While dealing with X-ray diffraction, it is more convenient to express higher order reflections in terms of the first order reflection from planes of higher (hkl). For example, a second order reflection from (111) planes may be considered equivalent to the first order reflection from (222) planes. Similarly a third order reflection from (111) planes may be considered as the first order reflection from (333) planes. This fact can be introduced into the Bragg equation by rewriting it as
Where, is the perpendicular distance between adjacent planes having the indices
represents |
|||||||
a) |
Crystal faces |
b) |
Lattice parameter |
c) |
Crystal systems |
d) |
Miller indices |
While dealing with X-ray diffraction, it is more convenient to express higher order reflections in terms of the first order reflection from planes of higher (hkl). For example, a second order reflection from (111) planes may be considered equivalent to the first order reflection from (222) planes. Similarly a third order reflection from (111) planes may be considered as the first order reflection from (333) planes. This fact can be introduced into the Bragg equation by rewriting it as
Where, is the perpendicular distance between adjacent planes having the indices
represents |
|||||||
a) |
Crystal faces |
b) |
Lattice parameter |
c) |
Crystal systems |
d) |
Miller indices |