Protein crystallography lies directly at the
interface between molecular biology, chemistry, and physics. It
is currently responsible for the majority of 3D structures of
proteins and nucleic acids solved to date. To solve the crystal
structure of a macromolecule by X-ray crystallography, we initially
require milligram quantities of highly pure protein. This is achieved
using molecular cloning techniques and column chromatography.
The purified protein is then placed under conditions that promote
a transition from the liquid to the solid phase. These conditions
are chosen to promote crystal formation as compared to random
aggregation of the protein (referred to as precipitation). Crystals
are simply a 3D array of identical molecules that interact with
each other in precisely the same way throughout the crystal. Protein
crystals vary in size between 0.05 - 0.5 mm. When crystals are
placed in a beam of X-rays (wavelength of 0.9 – 2Å),
a small portion of the X-ray beam is scattered in a direction
different from its original direction. This effect is referred
to as diffraction of X-rays. Thousands of diffraction events occur
for a protein crystal. The diffraction of X-rays by crystals is
mathematically related to two properties of the crystal: how the
molecules are packed in the crystal and the structure of the molecules
that makes up the crystal. By collecting the diffraction data,
we can determine the structure of the molecule that makes up the
crystal using computational algorithms.


In
the Center for Structural Biochemistry (basement of the Chemistry
building), we have an RU-H3R rotating anode X-ray generator with
an R-AXIS IV++ image plate detector. For data collection of frozen
crystals at 100K, we have a 600 series Oxford Cryostream.