Private: Chapter Nine
Strengths of Ionic and Covalent Bonds (9.4)
By the end of this section, you will be able to:
- Describe the energetics of covalent and ionic bond formation and breakage
- Use the Born-Haber cycle to compute lattice energies for ionic compounds
- Use average covalent bond energies to estimate enthalpies of reaction
A bond’s strength describes how strongly each atom is joined to another atom, and therefore how much energy is required to break the bond between the two atoms.
It is essential to remember that energy must be added to break chemical bonds (an endothermic process), whereas forming chemical bonds releases energy (an exothermic process). In the case of H2, the covalent bond is very strong; a large amount of energy, 436 kJ, must be added to break the bonds in one mole of hydrogen molecules and cause the atoms to separate:
H2(g) ⟶ 2H(g) bond energy = 436 kJ
Conversely, the same amount of energy is released when one mole of H2 molecules forms from two moles of H atoms:
2H(g) ⟶ H2(g) bond energy = −436 kJ
Bond Strength: Covalent Bonds
Stable molecules exist because covalent bonds hold the atoms together. We measure the strength of a covalent bond by the energy required to break it, that is, the energy necessary to separate the bonded atoms. Separating any pair of bonded atoms requires energy (see Figure 4.4). The stronger a bond, the greater the energy required to break it.
The energy required to break a specific covalent bond in one mole of gaseous molecules is called the bond energy or the bond dissociation energy. The bond energy for a diatomic molecule, DX–Y, is defined as the standard enthalpy change for the endothermic reaction:
XY(g) ⟶ X(g) + Y(g) DX−Y = ΔH°
For example, the bond energy of the pure covalent H–H bond, DH–H, is 436 kJ per mole of H–H bonds broken:
H2(g) ⟶ 2H(g) DH−H = ΔH° = 436 kJ
Molecules with three or more atoms have two or more bonds. The sum of all bond energies in such a molecule is equal to the standard enthalpy change for the endothermic reaction that breaks all the bonds in the molecule. For example, the sum of the four C–H bond energies in CH4, 1660 kJ, is equal to the standard enthalpy change of the reaction:
The average C–H bond energy, DC–H, is 1660/4 = 415 kJ/mol because there are four moles of C–H bonds broken per mole of the reaction. Although the four C–H bonds are equivalent in the original molecule, they do not each require the same energy to break; once the first bond is broken (which requires 439 kJ/mol), the remaining bonds are easier to break. The 415 kJ/mol value is the average, not the exact value required to break any one bond.
The strength of a bond between two atoms increases as the number of electron pairs in the bond increases. Generally, as the bond strength increases, the bond length decreases. Thus, we find that triple bonds are stronger and shorter than double bonds between the same two atoms; likewise, double bonds are stronger and shorter than single bonds between the same two atoms. Average bond energies for some common bonds appear in Table9.3, and a comparison of bond lengths and bond strengths for some common bonds appears in Table 9.4. When one atom bonds to various atoms in a group, the bond strength typically decreases as we move down the group. For example, C–F is 439 kJ/mol, C–Cl is 330 kJ/mol, and C–Br is 275 kJ/mol.
|
Bond |
Bond Energy |
|
Bond |
Bond Energy |
|
Bond |
Bond Energy |
|---|---|---|---|---|---|---|---|
|
H–H |
436 |
|
C–S |
260 |
|
F–Cl |
255 |
|
H–C |
415 |
C–Cl |
330 |
F–Br |
235 |
||
|
H–N |
390 |
C–Br |
275 |
Si–Si |
230 |
||
|
H–O |
464 |
C–I |
240 |
Si–P |
215 |
||
|
H–F |
569 |
N–N |
160 |
Si–S |
225 |
||
|
H–Si |
395 |
N = N |
418 |
Si–Cl |
359 |
||
|
H–P |
320 |
N ≡ N |
946 |
Si–Br |
290 |
||
|
H–S |
340 |
N–O |
200 |
Si–I |
215 |
||
|
H–Cl |
432 |
N–F |
270 |
P–P |
215 |
||
|
H–Br |
370 |
N–P |
210 |
P–S |
230 |
||
|
H–I |
295 |
N–Cl |
200 |
P–Cl |
330 |
||
|
C–C |
345 |
N–Br |
245 |
P–Br |
270 |
||
|
C = C |
611 |
O–O |
140 |
P–I |
215 |
||
|
C ≡ C |
837 |
O = O |
498 |
S–S |
215 |
||
|
C–N |
290 |
O–F |
160 |
S–Cl |
250 |
||
|
C = N |
615 |
O–Si |
370 |
S–Br |
215 |
||
|
C ≡ N |
891 |
O–P |
350 |
Cl–Cl |
243 |
||
|
C–O |
350 |
O–Cl |
205 |
Cl–Br |
220 |
||
|
C = O |
741 |
O–I |
200 |
Cl–I |
210 |
||
|
C ≡ O |
1080 |
F–F |
160 |
Br–Br |
190 |
||
|
C–F |
439 |
|
F–Si |
540 |
|
Br–I |
180 |
|
C–Si |
360 |
F–P |
489 |
I–I |
150 |
||
|
C–P |
265 |
F–S |
285 |
|
|
|
Bond |
Bond Length (Å) |
Bond Energy (kJ/mol) |
|---|---|---|
|
C–C |
1.54 |
345 |
|
C = C |
1.34 |
611 |
|
C ≡ C |
1.20 |
837 |
|
C–N |
1.43 |
290 |
|
C = N |
1.38 |
615 |
|
C ≡ N |
1.16 |
891 |
|
C–O |
1.43 |
350 |
|
C = O |
1.23 |
741 |
|
C ≡ O |
1.13 |
1080 |
Table 9.4
The bond energy is the difference between the energy minimum (which occurs at the bond distance) and the energy of the two separated atoms. This is the quantity of energy released when the bond is formed. Conversely, the same amount of energy is required to break the bond. For the H2 molecule shown in Figure 5.2, at the bond distance of 74
pm the system is 7.24 × 10−19 J lower in energy than the two separated hydrogen atoms. This may seem like a small number. However, as we will learn in more detail later, bond energies are often discussed on a per-mole basis. For example, it requires 7.24 × 10−19 J to break one H–H bond, but it takes 4.36 × 105 J to break 1 mole of H–H bonds. A comparison of some bond lengths and energies is shown in Figure 5.2 and Table 9.3. We can find many of these bonds in a variety of molecules, and this table provides average values. For example, breaking the first C–H bond in CH4 requires 439.3 kJ/mol, while breaking the first C–H bond in H–CH2C6H5 (a common paint thinner) requires 375.5 kJ/mol.
As seen in Table 9.3 and Table 9.4, an average carbon-carbon single bond is 347 kJ/mol, while in a carbon-carbon double bond, the π bond increases the bond strength by 267 kJ/mol. Adding an additional π bond causes a further increase of 225 kJ/mol. We can see a similar pattern when we compare other σ and π bonds. Thus, each individual π bond is generally weaker than a corresponding σ bond between the same two atoms. In a σ bond, there is a greater degree of orbital overlap than in a π bond.
We can use bond energies to calculate approximate enthalpy changes for reactions where enthalpies of formation are not available. Calculations of this type will also tell us whether a reaction is exothermic or endothermic. An exothermic reaction (ΔH negative, heat produced) results when the bonds in the products are stronger than the bonds in the reactants. An endothermic reaction (ΔH positive, heat absorbed) results when the bonds in the products are weaker than those in the reactants.
