SCIENTIFIC ABSTRACT ORLOV, V.P. - ORLOV, V.V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001238220011-1
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 3, 2017
• Document Release Date: June 21, 2000
• Sequence Number: 11
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

L
D
AUTHOR t Adam, N. V. ; Ben'kova , N.- P. ; Orlov,_ V. , P. i Tyrumina , L. 0.
ORG: none
Ix
TITLE: Secular variations of the geom, gpeti~. f ield based on data of a spherical
analysis
SOURCE: AN SSSR. Institut fiziki Zemli. Nastoyashcheye i proahloye uagnitnogo polya
Zemll (The present and past of the earth's magnetic field). Moscow, Izd-vo Nauka,
1965, 18-33
TOPIC TAGS: earth magnetism, geomagnetic measurement, spherical analysis, secular
variation
ABSTRACT: This article concerns the principal geomagnetic field studied by the method
of spherical analysis and its secular variations. The authors derive an analytical
expression which approximates secular variations. They examine on the basis of this
analytical expression certain problems of the nature of secular variations, and
attempt to use the results obtained for forecasting the field. The authors, having
previously used spherical analysis for plotting charts of isoporic lines in the polar
caps and having obtained sufficiently good agreement with charts plotted from obser-
vational data, conclude that the sum of. the first six term of a'spherical harmonic
aeries permits representing the morphology of secular variations with the same degree
Card

L 10913-67
NRt AT6021011
of schematization. This scheme is characteristic of modern world isoporic charts
plotted graphically from the data of magnetic observatories but without the element
of subjectivism inherent to the graphic method. Spherical analysis is recommended
both as a method of analytical representation and as a method of plotting isoporic
charts. Since one of the important characteristics of the planetary part of secular
variations is western drift, the authors estimated western drift for individual har-
monics by means of spherical analysis of a constant field and secular variations, and
by the shift of the centers of world anomalies. They also examined the latitudinal
and longitudinal distributions of drift velocity. The velocity values obtained from
the coefficients of spherical analysis of world charts of the total field for the 1955
epoch, and from the secular variation charts for the period 1954-1959, are calculated
The velocity values were found to fluctuate within -0.47 to +0.12 deg/year, two
characteristics being noted: 1) a decrease of the velocity for high-latitude obser-
vatories and 2) asymmetry in the distribution of velocity between western and eastern
hemispheres. The velocity values were higher for western observatories than for
eastern. To extrapolate secular variations to the present or forthcoming epochs, iso-
poric charts of 1954-1959 were used to forecast the secular variations for 1960--1965
A comparison of the coefficients of the spherical analysis of secular variations re-
vealed that, with the present accuracy, the coefficients higher than the third order
can be considered constant, and the coefficients of the first three orders change in
time within a set interval, fluctuating about averages that are constant or almost
constant in time. It is concluded that during a 50-year period the magnetic moment
can decrease by 0.5 . 1025 CGS, and that the position of the geomagnetic pole will

NR, AT6021011
shift along the latitudinal circle from 291*46' to 291*52'. Combining paleomagnetic
and analytical studies of the geomagnetic field can be quite fruitful, in particular
in regions west and east of the centers of world anomalies. Orig. art. has: 3
formulas, 6 tables and 6 figures.
SUB CODIt 12,06/ SUBM DATE: 2lSep65/ ORIG REFt 007/ OTH REY: 004

L 07493-67 LW(I)/PCC OWMD
ACC NRs AT6021014 SOURCE CODE: UR/0000/65/000/000/0066/0076
AUTHOR: Orlov, V. PI.; Sokolov, V. P.
ORG: none
TITLE: Secular variation of the 1!!!~saneti~c field and its anomalies
SOURCE: AN SSSR. Institut fiziki Zsul . Nastoyashcheye i proshloye sagnitnogo poly&
Zemli (The present and past of the earth's magnetic field). Moscow, Izd-vo Nauka,
1965, 66-76
TOPIC TAGS: secular variation, geomagnetic field, magnetic field intensity.,
ABSTRACT: The authors note the following with respect to the secular variation of theI
geomagnetic field and its anomalies. A characteristic feature of the overall pattern I
of the secular variation is that the changes of the geomagnetic field strength in the I
Southern Hemisphere are appreciably greater in magnitude than in the Northern Hemis-
phere. Since about 1955 the changes of the secular variation in the Soviet Union and
adjacent territories of Mongolia and China have become more pronounced than in the
preceding decades. The changes of the mean annual values of the secular variation
from 5-year period to a 5-year period in Eastern Siberia exceed 30 y, reaching 45 y
in certain places. Such marked changes have not been observed in the Soviet Union in
any case since 1825. The values of the secular variation in the Antarctic are much
greater and the pattern of its distribution is more complex, owing to the presence
Co;d 1/2

1 _Q7493-_6J______
ACC NR% AT6021014
of the center of the secular variation in the South Atlantic, than in the Arctic. At
present the south magnetic pole is shifting northward and westward. In the region of
Southern Africa and adjacent regions of the Atlantic and Indian oceans is a world
magnetic anomaly which is manifested by low values of H. The central part of the
region of low H values coincides with the focus of the negative values of its secular.
variation. The annual decrease of H in this region during the past 30 years was
6D---80 y/yr for a total of more than 2000 y. Thus there are grounds to assume that
this world anomaly owes its origin to the secular variation. Studies to elicit anom-i
alies, of the secular variation permitted the conclusion that an investigation of
these anomalies can be one of the methods of studying present-day tectonic processes
and the possibility is not precluded thatalong with other types of geophysical inves-i
tigations the anomalies can be of considerable importance for forecasting earthquakes.:
Orig. art. has: 6 figures.
SUB CODE: OB/ SUBM DATE: 21Sep65/ ORIC REF: 007/ OTH REF: 002

ACCESSION NR: AP40Z4736 8/0109/64/009/003/0553/05S6
AVTHORt Orlov. V" P.
TITLE: Calculating the propagation constants of a complex-shape waveguide by
coordinate conversion
6OURCE: Radiotekhn*- i elektronika, v. 9. no. 3, 1964, M-S56
TOPIC TAGS: waveguide. complex shape waveguide, waveguide propagation
cpnotant. coordinate conversion, irregular waveguide
ABSTRACT: The coordinate -conversion method is applied to an axially regular
waveguide having a complex-ohape croon-section. By introducing a now
coordinate system - curvilinear and nonorthogonal in the general case - the
complex cross-section can be turned into a simple planar figure, such as a circle
or a sguare. The original w&veguide is thereby converted Into & circular or
square wavegulde filled with a nonhomogensous anbotropic medium; the method
cmd Ila

ACCESSION NR: AP4024736
of eigenfunctions becomes applicable. The boundary problem for a waveguide
filled with a homogeneous. isotropic medium is described by the Maxwell
equations. The latter are transformed for a curvilin*ar nonorthogonal coordinate
system. TE- and TU-wave systems are determined by A. 0. Sweahnikov's
method (Zh. Yy*chial. matem. I matenLfisiki. 1963. 3. 2, 314). 04ig. art. has:
I figure and 11 foruml",,-
ASSOCIATION: none
SUBMITTED; 30M&r63 DATEACQ: l0Apr64 ZNCL: 00
SUB CODE: W NO RZIr SOVt 006 OTHER: 00 1
6
CWd 2/2

ORLOV, V.P.
Calculation of the propagation constants of wave guides with
complix shape using coordinate conversion. Radiotekh. i elektron.
9 no.3:553-556 Mr 164. (KIRA 17:4)

ACCESSION NR: AP4043668 S/0109/64/009/008/134511356
AUTHOR- Nikol'skiy, V. V.; Sukhov, V. G.; Korniyenko, D. L; Orlov, V. P.
TITLE: Calculation of a rectangular waveguide containing a longitudinally-
magnetized ferrite by the eigenfunction method
SOURCE: Radiotekhnika i elektronika, v. 9, no. 8, 1964, 1345-1356
TOPIC TAGS: waveguide, ferrite, longitudinally magnetized ferrite, ferrite
containing waveguide
ABSTRACT: Based on the Galerkin-Ritz theory, a method for calculating the
propagation constants of and fields in a rectangular waveguide partially filled with
a longitudinally- magnetized ferrite it; developed. The problem is solved as a
boundary problem for the waveguide cross -section; Maxwell's equations are
used. Phase shift and attenuation are calculated for a wide range of ferrite
characteristics,o/sizes and c6afigurations of the system. Programing time and
Card 1 /2.

