SCIENTIFIC ABSTRACT ZHIRNOV, D.F. - ZHIRNOV, V.A.

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
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• Sequence Number: 6
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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AUMOR: Zhirnov., 061

ITLE Low-level Bombing.Attack by a Flight (Bombardirovochnyy.
udar zvena s maloy.vysoty)
~PERIODIGAL; Xestnik yozdushnogo flota, -1958.. Nr 8., pp 16-25:(USSR)
ABSTRACT: The author,describes~in detail a map exercise carried
out by A~bomber squadron. The subject of the exercise
wast Combatactions by'a flight from low altitudes un-
der unfavorable weather conditions in daytime against
the launching sites of guided missiles. The map exer-.
cise,Xas preceded by a lecture from which the following
couldbe leavned:~Since the firing platforms of missiles
at a launching site are located at considerable dis-
tances from.'One,another,, they should be aimed at and
-hopping alti-
bombed..individually from a low or hedge
-tude,, usually with.the aid of an optical boLmbsight. The
types of:bombs.that could be used are: demolition bombs
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32 (1) SOV/84-59-10 36/53
~
-AUTHOR.- Zhirno i
V, N# E,ng neer
TITLE: Without the Intermediaries
.~..PERIODICAL::'; Grazhdanska~& aviatei Nr 10, p 26 (USSR)~
ya, 19590
ABSTRACT: The.author advocates thelelimination of the post of
airport radio operator which, in his opinionj is an
unnecessary'intermediary between the dispatcher and
the aircraft, and describes how the Rayonnaya dis,
petcherskaya sluzhba',(.R&y6n' '. Dispatcher Service)
operates.at Rostov airport without radio opera 'tors.
The.first dispatcher who began to work.without radio
operators~.wasl. Parafonov. His idea was supported
by the chief-.'of,URDS, I. Isayev, the deputy chief
of airportfor traffic operations, N..Kuzneteov,'the
chief dispatcher of RDS, P. Rubtsov, and the dispat-
cherT. Karaichev. Traffic is registered by the-MAG-
8 magnetic tape recorder, automated by a method Bug-
ge8ted by the technician.V. Shustov, and further im-
proved by the technician M. Kharchenko. The automat-
Card.,1/2 ed tape recorder operates only-during reception and

Without the Intermediaries. SOV/84 59-10 36/53
transmission,,,, When it runs'out of tape, or when the
tape~is torn, At is automatically replaced by a
reserve tapprecorderv ~A one-km long tape is used?
~n,one_day on short-wave, and-in 2
days on ultra short-wave channels. Efficiency ex-
.,perts.are now,trying to further improveAt so as to
make it capable of registering the beginning and the
end of a.contact, i e. register three time elements
(hour-minute-second~...: The 6-channel tape recorders
are located near the command dispatcher point..
'The remote control desk SKT-2 has been reconstruct-
ed so as to facilitate.the dispatcher's operations,
The.dispatcher has direct loudspeaker c8nnection with
the ADP, radio office and,transmitting center. The
KV-M radio receiving sets have been replaced by those
ot KIT,type. The example set by'Rostov airport has
been followed.,by.Stalingrad airport, and by the'ex-
tended ADS zone of Minerall.nyye Vody airport. There.
is 1 photograph.
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Sub~ect USSR/Engineering
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'Pub aio-a - 6A6.

uthors I and,'
0'.4 . Kdt --A, At" KAnds of Tech, Sci,
:,_Zhirnqv$
Title: Contihi6~i- ~blc4dbwn. from ~.high-p .ressure boilers Into
-p
the drtims'otmedium ressure boilers

Periodical
t -',TePloenerg_,e_tikap,',, 3... 2312L. 955:
Mr I
aiAthoi~s.-.~i~'~edti'gat~i'd"-~th6 'problem at-a poWer, station

ppe'd wi th: both do of boilers, They describe the:
6qui kin

dedonoefitjMtor-py tem, sed which consists of throttle
u
0
'valves placed in the'blowdown pipes of,every high-
pressure, b.oiler* These pipes are, connected with a
main,.pipeline.leading the"discharge Into the mediust-
~.-,,pressure boilers,-,-This'system was found tobe much
-blow-down Into the atmosphere,,
more economical than the
and also greatl y reduced scale formation on turbine
blades, The au thors present detailed analytical
calculations 'of the extent of the economy obtained, They
recommend the application of this system in other
power stations, -Three drawings.

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TITIS on the Pro
bleN of the Quasi-Classioal One-Sleotron
-
?unotions
W voprost, o kvaziklassioh eakikh odnoelektr
onnykh
funkteiyakh.'- Hussian)
PERIODICAL Zhurnal,lksperim.' i Teoret. Yiziki 1957, Vol-32p Ar 5,
pp'1252-1254~(USSR)
ABSTRACT The,matri;F elements of.different interaction prooesseis-
of matter.with the radiation field are estimated with the
aid,ofthe hydrogen functions or of the Slater's functiohs.
But.the results thus obtained are unreliable from a quanti-
tative point
of vlow.p as these,funotione either do not
,
consider at,all or consider onl' very incompletely the
y
influence upon the' radiating electron from the part of all
the other electrons ofIheatom. The authQr of the yaper.~
under review construed,approximate wave funotione for.aA
electron in bound state's taking-. into account the sariiiiing
influenoo,of'the ele'otroetatic interaction-ofthe &t6kie
61ectronsupon the radiating electron, The basio-.0oncept
of these computations is the combination of the statistical
method devised by Thomas-Fermi (for the computation of, the
effective electrostatic field acting upon a singl6 eleotron
CAIM 1/3 in the atom) with a generalized quasiclasaical method for

on the Problem of the Quasi-Clasaical One-Sleotron
Punotionso
the computation of~the ways funotions,in a giveir potential
field. The effective electrostatic field aoting,upon the
radiating electron is described in this context.by a
Thomas-Fermi potential with corrd'otions for the great and
small distances.from the nucleus. Because thisfield U(r)-
is a centrally symmetrical field,~the eigeifunctior~l have'
the same angular dependence as in the h arogen'atom.
.,Therefore the problem is reduced to the computationof
the radial funotiona I al (r) f rom',t~d ..,equation
r /dr 1' +1 /r2j
d :~nl Cul
ni
al n1
The'solution.of ~this equation is found with the aid Of
the quasi-olassical method,in Its generalized form dbyioed
-by:Fok and'Petrashen"S Foi'the approximate sigenvalues of
the energy L nl- a farmula,ia given. The paper under review
contains the computations of the energies of the atoms AC
and In-for the states -199 2al 2po 3're bi 3d.
and :4.p, as
well as of the Gd-atom~fbr the states 3PP 3d, 4P'and 4d.
CARD 213~ The energy.levels as computed here are in satisfactory

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51-'4,-2-2/28
AUTHOR: Zhirnov, 'N-. ~~I.
~TITLE:- Qia a ic la asical, "Single -Electron Functionslo Bound
States., 1 (0 kvaziklassicheskikh odnoelektroanykh
funktsiyakh. I. Svyazanny;,esQstoyaniya.)
PERIMICAL. Optika I Spektrosko i-Ya, 1958t VoI,IV, Nr#2v PP-125-137:
p
(UBSRY
.
ABSTRACT: In'1939 Petrashent,~(Refol)-following Fock's idea .(Ref.2),-,.
developed a'- comparatively simple method of .,dalculatida
-
:iave-fufictions.
of approximate, (WKB type-) single-electron
This method, made it possible to take into account,the:-
screening of-the niielear field, as well as -the 'exchange.
interaction of electronsin an atom. later the same
raethod :was, reported, by Miller'and'Good (Ref-3)-~ In'the:
present-paper the Petrashenl.-Fock method wasapplied to
calculation of~':radial functions of electrons in bound
states taking into account this soreening iffect of the
electrostatic field of atomic electrons on the radiating
electron. The'calculations are based on a simultaneousi
application,of.the statistiral Thomas-Fermi method (Ref.4)
for calculation':of the effective electrostatic field which
Card 1/3 acts on a single electron in a heavy atom, together with

51--49F-2- .28
On Quasiclassical Single-Electron Functions, If
the, quasiclassical method'of calculation of vave-functions
in a given, potential field. Thia-author used a Thomas-
Fermi potential, corrected at both short and 'long; distance B
from the nucleus The author calculated single-electron
siclassical rLial wave-functions for the 1s, 2s, 2p
ua
q
3ps 3d and 4p~states of silver and indium atoms.
These wave-7functions were used to calculate the relative
intensities:of the K-series lines of X-ray spectra of
silver andIndium. These intensities are given;in Table
4.' Satisfactory agreement was found between the
,calculated values and theexperimental data of RefS.10
and:11. : The author developed a method for an approximate.
repre sentation of-the quasiclassical single-electron.
wave-ftunctions in an analytic form. The author concludes,
that using the PetraBheul-Fock method we can find
approximate-single-electron functions which take into
account field structure in complex atoms, without
numerical integTation of the SchrIldinger equation. Even
the approximate'radial functions obtained on the basis
of the rather coarse Thomas-Fermi model allow us to study
Ca rd. 2/3 in a fairly precise manner some of the processes in more

51--4r 2-2 28
AUTHOR: Zhimov, No: I.P.
TITLE: on Quasiclassical'Single-Blectron FUnct ions II
:Continuous Spectrum States. (O.kvaziklassicheskikh
oelektronnykh funktsiyakh. II. Sostoyaniya
dn
o
nepreryvnogo spektra.)
PERIODICAL: Optika i Spektroskopiya.- 1958., Vol.IV, Nr*2t pp.138-143
(USSR).
ABSTPACT: Using the, method described in Part I (Ref.11 seethe
preceding.abstract) the author calculated.quasiclassical
single-electron radial wave-functions for electron
states in a continuous spectrum. The results were
obtained by solution of the radial Schxddinger equation
for an electron in:an electroiitatic Thomas-Fermi field.
It is shown'that at sufficiently high positive energies
-theradial eigenfunctions of an electron differonly a
little.from,the, corresponding hydrogen functions. The
paper is entirely theoretical. There are 1 table, and
5.references of which 4 are Soviet and 1 American.
A&;OCIATION: Moscow,State Pedagogical Institute imeni V.I. Lenin
(MOE;kovskiy gosudarstvennyy pedagogiche skiy institut
13ard 1/2 imo VOI. Ienina.)

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1,222-66 W(l) IJP(c)
ACCESSION Mi: AP5017M8 WV0051/65/01q/oe1/boo6/ooi1
AUIROlts 7-hirnov, 539-192
TMUS on -the 'true nature of ihe Fqfterg-Xlein-Rees method
SOURCE: OPMA I spektrookoplyap Y. 19.. no. 1.. 1965., 6-U
TOPIC TAM t molecular spectroccopy, diatomic moleculep quemitux oscillAtor
1ABSTRAM The purpose of this paper was to determine why the Rydberg-10.01n-Rces
(RKR) method for constructing potential energy curves for diatomic molecules
quasi-optical data leads to excellent results In regions Wfiere use-
d t
ful If It Is assumed that the method is quasiclassical, and to pcorer results in
regions where the condition of quasiclassical motion of the owlecules iv more validt
To this end, the author proves that the RKR method in real-ij a ccnnequence of the
generalized WKB method, not of the usual WKB method, and correapcadv to the case
where the vibrational proper-ties of a diatomic molecule are ftpproxI mated by using
the anharmonic Morse oscillator. Since the RKR Is thus not a qua-siclasoical meethodp
there in a necessity for further improving it by chooning a poterrtIFU ithoce asymp-
totic behavior In closer to that of the true potential ciu-". 07-1g. art. has: 19
formulas.
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1ASSOCIATIONC tione.J~,
SUBMTTED ENCLI 00 OUD com I OP
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24~05-66 ENT(1)/T IJP(c) AT
ACC NRt AX=60 SIXECE CODE: UWW51/6C/C),--)(,,/(-02/0'd!24/OL~29
AVTHOR: 'Zhirnov., N. I.; Vasilevskly, A. S.
ORG: none
TITIE: Application of the generalized WKB method to the study of the vibrational-
rotational spectra of diatomic molecules. I. Vibrational- ratational. spectrin of a
Morse oscill or
-SOURCE: Optika i spektroskopiyap v..20., no. 2) 1966j, 224-229
_'_.-TOPIC TAGS: molecular spectrum, vibration spectrum., approximation mothod, ]Wdrogen,
oscillator, perturbation theory
ABSTRACT: The authors p:~q e.& simpler method for calculating vibrational--rotational
poo_ - -
energy levels of diatomicfmole es, using a generalized M method in a fam close to
that previously derived by one of the authors (Zhirnov, Opt. i spektr. v. rr, 643,
1964). The ground electronic state of the hydrogen molecule is considered as an ex-
ample, under the assumption that the actual potential curve of the molecule can be
sufficiently accurately approximated by a Morse potential function. The vibrational
rotational levels thus obtained are compared with the existing experimental data and
with the results of the calculation by perturbation theory methods. The calculated
results are systematically high by roughly 100 em"I compared with the experimental
values. The causes for the various discrepancies are briefly discussed. The authors
thank A# N. Zavaruyeva for assistance with the numerical computer work. Orig. art.
1 table.
has: 22, formula& and
~
DATE 07Dec64/ ORIG PJW: 00 OTH REF: oo6
Sim
In . . .
42.00
Ed

