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CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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52<br />

of crystal planes appear at different angles, this forms the basis for identification of different<br />

phases. The angle of diffraction is clearly indicative of distances between the planes. The<br />

relationship between lattice plane spacing and angle of diffraction is given by Bragg’s law.<br />

n<br />

2dsin<br />

(2.4)<br />

In equation 2.4 n is the order of diffraction; is diffraction angle; d is the lattice spacing.<br />

Another important factor which helps in indexing an XRD pattern is the intensity of<br />

diffraction. The intensity is also a function of atomic scattering factors and miller indices of<br />

the planes. The atomic scattering factors influences intensity as the scattering centers in<br />

atoms are electrons. Therefore higher the number of electrons, greater is scattering from that<br />

particular atom. Phase characterization can be done just by comparing the diffraction pattern<br />

obtained for samples with that of previously reported patterns as given by database from by<br />

Joint Committee on Powder Diffraction Standards (JCPDS), International Centre for<br />

Diffraction Data (ICDD).<br />

Apart from phase characterization one can obtain information on particle size assuming the<br />

particles are spherical. For a bulk crystallite or a large crystal, scattering signal is sharp,<br />

however in nanocrystallites the peaks are broadened due to coherence lengths of X-ray.<br />

Therefore the broadening is related to size of the diffracting domain therefore of crystallite<br />

size.<br />

k<br />

D <br />

2cos<br />

(2.5)<br />

In the equation above, k is the shape factor and is generally close to 1; D is the crystallite<br />

size. The broadening of an x-ray peak is actually a combination of instrumental broadenings<br />

arising from incident x-ray peak breadth and detectors etc. Instrumental factors are

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