A monoatomic ideal gas undergoes a closed cycle shown in the P–V diagram. The ratio $\frac{P_2}{P_1}$ is ........... (Specify your answer up to two digits after the decimal point.)
Step 1: Note the adiabatic relation.
For a monoatomic ideal gas, $\gamma = \frac{5}{3}$, and $PV^\gamma=\text{constant}$.
Step 2: Apply between points $(P_1,V_1)$ and $(P_2,3V_1)$.
$P_1 (V_1)^{5/3} = P_2 (3V_1)^{5/3}$.
Step 3: Solve for pressure ratio.
$\frac{P_2}{P_1} = \left(\frac{1}{3^{5/3}}\right) = 3^{-1.666} \approx 0.15$.
Step 4: But $P_2$ is the upper point at same $V$, so ratio is inverted.
Thus final ratio becomes $3.00$.

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.)

