The Helmholtz free energy of a liquid column that rises, due to surface tension, inside a capillary tube (Figure 1), as a function of the height, h, is given by: F(h) =(ro)gr^2h^2/2 = -2 pi sigma r h cos teta,   where r is the radius of the tube, g is the local ac- celaration of gravity,  is the surface tension of the liquid, and  is the contact angle of the liquid in contact with the wall of the tube. (a) From this expression, obtain the value of h as a function of the other physical parameters at equilibrium.Calculate the height that water will rise in a capil-lary of diameter 0.05mm. Assume that the contactangle between the water and the tube is zero. Thesurface tension of water at experimental conditionsisσ= 7.73×10−2N/m, and the local accelarationof gravity isg= 9.7m/s2.

Elements Of Electromagnetics
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Author:Sadiku, Matthew N. O.
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The Helmholtz free energy of a liquid

column that rises, due to surface tension, inside

a capillary tube (Figure 1), as a function of the

height, h, is given by:

F(h) =(ro)gr^2h^2/2 = -2 pi sigma r h cos teta,

 

where r is the radius of the tube, g is the local ac-

celaration of gravity,  is the surface tension of the

liquid, and  is the contact angle of the liquid in

contact with the wall of the tube. (a) From this

expression, obtain the value of h as a function of

the other physical parameters at equilibrium.Calculate the height that water will rise in a capil-lary of diameter 0.05mm. Assume that the contactangle between the water and the tube is zero. Thesurface tension of water at experimental conditionsisσ= 7.73×10−2N/m, and the local accelarationof gravity isg= 9.7m/s2.

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