YISMVSKIY, Y.M.; MABM, S.A.; SPIVAXOT, V.P.
- - -- -: - .
Pamping out a flooded IsTel in the Xirgalissay ndne. Gor. sInw,
to.8t63-65 Ag 157. (Kin 1019)
1. Kirgalissayakoys shokhtontryupravloniye.
(Kirgalimmay-Nining enginseringy
(mine pumps)
r(M PW lip(e)
0 - ~,A 3 1 A I
48 SOURCE CODE: UR 0191166-t-00-070-07/OOYj-fW2-5---~
AUTHOR: Zhinkinal L, Ne; Vishnevskiy, F. N.; ZhLnkin, D. Ys.;
Zubkov, I. A. J7
ORG3 none
TITLE: Reaction of butyl orthotitanatLith phenyl methylphosphono-
chloridate t phosphorus oxychloride
SOURCEt Plasticheskiye massy, no. 7, 19669 23-25
TOPIC TAGSt butyl orthotitanate, phenyl mothylphosphonochloridatel
phosphorus oxychloride, polyorganophosphorustitanoxane 7/7W,4t9r-F,
P,#eAJL1X- 00,;-)j-0UJD I Adl-yMelE NrRC/0rG/,ej7l a"1,dM,ej.4- oe~0C7-,01V
ABSTRAM A study has been made of the reaction of butyl orthotitanata
(I) with phenyl methylphosphonoc hloridate (II) an with phosphorus
oxychloride (III). It up to 90C, I and Il taken in a 1/3 ratio react
as;follows:
*n(OC,H,), + 3CH3PO(OCgHjCl
C13lj(OC4H#) + 3CH3P0(CW:41l#)(0C6HJ
At above 100C the reaction products undergo condensatj'on to form a
polymer with a titanoxaneT ackbone. The presumed structure of the
Card I / 2 UDCj 67 B. 85+6713. 8 68. 24
1 _0620( - :
ACC NR, P 6 o'! 17-4-6-
polymer, Los
0
P-OcIffs
_T1__O_
rji'~_OC.H.
0 jx
A polymer with a high molecular weight is isolated by dissolving the
reaction mixture in acetone and precipitating with water. I and III
react in a similar manner; at higher reaction temperatures (170-180C)
a cross-linked phosphorus-contaLning polyorganotitanoxane is formed.
The polymer contains l.titanLum atom per phosphorus atom, and I
butoxy group per 3 titanium atoms@ The synthesized polymers withstand
temperatures of 190-200C. Orig. art. hass 3 figures.
SUB CODEs 079 11/ 1# SUBH DATE: none/ ORIG REFs 007/ OTH REFs 002
Card 2 / 2
VISIDIMKI'Y F.He
---
Manufp-,ture of rubberized hair frm the wastes of bristle and
brush raw materialso Kozho-obuys promo 6 nool2t25-26 D 164
(MIRA IW)
VISM3VITSKIT, G.D., dote., kand. tekhn. nauk
Introduction to the technical theor7 of deformations caused by
swelling and shrinkage of concrete. Sbor, nauch.trudoy IJSI no.26:
181-214 157. (MIRA 12:1)
(Concrete--Testing)
VISUM.SKIY, G. I.
Sinle dye Bpriqeroo Cbm.takh.opyt. CHWI n0.26:36-36 156.
(MIRA 11:11)
(Dyes nnd dyeing--Leather)
VISHMSKIY, G.I.
Couve7ors with continuous cleaning of screense 01motekboopyto
CHWI n0.26:42-44(,1560 (MMA 11:11)
onveying machinery)
", , ": i / - " -, -1 11 , I
/_11 I
t t - -Ir" rf , 1~_r
VISHNXVSKIT Glye
%all-size test rod for controlling central heating 879tsms. Tod. i
um tekh, m,1:26-30 A '58. (XIRA 11:1)
(Hot-water heating--RegulatoreY
VlSHWMSKIT-~- Met . VISHNEVSKIT, I.Ye.
Blectric sorption bygrometer. Tod,i san.tekb. no.7:16-20
Je 160. OGU 13:7)
(Hygrometry)
20490
S/191/61/000/003/015/015
B124/B203
LUTHORSt Panshin, B. I., Vishnevskiy G. Ye.
TITLEs Strength of glass Textolite in unilateral heating
PERIODICALs Plasticheskiye massy, no. 3, 1961, 71-73
TEM The strength of the unilaterally heated plastic can be
approximately calculated from the temperature gradient in the material
cross section and from the diagrams "stress - deformation" for different
temperatures; this procedure is, however, rather complicated and not
always dependable. Inaccurate results are obtained, particularly when
determining the strength of material heated on its surface to high
temperatures, which is due to the fact that the same zones of the material
in unilateral heating are subjected to thermal effects differing in in-
tensity and duration. Therefore, the experimental determination of the
strength of plastics used for unilateral heating to high temperatures is
particularly important. Fig. 1 shows a diagram of the apparatus used. A
flat 1.5-kv electric furnacev open on one side, with a 6-m= nichrome
heating coil working at 16 v and 80 a, is used for heating. The tempera-
Card 1/8
20490
S/I 9 V611000100310151015
Strength of glass Textolite ... B124/B203
ture of the heating element is automatically contr 81 led with an VD-01
(EPV-01) electron regulator. At 400, 600, and 800 C, the heat flows are
10,000, 32,000, and 80,000 kcal/m2.hr, respectively. An ordinary small
integral calorimeter of the radiation type is used to measure the heat
flows (Ref. 51 Teploenergetika no. 12 (1958)). The mechanical properties
of the plastic are determined either under a load varying with time
(Fig.2) or under constant load. The authors examined glass Textolites of
the types -14 (FN), r-K-91, (SK-9F), and KACT-.b (KAST-V) developed by
B. A. Kiselev and Ya. D. Avrasin and co-workers. The greatest drop in
strength corresponds to the unsteady period of heating. The binder of
glass Textolites FN and SK-9F starts burning at a surface temperature of
about 7000C. Since the material of the heated zone is separated into
layers, it is necessary to examine, besides the tensile strength, also the
bending and compressive strength in the plane of the foil. This is done
with an apparatus shown in Fig. 4. Fig. 5 shows data of tensile and com-
pressive strength of KAST-V glass Textolite, 2 mm thick, in the plane of
the foil in three principal directions. There are 5 figures and
5 references: 4 Soviet-bloc.
Card 2/8
20490
S/191,/61/000/003/015/015
Strength of gla
Card 3/8
zwo
20490
S11911611000100310151015
Strength of glass Textolite ... B120203
Le end to Pi 1 Basic circuit diagram of the test device. (1) Specimen,
(21 clampel & ;1ectric furnace for unilateral radiation heating of
specimens, (4) and 5) voltage regulators of the heater, (6) magnetic
starter, M-load, 8) lever*of the loading device, (9) device for
automatic loading, N) automatic electronic regulator of the type EPV-01,
(11) push buttons for nonautomatic switching-on of the heater, (12) thermo-
couple'for measuring and'regulating the heater temperature, (13) thermol
couple at the heated specimen surface, (14) thermocouple at the unheatek
specimen surface, (15) deformation feeler, (16) heat flow meter,
(17) electr?nic 3ffp-og (EPP-og) potentiometers, (18) rubber buffers.
Load, kg/mm time, min.
Card 4/8
Strength of glass Textolite...
Fig. 2. Dynamic conditions for the 40
tensile test with unilateral heating
of FN glass Textolite foil, 3 mm 36
thick
Legendt (1) Temperature of the
heater, (2) temperature of the
heated surface, (3) temperature of
the unheated surface, (4) tensile
to
0
strength at 20 C, (5) breaking point
in heating, (6) - (9) change in stress
at constant velocity of clamps and 0
loading of the specimen after 0, 1, 2,
5 minutes, (a) stress, (b) time, min,
(c) temperature.
