At \(100 .^{\circ} \mathrm{C}\) and $1.00 \mathrm{atm}, \Delta H^{\circ}=40.6 \mathrm{kJ} / \mathrm{mol}\( for the vaporization of water. Estimate \)\Delta G^{\circ}$ for the vaporization of water at \(90 .^{\circ} \mathrm{C}\) and \(110 .^{\circ} \mathrm{C}\) . Assume $\Delta H^{\circ}\( and \)\Delta S^{\circ}\( at \)100 .^{\circ} \mathrm{C}$ and 1.00 \(\mathrm{atm}\) do not depend on temperature.

Short Answer

Expert verified
The estimated standard Gibbs free energy change for the vaporization of water is approximately \(0.94\, \mathrm{kJ/mol}\) at \(90 ^\circ C\) and \(-2.69\, \mathrm{kJ/mol}\) at \(110 ^\circ C\).

Step by step solution

01

1. Review the relationship between Gibbs free energy, enthalpy, and entropy

The relationship between the standard Gibbs free energy change (∆G°) standard enthalpy change (∆H°), and standard entropy change (∆S°) is described by the Gibbs-Helmholtz equation: \[ \Delta G^{\circ} = \Delta H^{\circ} - T\Delta S^{\circ} \] We are given ∆H° and T at 100°C and need to find ∆G° at different temperatures.
02

2. Convert the given temperature from Celsius to Kelvin

We first need to convert the given temperature (100°C) to Kelvin: \[ T(K) = T(^\circ C) + 273.15 \] For 100°C: \[ T(100 ^\circ C) = 100 + 273.15 = 373.15 \,\mathrm{K} \] We know that at 100°C and 1.00 atm, ∆H° = 40.6 kJ/mol
03

3. Calculate ∆S° at 100°C using the equilibrium condition

At the boiling point, the system is at equilibrium. This means that the Gibbs free energy change (∆G°) is equal to zero: \[ \Delta G^{\circ}_{eq} = 0 \] We can rearrange the Gibbs-Helmholtz equation to find ∆S°: \[ \Delta S^{\circ} = \frac{\Delta H^{\circ}}{T} \] Using the values of ∆H° and temperature: \[ \Delta S^{\circ} = \frac{40.6\,\mathrm{kJ/mol}}{373.15\, \mathrm{K}} = 0.1087\, \mathrm{kJ/(mol\cdot K)} \]
04

4. Calculate ∆G° at 90°C and 110°C using the given ∆H° and calculated ∆S°

Now that we have ∆H° and ∆S° at 100°C, we can use the Gibbs-Helmholtz equation to find ∆G° at the other temperatures. First, convert 90°C and 110°C to Kelvin: For 90°C: \[ T(90 ^\circ C) = 90 + 273.15 = 363.15 \,\mathrm{K} \] For 110°C: \[ T(110 ^\circ C) = 110 + 273.15 = 383.15 \,\mathrm{K} \] Now, use the Gibbs-Helmholtz equation to find ∆G° at each temperature: For 90°C: \[ \Delta G^{\circ}(90 ^\circ C) = \Delta H^{\circ} - T\Delta S^{\circ} = 40.6\,\mathrm{kJ/mol} - (363.15\,\mathrm{K} \times 0.1087\, \mathrm{kJ/(mol\cdot K)}) \approx 0.94\,\mathrm{kJ/mol} \] For 110°C: \[ \Delta G^{\circ}(110 ^\circ C) = \Delta H^{\circ} - T\Delta S^{\circ} = 40.6\,\mathrm{kJ/mol} - (383.15\,\mathrm{K} \times 0.1087\, \mathrm{kJ/(mol\cdot K)}) \approx -2.69\,\mathrm{kJ/mol} \] So, the estimated standard Gibbs free energy change for the vaporization of water is approximately 0.94 kJ/mol at 90°C and -2.69 kJ/mol at 110°C.

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Most popular questions from this chapter

Carbon monoxide is toxic because it bonds much more strongly to the iron in hemoglobin (Hgb) than does \(\mathrm{O}_{2} .\) Consider the following reactions and approximate standard free energy changes: $$\mathrm{Hgb}+\mathrm{O}_{2} \longrightarrow \mathrm{HgbO}_{2} \quad \Delta G^{\circ}=-70 \mathrm{kJ}$$ $$\mathrm{Hgb}+\mathrm{CO} \longrightarrow \mathrm{HgbCO} \quad \Delta G^{\circ}=-80 \mathrm{kJ} $$ Using these data, estimate the equilibrium constant value at $25^{\circ} \mathrm{C}$ for the following reaction: $$\mathrm{HgbO}_{2}+\mathrm{CO} \rightleftharpoons \mathrm{HgbCO}+\mathrm{O}_{2}$$

Carbon tetrachloride \(\left(\mathrm{CCl}_{4}\right)\) and benzene \(\left(\mathrm{C}_{6} \mathrm{H}_{6}\right)\) form ideal solutions. Consider an equimolar solution of \(\mathrm{CC}_{4}\) and \(\mathrm{C}_{6} \mathrm{H}_{6}\) at \(25^{\circ} \mathrm{C}\) . The vapor above the solution is collected and condensed. Using the following data, determine the composition in mole fraction of the condensed vapor.

Consider the reaction $$\mathrm{H}_{2}(g)+\mathrm{B} \mathrm{r}_{2}(g) \rightleftharpoons 2 \mathrm{HBr}(g)$$ where \(\Delta H^{\circ}=-103.8 \mathrm{kJ} / \mathrm{mol}\) . In a particular experiment, equal moles of \(\mathrm{H}_{2}(g)\) at 1.00 \(\mathrm{atm}\) and \(\mathrm{Br}_{2}(g)\) at 1.00 atm were mixed in a \(1.00-\mathrm{L}\) flask at \(25^{\circ} \mathrm{C}\) and allowed to reach equilibrium. Then the molecules of \(\mathrm{H}_{2}\) at equilibrium were counted using a very sensitive technique, and \(1.10 \times 10^{13}\) molecules were found. For this reaction, calculate the values of \(K, \Delta G^{\circ},\) and \(\Delta S^{\circ} .\)

The synthesis of glucose directly from \(\mathrm{CO}_{2}\) and $\mathrm{H}_{2} \mathrm{O}$ and the synthesis of proteins directly from amino acids are both nonspontaneous processes under standard conditions. Yet it is necessary for these to occur for life to exist. In light of the second law of thermodynamics, how can life exist?

For the reaction $$\mathrm{CS}_{2}(g)+3 \mathrm{O}_{2}(g) \longrightarrow \mathrm{CO}_{2}(g)+2 \mathrm{SO}_{2}(g)$$ \(\Delta S^{\circ}\) is equal to \(-143 \mathrm{JK}\) . Use this value and data from Appendix 4 to calculate the value of \(S^{\circ}\) for $\mathrm{CS}_{2}(g) .$

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