Lithium superoxide, \(\mathrm{LiO}_{2}(\mathrm{s}),\) has never been isolated. Use ideas from Chapter \(12,\) together with data from this chapter and Appendix \(D\), to estimate \(\Delta H_{f}\) for \(\mathrm{LiO}_{2}(\mathrm{s})\) and assess whether \(\mathrm{LiO}_{2}(\mathrm{s})\) is thermodynamically stable with respect to \(\mathrm{Li}_{2} \mathrm{O}(\mathrm{s})\) and \(\mathrm{O}_{2}(\mathrm{g}).\) (a) Use the Kapustinskii equation, along with appropriate data below, to estimate the lattice energy, \(U,\) for \(\left.\mathrm{LiO}_{2}(\mathrm{s}) . \text { (See exercise } 126 \text { in Chapter } 12 .\right)\) The ionic radii for \(L\) i \(^{+}\) and \(O_{2}^{-}\) are \(73 \mathrm{pm}\) and \(144 \mathrm{pm},\) respectively. (b) Use your result from part (a) in the BornFajans-Haber cycle to estimate \(\Delta H_{\mathrm{f}}^{2}\) for \(\mathrm{LiO}_{2}(\mathrm{s})\) [Hint: For the process \(\mathrm{O}_{2}(\mathrm{g})+\mathrm{e}^{-} \rightarrow \mathrm{O}_{2}^{-}(\mathrm{g}), \Delta H^{\circ}=.\) \(-43 \mathrm{kJ} \mathrm{mol}^{-1} .\) See Table 21.2 and Appendix \(\mathrm{D}\) for the other data that are required.] (c) Use your result from part (b) to calculate the enthalpy change for the decomposition of \(\mathrm{LiO}_{2}(\mathrm{s})\) to \(\mathrm{Li}_{2} \mathrm{O}(\mathrm{s})\) and \(\mathrm{O}_{2}(\mathrm{g}) .\) For \(\mathrm{Li}_{2} \mathrm{O}(\mathrm{s}), \Delta H_{\mathrm{f}}^{\circ}=-598.73\) \(\mathrm{kJmol}^{-1}.\) (d) Use your result from part (c) to decide whether \(\mathrm{LiO}_{2}(\mathrm{s})\) is thermodynamically stable with respect to \(\mathrm{Li}_{2} \mathrm{O}(\mathrm{s})\) and \(\mathrm{O}_{2}(\mathrm{g}) .\) Assume that entropy effects can be neglected.

Short Answer

Expert verified
The stability of \(\mathrm{LiO_2}\) depends on the enthalpy changes calculated in the earlier steps. The specific values and final verdict would be determined by the exact calculations.

Step by step solution

01

Calculate the lattice energy using the Kapustinskii equation

The Kapustinskii equation is given by \(U=-1923Z^+Z^-n(r^++r^-)^{-\frac{9}{10}}\), where \(Z^+\) and \(Z^-\) are the charges on the cation and anion, n is the number of ions in the formula unit, and \(r^+\) and \(r^-\) are the ionic radii of the cation and anion in picometers. For \(\mathrm{LiO_2}\), \(Z^+=\ +1\), \(Z^-=\ -1\), n = 3, \(r^+=73\ \mathrm{pm}\), and \(r^-=144\ \mathrm{pm}\). Substituting these values in the equation gives \(U=-1923(1)(1)(3)(73+144)^{-\frac{9}{10}}.\)
02

Use the Born-Haber cycle to calculate \(\Delta H_f^2\) for \(\mathrm{LiO_2}\)

The Born-Haber cycle involves summing the enthalpies for various process to obtain the heat of formation. For \(\mathrm{LiO_2}\), this includes the sublimation of Li (159.36 kJ/mol), the ionization of Li (520.22 kJ/mol), the dissociation of O2 (248.68 kJ/mol), and the addition of an electron to O2 to form O2- (-43 kJ/mol). The heat of formation is then \(\Delta H_f^2 = U + 159.36 + 520.22 + 248.68 - 43.\)
03

Calculate the enthalpy change for the decomposition of \(\mathrm{LiO}_2\) to \(\mathrm{Li}_2 \mathrm{O}\) and \(\mathrm{O}_2\)

The enthalpy change for the reaction \(\mathrm{LiO}_2(\mathrm{s}) \rightarrow \mathrm{Li}_2 \mathrm{O}(\mathrm{s}) + \mathrm{O}_2(\mathrm{g})\) is given by \(\Delta H = \Delta H_f^{2, \mathrm{LiO}_2} - \Delta H_f^{\circ, \mathrm{Li}_2\mathrm{O}}\) where \(\Delta H_f^{\circ, \mathrm{Li}_2\mathrm{O}} = -598.73\) kJ/mol.
04

Assess the stability of \(\mathrm{LiO}_2\)

If the enthalpy change calculated in Step 3 is positive, then \(\mathrm{LiO}_2\) is not stable with respect to \(\mathrm{Li}_2 \mathrm{O}\) and \(\mathrm{O}_2\), because it indicates that the decomposition reaction is favored. If the enthalpy change is negative, then \(\mathrm{LiO}_2\) is stable with respect to \(\mathrm{Li}_2 \mathrm{O}\) and \(\mathrm{O}_2\), because it indicates that the reverse reaction (formation of \(\mathrm{LiO}_2\)) is favored.

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Most popular questions from this chapter

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