Problem 174
Question
The incorrect expression among the following is (a) \(\ln \mathrm{K}=\frac{\Delta \mathrm{H}^{\circ}-\mathrm{T} \Delta \mathrm{S}^{\circ}}{\mathrm{RT}}\) (b) In isothermal process \(\mathrm{W}_{\text {reversible }}=-\mathrm{nRT} \operatorname{In} \frac{\mathrm{V}_{\mathrm{f}}}{\mathrm{V}_{1}}\) (c) \(\frac{\Delta \mathrm{G}_{\text {System }}}{\Delta \mathrm{S}_{\text {total }}}=-\mathrm{T}\) (d) \(\mathrm{K}=\mathrm{e}^{\Delta \mathrm{G}^{\circ} / \mathrm{RT}}\)
Step-by-Step Solution
Verified Answer
Expressions (a) and (c) are incorrect.
1Step 1: Analyze each expression for correctness according to thermodynamic equations and principles
**(a) \( \ln \mathrm{K}=\frac{\Delta \mathrm{H}^{\circ}-\mathrm{T} \Delta \mathrm{S}^{\circ}}{\mathrm{RT}} \)**This expression relates the equilibrium constant \( \mathrm{K} \) with the change in enthalpy \( \Delta \mathrm{H}^{\circ} \) and entropy \( \Delta \mathrm{S}^{\circ} \) using temperature \( \mathrm{T} \) and the gas constant \( \mathrm{R} \). The Gibbs free energy equation at standard conditions is used: \[ \Delta \mathrm{G}^{\circ} = \Delta \mathrm{H}^{\circ} - \mathrm{T} \Delta \mathrm{S}^{\circ} \]The correct form for \( \ln \mathrm{K} \) is:\[ \ln \mathrm{K}=\frac{-\Delta \mathrm{G}^{\circ}}{\mathrm{RT}} \]Since the expression in (a) does not match, it is incorrect.
2Step 2: Confirm correctness of expressions (b), (c), and (d)
**(b) In an isothermal process \( \mathrm{W}_{\text {reversible }}=-\mathrm{nRT} \operatorname{In} \frac{\mathrm{V}_{\mathrm{f}}}{\mathrm{V}_{1}} \):**This is the equation for the work done in a reversible isothermal process for an ideal gas. It is consistent with thermodynamic principles.**(c) \( \frac{\Delta \mathrm{G}_{\text {System }}}{\Delta \mathrm{S}_{\text{total }}}=-\mathrm{T} \):**This expression is incorrect according to the Second Law of Thermodynamics. For spontaneity, the correct equation is:\[ \Delta \mathrm{G}_{\text{System}} = -T \Delta S_{\text{total}} \]Thus, it simplifies to \( -\Delta S_{\text{total}} = \frac{\Delta G_{\text{System}}}{T} \) and must be correlated with the sign of \( \Delta G_{\text{System}} \), not the division expression provided.**(d) \( \mathrm{K}=\mathrm{e}^{\Delta \mathrm{G}^{\circ} / \mathrm{RT}} \):**This represents the relation between equilibrium constant \( \mathrm{K} \) and standard Gibbs free energy change \( \Delta \mathrm{G}^{\circ} \), which is correctly described by:\[ \mathrm{K}=\mathrm{e}^{-\Delta \mathrm{G}^{\circ} / \mathrm{RT}} \]Indicating the exponent should be negative.
Key Concepts
Gibbs Free EnergyEquilibrium ConstantEntropyEnthalpy
Gibbs Free Energy
Gibbs free energy is a vital concept in thermodynamics, signifying the maximum reversible work a thermodynamic system can perform at constant temperature and pressure. The equation connecting Gibbs free energy to other thermodynamic quantities is:\[ \Delta G = \Delta H - T \Delta S \]where:
- \( \Delta G \) is the change in Gibbs free energy,
- \( \Delta H \) is the change in enthalpy,
- \( T \) is the temperature in Kelvin, and
- \( \Delta S \) is the change in entropy.
Equilibrium Constant
The equilibrium constant \( K \) depicts the ratio of the concentrations of products to reactants at equilibrium for a reversible chemical reaction. It serves as an indicator of the favorability of a reaction's completion.
