Question:

Addition of a pole at the origin to a transfer function rotates the polar plot at zero and infinite frequencies by a further angle of

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Adding a pole at the origin (\(1/s\)) to \(G(s)H(s)\) contributes a phase of \(-90^\circ\) at all frequencies \(\omega\).
Adding a zero at the origin (\(s\)) to \(G(s)H(s)\) contributes a phase of \(+90^\circ\) at all frequencies \(\omega\).
This rotation affects both the starting point (\(\omega \to 0^+\)) and the ending point (\(\omega \to \infty\)) of the polar plot.
Updated On: Jun 11, 2025
  • \( 90^\circ \)
  • \( -90^\circ \)
  • \( 45^\circ \)
  • \( -45^\circ \)
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The Correct Option is B

Solution and Explanation

In control systems, consider a transfer function \( G(s) \). When a pole is added at the origin, the transfer function becomes \( G(s) = \frac{k}{s} \times \text{(original terms)} \). In polar plots, the phase of a transfer function is determined by the angle it makes on the complex plane. For a pole at the origin (i.e., \( s=0 \)), the phase contributed by this pole is given by:
\(\phi = \angle(-s) = -90^\circ\)
This is because in the complex plane, a point at \(-90^\circ\) corresponds to a pole at the origin, hence the plot is rotated by \(-90^\circ\) at zero and infinite frequencies. Thus, the correct answer is:
\(-90^\circ\)
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