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On aperiodicity robustness

机译:关于非周期性的鲁棒性

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In this paper, the aperiodicity condition of a system's characteristic equation is first formulated for both continuous and discrete systems. It states that the roots of the characteristic equation have to be real, distinct, and negative for the continuous case, and real? distinct, and in the interval [0,1) for the discrete case. The coefficients of these equations are perturbed for an initially aperiodic system such that, in the limit, aperiodicity is violated. The values of the perturbed coefficients are determined and thus the robustness conditions are obtained, This approach to the topic is quite different from those that have appeared in the literature which first assume that the initial perturbation limits are known. Such approaches are quite similar to that first discussed by Kharitonov for stability problems. In situations where the initial perturbation limits are not known, the approach presented in this paper is a valid alternative. The solution presented in this paper is based on two formulations. The first is based on the critical aperiodicity conditions while the second is based on a theorem known in old literature which states that if the system is initially aperiodic, then Psi(s) = [F'(s)](2) - F(s)F "(s), where F'(s) = dF(s)/ds and F "(s) = d(2)F(s)/ds(2), should have no real roots. Here F(s) is the continuous system's characteristic equation. Now, in the limit when the above condition is violated, one obtains the robustness limits zeta(i). Both approaches give the same values. To obtain similar robustness limits for the discrete case, we can use either the linear fractional transformation z = s/(s - 1) which transforms the segment [0,1) in the z-plane onto the negative real axis in the s-plane and use the above conditions, or directly formulate the aperiodicity conditions in the z-plane. Both are discussed in this paper. An example is presented to illustrate the above formulations for obtaining the robustness conditions. [References: 24]
机译:在本文中,首先针对连续和离散系统制定了系统特征方程的非周期性条件。它指出,对于连续的情况,特征方程的根必须是实的,唯一的并且是负的,并且是实的?对于离散情况,间隔为[0,1)。对于最初的非周期性系统,这些方程的系数会受到干扰,从而在一定程度上违反了非周期性。确定扰动系数的值,从而获得鲁棒性条件。该主题的方法与文献中出现的方法完全不同,文献中首先假定初始扰动极限是已知的。这种方法与Kharitonov首次讨论的稳定性问题非常相似。在初始扰动极限未知的情况下,本文提出的方法是有效的替代方法。本文提出的解决方案基于两个公式。第一个基于临界非周期性条件,而第二个基于旧文献中已知的一个定理,该定理指出,如果系统最初是非周期性的,则Psi(s)= [F'(s)](2)-F( s)F“(s),其中F'(s)= dF(s)/ ds和F”(s)= d(2)F(s)/ ds(2),应没有实根。在此,F(s)是连续系统的特征方程。现在,在违反上述条件的极限中,获得鲁棒性极限zeta(i)。两种方法都给出相同的值。为了获得离散情况的相似鲁棒性极限,我们可以使用线性分数变换z = s /(s-1),它将z平面中的段[0,1)变换为s-中的负实轴平面并使用上述条件,或直接在z平面中制定非周期性条件。两者都在本文中讨论。给出一个例子来说明上述公式以获得鲁棒性条件。 [参考:24]

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