SCIENTIFIC ABSTRACT A. DNEPROVSKIY - YU.N. DNESTROVSKIY
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S
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December 31, 1967
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SCIENTIFIC ABSTRACT
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1e DNMOVSKIY, A.
2, USSR (600)
L. Drill (Agricultural Implement)
7. Advantages of checkraw planting.
Dost. sellkhoz- NO, 2. 1952
9. Monthly List of Russian Accessions., Library of Congress, __ Jm ua:7 1953. Unclassified.
TEMNIKOVA, T.I.; DNEPROVSKIY, A.S.
I -,
Chemical transformations of o~,-h-alo ketones. Part 10: Interaction
of dibenzoylbromomethiLne with nucleophilic reagents. Zhur. ob.
khim. 34 no.9:2845-2847 S 164. (MIRA 17zll)
1. Leningradakiy gosudarstvennyy univer.-itet.
D1T915!10VqKIyP S. P.
Sbornik zadach I prinierov po 1prsu ekonomiki. i T)Ianirovaniia sovetskoi. kooperativnoi
torgovl.i follected problems and examples for Wcourse in the economics and planning of
Soviet cooperative trnde7. Moskva, Izd-vo TSentrosoiuza, 1953. 275 p.
SO: Month1v List of Russian Accessions, Vol 6 No 6 September 1953
WWROVSKly 441 ZARIN, F.V.: VARDIYEU, K.I.
LA collection of problems for a courso in financing and craditine
of consumers' ccoperatives] Sbornik zadech po kursu finansiroyaniia
i kraditovantia potrebitellskoi kooperstsil. Pod red. S.P.Daeprov-
skogo. Moskva, TSeatraoiuz, 1955. 91 P. 041RA 10-11)
(Cooperative societies--Finance)
BOWACIINSKIY, Mikhail Borisovich, prof., doktor okonom.nouk; BYKOV,
Artemiy Nonstantinoviali, dotsent, )mnd.ekonom.nauk; DNMOVSKIY,
StepA~~ Petrovich, prof.; YAHMISKIT, Koisqy Mlarkovi7ch,
ekonom.nauk; t CHM, B.I., red.; BILMWO, L.S., red.izd-va;
POKICHEV, P.M., tekhn.red.
(Financing and crediting of the consumers' cooperative societies
of the U.S.S.R.] Finausirovanie i kreditovanie potrebiteliskoi
kooperataii SM- uchabnik dlia vusov. Koskya, Izd vo Mntro-
soiuza, 19-59. 4;5 P. ~MIRA 13:4)
b-ooperative societies--Finance)
SE M RYIKOV, S.V., prof., doktor ekonom.nauk; GOGOLI, B.I., doteent;
LIFITS, M.M., prof.; YWILOV, A.I., doteent; KISITAKOV, Ya.A.,
dotsent; GENKINA, L.S., dotsent; VASILOYEV, S.S., dotsent;
KIY, S.P., prof.; PIROGOV, P.V., dotsent; SMOTRINA, N.A.,
VS
cdl o iaaSTF; R4.G.', dotaent: KUZIN, N.I., dotsent; PISlWNOV,V.
reds' : .! xu=N, yu. , takhn.red.
[Economics of Soviet commerce] MconomikEk BOV8tskoi torgovli;
uchebnoe posobis. Moakva, Gos.izd-vo polit.lit-ry, 1959. 478 p.
(MIRA 12:12)
(Russia-Commerce)
GRIGORIYAN, G.S.[Hryhorlian, H.S.), dots.; KISTANOV, ls,A., dots.;
FEFILOV, A.I., dots.; GENKINA, L.S.[Henkina, dots.;
VASILIYEV, S.S.[Vasi..lliev,- S.S.), dots.; SEREBRTAKOV, S.V.,
prof.; DNEPRDVSKIj,-_S.Pj -P,j, prof.;
_T7V pqeprovskyi, S
PIROGOV, _rPFm_hov, P.V.], dots.; GOGOLI B I (Hoholl, B1.),
dots.; SMOTRINA, N.A., dots.; KULIKOV, O.G.[Kul*ik*ov, O.H.],.
dots.; KUZIN, M I., dots.; DEMIDYUK, V.F.[Demydiuk, V.F.], red.;
SKVIRSKAYA, M P:[Skvyralka, M.P.], red.; LEVCHC
-NKO, O.K., tekhn.
red.; SERGkYEV, V.F.[Serhieiev, V.F.], tekhn. red.
[Soviet trade economics] Ekonomika radianslkoi torhivli; pld-
ruchnyk. (By] G.S.Grigorlian ta inshi. Kyiv, Derzhpolitvydav
URSRP 1962. 500 p. (MIRA 16:U
(Russia-Commerce)
GRIGORIYAN, G.S., prof.; KISTANOV, Ya.A.f prof.; FEFILOV, A.I.y dots.;
GENKINAO L.S., dots.; VASIL' M , S.S.p dots.; SEREBRYAKOV, S.V.,
prof.; DNEPRGV,SK-I-Y-,.,S.P-., prof.; PIROGOV, P.V., dots.; GOGOLI,
B.I., doii~ri ekon. nauk; WOTRINA, N.A., dots.; KULIKOV, A.G.,
Prof.; KUZIN, N.I., dots.[deceased]; AVETISYAN, Ye., red.;
MUKHIN, Yu., tekhn. red.
[Economics of Soviet trade.1 Ekonomika sovetskoi torgovli;
uchebnik. 2-., dop. izd. Maskva, Politizdat, 1963. 519 P.
(MIRA 16: U)
(Russia--CoRnerce)
All
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AUTHORS: Dneprovskiyj_ I. S., Kolesov, G. M. SOV/48-22-8-6/2o
TITLE: Conversion Electrons of Some Neutron-Deficient Ho- and Er-
Isotopes (Konversionnyye elektrony nekotorykh neytrono-
defitsitnykh izotopov Ho i Er )
PERIODICAL: Izvestiya Akademii nauk SSSR, Seriya fizicheakaya, 1958,
Vol. 22, Nr 8, pp. 935 - 940 (USSR)
ABSTRACT: The absence of Tu-lines in the conversion spectra of the
isotopes of the erbium fraction permitted to regard the
sample as being sufficiently pure. Tu was well studied
by Gromov et al.(Ref 7) under similar con~litions- 4 groups
of lines with a half-life of T - 30, 3,5, 2,5-and 1 hours
W
ence concerning the lines
were found. The experimental ev
with T 1/2,~~30 hours (Table 1) well -agrees with the information
furnished by the papers given by references 2 and 3. Hence they
can be ascribed tc the transitions following the decay of
16o
Ho . The investigation of this well studied isotope was
not within the scope of this paper. In spite of a short
irradiation of the tantalum it stood out sufficiently clear
Card 1/3 to permit an identification of the lines. The erbium-isotope
Conversion Electrons of Some Neutron-Deficient Ho- and SOV/48-22-8-6/2o
Er-Isotopes
which decays with T 1/2 ~ 3,5 hours was found by Handley
(Khandley and Olson-(Olson)(Ref 5). Mitchel(Mitehel) and
Templeton~Templton)(Ref 8) determined the mass number (A)
of this isotope according to the time of passage through
the mass spectrometer as 161. It can be assumed that the
lines found by the authors which decay with such a hal life
can be ascribed to the transitions of thelgecay of Erif-1
and of his daughter isotope H0161. The Ho 1 with T 1/2 = 2,5
hours is known. Nevertheless this transition cannot be
assigned to this isotope. According to the experimental
conditions the observed half-life should be equal to 3,5
hours (Er16i). Hence the existence of an Er-isotope with
a half-life of 2,5 hours seems to be most probable. A
number of lines was also found which exhib-ited a half-life
of about 1 hour. The investigation of these lines With the
spectrometer at hand met with difficulties. The existence
of 3 lines was reliably determined (Fig 4, Table 8). The
authors expressed their gratitude to X.Ya.Gromov and A.V.