The enthalpy change, ΔH, for a chemical reaction is approximately equal to the sum of the energy required to break all bonds in the reactants (energy “in”, positive sign) plus the energy released when all bonds are formed in the products (energy “out,” negative sign). This can be expressed mathematically in the following way:
ΔH = ƩD bonds broken − ƩD bonds formed
In this expression, the symbol Ʃ means “the sum of” and D represents the bond energy in kilojoules per mole, which is always a positive number. The bond energy is obtained from a table (like Table 9.4) and will depend on whether the particular bond is a single, double, or triple bond. Thus, in calculating enthalpies in this manner, it is important that we consider the bonding in all reactants and products. Because D values are typically averages for one type of bond in many different molecules, this calculation provides a rough estimate, not an exact value, for the enthalpy of reaction.
Consider the following reaction:
H2(g) + Cl2(g) ⟶ 2HCl(g)
or
H–H(g) + Cl–Cl(g) ⟶ 2H–Cl(g)
To form two moles of HCl, one mole of H–H bonds and one mole of Cl–Cl bonds must be broken. The energy required to break these bonds is the sum of the bond energy of the H–H bond (436 kJ/mol) and the Cl–Cl bond (243 kJ/mol). During the reaction, two moles of H–Cl bonds are formed (bond energy = 432 kJ/mol), releasing 2 × 432 kJ; or 864 kJ. Because the bonds in the products are stronger than those in the reactants, the reaction releases more energy than it consumes:
[latex]$\Delta H=\Sigma \mathrm{D}_{\text {bonds broken }}-\Sigma \mathrm{D}_{\text {bonds formed }}$[/latex]
[latex]$\begin{aligned} \Delta H &=\left[\mathrm{D}_{\mathrm{H}-\mathrm{H}}+\mathrm{D}_{\mathrm{Cl}-\mathrm{Cl}}\right]-2 \mathrm{D}_{\mathrm{H}-\mathrm{Cl}} \\ &=[436+243]-2(432)=-185 \mathrm{kJ} \end{aligned}$[/latex]
This excess energy is released as heat, so the reaction is exothermic. Appendix G gives a value for the standard molar enthalpy of formation of HCl(g), ΔH°f , of –92.307 kJ/mol. Twice that value is –184.6 kJ, which agrees well with the answer obtained earlier for the formation of two moles of HCl.
EXAMPLE 9.16
Using Bond Energies to Calculate Approximate Enthalpy Changes
Methanol, CH3OH, may be an excellent alternative fuel. The high-temperature reaction of steam and carbon produces a mixture of the gases carbon monoxide, CO, and hydrogen, H2, from which methanol can be produced. Using the bond energies in Table 9.4, calculate the approximate enthalpy change, ΔH, for the reaction here:
CO(g) + 2H2(g) ⟶ CH3OH(g)
Solution
First, we need to write the Lewis structures of the reactants and the products:
From this, we see that ΔH for this reaction involves the energy required to break a C–O triple bond and two H–H single bonds, as well as the energy produced by the formation of three C–H single bonds, a C–O single bond, and an O–H single bond. We can express this as follows:
[latex]$\Delta H=\Sigma D_{\text {bonds broken }}-\Sigma D_{\text {bonds formed }}$ $\Delta H=\left[D_{C \equiv 0}+2\left(D_{H-H}\right)\right]-\left[3\left(D_{C-H}\right)+D_{C-O}+D_{O-H}\right]$[/latex]
Using the bond energy values in Table 9.4, we obtain:
[latex]$\begin{aligned} \Delta H &=[1080+2(436)]-[3(415)+350+464] \\ &=-107 \mathrm{kJ} \end{aligned}$[/latex]
We can compare this value to the value calculated based on Δ𝐻∘f
data from Appendix G:
\begin{aligned} \Delta H &=\left[\Delta H_{\mathrm{f}}^{\circ} \mathrm{CH}_{3} \mathrm{OH}(g)\right]-\left[\Delta H_{\mathrm{f}}^{\circ} \mathrm{CO}(g)+2 \times \Delta H_{\mathrm{f}}^{\circ} \mathrm{H}_{2}\right] \\ &=[-201.0]-[-110.52+2 \times 0] \\ &=-90.5 \mathrm{kJ} \end{aligned}
Note that there is a fairly significant gap between the values calculated using the two different methods. This occurs because D values are the average of different bond strengths; therefore, they often give only rough agreement with other data.
