Question:

The frequency response magnitude of a DT-LTI system tends to infinity when

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Poles act as infinite peaks in the $z$-plane, while zeros act as valley bottoms. If a peak (pole) sits directly on the unit circle ($|z|=1$), the frequency response magnitude evaluated at that specific angular location goes to infinity.
Updated On: Jul 4, 2026
  • Input is zero
  • Poles lie on the unit circle
  • Zeros lie on the unit circle
  • System is causal and stable
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The Correct Option is B

Solution and Explanation

Concept: The frequency response $H(e^{j\omega})$ of a Discrete-Time Linear Time-Invariant (DT-LTI) system is obtained by evaluating its system transfer function $H(z)$ directly along the unit circle in the $z$-complex plane, meaning we substitute $z = e^{j\omega}$. \[ H(e^{j\omega}) = H(z) \Big|_{z = e^{j\omega}} \] The rational expression of a transfer function is represented in terms of its poles ($p_k$) and zeros ($z_m$): \[ H(z) = A \cdot \frac{\prod (z - z_m)}{\prod (z - p_k)} \]

Step 1: Understand the geometric interpretation of poles and zeros.

In the complex $z$-plane: - Zeros ($z_m$): Points where the magnitude of the transfer function drops precisely to zero ($|H(z)| = 0$). - Poles ($p_k$): Points where the denominator becomes zero, causing the magnitude of the transfer function to approach infinity ($|H(z)| \rightarrow \infty$).

Step 2: Evaluating the behavior along the unit circle.

When the system frequency response is evaluated, the variable $z$ traces the path defined by $|z| = 1$. If a pole $p_k$ happens to lie directly on this unit circle, then at the specific frequency $\omega_0$ where $e^{j\omega_0} = p_k$, the distance from the point on the unit circle to that pole drops to zero: \[ |z - p_k| = |e^{j\omega_0} - e^{j\omega_0}| = 0 \] As this term resides in the denominator of $H(z)$, division by zero causes the overall frequency response magnitude to surge to infinity: \[ |H(e^{j\omega_0})| \rightarrow \infty \]
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