Two parallel glass plates are held vertically at a small separation d and dipped in a liquid of surface tension T , the angle of contact `theta =0^@` and density `rho ` . The height of water that climbs up in the gap between glass plates is given by

Two parallel glass plates are dipped perpendicularly in a liquid of density rho . The separation between the plates is ‘d' and the surface tension T. The angle of contact of glass is theta . The capillary rise of the liquid between the plates is

Two parallel glass plates separated by a small distance x ar dipped partly in a liquid of density ' d keeping them vertical .The surface tension of the liquid is T and angle of contact is theta . What is the rise of the liquid between the plates due to capillarity ?

Two very wide parallel glass plates are held vertically at a small separation d, and dipped in water. Some water climbs up in the gap between the plate. Let S be the surface tension of water P_(0)= atmospheric pressure, P= pressure of water just below the water surface in the region between the plates-

Two very wide parallel glass plates are held vertically at a small separation d, and dipped in water. Some water climbs up in the gap between the plate. Let S be the surface tension of water P_(0)= atmospheric pressure, P= pressure of water just below the water surface in the region between the plates-

Two very wide parallel glass plates are held vertically at a small separation d, and dipped in water. Some water climbs up in the gap between the plate. Let S be the surface tension of water P_(0)= atmospheric pressure, P= pressure of water just below the water surface in the region between the plates-

A capillary tube of radius r is lowered into a liquid of surface tension T and density rho . Given angle of contact =0^(@) . The work done by surface tension will be