A liquid of density \(800\,\text{kg m}^{-3}\) rises \(4\,\text{cm}\) in a capillary tube of inner radius \(0.2\,\text{mm}\). The capillary tube is dipped vertically in the liquid and the angle of contact between the capillary tube and the liquid is \(0^\circ\). The excess pressure inside the spherical drop of diameter \(2\,\text{cm}\) of the same liquid is
\[
(\text{Acceleration due to gravity}=10\,\text{m s}^{-2})
\]