Step 1: Use the relation between molar enthalpy of fusion and cryoscopic constant. The formula relating the enthalpy of fusion (\(\Delta H_f\)) to the cryoscopic constant (\(K_f\)) is: \[ \Delta H_f = \frac{R T^2 K_f}{1000} \] where: - \( R = 8.314 \) J mol\(^{-1}\)K\(^{-1}\) (universal gas constant), - \( T = 273 \) K (freezing point of water), - \( K_f = 1.86 \) K kg mol\(^{-1}\).
Step 2: Substitute the values into the equation. \[ \Delta H_f = \frac{(8.314) \times (273)^2 \times (1.86)}{1000} \] \[ \Delta H_f = \frac{8.314 \times 74529 \times 1.86}{1000} \] \[ \Delta H_f = \frac{1155152.5}{1000} = 6.1 { kJ/mol} \] Approximating, we get 6 kJ/mol. Thus, the correct answer is 6 kJ/mol.
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____