For both FCC and BCC crystal structures, there are two different types of
interstitial sites. In each case, one site is larger than the other and is
normally occupied by impurity atoms. For FCC, this larger one is located at
the center of each edge of the unit cell; it is termed an octahedral
interstitial site. On the other hand, with BCC the larger site type is found
at \(0 \frac{1}{2} \frac{1}{4}\) positions \(-\) that is, lying on \(\\{100\\}\)
faces and situated midway between two unit cell edges on this face and one-
quarter of the distance between the other two unit cell edges; it is termed a
tetrahedral interstitial site. For both FCC and BCC crystal structures,
compute the radius \(r\) of an impurity atom that will just fit into one of
these sites in terms of the atomic radius \(R\) of the host atom.