SCIENTIFIC ABSTRACT FILIPOVICH, O.P. - FILOPOWICZ, A.

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• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

24 (6)
AUTEIOR: -Filipovich, 0. P. SOV/54-59-2-7/24

TITLEs Some Types of Equilibrium States in the Terrestrial
Atmosphere (0 nekotorykh tipalch rav-novesnykh sostoyaniy ataodery)
PERIODICAL: Vestnik Leningradskogo, univeraiteita. Seriya fiziki i khimii,
1959, Nr 21 pp 49-62 (USSR)
ABSTRACT- In investigating the state of the, terrestrial atmospheref a
number of equilibrium states of the gas medium can be found.
For the accurate mathematical and-physical description,
publications do not yet bring their complete determination,
nor'is there a unified standpoint on the physical nature for
some of them. In this connectionp this paper considers some
basio types of equilibrium and puts forward their exact
determination. Above allp those states were investigated
which are of interest for the solution of various tasks of
the theory of the upper terrestrial atmosphere. 1) Ther modynamic
equilibrium: Some basic laws of the classic phenomenological
thermodynamics (Kirchhoff) are indicated according to the
book (Ref 1). These are integ7rated by a number of rules
resulting from the statistic -.onaideration of the state. In
Card 1/3 case of an ionization, the lax of Sakh is fulfilled. The

Some Types of Equilibrium States in the Terrestrial SOV/54--59-2-7/24
Atmosphere
radiation intensity of this.state is determined by a law of
Plank (equation 10), the density of energy according to
Stefan-Boltzmann (equation 11). 2) Local thermodynamic
equilibrium: The thermodynamic e:juilibrium is disturbed by a
=~5er of causes which do not allow the simple.iray of
consideration, but the latter is made possible by a separate
consideration of volume units. 3) The monochromatic
radiation equilibrium introduced by the astrophysicists is
considered a little more closely. It occurs if the energy of
the frGquency is absorbed by any volume element and completely
re-emitted by the same element. rn its physical sense) this
equilibrium is directly inverse to the local thermodynamic
equilibrium. 4) FinaUy, a type of mixed equilibrium is
oonsidereds local thermodynamLo aquilibrium and monochromatic
.equilibrium exist in parallel at the same time. At the end of
the article, the two stationary atates (energetic and thermic)
are dealt with. The radiation equilibriums and the connection
between all equilibriums mention,?d are discussed here. The
stationary state is also considered in its connection with the
Card 2/3 distribution of atoms over tho various energy levels. The

Some Types of Equilibrium States in the Terrestrial SOY/54-59-2-7/24
Atmosphere
equation of the stationary state for a certain discrete atom
le-rel is given. This level is exprossed by the statistic
equilibrium of various transitions from above and from below,
spontaneous radiation, unelastic collision of ist and 2nd order,
ionization, absorption. Finally, the author thanks
Professor K. Ya. Kondratlyev for valuable remarks. There are
8 references, I of which is So-iriot.
SUBMITTED: May 22, 1958
Card 3/3

66302
'AUTHORS: Kondratlyev, K. Y&.j Filipovich# 0. P,, SOT/50-59-12-12/23.
TITLE: On the Theory of Thermal Conditions in the Upper Atmosphere
PERIODICAL: Aoteorologiya i gidrologiya, 19599 Nr 12# PP 41-48 (USSR/%
ABSTRACT: The results of the theoretical investigation of factors deter-
mining the vertical temperature distribution in the upper at-
mosphere are dealt with. Recent experimental data and theore-
tical results refute the conception of a radiation equilibrium
in the stratosphere. Data of actinometrio radio balloons show
that active radiation changes with the altitude not only in the
tropo phere but also in the stratosphere. The paper by Ohring
(Ref M is thoroughly discussed. The most important conclusion
from this paper-is that the stratoaphere as a whole (between
the tropopause and the 55 km level) is not in a radiation equi-
librium, Although the papers (16t 20, 24, 36) convincingly show
that thethermal conditions of tho stratosphere are primarily
controlled by radiation, the problem of the part played by
other factors (in particular that of turbulent mixing) has re-
mained unclarified up to date. On the basis of the papers
Or 301 32) it can be said that &n extensive area of the meso-
Card 1/3 sphere (between 35 and 80 km altitude)t from 300 on the northern
LX

66302
On the Theory of Thermal Conditions in the Upper SOV/50-59-12-12/23
Itmosphere
0
hemisphere to.60. on the-southernpie nearly in a radiation
equilibriume Th-amoat important characteristic of the mesosphere
is the circumstance that its thermal o,Dnditions may be subject
to a direct Influence of the change in solar activity* Investi-
gations in the thermo- and oxosphere show that various authors
obtained strongly varying temperatures for altitudes above
100 km. (hie of the causes is the circumstance that there is no
connection between the various tempexatures. Strictly speaking,
the,term of temperature is only applice.ble to a thermodynamic.
equilibrium. In the case of a nonequiLlIbrium gas, it is very
difficult to determine the connection between various tempera-
tures. The assumption of a thermal equilibrium (Ref 2) at an
r-
altitude of 100-400 km can hardly be justified. It is more co
'
root to speak of part equilibrium steAes with different degrees
of freedom* In conclusion, the follolring is stated: It is quite
natural to assume that the terrestrial -atmosphere gradually
-loses its properties and - at.an altitude of 2pOOO - 39000 km
comes into contaot,with the interplanetary gas. On the other

Card 2/3 0
handq the temperature of the interplanetary gas is about 5,000 K.

PHASE I BOOK E)(PLOITATICV SOV/4878
Kondratlyev, Kirill Yakovievich an& Ollga, Petrovna Filipovich
joex
Teplovoy rezhim verkhnikh oloyev atmosfery (Thermal Regime in the Upper
Atmosphere) Leningrad,, Gidrometeoizdat, 1960. 355 P- 3,000 copies printed.
Resp. Ed.: K. Y&. Kondrat,yev; Ed.: Yu. V. Vlasova; Tech. Ed.: M. I. Bmynina.
PURPOSE: This book is intended for scientists interested in the physics and
meteorology of the upper layers of the atmosphere. It will also be useful to
advanced students of the field.
COVERUM: The book systematically analyzes problems concerning the thermal regime
in the upper layers of the atmosphere,. Numerous observational data. are pre-
sented and basic theoretical ideas, e;plaining the regularities of the thermal
regime, are put forth. The latest scientific1aformation on the ccaposition
and structure'6f the upper Were of the ataios]~ftere is characterized in detail.
Chapters T11-171I were written by Kondratlyeir; Chapters I-T-I and VIT-T-X were
written by Filipovich . The authors thank It. P. Gurov,
Titov,, and Ye. G. Shvidkovskiy. There are 472 references: 190 Soviet,, 272
English, 7 German, and 3 Fiench.
Can"4_-

M
Thermal Fegime in the Upper (Coat.)
TABIZ OF CORnM:
Forevord
Introduction
SOV/4878
Ch. I. Fandamutals of the Statistical Theory of Jases
i. Theconcept, of temperature
2. The IA,ws of statistical equilibrium
Ch. I.I. The Atmosphere as a Gas Which 'is Not in a State of
Statistical Xquilibrium,
1. On some states of equilibrium existing in the earth's
atmosphere
1. Local themodynamic equilibrium
2- Problem of the applicabi3ity'of Kirchhoff's law to the
,earth's atmosphere. Concept of partial local thermo-
dynamic equilibrium
3. Monochromatic radiative eq~zilibrium
4. Fadiative equilibrium
3
5
11
11
13
21
21
21
29
49
52

Thermal Regime in the Upper (Cont.) SOV/4878
5- Mixed types of equilibrium states 52
6. Stationary distribution of 'part~clt-,s by- states 55
2. Concept of temperature under condittons where thermodynamic
equilibrium does not exist 56
3- Some remarks concerning the applicabillty of the laws of
statistical equilibrium in the earth's atmosphere 63
Ch. IXIN, Indirect Methods for Determining the- Tlemperature at Great

kights 70
1. .
AC u ,~a method 70
2. Obse on of meteors 79
3- optical hods 86
1. Twili method 86
2. Pr6jecto sounding 98
3. Investi A a of the spectra of night wErglow and auroras 103
4. Apectroscopy f oxone log
4. R9Ai6 methods U2
1. Height of the h geneous &tmqsyhar.& 113
2. Effective coeffic of recombination 113

Thermal IL-gime in the Upper (Coat.) SM/4878
Ch. VIII. Theoretical Mais on the Thermal FAigime of the Thermo-
sphere and Exosphere 210
1. Application of the theory of radiative equilibrium to the
thermosphere 211
2. Theoretical models of the thermal regime ta3ting into account
the heat conductivity 214
3. Heating of the upper atmosphere by interplwetary gas 228
Ch. IX. Conservation of Energy Equation and Its AIT11cation to
the Problem of Tem
.peratdre Distribution in. the Upper
IAyers of the-Atmdsphere 240
1. Derivation of th~ conservation of energy equation 240
2. Discussion of the.beat conductivity equiLtion. 244
3. Some remarks on the theory of t4e ther=Ll regime 248
Ch. X. The R ole of Various Factors in Heating the lJkxr IAyers of
the Atmosphere 261
1. Ultraviolet radiation and X-rays from the stut 262
I. Rocket research OaLthe Ultraviolet and extreme
ultraviolet regLms of the solar spectrumt 265
Car&ZA-

Thermal.Begime in the Upper (Coat.) SC(V/43T8
2* Rocket research on the X-ray region of the spectrum 270
3. Results of theoretical calculations of' the distribution
of solar radiation energy in the ultraviolet and X-ray
regions of the spectrum 272
4. Discussion of information on theenergy cei-ried by
ultraviolet and X-ray solar radiation into the upper
atmosphere of the earth 274
2. InterplanetuT gas - 275
3. Accretion of the interstellar medium by th) sun and dis-
sipation, of particles from the colar atmosphere 278
4. Corpuscular streams 286
5- Electrical currents 2W
6. M&gnetohydrodynamic waves .297
7. Friction between the earth's atmoff9here and! interpl=etary gas 308
8. Micrometeors -- 308
90 Infrasound waves 310
10. Geoc.orona

Therml Regime in the Upper (Cont.)
Conclusion
Bibliography
Appendixes
AVAnAZZ: Libraa7 of Congreeg
SM/4878
32o
324
343
JA/dat/fal
3-2o-61

- ------ -- --
Some calculations of the.temperature distribution in the upper
levels of the atmosphere. Vest WD 16 nD.16:66-76 161.
(Atmospheric temperature) WIRA 34:8)

I I ob 1667 2107 "~j)-7
ARSE/T Filipovicht 0. P.
:26764
S/054/61/000/003/002/OD3
B-102/B203
TITLE: Calculations of tomperature distributions in the upper strata
of the atmosphere
PERIODICAL: Leningradikiy Universitet. Vestnik. Seriya f iziki i khimii,
no. 3, 1961, 66-76
TEXT: The author auggesta a method of determining the temperature
distribution in relation to altitude in tho upper strata of the atmosphere
by a simplified solution of the equation for heat conduction. For a plane
atmosphere,
a OT) + P - L - a (z) 8T(7~21) (10)
"~ -Z az a t
ia valid in first approximation, a and Y. being independent of tim,*a; X is.
the heat-conduotion ooeffioienti c is the specific heat of air;
div(xlVT) +P -L- a (oT); P and L are energy densities brought into or out
1) t
of the volume element V in the form of heat; z is the altitude above a
certain level. The difficult calculation of Eq. (10) is simplified by
Card 1/4

26764
si/054/61/000/003/002/003
Calculations of temperature.. B102/B203
giving P(Z't), L(z,t) and T(%,t) in the form of time-mean values (mean
values, barred) and fluctuations A... Thus one obtains, e.g., for
temperature, the two independent equations
62),
a aa r d-IT
_F �~_ -.&L-c , .'
)+ aP (13),
and therefrom e
dz' ~_!~_SP5(e)_!(e)jdz-, (14)
T(z) + Y M(-Zo) ~ . (.) x (I')
ZO) d.-
ZO z0
Finally, z
_T(Z) S + all (go) A Al.
(ZO) A
to
t
+ I
)S
(21)
A(zl) ZO
Card 2/4

~!6764
Oij'A1/61/,r)()0/003/002/003
Calxulnt.i~-,n- of B102/B203
j..~, obt-Y,*n, I %,ith nn:1 the timcavvra,ged value 7-Ai
(A collision cross section, awl n, = 1/2). The following must
be ~--novn for determining the temporiture diatri')ution: a) tbe,altitude
dl;; 1; r i bu i. on of the absorbed thermal onergy b) the altitude
dependonce of A(z), c)'the mean heat flux
OT(z 0) aT(v 0,11
Q(z 0 T A(7 0) a, - z(ZO) 0",
t1kvoii,-h-thL- u-pper bounlary, awl (3) the moi,n.tempernture at the lowc!r
boi.indarY, T(zl). Fig. 1 ghow:j routilts of a numerioal computation of
0 2
teimer-ature dintributiona for diffvvr,~nt fluxon F (aiven in ergs/cm Gee)
.1nd V=PJ)~, nn v"all aG F-B 12 Paw denotes the 11 value according to
F. Johnjon (Temperature in the hirrh atmosphove, Ann. greoph., jA1 it 1958).
In F(111 ) = X. 0 )aT(zj,)) , the nature of' the onergy.flux is still
0 0 .02
unclvrified, but according-to rla'.'a obt-alned fron npitniks and rockets i t
Vm,~ b,! due to corpimenlar radiation bclU,. The F vrAtion in Fij, 1
Cliol'on accordinp y S. 1M. Wurnov et, ;il. (DAV, L30, 3, 517, 1960)
to data b
Card 3/4

Colculationu, of t empera
(m 1,11C energy '7roups of
-Ire 5 fipurer, an-I
1114
267
ture. . . 61/000/003/002/W)
15Z
B1C2 B203
electil'oru in tile terre.-I trial radiation belt.
0 r e f C.- n0en 3 Soviet mil 3 non-Soviet.

KONDRATIYKVp KirinYakovlovichl FILIPOVICH, O.P., Otv. red.;
M.M.p red7v--E-R-fl-NW,-1Gr.,, tekhn. red.
YASNOGORODSKAYA
(meteorological reaearch by menas of rookets and artificie.1 satel-
lites) Metoorologicbeskie issledovimiia s pomoshchliu raket i
sputnikov. Leningrad$ Gidrometeore i7,d-vop 1962. 251 p.
(Rockets in meteorology) (MM 15%6)
(Artificial satellites in rateorology)

379n
11/654/62/000/002/007/012'
3)163/B138
AUTHOR: ziiizsni~~
TITLE: Height distribution of temperaturo in the thermosphere
PERIODICALt, Leningrad. Universitet. Vestnik,. Seriya fiziki i khimii,
no. 2, 1962,178-93
TEXTt The temperature distribution in the therraosphere (i.e. at heights~
over 100 kn) can'be determined theoretically from the generalized heat
conduction equation (0.P. Filipovioh, Vestnik tGU, no. 16, 1961) and from
experimental data collected by satellites on atraoapheric density, using
the equation of statics dp = -~gdz and the AdeA:1, gas equation p ,, nkT.
The second method is described, discussed in detail, and applied.to various
models Rf .he upper atmosphere. The results aro affected by the'aseumptions
made onberning the dependence of the partial concentrations of the gas
comp0aents on height. From an analysis of bhe-reaults it is conaluded
th4;t the main heat source of the thermosphere is the radiation energy from
the sun which is absorbed by photoionization and photodissociation.
A slow temPerature rise with increasing height beyond 300 km
Card 114

YURVW,
OF N,
Rap-ld exeoution of,dcveiop~ iont warkings.at the No. 1112 m4
of the Sakhal-'n~ip!17 I I Ine
4901' 40 no.&,20-22 4g '65,,

FILIPOVICH
- P S.10
Stand for fatigue teats of real gem. wheals of
Missions of a locomotive. Nauch. ZaFf. traction trane-
40-43 t6l Ode Politakhe inst. 39t
(MIRA 179.3)

ZABLONSM K'I,., kand.tekbn,nauk., do sent; TIELYJL~Evp M.S.,, kand,tekhrjA%&ukj
P 0 t
Pperating a herringbone reducing goara Veot. maeh.. 41 no. 5:33-37
My 161. (Ge&ringp Spiral) (KWA 140)

MR, N't
t IMF all,

7 w
---- )M'? Z~ ~-i1.11~4e,~, 4 . ~ ?.. %-,:~

ZABLONSKIY K.-I. -prof.1 ZOBM, N.P., doktA)r Ukhn. nauk, prof.;
YUMNO D3,, kand. tekhn. nauk, dotoont; FILIPOVICH, SOI&I
insh.; PORUMIMs M.A... inzh.
Stands for hardening treatnent and strength testing of the
traction transmission gearing of loccaotives. Trudy MnT
no.159175-88 162. (MIRA 16t6)
04comotives-Transmission de'vices)

ZABLONSMI K.I., prof.; YUDIN, D.L., kand,,takhn.nauki, dotsent; FILEPOVICH, S.I.,
inzh.
Methodology for the fatigue strangth Uisting of the teeth o.,"
dieBal locomotive gear wheels on a special stand. Trudy HIIT
no.20ot54-65 164, (MIRA JW)

USSR/Medicine,, Veterinary - Foot-and-Houth Disease Aug 52
1AVariations of The Virus in Foot-,and-Houth Diseases" 7. 1. Kindyakov, A# No BVadinov,
S. M. Filipovich, 0. S. Nikonova, Sci Res Vet Dist., Kazakh Affilitte, All-Union Acad of
.Agr Sci imeni V. I. Lenin
"Veterinariya" No 8, pp 21-27
Discussas the variations in types of the virus causing foot-and-mouth disease# Lists
,1+5 strains,, classified according to types Oj, A,, and C. On the-basis of expts, assumes
that there is only one parent vIr#s with the ability of change's its" bioimwxWlogical"
properties under the.inf-luence of out aide factors. States ~~ the major factor In
causing changes is the passage of the virus through the living organism of an animal
idth an acquired immunity to the disease, Authors recommend that herds of cattle that
have recovered from the foot-and-mouth disease should be kept apart from cattle in the
acute stages of the disease and that in research and treatment of foot-mouth, disease
consideration should be given to possible changes in the manifestation of this virus.
Recommend further research on the biol properties of the virus.
PA 233TU

W~, W 1-1 f

tendty) as a function of 10 are fteu for I and 11, hi accord
with their moWispersity. and nonlinear for the polydis.
Investigation of the structure of Name dkLsduby the
meth
d
f
ll
l perse M. Ca!.cu. of the vols. of pores of radius R. by the
d6t
ibu
th
o1
44 7048h)
h
d
A
C
o
o
sma
4trig
e Smattering
shits, 'A. M.
3
-
- of Xr - H.A.Poral-Ko.
VON Y -
e v
.
r
.
gave
tangent. met
o
.
(
tious (%): 1. 30 A. (97.5 ). 55 ~10) 97 (2.5): n. M A.
N
7r.7. w4
UT
Sxft R
o w 1952 ; cf. An
1 52.5 A. (32%). 126 (27), 240
78% , 88 (14:1,. 110 (8);
M
o/.. C.A. 45, 409
54831.-~-Thj - sman
,
Tt
-angle 'Wgtterl
i ). This ghvsis mean R, for134 A. (as against 40A. by
111effitA was it PlIe
o A 04mP
lcS oreviously Stu by t e
h
l
viwor-attsur
tion
th
d
h adsorption), and for 11 64 A. (as against. 100 A.). The
ThIs auce-
table for H
W for I and aLce
cement is
a
me
o
:
p
omoreneo y p9fous wi
th .
gr
p
V
'
.L 1-1an pore radius of 40.
(U) h gen y coam. -angle scattering
teriori that the small
nent proves n pos
IXW(913 with a most probable effective er 1usof100A.,
-
and (111) inh nethod has given the size distribution of the pores and not
:
This con-
s
nd 1H
of I
t l
i
th
f
h
ti
l
oin%cueously P
Crous the
vJ1ryh1
from
b
t 15 t
15 .
n
e ca
a
east
e
o
c
ti, a
t
e pnf
ect to H: Numericul estu
ith res
l
in
l
i
i
t
a
0u
o
g
0 A. The. seat g
v varled from ul to 2*30#
Plot
f l
I .
on
ess cer
a
e
us
s
w
p
for the Ist
of the accuracy of the x-ray deta. of R gives
.
$ O
0t
(Wattered ,
(mia.) A an error of - 3 A., I.e. about 5%. K. Thon

