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 \( 1.05 \times 10^4 \, \text{km} \).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)