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.
Two simple pendulums having lengths $l_{1}$ and $l_{2}$ with negligible string mass undergo angular displacements $\theta_{1}$ and $\theta_{2}$, from their mean positions, respectively. If the angular accelerations of both pendulums are same, then which expression is correct?
A particle is subjected to simple harmonic motions as: $ x_1 = \sqrt{7} \sin 5t \, \text{cm} $ $ x_2 = 2 \sqrt{7} \sin \left( 5t + \frac{\pi}{3} \right) \, \text{cm} $ where $ x $ is displacement and $ t $ is time in seconds. The maximum acceleration of the particle is $ x \times 10^{-2} \, \text{m/s}^2 $. The value of $ x $ is:
If the roots of $\sqrt{\frac{1 - y}{y}} + \sqrt{\frac{y}{1 - y}} = \frac{5}{2}$ are $\alpha$ and $\beta$ ($\beta > \alpha$) and the equation $(\alpha + \beta)x^4 - 25\alpha \beta x^2 + (\gamma + \beta - \alpha) = 0$ has real roots, then a possible value of $y$ is: