SCIENTIFIC ABSTRACT GINTSBURG, B. - GINTSBURG, M.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000515120007-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 26, 2002
• Sequence Number: 7
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

GINTSBURG.,j.ja,.,,doktor tekhn.nauk, prof.; RABINOVICH, A.Sh., kand.tekhn.-
nauk
"Investigating piston rings of tractor-type engines" by V. G.
Gonchmrenko. Reviewed by B.IA.Gintaburg, A.Sh. Rabinovich.
Vest.mashinostr. 42 no.9:84-87 S 162. (MIRA 15:9)
(Piston rings) (Goncharenko, V.G.)

L k166_6fi~J RMIWW
UR/9191/65/000/010/0042/0044-,5
ACCESSIONINIft; AP004508
44X 40
t A
AUTHORt. 16ova, Ye. I.; Kovarskaya, B, M.
Ab
TITIA: Po4r4gra-4W invostiption of the products of thtrmo- oxidative destruc-
tion`~Uf pol r on majoic and chlorendic anhydrides and ethylene
-7 -glycol
SOURCE: Plastichaskiye massy, no. 10, 1965, 42-44
IPPIC TAM poir plastic,. polarographic analysis, oxidative degradation,
chemical mochanici
ABSTRAM, The prioftcts obtained from thermal oxidation of a polyester resin
were analysod polarbgraphicAPI to help establish the mechanics of the destruc-
tive processi; -The Ool e g malsic
yesteritiv sti atod wag based on diethylene glycoi
slid c Mes ILIA 4:0, 0 rholar ratio), cured with benzoyl peroxide
. , hloreniia anhy
and diethan ohitne ikfityrenwISM'styrene in the -initial solutions). It was heat-
ed it 240C.f6r i- 4 I~Uis under an initial oxygen pressure of 200 mm Hg. Form-
aldehyde, sialdshyde, benzaldehyde and malsic acid were identified, No fumar,
-Coo 1/2

TI-L'INCHiEl K.S.; GIA'AsiJUIC, E.I.
Kir4tics of the en2~matic destiuction of the cell irembrane
of wi erythrocyte. bioZizi-ka, 7 no.2:21,4-247'62.(,Z,,A 16:8)
.,0
1. Listitut biologicheskoy fiziki A" SMY N si-va.
(Fj(ri,fIaLI-TM)

tell#$ *me
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I87).--AvW*%vpWdWw dam kg of twip4cm kw#
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n04 ONIONO VOWS" In do arky SUM of
delmilapmmW~ but a a ink" st4p nwopratioll is
AiomdiW AkA IRtw AK inMbited. IU region 4
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is
GINIBURC, 0. 1.
"Concernini! the FactorB which Cause the Loss of Repenerative 'apacities
in Tissues amonf, Anura ExtreirAties."
Dok- An., 30, No 6, 1941.

a t a a 0-~ a I I W
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rINFBURC, G. 1.
" Studies in icepeated Regeneration." Dok. AN., 45, No 6, 19U.
Mbr., Inat. Exptl. Mol., ra:,akh Acad. Sci., -IF,39-).,l;
Mbr., Innt. Gytologyp Histolopy & Emvlryolory, Acad. ljci., -19h1--
Mbr-, 2nd 'mloscow Med. Inst. imeni Stalin,
v

i !br. L _. . . I I
' Ins !'~ tl)tc- ~"' C% to-' OPY, His tology, sind c-g.-, Acad . -c J. (-194-/-)
11-1- "
-.1c, ,~rtulcii P.1-i on cf ;,_c,riona11-.! Different _rl:lr In I !~r , -, -'-,n ~:-,i 1 ,
in ~"!r '! an c "Ell I~Kimrin," Do k . A I,', : ,~ , ,~ o, . .- - .. ~ - 1. , , _.~s
I . I vt ~

G-1NTSBURG,G. I.
"Influence of Foreign okin on Development and ReVeneration of
Extremities in Anixan Amphibians."
Dok. AN, No 51 19hB.

GIITTSBnG. G. 1.
PA 43/43T63
*60be - MAI
Ovols ce ths
9ONM f
1
at* AW Mwk SM, Ildva Ser' Vol LIX.. No 4
DiMoribes OXMIamto whiab led to omalunim that
Cori= of regimmUy different skin does not
wtive part In regeneration of a llab but
domtl,y ratusft its dedifferentlation. Submitted
bi Aaadamloim 1. 1. Mmllpusnl Lm5 Roy 194T.
OT63

GINTSBURG, G. 1. 1
( - f,' /-1 1 r. . , I
1IRnle of S;dn In thm Regeneration of Organs. Regloynl Participation
of Dimelmilar Skin in the Regeneration of Ixtremitien In TsIlUmpte Amphib-
inne." Sub 20 Doe 51, 14opcow OblRet Pedagogical Inrt.
Dissertations pr~-sente(l for science Finil engineering degrees In Mop-
Cow dliTing lq5l-
SO& Sum. 110, L~i, 9 '-!Av 55

O"M, Vol. 5, 10.1
0 atobursOOM. (A.W. Severtsow Institute of Animal Morphology V.: Academy
!
; Science , Reatprreal Influezes of the transplant and the host In differient
agod transplants of extremities in tailless amplilb1s, 153-6
Akedowlys Nouk, B.S.S.R., Doklady, vol. 7F, no.1 I 1~4(

GINTSBURG, G. L
Homoplastic transplantation of certain embryonic tissues and
organs to adult mammals. Doklady Akad. nauk SSSR. 81 no. 3:
477-480 21 Nov 1951. (CLML 21:3)
1. Presented by, Academician A. I. Abrikosov 15 September 1951.
2. Institute of Animal Morphology imed A. N. Severtaov, Academy
of Sciences USSR.

GIIUSBIMG. 0.1.
Conditions and significance of wound epithelization for regeneration
of extremities in Amphibia. Doklady PAced. nauk SSSR 82 no-5-813-816
11 Fab 52. (CM 21:5)
1. Presented by Academician K.I. Skryabin 27 December 1951.
2. Institute of Morphology of Animals Imeni A.N. Severtsov, Academy of
Sriences USSR. . e,

BAW1NA, N.P.:GINTSBURG, U.I.:XUHCHAX, L.l.:POIXMYZV, L.V.:ROGALI, I.G.
Repair of cranial defects. Doklady Akad. nank SSSR 87 no. 4:673-
675 1 Doc 1952, (GIXL 23'-5)
1. Presented by Academician A. 1. Abrikosov 5 October 1952. 2. In-
stitute of Animal Horphology imeni A. N. Severtsov of the Academy
of Sciences USSR.

,~, GIMBURG, G. 1.
Replacement for skull defects In mature rate and dogs. Dok1. AN SSSR 87, No 5,
1952, pp 869-872.
When grafts consiting of bone of newly-born animals or of embryos are trans-
planted into the injured skull of adult animals, the tissue of the graft is
resorbed and replaced by freahly formed bone. Unless a graft is made,
only sear tissue is formed. Within the age limits studied (i.e., from embryos
to newly-born animals), the effectiveness of the graft increases with the age
of the donor animals. Presented by Aced. A. 1. Akrrikosov 6 Oct 1952.

Replaaement of bons defeets of the skull in mamm&ls. Trudy Inst,
morf,,zhiv. no.11:158-174 154. (MLU 8:2)
(Snal-.Wpr.1) (Bone 9-Transplantat ion)

b / /Y / 'S a
EXCEMA IOLA See-Z V61.9/8 ftaidlognate. W6
3614. G *Changes in the central nervous systent du-
ring regeneration of limb muscles (Russiar. text) DOKLA.
DY AKAD. NAUK SSSR 1955, 105/5 (1110-1113) Mug. 4
In young albino rats the entire skeletal musculature was removed from the left hind
lower leg, but large nerves and blood "matte were left Intact. lit one group the
excised muscles were cut up with scissor# and the pulp replaced in the wound.
Asepsis was not strict and Infection occurred. particularly In animals with the
reintroduced muscle tissue. Changes in the ventral horn cells of the spinal cord
were seen in both types of preparations. In rats with 'empty' wounds. paleness of
nerve cells could be detected after one day (the same on both sides of cord!), but
In 20-30 days the cells regained their normal appearance. In rate with stuffed,
wounds. even when there was no infection, the changes in the ventral horn cells
were more marked and longer lasting, with proliferation of glia,cells, while re-
storative changes were incomplete even 100 days after operation.
Meitman - Chicago, ni.

GINSBURG , G. I.
Some data on the role of the micronucleus in the accumulation of
nucleic acids in Paxamecium caudat=. Zhur. ob. biol. 22 no.6:
452-458 N-D '61. (ML-,A 14:11)
1. Inatitutg of Animal Morphnloi;y, U.S.S.h. Academy of Sciancos,
Moscow.
(GELL NUCLEI) (NUCLEIC ACIDS) (INFUSOUA)

GINTSBURGj G.I.
Autoradiographic study on thymidine-H'-inclusion in the
process of oogenevis. Zhur. ob. blol. 24 no.101-73 Ja-F'63.
(MIRA 16:11)
1. Institut morfologil zhivotnykb imeni A.N.Severtsova AN SSSR,
M013k-va.
)t"

IhT ~!,-A,~I chnr!lct ris~Acs Cr tul~low, c if)I .11n : 1
f., I! TI-c k r
!.noi . 111), .13/~, (, ) 4
t~olynmcdrlr colls v
tdr
micl.-!i nrlO, thtdir prc:;once cf cc,n-c,,m--,rt. Of 'UhIT
ti:!;Sllf., in th--- of ~y~!rs (r -hn:'uI,.,r cli,~,-cterivtic
f e!,. tur c s
So ti(m 'JI I Vc,-, ,. Yio I-t-

GINTSBURO. I.B,. inshener.
The construction of atpartment houses with SMAll ADartments. Blul.
tekh.inform. 3 no.6:4-8 Je 157. (HLU 10.10)
(Leningrad--Apartment houses)
t
,t~
1",

GINTOlf-Mr, I.B.,in2h.
I I.: ~.
Testing reinforced concrete autoclaves. BiiLl.tekh.iafo.-m. 5
no.P:7-9 F '59. (11,1RA 12: 4)
(Autoclaves--Testinp
("recast concrete constviction)

GINTS~Wj,jj.,.,jzzh.
Using assembly-line ivethod in building apartment houses along the
lanskoya Highway. Siul. takh. inform. po stroi. 5 no.7111-14 JI '59.
(MIRA IWO
kLaningrad-Apextment houses) kAssembly-lins methods)

GINTSBURG, L., doktor ywid.nauk
Vacations for workers and employees. Sots.trud 4 no.12:41-43
D 159. (HIU 13-6)
(Vacations, lbployee)

GTI.-,-, -:-- "
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.1 ( T.)
, ~. A , : ",
. It ~b, ~ ~ -. '. - 11 1 '. wor:-C,,~:y. L;,,, -, ~ .,.. ,, :06~
(~. I,, f . I
-1 !, I'
.f

GIMBURG, L.L.
Inginsering method of calculating automobile brakes. Avt.trakt.
prom. no.10:17-2D 0 154. (MIJU 7:10)
1. ATD-1
(Automobiles-Brakes)

GINTSBUHG, L.L.. aspirant
i~;bility of hydraiaic pover steering Fear, Izvovva.urheb.
2av.; mahinostr. no-7/8:134-144 '58. (HIRA 12:8)
1. ltookovskiy vechernly mashinostroitellnyy instit,it.
(Autono'bilse-Steering gear)

A Tj riiOR: ; I ,
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1,4 ,1C f, i
ula
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C 7;,

Card Llv 1 d I r),-- f it
ra n my r or Fi torriol, :0 r I ow
Ir "Oscow v
:o

GINTSBURG, L. L.
Calculating and selecting paraneters of the hydraulic eervo
system for power steeringt Avtoprom, tio.1:29-32 Ja 160.
(14nLk 13:5)
1. Goniidarstvonnyy soy-usW ordena Trudovogo Krunnogo Znameni
nnuchno-isslodovatel'skiy nytomobill W i avtonotornyy
institut.
(Motor vehicles--Steering gear)

GINTSBR,G L.L.
---- 11~1----.-
Comparative testing of' hydraulic and pneumatic oevomechanisms
for power steering. Avt.prom. no.2:3-5 7 '60. (MIRA 13:5)
1. Gosudaretvannyy ooyuzvy ordena Trudovogo Krasnoro Znameni
naudino-tepledovat9l'sidy avtomobill"yy 4 avtonotornyy Inetitut.
(Automobiles-Steering gear)

GINTSBUR ._Lt,~ q ........
Investigating vibrations of steering vbeels of automobiles caused
by the hydraulic booster of the steering pear. Avt.prom. no.7:
9-14 ii 16o. (MIRA 13:7)
1. Goaudaretyennyy soyusnyy ordena Tridovogo Kruenogo Znameni
nauchno-issledovatel'skiy aytomobilinyy i aytomotornyv inatitut.
. gear--Vibration)
(Au t omob, ile a-Ste a ri np

GINTSBURG,.L.L., Imnd.tekhn.nauk; VENDELIp V.Ye.
Doing the electric moasurement method for the study of steering
gear. Avt. prom. 27 no. 504-27 My I" (MIRA 14.5)
1. Gobudaretvannyy aoyuznyy ordena Trudovogo Krasnogo Znmeni
nauctato-issledovatel'skiy av-tomobillnyy i avtomotornyy institut,
(Autmobiles-Stearing gear) (Electric measurements)

kando takhno nauk
Sbimmy of front wheels of motor vehicles. Avt. prom. 28
no.7%8-12 J1 162. (KIRA 16:6)
1. Goeudaretvanrqy sovuznyy ordana TrudOvORO Krasnogo
Zn&meni nauchno-iseledovatellakly avtomobillnyy i av-tmotorMy
institut. v
(Motor vehicleB-Wheela-Vibration)

GINTSBURG, L.L., kand. tekbn. nauk; SYRYIN, G.A.
Hydraulic pumps of power steering boosters. Avt. prom. 29
no.7:27-30 Tl 163. (MIM 16:8)
1. Gosudarstvennyy soyuznyy ordena Trudovogo Krasnogo Znameni
nau(-ILno-i.qsledovatel-'skiy avt=obillnv
.y i avtomotornyy institut
i Moskovskiy avtozavod imeni LiLliacheva.
(Autoniobiles-Steering genr)

ioA. i-rom. 30
T",,-ntral Iryy ord(ina l:.!-,:C)"",,: o ohnc-
8slpd(-,vli t-t-I lsl~ i.,,, tivto:!.,)I.';. I fiv! A ~-rllyy !n:

GINTSaIMP kand. tekhn. nauk; FITTFRUIN, kand. ~ekhn. nank
Maneurrabillity of motor veh.,:-,rB. Avl.. prow.. 30 no.11-t-24-29
It IC-4 (wru 1822)
1. TSentrallnyy ordena TruJovogo Fzatmcigo Mifint-il ntj-!.),-hnr-
i8nledavatellshiy totomoblllnp 4 art--mctcrr7y

ACC NRi A117004800 SOURCE CODE:. un/o4l3/67/ooo/ooi/oi4o/ul4i
..LAVENTOR: Gintsburg, L. L.; Trikoz, A. A.
iORG: None
ITITLE: -A hydraulic power steering drive with hydraulic feedback for transportation
Yehicles. Class 63, No. 190224
1
!SOURCE: Izobreteniya, promyshlennyye obraztey, tovarnyye znaki, no. 1, 1967,
i140-141
;T,3IIIC TAGS: hydraulic equipment, mechanical power transmission device, drive train
i
IABSTILICT: This Author'n Certificate introducen: 1. A hydraulic po,6er steering drive
!with hydraulic feedback for transportation vehicles. The installation contains a
I
idouble-action master cylinder with two pistons connected by a rod and forming a central
;and two terminal working cavities. The rod connecting the pistons is power-driven I
.from the steering wheel. The unit also incorporates a hydraulic pump, a reservoir for
Ithe working-fluid, a power cylinder with rod connected to the turning mechanism, and
!a dis,;ributor with a cylindrical slide valve. The terminal cavities of the distribu-
itor are connected to the working cavities of the master cylinder. The remaining dis-
itributor cavities are connected by pipelines to the working cavities of the power
,cylinder, to the hydraulic pump and,through a filter.to the reaervoir. The derice
Card 1/3 uDc: 629-113-014-514-522.12

ACC NRt AP70014800
Also contains a hydraulic feedback cylinder with rod connected to the turning recha-
nism and working cavities connected to the terminal cavities of the distributor. To
,achieve correspondence between the positions of the steering wheel and the positions
of the turning mechanism, the central cavity of the manter cylinder is equipped with
,annular projections on the inside encircling the rod with sealing rings on the sides
,facing the inner surfaces of the piston. An opening between these annular projections
;corinects the central cavity to the overflow line. On the other side of each projectiod
,at a distance greater than the length of the piston is an opening connecting the cen-
v
~tral cavity to lines passing through choke valves to the reservoir. The working ca i-,
:ties of the master cylinder are made with bypass channels which connect these cavities
;to the central cavity when the pistons are at their extreme positions. 2. A modillica-
~tion of this drive, in which unilateral ring-shaped sealing sleeves are used on the
pistons in the master cylinder for compensating fluid leakage.
2/3

; ACC NR. AP700h8OO
ii

"=am-"Ponig Tablziffy'A; PASHMWTNIZ. A-To.. professor. otvatetyennyy
radaktor; LUViNA. F-L-, radaktor Isdatel'stva: GUSIVA. I.N..
takhnicheekly redaktor
[Leave for Industrial workers and salaried employees) Trudorye
otpusim rabochikh I alushashchikh. Moskva, Izd-vo A)md.nauk
SSSR, 1957. 129 P. (MLRA 10:7)
(Vacations, 16ployes)

GINTSBURG, M.
Increasing the life of bralce shoes nnd clutch disks. Za rul .
no.6-17 Jo 157. (MLRA 10:7)
(Notoreploo-Maintenanpe and rOPAir)

GINTSBURG, It.
Ins,ving automobile ongine starting in winter. Za rul. 16
no.12:12d D '58. (MIR& 12:1)
(Automobiles--Cold weather operation)

AKIMOVA, I., inzh.',;..U~TSBURGp M., izobretLtelf.
Heat the engine but not the radiator. 7'ekh.mol. 29 no-3:1-1
161. CgL'- 14:3)
(Automobile drivers)

GINTSBURG, M.
Let uq talk aboul. starting. Za rul. 21 no.8218 Ag 163.
(MIRA 16%11)

GIMbUM, M.,
Jelecting P. lubricating oil. Z& rul. 21 no.6t27 Jo 163.
(MA 16:3.1)

~Zbn AnvrastlMig" Ig jbL_X;jvgRheira kZ SM &VA RP41ftimu
,~Lm Praggis of I'lWait"al adencel Mmov
ifol. 45# No. 1p Siq)taibm- 1951, pp. 147
t'rcm Mmthly Ust of Russia Act-centons
P.-c-mber 1931, Val. 4 Moo 9s ps- 33

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A
ii46ur 144
j I OoA6 imdiall (media in which the circular plane of. poU16.
1wr
i% P (ble, obse
T*.! all 3, Aor4 fi~i, 444-455, Jul - Aup; 1954
Ari4, st -s 4t:elodtromaF..;netic waves and propagation in 11gyrotropic
sented- Tb6 prbrAgation of a flat electromagnstic wave is.
:a~,~%,y~-ed il';~ 1 *0 pbysi~',ial meaning of, the results obtained is e An
I)l " an'ihe ~ i%m-'space con nts of electromagnetic wave: (14axw1l's.
1M pro
C*14ion) - ~M those 1.5d an MillAtory coupled system wi h am I I o cillatidne,
(00,,4ulwkj);~s esta6lished. Further, the propaqation of a non-homQ9101MOUB.
ic 'is sttd-,
r n a,: VIAVO guidd filled with a 11gyrotropic
110&1 A d f6m fbir YAxwel-I's equations is derived (fC;r,*a"9YrO-,.
C ii T i; otropic wave-guide excitation is analyrzeds FihA33j'7
t) O'on.of e ctromagnetic wave in a wave-guide with a %Vrotro4d
D" 0 ite). transverse magnetic field is considered, Fifteen ire
S~rd~nces: 7' SSR;
mulish (1885-1954).
Tristit,iition 4*
Su:bmi~ted inril 24,,IM

77 .,.7

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USSR/IPhysics Waveguider, FD-3052
Card 1/1 Pub. 153 - 21/23
Author t Gintsburg, M. A.
Title i;tter to the editor. Anisotropic waveguide
Periodical Zhur. tekh. fiz., 25, February 1955, 356-juj
Abstract 'ae writer considers a waveguide filled with an anj!',otropic me-
dium, the Maxwell equations for the normax waves of such a wave-
guide reducing to equations of the 4th order for one unknown
function, which Is the component E or If. He treat..,j here the
special cat)e of a atedlum with symmetric tunsor.,; ej~. and Inik and
obtains from the Maxwell equations a 4th-order equation in the
E. component of E. He obtains the exoct solution for the rec-
tangular anisotrupic waveguide, and notes that for a different
contour of the cross section one can employ variational methods,
keeping in mind that the above mentioned equation for the nonaal
wtAve Ez.exp[i(kz-wt)] is the Euler-Ostrogradskiy equation for a
certain functional F given. Two references: B. A. Vvedenskiy
and A. G. Arenberg, Radiovolnovody (Radio waveguides], 1946; L. A.
Vaynshteyn, Zhur. tekh. fiz., 23, b46, 1953.
Institution
Submitted April. 29, 1954

f
AUTEIOR: GiTitsburil, 1.1. A. (Moscow) 24-10-17/26
------- - -_
Fracturinj!, racks by means of hit_~h frequency el,-,ctro-
magnetic fields. (Razrusheniye 6ornykh porod
vysohochastotnyini elektromagnitnymi polyaii)
PERIODICAL: IZvestiya Akademii Nauk SSSR, Otdeleni%,e Tekhnicheski1ch
Nau1c, 1957, No.101 PP.93-95 (USSR)
A.BSTRACT: Th,! main reloults described in this paper wero pro-lujitod
a~, L ,;ei~iinary of the Institute of Mining, Ac.Sc., U.S.S.R.
L
(Ijis,ti'LlAt Gorno,,,,,,-o Delo AN SSSR), May 13, '955. In this
paper a new riiethod is described of breaking-- up rocks and
ot"Iner solid bodies by means of non-uxiil'or.~. heatinL inside
a hiL;h frequency ~naGnetic field. The experiments were
carriod oui oil iron ore specimens (iron -quartzites) from
the 1(ursk Matriietir, Anomaly. Their miner'--lobicol
c0..:T)0s"-i0", Wa;i: (Luartz, ma[Lnetite, lienatite aiiiphibole-
c.,nd carbonates. The experimenus comprised tes~s with a
C_ n,
uniform :~iaL;iietic field of H = 100 Oe 40 c.D.s.? usil~,
("AMIltzite specii,.iens wei,~,-Lin[; between 5 and 20 -the
Lime un-IL-J.1 an~,earance of the first fracture was I to 2 mins.
The tests were sto-D-r)ed i,,,hen cracks virent riJit th-rough and
sub-divided the specimen into several parts (after 4 to 8
Card 1/3 11i"O. The averaSe temperature of the heated rock was

