SCIENTIFIC ABSTRACT NORKUS, P. K. - NORNEVSKIY, B. I.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001137320004-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 3, 2017
• Document Release Date: August 1, 2000
• Sequence Number: 4
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

IIORKUS,, P.N.
Use of an 0504 catalyst in titrimetry. Report 4z Determination
of chlorine dioxide and chlorite. Zhur,anal.khim, 20 noe5612-
614 165. (MIRA 18:12)
I* Institut khimii i khimichaskoy tekhaologii AN Litovskoy
SSR,, VilInyus. Submitted Harch 6,, 1964.

NOR-ARMAN, N.G.
........ ... ~.- -I.-I-1. .. 11
Effect of various oxygen pressures during irradiation on the
level of metabolism of phosphorus-containing compounds in the
roots of Vicia faba. Radiobiologiia 5 no.2:301-303 165.
OMRA 18:12)
1. Armyanskiy nauchno-issledovatel'skly institut zemledeliya,
gorod EcIniadzin.

IDIKENE, O.K, [Galdikieno,, 0.1
Determination of boric acid in a nickel-plating be-th. Zav.1--b.
31 no.IOM91-1192 165. (MA .19:1)
1, Institut khimii i khimichoskoy takhnologii AN' Lit(wakay SSR.

jI
U-ss R
bi and
VIM" R,
d that of in , . . Fin.. xt,
-42 -PrM a wcwk
is
1954, 7. 417 LAWS. d6tail"
LBUY the work of rAnkirchen and Uack (I. cIppl. PAys.. 1944,,
IOU1164) and c1 lim and Khavig (Z. phye, -Chrxt~. 1044. 193, 196)
R
:Who" OROU119-4 4rt giVin In dt4llil. It is now found that in'
glr~rr. a hot-stretchtd merpolyarnid6 thread to a Wd-strifthed
goin
(bct being derived from c-arninocaproic
heyarmide Wead
the In-tea" In t)W dtgre4 of (Irient;ItIC'n it l1bailar to that in
41u-tako ele-w-atAl fibrills of milwrl,olyarnides ; th'eje fbrilx Are
Obtalned thothttad. Tho-asl;ll,~EF
In thickrms Ixt-A-&n superpolyaWdo fibrils and polytthyltno
fibrils I% &ter-alned to be about IWA. ' this difference s~lsj:I exl4ts
for Yboose II& fiWill arul librild of native Wood cellalry.4% llatiye.
thd comerised cotton lad foy cldtjn,
gi!ptts ~re xep~,oduccd, (23 roferemccs.)

BJOIV., V.O.; U'TONTI, F.; LORKIEWICZ, Zq EHal~
Pace=uker treat~nent ir. Adams-Stak-6s syndrcme. Ccr vas& 7
nof2t93-100 165,
1. Department of Thoracic and Cardiovascular Surgeryp, Uni-
versity Hospital, Uppaala, Sweden, and the Surgical Depart-
.mentp Medical Auademy, Tcdz, Poland,

LORKZWrCZ, Z.; MORUINDp S.; THORE21, L.
Parenteral fluid administration thrcugh a catheter insertedl,
into the superior vena cava. Kardiole Pole 8 no,lt25-29 165
1, Z OddzIalu ChIrurgii Klatki Plersiovej Szpitala Hlejakiego,
Im. J. Strusia v Poznanlu (Kierownikt prof. dr. Je Moll);
z Kliniki Chirurgii Klatki Piersiovej i Sercowo-?Iaczp.4-wej
(Kierownikc prof. dr., V.0. BjUrk) i z Kliniki Chirurgicznej
Universytetu v Uppsali (Kierown1kc prof, dr. 0. Hulten).

NOMU. Imill. Zagrekb
Plea for reorpzlxatloa of wdical edwatton. A=odoo, sdrav.t
Bow. 11 no.3:67-81 1955.
(IMATION. wMICAL,
In rugosl.. reorgants)

ACC NRt ATu021362
SOURCP C03F.: UR/3174/65/000/055/0042/0043
an re,;.eaceAk 0
AUTHOR: Norm A. yu. Q.A%3q~, -SS c c-- jk~-)
!et
ORG: Ninth sov~ expedition (Devyataya sovetskaya antarkticheskaya, ekspe-1
antarctic
ditsiya)
TITLE: Seismic lobservations at NovolazarevLya station during the Ninth soviet
antarctic expedftion.
SOURCE: Sovetskaya antarkticheskaya ekspeditsiya, 195S- Informatsionnyy byulleten%
no. SS, 196S, 42-43
TOPIC TAGS: seismology, seismological station. seismic detection. seismic wave,,
ei 0 -
Antarctic s smicity. seismographA)SF seismograph, seismic background, microseism
ABSTRACT: Tnter~st of the seismic observations in Antarctic& was cente'red upon 11
weak earthqujikeg', since so far no strong earthquakes were ever originated and registe- .
red here. For this purpose, a system comprising three ultrasentitive short period sei-
smographs was idstalled at Novolazarevskaya station. Their optiAum registration Oerio4i
was .8. - .9 sej,, with the maximum amplification factor between 70,000 and 100,000. 1
During'~964, no 6arthquakes with antarctic epicenters were observed, although many di-J
h ak
stant--tarthquakes could be studied. The presence of very weak eart qu es assigned tol
an) was
an oceanic region 15 - 200 directly north of the station (on the zero meridi
noted. Its active zone is at the underwater elevation Shpis, which is situated under

ACC NRc AT602336Z
400 M of water, surrounded by Much larger depths of 2000- 3000 meters. The nature of
the general backgound noise, comprised of short period highly damped oscillations and
of microseisms due in part to winds. is discussed.
SUB COOB: So IT/ SUBM DATBs OSjune65/ ORIG RBF: OOL

LUXITANOTO V.I.; KYMIN. V.A.; SMY]MOT, I.I.; 330HOOT. A.U.;
TEWSKIT, X.6,; KILINUZOITA, OX; PUBMT. TUO..- OMM. V.V.:
MAIM11091T. T.M.1 IMMIMWIr. r.L.9 UFSMW.M, P.O.; KU=o
M.S.; RMATISHXMT, I.D.-, MTKIN. It.r.1 KOZMK.IKQT. 0.A.:
ZCUIN, G.M.; _XqRW
.. , . B..B.; TWICT, N.S.; SIMRYANIKOV. S*K.;
V=OT, N.G.; 101FIXOT. P.G.; TR.IUUMG, G,V.* iathas red.lid-va;
(MINSON, P,G., takha.red.
[Designing chief plans for Industrial plants; principal sathods]
Proskt1rovanis, genarallnykh planov promWahlenarkh predpr1latil;
osnovnyo polothealia. Kookwa, Gos.ixd-vo lit-ry pa stroit.,
rkh1t. I strolt.materialime 1960. 103 p.
WU 13t6)
Almdaidya stroltelstva I arktitaktary SSSR. rustitat grado-
strattellstva I rayonney planlrowki. 2* lauchno-isslodo"tel'skly
Institut gradostroltellstva Akedmall stroitel'stra I arkhitekt=7
US= (for Khorkhot. 'releaskly. Kellnikhcma). 3. GoandarstvanM in-
stitut, proyelctirovanlys mtallurgichookikh zavadov (Giprows) (for
Pleshkov). Wontin:med on zwzt card)

IlAn AccuraU Altimter for Geogmphical Studiditru rz. Tees. geograf obahch.,
829 N0.3j, pp 326-3299 1950
Tramlation M-15301t 21 Nov 50

AIMEOnV, Begs; -fUD=V# G.Sh.; GLLGOIRT. A.7.; KISLOU. A.K.; XCRUN.
I A - LrSGTKIT, K-A.-, fRLTrOTSEDr. KA.; SCROMF. M.M.. inthener,
-;~tor; WITROT, P.A., takhatcheekly'redaktor
Me of aerial photographs by railrosA location parties] Ispoll-
sovanis serofbtasniskor v polevykh tr'angirovochrqkh partitakh. No-
skva, Gos. transp. shel.-dor. IzI-vo. 1955. 130 P. (MMA 8:6)
1. Koscove Toesoyasnyy nauchno-Issledovatel'skiy institut thelegno-
dorozhnago strottel'stys, t proyelctIrovemiya.
(Railroads-Location) (Photograptq, Aerial)

PETROVO M.A.; NWW40 E.A.; VOLODDI.. A.P.; DENISOV, V.A.;
KOCHKONOGOVO V.P.; BEGMj, L.G.; BMANGV,, M.A.; TAVUiOV,
V.K.; YENIKEYLrV,, G.Sb.; BAWOVA, A.I.; KUDRYAVTSEVp
G.P.; HALYAVSKIY, B.K.; CHEGODAYEV, N.H.; S01111, V.S.;
GOVIKBERG, I.V., retsenzent; ENO-LIKE, V.A., retsenzent;
KHWK0Vq V.A.p retsenzent; ALIPERT, G.A., retsenzent;
ALEKMEV, B.H.9 retsenzent; IKLYAROV, A.A... retsenzent
ALEKSEM, Ye.P.j retsenzent
[Railroad surveying; reference and methodological hand-
book) Izvokantia zhaleznykh dorag; spravochnoe i matodi-
chaskoe rukovodstvo. Moskval Transport# 1964. 495 P.
(MrRA 18: 1)
1. Babushkin. Vseaoyusnyy.naacbiic-isaledovatellakly in-
stitut transportnogo stroitellstva. 2. Laningradskiy go-
sudarstiver,myy proyektno-izyskate1'skiy institut Gosudar-
stvennogo proizvodstvennogo komiteta po transportrLamu
stroitel'stvu SSSR (for Gonikberg, Engellke., Khrapkov).
3. Sibirskiy gosudarstvennyy proyektno-izyskatellskiy in-
stitut Gosudarstvennogo proizvodntve=ogo komitets. po
transportnomu stroitel'stvu SSSR (for Aleksayev, YeP.).
4. Moskovskiy gowidarstvemVy proyektno-izyskatellskiy
institut Gosudarstvernogo proizvadstvennogo komiteta po
transportnomu stroitallstvu SSM (for Allpert).

GORIMOV. Alakeandr TeeLl'yevLah, aauchnyy sotradnik; BUMER. Serafic
Alsksadrovich, nauahM notrudai1c; KALTATSUT, Boris
UrIllovich, nauchnyy gotradnik; YCRKAU Zdgar Artnravlah
nauchnyy isotrudnik; UTUMOT,
takhn.nauk, nauchnyy sotradnik; VASILOYRT, Tu.r.. red.izd-va;
ASTRIMA, G.A., taklared.
(Air levelling In surveying railroad lines: explorations of
mountaLuous aread AeronLvallroven.Le na ftyekantlakh pmtel
soobahchaniia: materialy LasledovaniL v goruol mestnosti,
Koskva, ltd-vo Akad.nauk SSSR, 1959o 272 pa (KIRA 13:3)
1. Chlea-korrespondent AN SSSR (for Gorinov). 2, Rulcovaditell
laboratoriL zhelasnodorozhaykh Lzyskanly Teasoymmago nauchno-
Lealedovatel'skago, Inatituta transportnogo stroltel'stya (TaN116)
Kintransstroys SM, (for Butler), 3. Laborstoriya thelecuadoroshnykh
izyekaaly Taosoyusnogo nsuahno-Lealedovatellskogo Instituta transport-
nogo strottelletva (TaNIIS) Kintranestroys S= (for all except To-
sL11yev, Astaflyeva).
(Aerial photogramwtry) (Railroads-Surveying)

i_-; :,- ~ - I --. -1 1 -
SIKIN, S.M., kandidat takhnicheskikh nauic: IURXO!, T.T., inihener.
Structural characteristics of the SI:-54 warp-knitttog amchine.
Log. prom. 27 no-1:34-37 J& '57. (WRA 10: 2 )
(Germany, Iket-Warping machines)

NORMU. Sa.
...... -.-
The AChT-l carding and knitting machine. Bial. tekh. ekon. inforo.
no.9:59-61 '59. (MIRA 13:3)
Ornitting machines)

ROWAN,, frantisok,, dr.
The now crialml codes. Ca spole 7 no.3:=-23 Kr 162o

NORMA-If, Frantisak, dr.
w
nis Econmic Code. Cs spole 10 n3.2:24-25 Ap f65.

-MMUN, frantisek, dre
A new regulation of the scononde arbitration. Cs spole 8
no.2:1-2 Ap !63, -
X4
11

NORMAN, Frantizek, dr. (Bratislava)
on thI3 new civil Code. Cs spoje 9 no.3:25-27 Je '64.

NOPUMAH, Frantisek, dr.
The new Civil Code. Gs spoje 9 no. 2:22-24 Ap 164.

:1, , ;'. ."! I !, " . 14, ~.- .
* ~ . , .. 1~ I . , ?~
I h p ri ~, q " ~~ v i I ~ 0 ~~ ! "? C, j , 9 n ,.; . -~ I : f ,- , -
I . W 0:3 t, 5 1 a " ii k i A Re?, b) r, I ~ ~~ , --, ,,, it, n aj n 't t~ ! ~ *,, I , n A!, fn i r i - " r f t '.', i t,! i -

NORM, Frantteek, dr,
. The new Civil Cods. Cs spoje 9 no.6,30-32 D 164,.

VAITSHTM, L. As g NORM e 0. JL
Wcul&tiv4g the cross sections of photolonization. of alm-lim
and gaMum atom* Opt. L spektre 6 no.2:149~451 Ir 660,
(KIRA 13:10)
(Ionization) (Al-manux) (WILUM)

6888U
0/051/00/906(0210011036
EFO 9591
AUTHORS. LO&A and.
-,ITLE. Calculation of the rasa-sections of
Aluminlum and Galli.qm Atoms
PERIODICAL: Q tik spel~troqkapiyaj 1960, Vol 8, Ur 2,
pp NT -alx5l (USSR)
ABSTRACT: The photo-,ionization cross-sectlon of an atom is Siven
by:
ZW2 2 F 2
-ao, a WF~,(Ordrl (1)
411
.0
where % is the Bahr radius; VMtt g3,L- and Pj,(r)
arq, respectively, the energy, statistical weight and the
radial, function of an optical electron in the initial stati,,
of the atom; the radial function of the final state
P9t(rl # is normalized to 6(c - Cli . The energy is s~ i-,.-
Cardl/5 irx Hydberg units and the other quantities mWe given in

68880
S/051/6o/oo8/o2/00l/036
Calculation of the Photo-iontzation CroF121/401-Holas of Aluminium and
Gallium Atoms
atomic units. The multiplin~v Q dopends only on the
orbital.and spin quantum nu~liersj in the cas *e of a single
electron. outside a filled shell QL4L = 2 max (1-1.)
To find the radial function of continuous spectrum
P.&I the authors used Seaton0s "quantum defect" expression
(Refs 2.3) for the case c 4,< W2 1
P.L(r) A(c, Z)(u.j (Ocos "ILZ W ~ v.,t(r)sin IWIL, (c)
2 2
A
'where ua(r) and v,L(r) are linearly independent
solutions of the Schr8dinger equation with a cioulomb field
I pl(c) is the quantum aumber defect extrapolated
Card2/5 r

68U0
1,2
Calculation of the Photo-ionization Cro W21/eIRIons of Aluminium and
Gallium Atoms
to optical electron states with positive energies.
For states with negative energies we have
TA = a - X K 1 (3) .
nt nixt naL - -?-Zxt
The functions u. and v. (r) were expanded as
Vr)
15 eries of Bessel4s functions of the first and second
type (Eqs 4-6). The calculated values of uct(r) and
v t(r) are tabulated for t = 2 apd, for t from
0 to O*L (Tables 1, 2). Using Tables I and 2 and the
published values of the self-consistent field functions for
the ground state (Refs 4,5), the photo-ionization cross-
sections of A.1 and Ga atoms were calculated. For both
Card3/5 atoms I for the ground state. Trial calculations

68880
S/051/60loo8/02/001/036
CaicuLation, of the Photo-ionization Cross!6206141991 of Aluminium and
Gallium Atoms
showed that, of the two possiblo values l
only t = 2 contributes appreciably to the cross-
section. The cross-sections obtained In this way
((r x 1018 cm2) are plotted as functions of the energy
(0 of the electrom removed (in Rydberg units) in a
figure. on p 149. In the case of Al the cross-section
decreases almost linearly with the energy
(Cf = 30 x 10-18 cm 2 at C = 0 and cr:'.X 4 x 10-18 cm2
at c = 0*12 Rydberg units). In the case of Cza the
cross-section falls more rapidly with energy (from
ar = 6 x lo`ta cm 2 at c = 0) reaching zero at
v = 0.08 Rydberg units; then the cross-section l8f Qff
risen with the energy, reaching d =K 0.6 x 10- cm at
c = 0#12 Hydberg units. This shows that, in spite of the
similarity of the external shells of Al and Ga, the
Card4/5 energy dependences of the photo-ionization cross-sections

68880
S/051/60/008/02/001/036
Calculation at the Photo-Lonization H2214%Utionu of Aluminiuat and
Gallium Atoms
of these two. atoms differ very considerably.
Unfortunately, the calculated values could not be compared
with the experlmental ones because no empirical values
are yet available for these atoms. Acknowledgment is
made to L,M. Biberman for his advice. There are
I figure, 2 tables and 5 references, 5 of which are
English, I & translation from English into Russian an
I Qerman.
SUBHITTED t June 20, 1959
Card5/5

S/051/60/008/04,/001/32
ZZ01/1691
on the Calculation of Photo-IouLtation Absorption
wLtIL ions. (Imparison of the expressions derived by the authors
with the exporiaeftal, data of Boldt (WO 6, 7) is given in Figs 2 and 3.
In these figures curves I represent the measured absolute emissivity
of am burning in pure oxygen (Fig 2) or pure aftrogen (Fig 3) at
pressures of I rtu.j the arc temperatures wore 10 600-13 0000K. if
the effect of fomtLon of negative ions and free-free electron
transitions are allowed for, the corrected antasivities are 60-701e lower
than those gLven by curves I in Leigs 2 and S. The corrected onlagLvities
agree better with the authors' calculations (curves 3 in Fige 2 and 5)'
than with 9=41d's values (curves Z' and 20). There are 3 figures
and 6 reforeaces, 2 of which are Inglish azA 6 Geman.
SUACITUDs July 1, 1959
U A 2 /Z

OILIOVAS I.V.1 MORMANg G,E.
Decrecae of potential of eleotran dstaaiment from nagati've
ions in a plasm-. Toplofis, vys. tesp, 2 tio.41517-52A
ji-Ag 164. (KMA 17:9)
1. Moskovskly onergetichaskiy institut i Mauohno-Issledovatell-
skly institut vysokikh texperatur.

BIBERMLM, LA; NOW P.~.; ULIYANOVI K.K.
Calculation of phatoionizatioa aboorption in atomic gases, Opt.
i spektr. 10 no.5t565--569 Yq 161. KM 2-4:8)
(Photoeleetricity)

s/o5z/62/012/003/002/016
EO32/E3i4
AUTHOR: Norman, G.E.
TITLE: Justification of the quantum-dafect method
PERIODICAL: Optika i spektroskopiya, v. 12, no- 3, 1962,
333 - 337
TEXT: It is pointed out thattl-equantum-defect method (QDM)
put fonirard by.Seaton (Ref. I - Monthly Notices Roy. Astron.
Soc-, 118, 04', 1958) cannot be regarded as rigorously justified.
In Seaton's method, the asymptotic beh2viour of the wave function
of an electron with positive energy k is characterized by a
phase 6(k 2). Seaton ,s2theory is criticized on the grounds that
his expression for 0(k ),which enters into the radial part,of J
the wave function, is taken by; analogy with a discrete spectrume
whereas it is not obvious why this should be so. Secondly, it
is not immediately obvious why the possibility of extrapolation of
11(E) follows from the possible extrapolation of O(E) and,
thirdly, Seaton bases his theory on Ham's results (Ref. 3 -
Solid State Physics (ed. F. Seitz, D. Turnbull), v.1, Academic
Card 1/3

s/on/62/012/003/001/M6
Justification of .... E032/E314
Press, N.Y., 1955), whereas Ham did not succeed in proving that
ji(E) could be extrapolated to A ow. energies. The author repoLrts
an attempt atajustification of the QDM in the present note. In
distinction to Seaton's approach, the problem is treated from the
point of view of the general theory of physical scattering. Use
is made of the effective-radius~ theory (ERT) and it is pointed out
that this theorylva not as yet been applied to the Coulomb field.
Transition from the continuous spectrtun to the discrete is
carried out with the aid of a substitution put forward by Landau
and Smorodinskiy (Ref. 9 - zhnF, 14, 269, 1944; j. Phys. ussn,
8, 154, 1944). The ERT method ~.s used to determine the phase of
the electron wave function as a function of energy for an electron
located in the field of a positive ion. Expressions are derived
for the bound states of an electron in an atom, i.e. a single
theory is constructed which is capable of treating both free and
bound states and thereby a relation is obtained between the
b(k2 ) and the effective quantum number n" , which define the
corresponding wave functions. The results are said to constitute
Card 2/3

S/051/62/012/003/001/016
Justification of .... E032/9314
a rigorous justification of the QDH which turns out to be a
simple consequence of the general theory of elastic scattering
by a centre of force. Acknowledgments are expressed to
L.M. Biberman who directed this work.
There is 1 figure.
SUBMITTED: January 30, 1961
Card 3/3

BIMMWO LN.; VOROB9UTp V,$.; XORW, G.Z,
Shergy exitted by an equilibrim plasm In spectral Unes Opt, L spektr,
14 no -3:330.-339 Mr 163. ZKM l6c4)
(PI--- Cronined gases)) (Hydrogen-Spectra)

MORmf'Gelle
I --- I
rr**-:f-re* o2satron transitions in the ton fi*'Id. Opt. i mpektr,
14 no.4t521-526 lp t63* .(PM 16:6)
(ions) (Quanum theory) 1~

L 98h7-61 BDS
AGUEMISMI NR.' AP30W575 S/O()51/63/()7 V005/0593/0597
AUTHOR: ,Sorman~ G. E.
r-photoionization of low-lying states and the
TITLE: Cross sections To
oscillator strengths of some line3 of ceYbon and nitrogen a:toms
SOURCE: Optika I spe".xoskopiya., vo 14, Y1.0. 5, 1963, 593-597
TPPIC: TMS 1hothionization Cross see- ion oscillator strengths, C, N
7
--A-WTRACT.,~- The- cross- sections- fqr~photoioniozation_fl~= tv). low-lying, states
of ciitbon: and of- nitrogen were - ialculated by the- method proposed, by Burgess and
Seatom- (Mori tic-es--ROYAL Aifton.___SOc.*_ 120, -121,; 1960)j usiziZValues found
Vith the aid of tablezi publishe*iL by these authors. The Btxrgess-Seaton method
-was chosen ovins to,Jts siiuplic itty and. reliability. . 'The calculated cross
-.5ectiona-eve plotted.- There-vi(re allo calculated,the oscillator- strengths
associated'vith:nine lines In -ihe- spe~:tva of -ea4h of -theise atow, corresponding
to transitionz -to the ground dj~Lte and low-lying sUites, The computed f-values

Apobuiau4m-- I -A
Card

ACCESSIOK URt "4009121 6/0056/63/045/006/1970/1977
AUTHOM Riborman, re. Kor'Normanf G. K.
TITLEt SewiempiricaL method for calculating the crown section for
the elastic scattering of slow electrons by atams,
SOURCZt Zhurnal. eksper. L teoret. fLzikip v. 4S, no. 6. 1963. 1970-
1977
TO?XC TAGSt electron atom elastic,scattering, slow, electron scat-
tering, scattering length, effective scattering ranget quantum do-
'feate isoelectronic extrapolation, elastic scattering, cross section,
electron argon sc4ttering, electron neon scattering, Ramsauer effect
ABSTRACT: rn view of the relatively scanty published data on elaa-
tic scattering of slow electrons by atoms, and in view of the felt
need for semiampLrLcal methods by which to calculate this scatter-
ing, the authors propose a method in which thescattering length and
1/3

AccEsszom uR.- AP4009121,
the effectLVe,r&nq0 Of electron 01afftic acattering from a neutral
atom can be determined-by isoetectronic extrapolation in terms of
the quantum defect of the electron in the ion fields. The method
is based essentially on the quantum-defect method proposed by Beaton
(C. R., garist v. 240, 131.7, L955) and the extrapolation is carried
out not with respect to 'Z but with respect to model potential para.-
meters which are chosen to correspond to experimentally known quan-
tum defects. By way of an example, the cross sections are deter-
mined for the elastic scattering of electrons by argon and neon
atoms at energies up to~ eV. The results obtained are in satis-
factory agreement with the available datat for exampLee-the gcatter-6'
ing Length was found to~be negative for a;gon and positive for
neon, in correspofiderice-with the fact that the Ramsauer effect is
observed for argon and not for neon, in spite of the fact that 'the
cross sections of argon and-neort turn out to be almost the same.
II:n conclusion we are indebted to A. Xh. 14nateakanyan and A. K.
Starostin,for many interesting discussions.*O Orig. art. hast 4
CGCd 2/3

MUM
ACCESSION URt AP400912L
figures, 14 formulas, and 2 tables.
ASSOCTAMOITt MoskovskLy energoUcheskLy Ln&tLtut (F-becow Powex-
Engineering rnatitute:)~
SUBMITTEDc 31~4ayO 'DATE ACQ; 02rob64 EKCLC 00
SUB CODEc PH NO REr GOW 004 OTHERt 026-
Cod 3/3

ACCESSION HR: AP4041567 S/0293/64/002/003/0441/0454
AUTHOR: BLberman, L. M.; Voroblyev, V. S.; Norman, G.E.; Yakubov, 1. T.
TITLE: Radiation heatLng In the case of hypersonLc flow
SOURCEt Kosml,cheskiye issledovaniya, v. 2. no. 3. 1964, 441-454
TOPIC TAGS: radiation heating, hypersonic flow, shock wave, aero-
dynamic heating. blunt body% boundary layer
ABSTRACT: The problem of the heating of a blunt body by shock-wave
radiation In the case of hypersonic flow (velocfties~-8 km/sec) is
examined with particular attention given to the case of heating
caused by flow under conditions where the gas is almost completely
dissociated following a density jump. General expressions are given
to compute the radiant fluxes. The main elementary radiation proc-
esses Involved In the determination of the plasiaa formed after the
density jump are analyzed. Methods of computing the contribution
of the Individual radiation proceises to the radiating capacity of
the air are presented. The radiation In the continuous spectrum
and In the entire aggregate of spectral lines is considered. Compu-
Card 1/X.7~7

ACCESSION MR: AP4041567
tatLons indicate that: 1) there is a broad interval of temperatures$
prsasures, and thicknesses of the radiating loyer in which the lines
make the major contribution to the energy emitted by the plasma, 2)
the total energy of a large number of weak lines, computed integrally,
with a growth of optical-densLty may noticeably increase the contribu-
tion of the individually commuted strong lines. and 3) in addition to
the visible lines, the lines in the ultraviolet may also play an im-
portant role. Computations were also made of the coefficients of
absorption and the degree of air darkening in the pressure interval
p - 0.001-100 atm and for temperatures to 20.OOOK. The values of
the flow parameters at which the radiant heat flux may exceed the
convective flow and caruse aerodynamic heating are found. The state
of the gas behind the shock wave ftont is discussed. The causes
for the departure from a state of equilibrium and the regions of
relaxation and quasL-statLonary LaequLILbrLum are analyzed. The
main processes determining the structure of the LnequLlibrium zone
at high flow velocities are explained. Orig. 'art. has: 5 formulas
and 3 figures.
ASSOCIATION:. none
Card 2/,V;~

M
ACCESSION N4:- AP4043002 S/OGSI/64/017/002/0176/OL79
AUTHORt Mormane G. E.
''TITLE: On the role of the negative nitrogen ion in the formation
of the conti:nuous spectrum of anitrogen and an air plasma
SOURCSS Optika L spektroakopLya. v. V. no. 2, 1964, 176-179
1 TOPIC TAGSc plasma charged particle, plasma concentrations plassa
spectral line, plans&. radiation, nitrogen, ion equilibrium
1ABSTRACTa Since little attention has been paid to this question so
f r,~the author estimates the cross section for photodetachment frCM
N , the role of N in the formation of the continuous spectrum from,
_plasmas, and the range of pressures and tempera-
nitrogen and air
tures at whiph U has a significant effect. The required binding
energy of N',Ls calculated by iso-electronic extrapolation an the
basis; of the- results of B. Edlen (J. Chem. Phys. va 33# 98. 1.960).
card 2/4

ACCUSZON ffi~s AP4043002
3
It in shown-~by indirect evidence *7
that the ground state P of t
ion to not ;ealized, and that the excited states 0 and a result
11 from the sticking of an electron to the excited states of t Is n trar-
gen atom anAIare metastable. The dominating ion is in the D state
fl and ix thii only one considered in the estimates. The photodotach- it
I
ment cross sections obtained forithe 0.75 and 1.7 eV levels of
Ur
10716
D), -are L.2. x and 4 x 107L CM2 respectivetr. Catcutatiahs'
of the relative absorption coefficient an a function of the tempera-
ture indicate a major role for the N ion, and show agreement with
the data obtained by G. Soldt (Zo. Phys. v. 154, 330t 19S9) at LOSOOKe
but tliere are too many unaccounted-for factors *(lifetimes of the
11 states of N * auto-ionization, deviations of concentration iron
equilibrium) for definite conclusions without additional experL;
ments~ "I aft grateful to L. 14. Biberman and X# To Yakubov.for so-
ful discussions*" Orig. art, hams 2 figureso
Card..

11 1
I
I
T .
i !
I
- I..,.. ... ... I ~. I

ACCESSION M AP4043003 0/0051/64/017/002/0180/0188
AUTHORSs Voroblyev, V. S.; Norman, G. E.
TITLEt Energy radiated by an equilibrium plasma in spactral lines#
X1.
SOURCEt Optika. i spektroakopiya, v. 17, no. 2, 1964, 180-188
TOPIC TAGgs plasma radiation, plasma spectral line, nitrogen,
oscillator strength, line broadening, continuous spectrum, line
spectrum
ABSTRACT: The method developed by the authors previously (with L. M.;
Diberman, Opt. i spektr. v. 14, 330, 1963) for the calculation of
line radiation energy is extended from a hydrogen plasma to include
a plasma of arbitrary composition. Account is taken of the specific
difficulties arising in connection with individual complex atoms,
such as differences in oscillator strengths, in the broadening
Card

ACCESSION U99 AP4043003
mechanism and in the values of the line half-widths, in the multi-
plet level structures, and in the overlap of certain series. The
specific broadening mechanisms of different lines of complex atoms
and ions are'taken into account, and expressions are derived for
the integral~contributions of aggregates of weak lines. The influ-
ence of the continuous spectrum is estimated. The calculation
method is illustrated with nitrogen plasma as an example for which
energy balances are calculated for several pressures and optical
thicknesses. It is shown that the results obtained.for nitrogen
i. are general enough to cast light on the relative role of iiiUvidual
proceijses. "in conclusion we thank L. 14. Biberman for interest in
the work and,for a discussion of the results. We are also ~jrateful
to 1. T. Yakubov for useful remarks." Orig., art* hast 1 figure, 10
formulas, and 2 tables*
ASSOCIATION: None
Card

L 1
com
0 M ON027637 cg 8 MVW%/65/(a9/005/06n./0661
AUTEORS Normanp Q E*
I none
TITL31 ',,Us@ of the C6ul" a2proximation In calculating the probability of
transitions (hpor presented gLt the L9nWilium on the-Intecalty and V~Prm of
Snmotral Une Contours hold In Kmngarsk on June 26 - July 27f 19"1
SOMOZ OpUka I spektroskopiya, ve 19, no#, 5p 1965j, 657-661
TOPIGTAGSs speotroscopyp spectral 33,n9,, oscillation, calculation
ABSTRACT i k. disawsim vas held on the, applicability -of the Couloib app-olimation
In th'O form aq*al,6pe4 by D. 9-0 Bataajp A., Damgmard (Ehil, Trans* Roy* Scoot
i Uadonp V.42p 101v- 1949)p and M. J,. Seaton ftnthly Notices Roy. Astrone SOOOP
'the probability of transitions from the
n8p 5"0 1958) far oaloulating
Istate with eQuivalent electrons, An inaccuracv of' #k o4-1-

*W
I au I M1kTj On conlivration
WMA __ror t4e-urmr state, AM one
call
VDG i-539ol82
'-ACC NR. AP6029,776 SOURCE CODE: uR/oz94j66jQG4fGG4/Q473/O419
I
AUTHORt Kobzav, Go A -Morman. G. E,t Seryakovp K, 1.
i OMMW-- -
ORG: Hoscow Power Engineering Institute (HoskbvskLy ener
instLtu-t-7; High Temperature Scientific ResTarch Institute
I
,Lssiodovatel'skLy LnstLtut vysokikh temperatur)
?ticherkty
Hauchno-
TITLEt Determination of photoionLzation cross sections from the oscil-
lator strengths of spectral lines
SOURCEt Teploflztka vysokLkh temperaturg v@ 49 not 4s 19669 473-479
TO#C TAGSs oscillator strength, photoionLzation, phototonlz&tLon
cra,se section, spectral line IletAwm-Arzoed rooss !7pCjrj0)
A3STRACT: It is pointed out that the photoionLzation cross section In
othe prethrashold region can be calculated by extrapolation, itess by
extrapolating a smooth curve drawn through the points representing the
oscillator strengths for a group of lines of a spectral serLeso Uaing
this mathod the authors calculated the cross sections for photoiouLza-
tLon from the ground state of At, Ga, In, and Sr. It is pointed out
that when both the cross sections for photoLoaLzatLon and oscillator
strengths have been measured, the correspondence between the cross
sections and the density of oscillator strengths can be used to deter-
3
Card

