Projectile Motion Problem: Solving for Time and Velocity | Homework Help

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SUMMARY

The discussion focuses on solving a projectile motion problem involving time and velocity using the equations R = 1/2 gt² and R+x = vt. The user derived time (t) as √(2R/g) and velocity (v) as (R+x)/√(2R/g), confirming the correctness of these calculations. Additionally, the conversation highlights the importance of understanding the relationship between centripetal acceleration and the variables involved, emphasizing the need to explore both methods presented by users NihalSh and tiny-tim for a comprehensive understanding.

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david1111
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Homework Statement


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Homework Equations


R = 1/2 gt^2
R+x = vt




The Attempt at a Solution


For a), I tried to find t first, which is equal to √(2R/g). Then, I put t = √(2R/g) into the equation R+x = vt, and I found out that v = (R+x)/√(2R/g), is that correct?

For b), is the answer (R+x)?
 
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hint: for the ball to reach the ground without hitting the rock, the condition is that the y-coordinate of ball should be greater than a certain height.

placing the origin at the center of sphere, ##R^2=x^2+y^2##
##(x,y)## are coordinates on the surface of hemisphere

use kinematic equation to determine the height of ball at each instant and replace ##t## from the equation.

taking ##x## as common coordinate, relate:

height ≥ ##y##

this is sufficient to solve the question. Try it.
P.S. My ##x## is different than the one asked!
 
hi david1111! :smile:
david1111 said:
For a), I tried to find t first, which is equal to √(2R/g). Then, I put t = √(2R/g) into the equation R+x = vt, and I found out that v = (R+x)/√(2R/g), is that correct?

For b), is the answer (R+x)?

yes, that's all correct, but you don't know what x is!

hint: what is the value of the centripetal acceleration? :wink:
 
Centripetal acceleration= v^2 / R? But, how to relate it and x?
 
what is the value of it?

(you can find the value without knowing the speed)
 
Hi david1111,

NihalSh and tiny-tim have offered two quite different methods. T-T's is easier but requires the assumption that if it is going to hit the rock again it will do so immediately. That can be justified by thinking about how the curvature changes in a parabola, but NihalSh's method avoids this. It would be quite instructive to do both.
 

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