Interstitial Sites: Size, Types, Applications, And Calculations

An important concept in crystallography is the idea of “interstitial sites,” which may also be called interstitial voids. They allow interstitial defects to occur. These sites exist in the spaces between atoms, and you can actually calculate their size and position with simple geometry.

In this article, I’ll explain how to perform these calculations, as well as the real-world differences that interstitial sites can make.

What are Interstitial Sites?

Check out this article if you would like a basic introduction to crystallography, but the main fact you need to know is that crystals are any material made of atoms that repeat in a certain pattern.

If you have any pattern which doesn’t fill space completely (and we model atoms as spheres that can never fill space completely), you end up with gaps.

Interstitial sites are empty spaces in a crystal lattice. Depending on the number of atoms surrounding that empty space, the interstitial site can be designated as triangular (3), tetrahedral (4), octahedral (6), or cubic (8).

Each interstitial site is empty in a perfect crystal, but since these are the regions in the crystal with the most empty space, imperfect crystals have an occasional atom in these sites.

Why are Interstitial Defects Important?

When the interstitial site is not empty, it is considered an “interstitial defect.” Defects allow some of the most important material properties, such as ductility in metals. There are many kinds of crystal defects (besides interstitial defects) such as grain boundaries, vacancies, and dislocations.

Interstitial defects usually happen when a small atom fills the interstitial site of a larger atom’s crystal structure. Usually, this strains the crystal lattice and increases the strength of a metal. There are entire alloys based on this principle, called interstitial solid solution alloys.

The most famous example of an interstitial solid solution is when carbon rests in interstitial sites of iron–this is steel. If you know anything about metallurgy, you should know that steel is one of the most important materials in the world–mostly because of the way metallurgists can make its phases interact. The strongest phase of steel, martensite, exists because of carbon’s interaction with iron’s interstitial sites.

For now, I should explain more about how to perform calculations with interstitial sites. However, near the end of this article I will explain how martensite arises from the difference in interstitial size between FCC and BCC iron.

4 Types of Interstitial Sites

There are 4 standard types of interstitial sites, categorized by the number of surrounding atoms. 

  1. triangular
  2. tetrahedral
  3. octahedral
  4. cubic

These 4 types of interstitial sites can be derived using the simple hard sphere model.

However, atoms are not perfect spheres, so interstitial atoms can sometimes be in other configurations, especially with complex crystal structures that may involve atoms of multiple sizes or asymmetrical interstitial sites. 

A triangular interstitial site has 3 surrounding atoms. All 3 atoms, and the interstitial site, are in the same plane.

A tetrahedral interstitial site has 4 surrounding atoms. These 4 atoms take the shape of a tetrahedron (4 equally spaced corners).

One simple way to imagine a tetrahedron is to take a cube (8 corners) and choose any 4 corners that are the maximum distance from each other.

An octahedral interstitial site sits in the middle of 6 atoms. This “octahedral” shape looks as if you stuck 2 pyramids together at the base. The shape overall has 8 faces, which is where the “octahedral” name comes from.

A cubic interstitial site is in the center of 8 atoms, which form a cube. The site is in the same spot as the center atom in a body-centered cubic (BCC) crystal.

Although I’ve listed 4 types of interstitial sites, only tetrahedral and octahedral are important for most materials. That’s because different interstitial sites have a different size compared to the surrounding atoms.

If you know how to calculate the anion-cation radius rules, calculating the regular atom-interstitial atom radius rules is identical . . . except that interstitials don’t really affect the bonding of the primary atoms, because there are so few.

As you can see, triangular interstitial sites require extremely small atoms, and it’s not really useful for most metals. For reference, hydrogen’s atomic radius (0.53Å) is about ⅓ of iron’s atomic radius (1.56Å), so even hydrogen is too small for triangular interstitial sites in iron [1].

LIkewise, a cubic interstitial site can be almost as big as the regular atom. Any crystal which has cubic interstitial sites (such as the simple cubic, or alpha-Po structure) are rare because they “waste” a lot of space. 

Although cubic and triangular interstitial sites are too large and too small for most applications, tetrahedral and octahedral sites play an important role in materials science.

In the following sections, I’ll calculate the size, number, and positions of octahedral and tetrahedral sites for the common crystal structures: FCC, BCC, HCP, and SC.

Interstitial Sites in Face-Centered Cubic

The FCC crystal has 8 tetrahedral sites and 4 octahedral sites.

Let’s calculate the size of those interstitial sites (R), compared to the size of an atom (r). I’ll start with the FCC tetrahedral void.

Remember, an easy way to do geometry involving tetrahedrons is to imagine that they are a cube that is missing half of it’s corners, like this.

As you may know, the atom that sits in the center of a cube can touch the atoms at all 8 corners. That means that the corner-to-center distance, or ½ of the body diagonal will be the radius of the interstitial site + the radius of the atom.

To start, let’s use this “imaginary cube” geometry to determine the corner-to-center distance.

Let’s call the length of one cube edge L_{edge}. (If you’re following the pictures below, I labelled the corners with letters). What we’re looking for is the length of the body diagonal, L_{body} .

You can solve this directly with the 3D distance formula, or just use the pythagorean theorem in 2 steps:

First, let’s find the length of the face diagonal, L_{face} . We know that (L_{edge})^2 +  (L_{edge})^2 = (L_{face})^2 . Rearranging tells us that L_{face} = \sqrt{2} \cdot L_{edge}.

Now we can set up a 2nd pythagorean theorem, with (L_{edge})^2 + (L_{face})^2 = (L_{body})^2. Rearranging this gives us L_{body} = \sqrt{3} \cdot L_{edge}.

If we know the length of the body diagonal, then the distance from the corner to the center is half of that, or \frac{\sqrt{3}}{2} times the edge length.

Now we need to figure out the edge length, by putting our cube on top of the tetrahedral interstitial site.

In FCC, the tetrahedral edge length will be the distance between face-centered atoms. Since this is the close-packed direction, this distance is 2r. When translating from the tetrahedron to our imaginary cube, the tetrahedron edge length becomes the cubic face diagonal.

So, we know that L_{face} = 2r. Earlier, we proved that L_{face} = \sqrt{2} \cdot L_{edge}, so L_{edge} = \frac{2r}{\sqrt{2}}.

Plugging this back into the pythagorean theorem and we find that the (L_{body})^2= 4r^2 + 2r^2.

2(r+R) = \frac{\sqrt{6}}{2} \cdot r

and finally, the radius R of the interstitial atom compare to the regular atom is:

R = r(\frac{\sqrt{6}}{2}-1) \approx 0.2247r

Calculating the FCC octahedral interstitial sites is more straightforward than the tetrahedral sites. Whether we view the FCC cell from the top, front, or side, the 2D projection looks the same:

To calculate this interstitial size, we’ll first calculate the size of a circle within that 2D plane. Then, we’ll add the 3rd dimension. Let’s view the FCC cell from the top–this is the (002) plane if you understand Miller Indices.

We have 4 atoms that make a square, with some space in the center. The diagonal across this square is the same as the edge length of the FCC cell. If you remember, for FCC a = 2\sqrt{2}r. If you don’t remember, let’s prove this again.

Since this is the close-packed plane, each circle on the corner of our square must touch another circle. The edge length of our cube is therefore 2\sqrt2 r.

We know that the distance from one atom to the center is  r + R  , and we can use Pythagorean’s theorem to put that in terms of the cube edge.

2(r+R)=2 \cdot \sqrt{2}r

 2R=2 \cdot \sqrt{2}r-2r


This tells us the maximum radius of the interstitial size within that plane. However, we need to check the size in the 3rd dimension, height. If you look at the FCC crystal from the front or side views, you notice that the cross section looks exactly the same. Everything is symmetrical, and you find the same value for R in every dimension.

So,  R = (\sqrt2-1)r \approx 0.4142   just like we thought.

I make a point to emphasize this because the symmetry assumption is NOT true for BCC.

Total volume of interstitial sites in FCC crystals:

 V_{interstitials} = 8 \cdot \frac{4}{3} \cdot \pi \cdot (R_{tetrahedral})^3 + 4 \cdot  \frac{4}{3} \cdot \pi \cdot (R_{octahedral})^3

where  R_{tetrahedral} =  (\frac{\sqrt6}{2}-1)r

and  R_{octahedral} =  (\sqrt{2}-1)r

The volume of an FCC cell is:


Hence, the fraction occupied by interstitial sites is:


So an FCC crystal can fill about 7% of it’s volume with interstitial atoms! Of course, if an FCC crystal was really filled with so many interstitial atoms, the lattice parameter would definitely distort and it would change to a different crystal structure.

Interstitial Sites in BCC

The BCC crystal has 12 tetrahedral sites and 6 octahedral sites.

Let’s calculate the size of those interstitial sites, compared to the size of the atom, starting with the BCC tetrahedral void.

This calculation is similar to the FCC tetrahedral interstitial site, but slightly more complex because the tetrahedron is not completely symmetrical.

If you look at the tetrahedral site, 2 edges have a length equal to the BCC lattice parameter, and the other 4 edges have a length equal to half of the body diagonal.

These values are \frac{4r}{\sqrt3} and 2r. If you’d like a proof for that, you can check out the BCC section in my article about calculating the atomic packing factor.

Instead of transposing our tetrahedron on a cube, we’ll now put it on a rectangular prism.

The body diagonal of this prism, L_{body} , is still  r + R . And we can still use a series of Pythagorean theorems like we did for the FCC tetrahedral site, but this time I”ll make sure that  L_{face} is only made of the short edges, and  L_{edge} considers the long edge, as labelled in the diagram above. You can switch the values however you like, but that’s how I will label them in these diagrams.

You can also use the 3D distance formula, which says that the square of the body diagonal will be the sum of the squares of each edge length. It works out the same.

We need to put the imaginary rectangular prism back on the BCC cell, as you can see above, to understand the relationships between the tetrahedral edges and the atomic radii.

As you can see,  L_{face} = 2r , and  L_{edge} = \frac{4r}{\sqrt3} .

 (2r + 2R)^2 =  (\frac{4r}{\sqrt3})^2  + (\frac{2r}{\sqrt3})^2

 R =  r(\frac{\sqrt5}{\sqrt3}-1)

Calculating the BCC octahedral site sizes can be done similarly to FCC octahedral sites, but you have to be careful about the asymmetry.

If you look at the cell from the top view, you see a nice cube where the cube edges match the BCC edge lengths. However, if you look from the front or side view, the cube has face diagonals which match the BCC edge lengths.

We can still project things into 2D, but we need to assess the top and front/side views separately. Let’s start with the top view.

In this projection, you can see that the interstitial site falls in the center of a square, where each corner of the square has an atom. The edges of this square line up with the edges of the BCC cube, and you know that distance is  \frac{4}{\sqrt3}r .

(If you didn’t know that the BCC lattice parameter is  a=\frac{4}{\sqrt3}r , I once again recommend my article about calculating APF.)

The geometry using Pythagorean’s theorem should be familiar by now. The face diagonal is  2(r + R)  and so   (2(r+R))^2 = (\frac{4}{\sqrt3}r)^2 +(\frac{4}{\sqrt3}r )^2  .

and finally that simplifies to R = r(\frac{\sqrt8}{\sqrt3} - 1)

But remember, we’re not done. Now we need to check the interstitial position in the 3rd dimension. The top and bottom atoms of the octahedron are the center atom in the BCC cell. In other words, the height of the octahedron is exactly the distance as the BCC lattice parameter,  a=\frac{4}{\sqrt3}r .

As you can see, that height is 2(r+R) = \frac{4}{\sqrt3 r}

and rearranging for R gives R = (\frac{2}{\sqrt3} -1)r

We need to compare the maximum values that we calculated for R, and (\frac{2}{\sqrt3} -1)r is smaller than r(\frac{\sqrt8}{\sqrt3} - 1). This means that the interstitial site could be larger if the top and bottom of the octahedral were farther apart. 

The true maximum value for R is (\frac{2}{\sqrt3} -1)r \approx 0.1547r.

Total volume of interstitial sites in BCC crystals:

 V_{interstitials} = 12 \cdot \frac{4}{3} \cdot \pi \cdot (R_{tetrahedral})^3 + 6 \cdot \frac{4}{3} \cdot \pi \cdot (R_{octahedral})^3

where  R_{tetrahedral} =  (\frac{\sqrt5}{\sqrt3}-1)r

and  R_{octahedral} =  (\frac{2}{\sqrt3}-1)r

The volume of a BCC cell is:


Dividing by the volume of the unit cell will give us the maximum volume fraction of interstitial sites in BCC.


So BCC can have about 11% of its volume occupied by interstitial atoms. (Theoretically, not in reality).

Notice that this is greater than the total volume of FCC interstitial sites, which should make sense because FCC is atomically denser than BCC.

Interstitial Sites in HCP

The HCP unit cell has 12 tetrahedral sites and 6 octahedral sites, which is exactly 50% more than the FCC sites. This shouldn’t be a surprise, considering that both FCC and HCP are close-packed, and HCP is exactly 50% larger than FCC.

Calculating the tetrahedral and octahedral sites for HCP works out exactly like calculating them for FCC. Remember, the difference between FCC and HCP is stacking order, so all that’s changed is the position of the interstitial sites within the stack.

For the tetrahedral site, we once again visualize the tetrahedron within an imaginary cube.

As you can see, the face diagonals of this cube are the close-packed direction and are therefore equal to 2r. That means this tetrahedron is exactly the same as the tetrahedron in FCC, so if you follow that derivation you end up with

R = r(\frac{\sqrt6}{2}-1)

The HCP octahedral sites also have each edge length = 2r, which is identical to the FCC octahedral sites

The geometry is the same, but I’ll work it out again because I can’t use some of the cubic shortcuts we did when calculating the size of FCC interstitial sites.

Let’s start by looking at the square cross section. As we just discussed, each edge of this square has a length of 2r. The space within the plane is (2(r + R))^2 = (2r)^2 + (2r)^2, which means R = r(\sqrt2 - 1)

We then need to consider the 3rd axis, the “height” of the octahedron. If we view the octahedron from the side, so it looks like a diamond, we see that both body diagonals are 2(r+R).

This is obviously symmetric with the body diagonal when we looked through the other perspective, but let’s keep going. We see that (r+R)^2 + (r+R)^2 = (2r)^2, and eventually we can reduce the “height” of the octahedron to r+R = \sqrt2 r, and therefore R = r(\sqrt2 -1), in every perspective. 

Thus, R = r(\sqrt2 -1) is the true maximum radius for an octahedral interstitial in the HCP crystal.

Total volume of interstitial sites in HCP crystals:

 V_{interstitials} = 12 \cdot \frac{4}{3} \cdot \pi \cdot (R_{tetrahedral})^3 + 8 \cdot  \frac{4}{3} \cdot \pi \cdot (R_{octahedral})^3

where  R_{tetrahedral} =  (\frac{\sqrt6}{2}-1)r

and  R_{octahedral} =  (\sqrt{2}-1)r

The volume of an HCP cell is:

V_{HCP}=S_{base} \cdot H=6 \cdot \frac{1}{2}  \cdot a  \cdot \frac{a\sqrt3}{2} \cdot \frac{4\sqrt2}{\sqrt3} =  6 \cdot \frac{1}{2}  \cdot 2r  \cdot \frac{2r\sqrt3}{2}  \cdot \frac{4\sqrt2}{\sqrt3} = 24\sqrt2

Hence, the fraction occupied by interstitial sites is:


Interstitial sites occupy exactly the same volume (6.94%) for FCC and HCP unit cells. That makes perfect sense since both crystal structures are close-packed with an atomic packing factor (APF) of 74%.

Interstitial Sites in Simple Cubic

Simple cubic has one cubic interstitial site. As you can imagine, it’s right in the center of the atom.

As you can probably guess by now, we can calculate the size of this interstitial site by realizing that the body diagonal is twice the radius of the atom and the interstitial site.

By the 3D distance formula or a couple applications of Pythagorean’s theorem, you can see that the body diagonal is \sqrt3 times the edge length of the cube. In the simple cubic crystal structure, the edge length is 2r, so

2(r+R) = 2r\sqrt{3}

R = r(\sqrt{3}-1)

Total volume of interstitial sites in SC crystals:

 V_{interstitials} = \frac{4}{3} \cdot \pi \cdot (R_{cubic})^3

and  R_{cubic} =  (\sqrt{3}-1)r

The volume of an SC cell is:


Hence, the fraction occupied by interstitial sites is:


Interstitial Carbon in Steel

A lot of steel’s unique properties come from the fact that iron changes from BCC to FCC at high temperatures, and carbon has to move between those interstitial sites.

