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Nonlinear Control Sy.. - Free

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6.4. L GAINS FOR LTI SYSTEMS<br />

where<br />

It follows that lullc_ = 1, and<br />

and the result follows.<br />

6.4.2 G2 Gain<br />

sgn[h(t)]<br />

1 if h(T) > 0<br />

l 0 if h(T) < 0<br />

y(t) = (h * u)(t) = bou(t) + t ha,(T)U(t - r)dr<br />

J0 t<br />

Ihol + f Iha(T)ldr = IhIIA<br />

0<br />

This space consists of all the functions of t that are square integrable or, to state this in<br />

different words, functions that have finite energy. Although from the input-output point of<br />

view this class of functions is not as important as the previous case (e.g. sinusoids and step<br />

functions are not in this class), the space G2 is the most widely used in control theory because<br />

of its connection with the frequency domain that we study next. We consider a linear timeinvariant<br />

system H, and let E A be the kernel of H., i.e., (Hu)(t) = h(t) *u(t), du E G2.<br />

We have that<br />

-Y2(H) = sup III<br />

(6.18)<br />

x xIIIC2<br />

1/2<br />

IIxIIc2 = { f Ix(t)I2 dt }<br />

We will show that in this case, the gain of the system H is given by<br />

00<br />

'Y2(H) = sup I H(.)I<br />

J<br />

f IIHIIoo<br />

167<br />

(6.19)<br />

(6.20)<br />

where H(tw) = .F[h(t)], the Fourier transform of h(t). The norm (6.20) is the so-called<br />

H-infinity norm of the system H. To see this, consider the output y of the system to an<br />

input u<br />

Ilylicz = IIHuIIcz =f [h(t) * u(t)]dt = 21r<br />

ii:<br />

where the last identity follows from Parseval's equality. From here we conclude that<br />

IIyIIcz < {supIH(Jw)I}2 I<br />

2r1 00<br />

r i-<br />

IU(JW)12dw}

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