| 1. | The terminal velocity is directly proportional to the square of the radius of the body. |
| 2. | The terminal velocity is inversely proportional to viscosity of the medium. |
| 3. | The terminal velocity is proportional to the difference of densities of body and fluid. |
| 4. | All of these |
Two small spherical metal balls, having equal masses, are made from materials of densities such that and having radii of 1 mm and 2 mm, respectively. They are made to fall vertically (from rest) in a viscous medium whose coefficient of viscosity equals and whose density is 0.1. The ratio of their terminal velocities would be:
1.
2.
3.
4.
| 1. | \(\dfrac{2}{9}\dfrac{{r}^{2}{\rho}{g}}{v}\) | 2. | \(\dfrac{1}{3}\dfrac{{r}^{2}{\rho}{g}}{v}\) |
| 3. | \(\dfrac{1}{9}\dfrac{{r}^{2}{\rho}{g}}{v}\) | 4. | \(\dfrac{1}{4}\dfrac{{r}^{2}{\rho}{g}}{v}\) |
Spherical balls of radius \(R\) are falling in a viscous fluid of viscosity with a velocity \(v.\) The retarding viscous force acting on the spherical ball is:
| 1. | directly proportional to \(R\) but inversely proportional to \(v.\) |
| 2. | directly proportional to both radius \(R\) and velocity \(v.\) |
| 3. | inversely proportional to both radius \(R\) and velocity \(v.\) |
| 4. | inversely proportional to \(R\) but directly proportional to velocity \(v.\) |
| 1. | the size of the raindrop |
| 2. | the viscosity of air |
| 3. | the acceleration due to gravity |
| 4. | all of the above |