Step 1: Given Data
Mass \( m = 200 \, \text{kg} \),
Spring stiffness \( k = 40 \, \text{N/mm} = 40 \times 10^3 \, \text{N/m} \),
Damping factor \( \zeta = 0.22 \),
We need to find the time \( t \) when the deflection becomes \( \frac{1}{50} \)th of its initial value.
Step 2: Damped Natural Frequency and Time to Settle
The damped natural frequency \( \omega_d \) is given by the formula:
\[
\omega_d = \omega_n \sqrt{1 - \zeta^2}
\]
where \( \omega_n \) is the natural frequency of the system:
\[
\omega_n = \sqrt{\frac{k}{m}}
\]
Substituting the values:
\[
\omega_n = \sqrt{\frac{40 \times 10^3}{200}} = \sqrt{200} = 14.14 \, \text{rad/s}
\]
Now, calculate \( \omega_d \):
\[
\omega_d = 14.14 \times \sqrt{1 - (0.22)^2} = 14.14 \times \sqrt{0.9516} = 14.14 \times 0.975 = 13.8 \, \text{rad/s}
\]
The time to settle \( t_s \) is given by:
\[
t_s = \frac{4}{\zeta \omega_d}
\]
Substituting the values:
\[
t_s = \frac{4}{0.22 \times 13.8} = \frac{4}{3.036} = 1.32 \, \text{s}
\]
Step 3: Final Time for \( \frac{1}{50} \)th of Initial Deflection
The time to settle to \( \frac{1}{50} \)th of the initial deflection is proportional to the logarithmic decay:
\[
t = \frac{1}{\omega_d \zeta} \ln \left(\frac{\text{Initial deflection}}{\text{Final deflection}}\right)
\]
For the ratio \( \frac{1}{50} \):
\[
t = \frac{1}{13.8 \times 0.22} \ln (50) = \frac{1}{3.036} \times 3.912 = 0.455 \, \text{s}
\]
Step 4: Conclusion
Thus, the time to settle is \( \boxed{0.455} \, \text{s} \), and the correct answer is option (4).