P4v/c-h VW
Category USSR/SoIA State 54sics - Structuarall Crystallography E-3
Abs Joixr Ref Zhur Fitika, Nc 2, 1957 No 3,681
Author Filipovich, V,.H,
Title ~f scattering of X-rays in Gases, Liquids.,
Amurphaus So2lds, ar& 11-lycrystals
Orig Pub Zh. tekhn. ftziki, 1955, 25) N:, 9, 16o4-1621.
I
Abstract The IntIrsity cf scattering from the inv~:Eitigeed objects is given by
the equition
where 2y
P r) r
is the ~ 10 ;e'd over the atoms
sum n~,er~t i, ~1~4 t ~ u. tAons (aveia
of each kina P.-A over the time) of the electron density aroand the cen-
ters eof +'., atoms of a given sort, multiplied by NjZj -- the total num-
ber of electr:,ns IrA these atcms . Inversion of the Fourier inteE;rml M
make5 it P,,-sslbl.e t'-- findPexperlmpntally, using known methods. Using
Card 1/1

Category , TJSSRISol,'.,i State Yhysics - Gt?!uctijxBI Crystal-Ii-graphy E-I
Abs Jour- z Ref Zlux*r - Flzika~. No 2-, 1957 llcl 01.
the Fourier methcd,, the watb-~r armayzes thet effect/ of the fact that I
(s) is experWettally unkn' -wn at s'-() and s The first of
these circumstances ts eliminate& by takix-fi; =to acenunt, the "z4!ro"
scattering 1:0 by the. average electron der-511ty, while the second makes it
P-sslble to obtainP,"r) -:av appr_-4.ximtely, and may result, in false de-
tails. Ir_trA)iciDZ the atmi-, fact--,rs and ellm, ating the gas scattering,
the autb,:~.r rbtair~s next th~_ well Im-m equaticn fLtr radial distribution
in liquids a?".1 amorph.-us b~-4ies, given by Warren and his associates for
the atcim-e~lectr,)n dernsitypoZ"e"', The. maxima nf' the Latter agree m6st ac-
curately with the interat6mic dietances. A specific example is used to
show that a sur-Plimentaxy s,:~urce :f pcssible errors is the usually-em-
ployed methvi oi mrmai-t-zation of the intenj3ilty curve over the distant
regions s., where this curve may fluctuate. False maxima may be identified
by the equal Itstances betweem, them (amourating to 6 r 2 ir/so) and by
2
the fact that -the ampLitude diminishes as I/r
Card 2/9

Category : USSR/Solid State Physics - Structural Crystallography E-3
AbB Jour : Ref Zhur - Fizika, No 2.. 1957 No 3682
Author :Filipovich, V.N.
Title Concerning the THbory of Scattering the X-rays in Cases, Liquids,
Amorphous Solids and,Folycrystals. II.
Orig Pub Zh. tekhn. fiziki, 1955, 25., No 9, 1622-1638
Abstract Fourier analysis is used to exemine the broadening the diffraction lines
of X-ray photographs of polyerystalline objects as functions of the dl-
mensions of th crystals and of certain defects in their lattice. The
author obtains in this n-nner a somewhat refined form of the Bertaut
equation (Bertaut, Z.F., Acts, crystallogr., 1950, 31 14) and the Stokes
and Wilson equation (see Wilson, A., Optics of X-rays, IL, 1990). The
sources of errors are indicated and the methodx for estimating the errors
are given for the calculation of the average characteristic mtgnitude
LK of the minute crystals in the specimen.
Card 1/1
7 Ir

1-1 I'VV/(-. "I/ T /V.
Category USSR/Solid State Phyaice - Structural crystallogrAphy
Abvqour Ref Zhur - Fizlkao No 1., 1957,,No 1059
Author Pdlipovich. V.N., Foray-Noshits, YO.A.,
Inst tngT,. MEaRry of Silicates~ USSR AcadwW of Scieness
Title On the Theory of Scattering of X-rays by Mscrosca.pic Isotropic Bodies
Orig Pub Dokl. AN SSSR, 1955, 105, No ;z,, 968-971
Abstract A new derivatioix Is given for the equations of the Fourier analysis of
curves for scattering by macro-isotropic (liquid, amorphous., and polycrystalline)
bodies. It is shovn that such an analysis gives a at--uctural.,;4cbarar-*teris+,ic
of the substance in the form of a function
/0
vhere ? (r)t) is the'Imstantaneous distribution of the electron density i3i
the speeimeai, and the bar',indicatse averaging vrer the tize of the x-ray ex-
posur% ' For macio-isotropic bodies., ~ ~,r) depen(le only on /r/;& r and is deter-
mined y the equation 4&
Y (r) = 114 7-1 f;,) -r-4Is I Ns 6 -h -~-s d. S
Vhere I(s) is the ocatterin intensity (s : 4-T sin -A,~Nkr's the scattering
Card 1/2

State Thysics - Structural crystallogxuphy E-3
Abs Jour Ref Zhur - Fizikaj No lt 1957 No 1059
angle). Since I(s) cannot Im determined experimentally at a;= 0 and at
6 the only thing that can be found in practice is the function 6C9,
(Fabinert I s prWiple), vbLere
is the averagt valu,6-of (r)-, W is approxtmwtely constant at aman value$
of r). An&logou6 equations, can be obtained if one introduces the atomic factors
f (a) and correspondingly the function of distributi~m density of '~point" ,
a
_Zms P" (A) This m%kes it necessary to calciilatt very accurately the "gas
sting of Ig (8)=T1 Wif (s) (stmtd oveir aIL types of atow) from X (a),
for otherwise the radial-~idtrib-4tion curv,!: (the imalove of (r)Yirill con-
tain falso details, vhich my occur in sAditiori'also as a result of calcula-
tingA~, (r) rather than I (r). Fals,_4 meadm'dNipaxently occured in the work
by Richter and his associates. (Referat. Zbljr--ja Fizika, 1953, 11557).
Card 2/2

4-1
rl-.Ml*ql-ltw-,l 6:9;-Zlarl~ III ~.~~XP ~11 --.. -- --, " '" t" ~-: N !-, zzSI: mklo~wlg twlstwWvl
.,~ i
t~r
I
i

V I I,_ I I V * I I
USSR/ Physical Chemistry - Crystals
Abs Jour Referat 2hur - Xhimiya., No .3.- 1957, 7241
Author
Title, On the Theory of Low-Angle Scattering of X-rays
Orig Pyb : Zh. tekhn. fiziki,.1956, vol 26, No 2, 398-416
B-5
Abstract : A previously described method WhIchim, 1956, 74171)
is'used in the elaboration of a th(mry of low-angle
scattering (LASC). The Fourier series obtained are
analogous to previously obtained results (G. Porod,
Kolloid Z., 1951, L41; 2) for bodies giving isotropic
LASC. Typical examples of LASC are! discussed as well
as the accuracy of the calculation of the radial dis-
tribution curve and a number of other characteristic
paraneters (diameter, curface, and volume of the scat-
tering heterogeneities) from the experimental data.
Card 1/1 33
------------
ill Vv/cw V, lv~
USSR Solid State Physics Struotural Crystallography E-4
Lbs Jour IRef Zhur Fizika, No. 6, 1967 No, 11683
huthor Filipov-10h, N,
:Intt 0f Scattering of X-rays at
Title-' Contribution to thG'ThGOrY
Small Angles.
Orig Pub Zh.' tekhn. 1966,_ 260~ 110 398 - 416.
Ostract theoretical works serving as a continuation of preceding
work (Referat Zhur Fizika, 1957, 3681, 3682) and which is
a generaliiation,and refinement of..t-he ocirresponding theory
by Porod (Forod, G., Kolloid Z, 1957, 124., 2). It is
explained that failure to takeinto accoltnt the zero
scattering and scattering at small angl0l's due to the pre-
senoe in the specimen of submicrosooPic irregularities of
the struoturemeasuring more than 10 -20 A, leads to a
loss of corresponding information on the structure of the
Card: 1/2
-- -----------

USSR / Solid State Physics / Structural Crystallography E-4
Abs Jour 3 Ref Zhur - Fizika, No. 5, 1967 No, 11588,
Author t-Filipovich. V.K,
Title v De-te-zMrn-a-fro--n-oT-Interatomic Distances from the Radial-
Distribution Curves.
Orig Pub : Zh. tekhn, fiziki, 1956, 26, No 2, 417 - 421.
Abstract : Continuation of previous works (Referat- Zhur Fizika,
1967, 3681, 3682) pertaining to the theory of scattering of
X-rays by macroisotropia bodies. A premise is examined in
detail and proven, that is prac ace the interatomic dis-
tanaes must be determined always fr2m tho curve r (P I (r)
and not from the ourves Ap'(r) or r (?" (r) (qP' is the
interatomio-distanoe density function). Also considered is
the problem of the possibility that the dimensions of the
minute crystals affect the interatomic distances, de-
termined from the radial-distribution ourve.
Cardt 1A