ACCESSION NR: AP4043668
techniques are discussed as well as the accuracy of calculation. Fundamental
characteristics of the system are -clarified by isolating various modes and by
analyzing their spectral composition. A few numerical examples are calculated
and data presented in graphical form. Orig. art. has: 15 figures, 9 formulas,
and I table.
ASSOCIATION: none
SUBMITTED: ZZMay63 ENCL: 00
SUB CODE., EC NO REF SOV: 005 OTHER: 005
cmd 21Z

NIKOLtSKIY, V.V.; SUKHOV, V~G.; KORNTYENKO, 0.1.; 0 IOV&-Il--
Design of a r6ctang-ular wavegulde with ferrite and ferr!te-
dlelectric fillirq and longitudiraj magnetization. PaiLlotakh.
i alektron. 10 na.110992-1999 V 165. (MIRA 18i11)

nR!,OV, V.P.,- POSTNILIKGV, V.V.; :;HTROBCKCV, M.Ya,.
Evaluation ef oy.7gen ~--)nt.--nt of germar,--umi and Ft'-':7cn
Obtained by vaculm spy&Y coa-ing. 'lhur.f.z.ktAv. 39 nc.~'U:~573-
2576 0 165, (MIRA 18:12)
.A. GorIkovsIx-y '.nvt.~',ut.
Submitted Jane 26,

AM17183

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ORLOVI V.P.; SHIROBOUN, M.Ya.
Idi&ption f nonpo2ar mo2.eau'--.s :,n g--i-w-n-lur arfl F ' icr-ri.
Zhur, riz. 1--him. 39 no.9:2215--.~218 S 165. ',8:10)
1. Gorikovskiy issladovatell3kiy fiziko-taakhni~tPEkly
institut. I

NIKOL I SKI Y, V.V. ; SUMOV, V.G. ; KOftMIYFNKO, D. I.; Mi LOV, V.P.
Design of a aquaroi waveguide with a longitudinally magnetized fer- -
rite using an eigenfunction method. Radiotekh. i claktron. 10 no.4;
618-625 Ap 165. (11,11RA 18 s 5)

8(2) PHASE I BOOK EXPLOITATION SOV/1290
Besekerskiy, Viktor Antonovich, V.P,_Orlov Polonskaya, and
, L.V.
S.M. Fedorov. Proyektirovanlye sledyashchikh sistem maloy moshch-
nosti (Design of Low-power Servo Systems) Leningrad, Sudpromgiz,
1958. 508 p. 9,000 copies printed.
Ed. (title page); Besekerskiy, Viktor Antonovich; Scientific Ed.;
Khrushchev, V.V.; Ed. (inside book): Shaurak, Ye. N.; Tech.
Ed.: levochkina, L.I.
PURPOSE: The book is intended for engineers engaged in the design
and development of servo systems. It may also be useful to stu-
dents of vuzes specializing in automatic control.
COVERAGE: The authors describe the principles of designing low-
power servo systems (100-200 watts). The first part of the book
deals with general problems of synthesizing servo systems. It
also discusses the requirements for stability, accuracy, and
smooth operation of servo systems at low speeds. The second part
describes problems of synthesizing some special types of* servo
C a rd;;;~

Design of Lower-power Servo Systems SOV11290
systems, such as gyrostabilizers, amplifiers with large
feedback.and servos using stabilizing and integrating systems.
The third part discusses problems or designing individual
system components. The material of the first and second parts
is based onta dissertation written by V.A. Besekerskiy. The book
does not discuss the theory of automatic control. The authors
assume that the reader has a sufficient background in the field
of automatic control and telemechanics. They thank Professor
D.V. Vasillyev and Docent V.V. Khrushchev for reviewing the
manuscript. There are ll~ references of which 104 are Soviet
(including 7 translations), and 15 English.
TABLE OF CONTENTS:
Foreword
3
Card 2/21

9(6) A6%003/0-1/003/016
90124 M
AMWHSt 60 Candidate of Technical Sciences, Senior Staff Member,
W-1, 3416,A., andidate of Technical Sciences# Docent
TEM: A FeLlow-W botrument System With Protection from Idle Phase
voltage
PEMD31;AL: Inestlys vyssh1kb uchebzWkb zavedenly. Priboroetroyanlye., 1960,
Vol. 3,, Nr 1, PP 18-25 (WSR)
ABSTRACT-. At the Eafedra avtonatikl i telamekhaniki (Chair of Automation and
Telemobanic4 the authors developed a follow-up system (Figure 1)
with a small-size amplifier (Figure 2,, photograph) In which a single
cycle Imy demodulator and a single-cycle key ap~hzlator8bn semd-
coadwtor triodes (FIgure 3) are used as a pr-ofWa-tion against the
Idle phase voltage. The calculation results of the formula for the
dstwlalmtlon of the tray%=4 sion coefficient and time ConaLtlot Of
the pmtection device are given, and the tranamlesion function and
the characteristics of the follow-up system are Investigated mathe-
wtioally, It in pointed out that the device Is very reliable at a
Card 1/2 frequency of one cycle and an oscillation amplitude of 16'. The

S/146/60/003/01/003/Olt'D
D002/DD06
A Follow-up Instrument System With Protection f!rom Idle Phase Voltage
curves showing the oscillations of the follow-up axis are illustrated
(FIMe 5)., and show that the amplitude error is very meall. The
article vao recommended by the Chair of Automation and Telemechanics.
There are 2 photographst 3 diaVams,, and 1 graph.
ASSDCIATIDE: Lealngradskly Inst1tut tochnoy makhaniki i optiki (Leningrad Institute
of Precision Mechanics and Optics)
SMMIM: November 21., 1959
Card 2/2

SOVA 24 - 57- 5- 5794
Translation from: Referativnyy zhurnal. Mekhanika, 1957, Nr 5, p 108 (USSR)
AUTHORS: Orlov, V. S., Charnyy, 1. A.
TITLE: Determination of Stratum and Well Parameters by Means of an
Isobaric Chart (Opredeleniye parametrov plasta i skvazhin pri
pomoshchi karty izobar)
PERIODICAL: Tr. Mosk. neft. in-ta, 1956, Nr 16, pp 113-1Z4
ABSTRACT- The representation of the potential O~ kp/~, is used in the form of
I N r2 + 6i2 Zrb cos(O-CLj
0 + -41-T- 1; q i i I (b (r, 0)
k i=1 loge 612 r2 + R 2r6i cos (0- a
Rk2 k
14ere zk is the mean potential along a perimeter rRk-, 4~ (r, 0 ) is
a regular harmonic function; p is the pressure; k is the permeability;
~L is the absolute viscosity; 6 i and ai are the ROlar coordinates of
the wells; q = Qi/h where Qi is the yield of the well and h is the thick-
Card I/?- ness of the stratum. The form of representation used above is

SOV/1 24- 57-5- 5794
Determination of Stratum and Well Parameters by Means of an Isobaric Chart
suitable for a regi(,n which is homogeneous and isotropic relative to the. parameter
a- = kh/~L of a piecewise nonuniform stratum. A circle of radius rh is drawn upon
the isobaric chart of the deposit, and the pressure ( and hence the potential) is
determined along the points on the circumference of the circle according to the
isobaric chart, which enables the author to set up the pressure function inside the
circle. The parameter a- is determined by comparing the pressure values obtained
by the method given above with the values given by the isobaric chart inside the
circle. The method of determining the reduced radii of the wells is given likewise.
A numerical sample is worked out. The method is incorporated in the book by 1. A.
Charnyy: Osnovy podzemnoy gidravliki (Fundamentals of Underground Hydraulics)-
Moscow, Gostoptekhizdat, 1956.
V. Ya. Bulygin
Card, 2/2

ORLOV, V. S., Cand Tech Sci -- (diss) "Isobar charts and
their application to the analysis at and regulation of the
-04 WIJA-~
process of expi d:t~~ of petroleum deposits." Mos, 1957.
16 pp (Min of Higher Education USSR, Mos Order of Labor Red
Banner Petroleum Inst im Academician I. M. Gubkin), 110
copies (KL, 52-57, 107)
_ 66 -

AUTHORS: Boriso . Yu. P., and Orlov, V.S. 93-57-7-11/22
TITLE: Interpretation and Use of Bottom Hole Pressure Build-up
Data for Isobar Map Construction (Interpretatsiya
dannykh vosstanovleniya zaboynogo davleniya i ikh
ispol'zovaniye pri postroyenii kart izobar)
PERIODICAL: Neftyanoye khozyaystvo, 1957, Nr 1, pp 39-43 (USSR)
ABSTRACT: The article analyzes the bottom hole pressure build-up
process and the possibility of using the data for isobar
map construction. The build-up characteristics for shut-in
wells producing from infinite formations of homogeneous
fluid and from finite formations of nonhomogeneous fluid
are defined by equations. Theoretically, the relationship
between the variation in pressure with respect to time
must be linear, but in practice it is not so. Miller and
co-workers (Ref.61, using an electrical analyzer, and also
Card 1/3

