Match the List-I with List-II.
Choose the correct answer from the options given below:
1. Triatomic rigid gas (A): For a rigid triatomic gas, the ratio \( \frac{C_P}{C_V} \) is \( \frac{5}{3} \) because there are no additional degrees of freedom for rotation or vibration. Thus, A matches with I.
2. Diatomic non-rigid gas (B): For a non-rigid diatomic gas, the ratio \( \frac{C_P}{C_V} \) is \( \frac{7}{5} \), so B matches with II.
3. Monoatomic gas (C): For a monoatomic gas, the ratio \( \frac{C_P}{C_V} \) is \( \frac{4}{3} \), corresponding to C matching with III.
4. Diatomic rigid gas (D): For a rigid diatomic gas, the ratio \( \frac{C_P}{C_V} \) is \( \frac{9}{7} \), matching with D matching with IV.
Final Answer $\text{A-III, B-IV, C-I, D-II}$.
Given the formula for the adiabatic index \(\gamma\): \[ \gamma = 1 + \frac{2}{f} \] Where \( f \) is the degrees of freedom: - For a triatomic rigid gas, \( f = 6 \): \[ \gamma = 1 + \frac{2}{6} = \frac{4}{3} \] - For a diatomic non-rigid gas, \( f = 7 \): \[ \gamma = 1 + \frac{2}{7} = \frac{9}{7} \] - For a diatomic rigid gas, \( f = 5 \): \[ \gamma = 1 + \frac{2}{5} = \frac{7}{5} \] - For a monoatomic rigid gas, \( f = 3 \): \[ \gamma = 1 + \frac{2}{3} = \frac{5}{3} \] \[ \boxed{\gamma = \frac{5}{3}} \]
A hot plate is placed in contact with a cold plate of a different thermal conductivity as shown in the figure. The initial temperature (at time $t = 0$) of the hot plate and cold plate are $T_h$ and $T_c$, respectively. Assume perfect contact between the plates. Which one of the following is an appropriate boundary condition at the surface $S$ for solving the unsteady state, one-dimensional heat conduction equations for the hot plate and cold plate for $t>0$?

The following data is given for a ternary \(ABC\) gas mixture at 12 MPa and 308 K:

\(y_i\): mole fraction of component \(i\) in the gas mixture
\(\hat{\phi}_i\): fugacity coefficient of component \(i\) in the gas mixture at 12 MPa and 308 K
The fugacity of the gas mixture is _________ MPa (rounded off to 3 decimal places).
The internal energy of air in $ 4 \, \text{m} \times 4 \, \text{m} \times 3 \, \text{m} $ sized room at 1 atmospheric pressure will be $ \times 10^6 \, \text{J} $. (Consider air as a diatomic molecule)
