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CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...

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peaks are found to decrease with increase in ethylene glycol content in the reaction medium.<br />

Table 7 shows the variation in average crystallite size as a function of relative amounts of<br />

ethylene glycol and glycerol in the reaction medium. From these results, it is inferred that the<br />

average crystallite size can be tuned by varying the relative amounts of ethylene glycol and<br />

glycerol in the reaction medium. The observed variation in the crystallite size with change in<br />

the relative concentration of the solvent has been explained based on the increase in viscosity<br />

of the medium with increase in the relative concentration of glycerol and associated increase<br />

in growth rate. XRD patterns are least square fitted to determine the lattice parameters. The<br />

values for un-doped SbPO 4 samples are a = 5.099(1) Å, b = 6.767(2) Å, c = 4.749(1) Å with β<br />

= 94.73. Corresponding values for the 5% Tb 3+ doped nanoparticles are a = 5.093(1) Å, b =<br />

6.769(2) Å, c = 4.733(1) Å with β = 94.69. There is no significant change in the values of<br />

lattice parameters for both doped and un-doped samples. This can be attributed to the<br />

comparable ionic radii of Sb 3+ and Tb 3+ under a coordination number of four. In order to<br />

check the nature of amorphous product obtained when pure ethylene glycol is used as the<br />

solvent, IR patterns were recorded for the amorphous product and it is compared with the<br />

patterns obtained from crystalline SbPO 4 sample. Figure 62 shows IR spectra of as prepared<br />

SbPO 4 sample obtained by using pure ethylene glycol, pure glycerol and a mixture of<br />

glycerol and ethylene glycol (10 ml each).<br />

Table.7. Effect of variation volume of solvents on the average crystallite size of SbPO 4<br />

nanomaterials.<br />

Volume of<br />

glycerol (ml)<br />

Volume of ethylene<br />

glycol (ml)<br />

Average crystallite size<br />

(nm)<br />

20 0 46<br />

10 10 28<br />

8 12 12<br />

0 20 -<br />

114

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