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(D) The height of the liquid column in a capillary tube is given by the formula $h = \frac{2T \cos 	heta}{r ho g}$,where $T$ is the surface tension

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Full length of the capillary tube

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(D) The height of the liquid column in a capillary tube is given by the formula $h = \frac{2T \cos 	heta}{r ho g}$,where $T$ is the surface tension,$	heta$ is the angle of contact,$r$ is the radius of the tube,$ho$ is the density of the liquid,and $g$ is the acceleration due to gravity.In an artificial satellite revolving around the Earth,the effective acceleration due to gravity $g_{eff}$ is zero because the satellite is in a state of weightlessness.Substituting $g = 0$ into the formula,we get $h = \frac{2T \cos 	heta}{r ho (0)} = \infty$.Since the height cannot be infinite,the liquid will rise until it reaches the top end of the capillary tube. Therefore,the water will rise to the full length of the capillary tube.

In a surface tension experiment with a capillary tube,water rises up to $0.1\, m$. If the same experiment is repeated on an artificial satellite,which is revolving around the Earth,water will rise in the capillary tube up to a height of:

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