Step 1: Understand the behavior of \( |H(\omega)| \) as a function of damping ratio \( \zeta \).
We are given: \[ |H(\omega)| = \sqrt{\frac{1 + 4 \zeta^2 \left( \frac{\omega}{\omega_n} \right)^2 }{\left[ 1 - \left( \frac{\omega}{\omega_n} \right)^2 \right]^2 + 4 \zeta^2 \left( \frac{\omega}{\omega_n} \right)^2} } \] Let \( r = \frac{\omega}{\omega_n} \). We want to analyze how \( |H(\omega)| \) behaves with respect to \( \zeta \) for different values of \( r \).
Step 2: Observe the trend.
When \( r = 1 \), i.e., excitation frequency equals natural frequency, the expression simplifies but the behavior becomes complex due to the resonance peak.
When \( r>\sqrt{2} \), the numerator increases faster with \( \zeta \) compared to the denominator. Hence, \( |H(\omega)| \) increases with increasing \( \zeta \).
Step 3: Analyze each option.
(A) Incorrect: At \( r = 1 \), the denominator becomes minimal, and amplitude tends to reduce with increasing \( \zeta \).
(B) Incorrect: At \( r = 0.75 \), increasing \( \zeta \) leads to a lower amplitude.
(C) Incorrect: At \( r = \frac{\sqrt{3}}{2} \), amplitude still decreases with damping.
(D) Correct: For \( r>\sqrt{2} \), the increase in \( \zeta \) results in a larger amplitude.
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