Carbon forms an interstitial solid solution when added to iron; the maximum concentration of carbon is about 2 wt%. The atomic radius of the carbon atom is much less than that for iron: 0.071 nm versus 0.124 nm [2]. In other words, the carbon atom is 57% as large as the iron atom.

From a simple APF calculation, you should know that BCC has a larger total volume of interstitial space than FCC. Earlier, we proved that directly.

However, FCC has the largest interstitial site. FCC’s largest interstitial site is octahedral, which is 41% of the atom size. BCC’s largest interstitial size is tetrahedral, which is 29% of the atom size. As you can see, it’s a lot easier to squeeze carbon into an interstitial site in FCC iron, compared to squeezing it in the smaller interstitial sites in BCC iron. This means that the solubility of carbon in iron is about 100 times higher for FCC than BCC!

As you heat up iron, it will change from BCC to FCC at 912ºC. Suddenly, the metal will be able to absorb a lot more carbon from the atmosphere.

When you cool down the iron, the atoms want to shift back to BCC, but now there’s too much carbon! If you cool it slowly, the carbon has time to get squeezed out and the iron can be BCC again. However, if you cool it quickly (quenching), then the carbon gets frozen in the interstitial sites and you end up with a distorted body-centered tetragonal structure.

I previously wrote an article about quenching (and tempering, a completely different process that is commonly confused with quenching), so be sure to check that out next!

Final Thoughts

Although introductory materials science classes might spend only one day explaining interstitial sites, the topic is important for understanding advanced metallurgy, especially about steel. With simple geometry, you can calculate the size of an interstitial site for different crystal structures.

Crystal StructureBCCFCCHCPSC
Octahedral Interstitial
Site Radius
0.155r 0.414r 0.414r
Tetrahedral Interstitial
Site Radius
0.291r 0.225r 0.225r
Cubic Interstitial
Site Radius
Fraction of a cell’s volume
occupied by interstitial sites

References and Further Reading

[1] CrystalMaker

[2] Callister W., Fundamentals of Materials Science and Engineering, John Wiley & Sons, Inc., 2001.

If you’re reading this article as an introductory student in materials science, welcome! I hope you can find many other useful articles on this website. You may be interested in a related article I’ve written about Atomic Packing Factor.

If you’re reading this article because you’re taking a class on structures, you may be interested in my other crystallography articles. Here is this list, in recommended reading order:

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
What are Point Groups
List of Point Groups
What are Space Groups
List of Space Groups
The 7 Crystal Systems

If you are interested in more details about any specific crystal structure, I have written individual articles about simple crystal structures which correspond to each of the 14 Bravais lattices:

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

Related Questions

What are self-interstitials?

Self-interstitials are when at atom fits into its own interstitial site. This will be more common with larger interstitial sites (such as simple cubic’s cubic interstitial site, or FCC’s octahedral interstitial site).

What is interstitial solid solution?

Alloys can be solid solutions, which means that one type of atom is dissolved in a metal. You probably think of dissolution in a liquid, like salt in water, but this process happens in solids as well. The 2 types of solid solution are “interstitial” and “substitutional.”

In a substitutional solid solution, the dissolved atom replaces the main atom in the crystal structure. In an interstitial solid solution, the dissolved atom sits in an interstitial site among the main atoms in the crystal structure.

If atoms are about the same size, they will tend to form a substitutional solid solution. If the impurity atom is much smaller than the host atom, it will form an interstitial solid solution.

What is interstitial diffusion?

Diffusion is when atoms move around by random vibration. For an atom to travel through a metal, it needs to move to an empty space. If the atom is the same size as most of the atoms, these empty spaces are vacancies. However, each interstitial site is also an empty space, as long as the atom can fit into it.

Interstitial diffusion is when a small atom–which can fit into the interstitial sites of another atom–is able to rapidly move through the crystal lattice of a larger atom. Interstitial diffusion is much faster than vacancy diffusion, because most materials have many more empty interstitial sites than vacancies. Small atoms such as hydrogen, carbon, nitrogen, and oxygen are most likely to experience interstitial diffusion in metals.

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