Step 1: Identify the given parameters and convert them to consistent units.
Radius of the capillary tube, \( r = 0.1 \, \text{mm} = 0.01 \, \text{cm} \)
Surface tension of water, \( T = 70 \, \text{dyn/cm} \)
Contact angle, \( \theta \approx 0^\circ \)
Angle of inclination of the capillary tube with the vertical, \( \alpha = 30^\circ \)
Acceleration due to gravity, \( g = 9.8 \, \text{m/s}^2 = 980 \, \text{cm/s}^2 \)
Density of water, \( \rho = 1 \, \text{g/cm}^3 \)
Step 2: Determine the vertical height \( h \) of the water risen in the capillary tube.
The formula for the height of the liquid risen in a capillary tube is given by:
\[
h = \frac{2T \cos \theta}{r \rho g}
\]
Substituting the given values:
\[
h = \frac{2 \times 70 \times \cos(0^\circ)}{0.01 \times 1 \times 980} = \frac{140 \times 1}{9.8} = \frac{1400}{98} = \frac{100}{7} \, \text{cm}
\]
Step 3: Relate the vertical height \( h \) to the length \( l \) of the water risen along the inclined capillary tube.
Let \( l \) be the length of the water risen in the capillary tube. From the geometry of the situation, we have:
\[
h = l \cos \alpha
\]
where \( \alpha \) is the angle of inclination of the capillary tube with the vertical.
Given \( \alpha = 30^\circ \), we have \( \cos(30^\circ) = \frac{\sqrt{3}}{2} \).
So,
\[
l = \frac{h}{\cos \alpha} = \frac{h}{\cos(30^\circ)} = \frac{100/7}{\sqrt{3}/2} = \frac{200}{7\sqrt{3}} \, \text{cm}
\]
There seems to be a mistake in the calculation or the provided options, as the derived value does not match any of them. Let's recheck the steps.
Revisiting
Step 2:
\[
h = \frac{2 \times 70 \times \cos(0^\circ)}{0.01 \times 1 \times 980} = \frac{140}{9.8} = \frac{1400}{98} = \frac{100}{7} \, \text{cm}
\]
Revisiting
Step 3:
The angle of inclination with the vertical is \( 30^\circ \). The vertical height \( h \) is related to the length along the tube \( l \) by \( h = l \cos(30^\circ) \).
So, \( l = \frac{h}{\cos(30^\circ)} = \frac{100/7}{\sqrt{3}/2} = \frac{200}{7\sqrt{3}} \approx \frac{200}{7 \times 1.732} \approx \frac{200}{12.124} \approx 16.5 \, \text{cm} \).
This still does not match the options. Let's assume there might be a slight misinterpretation of the question or a potential error in the options.
Let's reconsider the problem. The vertical height risen is \( h = \frac{100}{7} \) cm. The length risen along the inclined tube \( l \) is such that its vertical component is \( h \).
Therefore, \( h = l \cos(30^\circ) \).
\( l = \frac{h}{\cos(30^\circ)} = \frac{100/7}{\sqrt{3}/2} = \frac{200}{7\sqrt{3}} \).
If the question meant the angle with the horizontal, then \( h = l \sin(30^\circ) \), and \( l = \frac{h}{\sin(30^\circ)} = \frac{100/7}{1/2} = \frac{200}{7} \approx 28.57 \). This also doesn't match.
Let's check the units carefully. Radius in cm, surface tension in dyn/cm, density in g/cm\(^3\), g in cm/s\(^2\). The height \( h \) will be in cm.
Let's assume there was a calculation error in the options and try to match the closest value. \( \frac{200}{7\sqrt{3}} \approx 16.5 \). None of the options are close to this.
Let's re-read the question carefully: "with \( 30^\circ \) inclined with vertical."
We have \( h = \frac{100}{7} \) cm.
The length along the tube \( l \) is given by \( h = l \cos(30^\circ) \).
\( l = \frac{h}{\cos(30^\circ)} = \frac{100/7}{\sqrt{3}/2} = \frac{200}{7\sqrt{3}} \).
There might be an error in the question or the provided options. However, if we were to choose the closest option based on a potential approximation or a different interpretation, it would be challenging.
Let's double-check the calculation for \( h \).
\( h = \frac{2 \times 70 \times 1}{0.01 \times 1 \times 980} = \frac{140}{9.8} = \frac{1400}{98} = \frac{100}{7} \) cm.
Let's check the options' decimal values:
(1) \( \frac{82}{5} = 16.4 \)
(2) \( \frac{57}{2} = 28.5 \)
(3) \( \frac{71}{5} = 14.2 \)
(4) \( \frac{68}{5} = 13.6 \)
The value \( \frac{200}{7\sqrt{3}} \approx 16.5 \) is closest to option (1) \( \frac{82}{5} = 16.4 \). There might be a rounding error or a slight difference in the values used.