Lattice
Energy & Ionic Bonds:
Problem
6.58: Order the following compounds according to their expected
lattice energies: LiCl, KCl, KBr, MgCl2.
The
potential energy between two ions is given (here as a proportion) roughly
by
If
the signs on the charges are oppositive, we have a negative energy corresponding
to attraction. If the charges have the same sign, we
have a positive energy of repulsion. In a crystal lattice
containing ions, all these attractions and repulsions add up to the lattice
energy. For a given crystal structure these can be determined
by the above formula with an inclusion of what is called a Madelung
constant. We won't discuss that but do tell you that it is
a straightforward, albeit complicated and tedious, calculation!
The
two effects we look at are the charge sizes and the ionic radii.
The closer two ions are, the stronger the attraction and repulsion.
The larger the charges, the larger the interaction. Using those trends
as "barometers" for the size of the energies, we can easily order the above
species as
Problem
6.59: Order the following compounds according to their expected
lattice energies: AlBr3,
MgBr2, LiBr, CaO.
We
follow the same rules here as in the previous problem. Also, note
that, with aluminum bromide, we have four ions interacting, three with
magnesium bromide, and just two with the other two substances. However,
with CaO both ions of charges of magnitude 2. Putting those ideas
together gives us, then,
Be
sure to study this one carefully until you completely understand it!
Problem
6.61: Cesium has the smallest ionization energy of all elements
(376 kJ/mol) and chlorine has the most negative electron affinity (-349
kJ/mol). Will a cesium atom donate an electonn to a chlorine atom
to form isolated Cs+
and Cl-
ions?
To
understand this, let us add the energies to get the total energy.
The
total energy is positive and, hence, the process is not favored!
Problem
6.63: Look up the lattice energies in Table 6.3 and calculate
the energy change (in kJ/mol)
for
the formation of the following substances from their elements:
First,
we present the table:
Now,
we are ready to do the calculations. Note that the "reactions" sum
in the same way as do the energies. This is an important point to
note in that we shall be doing many things like this in many different
chapters! These are done without diagrams; you may wish to draw your
own as a valuable exercise if you are uncomfortable visualizing things
with just numbers.
(a) |
LiF (The sublimation
energy for Li is +159.4 kJ/mol, the Ei
for Li is 520 kJ/mol, the Eea
for F is -328 kJ/mol, and the bond dissociation energy of F2
is +158 kJ/mol.) |
(b) |
CaF2
(The sublimation energy for Ca is +178.2 kJ/mol, Ea1
= +589.8 kJ/mol, and Ea2
= +1145 kJ/mol.) |
Here we do things
in much the same way EXCEPT that we have two ionization energies for the
calcium. Otherwise, things are pretty much straightforward and easy
to pHollow. Also, I am trying a different format for this sort of
thing, so bear with me...
Problem
6.65: Calculate a lattice energy for CaH2
(in kJ/mol) using the following information.
Property
|
Value (kJ/mol)
|
Eea
for H
|
-72.8
|
Ei1for
Ca
|
+589.8
|
Ei2for
Ca
|
+1145
|
Heat of sublimation for Ca
|
+178.2
|
Bond dissociation energy for H2
|
+435.9
|
Net energy change for the formation of CaH2
from its elements
|
-186.2
|
Here goes another
rather involved calculation. However, it involves nothing more difficult
than addition and subtraction with one multiplication to give you some
practice... . Below, we let "U" denote the lattice energy; note that
this is reported as a positive number (whereas the formation of a lattice
is actually negative); hence, the handling of the minus sign on "U."
The lattice energy is released when the lattice is formed. As a positive
number, that means it is the energy needed to break up the lattice!
Why do things dissolve?
Is it maybe because of the relative sizes of the solvation and lattice
energies?
Problem
6.66: Calculate the overall energy change (in kJ/mol) for
the formation of CsF from its elements using the following data:
Property
|
Value (kJ/mol)
|
Eea
for F
|
-328
|
Ei1for
Cs
|
+375.7
|
Ei2for
Cs
|
+2422
|
Heat of sublimation for Cs
|
+76.1
|
Bond dissociation energy for F2
|
+158
|
Lattice energy for CsF
|
+740
|
From the number,
you can tell that this is one Devil of a problem. Note that this
is interesting in the context of its companion, which follows...
Problem
6.67: The estimated lattice energy for CsF2
is +2347 kJ/mol. Use the data given in Problem 6.66 to calculate
an overall energy change (in kJ/mol) for the formation of CsF2
from its elements. Does the overall reaction absorb energy or release
it? In light of your answers to Problem 6.66, which compound is more
likely to form in the reaction of cesium with fluorine, CsF or CsF2?
The
lattice energy for this molecule is large. But is it large enough
for the molecule to form? We now work out the steps and discuss our
conclusions.
For
this reaction, we see that the overall energy is positive. For the
reaction in Problem 6.66, the number was rather large and negative.
Thus, formation of CsF is very much favored over the formation of CsF2.
Congratulations! You have just solved what amounts to a good theoretical
problem.
Problem
6.71: Use the data and the result in Problem 6.63a to draw
a Born-Haber cycle for the formation of LiF from its elements.
Usually,
I do all the problems myself and eschew use of the instructor manual.
In this case, however, I feel it wise to spare you my horrid art work (there
are examples of that elsewhere if you really want to see it). This
is the answer as printed in the instructor's manual.
The
diagram makes the following few points clear:
-
Vaporization
of the lithium, splitting of the fluorine molecule, and stripping of an
electron from the lithium atom all require that we provide
energy to the system. You might call this part of the total energy
our "expenses."
-
The
electron affinity and the lattice energy are given off by the system.
You might call this part of the total energy our "dividends."
-
The
net result is a stable compound in crystalline form. For this, the
total energy is negative. However, we receive this energy (we are,
after all, the surroundings!). Thus, from our viewpoint, the net
result for the formation of a stable compound is, for us,
profits!
Several
of these points will be made more apparent in chapter 8. For now,
we just look at how the flow of energy into and out of a system pretty
much defines the system in terms of stability. To emphasize this
point, you should probably draw diagrams for problems 6.66 and 6.67.