Born Haber Energy Cycle
There is no denying the fact that an
electron can be transferred from one neutral (uncharged) atom to another. When
this happens, the atom from which the electron is transferred becomes a
positive ion or cation and the atom to which the electron is transferred
becomes a negative ion or anion. The transfer of an electron to or from an atom
involves energy. The energy required to remove one electron from an atom is
characteristic of the atom and is its ionization energy. The energy released
when an electron is acquired by an atom is its electron affinity. The electron
transfer can take place with a release of energy only when the electron
affinity of the receiving species is greater than the ionization energy of the
donating species, which is rarely the case, or, most often, when the resulting
ions associate themselves into a new configuration of lower energy. Most
electron transfer reactions occur when the ions once formed associate
themselves into structured lattices called ionic crystals.
Energy Considerations in Ionic
Structures
Ions with the same type of charge repel each
other, but ions of opposite charge attract each other. The simplest possible
ionic structure which might be stable is the gas-phase ion pair, which consists
of one cation and one anion held together by electrostatic attraction. It is
relatively simple to calculate how much energy would be gained by this
association using the Coulomb law of electrostatic attraction. The energy of
the attraction is given by
E = (2.31 x 10-16 J-pm) Z+Z-/d
where Z is the charge on the cation and anion
and d is the distance between the ions, in pm. The energy of the two
associated ions will be less than the energy of the two isolated ions by this
amount if the ions are of opposite charge. For sodium ion the ionic radius is
97 pm and for chloride ion it is 181 pm so the distance of separation of the
centers of the two ions is 278 pm. The energy for one ion pair, multiplied by
the Avogadro number NA, gives the molar energy of [Na+Cl-](g)
relative to the molar energy of the isolated ions as:
E = -8.31 x 10-19 J/molecule x
6.022...x 1023 molecules/mole
This is -500 kJ/mole, so the standard molar
enthalpy of formation of the ion pair estimated using the Coulomb law is -123
kJ/mole (-500 kJ/mole + 377 kJ/mole). Even for a single sodium ion and chloride
ion in the gas phase, it is the lower energy available through association of
ions of opposite charge that drives the formation of ionic compounds.
The ionic radii used in the calculation above
were the radii of sodium and chloride ions found in ionic crystals. They are,
however, very similar to the radii of these ions under other conditions. The
actual distance between the ions in Na+Cl-(g) has been
measured and found to be 236.1 pm.
Association of ions of opposite charge is not
normally into ion pairs. It is far more common to find ions in the form of the
solid ionic crystals, which are large ordered three-dimensional arrays of ions.
The diagram below is the Born-Haber cycle for
the formation of an ionic compound from the reaction of an alkali metal (Li,
Na, K, Rb, Cs) with a gaseous halogen (F2, Cl2). The
Born-Haber thermochemical cycle is named after the two German physical
chemists, Max Born and Fritz Haber, who first used it in 1919.
The enthalpy change in the formation of an
ionic lattice from the gaseous isolated sodium and chloride ions is -788
kJ/mole. That enthalpy change, which corresponds to the reaction Na+(g)
+ Cl-(g)
NaCl(s), is called the lattice energy of the ionic crystal. Although the
lattice energy is not directly measurable, there are various ways to estimate
it from theoretical considerations and some experimental values. For all known
ionic crystals, the lattice energy has a large negative value. It is ultimately
the lattice energy of an ionic crystal which is responsible for the formation
and stability of ionic crystal structures.
In view of the above, for real energy calculation, setting up intermediaries are important where the energy trend are considered according to energy scales.
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