CHM1 12 Bond Energies Collection

From UCDavis chemwiki

The heat changes which accompany a chemical reaction are caused largely by changes in the electronic energy of the molecules. If we restrict our attention to gases, and hence to fairly simple molecules, we can go quite a long way toward predicting whether a reaction will be exothermic by considering the bonds which are broken and made in the course of the reaction. In order to do this we must first become familiar with the idea of a bond enthalpy.

In other sections we point out that when a chemical bond forms, negative charges move closer to positive charges than before, and so there is a lowering of the energy of the molecule relative to the atoms from which it was made. This means that energy is required to break a molecule into its constituent atoms. The bond enthalpy D_X–Y of a diatomic molecule X—Y is the enthalpy change for the (usually hypothetical) process:

`XY(g) -> X(g) + Y(g)`

`DeltaH°(298 K) = D_(x-y)`      (1)

We have already used the term bond energy to describe this quantity, though strictly speaking the bond energy is a measure of `DeltaU` rather than `DeltaH`. As we have already seen, `DeltaU` and `DeltaH` are nearly equal, and so either term may be used.

As an example, let us consider the bond enthalpy for carbon monoxide. It is possible to establish the thermochemical equation

`CO(g) -> C(g) + O(g)`

`DeltaH°(298 K) = 1073 kJ mol^(-1)`       (2)

`D_(CequivO) = 1073 kJ mol^(-1)`

even though the process to which Eq. (2) corresponds is hypothetical: Neither carbon nor oxygen exists as a monatomic gas at 298 K. For triatomic and polyatomic molecules, the bond enthalpy is usually defined as a mean. In the case of water, for instance, we have

`H_2O(g) -> 2H(g) + O(g)`

`DeltaH°(298 K) = 927.2 kJ mol^(-1)`

Since it requires 927.2 kJ to break open two O—H bonds, we take half this value as the mean bond enthalpy and write

`D_(O-H) = 463.6 kJ mol^(-1)`

In methanol, `CH_3 OH`,however, a value of `427 kJ mol^(-1)` for the `O-H` bond enthalpy fits the experimental data better. In other words the strength of the `O-H` varies somewhat from compound to compound. Because of this fact, we must expect to obtain only approximate results, accurate only to about `+- 50 kJ mol^(-1)`, from the use of bond enthalpies.

It should be noted that this process can only be utilized when all species are in the gas phase.

Bond enthalpies for both single and multiple bonds are given in Table 1.

TABLE 1 Average Bond Energies in `kJ"/"mol^(-1)`.

As an example of how a table of bond enthalpies can he used to predict the `DeltaH` value for a reaction, let us take the simple case

`H_2(g) + F_2(g) -> 2HF(g)`      298 K, 1 atm      (3)

We can regard this reaction as occurring in two stages (Fig. 1). In the first stage all the reactant molecules are broken up into atoms:

`H_2(g) + F_2(g) -> 2H(g) + F(g)`      298 K, 1 atm      (3a)

For this stage

`DeltaH_I = H_(H-H) + D_(F-F)`

since 1 mol `H_2` and 1 mol `F_2` have been dissociated.

Figure 5 Bond-breaking-bond-making diagram for the reaction H₂+ F₂ + 2HF. When H₂ reacts with F₂, a strong H—H bond and a weak F—F bond are broken, while two extra-strong H—F bonds are made. The reaction is exothermic since more energy is released by the formation of the H—F bonds than is required to break the H—H and H—F bonds.

In the second stage the H and F atoms are reconstituted to form HF molecules: `2H(g) + 2F(g) -> 2HF(g)`      298 K, 1 atm (3b)

For which

`DeltaH_(II) = – 2D_(H-F)`

where a negative sign is necessary since this stage corresponds to the reverse of dissociation.

Since Eq. (3) corresponds to the sum of Eqs. (3a) and (3b), Hess' law allows us to add `DeltaH` values:

`DeltaH_"reaction"^° = DeltaH_I + DeltaH_II`

`= D_(H-H) + D_(F-F) – 2D_(H-F)`

`= (436 + 159 – 2 × 566) kJ mol^(-1)`

`= –539 kJ mol^(-1)`

We can work this same trick of subdividing a reaction into a bond-breaking stage followed by a bond-making stage for the general case of any gaseous reaction. In the first stage all the bonds joining the atoms in the reactant molecules are broken and a set of gaseous atoms results. For this stage

`DeltaH_I = sum_("bonds broken") D`

The enthalpy change is the sum of the bond enthalpies for all bonds broken. In the second stage these gaseous atoms are reconstituted into the product molecules. For this second stage therefore

`DeltaH_(II) = -sum_("bonds formed") D`

where the negative sign is necessary because the reverse of bond breaking is occurring in this stage. The total enthalpy change for the reaction at standard pressure is thus

`DeltaH° = DeltaH_I + DeltaH_(II)`

or

`DeltaH° = sum "D (bond broken)" – sum "D (bond formed)"`      (4)

The use of this equation is illustrated in the next example.

EXAMPLE 10 Using Table 1 calculate the value of `DeltaH°(298 K)` for the reaction

`CH_4(g) + 2O_2(g) -> CO_2(g) + 2H_2O(g)`

Solution (try this one on your own, here is a sketch to help you get started):

`= -814kJmol^(-1)`

The experimental value for this enthalpy change can be calculated from standard enthalpies of formation. It is `–802.4 kJ mol^(-1)`. The discrepancy is due to the unavoidable use of mean bond enthalpies in the calculation. 

Subpages (1): Example 10