
- A${\left( {\frac{R}{{3d}}} \right)^{\frac{1}{3}}}$
- B${\left( {\frac{R}{{6d}}} \right)^{\frac{1}{3}}}$
- ✓${\left( {\frac{R}{{24d}}} \right)^{\frac{1}{3}}}$
- DNone

Since the volume of the water forming bubble and drop is same,
$\frac{4}{3} \pi\left(R^{3}-(R-d)^{3}\right)=\frac{4}{3} \pi r^{3}$
$\Longrightarrow r^{3} \approx 3 R^{2} d\left(\text { neglecting } d^{2} \text { and } d^{3}\right)$
Ratio of excess pressure in the drop to the excess pressure inside the bubble is given by,
Ratio $=\frac{2 \sigma / r}{4 \sigma / R}$
Ratio $=\frac{1}{2}\left(\frac{R}{r}\right)$
Substituting the value of $\mathrm{r}$ gives $\left(\frac{R}{24 d}\right)^{1 / 3}$
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where $p =$ pressure, $\rho =$ density, $v =$ speed, $h =$ height of the liquid column, $g=$ acceleration due to gravity and $k$ is constant. The dimensional formula for $k$ is same as that for
