A satellite of mass m is orbiting the earth [of radius R] at a height h from its surface. The total energy of the satellite in terms of , the value of acceleration due to gravity at the earth's surface is -
1.
2.
3.
4.
The work done to raise a mass m from the surface of the earth to a height h, which is equal to the radius of the earth, is:
1.
2. mgR
3. 2mgR
4.
| 1. | \( {\left[{MLT}^{-2}\right]} \) | 2. | \( {\left[{MLT}^2\right]} \) |
| 3. | \( {\left[{ML}^2 {T}^{-2}\right]} \) | 4. | \( {\left[{ML}^{-2} {T}^2\right]}\) |
A body of mass m rises to height h = R/5 from the earth's surface, where R is earth's radius. If g is acceleration due to gravity at earth's surface, the increase in potential energy is -
1. mgh
2.
3.
4.
If a body of mass m placed on the earth's surface is taken to a height of h = 3R, then the change in gravitational potential energy is:
1.
2.
3.
4.
A particle is dropped from a height h = 3R above the earth's surface, where R is the radius of the earth. If g is the acceleration due to gravity on the earth surface, then the speed with which the particle strikes the earth surface is:
1.
2.
3.
4.
| 1. | \(\dfrac{g}{R}\) | 2. | \(\dfrac{R}{g}\) |
| 3. | \(gR\) | 4. | \(\dfrac{g}{R^{2}}\) |
A body of mass \(m\) is taken from the earth's surface to the height \(h\) equal to the radius of the earth, the increase in potential energy will be:
1. \(mgR\)
2. \(\frac{1}{2}~mgR\)
3. \(2 ~mgR\)
4. \(\frac{1}{4}~mgR\)
When a body of mass m is lifted from the surface of the earth to a height equal to radius R of the earth, the change in gravitational potential energy of the body is (g: acceleration due to gravity at the surface of the earth):
(1) mgR
(2) mgR
(3) 3 mgR
(4) 2 mgR
The work done to raise a mass m from the surface of the earth to a height h, which is equal to the radius of the earth, is:
1.
2. mgR
3. 2mgR
4.