Answer:
Volume of drop of
radius \[R=N\times \]volume of drop of radius \[r\]
\[\frac{4}{3}\,\pi
{{R}^{3}}=\,N\times \,\frac{4}{3}\,\pi \,{{r}^{3}}\] or \[r=\,\frac{R}{{{(N)}^{1/4}}}\]
Change
is surface area, \[\Delta A\,=\,4\pi \,({{R}^{2}}-N{{r}^{2}})\]
\[=\,4\pi
\,({{R}^{2}}-\,{{N}^{\frac{1}{3}}}{{R}^{2}})\,\,=\,4\pi
\,{{R}^{2}}\,(1-\,{{N}^{1/3}})\]
\[\therefore
\] Energy utilised \[=4\pi \,{{R}^{2}}\,(1-{{N}^{1/3}})\,T\,\]
Let
\[\Delta \theta \] be
the decrease in temperature therefore, energy utilised \[=\,m\,C\Delta \theta
\],
where
C is the specific heat of liquid.
Now
\[mc\,\,\Delta \theta =\,4\pi \,{{R}^{2}}\,(1-{{N}^{1/3}})\,T\]
or \[\Delta
\theta =\,\frac{4\pi \,{{R}^{2}}\,(1-\,{{N}^{1/3}})T}{mc}\]
Since
mass of drop, \[m=\,\frac{4}{3}\,\pi \,{{R}^{3}}\rho \]
\[\therefore
\] \[\Delta \theta =\,\frac{3\,\times \,4\,\pi
\,{{R}^{2}}(1-\,{{N}^{1/3}})T}{4\pi \,{{R}^{3}}\,\rho C}\]
\[=\,\frac{3T}{R\rho
C}\,(1-\,{{N}^{1/3}})\].
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