SCIENTIFIC ABSTRACT FOGEL, G. [FOHEL, H.] - FOGEL, YA.L.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000413410005-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 23, 2000
• Sequence Number: 5
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

(Fohell, 11.)
We increase and lower the cost of the produbtion of precast
reinforced concret:e. Sill. bud. 12 no.1l'-17-18 N 162.
(MIRA 15:12)
L Glavnyy inzh..Khersonskoy oblastnoy mezhkolkboznoy
organizatsii.
(Kherson Province-Precast concrete)

FOGIL. Maria, dr.
Radiological diagnosis of ratroperitoneal Inflammations. I.'--
Pancreatitis. YAgy. radiol. 6 no.4:155-i62 oat 54.
1. A III. oz. Babosseti Klinika (igaxgato; PqbamVi Pal dr. egyetemi
tanar) as a IIIe szo Balklinika (igazgato: Gomori Pal dre effetemi
tanar) rontgenintesetensk koilemenya, (vezetologel Maria drj
(PANCRIATITIS. diog.
x-ray)

A
pr 56
F GEL, M: and FEJPR R. Hontgenabt. III citir. Univ, -Ktin., III hied. Uni
fi' - BuJapest. *RlJntgenologiBche Verlinderungen varikOsen Ursprunges
am Magenfornix. Roentgenological changes of varicose ori-
gin in the gastric fold FORTSC1111.11ONTGENSTH. 1955, 83/2
(204-207) Illus. 4
")ort of 2 cases. The first base showed splenomegaly with cirrhosis and repeat-
gastric haemorrhages. The oesophagus contained characteristic varicose phe-
pena, and at the cardia an arcuate formation the size of a walnut was observed.
.,se findings were confirmed during splenectomy. The second case concerned a
)ng man who, after a fall with subsequent splenic enlargement and extirpation
'.Ps organ, had shown frequent haemoptyses and melaena since his childhood.
z oesophagus was roentgenologically normal. A nodular tumour, the size of a
Inut was found in the gastric fundus. The smaller curvature presented a niche-
:b formation which disappeared on compression. According to Melik-Arutjunoff,
~h pseudo-niches develop by elevation of the mucosa between 2 markedly pro-
"jing dilated veins, which are evacuated by compression. This wa confirmed
.bperation. -in spite of gastrectomy, the haemorrhages re-appeared, Oesophago-
~py then revealed venous dilatation in the oesophagus. Pape Vienna

FOGEL, Maria. dr.
Cortical form of osteoid outeoma. 14W. seboozet 9 no-3:151-155
June 56.
1- A Bu"P85ti 0rv08tud0m&DYt IkYetem 111. oz. Soboozeti Klinika
(igazgato: Kudasz Jozoef dr. egyatmi tana,r) rontganintemetensk
kozlemenye (Vezoto: Fogel Maria dr.)
(OSTSOPA, OSTBOID
cortical, x-ray ding. & differ. diag. (Run))

T:
56
2088. FOGEL M. and FEJER R. Rdntgenabt.. 111. Chir. Univ. -Klin., Budapest.
erostosis generalisata. G e n e r a I i z e d h y p e r o a t o a i a RADIOL.
CLI . (Basel) 1956. 25/2 (115-120) Illus. 6
Generalized hyperostosis in a rare disease of the skeletal system with changes in '-er
bone structure and shape, obliteration of joint spaces and calcification of liga-
ments. Investigations on 2 generations of patients enabled the authors to observe
the various developmental phases of the disease and the course of heredity. As I
far an the authors know, experiences on 2 generations have so far not been pub- it
lished.
..Z
-T
14 '.v
~R f

FOGEL, YARIA, 2d..
Rontgenasszisztensek tankonyve. Irtak: Furth Bela (et al.) 2., atdolg. kiad.
Budapest, Hungary. Medicina, 1957. 281 p.
Monthly List of East European Accessions (EFAI), LC, Vol. 8, no. 11, November 1959,
Uncl.

EXCMPTA 12DICA Soc.14 V61.12/5 Radiology May 1958
892. ~POSTBULBAR DUODENAL ULCERS - A postbulbaris duodenalis fekdlyek -
F o g e 1 M. and R o s s m a n n B. OrVOBtud. Egyet. 111. sz. Sebdszeti X11-
n1W;W_,_Tu_cTa_pest - MAG. RADIOL. 1957, 9/1 (11-16) Illus. 6
8579 of the duodenal ulcers develop In the bulb, I. e. in the first portion of the duo-
denum 2 cm. l6ng. 10176 In the second part 3 cm. long and 576 at a distance more
J: than 5 cm. from the duodenal base. Postbulbar ulcers are characterized by pains
j:i independent of the ingestion of food. The generally small postbulbar niches are
I accompanied by a long eccentric stricture uninnuenceable by spasmolytics, where-
as the pylorus and the duodenal bulb are atonic. and dilated.
GyargyI. - Budapest (XIV. 6*)

FOGELi Haria Dr SOMOGYI, Zsuzsa, Dr,
X-ray diagnosis of the ileocecal region; changes observed in the
Bauhin valve. Kagy. radiol. 9 no.4:206-211 Dec 57.
1. A Budapesti Orvostudomanyi Tgyetem 111. Sebeszeti klinika (igazgato:
Rubanyi Pal, Dr. egyet tanar) rontgen laboratoriumanak (vezeto; Fogel,
Maria) kozlemenye.
(IIWN, radiography
ileocecal valve in normal & pathol. cond. (Hun))

HMARY/Gonoral Problons of Pathology - Tunors u-4
Abe Jour Rof Zhur - Biol., No 79 1958, No 32723
Author Y_c_&ol Marie., Rcdnri Vorr.
Inst Not-Givon'
Title Carcinoma of the Duodonun.
Orig Pub t Orv. hotilap, 1957, 980 No 10-11, 279-281
Abstrect : According to postmortem dvtr, rnlignnnt now fomftions of
the auodenum compriso 0.03% of all tmor illnossos. A croo
is doocribcd of rdonocrrcinour vt the outlot branch of tho
duodonm. P--rtir.1 pnneroo-duod,3nactouy took plccep ca well
as rceaction of the stor-rch, the bile duct and pnncrenticau-
nostor.osol onthropo-entherooncstorose, end cholocynector-y.
The p--tiont quickly died. The nuthors consider thnt in spite
of the high postoperrtive fatality (--.,122%) in the cbsence
L,f r-otaBtasos, it is necessary to oonduct the rndiccl operction.
Card 1/1 777- . , I
Ij
422

PWIL, Maria; BOMOGYI, Zsuzaa; GAGS, Janos
Transposition of the pulmonary vein. Magy. radiol. 10 no.3:147-154 Sept 58.
1. A Budapesti Orvostudomanyl IL_-vetem Ill. Balklinika (Igazgato: Gomori
Pal dr. egyet. tanar) es Ill. Sebeszeti Klinika (Igazgato: Rubanyt Pal dr.
egyet tanar) rontgonoaztalyanak (Vezeto: Fogel Maria dr.) kozlemenye.
03M., PULHONART, abnorm.
transposition, x-ray diag., cane report (%n))

FOGEL, Maria, dr,
On roentgenological aspects of portal hypertension. Magy. sebesz. 15
no.2'.93-96 My :62.
(WERTENSION PORTAL radiog) (ANGIOGRAPHr)
a

JHUNGARY
FOOL-1, Maria, Dr; Medical University of Budapest, Department of Rontgen-
ology o,7~e III. Surgical and III. Medical Clinics (Budapesti Orvos-
tudomanyi Egyetem III. Sebeszeti es III. Belklinikajanak Rontgenintezete).
"Stricture Producing Esophagitis of Other than Alkaline Origin and its
Differentiation from Infiltrative Tumors."
Budapest, Magyar Radiologia, Vol XV, No 2, Apr 63, pages 65-72.
Abstract: [Author's English summary] The different forms of esophagus
stenoses are classified on the basis of nearly 500 examinations.
Inflammations due to non-alkaline causes are described with special
reference to their X-ray pictures thus facilitating their differentia-
tion from tumors. The differentiation between infiltrative tumors of
the abdominal tract of the esophagus and the cardiospasms as well as
the recognition of cancer developed from alkaline stenosis is fully
treated. The majority of the cases discussed by the author have been
verified by surgery and histological examinations. All Western refer-~--
ences,

FOGEL, Mariag Dr.
Dr. Gaza Molnar. Magy, rad-iol. 15 no-1:61+ Ja 163.
(OBITUARIES)

_,19GELI, Mariyafftgel, Marial, dots.; NAD1v Zoltan(Nagy, Zoltan],
SIUp Mafto [Ssiu,, Mario), doktor [translater)l .:
RAVAS, Yanosh [havasz, alknoe), aots., nauchn. rect.31,
ERDEI, Mikhay (Erdei, Mihhlyl, dots., nauchn. red.;
BERNAT D'yerd' [Bernkt, Gy5r ], otv. izdatell; ALEKSA,M.
I j
(Alekaza, MI, red.; CIURGE, I~.Wrgb, I.], tekhn. red.
[X-ray atlas of trailmatology] Rentgenovskii atlas po trav-
matologii. Budapest, 1964. 439 p. Translated from the Hungarian.
(MIRA 17:3)
1. Zaveduyushchaya otAelom rentgenologii III terapevti-
cheskoy kliniki Budapeshtskogo meditsinskogo universiteta
i Gosudarstvennogo Institute. Travmatologii (for Fogel').
2. Glavnyy rentegenolog Budapeshtskoy TSentrallnoy Trav-
matologicheskoy Ambulatorii (for Nadt).
HE,

FOGEL, Maria, dr.
Roentgenologic changes in the cardia following e3ophagofundostomy.
Magy sebesz. 17 no-4:210-215 Ag 164.
1. A Budapesti Orvostudomanyi Egyetem III Belklinika rontgenosztalya.

FOGEL,
Investigations on the properties of immine sera against N and N;
characteristics of human blood. Arch. 1-nin. ter. dosw. 4:35-43
1956.
I.Instytut Immunologii i Terapii Doswiadczalnej PAN we Wroclaviu
(Dyrektor: prof. dr St. Slopek) Mial 1--inologii) Kierownik: prof.
dr. H. Kowarzyk).
(BIDOD GROUM
N & N anti-M & anti-N sera of rabbit, possibility of
isolation of heterologous ar;t~bQdia)
(ANTIBODIIS
heterologous antibodies, possibility of isolation from
immune rabbit anti-M & anti-N sera)

DU, KRzimierz; SLOPEK, Stefan; BRML&, Urezula; FOGEL, Marian
Modifications of antigenic structure
a result of heterotransplantation on
5:329-345 1957.
(NIOPUSM, immulo 1.
antigenic structure of
after transpl. on mice
-. -
of Guerin's rat epithelioma as
mice. Arch. immun. ter. dosw.
Guerinis rat epithelioma. chwWoe
(Pol))

--- 1POGIVI N-: RLMIONKO, I'
(_..
Simple home-made apparatus for cauterization* Vrach.delo zio.5029
YT 159. (HIPA 12:12)
1. Khersonskaya, Oblastuays. bollnitea.
(GAUTIRY)

TM~ 9, N.D.; DOBRYKINA, M.A.
Simple device for pneumoencephalography. Vrach.delo no-5:521 MY 160.
(MIRA 13;11)
1. Khersonskaya oblastnaya bollnitsa.
(ENCEPHALQGR#HY),

FOGEL', N.D.; DOBRYKINA, M.A.,t
I
-- 4F
Table for lumbar puncture. Vrach. delo no.8:118-1-19 160,
AfZ 13:9)
1. Khersonskaya ablastnaya bollnitsa.
(SPINE-PUNCTURE) (MEDICAL INSTRUMENTS AND APPARATUS)

~, FOGEL?, N.D.; DOBRYKINAq M.A.
Result of kymographic registration of cerebrospinal dynamics tests.
Zhur, nom. i psikh. 60 no. 2tl72-174 160, (MIRA 14:/+)
1. Khersonskaya oblastnaya bollnitsa (glavnyy vrach A.F. Maksin).
(CEREBROSPINAL FLUID)

WG 'BD$ 'E C _____AFUC/A$D/IJP(Q____,
P AP3005241
056/63/045/00-'/Ca-6/0048
AUDILH: Borovik, Ye. S.; Volotskaya, V. G. Fogel', N* Ya.
Nam:
MiS: Deviations frcm Kohlerlt; rule, in _pUre aluminura
20'1963., 46-48
iSOURCE: Zhur. eksper. i tooret. 9iiq$ V, 45j
~TOPIC TAGS: aluminum, purity, magnetoresistance., Kohler's rule
T
IABSTRACT: The dependence of the resistance on the magnetic field was investi-
gated f cr very pura aluainum. samples at 20.4%. The purpose was to check Aiether
Kohler's rule is valid when R2'73/R,4.2 exceeds 2000. A noticeable deviation from
Kohler's rule is noted for hiift--purity aluminum samplep and it is pointed out i
~that both the behavior of the resistance in the magnetic field and the temperature
dependence of this resistance are anomalous, for reasons that are not clear as-
Iyet. . Orig., art. has 1 figure@
ASS OCI 9a CU 1. 'Fiziko-tekhnicheady institut Akademii nauk Ukrainskoy WR
:(Physicotechnica.1 Institute, Acad. Sci. Ukrainian SSR)
iSUEMITTEDi 15Feb63 DATE ACQt o6sep63 ENCM 00
SUB COM PH NO REF SOVt 005. OTHERt 001
Card 1/1

L 5~24_66 EWT(I)/EWT(m)/EPF(t)-2/E;WA(d)/EWP(t)/EW~(z ) E lip j ~ ( "~ I
R/I id)
ACCESSION NR: I AIIW21105 ~VWW/JG/Ga 9100il
Y104 Y V/
AUTHOR: Borovik, Ye. !.; Nev~L N. U.; LitvinnhR, -Yu. A.
c"flux jumps in hard a erconductors in pulsed
TITLE-. Study of Dv4pieti I , magnetic
fields
.SOURCE: Zhurnal eksperimentallnoy i teoreticheakoy Miki, v. 49,, no. 2. 3965P
;436-446
TOPIC TACTS: ferromagnetic superconductivity, niobium, nibbium compound, super-
"conducting all phase transition
ABSTRAM, NbaSn
The uthors investigated the rmgnetic-flux jumps occurring in
and NbZr'~fn pulsed magnetic fields. The samples were prepared by a prd'&65i~_de-
scribCd-elsewhere (V. D. Brodich et -al.., ZhETF v. 44, _U0, 1963), and the technique,
of producing strong magnetic-flux pulses was one developed by one of the authors
earlier (Borovikp with A. G. Limar', ZhETF v. 31, 939, 1961). The main measure-
:ments were made~at 4.2K.,'but some of the measurements of Xb3Sn were made in the
temperature range 14-5e;-3BK. The changer, in flux accompanying the jumps ranged
from 1 x 10-?- to 4 G-cm:2, and the jump durations ranged from 2 x 10-11 to 5 x 10-4
see. Each Jump is connected with a partial penetration of the flux into the super-,f
conductor. The relation between the jumps and the critical fields of the super-
Card

L 5354-66
ACCESSION NR- AP5021105
conductor is discussed
js as are various factora governing the magnitudes and dura-
tions of the jumps. It is concluded that the experimental data do not show con-
'clusively whether the obBerved flux jumps are associated with the existenceof ia-.
dividual regions of superconductivity with different parameters, or whether they f
are connected with some macroscopic processes which limit the rate of phase transi.'
tion. "The autho,~s thank Professor M. 1. Kaganff,,I, or a discussion of the work,"
- R.
Orig. art. has: 5 figures and I formu
'ASSOCIATION: Fiziko-tekbn1cheskiy institut Akademii nauk Ukrainskoy SSR Qbysico-
technical Institute, Academy of Sciencesp Ukrainian SSR)
summm-. l5mar65 EXCL: 0.0 ZICODEI 08,,-EH
NR MF SOV: oo4 onm oil
tki
Card 2/2

L 14500-65
h6m-~-~"W "4,048632 S/0048/64/028/010/1599/1616..
AUMOR: Soloviyev, V.G.; Fogel*, P.;
TITLE: Investigation of octupolo states of strongly defom~~d even-even
portj Fourteenth Annual Conference on Nuclear Spectroscopy held in Tbilisi 14-22
Fab 1965
_47
SOURCE-. AN SSSR. Izv. Seriya fizicheskaya, V.29, no.10, 19641, 1599-1616
TOPIC TAGS: nuclear physics, nuclear model, nuclear structure, excited state
ABSTRACT,-: This-,paper presents a systematic theoretical Investigation of the ener-
gies and-structures of-tlho-octupole~ excited states with j% w 3 and p = 0,1,2,3 in
strongly deformed even-even nuclei. The calculations are per-formed on the basis of
:the.superfluid model by the method of approximate second quantization. -she #!.3rived
secular equation is simplified on tho,assumption that the three octupole-oct-upole
Interaction constants (for the pp, nn, and pn interactions) are equal. Calculations'
performed for the even-even nuclei with mass numbers between 150 and M., and
between 228 and 254, Nilsson wave functions were employed, with the deformation
parameter 5 assumed to have the same value 0.3 for all the nuclei In the lighter
1/3

L 1450o-65
'ACCESSION NR- AP4048632
hos6 in the heavier gxuup. The octupole-octupole in-
-group, aiul the value 0.2 fort
teraction was also assumed to be constant within each of these two groups; the in-
teraction constant was so chosen as to give the Wat agreerrant with the expertmon-
,tal energies of the 0- states. The first two roots of the secular equation were
.calculated for the G-jl-, 2-, and 3- states, and the energy values, together with
the energies of the first and second bands and the corresponding experimental data
(when available) are presented graphically. The calculated values of the energies
of the lowest, l-, 2-, and 3- states Agree well with the experimental values, pro-
vided the effect of blocking is taken into account when it is important. 7he octu-
pole-octupole interactions are usually- important for I- ani 2~ states, and are usu-
ally negligible for 3- states. The structures of the octupole states are illustra-
ted by tabulating the contributions of the various two-quasiparticle statc3 for a
number of selectedt nuclei. In most nuclei the lowest 0- state is strongly collecti-
vized, whereas the I- and 2- states may be collectivized but are usually r.ither
.close to two-quasiparticle states. The 3- states may be regarded as two-quasipar-
ticle states with less than 1% admixture of other than the principal state. Re-
duced electromagnetic transition probabilities were calculated, and a.future paper
is promised in which these will be discussed. "In conclusion, we express our grati-
tude to N.N.Bogolyubov for an interesting discussion of the article, and to._K.H
2/3

3/3

ACCESSION NR: AP4010752 S/0020/b4/154/001/0072/0075
AUTHORS: Solov,yev, V.G.; Fogel',.P.; Korneychuk, A.M.
TITLE: Energies of cotupole collective states With I K 1 0
even-even strongly deformed nuclei
SOURCE: AN SSSR. Doklady*, v. 154, no. 1. 19b4., 72-75
TOPIC TAGS: energy, octiipole'collective state, deformed nucleus,
superfluid model, excitation state
ABSTRACT: Research based on approximate second quantization was
conducted on properties of atomic nuclei. Results were realized in
the area of spherical nuclei where energy states and probability of
electromagnetic transitions were computed. It was found that re-
search in the area of strongly deformed nuclei is limited, but basic'
equations are cited and the question of excluding the heated state
is studied. Based on the method of approxima-e second quantization
in limits of superfluid models of the nue , energies
leus were calcu-
lated for octupole collective states with IJLK =1 - 0 of even-even
'Card 1/2

ACCESSION NR: AP4010752
strongly deformed nuclei in areas of 15~,g k6 186 and 2286 A::5254.
The behavior of collective octupole state energy with K7r=.O is ex-
plained by introducing one new constantJt ; all remaining parameters
are specified earlier. Microscopic treatment of tbe-state based on
the superfluid model of the nucleus differs strongly rrom the
phenomenological treatment of the unified model of the nucleus.
According to the treatment of the superfluld nucleus model, the
octupole states in single nualei'are relatively low (lower than
tP
and Tof vibration state I
s), and possess clearly expressed collec ive
properties, but in other nuclei such states have high energy values
and are inherently similar to quasi-partlele excitation states. "In,',"
conclusion we are deeply grateful to academician N.N. Bogolyubov for!
interesting discussions and to G. Yunklaussen for his help In con-
ducting numerical calculations." Orig..art. has: 2 figures.
ASSOCIATION: Oblyedinenny*y institut yaderny*kh isaledovanniy
(Joint Institute for Nuclear Res*darch)
SUBMITTED: 06,-Tu163 DATE ACZ: 1OFeb64 ENCL: 00
SUB CODE: PH NO REF SOV: ~co4 OMER: 009
2/2

