12.1 Crystal Lattices and Unit Cells
 Page ID
 43268
The Unit Cell
There are 7 types of unit cells (figure 12.1.a), defined by edge lengths (a,b,c) and angles \(\large\alpha\), \(\large\beta\), and \(\large\gamma\). In this class we will only focus on the cubic unit cell, and there are three types of cubic cells that you need to be familiar with, and these are represented in figure 12.1.b.
 \(\large\alpha\) = angle in the x,y plane
 \(\large\beta\) = angle in the y,z plane
 \(\large\gamma\) = angle in the x,y plane
Figure\(\PageIndex{1}\): The 7 types of unit cells. In this class we will only look at cubic systems, and will identify 3 types of cubic unit cells (figure. 12.b)
Cubic Unit Cell
The cubic unit cell is the smallest repeating unit when all angles are 90^{o}C and all lengths are equal (figure 12.1.b). As such, each axis is defined by a Cartesian coordinate. Each cubic cell has 8 atoms in each corner of the cube, and that atom is shared with 8 neighboring cells. In the Body Centered Cubic Cell (BCC) there is an additional atom in the center of the cube, and in the face centered cubic cell, an atom is shared between two unit cells along the face. Please watch the YouTube video as this can help a lot.
Figure\(\PageIndex{2}\): Three type of cubic unit cells, each is described in detail below.
Video\(\PageIndex{1}\): "Lattice Structure Part 1", created by Mark McClure, narrated by Sally Vallabha of UNPembroke, https://youtu.be/Rmi1c7zr6Q
Simple (Primative) Cubic Unit Cell
Figure\(\PageIndex{3}\): Unit cell for primitive cubic cell and stacking diagram for Simple Cubic Stacking which this results in.
 1 particle per unit cell
 coordination number = 6
 52% of space occupied by particles
 Simple Cubic Stacking
 along Cartesian coordinates
 very inefficient and rarely seen in nature
Body centered cubic unit cell
Figure\(\PageIndex{4}\): Unit cell for body centered cubic cell and stacking hexagonal close packed structure it results in. This has a repeating alignment of ABABABAB where every other layer lines up.
 2 particles per unit cell
 coordination number = 8
 68% of space occupied by particles
 Hexagonal Close Packing (HCP)
 second layer sits in grove of first with third in grove of second and in line with first (ABA structure)
 Common with metals, including all alkali, Cr, V, Ba and Fe
Face Centered Cubic
Figure\(\PageIndex{5}\): Unit Cell for face centered unit cell, and diagram of Cubic Close Packed structure that it results in. Note each row has neighbors shifted from the Cartesian coordinate of their plan, and as you move up the lattice there is an ABCABCABC stacking , where every third layer is aligns. This is the form oranges would stack in a grocery store.
 4 particles per unit cell
 coordination number = 12
 74% of space occupied by particles
 Cubic Closest Packing Structure
 explained in video 12.1.a at 5' 26".
 along Cartesian coordinates
 very inefficient and rarely seen in nature
Determining Atomic Radii from Density, Molar Mass and Crystal Structure
The strategy is to use the following to calculate the volume of the unit cell, and then the length of each side. Once this is done, you can use the packing and the geometry of the structure to calculate the radii. The information you need are:
 density
 Molar Mass
 Avogadro's number
 number atoms per unit cell
 pythagorean theorm
So these all have a similar strategy
 Calculate Volume of Unit Cell (number of atoms in unit cell depends on type of cell)
 Calculate length of the sides of the unit cell (same for all)
 Use packing to figure radii (different for each type)
A. Simple Cubic Cell
Exercise \(\PageIndex{1}\)
A. Given the density of Polonium = 9.32g/ml, calculate radii of a Polonium atom if it forms a Simple Cubic Cell.
Problem: Polonium is the only element that is simple cubic (has 1 atom/unit cell). Note the length of unit cell is 2 radii, and thus if we can calculate the length of the unit cell, we can calculate the radius. When we say there is one atom per unit cell, we are not saying the volume of the atom is the volume of the unit cell. It is 52% the volume (see above).
Video\(\PageIndex{2}\): Solution to the radii of Po from its density.
 Answer:

