SCIENTIFIC ABSTRACT TSEDERBERG, N.V. - TSEDILINA, YE.YE.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001756920016-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 14, 2001
• Sequence Number: 16
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

It
-e t3i det r inavan 'I the toefficlent 0 &rmid
ryn n e m 0
Pcor.ducr.;ity foi a 94c~ ~by volurne, eolution (if ethyl alcohA
faf th6 t--mperarurc tang 75 to ~ 100 1. _N, I
--t4 ml D L. ru!., t Z T,kh, F,- 25
777 --Ti., .tit -1 tn,,-nal '.-ud d(tJ ("~f (he
range - 73 1~, 2,~-j' ,t i i FT~sturr viJ -a 1(-) ~tm.
In C-~:' '--1 1%e 1hr=)-A - --'d ~-)tb v.'rG-og
temp. T-~c ~,j~ stcatcr tl,.an
:Ani. the VAU~-S 111,1L DA77 and
I. k~%L~r Leach
( I )

.1-1 , - - 'c r,- , r 7
W ;-- I - , I
USSR/Ph,yeical Chemistry - Liquids and Amorphous Bodies. Gases, B-6
AbBt Journal: Referat Zhur - Khimiya, No 1, 1957, 303
Author: .TsederbergAWPV00*
Institution: None
Title: General Relationships for the Thermal Conductivity of Gases at At-
mospheric Pressure
Original
Periodical: Teploenergetika, 1956, Wo 7, 7-11
Abstract: The following formula is proposed for the thermal conductivity A of
gases: Ig WA(kp)) = a lg T + b (lgr)2 + c (ig-c) 3, where Z = T/T .
The following values are given for the constants a, b, and c: ~1)
For lg'r 0,
for diatomic gases, 0.9340, -0-0323, -0.0511; for triatemic gases,
i.44o, 0.0115, 0.2141. The maximum deviation of calculated values
for A from experimental values was � 11%, with an average deviation
Card 1/2

USSR/'Physical Chemistry - Liquids and Amorphous Bodies. Gases, B-6
Abst Journal: Referat Zhur - Khimiya, No 1, 1957, 303
Abstract: of t4.7% (for 15 measurements).
With a literature survey of 6 items.
Card 2/2

-~EDERBEKI, M. I'.; n. L.;
1%.T 41 - Y
"Experimental Determination of the Heat Conductivity of Liquid Oxygen," Zhu.r.ra7
Tekhnieheskoy Fiziki, No 8, Aug 56, pp 1849-18~,'
,,r,.
In an article titled (see above) the authors describe an experimental setup for
determining the heat conductivity of liquid and gaseous oxygen. They 'List the
results of their work and compare them with other published data.
The authors report that their data generally conform with those of BOROVIK (,e.
BCROVIK, Zhuxnal Eksperimentallnoy i tc-oreticheskoy Fiziki, No 17, 1947, P 328)
whereas Hamman's figures are in error by as nnich as 30% (G. Ham;,ran, Annal. d.
Phys., 32, 7, 1938, P 593)
The article presents a detailed description of the experimental methodology
and includes several drawings and -tables.

AID P - 5005
Subject USSR/Engineering
Card 1/2 Pub. 110-a - 7/17
Author Tsederberg, N. V., Kand. Tech. Sci.

Title Thermal conductivity of liquid binary solutions
Periodical Teploenergetika, 9, 42-48, S 1956
Abstract This paper presents the results of experimental
investigations of the thermal conductivity of ethyl
alcohol solutions in water. These tests were made for
checking the accuracy of results obtained by 0. K. Bates.
The methods of testing are described, and the author
compares his data with those of various foreign and
Soviet scientists. Recommendations are suggested for
applying the additive rule for the determination of
thermal conductivity on the basis of 15 solutions,
7 tables, 4 diagrams. 21 references.

Teploenergetika, 9, 42-48, S 1956 AID P - 5005
Card 2/2 Pub. llo-a - 7/17
Institution : Moscow Institute Of Power Engineering
Submitted : No date

Name;.-TSEDERBERG, Nikolay Valerianovich
Dissertation: Heat conductivity of liquid solutions
and compressed gases
1, Degree: Doe Tech Sci
b Affiliation: fnot indicateg7
Defense Date, Place: 29 Jun 57, Council of Moscow Order of
Lenin Electrical Engineering Inst
Certification Date: 10 Nov .57
Source: BMVO 24/57

r~u.
ril U-71 F~:;r
7i

rOPOV, V.N.; TSEENREMM, N.V.
Experimental determination of the heat of vaporization of liquid
fuels, Nauch. dokl. vys. shkol7; energ. no.1:161-168 '58.
(MrRA 11:10)
l.Rekomandovano kafedroy TOT Moskovskogo energaticheskogo instituta.
(Liquid fuels) (Heat of vaporization)

TSEMBERG, N.V.
Heat conductivity of a binary nolution of benzene in ethyl
alcohol. Nauch.dokl.v7a.shkoly; energ. no.4:189-193 158.
04IRL 120)
1. Rnkonandovana kafedroy tooraticheakikh nenov toplotekhniki
Moskovskogo energeticheskogn tnatituta.
(Hnat--Conduction) Onmene) (Ethyl alcohol)
vt*

Tech. Sc i. SOV/06-58-10-15/25
AUTHOR: 4pederberr
Popov, V.N. (Engineer)
TITLEt An experimental investigation of the thermal conductivity of
helium. (Eksperimentallnoye issledovaniye teploprovodnosti geliya)
PEMODICAL: Teploenerfretika, 1958, No.10. (USSII) pp. 61-65
0
ABSTRACT: 'Published work on the thermal conductivity of helium is reviewed.
experimental values over the pressure range of 1 - 212 kg/cm?-
have been published in only one work and relate to a temperature of
42.80C. The most reliable data for the temperature range - 200 -
+ GOOOC, at atmospheric pressure, are given in Table. 1. The maximum
error in these determ:Lnations is 1.83%. Determinations were made
of the thermal conductivity of helium under pressure, using the
hot-wire method in a glas13 measuring tube. At pressures up to 100
kg/cv.4 a steel bottle of helium was used, and at higher pressures a
mercury compressor. The helium was 99.8% pure, the remaining 0.2%
being nitrogen. Me measuring tube was in t'.ermostatically controlled
water, glycerine or molten salts, according to the temperature.
The apparatus is described, also the method of use and the way of
working out the results. Correction for radiation from the wire
and for the leads is explained. The main characteristics of the
measuring tube are given in Table.2. The methed of ageing is
described. The equipment was checked by determining the thermal
Card 1/2 conductivity of air, comparing the results with those of other authors.

An experimental investigation of the thermal conductivity SOV/96-58-10-15/25
of helium.
Agreement was to within 0.5% of the most reliable values. Graphs of
the thermal conductivity of helium an a functign of temperature on the
isobars of 1, 100, 200, 300, 400 and 500 kg/em4, and the results of
controlled tests at 10 kg/c~2, are given in Fig.3. The scatter of
experimental points does not exceed 1%. Published data of other
authors is included and agreement is good. The use of a logarithmic
co-ordinate system is proposed and the experimental results are plotted
in this system in Fig.4. Equation (2) accurately represents the
thermal conductivity of lielium under pressure. Calculated values of
the therm 1 conductivity recommended for practical use are presented
in Table.3. There are 4 figures, 3 tables and T Soviet references.
ASSOCIATIONz Moscow Power Institute (Moskovskiy Energeticheakiy Institut)
Card 2/2

SOV/96-5,",-13/?l
AUT'TIOR:
TITLE:
PERIODIC.'--~L:
ABSTIL-11CT:
Card 1/5
Popov, VJT. En6ineer
Doctor of' Tectmicul Sci,2uce
Vic Thermal Coiiductivity of Liquid Fuels
(Teploprovodnost' zhidkikh topliv)
-4 t;
Tcploene-r6-1ti'-u9 19581".Nr 11, pp 7?-76 (USSR)
ZxistinL: wor- on the thermul conductivity of liquid
fu,!!1, m-Linly .'merican and German, is briefly n~ferred
to. In Teplo-~~nar~~etiku 1957, Nr 8, the present
authors. described word- on the thermul conductivity of
1-eros,ni~,. The Predvoditelev-Vurj~aftit- formula for
calcul.Ainr, the thermul conductivity of' pure norraul
liquids is Ljv,~n. In order to virify the vulidity
of this formulu for othar muterials, deterrainLt ions

SOV/96-5 Pi-11-131?1
The Thtrmal Coiiductivity of Liquid FU-.18
of tlv~,n tt,)-erm-j conductivity, dcnsiL.
-,jLjt ty a~ad
rqp~cj fic li,~-It for bcnzino~ B-79 , diesel fuel Ii'o.3
with I sp-!cific '~;ruv~ty A ?0 C of 0.843 und initial
boiiilaL point Of 1'30 C, nd dits~l fuel I-Io.4.
with d Sptcific ';r'.jvity at ?0 C 8f 0.850 1-ty'litre
,.Lnd initial boilinp; point of' 190 C. TLe "ppurent
moLneular 7,,ei,.hts ird viscosities of thes,! fuels
d,~t,~rnqin,.!d by w.V. Swmcir~ivulova and
R.zj. Sul,~ym.:.nova. The thermul conductivity of the
:rael wa- dttermined by the use of four mntsurin~-,
tubes Similur to thost described in the prnvious
f-!~ the m.:.dn chLiructeristics of the tubes are
,~iv,nn in Tuble 1. The themul conductivity of
benzino.- B-70 vi"s investitLated at a pressur- of
10 atm ov~-r the temper-iture run6e +90-+110 0C. Vie
r2sults urn plott~!d in Fi6.1. and recorded in
Tablx.% I. The th?!rmul conductivities of diest!l
fuels NOS-3 und 4 .,Iere dttendned at 10 ed 50 atm
c)v,!r the temptr,itur,! run6,! - 50 to + ')50 C. The
Card p,15 r!sults for tilt form,!~r Lire j,~ivmn in aiid
Tuble 3 and for the latter in FiL;.3. und Tubl,~! 4.

S011/96 -5 3-11-13/21
Th,!~ Theri;iul Conductivity of Liquid Fuels
Th:~ root m(-,in squure error of individuul de. t erminut ions
of tKe.M,~l conductivitY is 1.3,,. Th~! rillitionship
betw-2.3n th-~ sp,~cific ---r-vity und tempertturt~ of Fu!!!
C.~
NO-3. ut vuriou-s press-arts is plotted in Fi8.4. und
t-.~bulat~-d in TLIjlt 5. Simil-Lr data for fuel ',.To.4.
-Lr~- given in FiL;.5. and Tuble 6. Table 7 ,,ives the
sp,~!cific k~r~ivity of benzin,~ B-70 "t atmosphe-ric
rt. The rilutioiisKip betw~,-in tne --pecific
rr,!ssu
L!!--A and thn tem-o!-r-Lturt Of fuel 110-3. at cor~.stunt
prtcsur,! is ,-iven in FiL~.6. and Tubl,! 8. Similur
du~tu for th~-- fuel 1ro.4. art biven in Fi-,-.7. and
Talul-!~ 9. Vulul!s of the specific heat o? benzine
T70.B-70 are ~ivem in Table 10. It vill be sn-in
frOm Fil's.110S.6 and 7. thut the pr~~ss-ar-! lhus no
c'
,-!ff-!ct or, t-i,-! sp~!cific Lnut in tl-.,e ran6e of 1-50 atm.
In order to verify tht accurucy of the of
Crue,oe (U.S. of Standards) and Pr,-dvoditel,!v-
Var,~uftil- the th,!r.%iul conductivitito of bl-,nzine B-70
11,Ard 3/5 and th,! tw diesel fuels wer!! calculated by these

The Therm,;.,11 Conductivity of Liquid Y`uels
SOV/96-5 P,-11--"3/?l
formulae uiad compurtd Uitil thC exp!nriaentul re-sults.
It is concluded that Cru6oels formula is in,kccur-,te
,Lnd that thf- Predvodittl~--v-Var-uftik formulu ~Lives
the absolute vulu#-, of therra,l conductivity of the
fu,~I- to -aithin 101,'4-'. The appurent molecular wei.lits
of th~- f~a,~ls in qu,~stion are biven in Table 11 us
(,,,--t,!-rminnd by a cryoscopic method. Experimental
results for the tla-erm,,~l conductivity us z.L function
of ttmpiruture ut atmospheric pressure for all the
fuels investi,-,uted in the present work are plotted
in Fi,;.8. Which also Lives data for 1~erosene T-1
and its h~!avy fractions. .'Jn empirical formula is
offer,nd for calculation of the thermal conductivity
of fuels ir. the specific ~,,ruvity ruriL.,! of 0.750 to
Card 4/5 0.850 kg/litre. This formula L;ives results

SOV96 -5
TF-~,- Thcrin-tl Co)iduotivity of liquid
,-j.ccurutt to within 4c, tho! o-Y.Lly dutu 6equired is
-.p-icific ~-r-~-vity of ti-i- fu-1 :it C. Thnr-
f'i r-r;, I I t.', 5 Sbviet references.
IISSOCIATIOil: Mosl-ov--iy iL.-titut
(MOSC-0'.7 POVV~r In.9tit-ate)
Card 5/5
lp

TSEDERREM, N.V.
Formulas for calculatIne the thermal conductivity of binary
solutions of liquids. IIauch.4okl.vys.shkoly; energ. no.l:
159-168 159. (KIRA 120)
1. Rnkomondovana, kufodroy tenraticheekikh oBnov toplotelthniki
Moskovskogo energaticheskogo instituta.
(Solutinn (Ghnnistry)--TableR, etc.)

AUTHORS: Tsederberj5,.JN.-,,.V.,,Doctor of
Morozova, N. A Engineer
X
TITLE: The Thermal Conduct vit of Carbon
from 1 to 200 kg/cm a Tem::)eratures
PERIODICAL: Teploenergetika, 1960, Nr
67647
SOV/96-60-1-16/22
Technical Sciences and
Dioxide at Pressures
up to 12000CY%
1, pp 75-79 (USSR)
ABSTRACT: There is increasing interest in the thermal conductivity
of carbon dioxide. Relevant tables have already been
published, particularly by Vargaftik, but further reliable
experimental results have since become available and
there was a need for values at higher temperatures than
he quoted. The present article uses published data on
the thermal conductivity of carbon dioxide to formulate
tables ranging up to 12000C. Use was made of the results
of numerous authors, and all their experimental values
for thermal conductivity of carbon dioxide are plotted
in Fig 1, which also gives the mean curve. The values
obtained by various authors are discussed. The mean
curve was used to determine the values of thermal
conductivity of carbon dioxide for temperatures from
Card 1/3 - 75 to + 12000C which is given in Table 1. The range

67647
SOV/96-60-1-16/22
The Thermal Co~ductivity of Carbon Dioxide at Pressures from
1 to 200 kg/cm. and Temperatures up to 1200 C,
from 800 to 12000C was covered by extrapolation. A list
is given of the data used to plot the thermal conductivity
as a function of pressure and temperature. Fig 2 gives
a graph in logarithmic coordinates: the difference
between the thermal conductivity at any given temperature
and that at atmospheric pressure and temperature is
plotted as a function of the specific gravity of carbon
dioxide at the test temperature and pressure. A mean
curve was plotted on this graph and equation (2)
corresponds thereto. Again the results obtained by
various authors are critically reviewed. Eq (2) was
used to calculate val-ues of the thermal conductivity
at the extreme ends of the curves, gt the critical point
and on isobars from 30 to 200 kg/cma up to the temperature
of 10000C. Fig 3 gives a graph of the relationship
between the thermal conductivity of carbon dioxide and
temperature from 0 to IOOOOC on isobars from 1 to 200
kg/cm2. The graph indicates that the thermal conductivity
Card 2/3 alters considerably with the pressure near the critical

67647
SOV/96-60-1-16/22
The Thermal CoBductivity of Carbon Dioxide at Pressures from
1 to 200 kg/cm and Temperatures up to 12000C
pcint. Graphs of the relationship between the thermal
conductivity and pressure along the isotherms close
to the critical temperature at temperatures of 32, 35
and 400C are plotted in Fig 4. Table 2 gives values
of the thermal conductivity of carbon dioxide on the
320C isotherm, Table 3 on the 350C isotherm and Table 4
on the 400C isotherm. It is concluded that the data
are in error by not more than 2%, and are thus more
accurate than Vargaftik's earlier tables. There are
4 figures, 4 tables and 22 references, 10 of which are
Soviet, 8 English and 4 German.
ASSOCIATION: Moskovskiy energeticheskiy institut (The Moscow
Power Institute)
Card 3/3

69205
S 2-00 s/096/60/000/06/018/025
E194/E284
AUTHORS: ,TsedP-rbQ-rK...N.- Doctor of Technical Sciences,
Popov, V. N, Candidate of Technical Sciences, and
Morozova. N. A., Engineer
TITLE: An Experimental Investigation of the Thermal Conductivit
of ArgonA
PERIODICAL: Teploenergetika, 1960, Nr 6, pp 82-87 (USSR)
ABSTWM: Previous experimental work on the thermal conductivity
of argon is reviewed. Published values for the thermal
conductivity of argon in the temperature range from
-200 to +6000C at atmospheric pressure from a number of
authors are plotted in Fig 1. Available experimental
data for the thermal conductivity of argon in the
temperature range from 300 to 11000C at atmospheric
pressure is plotted in Fig 2. It will be seen from
-200 to +200uC there is good agreement between the
results of all authors but there is increasing divergence
at temperatures above 2000C. The thermal conductivity
of monoatomic-gases at atmospheric pressure may be
calculated by expression (1) and the curve for argon
for temperatures of 0 to 6000C constructed by means of
Oard 1/4 this equation is plotted in Fig 1 and in general

69205
S/096/60/000/06/018/025
E194/E284
An Experimental Investigation of the Thermal Conductivity of
Argon
agreement is good. Values for the thermal conductivity
is argon at atmospheric pressure over the temperature
range of -200 to +6000C corresponding to the curve
given in Fig 1 are presented in Table 1. Higher
temperatures are not considered in the present article
because of the great; differences between the published
results of various authors. The thermal conductivity
of argon under pressure was studied by the hot wire
method using two glass measuring 1;ubes. The instrumenta-
tion and experimental procedure are described and the
method of working out the results was the same as that
used in determination of the thermal conductivity of
helium described in an article by the same authors in
Teploenergetika, 1958, Nr 10. The principal characteri-
stics of the two measuring tubes used in the tests are
given in Table 2. In checking the apparatus measurement-
were first made of the thermal conductivity of air and
good agreement was obtained with published results as
Card 2/4 will be seen from the graph plotted in Fig 3. Graphs

69205
S/096/60/000/06/018/025
E194/E284
An Experimental Investigation of the Thermal Conductivity of
Argon.
of the thermal conductivity of argon as function of
temperature on isobars ranging from 1 to 500 kg/cm2 are
plotted in Fig 4, in the majority of cases the scatter
of experimental points did not exceed 2.5%. Values of
thermal conductivity obtained by other authors are also
plotted in Fig 4 and it will be seen that the present
authors are in good agreement with some other published
work. On the basis of available experimental data
calculationsv.ere made of the specific gravity of argon
over the temperature range from2-90 to 10000C and
pressures from 100 to 500 kg/cm and the results are
given in Table 3. Table 4 gives values of the specific
gravity of argon on the upper and lower boundary curves.
Fig 5 gives the results of experimental data on thermal
conductivity of argon under pressure obtained by various
authors when plotted in terms of Eq (3), which is the
Card 3/4 empirical form of Eq (2) and it is concluded that this

59205
S/096/60/000/06/018/025
E194/E284
An Experimental Investigation of the Thermal Conductivity of
Argon
equation accurately describes the thermal conductivity
of argon under pressure. Table 5 gives values of the
thermal conductivity of argon at high pressures
calculated by means of Eq (3) and recommended for
practical use. There are 5 figures 5 tables and 22
references, 8 of which are Soviet, 11 English and 3
German.
ASSOCIATION: Moskovskiy energeticheskiy institut (Moscow
Power Engineering Institute)
/4

QQJ1/o96/6o/ooO/O1O/Ol2/0 2 2
E19VE135
AUTHORS: Tsederberg,-E.V.7 Popov, V,,N,,, and Morosova, N.A.
TITLE: Investigation of the Thermo-physical. Properties of
Helium in the Pressure Range 1 to 200 kg/cm2 and
the Temperature Range 0 to 6oo Oc,
PERIODICALs Teploenergetika, 19609 No 10, p 95
TEXT: The experimental equipment is described. Equations
are given relating the thermal conductivity and viscosity of
helium with temperature and pressure, and tables,of thermal-
physical properties are given, The tabulated data of thermal
conductivity and viscosity are determined on the basis of the
authors' own experimental work and also published work.
ASSOCIATION: Moskovskiy energetichaskiy institiit
(Moscow Power Institute)
Card .111

TSEDERMGI dikolay Valerianovich; POPOV, Valentin Ilikolayevicb; MORO-
-I--- -,- -- - ZOVA', Nadeihda AnIsImovna; FASSKAZCVp D.S., red.j VOROVIL, K.P.,
tekbn. red.
(Thermal and physical properties of,bellum) Teplofizicheskie svoistva,
geliia. MosWag Gos. energ. izd-vq, 1961. 3.18 p. (NMU 14: 8)
(Helium)

A11DRYUSHCHFNEO, A.I., doktor tekhn,nauk, prof.; TSEDLIU1111-K, N.V., dok-tor
tekhn.nauk, prof.
Problems concerning research in the field of therma'a Pleclric pwer
production. Izv. vys. ucheb. zav.; energ. 4 no.10:52-;5 0 '61.
(MIRA 14:11)
1. Saratovskiy politekhnicheskiy institu-, (for And-yushchenko).
2. Moskovskiy ordena Lenina energeticheskiy institut (for TSederbcrC),
(Steam power plants)

ACC N.R; G 27 57
Popov, V. X.; '&ocdorbcrj, N. V.; ..'orozova,
k;:"~;: .-,Ozco-.. 111stitto of `x;titut'
-.)o.-ii:::n-.al dotcr,~dnation of I-,cat ccyac~
ty of liquid pot-roloun jproduc'3
!'J-L;Z. "Oft' i no. 3, 11"66, W and p. 86
Ne/j r nqrv) 0/ 7 y
Tk~21C '2XS: petrolouz, produc It,' petrolcum fucl, diezel fuel, lulbricatin_r oil D5 (~ir-CU-.
fuel, '.S-1 petroleum fuel, 1-:-3 lubricantin- oil, lubeicatii,,Z; oill
tew;G DS dzezcl
-M The authorz -zirccent the rcivults of heat capacity o
fual (density 0.837 c/cu' cm), TS-1 fuel (0-7806 d cu C-3), ::-3 lubricatino oil O.b74
r-Icu cm) and AYl lui)A-catinC o-:1 (0.923 L/cu cz:). A calorimeter wish an adialu'-tic c-L
closure -,.az uscd for tostr' a'. atmomaheric pres--ure whilo for hij~%or prozouress an
cnclosurc was a?:)1icc!. 'Mo calorimatar3 wore c~-Icclkcd for tho kno;m ca-pacizier, of tollueno
an"- water, as in two ~;ra,)hs. ~`Iiu rasults of testo at different tcmi)oratur~:j ara
presented in two tabler. of wliich the fir3t. covers the testo perfori.-.ed at a prosz-are of
1 'CC/sq cm and tho second at 3 kr-/sq cm. OriG. art. has; 2 Graphs, 2 6ablc*.
S*,;.3 CODE: 9-1 / SUB:.', DATE- 10-Fob65
Card
UDGs 66~-5-,536*22.001.5

TSEDFRBERG, N.V., doktor tekhn. nauk, prof.; POPOV, V.N., kand. takhn. nauk;
I.I., inzh.
Expoirimental study of the visr;oalty of hydrogen. Teploenergatika 12
no.4s84-86 Ap 165. (MIRA 180)
1. Moskovskiy energeticheskiy instltut.

POPOV, VX. ; TSi,:!,,F7;,,jF*-. K;i.(),
Fxp(-,rJr,.ental fnvesstli,r-~~T.-,(,n cl' '.-e
petroleum ixoducto. Iz-,,. !;cheb. mv.; neft' i uaz P --,l:
79-81 165.
NA~v
Lo
ay~ R
'CM,

W-4
M.
IR-117RN
m - -1 1
M
M
ul

T~';I-I'liSALLUG, N.V. ; MCROZOVA, t1. A.
Expc-rimenf,al invostirratior, of t~,e ~,,aat con'dictiviv of fc.-7
petrolewn productp sanpl3:3. Izv.vys.,jcheb.zav.; no!'t' i pj;-,
no-4,71-74 164.
.MMA
1. Vozkovskly r-nr~rgt~--tichaokly instil~utl.

MAKAVETSKAS, R.A.; :OPOV, V.N.; TSEDERBERG, N.V.
Experimental study of the viscosity of helium and nitrogen.
Teplofiz. vys. temp. I no.2:191-197 S-0163. (MBA 17;5)
1. Moskovskiy energeticheskiy institut.

MAKAVETSKAS, H.A.; POPOV, V.N.; TSEDERBERGO N.V.
Experimental study of the viscosity of mixtures 6i'citrogen and
helium. Teplofiz* vys* tomp. I no-3:348-355 N-D 10. (MIRA 17:3)
1. Moskovskiy energeticheskiy institut.

ACCESSION NR: AP4004139 S/0294/63/001/002/0191/0197
AUTHORS: Makavetskas, R. A.; Popov, V. N.; Tooderborg, N. V.
TITLE: Experimental determination of the viscosity of helium and
nitrogen
SOURCE: Teplofizika vy*sokikh temperature, v. 1, no. 2, 1963, 191-
197
TOPIC TAGS: dynamic viscosity, viscosity, helium, helium vis-
cosity, nitrogen viscosity, gas analyzer, gas analysis, gas property,
gas viscosity, nitrogen, helium nitrogen mixture
ABSTRACT: With an aim at filling the temperature gaps in the exist-
ing experimental data, the coefficient of dynamic viscosity of
helium, nitrogen, and their mixture was investigated experimentally
in the temperature range 10--6600C and in the pressure range from 1
to 600 kg/CM2 using the method of Professor D. L. Timrot (Izv. VTI,
Card

ACCESSION NR: AP4004139
No. 3, 1940), which employs a capillary and an annular balance.
The smoothed data obtained from several sets of isotherms agree with
the experimental values within 2%. Orig. art. has: 3 figures, 5
formulas, and 3 tables.
ASSOCIATION: Moskowskiy energeticheskiy institut (Moscow Power
Engineering Institute),
SUBMITTED; 03ju163 DATE ACQ: 26Dec63 ENCL: 02
SUB CODE: AS, PH NO REP SOV: 004 OTHER: 006
Card 21t?,

