SCIENTIFIC ABSTRACT PAVLOV, V. S. - PAVLOV, V. V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001239620018-9
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 3, 2017
• Document Release Date: August 1, 2000
• Sequence Number: 18
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

ACCESSION FIR: AP4017401 S/0183/64/0091OD2/023.4/OM
AUDIORs Krugly*kh, A. A,; Pavlov, V. S.; Ty*khins'IW*y, 0, P,
TITIS: Vapor pressure of solid yttrium
SOUROEs Ukrayinalky*y fiz3r*chrW*y zhurnal, v. 9o no. 2, 1964, 214-215
TOPIC TAGS: yttrium. yttrium vapor pressure, yttrium vapor, clausing
coefficient, evaporation rate. yttrium sublimation, high temperature
evaporation
AMTRACT: Values for the vapor pressure of yttrium, obtained by Nesmayanov
et. al. on two different ocoasions (Vestnik MGIJ, No. 2, 40, 1962; Izv. A. N.
USSR, Metallurg-iya i Toplivo, 5. 117, 1962) differed by an order of magnitude.
Ackerman and Rauch obtained yet another sot of values maBs-spootromatrically
Chem. Phys. 36 (2). L". 196_27 The authors measured the vapor pressure
of yttrium over the solid phase between 1100 w-A 1480C by observing vaporization
rates at each value of temperat;are in a vacuum. A cylindrical tantalum
Card 1/2

ACCESSMN NR: AP4017401
crucible held the material, and temperatures were wasural with an optical
pyromater. The results coincided with those of Ackerman w-A Rauch, and am
expressed by the relation:
185W
10gPMM,--
T
"The authors thank H.S. Rudenko and M. M. Matyushonko for their discussion
of the results." Orig. art. has one table. one graph and one formula.
ASSOCIATION: Fizy*ko-Tokhnichny*y Insty*tut AN URSR, Khar~ov
(Physico-Tachnical Institute, AN UaS;Z)
SUEM17= t Z5Jul63 DATE ACQ % 1%w,64 ENCLs 00
SUB CODE: CH, EL NO REF SOVs 00) OTHERt 001
Cord 2/2

A
1. 345010-65 EVIP
0AW., E*-(b)A'A'A(c)
Pro4/Pa-4/pu-4 lip(c) ~JD/JW/JG/At/W
AUTHOIU,~ Kr~glykh, A. A.; Alat TikhInskiy,
~shenk~oN.~N. , Pavlov
F.
TITLED- Certain properties of gadolinium-beryllide
~SOURCS, Zhur'.' ln
na khImit. v. 16, no. 1. 1965, 285-28'
,.:TOPIC TAGS- r-operty, lattice structure
gadolinium beryllide, physical p density,
~Jnicrofia'rdness', dissociatiorv, sublimt ion -heat, -iapor Dress
Su"
-v-h6-: fo&- *'ini -pro rties of GdBe lattice struc--
-paratnete-r a 10.27- density
re-- 10. 005y, 3,363 gm
/cm3;
-rni~r,,c,ph-sk~nLiss.--.-140okg/myn2. This- intermetallic compound dissoci&4ed ap-
n-- 4
0 0
preciably aboive.-IOSOC:--'the-rate-of-Be-e -apo waa-ha6aiiura- 11
ratio
t6~V-.. or,, the gressu dB
A- a~lq e-ove&
Le
ef
Tkifh t of"" -in this teiii
b
ea s bli on perature
C
7 ~-eifigq -was 816~ m6i._ Orig. art. has:4,equation, I figure and 2 tables.:
card

L 44305-66
ACC NR- AP6019841 SOURCE CODE: UR/0370/66/000/001/0190/0192
AUTHOR: Amononko, V. (Kharlkav); 14u '~~
V. S.
All A~.A. (Kharlkov); a ko
(Khar'kov); Ti (Khar'kov)
ORG: none
TITLE. Evaporation rate of berylliu during dissociation of cerium beryllide
411 /It V
SOURCE: AAN SSSR. Izvestiya. Metally, no. 1, 1966, 190-192
TOPIC TAGS: beryllium, vacuum sublimation, ceriw-n compound, vapor pressure
ABSTRACT: 'flie article presents the results of an investigation of die evaporation rate of Be
during the thermal dissociation of die internietallic compowid CeBe as well as of die effect
of the addition of a small amount (0. .1 wt. %) of Ce on die evaporabill?y of/Be. CuBe 13 wa s o b-
tained by the vacuum heating of a stoichiomeLric nii-xture of thepo-Wdcrs of C,~ an(] Ile at 1150'C
for 3 hr, while the Be-0.4% Ce alloy was obtained by direct vacuum melting,6f die inetalEi. 'ne
i subliniation rates of die Be-0.417r, Cc alloy and of the products of dissociation of Cclie,3 were
determined by the niethod of evaporation from a cylinch-ical L~Lntaluni crucible with 'i rcsiaual
gas pressure of -!~ 2-10-6 111m jlg in the vacuu-ni chamber. The temperature was measured with
Card 1/3 UDC: 669.725.4

ACC NR: AP6019841
the aid of an optical pyrometer correct W 5,,~. Weighing of the crucibles was carried (jut
correct to �0. 0001 gby the continuous method on scales Mthout violating die vacuu-m. The
sublimation rate of Be with 0. 4% Cc was nicasured in Lhe temperature range ()20-1160'(',-
for this temperature range the saturated vapor pressure of Be over die Be-O. 4k Ce alkly is
described by the equation: log P = 9. 35-17, OOO/T. As for the sublimation rates of the compo-
nents of the intermetallic compound CeBe III during its thermal dissociation in the tempera-
ture range 1050-1250*C, the roentgenograms of the condensates gathered following evaporation
of the compound at 1100 and 12500C lack the lines of Cc and CeBe 13; therefore, appreciable
dissociation occurs above 1050T and flic entire sublimated i-natter may be referred to Be. 'ne
saturated vapor pressure of Be over the CeBc 13 compound during the latter's thermai disso-
ciation may be described by the equation: log P . 10. 475-18s 990/T. I'lie findingS were utilized
to plot curves of the saturated vapor pressure of the compoundE; and their components
(Fig. 1). Orig. art. has; I figures, 2 tables, 2 formulas.
3/3

ACC NRs AP60198,11
Fig. 1. Vapor pressure (11, nini 11g) of Be as a
function of temperature for:
I - pure Be; 2 - over the compound
CeBe 13 during its thermal dissociation
3 - over the alloy Be-0. 4% Cc 1 4 - pure
Ce
is 67
4
SUB CODEW SUBM DATE: 25JuI&I/ ORIG REF: 006/ OTH REF: 001
3/3
Cord

BwT(M)1ZWA(d)/EW?(t) XJPW JD
Ar-(; MRSA SOURCE CODE: ttfi/0120/66/000/001/0211/02.12
0.,
I)AV
AUMOM Kovtun.-G. P-se KruRlykh, A. A.
khartkov (Fizlko-
ti
7t,
TX=&.,. Appij~atue for zone refining of refractor-y metals
-.iBWRCZ: l.tekbnlka skeper1lenta, no; 10. 1966m, 211-212
4TOPIC-VAOS: refractory metal.. electron beam meltingo metal zone re-
finlng,,~molybdenum, metal ceramic material
The authors describe an electron-beam Instrument with elec-
beam focusing., Intended for zone refining.of refractory metals.
Thi device engpioys three plane-parallel beams of electrons with radial
cathodes-and focusing electrodes (Fig. 1). The use of plane cathodes
instead of annular cathodes eliminates contamination of the cathodes,,
vents electric.
pre discharges..and prevents contamination of the refined
_11ample., The.febusing system for each'electron beam consists of plane
anode-and:.cathode electrodes*bent at.1350,. Tests with metal-cexwdc
..W Molybdenuim:-rods up to 10mm i,n diameter have shown that*the rods could
1/2 UM 58-553-ra

:,Card 2/2

PAVLOV, Von, kapitan 2-go range
- .
M~~Ivxtion security to the control of naval forcen. Mor. abor.
47 not 1, 19-2 5 36 1164. (MIRA 180)

nar OV
t~or of, r, - - r.
g(,7

V n-W/Epr(a
L: 16367 0/910(bY Pr,4 MD ga)/ASD/AFW
AF G(
~ACCESSION NR: A?4048866*- J3V/J_G_ T_j0Qj----
AUTHM Xovtun, ~G. __P Krugly%lkh, A-.-.A;; Pavlov, V. S.-
3u
TITLE- Vapor press_ jrelf gadolinium and dysprosium
SOURCE: Ukrayinslky*y tizy*cliny*y zhurnal,v9,. -no. 10, 1964, 1OD-109J
TOPIC TAGS.: dadolinium, dysprosiumvapor pressure, heat of sublimation,
entropy of sublimation
ABSTRACT. The pressure of gadolinium and dysprosium vapor was determined
-over the-temperature intervals of 1120-1310C and 850-1075C respectively, using
Knudsen.' s. e ffusion method, by the. difference of the, weight of the tanta'.1,urn effusion
cell before'and after the experiment. The followirg equations describe the results
obtained for Gd and Dy , respectively: log P12. 03 - 23705/7', and
mm Hg
log Pmm Hg ~ 0. 79- 158'25/T. The heats-of sublimation were calculatpd: 108. 5
and 72. 4kcAl/mole for Gd and Dy, respectively. The respective _entropi~-_sof
zublimation-eq al 42-- -0 und
e 0
u e. has: 2 tables, 1
1/2
Card

