In Chapter 5, we used various approximations for the time delay, one of which is the

Chapter 6, Problem 6.65

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QUESTION:

In Chapter 5, we used various approximations for the time delay, one of which is the first order Padé:

\(e^{-T_{d} s} \cong H_{1}(s)=\frac{1-T_{d} s / 2}{1+T_{d} s / 2} .\)

Using frequency response methods, the exact time delay

\(\mathrm{H}_{2}(\mathrm{~s})=\mathrm{e}^{-\mathrm{T}_{\mathrm{d}^{s}}}\)

can be obtained. Plot the phase of \(\mathrm{H}_{1}\) (s) and \(\mathrm{H}_{1}\) (s), and discuss the implications.

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QUESTION:

In Chapter 5, we used various approximations for the time delay, one of which is the first order Padé:

\(e^{-T_{d} s} \cong H_{1}(s)=\frac{1-T_{d} s / 2}{1+T_{d} s / 2} .\)

Using frequency response methods, the exact time delay

\(\mathrm{H}_{2}(\mathrm{~s})=\mathrm{e}^{-\mathrm{T}_{\mathrm{d}^{s}}}\)

can be obtained. Plot the phase of \(\mathrm{H}_{1}\) (s) and \(\mathrm{H}_{1}\) (s), and discuss the implications.

ANSWER:

Step 1 of 4

The expression for the \(H_{1}(s)\) is given by,

\(H_{1}(s)=\frac{1-T_{d}\left(\frac{s}{2}\right)}{1-T_{d}\left(\frac{s}{2}\right)}\)

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