AUTHORt FILIPOVIORIV.N. PA 3557
TIM: -66-111-mtion Correction to Low-Angle X-Ray Scattering. (0 kollisia-
tsionnoy poprafte v teoril, rassoyaniya rentgenovskikh luchey Ix)d
uslymi, il-la=4 P Russian)
PER CDIOALi Zburn&1 Tekhn. Viz. 1957, Vol 27, Hr 5* pp 1029-1044 (U.S.S.R.)
ABSTRACT: A detailed demoription of the tasks of oollboation correction is
iven. Th wathod already described and applied in previous papers
z"hurnal ;ekhn.Fiz 956, Vol 26, Nr 2) 1955, Vol 25, p 1604)
t
1955, Vol 25p p M2)' Is employed. The methods employed for prem-
tioal oollivation correction are systemized iind further developed.
The complete solution in given of a problem (moerning a reo-
tangular gap and a homogeneously impining butidle, and a simplifiga
method of carrying out the correction to this case is suggested.
In a general fo= acme oollimation effects are investigated, viz.
the shifting of the interference ma3dman in the oase of an in-
crease of the length of the gap in the direction of the smaller
angles, arid the po&aib:Llitj of the vanishing of this =:d- i in the
came of an increase of the width of 'the gap. (With 5 Illustrations
and 6 Slavic References).
card 1/2

PA - 3557
Collimation Correotion to Low-Anglo X-Ray Soattering.
ASSOCIATICK: Institute for the Chemistry of Silloates of the loadeqy of
FRESEWM BY: Soienoe of the U.S.S.R., LeningreA
SUBMITTEM 14-1-1957
AVAILABLE: Library of Congress
Carcl 2/2

67186
7A 00 SC)V/58-59-7-15368
Translation from; Referativnyy Zhurnal Fizika, 1959, Nr 7. P 109 (USSR)
AUTHORS: Poray-Koshits, Ye.A., Filipovich, V.N.
TITLE: Some New Possibilities of the Small-Angle X-Ray Scattering Method'
PERIODICAL: V sb.: Metody issled. struktury vysokodispersn. i poristykh tel. Moscow,
AS USSR, 1958, PP 7 - 18
ABSTRACT: To extend the possibilities of the X-ray method of small-angle soa#ering
(SAS), the authors propose that a new experimental technique be adopted,
using a frame camera, a single- crystal monochromator with point focusing
of the primary beam, and various variants of an ionization device with two
single crystals. It follows from present-day SAS theory that one can use
the formula of Fourier analysis to obtain a number of new parameters in
addition to the radii of inertia. The comparison of these parameters, to-.
geiher with the simultaneous use ofthe direct results of Fourier analysis,.
permits a more complete and unambiguous analysis of the structure of the
scattering regions ef inhomogeneity- and, in particular, the determination
of their inner surface per unit mass of the sample, (In-t khimii silikatov).
Card 1/1 The authors' r6sum6

L 1- 0 _V_ -1 -C '_ 0-i - V
24(6)
PHASE I BOOK EXPIDITATION
C;OV/1409
.5oveshchaniye po metodam issledovaniya struJ~tury vysokoditgperanykh i poristykh tel.
2d, ieningred, 1956.
Metody issiedovaniya struktury vysokodisperonykh i porist3rkh tel; trady'vtorogo
soveshchdniya (Methods of Inveattgating the,Stracture of Highly Disperse
and Porous Bodies; Transactions of the Ekicond Conference) Moscow, Izd-vo AN
SSSE, 1958. 294 p. 2,000 copies printed.
Sponsoring Agencies: Akademiya nauk SSSR. Institut fizicheskoy khimii,and
Institut khimii sil-ikatov.
Reap -Ed.; Dubinin' M.M., Academician; Ed. of Publishing House; ftzumova, L.L.;
;;ch. Ed.:'Marko~ich, S.M.
PURPOSE: This book is inte aded for scientists, teachers and advanced'stu&As
interested in the structural analysis of highly disperse and porous bodies.
COVE?=: This collection contains reportij by members of various Soviet ifisti-
tutions of higher education: Institute of Physical Chemistry, AS UkrSSR;,
carci 1/ 9

Methods of Investigating the Structure of Highly (Cont.) SOV/1408
Institute of Chemistry, AS Georgian SSR; Far Eastern Branch, AS USSR;
Georgian Scientific Research Institute for Petroleum; State Optical Insti-
tute; Leningrad Technological Institute; Moscow and Leningrad State Universi-
ties; Far Eastern Polytechnic Institute; "Agrophysical" Institute, and others.
Introductory remarks were made by Professor N.A. Toropov, Director of the
Institute of Silicate Chemistry. Apart from reports under the four subject-
divisions (see Table of Contents), the collection includes discussions, con-
siderations and proposals adopted at the close of the conference.
TABLE OF CONTENTS:
Foreword
PART I. X-RAY AND EUCTRON-MICROSCOPH MEMD8 OF
STUDYING TEE STRUCTUMM OF HIGHLY DISPERSE AND POR-
OUS BOD33S
3
Poray-Koshits, Ye.A., and V.N. Filipovich (Institut khimii silikatov AN SSSR-
Institute of Silicate CliTm-istry, AS U�9i). Several New Possibilities of
a Small-angle X-ray Scattering Method 7
Cgrd 2/9

Methods of Investigating,the Structure of' Highly (Cont) SOV1408
Leontlyev., Ye.A.., and V.M. WkIyanovich (Institut fizicheskay
Xhimii AN SWR - Institute'of 'Physical,' Chemiatty, -AS'USfIci)
Electron-microscope Iavestiption of the Structure of Porous Bodics by the
Replica Method- 19
Discussion (by contributing authors and Ir.j. Wgin) 37
PART II - ADSORPTION MTHODS OF -STUDYING SUM M AND THE
RESULTS OF THEIR APPLICATION
A. Investigation of Systems Consisting of Spherical Particles
Kiselev, A.V. (Moskovskiy gosudarstvenny:f universitet imeni M.V. I nosova i
Institut fizicheskoy kbimii AN SSSR - Moscow State University imeni M.V. IAmono-
sov and Institute or Physical Chemistry., AS USSR). Corpuscular Structure of
Adsorbent-Gels 47
Radushkevich, L.V. (Institut fizicheskoy khimii AN SSSR-Institute of Physical
Chemistry,AS USSR). Capillary Condensation of Vapors in systems or Spherical
Particles 60
Karnaukhov, A.P. (Moskov skiy gosudarstvennyy univeraitet.imeni M.V. Lownosova-
Moscow State University imeni.M.V. Lemonosov). Capillary-Condensation
Mrs resis in Systems of Ideally Packed Spheres 71
CardW

Methods of Tivestigating the Strwt6~e of Highly (Cont.) aov/14o8
isikikyan, A.A. (Moscow State Uhiveiviiy imat N.V. Loomonosov)
Adsorption-Calorimetric Investigation of Capillary Condensation 85
Discussion (by contrDbuting authoraj V. V. Serpinskiy, Institut nauchnoy
informatsii AN SSSR- Institute of Scientific Information, AS USSR; and
N.N. Avgull., Institute of Physical Chemistry., AS USSR). 95
B. Applications of the Adsorption Method
.M'M.-*: (Institute of Physical Chemistry,, AS USSR)r-
Dabinin, YJ
Methods of Calculating Statistical Volume and SuLrface Distribution of
Sorbent Pores Based on Sorption Measurements. 107
Zhdanov, S.P. (Institute of Silicate, Chemistry, AS USSR)
Application of the Adsorption Nethcd for Investigating 3tching
Structures in Porous Glass 3.17
Neymark, I.Ye., R.Yu. Sheynfayn, and L.G. Swintsove. (Institut fizicheskoy
kh4mii imeni L.V. Pisarzhevskogo P11 USSR-Institute of Physical Chemistry
imeni L-V. Pisarzhevskiy,, AS UkrSSH) The Nature of - Mange
Shape a in
Sorption Isotherms of Various Vapors on Fluorinated Dilica Gals.. 128
card 4/ 9

Methods of Investigating the Structuxe of Highly (Cont. ) BOV140ES
Nabokov, V.S., Ye-N. Paleolog, and N.-D. Tomshov (Institut! Of Physical
Chemistry, AS USSR). Sorption Method of Determining thit Structures
of Protective Films on Metals.- 137
Tsitsishvili, G.V. (Institut khimii imeni P.G. Malikishvili Alcademii n-1c
Gruzinskoy SSR-Institute of Chemii3try imeni P.G. Melikishvili,, Academy of
Sciencos, Georgian SSR). Porosity Characteristics of Adsorbents With
Mixed Structure 146
Discussion (by contributing authors; K.D. Shcherbakova, Moscow State
University imeai M.V. Lomonosov)and D.P. Dobychin., Gosudarstvemyy
opticheskiy inatitut imeni S.I. Nhvilova-State Optical Institute imeni
S.I. Vavilov) 151
C. Comparison of the Results of Employing the Adsorption Method With
Data From Other Methods'of Stud4lng Structure.
Kiselev, A.V., V.M. Luklyanovich, and Ye.A. Poray-Koehits. Results of a
Complex Study of Adsorbent and Catalyst Structures Obtained by Employing
Adsorption, Small-angle X-ray and Electron-microscope Methods i6l
Card

Methods of Investigating the Structure of Highlv (Cont.) SOV/1408
Zhdanov, S.P., and Ye.A. Poray'-Koshits. Comperison of Results Obtained
From an Investigation of Porous Glass Structures by SWI-angle X-ray
Methods~ 180
Discussion (by contributing authors; N.M. Munkin and Ya.V. Mirskiy, Groz-
nenskiy nefltyanoy nauchno-issledmtellskiy inatitut- Groznyy Scientific
Research Institute for Petroleum; Yu.A. El'tekov', Institut organicheskoy
khimii imenl N.D. Zalinskogo AN SSSR-Institute of Organic Chemistry imeni
N.D. Zelins1dy, AS USSR; and M.P. Repkova, Moskovskiy inzhenerno-fizicheskiy
institut-Moscow Physics and Enelneering Institut) 190
PART III. METHODS (IF DETERMINING THE SPECIFIC
AREAS OF HIGHLY DISPERSE BODIES
Deryagin, B.V., N.N. ZakhavayevaL, M-V. Talayev,, and V.V. Filippovskiy
(Institute of Phy5ical.Chemistry. AS USSR). A Filtration Method of
Determining the Specific Area of Porous Bodies 203
Smirnova, A.M., N.G. Zaytseva, aml V.P. Sukhova (Institute of Physical
Chemistry, AS USSR). Employing Tagged Atoms to Investigate the Specific
Card 6, 9
0 AU4

Ykithods of Investigating the Structure of Highly (Cont.) SOV/140
Areas of Cementing Materials During the Hydration Process 214
Bykov, V.T.., and O.Ye. Presnyakova (IAboratoriya adsorbtsionno-
structurnogo i khromatoografiobeekogo analiza Dallnevostochnogo filiala
AN SSSR-TAboratory of Adsorption-Structural and Chromtographic
Analysis, Far Eastern Branch, AS USSR). A Dynamic Method of Investigat-
ing the Structure and Specific Area of Adsorbents 224
Y61ovidh, S.Yu., and L.Ya. Mmrgolis (Inatitute of Physical Chemistry, AS USSR).
Determination of Area and Structure of Active Manganese Dioxide by the
Absorption-Chemical Method. 231
Discuision(-'-by contributing authorsj A.T. Kalezova), K.I. Metveyevj A.K.
Khodskov, Institut tonkogo ftmellcheniya-Institute for Fine Grinding;
N. Gryazev, Saratovskiy gosudarstven*T universitet imani N.G. Cberny-
shevokogo-Saratov State University imani. N.G. Chernyshevskiy; and G.M.,
Osmolovskiy., Ieningradskiy gooudarstvennyy universitet imeni A.A. Zhdanova.-
Ieningrad State University Jjwni A.A. Zhdanov) 239
Cae- T/ 9

b6thods of Investigating the*Structure of Highly (Cont.) sov/108
PART IV. TEE "MRCM POROMTRY" MTHOD [POFS BI23 DISTRIBMION
ECTEWMATION BY TIE HIM=-INJECTION NETHOD]
Flacbenov, T.G., V.F. Wellobsya, and M. Ta. Pulerevich (Ieningradakiy tekbnol-
ogicheskiy institut imeni Lensoveta-Leningrad Tt~chuological Institute imeni
Lensavet). Studying the Structure of Pbrous Bodies by Mercury Fressuri-
zation, 251
S!imsnova, S.A. (Voyennays, akademiya, khimichaskoy zashchity imeni K.E. Voro-
ahiloya-Military Academy for Chemical Defense). Low-pressure Mercury Poro-
metry 259
7d%levskiy, N.I., and V.T. Rykov (Dallnevostochnyy politekbnicheskiy institut
imeni V.V. KvWbyaheva.. Yliadivostok-Far Eastern Polytechnic Institute imeni
V.V. Mwbyshqv, Vladivostok). Application of the Mercury Porometry Method
for Investigating the Macroporosity of Natural Sorbents 267
Discussion (by contributing authors; G.M. Belotserkovskiy, Leningrad Tbch-
nological Institute imeni. Lensovet; and M.F. Yanovskaya, Institut gornogo
dela, AN SSSR-Mining Institute, AS USSR) 272
Card 8/ 9
_5
In
W ~'t N I ~ P
A

Methods of Investigating the Structmv of Highly (cont. SOV/1408
PART V. MMPAZF DIWMION
Ehmkin,, N.M. (Groznn Scleabific lbuarch lastituto for Pbtrole=)j Andrepy,
Ye.A. (Institute of Physical C&-m-letry, AS USM)j and contributing authors. 280
Decisions of the Conference
AVAIIAME: Libisry of Congress
~N/fal
4-29-59
290
Card 9/9

SOV/81-59-15-532'9.19
Translation from: Referativnyy zhurnal. Kh1miya, 1959, Nr 15, P 138 (USSR)
AUMORS% Poray-Koshits, Ye.A., Filipovich, V.N.
TITLE1 Some New Possibilities of.the Method of X-Ray Scattering at Small Angles
PERIODICAL: V sb.: Metody issled. struktury vyookodisperan. i poristykh tel.
Moscow, AN SSSR, 1958, PP 7-18
ABSTRACT- A short description of a new experimental work on the method of X-ray
scattering under small angles (SSA) of the following devices: a) a frame
cameraj b) point focusing of a bunch by a monoohromator made of a quartz
crystal with barrel-sbaped curved planes; a) a double crystal-spectro-
meter with recording ty a counter. Some principal aspects of the theory
of SSA are considered. The connection of the functions of radial dis-
tribution with the intensity of the diffraction picture is shown. The
corresponding pictures for six types of.submicroscopic structure are
given. It has been shown that the Fourier analysis by SSA permits to
understand the structure of the scattered non-homogeneities.
M. Umanakiy/ Ll-
Card 1/1
"N

/ 61 - ~//
AUTHORS: Sineltnikov, N. N., Filipovich, V. IT., 57-1--29/30
TITLE: Adiabatic Calorimeter - an Instrument for Simultaneous Determi-
nation of Specific Heat and Heat Conductivity (AdiabgLticheakiy
kalorimetr - pribor d1ya odnovremennogo oprodeleniya teployemko-
sti i teploprovodnosti)
PERIODICAL: Zhurnal Tekhnicheskoj Fiziki, 1958, Vol. 28, Vr 1, pp. 218-221
(USSR)
ABSTRACT: The description of the calorimeter was given by the author already
in ref.l. By means of this calorimeter the actual specific heat a
of the material and its heat conductivity land therefore also
temperature conductivity a can be determined simultaneously. The
calorimeter is surrounded by a concentrically located preheater,
which consists of a thin nickel band forming an adiabetic shell
around the sample. The inner preheater, consisting of a molybde,
num wire, is located along the axis of the cylinder. Thus, the
construction of the calorimeter, from the point of view of tem-
perature distribi~tion on the sample practically corresponds to
an infinite cylinder. The experiment for the determination of the
actual specific heat consists in ceding thermostating (mainten-
ance of uniform temperature) of il-he sample, supply of a certain
Card 1/3 amount of heat by means of the inner preheater and temperature

Adiabatic Calorimeter - an Instrument for Simultaneous Determi- 57-1-29/30
nation of Specific Heat and Heat Conductivity.
measuring of the sample after the restoration of thermal equili-
brium. The feeding of the inner preheater is chosen in a way that
in the course of the whole process of preheating the radiation
strength of the wire remains constant. Thus, the temprature of
the shell will reuain equal to that of theperiphery of the sample
(luring the time of the experiment. The measuring of heat con-
ductivity which is made simultaneously with the measuring of spe-
cific heat is based on the properties of the nonsteady temperature
fit-ld of the problem investigated. A formula for ~is derived by
means of which heat conductivity cyn be determined in the case
that the quantity of the heat flow and the temperature increase
at the outer surface of the sample from the beginning of the
feeding of the preheater until the establishement of the equili-
brium state is known. On the other hand, since the total heat Q.
with which the sample was fed, and the total temperature increase
of the sampleA t = Lltj + 6t2 were determined the specific heat
c - Q/4 t can be computed. bleasaring results for the heat con-
ductivity coefficient of powderous quartz at normal atmospheric
pressure and at remnant pressures of an approximately 0,5 and
Card 2/3 5,jo-5 mm mercury column are given. In the first case heat trans-
0

Adiabatic Calorimeter - an Instrument for Simultaneous Deter- 57-1-29/3c,
mination of Speoific Heat and Heat Conductivity.
fer occurs at the cost of air convection, of heat conductivity of
the air, at the cost of the heat conductivity of quartz itself -
and of heat transfer due to radiation. In the second case air par-
tioipates iia heat exchange, air conveotion, however, practically
lacks. Heat transfer is due to radiation as well as to heat con-
ductivity of the air and of quartz. In the latter ca3e the air
practically does not participate in heat exchanLe and heat trans-
for occurs only at the cost of radiationand of heat conductivity
of quartz. Conclusively it is stated that with the rise of tempe-
rature the Ale of heat transfer due to convection decrease at the
cost of an increase of the Ale of radiation. There are 4 figures,
and 1 Slavic reference..
ASSOCIATION: Institute for Silicate Chemistry All USSR Leningrad (Institut
khimii silikatov All SSSR Leningrad)
SUBMITTED: July 13, 1956
AVAILABLE: library of Congress
Card 3/3

24(6)
AUTHORt SOV/57-58-12-12/15
TITLES: On the Theory of X-Ray Scattering by Distorted Crystals
(K teorii rasseyaniya rentgenovskikh luchey iskazhennymi
kristallami) -
1. Theory Without Atom Coefficients (I. Teoriya bez atomnykh
faktorov)
PERIODICALt Zhurnal tekhnicheskoy fizilci, 1956, Nr 12, pp 2716-2726 (USSR)
ABSTRACT: The present paper is a continuation of the papers cited in
references I and 2 and was written in the course of an
attempt to apply the method of Fourier (Purlye) analysis, which
has been employed already before, to the problem of x-ray
so*attering in distorted crystals. The application of the theory
of Fourier expansion allows to obtain simple and clear general
formulae and to relate the theories of x-ray scattering in
distorted crystals suggested by various authors. The paper
consists of two parts. In the first part the general theory of
scattering in crystals containing internal cavities, cracks,
and deformations is presented on the basis of a direct
expansion of the electron density intDa Fourier series without
Card 1/2 introducing atom coefficients. In the second part the same

