SCIENTIFIC ABSTRACT ALIMOV, Y. I. - ALIMOVA, Y. K.

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December 31, 1967
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80132 S/141/59/oo2/o6/oi4/024 Overall Stability of the Equilibrium Sfj,?2/FJ8J Iy-type Control a e 0 0 a Systems as W, , which satisfies the equation: n- 8V dVljfdt 21 - Psrxr W1 (30). s,r=l dxS Further, it is shown that if the elements Pij = Pji. (such that i A- J) of the determinant D21-1 1whos e diagonal elements satisfy Eqs 05)-07), can be chosen in such a way that all the successive minors of' the element are positive, the equilibrium state of the system (bserlbed by Bqs (6) and (7) and satisfying Eqs (5) is asymptotically stable (as regards the overall stability). The above theorents are sultable for constructing the simplified stability criteria of high-order systems. The systems with n ranging from 4 to 6 are considered. The author thanks Ye*A. Barbashin for directing this Card3/4 work- LK- BM32 S/l41/59/oo2/o6/ol4/024 E122~P3#2 Overall Stability of the Equilibrium Sta elay-type Control Systems There eire 13 Soviet references. ASSOCIATION: Ura,llskiy politekhnicheskiy institut (Ural Polytechnical Institute) SUBMITTED: June 8, 1959 Card 4/4 NALMOV, Tu. 1. Determiniag the peri!)dict\I of noncontinuous control. no-.9:83-&S '59- movements Of a class of relay systems Nauch.dokl.vye.shkoly; fize-mat.nauki (MIA 13W . 1. 1. Urallsidy politeldmicheskiy institut imeni S.M.Kirovao (Slectrac relays) (Automatic control) 240) AUTHORS: Skrotskiy, G. V., Alimov, Yu. I. SOV/56-.36-4-44/70 TITLE: The Influence of the Shape ol the Specimen on Ferromagnetic Resonance in a Strong Radio-Frequency Field (Vliyaniye fOrmy obreztsanaferromagnitnyy rezonans v sillnom radiochastotnom pole) PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959, Vol 36, Nr 4,, pp 1267-1271 (USSR) ABSTRACT: Expuriments,13,y (Refs 1, 2) it was shown that the decreases slowly in the direction magnetization oomponent M Z of the constant field H 0 with growing microwave power. This effect was theoretically investigated by Suhl (Refs 3, 4) and derived by, using the Landau-Lifshits equation (1): 4 M +d -1,-# ef3 jaH . . [4M tj - 0, -1 - I/M , cc> 0 0, for an a r.f. field h the amplitudes of which are great compared 1/2 to the threshold field h : h MAH0.08AH/41IM ) Card 1/3 c e S The authors of' the present paper analyze the exact solutions The Influence of the Shape of -the Specimen on SOV/56--36-4-44/70 Ferromagnetic Resonance in a Strong Radio-Frequency Field of (1) for noaspherical ferromagnetic specimens in an r.f. field of arbitrary amplitude (they had already derived the solutions in a previous paper (Ref 5). It is found that above a certain value of h the motion of the magnetization vector becomes unstable? The slow decrease of the magnetization component and the shift of the resonance field for field strengths h 0) h c are explained. At hD> h c the height of the absorption peah: decreases and its vidth increases. The results agree easentially with those obtained by Suhl. The dependence of M z on at ~ N. 10 for different values of a is shown by figure 1; figure 2 showii the influence exercised by the nonsphericity of the specimen upon m Z in dependence on a 2 with ~ N = 100; the diagram, fox oomparison contains the cur,ve M Z (a2) for a homogeneounly magnetized spherical specimen,, The denotations apply to a system of coordinaten rotating Card 2/3 round H 0 - Hz with the frequencyU , where (1) has the form The Influence of the Shape of the Specimen on SOV/56-36-4-44/70 Ferromagnetic Resonance in a Strong Radio-Frequency Field [-+ fl , [ .:~ 411 ef _-4 15 m an - 0, with via bi 0 h -W*/U " 0 a Lj a Lj There are 2 figures and 6 referencest I of .,hich is Soviet. ASSOCIATIONs Urallskiy politekhnicheskiy institut (Ural Polytechnic Institute) SUBMITTEDs October 28, 1958 Card 3/3 ALIMOV, Yu.I. Problom of the atavility of relay systems in automatic control. Izv.v7,s.uch9b.zav.; mat. no.1:3-10 160. (MIRA 13:6) 1. Ural'skiy poll[tekhnicheski7 institut imeni S.M.Ki;ova. (Automatic control) ALIMOV, Yu.I. New nethod of arriving at simplified criteria of absoliite stability,. Inzh.