SCIENTIFIC ABSTRACT SINEGUBOV, V.I. - SINELNIKOV, I.D.
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CIA-RDP86-00513R001550720020-9
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S
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December 31, 1967
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SCIENTIFIC ABSTRACT
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SAVOIENK0.1 M.K.; SHEGU36V, V.I.
Boundary layers between domains in transformer steel. Izv.
All SSSR. Ser. fiz. 25 no.12;1449-1452 D 161, (MIR.,. 14:12)
1. Inititut fiziki Sibirskogo otdeleniya AN SSSR.
(Ferrosilicon)
(Crystals-Magnetic properties)
(Boundary layer)
L 17600-63 EWT(1)/EW(q)/EWT(m)/BDS/ES(s)-2 .9/0%/63/044/(>)3/001/053
AFR~/ASD;'~ D-311JP(C)ISSD Pt-4 JD '170
AUTHOR: Savchanko, M. K. nnd Slne(;ubov, V. I.
617
TITIS: Inventleation of boundary lavers between dmains in
ferromenetic substances
V
Fj~,RJODJCAL: Zhurnal ekeparimentallnoy t tooretichaskoY fiziki, v. 44, no. 3,
1963, 781-792
WM: Following the pioneering work of L. D. L,!ndau and Ye. M. Lifshitz (Ref. 2:
Phys. Zs. Sowjetunion, 8, 153, 1935) qn uniaxial crystals, various otb3r researchers
developed a theory of boundary layersMor ordinary and maenetized multi-axial
crystal Because of the smU dimensions of the bound-ary layers, earlier
experime yielded only certain approximate values tor the afte, of t1ase layers.
To teat the theory more closely, the authors studied in their previouE experiments
(Ref. 12; Iz. AN SSSRJ, seriya fiz., 25, 599, 1961; 25, 1449, 1961) the width of
the layers as well as the distribution of magnetization within the la;ers using
the polar Karr affect.~ In the present paper they use essentially the same tape
registering -thod for the study of basic boundary
Card 1/2
1, '.7(.)oo-63
fir Mnwggn~,
Investigation of boundary layers...
S/056/63/044/01.5/001/053
types of transformer steel, nickel, and cobalt crystals. They found tha-. along
the cections of boundaries delineating the change in orientation of apontansous
ma6netization there is a fair. agreement with the results of theoretical calculations.
The width and the shape of the boundary depend on the properties of the taparated
domains and the boundary in iron silicide is one order of magnitude larger than in
cobalt, and another order of magnitude smaller th3n in nickel. An increase in
temperature widens tho boundary, and at temperatures at which the anisotropy
con3tant becomes zoro or changoe its sign, the boundary "dissolves." Mechanical
atreaces aubCtantially change the distribution of spin orientation within the
layer ac well as the cize of the layers. There are 11 figures.
ASSOCIUION: Inetitut fiziki Sibirskogo otdeleaiya Akademii nauk S&%
Institute of the Siberian Branch of the Academy of Sciences
SUMITMD: July 20, 1962
Card 2/22
ACCESSION XR: AP4023405
S/0048/64/028/003/0545/0552
AU771OR: Kiranskiy, L.V.; Drokin, A.I.; D501-crov, V.D.; Sudlkov, N.I.; Sinegubov,V.1
0
TITLE: Domain structure in Xerrites and its dynamics in varying and rotating mag-
notic fields 6ieport, Symposium on Ferromagnetism and Ferroelectricity held in Le-
nin.-rad 30 May to 5 Juno 1969
SOURCE: AN SSSR: Izvestiya. Seriya fizicheskaya, v.28, no.3. 1964, 545-352
TOPIC TAGS: ferrite, domain structure, ferrite domain structure, garnet ferrite,
garnet ferrite domain structure, spinel ferrite, spinel ferrite domain structure,
hexagonal ferrite domain structure, double domain structure, domain wall fino'struc-
turo
ABSTRACT: The domain structure of a number of ferrite single crystals having the
garnet, spinel or hexagonal structure was investigated. The powder method of VI.S.
Elmore (Phys.Rov.51,10,1092, 1938) was employed to reveal the domains. The polarity
of the domain boundaries was determined with the aid of the polar Kerr effect, em-
ploying a previously described technique (V.D.Dy*lgerov and A.I.Drokin, Kristallo-
gratiya,5,6,945,1960); A.I.Drokin, V.D.Dy*lgerov and B.V.Beznosikov, Ibid.9,3,465,
Card 1/3
ACCESSION NR: AP4023405
1962). The Yb, 11o, Er and Gd garnet ferritas were obtained as single crystals from
melts. Lead hexaferrite was also prepared in this way. Crystals of Co-Fe, VM-Fe and
Mg-Mn ferrites with the spinal structure were grown in an oxy-hydrogen flame.
Spheres of 4 to 8 mm diameter were obtained. These war annealed above the Curie
point and oriented in a magnetic field. The planes to be investigated were ground
flat, polished and treated with hot sulfuric acid to destroy surface mosaic. Lead
hexagerrite was found to have a domain structure similar to that of cobalt. The fer-
rites with the garnet structure had very complex domain structures, for which it
does not seem possible to construct a model. "Stringy" walls, double banded walls,
and curved walls were observed in different materials. The curved domain walls of
Cadolinium ferrito garnet would shift under the Influence of an applied magnetic
field. The domain structure of the spinal farrites was somewhat less complex. The
presence of double domain structure was established. Successive walls would have
opposite polarity, and in the presence of a gradually increasing magnetic field al-
ternate walls would first disappear, the ramaining walls disappearing only when the
field became stronger. Sometimes a single domain wall would separate Into two under
U
the influence of a Yield; in such a cas'e the two new walls would have the same po-
larity as the old, thus interrupting the regular alternation of polarity. Wide do-
Card 2/3
ACCESSION NR; AP4023405
nain walls were observed in which a Tine structure could be perceived. Such complex
vialls exhibited alternations of polarity, as though they wore composed of several
walls having opposite polarities. It is suggested that the double domain structure
of forrites may be due to the interaction between the two magnetic sublattices,
each striving to establish its own domain pattern. Orig.art.has: 5 figures.
ASSOCIATION: Institut fiziki Sibirskogo otdclonlya Akadomii nauk SSSR (Institute of
Physics, Siberian Division.. Academy of Sciences, SSSR)
SUMMED: 00 DATE ACQ: lOAprG4 ENCL: 00
SUB CODE: PH
Cand 3/3
HR REF SOV; 014
OMMR- 010
L 5o962-65 EWT(I)/EWT(m)/L%T(J)/T/EWP(t)/EEC(b)-2/EWF(b) Fi-4 IJF(c) JD/GG
ACCESSION MR: AP13011443 UR/0048/65/029/004/0617/0619
I.; Kazulln,V.A.; Turpanov,I.A.
AUTHOR: Savchenko, M. K.; Sin!jubov, V 34
:TITLEt The Bloch wall considered as a th.19
_A~ ~e I/Weport, Second All-Union
�ym~ os-tum on the Physics of Thin Ferromagnetic Films held 1!!~~--15july
J964/
i I
iSOURCE: AN SSSR. Izvestiya. Seriya fizicheskaya, v. 29, no. 4, 1965, 617-619
TOPIC TAGS: fgrromagnetic thin film ( domain structure
L
.ABSTRACT: It has long been known that individual Bloch walls may consist of
.sections of different polarity. Recently a theoretical explanation of the observed
;indications of varying polarity of wall sections has been advanced by S. Shtrikman
band D.Treves (J. Appl. Phys., 31, Suppl. 147, 1960). The calculations of these
i
,authors are briefly reviewed. The experimental part of the present study consisted
lof observation of domain walls by moans of the scanning apparatus developed by the
authors and used earlier for recording the distribution of magnetization across
Idomain walls (M.K.Savehenko and V.X.Sinegubovt Zhur. eksp. L toore fts., 44t 781,
11963)9 Tbe equipment :is based an use of the polar Kerr effect, and lacorparates a
Card
L 50962-65
ACCESSION MR: AP5011443
:narrow alit under which the specimen is slowly displaced. The results of the
observations are summarized in schematic form in the figure (Enclosure 01). -The
intervals of wall polarity (T in the figure) were fourA to 1xi very nearly identical
along, a given wall, in some crystals T equalled 40 to 42 microns. As cowpred with
the results of Shtrikman and Treves, the observed domain width proved to I)e about
half the predicted value, which may be taken as reasonably good agreement in view
of the fact that the calculations were performed for uniaxial crystals, w1lereas the
observed silicon iron was, as usual, triaxial. The conclusion is that regular
domain structure also obtains in the Bloch walls themselves; accordingly, a Bloch
.wall may be regarded as a distinctive type of thin film. Orig. art. has: 2
!formulas and 4 figures.
ASSOCIATION: Institut fiziki Sibirskogo otdeleniya Akadenii nauk SSSR (PhX!Lcs___
lInstitute, Siberian Division, Acad2!M of Sciences, SSSR); Krasnoyarakiy gosudarst-
,vennyy pedagogicheakiy Institut (Krann6yarsk State PedaMical Institute)
ISUBUITTED- 00 ENCL: 01 SUB Cool[: Nut 9C
~NR.REF SOV: 002 0=Rt 002
_Card,__2/3
L 50962-65
ACCESSION NR.- AP5011443 ZNCL40SURS: 01
4 4
4 4 4 4
4 4
Structure of doomin walls In different statess
a - after annealing, b In a field, o - after
removal of the field, d after demgnetlzation
by an alternating field of diminishing amplitudei,
~CarcL-3/3
L 8~48-66 EWT(l) IJP(C)
ACC NR: APS024686
AUTHOR: Drokin,
Vq 5-
ORG: Insti
Siberian De
SOURCE COLE: UW0056AS/049/003/0713/0719
1
A. I.; Sinegubovt V. 1.
fiziki Sibirskogo otdeleniya Akademii nauk SSSR) Institu-. I
of the Academy of-�SjMgg�_MR YI/ 1 ;5 -
TITLE: Investigation of the boundary layers between domains in some ferrites with
spinel structure
SOURCE: Zhuwnal eksperimentallnoy i teoretiches1coy fiziki, v. 49, no, 3, 19659 713-
719
ZI I t) Q
TOPIC TAGS: ferrite, magnetic domain boundary, mametic domain stnictm Kerr
effect, magwtization, metal heat treatment, manganese containing alloy, cobalt
ccnt&uung alloy# nickel containing alloyg crystal lattice paremeter
ABSTRAM This is a continuation of an earlier investigation of domain boundaries
in ferTites (Izv. AN SSSR ser. fiz. v. 28, 5450 1964), and deal with the domain
boundaries in single crystals of iricn-manganesej iron-cobalt, and iron-nickel fer-
rites, and with the influence of heat treatment on the changes in the boundary
layers between domains. The single crystals were gr-own by the Verneuil mathod and
Card 1/3
L 8548-66
ACC NR APS024686
their properties established by chemical and x-ray diffraction analysis. The in-
vestigation procedure, which is based on the Kerr effect, is described in detail.