PAVLOV, V.S.
Smil boring tools. VAshinostrottell w.6:21 Je 160.
OaU 13: 8)
(metal cutting tools)

TSITSIASHVILI, Mikhail Yur'yevich;__EA.VL_QL Vladimir Senenovich;
SOKOIDVP . , red. Ju __v-a,---UVjt6MVA,
L. G. , red.; LAPI NA, Z. D
N.B., tekhn. red.
(Modern methods for the loading and unloading of unrefined
sugar in harbors]Sovremennye sposoby peregruzki eakhern-syrtsa
v portakh. Moskva, Izd-vo "Morskoi transport," 1962. 89 p.
(MIRA 16:2)
(Sugar-Transportation) (Cargo handling)

ACC HR& AP6025592 SOURCE-CODEt /0433/66/000/013/0024/00241
MEN'TOR: Pavlov, V. V.; Levin, 1. A.; Birnbaum, 0. E.
None
iTITLE: A unit for testing aircraft parts under conditions of artificial icing and
!rain. Clas's 17, No.. 183222
jSOURCE: Izobreteniya, prcoyshlennyye obraztsy, tovarnyye znaki, no. 13, 1966, 24
j--C TAGS: flight simulation, simulation test, test chamber, ice, rain
ABSTRACT: This Author's Certificate introduces a unit for testing aircraft parts
under conditions of artificial icing and rain. The unit contains a closed chamber
with a refrigeration assembly, a vater distributing unit, heaters and a control panel
with measuring and recording instruments. The chamber of this unit is equipped with
a horizontal frame for mounting test parts. This frame is rotated by an electric
:motor mounted in the center of the chamber to simplify design and set up flight aimu-
,lation by rotary motion,
L
j Card 1/2 uDc; 62.1,58

, ACC NR: AP602599~ 1,
I I

31926
S/102/61/000/006/003/004
a, 3 1/ a 3 -0 X) D299/D305
AUTHOR: _PavlQY_. Y. (Kyyiv)
TITLE: Pinding approximate solutions to nonlinear differen-
tial equations of transient processes
PERIODICAL: Avtomatyka, no. 6, 1961, 52-59
TEXT: The solution is considered of a second-order differential
equation having a nonlinear term which is not proportional to a
small parameter. A fomula is obtained which is a generalization of
the results obtained (by other authors) for the linearized expres-
sions
f X'~Lx q(a)x + t
q a Tdxj
dt 60 (2)
and f ~Lx) ~Lx + q(a) + kql(a) x (4)
(.x I dt dt
Card 1/,i~,

Finding approximate solutions
The nonlinear second-order equation
d 2X dx 2 x
+ 2,k - + k x X, 1-
dt2 dt dt)
31926
3/102/61/000/006/00--,;/004
D299/D305
(5)
is considered, where P is a nonlinear function. The coefficients in
the left-hand side of Eq. (5) satisfy the inequality
k 2 _ k2< 0
(6)
the linear part of the control system has filter property; hence
the solution of the nonlinear equation can be approximated by the
solution to the linear equation. The solution of the nonlinear equ-
ation is expressed in the form of trigonometric series. By setting
in Eq. (5) F z 0, one obtains the linear equation whose solution is
Card 21A(~

31926
3/102/61/000/006/003/004
Finding approximate solutions D299/D305
x = a Cos (7)
dx
a cosr - 6ja sin (8)
where
a = a0e-At, Ot + T, CJ= 1/7- 72, a,= const, const
After transformations, one obtains the solution of Eq. (5) in the
form
n
X xi (12)
Card 3/7'

31926
S/10 61/000/006/003/004
Finding approximate solutions ... D299YD305
and the approximate solution
n
X v )COST for Y(a i ot + T ii(-a 1) (13)
where v and 7 are determined from Eqs. (7) and (8) and expressions
for the Fourier coefficients. After introducing the amplitude func-
tions, one obtains
n )t
x ao(i_,)e
ti
cos(W(ai)t +Ti)
(16)
Card 4

S/ 1 OY9,170,00/006/003/004
Finding approximate solutions D299 305
(where A andco are given by expressions). The obtained formula
(16) permits constructing the transient process determined by Eq.
(5). The difference is noted between expression (16) and analogous
expressions for differential equations with a nonlinear term, pro-
portional to a small parameter. Formula (16) yields an expre3sion
for equivalent linearization of the nonlinear term, viz.
(x' q I (a) jx L q (a) + Ag I (a) a +
dt dt CA.) 0 )2
+ ql(a)~ I X~ (2i)
(. 2 toi
Formula (21 is a generalization of the equivalent-linearization
formulas (2~ and (4), obtained for a nonlinear term proportional
to a small parameter. Hence formulas (16) and (21) are general
formulas which permit an approximate analysis of nonlinear control
Card 5/--;rjz-