Interpretation and Use of Bottom Hole (Cont,) 93-57=7-11/22
the All-Union Instrument Scientific Research Institute M11),
using a hydrointegrator showed that the 1-i-near relationsMi.)
is disturbed initially and that afterwards the bottom pressure
is proportional to the logarithm of time. FUTther-more, VNII
revealed that the coefficient of the angLe of the linear
relationship can either decrease or increase depending on
variation in the formation segments away from the well
[Fig. 11. An increase signifies a drastic decline in the
formation's permeability and a decrease stgnifies a rise in
permeability. The relationship between pressure and time for
a nonhomogeneous formation can deviate from the straight line
in either direction (Figs. 2,3). Up till now scientists main-
tained that only the permeability must be determined, and in
known cases of well imperfection also the piezoconductivity.
However, this may lead to inaccuracies since Lhe error
occurring from the calculations of the drainage area with the
aid of plots devised by V.I. Shchurov* and M. Muskat is
substantial and I.A. Charnyy's Ill evaluation of the drainage
radius is unacceptable. The authors conclude that the
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InterT,retation and Ilse of Bottom (~'ont.) 93-5 7 - 7 -1!/ 2 2
formation permeability around the wells, the Lmperfection of
wells, and the variation in per-meabtlity of segments away
from the wells can be determined with the aid of pressure
build-up curves. The data on pressure build-up are used for the
construction of isobar maps. Isobar map construction requires
knowledge of the manometer's time lag at the bore hole arl since
this is quite impossible to obtain the authors suggest taKing the
average pressure around the well and calculate it with the aid of
pressure build-up curves and thus eliminate the necessity of stop-
ping the well for the determination of the average pressure. An
isobar map constructed on the basis of average pressure will not
reflect the actual pressure distribution, but will eliminate
arbitrariness in the construction of static pressure maps. This
method of calculating average pressure is simpler and more reliable
than the one proposed by D.R. Horner iRef.3... There are 3 figure:;,
and 6 references of which 3 are English and 3 are soviet.
AVAILABLE: Library of Congress
Card 3/3 1. Pressure-Applications

11(0) sov/93-58-lo-ii/19
AU79DR: M*harskiy, E.D. and Orlov, V.S.
......... . ...........
TI=: Fluid Conductivity Estimation From Field Data on the D. Formation of
the Bavly Oilfteld (Otsenka gidroprovodnosti plasta Di Bavlinskogo neftyan-
ogo mestorozhdeniya po dannym promyslovykh issledovanty)
PMODICAL: Neftyanoye khozysystvo, 1958, Nr 10, pp 48-54 (ussR)
ABSTRRCT: In oilfteld development the fluid conductivity of geological form-
ations is determined by means of the formula E - kh/At , where k is the
permeability of the reservoir rock, h - the effective energy of the reservoir
rock, and At - the viscosity of the reservoir fluid. Wben these properties
are individuaily estimated from geological and geophysical data the results
are inaccurate. The accuracy of the results can be improved by determining
the entire kh/)L complex for each sector of the formation with data obtained
by hydrodynamic methods (Plef 1-2]. Bottom-hole pressure variation curves
based on hydrodynamic data can also be used for determining the imperfection
of wells Iflef 3]. When the pressure distribution in the formation and the
yield of the wells are known the fluid conductivity in the sectors of the
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Fluid Conductivity Estimation (Cant.) sov/93-58-lo-ii/19
formation as well as the imperfection of the wells can be determined vith the
aid of isobar maps. In case of plane parallel or plane radial flow the fluid
conductivity in sectors of the formation without exploitation or injection
wells is determined by the formulas of Darcy or Dupuy (Ref 41. In case of
complex flow and the presence of wells the fluid conductivity is determined by
another method (Ref 51. The authors employed hydrodynamic methods for de-
termining the fluid conductivity in the D formation of the Bavly Oilfield.
The curves of formation pressurv variatiA for certain wells are shown by
(Fig. 1). The isobar map based on strictly reliable data is shown by (Fig. 2).
The data used in drawing the isobar map and the pressure build-up curve are
given in the Table. The authors conclude that the fluid conductivity values
obtained with the aid of the isobar maps are completely reliable for the con-
struction of fluid conductivity charts such as presented by (Fig. 3). There
are 3 figures, 1 table and 5 Soviet references.
Card 2/2

11(0) SOV/93-58-3-1-9/15
AUTHOR: Andrimov, R.S. and Or
TIME: Determining the Effective Depth of Bullet Penetration in Oilvell
Perforations (Otsenka effektivnoy glubiny proniknoveniya puli v plaBt
pri perforateii skvazhin)
PERIODICAL: Neftyanoye khozyaystvo, 1958, Nr 11, PP 49-54 (USSR)
ABSTRACT- In formulas the hydrodynamic imperfection of wells is presented by
the coefficient 9 or by the r1duced radius of the vell. The equation for the
reduced radius is r. pr = rge where rs pr is the reduced radius of the weU,
r. - the radius of the bit, e the base of the natural logarithms; s = 81 + 82;
a1 is the coefficient of well imperfection owing to the degree of opening and
s2 - the coefficient of well imperfection owing to the method of opening.
According to V.I. Shchurov [Ref 1] the coefficients 9l and a2 can be determined
with the aid of given values for the following characteristics: c( = by
7S
d p and nD, a = h , where b is the opened capacity of the for-
D
D D
nation, h the effective capacity of the formstion.,e'- bullet penetration
Card 1/3

Determining the Effective Depth SM/93-58-11-9/15
depth in the rock, D - the diameter of the bit, d - the dimeter of the casing
perforation equalling the diameter of the bullet, and n - the number of shots
per meter of opened formation capacity. By this method the reduced radius of
the well is obtained from hydrodynamic data [Ref 2, 3, 7, 81 and the coefficient
of additional resistance to oil inflow is presented by the formula a r.
rs pr
where r. is the radius of the bit. The effective (h) and opened (b) capacities
of the formation are determined from geological and geophysical data and the sl
and s2 coefficients of well imperfection are determined with the aid of Shchurov's
graphs according to vhich a a a - Ha" the bottom hole data (n, D, d)
and the value of a le
2 it is ;9esib b the analysis of Shchurov's graphs to ob-
tain a - a (nD), as well as the relationship 9 a s2 (e ) which is para-
metric Lly &d in with nD and a. Ha" the Zues of s2, nD, and a it Is
possible to determine the value of E and consequently the effective depth of
the bullet's penetration in the rock. In the Temporary Instruction (Ref 5) the
curves were plotted at I = 0, 0.1, 0.25, 0.5, and 1.0. Therefore, the s must
be determined graphically at several values of e and the relationship 4z;en
82 and e plotted as in Fig. 1. The graphs in Fig, 1 are often difficult to
plot and to facilitate the calculation ofj the authors developed the analytic
equation s2 = s2 (nD., aj ) on the basis of Shchurov's graphs, and expressed
Card 2/3

Det ernining the Effective Depth SOV/93-58-11-9/15
the relationship between S2 and as follows:
82 = 1 - ___ - (99a2 - lka + 1.51) where
nD (0.413a - LOT a7 + A]
A !. 0.913ao'448 t0.378a-0'263 The authors determined the value of t(Table 1)
for six wells of the Zhirnoye ;Ilfield with the aid of this formula and. with
initial data from the VWTU Institute. Sindlarly they determined the minimun
effective bullet penetration depth (Table 2) for the Romashkino Oilfield em-
ploying initial daza obtained by Svishchev and Mikitko [Ref 6). This formula
,:!an also be applied to fracturing by =ans of torpedoes and to the evaluation
of the fracturing process. The accuracy of the results will depend largely
on the correct determination of the number of perforations per running meter
of opened formation, on the correct determination of the diameter of the bit,
and on the density of the perforations. It is concluded that the accumulation
of data on the effective penetration depth of the bullet in the reservoir rock
will help oil workers in solving many practical problems. There are 2 tables,
1 figure, and 10 Soviet references.
Card 3/3

ORLOV9 V*S~
1%
Using pressure charts in solving the problem on tho shifting
of oil boundiLrise. Trudy VMI 12:53-65 158. (KIRA 12:3)
(Oil reservoir engineering) (Atmospheric prossure-Naps)

BORISOV, Yu.]P.; ORWV, V.S.
Method for plotting "true" isobars. Trudy VNII 12:66-89 '58.
(KIRA 32:3)
(Oil reservoir engineering) (Atmospheric pressure)

VASIL'YEVSKIY, Vladimir likolayevich; IJMIN, Immanuil Llvovich; OIIWV.
jyacbeslav Sergeyevich; KRYWV, A.?.. red.; SAVIRA. Z.A.,
veduBhchIy-red-.a-FZ&OVA, I.G., takhn.red.
[Pressure maps in oil and gas production] Larty izobar v dobyehe
nefti i gaza. Pod red. A.P.Irylovs. Moskva, GoB.nauchno-tekhn.
isd-vo neft. i gorno-toplivnot lit-ry, 1959. 107 P.
(MIRA 12:10)
1. Chlon-korreapondent AN SSSR (for Xrylov).
(Atmospheric pressure--Kaps)

ONOPRITEEK0. V.P., kand.tekhn.nauk; STARSHINOV. B.N., kand.tekhn.nuuk,-
BRUSOV, L.P., Insh.; WZOVff. P.R.. In7sh,; BURMKOV. D.P..
lnsh.;- ORLOV, V.S., insh.
- ---------
Sintering of Krivoy Rog magnetite concentrates. Trudy Ukr.
nauch.-Inal.inst.mat. no.5:36-52 159. (MIRA 13:1)
1. Ukrainskly institut metallov, Krivorozhakly Yushnyy
gornoobogatitellrqy kombinat I Krivoroshokiy astallurgicheakiy
zavod.
(Krivoy Rog--Iron ores) (Sintering)

ORDFRIYENKO, V.P.1 ASTAKWV A.G.j STARSHINOV B.N - ORLOV V.S.; BURDYUKOV,
D.P.; ROVENSKIY, 11; KUSHNnW, V.A.01
Obtaining a high-bpaicity sinter out of Irivoy Rog iron ores.
Trudy Ukre naueb.-isel. inst. met. mo*6:7-22 1609 (MIRA 14:3)
(Irivoy Rog Baslils.-Irom ores)
(Sintering)

GORNOVOY, B.A., gornyy inzh.; BORISOV, S.S., gornyy inzh.; KOLIBABA, V.L.;
ORLOV, V.S.
Improving the breaking method In the Gora Blagodat' Mine. Gor.
zhur. no.11:73-74 N 161. (MIRA 15:2)
1. Nizhne-Tagillskiy gorno-metallurgicheskiy tekhnikum (for Gornovoy,
Borisov). 2. Nizhne-Tagil'skiy metallurgicheskiy kombinat (for
Kolibaba, Orlov).
(Sverdlovsk Province--Boring) (Blasting)

BCKSFJMN, A.A.; ORLOV, V.S.; KANYUGA, A.F.; FETRASH, I.R.
Mean formation, prosoure undor conditions of flooding gamey oil
and initial data for determining it. Naueh.-tekh, sbor. po dob.
nefti no,13:34-39 161& (MIRA 16:7)
1. Vsesoyuznyy neftegazovyy nauchno-issledovatellskiy institut,
Stanislavskiy TsNIL i liauchno-issledovatellskaya laboratoriya
neftepromyslavogo upravleniya Dolinamft'.
(Oil field flooding)

ORWV, V.S.; PRAVEDNIKOV, N.K.
Calculating fluid recovery in the multiline drive pattern.
Nauch.-tekb. abor. po dob. nefti no.l5sW58 161. (MIRA 15:9)
L VMDOYQWW neftogasovyy-issledovatel'skiy institut.
(Oil field flooding)

BDRISOVP YU.P.; MMOVI V.S.
Approximation method for calculating the recovery of petroleft
and water in pattern flooding. MrAv VNII no.37slOS-129 162.
(MIRA 166)
(Oil field flooding)

BOWER", A.A.; ORLgV, S.S.-
Determining the average reservoir pressure in various
petroleum production system. Neft. khoz. 1+0 no.5:45-49
my 62. (?GRA 15:9)
(Oil reservoir engineering)

ORLOVP V.S.
Analyzing the develapi*nt of an oil pool in water drive by
the material balance method. Nefteprom. del* no.3:33-36 163.
(MIRA 16:9)

I , J . , , . : , ': ~7`: -N ; 0 - : ~, , '. , ,
I ., 'I . ml , I : -t~ . , I . . ;'. ' '. -t ' -, , M , I - ,I W" ' 1 S ~, '3 ', P7, -., f' -;S- I ~ -'
. " . ': , rF? . , '. , ri. : r 1, , s 1 r e a ~ 1 ~ f, - . - I . .. ~,.! Y. !~ ~ -- tr . Pr) ~ o 1, . : , , * . .
r -,i~ - - -,-

BYROVP N.Ye.; KUCH.J'INA, M.'.; K-~-'.kFVA, Me.; BCR'MJVA, T.F.;
ALFSIN, V.V.; BOKSLFNAN, V.S.
Delineation of product'lon tire, !~ in the f 1PIdn t~f tiaq cls-
Carpathian region. Nai~,h.-Wkh. sbor. pc dob. neft'. ho.19:
0-12 '63. (MIRA 17:8)
1. Vsesoyuznyy rieftegazuvyy lrlst~lw+.

,~ 1 J -& ,
SURINP V.V., gni-nyy lnz-h.; ORLOV, V.S., gorri~y Jrizl;.;SlirHELKANOV,V.A, kmitek~. nau~.
Incrf.ai3ing rhr:j ecuntimir efrr-lericy of undlergrol.il,j miri.'I.g at. tbi
"Illzhnaiall Ilirie. Gor. zhu-r. no.6:212-23 Je '64. (!-u:tA 17:3~'
1. Garoblat:odatskr~ye ru(Ioul.ravlenlye (for SLLrJy-, Orlov). 2. 1 n!31 I uj,~
gornegr dela Urallsk-li-co f':ia-a kN SSSh (for Shchelkr-nov~.

GATTENBZ.LG-'A, Yu.i-.; DO-MiCV, ( . 1. ; 0'--.LLLTV `.' S - -L'-' ': Tl-;,
I . . p ~;
-stimat..rig etroloum foulction un the ittvii cii
t r
sbor. -o ~io,). nefti I o4. . - It il .'. ..
r I .- 1,
y neftei-azcv-.r:v ,iauclinc)-issltiuov,;t.-~il.-l-,.iy in tt t .
1. Vseso-.-uzn-T s 1 ~

11~
YMURTSOV, N.N.; ORLOVJS V.S.
Optimal distribution of the petroleum production Flan betureen objects
of independent development by linear programming. Nauch.-tekh. sbor.
Po dob. nefti no.24:121-125 164. (MA 17:10)
1. Vaesoyuznyy neftegazovyy nauchno-issledovatellskiy institut.

VEMKOFSKIY# K.B.; LUBENETS, I.P.; CRLOV, V.S.; SHCHELKAHCV, T-Al;
IDENISOV, Te.K.
Induced block caving at the Gora Blagodat' mine. Gor. zhur
no. 12:29-32 D 165. (MIRA
11 Goroblago4takeya'thelazorudnoys meatorozhdeniye (for
Wernikvim'*,1BfflGhbte, Orlov). 2. Institut gornogo dela,
Sverdlovsk (for Shchalkanov, Denisov)e

BORISOV, YU.P. ; YEGL:-.7-CYV, N.N. ;, CRLOV V.S. ; io";' ~ ~, "
-j
Efficient d~-stribution of oil prodLction betwee:. variol~s
Nauch. tekh. sbor. po dob. nefti no.27:94-98 165.
18.9',
1. Vsesoyuznyy neftegazovyy naucino-issledovatellskiy institut.

ORLOV), V.S.
Ultrathin photosensitive layers for electron micro.~cDplc
radioautography. Biofizika 10 no.1:192-194 '65.
(MTRA
1. Institut hiologicheskoy fiziki AN SSSR, Moskva.

t I;
K "' v - ~ . . ~ - -"! ", Yu.1'.. B'..'Kl)v, ;4.y,;*; -. i,. " p1, "
I . ., 0 .
I - ~ :) .: 'I , 1-1 ff'r flp U)(" dqv,~ loplimill, m., I , I , 11 ,
1 4 1 f 1 - I v %..-) bringJ ng triem J nto produ!~,, I on. lief t.
.. , 110. 8: 1 --.1 ;,p 165. ( M: ~ I., - - , I

ORWV, V. $-
The Smolensk L"ecembrists. Smolensk. Smo'enskoe obl. gos. izd-v:), 1951. 1')6 1). ~ 52 - 2 10"1 )
DK212-07

OPLOY, V. B.
ROSISVIL I A�0 D. p. Nmkovgkiy, V. S. Orlov fet &17 Smolensk, Szolgi z. 1952
202 p. Illus. (Gorods. Mao;enshchiny)
Bibliography: p. 201-L203j
SO'- 727J[/5
621.01
.12

ORIM 0 V. S.
Orlov, V. S. "The clinical aspects of adamntiLnoma of the
lower ~aw." First Leningrad 111edical IrLst imeni Academ-
ician I. P. Pavlov. Chair of Faxillary-Facial SurFery
and Stomatology. Leningrad, 1956. (Dissertation for
the Degree of Candidate in Medical Science)
So: Krii7hnaya letopis', No. 2?, 1956. Xoscm~~. Pages 94-109; 11-1.

