A catalyst particle is modeled as a symmetrical double cone solid as shown in the figure. For each conical sub-part, the radius of the base is \( r \) and the height is \( h \). The sphericity of the particle is given by:

The sphericity of a particle is a measure of how closely the shape of the particle approximates that of a sphere. It is given by the formula:
\[ \phi = \frac{\text{Surface area of a sphere with same volume}}{\text{Surface area of the particle}} \]
For a double-cone shape:
Volume of a single cone:
\[
V_{\text{cone}} = \frac{1}{3} \pi r^2 h
\]
Surface area of a single cone:
\[
A_{\text{cone}} = \pi r \sqrt{r^2 + h^2}
\]
Since the particle consists of two identical cones, the total volume \( V_{\text{total}} \) and total surface area \( A_{\text{total}} \) are:
\[ V_{\text{total}} = 2 \times \frac{1}{3} \pi r^2 h = \frac{2}{3} \pi r^2 h \] \[ A_{\text{total}} = 2 \times \pi r \sqrt{r^2 + h^2} = 2 \pi r \sqrt{r^2 + h^2} \]
Now, the volume of a sphere with the same volume as the double cone is: \[ V_{\text{sphere}} = \frac{4}{3} \pi R^3 \] Equating the volumes of the sphere and the double cone: \[ \frac{4}{3} \pi R^3 = \frac{2}{3} \pi r^2 h \] Solving for \( R \): \[ R = \left( \frac{r^2 h}{2} \right)^{1/3} \]
The surface area of the sphere with radius \( R \) is: \[ A_{\text{sphere}} = 4 \pi R^2 = 4 \pi \left( \frac{r^2 h}{2} \right)^{2/3} \]
Finally, the sphericity \( \phi \) is the ratio of the surface area of the sphere to the surface area of the double cone: \[ \phi = \frac{4 \pi \left( \frac{r^2 h}{2} \right)^{2/3}}{2 \pi r \sqrt{r^2 + h^2}} = \frac{2 \left( \frac{r^2 h}{2} \right)^{2/3}}{r \sqrt{r^2 + h^2}} \]
Thus, the correct answer is (C).
An ideal monoatomic gas is contained inside a cylinder-piston assembly connected to a Hookean spring as shown in the figure. The piston is frictionless and massless. The spring constant is 10 kN/m. At the initial equilibrium state (shown in the figure), the spring is unstretched. The gas is expanded reversibly by adding 362.5 J of heat. At the final equilibrium state, the piston presses against the stoppers. Neglecting the heat loss to the surroundings, the final equilibrium temperature of the gas is __________ K (rounded off to the nearest integer).
The residence-time distribution (RTD) function of a reactor (in min$^{-1}$) is 
The mean residence time of the reactor is __________ min (rounded off to 2 decimal places).}
Ideal nonreacting gases A and B are contained inside a perfectly insulated chamber, separated by a thin partition, as shown in the figure. The partition is removed, and the two gases mix till final equilibrium is reached. The change in total entropy for the process is _________J/K (rounded off to 1 decimal place).
Given: Universal gas constant \( R = 8.314 \) J/(mol K), \( T_A = T_B = 273 \) K, \( P_A = P_B = 1 \) atm, \( V_B = 22.4 \) L, \( V_A = 3V_B \).
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).