A body of mass m is placed on earth surface which is taken from earth surface to a height of h = 3R then change in gravitational potential energy is :
\(\frac{mgR}{4}\)
\(\frac{2}{3}mgR\)
\(\frac{3}{4}mgR\)
\(\frac{mgR}{2}\)
To determine the change in gravitational potential energy when a body of mass \(m\) is taken from the Earth's surface to a height \(h = 3R\) (where \(R\) is the radius of the Earth), we use the formula for gravitational potential energy.
The gravitational potential energy at a distance \(r\) from the center of the Earth is given by:
U = -\frac{GMm}{r}
where:
Initially, the body is at the Earth's surface, so its distance from the center of the Earth is \(R\). The initial potential energy (\(U_1\)) is:
U_1 = -\frac{GMm}{R}
When the body is at a height \(h = 3R\), the total distance from the center is \(R + 3R = 4R\). The final potential energy (\(U_2\)) is:
U_2 = -\frac{GMm}{4R}
The change in gravitational potential energy (\(\Delta U\)) is the difference between the final and initial potential energies:
\Delta U = U_2 - U_1 = \left(-\frac{GMm}{4R}\right) - \left(-\frac{GMm}{R}\right)
Simplifying, we get:
\Delta U = \frac{GMm}{R} - \frac{GMm}{4R} = \frac{GMm}{R} \left(1 - \frac{1}{4}\right) = \frac{GMm}{R} \times \frac{3}{4}
Given the gravitational force relationship on Earth's surface \(g = \frac{GM}{R^2}\), hence \(GM = gR^2\), substituting this gives:
\Delta U = \frac{g R^2 m}{R} \times \frac{3}{4} = \frac{3}{4} mg R
Thus, the change in gravitational potential energy when the body is raised to a height of \(3R\) from the Earth's surface is \(\frac{3}{4}mgR\), which corresponds to the given correct option.
The height from Earth's surface at which acceleration due to gravity becomes \(\frac{g}{4}\) is \(\_\_\)? (Where \(g\) is the acceleration due to gravity on the surface of the Earth and \(R\) is the radius of the Earth.)