L 61032-65 alVl) UP(c)
ACCESSIOR NR:
57
'AU11111011: P og -all P4
.-TITLE: Elea troE41~rj~l~ie transitions from collective states
"SOURCE: Yadernaya f izijr,4, v. 1y no. 5. i965, 752-757
TOPIC TAGS: eleotromagnotic-transition, collective zitate, Gamma
vibrational state, quadrupole state, octupole state, se-aond-quantiza-
,tion, superfluid model
-PBSTRACT: The author calculates within the framework of the-s4er.-
,flui(I model , the rpduced probabilities of E3, E2, and El electroinair-
netic transitions Xrom quadrupole or octupole states to the ground
ste:te of deformed even-even-nualei, by using approxinate second
quantization. The probabilities are calculated for H,2 transitioft~'
M--from the y vibrational states and of E2 and El trans'-tlons
pole states, using parameters which were determined 1),,r the author
earlier (with solovIyev and Korneychek, Izv. AN SSSR ser. fiz. v. 28,
no. 10, 1964 and elsewhere) the application of the model to E2 and EO
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ACCESSION NR: AP5014314
transitions frow p vibrational states isdiscussed, and it is shown
that this case is somewhat more complicated. Comparison with experi-`-
MP r)t,; shows that this model gives a good explanatlor of' the 0)~Perl-
I 'ja' -
a, .a on transitions between one-phorion -.tate', an.! the phoncri
Tr~ view of the good agreement obtalner] f-~r 1,~io ar.,i E`i
electro:7.iagnetic transitions, it is suggested that calculations within
the framework of the approximate second -quan tiza t ion method are
generally correct. 'In conclusions I wish to thank V. G. Solovlyev
il~,r su,-Festing the research and numerous discusslo:i~,,, a:--ii -A-.-rcT-ney-
wlh 'he
h M. Zheleznova and G. Yunaklauzen for assislancc w.
4 formulas, and tablEs.
caTcl-lal-,!~)ns.1 Orig. art. h I
Obtlyedinennyy institut yadernykh IsE,'erlovarlv (Joint
Insfitut;e of Nuclear Research)
S1JBMITTED* OqNov64 ENCLt 00 SIJB CODE: GP
N1( REF SOV- 004 OTHE R: oo6
Card

8 09 0
33438
S/064/62/000/001/001/008
B110/B138
AUTHORSt Kotlyar, I. B.) Katveyeva, G. N., Smolyan, Z. B., Fogel',
Ts. I., Gulyakov, V. M., Kudryavtsev, Ye. N.
tz ---------
TITLE: Continuous method of producing cyclohexanone oximes
PERIODICAL; Khimicheskaya promyshlennost', no. 1, 1962, 18 - 19
TEXT: A two-stage, continuous method of oxime production has been
developed. Not only could it be automated, it also produces better
quality oximes, and reduces losses of hydroxylamine hydrosulfate (A):
Cyclohexanone Solution of oxime in Solution of A
FS-tage IJ.4~ cyclohexanone Stage II
(NH Solution of (NH 4)2 s04 Oxime
4)2S041
solution - and A
Reaction I is conducted with an excess of cyclohexane, and II with an excess
of A. The formation of cyclohexanone oximes follows the reaction
Card 1/1

33438
S/064/62/000/001/001/008
Continuous method of producing... B110/B138
2 0~ 0 + (NH2OH) 2*H2so4--->2a NOH + H2so4+ H20, with H2so4 being
neut.calized by NH 3' Thusq the acidity indicates the stage of oxime
formation. Preliminary experiments were carried out to determine V, the
contact period which must elapse before the acidity of the reacting mass
becomes constant, and the percentage extraction of A as dependent on its
concentration in the initial sulfate solution. Results: T' - 15 - 20 min;
optimum A concentration 20 g/liter. B and the stage II sulfate solution
containing 20 - 25 g/liter of A pass continuously into oximator 1 (Fig. 1)
of stage I. The resulting mixture is passed into 2, where it is
neutralized with gaseous NH 3* The bottom layer in separator 3, spent
sulfate solution, is passed into an evaporator, the upper one (Oxime
solution and B) into collector 4, and thence into stage II oximator 5,
where it is mixed with a new A solution. NH3 is used in the stage II
neutralizer 6. The upper oxime layer in separator 7 passes to the next
stage, and the sulfate solution passes via collector 8 into oximator 1.
A stoichiometric ratio must be preserved between the fresh amounts of B and
A fed into 1 and 5. There are 1 figure and 2 tables.
Card 2/p --)

L i2i2o-66 EWP(s) /EWT(m) /WP(b)
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GsAm- -
~OURCZ COM UR/0000/65/000/000/0108/om
AUTHOR: Fogel',, V.
ORG None
T!TiE: Microheterogenecus structure of glass
SOURCE: Vaesoyunoye soveshchan2n vo steklodbra%mmu sostovan'
Leningrad, 1964. Stekloobr%7,noye soatoyaniye (Vitreous Btate)j I
soveshchaniya* Leningrad., I2d-vo Nauka, 1965,; 108-3-12 .:
TOPIC TAGS: lithium glass., silicate glass, glass property
/6,
ABSTRACT: Glasses of the binary system lithia-silica were studied. As
the L1,0 content increasesq the mean diametir-cT drop-sFa-ped vitreolxa micro-
phases, determined with an electron microscopes inereaaesp goes through a
maximium, drops to zero, then increases again. The drop-shaped phase is
thought to'be rich in lithium ions, A study of the solubility of binary
lithia-silica glasses in dilute hydrofluoric acid showed that glasses con-
taining 16-27 mole % Li2O behave quite differently from the manner predicted
theoretically,
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L 1212o-66
Ace. Nr. AT6ooo475
This divergence can be explained only by profound changes occuring in the
fine structure of the glasses during solution in HF. A study of the pro-
cesses of dissolution and crystallization of lithia-silica glasses revealed
that the formation and subsequent behavior of drop-shaped microphaaes in
the glass cannot be described by purely statistical relationships3 if this
were the case., then as the bulk composition of the glass changed, the com-
position of the microphases would also change statistically. This does not
take place, however, the bulk composition corresponds to definite chemical
ecimpounds., and the transition from one compound to another takes place in
discontinuous fashion. Primary and secondary phase-separation processes
are discussed. Orig. art. has: 8 figures,
SUB CODE: 07., n/SUBM DATE: 22M&Y65 OM MW: 008
ja
Car,*~2

Um/maginoering Jau 19he
Boilers
Heating, Indwrtrlal
"Installing Air Preheaters for %-11 Capacity Boil-
Ormw V. 0. Yogell, Candidate Tech Sol, 8 pp
OU M= Toplive No 1
In recent surrey by the Soviet State Institute of
Fuel Conservation it vas discovered that the mkjor-
ItZr of Installations were equipped vith -11 boiler
=Its producing at the rate of 3 tons per how.' Of
these boilers, 75% not equipped vith.any tnm of
liitsr collector Or air Tr6h*&tGr~ and than ayerage
20-25% fuel vaste. Basically, these boilers us*
IC
MR/RagineerIng (Ccntd) Jan . 19W
lov-grade coal, peat, and cordw6od. Mix fuel oon-
Ulaw high xwIsture ocntent, and It vould be vla* to
=0 preheated air. Describes installation of &jr
Vreheatere for sma'l-capacity boilers.
W 5LT14

Feb 49
Ireating,' Tndustrihl
Heat Exchange Systems
*&ating by HIgh-Temperat-ure Fluid. Heat-
Conductors Through Natural Circulation, " V. 0.
Togell, Asst Prof Moscow Inst of Fine Chem Tech,
4 pp
"Ircm Energet " No 2
Gives skeleton design of heating installation
baving a heat generator, outlet and return pipe
from the heat exchanger, and a condensing tank.
Heat conductor is a mixture of diphenyl and
diphenyloxide. Gives mathematical calculations
33/49261
VSM/Engineering (Contd) Feb 49
for diameter of conducting pipes, expendititre of
-conc
eirculating.beat luctor and its temperature
Vaile entering and leaving the heat exchanging
derice.
33/49T63.

0
A a c 0 a 44 4
' ' "' "'t
4 X t a $1 0 FU
IST ..a M LITT** I.VUITIR 40.0 at"Ovolls
Aill.06 Mott
I*,& --
VAIISM(A 4bot.
,eel
left
eel
ear
rayAlrull oil?
oar
i_'ILA (A.)AMIJ
'A IMP %j!tj%Aj-j
"Allsojads".61 JO "I"N 00
00
80,
00-
00 9 OrA
00- -1-11-1-Uld. ST or*
T v I
0 0 0 0 t* 0 0 0l

FOGEL'S V. 0.
UF~R/Electricity - Thermodynamics
Heaters
Aul; 50
?tSelection of Optirrvim Temperatures for High-Bniling Intermediate Heat-Carrying,
a
Agents in Industrial Installationsj" B. L. Uvshitss V. 0. Fogel', Candidates
Tech Sci, Docents, Moscow Inpt of ine Chem Technol imeni Lomonosov
"Prom Energet" Vo Bi pp 4-9
Gives table of design formulas from which optimum temperatures can be selected for
subject agents usnd for heating and cooling in industrial inEtallations. Includes
proof3 for these formulas which arevrorked out for both liquid and gas heat-carrying
agents.
PA 164T24

iiiiiii~ 41i~~--. 000-1 0
td
S,jlutious of fjie--~ equaticiis arcaLlo 6vqi for Cat part:i cr3r--
A pilies of sw--L- c-iffering in coml. Other cqitati-n-j
siaing c
are oven Cu, cyUndricJ :Lad rcctangular blinck 5t:apl, wiii
tables and C-dr,"en of sciale consts. us- Xtudersol! 9
r t-

FOGIILI' Y.O.
Iffect of thermal stresses ox the thernophyetcal chsraeterlstles
of Wead dough, MO. I kond. ~roa. 1 mo.2:10-13 7 157.
(KM 10.. 4)
I. 16440YUNVY nauchne-lefledovatellakty Institut khlobopokanay
prowshlennosti,
(Dough) (Heat--Transmission)

GENGRINOVICH, B.I.; FOGZLI, V.0.
Thermophysical characteristics of Industrial rubbers. Zauch.1
res.16 no.9:27-32 3 157. (MIRA 10:12)
1. Nouchno-imeledovatellakly institut shinnoy promyshlennosti.
(Rubber)

BIRKcAN, Yu1iy.BeneaiktoVich; IPOGZL', V-0-.. spetared.; TEMKINA, I.S.,
vedushchiy red. ... - ., -I -
LHigh-temperature beat engineering in the oils and fate industry
abroad) Yysokotempersturnoo teplosnabzhenis V 2hirovoi pro-
myshiennosti s& rubashom. Moskva. GW1NTIe 1959. 47 P-
(MIRA 13;6)
(Oil industries) (Beat engineering)

VOZNOVICH, PeD,; FORM,~.,.-T.Q.,~,kand.takhn.nauk, retsensent; LUKONBKIY,
Ns-
S.M., ka~d. i~snmuk# red@; LANOYBUTA, M.R.. red.isd-va;
ATTOPOVIGH, M.K.', takhn.'red.
[Oooling of atallurgical furusosv~'Iby mans of high tenmrstum
he t carriers] Okhlashdonis mtftilurgichoskikh pechal vyooko-
ts;;6raturaymi toplomositeliami, Kooky&, Goa.usuchno-takhn.
isd-ve lit-ry po ebernoi I, taystnot, metadluigli, 1959s 228 pe
(NIB& 12:7)
(Metallurgical furnaiss-Cooling)
i

YOGRI, V.0.
liffect of thermal conditions on the heating and cooling of
somtlimited bodies [with suwwu7 In Nnglish)e Inxh.-fizezhur.
no.1:87-92 Ja 159. (MIRA 12:1)
lo Inatitut tonkoy khimicheskoy takhnologii im. H.V.Lomonosove,
Moskva.
(Heat-Conduction)
W 0,~,,
T R

5W SOV/153-2-3-24/29
AUTHORS: Zanemonets,
TITLE: A New Method of Determining the Thermal Effect of the Reaction
of Rubber Vulcanization
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy. Xhimiya i khimicheskaya
tekhnologiya, 1959, Vol 2, Nr 3, PP 437-442 (USSR)
ABSTRACT: The new method developed by the authors is based on the determina-
tion of the heat balances from the results of thermographic
analyses (mothod of thermographic balances). The differential
equation for the heat conduction can be written down by taking
into account the inner sources of heat in the following form
(Ref 6): Ot . A 62 v (2).
+ L
a'T c7 cy
t denotes the temperature in the point observed, T the duration
of heating, 2 _ + 2L
t . a2t + Zt t
ax 2 ay2 az2
the Laplace operator, q v the thermal energy of the inner heat
sources with respect to the units of volume and time, X thermal
conductivity of the material and cy its thermal capacity by
volume. From this the following equation is obtained for the
desired development of heat (intensity of the thermal effect
Card 1/4 of the reaction):

SOV/153-2-3-24/29
A New Method of Determining the Thermal Effect of the Reaction of Rubber
Vulcanization
qv A A2t + a 7 at . q + q kcal (3)
. 2 aT A ak M3 time
I
(qX --X-& t .... amount of heat flowing thru the thermal con-
duction during unit time from the unit volume; q - -1 at
ak a -r ...
amount of heat which accumulates during the unit period in the
unit volume). On the basis of the investigations carried out
by the authors the temperature distribution in thin symmetrical
heated plates of the rubber sample corresponds to the follow-
ing formula; x 2
t - ta +(tc + tW) (6) (5)
(to 000 temperature of the center of the plate, tw **6 tempera-
ture of the surface, x .... distance of the point observed from
the center of the platev 6 .. half thickness of the plate).
The amount of heat q emitted due to the conduction of heat is
the following for suh a plate:
qX a2t 2A(tc-tw) ' 2XAt koa1 The mean
72 2 2 [m3 ti
Card 2/4 x 6 6 mej

SOV/153-2-3-24/29
A ffew Method of Determining the Thermal Effect of the Reaction of Rubber
Vulcanization
temperature of the plate may be computed from the following
21 +t
0 w at
equation; tM td. . _ to -3 (7)- (At - tc-tw....
6 3
0
temperature drop in the plate). From this the intensity of the
heat accumulation qak n the plate may be computed:
at M kcal
q OY - (8), and the thermal energy of the
A ' O'T M3.time
beat sources a the m ant concerned, which in this case is
charaoterized by the intensity of the thermal effect in the
vuloanization, may be determined from equation (3). The authors
tested this method in the investigation of the thermal effect
of the vulcanization reaction of ebonites from butadiene styrene
rubbers. Satisfactory results were obtained. The apparatus used
for the determination of the thermal effects is schematically
represented and exactly described. Figure 4 shows one of the
thermograme obtained. The method elaborated is suited for in-
vestigating the kinetics of the heat formation and for deter-
mining the initial 8atalbr the computation of the thermal effecT
Card 3/4 of the vulcanization process of rubber. There are 5 figures

SOV/153-2-3-24/29
A New Method of Determining the Thermal Effect of the Reaction of Rubber
Vulcanization
and 8 referenceal 5 of which are Soviet.
ASSOCIATION: Moakovekiy institut tonkoy khimicheekoy tekhnologii imeni
M. V. Lomonosova
(Moscow Institute of Fine Chemical Technology imeni, M. V.
Lomonosov).
Kafedra toplotakhnika (Chair of Thermal Engineering)
SUBMITTED: June 24, 1958
Card 4/4

SOV/138-59-4-4/26-
AUTHORS: Sandomirskiy , D.M.2 FQ52~~W.., and Mayzelis, B.A.
TITLE: The Thermo-Physical Characteristics of Latex Foams, Gels,
and Sponges ( Teplofizicheskiye kharakteristiki lateksnoy
peny, gelya i gubki)
PERIODICAL: Kauchuk i Rezina, 1959, Nr 4, pp, 13-16 (USSR)
ABSTRACT: In order to design plant for 'processing latex through
foams and gels into latex lpongel it is necessary to know
the the=1 diUusiYity.0C(m /hour), the thermal conductivity
, ) an4 the si3ecific heat at constant
(kcal.m7'hour_'der,_7
volume cy (kcal.m I deg-'L) of the material at these different
stages,_ A rapid method for measuring CC and 7, is necessary
since the material properties change during a fairly short
time. The specific heat cy can then be calculated from
cy = W/tt, A "universal calorimeter" was devised as shown
in Figure 1, and consists of two co-axial, open-ended
cylinders between which the latex foam is gelld and vulcan-
ised into a sponge. Heat is supplied by the spiral element
(3) at the axis of the cylinders which is fed from a
battery. One thermocouple (4) is mounted at mid-length on
the thin walled inner cylinder an,i the other thermocouple
Card 1/5 (5) is inserted into the sample material at the same level

SOV/138-59-4-4/2~5
The Thermo-Physical Chaxacteristics of Iatex Foams, Gelsj and
Sponges
and at radius r from the axis. The couples are connected
to a galvonometer through a change-over switch. The
heating element is fed with a definite current so that
the speRific aiourLt of heat k supplied to the specimen
(kcal,m hour- ) can be dete ined while the temperatures
at the two thermocouples t and t are logged against time
of heating-re The maximum~time of heating at which one
can neglect heat losses from the external surface of the
specimen (when the external rqdius R is 5 times the in-
ternal radius R.,) can be calculated irom Fourier criteria,
and under these conditions the temperature rise of the
inner cylinder wall t to the temperature rise of the
specimen t is a functfon cLf r/R 9 and the Fourier number
as.shown in Eq (1). The thermal condu--tivity_-can then be
deduced from Eq (2) by using the Biot number e * The
actual apparatus was constructed with R 10Z mm, r--lamm
and L = 200 mm. Table 1.5ives the relaiionships required
for the solution of Eq ( under these conditions. F is
found fromeNt/At anj the coefficient of thermal difAs-
ivitym from a= 1_1~-/ye Thermal conductivity X follows
Card 2/5 from Eq (2). Expdr ments were made on "Revertex" foams,

SOV/138-59-~-4/26
The Thermo-Physical Characteristics of Iiatex Foams, Gels, and
Sponges
foamed or extended to three times the liquid volume by
propeller stirring, The formulation contained thickening
and geliLting agents as for material intended for auto-
mobile seats. The coefficients-OL, X and Gv of the foam
were determined immediately afte~-foaming an the mixer.
The whole apparatus containing the foam was then placgd
in a heating chamber and the temperature raised to 60 0
to gel the foaml after which the same coefficients were
again determined. The temperature of the heating chamber
was then raised to 1430C, and the gel vulcanised into a
I'sponge'19 and the thermal characteristics determined again
in this state. Considerable scatter was experienced in
the measurements on the foam or the gel because of the
rapid change in their characteristics while the measure-
ments were being made. The more stable vulcanised Ysponge"
gave consistent results. Kinetic curves of c,,, X, andC~
Card 3/5against time rare given for latex foams as mixed, and for

SOV/138-59-4-4/26
.The Thermo-Phypical Characteristics of Iatex Foam59 Gels, and
Sponges
the gelating foams during syneresis, in Figures 2 and 3
respectively; the former curves were obtained using
material which.did not contain gelating agents. The course
of these curye?-is explained from the structural changes
in tbt6 materia which takes place during the processes and
,il demonstrate that constant characteristics are not
th
a ,ted during tho gelating and vulcanising stages.
c use of this, determination of the thermal coefficients
a made with foams five minutes after they were mixed and
w
e ended, and with gels thirty minutes frqm commenceEient of
e:Te
gelation without syneresisl which periods are similar to
production conditions. Table 2 gives the values ofGt, X
and c%- for foam (extendeg to three times original liquid
volume), of"the gal at 60 0, and of the dry "sponge" from
the same extension of foam at room temperature. Experim-
entally determined values a:re given in the table and also
values calculated by an addition. method working from the
corresponding characteristics of latex, water and air.
The difference between the experimentally cLetermined values
Card 4/5 and ;. the calculated values indicates that it is not

SOV/138-59-4-4/26
Tl~e Thermo-Physical Characteristics of Latex Foams, Gels, and
Sponges
possible to deduce values for other degrees of extension
or at different temperature from one set of dedta, and that
separate determinations should be made.
There are 3 figures, 2 tables and 8 references, 7 of which
are Soviet and 1 CzArman,
ASSOCIATION: Moskovskiy institut tonkoy -khimicheskoy tekhnologLi
im. M.V. Lomonosova ( The M.V.Lomonosov Institute of Fine
ehemical Technology, Moscow)
Card 5/5

LIVSHITS, BA., kand. tekhn. nauk; FIDGELI, V.O.. kand. tekhn. nauk
Intensification of the process In heat exchange:-s heated bjr
means of high-temperature heat-transfer agents* Proms energe
14 no.1:34-36 A 159. (MIRA 12:1)
1.Moskovskiy Institut tonkoy khimichookoy takhnologil Imeni
Lomonosova.
(Heat exchangers)

AUTHORS: Zanemonets, N. A. and Fogel~ V 0 SC"W138-59-2-7/24
TITLE: The Thermo-Physical Characueristi,s arA Thermal Effects
of V-Lt'canization of 11ar,d Rubber Mixtures Pre ared from
Butadiene-Styrene Ru"Ibors (Teplofizicheskiye
kharak-teristiki i terilo-v7ye effe'Ll-ty reakt.9ii
ifulkanizats-ii ebonitovyldi smesey -Lz butarliyen-
stircl~nykh kauchulkov) 11
PERIODICAL-. i ,zina. l9c;9,,,1Tr 2 pp 2a-2,' (USSR)
ABSTRACT: Experiments were carried out on -the thermal conductivity
of SKS ha:rd rubber mixtures ur-O the -thermal effec~ts of
mixtures containing 6 to 53% weight of sulphur to 100%
weight rubber dete-r-mined. Tha samples were prepared in
the Laboratoriya ebon4ta fLaborul-~).ry for Hard Rubber) of
the NIIRP and the pe-_?."entage of. free sulDhuiL, determined
in the samples after vuleaniza-tica. The thermo-physical
characteristics of, the samplas ware defined before and 0
after vul--anizgtion in the temperature IJ.mit Itetween 20
and 100 -to 1530 0 '-'*.n the apparatus shown in Fig 1. The
samples consisted cf twn foils (thickness 4 mm, width and
Card 1/4 length 40 mia) with a flat heater between them.

