Given the surface tension of water,
T = 75 dyne/cm
Radius r = 0.1/2 mm = 0.05 mm = 0.005 mm
density ρ=1gm/cm3, angle of contact, θ=0∘
Let h be the height to which water rise in capillary tube
Then
h=2Tcosθrpg=2×75×cos0∘0.005×1×981cm=30.58cm
But the length of capillary tube, h = 5 cm
c. The water will not overflow out of the upper end of the capillary. It will rise only up to the upper end of the capillary
The liquid meniscus will adjust its radius of curvature R in a such a way that
R1h1=Rh[hR=2Tρg=constant]
Where R is the radius of curvature liquid meniscus would possess if the capillary tube were of sufficient length
R1=Rhh=rhh1[R=rcosθ=rcos0∘=r]
=0.005×30.585=0.0306cm