OTUV -,-V..- f..
Apocynm
Current tasks in further cultivation of Indian hemp (apocynum). Sov. agron.
10 no. 4, 1952.
9. Monthl List Of Russian Accessions, Library of Congress, July - 19 , 2Uncl.

OR-Ls UP V # T'
USSR / Cultivated Plants. Plants for Technical Use. M
Oil Plants.' Sugar Plants.
Abs Jour : HDf Zhur - Bioli., No 8. 1938~ lid ~4M
Authors : Yakushkin, I.Vi; Orlov) "I.T.
Inst : Vot given
Title : Concerning the Flrx Variety L-1120*
Orig Pub : Lyon i konoplya, 1957, No 7, 17-19
Abstract : Variety L-1120 was developed by the Experimantal Station of
Smolensk by means of hybridization and controlled growth.
It was allocated to 10 percent of the total area for flax
cultivation. This variety yields high crops of fiber
and seeds, and has high resistance to banding, while its
drawbacks appear to reside primarily in the unsatisfac-
tory spinning capacity of the fibers. By raising the seed-
ing norm (up to 30 million seeds per one hectare), by earlier
harvesting, and by spreading and maceration of the chaff
Card 1/2

ORLOVO V.V., inzh.
Sources of errors of weighing devices with dial Indicators.
Priborostroanie no.3z28-29 ?4r 165. (M~F(A 18:4)

i .-. . ,. , ".I -'. !.
v - . k
%14 ialw
- . - , - , - *- I
Vrigt. L"IT 1 - . ). "-' : 1 :'1,
(Z'-,., , t i '.A )
t~n I'l ,~ *~~ ':~. 0~ :,n a--! in , I . .
(~, 1 - . *
1.
1,--10 ( 1 on o v -- h - n, -,. )

OR Y,-X-V-,4n2h. (stantatya Lershino); VINUICHA, V.S., inzh.
(stantelya Levehino)
Promoting the mechanization of snow removal operations.
Put' I put.khoz. 4 no.1:29 Ja 060. (MIRk 13:5)
1. Ilachallnik Levahinskoy distantail PermBkogo otdoloniya
Sverdlovskoy dorogi (for Orlov). 2. Levabinakuyu dintantsiya
Permakogo, otdoloniya Sverdlovskoy dorogi (for Vinnichek).
(Railroads--Snow protection and removal)

~- ORWV v v
Securing the stabilitv of the roadbed. Pat' i put.khos. 4 no.9:8
S l6o. (MIRA 13:9)
1. Bachallulk dietantsil, stantsiya lovshino, Sverdlovskoy dorogi.
(Railroade-Track)

GOLJDVANCYV .Taroslav Kirillovich; ORIDV, Vlgdimir Viktorovicht
CHMIKOVA, H.S., red,;'tg~G-IN, A.S., tekhn. red.
(Great figures of a great plan]Velikie tsifry velikogo plans*
Moskva, Sovetskaia Rossiiat 1962~ 62 pe (KIRA 15:9)
(Co=ndom) (Russia-Economic policy)

-OJWVm VeYet Inshener,
, 1-11?-Ir-,~O-,U~-~
Master plans for Industrial enterprises building organizations.
Strot.prou. 31 no.11:24-27 1 053. Mm 6:iz)
(Industrial buildings) (Construction Industry

LUKITANOT. V.I.; KYSLIN, V.A.; SHUTBROT. A.1.; KHOMMOT, A.Ta.;
MMUSEZY, M.S.; OLINIKHOTA, O.K.; PUSIMOT. L.To.; OZQL-!.T.;
ZLATMW]r Y. V.I.; VISHINTSKIT. JPA.; LAPSKIEW. P.G.; KAKWV.
M.S.; JMAVISHNIKOV, I.D.; LMIN, K.Y.; KOZEM110F. 0.A.;
ZOKIN, G.N.; NOFAM, B.B.; TMNOT. I.6.; BARURYANIXOT. S.M.;
VOUOT. N.G.; NOTIKOF, P.G.; FRIUMG. G.T., insh., red.isd-va;
WMINSON, P.G., takhm.red.
[Designing chief plans for Industrial plants; principal sethodal
Proakt1rovanie generallnykh planoy pronyahlonnyich predpriiotii;
onnoymp poloskimalle. Moskva, Gos.isd-vo lit-ry po stroit..
arkbit. I strolt.saterialan. 1960. 103 P.
(MIRA 13:6)
1. Akademlya stroitalletyo I arkh1tektury SSSR. Inatitut grado-
stroitelletva I rayouncy planlrovkI. 2. Nauchno-lealedovatel'skiy
inst-Itut gTodostroitel'stya Akademli stroltelletva I arkhitektury
USSR (for Khorkhot. Yelenakiy. Hellnikhova). 3. Gosudarstvannyy in-
st1tut proyaktiroyanlya metallurgichaskikh savodov (Giprows) (for
Pleshkov). (Continued on next card)

WKIYANCN, V.I.-. KHOMOT, A.Ys.; ZORKIN, G.N,; NORMM, B.B.; PIRSHIrov,
UTe.; LYTKIN, K.F.; KOMWNIKOV, O.A,; TANCHIN,
V.V.; ZLATOLrNSKIT, V.N.; MAKHOV, M.S.; BUKAYISHNIX07, I.D.;
WIT-OVA. L.H., red.izd-va; OSJ=O, L.K., tekhn.red.
[Instructions for drafting general Plano of industrial
enterprises] Ukazaniia po proektirovaniiu go-nerallnykh planov
promyeblennykh predpriiatii. Odobreny Gosudarstvennym komitetom
Soveta Ministrov SSSR po delam stroitel'stva 15 noiabria 1960 g.
Moskva, Gos.izd-vo lit-ry po stroit., arkhit. i Btroit.materialam,
1961. 131 P. (MIRA 15:2)
1. Akademiya stroitelletva i arkhitektury SSSR. Institut grado-
stroitelletva i rayonnoy planirovki. 2. Akademiya stroitel'stva
i arkhitektury SSSR, Nauchno-iseledovatelsekly institut grado-
stroltellstva i rayonnoy planirovici (for Luklyanov). 3. Akademiya
atrottelletva I arkhitek-tury USSR. Nauchno-ionledovatellskiy institut
gradontroitellstva (for Xhorkhot). 4. Giproavisprom (for Zorkin,
Normaiin). 5. Gosudarstvennyy soyuznyy Institut po proyaktirovaniyu
metallurgicheskik~ zavodov (for Fleshkor). 6. Gosudaretvenayy
institut po proyektirovaniyu zavodov tyazhelogo mashinostroyaniya
(for Ly-tkin, Kozhevnikov). 7. Gosudarstvennyy proyektnyy inatitut
N0.1 (for Temchin). 8. Gosudarstvonuyy proyektnyy institut Btrol-
tellnoy pronVehlonnosti (for Orlov, Zlatolinakiy). 9. Goeudaretvennyy
proyektmyy institut po promyshlonnomu transportu (for Kakhov,
Rukavishnikov).
(Industrial plants--Design and construction)

nM

MLOV, Va.
IrMbomarcom of the small Intestine In children. Test.khir. 78
uo.3018 Mr. 157. (K" 10:6)
js,kjtnik1'det*koy Oirurgii (;av. - prof. A.F.Zverew)
Sys lovskogo seditainskogo instituta. Adres avtora: Sverdlovsk.
Urallskiy savod tyashologo mashloostroyenlya. lovo-lkskavatornyy
poselok Ulji*skiy per., 4.29..ky.l.
INTMIU, MQU. neo'plasus
I.S.uphosarcom In child (Ran))
(LTNMOS=ONA. In inf. & child
small intestine (Rum))

MUNO V.V.
=t abdominpl trausa and acute appendicitis in children.
Veet.khir. 81 no.101128-129 0 058 (KMA 11: 11)
I* Is kliniki detskoy khtrurgii (sav. - Prof. A.F. Zverev)
Sverdlovskogo meditainakogo institutao' Adres avtora: Sverdlovsk,
Urallskly zavod tyathelogo mashinostroyeniya, Novo-BkBkRvPtoryny
poselok, d.29.
(ABDOMM, wds. & injo'
relation to pnthogen, of acute aDnendicttis in
child (Rum))
(APPENDICITIS, in inf. & child
acute, relation to closed abdom. trauma (RUB))

