To solve this problem, we need to calculate the change in energy required to transfer a satellite from one orbit to another around a planet. The energies involved in both the initial and final orbits will help us find the answer.
Step 1: Understand the energy formula.
The total energy \( E \) of a satellite in an orbit of radius \( r \) is given by:
\(E = -\frac{G M m}{2r}\)
Here, \( G \) is the gravitational constant, \( M \) is the mass of the planet, \( m \) is the mass of the satellite, and \( r \) is the radius of the orbit.
Step 2: Calculate the initial energy.
The initial orbit radius is \( 1.5R \). Thus, the initial energy \( E_1 \) is:
\(E_1 = -\frac{G M m}{2 \times 1.5R} = -\frac{G M m}{3R}\)
Step 3: Calculate the final energy.
The final orbit radius is \( 3R \). Thus, the final energy \( E_2 \) is:
\(E_2 = -\frac{G M m}{2 \times 3R} = -\frac{G M m}{6R}\)
Step 4: Calculate the change in energy.
The change in energy \( \Delta E \), which is the additional energy required to move the satellite to the new orbit, is given by:
\(\Delta E = E_2 - E_1\)
Substituting the energies from Step 2 and Step 3, we have:
\(\Delta E = -\frac{G M m}{6R} - \left(-\frac{G M m}{3R}\right)\)
Simplifying the expression, we get:
\(\Delta E = -\frac{G M m}{6R} + \frac{G M m}{3R} = \frac{G M m}{6R}\)
The additional minimum energy required to transfer the satellite from orbit radius \( 1.5R \) to \( 3R \) is:
\(\frac{G M m}{6R}\)
Thus, the correct option is:
\(\frac{G M m}{6R}\)
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.)