For a dynamical system governed by the equation
\[
\ddot{x}(t) + 2 \zeta \omega_n \dot{x}(t) + \omega_n^2 x(t) = 0,
\]
the damping ratio is given as \( \zeta = \frac{1}{2\pi} \log_e 2 \).
A displacement peak in the positive direction is measured as 4 mm.
Neglecting higher powers (\(>1\)) of damping ratio, the displacement at the next peak (positive direction) will be ________________ mm (integer).
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For lightly damped systems, the logarithmic decrement simplifies using \( \delta \approx 2\pi \zeta \), which makes peak-to-peak amplitude calculations straightforward.
For an underdamped system undergoing free vibration, the ratio of successive peak amplitudes is given by the logarithmic decrement formula:
\[
\delta = \ln\left(\frac{x_1}{x_2}\right)
\]
and for small damping,
\[
\delta \approx 2\pi \zeta.
\]
Given:
\[
\zeta = \frac{1}{2\pi}\log_e 2
\]
So,
\[
\delta = 2\pi \zeta = 2\pi \left( \frac{1}{2\pi}\log_e 2 \right) = \log_e 2.
\]
Thus,
\[
\frac{x_1}{x_2} = e^{\delta} = e^{\log_e 2} = 2.
\]
Given first peak:
\[
x_1 = 4\ \text{mm}
\]
So the next peak is:
\[
x_2 = \frac{x_1}{2} = \frac{4}{2} = 2\ \text{mm}.
\]
Therefore, the displacement at the next peak in the positive direction is \(2\) mm.