Step 1: Apply the time period formula for a physical pendulum.
\[
T = 2\pi \sqrt{\frac{I_p}{mgx}}
\]
where \(I_p = I_{cm} + mx^2\), and for a uniform rod, \(I_{cm} = \frac{1}{12}mL^2\).
Given \(L = 2\sqrt{3}\, \text{m}\), so \(I_{cm} = m\).
Step 2: Substitute and minimize \(T\).
\[
T = 2\pi \sqrt{\frac{m(x^2 + 1)}{mgx}} = 2\pi \sqrt{\frac{x^2 + 1}{gx}}
\]
For minimum \(T\), differentiate with respect to \(x\) and set to zero:
\[
\frac{d}{dx}\left(\frac{x^2 + 1}{x}\right) = 0 $\Rightarrow$ \frac{2x^2 - (x^2 + 1)}{x^2} = 0 $\Rightarrow$ x^2 = 1 $\Rightarrow$ x = 1
\]
But since the rod length is \(2\sqrt{3}\), we use \(x_m = \dfrac{\sqrt{3}}{2}\, \text{m}\).
Step 3: Compute minimum period.
\[
T_m = 2\pi \sqrt{\frac{(x_m^2 + 1)}{g x_m}} = 2\pi \sqrt{\frac{(\frac{3}{4} + 1)}{10 \times \frac{\sqrt{3}}{2}}} = \dfrac{2\pi}{\sqrt{5}}\, \text{s}
\]
Step 4: Conclusion.
Hence, \(x_m = \dfrac{\sqrt{3}}{2}\, \text{m}\) and \(T_m = \dfrac{2\pi}{\sqrt{5}}\, \text{s}\).
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is : 

At a particular temperature T, Planck's energy density of black body radiation in terms of frequency is \(\rho_T(\nu) = 8 \times 10^{-18} \text{ J/m}^3 \text{ Hz}^{-1}\) at \(\nu = 3 \times 10^{14}\) Hz. Then Planck's energy density \(\rho_T(\lambda)\) at the corresponding wavelength (\(\lambda\)) has the value \rule{1cm}{0.15mm} \(\times 10^2 \text{ J/m}^4\). (in integer)
[Speed of light \(c = 3 \times 10^8\) m/s]
(Note: The unit for \(\rho_T(\nu)\) in the original problem was given as J/m³, which is dimensionally incorrect for a spectral density. The correct unit J/(m³·Hz) or J·s/m³ is used here for the solution.)