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A.3. CHAPTER 6 319<br />

Condition (ii): H1 and Hi are linear time-invariant systems; thus, the ,C2 gain of H1 is<br />

Thus<br />

if and only if<br />

or<br />

'Y(H1) = j1G1j. = sup IG(7w)I-<br />

w<br />

ry(Hl)ry(H2) < 1 (A.17)<br />

G(7w)<br />

r [sup l[1+gG(.7w)J < 1 (A.18)<br />

rlG(yw)l < l1+gG(.7w)l dwER. (A.19)<br />

Let G(3w) = x + jy. Then equation (A.19) can be written in the form<br />

r2(x2 + y2)<br />

x2(82 - r2) + y2(g2 - r2) + 2qx + 1<br />

a,3(x2 + y2) + (a + 3)x + 1<br />

We now analyze conditions (a)-(c) separately:<br />

< (1 + qx)2 + g2y2<br />

> 0<br />

> 0.<br />

(a) 0 < a 0<br />

which can be expressed in the following form<br />

where<br />

a<br />

(x + a)2 + y2 > R2<br />

_ a+Q _ (/3-a)<br />

R<br />

2af<br />

2a,3<br />

(A.20)<br />

(A.21)<br />

(A.22)<br />

(A.23)<br />

Inequality (A.22) divides the complex plane into two regions separated by the circle C<br />

of center (-a + 30) and radius R. Notice that if y = 0, then C satisfies (x + a)2 = R2,<br />

which has the following solutions: x1 = (-/3-1 + 30) and x2 = (-a-1 + 30). Thus<br />

C = C', i.e. C is equal to the critical circle C' defined in Theorem 6.6. It is easy to see<br />

that inequality (A.22) is satisfied by points outside the critical circle. Therefore, the<br />

gain condition y(Hi)y(H2) < 1 is satisfied if the Nyquist plot of G(s) lies outside the<br />

circle C*. To satisfy the stability condition (i), the Nyquist plot of d(s) must encircle<br />

the point (-q-1 +30), v times in counterclockwise direction. Since the critical point<br />

(-q-1 +, j0) is located inside the circle C*, it follows that the Nyquist plot of d(s)<br />

must encircle the entire critical circle C' v times in the counterclockwise direction,<br />

and part (a) is proved.

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