The orthorhombic cell looks like a box with 3 different edge lengths. Base-centering means there is an extra lattice point at two opposite faces, which I will call the “top” and “bottom.”

Since base-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 body-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 in the center of two opposite faces. There are “base-centered orthorhombic” crystals based on the Bravais lattice, which exist with multiple atoms that overall displays primitive orthorhombic symmetry.

The base-centered orthorhombic unit cell would belong to space group #65 or Cmmm, with Pearson symbol oC2. There is no prototype or Strukturbericht for base-centered orthorhombic, since it does not exist with real atoms.

**The base-centered orthorhombic unit cell can be imagined as a box with 3 different side lengths, with an atom on each corner and at the center of the top and bottom faces. Pure materials never take this crystal structure, and it exists only mathematically. Base-centered orthorhombic has 2 atoms per unit cell, lattice constants a, b, and c, all angles α=90º, Coordination Number CN=2, and Atomic Packing Factor **.

#### Outline

### Common Examples of Base-Centered Orthorhombic Materials

**None.**

However, there are still materials with a multi-atom basis that have a base-centered orthorhombic Bravais lattice, such as α-U, I_{2}, and CdPt_{3}.

### Base-Centered Orthorhombic Coordination Number

You can think of orthorhombic as a distortion of the simple cubic crystal. Base-centering adds an atom to the top and bottom faces (similar to face-centering, but face-centering adds an atom to every face). Since each face is a rectangle, rather than a square, there are 4 nearest neighbors in the base-centered orthorhombic unit cell.

### Base-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 body-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 the face diagonal length would be , and the lattice parameter lengths would need to fit the 2D distance formula .

If parameter c was *also* be close-packed, the result would be a different crystal structure.

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

### Base-Centered Orthorhombic Atomic Packing Factor

There is no simple answer for the base-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 another half atom at the top and bottom, so the total is two 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 base-centered orthorhombic crystal structure does NOT exist in real life, and only arises by mathematical definition. There are many crystals which have a base-centered orthorhombic Bravais lattice, but these crystals have a more complicated “basis” which leads to its characteristic asymmetrical lattice parameters.

### References and Further Reading

If you want to know more about the basics of crystallography, check out this article.

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.”

**Single-Element Crystal Structures and the 14 Bravais Lattices**

If you want to learn about specific crystal structures, here is a list of my articles about Bravais lattices and their 1-to-1 corresponding crystal structure for pure elements. Base-Centered Orthorhombic is one of these 14 Bravais lattices and also occurs as a crystal structure.

1. Simple Cubic

2. Face-Centered Cubic

2a. Diamond Cubic

3. Body-Centered Cubic

4. Simple Hexagonal

4a. Hexagonal Close-Packed

4b. Double Hexagonal Close-Packed (La-type)

5. Rhombohedral

5a. Rhombohedral Close-Packed (Sm-type)

6. Simple Tetragonal

7. Body-Centered Tetragonal

7a. Diamond Tetragonal (White Tin)

8. Simple Orthorhombic

9. Base-Centered Orthorhombic

10. Face-Centered Orthorhombic

11. Body-Centered Orthorhombic

12. Simple Monoclinic

13. Base-Centered Monoclinic

14. Triclinic

Other articles in my crystallography series include:

What are Crystals and Grains

Introduction to Bravais Lattices

What is the Difference Between “Crystal Structure” and “Bravais Lattice”

Atomic Packing Factor

How to Read Miller Indices

How to Read Hexagonal Miller-Bravais Indices

Close-Packed Crystals and Stacking Order

Interstitial Sites

Primitive Cells

How to Read Crystallography Notation