Card 5/8
20490
S1191161100010031CI51o15
B124/B203
7-
7
, ! "M
/ "4 r.)
4'.:w;
.
0
2 J);!.
t
a)
Fig. 2
Strength of glass Textolite...
Pig- 4. Device for compressive tests of flat
glass Textolite specimens with unilateral
heating
Legend.-' (1) specimen, (2) guide bar, (3) and
(4) upper and lower clamp, (5) and (6).
centering ball supports, (a) heating.,
Card 6/8
Fig~ 4
20490
S/191/61/000/CiO3/01.5/015
B124/B 203
P -L~u
p,
Strength of glass Textolite....
Fig. 5
k
Card 7/8
20490
S/191J61/000/003/015/015
B124/B203
parmommue
Gwomme 0-
/0 .749 70 0 to 20 J,7
20490
S/191/61/000/003/015/015
Strength of glass Textolite ... B124/B203
Legend to Fig- 5: Tensile and compressive strength of KAST-V glass
Textolite foii, 2 mm thick, with*unilateral heating (heat flow
80,000 kcal/m -hr; temperature of the heater 800 C):. (a) loading along
the warp, loading along the filling, (8) loading at an angle of 450 to
the warp, ~92 temperature conditions during the test, (1) and (2) tvmpera-
ture of the heated and unheated spec amen surfaces. (a) Load, kg/cm~~,
(b) time, seconds, (c) temperature, C, (d) stretching, (e) compression.
PANSHIM, J..I.; VISH-NIEVSEM, O.Ye.
Determination of t~.e deformatAlity of glass textolite in stret&.
testing under conditions of unilateral heatinr. Plast.masEy n!.).10:
55-158 '61. (PIRA 15:1)
(Glass reinforced plastics)
VISHNEVSKIY, G.Ye,; LOZINSKIY, M.G.
Life of the VFT-S and KAST-V glass textolite specimen under t~e
conditions of one-sided heating. Plast.massy no.407-43 '64.
(MIRA 17:4)
-??915-66
EW(e)/SWT(m)/SWP(J)/T/M(m)-6/EWA(I)/EW~(v) ..Ijp(c) jo1ww1jGs1RX1
ACC M. AT6008655 (n) WE SOURCE: DR/0000/65/000/000/0113/0123
M. G,, (Moscow); Vishnevskiy. G. Ye. (Moscow); Pavlov. A. 1,
AUTHORSt Lozinakly
(Moscow)
ORG: none
TITLE: A study of the temperature and time dependqnce of the strength and
durability of sheet glass plastics AG_W~VM ZF-S~'under tension, compression, and
shear In conditions of programmed one-sided heatiM.
X3
SOURCE:
temperaturakh, 3d. Termoprechnost" materialov i konstruktsionnykh e1
(Thermal strength of materials and construction elements); materialy
soveshchaniya. Kiev, Naukova dumka, 1965, 113-123
TOM TAGS: glass plastic, glass product, svnthetic material, thermal property,
heat stability/ IMASH-11 inaterial testing machine, AG-AS glass plastic, EF-S
glass plastic .9 /0
ABSTRACT: The authors describe the IMASH-11 machine which was designrid and
developed at the Moscow Institute of Machine Science (Inatitut mashinovedeniya)
for the purpose of T'determining strength and deformation properties of sheet
Card 1 1/2
L 2297c,-66
ACC NR: AT6008655
plastic specimens. The machine is designed for shear, tension, and compression
testing In conditions of automatic programmed one-sided heating of specimens up
to 1300K with a temperature increase rate of up to 500 per second in air and in
an enclosed gas medium. A movable electric oven open on one side is used for
maintaining the programmed temperature. Regulation of the specimen temperature
is effected by automatically varying the distance between the oven and the spec-
imen surface. The construction and the methods of conducting testswith the
IMASh-11 machine are described by M. G. Lozinskiy and G. Ye. Vishnevskiy
(Ustroystvo dlya izucheniya zakonomernostey deformatsii I razrusheniya obratsov,
ByulletenO izobrotenly, !963, No. 9). The authors describe the conduct and
reaults of tests performed to measure the variation of the strength of sheet
specimens of glass plastics AG_4S and EF-S with the level of initial constant
stress. Strength and durability characteristics of the materials were measured
in conditions of tension, compression, and shear. The IMASh-11 machine is
shown An a schematic diagram, and a photograph shows the mounting of an RYK-1
camera used in recording shear deflections, Orig. art. has: 4 tables, 6 figures,
and I photograph.
SUB CODE: It/ SUBM DATE: 19Aug65/ ORIG REF: 00'?
Card 212
VISHNEVETSKTL lqpif_Antonovich(Vyshnevetsikyi, I.A.], kand. ekon.
nauk,- DEMIDYUK, V.F., red.[Demydiuk, V.F.J, red.; KOPMOU,
H.K., tekhn. red.
[The main economic tasks of the U.S.S.R.)Holovne ekonomichne
zavdannin SRSR. Kyiv, Derzhpolitvydav URSR, 1962. 50 P.
(MIRA 16:3)
(Russia-Economic policy)
- - I Rf B VS J
, VIS (Leningrad)
Uniform technology increases the mutual responsibility. Zhel. dor.
traru, P, 47 no.9:88--89 S 165. (MIRA 18~-q)
1. Nachallnik otdola podlv.-ezdnykh putey Tranaportnago upravlenlya
Leningradskogo soveta narodnogo khozyuystva.
VIS11.'.E1.'~KIYj_I.-aak Davidovich; 1A-UT, Andrey Alokntndrovichj UNLISHCHUK,
Potr Kondratlyevich; CIMMS, Mikhail Yurlyevich; MALAKHOV.
K.U., inzh., retsenzent; FREDE, V.Yu., inzh., red.; V(TROTNIKOVA,
L.F.0 tekJm. red.
(Industrial transportation sections and railroad stationn]Tran-
sportr4i tsekh i stantsiia. Moskvaq Trannzbeldorizdat, 1962.
58 P. (14IRA 15:11)
(Railroads, Induatrial) (Railroade-Froight)
VIASOV, N.I.; ZILIBIRW, A.A.; POVXRXUM, I.D.; SAMOYAL. 8.Y., redaktor;
VISHNIVSKIY, I.F., redaktor izdatel'stva; ANDWXY, S.P., tekhmi-
a a mr-mmir,
(Rapid capital repairing of blast furnaces] Skorostnot kapitalinyi
remont domennoi pachi. KharIkov. Ooo. nauchno-tekhn. izd-vo lit-ry
po chernoi i tevetnoi metallurgii, 1952. 99 P. (KLRA 9:8)
(Blast furnaces)
VLASOV, N.I.; ZILIBKRMAN. A.A.; POVIRENNYT. I.D.; SANCTAL, S.V., rodaktor;k.,
VISMOVSKIT, I.F., redaktor; ANMTNV. S.P., tekhnicheokiy- redaktor
(High-speed major repair work on blast furnaces] Skorostnoi kepitall-
zWi remont aomennoi pechi. KharIkov, Goo. nauchno-tekhn. izd-vo lit-
ry po ohernoi i tovetnoi metallurgit. 1952. 99 p. [Microfilm]
(HLRA 7:9)
(Blast furnaces-14aintenance and repair)
VISHNEVSKIY, 1,1.-. SKRIpI.Kp V.N,
- - -----
Scattering of phonons by cation vacancies in a spimel latt!ce.
