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Derivation of the Routh array : ウィキペディア英語版
Derivation of the Routh array

The Routh array is a tabular method permitting one to establish the stability of a system using only the coefficients of the characteristic polynomial. Central to the field of control systems design, the Routh–Hurwitz theorem and Routh array emerge by using the Euclidean algorithm and Sturm's theorem in evaluating Cauchy indices.
== The Cauchy index ==

Given the system:
: \begin
f(x) & \quad (1) \\
&
Assuming no roots of f(x) = 0\, lie on the imaginary axis, and letting
: N\, = The number of roots of f(x) = 0\, with negative real parts, and
: P\, = The number of roots of f(x) = 0\, with positive real parts
then we have
: N+P=n \quad (3) \,
Expressing f(x)\, in polar form, we have
: f(x) = \rho(x)e^ \quad (4) \,
where
: \rho(x) = \sqrt^2()} \quad (5)
and
: \theta(x) = \tan^\big(\mathfrak()/\mathfrak()\big) \quad (6)
from (2) note that
: \theta(x) = \theta_(x)+\theta_(x)+\cdots+\theta_(x) \quad (7)\,
where
: \theta_(x) = \angle(x-r_i) \quad (8)\,
Now if the ith root of f(x) = 0\, has a positive real part, then (using the notation y=(RE(),IM()))
: \begin
\theta_(x)\big|_ & = \angle(x-r_i)\big|_ \\
& = \angle(0-\mathfrak(),\infty-\mathfrak()) \\
& = \angle(-\mathfrak(),\infty) \\
& = \lim_\tan^\phi=-\frac \quad (9)\\
\end
and
: \theta_(x)\big|_ = \angle(-\mathfrak(),-\infty) = \lim_\tan^\phi=\frac \quad (10)\,
Similarly, if the ith root of f(x)=0\, has a negative real part,
: \theta_(x)\big|_ = \angle(-\mathfrak(),\infty) = \lim_\tan^\phi=\frac\, \quad (11)
and
: \theta_(x)\big|_ = \angle(-\mathfrak(),-\infty) = \lim_\tan^\phi=-\frac\, \quad (12)
Therefore, \theta_(x)\Big|_^ = -\pi\, when the ith root of f(x)\, has a positive real part, and \theta_(x)\Big|_^ = \pi\, when the ith root of f(x)\, has a negative real part. Alternatively,
: \theta(x)\big|_ = \angle(x-r_1)\big|_+\angle(x-r_2)\big|_+\cdots+\angle(x-r_n)\big|_ = \fracN-\fracP \quad (13)\,
and
: \theta(x)\big|_ = \angle(x-r_1)\big|_+\angle(x-r_2)\big|_+\cdots+\angle(x-r_n)\big|_ = -\fracN+\fracP \quad (14)\,
So, if we define
: \Delta=\frac\theta(x)\Big|_^ \quad (15)\,
then we have the relationship
:N - P = \Delta \quad (16)\,
and combining (3) and (16) gives us
: N = \frac\, and P = \frac \quad (17)\,
Therefore, given an equation of f(x)\, of degree n\, we need only evaluate this function \Delta\, to determine N\,, the number of roots with negative real parts and P\,, the number of roots with positive real parts.
Equations (13) and (14) show that at x=\pm\infty\,, \theta=\theta(x)\, is an integer multiple of \pi/2\,. Note now, in accordance with (6) and Figure 1, the graph of \tan(\theta)\, vs \theta\,, that varying x\, over an interval (a,b) where \theta_a=\theta(x)|_\, and \theta_b=\theta(x)|_\, are integer multiples of \pi\,, this variation causing the function \theta(x)\, to have increased by \pi\,, indicates that in the course of travelling from point a to point b, \theta\, has "jumped" from +\infty\, to -\infty\, one more time than it has jumped from -\infty\, to +\infty\,. Similarly, if we vary x\, over an interval (a,b) this variation causing \theta(x)\, to have decreased by \pi\,, where again \theta\, is a multiple of \pi\, at both x = ja\, and x = jb\,, implies that \tan \theta (x) = \mathfrak()/\mathfrak()\, has jumped from -\infty\, to +\infty\, one more time than it has jumped from +\infty\, to -\infty\, as x\, was varied over the said interval.
Thus, \theta(x)\Big|_^\, is \pi\, times the difference between the number of points at which \mathfrak()/\mathfrak()\, jumps from -\infty\, to +\infty\, and the number of points at which \mathfrak()/\mathfrak()\, jumps from +\infty\, to -\infty\, as x\, ranges over the interval (-j\infty,+j\infty\,) provided that at x=\pm j\infty, \tan()\, is defined.
In the case where the starting point is on an incongruity (i.e. \theta_a=\pi/2 \pm i\pi\,, ''i'' = 0, 1, 2, ...) the ending point will be on an incongruity as well, by equation (16) (since N\, is an integer and P\, is an integer, \Delta\, will be an integer). In this case, we can achieve this same index (difference in positive and negative jumps) by shifting the axes of the tangent function by \pi/2\,, through adding \pi/2\, to \theta\,. Thus, our index is now fully defined for any combination of coefficients in f(x)\, by evaluating \tan()=\mathfrak()/\mathfrak()\, over the interval (a,b) = (+j\infty, -j\infty)\, when our starting (and thus ending) point is not an incongruity, and by evaluating
: \tan()=\tan(+ \pi/2 ) = -\cot() = -\mathfrak()/\mathfrak() \quad (18)\,
over said interval when our starting point is at an incongruity.
This difference, \Delta\,, of negative and positive jumping incongruities encountered while traversing x\, from -j\infty\, to +j\infty\, is called the Cauchy Index of the tangent of the phase angle, the phase angle being \theta(x)\, or \theta'(x)\,, depending as \theta_a\, is an integer multiple of \pi\, or not.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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