4
\(\frac{1}{2}\)
\(\frac{1}{\sqrt 2}\)
\(\frac{1}{4}\)
To solve this problem, we need to understand the relationship between the kinetic energy and potential energy of a satellite orbiting the Earth. A satellite in orbit around the Earth is under the influence of gravitational force, and its motion can be analyzed using classical mechanics.
When a satellite orbits the Earth, its total energy is the sum of its kinetic energy (\(K\)) and potential energy (\(U\)). In circular orbits, it is known from physics that:
\(K = \frac{1}{2}mv^2\) and \(U = -\frac{GMm}{r}\)
where:
For a satellite in a stable orbit, the relationship between the kinetic energy and potential energy is given by the virial theorem, which tells us:
\(K = -\frac{1}{2}U\)
This equation implies that the kinetic energy of the satellite is half the magnitude of its potential energy. Therefore, the ratio of kinetic energy to potential energy (\(K:U\)) is:
\(\frac{K}{U} = \frac{(-\frac{1}{2}U)}{U} = \frac{1}{2}\)
Thus, the correct answer is that the ratio of kinetic energy to potential energy for a satellite moving in an orbit around the Earth is \(\frac{1}{2}\).
Therefore, the correct option is:
\(\frac{1}{2}\)
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.)