Step 1: Use charge conservation.
The total charge before and after connection must remain constant because the battery is removed.
Initial charge on first capacitor: \[ Q_i = C_1 V_1 = 10 \times 50 = 500 \, \text{pC} \]
Step 2: After connection, voltage becomes common.
Let \(C_2\) be the capacitance of the second capacitor and \(V_f = 20 \, \text{V}\). Final charge on both capacitors combined: \[ Q_f = (C_1 + C_2)V_f \] By conservation of charge: \[ Q_i = Q_f \Rightarrow 500 = (10 + C_2) \times 20 \] \[ 10 + C_2 = 25 \Rightarrow C_2 = 15 \, \text{pF} \]
Step 3: Conclusion.
Hence, the capacitance of the second capacitor = 15 pF.

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.)