A study was made of the width of domain boundariesq their polarity$ the riagnetization
distribution in them, and the influence of heat treatment on the width of the domain
boundaries. Plorts are given of the. distribution of magnetization in the boundaries
of 1800 and 710 neighborhoods. The results show that in the initial sta:-,e the
boundary domain width lies within 2.8-4.2 in iron-n-enganese fen-ite, within 0.25-
0.35 in iron-cobalt fervite, and within 8.9-9.5 for 1800 boundaries aad within
3.5-4.0 for the 710 boundaries in iron-nickel ferrite. When there is a change in
the structure of the iron-manganese ferrite, a double domain system is observed, with
boundaries exhib:kting asynnetric magnetization distribution. 7he magnetization dis-
tributicn is uniform in the 1800 boundaries in the irion-cobalt and iron-nickel fer-
rites. In the iron-nickel ferrite the magnetization distribution is as)mmtric in
the 710 boundaries, The boundary polarity is rmd= and may vary even within the
same boundary iJ, the latter is split by obstacles. In ferrites sensitivs to heat
treatment (ircn -cobalt and iron-nickel) the boundary decreases after heat treatment
the absolute values of the first magnetocrystalline anisotropy constants increaseq
-and the lattioe paremeters decrease only slightly. These changes agrw with Neels
theory. Orig. art. has: 5 figures and 2 formulas.
Card 2/3
I
L 8548-66
ACC NR: APS024686
SUB COEE 3 SS 9 uV
A
jw
Card 3/3
SUBM DAM llFeb65/ OFdG MIN 010/ 07H JEF: 005
6
SINEGUBOV,Yu.
-,
Development of all-purpose automotive transport In the White Rus-
sian S.S.R. Avt.transp. 33 no-5:5-6 My '55. (MIRA 8:8)
(White Russia--Transportation. Automotive)
SINIGUBOV, Yu.
New tariffs for automotive freight transportation Inside the
U.S.S.R. Avt. transp. 37 no.5:31-33 NY '59. (MIRA 12:8)
(Transportation, Automotive--Rates)
SINEGUBOV, Yu.
flow organization of automotive transportation unItn. Avt.tranflp.
18 no.1:31-32 Ja 160. (MIRA 13:5)
(Transportation, Automotive)
KITAYKVv A.; SINEGUBOV9 Yu.
New standards for Pallets. Ayt.transP. 39 no.2914,-17 7 161.
(NDA 14:3)
(Unitized d" systems-Equipment and supplies)
I.i
SIIZGUBOVJ W.
Regulationc for transportation rates should be specified.
Avt,trazujp. 40 n0-5:38 MY 1,621. (HUIA 15:5)
(Transportation;. Automotive-Pates)
PAVLOVICHEV, MikhRil Stepanovich; SINEGUBO , Yulian Konstantinovich;
SVIRNOV, O.S., red.7 GIEW=VA, Ye.N.,-..tekhn. red.
(Automotive transportation rates in the U.S.S.R.] Tarify
na av-tomobillnom transporte SSSR. Moskva, Avtotransizdat,
1963. 215 p. (MIRA 16:6)
(Transportation, Automotive--Rates)
w0
Antoninp Tvannvna
(e!.~stotonoretriyi) of tht- 'uestion of Early Diagnostics of Glaucoma
Diss-rt,ition for Cnnrlidite of a IAldical Science defy
- j ree. Chair of Eye
Disenses (he.:d, Prof. I.A. Belyaye--v) Siratov Xeflic! -1 Institute, 1941-
j-DiEGUB9VA) L. S.
USSR/Electricity - Dielectrics
Dec 51
IlEffect of Displacing Field on Magnitude of Dielectric Permeability and Dielectric Loses
in BaT'031" Ye. V. Sinyakov, Ye. A. Stafaychuk, L. S. Sinegubova, Dnepropetrcvsk State U
IIZhur Eksper i Teoret Fiz" Vol XXI,, No 12) PP 1396-1402
Study of thermal behavior of dielec permeability and losses of BaT'03 under effect of
disl' -ing elec field showed shift of Curie point toward higher temp. Found sharp drop
of t-..Lgent of angle of dielee losses and smoothing of its characteristic max under super-
position of strong displacing field. Observed distortion of hysteresis loop under dis-
placing field effect. Submitted 2? Jan 51.