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S 1JRMC01YE-.- /0 3T/ 610W1006 1 ra
AUTHOR: Z-hirnoy N
Io kovskiy p6d;ns'*Iut)
s
ORG: Moscow Pedagogical Institute m' V. 1. Lenin (M
Penetration p a
TITLE rob bility of a potential barrier in ~an approximation of the
generalized Wentiel-Kramer6-Brillouin method Part 2, Symmetrical,barriers
1J SOURCE:IVUZ. Fizika,~ no.~,6,1666~ 101-107
TOPIC TAGS: potential 1~arrier, approximation method, approximation
solution, enctration coefficient Wentzel Kram ers Brillouin method
P
.,ABSTRACT:, This study was undertaken in an, Attempt to eliminate the drawback
~of the approximate method,in.computing the penetration coefficients through one-
dimensional potential barriers (N.- 1. Zhirnov, Izv. vuzov, SSSR, Fizika, 'No. 4,
28, 1965). Such deficiency is removed in this work by superposing some com-
In
plementa'ry conditions on the base potential W(S). A new solution is given to,the
problem of the enetration of articles throu& symmetrical barriers. Orig.:art.-
P ~ . P
has: 26 formulas and 4 tab I es. (Author's abstract) Yfj~
SUB' CODE: 1. ;20 /SUBM D.AT"E:~07 J*u,165./ORIG REF:-.003/OTH REF: 002/
Lqard 1/1
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ACC NR
AP700V'34 COM
AUTHOR. Zhirnov, N#- I.-
ORG: ~MoscowStat,c Pedagogical Institutelm.' V,'T. lenin (Moqko1vSMY gwiped-
instaut)
t4on of *j-,0
TITLE: Pvnetration probability,of a potential barrier in approxima
neralized Wentzel Kram ers 13rillo'uin m ottfod Part3Asymmetrical bdrriers
ge
SOURC_E: IVUZ. Fizi-ka, no. 6,' 19616, 103-113
TOPIC TAGS: potential barrier, approximation method, particle energy,
approximate'solution, -particle motion, Wentzel kram ers, Brillouin method
ABSTRACT: The present study is a continuation f an earlier study or, th(_%
lut [o
penetration probability of a potential barrier. A new so r, is dcri,v(..d for the
~problem of the penetration of particles through one-dimensional asyrnmetrical
barriers;. the E.. -Aution is moreI pre cise than the previous one (N. I. Zhirnov, im
Vuzov, SSSR, Fizika, No.: 4, 28, 1965). The problem is discussed concernino the
limits of applicability of the generalized Wentzel-Kramers-Brillouirt method for.
C"

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com-outinLf the -.)cnetration Drobabilities of one-dimensional barriers. The anDroxi-
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Quasi-classical wave functions of Morsels oscillator and their use
in calculating Franck-Condon factors. Part 1. Opt. spekt. 15 no.
2sl66-175 'A9 '63- (MIRA l7sl)

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SUB CODE: PH
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DATH ACQ: 063op63
NO REF Sov. 008
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MRNOVO 9.1.9 kand.tekhn.nauki DZHURIMIN, S.P.., inzh. I
Operatimg peak -1(~id boLlar' PTVM-50-1 on insuts Gore khoze Moisk*
IMTRA lg"71

ZHII 0
N. I kand.tekhn hauk-
Experiment the AUrtm;ti &4j tment nd cps
JA Us a ration,of a
P
'peak-load PTV-100 water-heating bollerfor district 4eating.
Tenloonergatika. 8 no.c)t2o-~24 8t6l.'~ (MM l4s8)

