We first look at the lattice points of a space lattice. Considering the scattering from any two lattice points P1,P2 in given figure, seperated by vector r.The unit incident wave normal is S0 and the unit scattered wave normal is S. We examine at a point 'a' long distance away ,the difference in phase of the radiation scattered by P1 and P2.
If P2A and P1B are the projections of vector r on the incident and scattered wave directions, the path difference between the two scattered wave is -----
The vector S happens to represent the direction of the normal to a plane that reflects the incident direction into the scattering direction as shown in the following figure:---
If 2@ is the angle vector S makes with vector S0, then @ is the angle of incidence and from the figure we see that
|S|=2.Sin@ as S and S0 are unit vectors.The phase fifference (phai) is equal to (2.pai/lambda).path difference.
We have
For this condition , the separate scattered amplitudes add up constructively and the intensity in the diffracted beam is maximum. If a,b,c are the primitive translation vectors , we have for the diffraction maxima:-------
Where h,k,l are integers . We have for direction cosine:---
The Laue equation state that in a diffraction direction the dcs are proportional to h/a, k/b,l/c.
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