On the Theory of X-Ray Scat 'tering by Distorted SOV/57-58-12-12/15
Crystals. I. Theory Without Atom Coefficients
theory is shown but with atom coefficients and an indirect
application of tho methods of Fourier analysis. This theory is
more exact with regard to a description of the effects caused
by a shift of the atoms from the ideal positions as compared to
the theory without atom coefficients. The latter one, however,
ha's a less complex structure and permits to employ the methods
of Four'ier analysis of diffusion scattering to a much wider
extent. There exist simple rules for the transition between the
two variants of the theory. There are 2 figures and 6 references,
5 of which are Soviet.
ASSOCIATION: ..Institut kbimii silikatov AN SSSR Leningrad (Institute of
Silicate Chemistry)AS USSRJeningrad)
SUBMITTEDt August 30, 1958
Card 2/2

24(6)
AUTHORt SOV/57-58-12-13/15
TITLE: On the Theory'of-X-Ray-Scattering by Distorted Crystals (K
teorii rapsoyaniya rentgenovskikh luchey iskazhennymi
kristallaidi)
II. The Theory ContaIning Atom Coefficients (II, Tooriya a
atomnymi faktorami)
PERIODICAL: Zhurnal tekhnicheskoy fiziki, 1958,ANr 12, pp 2727-2738 (USSR)
ABSTRACT's On the basis of the application of Fourier (Furlye) expansions
(Ref 11) in the present paper a general kinematio.theory of
diffusion scattering in distortod crystals is constructed. Two
variants of the theory are presented: With and without .
application of atom coefficients. The first variant is mbre
convenient for using a Fourier analysis. The second variant is
more accurate and is applicable in a wide rangei There are ,
simnle rules for the transition between these two variants.,From
the..viewpoint of the theory of diffusion scattering developdd
in the present case the relation between the theories of various
authors of this problem as well as the range of application and
the accuracy of these theories may be determined withou.t
Card 1/2 difficulty. From the present and previous papers (Ref 11) may

On the Theory of X-Ray- S*pattering by Dis*torted SOV/57-58-12-13/15
Crystals. II. The Theory Containing Atom Coefficients
be deduced that the whole Fraunhofer optics of x-rave can be,
established rationally and exactly on the basis of a Fourier
analysis. The theory obtained in this instance exhibits the
character of a consistent theory of x-ray scattering by a
body of arbitrary nature. There are 11 references, 1 of which
is Soviet.
ASSOCIATION: Institut khimii sJlikatov AN SSSR Leningrad (Institute of
Silicate Chemistry)AS USSR,Leningrad)
SUBMITTED: Auguat 30, 1958
Card 2/2

FILIPOVICH., V. W.., Candidate rbys-MELth Sci (diss) -- "The kinematic theory ce
propagation of X-rays by macroscopically isotropic bodies". Leningrad, 1959,
16 pp (Leningrad order of Lenin State Tj im A. A. Zhdanov), 150 copies (KL, lqo 22,
1959,, 108)

FILIPOVICH V N
Theory of X-ray sezittering in dist-3rted polycrystals consisting
of three-dimensiond crystals. Fit* tvers tela ) no,6:1694-1701
Je 161. (MIRA 14:7)
1. Institut khimii silikatov AN SSSR, Leningrad.
(X Rays-Suittering) (Dislocations in crystals)

S/i8l/62/004/011/027/049
B125/B186
AUTHOR: _211JRavi chj_ V-,-!.
TITLE; Theoryiof X-ray scattering by oriented"polymers and other
systems with axial macroscopic isotropy
PERIODICAL: Fizika tverdogo tela,.v. 4, no. 11, 1962, 3244-3253
TEXT: This is a contiouatiort of the author's previous studies made on the.
same subject (V. N. Filirovich. ZhTF, 25, no. 14,' 1,955; FTT, 3, 1961). Two,
variants of a general theory of Fourier analysis of - - ! J"
-X-ray patterns are
considered, without and with atomic factors introduced. The formula for
the intensity of the coherent scattering of X-rays by a given macro-
isotropic body of axial symmetry and the reyers'al of the Fourier integral
may be written in the form
7
.,r ot P1(P,.-#JJ6(pp)#-~#,0)dpk,
Card 1/4

S/181/62/004/011/027/049
Theory of X-ray scattering b3,..,,. B125/Bi86
eirp Its 41di
A (PA: 2x
after having substituted r by r + z, and subsequent integration over a.
0 (Qp) is a Bessel function of zeroth rder, Q(r) is the electron density,
and 'a' Is aof Is0 2n/A. jpo is directed along-#the incident beam and a,
fies in the direction of qbservation. T(r) may be,considered a Patterson
function for the whole body. :.In view of the cumbersome procedure involved
in complete analysis only two pai-ticular solutions to the problem are given.
If 8Z 0, i.e. if there is an "equator" in the diffraction image,
1 0) 2% I.-PT. (P) Is (PP) (9),
(10),
pj(p, O)JO(pp)dp,
Card 2/4
7~*
e-! M -:0 r'~
5

S/161/62/004/011/027/049
Theory of X-ray scattering by*se B125/B186
F(p, '(P.
I. W
TZ is the projection of onto the plane which"is normal to the axis Z of
symmetry. If the packing distanceo'betwt-en the atoms and molecules are
V/
known it is possible to reach conclusions as to the character of the packing
and to make a mean estimate-,ai3 to the shape of the cross-section of the
molecules. That part of 9(r) which characterizes the zero scattering, may be
separated by putting the electron density Q(,r,6) M +.~Q(r).T(r lathe-form
function of the specimen, and q is its mean ele9tron den ty. When
sr
introducing the atomic scattering factors f (a) Qi(r-)e'("*") dv int6 the
intensity formula, then q can be written as the sum of atomic electron
densities. By introducing these factors into (WaAd (6) for bodies with
,axial macrosymmetry the equations
Card 3/4

S/laf/'62,/004/011/027/049
Theory of X-ray scattering by4.. BI;5/B186
Ept p?.'. (p, z) 10 (pp) el(-,,,)dzdp, (39)
#5
and
t ,tr
(40)
(P' ~20 P 19 (Pp) eds, dp
are obtained. The functions 91. show more pointed maxima than the functions
a4
y and exhibit also some "falst",,diffraction maxima.. There are 3 figures..
ASSOCIATION: Institut khimii silikatoy im. 1. V. Grebenshchikova AN SSSR,
Leningrad (Institute of the Chemistry 'of Silicates imeni
1. V. Grebenshchikov AS USSR, Leningrad)
SUBMITTED: June 26p 1962
Card 4/14
'e-
HIM

FILIFOVEH, V.N.
Theory of X-ray scattering in distorted polycrystals composed of
unidimensional minute crystals. Fiz.tver.-tela 3 no.?:1920-1932
a 161. (KM 14:8)
1. Institut kbimil allikatov AN SSSR, Leningrad.
(X rap-Scattering) (Dislocation in crystals)

'M
~VT

ACCESSION Nn: AT4019277 8/0000/63/003/001/0009/0024
AUTHOR% FIUP*Vioh,. V. N-
TITLE: -Initial stages of glass crystallization and the formation of glass ceramics
SOURCE: Simpozium po stekloobroupnomu sostoyanlyu. Leningrad, 1962.
'Stekloobraznoye sostoyaplye, vy*p, 1: Kataltzirovannays. krtstallizatelya stekla (Vitreous
state, no. 1: Catalyzing prystallizatlon of glass). Trudy* simpoziuma, v. 3. no. I
Moscow, Izd-vo AN SSSA, 1963, 9-24
TOPIC TAGS; glass, glass crystallization, glass ceramic, catalyzed crystallization,
liquation, vitrification, relaxation
I ABSTRACT: Since newly formed glitso is in an unstable state, the initial stages of glass
formation must involve some type of relaxation process, 1. e. the establishment of a
stable or meUwtable equilibrium. Two types of relaxation process are usually encountered
side by side: vitdfication as seen In the process of metastable liquation, and crystalliza-
tion, the reladve Importance of each type being determined by the composition of the
glass. After discussing the two..typas of relaxation,. the. author presents a formula:
" A)
1/3 -A
Card___

ACCESSION NR: AT4019277
for the rate of formation of the now
phase aW points out that this rate in maximal at
'given temperaWre defined by:
&#*A I A#A
(2)
T
He then points out that there are two possible mechanisms for the crystallization of a
complex glass: with precrystallization. liquation and without It, sind discusses the nuclea-
tion of the now phase from the point. of view of statistical thermcdynamics, citing
metastab e liquation of the non-eute-We and eutectic types as exiunples. The value of
I W j3 ((be - ) where r is the critical radius of the spherical nucleus and 10,
and Og are the ther2ly'namic potentials per unit volume of the crystal and glass,
respectively) Is calculated for several examples. In discussing the role of the nuclei of
crystallization during the formation of glass ceramics, the author outlines the require-
ments resulting from the need for homogeneity and fine dispersion in the ceramic
material, and discusses the rate and sequence of formation of nmv phases. Finally, the
author discusses the three VW of catalysis used to accomplish the crystallization of
commercial glass ceramics and &MAles the general principles of statistical physics and
2/3

