SCIENTIFIC ABSTRACT ZANADVOROY, P.N. - ZANATI, T.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001963730003-9
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 43
• Document Creation Date: November 2, 2016
• Document Release Date: September 19, 2001
• Sequence Number: 3
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

29589
AUTHORS: Gyunninen, E*Mef ~~LRadvorovL
Vlrakarovp G. I.
TITLE: The effect of a complex shape
free-running oscillator
B/108/61/016/011/005/007
D201/D304
N., Kotik, I.P.f and
periodic signal on a
PERIODICAL: Radiotekhnika, v. 16p no..Ilt 1961, 59 - 44
TFAT: The pure theory of phasing of oscillators presents difficul.-
ties which make the solutions of its problem practically impossible.
In the present article, the author consideve the solution of this
problem in its numerical context9 by means of a fast electronic
computer. Such a problem, as opposed to the purely analytical onet
is stated to be comparatively easy, but the quasilinear method of
analysis is applied for simplification and numerical substitution
of the equation of the oscillator, upon which acts the external fcr-
ce A(T). If x is the voltage at the gridt reduced to the amplitude
x of the steady state oscillations at the grid, w and 6 the fre-
m . 0 1
quency and attenuation of the osc~_'Lllating circuit, T = w0t dimen-
Card 1/7

~.The effect of complex shape
29589 S/10/61/016/011/U05/Q07
D201/D304
sionless time; average reduced slope of the valve.'pt Y9 S
and condtants, then the fundamental equation may be.represeRted.
as
2
'd
X*+ X MWOS*Ll arc xmj yA(,r). (3)
z 0 dr +
d-r
Practical values are now assigned to -the parameters of (3) thus:
0. 8; MW so-,. =1.12; 0.422; 10-2 and 10-3 0.1 and
0
04,01 are.the values resulting from practical assessment of the val...
ve parameters and regime. The acting force has been taken as havin!3
the form of consecutive lldistor~ed si-viuBoidal.pulses" A(T) with li-
near variation of amplitude and initial.phase. ThUA A(T) had the
form of
0,08(-C+3)-sInfc(0,8+0,02z)J, 0