Step 1: Using the Gibbs Free Energy and Equilibrium Constant Relation
The standard Gibbs free energy change \( \Delta_r G^\circ \) is related to the equilibrium constant \( K \) by: \[ \Delta_r G^\circ = - RT \ln K \] where: - \( R = 8.314 \) J mol\(^{-1}\) K\(^{-1}\) = \( 8.314 \times 10^{-3} \) kJ mol\(^{-1}\) K\(^{-1}\),
- \( T = 300 \) K,
- \( \Delta_r G^\circ = -11.5 \) kJ mol\(^{-1}\).
Step 2: Rearranging for \( K \) \[ \ln K = \frac{-\Delta_r G^\circ}{RT} \] Substituting values: \[ \ln K = \frac{-(-11.5)}{(8.314 \times 10^{-3}) \times 300} \] \[ \ln K = \frac{11.5}{2.4942} \] \[ \ln K \approx 4.61 \] Step 3: Finding \( K \)
Taking the exponent: \[ K = e^{4.61} \] Approximating: \[ e^{4.61} \approx 100 \] Final Answer: The equilibrium constant is approximately \( 100 \), which matches Option (2).
A piston of mass M is hung from a massless spring whose restoring force law goes as F = -kx, where k is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature T) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $ L_0 $ to $ L_1 $, the total energy delivered by the filament is (Assume spring to be in its natural length before heating) 