AM4006932 BOM EXPLOITATION S/
Tsederberg, Nikolay'Nalarianovich
Thermal conductivity of gases and liquids (Tcploprorodnost' Lazov i zhidkostoy)
Mose 01TO I GosenergoA'zdat , 1963. 4.0'8p. illus.,biblio. Errata slip inserted.
Editor: D. S. Rasskazov,, Technical Editor; N. A. Dulldyayev. 6000 copies.
TOPIC TAGS: thermal conductivity of gases, thermal conductivity of liquids,
hot wire measuroment, coaxial cylinder measurement, dilatometric measurement,
Burhorn apparatus, 13 000 K moasurem.-nt, Sonin polynomial, nitrogen plasma,
inert gas mixturcs, air plasma, additivity, clectrolyto solutions, liquid
petro'leua products
r-URPCSE A24D COVERAM This book is irl-ended for the parsonnel at scientific-
research institutes and design organization.- and bireaus, engineers and tech-
nicians in industry, and aspirants and students in higher educational institu-
tions 7
ExistinC experimental methods of measuring thermal conductivity are
reviewed, and basic typical experimental installations are described. Far-isti;ng
theories of the tharmal conductivity of Cases at atmospharic pressure and
formulas for computing the tbermal conductivity of gases and liquids and their
Card 1/3

AU4008932
mixtures are reviewed. Generalized relationships for the thermal conductivity
of gases at atmospheric pressure a-4 its dependence on pressure and temperature
are prezented. Reliable data are presented for the thermal conductivivy of
pases and liqaIds and their mixture.- for wide ranges of temperature and pressure.
Thanks are expressed to N. A. Morozova for rendering the author invaluable
aid In illustrating the monograph.
TABLE OF CCNTENTS (abridgedW
Foreword - - 3
Introduction - - ?
Ch. I. Basic methods of experimental determination of the coefficient of
thermal conductivity of gases and liq:aids - - 12
Ch. IL Review of formular, for computing the thermal conductivity of gases 11,"
Ch. III. Deteraination of the temperature dependence of the thermal conduc-
tivity of gases at atmospheric pressure - - 146
Ch. W. Computing the thermal conductivity of gases under presgure and in the
liquid state - - 160
Ch. V. The thermal conductivity of gaseous mixtures 231
Card 2/3

A)14008932
Ch. VT. Methods of computing the coefficient of thernal conductivity of a
plasma 261
Ch. V11. The th,-r--al conductivity of 1-4,quid-s at atmospheric pressure 224
Ch. VIII. The ther,--al conductivity of liquidc .inder prossmire 317
Ch. jX. The thermal conductivity of 'Liquid solutions at atmospheric pressure
323
Ch. X. The thermal conductivity of aqueous solutions of electrolytes 343
Ch. 'X.I. Thermal conductivity of liquid Dotroleum products and its dependence
on to-mperature and pressure 359
Literature 389
SUB CODE: u. PH
GTHER: 183
Card 3/3
Card
SUB1111TTEED: 26,TUN63
DATE ACQ: 290ct63
NR REF SOV; 197

TSEDERBERG, V. V.
"The Wool Quality of Kazakh Fine Fleece Sheep." Cand Sci, Inst of
Animal Husbandry, Alma-Ata, 1953. (RZhBiol, No. 7, Doc 54
Survey of Scientific and Technical Dissertations Defended at USSR Higher
Educational Insti.tutions (12)
SOs SM4. No. 556, 24 Jun 55

TSEI&WO. TeA Talerianovaa, kandidat sell skokhozvavstvennykh nauk;
,. F
SRVMO, Z.A., redaktor,- ZLOBIS. M.V.. tekhnicheskI7 redak-tor
[More high-grade wool] Bollshe vysokokachostveano7 shersti. Alm-
Ate. Kazakhskoe goe. Izd-vo, 1956. 22 p. (HLRk 9:10)
(Wool)

YEFREMV, G.V.; ZVEREVA, M.N.; TSEDUSUREN., TS.-
Separation of thallium from element impurities on an anion
exchanger. Zav.lab. 28 no.2:159-161 162. (MIRA 15:3)
1. Leningradekly gosudarstvenrqy universitet.
(Thalliumz-Analyois) (Ion exchange)

oifl L, F
US)3R/Cultivable Plants - Grains. H-2
Abs Jour Ref Zhur - Blol., 110 3, 1953, iqj46 K.
Author Tsedik-Tomashevich, Z.F., Skvortsrw, j~d-it-
'Inst
Title Corn in 1955- Zia 6. 1he Rayons of the South of the 11"35H.
-,) krip !ck
Orig, Pub 11,;oshva, Seilkh-):,giz, IJ-1 p,)., Ulus., 4 ruble-, N S
Abutrac.' No abstract.
Card L/-.

TSEDIK-TORASIIEVICII, Z.F., kandidat 'biologinheskikh nauk; SKVORTSOV. S.N.,
rAWM, P.r.."redaktor; PA72(3R, V.I., tekhnicheakiy radaktor
[Corn In 19551 Kukuruza v 1955 godu. Moskva. Goo. izd-vo selkhoz.
lit-ry. NO-3. [Southern districts of the U.S.S.R.] Ralony luga
SSSR- 1956. 380 P. (MIRA 9:9)
1. Nachallnik otdela rastenevodotva Glavnogo upravleniya sellsko-
khozyaystveanoy nauki Ministerstva sellskogo khozyaystva SSSR
(for TSedik-Tomashevich) 2.'.Glavnyy agronom otdela rasteniyevod-
stva (for Skvortsov)
(Ru-.sia, Southern--Corn (Maize))

1. TSE-DIK-TORASHEVICH, Z. F.
2. ussR (6oo)
4. Science
7. Protocol for drawing up scientific reports.
Doet. sellkhoz. No. 11, 1952
9. KonthlX List of Russian Accessions, Library of Congress. March 1953, UnclRssIf ied.

1. TSMIK-TOVASHMCII, Z. F.
2. ussR (6,oo)
4. Report Writing
7- Protocol for drawing up scientific reports. Dost. sellkhoz. no. 11, l-,52.
YonthL.- List of Russian Accessions, Library of Congress, March 1953. Unclassified.

1. TSEDjK-TPj-IASHEVjCH. Z. F.; NECHIMEUKO, N. A.
2. USSR (600).
4. Agriculture - Experimentation
7. Work results in scientific research institutes on agriculture for 1951.
Dost. oellkhoz. no. 5, 1952
9. Monthly List of Russian Accessions, Library of Congress, January -1953. Unclassified.

TSEDIK-TORASHE'JIMIt Z. F.
Trees
Intra-and interwretal relpWonshirs ~.etween trees. Sel. i scm. 19 NO. -., Y1.52.
9. Monthly List of Russian Accessions, Library of Congress, October 1953. Unclassified.

Trees
Intra- and intervarietal relationsi-.iTs ,,etween tre(:s. -Eet. i se.
Monthl- List of' ",.ussian Accessions, Librt~ry of ConFr(!ss, October

Bricks
Porous brick. bell. stroi. 2 no. 6 1'/47.
l'ontlily List of Lussian Accessions, librux-y of March

VORONOVA, Mariya, 7,tnr,,. lyevna; TSEDILIN, I.V. , red.
(AxaLlysis of the adninistrative operations of fishing
Industry enterprises] Analiz khoziaistvannoi deiatell-
nostl predpriiatit rybnoi promyshlennosti. Moskva, Fl-
nansy, 1965. 203 p. (MIRA 18s4)

De"ITRIYEVA, R.I.; ZHAGIRNOVSKIY, S.G.,- EOINAKOV, D.S.; HOMNIS,
Ya.l.; SD'OIOOVA, TS.Y.; TSEDILL, I V - SIIEYGA,',', G.I.;
X. I vG!IA, 'I
SMIMR) Y.D.; UZURIMICH? . red. i zd-va; TEIZ A . ,
tekhn. red.
(Auditing financial operations of the enterprises of regional
economic councils] Proverka finansovoi deiLtellnosti pred-
prilatii tioviiarkhozov. (MIRA 15:2)
(Industrial management) (Finance) (Auditing)

TSEDILIF,, S.A.; TSETLIN. V.14.
Siren for V;e acoustical coagulaticn of aerosols. Ak.-ust. zhur. 7
no.1:78-86 161. OMIRA 14:4)
1. Gosudarstvennyy nauchno-issledovatellskiy institut tavetnykh
metallov, Moskva. (Aerosols) (Coagulation)

20238
S/C"yr'j 1/007/CC1 /0071,/01';,
F000 -3, //SY) Bi 0,,B2C4
AUTHORS: Teetlin, V. M.
TITLE: Siren for acoustic coagulation of aerosols
PERIODICAL: Akusticheskiy zhurnal, v. 7, no. 1, 1961, 78-86
ThAT: The siren described was developed and tested by the Institute men-
tioned under Association. It is an axial sound generator, which is smaller
and of simpler structure than radial sound generators, and requires no
parabolic reflector. The fundamental frequency of the sound produced is
6-7 kc, and the intensity depends on the passat;e of air. Stator and rotor
are circular and have 75 openings wilha diameter of 3.9 mm on a pitch diarne-
ter of 200 mm. Fig. 1 shows a section of this siren. The ground rotor co!-r-
sists of an aluminum body,onto which a steel disk with 75 ope-.-.irrgs is
screwed. As may be seen from Fig. 1, air inlet 1 and stator 2 of the system
are detachably connected, which is of advantage especially for adjusting
the air -ap between rotor and stator. As maybe seen from close investioa-
tions of this siren, the aerodynamic resistance of the siren itself is not
great at the given working conditions. It follows herefrom that a decrease
Card 1/6

Siren for acoustic ...
20238
S/046/61/007/001/009/015
B104/B204
of the aerodynamic resistance in the air supply of the siren increaseethe
efficiency of these sirens. For measuring the sound intensity, the effec-
tive sound pressure was experimentally determined. In Fig. 3, the intensi-
ty I and the logarithmic level L are graphically represented as a function
of the radius. Further, it follows from the measurementathat the direction
diagram of the siren depends considerably on frequency. Measured results
concerning the acoustic efficiency are given in Table 3, where the efficim-r-
oy was calculated by means of formula I - N/QR, where 11 is the acoustic ef-
fi2iency of the siren, Q is the air consumption, and R the aerodynamic
resistance. Close investigations carried out on a coagulation chamber
having a length of 10.9 m and a diameter of 610 mm, which was erected in a
perpendicular position, were carried out. As sound insulation, a 100 mm
thick layer of slag was used. During the experiment, the coagulation cham-
ber was open at the bottom, while the siren was on top. In Fig, 79 L and I
are graphically represented as function of the radius.(as in Fig. 3),
measured at a distance of 5.45 m from,-the mouth of the siren. As subse-
quently stated, the siren described meets the demands made on it. There
are 7 figures, 6 tables, and 2 Soviet-bloc references.
Card 2/6

20238
S/046 61/OC)7/001/00
Y 9/015
Siren for acoustic ... 3,
3204
ASSOCIATION: Gosud arstve nnyy nauchno-i ssledova teltakiy institut tsvetnykh
metal lov Mo skva (State Sc ient i'Pic Research Institute of
Nonfe rrous Metals, Moscow )
SUBMITTED: April 19, 1 960
Legend to Fig. 1- 1) .1,1ou th; 2) stator;
10) 'rotor. (For Fig. 1 see card 6 of 6)

4 2
I X-
* ff.em i1 6
L,06 N,fm -~-,(Aj,1CK
Cm
N
I).%%
1.5 79 146 6 14.9 675 14,0 4,5 73 t47,2 17,1 855 14 6
1,5 117 149:7 30,4 921 10,6 4,5 107 152,6 59,2 1975 18:3
1,5 168 155,7 121.0 2576 18.4 4,5 157 158,0 253,0 5750 29,0
1,5 193 158,6 235,0 431!0 22,4 4,5 165 WO, I 3X3,0 7240 35,4
3,0 66 147,8 13.2 734 18,0 7.2 67 148,6 12,0 631 16.8
3,0 114 152.8 41,7 1105 15.0 7,2 125 150.0 65.7 1880 20.4
3,0 161, 157 7 129 0 2870 20 7 2 115
' 160 31 177 0
' 4120 25,4

3,0
182
159:21
182:01 3570 20: 7:2 9
16 162 3 280
01 5960 31,0
-r A (5 L E :5
Card 3/6

Siren for acoustic ...
Aj kI#
JO T1011, be,
20238
S/046/61/007/001/009/015
B104/B204
17 P1717
2
Legend to Fig. 3: Sound inteneity I (watts per cm ) and logarithmic sound
gauge L (decibbl) as a function of the radius of the mouth at a frequency
of 4-5 ko.
LeCend to Table 3: 1) Frequency; 2) air consumption in fiormal cubic meters'
per hr; 3) sound gauge L in decibbli 4) efficiency in watts; 5) efficien-,'
qr/tdr.cmis-umpt ion; 6) efficiency.
Card 4/6
7!
70

20230
S/046/61/007Ac1/000/C-15
Siren for acoustic ... B104/B204
`~Legend to Fig. 7: L and I as a function of the diameter of the coagulation
tube at a distance of 5.45 m fro-m the mouth of the siren.
Card 5/6

Siron f~r acoustic
Card 6/6
20238
g

TSETLIN, V.M.; DENISOVi V-F,; TAUDILIN, S.A.; Prinimali uchastiye:
SASIN, VIIIP ulndshiy nauchnyy ootrudnik; -UDIN, B.S., master;
DRACHEVA, T.V.., labarantka; MIKOV, V.T.p laborant;
SLOVIKOVSKIY, A.A.,, laborant
Investigating the effect of various factors on the process of
nonferrous metal dust coagulation in a sound field. Sbor.
nauch. trud. Gintavetmeta, no.19:595-60'7 162.
(MIRA 16:7)
(Nonferrous metals-Metallurgy) (Aerosols)
(Sound waves-Industrial applications)

TSEDILINq Yu.A.p podpolkovnik meditsinskoy Pluzbby
Significance of the gastroacopic method of study in achylous
states. Voen.--med. zhur. no. 6:71,74 Je 160. (MMA 13:7)
(GASMWCOPY) (STORACII-DISFIASES)

N,T..C-V, 1U.A.;
SOL:u c',.arLxteriz3,,icj o-~ A' -2 '.4cr, C)-'
high molecular llicy,;lic -'-",'.'".---cjcar.-crj izv.
otd. khim. nr-uk no. 1:171,-2.76 Jo-
1. Inotitut .,oolo~ii i
'01 3SSH.
(Dehydro~lan:;Aion) (D o,- -i,~ )(Illropune)

PETROV, Al.A.; SANIN, P.I.; TSKULINA, A,L.; BAGR1Y, Ye.l.;
YEPISIEV, V.I.
Synthesis and properties Of C2j cyclic hydrocarbons. flefte-
khimiia 3 no.4:465-471 Jl-Ag 63. (MIRA 1611l)

AUTHORS:

1 71
Petrov, Al. A., Ser.-iyenko, S. F" SOIJ!'..'~2 ::n '
/ _,-_ .1 1, `7
Tsedilina, A. L., Finlinskiy, A. It., Gallpern, G. D,
TITLE: The Isomerization of Saturated Hydrocarbons (Izomerizatsiya
nasyahchennykh uglevodorodov) Communication 3. The Isomeric
Transformation of Cyclanes (SoobshcheniYe 3. Izomernyye prevra-
shcheniya tsiklanov)
PERIODTCAL: Izvestiya Akademii nauk 333R, Otdeleniya khimichoskikh nauk,
1956, Nr 6, pp. 730 - 738 (USSR)
ABSTRACT: In various earlier papers the isomeric transformations of
alkanes are discussed, which develop in the presence of poly-
functional catalysts under hydrogen pressure (Refs 1,2), The
main purpose of thin paper is the inventigt-,tion of the rules
governing the isomerization of hydrocarbons and of the connection
between striicture on the one hand and kinetic and thermoflynamic
parameters on the otller. The catalytic inomerination of t~.e

'
cycloparaffin hydrocrti-bono C - C in tho prenence of a pol.% -
functional catalynt under hy~r
0-02 prensure was carried
Furthermore# it van found that the inomeri?~ation products of
the cycloparaffins C and C 5 corresi)ond with respect to their
~
Card 1/2 composition to the th
rmodyr-mic v-lues obtained ty calculation,

S -.'I 162_Cq_C_ 1 7'77
The Isomcriz,~tion of Saturated Hy'rocarbons,
Communication 3. The Isonoric Tranof ormi t, ion of Cyclarea
A mechanism for t1le i3o.-ieriz.,tion of cycloi)araffins was
suCgested, accordinS, to rhich t-e formation of uroattr~_te;!
hydrocarbons fiGures as the first sta'-e of reaction, Fuxther:-~ora
the influence exercised by presoure and terriperature u,--on the
direction of the reactions of cycloparaffins in tl-.e ~recence of
a polyfunctional cattilyst apts shown. There are 5 tables and 17
referencen, 8 of which are Soviet,.
ASSOCIATION: Institiit nefti Akkderii nnuY 3.5311 (Patrol*um Lit-Aitute ~.S USSR)
SUBMITTED: November 19, 1956
1. Hydrocarbons--Isomrism 2.
--Chemical effects 4, Tenerature..-Chemical effects
Card 2/2

5 (3)
AUTHORS: Petrov, Al. A., Sergiyenko, S. R., SOY/62-59-6-22/36
ffechitaylo, ff. A., Tpedili.na;_.A. k._.
TITLE: Synthesis and Properties of the Monomethyl-substituted Alkanes
of the Composition C 12-C 16 (Sintez i svoystva monometil-
zameshchennykh alkanovsootava C 12-C 16)
PERIODICAL: Izvestiya Akademii nauk SSSR. Otdeleniye khimicheskikh naulk,
1959, Nr 6, pp 1091 - 1097 (USSR)
ABSTRACT: Since the hydrocarbons of this structure are not yet suffici-
ently investilgated, the synthesis of the monomethylated al-
kanes with a boiling temperature of more than 2000 was investi-
gated. With this monomethylated alkanes one may synthesize all
theoretically possible isomers (there are only 29 com.pomda).
They are furthermore of interest because they have thermodyna-
mically stable structures and meet with all technical require-
ments of motorization. The hydrocarbons were synthesized ac-
cording to Grignard's reaction (magnesiumbromoalkyls with me-
thylketones). in this reaction the purity of the compounds ob-
tained depends in a high degree on the purity of the initial
Card 1/4 substances (alkylbromides). This fact was especially considered

