SCIENTIFIC ABSTRACT SMIRNOV. V.N. - SMIRNOV. V.P.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001651610016-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 24, 2000
• Sequence Number: 16
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SMIRNO-Vil V.N., otarsbiy prepodavatell
Choosing the size of working areas across tile pitch under the
conditions of the Prokoplyevsk-Kiselevok area. Izv. v-ys. ucheb.
zav.; gor. zhur. no.8:31-37 161. 011PU 15-5)
1. Kemerovskiy gornyv. institut. Rekomendovana, kafedroy
razrabotki mestorozhdeniy poleznykh iskopayemykh Kemerovskogo
gornogo instituta.
(Kuznetsk Basin-Coal mines and mining)

inzh,; V,,N,., in-zh,
olperations, I~iekhi av-tomzproizv, 15 no.11-
41-43 U 6a (MIFuk 14.: 11)
(Mining engineering ..-Tecimological innovations)

PETRENKO, A.A., gornyy inah.; SHIRNOV,_V.N., gornyy inzh.
Practice of using hardening filler in a mine. Gor. zhur. no.9:
32-34 S 162. ~ (KRA 15:9)
(YAne filling)

ARMPSKI-Y, Ye.V.; BORODULIN, A.I.; RYBIN, V.M.; SMIRNOV, V.N.
Measuring the average energy of electrons of a law-energy
linear accelerator. Izm. tekh. no.1li44-1+5 N 165.
(bUFA 18:12)

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appears imarlio than otherg
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X&I A 6173# ibiah. oan in�iomte.an .10AIllit on--lbort 'a nth
aica o_ng A~he,- pa The --pbsoluts,
linte ge/00. , 0
nxitles (in,er met) wares O'l
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L 24218-65 EVJTW/EPF(c)/EPF(n)-2/EPR Pr-4/Ps-4/Pu-4 DM
ACCESSION NR: AP5001268 S/0089/64/017/00610463/0474
(deceased)
AUTHOR: Kurchatov, I. V./- Feynbera, S. M.; Dollezhall,_N. 4.; 4Le~hchenkov,
P. 1, ; Drozdov F. S. ; Yemell vanov. I. Ya. ; Zhirnov, A. D. - Kazachenko M. A.
. . ..........
Knvazeytr G. D.; Kondr,atlyev, F. V.; Lavrenikov, V. D.; Morg~!n2v, N. G.;
Petunin.. B. V.; Smirnov V -P. TajyAin. F L1iM(jv, _A. G.; Chikhladze,
1. L.; Chulkov P.
TITLE: Pulse graphite reactoAGR
SOURCE: A tomnaya energiya, v. 17, no. 6. 1964, 463-474
TOPIC TAGS: pulse graphitle reactor, high neutron flux pulse, nuclear reactor
ABSTRAC7: The paper is a summary of the SSSR #322a report at the Internation-
al Conference on Peaceful Ys.es of Atomic Energ)Liin__Qeaetva,_1964. It represents
_a_n_~1abo`r__ation of the descriptio n of the pulse graphite reactor IGR given by
S. M. Feinberg at the Second International Conference. The pulse reactors are
used when a high neutron flux is desirable. The described reactor was in opera-
C.rd 1/2

L 24218-65 67
ACCESSION NR: AP5001268
tion for several years, and is still working without failure. Orig. art. has:6
figures
ASSOCIATION: None
SUBMTTBD: 00 ENCL: 00 SUB CODE: NP'
NR REF SOV: 002 OTHER: 001
Card 212

SMIRT)OV, V.P.
-- ----------- - .1
"Die polatographisebe bestimmung von ftorothan(1,1,1,-trijkluor-
-2-chlor-2-bromathan) im blut.w
Report submitted to the Oscillopolatography Course and Polarography Symp.
Jena, GDR lo-15 sep 1962

VALETOV-, V.V.; VESNIK, M.I.; GONCHAROV, I.S.; DY[ITROV, D.V.; LUNEV, A.A.;
MOKIN, M.I.; NESTEROV, S N.; SMIRNGV V P - ALEKSEYEVl s.A., re-
tsenzent; KARKAZOV., AOG.; reisenzdnt; KONDWOVICH, V.M., reteen-
zent; LEVIN, B.M.., retsenzent; M&LIKOV, A.N., retsenzent; SEGALE-
VICH, S.M., retsenzent; SHPACYIN, A.I., retsenzent; SHTERN, L.T.,
retsenzent; YAKOBI3 A.A., retsenzent; TIKHANOV, A.Ya., takhn. red.;
CIUOIOVA, Z. I. . tekhn. red.
(Establishing norms for the conswnption of materials in machinery
manufacture; manual] Normirovanie raskhoda materialov v mashino-
stroeni4-; spravochnik. Pod red. V.V.Valeto-va. Moskvay Goa. nauchno-
tek'hn. izd-vo mashinostroit. lit-ry. Vol.l. 1961. 583 P.
(MIRA 13:2)
(Machinery industry)

SM1.1alov.1 V.P., inzh.; SHIBANOV, A.A., l(ai.d.te-kLn.nauir
Using caisson shells made of pa-nel--type- eliament.E. Trans-. stroi. 14
-1 U.
nc. 1,, 1' -1.8 Ji 164,. (MIRA 18,,1)

SMIRNOV, Vladimir Petrovich. Prinimali uchastiye: LADITSKIY, V.F.,
knnd.tekhn.nnuk-, SILAPKIN, I.F., knnd.tekhn.nauk; MIKHAYLOVICH.
A.M., inzh.. KNORRE, G.F., prof., doktor tekhn.nauk, zaslu-
zhennyy deyatell nauki i tekhniki, red.; VOROHIN. K.P.,
tekhn.red.
[Boiler units] KotelInye ustanovki. Pod red. G.F.Knorre.
Moskva, Gos.energ.izd-vo. 1959. 303 P. (MIRA 12:8)
(Boilers)

4Lt1pqV,,_ Vyacheslav Pavlovich;. ROSHCHINA, L,', red.; NAZAROVA,, VIP
~d-aZM-y-~Fe,; ~OGIVA, N., tekhn. red.
(Tunisia; economic outline] Tunis; ekonoricheskii ocherk. Mo-
s-kva, Izd-vo sotsiallno-ekon. lit-ry, 1962. 70 p.
WIRA 15:6)
(Tunisia-Econow.ic conditions)