ACCESSION AT4019277

ACCIESSION NR-
AT4019285
S/0000/63/0031001/0053/1)066
AW'HOR: Kalinin&, A. H.; Fili 1. A.
_,_"~ieh, V. N.; Kolesova, V. A.; Bondar
TITLE: Crystallization produces of lithium silicate glass
SOIMCE: Simpozium po stekloobraznomu sostoyaniyu. Leningrad, 1962. Stekloobraz-
noye sostoyaniye, vy*p. 1: Katalizirovannaya kristallizatsiya stekla (Vitreous'
state, no. 1: Ca'talyztng crystallization of glass). Trudy* simpoztuma, v. 3, no.l.
Moscow, Izd-vo AN SSSR, 1963, 53-66
TOPIC TAGS: glags, silicate, lithium, glass crystallization, spectroscopy, absorp-
tion spectrum
ABSTRACT: The crystallization of glass of the L12O-SiO2system was investigated and
the succession of crystalline phases was foutid to depend on the composition of the
crystallizing glass and its thermal treatment. Thermograms of glass are plotted
and the problem of the existence of solid silica solutions in lithium disilicate
in the crystallization products of glass of high silica content is discussed. The
investigation was carried out by x--ray, thermographic and microscopic methods, as
well as by means of infrared absorption spectra. Two kinds of samples were studied:
Card 1/2

ACCESSION NR: AT4019285
some were found to range from the eutectic composition (30 mol.% U20) to pure
S102, and otherswere found to be of a composition ranging from metasilicate to
disilicate (36-48 mol.% LiZO). The temperatures of crystallization were 430, 480,
630, 900-960 C; time: 1-100 hours. Some samples were subjected to thermal treat-
ment over a temperature range of 430-960 C. The appearance of the different cry-
stalline structures (lithium disilicate, metasilicate, cristobalite, tridymite) in'
relation to the varying experimental conditions is discussed in -detail. Orig. art.
has: 7 figures and I table.
ASSOCIATION: None
SUBMITTED: 17may63 DATE ACQ,.. 2lNdv63 MiCL: 00
SUB CODE: HT)CP NOREF SOV: 007 urkm ow
AMR

TOROPOV, N,A.; RUMYANTSEVp P&F.; FjLIFQVICH,-.V..NI.-'
Kinetics of dissolution of CaOt 3CaO.SiO. 2CaO.SiO in the
liquid phase of cei~ent clinker, Mir. fiz. khim. .118 no.4:
974-978 Ap 64. (MIRA 17s6)
1, Akademiya nauk SSSR i Leningradskiy institut khImii silikatov.

L ij0j7+-66,: -EVIP(e)/EPA (s)-2/EW -(I,)/F-PA (w_)-2/EWP(b) Vr/I/GS/jVH_
EWP
ACCESSION NR: AT5013387, UR/0000/65/000/CIOO/0015/0019
AVOLOR: Filipovichs V. N.
TIM: Relationship between meltv~glass, and pyroceramic structures
SOIURCE: AN.SSSR. Institut khimIL silikatov ~trukturnyye prcvrashcheni~ya v
staklakh pri-povyshennykh temperaturakh.(Structural transformation
s in glats at
hi,gh'te-mperatures) Moscow, Izd-vo Nauka, 1965, ly29
TO?IG TAGS: pyroceramics glass stl7UCture
J., ABISTUCT: A classification of mell:s and glasses is made an the basis of them
natturi.i of th eir,crystallization,_w~tich either involves-decomposition into two
or more crystalline phases,or taket; place without it. Thet fluctuational strue-
ture of - glass - and the inhomogeneouti phase structure associated with liquation,
i processes in the glass are considered. . The structure of glass in inhomogeneous,
anti is a function of the conditions of its cooling and thermal treatments.
Modern concepts of the structure -of. complex glasses are discussed from this
point of view. The physical co ntent:of relaxation processes by which a metastable
anti stable equilibrium-is established in glass (vitrification and crystallization)
'art- described in qualitative terms~, The relationship between the inhomogeneous
Card
L
W

0'
~,~ACCESSXON NR: AT5013388
UR10000/65/000' )0
'/0010/0043
~UTHOPI, lilipovich,-Y.
0 of Of
:,TITLE-4. izati'n Asses 'Oriaation oj' riceramice
p
SOURC13: AN SSSR. Insti~ut ~~hixii -silikatoy pr rashcheni
max,
stckl.Ath_pri-povyshcnayk1; temperatiarakh.(Structural transformationd.in glass
high temperatures) Moscow, 'rzd-v* Nauka,'1965, 30-43
-TAW- pyroceramic, glass 'cr~staillization, glass propercy;
TOPM
-'OSTRACT.: The article presents a qualitative theory of the formation of pyro-":
ceramics in the course of crystall:Lzation-of glass startk;ig at low temper~atuke~s.-;
..:The sequence of precipitation of the phasea,the natu .re of the strilngth:'.
-:,Of oderamics the process::of fo-rmation of the pyroceramic, and the role of.)'.he
PYF
%-~chemital composition are'.discussed, In order to obtain high-quality
cerainics, it U necessary to attain a high nucleation rate in thei
crystalli
phase -1~hich precipitates f Irst. This may be achieved. by. utilizing the Jiquatvln
phenommon or by. -readi
using' ly.crystallizable.impurities which are sparingly'
t -treatment-is carried out prope
-soluble in glass. If-the subsequen heat yj
ne d1sper-Siori of,the first,phase,automatically,leads to a fine dispersion of-,',
Carc:
7'

.,I,;':.-ACCESS3'.ON NR: 'AT5013388
en
the subsequent gth~of the pyroceramic as a whole. All
-phases and to a. Mgh~ str
!.,degrees of.heat treatment should-be chosen at the lowest possible temperature
-,.-whLehi however* are combined with reasonable perLods of heat treatment, This
.!_-condftion follows from the requirenent that the crystal grwch rate be optimally
i',slow. The strength of the pyroceramLes obtained is due tc the high strength of
!.."the 9ITLe crystals and thin glass-interlayers; the limit of Lhis scrength is the.-,
i:,theoretical strength, and also the-strength of the bonding between the fine
'11~crystals (generally speakLng,._metastab1e_pfia'ses) and-the glass (small4ij,-so that
the development of cracks along thocry-Stal boundariao'Le hindereci. A pyro-
-!~:Ceramic Ls a stable _jdase-crvstallLne'avstem:---- the--transition to -&--stables
- _meta

..;0046 1 Intm loan I
--'VR/OM/65/000/WO,10l2A/0l34
ACCZSSXIN U AX50LI391
U
-darivg heatli of ~Uthiuvi aluminor
"the. cristallizatlida him
Trnz, Of quence mg
o5
AN SSSR. xvAtitut tchisdt,; sillliAtQ4 tt-uktuxnyy prm-ashchaviya ~V'
CaNTS-truc
polryshe kh tes"ratt tural tranvf Orimatile" in. gl" at-,
Una) 4 moscm Xad-vick SAUU,1-:19650 17A-134
TDPXC.IAW: lithiumi alumLabAlicItep lithitu glass,
"a i4mucturs xxaj dUfraction
-7h6 article Is io An *-ray. dif f ractiors study Iof tho'cryaWlt
"',7ABSTRACT:
tion 61!. cartaft glasses of the tOCMTY SY4t" Li- 0 L "007 during heating 7
2
startug at lov tem"Vaturese ~ tom-temperature crystafolgti6 proceed@ by
_~'-~'Overconing the lowest energy barders.-uhich leads to the formation of metastable
:crystallf~m phases. Ch prolongeCemposures to high temperatures, recrystalMW-
Ent-
-;-tL*n lAto stable phases takes placm in accordance with the phase diagraim.
--~-phasis Lis placed on tho'close'relAttionship, between the structures of the
glass and the* cvystallf~me', phases which first precipitate at low--ten-
afraturesaiy1t. ~*.,concludsd that Illass of the spodmene-6omposiLtion -and Qtktet'::-~

A
;
;!
0H RRI AT5013391
jACjZ 91
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,
j
Gueryptite.2
Vi -17 Role %) have - a
do Conteut'( ft
m~~ 81a, sea with a medUa role of -ions oo~ 104 aiff using
assive
h
e
p
or to P-quarte structure., 'T
sea is notedo t4e cracking-
rOC6131
j
at
on p
allir
in low-teaq)eratura Cryst
'
iftation.ja attributed to the ce' Ciri
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I
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fglass during c
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f aluminum and lithO"
o

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0f.& solid solution
.
14
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,
,
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lias-

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SIOB CME
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2lDec64

005
..REIF 9091.

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w. 1.
till

~0 kt r zld,~.-- oakea
t first at low-tempera
Wtiit t1iirt- -Prec. 0 tate;
ture. It 1EL, isd spodlawn*
-'ed-
(4-17, note have a
-Ma,
_i- P-0
i rAt-M-1: IAt fit a
solutLon of jXq"rt&& oiii art. lum - 4 figure* ond Itibia.
r7 T7
ASSOCT&
fti- 'edshchik6nL kkadmitLL
SSSK (Lnstitute of' Silicate Chemistry, AcadeL_t of Scievices, MR)
(!UXM=D- IlMar63 EXCL.- 00 ME-IMR. W-P
PC) PEE SOV: 005 OTHER: 007
N1 "N
E!
W

L 2213~46' EWP(9)1)W(
ACCES3100 HR: AP5022274 UR/0363/651001/007/1189/IMO
SJ6.41+546.46+546.264
PTIM, Kalininal, A. It.; Fulpovickg V. ff.
TITLE. ClystallizAtiog -Jdas he Cel~- Sio a steftl~
SOURCE: M SSSR, Imstiya, Nearganicheaklys materialy. v. 1. no. 7. 196,50
1189-1200,
"TOPIC TAGS: silftati glass, crystallization
ABSTRAM paper presents, results of-an X-ray diffractioll stwly of_crystal-
lizatLon Of calcium magneGiumAllicate glasses dur1mg beatiq, for -purpose
_the
of determining their usefulness as starting substances - for the development of nw
glass-crystallLne materials. -The glass compositions consideved correspond to
the 1two chemical compounds CaO.NgD.ZS102 (dLopsLde) and MaO-KSO-MOZ
(oke: ite) and a series of eutectics. X-ray phase analyaft was the princ
ipalL
Metb)d employed; additional methods were thermographLe-and alcroscopLe analyses..
The crystallization -was aa=led out either by a single stage or a multistage
thennal treatmmto .-A tendency for metastable crystaIlLue phase$ rich in-alkaliule
earth oxides to. precipitate first. was observed, A possible Interpretation of the
I ipes obtained is give's In terms of the. chemically, inhoweenems structure of tin
WN

KALININA, A.M.; FILIPOVICH, V.N.
Crystallization of glasses of the system CaO - MgO - SiO2. Izv.
AN SSSR..Neorg. mat. 1 no.7:3.189--:L200 Jl 165. (MIRA 18:9)
1. Institut khimii silikatov imeni I.V.Grebenshchikova All SSSR.

ill-.q sitT uq, &
piudfA with
untif LTY--eAd
tT4
rag

1 67
,
i
d
d d
lr
E
a
% prem
filwed, alkwO W, 4Kt*lc; oul.
und thcn cvippd. i-I wj;7 at
ru O'ut in ac=d-
for mg!dicimJ kzWl
M.