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8/0~1/60/009/006/006/018
AUTHORs Zhirnov, 1, 1.
TITLEv Interpretation* of the Vibrational Spectra of
NaDhthaleneqand:its,: Deutercted Derivative
PERIODICALs OptIka.'i spektr6skopiya, 1960, Vol.9.1 No.6, pp 734-741
TEM: -The author.reportsia,newl.more accurate, interpretation
of the vibrational spectra of-riaphthalene and octadeuteronaphtha-
lene (ClOH8 and ClOD8) The. author used mainly, the experimental
'work of:Lippin,cott. and O.'Reilly.,(Ref.1). . Values of some
taken from.YeLella.4 and Pimentel's work (Ref.2))
-and the 176-cm-l'-frequency was taken,;from the paper of Person
Pimentel and Schnepp (Ref ~7) :Approximate values of interatomic
distances.and valenc6:angles'were used (a figure on page 735).
These'distances and angles allowed for the fact that naphthalene
belongs to ~the point symmetry. group D2h and,they were quite
similar to the experimental.'values reported by Robertson (Ref.8).
....The.calculated.Ifundamental..frequencibs are listed in & table on
pages. 739-71FO The results obtained by the present author are
I lis te(.L In columns. 4and :those obtained by Lippincott and:
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Qaasi-Classical Solution,of.the,Radial 7697.7
Dirac Equations sov/56-37-6-;-17/55
-The methodwas developed forthe representation
_ .~of the approximate solutions in nalytical form.
a
The obtained approximate'single-electron functions
are continuous :throughout the entire region of the
change in the field. Therefore, there.is no need of
establishing.the special coupling equation as it
is'necessary by the Young-Uhlenbeck method (loc.
cit The,equation of eigen values during the transa--
for~ation Into.nonrelativistic approximation coincides
w1th.the
quantification rule of M. 1. Petrashen
,
(Doklady.Akad. nauk SSSR,, 50,147, 1945;-Uchenye
zap. Leningrad gos.~ univ., Ser. fiz.,, 7, 59.P'~1949).
: .~The shortcoming of the developed method lies in the
uncertainty of the magnitude of the error introduced*.

by the approximation of'
the wave function. However
this~error is considerably smaller than is the
case with the.equations of Young-Uhlenbeck and"R. HO
Good (Phys. Rev., 90, 131,~1953)- As an illustra-
tion, the~derived equations were used in the calculation
Card,3/4 of the fine',structure.of M term's of the Hg atom includ-

SOV'/96-59-7-9/26%
AUTHORS: Zhirnov,~N.I 'and-Krol ,..L Bi,.Candidates of Technical,
8 V. .,and Sh-chedrin, F.B.. Engineers
TITLEs A Large.Peak-load,Boiler House for Rational Heat. Supply. i
to Urban.Districts where Extensive Housing Conetruc ion
t
is qoing (]Kru pnaya pikovaya kotelInaya dlya':
ratsionallnogo teplosnabzhoniya rayonov massovoy zastroyki
dov)
go-rP
-PERIODICALi 2eploenergetika9,1959., IIr 7 P'P 36-41
USSR)-,
''ABSTRACT&During,the-peri6d 1959-1965--there.will be a Vreat deal of
-new housing cofistructlon*~in'~' 'a`~ number of towns, The supply
of heat;t6; such housing presents a number of.problew. _ The
provision of individual.boilers for each house is expensive
and.wasteful. Existing'designs of.regional boiler--houses
expensive and are not.well-adapted to the eventual use
of~district-heating power stations. Again, large district-
heating power.stations to supply the heat and in particular..
~to,~.cover peak loads, could not be constructed immediately,
Such stations-should-incorporate large cheap water-heating
Card 1/6 boilers to cover the peak loads, thereby reducing the cap-

SOV/96-59-7.-9/26
.A Large Peak-load-Boiler-Hoti'se for Rational Heat.Supply to*Urban
Districts where Extdnsiv6.Housing Construction is Going on
ital cost of the stations-by more.than 15%. Altho gh
suitable-boilers.'ha4e been developed by the All-Union
Thermo-4echhical~,Institute in:collabo'ration with the
~scow-Bran nergostroyl Institute, district-
.6h of the 'Orge
heating power, statioiis cannot solve the immediate problem
because theirconstruction must lag behind that of the
I-Lo.using.,,,It,was,accordingly necessary to develop largep
cheap.water-.heating boiler-houses, with peak boilers of
the All-Union-The=o-Teohnical Institute design, sited
directly amongst the housing or adjoining existing o.-
''future district-heatin,g-'power stations. At first, these
boilers will.be.-lo-he main source of heat supply; later,
when the distric~t-heating stations have been constructed,
-o-
they will be,us.ed t cover peak loads. The cos, of such
b,oiler:houses together with the heating systems is about
107.000 roubles per Ylkcal/hr of thermal output, or about
.20~roubles per square and the cost
metre of living space,
f heat produced is.abou-t 25 roubles per Mkcal/hr. which
Card 2/6 0
iqt con"'a'iderably less than With any other sort of heat

9,__59-7-9 6
A Large Peak-load Boiler.House for Rational Heat Supply to- UAan
'.Districts where Extensive Housing-Co st ction is Going on
n ru
on.Thermo-Technical Institute has
supply, The.All'uni
developed the de6iaii~for such a'peak water-heating boiler
~installation and together~with the Moscow Planning
~'Institute,has compared the economics of a number of diff-
erentl.methods of heat supply. A detailed description of,
the boiler house,is..then given,, and the general arrange-
ment is illus.trated'in Figure-1. It will contain three
water-heating-boilers type-PTV-100, each with a t~erzval
..Output of:100.Mkcal/hr, a furnace vdiiume of 246 m
.:radiation heating.surfac-9 ~f 396.7 m . a Convective.
-heating surface 'of 2 280 W, and a mean efficiency of
The thermal output of the.boiler house suffices
93
for a typi al:'distriat with a total housing area.6f
1565 000 m~, 1. For smaller sites two boilers type.--pTV-100,
or two or three si.D;ilar boilers type PTV-50, maybe used.
The boiler house is designed to burn natural gas and will
thus meet the requirements of Moscow,Kiyev ening-r
ady
Khai?kov', 'Rostov-n_u-n.o_m, LYov and a number of other towns.
Stand-by fuel-oil-burning-equipment is provided, increasing
n
Card 3/6 the.c.ost of the boiler housa by about 20%. As gas fail-
[1 4 i 1 j
71f? INN it's 111
V

SOV/1)6-59-7-9/2~E
A Large Peak.~load- B.oiler, Efouse for Rational Heat Supply to Urban,
Districts,Where.:ExtonsiVe-,Housing~Con6truc,tion:iq Going on
ure. sare not likely-to-last more than a few hours, this,
~equipment _. may prove unecessary. As will be seen:.from.
:the arrangement diagram given in Figure 2. the, station
has water-.treatment.equipment and system pumps for use
until the district-heating station is constructed.,+Later
on when the -bbile house is only covering peak loads
these accessories may be removed- alternatively, the,
corresponding,equipment in the associated district-,
heating stations may.be-smaller. De-aerators are in stalled.,
The water- 'treatment plant,ls.of the~sodium-cationite
typ*, and~'stores are provided for the necessary chemicals.
The gas and fuel--o'..l supply arrangemRnts are briefly
described. Boilers t e,PTV-100 operate on natural
yp
draught and.each,burner has its own draught fan. Tbe
on*stee"
C.Omm smoke-staok is erected on the middle boiler.
'A.central corxt-rol~panel is provided. When fuel-oil is
bur
ned speoi'al measures.are taken to prevent contamination
of the convective surfaces. Arrangements are made to del-,.
Card 4/~ iv,er caustic ma gne si t, eo r, 1 ime t othe

SOV/96-59-7_9/~22,1611
-Pea
-A Large k-load Boiler.Hbuso for Rational Heat Supply:ta~Urbaa
.,Districts where Extensiv6 Housing Constru,:ation is Going c"-
u perk
--part Jf the furnace in order,to makeA-he deposits
p
friable. the'.water returned from.the,distriet-heating
p04
system is..below the dew int Gf. the furnace it is,
~heated-by circulation of hot water. Provision is also
made~to wash'the convective.surfaces of the boiler with
-urve for
ot water4 to remove deposits. A thermal load,c
MOSCOW,,-.:given in Figure 4, shows--that'the boiler-house
will operale for only. 25 m- 30 hours per year,.with-4vhe~'Xull_.1
thermal load of 300 !Akcal/hr,, and that-the.load.would be,
above 80% for Pot-m.or 'e than 400 h *ours per year., ' During
the summer~ttheload would not exceed 60~.of the,' capacity
of one boiler~and.so this.period~can safely be Used,for
general overhaul,,, , hen, the boiler house is covering only.~
-peak loadap-its output will.still further be reduced,:even*
if,new consumers.areconnented in the meantime,
occurs it:,will,be,possible to 'use only two boilers, keeping.
the third in --eserve. It has been caloulated that thel,
::boilers willobe-hydro-dynamically stable with a water-flow''
ate diff ing from the rated value by 20%. In'the early
Ca r d 5/6- r er

BOV/96-59-7-9/26
'A~Large 2eak-load, 136i4',Ar.- ouse~ or.Rational,Heat Sup ly~ to-Vibaii
11 p
~-iiDistrict6 :where -Ext6nsiive Housing- Construo-tion is GoJ-ng ori-~
--stages beforeidll the~housing is cons'
vructed,.still
.:lower flow-rates.may-be-required and it will then~be
ne cissary to re-cir-oulate water"I',hrough the boilers
A high degree:of au tomstion will-be used and so .it-, is
expecIted.that the,.boilerhouse will be opezated by%shifts.
of three:men.ea; h. The total cost of construction of
house is aboiit
the boiler 6 4.00 000 roublea., of Which- the
r
fuel_,oiVhaadijfii t-osts 1 073-000 rouble"',
The main performance and cost data are tabi~la--ed for them
'd
new boilerhouse an forthe-old.type. XG-10, whi.c.,
muchmore.: expensivs. I' is 6xicluded 'that la-rge' peak.boil
er houses,with.water-heati g1bollers oes:PT'V-100
n ty~ or PTV,
.;50 have considerable advantages over emalller* boiler
o 'If
th se with -boiler 1
type KS-10 in respect
of both capit-al and running costs. Therefore, only boiler
.'houses,.:of, this kind sho-ul d be constructed in di.stricts
witk~-extensive new1ousing construction.
There ara~4,figures table and I Soviet ~eferent~e.
'ASSOCIATION: Vsesoyuzn" teplotakhnie.,haskiy Institut (All-Union
-1hemo-Technical

BR.AMZ-Ii-.Ye-- PARSHIM, A.A.,-. ROZXNOAUZ, I.N.; SMING,
A.
ceased]; AYZENWAT, red*; ZHMOT,
N.I.. raA-t TAR fffnV. 4-YA.- tAirlin-rad-

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ii *', . , ; , "
'ii., f'. ~4'; :t. ,
i i, p z I i w
.1 1 11 ', ::
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'AUTHORs Zhirnov, N.I.: SOV/51
TITLE s he Problim- of Interpretation of the Vibrational Spectrum cf.Coronene~
(K,voprosu ob interpretat~li kolobatellnogo apektra korousna)
NRIODIGALSOptika i Spektroskoplya, 1959.-Vol 6, Nr 2, po 162-167 tUSSR)
ens; expe
~BSTRAGT. Ext ive rimental data.on the vibrational a pectrum of co.ronene
(G24H12) are allroady,available (Refs 1-3)., Interpretation of this
spectrum ~ however, still meets.vith difficulties. The most reliable
method of determination of the symmetry of the vibrational frequencies,
based, on comparison of the Raman with the infrared spectrum, cannot be
applied bocausethase spectra of coronene have not yat been reported. The
point symmetry groupLD&-As deduced from similarity of coronouo and
benzene. Shpollskiy*(Ref 2) Pointad out that this similarity goes
further and that the strongest benzene frequencios are also present in
the coronene spectrum- :Among such frequencies are the 992 CM-1
fully'symmetrical vibrition of the benzene ring and 3070 cm'l -which
js Clos a to 3062, cm-1 of fully. a ymastrical vibrations of C--H bonds in
benzene. The presentpapar shows that this similarity between coronene
and benzene spectra ie due to the central benzene ring in coronane. 'The
conclusions arrived at are deduced from consideration or currents due
Card 1/2

.
i - -f 1! ].q : ~ !
I I , , p
I q J'j -11 I~i -1 j'~,i i,..,
1:1, ~ , . ~ t I
. !! . -. 1 ~ ." ~,, 1, 1 ,

L 13oo5-66 E14T(1) IJP(C)
AM MR; PPoOO1636 SOURCE CODE: UR/0051/65/019/006/087.'1/0873
AUIIiOR: Zbirnov, N.I.; Kronrod. L. A. 11:5
~ORG: none
TITLE:i Quasiclassical wave: on
-functi 'A~&r a Morse oscillator and their use in calcu
~Iating tranck-Condon factors. Ill. -Approximate calculation of Franck-Condcm fac-
itors on a computer
SQMCE Optika i bpektroskoipiya I v. 19, noi 6, 1965,
~TOPIC TAGS- oscillator theory, harmonic oscillator,
871-873
molecular physics, computer
'!ABSiRACT: An expression is derived for Franck-Condon factor-i by substituting oscil-
ilatory wave functions previously calculated by the Went zel-Kran*rq -Bri I I ouin method
'(N. r. zhimov, Opt. I Spektr. , 15, 166, 1963) in the formula for e lectron-vibra-
tional transitions in a diatomic molecuI2.. ne resultant integraAs are calculated
on an electronic computer with a relative accuracy of 10-7. The computer program is
described. The system was used for calculating the Franck-Condon factors for a
i-CarcIl/2- UDC., 5.119.192