Fiz, tvar. tels. 7 no.lOt2925-2939 0 165. (~UFJ- 18,11)
1. Ukrainskly nauchno-issledovatellskiy Institut ogneuporovp
Kharlkov.
67713
0 0
/019 41 0 SOV/126-7-3-9/44
AUTHORS: Goguzin, Ya. Y9. and Vishnevakil, I. I.
X-11"of Metals and Alloys. 5. (lasledoy-
TITLE: Investigation of Cree
aniye kripa metallov i splavov. 5.) Early Stage of Creep
in Plastically Deformed Filaments of Alloy
(Rannyaya stadiya kripa plaatioheaki deformirovannykh
nitey splave. Pb--Bn) lv~
PERIODICAL: Fizika metallov I metallovedeniye, Vol 7, Nr 3, pp 367-
371.JUSSR)
ABSTRACT: The present work was carried out with the aim of accurately
checking the interrelation between the kinetics of healing
of distortions and the kinetics of the initial stage of creep
in three substitutional solid solutions. The object for in-
vestigation was a solution of tin (25 at.%) and lead (75 at~%).
Such a concentration of tin is close to the limiting concen-
tration of the cK-solutio:h at euteetio temperature, and hence
it can be expected (Ref.2) that all effects associated with
the influence of deformation on creep will be shown very
clearly. The same method for making the specimens and
carrying out measurements was used as by Geguzin st alia
Card 1/6 (Ref.2). Two series of experiments were carried out.
67713
SOV/126-7-3-9/44
Investigation of Creep of Metals and Alloys. 5. Early Stage of
Creep In Plastically Deformed Filaments of Pb--Sn Alloy.
The experiments of the first series were carried out -with
the aim of finding the influence of the extent of Initial
distortion of the crystalline lattice of the solid solution
on the kinetics of the early creep stage. The specimen
was first plastically deformed. The experiments were
carried out at a constant heating rate (Ref.3) 70/min).
As can be-seen from Fig.1 tho healing of a portion Of the
distortions taking plaeo on heating causes creep to set in
at higher temperatures and leads to smaller elongations of
the specimen. The specimens were prepared as follows.
Filaments of the alloy, obtained by drawing through a steel
die of 0.3 mm diameter, were thoroughly annealed at 1900C
for two hours, after which they were compressed to different
degrees between polJehed steel plates. Measurements were
carried out on specimens having the shape of strip of
thicknesses: 0.18 rm (Ad = 0.12 mm); 0 .13 mm (Ad = 0. 17
and 0.09 mm ( Ld = 0.21 mm). The elongation was studied,
Card 2/6 both at constant heating rate LL)H = 50/min (Fig.2) and ~~/
67713
SOV/126-7-3-9/44
Investigation of Creep of Metals and Alloys. 5. Early Stage of
Creep in Plastically Deformed Filam nts of Pb--Sn Alloy.
in isothermal treatment at 1800G (Fig.3). All exper It ants
were carried out at a sPecifie load of
Rud = 6.2 kg/cm
In Fig;4 the time dependence of 8L/LoRud during continuous
creep of the specimens with different initial crystal lattice
distortion is shown. Experiments of the second series
were carried out with the aim of studying the kinetics of
creep of specimens having the same lattice distortion, loaded
at different rates. The heating rate was varied within the
limits 0.35 - 350OG/min. In Fig*6 the relationship
AL/LoRud = f(T) of equally deformed specimens on heating
at a constant rate is shown. The phenomena determining
the nature of the curves in Fig.5 can be conveniently
discussed by considering the dependence of the effective
yield strength of the investigated specimens on temperature
at constant heating rate. This relatignship was determined
from curves shown in Fig.5 with the help of the relationship
(Ref.3) &L e
Card 3/6 dT LoRud
67713
SOV/126-7-3-9/44
Investigation of Creep of Metals and Alloys. 5. Early Stage of
Creep in Plastically Deformed Filaments of Pb--Sn Alloy.
i LN L
The value of is found graphically by
dt LoRud
differentiating these curves. The dependence of x on T
Is expressed in the form of graphs 1n x = (P (T) in Fig.6.
As a result of the above investigations the authors have
arrived at the following conclusions:-
(1) The kinetics of creep of a solid so4ition depends
essentially on the degree of distortion0of the crystal
lattice of'the specimen.
(2) The creep of a specimen with distorted lattice under
isothermal experimental conditions is accompanied by
healing of the distortions. In specimens with a given
degree of initial lattioe distortion the healing process
is accomplished the later and the quasi equilibrium
condition setting in is the further removed from equilibrium,
the greater the initial deformation of the specimen.
Card 4/6 K
677"
BOV/12.6-7-3-9/44
vest on g Creet of Metals and Alloys. 5. Early Stage of
Rreep 1#11ast cally eformed Filaments of Pb--Sn Alloy.
c
(3) Experiments in which creep of specimens with a distorted
crystal lattio% at various heating rates, wRa investigated
have shown that the kinetics of distortion-removal from a
so1id solution is qualitatively analogous to the one observed
earlier in distorted metallic powders (Ref.3, 4). The
particular characteristic of this kinetiosconsiats in the
fact that the effective kinetic coefficient (in this case
the effective coefficient of yield strength) is not a
constant function of temperature. The non-constant nature
of the dependence of the effective kinetic coefficient on
temperature may be the result of the fact that the creep of
an alloy is determined by essentially different mechanisms
in various temperature ranges: by a dislocation mechanism
at low temperatures and by a diffusion mechanism in a
temperature range at which healing of dislocated regions in
essentially accomplished.
There are 6 figures and 6 references, of which 4 are Soviet
Card 5/6 and 2 English. tK
67713
""OV11 26-?-3-0/W~
Investigation of Creep of Metals and Alloys. 5. Early Stage of
Creep in Plastically Deformed-Filements of Pb--Sn Alloy.
ASSOCIATION: Khartkovskiy gosudarstvennyy universitet im. A. M.
Gortkogo, (Kharklov State University imeni A. M. Gor'kiy)
SUBMITTED: June 19, 1957.
Caid 6/6
VISHNEVSKlY, I.I.; SKRIFAK, V.N.
Temperature hysteresi3 of heat conduction In the breakdo-.n of so'&Jd
solutions. Dokl. AN SrM 163 no.2s418-421 Jl 165. (MA 18:7)
1. Ukrainskiy nauchno-isaledovatellskiy institut ogneuporov. Sub-
mitted December 19, 1964.
SUKHAREVSKIY, B. Ya,t la-PIRR~VSKIY,, 1. 1.
Polymorphous transformatton kinetics of ZrO
2. DoILL JS SSSR
147 no./+:SM-885 D 062. (MM 3A s 1)
1, Ukrainskiy nauehno-iosledovatelinkiy lnstitt~6ogneuporov,
Predstavlano akademikom N. V. Belovy a
(Zirconium oxide)
9w-( 'I.' ,
VISHNEVSKIY, I.I.; G-WRISIT, A.M.; SUKHAREVSKa, B.Ytt.
A
Study of the stabilization and destabilization processes
of the cubic modification ZrO2. Rent. min. syr. no-2:3-4
162, (MIRA 16:11)
1. Ukrainskiy nauchno-issiedovateliskiy institut ogneuporov.
VISHNEVSKIY, I.I.; SKRIPAK, V.N.
*-
Heat conductivity of graphite-containing refractories.
Ogneupory 29 no. 5:227-231 !64. (MIRA 17s?)
1. Ukrainskiy nauchno-isaledovatellskiy institut ogneuporov.
FRENKELI, A.S.; VISHNEVSKIY, I.I.; SKRIPAK, V.N.
Temperature distribution in the crown masonz7 of an open-hearth
furnace. Tnzh. - fiz. zhur. 7 no.12:32-38 D 164
(MIRA 1W)
1,, Institut ogneuporov, Kharlkov.
