Given a particle executing simple harmonic motion with mass \( m = 0.50 \, \text{kg} \) and force \( F = -50 \, (\text{N m}^{-1}) x \), we aim to find the value of \( x \) in the time period expression \( \frac{x}{35} \, \text{s} \). Using the formula for angular frequency \( \omega \) in simple harmonic motion, where the restoring force \( F = -kx \), with \( k = 50 \, \text{N m}^{-1} \), we write \( \omega = \sqrt{\frac{k}{m}} \).
Substitute the given values: \[ \omega = \sqrt{\frac{50}{0.50}} = \sqrt{100} = 10 \, \text{rad/s}. \]
The time period \( T \) is given by the formula: \[ T = \frac{2\pi}{\omega}. \]
Substitute \( \omega = 10 \) and \( \pi = \frac{22}{7} \): \[ T = \frac{2 \times \frac{22}{7}}{10} = \frac{44}{70} = \frac{22}{35} \, \text{s}. \]
Given \( T = \frac{x}{35} \, \text{s} \), equate and solve for \( x \): \[ \frac{x}{35} = \frac{22}{35}. \]
Clear fractions: \[ x = 22. \]
The calculated value of \( x \) is 22, which fits within the expected given range of 22,22.
The force is given by $F = -kx$, so $k = 50 \, \mathrm{Nm}^{-1}$. The mass $m = 0.50 \, \mathrm{kg}$. The time period for simple harmonic motion is:
\[ T = 2\pi \sqrt{\frac{m}{k}}. \]
Substituting $k = 50$ and $m = 0.5$:
\[ T = 2\pi \sqrt{\frac{0.5}{50}} = 2\pi \sqrt{0.01} = 2\pi \times 0.1 = 0.2\pi \, \mathrm{s}. \]
Given $T = \frac{x}{35}$, equating:
\[ 0.2\pi = \frac{x}{35}. \]
Substituting $\pi = \frac{22}{7}$:
\[ 0.2 \times \frac{22}{7} = \frac{x}{35}. \]
Simplifying: \[ x = 0.2 \times 22 \times 5 = 22. \]
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 : \(A_2 \rightleftharpoons 2A\)