SCIENTIFIC ABSTRACT NIKOLAYEV, V.I. - NIKOLAYEV, V.I.
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CIA-RDP86-00513R001137120001-5
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98
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Publication Date:
December 31, 1967
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SCIENTIFIC ABSTRACT
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MOU'VE7j, V.T.j FMXF~Mv, S.A.
Introducing a macUno for impregrating paper wit~-
resina. Biul. tekh.-ekon. Inform. Goo. rinuch.-Isal. inst.
nauch. I tekh. Inform. 18 no. 12r/.7-a D 165 (M'-MA 1911)
S/Or 63/044/002/064/o65
D 1 85"Y3 102
_ev., V. 3:-,cherbina, Yu. 1. , Karchev a kiy, A. I.
AUTHORS: '.Iikol!y It
TITLZ: The Y;asbauer effect in the compound FeSn 2
PnE TODICAL: Zhurnal eksperimentallnoy i teoreticheakoy fiziki. v. 44,
no. 2. 1965, 775-777
?FX7: The antiferromagnetic co=pouni FeSn 2 Is one of the mont in%eresting
objects to be investigated by the I'dosbauer metliol, 3ince b5th t:.E
i0otopes P057 anti Sn 119 are well nuitoci for atuiying nuclear I-r;,:i
absorption. The authors men.iured +he nbsorption of 14-4-e%
57, 270 days halflif..) and 2~.O-kov y-quanta (a-,u,--~e
(source Co
250 days halflife) by a 28 mp,/cm2 thick layer of Fe3n 2 depositel on a
Be dice. The intensity of the radiation passed thro-igh"he absorber was
measured with a Nal(Tl) crystal connocted with a single-channe" -j-alae-
height analyzer. The Fe57 a;,.gorption spectrum of the 14.4-kev q-ianta
contained six well resolved peaks, the distance of the 6uterzoat onea
Card 1/2
BOUMS CM61
AUTM I--Zasff, A. 11,
=I nomis
TITIS: mwmwl;/OffwtonWinwityawleila~Au& I
SOUM23 jMWOW9 b1
aw I tome Ichoskay Mild. Pialm v rodaktalyu.
ftilmhODAYGO Yo 4, 000 a& 1966P 315-32D
70PXC UM Mosobwoor effect,, maigaiwas compounde antiferromagnotimas, forroxagmetimev
114*1 temperature
AWTUM Sifte WAve offards the rwm opportunity of inveatigatisig the Ine". lee of
a Mostanco botb In the antiferromagnotle and in the forromagnotic state at the some
tooperstwes t1w autbors Investigated the Mosbauer effect an re" Impurity nuclei In
the crystal lattice of MhAva. So purpose we,, In particalwo to ascertain how Ww
transition of a v6stance to the forromeguetic auto affects the Signitude of the
magnetic rIeld acting an the noclaw or the lopwity stom. PkAlcular attention was
paU to Uw bdwvlor or the Nosebaver-offect probability in magnotte traneftruntloos.
On wiportmento wess made an a sample, previously used to Inveatid"S
the towwaftm ~* ~ -P of Ww magmatic pop" lee (Zhw T., 145P W# 3963)o so
MAws ongde was Uw r"latlow, emy". Ow atons or the lootep 66" were intreame"
into the "Wk% 14"104 by d1frulon. 7be obeafter in Um Nosebmaw-effeet sovertmeafts
vas a staial"41-steal ftil (W% ft). Us measurements Were WWI* with appWates at aw
L 04402-4t
ACC NM
interest to IM641846 the AM of the Nosebawr effect as & rtm 100 Of the
ft*IA am of Ot In s%b~%&Wqs in which the strIction to IA1160- I" as'
thwk At"adel" 1. 1. K"Will for cantimous Intereet in the Waft'l TV. A!-"
A. IL AtIMMO-71m fW WOM alse"SIOWS, Wd we X. MINIMUM am T. t--ftft-bff
TM- WO 61"trMic GFPMtW - GFQ -.60Y.-Ri: 3 ftiw"
.on coal OD/ "Ad"/ MW WWs oo6/ on MWr 003
Cud )/~ -n!k
L p7112-67 - M. (j)/E4T(ffi)/EWp(t)/E-Tj
ACC mm' APON104 SOMS COM Ult/0049/"/03 -0/004/0"9/09"
?I=$ 111VOStIgOtION of UW Mwebador fffect gq FAST nuclei Is nickel ferrite --cbraMU
91th a oompeasetlow point Z-IWW-rts All-Laign Caffifeapm On Uw obselop of rern- sod
AmtlfeEra~tlmm bold 2-7 Jaly IM in Sver4lovsk7 *
SOMCS: AN ~e lavestlyes Serlya fisickeekays, v. 30, na. 6, 19", 94#-n4
70PIC TAO5s ferrite, 11masbamer effecto Monabsuer spectrwo, spontaneous amesetisatlem,
magmetle offset# Ires
ASBTXACTo In view of the paucity of studies of theMossbouer effect In ferrite*, the
present investigation was undertaken with a view to deterelaing'Sho temperature do-
penderte of the amebsuer spectra charact*rIsIng the absorption of 14.4 heY Sammis rays
bY 70 auclel In a ferrite with a compendation point. The Investigated material was
nickel forrite-ebromits: NIJF02-xCrxO4 wIth x equal to 1*0 and 0.9; both substances
have tke Inverse spinal structure. Both the Curie point and the compensation point
of the two "nagnaltiong lie above temperature. The two specimens were systhe-
Mixed by the so-called "dry" psoc ure of the corresponding oxides (high purity grade)
All the masure~to were carried out with a stationary abseAwrV A series of curves
Cmd 1/2
1%~V~PMtt6 offoot of Corlims val4pris to fusetlawl diser"re of
oorton to do". FormA talme 119 orMlowss:6-7 056.
(Sam 10-M
GO*=. itemoses.
w"re, off. of Garlims walserls attract* One))
(?JAM,
Corlims vul4pria, off. so exper, "rebral corses &is.
tame))
QATSM. V.V.; lIKQlAUV,T.I.
Cou6bad effect of aeffoiao and strapheathia, Stul,skap.blal. t sed.
42 ma.110942 5 156. (NlaA 1021)
Is Is kafedry formakologil Toromashokogo seditelaskogo institute
(save kafedny doseas I V.I.Zmvmshwv) Prodslavlam 4systwiteltoWu
ableaft AM SM V.I.SkworteoVs.
(mmarshrrm. effects.
sm, Me with ceffetris (lbs))
(CAmIn, effects$
an Me with strophsathis, (Rue))
i"; Fit
Ri
viii,
A 181,1511 1 1!9 A 9:1 s I
ril-
ZAVIULAW, A.Y.1 NI4OLAM V 1.
Zffect of cytiton and Thermapols tincture on the *----*tic effoct of
apomarphino un&r allnical and experinental conditions. Zhur.neyr.1
paikh. 63 no-314Y)-445 161. (NUA 14%7)
1. Kafedra farmakologli (zav. - kand.med.nauk V.I.Nikolaysr)
Chitinskogo(wditsinskogo inatituta.
AMLEPTICB) (SWH PEA)
(VOKITING)
VASILAW9 S.I.; ~IA~MV MAXIII, N.S.
Q1MtIt4Uv9 det4rMiMUm of C&Aiac glycosides In solutions by
the MtW of objoeUve Im1nesewca analirsis. Apt. dela 11 rc.ls
34"" $46-F 162. (KIIIA 15s4)
2. ChlUjwkly medlUbwkly InatItut.
(C"UC GLMIDz-.S) (LUMMMENCE)
L 118o-g. ENV jAW(1A)AWt(tj/tW(b)
ACC NW; AP50"t Wei C'O-- MM11i 1.lVdWlf,51(*21(108103T3lo3-r7l,
r, r ~t. Aag 4SWUMS', 90 0,
8VjM: SkU0101 dope.!. t tearatidiesh* ftatki. Mole% v reft1ktatyx
(PrI1011"IYO)l ft's 2P Mae i;,~ 1~65# )T3~_)?T
TMC "at frow alley* N"~Owlfw attar. "t1ftrn=W"tfr witertott, order*$ alleyv
meet te"MMtW*
AT%RM"t To e%eek on the fWateme of w4piette Ordw ift the erm"I"d FVA* the
authors inrestigated the Notsbauer spectra of' Fe5T nuclei In Oft ccftpound at te"r-
sture T7--5WK. 7he swTle was prepared by a procedure described by M Mwo et, eLl.
