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, $x = 243$.
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):
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: