To solve this problem, we need to understand the behavior of a damped harmonic oscillator. The amplitude of such an oscillator decreases exponentially over time. The relationship can be expressed as:
\( A(t) = A_0 e^{-\lambda t} \)
where:
Given that the amplitude reduces to half in 10 seconds, we can write the equation as:
\( \frac{1}{2}A_0 = A_0 e^{-\lambda \times 10} \)
Solving for \( \lambda \):
\( \frac{1}{2} = e^{-10\lambda} \)
Taking the natural logarithm on both sides:
\( \ln\left(\frac{1}{2}\right) = -10\lambda \)
This simplifies to:
\( \lambda = -\frac{\ln\left(\frac{1}{2}\right)}{10} = \frac{\ln(2)}{10} \)
Now, we find the amplitude after 30 seconds. The equation becomes:
\( A(30) = A_0 e^{-\lambda \times 30} \)
Substituting \( \lambda \):
\( A(30) = A_0 e^{-\frac{30 \ln(2)}{10}} = A_0 e^{-3 \ln(2)} \)
Recognizing that \( e^{-\ln(2)} = \frac{1}{2} \), thus \( e^{-3 \ln(2)} = \left(\frac{1}{2}\right)^3 \):
\( A(30) = A_0 \left(\frac{1}{2}\right)^3 = A_0 \times \frac{1}{8} \)
Therefore, the amplitude after 30 seconds will be \( \frac{1}{8} \) of the original amplitude.
Amplitude decays exponentially in damped SHM: \[ A(t) = A_0 e^{-bt} \] Given: \[ A(10) = \frac{A_0}{2} = A_0 e^{-10b} \Rightarrow e^{-10b} = \frac{1}{2} \] Take log: \[ -10b = \ln\left(\frac{1}{2}\right) = -\ln 2 \Rightarrow b = \frac{\ln 2}{10} \] Find \( A(30) \): \[ A(30) = A_0 e^{-30b} = A_0 e^{-3\ln 2} = A_0 \cdot 2^{-3} = \frac{A_0}{8} \]
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):