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23 Nov 2019
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1.Energetics of diatomic systems II.
An approximate expression for the potential energy of twoions as a function of their separation is
PE
= âke2r+br9 (1)The first term is the usual Coulomb interaction,while the second term is introduced to account for
the repulsive effect of the two ions at smalldistances.
(a) Find b as a function of the equilibriumspacing ro. (b) Calculate the potentialenergy of KCl at its equilibrium spacing (ro =0.279 nm)
2.Energetics of diatomic systems III. An expression forthe potential energy of two neutral atoms as a function of their separation
r is given by the Morse potential,PE
= Poh1 â eâa(râro)i2 (2)(a)
Show that ro is the atomic spacing and Po the dissociation energy.(b) Calculate the forceconstant for small oscillations about r=ro. 3.Crystal lattice energy. Consider a one-dimensionalchain of alternating positive and negativeions. Show that the potential energy associatedwith one of the ions and its interactions with the
rest of this hypothetical crystal is
U
(r) = âkee2r(4)where the Madelung constant is
=2 ln 2 and r is the interionic spacing.
x.Hmt face="LMRoman10-Italic" size="3">
1.Energetics of diatomic systems II.
An approximate expression for the potential energy of twoions as a function of their separation is
PE
= âke2r+br9 (1)The first term is the usual Coulomb interaction,while the second term is introduced to account for
the repulsive effect of the two ions at smalldistances.
(a) Find b as a function of the equilibriumspacing ro. (b) Calculate the potentialenergy of KCl at its equilibrium spacing (ro =0.279 nm)
2.Energetics of diatomic systems III. An expression forthe potential energy of two neutral atoms
2.Energetics of diatomic systems III. An expression forthe potential energy of two neutral atoms
as a function of their separation
r is given by the Morse potential,PE
= Poh1 â eâa(râro)i2 (2)(a)
Show that ro is the atomic spacing and Po the dissociation energy.(b) Calculate the forceconstant for small oscillations about r=ro.
3.Crystal lattice energy. Consider a one-dimensionalchain of alternating positive and negative
=2 ln 2 and r is the interionic spacing.
ions. Show that the potential energy associatedwith one of the ions and its interactions with the
rest of this hypothetical crystal is
U
(r) = âkee2r(4)where the Madelung constant is
=2 ln 2 and r is the interionic spacing.