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A plot of ln k against (1)/(T) (abscissa...

A plot of ln k against `(1)/(T)` (abscissa) is expected to be a straight line with intercept on coordinate axis equal to

A

`(DeltaS^(@))/(2.303 R)`

B

`(DeltaS^(@))/R`

C

`-(DeltaS^(@))/R`

D

`R xx DeltaS^(@)`

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The correct Answer is:
To solve the question regarding the intercept of the plot of ln k against (1/T), we can follow these steps: ### Step 1: Understand the relationship between Gibbs free energy and equilibrium constant We start with the equation that relates Gibbs free energy change (ΔG°) to the equilibrium constant (K): \[ \Delta G° = -RT \ln K \] Where: - \( \Delta G° \) = change in Gibbs free energy - R = universal gas constant - T = temperature in Kelvin - K = equilibrium constant ### Step 2: Use the Gibbs free energy equation We also know from thermodynamics that: \[ \Delta G° = \Delta H° - T \Delta S° \] Where: - \( \Delta H° \) = change in enthalpy - \( \Delta S° \) = change in entropy ### Step 3: Combine the equations Now, we can equate the two expressions for ΔG°: \[ -RT \ln K = \Delta H° - T \Delta S° \] ### Step 4: Rearrange the equation Rearranging this equation gives us: \[ -RT \ln K = \Delta H° - T \Delta S° \] \[ -RT \ln K = -T \Delta S° + \Delta H° \] Dividing through by -R, we have: \[ \ln K = -\frac{\Delta H°}{R} \cdot \frac{1}{T} + \frac{\Delta S°}{R} \] ### Step 5: Identify the slope and intercept This equation can be compared to the equation of a straight line \( y = mx + c \): - Here, \( y \) corresponds to \( \ln K \) - \( x \) corresponds to \( \frac{1}{T} \) - The slope \( m \) is \( -\frac{\Delta H°}{R} \) - The intercept \( c \) is \( \frac{\Delta S°}{R} \) ### Conclusion Thus, the intercept of the plot of \( \ln K \) against \( \frac{1}{T} \) is: \[ \text{Intercept} = \frac{\Delta S°}{R} \]

To solve the question regarding the intercept of the plot of ln k against (1/T), we can follow these steps: ### Step 1: Understand the relationship between Gibbs free energy and equilibrium constant We start with the equation that relates Gibbs free energy change (ΔG°) to the equilibrium constant (K): \[ \Delta G° = -RT \ln K \] Where: - \( \Delta G° \) = change in Gibbs free energy - R = universal gas constant ...
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