Use the following data to estimate the standard molar entropy of gaseous benzene at \(298.15 \mathrm{K} ;\) that is, \(S^{\circ}\left[\mathrm{C}_{6} \mathrm{H}_{6}(\mathrm{g}, 1 \mathrm{atm})\right] .\) For \(\mathrm{C}_{6} \mathrm{H}_{6}(\mathrm{s}, 1 \mathrm{atm})\) at its melting point of \(5.53^{\circ} \mathrm{C}, S^{\circ}\) is \(128.82 \mathrm{Jmol}^{-1} \mathrm{K}^{-1}\). The enthalpy of fusion is \(9.866 \mathrm{kJ} \mathrm{mol}^{-1} .\) From the melting point to 298.15 K, the average heat capacity of liquid benzene is \(134.0 \mathrm{JK}^{-1} \mathrm{mol}^{-1} .\) The enthalpy of vaporization of \(\mathrm{C}_{6} \mathrm{H}_{6}(1)\) at \(298.15 \mathrm{K}\) is \(33.85 \mathrm{kJ} \mathrm{mol}^{-1},\) and in the vapor- ization, \(\mathrm{C}_{6} \mathrm{H}_{6}(\mathrm{g})\) is produced at a pressure of 95.13 Torr. Imagine that this vapor could be compressed to 1 atm pressure without condensing and while behaving as an ideal gas. Calculate \(S^{\circ}\left[\mathrm{C}_{6} \mathrm{H}_{6}(\mathrm{g}, 1 \text { atm) }] .[ \text { Hint: Refer to }\right.\) Exercise \(88,\) and note the following: For infinitesimal quantities, \(d S=d q / d T ;\) for the compression of an ideal gas, \(d q=-d w ;\) and for pressure-volume work, \(d w=-P d V\).

Short Answer

Expert verified
The total entropy calculated by adding entropy changes (in Jmol-1K-1) due to fusion, heating, vaporization and compression to the initial entropy given will give the final molar entropy of gaseous benzene at 298.15 K and 1 atm pressure.

Step by step solution

01

Calculate entropy change during fusion

First, entropy change associated with the process when benzene changes from solid to liquid at its melting point can be calculated using the formula: \[ \Delta S_{\text{fusion}} = \dfrac{\Delta H_{\text{fusion}}}{T_{\text{m}}} \] where \(\Delta H_{\text{fusion}} = 9.866 \, \text{kJ/mol}\) (enthalpy of fusion), and \(T_{\text{m}} = 5.53^{\circ}C = 278.68 \, K\). Substituting these into the formula yields \(\Delta S_{\text{fusion}}\).
02

Calculate entropy change during heating of liquid

Then, entropy change during heating the liquid benzene from melting point to 298.15 K is calculated using the formula: \[ \Delta S_{\text{heating}} = \int_{T_{\text{m}}}^{T_{\text{b}}} \dfrac{C_{p}}{T} \, dT \] where \(C_{p}\) is the heat capacity at constant pressure which is \(134.0 \, \text{JK}^{-1} \text{mol}^{-1}\), \(T_{\text{m}}\) is the melting temperature (278.68 K), and \(T_{\text{b}}\) is the given temperature (298.15 K). On simplification the integral yields an expression for \(\Delta S_{\text{heating}}\).
03

Calculate entropy change during vaporization

Next, entropy change during vaporization of benzene at 298.15 K is calculated by the formula: \[ \Delta S_{\text{vaporization}} = \dfrac{\Delta H_{\text{vaporization}}}{T_{\text{b}}} \] where \(\Delta H_{\text{vaporization}} = 33.85 \, \text{kJ/mol}\) and \(T_{\text{b}} = 298.15 \, K\). Substituting these into the formula will yield \(\Delta S_{\text{vaporization}}\).
04

Calculate entropy change during pressure change of gas

Entropy change during compression process of an ideal gas is calculated by the formula: \[ \Delta S_{\text{compression}} = R \ln \left( \dfrac{P_{2}}{P_{1}} \right) \] where \(R\) is universal gas constant (8.314 Jmol-1K-1), \(P_{1}\) is initial pressure (95.13 Torr = 0.125 atm) and \(P_{2}\) is final pressure (1 atm). Substituting these into the formula yields \(\Delta S_{\text{compression}}\).
05

Calculate total entropy change

Total entropy change is given by the sum of all individual entropy changes: \[ S^{\circ}[\text{C}_{6} \text{H}_{6}(\text{g}, 1 \text{atm})] = S^{\circ}[\text{C}_{6} \text{H}_{6}(\text{s}, 1 \text{atm})] + \Delta S_{\text{fusion}} + \Delta S_{\text{heating}} + \Delta S_{\text{vaporization}} + \Delta S_{\text{compression}} \] by substituting known values, the value for \( S^{\circ}[\text{C}_{6} \text{H}_{6}(\text{g}, 1 \text{atm})] \) is calculated.