SMIRNOV, V. C
All-Union conferenco of industrial efficien-c;, prowl's-rs inventors, and-
(k.-
Innovators. Neftianlk I no.12:27 D '56. .1RA 12:3)
(Petroleum industry)

:SMIRNOV, V.P., Inzhonor.
Tankn of mfficioncy promotarn nnd inventors. Stroi.pred.neft.prom.
I n0-3:28-30 Mv- 156. (HLRA 9:9)
(Petroleum industry) (Petroleum workers)

SMIRNOV V.P.- LRTOV, G.S.
L.;bL~
Outbreak of pulmonary plague in Gichigan in the W049011an People's
Republic. Izv.Irk.goe.nauch.-isel.protivochum.inst. 20:105-106
'59. (MM 13:7)
(GICHIGAN (MONGOLIA)--PLAGUR)

-SMIRNOV, V.P._
Iffectiveuess of chloropierin disinfection of piagmB infested
hides of wild-rodents. Izv.Irk.gos.nauch.-isel.protivochum.
inst. 20-121-123 159. (MIRA 13:7)
OHLoRopir.RIN) (HIDES AND SKINS--IDISINMTION)
(PIA(XJX)

,5?4iHNOv9 Iv~,!, ,
Frimi the diliry of' a phy.-I I "-,I fill. ini,tiettA With (typorimental plague.
Zhur, mi.krobiol. opid. A Immun, 40 rio~5,68-72 MY 1631
(AURA 17~6';-
.L. 1z Irkvitol.,ogo protl,vocimmnogo Institaitit Sibir-i I Dallnego
Vontoka.

ROZHNOVSKIY. AlIbin Antonovich; VAGANOV, P.V., kand.tekhn.nauk. reteenzent;
SMIRNOV, V.P., gornyy inzh., retsenzent; NNGANOV, I.I., gornyy
Inzh., red.; SKOROBOGACHNVA, A.P., red.izd-va; ZXF. Ye.M.,
tekhn.red.
[Placer mining] Razrabotka rossypnvkh mestorozhdanii. Sverdlovsk.
Goe.nauchno-tekhn.izd-vo lit4y po chernoi i tsvetnoi metallurgii,
1959. 336 P. (MIRA 12:8)
(Hydraulic mining) (Dredging) (Mining engineering)

SIMIRNOV, V.P.; KULIKOVA, V.L.; Sl`.Cl'---~WNIOV~, _.7.
Use of white ra'o for the determination of immnogerAc prcpez--.iz-s
of anticholera pi-aparations. Zhur. mikrobiol., epid. _i i=,u-n. 40
n0.9.'130 V63. (MMA 2?: 5),
1. 1z 'sk-,7o
t;
ills ti I~uta Sib--'--.:k i I'a-I

ACCESSION NR: AT4025314 S/0000/63/000/000/0237/0246
AUTHORS: 'Kovan, I. A.; Moskvin, Yu.~ L.: Rusanov, V. D.; Smirnov,
V. P.
TITLE: Investigation of plasma parameters in a strong magnetic
field wi..:h the aid of dopble electric probes
SOURCE: DidgnostikbL plazniy* (plarma'diagnostic's)-, ab. statey.
Moscow, Gosatomizdat, 1963, 237-246
TOPIC TAGS:' plasma, plasma'diagnostics, probe method', double probe
method, plasma in strong magnetic field, probe method accuracy#
Larmor radius, probe characteristic dimensions, charged particle
density, electron temperature, saturation current, effect of probe
size, probe current, probe current derivative
ABSTRACT: In view of the doubtful reliability of data obtained with
probes on a plasma in a strong magnetic field, when the particle
Card
FW--

ACCE3SION NR: AT4025314
Larmor radiulk is coinparableiwith the probe characteristic dimension,
the authors halve chlacked on'tbe probe readings by other diagnostic J~
means. The Plasma parameters measured were electron temperature andI.-I
chArged-particle density at'saturation. The electron temperature
wa.~i determined by plotting the derivative of the current with re-
S'p6ct to the"voltage against the probe voltage. The charged-particle;
deAsity was fheasured by determining the saturation current and also
by measuring the derivative of the probe current with respect to the..,
voltage in the vicinity of zero voltage. The effect of the probe .1
size was also investigated. It is shown that the probe measurementW'.
deviate from the others by as much as 40% and become particularly
unreliable in strong magnetic fields. Orig. art. hass 5 figurese
ASSOCIATIONs' None
DATE ACQ: 16Apr64 .-ENCL: 01
Mi.MWEDs -~,190ctO*
SUB CODE: PH ~NO REP SOV: 005 OTHER: 00
Card,~j2
4

L 26662-65
A
ACCESSION NR:
T5002708

of :
.,,:
th6A1stribution'-
distorti an
the. field,~.c d
ion in
of determining the
-
.
,,
.
,,.
,

ium~'okbit measurement e
b f~th
0
the gradient along.the equili
-
tion and distribution of the'.gradicint along the radius of the magn t-, -..~.._.~-,..-,~~

i'
:
'rbit. in
r um o
: on . the equilib
measurement of the relative grad ent
l
.
-
'
center of the electroma net: The principle of the' method, -developed..
9
consists of integrating the voltage from coi s placed in'the time-
varying magnetic field. The-..theoreiiic.al.premises-underlying the
d #..after which the design of the
ifferent measurements are.1de
ed
velop
l
.
-
measuring coils is-described,and the-circuitry of the electronic,in
tegrator is described.- circuit for-selecting the~,level of-the*
measured field is described..aiid the measurement accuraqy:discussed..:,_
Orig. art. has: 5 figures and:31 formulas..
ASSOCIATION: None.

~:"ENC4: 00, -SUB COM, NP'.~ EM%;
StMMITTED: 00
NR REP SOV: .000 OTEIER.,.~ 0031
Card

KOVAN, I.A.; KOZOROVITSEY, L,L. ; RUSANOV, 17,T), ; SMURINOV) V'P, - FRANK--
KAMENEETSKIY, D.A. , .. ___j
Magnetoaccustic resonance -n a toroidal system, Zhur. eks-,, ~
teor. fiz. 48 no.1-72_77 Ja '65. (MIRA 19:4)

ALISHITS. I., inzb.-khimik; SMIRMY, V., kand.tokhn.nauk. inzh.-
khimik
Ship rescue boats made of glass-reinforced plastics. Mcr.
flot 19 no.12:42-43 D '59- MlLk 13:3)
(Boatbuilding) (Glans reinforced plastics)

SMIRNOV, V.P.
Plastics for anticorrosive cements (from "Applied Plastics,"
no.10, '59.) Bet. i zbel.-bet, no.11:530 u 16o. (MIR--- 13:11)
(Plastics)

, - _VjAdimir Petrovich.,- SHAPILOV, V.M., retsenzent; OSIFOVICH, F.A.,
SM194OV,
red.; VITJdfIkfffA- S.A., red.izd--va; RIDNAYA, IN., tekhn.red.
.0
[Manufacture and assembly of ship systems from plastic materia1s]
Izgotovlenie i montazh sudovykh sistem iz plastmass. Moskva,
Izd-vo "Rechnoi transport," 1962. 65 P. (MIRA 15:5)
(Marine pipe fitting) (Pipe, Plastic)

---SMIRNOV, V.P.
New plastic materials. Plast.massy no.3:75 162. MRA 15:4)
(Great Britain-Ggass reinforced plastics)

SEWN(:V, A.; SMIMOV, --V..P-.l SHVEDCHIKOV, A.; SHVEDGHIKOV, A.; SEWNCV, A.
Plastics abroad. Plast.uzassy no.4:70-71 162. (YIRA 15:4)
(Plastics)

SMIRNOV, V.P.
Construction and testing of plastic lifeboats for inland naviga-
tion ships. Plast.massy no.8:40-46 '62. (KRA 15:7)
(Lifeboats) (Glass reinforced plastics)

ACCESSION NR: Ap4olftm S/0191/64/000/003/0059/004-;
AUTHOR: Smirnov, V. P.; Sosunov, N.A.
TITLE: Electric resistadee welding of plastics
SOURCE: Plasticheakiye maafjy*, no. 5, 1964, 59-61
TOPIC TAGS: resistance welding, electric resistance welding, plastic weldingp
plastic, pulsation welding, polyethylene tube welding, nichrome spiralling,
ABSTRACT: One of the new methods for welding plastics is electric resistance
welding with the use of special spirallings. This method, called pulsation welding,
is already being used in a number of industries. This process consists of three
stages: (1) preparation of the elements to be welded; (2) formation of the
electric spiral and shaping it into plastic rings; (3) pulsation welding of the
parts to be joined. The essence of this method is the joining of separate-#plastic
parts by a layer with an electric spiral by means of flashing cff contiguous.
surfaces. Plastics which have a high specific;volumetric resistivity are welded
by this method. These plastics include polye~hylenes, polyamides) polystyrenes,
etc. Polyethylene tubing, used as connecting._R~~jces~ in pol'yethelene collw
Cord

F
ACCESSION NR: AP4018170
assemblies and having r,~ichrome spiralling shaped in it, is welded by electric
resistance. These collars are made in the form of cylinders on metal drums. One
of these adaptations is shown in Figure 1. A special device'with a step-down
transformer is used for this type of welding. The device also has a timer which
assures the requisite holding time for heating of the spiral after the transformer
is cut in. The electric circuit diagram of this device is showa'in Figure 2. The
welding sequence is as follows: a Geat for the collar is prepared in the tubing
elements which are to be welded; the collar with the spiral is placed in the seat
of the union or pipe bell and the tube to be joined is inserted here; the ends of
i the spiral are introduced on the outside and axe joined by the current source; the
Aft
heated spiral fuses the polyethylene layer and tube surface sticking to it. er
heating up to about 120 C, the feed current,is cut off and welding is completed.
The heat-up usually takes from 30 to 40 seconds. The welding is effected at 36
volts. The timer controls the holding and current cutoff. OrIge art. has:
4 f igure a.
ASSOCIATICN: None
2/5
I'Card

ACCESSION NR: AP4016170
SURMITTED: 00
SUB CODE: IE, MA
Card rx.
LATE ACQ: 27mar64
NO. RET. SOV: 000
ENCL: 02
Onw: 000

AcassioN NR: AP4018170 SNCLOSURF t 01
Fig. 1, Attachment for Lnding the electrib
spiral, 1-metal cylinder; 2-polyeth-
.. elene layer; 3-nichrome wire; 4-stop.
Card 4/5

ACCESSION NR: AP4018170
ENCLOSURE: 02
FIGx 2 Electrical diagram of
attachment for electric resistance
welding of plastics. 1-to spiral;
2- 220 volt circuit.
WM
5/5

,!, 'i
I!. ", f N ,V.P.
-!~ T ,w rX tne we'ded are-ains of pla:3tics. Plast. mirissy no.10.52-55
It lz
. -.*, ~ .. - OMIRA 18.10) /

t I -1892-66 EWT(1)/EPF(n)-2/h"rC(m) TIP(c), WW
ACC NR- AP5026012 SOURCE CODE: IYP/10386/65/002/(108/0356/0360
0
AMMOR: Rusan6vp' V. D. SmIrnov, V. P.
ORG: none V1
TJTLE: investigation of oblique Tw
__nette sound waves of large RNP-Ittude
SOURCE: Zhurnal eksperimentnl-1noy, I tPorcticheskoy fl?,M. PislwA v robtiRktRiyu
(Prilozhentye), v. 2p no. 8, 1965, 356- 36-1
TOPTC TAGS: magnef.vacoustic effect, sbork wave forTmatinn, nonlineetr eff-et
ABSTRAC*T: This Is a continvatIon of eRrVer Investigations of littenr oblique
magnetic-sound waves (sometimes cailed I4bletles) (with I. A. Knvokn et &I., Conference-`
on Plasma Physics, Salzburg, 1961,.p.,205),,and is devoted to an investigation of the.
transition to nonlinear waves. large-amplitude shock waves were excited by a shock
circuit of 15 Me frequency. The magnetic field In the center of the excitin coil,
which was 30 mm long and 4o mm in radi -us, Increased to 800 oe within 2 x 10-9 see
(Fig. 1). 7be magnetic field in the homogeneous.part of the solenoid ranged from
200 to 2000, oe. The measurements were made for values of q = Hz.m&x/% (Hz.max--
maximum value of the magnetic field In the circuit in the centerof the group in the
absence of a plasma, No--constant magnetic field) ranging from 0.2 to I.T. The dis-
tance from the center of the loop to the magnetic probe ranged from 0 to 4o cm. The
results confirmed experimentally the influence of the wave magnetic field on the wave
propagation velocity. In addition, the dependence of the maximum wave mWetie.field
on the maximum excitation field was Investigated. From the observed dependence of
-Card--1/2

~42-66 EViT(1)/E,Fr(m)/T/EViP(t)/EWP(b) !JP(c)
j _ _ JD/GG
NR: AP5022741 SOURCE CODE: UR/0181/65/007/009/2856/2858
AUTHOR: Smirnov. V. P.
ORG- Leningrad State iversity (Leningradskiy gosudarstvennyy universitet)
TITLE: Band structure of rpuprou oXide
?
SOURCE: rizika tverdogo telai, v. 7, no. 9, 1965, 2856-2858
TOPIC TAGS: crystal theory, cuprous; oxide, energy band structure
ABSTRACT: This paper gives preliminary data from a theoretical calculation of the
energy structure of cuprous oxide in an attempt to explain experimental data on opti-
cal and magneto-optical absorption in crystals of this compound. For the uppeT va-
lence band, W25) = 0.151 atomic units, and for the lower conduction band E(rj)
-_`0.240 atomic units. This gives the width of the forbidden as 0.089 atomic units
(=2.4 ev) which is very close to the experimentally observed value AE = 2.3 ev. The
theoretical data indicate that the r25 level originates about equally from the 2p-.
-levels of oxygen and from t~e 3d-levels of copper. The next valence band (k = 0) is,
about 3 ev longer than the r75 band. However, it is not certain whether the symme-
try of this band is ris or rT5. These theoretical calculations (which were done On
a digital computer) confirm Elliott's model (R. J. Elliott, Phye. Rev. , 124, 340,
1961). Orig. art. has: 5 formulas.
SUB CODE: 20/ SUBM DATE: 09 AprG5/ ORIG REF- 004/ OTH RErz 004
Card
r

SMIRNOVY V.P.
Calculating the band structure of copper oxide. Vest.LGU
1
20 no.22:7-19 f61. (MILR~ 18:12)

F'~"rj. t,)/FTl ii P JD
A~C NRt A1116026731 SOURCP. 66b~: O-R/Of8l/66-/668-[dtO/2~fq~~19-:
AUTHOR: -Smirnov, V. P.
ORGt Leningrad State Universi im. A. A. Zhdanoy (1aningradskiy gosudarstvennyy
univorsitot) 11 0
TITLE: Band structure of the cuprous oxide crystal
SOURCE: Fizika tverdogo tela, v. 8, no. 8, 1966, 2519
TOPIC TAGS: cuprous oxide, semiconductor band structure
,UOMICTI The energy bands (upper valence band and lower conduction band) in the cu-
prous oxide crystal along axes of second,third, and fourth order in K-space were cal-
culated. Also calculated were censtants characterizing the curvature of the energy
surfaces at extremal points of the bands (with wave vector K = 0). The effective mas.-
for the conduction band was found to be equal to 0.456 of the electron mass,and con-
stants A, B and C for the triply degenerate valence band were found to be respectivel.3
equal to -1-073, -0.205 and 0.453. Consideration of spin-orbital interaction (in ac-
cordance with the perturbation theory) leads to splitting'of the upper valence band
into two bands, r,+ and I-,+. The splitting is equal to 0.06 eV (the r+ band is higher
than thef',+ band). This agrees ifith the experiment in order of magnitudel the dis-
tance between the limits of the yellow and green series of the exciton in the cuprous
oxide crystal is equal to 0-13 eV. The one-electron parameter k3d was used in the
Card 1/2

A LIFY I ~ -I ", - 1 11
I-Vl'~N I '. V M N! " V'
M;F, -A bind for r-tjznw-.j:: meaaure%entl in a Strong..
focue~!-.,- rlec..tron synchrotron in the 5C0 ~- IODCOG ce. I-ange.
t84. is,,'

KURCHATOY, !.V., (de:~easedj; FEMBER(-:, S.IM.- DOLLEMALI 'i.A..~,
A-LEESil,,-;H"E-,IKOV, F.I.; D-ROZDOV, F.S.; i--q'IEL'YAIIOV, I.Ya., ZHIR,011,
A.D.; KAZACFMIKO, M.A.,, KNYAZEIIA, G.D.; KCNDRATIYE-V. F.V.?
LAVRI~NIKOV, V.D.,-, MORGUNOIT, N.G.-, PETUNIN, B.V.; SMI-MOV .V-2-1 ;
TALIZIN,,.V.M.; FILIPPOV, A.G.; G'IIKHLADZE, I.L.;
SHETELEV, Ya. V.
Pulse graphite reac-t.--)r IGR. Atom. anez-g. 17 no.f-,:4(,3 D
(MIRA 18:1)

V. P.
Glasc -arull Elic'u're
of' c-lass furnaces wft~-clat cleapr~mr gres flues b-, fire. ,,, , I r
ec. pror,,. no. -, IP-~:,2.
... - or C 'ecember 1-95". Unclassif"ed.
-.ont~,Iv ILt of Pus~zian Accessi-Ons, F-bram, - -onvress ,

L I JIll IP.
4. Furnaces
7. Gleaning -as ductS i_.Ilrnin'~ ;.iiem, out and" i"ith recuperation of the tar,
Stek. i ker. 10 no. 5, 19,53.
9. Monthl List of Russian Accessions, Library of Congress, APHIL 1-1953, Uncl.

MSR/Miscellaneous Glass manufacture
Card 1/1 Pub. 104 10/12
Authors Smirnov, V. P.
Title Gas heated annealing farnaes
Periodical Stek. i ker. 9, 30 - 31, September 1954
Abstract t Description of a new conveyer-type gas-heated furnace for the kilning
of glass products. Drawings.