VISIMENSKIY, I.!.; SUMARE'VSKIY, B.Yn.
Role of cationic vacancies in the redox processes taking place
in ionic crystals. Dokl. AIN SSSR 160 no-3:642-645 Ja 165.
0,11W, 18:3)
1. Ukrainskiy nauchno-isoledoiatellskiy institut ogneuporov.
Submitted July 6, 1964.
AUTHORS i BhAkhtfn, D.M., Vish2mwaiciy, 1.1. 32-8-18/61
TITLEs of Fireproof Substances
Determin tion of the Thermal
in the Vacuum. (Opredelaniye teploprovodn6sti ogpeuporov v'vakukime)
PERIODICALt Zavodskays Laboratoriya, 1957, Vol.23, Nr 8, pp. 927-929 (USSR)
ABSTRACTt The paper mentions as example*the corresponding apparatus according
to the method by Mo Quarrie (Am.Cera.Soa.) by which the thermal
conductivity of fireproof pure oxides which are given the form of
ellopsoids of revolution is determined in the vacuum. It is said
that the use of such apparatuses is unsuitable for mass research
work due to the complicated form which the samples must have. In
this paper another apparatus is proposed (illustration given) in
which the determination of the thermal conductivity of fireproof
substances is carried out at high temperatures. The construction
of this apparatus is based on the principle of a hollow cylinder
with an absolute measurement of the stationary heat flow. Graphite
and tantalum are ruggested as materials for the performance of the
research in the vacuum, in order to keep a high temperature in the
experiments. Temperature of 16oo-17000C are suitable. (a deacript-
ion of the apparatus and its application is given). Aluminumoxide
and zirconiumdioxide samples of various porosity are here used sam-
ples for experiments. The obtained linear relation yields the poss-
ibility to proceed up to maximum temperatures of the sample inmea-
surements of thermal conductivity. It was found that samples with
Card 1/2 approximately the same porosity yield almost identical results. In-
Determination of the Thermal Conductivity of Fireproof Substances 32-8-18/61
in the 7acuum.
creased porosity reduces the thermal conductivity, but the charac-
ter of the course of temperature of the thermal conductivity coef-
fioient for a given material remains stable.
There are 3 illustrations.
ASSOCILTI.ONt All-thion Scientific Research Institute for Fireproof Substances
(Vaesoyuznyy nauohno-iseledovatel'skiy institut ognsuporov)
AVAILIBLE3 Library of Congress.
Card 2/2
VISHENSKIY., I.I.
Accuracy in the weighing of charge materials. Jzv. vya. ucheb.
zave; cherno mete & no,2:176-184 163. (KiRA 3.6..3)
1. Krivorozhskiy gornorudnyy institut.
(Blast furnacoo-Equip%nt end supplies)
(FGed mechani
. VISHRMKIY I.I.- SUKHAREVSKIY, B.Ya.; GAVRWH, A.M.
Methods of quantitative phase analysis of *C~ on the URS-301
diffractometer. Sborenauch.trud. UNIIO no.5015-323 161*
(Zirconium oxide-Analyaix) (Z rays-DiffractiorL) ('rMA 15112)
I.
VISIffZVSKIY,.,.j,I.; LYULICHEV, A.N.; SUNIMEVSKIY, B.Ya.
Evolution of gases frcm refractory ceramics heated in Mcuo.
Inz.-fiz. zhur. 4 no.12:94-97 D 161. . (MIRA 14sll)
1. InBtitut ogneuporovy Khartkov.
(Refractory materials)
(Vacuum apparatus)
ACCESSION Mt AP4038903
8/0131/64/OW/OD5/0227/0231
AUTHORSi Viahnevskiyj 1, 1,; Skripakp V, No
TITLEs Thermal conductivity of refractories containing graphite
SOURCEt Ogneupory*s no. 59 19640 227-231
.TOPIC TAGSt refractorys graphite refractoryp thermal conductivity, thermal elec-
tromotive force, grain orientatiA, platinorhodium thermocouple,, transformer
LATR 1, stabilizer SN 0,75, potentiometer P 306
ADMACT: An experimental device for testing thermal conductivity of graphite-
containing refractories was constructed bythe U11110 (Ukrainian Scientific Research
Institute of Refractories). Its design., based on the common cylindrical shell
.method, is shown in Fig. 1 on the Enclosures. Provisions are made for testing
cyclindrical'eamples 55 mm in diameter and 180 mm long with a central opening 16 Mm
'in diameter* A spiral heater consisting of RI-U6 wire wound around a corundum
tube was plAced in tho central oponingp insulated by asbostoo and light chanotte,
,Electric power was suppLied by a transformer LkTk-1 from the regulator SH-0.75. A31
.measurements were taken at teiVeratures up to 11-e-00 with platinxim-rhodium. thermo-
Card
'ACCESSION NR# AP4036903
icouples placod as shown in Fig. 2 of the bnolosureas Thermal conductivity
~coafficients were determined at 100-dogree intervals in the toWerature range
700-11OW and were calculated according to the formtlas
QlnLl
,where. Q - radial stream of heat generated per unit of time by a heater section
;with the length A t - temperature difference between the points rl and r2,
iMaximum theoretical error varied from 6-8%, Thermoelectromotive force was measured:
~(acca-racy to 0*001 mv) with a P-306 potentiometer and a mirror galvanometer
(10-7 v/mm). The results showed that thermal coefficients of graphite wore
,different in the directions parallel and perpendicular to the direction of material';
pressing. This was explained by the grain orientation originating in the process
of pressing. To increase the thennal conductivity of a graphite-containing
refractory lining the thermal flux should progress perpendicular to the direction
,of pressing. This would produce an approximate 40% increaae in the conductivity-,
If the thermal 1"lux must proceed parallel to the pressing directionp an atteaq?t
ACCEW1014 NRi APLO38903
should be made to obtain a fine texture of refractory material during its produc,-
tion and thus to increase its The experimental specimens were presented, &-A
some of their indexes were determined by 1, Pe Safronova, Orige arbe hasi 2
tables, 5 figuress and 1 formula.
;:ASSOCIATIONs Ukrainakiy nauchno-iosledovatollskiy institut ogneuporov (Ukrainian
Scientific Research Institute of itefractoriza)
SUBMITTEDt 00
SUB COM MH
DATE AGQi OJun64
NO RV SOV3 009
FMLt 02
OTM 1 002
Card 3/~
*oseq Te40w ZI C&reV -TT
i2upi-n quqw9o-soV9qsv -O-E
es'49-t-vto -'G'4GwoT'4u94od -6
124uTod JQlv9'q -9 fso49Gq99 -L
f TeTJFJ'4vw. 4142TTe.14-r-n jo r.2uTa -9
fuo'pvTr,suT Temmxj,~ -5 !r..TeuTman
9-rd,no*ow.x9q,4 -1 tsooaTd uo-rcuoVm
pus doad -C f 9-rdwies -a f jeq-eoq -T
2'4usTDTJJGOo A,4TATVnpjoo
TvuLw'ql 2ul-mseam aoi GoT.&Ga OT 02Ta
u
ACCESSION URt APLO38903 FUCLOSURS 02
P
A#
Fig. 2. Section of a sample and the distribution or
openings for thermocouple for the determination of
311 and X11 0
P - direction of stress in pressingj dotted 34nes show
orientation in the samples
Card
-visfolsyly, I.I.
Theoretical 3t,jdy co' ~,,Pmsirlon of the w,!i,,,hirF m-ch&riim
of jealm rnr.3. ;hor.nau,,~h.trud. KGRI no. .',1-,186-195 163.
(1411 RA 1717)
VIShNEVSKIY, I.I.; DZYUBENKOI M.I.
I I
Measurement of the thermal conductivitv and thermal d-"Nel-ijity
coefficients of refractories usin g the nonsteady-state method.
Inzh.-fiz. zhur. no.10:45-48 0 f64.
(141RA 17. 11)
1. Institut ogneuporov, KharIkov.
iACCESSION NRi AP4041724 s/ol8lA4/006/007/2168/2174
AUTHORSa Vishnevskiy, 1. 1.; Sukharevskiy, B. Ya.
TITLE: Influence of point defects on the thermal conductivity of
substitutional solid solutions with cation vacancies
SOURCE: Fizika tverdogo tela, v. 6, no. 7, 1964, 2168-2174
iTOPIC TAGS: crystal imperfection, thermal cond' tivity, solid solu-
UP
tion, magnesium oxide, phonon
ABSTRACT: To check on the contribution of vacancies to the scatter-
ing of phonons by point aefects of the crystal lattice, the authors
studied the variation of thethermal conductivity of magnesium
Ioxide in which the Mg2+ were~replaced by Fe2+ and Fe ions and by
cation vacancies through interaction between MgO and (14g, F02+)Fe3+0
The specimen preparation and the test procedure are briefly describeC
The measurements were made ati,-300-800K and at a concentration of the,'
card 114 L
1ACCiSSION NR: AP4041724
!substitutes for the Ng2+ ions 0-22 at. %. The results have shown
,that the presence of cation vacancies leads to a stronger dependence
of the thermal resistivity on the concentration than for substitu-
ttion of cations having the same charge. The results are explained
by taking account of the~role of the vacancies in the expression
for the diameter of scattering of phonons by point defects."'The
~Corrected expression describes the thermal resistivity of solid
!solutions with cation vacancies more correctly than the empirical
formula derived by Aliyev and Dzhangirov (M v* 5, 3338, 1963).
Orig. art. bass 4 figures and IS formulas.
!
1ASSOCIATIONi Nauchno-4soledovatel'skiy institut ognsuporov, Kharlkovi
I I
i(Scientific-Research Institute of Refractories)
'SUBMITTEDs 28Dec63
RMCM 02
SUB CODZa 82 UR INIP SOVI 010 1 009
Card
B/020/62/147/004/024/027
B1O1/B186
AUTHORS: Sukharevskiy, B. Ya. , Vishnevq_k~,
TITLE:- Kinetics of polymorphic conversion ~f Zr02
PERIODICAL: Akademiya nauk SSSR. Doklady, v. 147, no. 4, 1962, 882-1385
TEXT: Based on the research published in Western papers (F.A. Mumpton,
R. Roy, J.Am.Ceram.Soc., 43, 5, 234 (1960)i P. Murray, E.B. Allison,
Trans. Brit. Ceram. Soc., 53, 6# 335 (1954); C.T. Lynch, F.W. Vahidiek,
L.B. Robinson, J.Amer. Ceram. Soc., 44, 3, 147 (1961)) the transition of
monoclinic a-ZrO into tetragonal P-ZrO is discussed, and attempta were
2 2
made to explain the kinetics of this conversibn. A VPC-500 (URS-500
X-ray diffractometer was connected with a heater in such a way as to
allow X-ray analyses of cylindrical samples at 15500C- Preliminary
experiments showed the a-p-transition -to set inzat 11450C. Hence, the
change in X-ray pattern at a conatant temperature.of 1155OG was studied,
and the content of a- and 0-modification in the sample waa determined
from the intensity of lines.j The temperature interval of the
Card 1/3
jS/020/62/147/004/024/027
Kinetics bf polymorphic 'BlOI/B186
a-p-transition %as found tq depend on the preli!Dinary heat treatment o.'
the sample.- In the first isqthermal experimenti the a-P-transition ran
completed within 35 min. '4hg,,n r-epeating the experimental cycle with the
name sample,, complete converAlon could not be reaphed, even after 3 hre.
Finally, a -state of saturation characterized by.st certain amount V (T)
of inconvertible monoclinio: r4odification was re-aohed. The equation
-qt~' 7where C - A(T)/110-'4: M0), the percentage
(C t -COD WCO - C,~ - e CO a
of monoclinic modification 'o1 infinite isothermql,heating, is written
down for the concentration. Its correctness is proved by the experimental
values forming a straight 1 .ine in the coordinate system log(ct - cod
versus t. In the first experiment, C OD was found to be 1-5~6, in the
second one 15%, and in the'third one 20~6. The dssumption that the
temperature interval in the-a-p-transition of ZrO 2 is due to an internal
stress caused by a change in grain size, is comistent -,-iith the hypothesis
of E.B. Allison and I. Taylor,(Trans. Brit. Ceram. Soc.1 54, 11, 677
(1955))- Microscopic examinations showed the grains to grow up to ten
times their'initial size of'O.1 g when subjected to the first heating
Card 2/3
S/020/62/147/004/024/027
Kinetics of polymorphic BIOI/B186
test. Correspondingly, the distinctness of the 221 line of the
a-modification increased when the experiments werg repeated. There are
4 figures and I table.
ASSOCIATIONi Ukrainokiy nauchno-iseledovateltakiy inatitut ogneuporov
(Ukrainian Scientific Research institute of Refractory
Materials)
PRESENTED: July il, 1962, by N.V. Belov, Academician J,/
SUBMITTED: June 7, 1962
Card 3/3,
sUKHAREVSKIYO B-Ya.; VISIat-MUM.- -I-I.; GAVRISH, A.M.
Disintegration of solid solutions in the ZrO CaO system. fJokl.
Ali SSSR 140 no.4:884-887 0 161. (MIFL4 14:9)
1. Predstavleno akademikom N-V-Belovym.
(Zirconium oxide) (Calcium oxide) (Solutions, Solid)
KOVALIV, A.I.; VISHNIVSKIT, I.I.
Dynamic method of determining the elastic moduli of refractory
matorials at high temperatures. Zav.lab. 25 no.9,1109-1111
'59. OGI 13--1)
1. Ukrainskiy nauchno-issledovatellskiy Institut ognouporov.
(Refractory material's--Testing)
(Elasticity)
5/893/61/000/005/004/005
B117/BI86
AUTHORS: ViBhnevskiy, 1. 1., Sukharevskiy, B. Ya., Ga-irish, A. If,
TITLE: Method of quantitative phase analysis applied to ZrO2 using
the diffractometer of type Y PC-501CURS-500
0OURCE: Kharkov. Ukrayins,kyi naukovodoolldchyi inatytut
vohnetryviv. Shornik nauchnykh trudov, no. 5~,~2), 1961,
315-523
TEXT: A special method of quantitative phase analysia of ZrO 2 "Tag
developed lising the diffractometer, type JR-50i (URS-501) which eliminates
the background in x-ray picturer. The annular shape of the standard
specimen mnkea It posoible to keel) 'he illumination of the teat specimen
permanently constaat, even if the crons nection of the primnary bean is
inhomogeneous. The percentage content of monoclinic and cubic phasen is
determined with the aid of a calibrating curve cx . f('x/'stand)' it has
been shown that, Irrespectively of the lattice distortion of 6he specimen
Card 1/2
Method of quantitative phase ...
S/893/61/000/005/004/005
3117/B186
and its grain size (-,-60p), the amount of the monoclinic modification can
be determined from calibration curves for a specimen burnt at 8000C with a
grain size of < 604. Separate calibration curves have to be constructed
for determining the cubic modification according to the stabilizing
addition used. To determine the phase composition of ZrO 2 it is, therefore,
easier to use the diagram for the monoclinic modification. In the
determination of the concentration by the method suggested, the absolute
error is 1.2-5%. There are 5 figures and 2 tables.