Check Your Learning
Ethyl alcohol, CH3CH2OH, was one of the first organic chemicals deliberately synthesized by humans. It has many uses in industry, and it is the alcohol contained in alcoholic beverages. It can be obtained by the fermentation of sugar or synthesized by the hydration of ethylene in the following reaction:
Using the bond energies in Table 9.4, calculate an approximate enthalpy change, ΔH, for this reaction.
ANSWER:
–35 kJ
Ionic Bond Strength and Lattice Energy
An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid MX, the lattice energy is the enthalpy change of the process:
MX(s) ⟶ Mn+(g) + Xn−(g) ΔHlattice
Note that we are using the convention where the ionic solid is separated into ions, so our lattice energies will be endothermic (positive values). Some texts use the equivalent but opposite convention, defining lattice energy as the energy released when separate ions combine to form a lattice and giving negative (exothermic) values. Thus, if you are looking up lattice energies in another reference, be certain to check which definition is being used. In both cases, a larger magnitude for lattice energy indicates a more stable ionic compound. For sodium chloride, ΔHlattice = 769 kJ. Thus, it requires 769 kJ to separate one mole of solid NaCl into gaseous Na+ and Cl– ions. When one mole each of gaseous Na+ and Cl– ions form solid NaCl, 769 kJ of heat is released.
The lattice energy ΔHlattice of an ionic crystal can be expressed by the following equation (derived from Coulomb’s law, governing the forces between electric charges):
[latex]\Delta H_{\mathrm{lattice}}=\frac{\mathrm{C}\left(\mathrm{Z}^{+}\right)\left(\mathrm{Z}^{-}\right)}{\mathrm{R}_{0}}[/latex]
in which C is a constant that depends on the type of crystal structure; Z+ and Z– are the charges on the ions; and Ro is the interionic distance (the sum of the radii of the positive and negative ions). Thus, the lattice energy of an ionic crystal increases rapidly as the charges of the ions increase and the sizes of the ions decrease. When all other parameters are kept constant, doubling the charge of both the cation and anion quadruples the lattice energy. For example, the lattice energy of LiF (Z+ and Z– = 1) is 1023 kJ/mol, whereas that of MgO (Z+ and Z– = 2) is 3900 kJ/ mol (Ro is nearly the same—about 200 pm for both compounds).
Different interatomic distances produce different lattice energies. For example, we can compare the lattice energy of MgF2 (2957 kJ/mol) to that of MgI2 (2327 kJ/mol) to observe the effect on lattice energy of the smaller ionic size of F– as compared to I–.
EXAMPLE 9.17
Lattice Energy ComparisonsThe precious gem ruby is aluminum oxide, Al2O3, containing traces of Cr3+. The compound Al2Se3 is used in the fabrication of some semiconductor devices. Which has the larger lattice energy, Al2O3 or Al2Se3?
SolutionIn these two ionic compounds, the charges Z+ and Z– are the same, so the difference in lattice energy will depend upon Ro. The O2– ion is smaller than the Se2– ion. Thus, Al2O3 would have a shorter interionic distance than Al2Se3, and Al2O3 would have the larger lattice energy.
Check Your LearningZinc oxide, ZnO, is a very effective sunscreen. How would the lattice energy of ZnO compare to that of NaCl?
ANSWER:
ZnO would have the larger lattice energy because the Z values of both the cation and the anion in ZnO are greater, and the interionic distance of ZnO is smaller than that of NaCl.
