Two parallel glass plates are dipped partly in the liquid of density d keeping them vertical. If the distance between the plates is x, surface tension for the liquid is T and angle of contact is θ, then rise of liquid between the plates due to capillary will be
Let
h be height of liquid between the plates due to capillary action
l is length of plate in contact with liquid
weight of liquid of height (h) =d×V×g=dxlhg
vertical component of force due to surface tension =T(2l)(cosθ)
Vertical component of force due to surface tension balances weight of the liquid
∴T(2l)(cosθ)=dxlhg
⇒h=2Tcosθxdg