Callister Chapter 3: The Structure of Crystalline Solids

In the last chapter, we talked about the different types of atomic bonding. Here, we’ll go one step further and discuss how these atoms are arranged—that is, what types of crystal structures they can have. This Callister chapter puts emphasis on the most common metallic crystal structures (FCC, BCC, and HCP), but I will try to give a broader overview of all Bravais lattices followed by a review of X-ray diffraction and Bragg’s law.

Bravais lattices and symmetry

A Bravais lattice is as an infinite set of discrete points with an arrangement and orientation that appears exactly the same from whichever of the points the array is viewed. In other words, it is an array of points with translational symmetry. The basis is the actual atoms that are positioned on these lattice points. Thus, a crystal = lattice + basis. Crystals are built out of unit cells, which are the smallest repeating units that show the full symmetry of the crystal.

Symmetries can be described using space groups, which are the lattice’s translational symmetry plus other symmetry elements which are called point groups. This can be summarized by the graphic below:

There are seven crystal systems, each with their own symmetries. We can begin with the cubic system, which has four 3-fold axes and three 4-fold axes. By stretching or compressing the cubic system along one body diagonal, we obtain the trigonal system. Since we lose all the previous symmetries except along the axis we deformed, the trigonal system has only one 3-fold axis. Similarly, by stretching or compressing the cubic system along one axis, we arrive at the tetragonal crystal system, which has one 4-fold axis (along the axis we stretched/compressed). By deforming this system along a second axis, we get an orthorhombic crystal system. This will have three 2-fold axes perpendicular to each of the faces. Next, if we shear one face with respect to the opposite face, we will have a monoclinic system. The monoclinic system will have one 2-fold symmetry, since there is only one face around which you can do a 2-fold rotation. Lastly, by shearing a second face relative to the opposite face, we get a triclinic system, which unsurprisingly has no symmetries. These crystal systems and their parameters are summarized in the table below: