SCIENTIFIC ABSTRACT YAROSLAVSKIY, A.P. - YAROSLAVSKIY, N.YE.
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Collection:
Document Number (FOIA) /ESDN (CREST):
CIA-RDP86-00513R001962210011-8
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RIF
Original Classification:
S
Document Page Count:
100
Document Creation Date:
November 2, 2016
Document Release Date:
September 1, 2001
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11
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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A, P.
Role of cerebral cortex in mwdfasUtions of vestibular reflexas.
Vast-tt*ftolar. 1224p jnIY-Aus. 50. p. 10-2
1. Of the LOR (Otor!dn*Ur7ngc)Agic&l) CLUde (H*M--Howred
Worker in Solence Prof. K. L, nilov)) LenbWmd Swdt&M4bXtwdc
Medical Institute.
cum 19,9 50 Nov.,, 19,00
YAROSIAVSKIY,'A,.P. (Vyborg)
PINOMT,
- Unusual fore~p-bcdrof the Pharynx. Valt.oto-rin. 18 no.--'..-128
S-O"'i*36. ~"- (KLRA 9: 11)
OURM-YORNIGN BODIES)
I
Name: YAROSIAVSKIT, A. P.
Dissertation: Study of the effective action of certain drugs on the
degree :f manifestation of vestibulovegetative reflexes
Degree: Cand Med Sci
MiD Ik-alth P.SFSR, Leningrad Sanitatton and Hygiene Medical
Inst
Date,, Place: 1956, I/eningrad
Source: &-j-izhnava Let-pols', Wo 2, 1957
E N D
USJPRS/DC
DUPONT 7-424o
. . . . . .......... .- - - - - - - - - -
............
YAROSLAVSKIY, A.P., Cand Med Sci -- (diss) 11 Study of
effectiveness ofAaction of certain pharmacological
preparations7on the degree of pronouncement of the
vestibulovegetative rellexes." Len 1958 12 pp. (min
ofW ealth RSF5R- Len Sanitary HygienL-I Med Inst)
100 copies (KL, 39-58, 112)
77
YAROSL KIY. A.P. (Vyborg)
The influence of autonomic poisons on the intensity off autonomic
vestibular reflexes [with summary in EnglishJ. Yest.oto-rin.
20 no-5:32-36 S-0 158 (MMA 11:12)
(?,FMRIIM. eff act a
on degree & chnracteriatics of autonomic vestibular
reflexes (Rua))
(BESERPM. eff ect a
same (Rue))
(YESTOULAR APPARATUS, effect of drugs on
ephedrine & reserpine on degree & characteristics of
autonomic veatibulor reflexes (Rue))
YAROSLAVS A.Pe
(Vyborg)
Labyrinthine cormlinntions following intra-ruiral adnimistration of
cocaine solution. Vest.oto-rin 20 n0-5:112 S-0 158 (MrRA 11:12)
(LABYROTH,
cauand by iritrn-ttural oocol.no Infuaion (Rua))
(COGAIM11, inj* eff.
labyrintLne lesiona after intra-aural infusion (Rua))
-P
YAROSLAYSKIY, AsPe, R=Tq LoYao (Vyborg).
Free skin graft myringoplasty with the aid of Kolokoltsev's glues'
[with summary In Zngllsh]~ Veste*oto-rint 20 no.6-.36-38 N-D 138
(MIRA 11:32)
(BAR, MIDDIR. surg;
myringoplasty, free skin grrft using KolokoltsevIs
glue (Rus))
(SKIN, TRANSPLANTATION,
.same (Rua))
3,
asilum
YARGSIAVSKIY, A.F.t kandmed. nauk (g.Vyborg)
Penic:Ulln treatnent of paratonsUlary abscesses* Zhure usbop
nos. i gorl. bol. 23 no-067 Jl-Ag'63. (KIRA 16:10)
(TONSIIS ABSCESS) (PENICIIL-RI)
YAROSLAVSKIY, G.T.
The OML-12 and IML-7 macbines for cleaning and Insulating
large-dlameter pipes. Biul.tekh.--ekon.inform. no-7:
62-65 16o. (MIRA 13:7)
(Pipe--Cleaning) (Pipe-0jorrosion)
YAROSIAVSKIY, L. -Iand -1EV, -A. Yii-.
"Criteria for Evaluating Tone-Telegraphy Systems," Vest. Svyazi, I;o.4. 1954
Translation M-644, 26 Jul 55
Assistant Professor, Odessa Electrical Engineering ftat Communication InBt.
RZ-1.
4-
N'
3
YAROSLA.VSKIT L.I.- YAKHINSON, B.I.
31~tablishment of frequency at the out-put of an ideal
narrow-band filter with phase-frequency modalation.
Radiotekhnika 15 no.7:44-50 J1 160. (KM 13:7)
1. Daystvitellnyye chlemy naucbno-tekhnicheskDgo Obahchestva
radiotekhniki i elektroBVazi im. A.S.Popova.
(39lectric filters)
ff ff-MME."Llm
BOSYY, Nikolay Dmitriyevich, kand. tekhn. nauk. Prinimal uchastiye
BYKHOVSKIY, Ya.L., kand. tekhn. nauk; Y L*I.,
A-2-
kand. teklm. nauk; TKACHRIKO, L.N.p in .., red.izd-va;
BEREZOVYY, VA.., tekhn, red.
[commnication channels) Kanaly sviazi. Kiev Gostekhiz-
dat USSR, 1963. 391 P. WRA 16-12)
(Information tbeory) (Telecommmication)
A-'
T-v
SVERDLOV, M.P.; YETRIJKH114,, 11. N L.To ZUBOVSKIY,
L.I,-, WROV, V.S., TARAKAIJOVA, M.S.; ctv. red.: DATRAKOVA,
T.A~p red.
(New TT-17P and OTX--2S vo-ice frequency telegraphy apparatus
using transistor devl,~6s] Novaia apparatura tonallnogo te-
legrafirovanila na pol-aprovodrilkovykh pribcrakh TT-17P i
OTT--2S," infonnal.s4.:m-aT-; sborn`.k. M-,,skva, Svlazl, 1965. 125 P.
(MIlU 19:7)
ACC NRi AP7004659 SOURCE CODE: UR/OWI/~66-/00000i/005-1-/0052---I
sciences)
(Candidate
S.;'.Yaroalavskiy,
of technical
L. r.
AUTHOR: Usov, 1.
ORG: none
TITLE: Device for measuring pulse noise and interruptions in telephone channels
with variable integration time
SOURCE: Mekhanizatsiya I avtomatizataiya upravleniya, no. 1, 1966, 51-52
TOPIC TAGS: telephone equipment, electronic test equipment, noise analyzer
CV/)J/17r - 0-11 (Hr--C?AJ CJqrj&) X) E A-
ABSTRACT: A device for measuring pulse noise and short-term interruptions in
telephone channels used for voice-frequency carrier telegraphy and data transmission
in the 300-3400 cps frequency range is described. The portable device, developed in
the Kiev branch of the Central Scientific Research Institute of Communications, is
designed for general field use. It operates by generating pulses whose number is
proportional to the integrated value of the input pulse noise or interruption. Some
characteristics of the device are: input power range, 2105 2 5.105 and
2:106 2 2-106 nw; range'of short-tern interruptions, 1.5-3.5 neper; integration time,
0.5-5 msec;accuracy of the integration time, 5Z; input impedance, 600 ohm or more
than 7 kohm; maximum counting speedp 2000 cps; power consumption, 30 w; input
voltage, 110/127/220 v ('13Z) at 50 cps; operating temperature, 5-40C; size,
UM 621o391.17
ACC NRt AP7002669
~AUTHQR: Yaroslavalkiyp Lo P.
SOURCE COD3s--lft~/6'169/67'/012/ool/oll3/0114
iORG: none
:TITLE: Distribution of combined phase of a Bum of angle-modulated oinUBoidal signal
band narrow Gaussian noise
!SOURCE: Radiotekhnika i elektronika, v. 12, no. 1, 1967, 113-114
TOPIC TAG!-. signal reception, signal noise separation
ABSTRACT: J. Salz and S. Steinfs general formulas for distribution of combined phase
of a Bum of arbitrary-modulated signal and narrow-band noise (IEEE Trans., 1964,
IT-10, 4, 273) are too complicated for practical use. The present short note
proves that if the signal is only angle-modulated (no AM), Bimplor formulas can be
deduced from S. 0. Rice's results (BSTJ, 1948, 2-7, 1, 109). The distribution and mean
frequency 16rTor formulas are derived. Orig. art. has: 13 formulas.
SUB CODE: 09 SUBM DATE: 29Apr66 ORIG REFs 001 / OTH REF: 002
Card 1
Mgs 621,391.8226~
-Ll- 49
L 3oo4-66 :','WT(d)1FSS-2
ACCESSION NR: AP5020887 UR10106165100010081006210068
621.397-1:621-391.164-7
MUM: Lebedev, D. 8~.; YaroulavskV L. P
TITIX s. Eff icioncy of some methods of facsimile transmission
SOURCE: Elektrosvyazi, no. 8, 1965, 62-68
TOPIC TAGSt facsizile transmission
ABSTRACT: The AM, PCM with and without correcting codes, and bl-orthogonal-Bignal
methods of facsimile transmission are considered.Assuming certain characteristics
of the human eye (vision) and a constant-parimotor channelf the mini= signal-to-
noise ratio corresponding to still Invisible distortion-cauBed by a&utive
normal white noise Is evaluated. This table is reportedt
J__
C -to-noise average power
Here; A. is the signal
Method
At
AP
AMI
CAAt
ratio; C r. Ig
..
.
AM . . . . . .
I
I
~ nal
power and noise power#
and P aro the sig
P
s n
7-digit pCM 2.7 7 3.5 respectively. The table shown that the AM method
8-digit PCM requires a channel with the lowest traffic
(Wagner). 4,5 6 3,2 capacity (last column).
Bi-orthogon
2
.64
6,5
signals ~
Theenergy efficianc:y of-the bi-orthogonal method iB found to be 0-0285 and that
I of the AM methods 0,0048. Orig4-art, has: 13 formulas and -1 table.
r1
POLYAKOV, V.G.-, PEREVETIZEV-ORLOV, V.S.; YAROSLAVSKIY, L.P,; LEVITIN, L.B.
Conference of young specialists of the instLtute. ?robl,
pered. inform. no.16:91-93 164. (MLA 17:12)
1, Inatitut problem peradachi Informatail AN SSM
_L 18864-63 BDS--
ACCESSION NR: AP3003714 S/0109/63/008/007/1139/1144'
AUTHOR: Yaroslavskiy, L. P.
-All
TITLE: Problem of synthesis of parametric systems
SOURCE: Radiotekhnika i elektronika, v. 8. no. 7. 1963, 1139-1144
i TOPIC TAGS: parametric system
AtSTRACT: At variance with conventional formulations of the problem, the
author tries to find the law of parameter variation and the system structure on the
basis of a specified response y(t) of the system to a disturbing force f(t) that
belongs to a spocified class. - An approximate solution is found for the problem of
synthesizing a parametric system responsewise equivalent to a harmonic resona-
tor; also, the problem of (re)tuning such a system by varying the pumping fre-
quency is solved. The single-equation synthesis problem, however, does not
always have a general solution based on the specified class of force. The results
!Card
T
18864-63
;ACCESSION NR: AP3003714
show that: (1) a definite combination of two parametric amplifiers may have the
characteristics of the conventional resonant amplifier, and (2) to (re)tune the
parametric system so that it would retain all of Its characteristics within a fre-
.,,j,quency band, it is necessary to also (re)tune the corresponding nonregenerated
system. "In conclusion,. the author wishes to thank F. V. Bunkin, Yu. Ye.
D 9yakov, E. 0. )Airzabeklyan, and S. M. Rytov for their attention, interest, and
!valuable comments made in discussing the present work." Orig. art. has:
25 formulas.
ASSOCIATION: none
SUBMITTED: 30.Tun6Z DATE ACQ: 02Aug63 ENCL: 00
SUB CODE: CO, GE NO REF SOV: 004 OTHER: 003
;ord
USSR/Electronics Telegraphy FD-532
Card 1/1 : Pub. 90-8/13
Author : Yaroslavskiy, L. I., and Lev, A. Yu., Active Members, VNORiE
Title : Frequency spectr a of tone-frequency telegraph systems with amplitude
and phase keying
Periodical : Radiotekhnika 9, 64-71, May/Jun 1954
Abstract : Article analyzes frequency of oscillations spectra amplitude- and
phase-keyed by periodic telegraph signals. When the frequency of the
carrier oscillation is near the keying frequency, additional oscilla-
tions (besides carrier, upper and lower sidebands) appear in the line
spectrum. The amplitude and frequency of these oscillations depend
on the ratio between keying and carrier frequency and on the phase angle
of the carrier oscillation relative to the telegraph pulses. States
the tone-frequericy telegraph system with phase keying was suggested by
A. A. Pistollkors in 1931. Three references: 3 USSR.
Institution All-Union Scientific and Technical Society of Radio Engineering and
Electric Communications imeni A. S. Popov (VNORiE)
1. 04 5 6,-7 1 W'1'(d)/FSS-2
ACC NRs AP6033681
souRcE ooDE: uR/olo6/66/00/010/0026/0030
17
AV511OR: Yaroolavskly, L. I.; Vollfben,-AL.P.; qsov, 1. S.
ORG: none
TITLE! A method for increasing the transmission speed of discrete information
SOLME: Elektrosvy&z', no. lo, 1966, 26-30
TOPIC TAGS.: binary code, data transmission, encoding th--ory
ABSTRACT- Tile authors review variaticns in the duobinary technique for improving the
transmission of binary coded data. The technique treats a binary signal train to a
second binary encoding, which permits higher information transmission rates and gives
better resistance to transient noise effects. A direct form of duobinary coding is
seen in Fig, 1, wht~re (a) is the input binary signal. This signalis transformed
i -such *that its negative -going zero crossings yield (+l), 'but' it's
positive-going zero crossin&3 do not (0) , resulting in the duobinary singal of (b)
The 3.963 papers of Lender and Dramhall on the subject are cited, and -their findings
on the advantages of duobinary coding are confirmed. The cited authors credit tile
increased transmission speed to the fact that the energy spectrum of the duobinary
signal is only half that of the original; however, the present authors deny that this
045--67
ACC NR., AP6033681
(b) L-j urig. 1. Duob inary encoding
can be the reason, since a case can be shown where a doubled speed is achieved even
though the energy spectrum id unchanged, Another hypothetical example of duobinary
coding is given which would increase transmission speed by 1 1/2 times. Orig. art.
has: 6 formulas and 6 figures.
SUB CODE: 091 SUBM DATE: 2ojul65/ OTH REF: 003/ ATD PMSS: 5100
YAROSLAVSKIY;!L.%-.
652 Posobiye po proeyktitovaniyu kavalou stWazi po sinnerrichnym - liniyam.
Odessa, 1954. 20 Sm. (M-vo suyazi SSSR. Odes, Blektortekhn. in-t suyazi.
Kareora dallney suyazi). B,. ts. - Sosr. ukazany v kovtse teksra. Ch'...1.
Csobennosti proyeKircrvaniya kanolov suyazi po simetrichnyr, kabelt-iym
liniyam. 32s a chert. 300 ekz. - (54-55371) 621.39.o52.0012
SO: Knizhnaya Letopis, Vol lp 1955
VILIKHER,M.M.; YAROSLAVSKIIY, L.S. (Vinnitsa)
Clinical aspects and treatment of cholesteatomas and leptopachy-
meningorayelitis. Vrach.delo no-49 90-94 Apt63. (MnU .16:7)
1. Otdeleniye dlya bollnykh meningitom (zavo-Ye.A.ParetBkaya)
Vinniskogo oblestnogo tuberkuleznogo dispansera i neyrokhirur-
gichaskoye otdolaniye (zav.-L.S.Yaroslavokiy) Vinnitskoy oblast-
noy psikhonevrologicheskoy bollnitsy; naucbn-yy rukavoditelt
raboty - zwr. kafedroy nervnykh bolezney Vinnitskof;o moditainskogo
institata prof.P.M.Allperovieli.
YAROSLAVSKIT, M,, podpolkDvaik; LOGINOV, A., kapitan; VOIMIYJWO V., kapitan.
r-,-~=adla~~Ion and cheizical reconnaissance in a tank company. SLnkist
no*4:35-36 AP '58'
(Tank warfare! (chemical warfare) (Radioactive fallout)
f
tj V , T.I
KORITDORF, S.F.; BERNSHTEIN, A.S.; YAROBLAYSXIY, H.I.
(Radio measurements] R&dioi2marenila. Moskva. Goo. anorg. izd-vo, 1933.
464 p. (MLRA 7:6)
(Radio measurements)
KOMORY, Bergey Fordinandovich, BERNSUTM, ArkadLy Sargayovich;
YAROSrAVSKIY, Mikhail losifovich; RUBGRINSKIY, A.V., redaktor;
A" 'r~"ktor
F N. A.M..- teWhfahiA y
CRadio'measurements] Radiotakhnichaskie izmereniia. Izd. 2-oe, perer*
Moskva, Gos,energ. izd-vo, 1956- 399 P- (KLPA10:1)
(Radio measurements)
24(6) SOVI 112-59-4-7892
Translation from:. . Referativnyy zhurnal. Elektrotekhnika, 1959, Nr 14,. p 21 %fTJSSR)
AUTHOR: Yaroslavskiv, M. I.
TITLE: Investigations of Piezoelectric Resonators With Plates Made From
Untwined Quartz Crystals
PERIODICAL: V sb.: Plyezooptich. kristallosyr'ye, Nr 1, M., 1956, pp 131-138
ABSTRACT: Information is given about a method of building-up the monocrystal
range in quartz crystals by torsion. The outfit comprises a massive angle-
iron frame on which a movable muffle furnace is mounted. Rods are provided;
one of them is fixed, and the other can rotate and move along its axis in an
aperture of special caatilevers. The movable rod carries two adjustable
couplings (which serve to fix its position) and an ebony disk. A leather tape
with a suspcx%ded weight is placedalong the perimeter of the disk; the weight
produces an appropriate torsion-P.1 moment applied to the plate. The treatment
temperature is 500-5500C. Four illustrations. Bibliography: 7 items.
0. K. R.
Card I /I
. .... _T~.~ f-M
f) A ic~;
F2,
YHT~65Z,47 V5X-Y I-
1 ~7 / /_77
USSR / Electricity
Abs JOur : Ref Zhur - Fizika, No 4, 1957, No 9660
Author I Yaroslavskiy, M.I.
Inst : Not given
Title : Piezoelectric Resonators With Crystals that have Structural
Defects
Orig Pub : Izv. AN SSM, ser. fiz., 19560 20, No 2, 268-272
Abstract I Investigations were carried out on the parameters of quartz
resonators with crystals of X-, AT-, and BT-cuts to prove
whether it is possible to use in such resonators crystals
with internal defects. The results obtained were compared
with the paramtters of the resonators with defectless crys-
tals. It is shown that if bars of X cuts (+ 50 and -18-50)
or plates of the AT cut contain accumulations of gas-liquid
or solid inclusions, not exceeding 0.2 - 0.3 mm, does not
affect the parataters of resonators with such crystals. On
Card 1/2
G
USSR /KLectricity G
Abs Jour Ref Zhur - Fizika, No 4., 1957, No 966o
Abstract 2 the other hand, the presence of cracks or twins does not
deteriorate the parameters considerably, The inclusions
start influencing the parameters of high-frequency plates
at a thickness less than 0-3 - 0.4 mm. Resonators with
plates that are twinned in accordance with the Doffinet
law can have satisfactory equivalent and working parame-
ters, but a considerably higher temperature coefficient of
frequency. Resonators with plates that are tontaminated
by "azure needles" are not inferior in their pai-ameters
to reson& ors with defectless quartz.
Card 2/2
YARDSLAVSKIT, M.-I.; LYUTMXRG, R.M.; CHEWSHOV, T.N.
Instrument for the analysis of the piezoelectric properties of
crystals. Zhur.takh.fis.26:439-441 Ir 156. (KwA 9:6)
(Piesoolectricit.r--Xe&ourement)
i~4 ~;n-
X
.YAROBLAVSYJY, Cand Tech Sci-(disf3) "Physical prig iples and
methods of increasing the stability of quartz resonators." ~706, 195
8 pp (Acad Sci USSR. Inst of Crystallography), 1'.'0 CoPior, (KIL,30-58, 129)
SOV/?073-6-24/25
'AUTHORS., yaroslavskiy, M.I., Pozdnyakov, P.G. and Vasin, I.Ge
TITIE: the Form of the Oscillations of Doubly-convex Quartz
Lenses of the AT Cut (0 forme kolebaniy dvoyakovypuklykh
kvartsevykh linz sreza AT)
PERIODICAL: Kristallografii, 1958, Vol 3, Dr 6, pp ?63.4 +1 plate
(USSR)
ABSTRACT: A quartz lens cut from an AT-cut slice of quartz was
used as a piezo-electric resonator. The radius of
curvature was 250 mm (each face),, the axial thickness
8.7 mm and the square of side 82.5 mm was further trimmed
by a circle of diameter 89 mm. The fundamental frequency
was 212.6 kels and excitation was by electrodes applied
simply to the curved surfaces. The lens was su]gported
by four wires soldered to the edge at points 45 away
from the X and Z' axes. Dust figures (Chladny figures)
formed in lycopodium powder were examined. There was
always a nodal line perpendicular to the X-axis and as a
first approximation oscillations were pure shear waves
propagated along the X-axis (electric axis). It is
deduced that the supporting wires should be fastened at
two points at opposite ends of the nodal line lying along
Oardl/2 the ZI-axis. "Outline" oscillations at 53.8 kc/s can also
SOV/~O-3-6-24/25
On the Form of the Oscillations of Doubly-convex Quartz Lenses of
the At Cut
be easily excited. Here the nodal lines form a right-
angled cross along the X- and ZI-axes. Oscillators
operating in such a mode may have considerable (unstated)
advantages. Acknowledgments to Ye.D. Novgorodov,
I.S. Zheludev and A.I. Tiranov. There are 4 figures
and 1 Soviet references.
SUBMITTED: July 23, 1958
Card 2/2 USC0101-Dc-60.609
AUTHORS: Vasin, I. G., Pozdnyakov, P. G.,
Yaroslavskiy, M. I.
20-119-3-22/65
TITLE: A Precision Quartz Resonator of High quality and Small
Temperature Dependence of Prequency (Pretsizionnyy kvartsevyy
rezonator s vysokoy dobrotnostlyu i maloy temperatuxnoy
zavisimostlyu. chastoty)
PERIODICAL: Doklady Akademii Nauk SSSR, 1958, Vol- 119, Nr 3,
PP. 481-483 (USSR)
ABSTRACT: In the USSRjn recent years resonators with very high
(until 17.1 ) were developed, the quartz element of which
consisted of a biconvex polished nonmetallized lens in a
holder with air interspace (refs- 5-8). These resonators,
however, have only a very low mechanical stability. A further
particularity of these resonators in the quite high equivalent
active resistance Rq (at least 100 ohm). This complicaten
their application in such generators, which are installed
in a circuit with low-frequency bridge. In the precision
quartz resonator, which was developed by the authors, a bi-
convex lens with AT-cut was used. For the increase of the
Card 1/3 resistance of the resonator against external mechanical
A Precision Quartz Resonator of High Quality and Small 20-119-3-22/065
Temperature Dependence of Frequency
Card 2/3
influences the crystal was fixed by wire strings (which in
two points were soldered on to the front faces of the lens).
The electric voltage was conducted to electrodes, which
directly were applied upon the surface of the quartz element.
The wire strings simultaneously served as lead-in wires. The
gold electrode was applied by sublimation in vacuum upon a
chromium base, which was applied in the same way. Such a
construction made possible a reduction of the eq-jivalent
active resistance of the resonator to from 2 to 6 ohm. By
means of several experiments the following was found: Very
high electric parameters can be obtained? if lenses with
31.5 mm diameter and with 150 mm radius of curvature are
used. In this case no limitation to circular lenses is
necessary. By application of square lenses valuable quartz
material can be saved and by a correat choice of the para.-
meters a constancy of the parameters of the resonator in a
given temperature interval can be obtained. In most resonators
of the here described type no polished, but only out crystals
were used. Already with such a treatment resonators with a
factor of merit of at least 2.106 were obtained and in some
cases values of (5 to 6).106 were reached. By polishing the
A Precision Quartz Resonator of High Quality and Small 20-119-3-22/61;
Temperature Dependence of Frequency
quartz elements values of (7 to 9).10 6 were reached. The
lowest'temperature coefficients of the frequency were
obtained in resonators with quartz elements, which have a
certain here given shape and here given dimensions, whereby
the cut angles are YX1/350031 to YX1/35004'. The typical
temperature frequency characteristics of the resonators of
the here described tyre are illustrated by a diagram. The
thus constructed resonators were encased in helium filled
glass flasks (rV5 torr). The concrete valuee of the parameters
of some resonators are composed in a table. A more exact
investigation of the aging of the resonators still lies
ahead. There are 3 figures, 1 table, and 7 references, 4 of
which are Soviet.
PRESENTED: November 15, 1957, by A. V. Shubnikov, Member, Academy of
Sciences, USSR
.SUBMITTED: November 5,1957
AVAILABLE: Library of Congress
Card 3/3
AV T'r
8 24
S10701601OO510O,')1V-Le-rUl7
o0 E132/E36o
AUTHORS: Lhramov, L.V. and Yaroslavskiy, M.I.
TITLE: The Frequency Coefficients of Quartz Bars for Bending
Oscillations
PERIODICAL: Kristallografiya, 1960, Vol- 5, No- 5,
pp. 807 - 8o8
TEXT: A rectangular quartz bar, nearly square in the XZ' cross-
section and elongated in the Y' direction, undergoes bending
oscillation in the XY' plane. -It is excited by applying the
voltage between pairs-of electrodes parallel to the Y'Z1 and XY,
planes. It has a small temperature coefficient given-by:
A f/f c(T 0 _*T)2_10-6
6
where c (0.02 0.045)x 10- The frequency is given by
a
k (2)
2
a
y
Card 1/3
84M
S/070/60/005/005/oi2'/01-7
E132/E36o
The Frequency Coefficients of Quartz Bars for Bending
Oscillations
Where a and a are the dimensions along the X and Y axes,,and
x y
k is the frequency coefficient.
Published work has been almost exclusively concerned with the
cut at +50X(XYt/+50) . The values of k given vary between
5740 and 5790 ke/s.mm. The value of k has been found
experimentally by the present authors for values of ax/ayup
to 0.20 and tilts of -20x to +14ox . The change in Young:s
modulus with angle and with ax/ayIs also plotted. This was
calculated from a formula given by Mason (J. Acoust. Soc. Amer.
vol. 6, 246-9: 1935):
2 2 2
m ax Y (2n + 1.) a
f
43 fr-.2-
y y
Card 2/3
84M
S/07o/60/005/005/012/017
E132/E560
The Frequency Coefficients of Quartz Bars for Bending
Oscillations
where () is the density,
n the number of the harmonic (here n = 1) and
Y is Young's modulus.
A line giving the calculated variation of Y compares well
'with what is observed. It was calculated from the well-known
formula:
12 2 2
10 /Y 1.269 - o.841 cos 0 + 0-543cos E) - o.862s!n cose sin3y.
Acknowledgments are expressed to P.G. Pozdnyakov and I.G. Vasin.
There are 3 figures and 5 references: 1 German and 4 English.
SUBMITTED: December 30, 1959
'Card 3/3
34734
S/07o/62/007/001/020/022
0 6 E192/E382
AUTHORS: Vasin, I.G., Poz)nyakov, P,G., Khramov, L.V.
and YaroslavskAj M.I.
TITLE: Quartz resonators with slotted piezo-elements
PERIODICAL: Kristallografiya, V-7, no. 1, 1962, 150 - 152
TEXr: At audio and ultrasonic frequencies it istoften
necessary to employ quartz resonators having a low temperature-
frequency coefficient, a high quality factor, a low resonance
impedance and, in some cases, a wide resonance range which can
be achieved at comparatively small values of the capacitance
ratio C0 /CK. Such resonators are required, in effect, to
combine the merits of the resonators with rod-type piezo-
elements and the resonators with twin (bimorphous) elements
without having-their disadvantages. The authors designed
(Reif. 3: Author's Certificate no.;123573, July-28, 1959),
prepared and investigated a piezo-element of this type
satisfying the above requirements. This is achieved by cutting
narrow cavities (slots) in resonator plates or rods, the surface
of the slots being parallel to the edges of the plates or the
Card 1/3
-5-
S/07o/62/007/001/020/022
Quartz resonators .... E192/F,383
rods. Thin metal coatings, used as electrodes, can be deposited
on the surface of the slots. In this way,-the problem of
producing a crystal piezo-element with one or several internal
electrodes is solved. The electric field applied between the
internal and external electrodes has opposite directions, so
that linear deformations of opposite signs are induced in the
element. These result in its bending-in the plane parallel to Ic
the edges. In this case, the piezo-element with a slot is
analogous to a twin element and, consequently, it has a low
electrical impedance. On the-other hand, by using rods of the
XYt/ao cut, whose temperature-frequency characteristics are in
the shape of parabolas whose apex can easily be controlled by
changing the angle a 0 of the cut and by suitably arranging the
slots (as shown in the figure), the disadvantages of the
rod-type resonators can be eliminated (I.e. the inherent high
values of R K and L K are reduced). Further, due to the
large reduction in the equivalent inductance of the resonator,
its resonance range is significantly increased. It is also
Card 2/4
S/07o/62/007/001/020/022
Quartz resonators .... E192/E382
pointed out that the frequency coefficients of a slotted piezo-
element are slightly reduced due to the fact that its bending
strength is decreased. Due to the low resonance impedance of
slotted resonators their oscillatory jendencyls greatly,
increased in comparison with the solid piezo-elements of the
same dimensions.
There are I figure, I table and 4 references: 2 Soviet-bloc afid
2 non-Soviet-bloc.
SUBMITTED: June 8, 1960 (initially)
July 31, 1961 (after revision)
Card 3/1
YAROSUVSKI I.
Piezoelectric resonators vith crystals having structural defects.
Izv.AN SSSR.Ser.fiz. ~O no.2:268-272 7 156. (NLRA 9.8)
1. Vnesoyusnyy nauchpo-issledovatel'skly institut plyesooptiche-
skogo minerallnogo syrIya.
(Piezoelectricity) (Electric resonators)
ZX
M
t
.......... .I
a 6 6 a a 11 0 6
is
Is I I U M a Ill V H a
,A
00 A _osT &.0 )No MOM_
a P&OCLS
911111 Tke morood of a ,XtirrinAW apedra i
7errijbi and N. (1-.1'arobovskil, D&M. arsd. jji.
l"R.S.S., we,. Phyi.-q, Rust6n).-The
light coming fro", the source passes alteruatingly, with a
!re4uencY of socyrrial hundred per sec., throuph two abscorb.
ingobjectS.AftEriothit,h It loidecompt]. inan infrared mono.
chromstor and then strikes a nunwieclive recriver of in.
frared radiation connectirtl with an ax. amplifier isad a
galvanometer. When the two ob -ts are feltatiml, the
a witivarsometer 110C.4 1. wheresecir In the
lZIZIL."It No objvti ffiffrr in their absorption.
el I., &flmlool and thus registers a -41if.
ferelitlill" spectro1cfain. If the spectrum of a single
Libstance Is sought, a transparent traterisslorillierso empty
61fough Is intold as the t"wed object. Ab*orptk)n spectra
a obtained ley this methtal show hbarp pralls rising above
lit urn line. The setup L4 used for
obtaining q"y
!Pectra Of solid and liquid subsLaticts in the region front
00 w 2 u9p. The met btxl ii~ applied to bandit, enrre4ponding
to fundamental vibration Irequenclor-ii, which can be dc-
00
a
SnaLLWOVAL Lff�2&TVM CLAWICATM
0 6 a e a a 4 a a a 0 6 a a 0
It mitus law onati4i"io a
A-0 Poloist
00
lot
-90
911if
V 0
01111101
.00
11111111110
:0
too
Coo
loe
me
ago
goo
lee
lee
1110 1111
too
We 0
tectvi with v,,ry somalt sonnt~. -f MAICTiAl. endrwic"60 Prn-
vide thiclon"vi, of the voicirr rif 0.01 Inns. The reorrivrr in -
chief" a chandier Orel %ill, raf1m)"IT"I verrtalfle fllwf%j
whkh ulmorl, the infrarrd radiation nfntwf(vlivrl!f
ILrelindnary r%pt), rri,olt, wt-re o1olaivird In thc study -, i
hal-whiromy of at-nnatic eninjoil,. arel (it adm)rption, a4
he
rxprc~ssrd in the %hill oil afewerplicies bands. Hymingini
two (optical branche-, r-p-, the pore enenpmmilie and
ilitirinioit.,11te nitifi,oil wai applied lei intryinol. isitriar-
of 3011) of the NIll xrossil, a, st f"till let 111,11 inlrr.
1WI6111 ft-Uld thilit be 411)"VVII in the (UMIJUnriltAl A-441$-
by troquinorse resultcd in the appearance of an absorption
at ;W cm.-I; it f: interpreted m an intrease of the dipole
rnornent in the of formation vilwatitinit (if the terminal
carb(myl groups in quinone on account of hydrogen lgetiol.
ing with the h fro%rigr(Rtp4uftiyilrtkittittime. Inansi%l.
t
of phenol a Tanil tic, hydroxcu-boud (orutatioson cauwi
the Off band of the phenol to be shifted by S. 10; cin. -1.
S. Thnn
goodso Hit Oleew a-
__4 1 -1 ; NJ
U a a - K It 11
0 0 0 0 0 0 0
glass] 1111s Uses all
i;LrrIA L IIWO 0613VUSAad 3 a T
a I sa
o
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 9 0
PA 65T19
AROSLAVSKIYY N. G.
USM/ChGMiStry - Phenol, Spectrum of mar 1948
Chemistry - Spectra
"Application of the Method of Differential Spectra in
the Near Infrared Field for the Detection of Inter-
molecular Interaction in Several Aromatic Compounds,"
N. G. Yaroalavokiy, State Or& of Lenin Opt Inat,
Leningrad, 9 pp
"Zhur Fiz Xhiie Vol XXII,, No 3
Studies intermolecular interaction of aniline, phenol
and their compounds in various solutions at various
concentrations and temperatures by means of differen-
t1al infrared spectra. Reproduces and.analyzes 8pee-
trogram for the various solutions. Submitted 11 Apr
1947- 65T19
"M Walm
e
K~
j
REP!,
P
Id 111 It it It N is Is I? m 11 Is! Is M Ompolmit Also Us k U Allivisso di
I
'I L A-- X _T _(L
_1 -1 it st 1
A A 6 0 al " is
"
,
.
lit- A?.Cl t- cs~*Iilb I_t_ L
0 0 .4 A ca of the method of differ ential posictra In Ike
of 10 Ill* doptsettion Of nIOIPCU1&I 1:11414ACtion Of
some afommUc compounds. N. 4.. Var.o1o"kil 11 11.11vil
"C
ii-TWA
1
2
C
;
t 141
.
U.)
.
J. MY
1.
Illo'. 1XIIIIINIUM. p
ti -ps,
.
.
73(101N)sin Rtmiju); cf. 1. 40, PAW.
I. III% Were noulle between 1.0 good 1.11 1., 1110 title IAl 0
e
4 lluilille (1). to vilwatiolm of N-11. in
of v
flit I rot lowald momller A fly, r. It voo 11-voliz-1violl _V9 o
III (Tt'. Jimmie, 1,1106. avilmle. V.116. o1
411111,11 %hill 1. ovilivs,rd b% br-Ififlis 1111,01.1 1 1-0. r K.,
DO I'- The romfolps; voinjill. Ill fill% Ible (1, Vol, 1, 111,11,
-t toy tile * The title
0) lit t1l'ole cleArl . .111. of 1.
IAIIIM ivil'Imbamisle.-Il I's tile ollelt-114) illml 'AfIvelell I'v
00 It, 3141 .Ins of phr,o)"I (111 lit C0, have's Amlp I.-ak .I
1111
h
I t
)
1
AI
l
- .
tot.
ta,il
40-sopti.al at I
M . W
o-
It"stop.
A 111,11- .81 1310 0; tile 141i'l 11- It'd Alleet-I I-Y 1-6-4--lamt .00
00 U the covorn. (,f 11, Not lite I-A k lost. 2 il.o
.
Islas. at 1. 15 anti LM p. SIni. of I wiih It or ji-totto. 00
00 11 phenol Ill CCli show, in ailtin. is) the linti of the comIxi.
itrills, is lorakid 1.42j& which is doe rit [ter toa 11 looml Ise-
twerit N wal Oil or lit voiluoirrinvot of tile lost, of
Imm 1. Stifill. .4 1 wills (11 eel. how Zoo
'
*
' tile LWI-m title at 111211 truill. oilly'.111.1 .,Ilm of I wills I'll--
'I'licte is it(, wltvtivr als.
how it
t till
d
ho not
i
l
i
j
~ 4
.
t
s
a
t
c a
ustlithist lorlivren 1.2 unit 1.0 p its toollen I lipitoichlotitle,
, 'I. ionlyatil"I Climillilles life villulthill't X-It.
-
-
t-.L--A
A L kU-R-C
K A-L L ITV I-AV US I CA ASUFICATICK
1J..
u is AV NJ it:
i- r-j I A --- 1--- 0
v Ilk hA 0 4 a I ill so -k 11 3 4 T
m
it 9 K rt Is It x A 1 1.
0
i
0000 Co
to 11111 900 90 0 0 0 0 a 0 0 0
0 a 0 a a 0 0 0 0 0 0 0 a! 0 0 * 0 000ooe-60690604-
It Jq-t f 1i I i Vt -11, A A A A-14 - 14 D 'A 36 40 it U it " Orit,
111.1-1
0o
00
00
00
g 0
go
040 All
00
3
go
go
00
11,00
0
toe
IU06
ALLUNGKAL LITERAT LASSAPICATION
Lot C
11*0
I I I V ZA An L S 8 Flit 0 K a I it of 0 a a
U 0 AV 00 LS
1 1 . . a a .1 ; i .1 1 Will -",4
0 0 0 0 0 0 9 0 0 6 0 0
0,0 Is 11111411,4110 0 0 0 *a**.** 0 0 0
00.0-009 0 40 0 0 0 0 0
HEM MW
jr
I a L _AA M
a _I -
IV. ------ 4~ -*o
LD-r 1--l-L.-is U~ -i!i-
'-oo
Wf *4 absorption spectra of adsorbed molecules. atilt N -11 prsks of file aiNirl-l etw-fly, the
S', G. Yor"vidii) anti A. N. Tere"its. DAkjv A disappotrance of flit- 0 -11 lit-As is title to tile IurjlI.itj,)jl'd
-V411if -*-'T SI-S R-- 40, 165-800410).-Oll 9fAdUAl &dSQrP- It b9itils 0-11 ... N. At flit 34,ige ol greater suifice 0
flon of Cjl'e' und of toluene vapors, in reew, at room coircrit,,ts the N-11 pe4k lit 1.42 if Appe4r% shilte-I t'l
Oil VitfMIS Si()i sell 1110161113M Inkally only 0-11 longer W4VCS, fly Mill 0 WAVC 10 tile )CA of assoLd.
=: peaks corr"punding to the C-11 frequencies of Nit groups. *"If by WY-13 p rel-itive to file 1.014trtf Sit 00
the fins, and (in the Case. Of IZIUMC) to the CHS Smipsinthesoiji.ijilliN)IliiiCC)i. This deniunst r.at" loo
appeAr prollmstively, in position Weatkal to those7up., the weakeningolvatcuce Inad%orption. ThcC-liti4nd
me peaks in absorption fit CCJs soln., at the wmethrie, remjltts undisplAcol. The height of the N -11 peak,
the narrow 0-11 peak bm-ontes himAsingly Ac;Akcr. [a relative to thAt of flit C-11 peall. Is Clecrnisr'l in flit 'W. go 0
144he Adsorption of blow on account of Its low vapor soctird state, which Is altrilintril to flat interm-litio IW- z 0 0
pressure at room truip., the grAduill d1uppe"ance of (tie tween tilt Nit gtoup lind tilt Oil groups of file sulfav
0 Al peA pets lit long oviore the apprittauct of the C If -, of tile adoorlictit. The effrcis oliwirved %fib I'liSialAre re
9yen more pronounced lit C.14N. In tile A.Iorpt of
I'lloll. tilt 0-11 peak of tile AIIWWIICllt Milling narrow
and d6ippe-irs inuch, most shkwly thin with I'liNils; the 0
peak at 1.4 1 N p belonging i o I fir 011 group of PhOl I Appear*
cousiderably weikenetl an4l broidi-firtl lit longer w4vet. i-go
This Indicates chat the Oil firimps of tile 3io; Xt-I gre not
teadily ptfitittmi by flit Oil itioups, of 111011. 1. 11.1 100
rAnite of caltilliry conileimilion. there alipt-ar braid Coo
niallium characteristic of j~-k:n. 14 Off xroupi. N~ T.
six
YAnCOLAUXTY, N, G. PA 50/49T27
toga/ iiistry'- -Abserption SOCtra -Tun 49
Chemistry -,, Catalys.1s
'"Irtrared Absorption Spectra of Adsorbed
Molecules," N. G. Yaroolavskiy, Acad A. N.
Teranin, 31 PP
Nank SSSR".Vol LWI, No 5
Experimental-results cited predicate successful
'we..:of infraredspedtra in research on speciak
.cases of adsorption. Theory should. be applied
catalytic reactions. Submitted 19 Apr 49.
A RGMAII Tih? tyi - N
WM/Chemistry - Acridine, Alsiiro hg 49
Absorption .1pectra
"Problem of Structure of 9-Aminoacridine," A. Karyakin, A. M. Grigorovskdy, N. G.
Yarosla-eskiy, I+ pp
I'Dok Ak Naul: SSSRtI Vol LXVII, No 4
Unkike, other aminoacridines, 9-aminoacridine and. its derivatives, arivanol and acrichine,
possess great bacterial activity. Previous efforts to show that their characteristics were
'related to their atfmcttre and that they did not have the usual amino structure (A) but the
tautomeric structure of acridonimine (B) were unsuccessful. Study of absopp'tyion spectra in
ultraviolet and visual spectral fields makes the latter hypothesis reasonable. Data on
infnared absorption spectra confirm the assumption tha-i a 9-aminoacridine molecule has the
structure of (B). Submitted by Acad A. N. Terenin 2 Ju~ 49.
PA 3/50T13
(I--LI 4 11 1 S I
I I., "l-'T'no" "f awl
.rg ""n p(h 11-1 1~~ --f It gll.~i M-t
9t t1div, 'ierv m;,,Il I. I III ~ 2 r, " r, ~n with a 'peclal
illit,41i'll jj)UrrFOt?k4'II I ~ ith I 1'1-~i It-f-tor StwOrn were
tahctl af lemp'. up I" IMO , T-i". ,f th" Ml
harmonic III thc slI,-ctr;i of tho, 04-at, at thrie high trmjri~
indicated that Ixotth rI-,uIf holn the tirlsorption of
%~alcr. The nbrorption 13-1-d~ ~Aulfi~ll, all which c0:1clu-
slolv; Were "A, were asnigned wi fnfInw.%: )..365 p. 2r,
(frtt (1-11); la, 2,,;J(0-11 . . Y.Oforbedl, 1.48 ;.,
2v,( 0-11 1.00 14, P., + 6f(O--fl . )adsorbedj:
+ I G--H , . .); 2.21 p, 241;i0i), The
~and!i at I.W and 1.98 p were combination frcq-nnd:s,
where the two &Is were deformation mtA,!.i of tht silimite.
R. D. Kmss
0l the silk P,
Pil.
hist.. Lunilliffull). Mar. FIS. Khom. 24. (19 81 (VINI). -
11it shurptim spectruns Owl-een I and 2.4 .1 of porous
StAm (lit'rMity - 27'.~J vl;i% deld. after different treat-
'"ent of the ILtnt. 'rhe very shrp line 1.1141 s %at given
fly glaoi healed in a vartmen; it. i,itm.1ty Ulleff
file 11C.411119 frIllp. 41111 it diklillptAff'.1 At T -
111W and oil keeping the Rub,i In "loW air. This line i.
a higher hannonle of the vidency vibralloot of the Oil
groups clitnikkily bound to the glass surface (itil FA-011).
A line 139-1.441 s, appeared when the glass was blixed ill
air and disappeared an lumting, it helmat to (fit till
I the lul*wbed fill). The lint 1.4d"' "" 11"""llyt
#Lus uld. with 11#0 and Ill. . kept in
vWcuum at room itself$.); A4 it il Pfr%cllt al"J ill liquid
HgO, it inust belong to copilLLry coudemcd 1110. A
lint 1.101 is behaved like L.W-1.411 ;&till almi is Attributed
to LIAmmIlIml 11,0. The line 2.21 jA %m Ism AfTected fly
heemins or mc4litt-Wrigand inopt Im -11ir 1-1 Sit),; il Ilmy 1~
state of 1110 in Ad"Alcilts call be dchl. fly '-pt6vt IneAS34.
J. J. 11111cfInAll
and 1-670"). tii,;- Storm at ~11- wit 3 Ilia%. 1,47
(MV). 1.405(M77). and L&14(41M), unit at 6
tits hYd 06" name at lit's tFFF30
"utfatetif orft6w., Y Ait, sharp bands. 2 of which (belonging to the Nill #Mips)
N. N
4h"". Its "Ild N. fl.. vart"141v 1W trolarldal, with the altove Ist final, and the i-thrr :1 lie at
y AlItial. Nook XX N.M. ". Will, it I'll* I &J((MmI alld I ANniAll, 'the fine atillic.
M
ISICIP of the 1114111"1 111-tat"111111111 blind 0- 11 - I" the Ingkill an of Law, Irmps. fit tile livill miltulao,r. vial.
atollo.1 IWMI rots. (lot lidinionk- sit the 1110dollitubal Va.
lellear viblaillain fivillitill-Y C-11) ivan hivraillifutrail III the -.1 the o-11. banal to hister fircillencles anti is Mlistill'u-
+201and -11111".1n 16frOll, Hart of the Intertaillef of the Coniponenis of the band. The
RioH, DoOll. laillyvinyl air.. slymol, reivierlotal beet abill is gmtnt (IW200 cm.-I) for the mks. MeOll.
taticar, phlit".11010 fralts, oind efirst. Urea iin the latter. t.*tnlt, nuvii. and x1yearol. to amorphruis wirrose. the
law tile If flood N-If ... 0). Fair the low-temp. cletris.. structure cal the 0-11 ... don not change appreciably be-
it- W44 tilit'le of the athattervallon that ficittid air In a layer a I,een -.xj- and _ISD- as the disordered structure a the
firvar em. thick it(%-% not allsoill It, the levit'" so; &M 11 dious scalld Is KiW by the matalloki It bonds: the name
Floe do" Its abilanclokin spectrum In the range 00--2.0 " " in glaltryinrl sit!. and the pbmW.IICIIO redo. For
P".
MILsk the higher ovetloo"of the Yllwallocis 0-11. 0-41. . .. I&he tter . the sand do" arlitinge at higher temps bv-
.q_JI C__II (*-I). jIld llittir etiniblitalknis. Clyal. Sinn jig frotts +A0 &mat +601 owilig to dionlivilon of 16 it
MIC44 at 20' -hows a taburr banal 1.44 p, (0044 call- I) I -via s, Absenre of the man, M 1.45 s Its amorphous sts.
(itillairfluttwal 0, - 111 0,141 2 Illiantaiml bland h4tillft will' mar. prourvinol. gly"tol land tilt alm Indicates Ilia I large-
tvilirfs at I'Al 0 Wn'.ro vol. ' 1) ittilt LAX I& (Mr-41 ran. ' 1) Via- tically all Oil gra"Ilas are 11-biondod. fit tile Frain. I here are
fenpondlot [it 0-11 .. ': as the Intensity of thew hand" both free Oil (sharp max at IAU a) and If-bonded Off
chanIC with the lictildoo of the plims, of polaritallon. it (I.M a). as in eysl. picrow. The ot"W"ed do, , at Of the
may asiturned that IIFF7 lawkitiff to p"11114IId Oil 91MUP-51 intensity of the sh&M bands. from 211 to - 1801, In tilt rtsin
with different orientations In the crylital. At one and In crinit. suctow. Is thile to superfamiltion, of the shoet.
6n.1% 5 sharp prikka I.1W) it (W7 elo.'), 1-51011M). LA2 ways part of the 0-11... bond on the pftk of free 011.
(M7111, I.M(Mill), .41111 LARIUM). F41110411Y. III IVAIW,
vincil, tile 2 mail. at Z)*, I.&%M20) still 1 07 k.*4kMI Sit it I,
v.-f lwiftl with the shift ad the broad hand 10 1 ef *live$
1.P412(62141). 1 WWII), 1-050M on
Into 4 sharp billifill. wit I'll"Ing temp. If Thnn
YAROSLAVSKrf, N. G. - ----- --
USSR/Chemistry - Spectroscopy, 3mission
"Infra Red Enission Spectra of Heated Liquid and Solid Organic Films,".
X. G. Yaroslavskiy and A. N. Aleksandrov, Leningrad
Zhur Fiz Khim, Vol 26, No 9, pp 1278-1283
With the aid of sensitive USSR equipment, the authors obtained discrete iafra red
emission spectra ;n the range of 1-5 U from liquid, molten, and solid org compda
heated to 150-200 #G. The emission spectra represented a reversal of the absorption
spectra of the compda considered'. These emission spectra also showed the expediency
of applying the method to the mol azialysis of liquid, molten, and solid org compds.
q~umt comparison of the infra red emission and absorption spectra will enable detn
of the equil or non equil character of phenomena connected with emission.
263 T 17
USSR/Che.mistry - Adsorption Aug 52
"The Change in the Infrared Absorption Band of
OR in Microporous Glass During Low-Temperature
Adsorption of Oxygen and Nitrogen," N. G. Yarosl-
avskiy and A. V. Karyakin
"DAN SSSR" Vol 85, No 5, PP 1103-1106
The presence of OH groups on the surface structurt
of adsorbents dets the adsorption activity of the-,
surface. A piece of microporous glass was placed
under vacuum in a glass of vater and the absorp-,
tion spectra-measured after either 0 or N were
239T30
admitted to the vacuum. Cooling t6 -1800 shrinks
the OH group'band at 1.365 microns. On admission
of N, the intensity starts to decrease at the
usual absorption peak of 1.365 microns, and
increases at 1.378 microns. On admission of 0,
the usual OR peak immediately disappears. Sub-
Mitted,by Acad A. N. Terenin 26 May 52,
oj
I g1 .4 r" 1. 1 7"
~.j
7 1;,;(, ,- %-- -
m "N' lik i I"I". ....... I Y _L~ ~37%c, toc d-- of
fh~ Imm 60 A.. -i-1 11tv ill ~tjrfart: I(X) lq. ni. , i;. AI-it j~
--- I Spectra %vtrt: (nounur(d ill We r4,f:lfjll I to ::.h 14 witil ri
I'US cril 4oth ht, dircet witom.,Iic ri,:ordh,f,- wid by the
I%---
VartjAw4kil, CA. -.10, tv"W). li - was thitt trw
surface of the nutt "FW -f- WyerLd Will, (Arl Mv!i-
urellwilts were 111;1,11.4 ill Itir Hil'i Ill vitcuum alt(~r
!1MAtlaf at tcuip, 11m)- HIM". A %mrsow may. pt IAW.
1 .4 tit but(A go 011 - Ad~,O-A If,C)
1.40A, ~1"fj if C) I., Ill,. po,vl; h~-
'rho din"p, " . ' "C' ti the m:.1, ill t,ll 4,01, 1
fmwtioll of t ...... ( 1,1,,,r pti.... 13 k o I
(crtmbianti-, , 0 r;tt,-~ A ( )! 1 ;-4 11 .0 ) t -d I
At g,,~,tcr wav, If-, .,,c 1,; ... 4, 4
61,wrorrmn.- i,-t, moo, frinn
w:licit wr,, .%,I -,:~ .1 1~ -q-, 1 .1 ... ...
pheont, rold 11,C) ki and lot'j, ill,- 1-'k
p,r,ki, oid m ~ij p-, , ~1. -.1j. t''i
I-Al. ('- 1 1, 1, ~.. ~
CH mid NII Lpj,,:.a Nif Y jv.,t i wwi 1 11
groupr to furin I i - londs 0 --it. N. Smid i,
appear Ili pyridhw. Ad t .... k o( ph,: .. .... t
greatly clistlirb tbe Oil groups. Adzivrptiun of I,., will 0,
at -leg? urakcs the Oli penk disdripcar. N, Is de,orbcd
U;!V)lg return to mtin temp., hut 01 Is ffcsor;m_~I only by
hC41111; to 160- , (W. Agii,g of nflcjoporoo~ gj;,~'j on
swraga cuotfifi" tfi,~ ch,,ructcr of the (Al juroup5. S. 11.