Card 2/2
29997
S/170/61/004/012/'007/011
B104/B138
AUTHORSs Vishnevskiy,_L.,._I.-,,Lyulichev, A. ff., Sukharevskiy, B. Ya.
TITLEz Liberation of gases from vacuum-heated refractory ceramics
PERIODICAL: Inzhenerno-fizicheskiy zhurnal, V. 4, no- 12, 1961, 94 - 97
TEXT: The authors tested the corundum V 1 and V 2 (K1 and K2), aluminous
B r and'971 (VG and VL), and aluminosilicate refractories AA 1 and A ~2
(AL1 and AL2 ). The amount of gas liberated was estimated from pressure
variations in the experimental apparatus, which was evacuated prior to theA
experiment. The pressure variations were measured with AM -2 (LM-2) and
AT-2 (LT-2) pressure gauges and with a BMT -1 (VIT-1) vacuum gauge. The
test chamber was a steel tube 50 mm in diameter and 1500 mm long (capacity
about 3 liters). Eight cylindrical specimens 36 mm in diameter and 50 mm
long were placed in the center of the heating zone. To eliminate impuri-
ties, the specimens were previously annealed in air at 10000C for one
hour, Before starting the tests the chamber with specimens in it, was
evacuated to about 5- 10-5 mm. Hg. The specimens were heated to 9000C at a
Card 1/1-Z-
29997
S/170 61/004/012/007/011
Liberation of Cases from vacuum-heated ... B104/B138
rate of 60/min. As can be seen from Fig. 1, gas liberation peaks appear
at 300-4000C and 700-8000C. It is shown that the first maximum is re-
lated to desorption of gases I and the second to reduction of oxides.
Finally, tho quality of the various refractories is estimated from the
amount of gaaea liborated. The specimens were fjupplied by A. I. RoyzOn.
There are 2 figures, 2 tables, and 3 references: 2 Soviet and 1 non-
Soviet.
ASSOCIATION: Institut ogneuporov, g. Khar1kov (Institute of Refractory
Materials, Khar1kov)
SUBMITTED: February 10, 1961
Fig. 1. Temperature (or time) dependence of infiltration ( Ap, p/min).
Legend to Fig. 1a: (1) Kj; (2) K2; (3)Br(VG); (4)BJ1(VL); MA-~i (ALO;
(6)A.A2 (AL 2); (7) idle run system (without specimens).
Legend to Fig. 1b: (1) first toot; (2) after 2-hours in airl (5) after
50 hr; (4) after 250 hr in air 1 roasting at 10000CI (5) idle run.
Card 210
s/o8i/62/000/011/032/037
Z202/E192
AUTHORS: i3hnevski Sukharevskiy, B*Yas, and
-Vi sri 0 '.M.
Ga~vrishv~,.M.
TITLEj Method of quantitative phase analysis of Zr02 using
diffractometer YPC -50V (URS-50 I).
PERIODICAL: Referativnyy zhurnal, Khimiya, rio.11, 1962, 403,
abstract 11 K 189. (Sb. nauchn. tr. Ukr. n.-'i. in-t
ogneuporov, no.5(52), 1961, 315-323).
TEXT: A method of quantitative phase analysis using-URS-50 I
is developed. A characteristic feature of the method is the use
of a ring-shaped sample and the method of calculation which permits
elimination of errors arising from the determination of the back-
ground scattering of the X-ray photograph. It was found that the
preliminary annealing at 800 OC makes it possible to determine the
amounts.of the monoclinic modification independent of the mAgnitude
of lattice distortion present before annealing, and the grain size
(.--' 60 10. The error in the determination of the concentration in
the chosen method depends on the content of the phase and is of the
order of 1.5-5% absolute.
Card 1/1 [Abstractor's note: Complete tranalation-i
28(r,'
'/ P
AUTSORS: Kovalev, A. I., Vishnevskiy, I. I. SOV/32-25-9-32~53
TITLEt Determination of the Modulus of Elasticity of Refractory
Products at High Temperatures by the Dynamic Method
PERIODICALs Zavodskeya laboratoriya, 1959, Vol 25, Nr 9, pp 1109 - 1111
033R)
ABSTRACTs A method was worked out for high-temperature measurements of
the dynamic modulus of elasticity of refractories, allowing
to determine the normal modulus of elasticity E and the shear
modulus G simultaneously at any given temperature. This method
has already been used by A. I. Kovalev (Ref 1) for measurements
on metals. The sample is a parallelepipedon (30je3ox230 mm)
that is smaller in the center (16)06 mm and 80 mm long). That
part of the sample that was turned down to a smaller diameter
serves to localize the deformation and the zone of heat4na.
When the sample is fastened to a bracket of the apparatus
(Fig 1), it is possible to cause flexural vibrations or
torsional vibrations through magnet coilet the resonance
frequency of these vibrations being measured. During the test
Card 113 the sample is heated by means of an electric furnace (with
Determination of the Modulus of Elasticity of Refractory SOV32-25-9-32/53
Products at High Temperatures by the Dynamic Method
wire coiling of E1626 alloy). The vibrations of the generator
are transferred to a PS-64 scaler unit and the number of
pulses per unit of time is determined. The equations are
based on the assumption that the vibrations of the samj;le
lead only to a deformation of the turned down part of the
sample. Equations are given for E and G, according to which
these quantities can be calculated with an absolute error of
14 to 16%. Among other things it was established that with
Dinas-clay samples reliable results can be obtained, if the
turned down part of the sample possesses moment of inertia
of less than 0-5 CM4. During high-temperature tests dimensional
changes of the sample due to thermal effects are to be taken
into account"'I the correction to be made for isotropic
materials can be calculated according to an equation. The
reproducibility of the results of measurement was checked on
magnesite samples, wherefrom a maximum difference of � 1%
resulted. Diagrams of the temperature dependence of E and G
in commercial refractories of magnesite, fire clay, and
Card 2/3 Dinas clay are shown. (Fig 2). There are 2 figures and
Determination of the Modulus of Elasticity of Refractory SOV/32-25-9-32/53
Products at High Temperatures by the Dynamic Method
I Soviet reference.
ASSOCIATIONi Ukrainskiy nauchno-issledovateltakiy institut. ogneuporov
(Ukrainian Scientific Research Institute for Refractory
Products)
Card 3/3
VISHNEVSKIY, T.I.; SI!KfIARFVl--`K-rf,
uf".t of Point dr, ~!:;ts orn tha
snj.U,4cn3 wj tri ~:atir.;n ta z
NrAilelino-josledr;vat-e'Llski-y in3titut
VISHNEVSKIY, I.I.; FRENKELI, A.S.; SKRIPAK, V.N.
Heat conductivity of chrome spinalide. Fiz. tver tela 5 no.91
2691-2697 S 163. (MIRA 16:10) 1
1. Ukrainskiy nauchno-issledovatellskiy institut ogneupcrov, Kharlkov.
SHA TIM, D.K.; VISHMSKIY, I.I.
Determination of the.heat conductivity of refractories in a vaouas,
Zar. lab. 23 no.8:927-929 157. (KIRA 10:11)
1. Voesoyuznyy nauchno-issledawa~qllskljw.lastitut ogneuporov.
(Refractory v4swWo-Toettwe)
VISHNHVSKIY, MAKIN, A.T.; XTAUD, Kh.P.; LMKIN, B.P., redaktor;
WARALI~bWAI te.K., redaktor izdatel'stva; KIALINICHY99KOg F.P.,
tekhnicheskly redaktor
(Planning work and wages in construction brigades; practices of
Astonian buildbrol Planirovaaie truda i sarabotnoy platy v stroitell-
aykh brigadakh; is npyta stroak Istonskoi SSR. Koskva. Gos.izd-vo
lit-ry o stroit. i arkhite, 1957. 57 P- (KLHA 10:9)
tWages) (16tonia-Construction industry)
AUTHOR: VishnevakiZL I I Skripak. V. N.