SMMOV, V.P.
Simplified, continuous action, annealing furnace. Stek.i ker. 14
no.8:20-21 Ag 157. (MIRA 10:10)
(Glass furnaces)

AUTHOR; 72-58-3-12/15
TITLE: The Utilization Coefficient of Window Glass in Building
Must be Increased
(Povysit' koeffitsiyent ispollzovaniya okonnago stekla
na stroykakh)
PERIODICAL.* Steklo i Keramika, 19519, Nr 3, pp - 41-42 (USSR)
ABSTRACT: Following a suggestion by the author, glass-blocks were ex=
pu,rimentally manufactured in the following way in the Bemsicheskiy
of the Council of ~Jational Economy of Kaluga:
Sectors and blocks of 3 sections, as given in figures 1 and 2,
were manufactured of sheetd of window-glass of the dimensions
looo x 5oo x 3 mm. The weight of one section is 3,2 kilograms,
that of a block 9,6 kilos and the quantity of glass required
for one block is 1,8 m?. These sections which were manufactured
in glassworks, can be installed in buildings. By that means,
less glass is broken during transportation, and the glass-scrap
can be utilized, and the manufacturing expenses will be reduced
Card 1/2 in this way. Furthermore, qualified workers manufacturing the

The Utilization Coefficient of Window Glass 72 -58-3-12/15
in Building Must be Increased
wooden window-cases, will no longer be required for construction.
The mounting of the glassblock is simpleand no skilled worker
is required. Nor is a first-class lumber required for this. pur=
pose, since the glass-blocks are walled immediately in the voids.
Besides- the savings of high-quality lumber and qualified workers.,
the luminous area of the aperture of the window increases and any
thermal loss in winter is-avoided due to a complete hermetical
seal
There are 2 figures,
ASSOCIATION; berezicheskiy stekol"nyy zavod
( Glassworks)
AVAILABLE: 1- Glass--Applications
Card 2/2

nov V P,
JOV/ 7 2 - r~- e - 7-12119
Cof;,mon Salt - a Good Accelerator of Glass Melting
(Povarenn:mya soll khoro,3hiy u.9koritePvtxki stekla)
ps;iloDiCAL; Jteklo i keramika, 1958, Ur 7~ PP A~D - .1,1 (USSR)

.IBST~IACT:
I
M, P., Orlova, V,. V, Pollyak und I, D~ Tykachins'
-iy
(Ref 1)' state in their paper that 0,5~; Pq introduced
additionally into the layer to the basic composition
of glass increases the output of the tank furnacesby 10
in the case of maintainance of the usual glasi
imeltin- temperature level. This is confirmed as well by
the paper of the ClaS3 works Bytosh"' and "Veli-
kiy Oktyabr'".. The author Lssumes chat for the
!)_-ide the fluorides also
chem cal ac tivi ty
0f -NhiCll 1~3 110 tinCerijl' LO L1,--t the fluorid~--j. The
editor is, hc-never, of different opinion (Fef 1).
Further-ore the use of fluorides dezzands orot,~ctive
measures which _--re riot necessary in the case of chlorides.
Card 1/3 Th:L:3 is ,_13o confirmed by the atte:,.:pt to use t~heua in the

''al t -;of)d Accelet.-or of Glass Meltinj3 ju'V2-55-7-1 '119
Elass -1-1-orks Berezichi in the --eltin-- of medical g-lasn,
S ti 11 in !9AI6 common 3-~lt has been introduced into the
layer exceedinr7 the calculated composition by from
15 to 20 k1g1per ton, The composition3 of glass and
1 a.v e rare diven in 'tho table, The moisture content of
th,~ layer amounts to 3 The glass melting is
carried out in a tank --f-urnace of the type "simpleks",,
at a maximum temperature ol 14300 and in the case of a
mass outPut of 500 kg/m2 per day. 3y the introduction of
common ~L--lt into the layer 'the output of the furnace
increased by 28,-a above the scheduled output; the quality
of the glass mass was as well rapidly improved. Furthermore
the preparation of the common salt is described as well
as the melting process of the layer. There are 1 table
and 1 reference, 1 of Aich is Soviet,
A 3 Cj C L', T I ON: Berezicheski-y stL,'--ollnyy zavocl (Berezichi Glass *,iorks)
Card 2/ 3

"0=,r,ri Salt - :- Good kccelerator of Gia33 14,,ejtjyj~ 3011/ 72-58-7-12/19
1. Glass-Processing 2. Sodium chIcride-Applications 3. GIass--P--o-;e--t]'.=s
4. Glass-Test results
~;Urd 51 5

- .-- -
Operating glass furnaces with an increased heating area.
Stek.i ker. 17 no.4:35-37 Ap 160. (MIU 13:8)
(GlaBB furnaces)

SMIRNOV, V.P.
Yearly output. of double side-fired tank furnaces. Stek. i ker
17 no.8:35-36 Ag 160. (MIRA 13:8)
(Glaos furnaces)

S'm1j?IIOvIj--VI..1".. ----
Tank furnace for making
ker. 18 no.2:12-14 F
(Glass furnaces)
colored and superimposed glaos. Stek. i
161. (1,1DRA 14:3)
(Glass, Colored)

5mi"imm, v P.
Decorating glassware by printing a desicm a or-n"n:r pla-
t~
stek,~ i ker. 19 no.2:)5-36 F '62~ ( I j -. 3 ),
(Glassware)

S~LT'13GIV) V.P.
Manufacture anc, preparation of glrxs~, ir.-clds. Stek. i ker. 22 no.4:
3P-4C An 16:. (MIRA 18:5)

CHERKES, L.A.; STRUKOV, A. I.; VOLGAREV, M.N.; SMIRNOV, V.P.
Cirrhosis and tumors of the liver in choline and protein
insufficiency. Vop.pit. 19'no-1:3-16 -Ta-F 160. (MIRA, 13-5)
1. Iz laboratorii patologicheskoy fiziologii (zav. - prof. L.A.
Cherkes) Inptituta pitaniya ANN SSSR i iz kafedry patologichesk:6y
anatomii (zav. - chlen-korrespondent ANN SSSR prof. A.I. Strukov)
I Moskovskogo ordena Lenin& meditsinskogo instituta imeni I.M.
Sechenova.
(LIVER NEOPUSMS experimental)
(LIVER CHIMOSIS experimental)
(CHOLINE deficiency)
(PRCTICIN deficiency)
(N"RITION DISORDIRS experimental)

S'IIRNOV, V. P.1-Cand. Medic. Sci. (diss) "On Question of
Primary Cancer ol' Ll rcr (Clinical-anato.7-1cal and -ExMerimental
Investii-7atlon),ll Moscow, 1961, 16 pp. (Acad. Med. Sci. USSR)
250 coples (KL Supp 12-61, 288).

SMIRIIOV, V.P.
Experimental tumors of the liver in protein-choline insuffidiency.
Ar-kh. pat 23 no.2:51-59 16-1. (YjrA 14:2)
iLIVERS-TUMOM) (PROTEINS) (CHOLINE)

C C
t a -k a rr ~7 srir~n,4o~n
o :,,I na
Tien., Suctit-Ilova.

