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:
\(\frac{G M m}{6R}\)
Net gravitational force at the center of a square is found to be \( F_1 \) when four particles having masses \( M, 2M, 3M \) and \( 4M \) are placed at the four corners of the square as shown in figure, and it is \( F_2 \) when the positions of \( 3M \) and \( 4M \) are interchanged. The ratio \( \dfrac{F_1}{F_2} = \dfrac{\alpha}{\sqrt{5}} \). The value of \( \alpha \) is 
