In the ionic model, the bonding
is described as the electrostatic interaction between charged spheres, whose
sizes are given by the ionic radius.
In determining an ionic radius, it is
necessary to split up the internuclear separation into a contribution from the anion and
a contribution from the cation. This is most often done by assuming
the value of the radius of one ion, and then calculating the radii
of other ions from this basis. This standard ion is generally the oxide
ion, as it occurs in combination with many other elements.
Also, it is a relatively unpolarizable ion,
and so its size changes little with changing counterion.
The use of ionic radii to predict aspects of crystal
structure like lattice parameters, the lengths of the
axes of the unit cells, is often useful, but only when the values of the ionic
radii are taken form the same source, i.e. they use the same reference ion and
so have the correct relative sizes.
It should also be noted that the ionic radius
of a given ion changes with coordination number: As the coordination number
increases, the ions must get further away from the central ion in order to
accommodate more of them, and hence the interionic separation increases, and
the short ranged repulsion decreases, and the electron cloud on the central ion
can expand, and hence the central ion increases in size.
Hence, ionic radius increases with
coordination number.
The sizes of the ions can be used to predict
the structure that will be adopted when they are combined. In a cubic close
packed array of anions, for example, the octahedral and tetrahedral holes have
different sizes, and so cation might be expected to occupy the holes which are
just big enough to hold them. This is examined in terms of the radius
ratio.
The Radius Ratio
The radius ratio of a given pair of ions is
defined at the ionic radius of the smaller ion divided by the ionic radius of
the larger ion, ie. ρ = rs/rl.
Often the smaller ion is the cation (as the
reduced repulsion brought about by the missing electron tends to contract the
electron cloud), and the larger ion is the anion (as the extra repulsion from
the negative charge tends to make the ion expand).
Consider a simple cubic arrangement of
anions, with a cation in the center of the cubic cell (as in CsCl, which is
(8,8)-coordinate). As the cation decreases in size, it will reach a point when
the anions begin to touch, which unfavourable electrostatically, due to the
repulsion between like-charged species. At this point, the structure changes so
the anions are again separated by oppositely charged cations, an arrangement
which is electrostatically favourable, and the (6,6)-coordinate NaCl structure
is adopted. as this trend is continued, there will be a switch to the
(4,4)-coordinate ZnS structure. Similar arguments hold for structures of stoichiometry AB2,
and others.
Therefore, as the radius ratio decreases,
there is a trend towards structures of lower coordination numbers. The Radius
ratio rules are the prediction of structure adopted by a given set of
ions based on the radius ration of those ions.
The radius ratio rules are not universally
successful. As the degree of covalency in the bonding increases, the deviation
from the ionic model increases and the less reliable the choice of structure
based on the radius ratio becomes. The rules are least reliable for simple
compounds like alkali metal halides and alkaline earth metal oxides, and are
most reliable for complex fluorides and the salt of oxoanions:
in general, as the degree of ionicity increases, so does the accuracy of the
rules.
Although radius is a useful concept of determining coordination number and in understanding the structure of ionic compounds yet there are a few limitations to this rule.
(i) Each ion is considered as a hard sphere for determining the optimum arrangement of ions in the crystal lattice. This is far form reality and serious errors can be made if anions get polarized and the bonding the intermediate (partially covalent) in character.
(ii) Some compounds may crystallize in more than one modification with different coordination numbers. In such case, anion-anion repulsions and hence intern clear distance would be different.
(iii) Effective radius of a cation is greatly influenced by the anions with the consequence that the radius ratio changes. For example, AgF and NaF crystallize out in NaCI type of structure with coordination No. 6 and if we assume that the size of F- remains constant than Ag+ is bigger than Na+. On the other hand, for a given size for a chloride ion in AgCI and NaCI, the sizes of cations are reversed, that is, Na+ is bigger than Ag+. It is also true for their bromides. This is understandable because Ag+ is softer than N+ and introduces relatively more covalent character with Polarizable anions like CI- and Br-