Z
P,
LVSK T
and 0.
Structure of Aromatic Nitramines. Il. Infrared Absorption Spectra and
Structure of AryInitramines (Aryl "Ittraminic Pcids), ragle 13?5, Sborn-Lk st~!~ey
ro obshchzq khimll (Collection of Papers on General Chr-mintry), 71ol 11, -o,!3csw-
Leningrad, 1?53, nages 1680-1686.
State Inst of Applied Chemistry
i4l
USSR/Optics
K
Abs Jour: Referat Zhur-Fizika, 1957, No 4, 10517
Author Zheludov,, B.A., Stanevich, A.E.
Tnst : Not Given
Title : Recording Spectrometsr for the Long-Waye Infrared Region
Orig Pub; Optika i spektroskopiya, 1956, 1, No 4. 507-515
Abstract: The authors consider the features of the procedures in long,-wave
infrared spectroscopy and describe a high intensity spectrometer,
with diffraction gratings, intended for automatic recording of
spectra in the region from 20 to 100 microns and above. In the
instrument, constructed in accordance with the Pfund auto-collima-
tion scheme with a relative aperture of the collimating mirror of
1:2.2, there are employed two interchangeable r--c-lielett~.:: of 12
and 6 lines per millimz_ter, measuring 250 x 250 mm, ope-Yating in
the first order. The scattered short-wave radiation and of the
superimposed spectra of the higher orders are eliminated by using
Card 1/2
USSR/optics K
Abs Jour: Referat Zhur-Fizika, 1957, No 4, 10517
,reflecting (matted mirrors, crystal plates, and echelettes
working in the zero order) and trantmitting (quartz, polyethyleae
covered with lampblack, eta.) filters. Provision is male foi.
the possibility of employing the method of eelectiv'~ modulation.
and producing vacunm in the inF-trumert. Using a silite r3d at
14WO and a standard radiation thermocouple with a FEOU-17 Phatc-
electronic optical multiplier fed f=om the IKS-11 apparatus, re-
cords are made of ths =otation .5pe&.--a of abi=ption of vapors
of atmospheric water in the region from 19 to 100 microne with
a maximum resolution of 1.2 1.5 cm-1 and acauracY = 0-3 CM-1.
These results are consie-sred by the authox-a to be pr~51iminary.
Card 2/2
Y.AP
Ilk
Optics In the German Democratic Republic. Opt. I speldr. 1
no.8-.1025-1027 D '56.. (KLRA 10:2)
(Germany, East--Optics)
Yesorov, Yu. P., and Ye. A. Chamyshav. Speatra
of 3illooorganla Compoun6a Vith an Aromatic
RIAS 390
Garsalmvi
r,X., I.A. Taltavaidy, S.V. Neemlov,
wd V
P
e
.
Ishalletas in the RAAC* Prom
2
5 ;a
. 3%
KI-lov, B.A. Doable MOU04hrmator Vith Diffraction
(Iratinga 397
YarmalavakiT X.G. B.A. Zheludav, AM A. Yo. Stamovlob.
MGW6WIA32i;~"U. for Rglsitratlon of 14ag-wavip
rnfrared apeatris 399
Card 25'JO
PRIKIiWAO. A-F'
24 (T) 3 . PHASE I BOOX UPLOITATION SOV/1365
T-1yov. VnIvoraltet
MGtokJtIY I V4040yum2go movashchanlyA p9 spektrosicopil. t. It
molokul7mrsAya spektrosk.~,plya (Papers of the 10th A.11-Unlon
Conference an Spectr*acopy. Val. Is Mlectslar Spectroscopy)
1L'vov) Iza-vo L-YoY3 Ardv-ts, 195T. 499 p. 4 1 copies
printed. (Serl#st ft:910 Picychnyy zblrny1C' m.
Additional Sponsoring Agstw7t Akadvalym nauX SSSR. KoadesLys. po
spektrookopil. X4.t 'Jaxer, S.L.1 Tech. Ed.s Saranyuk, T.V.;
Editorial Boards tavlaterg, O.S., Aaadesdalan (Reap. Ed., Deceased),
Reporent, B.S., Doctor of Physical and rAthematical Soleness,
Fabelinskiy, X.L., Doctor of Physical and Kithazzatical Sciences,
Yaba4kavto V.A., Doctor of Physical and Mathematlaal Sciences,
Xaxm1ta1,lj, V.Q., Cs--A--date of Tla.~%;-Aosl Sciences, Ulakiy, S.M.,
Candidate of Physical ani Kathersatical Salmnass, Klizovskly, L.K.,
CWidate of Physical And Mat"cAtical Solanalkli, M1117ftnchuk, V-S-,
Candidate or Phjai%ial " FAtharAtical. Sciences and Glassbarmano
A. Ye., Candidate of Physical FAthexatical Llamas.
CAM 2/30
Postoyakly, r. Ya., L.F. Trefilova, Yu. N. Sheynker,
AW S.O. Bogomlov. Copl&a&ftty or Phertol Nuclei
in DlPhonrl Derivatives 388
c L
(7,
AUTHORt YAROSLAVSKIY,N.G. 53-2-6/9
TITLEt Ifeth)-Z'sand Devices of Infrared Spectroscopy (Longwave Range).
(metodika i apparatura, dlinnovolnovoy infrakrasnoy spektroskopii?
Russian).
PERIODICAL: Uspekhi Fiz. Nauk, 1957, Vol 62, Nr 29 PP 159 - 186 (U.S.S.R.)
ABSTRACT: In the following survey, which was compiled after the study
of 78 published articles, the longwave part (50 P-to more than
1000 I-A-) is taken out from the total infrared range and the
methods and devices are described which are necessary in order to
be able to carry out measurements within this range.
The following methods and devices are dealt witht
11 Method with a quartz lens
2 Method of total reflection
3 Method of selective reflection on crystals
4 Use of a diffraction lattice as monochromator.
SDectrometers for the lont-wave infrared ranze and
1) The particular features of infrared spectrometers
2~ Radiation sources
3 Radiation measuring devices
4 Description of spectrometers
Card 1/2 a) according to Randall
Methods and Devices of Infrared Speotroscopy.
bl according to Me Cubbint Sinton
a according to Bohn, Freeman,
d according to Meier
e according to Yaroslavskii Zheludov.
ASSOCIATION: Not given
'PRESENTED BYt
SUBMITTEDt
AVAILABLEt Library of Congress
Card 2/2
53-2-6/9
SOV/51-5-4-G/21
AV THORS Yaroslavskiy, N.G. and Stanevich, A.Ye-
TITLE; Rotational Spectrum
of 1r2Q in the Long -71avel ength Infrared Region
_
50-1500~L (200-7 e
m 1 ). (Washchatelonly spektrZ20 v d linnovolnovoy
l
infrakraunoy oblasti 50-1600~4 (200-7 em-
FZRIODICLL- Optika I Spektroskopiya, 1958, Vol 6, Nr 4, pp 384-392 (USSR)
ABSTR>: A vacuum spectrometer DIKS-1, described In Refs 11. 12, Yjas usod~
Aix optioo--accustieal receivar, developed by Pankratov (Ref 13), was
used instead of a thermo-element. The beat resolution was 0 12-0.3 am-
-
. The
and the mean error in vqve-number determination was 0.02 cm
intensities were measured to within 10%. Five interchangeable echelette
gratings were used s three of them were prepared in F.L.. Gerasimov's
laboratory and had constants of 0.0833, 0.1666 and 0.5 Lua k12, 6 and 21.
lines per mu) and the other two,vith 1.5 and 2.5 aun constanta,were v~~t
using a precision lathe. The light sources were a platinum ribbon
covered -with thoriumoxide and heated electrically to 15300K (for
50-100 fx wavelengths) and a mercury lamp FRK-4 (for 100-1500 p. waveleDgtb.-~;'
Figs 1 and 2 show the B20 vapour spectra in the 50-1500 p. region,
obtained'at pressures from 1 to 750 mm Hg, relative humidity of 80%
Card 1/3 and at room temperature. 105 absorption bands wore recorded in the
SOV/51-5-4--6/21
)Rotational Spectrum of HO in the Long-Wave length Infrared Region 50-1500f4
(200-7 am-1).
50-15OOtL spectral region. 94 of them were interpreted as
fundamental frequencies of the rotational spectrum and 11 of them as
acme of the fundamental frequencieu which appeared in the second
order of the spect=m. The table on pp 387-8 gives complete
interpretation of all the observed absorption bands. -r~o viavo-numbers
of these bands are compared with the wave-numbers calculated from the
values of rotational energies given in Ref 6. The difference between
the experimentally observed and calculated vave-numbers is about
0.02 cm-l, i.e. it lies within the experimental error. K6 3 6ives the
rotational Spectnua of H20 in the region 50-160014 kZOO-7 em-1). The
34 bands recorded or resolved for vie first time are marked with the
Ca rd 2/3
SOV/51-5-4-6/21
Rotational Spectrum of Ho in the Long-11avelength. infrared Region 50-15001A.
(200-7 cm-1).
plus sign The authors thank TIA. Fankratov anJ I'LL. Veyngerov
for supply of optico-acoustical receivers. There are 3 figures,
1 table and 16 references, 7 of -which are American, 6 Soviet and
3 Goxuian.
ASSOCIATION: Gosudars tve=yy optichaskiy institut im. S.I. Vavilova (State
Optical Institute imeni 3.1. Vavilov)
SUBMTTED; December 23, 1957
1. Water--Spectra 2. Spectrum analyzers--Equipment
Card 3/3
YAROSLAVSKIT, N.G.; STAMICH. A.Ye.
gimplified spectrometers for long-wave infrared region from 20
to 180 Inzh .-fiz. zhur. z2a. 6:50-55 Je '58. (MIRA 11:7)
(Spectrometer)
STANEVICH, A.Ye.--YAROSIAVSKIY, W.G.
ll~~
Comparative study of the radiation capacity of some infrared
radiation sources in the 20-110 wave range. Inzh.-ftz-.zhur.
no-7:49~-53 -Tl 158. (MM 11:8)
(Infrared rays) (spectrometry)
w-M
-~-P-- 4 i
.i-L
AUTHORS: Yaroslavskiy, N. G., Stanevich, A. Ye. S07/48-22-9-38/4o
TITLE: R tation Spectrum of H 20 Vapor in the Range of
50 1500P (20U 7 cm-1)(Vrashchatellnyy spektr parov
H20 v oblasti 5C 1500V (200 - 7 cm-1))
PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheskaya, 1958,
Vol 22, Nr 9, PP 1145 - 1149 (USSR)
ABSTRACT: This report presents the results for the investigation
of the rotation spectrum of H 20 in the range of
50 ' 1500 p at varying steam pressure and under
optimum recording conditions. The absorption spectra
of the H20 vapors in room atmosphere were recorded
with the long-wave vacuum spectrometer D1M,-1 (Refs 11,12).