31 2
S/10 6 1 /J 0 0/ 0 0 O'S /0 () _3,/ 0 0 4
Finding approximate solutions ... D2997D!3.05
systems with both "large" and "small" nonlinearities. As an ex-
ample, the determination of the transient process in the system
shown in Fig. 2, is considered. A comparison of the accurac of
results obtained by using formula(21) instead of formula (4~,
shows a considerablelrin in accuracy, hence the conclusion that
formulas (16) and (2 yield greater accuracy in the study of non-
linear systems. There are 5 figures, 1 table and 4 Soviet-bloc re-
ferences.
SUBMITTED: July 8, 1960
Card 6/?/'
Y

S/o24/61/ooo/oo6/oo9/oi;)
E140/E335
AUTHM Pavlov, V.V, (Kiyev)
TITLE: Improved form of equivalent linearization of
essentially nonlinear circuits
PERIODICAL1 Akademiya nauk SSSR. Izvestiya~ OtdeleniYe
tekhnicheskikh nauk~ Energetika i avtomatika
no. 6, ig6i, 67 - 73
TEXT-. The asymptotic method of N.M..Krylov and N,,N.
Dogolyubov previously applied to the approximate solution of
nonlinear differential equations has been applied under the
assumption of slowly varying amplitude and phase. This has
permitted the examination of systems with weak nonlinearitie~;
In order to consider systems with strong nonlinearities, the
present author proposes to apply the method where the decreuient
and frequency, and not the amplitude and phase, are slowly
varying functions, while the amplitude can vary at a finitc
rate in dependence on the numerical value of the decrement.
This method is applied to obtain expressions for the equivaleni
linearization of an essentially nonlinear element in a total
Card 1/2

ov-c~ S/02Ij/G2/GGG/OG1/OO,.;/GI~'
00 (w ,, 1 '4 E140/Z435
I
A UTHOR P"llov, V.V. (:i)-ev)
TITLE: Sym!-etricai singl.~!-frecuency forced osciliat,()n..~' :.n
nonlinear automatic control syste!-,is
PI~RIVDiC.~L: Alcade::iiya nai_11~ SSSR. IZ,%reStiyl. Otcleleniye
tel~hnichcs',~ikh nztu!~. Energetika i avtoriatika.
no.1, 1962, 133-137
TI:IX7,. The article concerns an application of the author's
previous work (Ref.5: Izv. AN 5SSR. OTN, Energetii-La i avio:,ialilia,
no.6, 1961). The essence of the method is to give a second-Order
i.~:,.,nroN-in~~ on the Krylov-Bogolyubov formul.-t, i'~'en t!ie
.I online 'irity cannot be giver by a function proportional To tile
small pzIra!:;eter E . An assumption of the method, both in 1!,,e
classical Krylov-BoL;olyubov wor% and the present, is that Cie
linear portion of the systei-.i has filter properties. Then ti-,e
method given in Ref.5 can be applied to the type of proble.i,
described by the title, The defects of the Krylov-3ogolyul-ov fl,
method in essentially nonlinear systems appear most strongly at
the low-frequency end of the frequency characteristics of the
Card 1/2

S/02 1! /62/cc)c /cci I--
Syr-=.,zetrical sin.-le-frec-,,,:enc,, . . . El~-O/E'135
investi,;ated system. An exa.-.-,j-,.Ie is calculated showing iii
this region the ii:,,T-)roved method .-ives results inuchcloser to I)e
exact solution (independently obtained) than the ciassical
aprroximation. There are 6 figures.
SUBMITTZD: ,:ay 5, 1961
Ca r d 2 /21

S/102/62/00C/002/004/004
D201 /D302
AUTHOR: lavlov, ~r._4yev)
TITL'--'t Jynietrical f-,in(-.le-frequency forced oscillations
in non-linear a-utomatic control syptems
Anomati?a, no. 2, 1962, 75 - 75
TEXT: The author considers the problem of using (1)
(a) (q(a) 2 ~q` (a)~ 2
-1
F(x,px) q(a) + q'(a) + ~,_ TO + 2 j
as given by him earlier for analysin of forced sinrle-frequency os-
cillations in a system having a really non-linear element. Lot the
system be described by
q(p)x + F(x, px) - S(p) f (t), P 5 d (2)
dt
Card 112

S/1 02/6?/000/002/C)C)4/0(;I,
Symmetrical single-frequency ... D201ID502
where .,(p) and S(p) - rulynominlo of at-~y deFroe with refil coraltarit
coefficients, the dei;ree of ,,k'p) beine, hirher than that of S(p); f(t). ell.
B sinSIt. Since the linear part of such automatic control systems has
the properties of a filter, then in the first approximation t'ne solu-
tion for the steadj state forced oscillations may be Bought in the form
of X=A sin (~tt+y). By considerine the complementary function of Eq.(2)
ana by several subsequent transformations of Eq. (2) it is shown that
the difference between the exact expression for equivalent lineariza-
tion of the reaulting equation and the approximate expression aq (-iven
by Krylov and Bogolyubov for the linearization of the non-
linear element, consists of a single correcting term .6 q, which is a
function of R and A. An example of linearization shows that this cor-
rectine factor lies in the region of low frequencies and its magnitude
depends on the magnitude of linearization factors. There are 1 figure
and 5 Soviet-bloc references.
SUBMITTEDt March 3, 1961
Card 2/2

PAVLOV, V.V. (Kiyev)
Refined form of equivalent lineari2ation of essentially nonlinear
appmetrical links, AvtonAtyka 7 no.602-54 162. (MIRA 16il)
(Automatic control)

PAVLOV, V.V.
Nonlinear differential equations and dynamic
Avtomatyka 8 no -77 163. 7)
.3t76 jK[RA 1,.
(Differential equations) (Programming (Electronic computers))
(Auto.matia control)

PAVLOV, V.V. (Kiyev)
Sufficient conditions for the invariancy of nonlinear systems.
Avtomatyka 8 no.4:65-67 163. (MIRA l6alO)

PAVLOV. V.V. (Kiyev)
Realization of invariance cond-itiorls ir, rlcal-i,--tar al.' ~ -
syste,%i3. 8 no.5:75-77 '63. i

*'.';~ (.~'.iyev)
. rj,,,I.- and fi- - - - .,,, ~ *, - . " 2, - , t! -. ~ '. I .- I - 1 1 -,,-
t,ux.' q v '. om" Lv I- F, - r- , ~ -

PAVLOV. V.V. (n yell) ; RA Ki TK,
conditions In nor.1 ~,, f,a7
9 no.5.,70-72 104'

~CC-17WFA-M28937 SOURCE CODE.- UR/0000/85/000/000/0113/0124
a lov V.
AUTHOR. P
V
-ORG.-: Nope.,
em nvarianoe conditions in multi-dimenslowd nonlinear
ITLE. Some j*obl -a in realization of I
autoinatio'control systems
~~.SOURCE-. AN UkrSSR. Slozhnyye sistemy upravleniya (Complex control systems). Kiev,
Naukova,dumlm, 1965, 113-rA4
TOPIC TAGS.- nonlinear automatic control system, automatic control the0j, circuit design
ABSTRACT- The author considers the following ploblem which frequently arises In connecUon
:wilh the design of autDmatic control systems. The system shown in Fig. I has an unalterable
sectioii based on a multi-dimehstonal controlled element. A controller must be synthesized
for maintaining Invariance In some set of coordinates of the controlled element either with
respect to some class of disturbances or with respect to all other variables in the system.
It Is further required that the invarlance resulting from synthesis of this control system must
belong to the class of pbysically realizable Invariance. The author shows that this problem
may be solved by Increasing the number of degrees-of-freedom of the entire system made up
of ob)ect and -controller. A class of automatic control Systems Is considered which operate
on the divergence prInciple with behavior which can be described by a sXstem of ordered
equations. Formulas are derived proving the -requirement for a controner which assures
QW, ~Ltl-

.:, 1 1. 1 .I . I .I. I. . : ; , . : I
. . . .- - , I . . . , , I . I
. : . 1 3

~ Ar,. '. i . " . ( !* )
I I - ' n
:.: i ;ii --- or, I "T'_9 of 1 riv a r ~ a: and tii 'or! c-my I --I-
),-, nc,.2:,?9-k!!~ I ~, r
Ix:Itk 1~:6)

AL16 J4K1..
-A
SOURCE CODE: UR/ODDO/65/000/000/0125/01.1-1
AV.7WOR; -BW 3L 3L
TITLE: Conditions fbr-~Asdl
lute Invarlaneb and autonomy In multidimensional automatic control
.systems, which are deser'Ibed by differential equations with discontinuity In the second member
SOIMCE.-. AN LJkrSSR., S1ozhnyyjD sistem upravlenlya (Complex control systems). Kiev,
y
TOPIC VAGS: nonlinear automatic control system, automatic control theEX, differendal.
ABSTRACT: 7he author conside s problems associatedwith derivation and proof of necessary
and sufficient conditions. for -Invariance and autonoray In automatic control systems with a
-con siderable degree of nonlineirity. Considerably nonDnear automatic control ByBtema are
deft'nod as #on with differential etpmtions of the form
F).Qj X1 X, MQ) 0 n-
OF OF OW s4 OIF
f
CtwJ:' 112,