198T13
CZECHOSLOVAKIA
SEDLACEK, J., Z.EJSE1(L_ K. 31N~Z-J;_ Chair of Pathological
Physiology, Chair 67f C~_e'mistry,Chair of Physiology, Medical
Faculty, Charles Unliversity (Katedra Patologicke Pysiologie,
Katedra Chemie, Katedra Fysiologie Lek. Pak. IKU), Hradec Kralove*
"The Influence of Diphosgene and of Anhydrides of N-Carboxy-
amino Acids on Breathing of Mitochondrias."
Prague, Ceskoslovenska Fysioloaie,Vol 15, 11o 2, Fab 66, pp 75-76
Abstract: The influence of diphosgens and of anhydrides.of
N-carb6l-cyamino acids on the activity of succinate oxydase of
mitochondrias of isolated rat liver was investigated. An addit-
ion of 0.137 mg of diphongene in 0,015 ml of 96A ethanol added
to 3 ml of a suspension of isolated mitochondria st9pped their
breathing. Similar addition of 0,1 mg of N-oarboxyanhydrid* of
vanillin had no influence on breathing. 2 Czech, I East
German reference. Submitted at '116 Days of Physiology" at
X08100P 27 Sept 65e
1/1
2069.
UC&
za amw..
Al n:' Abstr. No. 23. 60" for
ddert"ini 1 (0-04 to I ceop in a am
Si (2-6 to 5 by
rn Of a 59titczelot scinfivailtuandlin"lumarc a
steelimsco pa are desczibe& G. S. Sism
SIMWIiU, H*
Forfectirx, production. Sov. prcfgoiuzjr 7 no.17:4 S 159.
(MIRA 12: 11)
1.Pradoodn"ell tsekhovogo komiteta profeoyuza Ki-evskogo regene-
ratorno-r-zinovogo zavoda, g. Kiyev.
(Kiev--Rubber, Reclaimed)
Sln4'NIK, V.K.; LO!ENKO, A.N.
High-power ferrite-transistorized decoder with a short-circuited
turn for 512 outputs. Avtom.i prib. no.4:38-41 O-D 162.
(MIRA 16:1)
1. Lisichanskiy filial Instituta avtomatiki Luganskogo soveta
narodnogo khozyaystva.
(Electronic analog computers)
U5.')R/Elt,~ctricity - Ij,otor5, Indiletion
Sep 51
"Concerning ~;. I. 13hturman's Article 'Open S,wirrel Cages in S-:uirrel-Cages Inducti,--.
1-11otors',11 N. K. Arkhangel Iskiy, A. A. Minin, K. A. Chefranov, Engineer.-s, "Glavenergoneft'n;
G. V. Molchanov) Engr "Griproneftemash"
"Elektrichestvoll No 9, pp 81,82
The 1st aroup, from "Glavenergonefti," state that Shturman's method is c-uite unsatisfactory
and cite~'expts conducted by Sinellnikov and Zemlvanyy in the All-Union hec Eng Inst, in
which slotting of the end rings reduced the efficiency of the motors tested bv 4.5-5% and
the power factor by 17-19%, while increasing the starting torque by only 5-36%. Molchanov
.gives examples of succe3rful application of Shturman'3 method.
PA 196T55
SM7,1NIKOV, A,
7
Aerial prnsppctore of the earth's interior. Znan. oil& 31 no.8;
14-16 Ag 156. (MLRA qslO)
(Aeronautics in geology) (Radioactive substances)
SIMALINIKOV, A. (Leningrad)
WMVAMW~
No.1 automobile radio station. 7-dorov's 2 no.9:29 3 156. (MIJA 9:10)
(MOSCOW--AKBUIANGS SXRVIC31)
(RADIO-INSTALIATION IN AUTOKOBILES)
STALIMAKOVA, V.A., SINKLINIKOV, A.M.
Some features of water metabolism in desert rodents. Doki.An
Tadzh. SSR 2 no. 5:43-48 159. (MIRA 13:12)
1. Inetitut zoologii i parazitologii AN Tadzhikskoy SSR.
PredstAvleno chlenom-korrespondentom AN Tadzhikokoy SSR M.N.
