Given:
We are asked to calculate \( \Delta G^\circ \) using the formula:
\[ \Delta G^\circ = -RT \ln K \]
Step 1: Substituting the known values into the equation:
Given that \( R = 8.314 \, \text{J/molK} \), \( T = 300 \, \text{K} \), and \( K = 10 \), we substitute these values into the equation:
\[ \Delta G^\circ = -8.314 \times 300 \ln(10) \]
Step 2: Simplifying the equation:
Calculating the logarithm of 10:
\[ \Delta G^\circ = -8.314 \times 300 \times 2.3026 \]
This simplifies to:
\[ \Delta G^\circ = -5744.14 \, \text{J/mol} \]
Step 3: Converting to kJ/mol:
To express the result in kJ/mol, divide by 1000:
\[ \Delta G^\circ = -5.744 \, \text{kJ/mol} \quad \Rightarrow \quad \Delta G^\circ = 57.44 \times 10^{-1} \, \text{kJ/mol} \]
Final Answer:
The correct answer is \( 57 \, \text{kJ/mol} \).
Step-by-step Calculation:
The standard Gibbs free energy change \( \Delta G^\circ \) for a reaction is related to the equilibrium constant \( K \) by the equation:
\[\Delta G^\circ = -RT \ln K\]
where:
\( R = 8.314 \, \text{J K}^{-1} \text{mol}^{-1} \) (Universal gas constant)
\( T = 300 \, \text{K} \)
\( K = 10 \)
Substituting the values into the equation:
\[\Delta G^\circ = -8.314 \times 300 \times \ln(10)\]
We know that \( \ln(10) \approx 2.303 \).
Therefore:
\[\Delta G^\circ = -8.314 \times 300 \times 2.303\]
\[\Delta G^\circ = -8.314 \times 690.9 \approx -5730 \, \text{J mol}^{-1}\]
Converting to \( \text{kJ mol}^{-1} \):
\[\Delta G^\circ = -5.73 \, \text{kJ mol}^{-1}\]
Expressing in the required format:
\[\Delta G^\circ = -57 \times 10^{-1} \, \text{kJ mol}^{-1}\]
Conclusion: The value of \( \Delta G^\circ \) for the reaction is \( -57 \times 10^{-1} \, \text{kJ mol}^{-1} \).
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) 
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: