Calculation of Ionic Radii

Calculation of Ionic Radii

If we know the edge length of a unit cell of an ionic compound and the position of the ions in the cell, we can calculate ionic radii for the ions in the compound if we make assumptions about individual ionic shapes and contacts.

Example

Calculation of Ionic Radii

The edge length of the unit cell of LiCl (NaCl-like structure, FCC) is 0.514 nm or 5.14 Å. Assuming that the lithium ion is small enough so that the chloride ions are in contact, as in the figure below, calculate the ionic radius for the chloride ion.

Three images are shown. The first image shows a cube with black dots at each corner and a red dot in the center. This cube is stacked with seven others that are not colored to form a larger cube. The second image is composed of eight spheres that are grouped together to form a cube with one much larger sphere in the center. The name under this image reads “Body-centered simple cubic structure.” The third image shows seven horizontal layers of alternating purple and green spheres that are slightly offset with one another and form a large cube.

Ionic compounds with anions that are much larger than cations, such as NaCl, usually form an FCC structure. They can be described by FCC unit cells with cations in the octahedral holes.

Note: The length unit angstrom, Å, is often used to represent atomic-scale dimensions and is equivalent to 10−10 m.

Solution

On the face of a LiCl unit cell, chloride ions contact each other across the diagonal of the face:

Three images are shown. The first shows a cube of alternating green and purple spheres. A smaller cube within that cube is outlined and a larger version of it appears next. This figure is a grey cube that appears to be made up of spheres. There are small spaces between each sphere. There is a right triangle outlined in this cube and a larger version of it appears next. This right triangle has two sides labeled “a,” and the hypotenuse, which spans two half-circles and one full one is labeled, “r, 2 r, and r.”

Drawing a right triangle on the face of the unit cell, we see that the length of the diagonal is equal to four chloride radii (one radius from each corner chloride and one diameter—which equals two radii—from the chloride ion in the center of the face), so d = 4r. From the Pythagorean theorem, we have:

\({a}^{2}+{a}^{2}={d}^{2}\)

which yields:

\({\left(0.514\phantom{\rule{0.2em}{0ex}}\text{nm}\right)}^{2}+{\left(0.514\phantom{\rule{0.2em}{0ex}}\text{nm}\right)}^{2}={\left(4r\right)}^{2}=16{r}^{2}\)

Solving this gives:

\(r=\phantom{\rule{0.2em}{0ex}}\sqrt{\cfrac{{\left(0.514\phantom{\rule{0.2em}{0ex}}\text{nm}\right)}^{2}+{\left(0.514\phantom{\rule{0.2em}{0ex}}\text{nm}\right)}^{2}}{16}}\phantom{\rule{0.2em}{0ex}}=\text{0.182 nm}\phantom{\rule{0.2em}{0ex}}\left(\text{1.82 Å}\right)\phantom{\rule{0.2em}{0ex}}{\text{for a Cl}}^{\text{−}}\phantom{\rule{0.2em}{0ex}}\text{radius}.\)

It is important to realize that values for ionic radii calculated from the edge lengths of unit cells depend on numerous assumptions, such as a perfect spherical shape for ions, which are approximations at best. Hence, such calculated values are themselves approximate and comparisons cannot be pushed too far. Nevertheless, this method has proved useful for calculating ionic radii from experimental measurements such as X-ray crystallographic determinations.

This lesson is part of:

Liquids and Solids

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