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Chapter II Solution Growth….<br />

104<br />

(2.19)<br />

Where, v is the molar volume of the crystal, N is the Avagadro’s<br />

number and R is the gas constant. Equation (2.19) suggests a straight line for<br />

a plot of<br />

2<br />

1/ 1n S against 1n can be drawn with a slope given by,<br />

3 2<br />

16<br />

N<br />

m <br />

3 3<br />

(2.20)<br />

3R T<br />

Since B weakly depends on temperature. All the quantities in equation<br />

(2.20) are known except the interfacial tension . The interfacial tension of the<br />

solid relative to its solution can be calculated from the slope of the line 1/lnS 2<br />

as,<br />

(2.21)<br />

The energy of formation of a critical nucleus can be calculated from the<br />

experimental using following relation,<br />

(2.22)<br />

The radius of the nucleus in equilibrium with its solution has been<br />

computed as,<br />

2.24 Effect of Soluble Impurities on Nucleation<br />

(2.23)<br />

The nucleation rate of a solution or melt can be affected appreciably<br />

by the presence of mere traces of impurities in the system. Crystallization<br />

from solutions always proceeds in multi component systems, because even<br />

in the purest form there are some impurities. Impurities may be both in

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