SCIENTIFIC ABSTRACT LUNKIEWICZ, W.W. - LUNTER, S.G.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001030910004-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 13, 2001
• Sequence Number: 4
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

LUNKIEI,TICZ, W. W.
LUNKIEWICZP W. W. Ziemia we wszechswiecie (The Earth in the Universe). Warszawaj,
1949, P. 79.

LUNKIN, A. V.
Lunkin, A. V.- "C'a'rp in the central Vol -a (the Tatar Reoublic) and economical methods
for its -,sell, Trudy Tatar, otd-niya Vsesoyuz. nauch.-issled. in-ta ozerno-rech. ryb.
khoz-va, Issue 4, DO, P. 103-24, - Bibliog: 27 iteims.
SO: U-41101 17 July 53, (Letopis 17-hurnal Inykh Statey, No. 19, 19h9).

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I., raze4bbt ka - rJ s tej;t, avtdma t I ches kago. reguilrovanlya. s peremennoy strukturoy (148 t e-~
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, excellent re
processes wl t4 I nterdependent parameters
the changet,,Iiri"irotitro-1:~ignals, which are required by the static chisracterfsttcs~
-of th r-ol-led-object.- are only of suffic.1-ent rrAgnltude to compensate for the
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t -'-ja tMa article, the Idea Is extended to the design of an Integral -4
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f th --t---
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for maxlmum-pert~Urbatlon, the regulator compensates accurately for this per-turba--
tion tn one-cycle of the slave mechanism. All perturbations which are smaller
than themaximum require two or three cycles of the stave mechanism for compensa
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ASSOCIAVO Gosuda'r'stVenny* t tttut tsvetn *kh matallov, Moscow (State
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PETYAKSHEV, I.; LUNKIN, P.; REPINg I.[deceased]; YEGOROV, V., red.
[Rural builder) S&I'skii stroitell. Saransk, Mordovskoe
knizhnoe izd-vo, 1964. 46 p. (MIRA 17:10)
1. Starshiy proizvoditell rabot KovyWnskay mzhkolkhoznoy
stroitellnoy organizataii "Avangard", Mordovskaya, reopublika
(for Petyakshev). 2. Zamestitell prodsedatelya kolkhoza.
"Sovetskaya Rossiya" Krasnoslobodskogo proizvodstvemogo
-upravleni-ya Mordovskoy respubliki (for Lunkin). 3. Nacha-Ilnik
tsekha zhelezobetonrWkh konstruktsiy Ru2ayevskoy mezhkolkhoz-
noy stroitellnoy organizatsi$ Mordovskoy respubliki (for
Repin).

VASILITHY, Y.Y.; TBRICSHCHMIKO, N.P.; prinimal uchastiyel UJNIKIN. S.P.
~--
qualitative chemical somimicroanalysis. Part 3: Detection of
chloride ions in the reactions of the formation of Chronyl
chloride. Uch.xap.LGU no.272:153-161 '59. (MIRA 13:1)
(Chromyl chloride) (Chlorine-Analysio)

L 31006-66 EWP(e)/tWT(m)/M4P(t) IJP(c) JD/JGAal
ACC NRs AP6010449 SOURCE CODE: UR/0368/66/004/00~,-fo-24-S76-25
AUTHOR: Mokeyeva, G. A.; Lunlkin, S. P.; Feofilov, P. P. a
ORG: none
TITLE: Luminescence of praseodymium In silicate glasses 1~
SOURCE: Zhurnal prikladnoy spektrookopii, v. 4, no. 3, 1966, 245-251
TOPIC TAGS: praseodymium, ytterbium, luminescence spectrum, silicate glass, low tem-
perature effect
ABSTRACT* Data are g-*ven from a study of spectrally luminescent characteristics of
silicate glasses activated by praseodymium ions. The trivalent praseodymium cation
has two 4f electrons and a comparatively small number of singlet (ISO, IG4, ID2, 1166)
and triplet (3H, 3F, 3P) levels. Absorption and luminescence of crystals and glasses
activated by praseodymium are*detexmined by forbidden transitions between these levels
The absorption spectra of the glasses were studied in the spectral region below IV us-
ing an SF-4 spectrophotometer, and in the region of longer waves on the automatic SV-
-50 spectrophotometer made by the Shimadzu Comp~ny. The luminescence spectra were re-
corded on installations with diffri6i1E'ii6C_c;d7rciators and FEU-38 photomultipliers,
a cooled FEU-22 photomultiplier and a cooled lead sulfide photoresistor. Electronic
EPPV-60-3H and PS1-02 potentiometers were used for recording the spectra. The lumi-
UDC: 535.37
Card 1/2

ACC NRt AP6010449
nescence excitation source was generally a mercury lamp with a 436 my glass filter.
A diffraction monochromator was used for excitation in some cases. The luminescence
lifetime was measured either with a pulsed tau-meter in combination with a diffractiol
monochromator to isolate certain sections of the luminescence spectrum, or by an ul-
tratau-meter and a set of light filters. The first method gave the best s3ectral re-
solution while the second gave the highest accuracy for determination of T . Absorp-
tion and luminescence.spectra are given for glass containing 0.2% Pr2O3. The experi-
mental data show a high probability for nonradiative transitions from P levels to,
lower-lying states, particularly to the ID2 level which is the initial state for a
number of intense radiative transitions in the red region of the spectrum. When the
temperature is reduced to 770K, there Is a redistribution of intensities in the lumi-
nescence spectrum of trivalent praseodymium favoring the blue-green bands. It Is
shown that there is a nonradiative transfer of excitation energy between praseodymium
ions and between praseodymium and ytterbium ions which results in concentration quencl
ing of Pr luminescence in the first case and luminescence sensitization of Yb in the
second. Quenching due to nonradiative energy transfer from praseodymium to ytterbium
is less effective when the temperature Is reduced to 770K which may be due to a reduc-
tion in the overlapping of levels. Orig. art. has: 4 figures, 2 tables. 14
SUB CODE: 20/ SUBM DATE: 10Har65/ ORIG REF: 007/ OTH REF: 002
ATD PRESS: 4/-2 41/
2/2

T. I. LlInIkin? S
n on c
;kAdiCE cb!)I.":
T-fT P"Ca.,3111'el-ilclit of the spectral absorption of gla.-ser. colored with translition-metal
ions at increa.-.ed tumperAurcn
Cr
pti:~o-mcldianichcolmya promyshlenno.;tI, no. 8, 1966, 35-4o
PIC TAGS : Gil-*Lc,7-.to r
lass, boratc al;arn, ClArr. property, color additive, abrorption
6a-octrun, alozorption, tem.
peraturc depcndence
,~'STRACIP: I-- e purpose of the investigation wis to determine the character and causes
:Of ch'an'-es in -L-1-le ~Ibzzorption Lpectra of colorlr,-, ions in rlarsc-- at increased t-cr-,,)crO.-
,tV,I:Cs. Silic"c) borozlklicatc)* aluirmilicatc ', and phosphatc glasses ol- varying,,
ositions, with andwithout coloring ions, were tested. 51%e coloring ions used were
!Co'-, Cu -, Fc+2 and C17. %lie absorption spectra were measured in the visilble (-,xon
:1100 '60 750 nm), ultraviolet, and infrared regions at 20, 100, 300, and 1100C, execyt
the annealing temperature of the glass was lower than 4G-Oc, when the measurements
were made at 300C. The spectral absorption was also measured after the cooling of the
ple, to establish whether the chawe in the 3pectral absorption is reverrible. The
am
c:; in the abijorption
:xeL`U-!L;ation hilt; ~;hoifn that all glasnes exhibit- coaffion charwr
Ura, nam ely shift of the boundaries and of the max:Lma of the absorption bands toward
.the lonGer-wave region and smearing of the absorption bands. 7hese changes are re-
Card 1/2 uDc: 666-11: 535-34

L 1012:50-67
ACC NR` Al-60303:r3
versible in character provided the sample is not heated above the anneal'
U4,1 ter.7;era-
,ti,re. 'The changes are governed not by structural transformation but by in tensifi cation
of the thermal oscillations of the individual particles in the Glass. 'Llic smearing of
,tllic bands is under the influence of the coordination and valence transitions of the
~trancition-metal ions. The temperature shift can reach 20 - 50 wa for each 100C. It
is also concluded that the temperature variations of the spectral absorption of color-
ing ions can be used for the study of structural transformations in the glass. Orig.
,art. has: 5 figures.
~SUB~ CODE: DO SUBM DATE: 04jun66/ oRiG nEF: oo2/ oTH REF: ool
p~~d 2/2