Card 2/3 Kalyamin. There are 4 figureso 9 tables, ard 9 references~
M
Conversion Electrons of Some Neutron-Deficient Ho- and SOV/48-22-8-6/2o
Er-Isotopes
4 of which are,Boviet.-
ASSOCIATION: Institut geokhimii i analiticheskoy khimii im.V.I.Vernadskogo
Akademii nauk SSSR (Institute of Geochemistry and of Analytical
Chemistry imeni V..I.VernadskiyAS USSR)
Gard 3/3
It
3r,
it
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lp
1;
I 4r
4 91
Cpl.
a 0 :
44
Is q Cat;
22i - 6520, 0`72'0 7 7 2 1
so v/?,89-8) - 1 --t129
AUTHOR: Dnepro-v'skiy, I.'S.
TITLE. New Isotopes of Erbium and Holjrit-a~,,. Let,-_er --,o the
Editor
PERIODICAL: Ator,,,,naya ene-r,,gi,,,a, 191150, Vol 8, Nr 1, pr 41u-4-f (USSR)
ABSTRACT- Tlie authoi, investigated sp(~Ctl',l Of elect-ons
of el~bium isotopes obtained by bombardirg taritall-u! with
660 me-j protons from the Mal synchrocyclot-T,on. Spectra
were investigated by means ol- a Tr \[72 foc,,,,sing spectro-
d ~q ,
Craph type BPP-1. Ob5e*.-,,rincr at a solid ani~le- O."9Z of
4 77- of a I x -~O mriii source, i'-,he resol-vini; po7v,,er Of the
-Tc 'ield
Ba K-661.6 line was 0.2-0.25%. Ma -, i i e ~,L-
imeasurament_s were performed by means ~f a special flux
miet.ep -trhich enabled mea:-~~,irements or convursi.on llne-.
u,itli a halt'-]Lfe 11_~ ifln and bol!ov,
v 11 (~,, t ~~Ideterminati.on weve fror~i ().l. to 0.'J%, Am, c)j
More ti-ian 100 conversion lines '.o
Card 1/24 deficient isotopes of er'b-ii.mi and one a
New Isotopes of Erbium and Flolmium.
Letter to the Editor
'7721
SO-V/,9-E--'-7/2q
C-D T h e t a'*ZD I c- b :-- I c
-roup ,,j i t h a ~ia f - i f e T hr.
contains the-ir identification.
Gamma-Transit-ion in Nuclei of Erbium, and Dysprosium
hv
r)
,-;I E~ .2
320.5
Y, 7
9LI-D-9
GLIB.
T1, hr
2.L +
2 . r, + C)..!
+ 0.
2.4
2.4 0.
. -
2
t 0.1
2 . + 0.
2.,-) +- 0 .
Chanf-e of
nucleUS from v;h-id-l ~~,lt ipole
c- acter
transitic-in
.ar
Ou E2
6
67
Card 2/4
e v: C'. t 00 ~"'Tl! ara
Letter to the Fd i r S 7/2 9
Separati.ng hc1milm lorcm '..he erbli~Jm f1rac.-L"on, 2 hr after
rile lai:'ter vjas separal.-ed f.rom tanI-all~:,-i, the intens-ity of
of '~he
tn~ 11'ne cov-esn'onciin':- '~' a
d wn nu, c- 1 e Lis decreases r-c) a h a I I
y s p r s,
F v,-', m he a bc, v t ,Cac t s ,, h(~ ~I 10 V 0 C s tl- t2 _J 2C e
f" 0 Co I I r_~ v: _J 11 g c ha -1 n -
Er Hc Dy
Fner,j and. imen-oity rel,:-,tiuns _allcv:
,he e:iergy levels as E e v and F.,
kev 1-1+ 1) cf -~he first raratiic~rlal band of the e'.,en-e,rell
nucleus -f dyspros-Jum. According to DZh'_-'Iepo-.,, and Pelker
,.Defr,m-~ru,annye yadra. oblasT-i Nd-C)s. Dubna, one
can deduce from the relation be,ween the -ocsition of the
first excIted. levell and '~he numbe- of ncl-.trons '~-I-,at -rhe
ma s s number of the members )P IrIle chall-I is .5,
From the position cf A)e first energy levelc cone
`--e 'cr the colmsrani-.s ill '-he enercw eqllzation E AVI+i)-
2,1 T
Card Bi +1 ht-. va -." ues A '7 + 0 . a 0 0-.0oE
--ne Eof-.cr
Lettei
EA. S. Dzhelepov and K. Ya. Gr-c)m~-v
-he- discitssed 'he results,-%,.![-,ile
V.
0 . a did the
:5-:3mples. There llo I taL-~le; ana '~'
SUBMITTED
v.,ere consulted, and
1. A. Ylit-lando-..'a and
separatlion --,:' 1,-he
S-.:vie,- ref,el,ences.
Card lj,/ii
84711
S/056/60/039/001/031/041/XX
B006/BO56
AUTHORS: _DD~Mrovskij, I. S*9 Nemet3 L., Peker, L. K.