-fiz.zhur. no.6:35-41 Je 160, (MIRA 13-7) 1. Urallskiy politekhnicheskiy, institut im. S.K.Kirova, g. Sverdlovsk. (Automatic control) 16, si 5 o o 77 4;-~ OV/3. 03 - 2 1-1-19/2 2 AUTHM Alimo,j, TITLE: Letter to the Editcr. Remarks on the Study by Yu. S. Sobolev "On Absolute Stability of Some Cont-ro-1 Systems" PERIODT'ALt Avtcn,atika I telemekhanika, 196C~ Vol 2.1, Nr 1, pp 1143 -144 (.USSR) ABSTRACT, The study under discussion was published in Av--omatika I telemekhanika. Vol 2-0, Nr 4, 19r,79, In this study, a theorem establishes conditions for absolute stabilty at certain types of control systems. The writer of the letter shows that there are systems of 11-hi,--, type which are stable according to Rouse-Hurwitz cor.ditions, but which d~~ not satisfy the conditions of the above theorem, Tt Is astated that the theorem derived by Yu. S. Sobolev is Insufficient, to be used for solution of probi.emo- of' Lbsolute stability. There are 2 Soviet ref erence s . Gard 1/-, 85648 S/103/60/021/006/020/027/XX 10,52049 (M2 ell 113,111311-V) BO19/BO63 AUTHOR: Alimoir, Yu. 1. (Sverdlovsk) ILP TITLE: Determination of Lyapunov Functions for Control Relay Systems 11 PERIODICAL: Avtomatika i telemekhanika, 1960, Vol. 21, No. 6, PP. 720-728 TEXT: The author first gives the transmission function of an au*~qmaJLg___. control system in matrix representation, and studies the --~ability of the system in the phase space after introducing the term "trajectory of the system". The states of equilil)rium of a class of control relay systems are n determined, and the relation VW - = a iix ixi+ skp9(0)G is obtained i,j.l for the Lyapunov function after extensive calculation, This function holds for the systeas most frequently atudied in control theory, which are described by the matrix equation i . Ax + bp(G'), 6' - k`x (3), where A is a quadratic column matrix, and x, b, and k are n-dimensional column Card 1/2 85648 Determination of Lyapunov Functions for Control Relay Systems 3/103/60/021/006/020/027/XX B019/BO63 matrices,. The criteria derived for the stability of these systems are ex- pressed by the coefficients of the transmiss" fun tion. As the Lyapunov function is represented in an invariant form Ithe above-Mentioned criteria can be represented by elemen-~s of the matricesTA, b, and k. I. G-_ Malkin, A~ I. Lurlye, and JU M. Letov are mentioned. ~e- A. Barbashin is thanked for guidance and help. There are 15 Soviet references. Card 2/2 ALIMOV, Yu. T. Cand Phys-Math Sci -- (diss) "Several problems of the dynamics of relay systems in automatic control." Sverd:i-ovsk, 1961. 10 pp; (Ministry of Higher and Secondary S ecialist Education RSFSR, Ural IS)tate Univ imeni A. M. Gor'kiy~; 1',70 copies; price not given; bibliography at end of text; (KL, 7--61 sut), 217) 22830 S/19 61/002/001/001/008 h B I I 2YB21 8 AUTHOR: Alialovi Yu,, I. TITLE: Determination of the Lyapunov function for--systems of linear differential equations with constant coeffiqient PERIODICAL- SibLrskiy miatematicheskiy zhurnal, v. 2, no. 1, 1961, 3-6 TEXT: The criteria for the asymptotic stability of systems of linear dif- ferential equations with constant coefficient are based on the existence of a Lyapunov function whose) total derivative with reTect to time is a definite form. These criteria are generalizations of I. G. Malkin's cr,: 'teria for absolute stabilitr. In the present paperp thp author proves elcistence theorems for the Iyapunov function of nonstable linear systems, The proofs are analogous to oorresponding proofs of A. M. Lyapunov -and N. N. Krasovskiy. The system of differential.nequations considered: d)cs/dt _ V. I Pskxk' Psk i. const (s ........ , n) (1) exhibits the function- n av dir/dt - P W(x, . ..... Xn) (2) ax sk'k Card 1/2 DetermJnatLon of ... 22830 S/1 99J61 /'002/OC1 /001 /008 Bi I 2/B21 El as a derivative with respect to time of the Lyapunov function: V(xj, .... 9 X~' n The theorems proved are: 1) If all roots of the characteristic equation of system (1) have a negative real part, then there exists exactl3, one form V of degree m for every positive definite form W(X,t ..... I Xn) of this degree, which is no integral of sy,9tem (1). This form V satisfies con,! 'ition (2). V must be positive definite. 2) If among the roots A, of the "!haracteristic equation of system (1) there is at least one with a positive real pa and if for non-neeative integers m which satisfy the donditiM~; 1 Mn i.1 'i = " X M will never vanish, then there exists exactly one form 11 of degree m for every positive definite form N of this degree, which is no integral of system (1). This form V satisfies condition (2) and is positive definite. 3) If among the roots of the characteristic equation of system (1) there is at least one with a positive real part, then there exists a forn V of degree m and a positive number oc Sor every positive definite form W of this degree, which is no integral of (1). Thus, aV/dt - aV - W, V being positive definite. Professor Ye. A. Barbashin is thanked for guidance. There are 7 Soviet- bloc references. SUBMITTED: November 20, '1959 Card 2/2 gq5 S/lOY361yoj2/007/001/008 D IL,1000 (16 31/ //:Zl/ //,3~)' D252 D302 AUTHOR-. Alimov, Yu. I. (Sverdlovsk) TITLE: Application of Lyapunov's direct method to differen- tial equations with non-unique right-hand sides PERIODICA1,: iivtomatika i telemekhanika, v. 22, rxo. 7, 1961, 817-829 TEXT: A mathematical model is constructed for relay control sys- teiiis which expresses better their physical meaning than the usual model (differential equations with discontinuous right-hand sides). The obtained mathematical model is considered as LA SySt(!M Of equa- tions in contingencies to which Lyapunov's direct method can be applied. This method which is an extension of Lyapunov's stability theorems, consists among others of a theorem by Krasovs1.,-.yy, of the Ye. A. Barbashin and N.N. Krasovskyy theorems, (Ref. 13: Nekotoryye zadachi teorii ustoychivosti dvizheniya (Some Problems :in Stability Theory), Fizmatl-riz, 1959), and D. Veksler's theorem (Re:,L-. 16: 0 teo- remakh ustoychivosti d.lya sistem statsionarnykh differe',,_Ltsial1nykh Card 115 Application of Lyapunov's direct... D252/D302 uravneniy, Revue des Matl,-L6matiques pures et ;q)TAicluees, vol. 3, no.1). The normalized equations of motion of relay systeiit:; are; f (t,31) . f I t 9x 9 T (0 t: $ x (2) where f (t,x, and 0 there exists a set Ee C- El , mes Ee < and there exists a positive number n(C) so that U Fn(p) - F(P)IIM(R)< holdo for all pr-E'\E,r and n>n(S~). The function f(p) is called countable -valued on El if F(EI) is a countable set, where the inverse images of the points of M(R) are measurable Belts for the mapping F(p) of E into M(R). f(p) is called measurable if there! exists a sequence of countsble-valued functions fn(p) converging almost uniformly on SI with respect to f(p). The integral of a measurable f(p) is defined by ( f(P)dp = (B) ~ F(p)dp j~l El where (B) denotes a 2ochner - integral. Let E be the number iine, The Card 2/. S/020/61/140,/001/00'1/024 on the theory of dynamic syutems 0111/C222 The derivative of an anbiguoua f(t) , tCE , is defined by ALLtl - nin Sllt-!~'- f(t) dt h-i,O h where the limit value correnponds to the metric introduced above. Given the differential equaUon x - f(t,.X) M where f(t,x) is an ambiguouz function defined for xCR, -oo.< t