This problem involves a floating, oscillating cylindrical cork and relates its time period of oscillation in two different liquids to their densities.
For a floating object, the weight (mg) equals the buoyant force. Let the cork have mass m and cross-sectional area A. When floating in a liquid of density $\rho$, submerged to a depth h, the buoyant force is $F_B = \rho A h g$. At equilibrium, $mg = \rho A h g$. This means the mass of the cork is constant: $m = \rho A h$.
When the cork is displaced vertically by a small distance x from its equilibrium position, the change in buoyant force provides the restoring force.
This matches the form $F = -kx$ for Simple Harmonic Motion (SHM), where the effective spring constant is $k = \rho A g$.
The time period T of SHM is given by $T = 2\pi \sqrt{\frac{m}{k}}$. Substituting $k = \rho A g$, we get:
$T = 2\pi \sqrt{\frac{m}{\rho A g}}$Since $m = \rho A h$, we can also write $T = 2\pi \sqrt{\frac{\rho A h}{\rho A g}} = 2\pi \sqrt{\frac{h}{g}}$. This shows the time period depends on the equilibrium submerged depth and gravity.
Alternatively, focusing on the spring constant:
$T \propto \frac{1}{\sqrt{k}} \propto \frac{1}{\sqrt{\rho A g}}$Since m, A, and g are constant for the cork and setup:
$T \propto \frac{1}{\sqrt{\rho}}$Let $T_1$ be the time period in liquid 1 (density $\rho_1$) and $T_2$ be the time period in liquid 2 (density $\rho_2$).
Using the proportionality $T \propto 1/\sqrt{\rho}$:
$\frac{T_1}{T_2} = \frac{1/\sqrt{\rho_1}}{1/\sqrt{\rho_2}} = \sqrt{\frac{\rho_2}{\rho_1}}$Substitute the given time periods:
$\frac{T}{2T} = \sqrt{\frac{\rho_2}{\rho_1}}$ $\frac{1}{2} = \sqrt{\frac{\rho_2}{\rho_1}}$Squaring both sides to find the ratio:
$\left(\frac{1}{2}\right)^2 = \frac{\rho_2}{\rho_1}$ $\frac{1}{4} = \frac{\rho_2}{\rho_1}$Therefore, the value of $\rho_2/\rho_1$ is $\frac{1}{4}$.
For a travelling harmonic wave $y(x, t) = 2.0 \cos 2\pi(10 t - 0.0080 x + 0.35)$, where $x$ and $y$ are in cm and $t$ in s. The phase difference between oscillatory motion of two points separated by a distance of $0.5 \text{ m}$ is :
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 $330 \text{ m/s}$.)