To determine how the terminal velocity \((v_t)\) of a spherical raindrop depends on its radius \(r\), we need to understand the concept of terminal velocity and the forces acting on the raindrop.
**Explanation:**
Terminal velocity is the constant speed that a freely falling object eventually reaches when the resistance of the medium through which it is falling prevents further acceleration. For a raindrop, this involves the balance between gravitational force and drag force.
The gravitational force on a raindrop is given by:
\(F_g = mg = \rho V g = \rho \left(\frac{4}{3}\pi r^3\right)g\)
where:
The drag force \(F_d\) acting on the raindrop in a fluid is given by Stoke's Law (for small, spherical objects and low Reynolds numbers):
\(F_d = 6 \pi \eta r v_t\)
where:
At terminal velocity, these two forces are equal:
\(\rho \left(\frac{4}{3}\pi r^3\right)g = 6 \pi \eta r v_t\)
Solving for \(v_t\), we get:
\(v_t = \frac{\rho g}{6 \eta} \cdot \frac{4}{3} \pi r^2\)
Thus, the terminal velocity \(v_t\) is directly proportional to \(r^2\).
Therefore, the correct answer is:
| \(r^2\) |
This reasoning shows why the terminal velocity of the raindrop depends on the square of its radius.
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\(^2\)). 