1. Find the volume of the unit cell
\[\frac{1 atom Po}{unit cell}(\frac{1mol Po}{6.02x10^{23}atoms})(\frac{208.9gPo}{mol})(\frac{1ml}{9.32g})=3.72x10^{23}\frac{ml}{unit\: cell} \nonumber\]
2. Find the length of the unit cell
\[l=\sqrt[3]V]=\sqrt[3]{3.72x10^{23}cm^{3}}=3.34x10^{8}cm=334pm \nonumber\]
3. Find radii
Since each side is 2r, r is 1/2 half the length, or 167pm

.
B. Body Centered Cubic
Exercise \(\PageIndex{2}\)
Problem: Molybdenum forms body centered cubic cells, if the density of Mo is 10.28 g/ml, what would its radius be?.
This is the toughest, as the diagonal through the cell from vertices X to Y with length "c" equals 4 radii. It makes a right triangle with side a and b, the diagonal of a face, we note that a^{2}+a^{2}=b^{2} and a^{2}+b^{2}=c^{2}
 Answer:

1. Find Volume of unit cell:
\[\frac{2 atom Mo}{unit cell}(\frac{1mol Mo}{6.02x10^{23}atoms})(\frac{95.95g\: Mo}{mol})(\frac{1ml\: Mo}{10.26g})=3.11x10^{23}\frac{ml}{unit\: cell}\]
2. Find length of unit cell
\[[a=\sqrt[3]V]=\sqrt[3]{3.11x10^{23}cm^{3}}=3.15x10^{8}cm=314pm\]
3. Find radii
a. Find diagonal of face "b"
\[b=\sqrt[2]{2a^{2}}=\sqrt[2]{2(314)^{2}}=444pm\]b. Find diagonal through cube "c"
\[c=\sqrt[2]{a^{2}+b^{2}}=\sqrt[2]{314^{2}+444^{2}}=544pm\]c. "c" = 4r, so r=136pm
C. Face Centered Cubic
Exercise \(\PageIndex{3}\)
Problem: Calcium forms a face centered cubic cell with a density of 1.54 g/ml, what would its radius be?
 Answer:

1. Find Volume of unit cell:
\[\frac{4 atom Ca}{unit cell}(\frac{1mol CA}{6.02x10^{23}atoms})(\frac{40.08g\: Ca}{mol})(\frac{1ml\: Mo}{1.54g})=1.73x10^{22}\frac{ml}{unit\: cell}\]
2. Find length of unit cell
\[a=\sqrt[3]V]=\sqrt[3]{1.72x10^{22}cm^{3}}=5.57x10^{8}cm=557pm\]
3. Find radii
a. Find diagonal of face "c"
\[c=\sqrt[2]{2a^{2}}=\sqrt[2]{2(557)^{2}}=787pm\]b. since the diagonal of the surface is 4r, r=197pm
Crystal Defects
Defects in a crystal can give it unique properties. Defects occur when another entity becomes part of the crystal, and there are many types of defects, two that are worth noting are substitutional and interstitial.
Substitutional Defects
These occur when a different substance substitutes for one of the components of the crystal. For example Ruby is Al_{2}O_{3} with a few Cr^{+3} replacing Al^{+3} ions .
Figure \(\PageIndex{6}\): Substitutional defect
Interstitial Defects
These occur when a substance which is not part of the crystal fits into the interstitial regions, and does not displace a component of the crystal. Carbide steel is a form of interstitial defect where carbon enters the holes of the iron structure, and this affects its properties like hardness and ductility.
Figure \(\PageIndex{7}\): Example of an interstitial defect,

Contributors
 Bob Belford
 some images from anonymous
 some images from anonymous were modified
 some images from Chris P Schaller