ACCNI~_,01-b-0-3*1-5_0 SOURCE CODE: -UR/0368/66/oo5/oo6/o - 0/0734
AUTHOR: Mokeyeva, G. A.; Reysbakhrit, A. L.; LunIkins S. F.
ORG: none
TITLE: Nonradiative transfer of excitation energy between Yb", Nd3+, and Pr3l ions
in silica glass
SOURCE: Zhurnal prikladnOy Bpektroskopii, v. 5, no. 6, 1966, 730-734
TOPIC TAGS; excitation energy, ion energy, ion interaction %Y1,L10,47re. (944,-~*_"
ABSTRACT: An investigation was made ~f the transfer of excitation energy in silica
glass activated simultaneounly with two and three rare-earth ions, The investigatior,
of the interaction of Yb-Nd, Yb-Pr, and Nd-Pr ion pairs was based an the dependence,
of intensity and the duration of rare-earth ion luminescence on the concentration.
The pair interaction is rather complicated: the nonradiative energy transfer can
proceed in several ways and all three activators can serve as donors and acceptors
of excitation energy. In the case of the interaction of Yb-Nd pairs with the simul-
taneous activation of glasses-with Nd3t' and Yb 3+ ions, a sensitized luminesce.-Ice of
of ytterbium results from the nonradiative transfer of energy from neodymium ions in
the 4F 3/2 state to the unexcited ytterbium ions.' This leads to an attenuation of -the
intensity and to a shortening of the luminescence duration of neodymium. A reverse
enern transfer from ytterbium to neodymium, does not occur. In Yb-Pr the intcractfjon~;
of Yb + and Pr3+ ionB is of a dual nature. On the one hand, during excitation in the
Card 1/2 uDc: 666.11-01:535-37+535-34

4
-ACC-1~
absorption band of Pr3* ions a sensitized luminescence of Yb34* takes place. On the
other hand, conditions exist for the resonance transfer of excitation energy from I
Yb3"' to Pr3+- Thus, the praseodymium is simultaneously a sensitizer and a quencher_
for ytterbium luminescence. The quenching effect of praseodymium exceeds its sensi
tizing effect on,ytterbium. In Nd-Pr*a similar phenomenon takes place during
interaction of the activator pair Nd and Pr. The presence of Nd3+ ions provokes
quenching' of Pr3* lumineaccnee in bands which are bound with transitions from. the ID2
level. The praseodymium ions on their part render a strong quenching effect upon the
luminescence of neodymium. The authors thank P. P. Feofilov for 'his constant interesti -i,%,
and attention to the vork.and V. P. Kolobkov for useful discussions. Orig. art. has: 1,;
3 figures. (WA-141 (JAI
SUB CODE: 20/ SUBM DATE: 28Feb66/ OHIO REF: 003/ OTH REF, 003/

LUNIKIN, Yu.P. (Leningrad); POPOV, F.D. (Leningrad)
Effect of nonequilibrium dissociation on a supersonic flow
past blunt-nosed bodies. Zhur. vych. mat. i mat. fiz. 4
no.5:896-904 S-0 164. (MIRA 17:12)

SUBJECT USSR P_AYSICS CARD 1 2 PA - 1854
AUTHOR' LUNIKIN YU P. MISIN,G.I.
-F -
4 ' ~u_;m=ne
TITLE OFTre-V scence of the Front of a Shook Wave.
PERIODICAL Zurn.eksp i teor.fis,~1,fasc.6, 1105-1105 (1956)
Issued: ; / 1957
In the course of experiments carried out on a ballistic device a luminescence
of the front of the shook wave was observed in several gases (i.ECKEFUAAN,
R.SCHWARTZ, Phys.Rev., A.�I, 912 (1952) although the temperature behind the
shook wave in a multiatomic gas did not suffice for the excitation of
luminescence. The following hypothesis may serve to explain this phenomena:
on the occasion of a collision of the molecules on the front of the shook wave,
the energy of the direted motion goes over into the subordinated thermal
energy.' The computations carried out by C.ZENER (Phys-Rev-.a, 556 (1931))
showed that after about 10 collisions a MAXWELL velocity distribution of mole-
cules occurs, whereas the rotation- and oscillaticn degrees of freedom are
practically left without excitation ("frozen-in"). on this occasion the entire
energy goes over only to the degrees of motion of the progressing motion, and
the local temperature of a gas becomes much higher than the temperature of
the equilibrium established in the course of events.
After the.degrees of freedom of the progressing motion the electron levels and
the degrees of freedom of rotation are excited. According to the individual
properties of the molecules, at first the electron levels, and then the degrees

Zurn.eksp. i teor.fis,31,fase.6,1105-1105 (1956) CARD 2 / 2 PA - 1854
of freedom of rotation, or else both together can be excited. In either case
local temperature remains higher than equilibrium temperature. It is just by
this energy distribution which does not correspond to equilibrium, that the
observed-luminescence can be explained, overmore as it is the f r o n t of
the shook wave that is luminescent, where the degrees of freedom of oscilla-
tion are-not,yet excited in view of the fact, that for their excitation from
104 to 105 shocks are necessary.
Further excitation of the degrees of freedom of rotation and oscillation leads
to a decrease of gas temperature. which then tends towards equilibrium temper-
ature and to an extinction of the luminescence. The more rapidly the interior
degrees of freedom are excited on this occasion, the narrower will be the
zone of luminescence. In gases with multiatomic molecules the domain of lumi-
nescence will therefore be narrower than in monoatomic gases, where tempera-
ture drop is due only to a decrease of luminescence.
The above is,a translation of this short report.
INSTITUTION: Physical-Technical Institute of the Academy of Science in the
USSR.

AtTHOR: LUWKIN, Yu.P. (Leningrad) 40-5-1/20
TITLEi Boindary Layer Equations and Their Boundary Conditions in the
Case of Motion in a Weakly Thinned Gas for Supersonic Veloci-
ties (Uravneniya pogranichnogo sloya i granichwe usloviya k
nim v cluchaye dvizheniya v slabo razrezhennom 6aze so
sverkhzvukovymi skorostyami)-
PERIODICAL: Prikladnaya Mat.i Mekh.,19579vol.21)Nr 5,PP-597-605 (USSR)
ABSTRACT: In supersonic motions in great heights the free length of path
LM is comparable with the measurements L of the moving body.
Gases for which this occurs are denoted by the author as
"weakly thinned gases". The boundary layer equations are set
up in the weakly thinned gas according to Prandtl's method,
they differ, however, from the usual Frandtl equations by the
occurrence of higher derivatives in the velocities and in the
temperature; the pressure gradient in the direction of the nor-
mal is different from zero which is expressed by additional
terms. The boundary conditions for the derived equations are
derived according to the kinetic theory; these are generalized
conditions as they were set up for supersonic motions by
Maxwell and Smoluchove-ti. The limits of applicability of the
investigated equations are given with respect to the height
Card 1/2 as well as with respect to the velocity.

Boundary Layer Equations and Their Boundary Conditions in the 40-5-1/20
Case of Motion in a Weakly Thinned Gas for Supersonic Velocities.
The author thanks A.I. Gubanov for the suggestion for the
present paper.
There are no figures, no tables, and 11 references, 3 of
which are Slavic.
SUBMITTED: October 1, 1956
AVAILABLE: Library of Congress
Card 2/2

U N
AUTMRt MKIKINJU.Pe 57-6-19/36
TITIZ: OE tWIVA-Latua-sof Shook Waves. (0 strukture udarnykh
voln, Russlam)
PMODICALj Zhumal Tak"Fix., 19571 Val 27, Nr 6, pp 1276-1281
ABSTR&CTs By making use of the basic ideas of the hypothesis developed by
E.SERGER ("Weltra%ofahrt" - Nr 1, 4-9, 1954) the structure of the
shook wave Is here investigated. The following conclusions were
arrived ats
1.) The non-balanoed process in a shook wave can be invea tigated
if some zones# in which part of the molecule degrees of free-
clam a" in equMbrium and the other degreas of freedom are
"frozen inr are analyzed.
2.) Iu the excitation domain of the progressing degrees of free-
dam the gradient of the gas-parameters is at its '"21"Im-
3.) In a shook wave a domain with a thermal excitation and
ionization can exist at a temperature which ezoeeds equi-
librium temperature.
4.) The here mentioned method of a series approximation for the
purpose of determining the excitation oscillations. of dis-
sooiation. and of ionUation is auffioient3q slMla and
shown goc4 amvergence.
Card 1/2

AUTHOR Lun'kin Yu.F. 57-8-25/36
TITLE Gas Parameters at the Critical Point with Account of the Variable
Specific Eeat.
(Parametry gaza v kriticheskoy tochke a uchetom peremennoy teploy-
emkosti - Aussian)
PMIODICAL Zhar4al Tekhn.Fiz., 1957, Vol 27 , lir 81 PP 183o-1835 (U.S.S.1i.)
ABSTRACT There is no possibility to obtain analytic formulae for gas para-
meters if the variable specific heat cp is taken into account and
it is therefore necessary to apply numeral solutions. In T,1956 Vol
21, number 6 the author shows a hiethod for the consideration of
the dependence of the specific heat 0 on T and p as a consequen-
ce of oscillation excitation, dissociltion and ionization of the
gas on the occasion of its passage through an impact wave. This
method is also applied here. The following can be said on account
of the calculations: 1.- The taking into account of the variable
specific )feat leads to a drop of brake temperature and to an in-
crease of the density compared with the corresponding Talaes for
a constant specific heat. In the case of Mi-12 (ratio of the -ve-
locity of increasing gas flow and the velocity of sound) these va-
lues differ by almost look. 2, Change of brake pressure at thelex-
pense of variable specific heat in the case of Mi