The relationship between the temperature of a reaction, its standard enthalpy change, and the equilibrium constant at that temperature can be expressed as the following linear equation: $$ \ln K=\frac{-\Delta H^{\circ}}{R T}+\text { constant } $$ (a) Explain how this equation can be used to determine \(\Delta H^{\circ}\) experimentally from the equilibrium constants at several different temperatures. (b) Derive the preceding equation using relationships given in this chapter. To what is the constant equal?

Short Answer

Expert verified
(a) To determine ΔH° experimentally, measure K values at different temperatures (T) and plot \(\ln K\) against \(\frac{1}{T}\). The slope of the line equals \(\frac{-\Delta H^{\circ}}{R}\). Calculate ΔH° using \(\Delta H^{\circ} = -R \times (\text{slope})\). (b) The equation is derived using the van 't Hoff equation and integration. The constant C corresponds to the "constant" term in the given equation.

Step by step solution

01

(a) Using the equation to determine ΔH° experimentally

To determine ΔH° experimentally, we need to have equilibrium constants (K) at various temperatures (T). According to the given equation: \[ \ln K=\frac{-\Delta H^{\circ}}{R T}+\text { constant } \] This is a linear equation where the slope equals \(\frac{-\Delta H^{\circ}}{R}\) and the intercept is equal to the constant. By measuring K values at different temperatures (T) and making a plot of \(\ln K\) against \(\frac{1}{T}\), we can find the slope of the line corresponding to this dataset. Once we have the slope, we can calculate \(\Delta H^{\circ}\) using the formula: \[ \Delta H^{\circ} = -R \times (\text{slope}) \]
02

(b) Deriving the equation and identifying the constant

To derive the equation, we use the van 't Hoff equation: \[ \frac{\mathrm{d}(\ln K)}{\mathrm{d}T} = \frac{\Delta H^{\circ}}{RT^2} \] Now, we'll integrate this equation. Let's assume that the constant of integration is "C". Integrating both sides with respect to T, we get: \[ \int\frac{\mathrm{d}(\ln K)}{\mathrm{d}T} \mathrm{d}T = \int\frac{\Delta H^{\circ}}{RT^2} \mathrm{d}T \] \[ \ln K = -\frac{\Delta H^{\circ}}{R} \int\frac{1}{T^2} \mathrm{d}T + C \] Now, integrating the left side: \[ \int\frac{1}{T^2} \mathrm{d}T = \int T^{-2} \mathrm{d}T = -\frac{1}{T} \] Hence, the equation becomes: \[ \ln K = -\frac{\Delta H^{\circ}}{R}(-\frac{1}{T}) + C \] Simplifying the equation, we get: \[ \ln K = \frac{\Delta H^{\circ}}{RT} + C \] Comparing to the equation given in the exercise: \[ \ln K = \frac{-\Delta H^{\circ}}{R T}+\text { constant } \] We see that the constant C corresponds to the "constant" term in the given equation.

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Most popular questions from this chapter

Consider the vaporization of liquid water to steam at a pressure of 1 atm. (a) Is this process endothermic or exothermic? (b) In what temperature range is it a spontaneous process? (c) In what temperature range is it a nonspontaneous process? (d) At what temperature are the two phases in equilibrium?

Use Appendix \(\mathrm{C}\) to compare the standard entropies at \(25^{\circ} \mathrm{C}\) for the following pairs of substances: (a) \(\mathrm{Sc}(s)\) and \(\mathrm{Sc}(g)\), \(\mathrm{NH}_{3}(g)\) and \(\mathrm{NH}_{3}(a q)\) (c) \(1 \mathrm{~mol} \mathrm{P}_{4}(g)\) and \(2 \mathrm{~mol} \mathrm{P}_{2}(g)\), (d) C(graphite) and C(diamond). In each case explain the difference in the entropy values.

(a) If you are told that the entropy of a certain system is zero, what do you know about the system and the temperature? (b) The energy of a gas is increased by heating it. Using \(\mathrm{CO}_{2}\) as an example, illustrate the different ways in which additional energy can be distributed among the molecules of the gas. (c) \(\mathrm{CO}_{2}(g)\) and \(\mathrm{Ar}(g)\) have nearly the same molar mass. At a given temperature, will they have the same number of microstates? Explain.

The reaction $$ \mathrm{SO}_{2}(g)+2 \mathrm{H}_{2} \mathrm{~S}(g) \rightleftharpoons 3 \mathrm{~S}(s)+2 \mathrm{H}_{2} \mathrm{O}(g) $$ is the basis of a suggested method for removal of \(\mathrm{SO}_{2}\) from power-plant stack gases. The standard free energy of each substance is given in Appendix \(\mathrm{C}\). (a) What is the equilibrium constant for the reaction at \(298 \mathrm{~K}\) ? (b) In principle, is this reaction a feasible method of removing \(\mathrm{SO}_{2} ?\) (c) If \(P_{\mathrm{SO}_{2}}=P_{\mathrm{H}_{2} \mathrm{~S}}\) and the vapor pressure of water is 25 torr, calculate the equilibrium \(\mathrm{SO}_{2}\) pressure in the system at \(298 \mathrm{~K}\). (d) Would you expect the process to be more or less effective at higher temperatures?

(a) What is the meaning of the standard free-energy change, \(\Delta G^{\circ},\) as compared with \(\Delta G\) ? (b) For any process that occurs at constant temperature and pressure, what is the significance of \(\Delta G=0 ?(c)\) For a certain process, \(\Delta G\) is large and negative. Does this mean that the process necessarily occurs rapidly?

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