(J. ftn. Boc. Japan v. 18t 589, 1963). The initial components were Ar7eco Irnn and
gerranium. X-ray structure analysis has established that the ';nmple rrcduced con-
tnint a phase with hexagonal structure, having parameters a - 5-M5 A RM c o 4.054
Investigations of the ragnetIzottion of tht sample in the Inter-ral ~W-500K have
shcnm that there are no ferromgnetic ImIT, ritieS idth Curie points above room temper-'
attire. In the expertmentq on the Mossbauer'effect the We sample van used an an
abitorber. The saurce of radiation was Co5r introduced In stainless stetl. 7*he Moss-
bauer npectrum of the FeS7 contained all Aix resolved ecuponente of Vie lqperflne
strmcture, thus evidencing the magnetic splitting of the gr(nind and excited levelz of!
Fe,V aml drwnstratt". directly that Ff4)e hap an ordered rotgnpt1~ Ptri)rttire at rr^-"
Card
L 1188~__66
ACC NR, APWAO.17
temperature. The magnitude of the local magnetic field at-f-Ing an the Iron nuclef
in this case 123 f 3 koe. Analogous spectra vere obtained also for other temperatures
It In alto concluded thnt FeGe Is antiferromagnetic. Exprtrapolation of the temper-
ature dependence of the nuclear magnetic field to zero yitlds a value T - 411 t "K
for the Neel point of FeG. Authors thank 1.kK. KIkoin for interest in the vork, i-UL.-i
L'P4. KMan for discuselorm, 'fl. W. Kuznetsay and Vvi1;5Bo_gachev for help in adjusting
the exlwinen-W setupp aM P.vF.' Petrov and V.11A..Somenkov for the x-ray structure.
anialysis of the. sample, Orig. aft. last 2 figures,
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riessolov.-obti 1. G. J,PUZHININ, V. 1. NIAOLAYEi. 1. S. A. 1. :AZAr-EVA.
Zhurnal prilrl. xhlmil, 1A), No. ~, 9. 781-j2.--Bibliarr: P nezv.
601 Letoplo' ZhurnollnyKh Statey. ~ol. J~t, 1-~4)
1
NMUYEVO V9 I*
USSIt/thadstry - Salts
Brims
Aug 49
Ghtparing Complex SmIts Crystallised Frew the Brines of Kers-Bogms-col," I. G.
Drushinino V. I. Nikolayevo 1. S. Chelyadinat A, 1. lavers"t Inst of Gen and lwrg
Chun, Aead Swi VMq 6 Vp
NZknw Prik R"w Vol IIII, No 8
wara.-Bolas-Cool brines give variable yields of alto,, depending on the ta%perature.
At 00 cg Uws is rem y high yield of ampestum sulfatom; above 25' C, astmkhwdtom
is obtainedl and t:low Cp airabilate is the chief product. Saturated sodiis sulfate
solutions yield as mch as 268 kg of odrabilate per 1 cubic mater of solution. SubmItted
5 Jan 49.
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31625
N ')DO 8117/BlOf)
AUTHORS: Dobryakov, D., Krumin', Y11., KlyRVin', U., !iikOlayOV, V.
.1 ..............................................
TITLE: Investigation of the possibility of conveying spherical
conductive bodies by means of a magnetic traveling field
PERIODICAL: Akademiya nauk Latviyokoy SSR. Izventiya, no. 12 (175), 1?61,
55 - 60
TEXT: Ponderomotive forces were determined, which are necessary for
conveying solid and hollow spheres placed in the magnetic traveling field
of a cylindrical inductor. Experiments were conducted to convey solid
apheres of various materials in a magnetic traveling field inductor under
dynamic conditions. For the motion of a sphere in a tube, an approximate
equation was derived under the following assumptions: (1) the friction in
proportional to the velocity of the sphere, F friction ' kvi (7) tho
acceleration of the sphere is constant, dy/dz - a - const.; (3) the
electromagnetic force F em does not change with velocity (holds for a amill
r:nge of velocities)l (4 ) the energy consumed by the rotation of the sphere
C rd 14
-NXCFATM, 11ktor Goorg1jewlah; CHIGOW. loalf Xekharowlah; MISM. T.W.,
[Distrlbutlon sW mltlvotlon of frult i-A berr7 "aloe and
varletles In North Ossetia] lassashchov.& porod 1 sortev plodavo-
larAmpich kulltur I W&od so alai v uslovilokh lbversel Oeetll.
