To solve this problem, we begin by considering the properties of simple harmonic motion. For a particle performing simple harmonic motion with amplitude \( A \), the velocity \( v \) at a displacement \( x \) is given by:
\( v = \omega \sqrt{A^2 - x^2} \)
where \(\omega\) is the angular frequency. At \( x = \frac{2A}{3} \), the initial speed \( v_1 \) is:
\( v_1 = \omega \sqrt{A^2 - \left(\frac{2A}{3}\right)^2} = \omega \sqrt{A^2 - \frac{4A^2}{9}} = \omega \sqrt{\frac{5A^2}{9}} = \omega \frac{\sqrt{5}A}{3} \)
When the speed triples, the new speed \( v_2 = 3v_1 \):
\( v_2 = 3 \times \omega \frac{\sqrt{5}A}{3} = \omega \sqrt{5}A \)
For the new amplitude \( A' = \frac{nA}{3} \), we write the expression for the new speed:
\( v_2 = \omega \sqrt{A'^2 - x^2} \)
At \( x = \frac{2A}{3} \), \( v_2 \) is also:
\( \omega \sqrt{A'^2 - \left(\frac{2A}{3}\right)^2} = \omega \sqrt{\left(\frac{nA}{3}\right)^2 - \frac{4A^2}{9}} \)
Equating the expressions for \( v_2 \), we have:
\( \omega \sqrt{5}A = \omega \sqrt{\frac{n^2A^2}{9} - \frac{4A^2}{9}} = \omega A \sqrt{\frac{n^2 - 4}{9}} \)
By canceling common terms and solving for \( n \), we get:
\( \sqrt{5} = \frac{\sqrt{n^2 - 4}}{3} \)
\( \sqrt{5} \times 3 = \sqrt{n^2 - 4} \)
Squaring both sides, we obtain:
\( 45 = n^2 - 4 \)
\( n^2 = 49 \)
So, \( n = 7 \) as \( n \) is positive. Thus, the value of \( n \) is 7, which falls within the expected range of 7 to 7.
At \( x = \frac{2A}{3} \),
\[ v = \omega \sqrt{A^2 - \left(\frac{2A}{3}\right)^2} = \omega \sqrt{\frac{5A^2}{9}} = \omega \frac{\sqrt{5}A}{3} \]New amplitude is \( A' \):
\[ v' = 3v = 3 \left( \omega \frac{\sqrt{5}A}{3} \right) = \omega \sqrt{(A')^2 - \left(\frac{2A}{3}\right)^2} \] \[ \omega \sqrt{5}A = \omega \sqrt{(A')^2 - \left(\frac{2A}{3}\right)^2} \]Squaring both sides:
\[ 5A^2 = (A')^2 - \left(\frac{2A}{3}\right)^2 \] \[ (A')^2 = 5A^2 + \left(\frac{4A^2}{9}\right) = \frac{45A^2}{9} + \frac{4A^2}{9} = \frac{49A^2}{9} \] \[ A' = \frac{7A}{3} \] \[ \therefore \, n = 7 \]In an oscillating spring mass system, a spring is connected to a box filled with sand. As the box oscillates, sand leaks slowly out of the box vertically so that the average frequency ω(t) and average amplitude A(t) of the system change with time t. Which one of the following options schematically depicts these changes correctly? 
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): 
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
The magnitude of heat exchanged by a system for the given cyclic process ABC (as shown in the figure) is (in SI units):