Harzikulovym.
(Rodentia) (Desert bauna) (Water in the body)
KORSUNSKIY, M.1.. drec~r Fizi~c~-matematicheskikh nauk, professor; LAGUNOV, A.S.,
kandidat tekhn-lchaskikh nauk; BAYVJ9L'. L.P., kandidat tekhnicheskikh
nauk; SINEUNIKOV, A.N., kandidat tekhnichaskikh nauk.
Indicator for registering changes In clearances in steam turbines.
linergomashinoBtroento 3 no.5:26 My '57. (KIM IOW
(Steam turbines)
S/115/60/000/05/25/034
BO07/BO11
AUTHORS: Korsunskiy, M. I*, Lagunov, A. S., Bayvell. L. P.,
Sinellnikov. A. N.
TITLE: Use of -Radioactive Isotopes for the Measurement of Vapor
Moistness
PERIODICAL: Izmeritellnaya tekhnika, 1960, No. 5, PP 50-52
TEXT: A method of measuring vapor moistness in offered here. It bases
on the determination of vapor density after absorption of P-particles.
A radioactive sulfur isotope was used for the purpose. Investigations
were first conducted in the laboratory. Source activity and counter
were selected, the optimum distance between isotope and counter as well
as the absorption coefficient were determined. The experimental setup
shown in Fig. I served for the Investigations. The setup in briefly
described along with the investigation course. An aluminum vessel pre-
pared for the purpose and shown in Fig. 2 was used as source. Radiometer
5 -2 (B-2Vserved as recording device. To determine the vapor density
it was-iii"cessary to determine the mass absorption coefficient of
Card 113
Use of Radioactive Isotopes for the S/115/60/000/05/25/034
Measurement of Vapor Moistness B007/BO11
electrons for which no data were found in publications. The mass absorp-
tion coefficient g' was first determined in the experimental way in the
laboratory as the tangent of the inclination angle of curve
1n f(qd). I is the intensity of the electron beam before passing
0
0
through the material layer, and I the intensity after passing through
a layer of a thickness d. q is the Absorber density. In this way,
A' = 197 cm 2/g was found for overheated vapor. The vapor density Q was
then determined from formula (4)- With a view to testing the method
described here, the system shown in Fig. 3 was assembled at the C_
Kharlkovskiy turbinnyy zavod (Kharlkov Turbine Works). The section
through the measured portion is shown in the same figure and described.
In this test, g' - 200 cm2/g was found for overheated vapor which fits
the vplue obtained in the laboratory. The moistness degree y was determin-
ed from the g' and Q values obtained. It is pointed out in conclusion
that the investigations carried out have proven the possibility of
measuring the mean moistness in a vapor flow without drawing off,
Card 2/3
Use of Radioactive Isotopes for the S/115J60/000/05/25/034
Measurement of Vapor Moistness B007/B011
irrespective of the state and the drop size of the moistness contained
in the vapor. There are 3 figures and 1 table.
C
Card 3/3
SINELINIKOVp A.N. (Moskva)
Traveler with a camera; Z.Z. VUogradovto 80th birthday Priroda
51 no.12:114 D '62* NIRA l5tl2)
(glinogradovs, Zakhar Zakh&rovichv 1882-)
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Khlv~ Mr. J. Man. Moncoet), (5), Tho reactlm :f dlfff,~rv,-11,,
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o0kii MCV tho pjrolysl 9 of q!"a13 ter' at 0jW to I 1000C. it was cetabliqhod
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coiw; tllzc ve r!aot Ivi ty of cmerber colco doug nor. dopcond mch on tro
of Its subsequent tmat,,.-ont; that differont shale cokes havo selmllar
reactivitlevi, lying boVevn those of coal cokO and peat coke. In crder to
dimini-h tbo c!Tbcn d1oxic'-i ccntQnt of V-0 gas produced, ow is raccmnded
to me the gan Itsolf fcr ?,oriling tho C!Ko in ovans filth botrtv. cutlets far
tM :3taat,,?,gi!j ritittro, avI not gtean an Ig u.-tal, slive at oooling ".ono
tarq),.%raWYvs ar=4 7500C Vii) w,'bon diaxida fcrrco by diescelatIm or
aaxbcnates camot Lo redwid to carbon dioxide at all ccz*lat~aly. W11r--n tim
ovens Kave top outlots fw tN Ca~, stonit cooling should InC41ca3a 1143 y1old of
viater gas Ur~OuE~h furtbor of the coke taking place at high
temratums.
