written 8.4 years ago by | • modified 8.4 years ago |
Mumbai university > FE > SEM 1 > Applied Physics 1
Marks: 8M
Year: May 2014
written 8.4 years ago by | • modified 8.4 years ago |
Mumbai university > FE > SEM 1 > Applied Physics 1
Marks: 8M
Year: May 2014
written 8.4 years ago by |
In powder method, a specimen is finely powdered and taken in a thin walled capillary tube.
The specimen consists of tiny crystals or crystallites which are oriented randomly.
When a narrow beam of X-ray incidents on the specimen, it comes across few crystallites with planes at glancing angle θ so as to satisfy Bragg's Law.
Since all the orientations are equally likely, the diffracted rays will form a cone with the line of incident beam as the axis and the semi cone angle θ.
These diffracted beams are detected by placing a photographic film along the circumference of the circle with specimen at the center.
If "L" is the circumferential distance from the two extreme edges of cone formed by the diffracted X-rays and "R" is the radius of the circle along which film was placed, then;
$$\frac{L}{2πR} = \frac{4θ}{360}$$
$$ ∴ θ = \frac{45 L}{πR}$$