24-10-17/26
Fract47ing rocks by means of high frequei-lcy el,-ctromagnetic fiel,--s.
300 to 4-500C and, as a result of 'Uhe hcabin,,-, the rocks
bec,me extremely brittle. Furthermore, experim(.nts were
carried out with the field of a circular turn so that the
maGnetic field was concentrated inside the turn and only
a awall volume of the specimen was heated, whereby the
parameters were as follows: H - 100 to 200 Oe,
f - 240 c.p.s., turn diameter d = 9 cm. The first
friactures appeared after about 35 secs. The duratiou of
crack formation does not depend on the specimen sizol
since the coefficient of heat conductivity of rocks is
very small; however, cracks which start in the heated
volLuae propagate throughout the entire body of the rock
and lead to splitting up of large rock blocks (0.5 to
1 ton) with a small expenditure of energy since the heated
vylume is sinall. For splitting up a specimen of 500 k~,
the calculated power requirement is about 7 k1V and for a
breakinS up time of 12 mins this corresponds to an energy
requirement of 1.5 klVh. Thereby, the power taken up by
the generator from the supply system is about 50 kW ands
therefore, it is necessary to desip a special Generator
for supplyinG current for breaking up ferromagnetic rocks.
Card 2/3 The magnelu,ic method of breaking; tip rocks is also suitable

SOVI/I 6 1~_*7_~1/21,
AUTHOR: Gintsburg, M.A.
TITLE: Surface Waves at the Boundary of a Gyrotropic Mc(,ium
(Povorkhriontnyp) volny Yin ,,rqnits(, girotropnoy s~redy)
PERIODINAL: Naucl,.n.yye doklndy vysshey shkoly,

elektroniRa, 195H, Nr '39-47 (USSR'
p p
ABSTRACT: The author discusnes nurl'llco wavei; lit tho lmurid ill-,
of gyrotropic and isotropic medin. flil, 1,.axwoll equn-
tions show that the waves are propagated only in one
(valve effect) alien both media litive certain
magnitudes of f' and p (electrical and i.%-ignotic perme-
ability). The conditions are presented for the pro-
pagation of direct and inverse waves along the bound-
ary of the division. The results of the investiga-
tion are used for analy.-ing -yrotropic plates, a more
comrlicated independent system. The results of this
paper may Ibe used iisa first approximation for 3olvin.,T
t~l
surface wave prol)lems in the ferrite plate of a wave
,,uj de. The miACnitudes i and obtained frof-,i the
Card 1/3 equation

SOV/162-58-3-6/26
Surface V;avei3 at the Boundary of a Gyrotropic Medium
2 2
PO (U OP0 0 U
may be placed (if the plate is not too close to the
vialls of the iyavmuide) as a first approxiiintion
h=h (0) f A h, e =~ (+4,-' ,Into the transcendental
equation of a wave guide with a thick ferrite plate,
and using Newton's method, correctionsi)h,Z-~,to be
introduced into the walls, may be found. (The magni-
tude u has the physical meaning of a factor for the
delay of the waves by the boundary of the division,
showing how many times the phase speed of a surface
wave is slower than the speed of a plane wave of the
same frequency in a vacuum). Instead of the walls of
a wave guidet one may assume a second ferrite plate
with a field in the opposite phase, as suggested by
B.Z. Katsenelenbaum. For satisfying the boundary
conditions at both metal walls, two infinite rows
Card 2/3 of such plates are required. The author expresses

SOV//I 62 -59- -3-6, `~O'
Surface Waves at the Boundary of a Gyrotropic Medium
his gratitude to B.Z. Katsene1pnbatim forcongidering
the results of this paper. There are 6 graphs, arid
7 references, 3 of which are English an(I 4 Soviet.
JIM;ENTED: Presented At a seminary on radio-spectroa-opy at the
Fizicheskiy institut AN SbR imeni Lebedeva ~Insti-
tute of Physics iment Lebedev, AS UbbR)
SUB1,111TIM: Pebruary 13, 1958
Card 3/3

; I , 1, ": :: ". '. , I I .. i,. ,
.a f. i; -: w.,nv,t, ~n 1 1,(,- !,w.inrlary of i7rotropir melin.
(MIRA 11:9)
~, 17..wn 1. 1 (1 ~lr . ~' I Z. it, nr). (,: V15-1617 jo 1~i3.
tbn,,,rjr)

24(3) 2; ~11 5 , -A , I
111 H OR Girtqburg, W.. A.
TIT LE : The Exchange-Eff acts in Ferromagnetic Resonance (Obirli-nnyye
effektypri ferromai~nitnom reLonanse)
HPIODICAL; Zli-iii-nal eks,erimentallnoy i
Vol ~'), Tir 4, PP '1047-104") OTSSR)
.,',-BSTRACT: Tfie present paper elal~orateu ti unifolm 1~,%v for Vie di:iier:i~on
of transversal electroma(-netic and ijpin w&ves, which taken
both the relativistic and cxchange-intQraction into account.
With a shortening of' the wavelength (on the condition ca- ccnst)
the relative sianificance of the disi,lace:.-.ent currents is 2'e-
duced more and more, but V)e anonnt of tlie forces
increases. Inotead of trannversal electromarnetic waves,
qpin waves are in this case obtiiinr-J. TIte ,iuthor procee-,Io from,
the usual equatior6of motion of ma,-netization:
1.
dhl/dt - y ~(Tfexa')/%) [M611] + [M11]j . flere It ex denotes the
effective field of the exchtinge for-ces, a - the lattice constant,
Ctird 1/A_!.- hi the saturation mngnetizzation, 11 - the ri:~-nctic field

The Exchange-Elfects in Ferromagnetic Resonance '~o*~~V~l",(,-~,.-i"-Atli"J~2
strength of the sample, y - the ratio betwe. n the maimetic
_k qiia moment- y - ".9 iie(-cycl
moment nf the electron anj it N
4
1. + h. 'fere
Oereted. The author 1.ute + i, if - if
notes the internal statistical fiold in the I e, Il' nd Ll
the hirb-frequency components uf the :~Ial'netir field and of
m,gnetlzation respectively. Expreoniong are lt-rivod for the
rooponents of the %enfjor of mgmetic permpW;ili~,v and for the
liaporsion law (i.Q. for the corr-,lation !)etwe4qi 4) tind k).
Thin dinpersion equation has ') ra,!icala corresponding to tile
three branches of dispersion. '7he aforementioned ~Iispersion
equation goes over (if displac;ment currents are nef-,lected)
into the equation of statistical approxiination (i.e. into the
dispersion law of -the spin waves). The chirticter of the dis-
persion curves can be investigated in the best manner for the
special cases 9 . 0 and Q - n/2. For~=Othedispersion equation
has three positive solutions. For 9 = n '/2 2 waves are ossible
one of the type E and one of the tylle II. There tire 'j refer-
ences, 2 of which are Soviet.
Card 2111,

GINTSBURG, M.A. ( ;nslutor)
406M~, - -
r, Thnnry of (i,.ectrn.Wnstic wave propagation in j:3rrcrWnPtlc
media [from "Rev. Mod. Phys.-I 28.3. 1()561. P. 14pstnin. Uaps
fiz. nauk 65 no.2:283-)Il Jo 158. (14IRh 11:9)
(Ferratne) (IRAMO WaVOR) (IpStPin. P.)

GINTSBURG,-,.-kA,_
-- -- --------- ---
Hadar measurements of the thickness of ice layers. Izv.AI
SSSR.Ser.geofts. no.6;872-874 Je 160. (HMA 13:6)
(GlAciological research) (Radar)

36
S/5761/10/ooo/ol?/oo6/oI2
E032/EI14
AUTHOR. Gintsburg, MA.
TITLE: Electric double layer at the surface of' a satellite
SOURCE: Akademiya nauk SSSR,. Institul zemnogo magnetizma,
ionosfery i ras pros t ratten iya radiovoln,, Trudy,
no.17(27). Moscow 196o, Hasprostraneniye radiovoln
i ionosfera, j.87-202.
TEXT, A satellite moving through the ionosphere becomes
e-harged and an eJectric. double layer is formed at its surface.
A knowledge of the propert:Les of this layer is important to the
theory of Lhe interaction of a Batellite with the ionosphere,
since the double layer determines the boundary conditions and has
an effect on the physical processes which occur in the immediate
neighbourhood of the satellite. Three equations are available in
the literature for the description of the electric field in the
double layer. These equations, however, are different and predict
different potential distributions. The aim of the present review
is to examine these differences. The review was completed in
January 1959. The first approach is to use the classical double-
Card 1/ 6

30'?.36-
Elestric double ILlyer At tile siirfa~ S/57o/6o/ooo/ol-//oo6/o12
E032/1' I Ili
layer theory as used in ele--tro--hemistry and the ~A)k-mi.3try c!'
colloids. where charged particles (ions) in the double layer are
In a state of thermodynamir- equilibrium and ar- thi~refore
dasf,rihed by the Maxwell-Holtzmann distrtbut ion
2
mu
F (u x) C_ 5-T ' KY
where: u is the velocity, tv the potential, I? and m the
~~harge and mass of the particles, and t the lemperature,
The present author discusses the one-dimensional :ase only, i.e.
the case where the potential ~p is a fxinct~on of a single
coordinate only, Knowing the distribution function for the ions
and the electrons, one can calculate the field in the double laver
by solving the one-dimensional Poisson equatiow,
E .-Cq)
d2 li-T~' kTj
+ 4,,n,c
dK
Card 2/6

30936
Electric double layer at. the surface , S/57o/6o/ooo/oI7/oo6/oI2
E032/EI14
It is shown that the solution of the Poisson equation for the case
where the distribution given by E(I.(I) holds is
kT- 2 in , Z/2 (I * e- + + e- (9)
-z/2,,
where. I ?V11Rj, Rd is the Debye radius., z = cln,AT,
~o~ is the potential of the satellite, and C is the numerical
value of the electronic charge. The double layer may be divided
into two regions: in the first region E tP I AT ';;, 1, i.e. the
potential energy of an electron or an ion within the layer is
greater than the thermal. energy, while in the second layer
e 191 /kTct I and the potential energy may be looked upon as a
small correction to the thermal energy. In the thermal region
the space-charge consists largely of ions and the electron
concentration falls off exponentially, while in the second region
the space-charge iB made up of ions and electrons, both
concentrations being small. As an example it is estimated that
at 300-400 km from the earthis surface the maximum thickness of a
Card 3/ 6

30936
Electric double layer at the surface ,, S/570/60/000/017/006/012
E032/EI14
double layer is of the order of I cm. on this theory the field
strength at the wall of a satellite increases exponentially (in
absolute magnitude) with the potentiai T,, reaching 47 kV/,,m at
-3 V. It is this property which, together with the
dependence of the capacitance of the double layer on tpc, may be
used to compare the theory with experiment and to select the
correct model for the double layer by independent measurements of
E and T., The second approach is to use the Langmuir-Bohm
equation (Ref..6,,. 1. Langmuir, Phys. Rev., v 34 876, 1929;
Ref.7~ D. Bohm, The characteristics of electrical discharges in
magnetic fields, ed by A. Guthrie and R. Waknrling. McGraw Hill,
N.Y_ 1949, chap,3). Here, as before, the ele-tron distribution
is assumed to be of the Boltzmann type but the ion distribution is
no,~. On this approa.-h the Poisson equation assumes the forms
2 c (T - 'p,
d 4j"tcn C - P --~.
dX2 kT (12)
Card V 6

30936
Electric double layer at the surface- S/570/6o/ooo/ol7/006/012
E032/E114
This equation cannot be integrated and must be solved numerically.
The advantage of Eq.(12) is that in deriving it, it is not
necessary to assume either a perfectly reflecting wall or thermo-
dynamic equilibrium. However, this equation does not take into
account the thermal motion of ions which is, in fact, neglected.
The third approach is due to R. Jastrow and C. Pearse (Ref.2:
J. Geophys., Res., v.62, 413, 1957). Here the Poisson equation
is of the form:
d2y = 43rn (e C(P/kT
dx2
and again, the potential distribution can only be evaluated by
numerical methods. The paper is concluded with a general Vr
discussion of the effect of the magnetic field on the above
phenomena. Acknowledgments are expressed to the workers of
IZMIRAN, G.M. Sonnovskaya and Yu.G. Ishchuk, for assistance.
There are 19 figures and 11 references: 5 Soviet-bloc and 6 non-
Soviet-bloc,, The four most recent English language references
read as followst
Card 5/6

30936
Electric double layer at the surface ... S/570/60/000/017/006/012
E032/Ell4
Ref.2: R. Jastrow, C. Pearse. J. Geophys. Res., v.62, 413, 1957.
Ref,3: E. Verwey, J. Overbec.k. Theory of stability of' lyophobic
colloids, N.Y. - Amsterdam, 1948.
Ref-5: R. Smith-Rose, Proc. IRE, November 1958. VJ/
Ref.7; 0. Bohm,, The charactoristics of electrical discharges in
magnetic fields. ed, by A. Guthrie and R. Wakerling,
McGraw-Hill, N.Y., 1949, chap 3
Card 6/6

30938
S/57o/6o/ooo/ol7/008/0I2
3, E032/E114
AUTHOR: Gintsburg, M.A.
TITLE: Surface waves on the boundary of a plasma in a
magnetic rield
SOURCE: Akademiya nauk SSSR. Institut zemnogo magnetizma,
ionosfery i raslirostraneniye radiovoln. Trudy.
no.17(27). Moscow, 196o. Rasprostraneniye radiovoln 1
ionosfera, 208-215.
TEW This paper was first read at a seminar of the Otdel
dlinnykh radlevoln (Division of Long Radio Waves) of' IZMIRAN in
December 1958,
The problem is formulated as follows. Consider two semi-infinite
media separated by the plane y = 0 (Fig-7). The z-axis is in
the direction of the magnetic field, the halt'-space y > 0 is
occupied by air (co = lio = 1) and the half-space y < 0 is
occupied by plasma. The properties of the plasma are
characterised by the tensor
Card 1/ 7

Surface waves an the boundary of ...
El - ;E2 0
Ic 2 E2 0
0 0 C 3
30938
S/5?0/60/0()0/017/008/012
E032/E114
(1)
When the waves are propagated in the direction perpendicular to the
magnetic field there are two possible types of normal waves, namely
type H (Ez / 0, Hx / 0, H = Hz = 0) and waves of
y / 0. Ex = Ey
the type E (Hz 0, Ex / 0, EY / 0, IIX = 1iyz Ez = 0). Of these,
only the E waves can propagate along the boundary of the plasma.
It is shown that in the plasma
I raHz - ir 8Hz Y2 - rh- (3)
x lk C dy Ak ej
0 L r ax 0
where: k. = w/c is the wave number in vacuum, C2/C11
and (E 2 _C2Vel.
2
Card 2/ 7

30938
S/57o/6o/ooo/ol7/OO8 /012
Surface wavea on the boundary ef ...
E032/Eli4
Fcr Y > 0, 8 H
E 1
-
~ T z
- = - YJ H (4)

x I
R
ay 3 k z
" 0
Using the condition that Ex and Hz must he continuous across
the boundary, one ca ii find the characteristic equation for the
phase veloci.ty of th e surface waves. It is shown that
E IV':2 - I . ArUl - - T-11
E 7
,
where u a h/ko and is the ratio of the phase velocity in vacuum
to the phase velocity in the medium, Four cases then arise:
1) C'~ > 0 r > 0, C, -> I . The condition for the propagation
is then: C.L t. > r > [E.L (~L - 1)] 1/2 (10)
2) > o b,.,,, < j-, r >o. Ifere the condition for the
propagation of the direct wave is:
Card 3/7

3,-,938
Surface waves on the boundary of' S/57o/6o/ooo/ol7/006/0l2
E03'-'/EI14
r I > E 1/2
3) C-L < 0 but ICLI < i, r > o. As before, on3v the direct
wave -i-s'-p-rapagated here and the condition ijq: -4-
1/2 " I (IL))
0 - ci) > > c,,
4)
and th? condition for the reverse wavL- is~
I CJ. , , I > F, (14)
Thus, for sufficiently small r% both waves can propagate but
the4-r phase velo:;ities and the field distribution will be
d.-.fferen-, The second ,aBe considered is that where !11-
Car J 4/ -,7

30938
Surface waves on the boundary of S/57o/6o/ooo/ol7/oo8/ol2
F,032/EI14
boundary y = 0 separates two gyrotropic media (two plasma layers
with different electron concentrations). Medium 1 is described by
the tensor Cik and medium 2 by Zik- The equation corresponding
to Hq.(7) now becomes:
-2-
E u - C + c
L _Lr r (15)
F-I C.L
and the propagation conditions are as follows:
LJ~
1) C.L > 0, > 04
LC, ( C I/ < cj~ c (17)
-&~ CL r c.L _L. C.L
2) C.L > 0, + --0:
III < 0 1~I --
le (C.L 1/2 > ej. C.L + (18)
C-L
Card 5/7

30938
Surface waves on the boundary of S/57o/6o/ooo/ol7/008/0l2
E032/EI14
3) c > 0' < 0' + 0, C, r + r 0
61 ICI C.L CI
LI - -j (direct wave) (19)
c.L C.L 1/2 > C
C ci
an'.
+ (reverse wave). (20)
C-L
C < 0, "C < 0;
(21)
where for r>o the reverse wave is propagated while for o
the direct wave is propagated. The analysis can be extended to a
set of parallel layers. Acknowledgments are expressed to
Ya.L. Allpert for discussing the results,
There are 4 figures and 5 references. 2 Soviet-bloc and 3 non-
Soviet-blo::. (including I Russian translation fron non-Soviet
Publication. The English language references read as follows:
Card 6/1,

30938
Surface waves on the boundary of ... S/57o/60/OOo/017/oo8/ol2
E032/EI14
Ref.4: W. Pfister, J. Ulwick, J. Geophys. Res., v.63, N 2v 301,
1958.
Ref.5: J Jackson, J. Seddon. J. Geophys. Res., v.63, N 1, 197,
1958.
,-t
Card 7/7

S/181/60/002/05/24/041
B02O/BO56
AUTHOR: Ginteburg, M. A.
TITLE: Spin Waves
PERIODICAL: Fizika tverdogo tela, 1960, Vol. 2, No. 5, PP- 913 - 921
TEXT: The present paper was read at the Seainar of the Theoretical
Department of FIAS on January 7, 1959. The basic relation in the theory
of spin waves T'sas known, the dispersion law - the dependence of the
wavelength A on frequency. Hitherto, the theory of spin waves had been
based upon a dispersion law (Refs. 1-3) which is mathematically ex-
pressed by equation (1). On the basis of the statements made in the
paper, the question arises as to the manner in which transition from
spin waves to electromagnetic waves0takes place, as to the nature of
the waves in the transition zone, and as to the part played by aboorp-
tion. Thio question is briefly dealt with by the present paper. In case
A a lose-free ferromWetio is studied. At 0 - 0 the dispersion law
eq ation (2)) takes the form of (4)- With an increase of frequency in
4)u, this equation continuously goes over into equation (1) (see Fig.1 /C
~
Card 1/2

The Theory of Spin Waves 8/181/60/002/05/24/041
B020/BO56
In Fig. 1 the solid curves represent the dispersion law (4) and the
analogous relation for 0 - %/2, whereas the broken curves illustrate
the dispersion law (1). The next paragraph deals with the case of real
ferromagnetics. Fig. 2 shows the curves kl((,)) and k2((.) for both
branches of equations (8) and (9) (solid curves), whereas the broken
curves illustrate the dispersion law (1), where ki is the wave number,,
and the inaginary part k2 is the damping coefficient (k in equation (9)
is complex: k - k1 -1k 2)' A further paragraph deals with the dispersion
law of spin waves for an arbitrary direction of their propagation. The
position of the branches of the dispersion curves for this case is
given in Fig. 3. There are 3 figures and 15 references: 3 Soviet,
2 German, and 10 British.
ASSOCILTION: Institut zennogo magnetizza, ionoafery i rasproatraneniya
radiovoln LN SOSR (Institute for Terrestrial Magnetism,
__the-1onosp 9 d the Propagation of Radio Waves of
the AS USSR)
SUBMITTED: January 10, 1959 V/C
Card 2/2

S/141/60003/coo/oCIG/02.5
9, ?ezll (also 1036,) low) E] 3 3 /1,,- 3 6 1
AUTHOR: Gintsbu. ,
r.5; M. A.
. ...............
TIT L.!,.* Oil tile Possibility of' Lxciting Radio ,iaves by :molar
Corpuscular Streams
1;:,RICJICjXL-: lzvestiya vysshikh uchelmy1di zavcdci!iv,
lladiofizika, 1960, Vol. 3, No. 6, pp. ()U3 - 966
TEXT: A streiam of particles moving in a plasma in tile
dirtction of an external tuagnetic field can radiate
clectroi,nagnetic waves. This can be applied to the case of
ions and electrons from the Sun moving in the ionized atmuspere
of the harth. A Maxwellian velocity distribution is assumed
in the stream (with a small correction due to tilie I.rp-sence of
a field). (All terms in the equations are used to a ~'irst-
oraer approximntiun. ) An expression is then derived for the
effective electrical conductivity . The problem is restricted
to trying to find a value for the wave number whicil will)
correspond to instability of the solar corpuscular streati-, in
the Earth's exosphere - this bein-g the conctitior for radio
waves to be emitted. 1n practice Uis i,.ieans that on.e looks
Card 1/~ -
S

21169
S/141/60/003/006/-OU8/025
On the Possibility of .... E133/E361
for a value of w and k for which the iifaginary part of
the equation;
M2
+ ut h) W(z
k ;.a 1), (1)
I., S,
is negative. The extraordinary wave is considered first
Lmd it is shown that this condition 1.9 fulfill.ed if
U2 + ..,-2 II/W (5)
holds (where u 2 is the ion velocity,
v-, is the phase velocity of!the waves, and
is the Larmor frequency of the ions).
H
The axtraordinary wave is excited by ~he ions and not by the
Card

21169
S/141/60/003/Ouu/006/025
On the PoBsibility of .... E133/E361
electrons. Fig. I shows the dependence of v, (Curve A) and
u2 (Curve B) on frequency. v. has a maximum at 1/2 W
kwhere wif is the Larmor frequency for the electrons).
U2 has a minimum value at W = 2.7 --Z H , at which Point
it is equal. to 2.6 v- (where v. is the plinse velocity
3. A
of hydromagnetic waves). Ion streams with velocities greater
than u 2,iflin therefore excite an extraordinary wave in the
plasma. The electron stream excites waves of opposite
polarization. The dispersion of' these, however, is determined
by the ions. In order to excite the waves it is necessary that
the increment (the imaginary part of the angular frequency)
due to the corpuscular stream should be greater than the
decrement (that is, the damping due to collisions and
cyclotron resonance absorption). The author next considers
typical conditions in the Earth's exosphere, at a distance
of 26 x 103 kin from the centre of the Larth (Ref. 4). It is
Card 3/~( -

21169
s/141/60/003/006/006/025
On the llossibi~'ity of' E133/061
shown that the velocity of solar corpuscular streanis is Last
enough to excite waves. For a stream velocity of
6.5 x 108 cm sec -1 , three ranges of frequency are excited:
- 5 C.P.B., 850 c.p.s. and 7 600 c.p.s. The low-frequency
range is probably connected with micro-pulsations of the
Earth's magnetic field. Assuming an average stream velocity
of 2 x 108 cmsec -1 1 the requirements for instability are
satisfied in the ionosphere jh < 700 km) and in the outer
radiation belt (h ~, 2-5 X 10 km). Observations of low-
frequency radio waves from corpuscular streams by R. Gallet,
R. Helliwell, and G. Ellis (Refs. 6-8) agree well with the
predictions of this paper. Eq. (5) also demonstrates the
predicted correlation between the radio waves and magnetic
activity. The author estimates the amplitude of the excited
geomagnetic pulsations to be about 10 - 100 y
Card 4/,6.,-"

CJ-LV7
b/14 1/60/cIG 3'/uuu/ o(,:6'/o L.'
oil the 1-0.-~.-iibj.-Iity of ....
There are .1 fif,tirc and 11 roferences: 5 ioviut and
u non,scivict.
ASSUCIATION: Institut zewriogo iuagnotizinn, ionosfery i
ru.-i pros trazierdya racliovoln AN S,OSR
(Institute of ;I-Arth N'aunetism, onosphere and
1 .1
1,ropagation of Radio 'daves of the AS U3!~it)
SUMMED: February 1, 196o
Card

20433
S/109/60/005/012/031/035
qq, /yr;, /so -I-, /S3 I E032/E511,
AUTHOR: Gintsburg, M.A.
TITLE: The Dielectric Constant Tensor for a Plasma and a Beam
PERIODICAL:Radiotekhnika i elektronika, 1960, Vol.5, No.12,
pp.2o6O-2o62
TEXT: Shafranov's formula (Ref5.1 and 2) is used to calculate
the components of the dielectric constant of a plasma-beam system
under the following assumptions:
1) the plasma obeys the Maxwellian velocity distribution;
2) a charged particle beam (ions and electrons) is passing through
the plasma. The beam is assumed to be infinite atid the velocity
distribution in it is also Maxwellian and given by
[(Vz - U)2 + v 2 + V21
fo,n(v) = C exp 2 X y
where u is the velocity of the beam and s = ~2xT/m is the
thermal velocity 9f the ions (electrons) in the beam. The external
magnetic field H 0 is assumed to be uniform and such that
Card 1/5

2o433
s/log/60/005/012/031/035
E032/E514
The Dielectric Constant Tensor for a Plasma and a Beam sH
Holl Oz,ujj Ho. The following notation is employedt w * is
H MIJC
the Larmor frequency, w, is the complex frequency of the wave
(W = W1 + iy), Nt is the corcentration of particles of the t -th
type, T& is their kinetic temperature, ut is the vejocity of
the directed motion and k is the wave vector (E,H-e 107r, - WO I
Zf k O,k, The subscripts 1 and 2 refer to electrons
x
and ions in the beam and the subscripts t= 3 and -t= 4 refer to
electrons and ions in the plasma. The plasma frequency is denoted
by Wo 4V e N kxst
MI WH't
-Z2 21 z t2
and W(Z) = e + S e d) is the probability integral.
J-17 0
The functions Fn(x)l �n (h) and fn(k) are defined by Eq.(l) and
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E032/Z514
The Dielectric Constant Tensor for a Plasma and a Beam
using the expansion 00 in conjunction
-:LoL sin in
e We-
n
i with Eq.(5) of Ref.2), the dielectric constant componente are found
to be given by
4D - uk F'(A)
IV R W (2)
XX L-X~-
0) W-Uk
::W ~ ~~* -, W (S"'n
WO
(a-uk
(k) + noq) W
(or -;k-,
W2 w-uk
(k) W
w2 sks
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E032/E514
Tensor for a Plasma and a Beam
The Dielectrie constant
Q)1 to - uk
six W It +
to - RMjj* (7)
uka I + I Y-n -W sil.
OD (D (1)
n sk,
[say
Wr
Uk
VO M, W.001.,
IVI
Uk
Att'a -mald, (v - uk.)
W (2
+ (sk
ried out between
the summation over n
In these forma 4 is
the summation sign over
and +ao and
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E032/E514
The Dielectric Constant Tensor for a Plasma and a Beam
omitted. These formulae hold for a plasma with any number of
beams (all parallel to H 0 ) and can be used to solve various
problems in radio engineering, including numerical calculations on
plasma amplifiers, calculation of the absorption of waves in the
plasma near the gyromagnetic resonance, calculation of the
excitation of waves in the ionosphere by an ion jet and other
problems in which the elementary theory is insufficient and the
thermal motion of the plasma particles must be taken into account.
When T -+ 0, these formulae become identical with the formulae of
the elementary theory (g YZI 9 ZY , Cxz'azx -+ 0, C yy -IN 9xx ), while
when u --~ 0 the formulae become identical with those obtained by
Stepanov and Sitenko (Ref.4). These are 4 Soviet references.
SUBMITTED: June 1, 1960
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5/033/60/037/oo6/005/022
3,17;0 2 6, //,Z E0-52/E.9111
AUTHOR: Gintsburg, M. A.
TITLE; Generation of Plasma Waves by Solar Corpuscular Streams
PERIODICAL: Astronoinicheskiy zhurnal, 1960, V01,37, No.6, pp-979-982
TEXT. It is shoim that solar corpuscular streams should excite
plasma waves in the exosphere and tfie Earth~s ionosphere. A
numerical solution is obtained for the dispersion equation for a
solar corpuscular stream in the Earth's exosphere. It was shown ill
Refs. 2 and 3 that the kinetic equation describing a beam-plasina
system can bo written in the form,.
4
l r I + i fT ZYW (Z I
---ff -2
Z=l atk
w + i Y k Ut, +
where Zt, = Xt + iY
kS,
Z
and W(Z) = e-Z 2( 1 + 21 t"dt)
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E032/E5i4
Generation of Plasma Waves b- S,:7,.ar Corpuscular Sti-f-Ins
.Y
and the remaining symbols are as follolis, Nf, - concentration of
particles of the e-th type, T~' their temperature, 4; - their charge,
S4- thermal velocity, U Velocity of the directed motion, a
Debye radius, -Jj' - effective number of collisions, k - wave number
of excited plasma wave and I = 1, 2~ 3, 11, where these numbers
refer to the electrons and ions in the solar corpuscular stream and
electrons and ions in the plasma through which the stream is
passing, respectively. These equations are solved numerically for
the following numerical parameters4
A: Solar corpuscular stream:
T = 300000K, U2 = 10 8 cm/sec. N., ~ 10 U 1 7 0
B: Exospbere (h 2000 km from thc. Eaj-th s ,;uz tace)
T = 30000K~ N 1000 cm-3
The numerical i-eqults obtai.tied as ave follows
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E032/E514
Generation of Plasma Waves by Solar Corpuscular Streams
(W/k) - 8 6
1 o.9645-10 cin/seci (w/k)") 0 9986-10 cm/sec;
f 315 kc/s; f.. 110 kc/s,
X., 3 m; #\2 9 m (k - wavelength)
Thus, the protons of the solar corpuscular stream can excite
electron plasma waves in the exosphere, the frequency being close
to the proper frequency for electrons in the plasma f --., 300 kc/s.
Measurement of the frequencies of these waves would porovide
information on the parameters and nature of corpuscular streams.
Plasma waves will be propagated only at frequencies close to f 0
Since f 0 is proportional to the concentration N and the
latter increases towards the Earth's surface., it follows that plasma,~
waves which originate at large altitudes cannot penetrate towards
the Earth's surface. However, plasma waves (without a magnetic
field) can become transformed into electromagnetic waves on
scattering and can reach the Earth's surface in this form. it
follows that, in addition to polar auroras and magnettc variations,
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R032/E514
Generation of Plasma Waves by 5-1:ir Corpuscular Streams
solar corpuscularoitreamg shoii1d produce radio noist, in the
frequency range 1 - 10 cps on the Earth's surface. Dowden (Ref 9)
has reported radio noise of exospheric origin on 230 kc/s and the
present author identifies this with the above waves. Owing to the
screening effect of the ionosphere, this noise is best observed
from a rocket or a satellite. Plasma waves can also be excited by
beams under laboratory conditions, In recent years considerable
effort has been devoted to possibilities of ion jet propulsion.
The ion beams producedin these experiments may also generate plasina
waves. A graphical method is described which can be used to
estimate the stability of the ion beam under these conditions.
Acknowledgments are made to N. N, Mayman for valuable advice.
There are 2 figures and 9 references-, 6 Soviet and 3 non-Soviet.
ASSOCIATION'S Institut zemnogo magnetizma, ionosfery i
rasprostraneniya radiovoln Akademii nauk SSSR
(Institute of Terrestrial Magnetism, Ionosphere and
the Propagation of Radio Waves AS, USSR)
SUBMITTED: January 28, 1960
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AUTHOR: Giritsburg, M.A.
30253
S104 6 1 /000i, 0 11/005 /00 15
D239YD303
T].TLE: On a new mechanism for the excitation of micro-)u1sa-
tions in the earth's magnetic field
PEIRIODICAL: Akademiya nauk SSSR. Izvestiya. Seriyu geofiziches-
I
Kaya, no. 11, 1961, 1979-1691
TEXT: The radiation from a single ion in the solar corpuscu-lar
stream (SCS) interacting with tile earth's magnetic 'field is con
sidered. Apart from radio frequencies, solutions are found for 1ow-
frequency mhd-waves in the range 0.1 to 0.001 cls and it is sug-
---,ested that these are components of the earth's short-period va-
riation field. It is shown in the course of the theory that the
ion must be travelling at super-critical speed (i.e. wit, h a vel.o.-
(-Jty i,reater than that of radiation in the plu,
sma) in order to ra-
diate In this mode. The cases are divided into two, aocording as
u, the velocity of the ion, is greater or less than the velocity
v of radiation in the plasma. For the subcritical case, the ex-
Card j//6