The Born-Haber Cycle
It is not possible to measure lattice energies directly. However, the lattice energy can be calculated using the equation given in the previous section or by using a thermochemical cycle. The Born-Haber cycle is an application of Hess’s law that breaks down the formation of an ionic solid into a series of individual steps:
- ΔH°f , the standard enthalpy of formation of the compound
- IE, the ionization energy of the metal
- EA, the electron affinity of the nonmetal
- ΔH°s , the enthalpy of sublimation of the metal
- D, the bond dissociation energy of the nonmetal
- ΔHlattice, the lattice energy of the compound
Figure 9.25 diagrams the Born-Haber cycle for the formation of solid cesium fluoride.
We begin with the elements in their most common states, Cs(s) and F2(g). The ΔH°s represents the conversion of solid cesium into a gas, and then the ionization energy converts the gaseous cesium atoms into cations. In the next step, we account for the energy required to break the F–F bond to produce fluorine atoms. Converting one mole of fluorine atoms into fluoride ions is an exothermic process, so this step gives off energy (the electron affinity) and is shown as decreasing along the y-axis. We now have one mole of Cs cations and one mole of F anions. These ions combine to produce solid cesium fluoride. The enthalpy change in this step is the negative of the lattice energy, so it is also an exothermic quantity. The total energy involved in this conversion is equal to the experimentally determined enthalpy of formation, ΔH°f , of the compound from its elements. In this case, the overall change is exothermic.
Hess’s law can also be used to show the relationship between the enthalpies of the individual steps and the enthalpy of formation. Table 9.5 shows this for cesium fluoride, CsF.
|
Enthalpy of sublimation of Cs(s) |
Cs(s) ⟶ Cs(g) |
ΔH = ΔH°s = 76.5kJ/mol |
|---|---|---|
|
One-half of the bond energy of F2 |
[latex]\frac{1}{2}[/latex] F (g) ⟶ F(g) |
ΔH = 1 D = 79.4kJ/mol 2 |
|
Ionization energy of Cs(g) |
Cs(g) ⟶ Cs+(g) + e− |
ΔH = IE = 375.7kJ/mol |
|
Negative of the electron affinity of F |
F(g) + e− ⟶ F−(g) |
ΔH = −EA = −328.2kJ/mol |
|
Negative of the lattice energy of CsF(s) |
Cs+(g) + F−(g) ⟶ CsF(s) |
ΔH = −ΔHlattice = ? |
|
Enthalpy of formation of CsF(s), add steps 1–5 |
ΔH = ΔH°f = ΔH°s + [latex]\frac{1}{2}[/latex]D + IE + (−EA) + (-ΔHlattice) Cs(s) + [latex]\frac{1}{2}[/latex]F2(g) ⟶ CsF(s)2 |
|
|
|
ΔH = −553.5kJ/mol |
|
|
|
|
Thus, the lattice energy can be calculated from other values. For cesium fluoride, using this data, the lattice energy is:
ΔHlattice = (553.5 + 76.5 + 79.4 + 375.7 + 328.2) kJ/mol = 1413.3 kJ/mol
The Born-Haber cycle may also be used to calculate any one of the other quantities in the equation for lattice energy, provided that the remainder is known. For example, if the relevant enthalpy of sublimation ΔH°s , ionization energy (IE), bond dissociation enthalpy (D), lattice energy ΔHlattice, and standard enthalpy of formation ΔH°fare known, the Born-Haber cycle can be used to determine the electron affinity of an atom.
Lattice energies calculated for ionic compounds are typically much higher than bond dissociation energies measured for covalent bonds. Whereas lattice energies typically fall in the range of 600–4000 kJ/mol (some even higher), covalent bond dissociation energies are typically between 150–400 kJ/mol for single bonds. Keep in mind, however, that these are not directly comparable values. For ionic compounds, lattice energies are associated with many interactions, as cations and anions pack together in an extended lattice. For covalent bonds, the bond dissociation energy is associated with the interaction of just two atoms.
Footnotes
- 4 This question is taken from the Chemistry Advanced Placement Examination and is used with the permission of the Educational Testing Service.