Ordstmikides, Severe-Osot I askes, knisbace 1901-woo 1960o 57 pe
(WIU 1413)
(Ossetia--rftlt aultnre)
21356
)Lilt , ILI ISO J,-* 11401 1155 S/126/6i/oil/004/003/023
8032/9314
AUTHORSj Karchovskiy, A.I. and Nikolay_qyj__V*I#
TITLgt Hall Effect in the Motsmagnstic Alloy HnAu2
PERIODICAL: rialks m*tallov I metallovedenire, 1961. Vol. 11,
No* 4, pp. 519 - 524
TZXTt Since the experimental data reported by various
authors (Moyer, T&Slang *t &I - Refs. 2-3) on the magnetic
properties of MnAu,ioro not in complete agreement. the present
authors have Inves gated the Hall effect, the paramagnetic
susc opt Lbility,magnotisat Ion and the magnotocalaric eff*cttn NhAu2.
The MnAu 2 alloy was prepared from 99.99% pure Au and electrolytic-
ally pure Mn, taken in the stoichiosetric ratio. The alloy
was prepared using the method describod by Meyer and Taglang
(Ref, 2). The Hall effect was measured on rectangular specimens I
placed In an argon atmosphere in magnetic fields up to
36 000 09. The paramagnetic susceptibility was measured by 44
the Gouy method and the magnotisation was determined by the
ballistic method. No correction was made for the demagnttisation
Card 1/5
21356
Hall Zffect 3/126/6i/oil/004/003/023
2032/8314
(Curve a is taken from Ref. 2; Curve represents the
results Ot KU8Gmann and Raub - Ref. 4; Curve 8 represents
the results of Klitsing and GL*Iesa*n R*f. 4 and
Curve'L represents the present results). The magnetocaloric
affect was measured in the range 90000 to 36 000 09, at
temperatures between +20 and -140 C. The ferrosagnetic Curie
point, as determined from the magnstocolosic effect maximum
in large fields, was found to be 100 + I C. The temperature
dependence of the nagnstocalorle effsZt was found to be
entirely analogous to that found by Meyer and Taglang (R*f. 2),
and indicates that the alloy Is antiferromagnetic in weak
fields. Thus, the dependence of the Hall effect on the
external magnetic field in the metanagn*tIc alloy MnAu2 below
the Neel point suggests that the mail effect In mete"gnetice
shown the same regularities as in ordinary ferromognotics.
Acknowledgments to Academician I.K. Kikotn for attention and
discussions, to V.I. Kutaytsev for assistance with the
preparation of the alloy specimens and to A.S. Nikishin for
assistance in the experiments.
Card 3/5
ieI356
S/1 26/61/011/004/003/023
Hall Bff*ct .... C032/2314
Fi,%. 41
a
:j
i
I
I
i I- -..- C.ard.5/5-. -
it %4 1 14 9J-
14.1 Ito 1041
30415 1
S/126/61/012/003/006/021
9032/9314
AMHORS: Karchevskiy, A.I. and
TITLIt: On the Hall effect In the metamagnotic alloy MnAu2
PERIODICAL: Fixika metallov I metallovedoniye, 1961, Vol. 12,
No. 3. pp. 372 - 375
TEXT: Recent interest in the properties of MnAu2 is due
to its metamagnotic behaviour: in a sufficiently strong
magnetic field the alloy experiences a transition from the
antiferromagnetic to the ferromagnetic state. Previous work
by the present authors (Ref. I - YMN, 1961, 11, 519) shows that
in a wide range of temperatures and magnetic fields the [fall
e.m.f. in metanagnetics may be represented by
aH M R0H + RII W
V~
where R0 is the classical Hall constant,
R is the ferromagnetic [fall constant,
Card Iit
3 k5l
5/i26/61/O12/OO3/OU6/G;-'l
On the [fall effect .... E032/IC3i4
I is the magnetisation, and
If the true magnetic field in the specimen.