On i new mechan'Lom for tee
30283
S/04yor 1/000/0 1 1/005/005
D239 1)303
pression for the Larmor frequency as receivel by an observer fiKed
w. r. ". the plasma, &P , is
(.) I , 11
I- N cos 0
J-12L, t"le frequency of the -Iclii, N is ti,e refra(.tive
-Iiilex of ,.!.,e plasma- arid 0 is the aii6l& betweei-, u !1116 'tile, wave -vec-
ter. Por 'he, super-crit.-IcIll case the mechanism of rudi~iticn mriy
u r I
of either the ~!yclotroia or Chereiikov type. For the
The e(jlX, ticn correspoiid it- to ( 1io
u
c

30283
S/04 9/6 1/000/0 1 1/005/00r;
On a new mechanism for D239/'D'~03
of the anomalous Doppler effect. 'For each ca3e of' interestl now, 'he
1~rocedure is to write -the expression for 14 and by some mlanii:ui-
L-a obt:tin a relation between ~ and u/vA where 7 is 'Iefirle(I byl,)":b,
Q being the symbol for 2W-times the frequency ob6erved. In the simp-
lest case where the ion is travelling down a line of force and cen
siderin:r the wave of in,".6netosonic type this reiat~on ii3 is
VA
The equation whioh has three rDoto given approxim:1tely by 'A""
2 2
(U,/V ) and 1/0t - (u,/v, where 01, ~ m/E
A
E,x-iphed for variou:; ca.,.~es. Insertin, typic.,~il va,!UeS the 1, 0 v
corresponds to a frequency of 0.406 c/s. The (,.aisles where 0 IS fin.'te
and of Cherenkov radiation are also treated in d"tail. The or
rad:i;i-,.dc,n from PrOtO1113 ill the inner radiition belt 'lie
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On it new
3r,2 83
3/1 '04 q `6 1 "000/0 '00",''005
D -5 9N 5 0 !~
i. tu iorl 'o r 0 f t he r E! I U t i V i , t i c Du 1) 1 e r (i Wl 0 li
7 7 -
Cos
c
Ali-ten wvt- 110W Considered . The equit'

P 2
)
T/M
T/M
Q [ c
i

DI Al (if Illasses of '0. SCS -'I";
p .0
T is, the 1,-.netic 1--llE!rgy of the icn. Likel-.-
fot T = ','-,.0 1-1 cV,

'100 Km, F 0. " 7 In tgeclplrly~~ i,. ,l I upperl'i 1 x1-16
- 1 16
t.a,rr3 ,,,

On ~i new Ilechani sm f 3r
30253
6/04'.)/c, " /1000/0 '100'~/00:-
1) -9/ D 5, 0 3
t1le focu."'-'ill'~ affect Or the field Which I--
group-vel-j(.-ity voctor elo~-,er to tile field-11ne dlre~ ti:ln tlim'.'
wave-ve2t,).,,. The attenivition Fand polarization cf' the 1ow--freq',itn.y
~-.uves are nI.,;o disCus,;ed. It is concluded that, 1-1 ion a i * h
subc ri tical vel oi.-i ty trnv ell ing n I oi)g the f i el d -:j mli' I d 1 ~A t
(i.e. there io no incoherent radiation with u '~,)hereril r,:L--.
< vA
diation also disappears. However, tile 1JUSIA1011 i'; radi-~U.l 1~ d I ffe-
reiit for ions travelling witl-.. super-critical jelo~2ities, where bolh
coherent and incol-lerent radiation at very low frequen-les In 1)n
mhd-riode are possible for all directions of the icri re-,~i'-Ive to tile
field. There is a mAthematical appendix. There are I figure, I
11able and 25 references: 15 Soviet-bloc and 8 rlon-SOVi'Ct-bloc. The
4 most recent references to the English-linEu~ige publiofl~-icn'3 read
as follows: M. Sugiura, Phys. Rev. Letters, 6, 255? 19~1; R. 3an-
tirocco. Proc. IRE, 48, 1650, 1960; W. Murcrlay, J. R:)pe, Prcc. IRE,
49, 811, 1961; J. Pope, W. Campbell, J. Geophys, (-:-, 1~60,
ASSOC"IATION. Akademiya nauk SSSR, In.~3titut zemnogo m6netizma,
Card 5/6 lonosYery i rasprostrarjenly-,i riidlovoln (Academy of