A capillary tube of radius ' $r$ ' is immersed in water and water rises to a height of ' $h$ '. Mass of…
A capillary tube of radius ' $r$ ' is immersed in water and water rises to a height of ' $h$ '. Mass of water in the capillary tube is $5 \times 10^{-3} \mathrm{~kg}$. The same capillary tube is now immersed in a liquid whose surface tension is $\sqrt{2}$ times the surface tension of water. The angle of contact between the capillary tube and this liquid is $45^{\circ}$. The mass of liquid which rises into the capillary tube now is, (in $\mathrm{kg}$ )
$5 \times 10^{-3}$
$2.5 \times 10^{-3}$
$5 \sqrt{2} \times 10^{-3}$
$3.5 \times 10^{-3}$
Solution
We knows height of water rise in a capillary tube
$
\begin{gathered}
h=\frac{2 T \cos \theta}{r d g} \\
h_1=\frac{2 T_1 \cos \theta_1}{r d g}, \quad h_2=\frac{2 T_2 \cos \theta_2}{r d g}
\end{gathered}
$
Given, $h_1=h, T_1=T, \theta_1=0$
$
\therefore \quad h=\frac{2 T}{r d g}
$
Given, $T_2=\sqrt{2} T, \theta=45^{\circ}, \cos 45^{\circ}=\frac{1}{\sqrt{2}}$
$
\therefore \quad h_2=\frac{2 \sqrt{2} T \times \frac{1}{\sqrt{2}}}{r d g}
$
From Eqs. (i) and (ii), we observe
$
h_2=h \text {. }
$
Hence, same mass of liquid rises into the capillary as before $5 \times 10^{-3} \mathrm{~kg}$