SOV/138-59-2-?/24
The Thermo--Physical Characterlstics and Thermal Effects c~f
Vulcanization of Hard Rubber Mix"Gures Prepared from Butadiene-
Styrene Rubbers
where they -were
They were placed in an ultra-thermosta~'
kept at a constant tem 'Derati.,Z-e (+ 0.05 C). A formula
is given for calculating tl-t-. cceffi-_,ient of heat
conductivity of the samples. The composition cf six
tested samples is given in Table 1. 1-7he graph In Fig 2
in&icates that the heat conduct-ivity of the samples
SKS-10 and SKS-30 decreases with iri:_-re~-sing temperature,
remains practically constant in 2.ase -;f the sample
SKIQ-=O, and increases with -cempir-at-are in the
'JCj4tiO--j Of bhe a::celerator
sam-nies SKS-60 and SXS--90, A,
diphenyl guanidine owases a decr-ase 'n the coefficient
Of heat condr-etivity of the m-.c with incr'-,%asing"
C~
temDerature. Aft__ vul-p n`zation `7he he-it conductivity
'2r6 ~was C, to !&/~ h"
in mast samples, at 153 1 gher than it
was in the raw Plix at the same temDe--at',ire. The
temperature coraduct-j:yity of the sari samples was found
Uo be decreasing with the rise of te-jjreTa4-jj_:-e (Fig 3)
An ana-10gOUS decrease of the t;-.rzi-oerat1arc- --onductivit3r
Card 2/4 was also fo',;.nd wher, Li-.-Iii

SUV/138-59-2-7/24
The Thermo-Pir/sical Chara,;ter-'._,Ai~-..s and Theriijal Effects .)f
Vulcanization of Hard Rubber MIxturez Prepared from But-adiene.-
Styrene Rubbers
characteristics of tyre mixt-ures. The '511emr1al effects
cf the v,,ilctanizati-n process of hard butadiemc-styrene
rubber i:,Lxtura~3 were determir_,ed by a mE;thad )ropCsed
b-,,,, the authors is based on thE! thecr-7 of heat
0 -ii o 41
I- -ivity of therir.C.gramE ,,,btained -he
Ar. e, ,ation f~:,r c?. ~;,alating the
t,~,ta"_,. thsrmai effei-,t is Fi..g .'r': :) --hermogram of
an SKS-30 sample; lable 2: the thermo-physice.-L
samp.,~s at. a temperature
~f 1.50 C. TI_-e Jmtemsit-y cf the therrfal effect of these
s
1~ in
a-nip , s vias a-ad is shown - th~a of -a
'-7h:, maxim-~,,m thema-I ef"e-tt o c: r,
,aes,~ mLy-tux-ec. 4 't.~_% 5 hc,---,-,-s after the ~-.,uuaencement- of
heat_-'*_-_ts and vas for th.-~!-,.e which had an
4r.c:cea_!:-od numbex-r- of droub'_-s b~-,nds. The. theimal effe-~t
was t,) N%~,ien an
a-.celeraT,or zo the Re8i~jts Df caloulations cf
Card 3/4 the therm-al --f at.i. ~~n a2?e. ;s--*,.-ver,. --'Ln Table 3

SOV/138-59-2-7/24
The Thermo-Physical Characteristics and Therfaal Effects of
Vulcanization bf Hard Rubber Mixtures Prepared from Butadiene-
Styrene Rubbers
and Fig 6. At an equal percentage content of bound
sulphur the thermal effects of the vulcanization of hard
butadiene-styrene rubbers are much lower than for
natural rubber (about 3 times lower than data given by
J. T. Blake - Ref 3, and 25% lower than values quoted
by R. S. Jessup and A. D. Cummings - Ref 4).
There are 6 figures, 3 tables and 4 references. 2 of
which are Soviet, 2 English.
ASSOCIATION: Moskovskiy institut tonkoy khimirheskoy
im. Lomonosova (Moscow Institute for Fine
Technology imeni Lomonosov)
tekhnologii
Chemical
Card 4/4

ZANXMONNTS. N.A.; FOGILI. Y.0.
New method of determining the thermal effects produced b), the
vulcanization reaction of rubbers. Izv.vye.uchob.zav.;khim.
i kbim.tekh. 2 no.3:437-442 159. (MMA 13:8)
1. Moskovskty institut tookay kbimichaskoy tekhnologii imeni X.T.
Lomonosava. kaf^Ara toplotekhniki.
(-4ubber--Thersal properties) (Vulcanization)

89062
IT. 91 Po S/138/60/000/010/004/008
IT i S" A051/AO29
AUTHORt Fogel', V.0.
TITLEt Investigating the Thermal Conditions of Vulcanization of Heavy Rub-
ber Articles by the Method of Electrical Modeling
Iq
PERIODICAL: Kauchuk I rezina, 1960,~No. 10, pp. 23 - 29
TEXI!t The author recommends the method of electrical modeling for investi-
gating the vulcanization conditions of compact rubber articles, which does not
require thermal measurements. Thermal measurements are labor- and time consunbg
and do not give accurate results due to distorted temperature showings of the hot
junctions in the thermocouples used. According to the authors, electrical models
are conveniently used for studying the processes of heat exchange in various in-
dustries and in the rubber industry in particular. It is stated that the physi-
cal processes of the actual body can be modeled if the mathematical description
of these processes in both the actual body and the model are the same. This is
the case for thermal conductivity and current distribution in a circuit withdls-
tributed resistances and capacitances. It is shown that the heat conductivity
processes can be modelled by the electrical analog method, i.e., the change in
Card 1/9

89062
3/138/60/000/010/004/008
A051/AO29
Investigating the Thermal Conditions of Vulcanization of Heavy Rubber Articles
by the Method of Electrical Mcdeling
time and space of the teraperature in the actual body can be evaluated from the
change in the voltagesU relative to time and space of the model (Refs. 1, 2). An
example Is givent for a uniform heat flow, the specific heat flow is determined
according to Fourier's law: q - -Adt (1), where % is the heat-conduating co-
efficient In kcallm - h - OCI dt 9% nt in OC/m. For a
OT%- is the temperature gradie
circuit with distributed resistanoes and capacitances the current intensity Is
according to Ohm' 5 law i - -1- " (2), where R - Rsum/1 is the resistance of
R O-x
1 m of the circuit in ohm/m, and dU/d% is the voltage gradient In y/m. The dif-
ferential equation of the heat-conduoting process (Fourier's equation) for a uni-
form flow of heat in a body with constant heat-physical characteristics ist
07 t d2U
8~- = a (3), where a is the coefficient of temperature-conductivity inm%-
The differential equation of a long line (telegraph equation) for a circuit with
distributed resistances and capacit IT ces in the absence of leakage in the oapac-
itors can be expressed: du I (P U (4), where C Csum/l is the capacity of
W T TU =OX
Card 2/9
i~~, ~,P

'9*138/60/000/010/004/008
A051/AO29
Investigating the Thermal Conditions of Vulcanization of Heavy Rubber Articles
by the Method of Electrical Modeling
of I m of the circuit, in farad m; RC - RsumCsuff/12 is the product of the capao-
ity by the resistance of 1 m of the circuit, in see/m2. It is pointed out that
Equations 1 and 2 and also 3 and 4 are only different in nomenclature of the
physical values, but are the saw from the mathematical point of view. In order
to make this type of comparisons 1) the initial temperature and voltage distri-
bution must be the same, 2) the change of the temperatures and voltages at the
boundary lines of the bodies must comply to the same law (Fig. 1), 3) the ratio
of the experiment duration on the model T2 to the duration of heating and cooling
of the actual body,%j, must not be selected arbitrarily, but based on the equal-
ity of the similarity criteria, which characterize the processes of thermal con-
ductivity and electricity distribution in the circuit, having distributed resist-
at
ai., ~ and capacitances (i.e., Fourier's criterion). FOthermal - a (5), where
Tj the heating or cooling time of the actual body in hours, is obtained from the
analysis of equation 3, for a plate with a thickness of 26. For a uniform elec-
trical circuit with distributed resistances and capacitances Fourier's criterion
based on an analysis of equation and assuming that 1 = 26 is equal to:
Card 3/9

89062
S/138/60/000/010/004/008
A051/AO29
Investigating the Thermal Conditions of Vulcanization of Heavy Rubber Articles
by the Method of Electrical Modeling
FOelectr. ' 3,600 T2 W 14,400 Tp (6), where T2 is the duration time of the ex-
TC-6 2- Raum Osum
periment on the model in hours. The time range PIC must comply with the criteri-
S2 . R C a
on equality of similarity Fothermal - FOolectr., thus, Mr -It, A==_ (7),
14,4008T
where Rsum and CSUM are the general resistance and capacitance of the model, a
is the temperature-conductivity coefficient of the plate (m2/h), and 6 is half
its thickness in m. The model is prepared in the form of a lattice with the re-
sistances and capacitances located on the points. If the number of joints in
the grid is equal to n, the resistance of one point is R1 and its capacitance Cl
an expression for the time raAge is obtained, considering that Rsum - nRj, and
neRiCia
csum = nCj, viz., MT= i2 . (7a). The YCM-1 (USM-1) universal lattice
Ti 14,40047 .
machine, intended for the approximate solution of hydrodynamic marginal problems
and that of the resistance of materials Is being prepared for production. Its
shortcomings are Its complexity, high cost and the relatively high discrepancies
in the results. It is suggested that simplified electrointegrators fed by d-c
and not a-c be introduced. The YVAU-1 (UMEI-1) unit is presented (Fig. 2) to be
Card 4/9

