A cylindrical block of mass M and cross-sectional area A floats in a liquid (density ρ). When displaced vertically and released, it oscillates. We need to find the oscillation period.
At equilibrium, the block's weight (Mg) equals the buoyant force. Let the submerged depth be h. The buoyant force is $ F_B = A h \rho g $. Equating forces:
$ M g = A h \rho g $
If the block is depressed by a small distance x, the submerged depth increases to (h + x). The new buoyant force is $ F_B' = A(h+x)\rho g $. The net upward force, acting as the restoring force, is the difference between the new buoyant force and the weight:
$ F_{restore} = F_B' - Mg $ $ F_{restore} = A(h+x)\rho g - A h \rho g $ $ F_{restore} = A x \rho g $ This force opposes the displacement x, so the restoring force is $ F_{restore} = - A x \rho g $.
Using Newton's second law ($ F=Ma $, where $ a = \frac{d^2x}{dt^2} $):
$ M a = - A x \rho g $ $ M \frac{d^2x}{dt^2} = - A x \rho g $ The equation for SHM is $ \frac{d^2x}{dt^2} = -\omega^2 x $. Comparing, the square of the angular frequency ($ \omega^2 $) is:
$ \omega^2 = \frac{A \rho g}{M} $
The angular frequency is $ \omega = \sqrt{\frac{A \rho g}{M}} $. The period (T) is related to angular frequency by $ T = \frac{2\pi}{\omega} $.
$ T = \frac{2\pi}{\sqrt{\frac{A \rho g}{M}}} $ $ T = 2\pi \sqrt{\frac{M}{A \rho g}} $
The derived period of oscillation is $ T = 2\pi \sqrt{\frac{M}{\rho A g}} $. This expression matches Option 3. The provided correct answer is Option A.
A simple pendulum has a bob with mass $m$ and charge $q$. The pendulum string has negligible mass. When a uniform and horizontal electric field $\vec{E}$ is applied, the tension in the string changes. The final tension in the string, when pendulum attains an equilibrium position is _________.
(g: acceleration due to gravity)
In an open organ pipe $\nu_3$ and $\nu_6$ are $3^{\text{rd}}$ and $6^{\text{th}}$ harmonic frequencies, respectively. If $\nu_6 - \nu_3 = 2200 \text{ Hz}$ then length of the pipe is _________ mm.
(Take velocity of sound in air is $330 \text{ m/s}$.)
| List - I | List - II |
| A. $\sin^{2} \omega t$ | I. Periodic with time period $T=\frac{\pi}{\omega}$ but not simple harmonic motion (SHM) |
| B. $\sin^{3} (2\omega t)$ | II. Periodic with time period $T=\frac{2\pi}{\omega}$ but Not SHM |
| C. $\sin (\omega t) + \cos(\pi \omega t)$ | III. Periodic with time period $T=\frac{\pi}{\omega}$ and SHM |
| D. $\cos \omega t + \cos 2\omega t$ | IV. Non-periodic |
A simple pendulum has a bob with mass $m$ and charge $q$. The pendulum string has negligible mass. When a uniform and horizontal electric field $\vec{E}$ is applied, the tension in the string changes. The final tension in the string, when pendulum attains an equilibrium position is _________.
(g: acceleration due to gravity)
In an open organ pipe $\nu_3$ and $\nu_6$ are $3^{\text{rd}}$ and $6^{\text{th}}$ harmonic frequencies, respectively. If $\nu_6 - \nu_3 = 2200 \text{ Hz}$ then length of the pipe is _________ mm.
(Take velocity of sound in air is $330 \text{ m/s}$.)