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Have you ever wondered why common salt is NaCl rather than NaCl_2 or NaCl_3? Here's your chance to investigate this mystery!
In case you haven't seen a Born-Haber cycle before, one is illustrated below for LiF:
[http://en.wikipedia.org/wiki/File:BornHaberLiF.PNG]
Using the data below, construct a Born-Haber cycle for NaCl and NaCl_2 . Calculate the lattice enthalpy for NaCl, and the enthalpy of formation of NaCl_2
\Delta H_f(NaCl) = -411 kJ mol^{-1}
\Delta H_{latt}(NaCl_2) =-3360 kJ mol^{-1}
IE_1(Na) = +496 kJ mol^{-1}
IE_2(Na) = +4563 kJ mol^{-1}
EA_1(Cl) = -349 kJ mol^{-1}
\Delta H_{sub}(Na_{(s)}) = +108 kJ mol^{-1}
\Delta H_{at}(\frac{1}{2}Cl_{2\ (g)}) = +121 kJ mol^{-1}
From looking at the signs and relative magnitudes of the two calculated enthalpies of formation, can you explain why NaCl_2 is not formed?
What are the major contributing factors in the mathematical expression for the enthalpies of formation which makes the formation of NaCl_2 so unfavourable? What does this tell you about the likely formation of NaCl_n, where n > 2 ?
As you may have guessed by now, the contsruction of Born-Haber cycles are quite laborious, and also rely solely upon experimentally determined enthalpy values. In many cases these enthalpy values may not be present, and so a reasonable prediction of a lattice enthalpy can be calculated by the Born-Lande expression (which is shown below). This equation assumes that ions are hard spheres held
together solely by electrostatic attractions.
E = -\frac{N_AMz^+z^-e^2}{4\pi \epsilon_0r_0}(1-\frac{1}{n})
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