89062
,9/138/60/000/010/004/008
A051/AO29
Investigating the Thermal Conditions of Vulcanization of Heavy Rubber Articles
by the Method of Electrical Modeling
used for modeling thermal effects of vulcanization. There are no auxilliary at-
tachments, its area is 2 M2, the cost about 5,000 rubles. It is suggested that
the BC (rOCT 2825-55) - VS (GOST 2825-55) type wireless carbon resistances be
connected to each grid, produced with 100 to 910 kohm for an operating voltage
of 350 v and hermetically sealed thermo-resistant paper capacitors of the BrT
(BGT) type with a rated maximum capacitance of 10 Pf for a workinS voltage of
200 v d-a be used az the ~;apacitanoes. In assembling the grid, special attention
should be given to th-e distribution uniformity of the resistances and capacitwxms
along the. joints. As source of direct current the author recommends using eitlier
the 70-AMqr-5 rOCT 7534-55 (70-AMTsG-5 GOST 7534-55) type "Druzhba" battery or
the alkaline cadmium-nickel battery of the 64-AP-2,25 (64-AKN-2.25) type or the
BCA-III (VSA-III) type selenium rectifier with a filter made of a choke and two
capacitors for smoothing down the pulsations of the rectified voltage. All
recommended sources yield a voltage Of 6"0 - 80 v. D-c from the source is f, e: 7to
two voltage dividers in the form of sliding wire rheostats with a resistance of
5,000 ohms. Portable multi-limit magneto-electrical d-c volt-meters are suggest-
ed for measuring the voltages at the dividers, viz., the M-106/1 (M-106/1) type
Card 5/9

89062
S/138/60/000/010/004/008
A051/AO29
Investigating the Tbermal Conditions of Vulcanization of Heavy Rubber Articles
by the Method of Electrical Modeling
of 0.2 class, where for 75 v the value of one division of the mirror scale is
0.5 v. The C-95 (rOCT 1845-502) - S-95 (oosr 1845-52) type electrostatic voltme-
ter is suggested for meaturing the voltages in the points of the lattice. The
voltage range is selected depending on the voltage of the energy source and the
magnitude of the scale of electro-measuring Instruments expressed by the formu-
la: Mu - (U - Uo)/Ikt - to), and never exceeding: 75 = 0.47, where 75 v is the
160
scale of the electrostatic voltmeter and 1600C is the maximum temperature in the
vulcanization of casings. The initial condition of the heating process of the
compact rubber articles is usually t1he uniform distribution of temperature, to
const, which correBponds to the initial voltage of the model, Uo = 0. Thus, the
temperature field In the actual body can be determined according to the distri-
bution of the voltages in the model, i.e., t = to + -U (8). Calibrating ex-
I WU_
periments on a simplified electrointegrator YM30-1 (UMEI 1) conducted with known
exact analytical solutions of the temperature field equation in the plate showed
that the discrepancy in determining the temperatures using the electrical model
Card 6/9
P

A051/AO29
Investigatin~g the Thermal Conditi ons of Vulcanization of Heavy Rubber Articles
by the Method of Electrical Modeling
method did'not exceed 1.5 + 2~. An-*eiample of 'this experiment is presented 4n
determining the thermal ,conditions for.the vulcanization of casings.of.the 260-20
size in an individual vulcanizer; Temperatures in the clown, sides.and rim of
the casing.were determined. Summarizing the'resultd of his expe?itents, the au-~
thor points out that the electrical model method is less laborious and is more
accurate than measuing temperatures directly with thermocouples. Using the eleo-
tro-models one can also determine the effect of a change in the parameters of
the heat carriers, size of the boiling chambers, composition and temperature
conductivity of the component parts of the casing on the vulcanization process.
There are 2 diagrams, I photograph, 2 graphs and 3 Soviet references..
ASSOCIATION: Moskovskiy institut tonkoy khimicheskoy tekhnologii im. M.V. Lomo-
nosova (Moscow Institute of FineChemical Technology imeni M.V.
Lomonosov)
R
4L

IJ9062
S/138/6o/ooo/o1o/oo4./oO8
A05-11029
Investigating the Thermal Conditions.of Vulcanization of Heavy Rubber Articles-
by the Method of Electrical Modeling
Figure 1: Diagram of a uniform plane surface
P dv Xl heat flow (a) and diagram of its displacement.(b)
q41XI 414
'd
dx Y
Ix
-TT 7-T
-T T Tj' --r
Card 8/9
a Maw
M"mmmy
F 'T"'UN,

S/138/60/000/010/004/1-308-
A051/AO29
Investic,ating the Thermal Conditions of Vul'canization of Heavy Pubber ArtIcles
by the Method of Electrical Modeling
Fig. 2: Circuit diagram of a.*
simplified model of an'.
electrointegrator (UIL~7-,T-l),
for investigating thermal
conditions of vulcaniza-
tion!. -4T J- + + T T1
T T
a) -ener,-,y qource b) voltage
dividers (sliding rheostats)
..c) electromagnetic volt-
metersj.d) constant carbon
recistance, e) capacitbro
f) switch, g) electrostatic
voltmeter.
F T
Card 9/9-

20665
S/138/61/000/003/005/006
A051/A129
AUTHORS: Sandomirskiy, D. M.; Itogell, 1. 0.; Khazen, L. Z., and
Khu Yu-Mu
TITLE: The effect of the gelatinization process of latex on the change
of its heat- and electro-conductivity
PERIODICAL: Kauchuk i rezina, no, 3, 1961, 26-30
TEXT; The authors have investigated some simple systems consisting of
latex and a small quantity of gelatinizing agents, in order to determine the
kinetics of the processes taking place during gelatinization, e. g., changes
in the heat- and electro-conductivity and the drying of the gel formed. A
spherical bicalorimeter (Fig. 1) was used for investigating the heat-conduc-
tivity. This is a metal.aphere surrounded by a thin spherical layer of the
investigated liquid. Under regular conditions the difference of the temper-
atures of the thermostat medium and the center of the bicalorimeter is ex-
pressed by the formula:
tf - t - (tf.-to)e-mz or ln(tf-t) ln(tf-to) ml: (1),
Card 1/7

20865
S113 61/000/003/005/006
The effect of the gelatinization process of... A051YA129
where tf is the thermostat temperature, to - the initial temperature of the
bicalorimeter. t -- temperature of the central part of the bicalorimeter cor-
responding to the duration 'C of its heating up, m - rate of heating. Figure
2 shows the relationship of ln(tf-t) to the duration of the heating. The
coefficient of the heat-conductivity of the liquid ;4 is determined from the
formula:
12 1
where 1 = Di/D2 is the rELtiO of the internal and external diameters of the
bicalorimeter; Cjrj - the thermal capacity of the metal sphere; Cr - the
volumetric thermal capacity of the investigated liquid. In the experiments
the method of regular heating of the bicalorimeter was supplemented by the
method of stationary internal heating of the sphere, inside of which a heater
was placed. For the case of stationary heating of the double-layer sphere,
the heat conductivity coefficient is expressed by
aver.*4 (3a)-
Faver.-At
The quantity of heat transmitted through the layer (Q tatio ar ) was deter-
mined from the expenditure of electric energy by the Rea eK ~he method of
Card 2/7

20865
B113 6,1/000/003/005/006
The effect of the gelatinization process of ... A051 YA129
regular conditions was used to determine-the relationship-~ of the latexes
and the gelatinizing mixtures to the temperature,and the scationary condi-
tions method was used for determining the kinetics of the "change during
the gelatinization process and that of syneresie. In order to determine the
effect of gelatinization on the heat-conductivity, the kinetics of the tem-
perature change relationship to the heat-conductivity was investigated both
for revertex and latex L-7 (Figs- 3t 4)- It was noted that immediately after
gelatinizing agents are introduced into the latex mixture, processes occur
causing a decrease in the heat-conductivity of the system. Th~R results ob-
tained showed that after.the system has reached a certain degree of stabili-
t;~ even before the formation of a solid gel.,. structures are formed in it
gradually, which sharply limit its mobility in certain sections, hampering
convection, diffusion and heat-exohange and thus.decreasing the heat-conduc-
tivity. The change of,the latter and.that of the electro-conductivity does
not.stop after'.the formation of the solid gel: both the electric resistance VYN
and the heat-conductivity intrease. The heat-conductivity was measured when
the discharging liquid was removed from the system, in order to determine
the effect of the syneresis on the thermal-conductivity (Fig. 6). it is
pointed out that the change both in the heat-conductivity,as well as that of
Card 3/7

20865
S/138/61/000/003/00VO06
The effect of the gelatinization process of.... A051/A129
the electric-:iZes-Istance due,to syneresis,begine b*efore-the removal of the
liquid phase be~,ames apparent. A study on the change in the electric con-
ductivity of the latex gels, when these dry out showed that this process dif-
fers.from. the.drying put of the latex in the usual film-formation. The ab-
sence of a.change inj the concentration at the moment of gelatinization bring3
about the condition,,whereby the fact of gel formation proper does not af-
fect the relationship of the electric resistance to the moisture content in
the system. There are ~ gra'phs, 2 diagrams and 6 references: 5 Soviet,
T :Engl i oh z
ASSOCIATION:-Moskovskiy institut tonkoy khimicheskoy tekhnologii im. M. V.
Lomonosova (Moscow Institute of Fine Chemical Technology im.
M. V. Lomonosov)
Card 4/7

LIVSHITS, B.L.; I~OGEL', V.-O.
Relation between the mixers and the beat exchange in a reactor Ath
welded semitubes. Lakokras. mat. i ikh prim. no-5:70-74 '61.
(MIRA 15-23)
1. Moskovskiy institut tonkoy khimicheskoy tekhnologii imeni
Lomonosova.
(Beat exchangers) (Paint machinery)

23424
S/094/61/000/008/002/003
& 0 0 E194/E484
AUTHORS: Livshits, B.L., Candidate of Technical Sciences and
_EogeLl, V.0., Candidate of Technical Sciences
TITLE: Liquid ditolylmethane, a new high-temperature heat
transfer medium
PERIODICAL: Promyshlennaya energetika, 1961, No.8, pp.23-27
TEXT: High-temperature heat transfer media of current industrial
application include mineral oils, glycerine, silicones, diphenyl
mixture, molten salts and'liquid metals; new types of heat
transfer media are being introduced,-namely aromatic oils and
ditolylmethane. For industrial processes in the temperature
range 250 to 3000C, normal mineral oils and glycerine are of
inadequate thermal stability, whereas molten salts are only
suitable for temperatures above 3850C. None of the existing heat
transfer media adequately covers the range 250 to 3000C. New
types of fluid being developed for this application in the USSR
and abroad include hydrocarbons of the diphenylmethane series which
are synthesized in the USSR and aromatic oils such as mobiltherm
6oo. The hydrocarbon of the diphenylmethane series of the
greatest thermal stability is ditolylmethane, the principal
Card 1A

