To determine the length of water rise in a capillary, we use the capillary action formula:
\( h = \frac{2T \cos \theta}{r \rho g} \)
Where:
Substituting these values into the formula:
\( h = \frac{2 \times 0.07 \times 1}{0.0001 \times 1000 \times 9.8} \)
\( = \frac{0.14}{0.98} \)
\( = 0.142857 \) m \( = 14.2857 \) cm
However, since the capillary tube is inclined at \( 30^\circ \) to the vertical, the actual length of the water column along the tube, \( l \), is given by the relationship:
\( l = \frac{h}{\cos 30^\circ} \)
Where:
Calculating \( l \):
\( l = \frac{14.2857}{0.866} \)
\( \approx 16.5 \) cm
Thus, the length of water risen in the capillary tube is \( \frac{82}{5} \approx 16.4 \) cm, which matches closely with our calculation due to rounding.
The correct answer is: \( \frac{82}{5} \)
Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity)