SCIENTIFIC ABSTRACT KHALANAY, A. - KHALATNIKOV, I.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000721710012-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 17, 2001
• Sequence Number: 12
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

S/103/63/024/002/001/020
D201/D308
POPOVI V.11. and'~hgjfln"t A. (Bucharest)
TITLE. A problem of the theory of optimum systems with
delay
Avtomatika i telemckhanika, v.' 24, no. 21 19639
133-135
The authors show that, given a system
-:~'w itwx(t) B(t)x(t - -V) + I-I(OuMt x(t) - 4P(01' tg[. too),
and the :CunctionaL
IM (X*(t)F(t)x(t) + x*(t 'r)G(t)x(t le) + u*(t)H(t)u(0) dt,
whose I? G, H arc symnetrical matrices greater than or equal! to zeraq
the optimum control u(t) has the unique solution- u(t)
G ard 1/.?.

AP4033352 S/0103/64/025/003/029010301~
ACCESSION NR:
!Card
AUTHOR: Khalanay, A. (Bucharest)
TITLE: Absolute stability of some nonlinear controlled systems with delays i.1.%
SOURCE: Avtomatika i telemekhanikaj ve 25,.no. 3, 1,964, 290-301
TOPIC TAGS: automatic control, nonlinear auto"tic control, automatic control "I
stabili
,ty
ABSTRACT: W M. Popovto findings in the theory of nonlinear-plant stability
have been successfully used in investigations of sampled-data systems and delay i I
systems. The Popov method p4irmits determining the conditions which-ensure a i
definite asymptotic.behavior of the solutions of nonlinear integral equatiohe: of thin
Jorm:
L
'1/2'
2%

ACCESSION NR.* AP4033352
Seven particular caseji'of the s
a
tability of nonlinear delay. systems. are.tr -ated
mathen-atically on the basis of Popov's method. Orig. art. has: 80 formulas.''

ASSOCIATION: none

. '1-
SUBbUTTED: 24Apr6S'.::- -DATE ACQ: 1 SMaj64 ENCL: 00
.
P IE

SUB CODE:
OTHER: 00
NO REF SOV

Q. T
lil~qR- Vlhuv,-`~~-,*.~.,~,~ ~i
. ...... ...

RON

KHALARAY, 1).S.
Device for unloading pipag Of large diameter. Rate. J isobr. predl.
v strol. no.89:10.11 054* WMA 9:6)
(PiPe-42ranaportatloz) (Loading &M unloading)

THALAMAT, D.S.
4 ~, -
Device with self-wedging clamps for moving steel sheet$
Rate. i Izobr. predl.v stroi. no.09:14-15 154.(MIU 9:9)
(Conveying machinery)

DUBROVIN, Ye.; KARMALISKIY, 0.; FILATOV, G.; LOKOTKOV, A.; LEBEDINSKIY, A..;
BARANOV, I.; MSEVICH, P.; BABENKO, Ye,; GOLITSYN, A. (Ozery, floskovskoy
obl.); SHCHEPOTIN, 1. (Oz6ry, Moskovskoy obl.); XHALA~GOT, A. (Snezhnoye,
donetskoy obl.); KUZIMICWNZ~ N. (Snozhnoya, Donetskoy--~bi-)~ SIPITSA, A.
P
inzh. po ratsionalizatsii
This is the way we live. Izobr. i rats. no.lOr4-5, 23 163.
(MIRA 17:2)
1. Ghlen seveta obs4abastvennogo konstruktorskogo byuro zavoda im. V.I.
Lenina (for Karmallskiy). 2. Predsedatell Amurskogo oblastnogo Eoveta
Vses6yuznogo obshchestva izobretateley i ratsionalizatorov (for Filatov).
3. Predsedatell Chelyabinskogo promyshlennogo oblastnogo soveta Vsesoyuz-
nogo obshchestva izobretateley i ratsionalizatoftv (for Lokotkov). 4o
Starshiy Odeaskogo zB#oda imeni Dzerzhinskogo (for Letedinskiy).
5. PredseloPeltzavodskogo soveta Vsespyuznogo obshchestva izobretateley
i ratsionalizatorov (for Baranov). 6. Predsedatell soveta Vsesoyuznogo
obshchestva izobretateley i ratsionalizatorov Irkutskogo z oda tyazhelogo
mashinostroyaniya imeni Kuvbysheva (for Mitgevich). I

S/122/62/000/002/003/007
D262/D301
AUTHOR. Khalangotq D.V., Engineer
TITLE. Selection of basic parameters for pneumatic plunger vibrato!N
PERIODICAL. Vestnik mashinostroyeniya, no. 2, 1962, 43-44
TEXT3 The author attempts to find a general relationbetween air pressure
in the pneumatic supply line, average vibration frequency, diameter,
strokag and weight of the plunger. The effective energy of compressed air
in thecylinder of a two-way vibrator is given by Eq.(3)
_ 2
E 092p ZM- S Kgcm (3) (D P and SP - plunger dia and travel
respeztively, P - mean effective pressure; the author states that it was
found from expefimentaL data that P e=O.1 Ps I PH being the supply line
pressure. This equation is equivalent to Eq.(4)
Card 1/2
m U 2
-P---2 Kgcm (4).
e 2

S/122/62/000/002/003/007
Selection of basic D262/D301
G
_R_ q - mass of plunger, V - mean plunger -velocity). The final
resull in given by Eq.(6) 77 p 1)2p = G S n 2 (6), and if the hottsing
a p *P P
of the vibrator is movable the final equation will be Eq.(13)
';I'D2 2G S2n2 (
G
(),2 p + S 1 + D ) (13), In - number of
8 4 p h Gh p
double strokes of the plunger; Gh and Sh are plunger housing weight and
travel respectively). Comparison of tho theoretical and experimental
results has shown that the error does not exceed 15%~, There are 2 Soviet-,
bloc references.
Card 2/2

KU1A-TWTy (;.V. , gornyy insh.
Using movable battery stuils in inclined seams. Ugolf Ukr,
4 no.8M-hl Ag 160. (MIRA 13:9)
(Mine timbering)

KULANGOT, G.V.1 kand.f.ekhn.nauk
fho mothods of roof control in inclined seami. U9011 39
no.2:15-18 F 164- (MIRA 17:3)
1. Donetskiy nauchno-isslodovatal'skiy ugollnyy institut.

.KHA.LANGOT -QS--#-Inzh.
Safety measures in roof control In walls of slope beds. Bezop.truda
v prom. 5 no.3:3-4 Mr 161. (MIRA 140)
1. Donetskly nauchno-iseledovatellskiy ugolthyy institut.
(Mine roof bolting~~fety measures)

KOSHKINAV T.V.; KHALANSKIY, A.S.
Burrows and refuges of the Norwegian lemming (Lemmus lemmus).
Biul. MOIP. Otd. biol. 68 no.lsl6-2.4 ,Ja-F 163. (MIRA 17:4)
~-S4,7D'Ii,'~, WIN

KOSIMINAl T.V.; KHALAWKIYj
Mass multiplication of NoAtOgian lemmings in the southGrn part of
the Kola Peninsula# Biul, MOIP, Otd, biol, 65 no. 4:112-114
J1-Ag 160. (KOIA PMNSULA-LE-14INGS) (MIRA 13:10)
F i V' -

KOSHKINA, T.V.; MULANSKIY, A.S.
Age-related variationa in the skull and an analysis of the age
composition of populations of the Nox%regian lemming (feimas lemmus).
Biul. MOM Otd. biol.-66 no.2:3-14 Mr-AP I MRA 14:6)
(KOLA PFNINSULL-IEMNGS) NBU)

KOSHKINAP T,V,;-_KMANSIIY, A.S.
Reproduction of*the lemming Lemmus lemmus L. on the Kola Peninsula.
Zool. zhur. 41 no.4:604-615 Ap 162. (MRA 15W
1. Natural Reserve of Kandalaksha.
(Kola Peninsula-Lemmings)

i" (0)
5 T119 3 - 5 8 - 97
AUTHOR:
effekti,in,~m" p='d--rzh--inlya n~--L
FERIODICAL: Neftya:.-,cyf.% k:,.,,)zyi9.yN-,~-,va.. -1958.9~'&Nr 9, pn -"'C-1.3 170SR)
ABSITRACT: The with V.-S. K7:.:--,hk--) [Re-f con:~Rrning
thg~ of pr-w~r,',;.re at ths
Akhty--sko-P.~.,.g",r;,Iy.-cakiy Oilftelft. Data obtallned by the
Krasnolllar Depar.-Ment of the VIC-LI-neft' show that
the 7.8.7. million xr4ble Ity th~- PFD - t a rilch
Podderzhmili-ya. p.-.art~)-,rogn,
Se-atlon) fx,~,-m Z953 through 2.956, -xiz: "k-jr fo~.,
by :~960. the authox, that C9
aohieve,,3 pxdw~ to 1960 if thB 2-7 vAll -I--'- o--, 40
per-en'"of thfi expe*.me3 with viln-1zh the Prli!~Su'ra Mal-ntenance
sec,,ion was ihar&~d by thp, Ab-",--neftl INPU were
C ard 1/2 ex,,,--,.udrd fv~j "h-.1 Has rol--

