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The attenuation (magnitude) produced by a lead compensator at the frequency of maximum phase lead \({\omega _m} = \sqrt {ab}\) is
1. \(\sqrt {\frac{b}{a}}\)
2. \(\sqrt {a + b}\)
3. \(\sqrt {b - a}\)
4. \(\sqrt {\frac{a}{b}} \)

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Correct Answer - Option 4 : \(\sqrt {\frac{a}{b}} \)

The transfer function of lead compensation is given by:

\({K_{lead}}\left( s \right) = \frac{{{K_c}\left( {s + a} \right)}}{{\left( {s + b} \right)}},\;a < b\)

Here, the zero is dominating over the pole.

If a pole or zero is close to the origin, then it becomes more dominating.

The magnitude of lead compensation is given by:

\({\left| M \right|_{s = j\omega }} = \sqrt {\frac{{{\omega ^2} + {a^2}}}{{{\omega ^2} + {b^2}}}} \)

The maximum lead attenuation at a frequency of:

\({\omega _m} = \sqrt {ab} \) will be:

\({\left| M \right|_{{\omega _1} = {\omega _m} = \sqrt {ab} }} = {\left. {\sqrt {\frac{{{\omega ^2} + {a^2}}}{{{\omega ^2} + {b^2}}}} } \right|_{\omega = \sqrt {ab} }}\)

\(\sqrt {\frac{{{{\left( {\sqrt {ab} } \right)}^2} + {a^2}}}{{{{\left( {\sqrt {ab} } \right)}^2} + {b^2}}}} = \sqrt {\frac{{ab + {a^2}}}{{ab + {b^2}}}} \)

\(= \sqrt {\frac{{a\left( {a + b} \right)}}{{b\left( {a + b} \right)}}} \)

\( = \sqrt {\frac{a}{b}} \)

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