SHERBAN, P. (Serban, P.]; TASHKY, TS. (Tasca,, T.); FILIPPOVICHI, A,
[ZLliko H. [Cons tantine,scu,, M-I.;
y~ _AJI KONSTANTINESKO
, ;A a,
KOSTYCHESKOP P, LCostachescup Po)'(Bukharest)
Letterer-Siwe disease (tumorous form with lipidosis). Arkh. pat.*
27 no-5:19-24 165- (MIRA 18:5)
w, P~- 05R.
A

SISAMqj H,M.;,-_Fl~~IPOVICI# I.I.
Synthesis of protiins and cellular structures. Analele biol 14 no.2s
39-56 Ap-Je 060. (Em 9tu)
(PROTEINS).. (CELLS)

FILIPOVICIS J.
"The Forest and Arborescent Plants, Basic Elements in the Aesthetics of landscaposem
p. 22 (Ra~vista Padurilor, Vol. 68, No. 9, Sept. r:.53, Bucuresti)
Vol. 3, No. 3
SO: monthly list of East European Accegsions,/Library of Congress, ell arch,1954, Uncl.
-----------

FILIPOVICT, J.
"Problems of watering in siivicultural technique". p. 107, kREVISTA
PA=ILOR. Vol. b9. No. 3, Mar. 1954, Bucurest, Itumania)
SC: monthly List of East European Accessions, tZEAL), La, Yol. ),
No. 12, vac. 1954, Uncl,

FMAUVOCI, J. I qmmmm
Pseladotauga taxifolla Britt. in the Nadragu baain, Cavaran Forest District.
p. 449 REVISTA PADUfdI0Rq WCURESTI.. RUYANIA Vol 70,, No. 10, October 1955
SOURCz.- East European Accessions List (EEAL) LC Vol 5., No. 41, June 1956

GMELPIEZ11)) !1.1 dr. inj,.; FILTPOVICij J., co-it'. ilv!.
.Fropertlei and uses of -t.be tica.,. of thia lp~.lies. Ind :
Diii-mabil 14 .7,-, '63.

MILC,Jil;,VlC, B.1).; FIL.El'OVIC--MC),~~"IOVLJi,',VkC, V; DJI'FOVI~:, De--Inka
ReIntion between the nature and the poisition of the queen and
the changed structure of bee colony. Bul n~, nat !ANIJ 3? no.9.,,-;]-
44 163.
Dependence of socioty on the -ohse
of queen's 11fk, lbid.*145-49
Role of out-of-function. cmeen in a col( ty of a von.,;tunt numl,,or
of bee workers of (Ufferent age. Did :51-51
-i
Cueen substance and the mec~Anism of queen effpct in honeybee
colony. Ihid.:55-61
1. Submitted March 31, 1961.

GASPAROV,, Antud,, mitetaki pWwvniko doc.., dr.; PETKOVIC,, Darinka, dr,;
TILIPOVIC-RISTIC, Branet, dz~.; PRTROWC,, Milentije.. sm. kapetanv dr.
Aspiration biopsy.of the-mucous membrane of the lar 5 intestine.
(Tecbnic and histological results in 1,,336 patiental. Voj.s=.preglo
18 no.3t269-272 Mr 161.
1. Armijoka bolnica u Beogradu,, Interno odeljenje.
(COLON pathol) (BIOPSY)

r C_- f-171,.
f
177,7777.
qg"
V,
'k
i-6"4 0 cm. caldficadotLAaman
di.
Nway 6'requfxev~duts for C"iAtlon of several
fm
"U'l4edolgAn boadiands. Gemgi Tilipovski and
OV -
ismzbjr-- ----------
;~~Tbs* Touovdd (UuI*.'Skcpk; YuAgSvla). God
_4
OW Wdsko~-.Sowimima_ Fak. U*iv.,Supjc 6-7, &-1n
-"XPub.
'-19M IMXin CyrilUc. blan).-A
i44- itwr exib6dying results, 61 an CIV=ive xco.~
0
o

ITEiGFBARIto V.; ,*,I--;IIC, M.; FILIP(LVSKI, G.; A.i -:.
Classification of soils of Yugoslavia. Zemljiste b-ILiks. 12 no,
1 1
1/3-.21-44 Ja-D 163.

FILIPOVSKI, G.
1,1--. infints, water,
COM7,11-Tiff-On-of boron solnble compounds ii.-i some sed
and soils in Macedonia. Zemljiste biljka 12 no.1/3:11.2-1419
Ja-D 163.
1j, Faculty of Agriculture and Forestry of the Uniw-rsity of
Skopje, Skopje.

Fuipo-gs
TWMOLOGY
PERIODICAL: AUTOMOUL. 70L. 3., no* 2, Feb. 1959
Filinovsky, 0. Economical operation and its effe~,t on the design of.,
motor huses. p. 60.,
-JT-. Forduction of Cars in Sweden. p, 66.
Yonthly List ur &-vat "-P-6411 Acdogglonn (IM!
Flay 19-59Y Unclass.

IV r

v i'

it at.. C 'A47, 41 73~--
fravik-is
-pe) wn~ ttted ~- mbbit4- Th
c cafW'y
ii-ac-mutc. frittlilas 6, Ta 1 Ott! grcatt-t d7rct q thc
in (if the attitl"N-
~J"f' "lilt mid jrji;Tej5

crIN wete Albnattd b ? (mg, 5 thq-~ I-At. r-11,011 -
fru
Im
'0. (fraction V), foliq%vull by I extits. -Kith CIICII (f -action
;c-141;6A 1,O)II-etliff (fract aft 1),
TheL rc 3 times-widl Z,7r, AcUll ar'd 3
1"
c cxt-x. with OAX N -A N-ffract6i 5).
Illo r4okliffilig
'If I was c*VL G tim" V061 0.11 "M Nafill Orat, Wit 0, tucilimi-

Nat) If I I1(;n*
llrc%'Itt~ ItA ifi~ itsi4an. "ttaled With 10%
f; (fcjrIbti 7); -Afj. NLO smfwu5jQvi qf th : drI,-J
frA'Mm'5 wlv tl~rit for bz its. !Tlt~

QRUI)ZINSKAj PArbaral FlIJPDWICZ, Aliajai
Two cades of ph6togehid opliapay vith autaprovoking of
saisures. Neurol, nautochir. psychiatb Pol. 15 n6.3:
485-488 MY-Je 1656
1e Z KUniki Reurolooicinej Slaskiej AM (Kierownik:
prot. dr, med. WA Ohlopidki)t

FUUAN,.A.D., kand. ~tekbn-e.--.nault;.~-SADOVSK-IYj G.I., kand. tekhn. nauk;
ZHMURKO, P.T., gornyy--inzh.;JjUU-LINKOV A.1. gornyy Inzh.;
~-J-
KOREN IKOVP I E.N., gorvyy- inzh.; SHABLYGINp A.Lt kand. tekhn. nawc
Searching for optimal parameters of the induced block oaving system
at the "Zapoliarnyyw mine. Gor. zhur. no..6%19-24 Je 165. (IaRA l8t7)

WKS-WMMSKA, A.; IAPMSKI, A..,; FILIPOWIC.Z,, A.; GRABOWSEA, U.; RXITMISKA,
H.; WITKOWSKA, B.
Significance of agglutination reactions in dysentery in children. Pediat.
polska 34 no.2:145-152 Feb 59.
l**.Z II Xliniki Chorob Dziaoi A. M. w (Wansku Kieramnik: doc. dr made
Aa Marlm-Sakrzewska i a Wojewodzkiej Staoji Sanitarmo-3pidermiologiezuej
W Gdansku Dyrektor: dr med. A. Iiapinski. Adres: Doe. dr med. Harks- Zak-
rzewska, ifarazawa, ul. Sienna 60.
(DYSMMIRY. 33ACILURY, in inf. & child.
fecal aggl-~A. test (Poi))
(AGGL'UTMTICK, :
Shigella agglut. test of faces in dysentery in citild. (Pol))

VIIJ,OSZEWSKI, 3dward; DYSZY-IAU13E, Barbara; ~ILIPOWIGZ 4Aijt3A--
Bone marrow In -rheumatio disease in children. Pedlat.,polska 35
no.14-19 Ja. 160.
1. Z Kliniki Chorob Dzieci A.M. w W&rsslxwis- Kierownl3c, prof.dr.
med. R. Baranski.
.(RMWMTIG FIVER pathole)
(BONE MARROW pathol.)

FILIPOWICZ A.; CRUDZINSKA, B.
The clinical picture of temporal seizures in childr(m accor-
ding to data of the Neurological Clinic of the Silesian
Academy of Medicine In Ubrzw. Neurol. neurochir. psychiat.
pol. 13 no.6:815-818 N--D'63
1.~ ~'Kliniki Neuro"&Ogicznej Sl. AM w 2hbrzu; kierownik: prof.
dr. W. Chlopicki.