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Most popular questions from this chapter

Briefly describe each of the following ideas, methods, or phenomena: (a) absolute molar entropy; (b) coupled reactions; (c) Trouton's rule; (d) evaluation of an equilibrium constant from tabulated thermodynamic data.

Titanium is obtained by the reduction of \(\mathrm{TiCl}_{4}(1)\) which in turn is produced from the mineral rutile \(\left(\mathrm{TiO}_{2}\right)\) (a) With data from Appendix D, determine \(\Delta G^{\circ}\) at 298 K for this reaction. $$\mathrm{TiO}_{2}(\mathrm{s})+2 \mathrm{Cl}_{2}(\mathrm{g}) \longrightarrow \mathrm{TiCl}_{4}(1)+\mathrm{O}_{2}(\mathrm{g})$$ (b) Show that the conversion of \(\mathrm{TiO}_{2}(\mathrm{s})\) to \(\mathrm{TiCl}_{4}(1)\) with reactants and products in their standard states, is spontaneous at \(298 \mathrm{K}\) if the reaction in (a) is coupled with the reaction $$2 \mathrm{CO}(\mathrm{g})+\mathrm{O}_{2}(\mathrm{g}) \longrightarrow 2 \mathrm{CO}_{2}(\mathrm{g})$$

Comment on the difficulties of solving environmental pollution problems from the standpoint of entropy changes associated with the formation of pollutants and with their removal from the environment.

For each of the following reactions, indicate whether \(\Delta S\) for the reaction should be positive or negative. If it is not possible to determine the sign of \(\Delta S\) from the information given, indicate why. (a) \(\mathrm{CaO}(\mathrm{s})+\mathrm{H}_{2} \mathrm{O}(\mathrm{l}) \longrightarrow \mathrm{Ca}(\mathrm{OH})_{2}(\mathrm{s})\) (b) \(2 \mathrm{HgO}(\mathrm{s}) \longrightarrow 2 \mathrm{Hg}(1)+\mathrm{O}_{2}(\mathrm{g})\) (c) \(2 \mathrm{NaCl}(1) \longrightarrow 2 \mathrm{Na}(1)+\mathrm{Cl}_{2}(\mathrm{g})\) (d) \(\mathrm{Fe}_{2} \mathrm{O}_{3}(\mathrm{s})+3 \mathrm{CO}(\mathrm{g}) \longrightarrow 2 \mathrm{Fe}(\mathrm{s})+3 \mathrm{CO}_{2}(\mathrm{g})\) (e) \(\operatorname{Si}\left(\text { s) }+2 \mathrm{Cl}_{2}(\mathrm{g}) \longrightarrow \mathrm{SiCl}_{4}(\mathrm{g})\right.\)

In a heat engine, heat \(\left(q_{\mathrm{h}}\right)\) is absorbed by a working substance (such as water) at a high temperature \(\left(T_{\mathrm{h}}\right)\) Part of this heat is converted to work \((w),\) and the rest \(\left(q_{1}\right)\) is released to the surroundings at the lower temperature ( \(T_{1}\) ). The efficiency of a heat engine is the ratio \(w / q_{\mathrm{h}}\). The second law of thermodynamics establishes the following equation for the maximum efficiency of a heat engine, expressed on a percentage basis. $$\text { efficiency }=\frac{w}{q_{\mathrm{h}}} \times 100 \%=\frac{T_{\mathrm{h}}-T_{1}}{T_{\mathrm{h}}} \times 100 \%$$ In a particular electric power plant, the steam leaving a steam turbine is condensed to liquid water at \(41^{\circ} \mathrm{C}\left(T_{1}\right)\) and the water is returned to the boiler to be regenerated as steam. If the system operates at \(36 \%\) efficiency, (a) What is the minimum temperature of the steam \(\left[\mathrm{H}_{2} \mathrm{O}(\mathrm{g})\right]\) used in the plant? (b) Why is the actual steam temperature probably higher than that calculated in part (a)? (c) Assume that at \(T_{\mathrm{h}}\) the \(\mathrm{H}_{2} \mathrm{O}(\mathrm{g})\) is in equilibrium with \(\mathrm{H}_{2} \mathrm{O}(1) .\) Estimate the steam pressure at the temperature calculated in part (a). (d) Is it possible to devise a heat engine with greater than 100 percent efficiency? With 100 percent efficiency? Explain.

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