In thermodynamic terms, \( K \) is directly related to Gibbs free energy using the formula:\[ K = e^{-\Delta G^{\circ} / RT} \]This connection is pivotal because it links the concepts of thermodynamics with chemical equilibrium. When \( \Delta G^{\circ} \) is negative, it results in a large positive \( K \), signifying that the products are favored.
The temperature dependency of the equilibrium constant can be clearly differentiated using the Van 't Hoff equation:\[ \ln K = \frac{-\Delta H^{\circ} + T \Delta S^{\circ}}{RT} \]This indicates how changes in temperature affect \( K \), essentially amending the favorability of either the products or reactants at equilibrium. A thorough understanding of \( K \) solidifies one's grip over the dynamic nature of chemical systems.
In thermodynamic terms, \( K \) is directly related to Gibbs free energy using the formula:\[ K = e^{-\Delta G^{\circ} / RT} \]This connection is pivotal because it links the concepts of thermodynamics with chemical equilibrium. When \( \Delta G^{\circ} \) is negative, it results in a large positive \( K \), signifying that the products are favored.
The temperature dependency of the equilibrium constant can be clearly differentiated using the Van 't Hoff equation:\[ \ln K = \frac{-\Delta H^{\circ} + T \Delta S^{\circ}}{RT} \]This indicates how changes in temperature affect \( K \), essentially amending the favorability of either the products or reactants at equilibrium. A thorough understanding of \( K \) solidifies one's grip over the dynamic nature of chemical systems.
Entropy
Entropy \( S \) is a measure of the disorder or randomness in a thermodynamic system. The concept becomes essential when discussing spontaneity and the direction of processes. Entropy change \( \Delta S \) can be understood as the measure of energy dispersion in a system. The Second Law of Thermodynamics states that the total entropy of an isolated system can never decrease over time.
Thermodynamically:\[ \Delta G = \Delta H - T \Delta S \]The balance of these components, enthalpy \( \Delta H \) and entropy \( \Delta S \), dictates the spontaneity of a reaction. Processes with positive \( \Delta S \) are often spontaneous because they conform to natural tendencies of systems to disperse energy.
Thermodynamically:\[ \Delta G = \Delta H - T \Delta S \]The balance of these components, enthalpy \( \Delta H \) and entropy \( \Delta S \), dictates the spontaneity of a reaction. Processes with positive \( \Delta S \) are often spontaneous because they conform to natural tendencies of systems to disperse energy.
- High entropy configurations signify likely states under equilibrium.
- Entropy changes also determine how temperature affects reaction spontaneity.
Enthalpy
Enthalpy \( H \) is a measure of the total heat content of a system, functionally defined as \( H = U + PV \), where \( U \) is internal energy, and \( P \) and \( V \) are pressure and volume, respectively.
It reflects the heat absorbed or released under constant pressure when a process occurs. A positive \( \Delta H \) indicates an endothermic process, while a negative \( \Delta H \) reflects an exothermic process.
In terms of Gibbs free energy, enthalpy plays a direct role in calculating spontaneity:\[ \Delta G = \Delta H - T \Delta S \]A lower enthalpy generally drives systems toward equilibrium by reducing \( \Delta G \) when not counteracted by entropy changes. The connection between enthalpy changes \( \Delta H \) and the equilibrium constant \( K \) is also described by the Van 't Hoff equation, which examines how temperature variations impact system balance.
It reflects the heat absorbed or released under constant pressure when a process occurs. A positive \( \Delta H \) indicates an endothermic process, while a negative \( \Delta H \) reflects an exothermic process.
In terms of Gibbs free energy, enthalpy plays a direct role in calculating spontaneity:\[ \Delta G = \Delta H - T \Delta S \]A lower enthalpy generally drives systems toward equilibrium by reducing \( \Delta G \) when not counteracted by entropy changes. The connection between enthalpy changes \( \Delta H \) and the equilibrium constant \( K \) is also described by the Van 't Hoff equation, which examines how temperature variations impact system balance.
- \( \Delta H \) helps predict heat flow tendencies.
- Detailed knowledge of \( \Delta H \) guides the studying of reaction energetics and pathways.
Other exercises in this chapter
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