Step 1: Understanding the question.
We need to find which function has a discontinuity in its second derivative at \(x = 0\). Functions involving absolute values often cause discontinuities in higher-order derivatives.
Step 2: Evaluate derivatives.
For \( f(x) = x|x| \), \[ f(x) = \begin{cases} x^2, & x > 0 \\ -x^2, & x < 0 \end{cases} \] \[ f'(x) = \begin{cases} 2x, & x > 0 \\ -2x, & x < 0 \end{cases} \] At \(x = 0\), \(f'(x)\) is continuous (both sides approach 0). \[ f''(x) = \begin{cases} 2, & x > 0 \\ -2, & x < 0 \end{cases} \] So \(f''(x)\) is discontinuous at \(x = 0\).
Step 3: Conclusion.
Hence, \(f(x) = x|x|\) has a discontinuity in the second derivative at \(x = 0\).

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.)