ORLOV., V.V..,. BYKOV, I.M.
Intubation anesthesia in pediatric urology. Urologiia 25 no. 5:9-12
s-o 6o. (MIRA 14:1)
(UROLOGY) (INTRATRACHEAL ANESTHESIA)
(PEDIATRIC ANESTHESIA),

AUTHOR: GRMLOVA.Z.1.,UMOVSKIT.B.G., KAMAYEVA.V., MWV,V.V. 84-5-1A2
TITLE: Measurements of Neutron Resonance Absorption in-the Reactor uf the
Atomic Power Plant. (Izmjreniye rezonansnogo pogloshoheniya neytro-
nov v reaktore atomnoy eWtrostantaii, Russian)
PJWODICAI4 Atcuraia Energiia, 1957,'Vol 2, Nr 5, pp 4114+15 (U.S.S.R.)
ABSTUCT: According to three different for-11se, which. besides the known or
estimated characteristic number, contain the ratio
R
Y between the number of resonanoe-ceptured neutrons in a fuel
element in 238-U and the number of captured therml neutrons, as well
as by measuring this ratio the probability I - f of resonance
capture on the occasion of the moderation of a fast neutron was oom-
puted.
The ratio of the unudum-graphite lattice was carefully maintained in
an experimental channel while measuring we carried out by comparing
the activation of an uranium sample enclosed in a cadmium shell and
of an open one, an well as by comparing
R of uranium and a resonance indicator with known thermal capture
;F
cross section and resonance integral.
Card 1/2

84-5-1/22
Me"urements of Neutron Resor-noe Absorption in the Reaotor of the
Atomio Power Plant.
Results, whioh amount to an average of 0,900 t 0,015 for the
reaotor of the Soviet Nualear Power Plant, agree well with me
another an well as with theoretio&lly ocuputed results. (2 Illu-
strations, 3 References).
ASSOCIATICK: Not given
PJMSEMM B1.
SUBOTTED: 2.11-1957
AVATIMLE: Library of Congress
Card 212

AUTMR: GORMV 69-96
,pL[. , ORLOV,V.V- MM'NZOV, T.D. 11/30
TITLE: ature ependenoc of' the 51.~uctive Resonanne Intepml.
The Temper
(Temneraturnaya zavisimost' ef fektivnogc resonwwwgo intsgrala
Pogloachea")
PERIODICAL: ittomnaya hnergiyi, 19)7, Vol 3, Nr 9, -1p 252-255 (U.S.S.R.)
ABORACT: The temperature dependence is theoretically derived and as a re-
sult the function ~ ( ~ S -I') is graphically represented. On the
It
ordinate the 71 -values from 1 3,6 (in 0,1 - steps) . and on the
abscissa thel values from 0,1 to 1000 (in the logarithmic scale)
a
are plotted and the curves for ~ 0.04; 0,05; 0,075; 0,1; 0,15;
0,2; 0,3; 0,4; 0,5; 0,75; 1; 2; are dravm. (With 2 Illustrations
and 2 Slavic References).
ASMOIATICK: Not given
FWD= B jr:
SUBMITTED: 18-3-1957
AVAILABLE: Library of Congress
Card 1/1

AUTHDR: Orlo-r, V.V. juv/89-4-6-4/30
TITM- Muttal Soreening of the Block-q of Resonance Absorption of
Neutro". in a '101oae4 Packed" Lattice (Vzaimnaya ekranirovka
bloko,r rwonaDsnogD poglotitelya ney-tronavv"tesnoy" reshetka)
PMODICAL Ato=aYa anergiya, 1958, Vol 4, Nr 6, PP 531-538 (USSR)
ABSTRACT: The mutu&l .9vr-5,aning effect between blocks and layers of a re-
sonan-ce. absorption ia ~talmlated theoretically for the case in.
whi--b the thickness of the moderator, by which the absorption
Llockq are separatAd from each other, is of the same order of
magnitude or ;3saller than the free length of path of the neutrons
in th." modbrator. In calculation it is assumed that the blocks
are amall and that the absorption ooeffioient can be described
by the Briii.-Wigner formula,
Resonance absorption 1B zaloulated for the following cases,
especially the sore-aning oootfficients f(p), k being cal-
c-ulated and t&bulatta.-

1
1.)Lattlo-zts of parallel lates
2..)Rouni lattlc,-i with, 8.5
a qylindrirAal block, b) a ring-shaped
card 1/2 it 10 t1.

KutuF-l Sere-suing of the Blacks of Re3orar,:--e Absorption 36 7/89 -1, .6--1*130
of Neutrons in a "Closell Pa*ed" Lattice
3.) RIrg. --ihaped ptuetry of the absorber.
It vr.,,.4 poasibl-a to iihow that the appro)dmti*we axchange of the
aotu--O arrangement of a lattice of oylindrIcal blocks is equiv-
&lent to a xx)uTkd lattios. The calmUtions carrled oixt for the
ayat-v of pax%illal plates mAe i~~ possible to check the accuracy
o~ the rasults obtained ty Petrov (Ref 1). Them iq good agree-
men~, Thera &.-a 3 fljpax~~.-j, 6 tables and 3 Scyl-et re-fereness.
SUMITTED, 140---,mt~er 4'' ;9,-.,
1 2 Neutron absorners-Theor',
3. A~sorbe-.c:- -Mate--ials
Card 2/2

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121 (9)
'LUTHORS1 Kochergin, V. P., Orlov, V. V. SOY/89-6-1-4/33
TITLE% Length of the Moderation of Neutrons kDlina zamedleniya
neytronov)
PERIODICALt Atomnaya energiya, 1959, Vol 6, Nr 1, pp 34 - 41 (USSR)
ABSTRACTs The integral equation of the moments of the neutron spatial
distribution function in an infinite medium with infinitely
thin isotropic sources is derived and an approximated solu-
tion for the equation is developed. The energy moments and
angle-zoments of the neutron distribution function are
expressed by the experimentally determinable angular distribu-
tion of the neutrons for the case of an anisotropic elastic
scattering on the nuclei for various neutron energies. By
making use of the experimental data for the total cross
section and the angular distribution of elastic neutron
1 2 9 12 16
scattering on the nuclei H , D , Be , C and 0 formulae
were derived for the moderation length of the neutrons. By
means of these formulae the moderation length in the follow-
ing moderators was determineds water, heavy water, graphite,
Card 112 beryllium, and beryllium oxide. A comparison between

Length of the Moderation of Neutrons
SUBMITTEDs
experimental and calculated
agree with thc former with
Work was discussed with G.
Mathematical Sciences. V.
Z. I. Shemeteako took part
are 4 figures, 1 table, and
June 21, 1958
SOV/89-6-1-4/33
values shows that the latter
an accuracy of up to about t 5%.
1. Marchuk, Doctor of Physico-
S. Gudkov, Z. P. Drobyshey, and
in the calculation work. There
4 references.
Card 2/2

r:-I ( 8)
AUT11ORS. Broderp D. L.p Kutuzov, A. A,, Levin, SOY/89-7-4-1/20
V. V., Urlov, V. V. Tarusova, A. V.
TITLEj The Passage of Fast Nbutrons Through Lead and Iron
PERIODICAL: Atomnays. energiyal 19599 Vol 7t Nr 4P PP 313-320 (USSR)
ABSTRACTs The present paper gives the results obtained by measuring the
spatial distribution of fast neutrons (originating from
monoenergetic neutrons of the energy E - 4 NOT and E - 14 .9 an)
and of neutrons of atomic reactors in Tron and-leaA. first,
the experimental arrangements are discussed. The reactor of
the Pervaya atomnaya elektrostantoiya (First Atomic Power
Plant), an experimental nuclear reactor of the VVR type with
ordinary water and enriched ursanium, and a neutron generator
were used as neutron sources. The spatial distribution of
neutrons in iron and lead was measured by means of a neutron
generator, a neutron detectorg and D- and T-targets. A
Th 232_fission chamber and threshold indicators fAl 27 (n'p)Mg 27f
P31 (n,p)S13l, and S32 (n,p)P 32 ) were used as detectors. The
distribution of thermal and epithermal neutrons was measured
Card 1/3

