Horizontal Range and Maximum Height of a Projectile

AI Thread Summary
The discussion focuses on solving a projectile motion problem involving a ball thrown vertically upward. The key point is to demonstrate that the total time for the ball to return to the ground is twice the time it takes to reach its maximum height. To find this, participants suggest using kinematic equations, specifically V = Vo + at and d = Vo*t + ½at². The velocity at maximum height is zero, which helps in calculating the time to reach that height. By applying similar calculations for the descent, the total flight time can be determined.
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Homework Statement


A ball is thrown vertically up from y=0 at time t=0 with vinitial=v0j. Show that the time it takes for the ball to reach the ground is twice the time it takes to reach its maximum height.


Homework Equations


h=(vi2sinthetai)/2g
R=(vi2sin2thetai)/g


The Attempt at a Solution


I have no idea where to start solving this problem.
 
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It is a purely vertical motion problem, so you can use just
V = Vo + at and d = Vo*t+½at²
Looks like you will have to get an expression for the time to maximum height and the time of the full flight back to ground.
It will be most helpful if you can see what the velocity is at maximum height and just before it hits the ground.
 
I think I just have trouble figuring out what I need to solve for and what values to substitute where.
 
What is the velocity at the point of maximum height?
Substitute that into V = Vo + at and you will have the time of maximum height.

Do a very similar thing for the point where it hits the ground, and you'll have the full time of flight.
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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