# Face-Centered Orthorhombic Unit Cell

The orthorhombic unit cell looks like a box with 3 different edge lengths. There is an atom shared among the 8 corners of this box, and “face-centering” means there are additional atoms centered on the faces of the box.

Since face-centered orthorhombic is one of the less-common crystal structures, I’m assuming someone searching for this is a somewhat advanced student in materials science, so I’ll give you the facts quickly and with little explanation. If you are new to materials science and don’t know what something means, you can check out my articles on the FCC, BCC, or HCP crystals, which explain terminology more slowly.

As far as I know, there are no real-world materials that exhibit a face-centered orthorhombic unit cell. If this structure were to exist, it would be a box with 3 different side lengths, with an atom on each corner and on each face. There are crystals based on the face-centered orthorhombic Bravais lattice, which exist with multiple atoms that overall displays the proper symmetry. If it were to exist, the face-centered orthorhombic unit cell would belong to space group #69 or Fmmm, with Pearson symbol oF4. There is no prototype or Strukturbericht for face-centered orthorhombic, since it does not exist with real atoms.

The face-centered orthorhombic unit cell can be imagined as a box with 3 different side lengths, with an atom on each corner and on each face. Pure materials never take this crystal structure, and it exists only mathematically. Face-centered orthorhombic has 4 atoms per unit cell, lattice constants a, b, and c, Coordination Number CN=4, and Atomic Packing Factor .

### Common Examples of Face-Centered Orthorhombic Materials

None.

However, there are still materials made of multiple kinds of atoms (or a multi-atom basis) that have a face-centered orthorhombic Bravais lattice, such as TlF, γPu, or αS.

### Face-Centered Orthorhombic Coordination Number

You can think of orthorhombic as a distortion of the cubic crystal. There are 3 faces with different shapes, so with an atom on the center of each face, the nearest atoms would be shared only along the face for 4-fold coordination.

Face-centered orthorhombic has 4 nearest neighbors, but remember there are no real materials that take this crystal structure.

### Face-Centered Orthorhombic Lattice Constants

The orthorhombic shape is like a cube, where all sides are at 90º to each other, but with edge lengths distorted so there are three different edge lengths. Thus, the face-centered orthorhombic crystal has 3 lattice parameters: a, b, and c, which have an angle of 90º to each other.

If we try to stay within the hard sphere model, we see that the close packed direction would be along one face diagonal. If the atoms touched in that direction, half of that face diagonal length would be ; however, it’s dubious to apply real-world constraints to a crystal that doesn’t exist in the real world.

By definition, body-centered orthorhombic has 3 lattice constants of different lengths: a, b, and c; each at 90º to each other.

If you wanted to describe the simple orthorhombic crystal with math, you would describe the cell with the primitive vectors:

### Face-Centered Orthorhombic Atomic Packing Factor

There is no simple answer for the body-centered orthorhombic APF, because the answer changes depending on the side lengths.

The volume of an orthorhombic unit cell is , obtained by multiplying the lattice parameters times each other.

There is 1 atom split between each of the 8 corners of the cell, and a half-atom on each of the 6 faces, so the total is four full atoms with a spherical radius of .

This allows us to write the theoretical APF in terms of the atomic radius and lattice constants:

### Final Thoughts

The face-centered orthorhombic crystal system does NOT exist in real life, and only arises by mathematical definition. There are several crystals which have a face-centered orthorhombic Bravais lattice, but these crystals have a more complicated “basis” which leads to its characteristic asymmetrical lattice parameters.

If you weren’t sure about the difference between crystal structure and Bravais lattice, check out this article.

I also mentioned atomic packing factor (APF) earlier in this article. This is an important concept in your introductory materials science class, so if you want a full explanation of APF, check out this page.

If you’re interested in advanced crystallography or crystallography databases, you may want to check out the AFLOW crystallographic library.

For a great reference for all crystal structures, check out “The AFLOW Library of Crystallographic Prototypes.”

The 14 Basic Crystal Structures

If you want to learn about specific crystal structures, here is a list of my articles about Bravais lattices and some related crystal structures for pure elements. Face-Centered Orthorhombic is one of these 14 Bravais lattices and also occurs as a crystal structure.

Other articles in my crystallography series include: