To solve this problem, we need to make use of the adiabatic process relation for an ideal monoatomic gas. In an adiabatic process, the relationship between pressure and volume is given by:
\(P_1 V_1^\gamma = P_2 V_2^\gamma\)
Where:
From the problem, the gas is compressed to \(\left(\frac{1}{8}\right)^{\text{th}}\) of its initial volume. Thus, we have:
Substituting the values into the adiabatic equation, we get:
\(P_1 V_1^{\frac{5}{3}} = P_2 \left(\frac{V_1}{8}\right)^{\frac{5}{3}}\)
We can simplify this equation as follows:
\(P_1 V_1^{\frac{5}{3}} = P_2 \cdot \frac{V_1^{\frac{5}{3}}}{8^{\frac{5}{3}}}\)
\(P_1 = P_2 \cdot \frac{1}{8^{\frac{5}{3}}}\)
Rearranging for \(\frac{P_2}{P_1}\), we get:
\(\frac{P_2}{P_1} = 8^{\frac{5}{3}}\)
Calculating the value of \(8^{\frac{5}{3}}\):
\(8 = 2^3\), so \(8^{\frac{5}{3}} = (2^3)^{\frac{5}{3}} = 2^5 = 32\)
Therefore, the ratio of final pressure to initial pressure is 32.
Hence, the correct answer is 32.
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)