The Passage of Past Neutrons Through Lead and Irft BOV/89-7-4-1/26
by means of a U 235_fission chamber. The results of these
measurements in iron and lead are shown by 4 diagrams. The
authors then theoretically investigate an infinite homogeneous
medium in which an unbounded, pUne isotropic source of mono-
energetic neutrons with the energy EO is located. Neglecting
the moderation of neutrons in elastic cattering# the kinetio
equation for the neutron collision den:ity tf(f,E) is written
down. The inelastic scattering is here &soused to be isotropio.
The aforementioned equation is then transforned 'by means of a
Fourier transformation, and is solved by employing the method
of spherical harmonics. The calculation is then followed step
by step, and the asymptotic solution is explicitly written
down. A formula is written down for the neutron flux with the
energy E in a medium with point source. The results shown by
some diagrams for iron agree well with the experiment. The
same also applies to the results for lead. The computation
method suggested makes it possible, if the differential cross
sectla4 of elastic and inelastic scattering of neutrons .*Ze
sufficiently well known, to determine the spatial- and enLrgy
distribution of neutrons in thick layers of matter having
Card 2/3 comparatively high nuclear charge numbers (e.g. greater than 56)

The Passage of Fast Neutrons Through L-ad and Iron SOV/89-7-4-1/28
with aufficient accuraoy. At 'Large distances from the source,
the neutron spectrum is enriched with considerably slowed-
down UeUtTMB. If the energy distribution is known, th,3 shield
may be calculated according to the multigroup theory. The
authors thank Professor A. K. Krasin, Candidate of Teohnioal
Sciences A. N. Serbinov, and the ozientific co-vorker
V. A. Romanov for their constant interest in the present
paper and for their collaboration in the experiment. Pesides,
the authors thank V. G. Liforow, Z. S. BliBtanov, and V. S.
Tarasenko for their assistance in the experiments. S. A.
Kurkin assisted in working ry-tt the calculation method, and
M. B. Yegiazarov, V. S. Dikare-v, V. G, Madeyev, Ye. N. Korolev,
and N. S. Illinsk�y further took part in the experiments.
There are 9 figures aud 14 references, 4 of which are Soviet.
SUBMITTED: January 21, 1959
Card 3/3

ORIDV V.V.t GOLASHVILI, G.V.; VASKIN, A.I.
[Resonance absorption of neutrons by a block] Rezonansnoe
pogloshchenie neitronov blokom. Moskva, Glav.upr. po is-
polIzovaniiu atorrmoi energii, 1960. 16 p. (MIRA 17:1)

LUKIYANOVJ, A.A.; OALOV, V.V.
[Effect of the resonance structure of cross sections or.
neutron diffusion] Vliianie rezonansnoi struktury se-
chenii na diffuziiu neitronov. Floslcva, Glav. upr. po is-
pollzovaniiu atomnoi energii, 1960. 19 p. (MMA 17:1)
(Neutrons-Capture) (Neutrons-Scattering)

O=V, V.V.
(Albedo equations in neutron diffusion and deceleration
theory] Allbednye uravneniia v teorii diffuzii i za dle-
niia neitronov. Moskva2 Glav. upr. po ispollzovaniiu
atozmoi energii, 1960. 21 p. (AURA 17:2)

ORIDV, Vj., kand. fiz.-mat. nau , red.; TSYPIN, S.G., kand. fiz.-mat.
nauk, red.; KAZANSKIY, Yu.A.ftranslatorl; KUKHTEVICH, V.I. (translatorl;
MATUSUICH, Ye.S. [tranolatorl, NIKOIAISHVILI, Sb.S. [translatorl; SI-
NITSYN, B.I. [translator]; YUS, S.V. (translator!; VISKCYVA, M.V., red.;
RYBUNA, V.P., tekhn. red.
[Protection of transportation units having nuclear engines; translated
articlesl Zashchita transportrjykh ustanovok s iadernym dvigatelem;
sbornik perevodov. Moskva, Izd-vo inostr. lit-ry, 1961. 619 p.
(MIRA 14: U)
(Fadiation protection) (Nuclear reactors-Safety measures)

S/058./6Z/000/004/024/ 160
A058/A101
AUTHORS: Marchuk, G. I.. Orlov, V. V.
TITLE': On the theory of conjugated functions
PERIODICAL: Referativnyy zhurnal, Fizika, no. 4, 1962, 57, abstract 4B427
(V sb. "Ney-tron. fizika". Moscow, Gosatomizdat, 1961, 30 - 45)
TE)r,T: The authors analyze an arbitrary linear equation for.a 9x) funct..;,n,
where x is the set of all variables characterizing the p(x) state ey offer a
general determination of the conjugated function, conjugated equation and value.
Iney forniulate a perturbation theory. The general formulae are concretized on
the example of radiation (or neutron) transfer theory. The authors give examples
of some functionals used in transfer.theory, and exampleo of using perturbation
theory.
A. Galanin
[Abstracter's notes Complete translation]
Card 1/1

32983
s/641/61/ooo/ooo/o,o/o7,z
B104/B102
AUTHORS: Luklyanov, A. A., Orlov, V. V.
TITLE% Effect of the cross section resonance structure on neiatrcr.
diffusion
SOURCE: Krupchitskiy, P. A., ed. Neytronnaya fizika; sborn-ik sti~tr-v
Moscow, 1961, 105 - 115
TEXTs The authors derive expressions for the cross section and the
diffusion coefficient of a neutron flux for the case of a resonant inter
action of the neut 59 s with the nuclei of a medium. The resonance chara-
teristics of the U nucleus in the enerizv ranRe of 200 ev to 50 kev are
determined and the diffusion parameter for different U 238 concentrations V-1
different temperatures and energies are averaged. The diffusion cros6
section and the diffusion coefficient depend essentially on the U 238
centration in the mixture and on the temperature of the medium, For
E< 50 kev the single-level approximation gives sufficiently accurate
values if the effective resonance vidth does not exceed the mean dAst.incr-
Card 1/2

32983
3/641/61/000/000/010/n-37,
Effect of the cross section B104/B102
between the levels. In this range the resonancewidth is (T -
3000K, E in ev). In the energy range above 50 kev self-screening decre~t
sea considerably, and the resonance width exceeds the mean distfince I-et';wl"'.
the levels. The maximum resonance cross section is then
fy(O' ~ ) - E' 0-(O)1 , where a-(O) - 411A' -At T - 300'K1 -0.1 Th--s, z
2
E>?30 kev, o-(O,f) can be compared w-ith the potential scattering crr~~S
0 j . 2.6-10 2
section or ;zzlO barn: cr(o, i' 0.1(barn)'_ 30 barn. T]-1
s F2 E(kev) Ekkev)
authors thank I. I- Bondarenko and I, V. Gordeyev for taking part. in -.17-F
discussions There are 1 figure, 4 tables, and 12 references. 5 Sov-_et
and 7 non~-Soviez. The four most recent references to English-lancraaFe
publications read as followst Wigner E., J, Appl.. Phys., 26 26o
Dresner L., Nucl, Sci, and Engng., .1, 68 (1956); Lane A, M . 1~ynn i. E,
Proc, Phys. Boo., A70, no,. 8, 557 (1957); Macklin R. L., Pomerance H D,
Progress in Nuclear Energy, .1, no, 1, Pergamon Press, Lond_ 'Q1156
Card 2/2

32984
3/641/61/,)00/000/01 1 /() 7 7
J3104/B1 02
AUTHORSt Orlov, V. V., GoInalivill, T. V., Baskin, A. 1.
T I TL N,-%utrr)n rbsonrince absorp+ion in a lump
301IRCF: Krupchitskiy, ?. A., ei. Neytronnaya fizika; sbornj'K
moscow, 1961, 116 - 124
TLIXT iThe au thors A eve I op a rener-i 1 f ormu I a f or the ef J v-c t i ve
intorral which takes account of the scritterinf- nn! the SIO-,,Anfr
neutrons in a lump aj well as the P03W)ility of q neutron
the lump. A survey is Viven of the formulas of the offective regonanc.-
intetrral which have alrt~ridy been lefilt with (v.archijk G. I., Uhi!31t-nn~., ,
metody raschct3 yadernykh reaktorov, - Numorical methods of T-C -IC tor -'11, 1: -
lation - '.1. X.U. AtO;ni 7 1 it, 195"; Gal!,nin A. D., Ttoriy.9 yadernykh i-!.-
torov na teplovykh ncytrnn.,!kh - ryr~ of t~.i-rmal re,-ctars - Ato(!ij7 I-tj
p i n r a d B. , Cho rn 1 ck JC o rn t-o c t~ ti i r t- n o. 1 IA 7, C n r d -1 r. e ri -: t i I
nal Conference on the POLICOfUl 1)3eS (if Atowic Enerry, Cnneva, 1'; 9).
authors derive 'Riemer's formul! for the ro3onance int(-,Fral J,,,, + il/ i
Card 1/3

