EXAMPLE 15-10 Using Hf^0 Values: Hess’s Law
Use the following information to determine Hf^0 for PbO(s, yellow).
PbO(s, yellow)CO(g)88nPb(s)CO 2 (g) H^0 rxn65.69 kJ
H^0 ffor CO 2 (g)393.5 kJ/mol and H^0 ffor CO(g)110.5 kJ/mol
Plan
We again use Hess’s Law in the form H^0 rxnnHf products^0 nH^0 f reactants. The stan-
dard state of lead is Pb(s), so H^0 f Pb(s)0 kJ/mol. Now we are given H^0 rxnand the Hf^0
values for all substances exceptPbO(s, yellow). We can solve for this unknown.
Solution
We list the known H^0 fvalues:
PbO(s, yellow) CO(g) Pb(s) CO 2 (g),
H^0 f, kJ/mol: H^0 f PbO 2 (s, yellow) 110.5 0 393.5
Hrxn^0 nH^0 f products nH^0 f reactants
Hrxn^0 H^0 f Pb(s)H^0 fCO 2 (g)[H^0 f PbO(s, yellow)H^0 f CO(g)]
65.69 0 (393.5) [H^0 f PbO(s, yellow)(110.5)]
Rearranging to solve for H^0 f PbO(s, yellow), we have
Hf PbO(s, yellow)^0 65.69393.5110.5217.3 kJ/mol of PbO
You should now work Exercise 42.
For all practical purposes, the bond
energy is the same as bond enthalpy.
Tabulated values of average bond
energies are actually average bond
enthalpies. We use the term “bond
energy” rather than “bond enthalpy”
because it is common practice to
do so.
15-9 Bond Energies 609
BOND ENERGIES
Chemical reactions involve the breaking and making of chemical bonds. Energy is always
required to break a chemical bond. Often this energy is supplied in the form of heat.
The bond energy (B.E.)is the amount of energy necessary to break one moleof
bonds in a gaseous covalent substance to form products in the gaseous state at
constant temperature and pressure.
The greater the bond energy, the more stable (stronger) the bond is, and the harder it is
to break. Thus bond energy is a measure of bond strengths.
15-9
We will consult Appendix K, only after
working the problem, to check the
answer.
Problem-Solving Tip:Remember the Values of Hf^0 for Elements
In Example 15-10, we were not given the value of Hf^0 for Pb(s). We should know
without reference to tables that H^0 ffor an elementin its most stable form is exactly 0
kJ/mol. But the element mustbe in its most stable form. Thus, Hf^0 for O 2 (g) is zero,
because ordinary oxygen is gaseous and diatomic. We would notassume that Hf^0 would
be zero for oxygen atoms, O(g), or for ozone, O 3 (g). Similarly, Hf^0 is zero for Cl 2 (g)
and for Br 2 (), but not for Br 2 (g). Recall that bromine is one of the few elements that is
liquid at room temperature and 1 atm pressure.