L -13005-66 -
ACC NR: AP6001636
-.4number of progressions of the'second"Infrared band system in the CaO atoleculc The
:results are compared with those obtained by numerical integration. Agreement is
,generally satisfactory and the exceptions are discussed. The authors take this oc-
casion to thank r. S. Orteriberg for discussing the work. OvIg. art. has., I table,
"13 formulase
1SUB CODE: 20/ SUBM DATE: 290ct64/ ORIG REF., 003/ OTH RM, 002
jrn
2-

A ~7 AG-IM n-jv
ORG: None
Tr=i Regarding T. Tietz's note "sigenfunct ions and aigenvalues of the rotatiavAl-
oscillating states of diatomic molecules"
SOURCE: Optika i spektroakopiya, v. 19, no. 6l 1965, 990-991
TOPIC TAGS: diotomic molecules molecular physics) v
ABSTRACT: The author critLetzes the position of T. Tietz Olature, 2010 6950 1964)t'--
who proposed that the potential energy of a diatomic molecule be described by the
function A B n(n +1)C2
U W De E, + J2 + -(I W
r 2K466 I' x)2
where k -re ; , and constants A, 8, C; and n are determined from the
condition -hz
U (r U' (rd - 0; U', (re) a k 41y2 ALC2 V2
and the formula lor constant ae, linking oacill:tion and rJation
&e 11 + re Utle (ra)] .64
-m N

L 1
CC MR, AP6001664
It is briefly demonstrated that Tiatz's premise is not correct. Orig. art. hasi0
10 formulas.
SUB CODE: 20 SUBM DATHt O9Nov64 ORIG REFt 001 REFi 004

L 8604~-66--~~E'(IT~(0)/tqT(l)::~,-,i;~ P,( GG
rj
ACCESSION. MRt .AP502L16k UW01391651000100100010034
TM.~ 10i ed WXA
Probability-off-p --of potentW barrier In the generalls
1*'P~ss*Ufty of refining the Miller-Good wthod
SOURCE: rAm. rizika,, a*. 4,, i965,p 28-34
TOPIC TAGS: nuclear potential barrier.. Schrodinger eVationt quantum the
approximate solution
ABSTRACT-v;-.The possibility of further refinement of the Hiller-Good method (Pbya.
Rev. v. 91p 174j, 3,95~) for calculating the transparency coefficient is considered
for a one-dImenslonal entlal barrier with a single Vnm. -ne problem con-
slats of obtaining approximate solutions of the Schrodinger il'yation from the exact
solution of an auxiliary equation by the generalized WKB method. The Eckart p4D--
+^n+ial barrier Is considered as an example. It Is concluded that the tranaltion
in the quasiclassical Petraohent-Fok aWoximation to a new basis chosen vith al-
lowance for certain requirements results in considerable refinement of the results
obtained by the Hiller-Good method. The nev approximate method makes it posvible
to obtain correct Wormation about the energy dependences of the transparency and
~d 2,

)Ns Momkovskiy pedinatitub imeal V. 1. Lenlns (Moocow PedagQocal tll-
y q , .57-5'- 4 - -- -
i ,I I
I " ;

.:! 1.
, 1:
1 [:~ I, i !, III;" 111 -.1 ~ I I 111' ~i I I"l, I r~~ 1: 1 ~ I I V, I N' ~
; I

L 1996-66 EWT(d)/FS9-2J
'~We =71~~726490
SOURC& GODEt UR/0266/65/CX)0/019/0o25/bo4
AMTHOR, Uirliov, A. V
ORGs none
TITLE-. Device for synchronization of,discrete automtic phase controls Class 21)
SOURCES. ByvLUetenl- izobratenir i tovaj:;jkh snakovj, no. 19, 1965.p 25
_Twic TAGSt, sYnchronous.,comanicati. n, phased -locked commudcation
i'V i
~ABSTRACTv,'Thii-Autho ertif cate, d a for Bynchronization of
_.prqaents a 01jid
phase ddi_~trdle To decrease the netting time after temporary intorruptions wd to
increase the freedom from interference, two logic "NO" and "ORO units arb colmected
in series*in the automatic phase control circuit. The units are controlled by
exclusion and insertion, pulses from tuo corresponding pairs of triggera Wing an
auxiliaz7 pulse Bequence from a local master pulse gawrator.
SUB CODEs EC/ SUBM DATEs 3.6Dot63