TITLE: The Decay of Er 16
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
vol. 39, ~o- 1(7), pp. 13-15
T3XT: After a short introductory discussion of the results obtained by
other authors vhen investigating the 'transition energies of Br16i, the
authors of the present paper give a report on their own results. For
the purpose of explaining the nature of the transition hY = 826 kev
161
of Er , they bombarded tantalum with 660-Mev protons from the synchro-
cjyclot-.ron of the Ob:1yedinenrryy institut yadernykh issledovaniy (Joint
Instituteof Nuclear Research) and investigated the radiation accompanyirg
the erbium decay by m~_ans o7f a scintillation spectrometer and a double
-focusing 0-spectrometer. The half life of this transition was measured
as amounting to (190+10) min, the energy determination gave a value of
(826..5+1.5) kev. For-the purpose of determining the conversion coefficient
84711
The Decay of Er 161
B/056/60/039/001/031/()41/'XX
Boo6/BO56
of 1;his transition, the electron conversion line ratio and the ratio
of the photopeaks of the gamma s ectrum of this transition and of the
661,,6-kev transition of the BaM nucleus had to be measured. In this
connection it was necessary to take the radiations of the two isotopes
Er 160 and Er1589 which also existed in the preparation, into account; the
greatest correction was furnished by the gamma transitions 648 and 851 kev
of the Ho158_dec4. In an earlier paper, these transitions had already
been investigated and had been identified as E2--transitions between the
second and the first rotational band. The intensity ratio I /I
1826 1848i851
was determined as amounting to 4.0 + 0.2~ If all corrections are taken
into account, a K = 0.008 + 0.002 was obtained for the K.-conversion coeffi-
cient of the 826-kev transition. According to the tables by L,. A. Sliv
and N. I. Band, this gamma transition is of the !ype M1 or E3. In order
to arrive at a decision, the intensity ratio of the conversion lines K/L
was measured and a value 7.0+0-8 was obtained, which excludes the E3.-type.
The intensity ratio of the gamma transitions 211 and 826kAv was measured as
~_ -3 ~ 1A
84711
The Decay of Er 161 S/056/60/039/001/031/041/XX
Boo6/BO56
amounting to I y 826/,j 211 ~ 8*0 + 1-5. All results obtained by measure-
ments are represented in the following decay scheme,:,.
3/f
5/2- [53~1 8
826
1/2+E4'1] 211 1M1
211
7/2- [52g 0 E3,' 161
nTr7'H11(1' ,,, 67 Ho 94
The authors finally thank I. A. Yutlandov and S. Khaynatskiy for carrying
out the chemical work. There are 1 figure and 9 references: 4 Soviet
and 5 US.
ASSOCIATION: Institut geokhimii i analitiche8koy khimii Akademii nauk
SSSR (Institute of Geochemistry and Analytical Chemistry
Card 3/4 of the Academy of Sciences, USSR)
161
The Decay of Er
SUBMITTED: January 14, 1960
84711
S/056/60/039/001/031/041/XX
B006/BO56
6x .
Card 4/4
GROMOV, K.Ya.; DNEFROVSKIY, 3~.S.
Study of conversion electron spectra of neutron-Ldeficient
erbUm and holmium isot6pes. Izv. AN SSSR. Ser. fiz.
2 5 po.9: 1105-11U . 161. (MIRA 14:8)
1. Ob"yedw-nnn institut yadernykh issledowAy i Institut,
gookbimii i analiticheakoy khimii im. V.I. Ve'rnadskogo AN
SSSR.
(Internal conversion(Nuclear physics))
Erbimri-Isotopes)
Mlmium-lootopes)
DNFPHOVSKIY, V., kapitan-1 pomoshchnik mlihmika
Pechora noeda a fleet of pusvenger vussels. Rach.tranap. 23
no.908-59 S 164. (IMIA 19t1)
1. Pecherskoye parokhodstvo.
DNEPROVSKIYO V. M.
V. M. Dneprovskiy, "on the choice of the intermediate frequency of a superheterodyne
receiver." Scientific Session Devoted to "Radio Day", May 1958, Trudrezervizdat,
Moscow, 9 Sep. 58.
An investigation of the influence of combination components of the mixer current
on the operation of a superheterodyne receiver permits simple expressions which determine
the cho~Lce of the intermediate frequency to be obtained. It is shown that it is possible
to avoid reception on additional channels only f or a limited number of cmbination
frequencies.
A comparative estimate is given of two methods of forming the basic intermediate
frequency signal (fr fs and fr fs) in terms of the degree of the effect of the cCMgi-
nation frequencies on the operation of the superheterodyne receiver.
As particular cases of the analysis, recommendations are given for the choice of
the intermediate frequencies of an unadjusted superheterodyne receiver, an adjusted
superheterodyne receiver with a tuned preselector, a tuned superheterodyne with an untuned
wideband preselector and a superheterodyne receiver with multiple frequency conversion.
80
1 ~6p
0/011
31,10Y86 04/06/007
B
B014 B014
AUTHORs Dneprovokiy,_V. I.
TITLEs The Effect of the Combined Current Components of a Mixer on the
Selection of the Intermediate Frequency
PERIODICAL: Radiotekhnika, 1960, Vol. 15, No. 4, pp. 63 - 72
TEXTj In the paper under review, the author describes a universal method used
to analyze'the effect of the combined current components of a mixer on the
selection of the intermediate frequency. A survey of the general conditions is
given in the first part. Equations (100 (11), and (17), (18) are developed,
which permit to estimate the number of superfluous channels by the proper selec-
tion of an intermediate frequency. It is, however, not possible to work out
general recommendations for this purposet but only for each individual type of
mixer and receiver. Crystal mixers have the largest number of combination fre-
quencies. Calculated and experimental data for typical modes of operation of such
mixers are summarized in Table 1. Superheterodyne receivers as well as the de-
mands made on the preselector and the width of the range of intermediate fre-
quencies are studied in great detail. Next, the author describes an improved
Card 1/2 1r
80164
The Effect of the Combined Current Components of a Mixer S/106/60/015i'04/06/00-1
on the Selection of the Intermediate Frequency B014/BC14
superheterodyne with unmodified broad-band preselector. The limits of inter-
mediate frequencies calculated here are summarized in Table 2. On this basis the
author explains how it is possible to avoid superfluous channels. The last part
of the article is devoted to the multiple conversion of frequencies. Two cases
are described in which this frequency conversion is used. In the first case,
good selectivity is intended to be warranted with respect to the mirror and
additional channels, while spectrum analyzers are used in the second case. Ana-
logous conditions for the selection of intermediate frequencies are derived.
There are 3 figuresp 2 tables, and 2 Soviet references.
SUBMITTEDt January 12, 1959 Vf
Card 2/2
1P
L 07 Z 6-67 Ewr (l)/W(m)/zwP (t)/tri ijp(c) jp/AT
ACC NR- AP6025280 SOURCE CODE: LrR/03B8/66/000/003/0128/0130
4/ 7z-
AUTHOR: Dneprovskiy, V. S.; Parygin, V. I. ~31
OP%G: 11 ity (Kafedra fiziki
,?:Went Q~ OA6 llatiq sics . Moscow state
.T.La Uaivers
c
koleban y, oskovskiy uftarstvennyy universitet)
TITLE: Influence of efeocs field on the edge of the main optical absorption band
t c
in semiconducti _ ingle crystals CdSxCdSe.,-x
V
'&J3TJ"RCz:: Moscow. niversitet. VezAtnik'. Scriya III. Fizika, astroncmiya, no. 3, 1966.,
128-130
TOPIC TAGS: cadmium compound, abaorptioti edgep absoxTtion coefficient, electric fielt
ABSTRACT: The authors investigated samples of semicodductor single - XyRtpal- mixturps
CdSxcdE;e3.-x, in which the absorption edge can be located in the wavelengtb region
0-5 - 0.7 V, depending on the compositioz~. The samples vere made in the form of
polished bars measuring 8 x 2 x 1-5 mm with contacts deposited on the end faces. The
high resistivity of the samples (P - 101c' ohm-cm) made it possible to produce in the
crystals const" fie44 UP to 3 x 104 V/cm. The shift of the absorption edge for
the crystal C~~6.5=eo.5.. by 30 A. was cbserved at somewhat lower value of the ex-
ternal field and foil-he crystal CdSo.7CdSeo.3, apparently due to the larger slope of
the absorption edge of the sample employed. The results show also that the absorp-
tion coefficient increases in near-parabolic fashion with increasing electric field.
The inertia of the effect will be the subject of further study. The crystals were
grown by Ye. A. Huzalevskiy. Orig. art.bas: 2 figures.
SUB CODE: 20/ SUBM DATE: OlBep65/ ORM MW: 0031 OTH MW: 002
CO,d 1/1 UDC: 621.315.593: 535
IT W/E
WeVEdT(m) np(c)
ACC 14R: AP6015799 BOUBCE CODE: UB103MI6610031010103851038.9
JAUTHCR: Dnepro4~kVj,X,-.,.-6,.., Jg- hkoL D~ N. 1~enin A. No
ORG: rlw-ac- sity im*'
-ZASR~ ~ment of the, Moscow I~tate UniYer M. V. U)monosov (Fizi-)
ak--f ~versltet '
cheskiy RL ul'i aF-7--,
TITIZ: Photoconductivlty atricti under the inrluence of laser radiation
L/of diele
SOURCE: Zhurnal eksperimentallnoy i.teoreticheskoy fiziki. Pialma v redaktsiyu.
FriloibeniYey v- 31 no. 10y 1966s 385-Y~9
TOPIC TAGS: photoconductivity,, laser eallasionj ruby, Aoser$ sodium chloride, aluminum
wtide,, photon
ABSTFUtCT-. '~Tfie iuthori wresent- prelimina
ry results of -experimento aimed at observiq;
the photoconductXvity induced In unculored WaC1 w2d A1203 single crysteas by radia-
tion 1'rom a pb e ample vas placed in a parallel-plate
Blaser. The investigat d s
capacitor,charged to a voltage Ro - I kv~. The laser i'lash induced in the capacitor
a charge which was observed on an oscilloscope. To increase the radiation density
(by a factor of -5) and to reduce the beam dimens.11ons'r a cylindrical telescopic SYS!-.
tem, wex used. To wiroid effects connectea with tbe spate charges., the voltage 'was
applied to the capacitor only just before the flach; the capacitor was short- aircuited
during the intervals between the flashes - The logarithmic plots of maximum charge
Ys. radiation density (8) turned out.to be essentially rbraigbt'llnea (corres-
ponding to Q Sn) w.11th slopes n 4 i9 i o.4 for )W1 and n 3 1 0 -3 for A1203. The
Cc 1A
~1 26131-66
ACC NRs AP6015799
.charge growth time was -0.2 msee in both cases., this being apparently due to the pre-
sence of shallow traps. 7he authors attribute the observed effect to marty-photon ex-
citation of the electrons in the conduction band. The experimental values of S can
be reconciled with theoretical estimatets of the probability of n-photon abs9rRtion
if the radiation energy averaged over the beam cross section is 13) - 3.00 W/cnr for
NaCl and 20 Mw1ce for Ale%. It ia pointed out in the conclusion that the ob-
servation of many-photon absorption in Laser media is of interest for the study of
the mechanism whereby they become demage-d at large generation leirelsp and for the
determmtion of the limiting laser power. The experiments also yield-an estimate
of the limiting radiation density Smax tit vhich the gain, in ruby is offset by three-
photon absorption. This is found to be Smax - 3 x .109 w/cRP., which is two orders of
magnitude smaller than the value of -$.-I, calculated by F. ~,V,_Bunkin and A. ~ M. Pro-
khorov (zhETP v. 48, io84, 1965). The authors thank S..AO' tdduwinov and R. V. Kklokh-,
-lov for valuable advice and discussions Orig. art, has: 1 figure and 2 formulas.
SUB CODE: 201 SUBM DATE: :.OIMw&/- MIG REF: 002/ OTH REP: 005
212:~~
NIKITIN, A.T.; VASYUTINSKIY, N.M.; DNEr-ROVSKIY, V.Ya.
. DBvices for noneontact reasurements of wail thicknes3 of nry thir,
walled pipes. Avtom. i prib. no.2%34-36 AP-Je 165. (MI;U 180)
v
PME I BCOK XXP~DITATION SOV/4999
VladimiravY Yevge*y Vladimirovich, and Yevgeniy Vasillyevich Dneprovskiy
Alr,tivnyy i avtomaticheskiy kontroll dLbtaley na stank-Akh-avtonataLkh i
avtcmaticheskikh liniyakh (The I.Peadback and Auiamatic Control of Parts on
Automatic Machine Tools and Autamwhic Lines) Minsk, Gas. izd-vo BSSR, 1960.
138 p. 2,000 copies,printed.
Ed.: S. Pollskly; Tech. Ed.:-N. Stepwiova.
PURPOBE: This book is intended for j*rsonnel dealing with the automation of pro-
duction, and-especially for those concerned with problems of automatic control.
COVERAGE: The book, based on Soviet and non-Saviet sources, presents an analysis
'of methods and devices used in the feedback and automatic control of partd in
the machine industry. Particular attention is given to types and systems of feed-
back control, the construction of transducers, and the use of transducers in vari-
ous types of automatic machine tools and production lines. Chapters I,II; IV, .
V.- and VIvere written by YeV. Dueprovskiy, Engineer; Ye. V. Vladimirov, Engineer,
wrote chapters -So'book was written under t,ie supervision and
with the participation of G#K. Goimwkiy, Candidate of Technical Sciencen.
DNEPROVSKIY 1e V
Active control of latheve Sborstrude.TmBt&mash.i avi-om.AN BSSR no.l-.
47-55 161. (14IRA 1635)
(lathes-Numerical control)
DN&PROVSKIY, Ye.V.
Automatic readjustment of' metal-cutting tools. Mauhinostroital
no#10:23-24 0 t6l. ~ (MULk 14 -- 9)
.. (Metal cutting tools) (Electronic control)
DI'
vE 111. _ ya.;,.