L 20974-M W(d)/ZfP(.V)/E7t.TP(k)/LW(h)/W(I)
ACCESSION NR-. APSM886. UR/0280/65/000/002/0153/0156
AUTHOR: Pavlov, IV. V. (Xiev)
-no
inear automatic
TITLE:, Invarlancy1and autonomy I multivariable essentially nl
systems
SOURCE: AN-555RO Izvestiya. Tekhnicheskaya: kibernetika, no. 2, 1965, 153-156
TOPIC TAGS. multivariable control system. automatic control, automatic control
designLVsutomitic control. system, automatic control theory
....'ABSTRACT: Tiw.n'e essary and sufficient conditions of absolute invariance are
C
Ovail by:
~F' L
NJ) V\jj#) for all C We,
rM
for allf-a-M.
They are valid for automatic -control systems deicribable by the canonic sets of
equations:
t rArd 1/2
7-1

1-024 5_-61 EW I d ) INE ( V I I AW-F-WIP&A
6018017 SOURCE CODE: UR/0102/66/000/003/0015/0023
I AVMR: Pavlov, V. V. (Kiev); Melyeshev, A. M. -- Heleshey, A. M. (Kiev)
ORG: fio~e
TITLE: Compensation of perturbations and autonomy of infinite-dimensional systems
SOURCE: Avtomatyka, no. 3, 1966, 15-23
TOPIC TAGS: automatic control theory, computer simulation, analog computer, auto-
matic control system Iq
ABSTRACT: The authors study the problem of synthesizing control systems which
would insure autonomy and invariance of a finite number of degress of freedom for
infinite-dimensional objects. An ordered system of equations is given for an in-
finite-dimension%l object treated as a finite-dimensional controller. Expressions
are given for the control organs of an invariant system. The system was simulated
on an analog computer. It is shown that invariance may be produced with the aid of
a finite-dimensional object If certain conditions are maintained. An example is
given of the control system of an elastic object consisting of a uniform beam with
a tracking force at its end. It is further shown that the coordinates characteriz-A,
Ing the notion of the center of mass of the object do not depend on the coordinates

Subject USSR/Electronics AID p - 715
Card 1/1 Pub. 29 - 8/26
Authors PavlOv, V. V., Foreman and Golovin, A. K-, Technician
Title Ele ctronic time relay
PeTiodical Energetik, 9, 15-16, S 1954
Abstract The authors describe briEfly the relay of their own
design. The editors in a note warn against Using
this type of relay in protective circuits. 2 drawings.
Institution None
Submitted No date
p,Lvwv, V.V., inzhener.
C41- Semicondue tor parts for telephone systems. Vest-sviazi 16
no.9:34 S '56. (Mak 9:11)
(United States--Semiconductors)

meitianfet, mad OqMn

AV
7-1

K77
-4nd, 6
-A ota multi3take *,S.-arnplifi I'alor
-Thcrhamc

12
Tmd i x4tivilwator, r"

ni
xkl~ala jut,
-wn are
talmlatet.
A7-

REGULATION & REMOTE CONTROL
"Use of Germanium Transistors in HIgh Frequency Apparatus for
Telemechanies Communication, and Protection" b,. Engineer
V.V. Pavlov, Flektritcheskiye Stantsli, No. 5, May 1957, Pages
P brl.ef survey article, describing the operation of
tranststor and LndicatLng possible appi4cation for use 1.1-i
power system protection and telemetering, to replace ordinary
vacuum tubes.
Card 1/1 41
L~ C, V
pAVWV, V.y., mgt9r; 00LOTINg AoXv, tekhnik.
-Wopmr"" conneatIVS ZU gwitchboards. 1hurgetik 5 no.12:19-20
Now method of (MIRA 10t12)
1) 157, (xiectric power pl&nts-Squipment and suppliem)

PAVWV. V.V.. ft2henar. . . ., ! - - ; t, ~ ,
,--- -C tysm- - "I, - kdIeiixj-j*ht --beam. -Test. eviazi 17 no.7:
- 33 "5, , 01,5,5 F. y a., ~*",* (MIRA 100)
(Telephone)

PATWV, V.T., Insbener.
Using germanium triodes In higb-frequancy tolovochanics, cov,-
wmIcation and "lay apparatus. Blek. a&&. 29 no.5:59-61 W
157. (MLRA 10-6)
(Tmnsistors)

PAVLOV, 1Jt..,rea. (translator]; KODKIED, I.I., red.; IARIONOV. Me..
tekhn. red.
(Use of transistors in relay-type proteative equipment, measuring
spjarstus, and telemechanice eqdpmnt for power systems] [Trans-
lations from the Anglishl PoluprowodmAkovys triody v apparature
releizol sashchity, 12nerenli i telemekhaniki A14A eizergosistex.
KDakra, Goo. emarg, izd-To, 1958. 63 p. (KIRA 11:10)
1. Goguftrstvennn trest po organizatell I ratelonalizateii
rayonnykh elektrichecidkh stantsiy I setey, Moscow.
(Transistors) (31lectric power distribution)

, YA v-'V.Y.
Practical calculation of Internal noise In radio receivers
equpped with junction triodes. Poluprov.prib. I ta prim. nn-3:
162-174 158. OURA 12:4)
(Radio amplifiers--NDise)
(Transistors)

Senicondactor Triode
Radio Receiver Sets (0 raschete VAUtrennik?4.-zbuqOV XwUqPrWewVk-h
ustrWstv na polapmodnikoVkh triodAkh)
vol. li, Nr. q. IT.
!3:'; 'in fT; al et hOQ 0 fCQMPLA tI fig Et 1. -i M ifl J Ar :n#i aC
radio equipment with semiconductor :ri-2den
fact.or F specifies the ratio of' the actaai t
triode output and that nc:se lev~?l occijrr-,nA n i,
tolle which give2 tiip same amp~-,i-eRtl ) n r~ ~ I i to j,:~
This -&ay of designating thf se-. no-s.,
as it is arplicable to all rhdi..
representea by fourpoles. hlurecver it perm, t ii.pn rt.
tube noiLE, ditf, the nv,jt p-ducea ri i),Au.,- r -1
Under oth er, i!. I on p r i i
the cir:.i-' J:a,7r,7km r .1 T t -a
al-derably, hC?.*ev-:,r. -,v itn n 7.
tlial is t:) pith lh~
('.a rd current a n d t. n & c. 1) ~- re tr-nal f'r e I u cn r~- Y

Sexicandactor Triode Radio Receiver
Bete
~xh. L, its Cha r~~ - ! -21*., ) t '. c"n
I ai , a nd :)I' high f req-,aenc i ee 1 n .3 1;- 2rn e:-.. -
J, 21 1~~ our tasic -:~3mpcnents of set n,).,se can be
ga isned Rk? i The semiconduct or noise i s _,a-is tdit 'Y -i
0 hypothese.i by I
processes. The tw 13 ni r. i
a, 4p~ulncd. Variouq types of noise itz- in,ez- , e7,
ty current divivion in the tr4od~?s, the
e-'ICT, ~alzsed by the discrete microstructure of -t,e
cii,-ent In '.h;-, semiconductor, the thermal noise caused b.y tr~-
~f the crystal lattice anrl by the :!arr.-:,~
P c?.-irges. T~.fse three types of noise together D-
duct th~, r-ise. ~,.T-mulae 14) and (1'1,1, SPE-Cifying F
4 clrcai,~ X ;1, -matter or with a commrn bas_-,~z. r-~srtc_
,eiy derived. -,,:raing to these formulae it is po~isil-
compu*~- fur ~ cancain w~*.h an accuracy sufficlent fur C
i;ut,,,I.ion. -_~n at, leve,. The noise factor of ewDii-
ers st-miconductor triode's can also te meas;ired :nim,
Hert -i,,, usual tube melhid c.-.n be u,.?(:fd. Tnere ar,f ~R
J;~j referun:~e_~, 5 of whl-'211 ar-

11
10V/108-13-9-~/26
On the Computation of the Set Noise in SIMICCO& 21=ode Radlo Pwinelver
BffLD ,
SUBMITTEDt December 18, 1956 (initially) and August 14, 1957 (after re-
vision)
Card 3/3

8(2)
AUTHOR; Pavlov, V. V.v Engineer SO V/1 19-r9- 1-1 ",'2C
TITLE: Modern Foreign Semiconductor Diodes and Triodes (SovremE?nnyye
zarubezhnyye poluprovodnikov-yye diody i triody)
PERIODICAL: Priborostroyeniye, 1959, Nr 1, pp 3C-31 (USSR)
ABSTRACT: This paper deals with a report on two papers publia))ed in
English and one paper published in German, i.e.,
Proceedings of the IRE, Nr 6, 1958~ pp 12A-13A, 955-96s;
Electronic Industries, lir 6, 1958, Pp 73-101, 111-1391, 365;
Electronik Nr 7, pp 221-227.
There are 2 tables.
Card 1/1

9(6)
AUTHOR: Payloy. V.-V.,--Engineer SOV/119-60-1-7/14
TITLE: The Calculation of the Set Noise in Amplifier- and Meaeuxing
Apparatus With 3emiconduQtor Sarface Triodesc:~
to
PERIODICAL: Priborostroyeniye, 1960, Ur 1, pp 113 - 20 (USSR)
ABSTRAM As semiconductor triodes produced in series have a relatively
high noise-level, methods for the reduction of this noi3e and
of calculating the set noise must be developed. Problem3 of
practical calculatioh methods for set noise-in the construction
of measurement apparatus are here dealt with, it being assumed
that set noise is produced only by internal effects in the
semiconductor triodes, the author confining himself to problems
of calculation, four components of set noise are givent
ty gemiconductor noise in the collector circult. 2) Noise of
the Schottky effect in electron-hole transitions in the emitter
and collector.~)The noise of the division of the emitter
currentlinto collector and basic current. 4) The thermal noise
of the basis. In practical calculations only the semiconductor
Card 1/3 noise in the collector is taken into accounts and the author

