Question 6.11: The capillary rise h, of a fluid of density ρ, and surface t...

The capillary rise h , of a fluid of density \rho , and surface tension \sigma , in a tube of diameter D, depends upon the contact angle \phi , and acceleration due to gravity g . Find an expression for h in terms of dimensionless variables by Rayleigh’s indicial method.

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Capillary rise h , is the dependent variable of the problem and can be expressed in terms of the independent variables as

h=A \rho^{a} \sigma^{b} D^{c} g^{d} \phi              (6.50)

where A is a dimensionless constant.

( \phi is not raised to any exponent, since it is a dimensionless variable and hence an independent \pi term).
Expressing the variables in terms of their fundamental dimensions in the above equation, we get

\mathrm{L}=\mathrm{A}\left(\mathrm{ML}^{-3}\right)^{a}\left(\mathrm{MT}^{-2}\right)^{b} \mathrm{~L}^{c}\left(\mathrm{LT}^{-2}\right)^{d}

Equating the exponents of M, L and T in LHS and RHS of the equation, we have

a+b =0

-3 a+c+d =1

-2 b-2 d =0

Solving these three equations in terms of a, we get

b=-a

c=1+2 a

d=a

Substituting these values in Eq. (6.52), we get

h=A D\left(\frac{\rho g D^{2}}{\sigma}\right)^{a} \phi

Or  \frac{h}{D}=A\left(\frac{\rho g D^{2}}{\sigma}\right)^{a} \phi

This is the required expression.

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