I .., I I... - ~,, " , ~. :,", 1, .,
Cominarative ecological stvd:;e~i of the ar-1, r~--srlrat--cn
of planto in the Kuray Ranje. arudy TSSBS no.7:1.C-*---')-'(,, 164.
'17
0 HL-k 17:11)
3
3/208/62/002/001/007/016
D299/D303
AUTHORS: Dnestrovskiy, Yu.N., and Kostomarovq D.P. (Moscow)
TITLE: Propagation of electromagnetic waves in a plasma
normal to the external magnetic field
PERIODICAL: Zhurnal vychislitellnoy matematiki i matematicheskoy
fizikit v. 2j no. 1, 1962t 97 - 106
TEXT: The propagation of electromagnetic waves in a direction nor-
mal to the external magnetic field is considered. The existence
and uniqueness of the solution is proved by the method of successi-
ve approximations. Thereuponp integral transforms are used for con-
structing solutions to the problem with initial conditions and the
problem on wave excitation by side currents. Those solutions show
that notwithstanding the presence of complex roots in the correspm-~- V~
ding dispersion equationg no energy transfer takes place from the
plasma to the electromagnetic field (or conversely) during wave-
propagation under steady-state conditions. In the linear approxima-
tion, plane-wave propagation in a plasma is described by equations:
Card 1/6
33293
S/208/62/002/001/007/016
Propagation of electromagnetic ... D299/D303
8/ + v. Lf + '- [v, 11.1 ff-0 E 0/0 (1)
T, ax -M-- a-V M av,
rot 11 = I Lr- + L" j +j(--,) (2)
C at C C
rot. E (3)
at
J=C~/V&V. (4)
HO is a homogeneous magnetic field, normal to the direction of pro-
pagation. After computations, the problem reduces to two indepen-
dent systems of integro-differential equations in the field compo-
nents. For these two systemst existence- and uniqueness theorems
are proved. The proofs are based on the method of successive appro-
ximations. This method (besides proving the existence and unique"
ness of the solution) permits finding a majoraait estimate for the
solution and to investigate its behavior at the initial stage of
the process. But this method is unsuitable for studying the behavi-
or of the solution at t ---> oo which is of great interest in practi-
ce. This can be achieved by the method of integral transforms whic-
2/6
33293
5/208/62/002/001/Qq7/016
Propagation of electromagnetic D299/D303
yields explicit expressions for the solutions. Thereby, it is assu-
med that the side currents are harmonic functions of time. The
first system of integro-differential equations is considered; a
Fourier transform (with respect to x) is carried out, and a Laplace
transform (for t); the obtained algebraic system of equations is
solvedp yielding the result:
(0, k) 1, 208" (Q. k) 8.(Q, k)= k) (21)
(9-ca) D, (0, k)'. (0 -co) D, (Q, k)
Here cr.' XPY is the'Fourier-Laplace image of the electric-field compo-
nents:
CO Go
einidt ~ (22)
iW
__C0
D, (.Clt k) = k 2 c 2E LCI 2 (F-1 1 E22 '-21'12)'. (23)
The singularities of the functions t X and ~ y in the complex plane
f2 are the zeros of'the functions D 1 and the point w. The
Card 1/6
33293
3/208/62/002/001/007/016
Propagation of electromagnetic ... D299/D303
equ,ation,Dj(,CIf k) = 0 is the dispersion equation for the type of
wwres under consideration (extraordinary wave). By means of Mell-
in's transform, one obtains the originals from the images (21),
(w, k), I Vom
E. (t, x) +
_EV 01 X)
.k) Rx-an') (25):
V~,
+ YJ (o).,k) --'D-
Owing to dissinative processes- the free oscillations are damped
and the solution for t ---+ co is determined by the side currents on-
ly. These forced oscillations are separated by means of the princi-
ple of limit absorption. The first terms in Eq. (25) describe pure-
ly forced oscillations which determine the electromagnetic field
for t --~,cot (steady-state conditions). Thus
VR; X) 00 + iv) a-, (wt-kx) BIB ((0 + ivi k (26)
HMIV A D, ((o + iv, h)
Ey (t, x) o 813 (,a + iv, k
Card 416
p/ZO8/62/002/001/007/016
Propagation of electromagnetic D299/D303
'); 'it is
By considering the dispooltion of the roots of Eq-'(2~'
found that integral (26) can be computed along the real axis. As-a
resultf, the field in the region xl.~> Ot- 113 determiqed as -the -sum o;~
the residues at the zeros of the ft'Action, -Dl (W;~:k) j viz.
aW ei (k~x-ta') Px(-) e7i (k,,m+.O +
E=Q,x)=Ivt2 X., 'Y (27)
n
+1(,Jn) ipz (n)-
+ 2] T,(1), e"':"' X. . e+ 6x1. V ~-tNx) Cqnx-iwt
where a, and are constants. The first sum in (27) represents
undamped waves with phase velocity directed from the source away,
the second sum -- undamped waves with phase velocity towards the
source, the 3rd and 4th sums represent exponentially damped solu-
tions and standing waves, respectively. It is noted that (notwith-
standing the complex roots), no energy transfer between plasma and
electromagnetic field takes place. Further, the dispersion equa-
tion D2(a I k) = 0 is derived.(for the ordinary wave). The above
solutions were constructed on the.assumption of zero initial condi-
tions. In case of nonzero initial conditionsp the solution can be
obtained entirely analogously. In conclusion it is noted that the
Card 5/6
;""3
S/20 62/002/001/007/016
Propagation of electromagnetic ... D299YD303
solution (25) was obtained formally, without ascertaining its con-
ditions of applicability. There are 3 references: 2 Soviet-bloc
and 1 non-Soviet-bloc. The reference to the Dinglish-language pub-
lioation reads as followei E.P. GrosBf Plasma oscillations in a
static magnetic field. Phys. Rev., 1951, 82, no. 2, 232-242.
SUBMITTED:
July 18-t 1961
Card 6/6
DNEtTROV, - G. In.
Stock and Stockbrec.-~ing
Diversified economy on a progressive collective farm. Sots. zhiv. 14 No. 7, 1952.
9. Monthl List of Russian Accessions, Library of Congress, December 1956, Uncl.
2
-Brutleim at &Pro-awtal omilliiiitimill Tuba WA an us"lopil"Ut W a
TrCkwolo" for Their lFirmuchon. -A. 11. smirvaclu.
