In a vibration isolation system, the concept of transmissibility is crucial. Transmissibility, \( T \), refers to how well a system isolates vibrations and is defined as the ratio of the output amplitude to the input amplitude.
The expression for transmissibility in terms of the frequency ratio \( \omega_r = \frac{\omega}{\omega_n} \) (where \( \omega \) is the forcing frequency and \( \omega_n \) is the natural frequency of the system) and damping factor \( \zeta \) is given by:
\[ T = \sqrt{\frac{1 + (2\zeta\omega_r)^2}{(1 - \omega_r^2)^2 + (2\zeta\omega_r)^2}} \]
For \( \omega_r < \sqrt{2} \), we can analyze the condition for transmissibility:
When damping is low, the peak occurs at frequencies lower than the natural frequency, making \( \omega_r \) important. For \( \omega_r < \sqrt{2} \), especially as it approaches 1, we generally find \( T > 1 \).
For higher damping levels, while the amplitude is decreased, transmissibility \( T \) remains greater than 1 due to the dominance of the denominator, specifically the \((1-\omega_r^2)^2\) term when close to resonance.
Thus, considering all damping factors and given \( \omega_r < \sqrt{2} \), the transmissibility \( T \) remains greater than unity.
The correct conclusion: greater than unity.