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f 'h( S!tdu C"ie. v1'r clarifficati;'11 '31 this rjuc~ii'~n
~rdtit L pc cfrj~, iu~:d I,), jp~
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11,6 1., rvk-.i Mira the! g-as throuih
-..mi T."r'-Oam W!~Ilc' nh~n with (:~'Le r-r-A
I,., a ~ I ~r'k!* I ;--is ( Lm 1 501"01 tLe H.~'rea-a:IL3 Im IrL-
'I with thl~ Mintfal part of th~: c(,kr. T hia
applic- to the Ca and Mg oxidu nrid ab) to their
%';ilh thc-. tr-olp. One HTS cortrrlt Or-
flud at fp,0' 6 oz;'Y 4-,5':C, N,
SINELINIKOV,A.S.
Ignition limits of shRle gas. Trudy VNIIPS no.3:120-124 '55-
(MLRA 8:12)
(Bnltic Sea region--Oil shales) (Hydroenrbons)
SINEWNIKOV,A.S.
Processing Kashpir shale In gas generators of the Kohtla-Jarve
plant. Trudy VNIIPS no.3:209-218 155. (KLRA 8:12)
(Baltic Son region--Oil shales) (Hydrocarbons)
3MMOMIN, B.S.; SINFLINIKOV, A.S.
Shale-gas genmrators of higher prortuctive capacitr. Trudy VI,'1IIIS
no.4:63-R4 '55. (MIU 13:4)
(Oil shales) (Gas producers)
moo
DiMIFOGITIC11 (F V'C1'iTfc!j,' E Fr,.ql U
i!PZTATURE CAPICT"ATICIf CF, V;,%-L!r3. D~,=Lrln, Z~,S, 'my"
SImAsnihoy, A,3, ilv~f-,,,pu*.. mwch.-Issled Ir:;t:. Pcrcrab. 031".n.
1955, (10, 92--Sr9; ct',Mr- In RPG "h-
OG), 51359). A 15 r~,i tubil, I r1
lcn~' had 3CO mi of IC5 lmt~tli flll~ul vArAl I;Cf) Arh Coke In
N'Ith Ote LL.1-, of (-1 IrA
.3 t, .5 ~,17.
tl~.e cr)::o ccn:;tuit ar 8 to D~ :;t:c owl U,.c tm, ;cmrullu in che
P~Toly:;13 -.tne frui 7CUI to ]CUPC the Yield -,f u:s Ir-,'rc::Ocd n*aj
0.36 Cu O,CZ cux/xr, of ~;halc, rut tho ccrccncm-rIcn of ~:~iu=atc~i and
mratua-dred hydrccavb,~m; M It, jccrc-a:;cd, aul z~,!2 ca-2,7,rIfIc v,:luc of
the Gos. IIGVICVC'r D~IC t0ta-' 1101d Of bMt for a ;flvcn qi.,3sitlty of 5~jalo
Increased. Incre3slim uic ccn-,~-.cr t1,.1(3 (it ccj-i43L.3jjr, t.,.,pc~jmtjirc ~nvc the nme
reoults. VarlatiLn In C,.,rpo3ItIvn and voluw of W frcr,, lfw tmprrature
carbonisatIm ~urlnr pyroLysln v-,- studlc