ORG., Ukraiqe;~R_ei~,Arch Instltute5g Refractory Matgrials.- Kharlkov-_(Uk
nauchtio-issledovatellskiy insticut ogneyporov)
TITLE: Scattering of spinel lattice
phonons by cation vacancies in a
SOURCE: Fizika tverdogo tela, v. 7, no. 10, 1965, 2925-2929
~7
ainskiy
TOPIC TAGS: phonon, cation, crystal lattice, phonon scattering
ABSTRACT: The special role of vacancies in procesaes of thermal wave scattering
is caused by very large distortions as compared to additions of a substitute.
Characteristics of the concentration dependence of heat conductivity in soli
solutions of a substitute-subtraction with spinel structure, containing a la ge
quantity of cation vacancies were investigated. Measurements confirmed the
hypothesis on the effect of vacancies on phonon spectrum of the lattice, as I
result of -which the concentration dependence of thermal resistance shodld be
expressed by an alternating polynomial of the 4th degree. Solutions of
Card 1/2
26641-66
ACC NR: AP5025366
Orig, art. has: 3 figs. 5 formulas, and I table.
-Ah03 were used.
M91204
Ao/ SUBM DATE: OlApr65/ ORIG IM: 003/ OTH REF: 010
SUB CODE:
Card 2/21, 1
it
/0
ACC NR, AP6024507 SOURCE CODE: ui~ 181/66/008/007/22o2/2264
AUTHOR: Vishnevskiy, I. I.; Skripak, V. 1.
ORG: Ukrainian Scientific-Research Institute of Refractory Materials (Ukrainsk1y
i nauchno-issledovate~lskiy institut ogneuporov)
TITLE: Thermal conductivity o spinel-ferrites in the interval 300 - 1000K
SOURCE: Fizika tverdogo tela) v, 8. no. 7, 1966) 2262-2264
TOPIC TAGS: ferrite,,thermal conduction) temperature dependence, Curie point, second
order -phase transition, specific heat
ABSTRACT. In view of discrepancies in the published reports on the absolute values 1
And temperature dependence of the thermal conductivity of ferrites with spinel struc-:
cure, the authors inveqtigated the temperature dependence of the thermal conductivity
of the ferrites YgFe,204, NiFe2O3, Lio.5Fe2.5041 ZnFe2O4, and NixZn.,-xFe2O4 (x = 0.4,:
0.5, 0-7), synthesized by a standard ceramic technique and treated thermochemically,
to obtain maximum oxidation. The measurements were made in a nitrogen atmosphere by
a planar stationary method, using an installation similar to that described by Ye. D..
Devyatkova et al. (M v. 2, 738, 1960). The temperature dependence of the thermal
conductivity was found to be linear in all cases, in accord with Euken's law, with a
s4ght jump uccurring at the Curie temperature, attributed to the jump of the specific
he4t at the second-order phase transition point. The changes in specific heat and in
the,thermal conductivity at the point of magnetic transformation were determined for
Card .1/2
L 05633-67
A6~-k~ ~~2V5
all but the mixed ferrites. Deviations from data by others are attributed to the IVe-:
sence of a large number of impurity ions or to partial reduction of the ferrites. the!
I I
authors thank Ye. I. Aksellrod for making the magnetic measurements. Orig. art. has: 1
2 figures and 1 formula.
SUB CODE: 2D/ SUBM DATE: OqDec65/ ORIG REF: 010/ OM W.' 007
2/2
YEGOROV, I.Ye.; VISHNEVETSKIY, I.M.
The elevator system and its needs. Gor. khoz. Yosk. 37 no.11:
19-23 M 163. (MIRA 17:1)
1. Upravlyayushchiy trestom ALiftremont" Moskovskogo gorodskogo
zhilishchnogo upravleniya (for Yegorov). 2. Glavnyy inzhener
tresta rLiftremont" Moskovskogo (for Vishnevetakiy).
- BLOBOZHANKINO A.D.
Tuberculosis of the stomach. Xhirurgiia 35 no.12-.97-98 D 159.
(NLRA 13:6)
(MBIRMWSIS GAF)TROIMSTINAL case reports)
Fo esters of tha 1%t'ab-'t Fores, 0-~js-:!rvatio-~ S.a:.i(,iI. L,-S i S~-epl
9. Monthly List of Russian Accessions, Library of Congress, June 1963. Unclassified.
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VISHNEVJ-KIY, LV.
Vishnevskiy, I.V. "The anatomic properties of the temporal and subtemporal depressions",
Trudy Voyen.-mor. mad. akad., Vol-,XI, 1948, P. 284-301, -Bibliog: 21 items.
SO: U-3042, 11 March 53, (Letopis Inykh Statey, No. 9, 1949)
VISHMSKIY, G.Ye.; VISHNSVSKIY, I-Yet
Alectric sorption hygrometer. Tod.i san-takh. n0-7:16-20
Ja '6o. (XIBA 13:7)
(Hygrome try)
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VISMEVSKIY, K.P., irah.
Analysis of the efficiency of water conduit protection
devices from hydraulic hammer. Vod, i san, tekh, no.10:18-21
o l65. (MIWi 18:11)
vis'Aumif K.Pop izxzh,
Calculating hydraulic jump with the use of electronic Computers.
163. (MIRA 170)
Trudy Giprovodkhdza no.22,137_140
s/196/62/ooo/oiO/021/035
E073/E155
AUTROR: Vishnevskiy, K.P.
1~
TITLE: Investimi-Aion of the heat transfer in the layer by
the method of the regular regime
PERIUDICAL: Referativnyy zhurnal, Elelctrotelchnika i energetika,
no.10, 1962, 3, abstract 10 G16. (Tr. K-uybyshevsk.
aviats. in-t, no.12, 1961, 185-1-92)
TEXT: The conditions of heat transfer during cooling of
lump materials in a layer are elucidated, and the relations
necessary for *practical calculations are derived. Solutions are
obtained by applying the theory of the regular regime. For the
case of cooling of lump materials in a layer, the ordinary
equations of thermal regularity can be applied provided the
non-uniformities in the thermo-physical characteristics and'the
heat-transfer coefficient are averaged with respect to time or
temperature for the time interval under consideration. A
simplified calculation method has been'based on the developed
theoretical solution. 4 references,
Card 1/1 CAbstractor-s note: Complete translation.j
VISHIIEVSKIY~ --- K.F. , - --
Mechanized calculation of circular water-supply systems Vod. i san.
tekh. no. 4:20-24' AP 161. Z14IFA 14:4)
(Water-supply engineering-Tablest calculations, etc*)
8(6)
!Z-5'~t-4-6535
ii-cm: Referativn7y zhurne-1 119.50 4, 7? 18 (TUSSR')
AUTHOR: Kcdzyachev, L. 1. , and K. P.
TITLE: IIC:- Oel--c-t:Lon o-J.' ~h;a Dete:~mir-;-.-xv
Eauivzdunt Ldameter .-i -.-ompul'in- tht! Heat-Yranafe:,-
mot.,r,:-. of a Liquid in z Pipe
1957, Nr 7, -11-45
PER*fOD!rA',',: Sb. awachn. tr. '-K,-yb-j.-3hevak. industr.