Synthesis and Properties of the Monomethyl-substituLed SOV/62-59-6-22/30'
Alkanes of the Composition C 12-C 16
in the present investigation. The methylketones were obtained
by decomposition of the corresponding alkyl-acetoacetic acid.
As intermediates tertary alcohols were at first obtained which
were dehydrated at 2800, redistilled , and hydrated 0in the
autoolave on nickel. at a temperature of from 150-170 . The tem-
perature at which the hydrocarbons obtained crystallize was de-
termined by plottingthe heating curve by means of the photo-
-recording Xurnakov pyrometer. The purity degree was determined
by means of a special thermographtc device.N. 1. Lyashkevich,
to whom the author3 express their gratitude, carried out the
measurements in the laboratory for petroleum chemistry of the
institute mentioned in the Association. The purity degree of
the synthesized hydrocarbons was 97-98%. The thermogran was re-
corded by a special aluminum block which was designed in the
Institut obahchey i neorganicheakoy khimii AN SSSR (Institute
of General and Inorganic Chemistry of the AS USSR). By this au-
tomatic recording of the heating curves the melting process
could be fixed exactly (Fig 1). With almost all compounis ob-
Card 2/4 tained two stages in the melting process (-46 and -45.4 melt-

Synthesis and Propertie3 of the Monomethyl-substitut--d SC7/62-5~`-6-22/1-zl~
'Llkanes of the Composition C 12-C its
ing and crystallisation temperature) were obsF~-~rved, The pre-
perties of the hydrocarbons are given in a table by which it is
shown that the density and the refractive index scarcely de-
pend on the position of the outer methyl groups in the mair.
chain, what in wall in line with data by Tatevskiy (Ref 5).
The crystallisation temperature is, however, strongly influ-
enced by these methyl groups. The change of the crystallisa-
tion temperature at the transition of one homolog to the other,
and of one isomer into the other is not steady (Figs 2,3 with
comparative data from Ref 10). This unsteadiness is caused by
the pres3nce of either an even or an odd number of hydro(.arljons
in the raair. chair.. The transitior, from an odd to an even riumber
of hydro,arbons exurts a parallel influence on the melting
point, the reverne transition, that is an increase in the mD-
lecular weight, exerts an antiparallel influence. The laws
holding for paraffins, olefins, and greases, which are well
known, may thus also be applied to ramificated all-anes. The
crystallisation process of the latter takes place by forming
Card 3/4 such crystals as exhibit the shortest possible carbon chain.

Synthesia and Propertiee of 'Who
Alkanes of the Composition C
12-" 16
There are 3 figures, 9 table, and 11 references, 5 Df which
are Soviet.
ASSOCIATION: Inatitut nefti Lkademii nauk SSSR (Petroleura Institulklu of the
Academy of Scioncou, USSR)
SUBMITTED: September 5, 1957
Card 4/4

L 15486-6 3 6WP(j )1EPF(c Pc-14/Pr-14
ACCESSION ITR: AP3005445 3/0204/63/003/004/0465/0471
AUTHORS: Iletrov, A3, A.; qanin, P. I,; Tsedilina,
agri Ye. I.; Y8j~fS-5`eV-'-'V. r"
B
TITLE: Synthesis and properties of C sub 24- drooarbons'~
~SOURCE: Neftakhimiya, v. 3. no. 4. 1963P 465-471
TOPIC TAGS:- C sub 24-hydrocarbon synthesis,, hydrocarbon structure,
naphthene
ABSTRACT: The following 24 now C24-hydrocarbons containing varied
structures including 5- and 6-membered naphtheneirings of different
T-c-scribed. 10-cyclo-
degrees of substitution were synthesizea an Te
enty1nonadecane; 1-methyl-2-octadecylcyclopentans; 1.7-dicyclopentyl-
;heptylheptane; 1.7-di-(3-mothylcyclopentyl)-4-anylheptane; 1,10-di-
.4-dirrothylcyclopentyl)-docane; 1#7-dicyclopentyl-4-(B-othyleyclo-
~!ntyl)-heptane; 1-phonyl-4-hexyl~7-CYclopentylheptane; 1-cyclohoxyl-
hexyl-7-ualopentylhoptane; 7-( -eyelopentylphenyl)-tridecane; 7-
4-CYcloPentYleYelohoxyl)-trideoane; 1#7-dicyclopentYl-4-benzy1o
Card 1/2

L icif86-63
ACCESSION NR: AP3oo5445
heptane; 1.7-dicyolopentyl- etbyloyclohaxylhoptane; 6-(2,,4,5-tri-
mothylphenyl)-pentadecane; k:1(112,4,5-trimethyleyelohoxvl)-pentadecane;
1-phenyl-3-(2.5-dimethylbenzyl)-nonane; 1-cyclohex,71-3-(2.5-dlvethyl-
me~hylcyelohexyl)-nonane; 1,,l-di-(4-iso ropylphenyl)-haxane; 101-di-
(4-isoprop lcyclohoxyl)-hexane; 1 1-di-~2#4,5-trimettUlphenyl)-hexane;
1.1-di-(2,~,5-trimethyleyelohei.-yll-hexane; 1,3-di-(5-indanyl)-2-pro-
pylpropecne; 1,3-di-(5-hydrindarL71)-2-propylpropana; 1-phanyl-4-(2-
dodecyl)-benzeno; 1-cyclohexyl-4.-(2-dodecyl)-cyclohexane, "Synthesis
(of 1.3-di-(5-indanyl)-2-propylpropane) carried out by L. N. Stuk-
,anov . orig. art. has: 29forirulas.
ASSOCIATION: None
SUBMITMD: 00. DATE ACQ: 06Sep63 ENCL: 00
SUB CODE-. CH NO REP SOV: 008 OTUR: 007
t
Card 2/2

84858
IOU
S/06 601000101010121018
B01 5YBo64
AUTHORS. Petrov, Al. A., Bergiyenko, S. R. 1A4"WqL"1&.
Sanin, P. I., Nikitskaya, Ye. A~, and Nechitaylo, N. A.
TITLE:
PERIODICAL:
Synthesis and Properties of High-.molecular Hydrocarbons of
Mixed Structures., Information 1. Synthesis of Hydro,.~arbons
of the Composition C24
Izveetiya Akademii nauk SSSR. Otdeleniye khimicheskikh
nauk, 1960, No. 10, PP- 1848 - 1857
TEXT: The authors synthesized several hydrocarbons that., up to a cer-
tain extent, may serve as models for the hydrocarbons contained in high-
boiling petroleum fractions. The present paper reports on the synthesis
and properties of 23 hydrocarbons with mixed structures~ containing 24
hydrocarbon atoms per molecule. Compared to a similar investigation car-
ried out by R. Schiessler et al. (Ref.2), the present studies were made
on a larger scale. The influence of the degree of cyclization of the
hydrocarbon moleculesq the effect of the relative position of some
cycles in the paraffin chain of the molecules, and the effect of the
Card 1/3

84858
Synthesis and Properties of High-.molecular S/062/6o/ooo/o1O/012/018
Hydrocarbons of Mixed Structures. B015/BO64
Information 1. Synthesis of Hydrocarbons of the Composition C 24
degree of substitution of the aromatic or cycloparaffin rings in the
molecule upon the properties of' the whole molecule were investigated
(cf. Scheme of the structural changes). The hydrocarbons were syn-
thesized by the Grignard reaction. The alcohols were dehydrated in the
vapor phase by means of an aluminum catalyst used (method of the
-4 Emp
American Petroleum Institute) this wash however, done in vacuum (3 N
Purification was carried out by distillation and absorption, The condi-
tions of synthesis are described in detail for 1,1-diphenyl dodecane
while only a short information is given on the preparation of the re--
maining 22 hydrocarbons,, Since a peculiar behavior of 2#4,6-trimelhyl
chloro benzyl was observed under the preparation conditions of the
Grignard reagent, the characteristics of the roaction between methylated
benzyl halides and magnesium are discussed (Table 1, data on diaryl
ethanes obtained by reacting some substituted henzyl chlorides with
magnesium), Table 2 gives the structural formulas and the most important,
properties of the 23 hydrocarbons obtained. The anomalies of viscosity" '
as a function of the temperature of the polymethyl-substitutAd benzenel
derivatives are remarkable, the aromatic hydrocarbons having
Card 2/3

8485B
Synthesis and Properties of High-molecular S/06 6o/ooo/olO/012/018
Hydrocarbons of Mixed Structures. BO15YBo64
Information 1. Synthesis of Hydrocarbons of the Composition C 24
several methyl groups on the ring have a much higher viscosity than the
monosubstituted isomers. In the near future, the authors will publish
a paper on the physico-chemical properties of the hydrocarbons described
here (data on various spectra). There are 2 tables and 10 references:
5 Soviet, 3 US, 1.German, and 1 British.
ASSOCIATION: Institut.geologil i razrabotki goryuchikh iskopayemykh
Akademii nauk SSSR.(Inatitute of Goology-and Proapeq~tng_
of Mineral Fuels of the Academy of Sciencee,USSR)
SUBMITTED: May 6, 1959
Card 3/3

