written 8.4 years ago by | • modified 8.4 years ago |
where (a= 2.125 $A^0$). Consider the case of second order maximum and λ=0.592 $A^0$ -
Mumbai university > FE > SEM 1 > Applied Physics 1
Marks: 7M
Year: Dec 2012
written 8.4 years ago by | • modified 8.4 years ago |
where (a= 2.125 $A^0$). Consider the case of second order maximum and λ=0.592 $A^0$ -
Mumbai university > FE > SEM 1 > Applied Physics 1
Marks: 7M
Year: Dec 2012
written 8.4 years ago by |
Bragg's Law:-
Consider a regular arrangement of atoms with inter-planar distance "d". An X-ray beam is incident upon the surface at glancing angle "θ"
Let us assume that the path difference between the scattered rays BC and EF as ∆=nλ thus producing constructive interference.
Now,
∆ = PE + EQ
∴∆ = BE.sin θ + BE.sin θ
∴∆ = 2BE.sin θ
∴∆ = 2d.sin θ
But, ∆ = nλ
∴nλ = 2d.sinθ
This, is the required expression for Bragg's Law
Numerical
Given:-
Miller Indices: (1 0 0) = (h k l)
a = 2.125 $A^0$
λ = 0.592 $A^0$
n = 2 (Second order maxima)
To Find:- Glancing Angle (θ)
Solution:-
We know that,
$d = \frac{a}{\sqrt{h^2 + k^2 + I^2}}$
$d = \frac{2.125}{\sqrt{1^2 + 0^2 + 0}}$
$d = 2.125$
Using Bragg's Law,
∴ nλ = 2d.sinθ
∴2 x 0.592 = 2 x 2.125 x sinθ
$∴θ = 16.176^0$