非线性控制问题的分布式补偿器

D. Russell
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Under these assumotions one can show that for � > �0 there is a unique periodic solution yp(t, �) near y = y = 0 with weriod T(�), a smooth function of � with-T(�0) equal to the common period of all solutions of the linear oscillator equation y + ?k/?y(�0, 0)y, having average amplitude A(�) =1/T(�) ?0 T(�)((yp(t, �))2+(yp(t, �))2)dt The question which we address initially is: suppose u(t) = 0, g = 0 in (I) and we have a single measurement (t) = ay(t) + by(t) available from the system (I). Assuming fixed for the present, ?p(t, �) = ayp(t, �) + byp(t, �) will be the data obtained from the periodic solution yp(t, �). How may we obtain an estimate of the system state vector (yp(t, �), yp(t, �)) from present and recorded bast values of ?p(t, �)? With T = T(�) assumed fixed, let us consider the system with delay w(t) = v(t) v(t) = v(t-T). (II) The oeriodic function ?p (t, �) is a particular output corresponding to a particular solution of this system. For w(t) = yp (t, �), w(t) = v(t) = yp(t, �) will satisfy (II) if yp (t, �) is periodic with period T. Then ?(t) = ?p (t, ) = aw(t) + bv(t). (III) The question now becomes one of constructing an observer (cf. [2]) for the system (II) based on the observation (III), so that the estimated state will tend, asymototically, to the state (yp(t, �), yp(t, �)) in an appropriate sense. Our paper will concern the construction of the estimator and the nature of the convergence of the estimate. We will also discuss feedback synthesis of the control u(t) from this estimate. We will also deal with the case wherein a controlled elastic system x = Ax + cy(t) + dy(t) + fu(t) (IV) is coupled to the nonlinear oscillator (I).","PeriodicalId":269680,"journal":{"name":"The 23rd IEEE Conference on Decision and Control","volume":"43 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1984-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A distributed compensator for a nonlinear control problem\",\"authors\":\"D. Russell\",\"doi\":\"10.1109/CDC.1984.272202\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Many systems exhibiting self-excited oscillations of determinate amplitude may be modelled by a system of differential equations which includes the scalar nonlinear equation (cf. discussion in [1]) y + h(�, y, y)y + k(�, y) = u(t) + g*x(t) (I) where h, k are smooth functions involving a bifurcation parameter �. 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引用次数: 0

摘要

许多具有确定振幅的自激振荡的系统可以用包含标量非线性方程(参见[1]中的讨论)y + h(, y, y)y + k(, y) = u(t) + g*x(t) (I)的微分方程组来建模,其中h, k是涉及分岔参数的光滑函数。我们假设,一致地,yk(, y) > 0, ?k/?Y(, 0) > 0,得到?0 ?K (, y)dy = ?进一步,我们假设函数h可以表示为h(, y, y) = -h1(, y)y + h2(, y)(y)3…在整个感兴趣的y区间内,h1 (, y)一致地> 0。同样,我们假设存在一个值,设为0,使得(- 0)h2 (, y) > 0,在同一区域。在这些假设下,我们可以证明,对于> 0,在y = y = 0附近有一个唯一的周期解yp(t,),其周期为t(),一个光滑的函数,其周期为- t(),等于线性振子方程y + ?k/?y(' 0,0)y,平均振幅A(') =1/T(') ?0 T(')((yp(T, '))2+(yp(T, '))2)dt我们最初要解决的问题是:假设u(T) = 0, g = 0在(I)中,我们有一个单一的测量(T) = ay(T) + by(T)从系统(I)中可用。假设目前固定,p(T, ') = ayp(T, ') + byp(T, ')将是从周期解yp(T, ')中获得的数据。我们如何从p(t,)的现有值和记录的基本值中获得系统状态向量(yp(t,), yp(t,))的估计?假设T = T(T)是固定的,我们考虑时滞w(T) = v(T) v(T) = v(T -T)的系统。(II)周期函数?p (t,)是对应于该系统的一个特解的特定输出。对于w(t) = yp(t, '), w(t) = v(t) = yp(t, ')满足(II),如果yp(t, ')是周期为t的周期,则?(t) = ?p (t,) = aw(t) + bv(t)。(III)现在的问题变成了基于观测(III)为系统(II)构造一个观测器(参见[2]),这样估计的状态将在适当的意义上渐近地趋向于状态(yp(t,), yp(t,))。本文将讨论估计量的构造和估计收敛性的性质。我们还将从这个估计讨论控制u(t)的反馈综合。我们还将处理这样一种情况,即受控弹性系统x = Ax + cy(t) + dy(t) + fu(t) (IV)与非线性振荡器(I)耦合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A distributed compensator for a nonlinear control problem
Many systems exhibiting self-excited oscillations of determinate amplitude may be modelled by a system of differential equations which includes the scalar nonlinear equation (cf. discussion in [1]) y + h(�, y, y)y + k(�, y) = u(t) + g*x(t) (I) where h, k are smooth functions involving a bifurcation parameter �. We will assume that, uniformly in �, yk(�, y) > 0, ?k/?y(�, 0) > 0 and that ?0 ? k(�, y)dy = ?. Further, we assume that the function h may be expressed in the form h(�, y, y) = -h1(�, y)y + h2(�, y)(y)3... with h1 (�, y) > 0 uniformly throughout the y interval of interest. Also, we assume that there is a value of �, call it �0, such that (�-�0)h2 (�, y) > 0, in the same region. Under these assumotions one can show that for � > �0 there is a unique periodic solution yp(t, �) near y = y = 0 with weriod T(�), a smooth function of � with-T(�0) equal to the common period of all solutions of the linear oscillator equation y + ?k/?y(�0, 0)y, having average amplitude A(�) =1/T(�) ?0 T(�)((yp(t, �))2+(yp(t, �))2)dt The question which we address initially is: suppose u(t) = 0, g = 0 in (I) and we have a single measurement (t) = ay(t) + by(t) available from the system (I). Assuming fixed for the present, ?p(t, �) = ayp(t, �) + byp(t, �) will be the data obtained from the periodic solution yp(t, �). How may we obtain an estimate of the system state vector (yp(t, �), yp(t, �)) from present and recorded bast values of ?p(t, �)? With T = T(�) assumed fixed, let us consider the system with delay w(t) = v(t) v(t) = v(t-T). (II) The oeriodic function ?p (t, �) is a particular output corresponding to a particular solution of this system. For w(t) = yp (t, �), w(t) = v(t) = yp(t, �) will satisfy (II) if yp (t, �) is periodic with period T. Then ?(t) = ?p (t, ) = aw(t) + bv(t). (III) The question now becomes one of constructing an observer (cf. [2]) for the system (II) based on the observation (III), so that the estimated state will tend, asymototically, to the state (yp(t, �), yp(t, �)) in an appropriate sense. Our paper will concern the construction of the estimator and the nature of the convergence of the estimate. We will also discuss feedback synthesis of the control u(t) from this estimate. We will also deal with the case wherein a controlled elastic system x = Ax + cy(t) + dy(t) + fu(t) (IV) is coupled to the nonlinear oscillator (I).
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