifilter with a bandwidth on the* ordor of 0.1 cai-1. Under the, conditions described,
'&,distinct. signal was, recordedp evidencing a decrease in the absorption of the
,-resonant light by,.the potassium attvns in vessel 2 during the time of action of the
TAder'puls'e (20,40och the laser operated in the monopulse mode by using bleaching
ft1ters- KS-19. lfo' verify that the change in the light absorption was not, co nn'ected
*ith some experim6nt.al errors the authore checked: (1) that the signal vanished
when -the p'ot~asiuin, light was turned off; (2) that the signal vanished when the potas-,,,-7.
sium-yapor was frozen out in vessel,2 (*ith the 411,11mination on the photamultipli'e"
I
,maintalred Wthhe'previous'level); and (3) that the'signal vanished when the oparatin~
i~qde of lamp wa~ forced.so as to broaden the emission line (the broadening was
MP
confirmed _by th ~e. ~eervatione). 7he viinima laser radiation power densit-,V. at which
y the.
Card 3A

------------
ACC NR& AP?OD76BI
th6'~Uaching sigral was produced was -10 Iq(/CM2 correaponding to an electric field
Lght of 105 V/cme The half-width of the spectral emission line
is estimated att.
x
1.0 cps, so.that the observed shift van of the same orders
T14 gixth6re thavik Ao Godina for providbig the high grade polaroidea, Orig. art,.
haas Vrormula An I figure$
SUB W09t, 20 bM UTEz., 30*ov65 OHM IUW t, 001
OMI W: OD3

KHMMAHDV,, G*U.,--dotsent; VOWTSOVA.. Z.I.v nauebmn sotrudnik
Mearratione on opantions for tramplanting Stensents duct into
the conjunctiwa owrity in 3*ropbtha3.mia* Oft.zhur. 16 no,69345~-
347 161. (M"RA 14tlO)
1. lw.Daohkirokogo i2auabno-looledorateltakogo trakhomatozn.ogo
instituta (direktor - H.S. 7anatarova).
'(CONMMVA) (CONJUNTIVITIS) (PAROTID GIJ")

BUREYKO, V.S., kand.tekhn.nattk; GRINs-JITEyN
lnzh. M*R,op inzh,.l KHODSKAY-A. R.1.,
SOMe PrOblems of 'he technology of produoing agloporite from
c3AY raw material. Sbor.trud.VNIINSM no.68159-166 162.
1. Nauchno-issledovatbleskiy :Lnstitut stroitellnykh(MM .15212)
soveta. narodno kh materlalov
C 50 MaYstvil Belorusskoy SSR.
(Aggregates (Building materials))

MMBORODDY M A., (Besbarodsup M*A.It akademik; K,HOD,SKIT~I.L,*_Gol-,[Khodakip loflojg
A'oi&rt'1,m 6f ko~rilf"A12C~ glass.' Testist AN'BSSR.' Bero-fix-tokh.
rJav, nootw-W 159-0 Oam i3t3)
1. -AN ~BSBR.
(Glass)

B/081/61/000/012/019/C)26
B110/B216
AUTHORS: Bezborodov, M. A., KhodBkiy, L. G.
TITLE: Lead phosphate enamels for aluminum
PERIODICAL: Referativnyy zhurnal. 1(himiya, no. 12, 1961, 396, abstract
12K374 (12K374)(11,9b. nauohn. rabot. In-t obahch. i
neorgan. khimii AN BSSR", 1960, no. it 72-83)
TEXT; The authors studied the range of compositions of the system
K20 + PbO + Al203 + B203 + P2O,j characterized by low softening point
(414-4250C) high thermal expan;iion coefficient (132-156.3-10- 7) and
resistance to boiling water with a view to preparing enamels suitable for
aluminum. The following property changes with composition were determined
for this system: Thermal expaneiion, density, and temperature at which
softening begins. A series of white enamels with properties rendering
them suitable for decorative coatings ivere prepared on the basis of a
glass of the composition (in mole%): K 20 - 20; PbO - 30; Al 2 03 ' 15;
B203 ' 10; P2 05 , 25- [Abstraoter,s note: Complete translation.]
Card 1/1

BMBDRDWV, N.A.; KHODSKIT,.L,,G. ~
Glasses of.the system ~20 - PbO - Al 0 - B 0 -P 0 as a base for
2 3 2 ) 2 5
enamels on aluminum. Dokl,AN SSSR 4 no.3:116-119 Mr 160.
(MIRk 13-6)
(Glass) (Enamels and enameling)

KHODOWY, L. G., CAND'TecH Sai, OF THE
VITREOUS SYSTEM K 0-P60-Al 0 -B 0 P 0
2 ~ 2 3 2 3- 2 5 AS 1W BASES -itr
e***e**- FOR ALLUMINUM," MINSX9 1961. (BELORUSSIAN PCILYTECH
INST GHAIR OF -IECHNI)LOGY 00ULAGS). (KL-UV9 11-611, 223).

L 06490-67., EWT(m)/EWP 0) WH
XC NRt 28303 R_'CE'_CODEi Ijk/
'6
AUTHORt ?-I t yov M -A "ki L. 0. ~Fisyuk 0. K.; Bolutonko, As L; ~5'
ve
Strugachp
ORG: Insti-tute of
(Institut obshchoy i neorga-
TITLEt Some properties of glasses based on the systems BaO-=2-B~(~p B&04024205p
BaO-TiOZ-SiO2
SOURCES AN SSSRo Izvestiya. Noorganichaskiye matorialy, vo 2p no. 6, 1966v 1119-
1123
tOPIC TAGS: borato glass3' phosphate glass, silicate-glass# titanium dioxide
AJISTRACT: Glasses of the systems IkO-Ti%.~B BaO-TiO2-P205 and BaO-TiO2-SiO2 wore
synthesized'from barium carbonatep -im-Onium monohydrogen phosphatev boric acid, ti-
tahium dioxide and quartz sand by violting at 1300-1400*Cp and the properties of the 1
glasses were measured on annealed crylindrical specimens. The dependence of the volume'
electrical resistivityp tomporature of the start of softenings chemical stability (to
boiling in distilled water), donsity, and microhardnoss on the composition was moas-
ureds, and the crystallizability wats determined from tests in a gradient furnace and
from thermographic studies. Titan',Lum was shown to decreaso the electrical resist
of the glassesp particularly when A is present in a lower oxidation state.
1/2 UDCI 539.213
ACC
not more than on& comp
Studied; in 5 ound Is fOrmed during t
ilicate glasses# bariwa silicot,j he 0I:U"IUUUPn of the glasses
14W-melting glasses with a high el tanate Bao.Ti,, .
thGsized, and Oatrical resistiit, SiO2 crystaulzes..out
'were found to h -h ohr
5 figures and 2 tables, "atisfaCtorr chomic 10 4 cm) were syn'
SIB CODES 11/ -.UBH al StabIlity* (~,igo art, h& ;S
DAMS 28jur,65/ oRG RFV, 013/ OTH REFS 003

KHODITKIII, 1,. 1. ; YHOZITISXIJ'~ 1. 1. ; GuLAMOVA, V.. p.
"Experienoe in making cultures of the measles virus.:,
Report submitted at the l3th All-Union Congress of Hygienists,
L'pidemiologists and Infectionists. 1959