The thermocouple and the photoelectron optical multiplier
was replaced by an optic-acoustical radiation receiver.
This device was recently developed by N.A.Pankratov
(Ref 13). It permits to measure the absorption spectra
6
of different objects in the range of 50 -, 1500 with
Card 1/2 a maximum resolution of 0,2 0,3 cm an avera&re accuracy
Rotation Spectrum of H 20 Vapor in t*,,e Range of SOV/48-22-9-38/40
50 1500 ~,(200 -.- 7 cm-1 )
Card 2/2
of the wave numbers of 0,02 cm- 1 and an error of the
intensities less than 10~4. The readings are recorded
on an automatic recorder. In order to cover the entire
spectral range 5 interchangeable gratings were used:
three of these with constants equaling 0,0833, o,1666
and 0,5 were produced in the laboratory of F.',,.Gerasimov
and two, with the constants 1,5 and 2,5 were produced
on a precision milling cutter. A thorium. oxide coated
platinum band heated to 15600 was used as a source
of radiation in the range of 50 100 V . In the range
100 -~-- 1500 p a mercury lamp 'MK-4 was used. In order
to exclude the spectra of higner order and that of the
diffuse ohort-wave radiation, a selective modulation
at a frequency of 9 c and reflex filters and pass filters
were used. 105 absorytion bands were recordedin the
entire range investi~;ated. 84 were interpreted to be
ground frequencies of the rotation spectrum and 11
to be second order frequencies (Table). The scheme of
the rotation spectrum is given in figure 2. There -are
2 figures, 1 table, and 13 references, 3 of which are Soviet.
-J
.24(7) SOV/51-6-6-15/,34
AUTHORS Yaroslavskly, N.G. and Stanovich, A.Ye.
TITIE: Rotational Spectma of H20 Vapour and Absorption by Moist Air in the
Wavelength Region from 40 to 2500 Microns (Vrashchateltnyy spektr
parov H?O I porloshcheniye vlathnogo vozdukha v oblasti dlin voln ot
40 do 2500 mikron)
PERIODIGAL:Optika I spektroskoplya, 1959, Vol 6, Nr 6, pp 799-801 (USSR)
ABS TRACT: No experimental data have yet been publisned on the rotational infrared
spectrum Of H20 vapour at wavelengths longer than 1400 It (for the
rotational spectr= of H20 below 1400 -~L see an earlier paper by the
present authors, Ref 1). The present paper reports experimental resultz
obtained in measurement of the infrared spectrum Of H20 vapour particularly
in the region 1400-21500 -p (7.15-4.0 cm-1) a ad absorption by
atmospheric air in the region frcm 40 to 2500 ji. The spectra were
recorded by means of a vacu-um Infrared spectrometer DIKS-1 developed
earlier (Refs 5-7). To cover the whole region from 40 to 2500 ji the auihor-i
used six echelettes of 270 x 270 mm dimensions and the following
constants -. 0.083(3) , 0.166(6), 0.50, 1.50, 21. 50 and 5.00 mm. A mercury
lamp FRK-4 was used as the source and an optico-acoustic receiver
O&P-1 with a crystall1ne quartz window 7ms employed. The spectrawere
ca rd 1/3
SOV/51-6-6-15/34
Rotational Spoctrum of H20 Vapour and Absor-ption by Moist Air ir, the Wavelength
Region from 40 to 2500 Microns
recorded by means of an electronic potentiomater EPP-09. Tho spectra of
higher ordor6 than the first and scattered short-mvelength radiation vere
removed by selective modulation and by various combinations of reflection
and transmisnion filters. Fir, 1 shows the 1000-2500 Ii absorption curve
(II) of a columu of air 7.5 = long at ZOOG and 60~9 reltitiva humidity.
Curve I in Fig 1 raprosents the eminsion spectrum of the mercury lamp
FU-4 recorded uader tne ssuaa conditions as curve 11. Comparison of the
curves I and 11 shows clearly an absorption band of atmospheric air at
1634 IL. This band is due to water vayourn present in air and corresponds
to the transition 2270 3-2 (6-12 cm-1) between rotationai levels of'R20
whose energies were calculated by Benedict at al (Ref 2). This band vas
observed using microradiowaves at ion It (6.14, em-1) by King and Gordy
(Ref 3). Fig 1 shows that, apart from tue band at 1634 MIL, atmospheric
air absorbs very little between 1200 and 2500 IL. Fig 2 gives the
spectrum. of the optical density D In the region 40-25C0 It for a column
of air of length 10 m at 200C, 760 mm Eg ana b0% relative humidity.
Ca rd 2/3
A V151 - 6-'j-1 5/34
Rotational Spectrum of H20 Vapour and Aheorp-tion by Uol5t Air in the ifareleng-th
Region frwi 40 to 2500 Microns
Fig 2 shows that thore are three rogione or high transparon::ys at 3,17AD IL,
1300 -ji and from 1700 i~t to 2500 IL ( and pro',Ably beyond). The authora
point out that the errors in dotemination of the optical aensity in
the last two reglow of transparency were sevoral timeD higher tnan tne
quantity measured. Thore are 2 fiKuros and 7 references, 4 of wnich
are Soviet and 3 Enr.Lish.
Card ~4/3
3 10 66583
SOV/51-7 -5-7/21
AUTHOM Yaroslavskiy, N.G. and Stanovich, A. Ye.
TIT LE The Long-" Navelon&th Infrared Spectrum of H20 Vapours aM ~%bsorotion
in Ataospheric Air in the Ro,-,ion 20-2500 IL (500-4 cm-1).
P3RIODIML; Optika I spoktroskopiya, 1959, Vol 7, Wr 5, pp 626-631 (USSR)
ABSTRACT: The authors reDort a study of the rotational spectrun of H20 at wava-
lengths from 1400 to 2500 IL and of transparency of atnospheric air in
a closed room at wavelengths from 20 to 2500 IL (transparency of air
between 18 and 2500 ji is governed by absorption of water vapour present
in air). A DIKS-1 infrared spectrometer was used in the first order
-with six echelettes of 270 x 270 mm dimensions. Three echelettes with
122 6 and 2 lines/mr, were :~7ade on a precision ruling machine in
F.M. Gerasimov's labor--IDry. The other three achelettes vith 1.5, 2.5
and 5.0 mm constants and a blaze angle of about 100 were zr~do using
an ordinary milling rimchine. The following sources wero used: a
platinum ribbon, -covered -nith yttrium oxide and heated to 120000 (it
was used in the 20-50 1,. ragion) and a morcury lamp IPRK-4 (in the
50-2500 IL region). Optico-acoustic receivers with hermetically sealed
chambers, fitted -~;ith caesium iodide and quartz windows, -were employed.
The spectra were recorded autom%tically with an electronic potentiometer
C-i rd 1/3 EPP-09. The wean error in determination of wave numbers amounted
d2u
]FAR-M
~ -- --7--T 7~
-F,
66583
SOV/51-7-5-7/21
The Long-Wavelength Infrared Spectrum of H20 Vapours and'Abaorption in Atnospheric
Air in the Region 20-2500 ji (500-4 cm-1)
to 0.02 cm-1 and the error in determination of transmission varied
fron 3 to 57~ The spectra of higher orders and scattered short-
wavelength radiation were practically eliminated by the use of coalpensated
selective modulation of the light beam, achisted by means of various
combinations of reflection and absorption filters. In this way the
short-wave scattered radiation was reduced to 3-5%. The results are
shown in Pigs 1-3. Curve I in Fig 26 represents the energy distribution
in the spectrum of the mercury lamp FRK-4, which was continuously pumped
to Iceap the pressure at about 1 mm Hg;, curve II of the sane figure
rapresentA the spectrum of the same lamg when It was filled with air,
which contained 10.5 g- of water per 1 m (relative humidity 60/%*) at
20OG and 760 mm Hg. Comparison of curves I and II shows a clear
absorption band at 1634 ji (V - 6.12 cm-1) -which is due to E20 vapours
and represents a transition between the rotational levels with quantum
numbers J.~" = 22 and J~ = 3-2, whose energies were calculated by
Binedikt, Masson and Shaw (Ref 6). The wava-number of this band
(6.12 cm-1) agrees, within_the experimental error (0.02 am-1), with
the -wave-number of 6.14 cm 1 (1628 ji). determined by microwave
Card 2/3 spactroscopy (Ref 6). The absorption by air in a closed room at
20-2500 )1 is shown in Figs 1 and 2, -where curves I represent the results
66583
SOV/51-7-5-7/21
The Long-Iftvalength Infrared Spectrun Of H20 Vapours and Absorption in Atmospheric
Air in the Region 20-2600 Ii (500-4 cm-1)
obtained at 1 ma H& and curves II represent results obtained in a 7.6 a
long column of air at 760 mm Eg pressure, 2000 temperature and absolute
humidity of 9.5-10.5 &3. The deep minimum on curve I (Fig ld) at
78.5 It (125.5 cm-1) is due to absorption by crystalline quartz of which
the windows In optico-acoustic receivers were made. Fig 3 shows the
results obtained, re-calculated in the form of optical densities D10 for
a column of air 10 a long with 10.5 g/m3 of water. The authors point out
that the precision of measurements of the optical density of atmospheric
air in the regions -where it is highly transparent is comparatively low due
to the small absolute values of absorption. Fig 4 shown that in the regicm
of very low absorption (1200-1500 ji and 1700-2500 ji) the error is several
times greater than the measured absorption. Consequently when absorption
is measured in these regions the length of the absorbing column of air
should be made as long as possible. TbKe are 4 figures and 15 references,
5 of which are Soviet, 8 English, 1 French and 1 German.
B'UBMI TTED i March 24, 1958
Card 3/3
20727
s/o5l/61/010/004/005/007
E032/E314
AUTHORS: Stanevich, A.Ye. and Yaroslavskiy, N.G.