The Calculation of the Set Noise in Amplifier- and SOV1119-60-1-7/14P
Measuring Apparatus With Semiconductor Surface Triodes
gives formula (1) for the average voltage of this noise. The
decrease of semiconductor noise depends on the progress madd
in semiconductor production methods,. For the mean voltage
of noise produced by the Schottky-effect formulas (2) and (3)
are given. A decrease of this noise may be attained by re-
duction of the emitter- and collector current as well as of
the working temperature, Further, the equations (4) and 5)
are given for the mean voltages of emitter-current division
noise and thermal noise,. A formula for the probability of
the occurrence of white noise pulses with a certain minimum
magnitude is then given. The author next investigates the
internal noise on the basis of figure 1, Five noise-sourties
are given, which are arranged in two groups for practical
calculation, corresponding to the in- and output of the triode.
By means of formulas (6) and (7) the coefficients of internal
noise for emitter- and collector basic circuits (skhemy s
obahchim emitterom) are calculated, Formula(g) is given for
Card 2/3 the purpose of calculating this coefficient of a cascade /

The Calculation of the Set Noise in Amplifier- and SOV/119-60-1-7/14
Measuring Apparatus With Semiconductor Surface Triodes
circuit. In the case of the practical calculations, the
correlation between the mean voltages of emitter, and
oolleotor-noise need not be taken Into account. The internal
noise depends on the triode parameter, the mode of Pperation
of the scheme, and on the internal resistance of the signal
source. Selecting the mode of operation with the least
internal noise is discussed on the basis of the diagram In
figure 5, i'n which the inner noise coefficient has a minimum
in the frequency range Il. For the reduction of set noise,
the triodes must be used in a circuit, in which a low eivittea
current, low collector voltage, and small temperature
fluctuations occur. There are 3 figures and 4 referenceo,
I of which is Soviet.
Card 3/3

201445
S/11 61/000/003/009/013
C>-O (2 9a 2 ) /1.3 S' 4~' 1/6 B124YB204
AUTHORt Pavlov, V. V.
TITLEt d.c. measurement amplifier with semiconductor triodes
PERIODICALs IzmeritelInaya tekhnika, no. 3, 1961, 35-40
TEXTs Examination of the operation of d.c.-to-a.c. transformers with Ge
and Si semiconductor triodes of various types (A2 (D-2), A7 (D7),A20
(D20)) showed that the sensitivity threshold is at 5-5 mv. The trans-
formation coefficient, i.e. the ratio of the d.c. voltage drop over the
output to the d.c. voltage, has a value of 0.5 to 0.7. A sinusoidal
voltage as well as rectangular pulses may be used in transforming. Trans-
formers with germanium diodes have unsatisfactory temperature
characteristics; their voltage drift amounts to an average of 0.8 mv in
the case of eight-hour operation, also on fluctuations at room tempera-
ture. Transformers with silicon diodes operate, even on temperature
fluctuations by up to 450C, with a voltage drift of around 0.1 mv and a
current drift of 10- 10 a (after 8 hr). Low d.c. voltages may be trans-
formed on the basis of the Hall effect with the sensitivity threshold at
Card 1/8

2D U5
S/115/61/000/003/003/012,
d.c. measurement amplifier... B1241B204
5()kv. However, the transformation coefficient of such transformers is
small and the latter are not stable on temperature variation. An
interesting type are transformers of small d.o. signals to a.c. signals
by means of semiconductor triodes. A sinuscidal or rectangular trans-
formation voltage is applied across base and emitter or collector of the
triode, while the measured d.c. signal is led over a resistor to the
electrodes of the emitter. The triode base current varies according to
the effect of the transformation voltage between 0 and ib max' Vhen the
input d.c. voltage is zero, then the output voltage is zero, too. On the
action of a d.c. voltage, the triode soon closes the circuit and becomes
saturated, which leads to the result that at the output of the triode an
alternating voltage appears, with a rectangle-like shape and an
amplitude proportional to the measured direct voltage. The lower limit
of direct voltage that can be transformed by such transformers is deter-
mined by the residual voltage u res and the residual current i res of the
triode. In the case of inverse connection of the triode, the residual
parameters are smaller than in the case of the usual connection with
common emitter; for this reason, in measurement transformation of weak
Card 2/8

d.c. measurement amplifier ...
20445
S/11 61/000/003/009/013
B124YB204
d.c. signals Just the inverse triode connection has to be employed. The
schematic diagram of a parallel and of a successive-type transformer with
inversely connected semiconductor triodes is shown in Fig.1 (a,b), and the
equivalent scheme is analyzed in Fig.1 (v). The voltage across the out-
put of the transformer during the half period of contact breaking is
Ucbz Ec + 'res (Rc+R) (4), where R res