11(0)
E3onomic Gain fpm
Li chz gF,-' fra, thin-, gU3
we---.'-z wrlll", Bt th~~ tamp, of T-.,.,ansfar
pz,a -S.'n Fi%oill ,.i poor td;dt-e (R!lf"31 'a-ha'; 4-IA-&,-Iy
o
ly 60,000 t-ln-~n of g -as
n urn, whian
1. n "j'!. W6,2J..", they ra-!.a2. ',,h,-, Ut '-f ~ia
--y m*.',:*.".., t*-'.D.'-' 285POOO 4*'--'-'
41.4:; fncx 2... lfe:~ a',~,,o Points
by r:-,wp*-.-,-y.-.ng AYaP gmpn'.. E-nd OthRr
of fo the
Th that. i~; i"I vn:'y
f:v3M P::-
ly zdna= In
kray wi:~ --y k:'.Fp e.7--.d cc~ P.:- maiz.. 9z ans,
r
C and 2/2

KHAWOV, G.A.
Method for calculatixg the cost of water or gas injection for
the Akhtyrokoye-Sugundyr field. Trudy XY YNII no.2:151-160
'59. (MIRA 13:11)
(Akhtyrokoye-Bugund.vr region--Oil field flooding--Costs)

KHALAPOV.- G.A
Method of calculating economic indices. Trudy Kr- VNII no.7:
109-131 161. (MIRA .14:12)
(Oil fields-Production nethods)

MAIAPOV, G.A.
Technical and-economic analyois of the development of
Akhtyrskoye-Bugundyr typo oil pools. Trudy KF VIIII no.7,.132-138
161. (MIRA 14:12)
(Akhtyrakoye-Bugundyr region-011 fields-Production methods)

GUSZYNOTP R.N., doteent; KHAIAPOVA, A.Kh.; BAGIRBEKOVA, L.K.
"on
Result of examining women cotton workers in rural areas of Azerbai-
jan. Akush.i gin. no.2123-25 no.2:23-25 Kr-Ap 155- (HLM 817)
1. Iz Azerbaydzhanskogo nauchno-iseledovateltakogo institute. okhra-
ny materinstva I cletstva (dir. I.Ta.ParaAm-heva).
(IIMUSTRY AND OCCUPATIONS,
gyn. exam. of cotton workers)
(GYNECOLOGY,
g3rn. exam. of cotton workers)

4 a 0 9 C a 0 9 4 0 a at - a -7
. W-gjo-
WJW-Wg-W-411 "IMP so **Goes 69000*0 -
11 Is 11 1 a it a a a a is 0 X-X A 31 9 9JA A Is
I V 9 H 0 41 #2 U 0 GCO,
f I VA-A MAX W... I-k-l A-1A a
A a L 4 -A. L a V P a I- I-L. kA h A ~-,* 0 1 1 --1i6 0

viev"Ift de ""m Is Ad me
==Idt! V. S.
too" dwreft ad the addidmrr. 0 0

--2
-d
l
kh
S
im. te
.
mspro
Vemehn-drit. IsdeAmeadya Amike-Ki

' IMS, of the MaWijinS actim of
h
h
h

off
.
rn t
e
at w
s muspe"ov* OKmrd t
af)" an -T-Sp" -.-
.-W y dit*ced by pure water
so Y vm%b6j UK PSOME) a stahwation Mal. Was ab-
f di
"
d
hi
h
imu
egrw o
spr
e
Upon turther was
ng t
I so
oedastheresuftolautocoegulation. Thecourwof
I-es
this vwwgmtjyimrelstioototheubcouttnt
i
h
t
mW condition of o"flom of the v1phite Oreatment w see

l nfoW. 1U 10 - ad VmpWw sampesudommI by
=00
06 al ou" of took Is bacread"ceacesaration. StsbWastion
V
b
d
F
h
i
d

otj! .
u
am,
.
e
r
eftem
loodmoze =d Ow mwftd of It
-'
-
'
r. * 0
-
hK"
Khalmdubel9l-101.-AtntLhod for the quant.
, o0
004 d6persion of graphite xu%pmqioas is de.
a c
scribed. which was used todes. the effect of the conm of the
subUiscr - - Owdistributimmolperticle du in the muspen.
0011 sion. Investigadmof the effectof tannin cown. on the pro-
doz tective wOm Is a b% VaWte sospension In (H N N&OH
soln, mbmd tMt increasing the tsaWn ca". from 0 to
66 b
ldi
i
h
d
A
g .
e mo
sta
tat
pro
m, t
0.07% rawlted is a mad
00 # able pwtkk " %BWX from 75 to 37j. in diam. Fur.
-
'90
1 ther adda. of W-J" (to 01%).incrramed the stabitity
dd
,1 n.
only &Ugbdy. drereadng particir an to 20-30 m. A
40 or the protecdve coUaid beyovid this coarn. gradusHy
produced a sensitization. the part1cle s6v hwes-ing frmn

ASN-SLA
& Is UNWAL LITINATWI CLASSOKATION
Lt
94 It
40 t!
a.. 4.!-, 1
43&L110.1 ot,w ewt a.,2t.
'I

U v '0
"
o Or It Rd its welm it v
n An A a 0d 0 4 1 1 IN DO 9 A a
0 1 !Z4
0
so 0 *see
0.0 0 0 0 eme of tv n t
a 000 0 a so as 400
Go* 0 0 0 00 0 0 00 0 : V 0 Wa 0 0 9 6 a 0 0 0 0 4 a 000 0 0 0
.6
0 *10 0 0 6 * 0 S * 9 0 * S 0 0 * 0 re 0
ISO*
ties
life*
gas

4! 0 0 0 0 6 9 0 410 6 6 6 6 0 ag 4 4 6 a 4 _. a e e 9 a ~ a a
40 a 9 0 V & 6 9 0 0 0

00
211 to 311 P. 11CAM84" gidgect of koala tga so
so
go at a" Idaft of V609" at didwast ft Values of the
&_
41
i
O
S
b
f
N
N
o
04 M.
-Srr
6PIn
M MW
.
vr
Y
.
a, Ibid. g
Id.-TIN alklillizabillty of NMM and Alifficrogir graphitt mg.
00
0 Pemkm in Un clidised and 2MMakfited conditirgas was

90 deld. bY Mediniggiatometric Mittliods Loth in the stwom 80
ni tanwo And at c . tingengin comm. (025 1QZO%r) end
00
at vorlow N&OII Cnick-us. of Lite distict" mr,lium (hun;
10-1 to 10-6 M. 11% tM ""me cif UNWO OW littat"t
degree of disiperelon was rndwd at a X&OH conen. W
10-4N. In tbecomeol oxidized (with chromic ")Kure
creighits. coodAegrably treater stability (ur degree of dis. 00
Pirridoll) WU observed during washing; Men during We
-
(
ddi
71
9
00
ff
rose ploct I o
a
*
1. In the CoAc of towited
8g
Aliberviv VVWW coodidusas were oppositgg the dispeggLion so
twins grotti du~~ .4 Naull than at range.
=
of
00 'ponding ta ,ug out of the alitak A

99 "sdistiri.
SZ
_
observed with the nocioligligged
r
X 00

09 jrrvphitr.
veove
watig s
ab
Uiutl= of gmpMe imispeadou in
di
orition media
drowli
nes) b
War
b 0 41
00 g
i
i
v
y
y p
substances. H. 9. Ven%tlum and E. At. Srettva. ibid.
7 00

00 I 1
s -W.-The degree of cliqgersion of vagrisp" graphite stis-
i
b
i
li
id
C
W C
1
h
H
i of

00 ons
sir
pen
n nonpu
4 mints. w
s (
a &
t
qu
4
J
dAber hydirorgurbons) was investigated in the prveram td so
vsrious PoW. surism-activr stelgilliarfs (fatty s6dj, sks.. 00
00 auggines.plicauls). IncontrzAtti~dwiribehavkwinaq.suln

00 pensioul, BU thew . p =-~ctivvpub%t&nmsctvda- 09
ittabWsomsin ftwh .."' wdis. Ttigutw'. r.1, 00
09 is useful in predic x the staNhit"S ;x'wer of the cumpis.
410 * 0
so 00
00 of
so 00

0 41 0 0 9 0 0 0 0 e 9 40 0 0 0 0 0 0 0 0 0 a 0 1111 0 0 0 0 0 0 0 o 0 0 9 0 0 0 0 0 1111, 0
0 0 0 0 a 0 0 a 0 0 0 0 0 0 0 0 0 0 0 is 0 0 0 0 Is a 0

0 0 0 0 0 0 * 0
MA)SOXIO all Ain ma bit upit .1 ir ii a a
A -A-J A A L 11- 1 A-V I-LU A-k AA IN QC 0 It ;.I
Liu
V. A. it %I N. N. 'wi 1:11 43.
i I -
CAM. lemy. Im. it, um U. kil
go
Seri for Ow StAtmilldttf OffickarY was inves0satcd
o with t'W =OPmk e%sf"Pk lot &its- ln I'vd, N-ificaliy, th,
g: tin the. rillillailwatum, xSe
W CsIts 604 Its in ail. u4nu.) In I, t4ligin W 11W tn. the 9W.
fWT WtiVitY Cd tht SUAMin 00 111C OqUld IAKAlUlA7ZII:r
(WOUl-boramm). UK adpwrlim sm vaphite Coo
*An#.. In which sata. Is reached at very km (vum., slid coo
of StAbilialioda actioa of allwits ted gTa hite -414-
p
we" Invelligatcd. 141~ or.. MO."
*0 S
ti
wool
go
Joe
It
1 a 'N I do a 1 0 0 qx~
0 dA4
e
10!
0 0 go 0 0 0 00 so

0 6 4:4 4114 4
* 1 4 a 4 Q 4 0

I 6 Ic 4 is is it is AD 41 J2 J3 A is )a v 11 Ll Is
L a -" I P a a I I T I -A, I A 464 so 11 a W 0 p 0 0 f .6

j.D*%nWM*& hat"lls of War fotd wet.,

00
I'tv*- of I. .04
06 A. A. ll-whihngk

41
0 0
00 SOO
"fe
00
so
Asa It a OlAtibrOLAt tiffWal"I CLASSIVICAM" '00
0 0 77-
I AA I I V N 0 - - N '1 81 13 1 S 9
70 -4 t010 -964 On IRS "Ittv if M'.iln I I
0l " a - - q r . 1 4 6 a 4 a ' a ..... 0 ~"0 0 0 0 0 0 0 0 9 0 a 0 0 0 0

0 0 0 a a 0 0
w
q it 4 it 16 It 4 It 23 N a is v a 10 ~a if v u 10 0 ft u st a a 41 .1 a a r

I AA 08 (A PP Elie I I A k -

hos
te In the twilpt
the (cell
f the
D
t
l
ti
n
h
:
erm
na
o
o
a
e
,
p
p
0
water and the uAl*. V. V, Kh.461,-m, L. A. 11rimsilim
14"d 1. "". Comrov. lm~:
0
1,11w) i934, No. Z, A crit. tevww -4
A A. 1L.Ild...

00
00
so
so
'00

as*
see
@t
zoo
010
too. 00
00 '00
of,

e0
A I �,SL A SIVALLUPWAL LITINAIL-01 CIASUFKATICO cz Cl
90 tV to
It
,
It v 11 0 1 w
o
; 0 v
t
at 0
i
0 n I %a afto

rWwl
ir i. . . . 4 . . .
6 4 4 6 0 4 6 4
6 4 4
V A 4; 4~ 0

A z
00 *
L I V T 4A N W (f j f
r
f
-

'Me problem d a deal mdtlklilld Of Water W'th We-
* so
00 j ep4oUAk. lad.
n"ta. E %, Khlkla inji. Ismiliyu J
-
*-tj~--3r-V:-2Tri- rdame with elpts. de-
VOW
,u
.
wfilvd. it. is stated that finmd uJimling of w&ttr with
i
h
00 t
ph'Aphatc is in(xv expen,ive and Ic- cly-tive than w
NwIlthusk
A
A 0
00 .
.
00

00 roe
coo
so
00

so*

96

90 f

too
'
.1
Iwo ft
0 0 0 0
a
o 0 0 0 o 0 a

If :1 8 Ain NOXNAPAI UJIMMIJOW xxv I
AS IL A -1-3 a m 0 UfJL-I. I --- L_j_-L_ A__A__ A- J.-
Oil A." 1-41 4.000%
At
611110
04111 j
'fathoile for MO AUt*Mft (101nni"dOM 0( &MAIJALity -00
44 and hardnese of 'Water-vapor Condensate H. V. Khalap.
-,Init L E Sto-his and A. 4'. Manitt, '00
00 a 7 details are jivv:'bv #?w p,F"lw ~41110
and rontinuinji; sulmnatic detnR. tit alky. 4\'AIIC(ht anj
06 hi'll'iess 1C4) 4 tap, tx)ikr feed and Ax-m4matc wiler, .00
baw,l on ripil, rerberking of known prmtdorrs. %1A%.
0 alky, of 0.5 * It can be drid, at It) 19" with Aluarin rrd At
0 indivator M ml. fq 1% in I(X) ml. ( the gain.) if) file pholip-
vlev. culorivot(tr. The Leituan method it t,y
4114 .3 Milmlavqkil and Vavilova (C. A 31, 4111411 gives hightv
a" firste results In the periodic P~utoncphrkmtteffsc tk-tn'
-I hardneu. but emiumes considerabje little (50 M min. 1 000
j. and large amts. of the reagrnt. The Winkler reactut jK
oleale) can be used for the rmlinums suirmnsisc kin. 2*0
oil of hardrim, Wcause of the high dispersion and stability of 0101111
a lite furboty. but is not %uhril bw Iow C2 nmCni" %ince
in Wife amm it Oves rolvoi-rd .411%, I'liv app. of-, fflu,- Soo
teaft,tt and cirwitted. Chkc Bulk !coo
Ott
sITALLUMICKAL goo
a D a v
--.7- -1~- ~qq ~~Cr `1 9 3 T Aft A 1 4 Od 0 0 0 1 Ir 0 11 A
C ; , ZA
U 9 AV Q 11 It 19 It MW a NA
14 0 00 0 00 0 4P 0 '0 0 0 4 00 0 0 a 0 0 * a 00 0 0 0
eo * 0 0 0 *, 00 0 0 0 0 0 0 0 0 00 0 0 00 0 00 0
00 0 0 0 0, 0 0 40 0 0 49 S 0 0 0

i(PAUPMUL. -M V. A
Food Water Purification
Bubbling in deaerators of feed water.
Elek. Stn., 23, No. 4, 1952.
Inzh. Teklmichaskoye Upravleniye MES
Monthl- List of Russian Accessions, Library of Congress, August, 1952. THICLASSIFIED.

1. XOTt A.A.; KOMAR, R.V., ENG.; MiALAPSINA, YEN., ENG.
2. USSR (600)
4- Steam Turbines
7. Preventing the clogging of turbines with salts. Elek.sta. 23 no.9, 1952.
9. Monthly List of Russian Accessions, Library of Congress, January .1953. Unclassified.
a p~e ~5
ri Av, R
M-
M

KHALAPSINA, Ye.V., inshener.
Aiding the student of the now .*%lee of technical operation of electric
power stations and networks." Chapter 16. Water regimen and chemical
control of electric power plants. Bnergetik 2 no-5:32-36 Ny 154.
(KIBA 7:6)
(Electric power stations)
-

, 0
0 0 0 0 0 4 0 00 0 4
0 00

a .1 41 #1
8
N Ik' Li
I I #
0 1 to it it %4 1' A PA N N it I
k
f 111 In J:
A
4
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f
P!9166 7-~O 0
;
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0:
00
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00 .00

0 Oxidation in the
1upid dotIMID11094 old A SWIT
I O"throquilla"t.
.1 I-
-11
01
ti

00 W
ou
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produt
S. 117,01011
C
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110v&. III ill .
1 4.11 tile! 1111C1111"tum
t" I flit
i

09 .3 f,111
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.
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tie 41
go.
A 1 0 - I L Sfl&LLUOGK&L LIT110141"I CLAWFKATION Ir V,
We
u Ts kv K) Is -w
cl it of Kw AA A
o o o 0 0 0 0 0 0 4 4 0 0 0 0
Z440 0 0 0 0 o q o : 0 of lop Os of 0!0 0 0 9 0 0 000 99009

KHAIASI 0. (Budapeaht)
Limit equilibrium of reinforced concrete plates. Izv.AN SSSR Otd.
takh.nauk no.8:42-54 Ag 156. (MLRA 9:9)
(Blastic plates and shells) (Concrete slabs)

Z.
Profnssionnl Schoolinr im tho Textile Tr!ido In l'unF-,nn,. Lokn
Prom-shlenost (Lipht Industry), 1';'2:h2: Feb 55
OJ C~l ,A~ kip
N
P

GALAII I N , K. Y . ; A arti. tekhn. naak; 31VIVAI I ~, , 1~ T. ;- I 11"UN , Y-a. A.;
?~HAL;-3fl, it. red .
-.1-- v
vu.'t-4rig onad'ItIons alld tile rcium(Ary if disr,
t,-,,j ~If x~one(,ui.~Jng mazhines] (jptAv,.,,]'rqje renimy n--anila
I gf,,cmeti 1-1a reztcrv diskov urmneri 7.7.ykh mashin. E 1:. 1, t n!tv ,
- I
KfirGia rr:..-id,)vF.-nInAe., 196", 103 P. (1.,,II;A 28:9)

jo -MiALATIAN x Ot 110
2, USSR (600)
4. Runoff
7. Some problems in organizing and increasing the accuracy of water supply work.
Izv. AN SSSR. Otd. tekb. nauk. No. 8s 1952.
9. Monthly List of Russian Accessions, Library of Congress, January -1953. Unclassified.

SIDDRENKO, M. V.; ALEKSANDROV, A. V.; KHALATIN, N. L
00peration of the largest system of gas supply and its work
during peak load periods (on the example of Moscow system of
gas mains).*
He rt t be submitted at the 9th Intl, Gas Conference Hague,
1-rSept01964.

[dplqeasedj
Mineralogy and geochemistry of the terrigenous formation of the
Lower Garboniferous in the southern part of the Kama-Kinell
Depression. Sov. geol- 4 no.8:127-137 Ag 161. (MIRA 16:7)
L Moskovskiy gosudarstvennyy universitet imeni Lomonosova*
(Kom Valley--Geology,, Stratigraphic)
(Kinall Valley-Geology, Stratigraphic)

; KHALATIII S A red SVETLA
PETRGV., Mikhail Filippovich .$ y 'YEVA, A.S., red.
izd-vaj LOBANKOVAp ReYe., tekhn, re .
[Cedar forests and their utilization] Kedrovye less i ikh ispoll-
zovanie. Moskva) Goslesbumizdat, 1961. 129 p. (MIRA 14:9)
(Forest products) (Cedar)

BARMN. B.F.; KOIMUSIMV, V.A. I ~MLATINLIAILM"
Outting in on a gas line with the use of rubber balls. Gas.
promo 4 no.7s49-50 JI 159. (laU. IWO)
(Gao, Natural-Piplines)

BARMIN, S.F.; KOIMASHIV. V.A.; KHALATIN, V.I.
Emergency repair service of gas pipelines. Gaz. prom. 4 no.12:41-42
D 159. (MIRA 13:3)
(Gas pipes--Maintenance and repair)

irl~~,~,~,,~*14"~~r~lill~;-~Z-'. Wv~, 11 4~* t~,.,. ~, -
I
ICH&UTIVO Vejeo JONDRASHIVI TOAS, WMIN, S.y.0 MAGAWIX, Tas Me
Gaz.prome 5 no.2:40-41 Y 160.
interconnecting gas mains*
(oas, Natural--Pipelines)

311DOREINKOP M.V.; KHALATIN, V.I.
Underground sUnrago Of gas for Mc'5vvw- Gaz.pronl. 10 no-3:47-12
165,, (,M I RA 18: 5)

BARMIN, S.F.; KONDRASHIV, V.A.; KHAIATIN, V.I.
Ball cocks on main pipelines. Gaa.prom. 5 no.9:43-43 S 160.
(MIRA 13:9)
(Gas, Natural--Pipelines)

SIDOMKO., M. V-j ALEKSANDROVj A. V.; XMIAM., V. 1.
*Operation of t1i largest gas supply system and its functioning
under peak loads."*
Report to be presented at the 9th Intl. Gas Conferencep The Hapey
1-4 Sep 1964.
R

Sjy.ji~E`Ko, t-I.V.; A11,KSANDROV, J...V.; MHAIATIN, V.1.
Operating a large gas-qupplY SY3t8m- flaz- prom. 9 nc).8:5-.10 164-
(MIRA 17:9)

KRAL.kTIN, Y.N. [deceased)
Characteristics of facies of the lower Ourboniferous formation
in western Kinell-Cherkassy District of the trans-Volga portion
in KtWbyahev Province, Trudy, Inst. geol. i razrab. gor. Iskop.
1:226-239 16o. (MIRA 14:1)
(Kinell-Cherkazzy District--Goal geology)

A
004
Sol
fat
too
40
0
l=Uad to dwkk 4060ft of d
am,
O,:lzkw.,x Tww. Fig. Hirp
7- IM).-Ths tb-7
,g, m
tztamkd to the oaustatim-y probkm
dww*u wkh eqma mobUkko of Ow two kal.
lo WMCII VIA czta~wl cW. idd b *qptkd st tk* mommt
0. 1% Vdaft of dm joa Is a I I of 3 a4dki-
dtw to dw mumd &M the imk AM
dkM TIN, Isw ~l luktim -4 ti~
Ckc. 0004L A~EMEA I is tompla: In tU MmIdixg - of
wftk extend A deccemas NrM I to k$ s"WeArY
N. Thm
'041
0
11"m tl"vslww NNW ra"iftv
r*
600
" 0
'too
we*
goit
ves
b u a &v so ;c TIC01 slaw 0 a 0 1 v a 0 a a

ATUZ TUSORY OF Tog VISCOffiTy or HSLJUM
2. CALCULATION Of THIC Vp.~WITY COEFFICIEHT-
j&2.1&nd6 and L ~&~~Trjinjqjated from
109-26(1949). 33p.
ftspil'
I To-orst. Fit. LO,
Zhur.
The kinttie equAttuns (or rotons and phononS Its solved
fS 9 by using effective differential cross sections for the
scattering of elementary excitations (phonons and rotons)
by each other, as obtained in the first pzrt of this worit. It
Is shown that the visew-fty coefficient of He 11 to composed
of two.parts: one caused by scattering of rotone ('roton
adscoally") and not dependent on temperature; the other
caused by scattering of phonons ('phonon viscosity") and
sharply increasing with fall in temperature. The expert.
mental values for the viscosity coefficient In He 11 appear
to be bt good agreement with theory. (auth)
%X Town OF TUB VISCUM Oy FXIjVM $L
L Q2w" OIF 41jAWNWART ~A "^i
asum 11,- and L Trans-
tMed trim thur. Eksptl' I Tooret. Fit. 19, 637.50(1940).
A 6*ory dsocriblog tile viscosity characteristics of He U
to Oessated. This P -tion deals principally with later.
0064111 An4f Wilation considerations hued wt phonon and
AMP-

_V-
iiJL~ -

O-d~
ex
"em
. ry'. slqp'~-
34. jW;Z TWd. II
V, hIms r. cilow Of OW
I ot It C"
" vima
1. M. ~bzls=v.
lllwl~--' -~Iut A
.11~ .110
1 .
1
a M"'!-
= ",u,.
x wbk~
fit It 1,
,her JhAll

USBRINUCIew Pbysics, - Dirac t a 51
Equation
'Radiational Corz ctions Added to: Dirac's FAIua-
tion (in Novrelativistic Approximation')" A. Ale.
Abrikosov, 1. X. Khaltnikov, Inst Phys Prdblenw~
Acad Sci USSR
Zhur Eksper I Teoret Fiz" Vol XXX, No l..
vp 69-78
Calculates shift in energy bevels of electron
In external fld due to interaction with its ovu
f1d of radiation. Divergences appearing In the
talk. 174TS1
UM/Nuclear Pb7sics Dir*c's i-an 51
E4uati= (Contd)
comPutatious are eliminated by rejection of te
Aot depending upon external fid. This leads to con-
PIderable simplication and to great uniqueness in
COMPutationO in comparison w1th results pubUshed
earlier. In computations new method is used to ob_
tain reduction relations. i
Submitted 16 Apr 50-
0
174T51

0% 0 0
1*4 0 0 _

X a it 9 u 14 a ft L? x p v
'
1 0

0
41 fa a a

00 0
A Amy
014.0to; -.". .. 1 -.1
*#DC#Iilf AN* 0

00
!.00

a MG
0:
d RAWATION CORUCTIM ni ?Us PROBLItM or TNg
SCArrgRM Or AN RLRCrWM I
N AN KL9CTR0-
0 KWHITIC IFMW. A. A. Abt*Dsw wd L M. KUwaMOT,
0 11 Zb-j.!~". I Tforst. Fix. 21, 439-35(toolf
0 R.. ) 400

0* 3 A r~WJvWAftUy-bwMr"" M~thod ol CatmIslim *I
=00
r"Wim tormilms (is Uw apgrontn"j" go/bc) $or an
coo
040 td~-ts- bd- - eketroft ad &a aderma field is
"w
rimci
LI ex
i
i coo
0 praft
ms aft
w=uw for
p
p
ar"falruy km ftelde. For the slimshmma, of LknAfte ZOO
Rd cOrrIGPOOM to observed dtoda, a proce&re
evi-W beisrs d a am I lyp Ig
00 1 istrodecod. ("th)
00
0 Zo 0

