To determine the internal radius of the capillary, we use the formula for capillary rise:
\[ h = \frac{2T \cos \theta}{r \rho g} \]
Given that water completely wets the glass, \( \theta = 0^\circ \), so \( \cos \theta = 1 \). Thus, the formula simplifies to:
\[ h = \frac{2T}{r \rho g} \]
\[ r = \frac{2T}{h \rho g} \]
\( T = 73.2 \, \text{dyn/cm} = 73.2 \times 10^{-5} \, \text{N/m} \),
\( h = 1.0 \, \text{cm} = 0.01 \, \text{m} \),
\( \rho = 0.996 \, \text{g/cm}^3 = 996 \, \text{kg/m}^3 \),
\( g = 980 \, \text{cm/s}^2 = 9.8 \, \text{m/s}^2 \).
\[ r = \frac{2 \times 73.2 \times 10^{-5}}{0.01 \times 996 \times 9.8} \]
\[ r \approx 0.001496 \, \text{m} = 0.1496 \, \text{cm} \]
Rounding off to two decimal places, \( r \approx 0.15 \, \text{cm} \). The calculated internal radius of the capillary is \( 0.15 \, \text{cm} \), which is within the expected range of \( 0.148 \, \text{cm} \) to \( 0.151 \, \text{cm} \).
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