Step 1: The amplitude of the damped oscillator is given by the exponential term in the displacement equation: \[ A(t) = A_0 \exp(-0.2t) \] where \( A_0 \) is the initial amplitude.
Step 2: We are asked to find the time when the amplitude becomes \( \frac{1}{e^{1.2}} \) times its initial amplitude. This means: \[ A(t) = \frac{A_0}{e^{1.2}} \] Substitute the expression for \( A(t) \): \[ A_0 \exp(-0.2t) = \frac{A_0}{e^{1.2}} \]
Step 3: Cancel \( A_0 \) from both sides: \[ \exp(-0.2t) = \frac{1}{e^{1.2}} \] Taking the natural logarithm of both sides: \[ -0.2t = -1.2 \] \[ t = \frac{-1.2}{-0.2} = 6 \, \text{s} \] Thus, the time required for the amplitude to become \( \frac{1}{e^{1.2}} \) times its initial amplitude is 6 s.
The displacement of a particle executing simple harmonic motion is \( y = A \sin(2\pi t + \phi) \, \text{m} \), where \( t \) is time in seconds and \( \phi \) is the phase angle. At time \( t = 0 \), the displacement and velocity of the particle are 2 m and 4 ms-1. The phase angle, \( \phi \) =