Solution:
The frequency of oscillation of a compass needle in a magnetic field is given by: $$ f = \frac{1}{2\pi} \sqrt{\frac{MB_H}{I}} $$ where:
$f$ is the frequency of oscillation
$M$ is the magnetic moment of the needle
$B_H$ is the horizontal component of the Earth's magnetic field
$I$ is the moment of inertia of the needle
Since $M$ and $I$ are constant, we have:
$$ f \propto \sqrt{B_H} $$ $$ f^2 \propto B_H $$ Also, $B_H = B \cos \delta$, where $B$ is the total magnetic field and $\delta$ is the dip angle. So, $f^2 \propto B \cos \delta$. Let $f_1 = 20$ oscillations/minute and $\delta_1 = 30^\circ$.
Let $f_2 = 30$ oscillations/minute and $\delta_2 = 60^\circ$. Then, $$ f_1^2 \propto B_1 \cos \delta_1 $$ $$ f_2^2 \propto B_2 \cos \delta_2 $$ Therefore, $$ \frac{f_1^2}{f_2^2} = \frac{B_1 \cos \delta_1}{B_2 \cos \delta_2} $$ Substituting the given values: $$ \frac{20^2}{30^2} = \frac{B_1 \cos 30^\circ}{B_2 \cos 60^\circ} $$ $$ \frac{400}{900} = \frac{B_1 (\sqrt{3}/2)}{B_2 (1/2)} $$ $$ \frac{4}{9} = \frac{B_1}{B_2} \sqrt{3} $$ $$ \frac{B_1}{B_2} = \frac{4}{9\sqrt{3}} $$ We are given that $\frac{B_1}{B_2} = \frac{4}{\sqrt{x}}$. Therefore, $$ \frac{4}{\sqrt{x}} = \frac{4}{9\sqrt{3}} $$ $$ \sqrt{x} = 9\sqrt{3} $$ $$ x = (9\sqrt{3})^2 = 81 \cdot 3 = 243 $$ Thus, $x = 243$.
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,


What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)