A stone is released from an elevator going up with an acceleration a. The acceleration of the stone after the release is?
Answer to this question is only g. But why does a does not influence the stone.
A stone is released from an elevator going up with an acceleration a. The acceleration of the stone after the release is?
Answer to this question is only g. But why does a does not influence the stone.
It's simply Newton's second law. What are the forces acting on the stone after its release? Well, it's completely out of contact with the elevator, so there's only the force of gravity, meaning that $m\mathbf{a}_\text{stone} =\mathbf{F} = m\mathbf{g}$, i.e. $\mathbf{a}_\text{stone} = \mathbf{g}$.
Of course, I'm assuming that we're talking about the acceleration of the stone in the reference frame of the earth. The relative acceleration between the stone and the elevator would be $\mathbf{a}_{\text{stone/elevator}}=\mathbf{g}-\mathbf{a}$.
The elevator is accelerating because there is some force acting on it (presumably the cable). While you are holding onto the stone, that force is transmitted through to the stone via the floor, your body and your arm, so the stone accelerates also at the same rate as the elevator.
As soon as you let go of the stone, the force from the cable no longer acts on the stone. The lift carries on accelerating (presumably slightly more now, since the cables don't have to accelerate the stone as well), but the stone is free to fall under gravity only.
Hence, in the reference frame of the outside world, the stone only falls under gravity ($g$).
In the reference frame of the elevator cabin, the magnitude of the acceleration will indeed be $a + g$.