SMIRNOV, V.P., dotsent, kandidat tekhnicheskikh nauk.
htx-
Comparative characteristics of ash washing units used for low and
compound pressure hydraulic ash removal In heat-power electric plants.
[Trudy-] MVTU no.15:90-135 152. (MLRA 8:5)
(Steam power-plants) (Ash disposal)

SMIRNOV, V.P., kandidat tekhnicheskikh nauk, dotsent.
Adjustment and testing of the VS 175/210 type of ash-sluicing
apparatus designed by V.P. Smirnov for periodical sluicing In
hydraulic ash removal systems in thermal electric power plants.
[Trudy] MV7U no.59:88-108 '55. (MLRA 9:5)
(Ash disposal)

SMIRNOV, V-P, kandidat tekhnichaskikh nauk, dotsent.
Adjustment and industrial testing of the experimental VS-3,0
continuous sluicing apparatus designed by V.P.6mirnov for hy-
draulic ash removal systems in thermal electric power plants.
[Trudy] KVTU no-59:109-123 '55. (MLRA 9:5)
(Ash disposal)

SMIRNOV, V. F.
"Electrospark Strengthening of Cutting Tools," AvtomobilInaya i Trak-
tornaya Promyshlennost' (1950) No 12, PP 17/20.
B-73331, 1 Apr 54

SMIle-luv, V. P.
"'Mectrolytic Depo2ition of Aljoys on a Copper 3-ase for Protect ive-Decorative
an-A, Technic!,l Purposes." Sub 5 Mov ~l Krw Inst of Nonferrous Metals and Gold
im.eDi U. I. Kalinin /Cand. Technicil S~i. .
Diss-rtations presented for science and engineerIng derrees in Moscow durin,,-, 1951.
SO: Sum. No. 48o, 9 MaY 55

Sm-mov, V. -1 .
Electric Srark,
Toucrhening died: b-, m
, eans of an electric spark. Avt. trakt. prom. No. 1, 1952
Montbly List of Russian Accessions, Library of Congress, June 1952 Uncla5sided

I t I ~ (" , .
.II
SMIRNOV, V.P.-. inzh.
Building up electrodes by electric are in a nitrogen jet. Mushino-
stroitell no.1%24-25 Ja 158. (MIRA liti)
(Electroplating)

3~1%157 4/61/000/004/'002/009
B108 138
AUTHOR:
TITLE: Semi-classical approximation in band theory
.PERIODICAL: Leningrad- .'. Universitet. Vestnik. Seriya fiziki i khimii,
no. 4, 1961, 35 - 38
TEXT: The author considers the uniform motion of a particle in a periodic
potential field:
(_ d' + V(X qr(x) = EYW with V(X 4- a) = V(x). Functions correspondinE; to
dx2
an allowed energy level have to fulfill the boundary conditions V(a) = Xv(O),
J..-I(a) =Xy'(0) where IXI = 1- This problem is solvedin semi-classical
approximation within one elementary cell (0,a). It is assumed that E< V MaX
(Fig. 1). The domains I and II are interrelated by the formulas
Card 1/4

S/054/61/000/004/002/009
Semi-classical approximation... ~108'/B138
X
q 2 exp qdx' 2p 2sin pdx' +
4
X, (3)
X,
q exp qdx' P c os pdx' + 4
(S
and the domains III and II by
L
q exp qdx') - 92P S111 Pdx'
XX Q
__I X L (4)
q Ir exp qdx' P 2 cos (r'pdv'_L
X
1/2, V(X)> and p ft - V(x)) 1/2 V(x) < 6. By linear
here q (v (x) - e )
combination of these ex~3ressions the author obtains the transcendental
Card 2/4

S/054/61/000/004/002/009
Semi-classical approximation- B108/B138
eauation cos 3.ch(4 + ln2) = cos ka f(E) where
X2
,.3=r f pdxl. The effective masses are determined by two-fold differentiation
of the above transcendental equation. Parameters b and c are introduced:
d 2
+ bV/*
_:L) -V(x) = F,,V(x). The depth of the*potential well is
c
dx2 1kc
proportional to b, the lattide constant is proportional to c. The number
of bands in the potential well is calculated as
V.I. -V (x) d_~ 4- arccos 0,8 (13).
The author thanks Professor P. P. Pavinskiy for discussion. There are 2
-figures and 3 references: 2 Soviet and 1-non-Soviet.
Card 3/4

S/054/61/000/004/009/009
,9 4f, B102M38
AUTHOR: Smirnov, V. P.
TITLE: Effective mass calculation in band theory
PERIODICAL: Leningrad. Universitet. Vestnik. Seriya fiziki i khimii,
no. 4, 1961, 149 - 151
TEXT: A relation derived by P. P. Pavinskiy (Vestnik Leningr. un-ta,
v(l)-du(l)
no. 10, 1961), M/M -d dx, (1), is used for variational
1 = 1 - 2 * x
calculation of the effective mass m*. The problem is solved for one-
dimensional motion of a particle in a p'eriodic field V(x), with period a.
The extremum of the 1-th band is assumed to be at k = 0. Integration
is carried out over a unit cell, u(") is-the normalized wave function
at the bottom(or ceiling)of the 1-th band and v(i) is a periodic func~iqn,
satisfies the relation A(l)v(l)=.('- d2 )v(') = 2 dukl)
which 2 + V(x) - "i dx
Card 114 dx

S/054/61/000/1004/009/009
Effective mass calculation... B102/B13B
where is the energy at the bottom cei of the 1-th band. With
r n) iM
1-1 Idu dx
dx (n)
v v + v v 2' 13 (n = 1,2 ... 1), and
1 2 1
n=1 --n (l)-du(l)
V2 can be determined from the condi'tion I (v2 2 v2 2dx,
which.gives the minimum of V2 in the subspaces- 2 in which the
operator AM is positively definite. For the bottom of t'he band (l = 1),
this minimum is given by I(v(1)) = -% - 1, from which the effective mass
mi
can be determined. A similar method can be also used in the three-
dimensional case, provided a relation analogous to (1) holds and the
I-th zone had an extremum at k = 0 and is not degenerate at this point.
The periodic amplitude of the wave function satisfies
j)24_ V (9)
r k r
and for small k
Card 2/4

S/m/61/000/004/009/009
Effective mass calculation ... B102 B138
+ k~k~ WM
k.t
it UM +
+ Y, Ar.k~rn
E, (V ~ : (;F ) ~*
uations the tensOr Of the reciprocal effective mass,
hold. From these eq
1 can be determined,
m + w] d;.
M~i.)
in,
If the coordinate axes coincide with the principle a*xes of this tensorg
in 1~2 d; (16)
(nit it")
(L. 2 V..M
M,)
Card 3/4

