To determine the escape velocity for a sphere on Earth, we need to understand the concept of escape velocity itself. It refers to the minimum speed required for an object to break free from the gravitational attraction of a celestial body, such as the Earth, without any additional propulsion.
The formula for escape velocity $v_e$ can be derived from the energy conservation principle. The kinetic energy (KE) of the object needs to equal the gravitational potential energy (PE) at the surface of the planet. Therefore, we equate the kinetic energy to gravitational potential energy:
\[\frac{1}{2}mv_e^2 = \frac{G M_e m}{R_e}\]
Where:
We can simplify this formula by canceling $m$ from both sides:
\[\frac{1}{2}v_e^2 = \frac{G M_e}{R_e}\]
By multiplying both sides by 2 to solve for $v_e^2$, we get:
\[v_e^2 = \frac{2 G M_e}{R_e}\]
Taking the square root of both sides gives us the escape velocity:
\[v_e = \sqrt{\frac{2 G M_e}{R_e}}\]
Therefore, the escape velocity of the sphere is represented by the expression \[\sqrt{\frac{2 G M_e}{R_e}}\].
Comparing this result with the given options, the correct answer is:
\(\sqrt{\frac{2GM_e}{R_e}}\)
This calculation assumes that the effect of air resistance is negligible and that the escape is happening close to the surface of the Earth.
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.)