Neutron r -nnance ...
32914
B10,11/B102
wherc a 1,~ th(.- volume, ab!3orption, b th.: suf-fac, absorption, o1:'
mean free n,--utron path in the lump. If the rtsonance cro.9- slotlcn
i vc n by thr Brei t- - i rn.- r f ormula x y
r ri,
E und ' are the ~inervy and tha r,,.,:oranc-: wi Itb,
rrsnn.-incp intti-r-fl is viv n by
r 11
exp I h.
.it'd slronr resonaricc t ~,. ojuantities .1ti. 11/1 !n.~ pnt '11A I
cress st~ction, can b,: n,~ j- I r= c t. d -ii ns t C
t 0 t -11 t.1:'OS f-10 11 crr~, f;ce-tion. Tt,c volu- '.ibsorp~inn n-
t-rnr, -:-:,t1on m-ty or inor- i-c- i p ri f'.-
"r i, rjr- ~g r of Oic trr
I/- to: 1. 1. '~'I:

32984
S/641/61/000/OCj"_! 2 1
Neutrcn resonance B'04/BlO-,'
Pomeranchuk (Reaktorstroyeniye i teorlya reaktorov Dokladj
delegatsii na Mezhdunarodnay konferentsil po mirnomu ispol'zz,van;~Y_ ~L-_
noy energii Izd-vo AN 333R, 1955, p- 22) are mentioned. There ar-
2 figures and 9 referencesg 7 Soviet and 2 non-Soviet
Card 3/3

9 ~C('
AWHOR:
S/058/6Z/000/004/030/'160
AO1_,8/A1Ol
TITLE: Albedo equations in neutron diffusion and moderation theory
PERIODICAL: Referativnyy zhurnal,'Fizika, no. 4, 1962, 60, abstract 4B452
(V sb. "Neytron. fizika". Moscow, Gosatomizdat, 1961, 179 - 191)
TEXT: The author examines albedo matrices and transmission functions for
simply shaped bodies (sphere, plate, cylinder) in a multigroup diffusion approxi-
mation. Examination of unilateral fluxes in a diffusion approximation, limited
by magnitudes of the order of film thickness, yields albedo-matrix and trans-
mission-function expressions for thin films. Expressions are derived that deter-
mine albedo matrices and transmission functions of double films through albedo
matrices and transmission functions of simple thin films. Singling out of an
infinitely thin double film in a finite film leads to a system of feur matrix
nonlinear differential equations (non-independent ones) determining albedo matrices
and transmission functions. In particular problems, e.g. for a semi-infinite
medium, these equations can be simplified. In a limiting transition to continuous
Card 1/2

I
Albedo equations in ...
S/058/62/OW/C)04/()30/160
A058/A101
distribution of groups, equations are derived that determine albedo matrices and
transmission functions in the age-diffusion approximation. For the case of con-
stant cross sections and a semi-infinite medium, an explicit solution is obtained.
B. Kochurov.
[Abstracter's note: Complete translation]
Card Z/ 2

9936h
S/08 61/O1C/QC2/C!(1,'01f-
3102Y3200
AUTHORS: Dreshenkova, Ye. B., Orlov, V. V.
,i,;% - r~.-~;,,,-.~~-,,,~.".,-~.~,~~,.I
TITLE: The solution*of the equation of motion for a mbdium with a
one-directional point emitter
PERIODICAL: Atomnaya enerGiya, v. 10, no. 2, 1961, 175-177
r
.-LErad F( t-tx) - -P(4) X 2WK 21t
0 0)b(X-,X 0). By means of the reciprocity theorem
-4
G
( 07E of 0) = G+(4 0 7) and/or after integration over
r,E,.-;; r n ropEopa ;r tE tri
+ -+ -4 -4
dT : G r r 'i"1 G (r E in ;r,E~ where G
0( 'E;`0 1E0 0) 0 0 0 0 .(Gda, the solution of
this equation may be transformed into the solution of the equation of motion
Card 1/7
TEXT: The present "Letter to the Editor" presents the solution of the equa-
tion of motion for a gamma radiation emitted from a point source in one
direction in a scattering and ab orbing medium.

89364
S/089/61/010/002/016/018
The solution of the ... B102/B209
- 0 grad F* (r, 0, %) = -Ii (%) F* (r, 0, %) +
)L+2
+ dX'K (k. %I) dQ'P* (r, x
21g
(2)
G(rgE,n;r0 E0 f'0) is Green's function of the equation of motion which des-
-4
oribes the radiant flux with energy E in the direction of motionfi. (them,
sinGle point source emitting the energy E is assumed to be located at rot
-4
its direction of motion isr.0 . F(-r4,,-n*,X)Odenotes the radiant flux at the
-4 -4
point r with wavelength 4 in.the directionn; K(?,I,k)
2 2TL_ (A,_1)2-
nZnr (A/X,) + 2(A'-A) + stands for the probability den-
0
s4ty of Compton scattering with a change of the wavelength from A' to
g(4) denotes the absorption coefficient. The total-flux distribution of
Gamma radiation may be determined according to the formula P OW,Xv)
Card 2/7

89364
S/089/61/010/002/016/015
The solution of the ... B102/320-
F+(r 0 1-10;t0 Considering the symmetry of the source and -ith
and
one obtains
dR R 0~
)L+ 2
IL (k) FO (R. A-K (1, X-) dQ* x
6(R
xF'(R. 2n -%').
+X)+ 6 (X
(3)
By expanding the conjugate flux into a spherical harmonic F+(R,_f,X)
~00
21+1 F+(R,2L)P,(3) and substituting in (3), multiplying by Pl(,) and-*
4
.0
integrating over d7,1 one obtains the equation for F+(R,X):
Card 3/7,

e9364
S/089/61/010/002/016/018
The solution of the ... 31021B209
(1+2+1 ) F,
R an
+ F' *, (R,
21+1 R OR
&+2
- p ().) Fj' (R, )') +dX'K x
(5)
RI
By multiplication by R n and integration over the entire volume, the fol-
lowing is obtained for the moments b (x):
l,n I
Card 4/7

89364
S/089/61/010/002/016/018
The solution of the B102/B209
21+1
x Mbi, (%)+
).+2
+ ~ dX-K (1, 1-) ~Pj (i - X- +),) b,, I M +
X
Me
+ 4.0 (X- X') 8106T,.
bi. n"(X) RI&F, (11, X) 4nRldR.
This equation determines only thosemoments b 1,n (X) for which 1 n and 1
and n are of equal parity. With
Card 5/7

h9jr,4
s/o8 9/61 /ol 0/002 /016/018
The solution of the B1. 02/R2.09
N
Fil (R. X) = -7~.jp Y,
Ik-0
N
Fjj+ I (R. ))=-e-"
Yj (k) (;LR)II.
n-0
where a21,n (4) and c21+1,n (X) are solutions of the system of N+1 equations,
one obtains
N
b21. 2m (X) (n+2m)l
"-0
N (7)
b11+1, 2m+1 (%) =I
n-0
Card 6/7

A9364
S/08 61/010/002/016/018
The solution of the ... B102YB209
with m - 1, 1+1, 1+2, ... I+N. The solution of system (7) permits to -x-
press the coefficients a2l,n (A) and c21+1,n (X) in terms of the even even
and odd-odd moments which were determined from (6). The higher the moments
known, the more accurate one can calculate F+(R,X). In solving this problem,
I
it is expedient to eliminate the unscattered radiative flux from the aqua-
tion of moments (6), which may be brought about in the usual way. In crr,
clusion, the authorE thank V. F. Turchin, G. I. Marchuk, and Sh. S.
Nikolayshvili for their discussions. I. I. Bondarenko is mentioned.
There are 6 references: 2 Soviet-bloc and 4 non-Soviet-bloc.
SUBMITTED: August 25, 1960
Card 7/7

20180
8/089/61/010/003/010/021
B102/B205
AUTHORS: Luklyanov, A. A., Orlov, V. V.
TITLE: Theory of the cross sections of heavy nuclei within the range
of partial overlap of neutron resonances
PERIODICAL: Atomnaya energiya, v. 10, no- 3s 1961, 262-264
TEXT: In Ref. 1.("Neytronnaya fizika", Gosatomizdat, Moscow 1961), the
authors presented a universal theory of the calculatior. of cross sections. Y
In the present "Letter to the Editor",. they suggest a simple method of
calculating cross sections within the range'of partial overlap of resonances.
In an infinite homogeneous medium, the cross section is given by
+6 E1+ E
- ii (cfx/cf)dE#/ (1/0)dEl, where d is the total cross section,
and ax the reaction cross section; E is a certain energy range, within which
the collision density varies insignificantly. The cross section in the
Care. 1/ 8