O
f '440
l

t
i boo

-
- t:00
to 0
00 U 00
0
Wo $*fool At 4-1 got Itill ad-ci.-V- 111
5 1 V ZA 0
AV so At!; I a tw 5a a
KO a 94 3 t
0 000 a 0 0 0 0 0 0 0 0 0 a 0 0 0

t

0 0 00 0 0 0 0 0 t 0
0
: , -

s
0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 4 0 0 0 0 0 0 0
4, 1

Mective, Sweet; ed Hip OR4 velseffy of 964"d lewd Its
IBM. ftyl. rtablems, Act 3R.-USS.R.. Uopcow),
CWhOy Ak-W. Ndak S.SZ.R. 19. 67-%1961): d. preceding
obstract.-The d. of the sonnal part of fit it, 06. IN Men.
.-POOM 010"Of fir4andowal HO, Dnic"dingan Whelk"
the towntntum Po vort"pooding to the rain. of emigy is
sem or differeni from wrn. #a - (0/00-TO of .
SW
(0104)EW 1k r). r"p.. with ft. - at. Kum of He'; Site
co'" * x - + X-J. whttv X. *nd NO Arv the
i Now. of fit, and Ift?. *Sam in the w1n.; P - e4rcliwe Saw"
of lie' In the dil. soln. In Ile. in the mw idtcnwtlvv.
p - P./34rr. ix. p 6 d"wndent oil the t U0420T.
nwatso(Lyntanand Fsifb&nk(C-4.4S.W=4thtvtjoc.
fty C, of 2ad Sound In met". of fit' In Iic4 permit. with the
aid of Pewiterantchult's formula Ce (o4/^)( [(So +
Ax1,w.)*rAC* + Us/2"O + (krz/vOl tabu P. -
o - o. - d. of dw vu uid W - eatmity, Ce - bftt
capecity of pun - - 1). caks. 44 mid ' P , of m. The
revull iso - 8.5wv( best a* - mamolthe, - )wkbs
Scattering not exteeding 8%. Independent of tevap. Came-
quently, ps - 0 at the min, saw L~. the aserp of lbq
XP- It h even diffemt
impurity Is of the form A tOXY,
Gmwn ftro. o would change by 33% betw"a IM&M I.M.
The vrrur of L. and F.In conchodim that p. Pd 0 tko in their
MANUmption that is - 3. Le. equal to tht at. nian of 110.
whereas actually 0 Is Steady 3 times as great. Knowietla
of 0 permits plotting of C. " a function at the Stop. at
different coacns. wW as 4 ItuSetion of the cown. at diffeml
The results an sit in in graphs. N. Than

11 Jul 51
-Sound. of Large Avigaitau in -welium T.T I -'I. M.
t Inst of Ptws Problem 420M't 78vilovp
Acad Sel USS
"Dok Ak Wauk SSSR" Vol No 2, pp 23T-240
Considers the problem of the propagation pf sonic
oscillations in helium II in the 2d &:pprazimtion-
The lat approximation is represented Iby the 801i
obtained from the linearized systela of bydrodyAsMiC
eqs. Cf. Osborne and Temperley, Proc Phyi Soc,
Ot, 1951. States that the 1st sound represents a
vave of caupression and rarefaction, and the 2d
sound is a property characteristic only from belim
.214776
11 and. represents a tenp wave. Submitted 14 May
51 by Acad L. D. Landau, vho also gave an interest-
ing discussion during the work.
214
0

KIIALATNIKOV, T. M.
MAIATNIKOV, I. Mt. - "Investigations of the Theory on Superfluidity." %,b 17
MAY 52, Inst of Physical Problems imeni S. I. Vavilov,, AW Fci USSR. (Dis-
sertation for the Degree of Doctor in Physicomatheiatical Sciencr!s)..
SO: Vechern!Lva Moskva January-December 1952

gi
:R =R.ff,
V -M Kpir- R,
0", A
AR.
pm

oz tha
-tj~,i4k ftgr jMa ta, This mork
T rv tly- al -,T.--* t-C.- - ef - I I
US"
ow, - , M,
apAM
MIMTR -2
Ml
V M."M
am WIM "t,

fUr
coudutfTtty &ad da"sidon at somil In hog=! 601--
K"tnirkoy. Tkur. gktpit. i riaret. As. U.
USS It a L-Z4(TM27-.-5Mww AF=r 56A, 433(190).-Thc Meff. 0U
thermal coad. c (d. precetRug abstr.) is caicd. explicitly %a.
niw~ftg thd exclUtiom 44ctn= d He 11 - Bees,
=Mau thermal expaarkm of He It. c does not
Lot* the abxcptka of In mad (thus kzvi=g the I
formula (A Khalatalov (CA - 45, VA lig) machanced) but!
;m~ an thuirptim of 2ad wund largef than that przvf~'
?onsircOM. (loc. ct~.) due to viicaus effzcts. hyudugmctrc~
m-ccut expd. d4ta, new vatucs a( a. p*. w4 ot an dcri;Ttd~
iwd the Avurptfou cw3s. ol lu and Zud wund are cAkd4:
-numerically as func(ious of temp. (the results for fit
at not sigui6ca-tly diffeicnt fr,= tho%~ -kd. previo-"u-ally,
(loc. ca.)). It appew" that for frequencies cd ctrdcr 104
cycles/sm. Uitre tbauld be aa appreaaWc absQrptku ut Zad
Vx1n4 - El

K Tj,
,.LAT-7
.!K071 ) I. 1.I.
"HYdrot-nardcs of Solutions of Txtrancous Particles in Helium 11 It
4
Teoret Fiz SSSR, 23, pp 169-181, 1952 Zhur 0--sper i
DS17Z
Trarslabion

USSR/Physics - Hellum II Sep 52
"Discontinuities and High-Amplitude Sound in
Hell= II)" I. M. Khalatnikov) Inst of Phys Prcb-
lems) Aced Sci USSR
"Zhur Eksper i Teoret Piz" Vol 23, No 31 pp 253-264
Outlines conditions which should be fulfilled at
the discontinuities of He II. Shows that only 2
kinds of discontinuities are possible in a super-
fluid: pressure and temp discontinuities. Analyzes
the propagation of high-amplitude-sound in the
superfluid. Author is indebtedto Acad L. Landau.
Received 7 May 52.
2M82
(eA 16-no. 44P:.r4*,r 73)

USSR/Physics - Helium 3:1
Sep 52
Sound in Solutions of Foreign Particles in Helium
n and the Dissipative Function of Solutions," I.M.
7U
Xhalatnikov, Inst of Phys Problems, Acad Sai USSR
"Zhur Eksper I Teoret Fiz" Vol 23j, No 3, PP.265-274
Rqs. of hydrodynamics derived in a previous vork
(I. M. Khalataikov, "Zhur Eksper i Teoret Fiz"
233, 169, 1952) in case of coned solns in He II are
applied to the problem of sound propagation. Gen-
eral exWessions detg velocities of Ist and 2nd
sound in He n am derived. The form of the dis-
sipative function of solutions is clarified. It is
OhOvn that, besides the kinetic cGe" of pure
.He 11, a soln has 2 more coeffs., that of dif:ru-
BiOn and that of thermodiffusion. Author Is in-
debted to Acad L.D. Landau and Profv.p. Peshkov.
Received 7 VAY 52.
Ft r6 no w0 so, o+
227T83

-Y K 0 Vl i
2. USSR (600)
1'. .5tutistical N.,cI,wIJ-c3
7. Mettod for L-e corqjutation of a statistical sun. Loki. AIi SSSR, iiio. L, 1952
Analyzes F. 7eynman's problem (Phy aov 5~4,loa (1951)) of co;:,,:mtinr iriui
exponential eq)ressions contg norl-cmunuting ooerators. Applies hi-s methodi, wlIch
he considers sirrpler than the previous ones (see E. Vigner, Phy Rev 40 (1232);
J. Kirkwood, ibid. 44, (1933)0, to,cor-.putation of the st~ttistical --un, of system
characterized by 'lamiltonian 11 z V + U(r), Indebtcd to Acad. L. D. I-midau and
2R
A. A. Abrikosov. Presented by Aca . L. D. Landau 8 Oct 52.
2 5 5 T 11,5
9. Monthly List of Russian Accessions, Library of Congress, -February -1953. Unclassified.

