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What is DeltaG^(ɵ) for the following rea...

What is `DeltaG^(ɵ)` for the following reaction? `1/2 N_(2)(g)+3/2 H_(2)(g) hArr NH_(3)(g), K_(p)=4.42xx10^(4)` at `25^(@)C`

A

`-26.5 kJ mol^(-1)`

B

`11.5 kJ mol^(-1)`

C

`-2.2 kJ mol^(-1)`

D

`-0.97 kJ mol^(-1)`

Text Solution

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To find the standard Gibbs free energy change (ΔG°) for the reaction given the equilibrium constant (Kp), we can use the following relationship: \[ \Delta G^{\circ} = -RT \ln K_p \] ### Step-by-Step Solution: 1. **Identify Constants**: - The universal gas constant \( R = 8.31 \, \text{J/(mol·K)} \). - The temperature \( T = 25^\circ C = 298 \, \text{K} \). - The equilibrium constant \( K_p = 4.42 \times 10^4 \). 2. **Convert Kp to Natural Logarithm**: - We need to calculate \( \ln K_p \). - First, calculate \( K_p \): \[ K_p = 4.42 \times 10^4 \] - Now, find \( \ln K_p \): \[ \ln K_p = \ln(4.42 \times 10^4) \] 3. **Use the Change of Base Formula**: - To convert from natural logarithm to base 10, we can use: \[ \ln K = 2.303 \log_{10} K \] - Therefore: \[ \ln(4.42 \times 10^4) = 2.303 \log_{10}(4.42 \times 10^4) \] 4. **Calculate Logarithm**: - Calculate \( \log_{10}(4.42 \times 10^4) \): \[ \log_{10}(4.42 \times 10^4) = \log_{10}(4.42) + \log_{10}(10^4) = 0.646 + 4 = 4.646 \] - Now, substitute back to find \( \ln K_p \): \[ \ln K_p = 2.303 \times 4.646 \approx 10.688 \] 5. **Calculate ΔG°**: - Now substitute \( R \), \( T \), and \( \ln K_p \) into the ΔG° equation: \[ \Delta G^{\circ} = - (8.31 \, \text{J/(mol·K)}) \times (298 \, \text{K}) \times (10.688) \] - Calculate: \[ \Delta G^{\circ} = - (8.31 \times 298 \times 10.688) \approx -26,500 \, \text{J/mol} = -26.5 \, \text{kJ/mol} \] 6. **Final Answer**: - Therefore, the standard Gibbs free energy change for the reaction is: \[ \Delta G^{\circ} \approx -26.5 \, \text{kJ/mol} \]

To find the standard Gibbs free energy change (ΔG°) for the reaction given the equilibrium constant (Kp), we can use the following relationship: \[ \Delta G^{\circ} = -RT \ln K_p \] ### Step-by-Step Solution: ...
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