ABSTR-AC,7: 'ZIlie-orat'-cal ha Z i z Jx g i v ea to t h P su g g e --v` io v- cA cd rz rn.1, c 12 n
IM. A. hlil~heLYCV, which iz: the avezz-.ge liquid tc-.-npe-.r3.t=e is '-,e
ti--,:. t~ etermining tcimperature , and tite cq~.tlvalent diarric.er is --- .'0 11'. t-.- Vie
dr-termln3jag di-----v~nsi~m; thiEi dirmoter ic equal to Vhe qUrd-:.u.AC(!
area �ivided bly the en-re (wetted) perimeter of t'he crcos-:iec,'i~a,
ti'Le f;r-ct t1hat only a part of Oie perimetez.: pla- role in 11-he
ye P
Pz--viz!e -wvo-:1, z balance cf energieE passing through an em'.em~nt I,-- tl,-F- vorZace
that limillz3 the :rcgicn in queation. ;-a cornplle~~-.. To r,?-1cu:---L'-.e tl%c -4-*r-1::kaasc ;:!f the
Card 1 !?
SOV11 12-59 -4-6535
Theoretica.' Basis for the Sol'cctioa of the Determining Tem.-ceralcure and
boundary hydrodynamic layer, the balance between the pressure drGF in t'he
pipe cross-section and the shearing stress applied at the average-atream
boundary is considered. A mathematical expression of this balaace, after
some transformations, results in an equation of the heat-transfer h7drody-aamic
theory; this demonstrates the close association of the hydrodynamic theory and
the bo-andary-layer theory, on the one hand, with the problem of selecting the
determining temperature and equivalent diameter, on the other.
M. 14. N.
Card Z/Z
SOV/124-57-3-3200
Translation from: Referativnyy zhurnal. Mekhanika, 1957, Nr 3, p 80 (USSR)
AUTHORS: Kudryashev, L. I., Vishnevskiy, K. P--
TITLE: On the Calculation of the Coefficient of Convective Heat Exchange
During Condensation of Steam on Vibrating Tubes (K raschetu
koeffitsiyenta konvektivnogo teploobmena pri kondensatsii para na
vibriruyushchikh trubkakh)
PERIODICAL: Sb. nauch. tr. Kuybyshevsk. industr. in-ta, 1955, Nr 5, pp 160-
165
ABSTRACT: The author derives a semiempirical criterional formula for the
Nusselt number for the heat exchange during the condensation of
stearn on vibrating horizontal tubes.
G. A. Tirskiy
Card 1/1
IZ4-58-9-9976
Translation from: Referativnyy zhurnal, Mekhanika, 1958, Nr 9, p 75 (USSR)
AUTHOR: Vishnevskiy, K
TITLE: On the Resistance and Heat Exchange in a Pulsating Flow (K
voprosu o soprotivienii i teploobmene v pul' siruyushchern potoke)
PERIODICAL: Sb. nauchn. tr. Kuybyshevsk. industr. in-t, 1956, Nr 6,
book 1, pp 207-212
ABSTRACT: The author adduces certain concepts on the investigation of the
problem of the resistance and heat exchange in a pulsating flow.
Transverse pulsations are examined. The author suggests the
introduction of the ratio of the pulsating velocity component -10
to the mean flow-velocity component w0 as a similarity criterion.
1. Pulsating flow--Heat transfer V. S. Avduyevskiy
2. Heat transfer--Theory 3. Pulsating flow--Resistance
Card 1/1
TIT c! 'I r7,P-, '(T 77, F.
ll-stimr,Uon -if he.nt-exlh--in~e durinc- 1~oolirg ir the 1-y:~r of -rain
7~enort -,zenent-I tli,~ ll-~!ni---)n ',onfirrmce on lsl-~-A-,~nl T~ass-71xch-m-a-,
Abst Journal: Referat Zhur Mekhanika, No 3, 1957) 3200
Author: Kudrashev, L. I.., Vishnevskiy., K. P.
Instituticm: None
Titlet On the Calculation of the Coefficient of Convective Heat Exchange
During Condensation of Steam on Vibrating Tubes
Original
Feriodicalt Bb. nauch. tr. Kuybyshevsk. induatr. in-taj 1955) No 51 160-165
Abstracti Derivation of a semiempirical, criterial. equation for the Nusselt,
number for heat exchange durin&,condensation of steam on vibrating
horizontal tubes.
Card 1/1
.9/124/60/000/00-1/1:' ..~/017
A005/AOC I
Translation from: Referatlvnyy zhurnal, Mekhanika, 19-160, 60, 2, p. 79, # 3472
AUTHOPS.- Fulryashev, L' . I., Viehunevskiy. K. P.
'ITTIX; On the Theoreti.~al Substantiation of the Cal,--alatlon Equatlon for ":qe
Corriective Heat-Excl~ang- Oo,-'Pficient at M,,tIc,n -n.-er
Tnt?=,al-ProbIem Co-M-1-til S i
PERIODICAL; Sb. nx--,.-;bn. tr, Kiybyshevsk, industr. In-ta, 1957, No. 7, pp. 33-40
TEXT: The ai;4-hors attewt, to subs"alitiate the known emp4ric expcner,'Aal
fornrila of the Lnter,~onnecti-on between the Nusselt number and tte Reynolds- and
Prandtl-numbers, usir~g +~re early rtwa-layer" Prandtl s,~.h,-tmA (lamilpar eutl"er,
tulrbui~~nt layer) . Exponential formulae with the sqm.,~ power exponent, equal to
the known empirical exporents 1/6 and I/IQ are ,sed f.-
the arithmetic mean from t
the velo:-ity- and temperature patterns in the turlyllezil, lay-ir. The -~oxv'!-ntlona]
empirit2al exponential foivila. is also used for the re3istane
Using tbeze empirisal data and ba,,irZ on the Impalee- a:-,.,I Uhem- al-balanr'.3-
fo:iraiae, the authore set. up their theoretIcal 7-1i autto-r? d- n:,'
Card. 1/2
S/124/60/000/003/013/017
A0051AW!
On -the Theoretical Subst-wit-14ation of the Cair-ulation Equatlc~n for the
Heat-Rx,change Coefficient at Tarbulent Mn'.-.'Lon. Under, intarnal-Frobl-~m
mention the l1mits of th-a Prwndtl ni-Lrrh,~-r wLI.4eps, -jhl-,h they ascume
conclusion to be tiae. At the othsr hail, It is known that th5
Is not Joustified for large F,randtl numbars and rnist b5 rapls.2~~d s, mo.-.-i
rigorous scheme, whiqh J-3 th6
zone, tuft-,.il.~,nt layer) eetablishel by ft-mait In *,he
Card 2/2
Zhw., 10.1
1,70 mrfm., M
th,
, , - 1--l
'In ~AJAI. rv?.ull, Inf. clljp~ncnl ci-l-un
Of rj-,,
11r. Mill.
XEIUR ZUR CAFX6TsW, Walther; VISHMSKly. X.P. [translator]; NEHIROV,
Yu.G. [translator]; -VASKANOV, V-.V..red.
[Instrumental mathematics for engineers] InatrumentalInsia
matomatika dlia in2henerov. Moskva, Fismstgiz 1959. 379 P.
Translated from the German. (MIRA 14:2)
(Mathematical instrwwnts)
VISMWSM, K. P.
"Cal lbilation Of Heat Transfer in a Layer of a Gramdar Material."
Report submitted for the Conference on Heat and Mass Transfer,
Minsk) BSSR, June 1961.
vislawsKly, K. P.
I---- - - - - , , - __ -
"Heat -transf er calculation for the heating and cooling of a bed rf'
fraEgwnted material by a cross flow of gas."
report submitted for 2nd All-Union Conf on Heat & Mass Transfer, Minsk, 4-12
May 1964.
Sci Res Inst of the Cement Industry.