S/054/61/000/004/009/009
Effective mass calculation ... B102/B138
re~~ults. The author thanks Professor P. P. Pavinskiy for discussion.
There are 4 references: 3 Soviet and 1 non-Soviet. The reference to the
English-language publication reads as follows: T. Bardeen. Chem. Phys., 6,
367, 1958-
t
Card 4/4

31985
s/142/6i/oo4/oo4/oo6/ol8
E192/E382
AUTHORS, Bobrovnikov, M~.S.., Starovoytova, R,P, and
Sti,iirnov ..-.V. P.
TITLE- The efficiency of excitation of surface waves by a
lumped source on an impedance plane
PERIODICAL,-. Izvestiya vysshikh uchebnykh zavedeniy,
Radiotekhnika, v. 11, no~ 4, 1961, 432 - 438
TEXT~ The problem of lumped excitation of an infinite
impedance plane by a magnetic current filament is considered.
The plane has an isotropic impedance and represents the simplest
delay system. The impedance plane, t-rhose surface coincides
with the coordinate plane y, z (see Fig. ill is excited by an
infinitely long magnetic current filament j ~ which is
parallel to the axis y ~ vrhich is situated at a distance x 0
from the impedance plane-; t hus'-
m = IM6(x - x0)6(z)
Card 146"i

31965
S/142/61/oo4/oo4/oo6/ol8
The efficiency of F,192/E382
where x = x and z = 0 are the cQord:Lnates of the source, and
0
1m is the amplitude of the source,,
Under these excitation conditions only the three field components
are produced, namely - E X~ Ez and H y . The component H y
can be found by solving the Maxwell equations, while the other
field components can be expressed in terms of H . The
y
boundary condition at the impedance surfacce is~-
E1z = Z HY/x=o
where Z is the surface impedance., It is shown that the
surface-wave component of the magnetic field is given by.-
Card 2/1~'

g98
S/142/017COV004/006/013
The efficiency of .... r,-192/E382
(__2
Jm2 k F
C + A-d (I Q,,)n (kx.)n'~_'_
n-I
I-) I Q
2)1,,-.,(2k x,) -I, (2kx,) it --_ - - -I- ____
1-4
I VvIl 21t - 1
where Z -iQ By anaLyzing the above formulae (-and
comparing the results with some experimental data) it is
concluded that a plane electromagnetic wave iiapinging on an
infinite uniform impedance plane does not excite surfz,.ce wave,
On the other hand, i%rhen the surface 't-,raves are e.-.:cited by a
lumped source, the efficiency of excitation depends on the
delay coefficient P = h 0/k and the distafice of the source
from the impedance plane. An optimum height for the source
I
above the impedance plane can be determined for every given
value of Thus, for example, for P = 1.25 tile iii-triiest
Card 4/~-

S/142/61/004/00VOO6/018
The efficiency of .... E192/E382
efficiency of n = 0.981 is reached for x 0A = o-16. The-,
excitation efficiency near to unity can be achieved for
compratively low values of the delay coefficient 1-05
1.2).
There are 5 figures and 6 references: 2 Soviet-bloc and
4 non-Soviet-bloc. The four En-lish-language references
mentioned are: Ref. 1 - A.L. Cullen - PIEE, 1957, C 104, no. 6,
237; Ref. 2 - G.I. Rich, PIEE, 1955, B 102, no. 2, 237;
7
,Zcf. 3 - A.L. Cullen, PISE, August, 1955, 101, 4, 225 and
Ref. 4 - I.W. Dunkan, IRE Trans., 1959, MTT-7, no. 2, 257
ASSOCIATION: Kafedra radiofiziki Tomskogo gos. universiteta
im. V.V. Kuybysheva (Department of Radio Physics
of Tomsk State University im. V.V. Kuybyshev)
SUBMITTED: August 28, 1960 (initially)
November 3, 1960 (after revision)
Card 5/6'

SI4IPjIOVyV. P.
Effective masses of an electron moving in a periodic field.
Vest LGU 16 no.16:34-39 161. (MIRA 14-:8)
(Electrons)

-3.760
s/i4g/62/005/003/001/009
E192/E382
AUTHORS: Bobrovnikov, "...S. and
TITLE: Field in the near zone of the source for the case of
lumped excitation of an impedance plane
PERIODICAL: Izvestiya vysshikh u_chebnykh.zavedeniy,
Radlotelchnika, v.-5, no. 3, 19G2, 321 - 325
T EXT The _-eneral e.-:pression for the magnetic-field
coi-.1ponentH for the case of an infinite impedance plane w1iose
Y
surface coincides with the coordinate system yz (See-Figg. 1)
and is excited by a mag-netic -current thread j n , situated at
a distance x 0 from the impedance plane and parallel to the.
axIs y is in the form (Rcf.- 1. The authors and II.P.Starovoytova,
Izv. vuzov SSSR - Radiotelchnilca, 1961, V.3, no. 4, 432):
Card 1/ 4

Pield in the zicar zone ....
s/11,2/69-/005/003/001/009
E192/E382
f iKZ
m oo ~cos x,v - - sin
2KI v 0 ei". eihz dh (1)
y c v + KZ
<
ixZ
os xv sin xv
i,-
y 2-!:j v a -1c0 eiliz. dh
v + xZ (2)
0 <
N" 0
Card 2/4

S/142/062/005/003/001/009
Field in the near zone .... E192/E382
where !M is the amplitude of the ma_cmetic curr ent
= VI~2 _ 112
Z = !Q is the reactive impedance and v
T`ae radiation field and the surface wavo for the far zone in such
a 'Ref. 1. HOITOVer, Cqs. (1) and (2)
system was determined in
,
can be also used to determine- the field in- the near zone. The
field is given by the Sencrdl expression:
1-1 = Hr-I + A
y y
L
ihZ
e dh
v + EZ
(0")
whore t1ic first coauponent rc,3resentsthe surface wave, -i-thilst-
t1ie second component ,ives the non-surface wave. The integral
can be evaluated comparatively easily and it is shown. that the
non-surface wave is appro:~cimately _--iven by:
Card 3/4