Ell
-29
NO!,
4.z

Khalatnikov, I.N.
Rege-.rch on the theory of
a-Aperfluidity (0,,.: ies of
articles)
LI,3titrte of 1-1,qslcal Problems
AcaderW .-,f Sciences U-SR

A 11

USSR/Physics Relativistic hydrodynamics FD 977
Card 1/1 Pub. 146 - i/2o
Author Mialat'niko_v, .1. M.
. ...... ...
Title Some problems of 4,elativistic hydrodynamics
Periodical Zhur. eksp. i teo*i~. fiz.,'27, No 5 (11), 529-541, Nov 1954
Abstract The author develops a variational method which permits one to find the
equations of relativistic hydrodynamics. He finds the relativistic ana-
log of potential motion. He clarifies the form of the Bernoulli equa-
tion for such motion, and discusses the properties of the relativistic
shock adiabatic and also the propagation of sound of large amplitude.
Finally the author finds the exact solution of the general one-dimen-
sional problem in relativistic hydrodynamics. Ackmowledges the helpful
counsel of Academician L. D. Landau and S. P. D'yakov (just recently
deceased). Four references, two USSR (e.g. L. D. IAndau and Ye. M.
Lifshits, Mekhanika sploshnykh sred [Mechanics of continuous media],
2nd edition, 1953).
Institution Institute of Physical Problems, Academy of Sciences USSR
Submitted January 7, 1954

Rg
tj~ 1~-,!

USSR/Physics Quant. electrodynamics
Card 1/1
Authors I Landau, L. D., Academician; Abrikosov, A. A., KhalataikoTp 1. H,
Title s Asymptotic expression of the Green photon function in quantum
electrodynandco,
Periodical t Reports of the Acad. of Scs. of the USSR 95, 6j 1177 - 1180p
21 Apr 19 54
Abstract An asymptotic expression for the Green photon function (D
y W)
used in quantum electrodynamics is derived. The article contalas
a diagram,
Inatitutim i Acad. of Sea. of the USSR
Submitted
t 25 Feb 195.14

Card 1/1
Authors Lawlau, L. L. Academician; A.
Title I Electron trass in quatitiim ell c-ctrody;,z,..-.iics
Periodical I Dokl- AN SSSR, 96, Ed. 2, 261 - 264, ~,Z-y
Abstract The problem of electron Liass ano partic;ilarly tne problem con-
cerning the role of the electro-majiptic and nat-I-1ral izass of t'le
electron is o;ic of the most interesting problems of qtiaritum.
electrodynamics. Of basic importziace In solving this problem
is the characteristic of the Green function of the electron G(P)
when pevm. Equations enabling one ta solve such a problem are
given. Three references all USSIto
lastitution. .......
Submitted s "rch 6, 19511

VI'U.L If
111T/T 4t+; MAO, , - . -
akademikl KIIAIA"IKOTt ism*
Az'Omalous abso
rP'lOn of sound near to
Dokl.AN SSSR 96 no.3:469..472 Ny 154.
(Low temperature research) (Sound
the 1000nd-order phase transition.
(MLRA 7:6)
waves)

A A C .".i. TirlatrI11101-
gon-i
RM
TRI go,
P5
LV

n .1 i T-, t z;
MR

_q8SHIPhys ics Eleettodynamics FD-2219
Card 1/1 Pub. 146-24/25
Author Mals~p_nikov, I. M.
Title Representation of Green's functions in quantum electrodynamics in the
form of continual integrals
Periodical Zhur. eksp. i teor. fiz, 28, 633-636; May 1955
Abutract In quantum electrodynamics Green's functions for one or another problem
can be written in the form of matrical elements of certain T-ordered prod-
ucts of electron and photon fields taken between states of a nondisturbed
vacuUm; e.g. the Green function for the one-electron problem has the form
Gab(x,xl)- ave. [T(Ya(x)Y;(x,)S/S I where Svac is the average vacuum
value of the S matrix S-e%P[-ijHZa~dx'j and T designates the operation of
relativistically invariant chronologization (D. Glaser, Phys. Rev. 91,
1953). The author's aim in the present note is to represent the expres-
sions for the Green's function in the form of continual integrals in the
space of poi V and A functions (loc. cit.). He thanks Academician L. D.
Landau and B. L. Ioffe. Five references, including one USSR: I Gellfand
and R. Minlos, DAN SSSR, 97, 1954.
Institution Institute of Physical Problems, Academy of Sciences USSR
Submitted December 25, 1954
INNOM
5 Mj-~, '01,wim 27-~
i-MME
.5, WRIT,
nl-;~Ix 1_0

ra~

adlaot trl=fft=&u4* Ot the urtan functm d
in*
charg parwas. L. E). Iandau and 1. U. Khalatnikov
'
C
t
.
- .
a
a
ZA&w. FAstC i Ttilrd. Fis, zo. W-Wiqw-~Tlie p(Ob
f
h
6
t
, b"iAvvdolb*w todea cr&dkftttma3fcCMlLdauc
1,,
,
Green fu=tion and 0l t1ta MIX, for ctuirged pWick-5.
w(lich am later-Aing ith in clertrarnagrictic field.
Wtmcr jacv-b-

llw~ V'.' s s R

ge, '~r n g~~'
W. I KIT.
00

USSRi _Phy6ic5 --iL;CoGi11y----- - -FD-28&----
Card 1/1 Pub. 146 - 21/26
Author Khalatnikov, I. M.
Vol
Title Second viscosity of monoatomic gases
Periodical Zhur. eksp. i teor. fiz., 29, August 1955, 253-254
Abstract As shown (L. D. Landau, Ye. M. Lifshits, Mekhanika sploshnykh sred
[Mechanics of continuous media], Moscow-Leningrad, 1944), a mono-
atomic gas obeying Boltzmann statiatics and possessing an energy
spectrum of the form ep2/2m does not possess second viscosity. In
the present note the writer shows that this result holds true also in
the case where the monoatomic gas (an ensemble of particles each of
which is characterize by three degrees of freedom, i.e. by a 3-&Lmen-
sional. momentum vector p) obeys quantum statistic, Fermi or Bose, if
only the energy is a power function of the momentum of the particle:
e = apn. Two references: e.g. Landau, Lifsbits, Statisticheskaya
fizika, GITTL, 1951.
Institution : Institute of Physical Problems, Academy of Sciences USSR
Submitted : March 28, 1955
D 4194-2.1. P11

tic pg--'5~g'
44

pp,
T 'INN
4, C
SUM,-
U-0 SUR

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-Category-: USSR/Atomi~ u~I'Nlolecular Physics - Low-Temperature physics D-5
Abs Jour : Ref Zhur - Fizika, No 1, 1957,No 885
Author : Xhalatnikov, I.M.
Title the Propagation of Sound in Moving Ifeliftri II. Ancl on the Effect of the
Heat Flow on the Prop~Lgation of the Second Sound.
Orig Pub :Zh- eksperim. i teor. fizilti, 1956, 30, No 3, 617-619
Abstract :Analysis of the equations of propagation of the ordinary and second sound
in He II in the presence of arbitrary (constant) velocities of the com-
poAbnts. It is shom that during the propagation of the traveling wave of
the second sound along the thermal stream in He 11, an "erosion" of the
second sound will =cur. An equation is given for the magnitude of this
effect-. Tba crosiobimay 6ccur both along the direction of the thermal flow,
as well as in opposition to the flow, depending on the temperature of He II.
It is shown that the effect of the thermal stream on the velocity of the
standing waves of the xecond sound is a second-order effect.
Card 1/1

I all_-Ir~-"t,-Otvlk-1)444~l---f-~~,~- - -_.- F~ I
Q"M A
SUBJECT USSR / PHYSICS CARD 1 2 PA - 1885
AUTHOR CHAJATKIKOViI.11.
TITLE The Elsotrodynamics of the Charged Scalar Particles.
PERIODICAL gurn.ekep.i toor.fis,31,fase.6,1062-1078 (1956)
Issued., I / 1957
L.D.LANDAU, A.A.ABRIKOSOV and I.M.CHALATNIKOV investigated the asymptotic be-
havior of GREEN'S functions in the ease of high momenta of electrodynamics
with spin 1/2 by means of the direct solution of integral equations. The
corresponding steps are taken in the course of the present work with respect
to the electrodynamios of the partioles with spin zero in KE ME RIS formalism.
At first KEMMERIS P-formalism is discussedl it is very similar to DIRAC'S
equation for the electron. Also the interaction between mesons and the else-
tromagnet~o field can be described by means of the KLEIN-GORDON- and also by
means of P-formalism. The scattering of light by light results in a finite
expression in the case of summation over all permutations of the emitted
quanta. The following is discussed in detail: GRFXNIS function of the photon,
GREEN'S function of the meson, the basic equations, and the gradient trans-
formation of GREEN'S function of the meson.
Summary: The present investigation shows'that the eleotrodyn&mics for spin
zero in formally similar to that for spin 1/2, but conditions in this in-
stance are, in general, more complicated. When deriving the integral equa-
tions the results obtained by the perturbation theory must be widely used.

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lay
RIM -115R -4

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SUBJECT USSR PHYSICS CARD 1 / 2 PA - 1550
AUTHOR CHALATNIKOV,I.11.
TITLE The Hydrodynamics of Helium II.
PERIODICAL Usp.fie.nauk, 60, faso. 1, 69-160 (1956)
Issued: 11 / T-956
Comparison is invited with the author's previous work entitled:"The Theory of
Kinetic Phenomena in He III', Usp.fis.nauk, a, 673 (1956). This survey is
arranged as follows:
I.The hydrodynamics of He II: The hydrodynamic equations of He 11 which apply in
the case of any (not smaliT velocities of motion (two motions are supposed to
take place simultaneously in He II: a supersonic potential motion and a normal
motion);-the dissipative function for liquid He II, Bound in He II (its propa-
gation in Ile II is described by a system of nonlinear equations which can be
linearized in a given case); the absorption of sound in He II (the relaxation
times which characterize the produation of excitations in He 11, the absorp-
tion of the first and second sound in He II)j on the anomalous absorption of
Bound near the A point.
II. The hydrodynamics of the solutions: The equations of the hydrodynamics of
the solutions of foreign particles in He II (the behavior of the dissolved
foreign particles, normal thickness, entropy, heat capacity), dissiDative pro-
cesses in the solutions, sound in the solutions of foreign particles in He III
the hydrodynamics of the solutions of two superliquid liquids.
Usp.fis.nauk, ~0, faso. 1, 69-160 (1956) CARD 2 / 2 PA - 1550
III. Discontinuities and the sound of hijzh amDlitude in He II: Discontinuities
in He II (pressure jumps, shook waves, temperature jumps), sound with high
amplitude in He II, on the propagation of sound in moving He 11, and on the in-
fluence exercised by heat flow on the propagation Of Becond sound,
IV. The heat traiiit4i-between solids and He II: The quantization of elastic
waves (longitudinal, transversal, and surface waves), the energy radiation of
the oscillating surface of a solid, the energy exchange on the occasion of
collisions of rotons and phonons with a solid wall; the heat transfer between
a solid and liquid He 11, the passage of second sound through metal plates,
the absorption of second.sound on the walls of a cylindrical vessel.
INSTITUTION:

"'M

11 4- /Tz'j, j, - ;+- I -)
rxw' ~ / 1- A yfj .
SUBJECT: USSR/General Nuclear Research 25-4-3/34
AUTHORt kbrikesovq A.A., Doctor of Physioanathematioal Sciences
Khalatnikovo I.M., Professor of Physicomathematical Sciences.
TITLEt Interaction between elementary particles (Vzalaodoystviye
Elementaraykh Chantits)
PERIODICALs Fauka i Zhizn' April 1957, # 4, pp 9-10 (USSR)
ABSTRACTi This article deals with the very important problem of modern
physics - the study of interactions between elementary
particles. Without a detailed theory based on such research
it is impossible to understand the nature of the forces acting
in atomic nuclei, their strueturet and theriphymics of numerous
nuclear processes. Physicists all over the world are interested
in the theory on the interaction of elementary particles. The
latest physical theory in a development in the direction of
former ideas. The basic object of studies covering contempo-
rary physics are the elementary particles of the matter we are
surrounded by. One of these particles is the electron.
L.D. Landau, I.Ya. Pomeranchuk and the authors of this article
Card 1/2 were the first to find methods of analyzing the interaotioda
TITLEt Interaction between elementary particles (Vzaimodeyetviye
Elementarzykh Chastitg) 25-4-3/34
of arbitrary forces, The results were quite unexpected. It
was established that the interaction becomes weaker when the
area is smaller on which it is spread. The situation changes
entirely with regard to nucl ear forces, i.e. force@ acting
b:tween particles inside an atomic nucleus(protons and
n utrons). Those interactions are very streag.
ASSOCIATION:
PRESENTED BY3
SUBMITTED:
AVAILABLE: At the Library of Congress
Card 2/2

-60
"I'o A~N~~iWa I iM N -VE

AMOR KHALATNIKOViouo 56-4-3/52
TrUis The Hydrodynamics of the Solutions of Two uuporliquid Liquids.
(Gidrodinamika rastvorov 4+kh svorkhtek-achith Ahidkostey -Russian)
MUWICAL Zhurnal rjksporlq. i T#oret,Fiz4il957,V61 3~,Nr 4,pp 653-657
Received 7/1957 Reviewed 8/1957
A&ITRACT When deducing the equations of this hydrodynamics the author starts from
the laws of conservation. Bgth superconductive liquids may, for instance,
be liquid He' and liquid Mo. IN this case three motions are in princip-
le possible in the liquid- a normal o4a with the velocity V,-I and two
suparliquid ones with the velocities val and V.11respectively. When do-
ducing the motionag the liquid in such a system.of reference is assumed,
in whichihe normal(and not the suparliquid)part of the liquid is at rest.
ht first an expression is given for the total energy ofthe liquid. Next,,
the form of thermodynamic identity(?) id derived. On the occasion of the
transition~of the system of reference connected witn the normal motiono
the inner energy had to " regarded as a function of donsitygentropy
and relative velocity. Next, the laws of conservation are given for the
energy E., the momentum of the liquid,, the amount of matter and entropy.
By utilization of these laws of conservation the form of the unknown func-
tions has to be determined. Carrying out of computat,iona is followed
stop by step. After investigation of various bounaary cases the form of
the unknown functions can be determined uniquely. The existence of three
motions in the solutions of the superliquid liquids may lead to various
Card 1/2 peculiar phanomena,i,e. to the propagation of three types of sound o3cil-

5r.-4-33/5?
AUTHOR MALATNIKOV, I.M.j AMIXOSOV0 A.A.
TITIZ The The 7dyfi-sm-fe-s of Liquil He3
(Temodinamika zhidkogo He3, Russian)
PERIODICAL Zhurnal Exsperim. i Teoret. Fiziki, 1957, Vol 32, Nr 4, PP 915 - 919
(U.S.S.R.)
ABSTRACT Starting out from Landau's model of the Fermi liquid (L. Landau
, Zhurn.
,
eksp. i teoro fisas Vol 399 p 1o58 (1956), the paper under re7iew inve-
stigates the thermodynamics of liquid helium,, In case of small deviation$
of the distribution function Am its equilibrium value at T 0 It is
Poo ible to represent the excitation energy in the form of E F_ (p) +
+Yf(pip') Y (pl)d9-1 dr' a gdp dp dp7/ (2 ")30
x y tril In this context,
we have Y a n n., and g, 'denotes the statistical equilibrium, C does
;
not depend on th
spin. In the usually accepted model of the ideal gas
of the excitations, the energy G (p) is written in the from of pl/2m,
with m denoting a certain effective mass. But the results obtained with
this form of the spectrum 'are not in very good agreement with the expe-
rimental data. Therefore the authors of the paper under review investi-
gate for F (p) another function proposed by L,D, Landau, nimely
E W a (P - Po)* / 2mo with m denoting the effective mass. In this

Card 1/ case, the distribution function is a T - 0 not a 3phere in the impilse
2 space, but rather a spherical layer, In the paper under review its au-
ASSOCIATION
PRESENTED BY
SUBMITTED
AVAILABLF,
Card 2/2
The Thermodynamics of Liquid H03
- 4..,1,3 / 5 *2
thorn considerthe thickness of this layer to be small as compared +,o
its radius p . In the case of the spectrum F_ (p) - (P-P )2/2m, the tem-
perature of 9he Fermi liquid Is auitablej, as a principlSt only for such
temperatureb at which the deviations from the distribution function cor.-
responding to zero are Bmall- In the model of the ideal gas# this cor-
responds to the temperatures T%t T s with T denoting the temperaturi
of the'degennution, In this context there eRists a temperature rangep
namely T > T . In which the deviation of the distribution function cor-
responding tS zero ia Bmall. This circumstance makes possible the com-
putation of the thermodynamic quantities in the Fermi region and in the
Boltzmann region. The above-mentioned spectrum corresponds in a better
way to the experimental data than the model of the ideal gas. On the
other hand, this improvement is inot so considerable as to exclude the
model of the ideal gas for Hea. Then the paper under review concludes
by discussing the heat capacity, the entropy and the magnetic suseePt,
bility in Freater detail.( 3 reproductions).
Not given
Ijibrary of Congress

AUTHOR
TITLE
PERIODICAL
i-I " I ? , I I
f-j r , -- , r-- , j
KHALATNIKOV I *M.,ZHARKOVV.N. 56-5-22/55
-Th-e-Ti~e-or A~cijilffusion`and of Heat Conductance of the Weak So-
lutions of He3 in Helium II.
(Teoriya diffuzii i teploproyodnosti slabykh rastvorov He3 y ge-
lii II - Russian)
Zhurnal Eksperim.i*Teoret.Fiziki,195'1,Vo1 32,Nr 5,PP 11o8-1125
N.S.S.R.)
IBSTRACT The paper under review employs Landau's theory of the superflui-
dity of Helium II. In order to determine the dependence of the ki-
netic coefficients of the solution upon the temperature and u-
pon the concentration, it is necessary to determine the distri-
bution functions which describe the behavior of gases of the ele-
mentary excitations in presence of zero different temperature
gradientag of a concentration op and of a velocity T The distri-
bution functions are defined as solutions of a kinbtyc equation.
At nonvanishing temperature gradients and concentrations there
originates in the solution a motion of the normal and of the su-
perfluid part of helium II, and this leads to additional terms
in the left aide of the kinetic equation. The kinetic equation-
as obtained by taking into account the.ndditional terms- for the
admixture excitations in a weak solution of He3 in helium II is
written in its explicit form in the paper under review. Then in
this equation those terms are left aside which are connected with
Card 112 the first and the second viscosity of the solution. The next chap-

77m,
AVTHOR KRAUATNIKOY 1-14, 56-5-21/55'
~
TITLE _N
~e ~~Une ~0; rodYnamic Waves and on the Magnetic xangen-tial Shocks
in Relativistic Hydrodynamics.
(0 magnitogidrodinamicheskikh volnakh i magnitnykh tangentsiallnykh
razryyakh Y relyativistakoy gidrodinamike - Russian)
PERIODICAL Zhurnal Eksperim. i Teoret.Fiziki,1957,Vol 32,Nr 5,PP Ilo2-1107(USSR)
ABSTRACT Let the magnetic field enclose an arbitrary angle with the direction
of propagation ofthe wave.In this context, the ultrarelativistic e-
quation of state E- 3P is not presupposed. but the entire conaiderat-
ion of this question is rather conducted for an arbitrary equation
of state. The author furthermore investigates in his paper the pu-
rely magnetic tangential shocks in relativistic hyCxodynamics, at which
the thermidynamic magnitudes remain constant.
The magnetohydrodynamio waves in relativistic hydrodynamics. First of
all, the expressions for the energy momentum tensor in relativistic
hydrodynamics and for the energy momentum tansor of the electromag-
netic field are written down. In this context, a mddium with in-
finitely high conductivity is examined. The electric f
.ks and the
magnetic field are connected by the equation Y H . The con-
ditions prevailing at the shook places can be expressed for such a
motion by the continuity of the relevant components of the complete
energy momentum tensor. The conditions resulting therefrom are written
down in their explicit form in the paper under review. Thus the first
Card 112 pair of the Maxwell's equations in still taken into account. The ma-
On the Magnetohydrodyngmic Waves and on the Magnetic ' 56-5-~l '55
Tangential Shocks in Relativistic Hydrodynamics.
gnetohydrodynamio waves can be considered to be a boundary case of
shocks of very low intensity. The present paper lists the equation
for the front of propagation Of these %ayes for the general oase.In
the general Case tWO W&TG8 are propagated with different TelOCitieS-
In the ultrarelativistio case particles can be created at high tem-
peratures. The second chapter of the paper under review deals with
such tangential shocks at which the thermodynamic magnitude remain
constant. Here again the present paper follows the computations step
by step. In the tangential shocks here under considerationg the ve-
locity does not change its absolute value, but this vector rather
change only its direction at the shock places.
( 1 reproduction )-
ASSOUIATION Inatitute for Physical Problems, Acadamy of Science of the U-S-S-R-
PRESE14TED BY
SUBUITTED 8.6-1956
AVAILABLE Library of Congress.
Card 2/2

A"i
AUTHORS; Arkhipov# R#Gt# "alatnikov, I.M. 56-3-30/59
TITLE: Propagation of Bound at the Boundary 3etween Two Superfluid
Phases (Rasprostransai uk cherez granitsu mazhdu dvumya
overkhtskuahimi fasamile ZV a
PERIODICAL: Zhurnal Skeperim. i Teoret. Fizikiv 1957, Vol- 33, Nr 3,
pp. 758-764 (USSR)
ABSTRACT; The passmge of the first and the second sound at the boundary
between two"auparflaid"liquids is discussed theoretically. It
could be proved that a conversion from one into the other is
possible. Also in this case it is called conversion. The corre-
apoading equations are given for the energy flow of the reflected,
deflected, and converted waves, namely for the first and the
second sound:
1) Both liquids are "superfluid". Concentration vaiuss differ
(4 0 ) 2 813/&g )? 1
2) Both li uids are "superfluid". Concentrationvitues are nearly
equal. ~~Lo)29B/&Z/ I.
3~ The second liquid is not "superfluid"
4 The first liquid is not "superfluid".
Card 1/2 There are 5 Slavic references.

f/I 19 Z-
56-3-47/59
AUTHOR: Khalatnikov, I.M.
TITLE: On the Hydrodynamical, Fluctuations in a Superfli4d Li quid
(0 gidrodinamicheskikh fluktuatsiyakh v sverkht'ekuchey zhidko-
sti) (Letter to the Editor)
PERIODICALt Zhurnal Eksperim. i Teoret. Fiziki, 1957, Vol- 33, Nr 3 (9),
pp. 809 - 811 (USSR)
ABSTRACT: L. Landau and Y 'e. Lifohits (Zhurnal Eksperim. i Teoret. Fiziki,
1957, Vol. 32, pp. 618) computed the fluctuations of the hydro-
dynamical quantities in classical hjdrodynamics by the intro-
duction of "foreign terms" into the equations of motion. The
author computed by means of this method the fluctuations of
the hydrodynamical quantities in a superliquid liquid. For the
sake of generality it is assumed here that foreign particles
are dissolved in the superliquid liquid. Because of the un-
usual simplicity of the method this in no way complicates com-
putations. First, the rather voluminous equations of the hydro-
dynamics of the solutions of a superliquid liquid with foreign
bodies are written down. The following quantities are intro-
Card 1/2 duced into these equations t The extraneous tensor of the mo-

AUTHOR: Abrikosov, A.A. Khalatnikov, I.M. 56-5-1-V46
TITLE: On a Model of a Non-Perfect Fermi Gas (0b oduoy modeli
neideall nogo Fermi-gaza)
PERIODICAL: Zhurnal Ekaperiz. i Tooret. Fiziki, 1957, Vol. 33, Nr 5,
pp. 1154-1159 (USSR)
ABSTRACT: Computations by Huang (ref. 1) and other scientists of the proper-
ties of non-perfeat Bose- and Fermi gases consisting of particles
the measurements of which are small compared to their average wave
length, are extremely voluminous. Another method of computation
is now proposed 'by meazs of which it is compiratively easy to com-
pute the thermodynamical quantities of Huang's model for the case
of the Fermi statistic.
The energy of the basic state (2) and the effective mass (v/m*)
of the excitation of a Fermi gas irj-.
Card 1/2
56-5-13/46
1 On a Model of a Non-Perfect Fermi Gas
4k 6 3 113
(8) ?`h I)J
E E
and IM
Tn
There are I figure and 6 references, 3 of which are Slavio.
ASSOCIATION: Institute for Physical Problems AN USSR (Institut fizicheskikh
problem AN SSSR)
SUBMITTED; April 24v 1957
AVAILABLES Library of Congress
Card 2/ 2

"New Symmetry Proporties of Elementary particles," by A. A.
Abrikosov, Doctor of Physiconathematical Sciences, and Prof
I. M. Khalatnikov, Institute of Physical Problems imeni S. I.
'y
Vavilov, Academy of Sciences USSR, Prtroda, o 5, may 57, pp
5-10
This work reviews the parity nonconservation problem and explains
Landau's "combined inversion" idea. Popular language is used throughout.
Lee and Yang's two-component theory of the neutrino and experiments at
Columbia to verify the theory are discussed.
The article includes the following remarks on Landau's theory:
D. Landau proposed that there is no simple symmetry with respect
to charge conjugation such as the symmetry with respect to inversion.
However, there does exist symmetry with respect to a combination of
these two operations. L. D. Landau called this 'combined inversion'.
This- means that everything remains unchanged If all directions are simul-
taneously reversed and the particles are replaced by antiparticles.

"It is easily seen that under these conditions empty space does Udt
exhibit any asymmetries, since there are no electric charges in it.
Tbus, according to Landau's idea, it is not the space which is asymmetri-s
cal, but the particles in it, Landau clarified his notion with the
following example. When any object is placed in front of a mirror, it
seems to us that the reflection which we see Is identical to the object,
with the exception that everything on the left side of the object is
on the right side In the reflection. In actuality, this is not so.
The reflection which we see in the mirror would, if it actually existed,
differ from the object in the fact that it consisted, not of atoms, but
of ahtistoms (poBitrons, antiprotons, and antineutrons).
"It is well-known that a particle is annihilated when it collides
with its antiparticle.... Since the object cannot pass through the
mirror and its reflection is not a real object, there is no danger of
its being annihilated by its reflection. (U)
7

AIRIKOSOV, A.; KHkIATNIJOV, I* duct,v,tro Usp. fiz. liauk'o 6 no.4:551-591
Modern theorY Ou aupercon (MIRA litio)
Ag 158- (superconductivitY)