H*(g) + CI(g) + e- T+106 -349 TH*(g) + Cl,(g) + e- H'(g) + CI-(g) solv +1312 H'(g) + CH(aq). H(g) + Cl,(g) +218 son G°(H+) |글(g) + 글디,(g) H'(aq) + C(aq) H4,G°(H",aq) +A,G°(Cl-,aq}} Figure 3D.3 A thermodynamic cycle for discussion of the Gibbs energies of hydration and formation of chloride ions in aqueous solution. The changes in Gibbs energies around the cycle sum to zero because G is a state function. Gibbs ene rgy, G

Chemistry
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ISBN:9781305957404
Author:Steven S. Zumdahl, Susan A. Zumdahl, Donald J. DeCoste
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Chapter1: Chemical Foundations
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Problem 1RQ: Define and explain the differences between the following terms. a. law and theory b. theory and...
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Construct a cycle similar to that in Fig. 3D.3 to analyse the reaction 1/2 H2(g) + 1/2 I2(s) → H+(aq) + I(aq) and use it to find the value of the standard Gibbs energy of formation of I(aq). You should refer to the tables in the Resource section for relevant values of the Gibbs energies of formation. As in the text, the standard Gibbs energy for the process H(g) → H+(g) + e(g) should be approximated by the ionization energy, and that for I(g) + e(g) → I(g) by the electron affinity. The standard Gibbs energy of solvation of H+ can be taken as −1090 kJ mol−1 and of I as −247 kJ mol−1.

H*(g) + CI(g) + e-
T+106
-349
TH*(g) + Cl,(g) + e-
H'(g) + CI-(g)
solv
+1312
H'(g) + CH(aq).
H(g) + Cl,(g)
+218
son G°(H+)
|글(g) + 글디,(g)
H'(aq) + C(aq)
H4,G°(H",aq) +A,G°(Cl-,aq}}
Figure 3D.3 A thermodynamic cycle for discussion of the Gibbs
energies of hydration and formation of chloride ions in aqueous
solution. The changes in Gibbs energies around the cycle sum to
zero because G is a state function.
Gibbs ene rgy, G
Transcribed Image Text:H*(g) + CI(g) + e- T+106 -349 TH*(g) + Cl,(g) + e- H'(g) + CI-(g) solv +1312 H'(g) + CH(aq). H(g) + Cl,(g) +218 son G°(H+) |글(g) + 글디,(g) H'(aq) + C(aq) H4,G°(H",aq) +A,G°(Cl-,aq}} Figure 3D.3 A thermodynamic cycle for discussion of the Gibbs energies of hydration and formation of chloride ions in aqueous solution. The changes in Gibbs energies around the cycle sum to zero because G is a state function. Gibbs ene rgy, G
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