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In
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limwitcroititimat the m,,rL-,;o
srmlij" witinj to sitim-aling brilth-omo awl (tit fulm-s Ithidt inuild Iw drsuls
'AlislActmilv. indirAted that C&TI-411 to r.%%,qVA 'PrAlwUl tAmh Iltu
MbrililmliM. TIJV C-ArbOll -4 AN ilitTWXI 91-1-11 'Ail h I IP-* .111 -fill " IliAd gIn IM 4
and, w R ltwm-r uxlen', mith mork-i scroll 4-4111tAllimpletl 'Ailli graldilt.-.11
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hard u tubtv illivuld be given & iturm-Miuviug anwal at Vo#
rhis *ill rliw~natv any tnWemy to ent-L Ili the men-uti.-miftl,
"'t. F,-r mail-Itir ati;sealinz u-- lmj.~mtun~ almv if.,
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For imneAlirigst tilt- unrL,. hobling bw 2 I'm at It"- Hillp-.41mg. Irmp #Aw-
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vio, tnarLed alect ou the prulirrtitt of thi- lutxz ajid tan to- rl"~it to Puit
;br Capaejt-j- lif lilt- IM-. A ~4111141111, 4 druilihig I~wo~ (mlurisom~ I.-r
Wit. &%,LqA Wr the I tul- -VIIAmm~ I....
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i-ml JwIO N JIKIJ Vt.J1j.JIe-j14dftUjiDg lUllfil-AtIt Walt .-I
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at " 0 1 9 14 Tom
it Mi 00 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 6 a 0 0 a 0 a
: : : *
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0 0 0 0 0 0 0 a 0 0 0 0 411 0 0 0 0 9 0
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-
4'q Y ~Y'4 rjo'c
1M'1WW=Q- JJIWIAV 2011'amovich; BOGOLYUBMY, V.I., inzhenor, retsen-
zenr'; 1--A1% BAV, 2e.9P.",'W1nzhener, retsenzent; SEPICHIM*,TSKIT, U.S.,
redaktor; WARO NU, S.N., redaktor; EXEMM, O.G., teldinicheskiy
redak"or.
[Drawing of nonferrous metals and alloys] Volochenie tovetnvkh matik-lov
i aplavov. Moskva, Goe.nauchno-tekhn.12CI-VO lit-ry po chernoi i
tovetnoi metallurgii, 1954, 270 P- (MIRA 8-3)
(Metal clraving)(Nonferrous metals-Metallurg7)
MSTROVSKIY, IA.; YUIMTS. LA., redaktor; LARIO1107, G.Ye., tok-halchs-
- -'--,9kWrddW'br
[Drawing tool] Volochillryi instrument. Moskva, Goo. energ. izd-vo,
1954. 188 p. (MLRA 7:10)
(Metalworking machinery)
(Metal drawing)
z _*ch; PCNBRLNTSJV,
DNBSTROVE~TJY,X~XoW, ~nwlpv 'Sergey Rikolayevich;
mnonTiTkii, kgzd. takhn. wuk,.'rotsenzent; POSTNMDV,
N.N., inzh., retsenzent; AZHMIWV, V.S., rod.; KOSOLLMA, Z.F.,
red. izd-va; BERWY, A*P-P, tekbn. red,
[Concise manual on.workizig, nonferrous metals and alloys] KratUi
spravochnik po obrabotka tovetnykh matallov i splavov. Moiakva,
Goo. nauchno-telchn. izd-mv lit-ry po chernoi metallur 11 1958.
4,06 p. ~Ml& 11:8)
(Nonferrous metals-Metallurgy)
DNESTROVSKIY -Nikolay Zei'manovich; IIOMEWTSKV, Sergey Niko3.ayevich
N-oceamedj; =7-9TV.--f-d-eRased]; SPIPICHINETSK11, Ye.S., kand.
takhn. nauk, retsenzenti POS7241KOV, N.N., inzb.p retsenzent; RZHEZ-
NIKOVI V.S., red.; KOSOLMVAq E.F.j red. izd-va; BEUV, A.P., takhn,,
red.
(Brief manual on the treatment of nonferrous metals and alloys) Krat-
kii spravochnik po obrabotke tsvetnykh metallov i splavov. Moskva,
Gos. nauchno-tekbn. izd-vo li-t-ry po chernoi i tsvetnoi metallurgii,
1961. 410 Pe (MIRA 14:8)
(Nonferrous metals) (metalwork)
PHASE I BOOK EXPLOITATION SOV/5530
Smiryagin, A. P., N. Z. Dnestroy!kiy,_A. D. Landikhov, N. N. Kreyndlin,
G. N. Krucher, V. A. Golovin, B. L. Urin, and V. N. Golldreyer
Spravochnik po obrabotke tsvetnyich metallov i splavov (Handbook on the
Processing of Nonferrous Metals and Alloys) Moscow, Meta-Uurgizdat,
1961. 872 p. Errata slip inserted. 9, 300 copies printed.
Ed. (Title page): L. Ye. Miller, Candidate of Technical Sciences; Ed. of
Publishing House: K. D. Misharina; Tech. Ed.: M. K. Attopovich.
PURPOSZ!: This handbook is intended for technical personnel of metal-
working and machine -building plants, design organizations, scientific
research institutes, and laboratories, and for students at schools of
higher technical education.
COVERAGE: The handbook discusses the physicochemical and mechanical
properties of certain elements and the composition and properties of
Card--ij:#-
Handbook on the Processing (Coni.) SOV/5530
nonferrous metals and alloys, and includes an explanation of the theory
of principal methods for the hot and cold working of nonferrous metals
and alloys, Reference material on designing, engineering- economic
planning, quality control, and other aspects of production is systematized
and presented. Each part of the handbook contains explanations of prin-
ciples underlying basic procesiies, presents formulas for process and
engineering calculations. analyzes properties of metals and alloys, gives
parameters of accompanying and secondary processes, and describes
equipment and tools and their'o'perational parameters. The authors
thank I. L. Perlin, Ya. F. Shabashov, and M. F. Bazhenov. References
accompany each part, as well as varioub chapters. There are 130 refer-
ences, mostly Soviet.
Carli-Z/ 9~-
Handbook on the Processing (Conl:.) SOV/5530
PART VI. WIRE MANUFACTURE
(by N. Z. Dnestrovskiy, Engineer]
Ch. I. Basic Principles of Hot Shape Rolling 496
Ch. II. Rolling of Wire Rods and Strip Billets 532
Ch. III. Fundamentals of the Drawing Process 576
Ch. IV. Wire Drawing 615
Bibliography 712
Cq~r&w
CHININAY N.S.: NMLISKAYA9 M.N.j DUESTROVSM.-B.Z.; PEMVA.. OA.
F,2ect,ro;ytio polishing of recit4mgular wires. Biu1,tekh*-ekoa*inf6im#--
Goo.nauch.-issl.inst.nauch. i tekhAnform. no*4;15-17 162,
(MIRA 15-7)
(Electrolytic polishing)
PHASE I BOOK EXPLOITATION 911
Dnestrovskiy, Nikolay Zinov'yevich and Pomerantsev, Sergey
N101-ay-e-VI-eff-
Kratkiy spravochnik po obrabotke tsvetnykh metallov J. s lavov
(Handbook on Workin -of Nonferrous Metals and Alloys~ Moscow,
Metallurgizdat, 1959. 406 p. 11,500 copies printed.
