First slide
Gravitaional potential energy
Question

When a projectile attains the escape velocity, then on surface of planet its

Moderate
Solution

If u = Ve

We can Write

\large u=\sqrt{\frac{2GM}{R}}
\large \Rightarrow \frac{1}{2}mu^2=\frac{1}{2}m.X\frac{2GM}{R}\\\\ \Rightarrow \frac{1}{2}mu^2+(-\frac{GMm}{R})=0\\\\ \Rightarrow KE+PE=0\\\\ \Rightarrow |K.E|=|P.E|

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