TITLE: Absorption by Liquid Water in the Long Wavelength
Region of the Infrared Spectrum (42 - 2 000 ji)
PERIODICAL: Optika i spektroskopiya, 1961, Vol. 10, No. 4,
PP. 538 - 540
TEXTs The aim of this work was to investignte tho
absorption by liquid water of 42-2 000 1i radiation and to
check on the data reported by Rubens and Ladenburg (Refs. 13,
14) and Cartwright and Errera (Refs. 15-18) in the region up
to 300 IL. The measurements were taken with the vacuum long-
wavelength spectrometer AVK'--', (DIKS-1) described by
Yaroslavskiy, Zheludov and Stanevich in Refs. 20-22. Fig. I
shows the transmittance T and the optical density D of
ordinary water in a 13 4 layer at room temperature. The dashed
curve in this figure shows the absorption constant calculated
from the formulas
Card 1/4
20727
S/051/6i/olo/oo4/005/007
Absorption by .... E032/E314
1
1n -
T
k
41Td
where T is the transmittance in relative units,
X is the wavelength in p, and
d is the thickness of the absorbing layer in 1L.
The analogous results for heavy water are shown in Fig. 2,
In thesB figures, S is the spectral alit width6 -L- . v is
the time constant (sec) multiplied by the rate of recording
(cm/sec). Comparison of these data with those reported by
Rubens et al (Refs. 13-18) shows good agreement at
X = 52, 152 and 313 ji,. The wave numbers of the absorption
maxima shown in Fig. 1 are, respectively, 232, 210, 191,
175, 160 and 145 cm -1 while those in Fig. 2 are 221, 196,
Card 2/4
-P
zu
s/o3l/61/010/004/003/007
Absorption by .... E032/E314
181, 166, 156 and 140 cm- 1.
There are 2 figures and 23 references: 4 Soviet and
19 non-Soviet.
SUBMITTED: September 24, 196o
4 (6 AW
Fig, -1 MV 4. so NO 200 .500 IVOO ZOOO
230 200 *0 100 50 zo 15 10 5
VOCAI-I)
No. 1. 11ponywcanwe (T), onrx4e~Hnn anoTuoe?i. (D) H VOH8ZdTenb norjYou4e-
313111 (k) MHAROR DOAIJ DPH TOnUMIG Uton 0.01111 uv,.,B o6narTif 42-2M wx.
CUCHTpall"Aff MjfVjMA Weall (8 Clt~): I - V - nPOTV8D.'AeHH6* DOCTORHI109 OveXCIVIt (8 Celt.)
nPilemlloycluIRTeAsmoro YCTpOOCTRO un atopam pemcTpatum (a ew-Icen.).
z0
OACm ta
T.U
0.2CM-1
20727
s/o5l/61/010/004/005/007
Absorption by .... E032/E314
Fig. 2:
Tax) B
40 50 100 zoo 300 YOOO ze
too
250 zoo IJO 100 50 20 f5 10
Pitc. 2. flpoaycitauue (T) OUTWIeCttan tMOTHOM (D) a UOHMTenh norno-
inettart (k) IXUAKOR *TgmeroA* BOAunpa Torugime enoit 0.013 mtc n oftam
Card 4/4
STA14EVICHY A.Ye.; YAHOSLAVSKIYP N.G.
. Transmission of organic solvents in the long-wave infrared
spectral region. OptA spektr. 11 no.1:61-66 il 161.
j OUU 14: 10)
(Solvents) (Molecular spectra)
ST,'~!~ZVIGJ!v A.Yue; - 7'0 '61'Iy T' G
.~L J44 d
lnfr~-rad L.-cr;.tion voctixum ~,f the 'qCro~;,jn '-ond
in V,.a lilitit' ard in hydrat3p, DokJ. T'T 15-1
no. Er-kp 161. (:.:IRA 1/,:2)
Teranirrym.
-c, un bo-.4ing-Spoctm)
R-MI,
___ -M
FRISH, S.E., otv. red.; BOB3VICH, U.S., kand. -fiz.-matem. nauk, red.;
VOLIKENSHTEYN, M.V., doktor fiz.-matem. nauk, red.: GALANIN,
M.D., doktor fiz.-mtem. nauk., red.; DRUKAREV, G.F., doktor
fiz.-matem. naukq red.; YEL'YASHEVICH, M.A., akademik, red.;
KALITEYEVSKIY, N.I.,, doktor fiz.-matem. nauk, red.; KUSAKOV,
M.M.,, doktor khim. nauk, red.; LIPIS, L.V., doktor tekhn.nauk,
red.; PEKAR, S.I., doktor fiz.-matem. nauk.. red.; PROKOFIYEV,
V.K., doktor fiz.-matem. nAuk, red.; SOKOLOV, N.D., doktor
fiz.-matem. naukp red.; FEOFILOV, P.P., doktor fiz.-matem.
nauk, red.; CHULANOVSKIY, V.M., doktor fiz.-matem. nauk, red.;
SHPOLISKIY, E.V., doktor fiz.-matem. nauk, red.; YARDSLAVSKIY,
,; LEKSINA, I.Ye., red. izd
_I.G,.-kand. fiz.-matem. nauk, red,
va; PENKINA, N.V., red. izd-va; NOVIGHKOVA, N.D.g tekhn. red.;
KASHINA~ P.S.p tekhn. red.
(Physical.problems in spectroscopy]Fizicheskie problemy spektro-
skopii; materialy. Moskva, Izd-vo Akad. nauk SSSR. Vol.l. 1962.
:2)
471+ P. (MIRA 16.
1. Soveshchaniye po spektroskopii 13th, Lmingrad, 1960. 2. Chlen-
korrespondent Akademii nauk SSSR ifor Frish). 3. Akademiya nauk
Belurusakoy LSR (for Yellyashevich).
(Spectrum analysis)
YAROSLAVSKIY, N,G.
Analytical applications of long-wave infrared spectroscopy (survey).
Zav.lab. 28 no 8:%4-949 162. (MIRA 15811)
ispecitrum, Infrared) (Spectrochemistry)
FILIPPOV., O.K.; YAROSLAVSKIY, N.G.
Transmission of long-wave infrared radiation (40-200A) by heated
crystalline and molten quartz. Opt. i spaktr. 15 n04-- 58-561 0
163e (IL 16:11)
EFSHTSYN, L.,M.; TAROSLAVSKII, N.G.
Long-wave infrared'ispectra'(400-20 am-1) of diphenyl i0donium
Balta. Dokl. AN SSSR 149 ncW865-868 AP 163. (MM 16:3)
I,, Moskovskiy gosudarstvennyy un iversitet im. Lomonosova.
Predstavleno akademikom A.K.Nesmoyahovym.
(Iodonium compounds-Absorption spectra)
MOM
YAROSLAVSKIY, N.G.; KONOVALOV, L.V.
'Long-wave absorption spectra of complex compounds of aniline with metals.
Dokl. AN SSSR 162 no.1:144-146~. My 165. (MIRA 180)
1. Submitted November 9, 1964.
MET
------------
. . . . . . . . . . . . . .
L 05699-67 EWr (1)/EW7 (m) /90(t) /Fri IJP(c) GOAN-rAl')
XCC NRt AF6W352 SOURCS CODEt-w6~67-16&166~loiij-loooi-lbooi~I
AUTHORI Stanevichp A, To,; Taroslavokiy, N. G.
,OROS none
TITLES Absolute emissive power of PRK-4 mercury lamp in the longwave infrared range
(50-2000 4)
SOURCES Optiko-mekhanichaskays. pro?tqshlennostlp no. 5p 1966p 1-4
TOPIC TAWS light eadesion, emissivity,, mercury lamp
ABSTRACTt Masurements of the absolute emissive power of a PRK-4 mer lamp were
I
made under its normal operating conditions (current of 4 A) in the range of 50 to
~?qMjiwith a DIKS-1 spectrometer. -The emitted energy Ev was determined from the sig-
ndl-to-noiae ratio measured at various points of the spectrumq and from the values ob-
ta*nedv the spectral intensity rV was calculated. Comparison of the absolute emissi4e
poker thus obtained with the emissive power of a black body shows that in the range I
ab6,*vo 200 p the radiation intensity of PRK-4 surpasses that of a black body at 1500*p
and~at 1000 A reaches a value corresponding to the radiation of a black body heated to
approximate3,v 60000K. The spectral range for the most effective use of the mercury
lamp and thermal sources of radiation was determined by comparing their relative radi-
ation intensities: in the wavelength range above 130 pp the radiation intensity of the
mercury lamp surpasses that of a thermal source (platinum strip coated with yttrium
UDCS
gum
ACC NRI AP6026352
oxide). However, since the Intensity of shortwave radiation of a mercury lamp is much
lo,wer than that of thermal aources of radiation.. the use of mercury lamps in spectrom-
store with schelette gratings can also be effective in a shorter spectral rangeo
azt. h" t I figure and I table.
ava G=9 13/ SUER DATER O1N*v65/ WM RUB 006/ GM, RUS 004
L
PCtard ?12
CC NR3 AP7005651 SOURCE CODE: uR/o4l3/67/000/002/0100/0101
INVENTOR: Lobachev, M. V.; Sakoltskiy, N. N.; Stanevi~h, A. Ye; ~aroslavjkiy, 17. G.
ORG: None
TITLE: A double-beam spectrophoto*cter. Class 42, No,. 190615 (announced by the
Leningrad Opticomechanical Society (Leningradskoye optiko-mekhanicheskoye ob"yed-
ineniye))
7r
SOURCE: Izobreteniya, promyshlennyye o*6jraztsy, tovarnyye znaki, no. 2, 196T, 100-101
TOPIC TAGS., spectrophotometer, IR optic system, diffraction grating, optic instrument
ABSTRACT: This Author's Certificate introduces: 1. A,double-beam spectrophotometer
with diffraction (echelette) gratings for operation in the far infrared spectral
region (50-1000 V). The luminosity of the instrument is increased by making the grat-
ings 1.5 times longer in the direction of the lines than in the direction of disper-
sion. 2. A modification of this spectrophotometer designed for measuring reflection
spectra. A prism 'is mounted in the cell compartment with reflecting surfaces which
break up the radiation flux with simultaneous displacement of the focusing elements.
1/2 UDC: 5:5-853-36
ACC NR.
YAROSLAVSKrY, N.Ye., inzh.
Glass pipes and their use, &ergetik, 13 no,7:33-36 JI 165.
(MIRA 18%8)
USSR /Zngineorlng
B ilerp High Pressure
0
Scale Removal
"Operation of a High-pressure 33~iler Unlt')'
IP-1. Sipunov, X. Ye. YaroslavskV, Engineers,
4 pp
"Blek Stanta". No 3
At present there are five boiler w7.J+.:; opersting
at 80 atm and 5000 C. Discusses scale removal.,
operation'of superheaters and regalation'of
.superheat, separation of steam, injury to
s of the vater economizer, etc. XconmW of
iw '38/*9T48
US.'Wingineering (Contd).
these high-pressure units still does not exceed
that of average-pressure stations.
49T48
YAROSLAVSKIY, N.Ye.9 inzh.
Design of the heat supply system of the construction site of the Bratsk
Hydroelectric Power Station. Elek. eta. 34 no.11:43-47 M 163.
(KRA 17; 2)