ACC NRt AP6029770
mine the accuracy of the experimental results. Using the available
experimental data* it has been established that under conditions such
as occur in plasma (shLfeLng of the threshold) the cross sections for
photoLonLxatLon extend toward the long-wavelength region past the ideal
threshold frequency. When enough data on oscillator strengths are
available, the present method of calculating the cross sections for
photoLonLzatLon Ln the prethreshold region In more reliable than the
Burgess-Seaton methods OrLmo art* has: 5 figures. ICS)
SUB COM 20/ SUBH DATEs
19Jul65/ ORIG REFt 016/ OTH RM 031
h S

51066160/000100410041004AX
A053/AO29
AUTHORt 9 ~E~~~neer
TITLEt Now Method. of Manufacturing Bimetal Tube Gratings for Heat
Exchanging Apparatus
PERIODICALt Kholodiltwa tokhnika, 1960, ITO. 4, PP. 47-49
TEXTt The article describes a. new method of manufacturing bimetal
tube gratings, developed bjr the Krasnodarskir kompressornyr zavol (Krasao-
or -mm. steel sheet.
dar Compress . Plant). The grating is out to size froma, 40
On one aide of the circular plate a recess is sut which is T3 mm smaller in
diameter than the plate. Taking into account allowance for shrinkage of the
copper the mechanical machining of the recess is about 19 mm &esp. No tube
holes are drilled in the grating which for the process of bimetallization,
is given, the form of a. smooth disk with a, recess to be filled with copper.
A. boiling hot solution of borax (50 g borax per 100 g water) is then applied
by brush to the interior surface of the disk. After drringt a 2 mm. lay-er
of powder@& borax is spread out and oeverecl with a lid made of healproof
steel. The disk thus prepared is placed. into & gas oven and heated. to
Card 1/2

EXCMM ::EDICA.' See.14 Vol.U/7 Radiology Jul 57.
t L91. NORMAN Kh. K. Inst, of Exp. and Clin. Med.. Acad. of Scl. of the Estonian
jli7-4;1nvesttga; ion of the intensity of the red cells
SSR. Ta n t
phGsphGrus exchange by means of radioactive isotopes
in cases of th (Russian text) VESTN. RENTGENOL. RADIOL.
1956. 3 (3-61 Illus. 3
Eighteen cases of pulmonary tb, and 3T cases of tb meningitis were investigated.
together with a control group of 5a normal Individuals. Radioactive phosphorus
(P3zj was used as art indicator. The amount of inorganic phosphorus absorbed by
erythrocytes In certain conditions wag taken air An index of the Intensity of the
phosphorus exchange.,It is known that in physiological conditions one million of
erythrocytes can Absorb T.5-16.7% of phosphorus. This falls to 5.9-9% during art
exacerbation of a severe pulmonary th or tb meningitis. and again approaches
normal values when the clinical condition improves. When treatment with strepto-
mycin and (sonfazid is effective this figure also approaches. normal values parl-
pasatt with clinical Improvement. It was proved on normal animals that atrepto-
mycin and Isoniazid by themselves do not induct any, changes in phosphorus meta.-
bQ1Istn.,pf_the red cells. Nevskaya - Moscow

AUTKCR*, Worn
TITLE: Pne"atia Regulators he Tallix&4 ftatory (Pnevastiaheakiye
regulystory Tallinekogo, zaroda)
PERIODI M: Priborostroyenlye, 1958, Wr 8, pp. 24 -27 (USSR)
LBSTRACT: -The factory IM at Talliuk.- has since 1951 been developing
and producing a number of patumatic regulators which have
alrsady~been in use on a large scale especially in the Soviet
canned fish industry and in the tobacco fermentation industry.
Three different types are described-in detail. Their data are:
Denomination M. PR W-11
Range of temperature regulation
In 00 40-140 15-65 40-200
Range of regulation of relative
moisture in % - 98 -
Recording errors and errors
in temperature regulation in OG + 1 + 1 + 2
Kaximm durs~tion of a cycle
Card 1/2 'cif regulation In hours 20 268 24

BOV/ii9-58-8-11/16
Fasumatio It"rulators of the TallinAL.Yaotory
Denomination FPS,- PR 993-.
Value of division of disk diagram:
for temperature In oC 1 0#5 2
for time in minutes 15 ISO 15
pressure of couprossel air
in kg/OU2:
up to the reducer 2-5 2-5 2-5
bojond the reducer 1"1 101 iti
air consumption in Nn5/h
(approximately) 2 2 1
food voltage in T 12 220 220
required output In U 26 10 14
length of capillary in a 10 12 15
dimensions of the apparatus in mm, 155-05 540.460. 4270.406.
.540 .200 185
weight of apparatus with
reducer in-kg 35 45 27
There are 9 figures and 2 tables.
1. Pneumatic apparatus-EquipnEmt 2. Pneumatic apparatus-Per-
formance 3. Temperature-Control 4. R
Card 2/2 pldity--Control

KALMU,~ F4P., k&nd.Uk"=dc,- HOMO, ",Lnzh.
Tochm] gy of mo=rsaturing bimtanio pipe grmt~.cz for sea-
,goirg venaels. Sudostroanis 27 no.9.-61-62 S 161. (HM 24: U)
(Heat exchangers) (Ketal cladding)

KARTINSIDN, M.N.; NOW5, K.Kh.,- ZALISFATA, Ttt.K,.
I-- --.. --- ... ''.
Embarb leaves as a nutritional source of vitamin 0. Tep.plt. IS
no.5t82-83 S-0 159. (KM 13: 1)
1. Is kafedry bioTchimli (wave - prof,doktor med.nauk 1. Yoxtinsou)
Tartuakage osudarstyanuo o =1versitata.
I Chanel
(TITAKIN (; chow.)

LMIN. D . f__K - GOLUBET, B.; SOROKIN, K*; KAKSIKOT, K.; ALEKSAMOT.
4 LOR-M. S I MT ~ - 0
9 --TAICISOT
. r. . . A.; rILICHM. A.; SATSLOYET. V.
Representatives of the people. Mast.ugl. 7 no.4:3-7 Ap 158.
(Russia_-Politics and governmeat--3icgraphies) (MIRA 11:4)

Comparative evaluation of various methods of 1==Jz&t'j'on
with typhoid fever vaccine. Zhur.nikrobiol., epid. i
Imn, 42 no,12t44-48 D 165.
(KM 19t1)
1. Voyeana-meditsinakaya ordena Lemina akademiya Iment
Kirova.

37929
3_q,,77oo
S/1si/62/d04/PO5/017/055
B125/B104
AU'MORSs Dir, Go L., I ~~,E_and Pikus, Go Ye.
TITLE: Galvanomagnetic effects in sewiconductors with degenerate
bands
PIA.,10DICALt Fizika tverdogo tela, v- 4, no- 5* 1962, 1180 - 1195
TEXT:. The more precise theory of galvanomagnetic effects in p-type Ge
semiconductors presented here furnishes substantial corrections to the
numerical values of the galvanomagnetic constants and explains the depea-
dence of the Hall constant on the magnetic field observed experineatally.
Allow for the influx of carriers from other bands*involves "crossed relax&-'.
tion times", changes the distribution function of light holes more than
that of heavy ones, and likewise changes the contribution of the various
types of carriers to the kinetic coefficients. Owing to the small con-
tribution of light holes to the electrical conductivity, the effects due to'
light and heavy holes make about the same contributions. The relaxation
times of lonGitudinal vibrations.for are given by
Card 1/5

S/ 10 116 2/004/005/017105 5
Galvanomagnotic effects in ... B1257BI04
0 -lip,
DI
1 4 (2.14)
-q 0 .0.
2 2
vi th -9/a and _tW - '1/'2- Here, a and b are the constants of the
deformation potential, m 1 and m 2 are the effective masses of light and heavy
i
holes', respectively with tj 4 0 and small values of the relaxation time
)a
V22 of heavy holes will always be a little shorter than the relaxation tine,
of light holes. In the case of scattering by acoustic vibrations of
J
the lattice at [-->O, the inverse relaxation times are given by
Card 2/5

5/18 1,,'62/004/005/01 T/055
Galvanomagnotic effects in B125/BI04
3C2
I
f
Tit .1111, T, I-I I
47 C12-
---i T'=V
4. Crt
Tin" TIn I
[4 (1 -'q) -4- 3-q cc'
r
1, and "2 2may differ considerably. ~"22 reaches a maximum at In:0-75-
Using the transition probabilities for scattering inside and between the
bands one obtains the relaxation times
Card 3/5

5/isi/62/004/005/017/055
Galvanomagnetic eff'ects in ... B12)/B104
(3-7) and,
1-+-! 2 (3-8) kith
TS(T)= '21 3, (3-9)
(1 1,30 (,-*O)z 2
for rcatterine from ionized impurities. In (3-7) 1 ij and 1+(x "%Mien
In the case Y,2IL2 A eK1, rhich is important in practice, is reduced~
m i
2 1 e4%jV f 91de
toOP) - InOmE/k )-5/2. v-(
In (3-12)
holds for a Gimple band if k2ff/4 M *6 1 - Heavy holes make the greatest
contribution to the electrical conductivity. The contribution of light
holes z,.mounts to rr /r of the share of heavy holes, viz. 361jS at
11 22
11 ' 722 for Ot and 21/j' for 0-75c,4. For 0, the hole mobility
Car(I 4/5 -------

3/isl,,'62/004/005/017/055
Galvanomagnetic effects in B125/B104
calculated with the aid of the present theory is twice that obtained by
'Who simple theory. In the case of weak fields and for rL - 0 and 0-75,~
i
the con6ributions of heavy holes are 26 and 64,;, respectively, and increase
with increasing maGnetic field strength. At 800 K and a concentration of
centers of about 10 13CM-3, scattering from impurities is negligible. The
calculations are to be continued. AveraCe values for the constants of the.
deformation notential are ;,7iven in an appendix. There are 6'figures and
1 *%-,able. The most important English-language reference is: C. Herringo
E. VoCt. Phys. Rev., 101, 944, 1956.
ASSOCIATION: Inatitut polupro-odnikov All SSSR, Leningrad (Institute of
.Semiconductors AS USSR, Leningrad).
Institut fiziki i matematiki AN Lit. SSR, Vilfnyus (Institute
of Physics and !:.athematice AS Litovskaya SSR, Villnyus)
SUP"TITTED. December 23, 1961
Card 5/5

Ithin
S/184 AC2 004/010/008/065
AUTHORS: Mormantasl E., and Pikus, Go Ye.
TITIE: Thernomagnetic effects in semiconductors with degenerate bande
PERIODICAL: Fizika tverdogo tela, v. 4, no. 10,-1962, 2692-2707
TEXT: The thermomagnetic coefficients in p~-type semiconductors with
degenerate bands are calculated on the basis of the exact theory of carrier
scattering (Go L. Bir, Go Ye. Pikus. FTT, 2, 2281, 1960). In this way it
is possible to consider band-to-band transitions and their effect upon
entrainaent and relaxation processes. For easier calculation the
isoenergetio surfaces of light and heavy holes are approximated by certain
median spheres, the constants b and d or the deformation potential are
replaced by their mean values, and the crystal Is assumed to be elastically
isotropic with the constant.o 440 Scattering of phonons from holes is
taken to be negligible. Results: the thermo-e. i. f. a, the Narnst-
Ettinghausen coefficient Q# and the change of the thermo-ea m. f.t Ap., in
a magnetic field consist of two partso one of waich is due only to
Card i/fp

Thdrmomagnetic effects in
3/181/62/004/010/008/063
BIOS/BI86
interaction of the carriers with the equilibrium ph9none (superscript p) and
the other only to the entraincent (supersoript ph).-7 The hole parts of the
ooeffiolents have the form
.P (2
(7) )11
3% kau2 I LOW9 - LOAM
III t(AM12 h (AM121
14-13
ZMAM ~,LMAQ)
The oubscripts.'i,and 2 refer to light and heavy holes, respectively. The
Parts of the.coefficients due to longitudinal phonons are
Card 2/5

Thernonagnetio effects in ...
8/181/62/004/010/008/063
Bioa[3186
MIF40= vj- Gm Cj
2 -611- --Or t . 1.
C AMB(?" - -L P, AOBM
4
ir, I(AM111 - -I!- ?j (0421
4
VIAM BOW)
4
and the total phonon parts are
(16)
(17)
Card 3/5

5/161/62/004/010/008/063
Thermomagnetic effects in BIOS/BI86
a114 MPAM (25)
QF4=QF14fl 1-*-L2CA(H)
a; (26)
AaO= Alw0fl-i-22
a,
(27).
The quantities A, L, G, and B involve the relaxation times IV, Iand T.2
as well as e -k and Z are complicated functions of H. The
entraindent due t6 rknaverse phonons plays a minor.role and .can therefore
be neglecte Ing comparisons with experizental data (c. Herring.
Phys~ Rev., 959 954, 1954). There are 8 figures.
Card 4/5

Thernomagnetic effects In oeo
5/16IJ62/004/00/08/063
B108/B186
ASSOCIATION: Inatitut poluprovodnikov AN SSSR Leningrad (Inatitute of
Semiconductors AS USSR9 Leningrad); rnstitut fiziki I
matemattki AN Litovskoy SSR9 VI;lRyus (Institute of
Physics and Mathematics AS-LitovabWa SSR, Wilfayus)
SUBMITTED: 'April 28, 1962
Card 5/5

RASHKOVSKIY, S.; HOEMANTAS, E.; EVA, V.; CUDCUITE, M. [Oudonyte, M. I
In tho Department of Msyst co technical and FAthezarlcal Sciencea.
Trudy All Ut. SSR. Ser. B. no. 4023-228 t65 (HIRI 19 0

NORKASTAS9 F. K.:
NORKANTAS, P.K.t RTraining racing skiers in the younger classes under twilight am
nighttime illumination (in the basic training period(". Leningrad, 1955. State
Order of Lenin and Order of Labor Red Banner I 3t of Physical Culture imeni P. F.
Lesgart. (Dissertations for the Degree of Candidate of Pedagogical Sciences.)
So. Knizhnsys, letopi 1. No. 49, 3 December 1955. Hoscow.

NAZaOVp S.M.; KUGRKMV, U.K.; NORMTOV,, L
Cementing lov-temperat=o gas wells. Kaft, khoz. 42 no.7:26-28
Jl 16,4, (MIRA 17: 8)

alldol-PINAP G.G.; 11ORmATOV, A.;
velocity and absorpticn c'
Uolutions. Veot. 144sk. un. ser. 20 no. :,1-72
165. (,, 3.~: 3
1. YafEdru fiziclieskoy khitaii i Ijj)(~rtttoriya -m,-,Iekul.-,arn,,lY
ak-ustiki Mlosk o oblast-noito j,,eduFoglchef:llcg.0 instituta.
ovskog

-L 45804-66 Wr(1)/T/&fP(k) al
ACC NRsAR60233o6 SOURCE CODE: UR/0058/66/000/003/H071ACOYT2
AUTHOR: Y0rm&tQTLAi_!(dz rev V. F.; Belinski-y. B. A. (P ?
!L~ 15
TITLE; Investigation of the coefficient of absorntion and promAgation lre122LU of
'ultrasonle MMLA In the quaternary system acetic acid - etkILk acetate et~Xl ale
hol - weter
SOURI Ref zh. Mika, Abe. 3Zh499
REF. SOURCE: Tr. X-y Mezhvuz. nauchn. konferentsti n primenenlyu malekul. akust. k
isaled. veshchestva I v-nar.--kh-ve. Tashkent, 1964, 161-164
TOPIC TAGS: ultrasonic velocity, ultrasound absorption, aqueous solution, absorption
coefficient, temperature dependence, acetic acid, frequency characteristic, relexa-
tion process
ABSTRACT: An investigation was made of the coefficient of absorption and the velo-W
city of ultrasound in a system consisting of acetic acid (T9.2%), ethyl acetate (00%
ethyl alcohol (200, end 1 - 80% water added. The component liquids were subjected
to chemical purification. The accuracy of measurement of the absorption coefflcle~t
'was from 5 to 2% at frequencies 5 -- 85 Mae, that of the velocity was 0.3%, and that
1/2

