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Question: A small steel ball of radius \(r\) is allowed to fall under gravity through a column of a viscous li...

A small steel ball of radius rr is allowed to fall under gravity through a column of a viscous liquid of coefficient of viscosity η\eta. After some time the velocity of the ball attains a constant value known as terminal velocity vTv_{T}. The terminal velocity depends on (i) the mass of the ball mm, (ii) η\eta, (iii) rr and (iv) acceleration due to gravity gg. Which of the following relations is dimensionally correct

A

vTmgηrv_{T} \propto \frac{mg}{\eta r}

B

vTηrmgv_{T} \propto \frac{\eta r}{mg}

C

vTηrmgv_{T} \propto \eta rmg

D

vTmgrηv_{T} \propto \frac{mgr}{\eta}

Answer

vTmgηrv_{T} \propto \frac{mg}{\eta r}

Explanation

Solution

By substituting dimension of each quantity in R.H.S. of option (1) we get [mgηr]6mu=6mu[M×LT2ML1T1×L]\left\lbrack \frac{mg}{\eta r} \right\rbrack\mspace{6mu} = \mspace{6mu}\left\lbrack \frac{M \times LT^{- 2}}{ML^{- 1}T^{- 1} \times L} \right\rbrack

=[LT1]\lbrack LT^{- 1}\rbrack.

This option gives the dimension of velocity.

[mgηr]6mu=6mu[M×LT2ML1T1×L]\left\lbrack \frac{mg}{\eta r} \right\rbrack\mspace{6mu} = \mspace{6mu}\left\lbrack \frac{M \times LT^{- 2}}{ML^{- 1}T^{- 1} \times L} \right\rbrack=[LT1]\lbrack LT^{- 1}\rbrack