Provided Data:
- Satellite orbital period around planet: \( T_1 = 6 \, \text{hours} \)
- Geostationary satellite orbital period around Earth: \( T_2 = 24 \, \text{hours} \)
- Radius of geostationary orbit around Earth: \( r_2 = 4.2 \times 10^4 \, \text{km} \)
- Mass of the planet: \( M_1 = \frac{M}{4} \) (where \( M \) is Earth's mass)
Step 1: Applying the Time Period Formula for Circular Orbits
The time period \( T \) of a satellite in orbit is calculated using:
\[ T = 2\pi \sqrt{\frac{r^3}{GM}}. \]
The ratio of the time periods for the satellite and Earth's geostationary satellite is:
\[ \frac{T_1}{T_2} = \left( \frac{r_1}{r_2} \right)^{3/2} \left( \frac{M_2}{M_1} \right)^{1/2}, \]
where:
- \( r_1 \) and \( r_2 \) represent the respective orbital radii,
- \( M_1 \) and \( M_2 \) represent the masses of the respective planets.
Step 2: Inserting Given Values
With the given values substituted:
\[ \frac{6}{24} = \left( \frac{r_1}{4.2 \times 10^4} \right)^{3/2} \left( \frac{M}{M/4} \right)^{1/2}. \]
Simplified expression:
\[ \frac{1}{4} = \left( \frac{r_1}{4.2 \times 10^4} \right)^{3/2} \times 2. \]
Dividing both sides by 2 yields:
\[ \frac{1}{8} = \left( \frac{r_1}{4.2 \times 10^4} \right)^{3/2}. \]
Taking the cube root:
\[ \left( \frac{r_1}{4.2 \times 10^4} \right) = \left( \frac{1}{8} \right)^{2/3} \approx 0.25. \]
Consequently:
\[ r_1 \approx 0.25 \times 4.2 \times 10^4 = 1.05 \times 10^4 \, \text{km}. \]
The calculated orbital radius for the planet is \( 1.05 \times 10^4 \, \text{km} \).
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 