Reviewers: Shpichinetskiy, Ye.S., Candidate of Technical Sciences,
and Postnikov, N.N., Engineer; Ed.: Rzheznikov, V.S.; Ed. of
Publishing House: Kosolapova, E.F.; Tech. Ed.: Berlov, A.P.
PURPOSE: This book is intended for engineers, designers and other
personnel who need b,asic information on the most widely used
nonferrous metals and alloys.
COVERAGE: This is a handbook containing information on the basic
properties of the most widely used nonferrous metals and alloys
and methods of cold forming and hot forming them. Various
Card 1/8
Handbook on Working of Nonferrous (Cont.) 911
formulas for calculation of basic data in rolling, drawing
and pressing of nonferrous metals and alloys are given. The
author thanks A.P. Smirnov for help in preparing the book.
Chapters I, II, and-III were written by S.N. Pomerantsev,
Chapter.V by N.Z. Dnestrovskiy and V.V. Zverev, and Chapt 'ers
IV, VI) and VII by N.Z. Dnestrovskiy. There are 26 Soviet
references (including 4 translations).
TABLE OF CONTENTS:
Foreword
3
I. Physical and Manufacturing Properties of Nonferrous Metals 5
II. Chemical Compositions and Mechanical Properties of
Nonferrous Metals and Alloys 11
1. Aluminum 11
2. Aluminum alloys- 19
3. Magnesium and iti~ alloys 31
Card 2/8
Handbook on Working of Nonferrous (Cont.) 911
4. Copper 3
5-
Copper-zinc alloys (brasses) ~
4
6. Tin bronze 64
7. Tin-free bronze 72
8. Nickel 84
9. Nickel and copper-nickel alloys 85
10. Tin 112
11. Lead 114
12. Tin babbits 116
13- Calcium babbits 117
14. Zinc and its alloys 118
15. Solders 122
16. Titanium and its alloys 126
17. Zirconium 130
18. Termostatic bimetals 134
III. Hot and Cold Rolling of Strips, Sheets and Bands 138
1. Basic definitions 138
2. Formulas 143
Card 3/8
Handbook on Working of Nonferrous (Cont.) 911
3. Strip-, sheet-j, and band-rolling mills 156
4. Brief information on rolling of strips, sheets and
bands 174
IV* Extrusion 181
1. Determination of press pressure in forward extrusion 181
2. Extrusion presses 189
3. Brief information on extrusion 198
V. Hot Rolling of Shapes 205
1. Basic definitions 205
2. Formulas 210
3. Rod-rolling mills 218
4. Basic information on roll design 223
5. Brief information on hot rolling of shapes 251
VI. Drawing 258
1. Basic definitions 258
2. Determination of forces in drawing of circular
solid shapes 263
Card 4/8
Handbook on Working of Nonferrous (Cont.) 911
3- Sequence of operations 2 3
4. Wire-drawing equipment 210
5. Brief information on wire drawing 322
VII. Bar and Tube Drawing 341
1. Determination of forces in drawing of tubes 341
2. Bar- and tube-drawing equipment 342
3. Brief informatlob on bar and tube drawing 352
4. Cold pilger rolling of tubes 36o
Appendices 362
I* GOST (All-Union 41tate Standard) 2771-57. Recommended
Tole'rances for Round Wire in Diameter From 0.005 to
16.0 mm. 362
II. Standard Grades of Rods and Shapes Drawn From Nonferrous
Meta.ls and Alloys 365
Card 5/8
Handbook on Working of Nonferrous (cont.) 911
III. GOST 1945-46.. Standard Sizes for Rods Drawn From
Nonferrous Metals and Alloys 367
IV. Nomenclature of Tubes Drawn From Nonferrous Metals
and Alloys 368
V. Approximate Weights in kg. per sq, m. of Nonferrous
Metal and Alloy Sheets, Strips and Bands 369
VI. Approximate Weights in kg. per 1000 m. of Round
I Copper Wire 370
VII. Approximate Weights in kgo per Linear Meter of
Nonferrous Metal and Alloy Rods 385
VIII. Approximate Weights in kg. per Linear Meter of
Drawn Copper Tubes With Outside Diamvtvs up to 100mm- 386
IX. Approximate Weights of Drawn Copper Tubes With
Outside Diameters of 100-360 mm. 389
Card 6/8
Handbook on Working of Nonferrous (Cont.) 911
X. Approximate Weights in kg. per Linear Meter of L62 Brass
Drawn Tubes 390
XI. Conversion Table (Inches to Millimeters 393
XII. Conversion Table (Decimals of an Inch to Millimeters) 395
XIII. Conversim Table (Fractions of an Inch to Decimals of
an Inch and-to Millimeters) 396
1
XIV. Conversion Table (Feet to Meters) 397
XV. Conversion Table (British Pounds to Kilograms) 398
XVI* Conversion Table (British lbper sq-ine to k6 per
sq, lam.) 399
Card 7/8
. .11andbook on Working of Nonferrous (Cont.) 911
XVII. Conversion Table (Tons per sq. in. to kg. per
sq. mm.) 401
Bibliography
AVAILABLE: Library of Congress
Go/her
12-15-58
403
Card 8/8
.4. /V
USSR/Wtthema-lics Proper values
Card 1/1 : Pub. 129-8/18
FD-1505
Author : Dnestrovskiy, Yu. N.
Title : Variation of the eigenvalues when the region of the boundary varies
Periodical : Vest. Most. Un., Ser. 'fizikomat. i.yest. nauk, 9, No 6, 61-74, S6P 54
Abstract : Continuation of previous works by author (DAN, 63, 6: Warilation of
the eigen values in the case of fixing within the region, "Disserta-
tion of Moscow Univ., 1948) studying variation of eigen functions in
the case of additional fixing within a small region near the limit or
near the nodes. The variation of the eigen function will be expressed
in smaller terms, while the concept of capacity loses its meaning.
Indebted to Prof. A. A. Samarskiy, Eight references including 2 foreign.
Institution : Moscow University, Chair of Mathematics of Physics Faculty
Submitted : May 23, 1953
DMIRCIVSKIY, Yu. X.
DNESTROVWIKIY, Yu. N.-. "On the change in natural values in changing fieldt. Moscow, 1955.
Moscow State U ineni M. V. Lor.,onosov, Physics Faculty. (Dissertation for the Degree
of Candidate of Physicomathemathical Science)
SO: Knizhnoya Letopis', No. 40, 1 Oct 55
SUBJECT USSR / PHYSICS
AVTHOR DNESTROVSKIJ,JU.N.
TITLE The Modification of
Resonators.
