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:
\[ 5A^2 = (A')^2 - \left(\frac{2A}{3}\right)^2 \] \[ (A')^2 = 5A^2 + \left(\frac{4A^2}{9}\right) = \frac{45A^2}{9} + \frac{4A^2}{9} = \frac{49A^2}{9} \] \[ A' = \frac{7A}{3} \] \[ \therefore \, n = 7 \]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 : \(A_2 \rightleftharpoons 2A\)