To solve the problem, we begin by understanding the relationship between the frequency of oscillations and the mass attached to the spring, given by the formula for the frequency of a mass-spring system: \( f = \frac{1}{2\pi}\sqrt{\frac{k}{m}} \), where \( k \) is the spring constant and \( m \) is the mass.
For mass \( m \), the frequency is \( f_1 = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \).
For mass \( 9m \), the frequency is \( f_2 = \frac{1}{2\pi} \sqrt{\frac{k}{9m}} = \frac{1}{2\pi} \frac{1}{3} \sqrt{\frac{k}{m}} = \frac{1}{3} \cdot f_1 \).
Thus, \(\frac{f_1}{f_2} = \frac{f_1}{\frac{1}{3}f_1} = 3\).
Hence, the value of \(\frac{f_1}{f_2}\) is clearly \( 3 \), which falls within the given range 3,3.
Given: - Mass of first system: \( m \) - Mass of second system: \( 9m \) - Frequencies: \( f_1 \) and \( f_2 \)
The frequency of oscillation of a mass-spring system is given by:
\[ f = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \]
where \( k \) is the spring constant and \( m \) is the mass.
For the first system with mass \( m \):
\[ f_1 = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \]
For the second system with mass \( 9m \):
\[ f_2 = \frac{1}{2\pi} \sqrt{\frac{k}{9m}} = \frac{1}{2\pi} \cdot \frac{1}{3} \sqrt{\frac{k}{m}} = \frac{f_1}{3} \]
\[ \frac{f_1}{f_2} = \frac{f_1}{\frac{f_1}{3}} = 3 \]
Conclusion: The value of \( \frac{f_1}{f_2} \) is \( 3 \).
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 : \(A_2 \rightleftharpoons 2A\)