The Hall e.m.f. eH is referred to unit current density an%l
unit distance between the Hnll electrodes. However,
I.G. Fakidov and V.,N. Novogrudskly (Rof. 4 - FMM, 1~)60, 10, 158)
have reported that when the alloy MnAu2 gots over into the
ferromagnetic state the slope of the oil (1) curve changes by a
factor of 3. On this basis the authors of Ref. It conclude
that the Hall effect in antiferromagnetic and ferromagnotic
states Is of different origin. The present authors, on the
other hand, now point out that this conclusion is erroneous
since the bend in the eHM curve is due to the fact that the
Ifall e.m.f. of MnAu, consists of two components, only one of
which is proportional to the magnotimation (c.f. Eq. 1).
Fig. I shows the magnetisation dw (cgs/g) of Hall specimptis
as a function of the magnetic field H( kOe~ These curve-, are
corrected for the demagnetizing factor. The two .1-InAu 2 specimens
Card 2/~,.,
3G451
S/126/6i/ol2/oo3/oot.)/rj,_,j
On the 11al I effect E032/E311#
t o H r 0 . However, it must be emphasised that thp
correspondlwt curves must be plotted aa a function of the tt'lip
field in the specimen. The valuns of R fou MI)OCIMP11" I I r) (I
- to -I C 2
2 were found to be - 19 x 10 and -15.5 x 10 Vg/A S&usn ca
Usinz these values of RI , one can exclude the second component
of Eq. (1) and determine the classical component of the Hall
effect. A plot of A "n ~ 'ii - RII as a function of the
H wan found to give a straight line passing through the ot-igin.
This fact leads the present author to the conclijslon thrkt thra
mechanism responsible for the Hall effect in both the forro-
magnetic and antiferromagnetic states of %InAu,, is the same.
Acknowledgments are expressed to Academician I.K. hikoin ano
Yu..'I. Kagan for discussions. (Abstracter's note - thi,4 i,~ an
Abridged translation.3 'rhore are 3 figures and 11 referc-ticf,n,
3 Soviet-bloc and I non-Soviet-bloc. The English-lan~,ijav,(.
reference quoted is: Ref. 2 - E.M. PlIgh - I'llyn. i?(,V., 1,130, '16
1503.
SUBMITTED: January 10, 1961
Card
ACC MR, AP5021898
621.431.74-5
AUTHOR: Nikolayevi -V. 1. Qf~lngrad)
TITLE: Tho determination of the time spent by an operator solving the problem o( ship power
plant control.
SOURCE: AN SSSR. Izvestiya. Energetika. 1. tranSP017t, no. 4, 1965, 130-146
TOPIC TAGS: automatic control system k ship component, man, power plant
ABSTRACT., Automation of ship operation reduces drastically the number of operating per-
sonnel needed but, at the same time, fnercises the importance of their actions. The present
aut)ior c,;talollshes a model of the action of operators (viewed aB components of the control. sy9-
trm) of-Ehip pwxcr phints and -Jtcr a thorough theoretical anmlysla & rives expressionn for
("Irrying omfl th(' individual operations conf:t1tutinr the control process. The proceising of
w1p.11"rous w(perim(intal (kta shows that thcre vx1hts'a goneral conncctlon betwren th
0 amo!int of,
informatkin and th( tinlc neressary for its reception and conversion. However, under compIrx
cordlitforks thiti conn(1-tion may t)-,- distorted by side factors which may be reveak-d -on] aftrr
an uxtrcmely careful analYsic of all circumstances. 'ill,: present Inquiry will have to tv, nupple -
mented In the futurv by the -tudy of the probability of Jncorrcel actJons on the part of frperatorn.
Or1r. art. hap: GI formulas and 4 firiirvn.
ASSOCDMON: None
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