\(145.4 \times 10^{–6} \text{ms}^{–1}\)
\(118.0 \times 10^{–6} \text{ms}^{–1}\)
\(132.6 \times 10^{–6} \text{ms}^{–1}\)
\(123.4 \times 10^{–6} \text{ms}^{–1}\)
To find the terminal velocity of a water drop of radius \(1 \, \mu m\) falling under the influence of a viscous force in a medium where the buoyant force can be neglected, we use Stokes' Law.
Stokes' Law for the drag force (\(F_d\)) experienced by a spherical object moving through a viscous fluid is given by:
\[F_d = 6 \pi \eta r v\]where:
At terminal velocity, the gravitational force acting on the drop is balanced by the drag force:
\[F_g = F_d\]The gravitational force (\(F_g\)) on the water drop is given by:
\[F_g = \frac{4}{3} \pi r^3 \rho g\]where:
Equating \(F_g = F_d\) gives:
\[\frac{4}{3} \pi r^3 \rho g = 6 \pi \eta r v\]Solving for \(v\), we get:
\[v = \frac{2 r^2 \rho g}{9 \eta}\]Substituting the given values:
\[v = \frac{2 \times (1 \times 10^{-6})^2 \times 10^3 \times 9.8}{9 \times 1.8 \times 10^{-5}}\]Calculating the above expression:
\[v = \frac{2 \times 1 \times 10^{-12} \times 10^3 \times 9.8}{1.62 \times 10^{-4}}\]\[v = \frac{19.6 \times 10^{-9}}{1.62 \times 10^{-4}}\]\[v = \frac{19.6}{1.62} \times 10^{-5}\]\[v \approx 12.34 \times 10^{-5} \, \text{m/s}\]\[v \approx 123.4 \times 10^{-6} \, \text{ms}^{-1}\]Therefore, the terminal velocity of the water drop is \(123.4 \times 10^{-6} \, \text{ms}^{-1}\), which is the correct answer.
Water flows through a horizontal tube as shown in the figure. The difference in height between the water columns in vertical tubes is 5 cm and the area of cross-sections at A and B are 6 cm\(^2\) and 3 cm\(^2\) respectively. The rate of flow will be ______ cm\(^3\)/s. (take g = 10 m/s\(^2\)). 