According to Kepler's Law, the time period does not depend upon the mass of the satellite it only depends upon the orbital radius.
1:2
1:16
1:32
1:2√2
To solve this problem, we need to find the ratio of the time periods of two satellites, A and B, orbiting the Earth. This requires us to use Kepler's Third Law, which states that the square of the time period T of a satellite is proportional to the cube of the semi-major axis a of its orbit:
T^2 \propto a^3
For a circular orbit, the semi-major axis a is simply the distance from the center of the Earth to the satellite.
Let's calculate the time period for each satellite:
Now, we need to find the ratio of their time periods:
\left( \frac{T_A}{T_B} \right)^2 = \frac{(R + r)^3}{8r^3}
Taking the square root on both sides, we obtain:
\frac{T_A}{T_B} = \sqrt{\frac{(R + r)^3}{8r^3}}
Under the assumption that the orbit radius for both satellites is large compared to the Earth’s radius, we can simplify this to:
\frac{T_A}{T_B} = \frac{(R + r)^{3/2}}{(2r)^{3/2}} = \frac{1}{2\sqrt{2}}
Thus, the ratio of the periods T_A\) to T_B\) is:
1:2\sqrt{2}
The correct answer is 1:2√2.
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.)