Prove that an object, if thrown up under gravity

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An object thrown upward under gravitational force will take equal time to reach its apex and to return to its original position, assuming constant acceleration and ignoring air resistance. The vertical component of the initial velocity decreases due to gravity until it reaches zero at the highest point. The time to rise can be calculated as T1 = (initial vertical velocity) / g, and the time to fall back is T2, which is equal to T1. This symmetry arises because the equations of motion are invariant under time reversal, confirming that T1 equals T2. Thus, the time taken to ascend and descend is the same.
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Can you show me how to prove that an object, if thrown up under gravitational force, will take the same time to reach the apex of it's trajectory as it takes to fall back to it's original position? (ignore air resistance)
 
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You are then assuming constant acceleration. You should be able to write down the standard formula for the height of the object at any time t, for any initial speed v0. Find the time until it reaches its highest point and the time until it comes back to the original height. Observe that the first time is exactly half the second time.
 
mahela007 said:
Can you show me how to prove that an object, if thrown up under gravitational force, will take the same time to reach the apex of it's trajectory as it takes to fall back to it's original position? (ignore air resistance)

well its easy
For parabolic path
because the time to rise and fall is affected by gravity (and gravity affects upon vertical velocity)
Break the velocity u into ucosx and usinx (x is angle)
here is vertical velocity is usinx
since it is affected by gravity its value decreses in maximum height that is V=o
and a = -g
that is thime to rise T1= o-usinx/ -g = usinx/g
and similarly after reaching the highest point than the gravity favours downward velocity and now velocity goes to increase and becomes maximum at the hitting the ground
At u=o and v= usinx
a=g
T2 = usinx-o/g
=usinx/g T1=T2
hence proved
 
If we consider forces F(x) that depend only on position x, then Newton's law takes the form:

x'' = F(x)

This equation is invariant under time reversal t -> -t since by the chain rule on the LHS we have minus time minus is plus, and the RHS is manifestly invariant. Therefore under these conditions the laws of mechanics are invariant under time reversal, from which the proposition stated by the OP follows as a corollary.
 
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