PERIODICAL Dokl.Akad Nauk 111,
Issued: ; / 1~5_7_
CARD 1 / 4 PA - 1975
the Eigenfrequenoies of Electromagnetic
faso.1, 94-97 (1956)
The problem of the modification of these eigenfrequencies in the case of a
slight modification of the shape of the resonator or the introduction of
small, perfectly conductive bodies into the interior of the resonator, was in-
vestigated by many authors by the perturbation method. Because of the compli-
cated nature of the problem all authors were content with the first approxima-
tion, and the problem of higher approximations was not raised. However, for the
problem of the introduction of small conductive bodies into the interior of
the resonator the result obtained by means of the first perturbational approxi-
mation is too rough. On the occasion of attempts made to improve the results of
the perturbation theory for bodies of special shape (sphere, rotation ellipsoid)
the problem regarding the degree of accuracy of the formulae obtained remained
open. The present work investigates the modification of the eigenfreqixencies
of the resonators by the method of successive approximations, on which occasion
convergence is proj~ved first. For the modification of the eigenval, a
general formula is obtained from which results the formula by MAIER and SLATER
for a spherical conductive body.
The general method is also suited for the problem of the modification of eigen-
values as a result of a modification of the parameters E and eL within the re-
Dokl.Akad.Nauk 111, fasc.1, 94-97 (1956) CARD 2 / 4 PA - 1975
sonator. The results obtained in this manner are then compared with the first
approximation of the perturbation theory. It is further shown that, on the
occasion of the introduction of a small dielectric body into the interior of
the resonator, the perturbation theory offers a result for the modification
of the eigenvalue that differs considerably from the true result.
In a closed volume T with perfectly c.onductiveb ndary r the problem of the
free oscillations of an electromagnetic field E, is here. investigated for
the case of lacking spa-tial flows ands charges const - 1):
> 2 --~ -) --31 1 -31 1
curl curl E - k E inif, [,E, n O.to H (1/k) curl E. Here the homo-
I
geneous integral equation BOO - I Kt(M, MI) E (MI)dT Mt is investigated.
Here Kt(M,MI) denotes GREEN'S tensor for the volume T which satisfies the
following conditions: K t . rt + 9t) f' - I/4nrMM,, div t - 0. Ft denotes
the"transversal"part of the fundamental tensor I" and I the unit tensor.
Furthermore it is true that curl curl K t - 0, div K t - 0 in T at M ~ M1
1KtP 0 on The latter equation determines the nucleus X,(H,.Ml
univocally.
Theorem: In order that E be an eigenfunction of the problem set here it is
necessary and sufficient that 9 be an eigenfunction of the above mentioned
integral equation.
'Dokl.Akad.Nauk 111,fasc.1, 94-97 (1956) CARD 3 / 4 PA - 1975
It follows from this theorem as well as from the aforementioned conditions
that the nucleus Kt is symmetric, integrable-in the square, steady in the
average, and positively definite. Herefrom follows the convergence of the
method of successive approximations for the equation mentioned above. For the
domains of T for which the tensor K t exists there exists a discrete spectrum
of eigenvalues and eigenfunotions of the problem investigated here. The
terms of the functional sequence of the method of the successivo approximations
of the equation mentioned at the beginning satisfies the following relations:
ErL M ( KtEn-2dT. Therefore, on the basis of the theorem mentioned, these terms
T
are also solutions of the following boup4ary value problems:
curl curl div 0 to From the functions
n 2 = 0 in T, I E
Ennumerical consequences can then be built up for which the recurrence formula
is valid.
It is then presupposed that the volume T is slightly modified either as the re-
sult of a deformation of the external boundary or of the introduction of small
perfectly conductive bodies: T = T + g, where g denotes a small domain with the
boundary 2 + g. --> A --)
Next, the problem curl curl E E in 'r, [1, 4n 0 to F + ~ is investigated
in the domain 7, and:
A (k) and E (k), H(k ) denote the eigenvalues and eigenfunctions respectively of
Dokl.Akad.Nauk 111,fasc.1, 94-97 ('1956) CARD 4 / 4 PA - 1975
this problem. The aforementioned p lem is investigated by the method of aucces-
sive approximations. The functional, are searched for in form of a sum of the
'? : In this way
solution of the problem I and a orreotion function
_+ --> n -4 .3 n
En - ejAj + f n is found, where f n satisfies certain boundary conditions mentioned
in this connection. Next, the eigenvalue P) is determined and the definite
formula is written down. This formula differs from the result of the perturba-
tion theory. The formulae obtsined are specialized al-so for the case that a small
perfectly conductive spherical body waa introduced into the interior of the reso-
nator. The results obtained 1jy MAIER and SLATER for a small sphere agree with the
results o'btained here, and therefore the author describes them as correct.
The meth.-od of successive approximationo is also suited for the problem of the
modifice,tion of eigenvaluea on the occasion of a modification of the parameters
6 and 6-U. in the interior of the domain T. Such a modification is especially
mentioned because of the introduction of a small dielectric body into a
homogeneous endovibrator, aiid it is specialized for a small sphere.
T-*NSTITUTION: Moscow State University
AUTHORSs Dnestrovskiy, Yu. -N-t Kostomarov, D.P. 20-3-8146
----------
TITLEj The Radiation of Charged Particles Flying Past Ideally
Conductive Bodies (Izluoheniye zaryazhennykh chastits pri
prolete vozle ideallno provodyashchikh tel).
PERIODICAL: Doklady AR SSSRI 1957, Vol. 116, Nr 3, pp. 377-380 (USSR)
ABSTRACT: The present report investigates the general problem referred
too in the title, in. non-relativistic approxiration. The
authors investigate the radiation of a punctiformly charged
particle with the mass m and the charge e in flying past
the ideally conduotive surface 3 . The surfa,~e S is
assumed to be axially symmetric and to have tae equations
r - h1(s), z - h2(s)j here s is the length of the arc
(-00n - Of one of these roots tends toward zerop and the other towara +cD.:
,Outside' these ranges (1) shows no real roots for W< 6) . For WK EJ there
0 0
are ranges near the resonance frequencies, where (1) has neither real nor
imaginary roots. But'(1) has an infinite. numbler of complex root
quad .ruple8 k Pa jqn (m), k = -p. 1q..
CELrd 215_
24713
S10561611040100510131019
.0
t
Dispersion.equation for an ordinary ... B109/B212
for any value of (.A/ nIA,,., If LJ has to be calculated as a function of
real wavo numbers k W (k)), . then it is necessary to determine 'the
intersections of the lines N kc/Ogo; (dotted line in Figs. I and 2)
with the function N . js(a, P, y) in order t o fink the real roots of (1
A pair of roots W. +-GJ of Eq. (1) corresponds to edch point d", N
An analysis shows that the number of intersections is infinite. Numbering
the abscissas of theae points according to their increase, ( a< a2