ACC NR, AR6023306
of the temperature OAC. Relaxation absorption vas observed In the mixtures regardr,
less of the nature of the relarAtion processes in the components. The absorption 14
mixtures with 23% water Increases with temperature. At frequency 4t 20 Kcs, the abs6r.
ption os ultrasound In the mixtures does not depend on the vater concentration (at'10
-- 50% water). A minimum of the temperature dependence of the coefficient of absolt-
ion is observed at 80% water concentration. At large water concentrations, the fre!Y
quency dependence of the coefficient of absorption and the velocity of ultrasound 11z'
the mixture are determined by the behavior of the acetic acid - water mixture. Th4
relaxation parameters and the velocity of ultrasound are given for different water 0
concentrations at 20C. The~frequency of the relaxation does not depend on the con-~
centration of the water within the limits of experimental error. L. Marcy. [Tran-
slation of abstract)
SUB CODE: 20
2/2

AID P - 4921
Subject USSR/Electronics
Card 1/1 Pub. 89 - 5/17
Authors : Raudsepp, Yu. and Normet, A.
Title : Radio receiver "ESTOMIYA"
Periodical Radio, 7. 21-259 Jl 1956
Abstract The authors describe in detail a new superheterodyne
receiver of the "ESTONIYA" type produced by the Tallin
Factory "PUNANE REV of the Ministry of the Radio
Engineering Industry. The receiver has 12 vacuum
submiftaftre-tubes. A detailed connection diagram and
several components are explained at length. Seven dia-
grams and drawings, 2 tables of specifications.
Institution None
Submitted No date

r-- NORW$g V.A.
CaordLnatioa of w3rk in the field of electric ~fttarso Pribaroatrosuls
jwg4s29 jl~ t63- (KEEL 16t4)
(11*4tric =tars)

A.
Cotton Baling
Expanding the standard dimensions of baling areas. Milopkovadstvo no. 4, 1952
0
9. VOnthl List of Russian Accessions, Library of Congress, Aueust 1952. RM, Uncl.

Tawnwo Y."
hasibility of exPanding the sintering Interval of loose brick
da-Ing firlugo Vay, iddso shur, nueltBO45 162. (KIRA 14: 1)
1, Bradneasiatakly politakhnicheskiy institut I Inxtitut khtaii
AN NOR.
(pric") Mesa)

NMUMEELMMOV, U.; TADZHIM, F.O.
Effect of calolcm cartaints, on the FbPl=mx*d=U'Ja &'rvPcrtlm
at a c4acined U104d crack* V&b.khim.%h=. ao.479-4 f6l-
(KIRL, 14-.8)
1, rustitut khimii AN VxSSR.
Ovareat products)

proCadsor, dektor takhnichaskikh aauk, xasluzhauj7
dLeyatelf nauki E takhatlet; ITAKOY. profeasor. daktor
tak#alcbL*aktkh nauk; FEZ=, A.T., doictor takhnichaskEkh nauk;
RAZVKOVSXI'r, U.N.. daktor takhnichbakikh nauk; DKIMUM. A.5..
dot eat, Imadidat tekhnichaskilch nauk;'Agug"r- R-r-- dotseat,
kaudid4t tekhaichaskl1rh cauk; BASMIN. A.T.. dotsent, knudidat
takh4tchegkikh vAuk-. KAKOTWV, V.T*,* datesat, kandidat telfticha...
ek1kh amak; RTZHOT# P.I., dotseat, ksadtdat takhaichaskikh :zamk:
MUTIRKAMs, A.G., imadidst takhatchaskikh nsmk-. URTSMUOT, T.D.,
kandidst takhatchesicikh nauk
On the article qlavelopmeat of amtomstic control aad telesechanice
in the fifth ftys.-year p1se. Ayton. t telem- 15 ELO.1.78-79 .14-]F
154" (KIRA 10
1. leatagradekty olsktrotakhatcheskly instlUtt in.
Ionina.
(Automstio control) (Ramots control)

MoffAXOT, K.K.; SCUMBUT Sa.. ratecaeut; SMRS. P.L.. rodaktor;
S--=
TO=OKI 110he-slav r*d&IL-tor
[Selection of electric motors for powered deck machinery] Irybor
sUktrolviotalat p4aabuykh slektroprtrodar. Ionalacmd, rsd-wo,
'#Korskoi transportO 1955. 267 P. (KM 9:7)
(Ileatric motors)

o Kqj -5, 'j,
LUMAKIN" A.Tw.: BATID, V#T., kandetakhn.nauk; BOLDYM, G.L., Wk.
MRINSIrr, R.I., kand.tolrau.nauk. (tots.; ROSM. re.l.. insh.
Comparing tho static and druslo characteristics of two " three-
stage longitudinal field rotary amplUlers. Ilelctrichestva no.12:
24-26 D r57, (KIRA 10:12)
'L
I,Lsul'T adsicly olaktrotakftnicheekly Institut im, Ultyanom
(zentua, 2.Chlen-korreepandent AN WE (for Alakzgeysv).
(Ilectric generators)

-3mrp. S-r- land. ~skhn. nauk; RLTKO, T.r.0, I=d* teldme neak;
BAKOIATKITI. G,X,, land.takhn. rAuk; rM9MM, P.T., Insh.
1C. ~
Sal4atigg alrault parameters for auto=tla coutral, windings of (deoral
electric propulsion eqlmipmnt. . ikdoatroania 2Z Ci.,a.23] no.latza-31
0 157. (K=k 110)
(Kartuo dieset sagines) (Ihip propulaton, Ilectria)

No.RNIEVSK . Boris Ivanovich; TAUTMT. Iyan Afanas Oyevich.-I WJR&TOT. 1.1. 0
end.;
[Electric power plants and networks
chaukle stantsti, L eett. Lenivgred.
1958. 76,7 P. , 1. 1 1." *
(Zlectricity an ships)
for ships] Suda"s alaktri-
led-vo "Rechnot .tma4port,"
~ CNIRA 11:12)

AUTHORS: Nornevskiy, B. I., Docent, Candidate of Technical 105-58-3--".131
._9c_1_0~nces,BaYko, V. F., Candidate of Technical
Sciences, Uallsheyakly, V. Ye., Candidate of Technical
Sciences, Kuropatkin, P. V., Ehgineer, Rosin, Ye. I.?
T IT L N., 00!fm"rinon nf No- and Throe-St.Ve
Rototrols (Srayneniye dvukh- i trokhatupenchatykh
alek-truwavainnykh usiliteley s prodolInym polem)
PERIODICAL: Elektrichestvo, 1958, Nr 3, PP. 9-14 (USSR)
ABSTRACT: In recent time a series of works with the three-stage
amplifier with longitudinal field were carried out in the
laboratories of LETI, LVIMU and LIMT. The results of these
investigations are given here. At first the operation
principle of the three-etage amplifier is given and by the
ex=ple of a fourpole machine it in shown, how the
amplification stages are formed in a three-stage amplifier.
In the second part a comparative evaluation between the
three-stage amplifier with longitudinal field and a two-stage
Card 1/3 amplifier in carried out. On the strength of the given

Comvarison of Twn- and rhrec_S~.aec Ro4 tj~ojs
U0 105- 58-17-2/31
experimental data it is shown that in the case of one and the
same maGneto sjotemt of approximately equal weight of the
effective materials, of one and the same S - and i y- the
velocity increase of the electromotive force at the output
of the three-stage amplifier is higher by the two- to 2,5 fold
than in the case of a two-stage amplifier, 6 is the
compensation degree of the armature reaction by the
compensating current 1 24 between the brushes 2-4 in the
amplifier armature. On the other hand, the three-stage
amplifiers in comparison to the two-stage amplifier are more
inclined toward fluctuations and toward self-excitatica which
is due to the increase of the total amplification factor and
the phase lagging. The three-stage amplifier has a somewhat
simpler system compared to the two-stage amplifier,
Comprisingly it is said that the three-stage amplifier in the
case of one and the same control output Is more quickly
effective compared to the two-stage amplifier and that in
the case of one and the same quick effect the three-stage
Card 2/3 amplifier is controlled by a lower putput.

Comparison of Two- and Three-Stage Matotrols 105-59-3- 2131
There'are 8 fieures and 7 references, 4 of which are Soviet
ASSOCIATION: Leningradskiy elektrotekhnioheskiy institut imeni Ullyanova
Lenina)
Leningrad Inatitute of Electrical Engineering imeni Ullyanov
Lenin))
~
SUBMITTED: May 21, 1957
Card 3/5

NGP,NEV~Kly 0. 1.
A.UXSiW. A.Te.,prof.; RLTXO,
tekhn.nauk, datg.; XATMOT# T-N-,In9h,; TUDIAL, r.3F.vlnzl2.
Selecting paraaeters for two-stage longitudinal field rotating
amplifiers. Sbor.LIIZHr no.159:207-M 158. (KML 12:2)
1, Chlen--korrespondent AN SM (for kleksayev).
(Rotatinc amplifiers)

ALVEMUT, A*To.,prof.; BLT1O# T*rv,kMn11,tekhn.nAuk-. BOMYW, G.D-.inzh.;
NCBIWSUT,,,Bvl.,pkwd.,tekhn.nauk, late.; ROSIN, Te.1.9inzho;
--Cffdftt&. tekhn.nauk, date.
Internal feedbacks In tuatistage amplifiers with varicne numbers
of terminal pairs. SboreLIrZEM ne.159:232-235 158o
(MM& 12:2)
1. Chlen-korrespondent AN SSSM.(for Alakseyev)-
(Rotat Ing ampuf iers)

BXDIV, T.Va; MOMOV, Til.l.; HWLYMIU, Tu.B. - KIMYLOT. 7.A, -,
0,
golf-excited synchronous 6-andrators with direct phaue com-
pounding. Blul.tokh.-akan. inform. no.5t48-50 659s
(KIRA 12: 8)
(Slactric &saerators)

AUTHORS: Bedin, T.T., Kaks1mov,,Ttx.I., F4gineers. G1lerov1c12,TmjE.,
Student, Nornevskly,,B.1 Candidate of Technical Saieaoes.
ITLE: Improvements to the Static Characteristics of Synchronous
Alternators with Compounded Self-exoitatioa.
PERIODICAL: Vestaik elektropromyshleanosti 1959, Nr 8, pp 42-46
(USSR)
ABSTRA.CT: For power and high-frequenay supplies, extensive use is now
being made of low-output synchronous alternators with
compounded self-excitation derived from metal rectifiers.
Thl 's article compares the static and dynamic characteri-
stics of an alternator type 04-7 230 Vs 200 als, 14 kVAp
using the excitation circuit of S.B*Yuditskiy and a new
cirouit developed by the Leningrad Eleotro-Technioal
Institute imeni Lenin. Yuditskiy's circuit Is given in
Fig 1 and it will be seen that the metal rectifiers that
provide the excitation are supplied from a three-winding
transformer. There are two primary windings,, one connected
in parallel with the generator terminals and the second in
series with the load. The voltage winding is separated
Card 1/4 from the secondary and current windings by a magnetic shunt.

SOV/110-59-8-10/24
Improvements to the Static Characteristics of Synchronous
Alterudtors with Compounded Self-exaLtation,
The external characteristics of a synchronous generator
with this method of excitation are plotted in dotted lines
In Fig 2, which shows that the voltage variation is about
! 6% Y&ea the load is raised from zero to rated value and
when the power factor alters from unity to Oe3. Fig 3
shows an osaillogrem of the current and the generator
terminal voltage when rated load at 0*3 power factor Is
suddenly applied; the greatest voltage-drop is about 22%,
and rated voltage is restored in less than 0.1 asoonds.
with this circuit a remaneat voltage of the order of 20 to
25% of the rated value is necessary to ensure reliable
self-exaLtation, and so the rotor must be made of special
steel of high ooeroivity, The osoillograms In Figs 4a and b
show the process of self-excitatioa under various conditions
of remanent, voltage. Table I gives values of generator
remanent voltage at which self-exoLtation occurs, and it
will be seen that if the remanent, voltage Is leas than
10 to 15% of rated voltage the generator does not excite.
Card 2/4

SOY/110-59-8-10/21-
Improvements to the Static Characteristius of Synchronous
Alternators with Compounded Self-excitation,
More reliable excitation may be obtained by altering the
position of the magnetic shunt, but this has disadvantages.
This defect of the system of excitation may be overcome
by the improved excitation circuit shown in fig 5. It
differs from the previous circuit in having a capacitance
connected in series with the voltage winding and in having
no magnetic shunt. Because of the capacitance, self-
excitation occurs with a remanent voltage of the order of
1% of the rated value. Consequently, this circuit does
not entail the use of special steel in the rotor. The
oscillograms of Figs 6 to 8 display the process of self-
excitation for various values of remaneat voltage and sho-a
that the generator fails to excite only if the remanent
voltage is less than 1%. A method of design has been
derived by which the circuit conditions may be adapted to
suit the available remanent voltage. Characteristics of
some stabilising transformers designed for different
values of remaneat voltage are given in Table Z. The
presence of capacitance in the circuit of the summating
Card 3/4

SOT/110-59-8-10/24
Improvements to the Static Characteristics of Synchronous
Alternators with Compounded Self-excitation,
transformer also improves the regulation at heavy load and
low Power-factor. The bold lines in Fig 2 show the
external characteristics of a synchronous generator type
ChS-7; the circuit of the excitation system is given in
Fig 5. When the load is altered from zero to fall load
and the power factor from unity to 0.3$ the voltage
variations do not exceed 1 5%. Fig 9 shows.aa osaillogram
illustrating the sudden application of 10ep load at 093
power factor. It will be seea that the voltage drop was
2?.% aad that voltage was restored to the rated value in.
about 0,02 seconds. The characteristics of the systems
investigated, their weights and dimensions, are given in
Table 3 and indicate that both the original and new voltage
regulators are of approximately the same weight and
dimensions. There are .9 figures and 3 tables.
SUEMITTED: February 25, 1959.
Card 4/4

/v 0 917 v
inzh.; MMLTMINp
'rlm.B,,,,Anzh.; KIXHAYWV, V.A.. kand.tekhn.nauk; X)RMMKI'r. B.I.. Icand.
takhti.nauk
System of self-excltation and compounding for cynchronous generators
uss4 on ships. Sudostroenle 25 no.1:56-62 Ja 159. WHA 12:3)
1. Chlen korrespandent, AN SSSR (for klekseyaw)*
(Ilectric glinerators) (liectricity on ships)

VASIWTU, D.V.; HINWWVp V-Ae; NCMVSK3Xj,_B.1 WWKOt O.P.j,
_t; DL
otarobiy naucbmy7 Botr.,-,, VaT.--t-WFm. uauk.,, retaenzowt;
MUFJSOVp I#I*# dato.p kwA# tekhu. nau?., retseumtj
REYNGOLtDp Yu.k.r kand. tekba. mauk.. dots*.# retamseat;
BAYKDt V.1?.p kand. tekhnnaukp dote.,, nauebrqy red.; KMINL,,
Te.V., red.; KRYAKOVA, D.M*, tekbno redo
(Automatic control oystem for ships] Sudovye &vtorAtisirovwt-
vqe ustenatki. TAningradp Gos. soiusnos izd-.vo sudastroit. pro-
myeblep 19610 595 p0 (KERL' 15:2)
(Marine engineering) (Automatic control)

FEDIN, Vladimir Tasillyevich; ILYASOV, Viktor Andreyevich;
MUSMOV, rarly Ivanovich; HERUMIN, rurir
Borigoviah; IAIKHAYLOV, Vladimir Aleksandrovich;
MORNEVSKIY, Boris Ivanovich; YEVSEYEV, V.I., red.
(Automatic control of mar1ne Wchronous generators;
systems of direct compounding; static conditions] Avto-
matizatsila sudovykh sinkhronnykh generatorov; sistemy
priamogo kompaundirovanlia: statichesicie rethimy: Ucheb-
noe posobie pa kursu "Elektroenergetichaskie ustanovki
sudov." Leningrad, Leningr. elektrotakhn. in-t im. V.1.
Ollianova (Lenina), 1962. 91 p. (MIRA 16:10)
(Electricity on ships) (Automatic control)

XON07ALOV, H., LM02.; MaJOPAAk P - 1.
kand.tekhnnAak; HaRMSMEY,
prof.; NIKEL16HPURG, I.r Insho; GEMMMU iniv.-
,J%tomatic regulation of vdtagG and the distAbution o! loads
during the parallel operation, of suspended ship generators.
Nor. flot 23 no.21t27-30 N 63, (MIRA 16:12).
1. Loningrads vyss 6y~ inzhefternoye morskoye uchdilihcha Lhi.
admiraU Makarovao