Field in the near zone ....
T'r
il:z+ir,
H e
y 0
s/14 2/6 2/005/CO5/00l/G_-9
E192/E382
WI)
Q~ -F2W, ~ Z 1'.Z
This shows that in the case of lu7jYj3d excitation, the non-
surface wave decreases as 1/(KZP - , i.e. faster than for the
case of hu ideally conducting plane. The non-rurfacc ';.,ave for
the near zone was calculated by a di-ital com--,uter and the
results are given in a figure. Therc are 4 fiZures.
ASSOCIATION: Laboratoriya radiofiziki SFTI pri Tomiskom
gos. universitete im. V.V. l,.uybysLieva
(Radiophysics Laboratory, SFTI, of Tonisic State
University im. V.V. Kuybyshev)
SUBM'ITT ED: Julie 5, 1961
Card
;Y~

S/0:-,-8/6 2/000D/006 / i 0 5/136
r? A06 2/A 10 1
Jml..nov Vj
r ~- c. v i r y a4,ra m Z c. ioriz --)n t..3 jIni, a r. r e nna s
--C! T-1 7t CA L ZhUrnal, Fizi,ka, no. 6, !(J62, 16, abstract 6Zh113 ("Tr.
in-.ta T,~mskom un-ve". 1960, no. 39, 72 - 76)
~_s ar- wlvr-n -a _:~t-~idy .--If arrays ~f ring antennas, consisting
-n tf -a~ - rry , an equal amplitude
I v r -3 vit-i _~r~, In which the cu. --nT. has
'Q~- Lhal- '_~'an;Z~ I.; 2,,r ai-:qng the circle on which they am arranged. An
f.-Ir the eleotric field intenSity of two vibrators arranged
a D g r ,.e r . The curren!~ -tn the vibrators is distributed accord-
law, i is -,,h,= number cX wavelengths that can be placed on
to ~_n rr,_~
-n,- irzl~ on which v,brat,.~rs are errang, d. Direettity
diagrams are calculated
It is noted that the directi-
0-4; 0.5; 1,0~ 3.00,
0,
v i W, ra i r-, i ic h iI I the Circ"lar' e (Emin/7max 7) can be obtained
vilb!-T-rs, Ced in phase -pposition, When increasing the length
-n vihich t1l.e vltrat,)vs are ar-i-anged, the directivity diagram
jj_
2-

FELIDSHTEYN, A.L.; SKIRNOV; V.P.
Characteristic impedance of a rectangular wave guide. Radiotekhnika
18 no-4:78 Ap 163. (MIRA 16:5)
1, Deystvitellnyy chlen Nauchno-tekhnicheskogo obshchestva
radiotekhniki i elektroavyazi imeni Popova.
(Wave guides)

ACCESSION NR: AP4040750 S/0142A4/007/002/0171/0179
AUTHOR: Bobrovnikov, M. S.; Mironov, V. L.; Smirnov, V. P.
ITITLE: Excitation of surface waves by a discretely-distributed non-
'projecting source
SOURCE: IVUZ. Radiotekhnika, v. 7, no. 2, 1964, 171-179
TOPIC TAGS: surface wave, directional patt-ernt antenna configura-
tion, antenna directivity
!ABSTRACT: An analysis is made of surface-wave launchers consisting
!of several arbitrarily spaced parallel unphased magnetic-current
filaments imbedded in an impedance plane. The efficiency of surface-I
;wave excitation of such a source is compared with that of a concen-
!trated source. The amplitude ratios and phase relations at which
;no surface waves are excited, or at which the launched surface waves I
,propagate in one direction only, are deterinined analytically. It is
, Card 1/2

:ACCESSION NR: AP4040750
shown in particular that in the case when there are only two current
filaments, the surface-wave-launching efficiency exceeds that of a
;concentrated source, and that directional launching of the surface
~waves is possible if the currents are properly phased. Orig. art.
1has: 10 figures and 16 fomulas.
:ASSOCIATION: None
7SUBMITTED: 06Dec62 DATE ACQ: ENCL.: 00
iSUD CODE: EC NR REF SOVz 001 OTHER:* 001
Card 2/2

T, 25751-65

ACCESSION NR: AP5002039

ans.
cou ling systems (IRE Tr
p
19 jv' noi-
-6 573).
8 figures and 34 formulas

-ATION: none
ASSOCJ

SUBWTTED:. 18Mar63 ENCL: 00

UB CODE EG
NO REF SOV: 00

THM., 00Z bb.

i

Card 2

an ,n,,,edance Cylinder 'n an
L'a
~rq.,edcirce :" - -agnetic cur-rent loou coaxial to the impe-
. Lane rjy am -
Cylinder, Radiotekh, i elektron. 9 no.10:1812 ILF20 C It-,4;
4

BOBROVNIKOV,. U..S.; GOSHIN,,' G.G.; SMIRNOV, V.P.
Effective excitation of radial cylindrical surfEbb ,mves.
Radiotekh. i elektron. 10 no.6:1023-,1028 Je 165.
(MA 18.-6')

SMIPWOV3, V.P. I
Excitar-ion of su-rf--ce waves. Iz,.r. vys. ucheb. zav.; fiz. no.5: 4'
182-184 '63. 0%9-RA 16,12)
1. Sibirskiy fiziko-tekhnicheskiy instuitut pri Tomskom gosudarst-
vennom universitete imeni Kuybysheva.

FELIDSHTEY111, Aleksandr LIvovicii; YAVICH, Lev Raftielovich; SMIRNOV,
_'V . a14. -Tetro ich: PE?EKS, red.; B1JL'DYA.YEV-,-TT-.A.'__ _"
.it I
tekhn. red.
[1-:anual on the elements of waveguide technology] Spravochnik
po elementam volnovodnoi tekhniki. Moskva, Gosenergoizdat,
1963. 359 P. (MIRA 17:2)

SMIRNOV, V.P., izzhenar, rodaktor; nVZNNR, A.S., redaktor; TOKIR, A.M.,
'-teklmichenkiy rodaktor; SMOL'YAKOVA, M.Y., tekhaicheakiy redak-
ter.
(Fire prevention norms In planning the constructiox of lumber-
yards] PrOtiTopozharnye nermy stroitallnoge preektiroyaniia
skladev lesnykh materialOT (N129-55). Moskva, Ges.izd-Te lit-ry
pe stroit. I arkhitekture, 1955. 24 p. (MLRA 9:6)
1.Ruesia (1923- U.S.S.R.) Gosudarstvonnyy komitat po delam
streitellstv&.
(Fire preventioa-Laws and regulations) (Dimberyards)