When a capillary tube is dipped in a liquid, the liquid rises to a height h in the tube. The free liquid surface inside, the tube is hemispherical in shape. The tube is now pushed down so that the height of the tube outside the liquid is less than h. Then
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Explanation:
Consider a capillary tube of radius r immersed in a liquid of surface tension T and density ρ. The height to which the liquid will rise in the capillary tube is given as
rρg
2Tcosθ
=
Rρg
2T
or
hR=
ρg
2T
which is a constant.
Thus we get
h
1
R
1
=h
2
R
2
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