Given:
- Time period of the satellite around the planet: \( T_1 = 6 \, \text{hours} \)
- Time period of a geo-stationary satellite around Earth: \( T_2 = 24 \, \text{hours} \)
- Radius of geo-stationary orbit around Earth: \( r_2 = 4.2 \times 10^4 \, \text{km} \)
- Mass of the planet: \( M_1 = \frac{M}{4} \) (where \( M \) is the mass of the Earth)
Step 1: Using the Time Period Relation for Circular Orbits
The formula for the time period of a satellite in orbit is given by:
\[ T = 2\pi \sqrt{\frac{r^3}{GM}}. \]
Taking the ratio of the time periods for the satellite and Earth's geo-stationary satellite:
\[ \frac{T_1}{T_2} = \left( \frac{r_1}{r_2} \right)^{3/2} \left( \frac{M_2}{M_1} \right)^{1/2}, \]
where:
- \( r_1 \) and \( r_2 \) are the radii of the orbits,
- \( M_1 \) and \( M_2 \) are the masses of the respective planets.
Step 2: Substituting the Given Values
Substituting the given values:
\[ \frac{6}{24} = \left( \frac{r_1}{4.2 \times 10^4} \right)^{3/2} \left( \frac{M}{M/4} \right)^{1/2}. \]
Simplifying:
\[ \frac{1}{4} = \left( \frac{r_1}{4.2 \times 10^4} \right)^{3/2} \times 2. \]
Dividing both sides by 2:
\[ \frac{1}{8} = \left( \frac{r_1}{4.2 \times 10^4} \right)^{3/2}. \]
Taking the cube root:
\[ \left( \frac{r_1}{4.2 \times 10^4} \right) = \left( \frac{1}{8} \right)^{2/3} \approx 0.25. \]
Thus:
\[ r_1 \approx 0.25 \times 4.2 \times 10^4 = 1.05 \times 10^4 \, \text{km}. \]
Therefore, the radius of the orbit of 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 

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(Given: $g = 10\,\text{m s}^{-2}$) 
Method used for separation of mixture of products (B and C) obtained in the following reaction is: 