To solve this problem, we need to find the angle at which the water meets the capillary tube, i.e., the contact angle \( \theta \). We can use the formula related to capillary action:
h = \dfrac{2T \cos \theta}{\rho g r}
Where:
- \( h \) is the height of the liquid column (in meters)
- \( T \) is the surface tension of water \((0.7 \, \text{N/m})\)
- \( \rho \) is the density of water \((1000 \, \text{kg/m}^3)\)
- \( g \) is the acceleration due to gravity \((9.8 \, \text{m/s}^2)\)
- \( r \) is the radius of the capillary tube \((0.25 \, \text{mm} = 0.25 \times 10^{-3} \, \text{m})\)
The tube projects \( 2 \, \text{cm} = 0.02 \, \text{m} \) above the water, which means the height \( h \) that the water can rise is given by the projection height:
h = 0.02 \, \text{m}
Substituting these values into our equation:
0.02 = \dfrac{2 \times 0.7 \times \cos \theta}{1000 \times 9.8 \times 0.25 \times 10^{-3}}
Rearranging gives:
\cos \theta = \dfrac{0.02 \times 1000 \times 9.8 \times 0.25 \times 10^{-3}}{2 \times 0.7}
Calculating this:
\cos \theta = \dfrac{0.02 \times 980 \times 0.25 \times 10^{-3}}{1.4} = \dfrac{0.0049}{1.4} \approx 0.0035
Using the cosine inverse function:
\theta = \cos^{-1}(0.0035)
Upon calculation, \( \theta \approx 70^\circ \).
Therefore, the angle at which the liquid meets the tube is \( \theta = 70^\circ \). The correct answer is:
- \(\theta = 70^{\circ}\) is the correct answer.