An ideal gas undergoes an isothermal expansion along path AB, adiabatic expansion along BC, isobaric compression along CD, isothermal compression along DE, and adiabatic compression along EA, as shown in the figure. The work done by the gas along the process BC is 10 J. The change in the internal energy along process EA is 16 J. The absolute value of the change in the internal energy along the process CD is ............ J. 
Step 1: Recall the first law of thermodynamics.
\[ \Delta U = Q - W \] The internal energy change over a complete cycle is zero: \[ \sum \Delta U = 0 \] The work done over one complete cycle equals the total heat absorbed: \[ \sum Q = \sum W \]
Step 2: Analyze given processes.
- For isothermal processes (AB and DE): \(\Delta U = 0\). - For adiabatic processes (BC and EA): \(Q = 0\), hence \(\Delta U = -W\). Given \(W_{BC} = 10\, \text{J}\) ⇒ \(\Delta U_{BC} = -10\, \text{J}\). Also, \(\Delta U_{EA} = +16\, \text{J}\).
Step 3: Apply energy balance over full cycle.
\[ \Delta U_{BC} + \Delta U_{CD} + \Delta U_{EA} = 0 \] \[ (-10) + \Delta U_{CD} + (16) = 0 \Rightarrow \Delta U_{CD} = -6 \, \text{J} \] Hence, the absolute value of internal energy change: \[ |\Delta U_{CD}| = 6 \, \text{J} \]
Step 4: Conclusion.
The absolute value of the internal energy change during process CD is \(6\, \text{J}\).

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.)