23424
S/094/61/000/008/002/003
Liquid ditolylmethane E194/F.484
physical characteristics of which are given in Table 2.
In order to investigate the problems associated with the
application of liquid ditolylmethane, the Moscow Institute of
Fine Chemical Technology imeni Lomonosov (Moskovskiy institut
tonkoy khimicheskoy tekhnologii imeni Lomonosova) made a pilot
heat transfer rig. The coil, heated by town gas, has a thermal
rating of 10000 kcal/hour. In the tests, cotton seed and castor
oil were heated in the kettle to a temperature of 2600C by liquid
ditolylmethane at a maximum temperature of 3200C. Design
details of the plant used are given. The tests on this
equipment lasted 18 months with many starts and stops. The
number of hours during which the ditolylmethane reached
temperatures up to 3200C was 700 hours. The most important
property of high temperature organic heat transfer media is the
thermal stability. During the 18 months operation the viscosity
of the ditolylmethane rose by 5 -10% which should correspond to a
resin content of 3 -6%. According to existing rules, a heat
transfer medium need be changed only when the resin content is
greater than 10%. To check this point the resin content of the
ditolylmethane was specially determined and it was found to have
Card 2/4

23424
S/094/61/ooo/008/002/003
Liquid ditolylmethane ... E194/E484
risen to just less than 5%'whilst the coke number rose from
o to o.67%. Thus the thermal stability of ditolylmethane at
temperatures up to 3200C was completely satisfactory. The heat
transfer rate was adequate with a flow speed of 0.48 m/sec in the
coils. The heat transfer coefficient results are in good
agreement with data calculated by the usual procedure using the
tabulated data given. Ditoly1methane is better than the usual
diphenyl mixture in flash point and similar properties. It is
accordingly recommended that liquid ditolylmethane should be used
for heating and cooling of-high temperature industrial heat
exchange equipment. There are 3 figures and 2 tables.
Table 2. Thermal and physical properties of liquid ditolylmethane
Legend: 1 - temperature OC; 2 - saturation pressure, atm;
3 - specific gravity of liquid kg/m3; 4 - true specific heat of~
liquid, kcal/kgOC; 5 - liquid enthalpy kcal/kg;
6 - thermal conductivity of liquid kcal/ h OC-9
7 - dynamic viscosity of the liquid x 10 M2;
8 - kinematic viscosity of the liquid x 10P.sec/
M2/sec.
9 Pra dtl's criterion.
Ca;d 39

trN
0
01%.
CIQ
0
0
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CC)
0
10
0
C%J C> -P
S."
~f co
%D 41
%-~ W
ir *,,
a% _:r
001.
N, q
to W
o
VOT tvz;*o E'Ll oGO,O 9,80Z jv'o 969 Gr z OST
WG 6K;'0 6'L I ZSO'O VOOZ O&R'0 SOL tr'Z Olt
9'G SSVO 9'9 1 fSVO VC61 LOWO GIL 96' 1 OCP
P9'6 1 9VO, V61 M'O 0,91 CGL'O 2CL Z9'l 06C
V9,6 Gqz,0 I V M'O C,gzl ORL'o ITL ~V I Dip
DV6 LLZ'O O'IZ; 090:0 9-991 99L-0 tI,L 01-1 OW.
IVG 9rVO, CIZ Z90 0 1'191 ZgL'O tRL OWO 066
IC 6 SWO OU VA'O WES I GEL'O t9L - M
6T 6 LOVO, ?;'kZ 990'0 C'9~ 1 SFW0 ELL - 0L6
EV6 61C'0 R'9Z R9O'O CR I ZWO KIL - OM
PG'6 9M'0 I 'LZ OLO'O O'Z-C I P69'O 7,6L - M
n'6 I SE'D t.*SZ Z;LO'O VSZI t99'0 108 - OVZ
5L'6 OLVO 9'0C tLO'O VIR I I I L9'0 018 -
0'0 1 EWO 9'M 9LO'O L'I I I L99'0 619 - OZZ
t'0 1 61 t'O VC-C LLO'O VS0 I tWO 8Z9 - 019
L'O I Lff"O I W 6L0'0 S'SG OC9'O M - 006
I'l I 6Lt'O VI t I SO'O 9'M 919'0 RR - 061
9,11 819'o I 'Gl- CRO'O 9,99 C09,0 !;Sg - 091
VZI Z9S'O 9'6t M'O S'09 689'0 f98 - OLI
L'Z I Vi9'O WK LSO'O L'tL 9L9'O US - 091
slet CL9'O V09 6S0'0 0'69 Z99'0 089 - 091
Vill ZWO VL9 160'0 WC9 09'0 689 - 01`1
C'91 9Z9'0 9'SL C6O'O 0'99 M'O 968 - OC 1
9'91 LWO 9'99 9GO'O 9'Z;g I ~-9'0 906 - 0Z1
0'81 90'1 L'LG 160,0 9'Lv 809,0 VIG - Oil
1'61 61'1 MI G6O'O 9'ZV VGVO ZZ6 - 001
9,1Z 9VI 6ZI 101'0 L'LC OSVO M6 - OG
VtZ 69'1 Z*.Si COI'0 O'CE Z9VO SE6 - 09
WLZ 99'l 6L[ tOl'O V'S-Z CSVO M - OL
GIOC Ll,z liz 901'0 6'a OWO C96 - 09
6*GC 69'Z SSZ SOVO 9'61 9W0 096 - 09
VIV OVE 91C 01 VO G'S I ZWO 996 - OV
I '6t WE 16C Zll:O C: 11 66VO 9L6 - 'OP
8'/-g Wt SSI, t1 1 0 J, L SWO C86 - M
=I CX14 I-. X= 11 10
RZ
7E
2
X
.
Zo
k - L,
a
--.
r9 = 0

7 I
C)

LIMITS, -
Intensifying the heating of'reactors when liquid high temperature
heat carriers are used. Lakokras.mat.i ikh prim. no.1:74-78
162. (MIRA 15:4)
1. Moskovskiy institut tonkoy khimicheskoy tekhnologii im.
N.V.Lomonosova.
(Chemical reactors) (Liquid fuels)

FOGFLI, V.O.; ALEKSEYEV, P.G.
~ - ' __
New compound method for determining the thermophysical characteristics
of polymers and their relation to the parameters of the external
medium, i.e., temperature and pressure. Inzh.-fiz. zhur. 5 no.2:
35-41 F '62. (MIRA 15:1)
1. Institut tonkoy khimicheskoy-tekhnologii imeni M.V.Lomonosova,
Moskva.
(Polymers--Thermal properties)

S/138/62/000/005/007/010
A051/A126
AUTHORS: Fogel', V.O.; Lepetov, V.A.; Agayants, I.M.
TITIE. Thermophysical characteristics of raw rubber mixes and their rela-
tion to temperature
PERIODICAL: Kauchuk i rezina, no. 5, 1962, 26 - 29
TEXT: The thermal and temperature-conductivity, as well as the thermal
capacity of raw rubber mixes were determined experimentally at various tempera-
tures. Four raw tire mixes, based on CM -30 APM (SKS-30ARM) and NR were used
as investigating materials in addition to one vulcanized mix (casing), based on
SKS-30ARM for reference. The method used to investigate ebonite mixes was used.J
A new calorimeter (Fig. 1) was developed for determining the thermal capacity.-
Ethyl glycol served as the calorimetric fluid. A comparison of the thermal co-
efficients of tire mixes based on SKS-30ARM and ITR showed that these, as a rule,
are higher than those for mixes based on SKS-30ABI~. The authors con6lude that
the thermal conductivity of the raw tire mix, with a temperature range of 30
1000C, changes very slightly. This leads to the possibility of calculating the
Card 1/3

3/138/62/000/005/007/010
Thermophysical characteristics of raw rubber .... A051/A126-
temperatures in the vulcanized art'cles, using the Furje differential equation.
The temperature conductance of the raw tire mixes drops and the thermal capacity
increases with the rising temperature.
ASSOCIATION: Moskovskiy institut tonkoy khimicheakoy tekhnologii im. M.V. Lomo-
nosova(Moscow Institute of Fine Chemical Technology im. M.V. Ioomo-
nosov)
Card 2/3

Thermophysical characteristics of raw- rubber
Figure 1: Diagram of the set-up for determin-i
ing the thermal capacity of tire mixtures.
1 - calorimeter; 2 - battery; 3 rheostat;
4 - ampereirfeter; 5 - thermostat;, 6 - thermo
couple; 7 mirror galvanometer; 8 - heater; J_
9 sample.
S/138/6P-/000/005/007/010
A051/A126
2
Card 3/3

11UT11011j:
TITLE:
PERIODICAL:
33470
.S/170/62/005/002/002/009
B104/B138
Fogel', V.' 0., Alekseyev, P. C.
A now method permitting simultuneous determination of the
thermoph,ygloal dhavaetaristian of p6lymora and their dopon-
dence on thE temperature and pressure of the external medium
Inzhenerno-fizicheakiy zhurnal, V. 5, no. 2, 19629 35 - 41
TEXT: A new method permitting the simultaneous determination of the
coefficients of heat conduction and tbermal diffusivity of high polymers
has been developed at the Kafe dra promyshlennoy teplotekhniki Moskovskogo'
instituta tonkoy khimicheskoy tekhnologii im. M. V. Lomonosova (Department
of Industrial Beat Engineering of the Moscow Institute of Fine Chemical
Technology im. M. V. Lomonosov). Measurements can be made above and below
00C and at different external pressures. Two plates 3 - 8 mm thick (2)
(Fig. 1) are pressed into metallic mold (3) by means of plate (1). A
quick-response heater (5) is insert6d between the two plates. The tempera-
ture is measured wiii- thermocouples (4). At the b4ginning of the ex'peri-
ment, the temperature of the samples is equal to that of the liquid in the
Card 1/0

33470
S/170/62/005/002/002/009
'A new method permitting B104/B138
thermostat. The heater imparts a ednetant specific heat current q~ const
to the internal surfaces of the two-plates. By separating the variables
one obtains
q
1 yk sin [(2n- I),. 7C
X
(2n 2-8
-Xex
-(2n- I
P
P
for the case under consideration, where tis the plate temperature at a
point at a distance x,from the external surface, t is the temperature of
the liquid in the-t4ermostat, q. - ql,(fis the place thickness in m, A is
w
the heat conduction coefficient, a is the coefficient of thermal diffusivi-
ty, and.,r is heating. time in hrs. With the. notations (t-to)4/C)"b'/tk n'
(2n-l)rr/2, and ai/~2 _'Fo, this equa tion acquires the form
..CarU2
M
4
- --- !~ 1 ~ -,- ~ -:
E

33470
S11 70/~2/005/002/00Z/009
A new method permitting ...
6 -2 31n POW exp 10. FO).
P2
.;,The heated surface of-an unbounded plate-
is then given by
exp
to) x 10. FO)
qW
1 -0.8.1.06 ex p 2,4674 Fo) + xp 22,2066 Fo) +
+ exp(- 118,6904 Fo) +
25
-.7- -. I - 2
Results obtained b4tween -60 and +TOO C and at pressures up to 60 kg/cm
are in goods agreement. The Komitet po delam izobreteniy i otkrytiy pri
SM SSSR (Committee for Inventions and Discoveries at the Council of Minis-
ters USSR) certified the authors's certificate no. 693453/26 for the appa-
ratus described abovq. There are 2 figures, 2 tables, and 5 references:
4 Soviet and I non-Soviet.
Card

33470
5/170/62/005/002/002/009
A new method permitting ... B104/B138
ASSOCIATION: Institut tonkoy khimicheskoy tekhnologii imeni M. V. Lomonos-
ova, 9. Moskva (Institute of Fine Chemical Technology imeni
M. V. Lomonosov)
SUBMITTEDt July 28, 1961
Card 4
X

FOGELI) VOO.
Heat exchange in the vulcanization of tire castings in an expandor-
vulcanizer. Kauch i. rez. 21 no.7:30-34 JI 162. (MIR& 15:7)
1. MoskovsUy institut tonkoy khimicheskoy tekhnologii imeni
Imonosova. (Tireep Rubber) (Vulcanization)

S/032/62/028/012/022/023
B104/B1606
AUTHORS: Fogel' V 0., and Alekseyev, P. G.
T1TLE: A device for simultaneously detercining the coefficients of
hent conductivity and of thermal diffusivity of polymers
PERIODICAL: tlavodskaya laboratoriya, v. 28, no. 12, 1962, 152e-1529
TEXT: Two plates 11) of the material to be-tested are c1amiped together'in
the device (Fig.). Between them*is a flat electrical heater which supplies
a constant quantity of heat per unit time to the plates. TI,- e thermostat (7)
keeps the outer surface of the plates at a constant temperature. The
temperature drop across the plates is determined with thermocouples. The
Fourier number and t;anrA - AF0Wr are determ.ined, and the relation Fo's f(-r)
is plotted from the temperature arop using a method developed in a previous
paper (V. 0. Fogel', P. G. Alekseyev. Inzhenerno,-fizicheskiy zhurnal, v. 5,
mo. 2 (1962)). The thermal diffusivity a - 62tana and the heat conductivity
~ - qwb/Atsteady can be calculated if the thickness 6 of the specimen is
known. The device can be used' at temperatures between -60 and +2000C and at
Card 1/2

A device for-simulltaneot;sly...
2.
pressures of from 1 to 100 kFI/cm
3/07, 62/0~6/01 2/0221021d
BlG4X186
Thvre is 1 fij;ure.
ASSOCIATION: Mloskovskiy institut torikoy khimichesko) tekhnoloiii im.
i'. V. Lomonosova '(Moscow Institute of Fine Chemical '2eennoioe
imeni 1M. V. Lomonosov)
Fie. Device for simultaneously
determining the ther-al diffusivity and
heat conductivity of pal3~mers.
!j i"
Card 2/'2

S/153/62/Oo5/oo6/o1o/ol5
B075/,9336
AUTHORS: Fogel', V.O. and Alekseyev, P.G.
TITLE; Investigation of the dependence of thermophysical
characteristics of polymeric materials on temperature
and pressure
PERIODICAL: Izvestiya vysshilch uchebnylch zavedeniy, khimiya L
Ichimicheskaya tekhnologiyai v- 5, no. 6, 1962,
965 - 970
TEXT: A new method and apparatus were developed to
investigate th)e dependence of heat conductivity and heat capacity!
of polymer sheets, 6 mm t~lck, on temperature (-60 to 200 00!
a'nd pressure (up to 150 Isg1cm In the apparatus the sheets ar 8
inserted in a metal press im;narsed in a thermostatic bath at t j(;9
0
A thiA electric heater of low thermal inertia is placed between
the sheets. Heat is generated by the element for various time
intervals, which produces a temperature difference across the
sheets of ZNt = t' measured by a differential thermocouple,
w 0
oefficients of heat and temperature conductivity of an
The c
Card 2
N

S/153/62/005/Oo6/010/015
Investigation of .... E0751r,,336
organic glass and protective rubber elastomer based on
CKC-~O FAM (SKS-30 AN) increase slightly with pressure a~ a
constbLnt temperature. Initial pressures of 2 to 10 kg/cm are
necesbary to obtain good thermal contact between the polymer ,
sampl6s, the heater and the compressing surfaces. The temPeratur
conductivity decreases with increasing temperature (from 50 - 10A
whichiis explained by the increasing heat capacity of the polymers.
The heat conductivity increases with temperature initially but
decreases slightly at the higher temperatures. An increase in
pressure is followed by a slight.increase of the heat conductivity
and heat capacity of the tested polymers. There are 4 figures and
1 table.
ASSOCIATION: Kafedra promyshlennoy toplotelchniki, Mosl-.ovslciy
institut tonkoy khimicheskoy telchnologii im.
M.V. Lomonosova (Department of Industrial
Heat Engineering, Moscow Institute of Fine
Chemical Technology im. M.V. Lomonosov)
SUBMITTED: November 9, 1961
Card.2/2

-FOGEL', t. ~q,; ALMEMp P. G.
Device for wiwal+mmeous determination of the coefficients of
heat and teMerature conductivity of polymeric materials.
Zav. lab. 28 no.1211528-1529 162. (MIRA 36:1)
1. Moskovskiy institut tonkoy khimicbeakoy tekhnologii im.
H. V. Lomonosova.
(Polymers-Thermal properties)

GRAIIOVSKAYA2 I.R. I inzh.; 1POGEL't V.O., dot sent
Devic6b for heating high-temperature liqaid heat carriers. Prom.
enerd. 18 no.llt22-26 N 163. (MIRA 161l2)
i
i
.1

EWT(m)/EPF(c)/T
L 15701-'5 Pr-4 A,SD--i/AFP-TC./Al~rrC/AEDC(a)/SSP./!3-')/
AS(MD)-2/JW;D(P)-3 MID-TAJE
ACCESSION NR: AP4047529 S/0094/64/01)0/010/0033/003T
i_5
AUTHOR: Fogel, V. 0. (Candidate of technical sciences); Granovskaya, I. R.
(Engineer)
TITLE, Using aromatized petroleum oils as a high -te rripe ratu re heat carrier
SOURCE: Promy*shlennaya energetika, no. 10, 1964, 33-37
f TOPIG TAGS: heat carrier, heat tranafer, petroleum oil AMT-300
petroleum oil
ABSTRACT: The experimentally determined thermophysical characteristics of
Soviet AMT-300 petroleum oil and American M600 ("Mobiltherm") oil are
tabulated. the characteristics of both oils are very close except ior the vapor
pressure (lower with AMT-300) and the congelartion point (-30C for AMT-300 and
-7C for M600). The thermal stability of both oils was tasted by residual-gas
pressure in a flask with heated oil. at temperatures under 3ZOC, the stability of
AMTL -300 oil was found to be somewhat higher than that of M600. Further
experiments involved circulating the oil through a closed tubing circuit for 750 hrs
~Card 1/2

L 15701-65
ACCESSION NR: AP4047529
at 300, 315, and 330C. It was found that during the first 100 hrs, the heat-
tranafer factors considerably decreased due to formation of a carbon-film depoz!,#
on the inside of the tubing. The coking value, resin content, and viscosity were
measured at various stages of the experiment: the deposit thickness was 0.04 and':
0. 05 mrn for AMT- 300 and M600 oils, respectively. The authors' conclusions
are: (1) AMT-300 la equivalent to or has an advantage over M600; (2) AMT-300
rnay be used as a heat-transfer agen at Z00-315C in industrial installations.
Orig. art. has: 2 figures. 9 formulak, and 3 tables.
ASSOCIATION: Moskovskiy aviatuionny*y i.-stitut (Moscow Aviation Institute);
IAL)skovskiy institut tonkoy khimicheskoy tekhilologii (i~,'oscow Institute of Fine
Chemical Engineering).
SUBMITTED: 00 ENCL: 00
SUB CODE: FPj TD NO REF SOV: 001 OTHER: 000
Card 2/2

Am- N91 _-AM03067
SOURC CO E~_W6
AUTHORI Fogoll, V. 0. (Docoaaod); Ovchinnikovq V. A.
ORG.' Daparttment of Industrial Heat Engineering, lbscow Institute of Fine Chemical
Technology Lra. M. V. Lomonosov (Kafedra promyshlonno7 toplotakhnikip Moskovskiy insti-
tut tonkoy kh W chaskoy takhnologii)
TITLE: Now method for determining the thermal stability of high-temperature liquid
heat carriers
SOURCE: IM Xhimiya i khimicheskaya takhnologiya, v. 9, no. 4, 1966, 673-673
TOPIC TAGS: heat carrier# activation energy, thermal stability, surface scaling
ABSTRACT: A new method has be n developed for dotormining the thermal stability of
hi3h-temperature liquid heat carriers (HLH). It is based on the following assumptions:'
(1 7he BIH circulates in a closed testing unit; (2) A definite and constant amount of
heat is supplied to the unit in the experimental part; (3) The decomposition of the
HM is continuously chocked by determining the efficiency of the heating surface, do-
fined as the ratio of the experimental valuo*of the heat transfer coefficient to the
value of this coefficient for a clean surface. It is shown that even a small thick-
ness of scale, of the order of 10 microns, causes a considerable decrease (11-30%) in
the efficiency of the heating surfacep so that this quantity can be used for determin-
ing the thermal stability of the HLH. The rate of decomposition of the HLH is db-.~*.
I'CoM 1/2

-A-CC NRt A-P603-4207
tained from the. rate of change of the scale thickness. The proposed method also per-
mits the determination of the activation energy of decomposition of the HLH.- Orig.
art. has& 4 figures and 8 formulas.
SUB CODE O~ SUBK DATE& 23J&n65/ ORIG REFs' 007/ OTH RUI '001
rd' 2/2

S/147/60/000/02/012/020
E031/E413
AUTHORt Zoiell, Ya.Lj (Deceased) (Moscow)
TITLEa On the Turbulent Flow of a Fluid
PERIODICAL31zvestiya vysshikh uchetnykh zavedeniy, Aviatsionnaya
tekhnika, 1960, Nr 2, PP 105-109 (USSR)
ABSTRACT: The method is based on an empirical relation between
the forces of apparent viscosity caused by the
turbulent mixing and the time mean of the velocities.
Flow in a circular cylindrical pipe is considered in
order to determine the viscosity coefficient of the mean
flow. First, the velocity distribution is determined by
consideration of the equilibrium of an elementary volume
of fluid. The analysis is carried out for two simple
laws relating the viscosity to the mean velocity. The
results are compared with experimental data. For the
fix-st law good agreement is achieved at large Reynolds
numbers but for the second law agreement throughout the
turbulent domain is achieved; there is divergence in
the laminar domain. The second law can be used to
solve the problems of turbulent flow between plane
Card 1/2 parallel walls and between co-axial cylinders. There