AUT11ORS Tectlin, V.11. wid Tsedilin, S. A, 130-58-3-14/ 21
TITL-E- A sonic siren for dust cLt,:hing (Zvuh-ovaya sirena dlya pyleniavlivai iya)
P12110DICAU Tevetnyye Metally, 1958, Nr.,3. pp. 76-78 (Usq1t)
ABSTRACT:, The very finely divided sublimates arising in non-ferrous Metals
production are diffi,~ult to trap. The -~oagulat,2,on of such particles
is assisted by sonic vibrations and the authors describe u siren for
this purpose designed. built and tested in Gintsvetmet, The working
parts of the siren (fig.l' have 75 circular holes with their centree
on a circle of 200 mm diameter, The siren consists of two halves
(the casing and the stator), which fa.:ilita+,es its assembly and control
of gape between the working parts.. The authors discuss the choice of
hole diameter and shape of gas passarw, rotor holes are made 0.3 mm
less in diametcr than thr- 4.2 mm diameter stator holes, and the latter
are conieal with the lar:,er diameter 7.2 = The axial gap between
rotor and stator is les!~ than 0.05 mm. Pressure drop and noise
intensity arc plotted (figs. 2 & 31: against. air flow ('30-500 nm3 /hour
Thr freflucnoY generated in 3 kilohertz There are 3 figwes.
ASSOCLATION Gintsvetmet
JIVAILIBLE!: Librz!ry of Gongrc.-3s,
1. Sound-Applications 2. D-ust-Effects of sonic vibratiom
Card 1/1 3. Soniz vibre t ions.- A ppl-ication-~

- I , f I - I I/ I /
/ i--l I- I, i I - rIfi
TMILIK, T.M.g TMILIN, S.A,
... ~ 7
Sovad ~irsn for dust doUctioa,
1e, Gistevatmot.
(lonforrow "tall-vatallusy)
T**to wt, 31 ao,3i76-78 mr i58,
(KXRA IIA)
(Fly ask)

TMILINO ToNal TMILINg S*As,
1A W,~~-i-~ -
So=d alroz for dust detectica. Unto wto 31 30*316-78 Wr 'A
(MIRA Ilt4)
I*' GlAtevetwot*
(lionferrous "tale-Netallurgy) My ash)

S/570,VIVOOO/017/012/012
q, C1140 10 E032/E114
AUTHORS: Vsekhavyatskaya, I.S., and Tsedilina, Ye-.Ye.--
TITLE: Amplitude correlation function for signals scattered
from a perfectly rough screen
SOURCE: Akademiya nauk SSSR. Institut zemnogo magnetizma,
ionoafery i rasprostraneniye radiovoln. Trudy,
no. 17(27). Moscow, 196o. Rasprostraneniye radiovoln
i ionosfera. 287-291
TEXT: A talculation is reported of the amplitude correlation
function for signals reflected from the ionosphere with allowance
both for random and directed motions in the ionosphere. The
problem is solved for a plant ionosphere located at a certain
height above the observer and looked upon as a perfectly rough
scattering screen. The calculation is illustrated in Fig.l.
Let -;rl be the drift velocity of the screen, "r. the root mean
square -velocity of random motion, and suppose that a spherical
wave is emitted from the point of observation 0 which is the
origin of the polar coordinate system. Assuming that the random
motion velocity distribution is of the formi
Card 1/4

30942
Amplitude correlation function for ... S/57o/60/000/017/012/012
E032/Ell4
(u - V I sin 0 co
W(V) exp (2)
2
0 2/P,7:. 2Y0 - 2fo
where: u = v + v, sin 0 cos ~p, v2 = V2, f f - and
0 0 S _t
fo _s the zarrier frequency, it can be shown that the energy
scattered by an -element dC)_ in the ionosphere is given by:
2 ( 2fv I
W(f)dO dT dl~ exp - C f - r - sin e Cos P)2]
2 2 0
2 /2,Fv f 8v f C
0 0 0 0
sin 0 cos 0 d0 dW df. (3)
Using this expression for the scattered energy, the author shows
that the auto-correlation function is given by:
Cazd 2/4

30942
AimilAt'Llde ctij-r-elat ion I tinction for . . .S/570/60/000/017/012/012
E032/EI14
8TC2 f2T2v2 j1
(T) exp (16)
e
R c2 2 Tf 0v1
c
This is a general expression which holds in-the presence of both
random and directed motions. The formula obtained for this ~J_
coefficient by Booker et al (Ref.6: Booker, Ratcliffe, Schinn.
Philos. Trans. Roy. Soc., v.242, 579, 1950) is a special case of
this expression. Acknowledgments are expressed to Ya.L. Allpert
for suggesting thiis problem and to Yu.K. Kalinin and
L.P. Pitayevskiy for discussions. It is pointed out in an
appended note that an analogous result was obtained by a somewhat
different method by J.E. Drummond W. Atm. Terr. Phys., v.9,
282, 1956) but this paper became available to the present authors
after the present manuscript was submitted for publication.
There are I figure and 7 references: 2 Soviet-bloc and 5 non-
Soviet-bloc. The four most recent Enjiish language references read:
Card 3/4

1" h-
Amplitude correlation function for ... sA1o/6o/ooo/ol7/012/(.,J2
E032/Ell4
Ref.2t Ratcliffe. Rept. Progr. Myn., v.19, 188, 1956.
Ref-3: R.B. Banerji. Proc. Phys. Soc., B 66, .105, 1953.
Ref.4: R.B. Banerji. J. Atm. Terr. Phys., 6, 50 (1955).
Ref-5: E.N. Bramley. Proc. IEE, p.III, v.98, 19, 1951.
Fig.1
Card
r

GUREVICH, A.V.;_jSEDILINA, Ye.Ye.
Effect of a constant electric field on electron temperature in
the ionosphere. Geomag. i aer. I no.10440 Ja-F 161,
NIRA 14:7)
1. Fizichoskiy instttut AN SSSR imeni P.N. Lebedeva i Inatitut
zenuiogo magnetizma, ionosfery'i rasprostranoniya rad1ovoin AN
SSSR. I I *VPW A
(Ionosphere) (Electrons) (Electric fields)

42128
AUTHOR: rscdiiina, Ye. Ye.
S/203/62/002/002/003jO 17
1046/1246
-_________ I
TITLE~ Temperature of electrons in the ionosphere in a constant electric field
PERIODICAL-. Geomagnetizm i acronomiya, v. 2, no. 2. 1962, 242-248
TEXT: In I - 5 jiV/m electric fields oriented along the gcomagnetic field in the ionosphere at altitudes
over 200 km, electrons attain two stable temperature states: (I - 2)-10-1 deg. and (10 -- 30).103 deg. The
characteristic time required for the electrons to heat up in this tcmperature interval ranges from 10 to 300 sec.
The resulting current density is 0. 1 to 10 milliamp/ra2. The minimum dimensions of the electric field required
to start the heating-up effects at altitudes, of 250 to 5500 km are 10-30 kni along the magnetic field, and 100 m
across. The additional magnetic field produced by such cylindrical regions less than 2 km across is masked by
the daily variations inthe geomagnetic field. The accelerating electrons change the degree of ionization
noticeably if the electric field remains effective for at least I - 10 hours. All the conclusions are in agreement
with the experimental results, and the heating-up mechanism may thus also be responsible for large-scale
inhomogeneities in the ionosphere. There arc 7 figures and 5 tables.
ASSOCIATION: lZMIRAN
SUBMTTED. January 9, 1962
Card 1/1

3/203/62/002/005/003/010
1046/1246
AUTHOR: Tsea n
TITL'--': The Loppler effect in magnetoactive ionosphere
P-71 ~ 10 1, 1 C A LGeomagnetizr, i aeronomiya, v.2,*no-5, 1962, 665-672
TEXT: This is the first analysis of the Doppler effect of raoic-
si&nals which allows for the geomagnetic zield. The roppler fre-
quoncy shift in a m~.e--netouctive medium differs frow the analoE4ous
,--iiift in an isotropic mecium by-a term which is proportional to
0 'W (CUH the gjroscopic frequency). This adcitional term i-- olf
no Qonsequence in the difft'erential Doppler effect for cohereInt
frequencies, since here (&) '.14d ) /-< 1. In 'the rotational Doppler
effect (otherwise knovai aS tic Faraday effect: -time depenuence- of
the rotational an6le of the pl,.ne of' polarization of receivec i r~,Cio-
Waves), the acuitional ter.,., introcuce-, nev. significant factorz
(sinusoical modulation of the rotational 1:,opl;ler effect, for in-
stance). These were overlookeo by C;-rriott ana by Kelco (Ref.5:
Cara (112,

S120 3/62/002/~ 05_/C 0 ,/r
The Doppler effect ir, ... 1046/1246
0.41.'Carriott. J.Geophyc.,Iie!~., 1960, 65, 1150; Ref.6: E.,'V..1'.c-1co.
J.Geophys.Pes., 1960, 66, 1107) because of their failure to allow
for -the eomagnetic fiela. The analysis is of particular signifl-
cance because of the gro,.-:ir,,g u-,e of the cifferential and the rota-
tional Zoppler effects in ionospheric electron density determina-
tions with rockets and artificial satellites. There ie I figure.
A'Lc3,S=IATION: Institut zewnoi_:-o xa6netizma, ionos-Afery i ra'sprostra-
neniyu raaiovolr. AN SSSR (Institute of the Terrestrial
Magnetism, tiie Ionosphere ano Propac;ation of' Radio-
waves AS' U'SSR)
SUB14ITTED: June 18, 1962
Card 2/2

ACCESSION HR: AP.4040710 S/0203/64/004/003/0503/0508
1AUT11OR: -TsedMus, Ye. Ye.; Khary*bLna, A. A.
TITLE: Study of the nonhomogeneous structure of the ionosphere on the
lbasLs of radio observations of the artificial earth satellites
lCoamos 1, Cosmos.2, and Cosmos 11 at coherent frequencies
1SOURCE: Geomagnetizm L aeronomiya, v, 4, do. 30 19640 503-508
TOPIC TAGS: Cosmos 1, Cosmos 2, Cosmos 11, ionospheric Lnhom6ganaLtyp
artificial earth satellite, doppler shtft, coherent frequency, ionos-
pherLc Lnhomogen.sity, ionospheric Lnhomogensity spectrum, coher,
oscillation
1ABSTRACTt The phase differences Ln the coherent oscillations radiated
ifrom Cosmos 1, Cosmos 2, and Cosmos 11 at 20.005 and 90.0225 mc were I
Irecorded in 1962 and 1963 at various Soviet stations. The recording&;
!were made for varLous-montha and for different hours of t" day.
,'Heasurement of these phase differences made it possible to obtain the!
ionospheric Inhomogeneity spectrum W(p)e Analysis of this spectrum
1/2
0",
Jr,"

ACCESSION NRs AP4040710
!showed thatt
11 1) W(p) has three steady maxima at 14-16,
jjP2 N 28-32 'and P % 90-110 km; 2) appirentlyi tAe lengths of p1,
C02, and 03 do not Aepend on the hour of the day or season; 3) an in-
i.ve tigation of the dependence of W(p) on altitude revealed that the
,imaximum number of inhomogeneitieti occurs at 50-100 km below the main!
,maximum of the F region; 4) the total number of inhomogensities de- i
an Increase in altitude; and 5) small-scale inhomoieneL-1
,Icreases with
ties - p % 1 km - have not been detected at altitudes above
350-400 km. Orig. art.-hass 5 figures and I table.
ASSOCIATIONi InstLtut zemnogo magnetLzma, Lonosfary*L rasprostranonLya
radiovoln AN SSSR (InstLtuts of TerrestrLal Hagnation, lonosphtre and,
Radio Wave PropagatLono ~N SSSR)
SUBMITTEDs 24Aug63 ATD PRESSs 3048 ENCLi .00
SUB CODZ: OP9~33:; NO REP SM 005 OTHERs 001
Card,' 22

AGGE;51014 lift: AP404071h 3/0203/64/00h/003/056h/0566
AUT11ORt- Tsedilinaj Ye. Yes
TITLE: Three-dimensional modulation of the Doppler shift in frequency of radio
waves received from artificial satellites
SCURCE: Geomagnotizm i aeronomiya, v. h, no- 3, 1964, 584-586
TOPIC TAGSt Doppler effecto radio wave, artificial satellite/ Cosmos I, Cosmos IIj
Cosmos XI
ABSTRAM The author points out that records from Cosmos I# Cosmos II, and Cosmos
XI indicate that modulation of the Doppler shift is due chiefly to inhomogeneiLies
along or near the orbit of the satellite. She attempts to show that this conclusion
may be reached theoretically by virtue of the fact that the Doppler shift due to
inhomogeneities along the orbit of the satellite is always proportional to the
velocity of the satellite al it path. She begins with an equation from N. A*
o 01jGeos
Mityakov and E, Yee Hityak va magn. i aeronomiyal 1963, 3) No- 5, 850)j defining
the Doppler shift in a two-dimensional approximation for the cane when the electron
concentration dopands on the three coordinates xp y, and z* These coordinates are
so chosen that the vertical plane xOz passes through the.satel-lite and the point of
observation. After analytical evaluation of electron concentrationp the resulting

ACCMSION NR.- Al-'hOhO7lh
Al ze
11equation simplifies to "MA I Cos AN, (S,)
where xcl is the satellite velocity at x1, parallel to the plane of the orbit and to
the surface of the earth,, i is the satellite velocity along the z axis, z is the
c c
height of the satellite, X2 and X, are linear scales of inhomogenciLy along x1 and
talong the line connecting the source with the point of observation, respectively)
:and N. is the initial electron density. The amplitude of three-dimensional nodula-
tion of the Doppler frequency shift i's thus found to be proportional to the satel-
Jite velocity along the orbit, and this leads to an increase in the amplitude of
i
.modulation of thio shift. The conclusion nends detailed proof and stricter consid-
leration of the height dependence of modulation depth and periodic structure. "In
conclii3ion, I express thanks to Ya. L. Allpert for his remarks during discussion of
ithe paper." Orig. art. has, 9 formulas.
ASSOCIATION: Institut zemnogo magnetizma) ionosfery* i -asprostraneniya radiovoln
'AN SSSR (Institute of Terrestrial Magnetiomf the Ionosphere, and Propagation of
Radio Wavesp AN GSSR)
2/3
Card

till; AP4040714
S"'MEDS 27Doc6.3
SUB CODL?j ES, SV NO REF SOVS 005 oo
OTIIER: 000
,qqrd 313

I~., (- ) ~, HR k , -: If"
~ I . . , . . ~.~ 1, , 1 f , , 1 , ~ . - , , , 't I f-I ,
I - , I F. 1 1. 1~

L 33279-66- EWT(J) IJP(c) AT
ACC NR: AP6011695 SOURCE CODE: UR/0203/66/006/002/0255/0265
I/
AUTHOR: Gurevich A. V.; Teedilina, Ye. Ye. o/7
0: Phmics Instit J~-
OR ufe tf, b
161 edey AN'SSSH..jFlz1cheskiy inBUtut AN &93R);
Institute of Terrestrial Magnetism, the Ionosphere, and Radio-wave Propagation, AN SSSR
(Institut zemnogo magnetima, lonodery I rasprostranenlya radlovoln AN SSSR)
TITLE: Character of dispersion and form of inhomogeneitles in plasma
SOURCE: Geomagnettzm I aeronomiya, v. 6, no. 2, 1966, 255-265
TOPIC TAGS: plasma magnetic field, plasma diffusion, plasma charged particle
ABSTRACT: The authors analyze the character of dispersion In plSMa in a magnetic
field of Inhomogeneftles whose dimensions are many times _ n the free path length
of the particles. It Is shown that in the absence of drift the disturbances oSA e particle
concentration In an inhomogenelty decremies with time in proportion to 1/t , the same as
in ordinary diffusion. The form of the Inhomogeneity, however, appreciably differs from
ellipsoidal. The asymptotic behavior of the disturbances of the concentration changes
qualita9vely at large distances: with an inFeas f th d rease only by the power law
6N 1/r and not by the exponential law ON r'o I n
-exp r /rDatwehoich Is characteristic for
Card 1/2 C 550.388.2

L 33279-66
ACC NR: AP6011695
ordinary diffusion. The rate of movement of the inhomogeneity across a magnetic field
many times exceeds the rate of transverse diffusion of electrons. It is shown that in the
presence of drift of charged particles in the plasma the dispersion of the inhomogeneities
no longer bears a diffusion character. A new (I'dispersion'l mechanism plays an Ix1portant
role of scattering. Disturbances ofjbp concentration decrease in proportion to A , and
in one direction in proportion to 1/t'/". The form of the inhomogeneity is severely drawn
out in a direction which does not coincide with the direction of the magnetic field in the
plasma. The ratio of the longitudinal and transverse dimensions of the inhomogeneity in-
creases in proportion to the square root of f- with the course of time. it Is found that dis-
persion scattering substantially changes the character of the decrease of the concentration
of particles in an inhomogeneity and completely determines Its form. However, theauthors
point out that drift Itself and the dispersion of the drift velocity in no way affects the ampli,
tudes of the Fourier component of concentration disturbances. During diffusion the ampli-
tudes decrease exponentially with time. Therefore, although dispersion of the drift velo-
city leads to scattering of the inhomogeneity and substantially affects the particle concent-
ration and shape of the inhomogenelty, it does not change the scattering cross section of
electromagnetic waves since the corss section depends only on the amplitudes of the com-
ponents of the Fourier disturbances of electron density. The authors thank YjLAD_jXb3k.
for performing the numerical calculations. Orig. art. has: 3 figures and 32 formulas.
SUB CODE: 20 SUBM DATE: 24May65 ORIG REF: 005
Card 2/2
--f 5~'z i6 M2, M.