a ball is thrown straight up from the ground with speed v0 . at the same instant, a second ball is dropped from rest from a height h , directly above the point where the first ball was thrown upward. there is no air resistance.
They collide at time t=hv0t=\dfrac{h}{v_0}t=v0h, at a height 12(h+v02g)\dfrac{1}{2}\left(h+\dfrac{v_0^2}{g}\right)21(h+gv02) above the ground, provided the collision happens while both are in flight.
Set up the motion
Take upward as positive and the ground as y=0y=0y=0.
- Ball 1 (thrown up from ground):
Initial position y1(0)=0y_{1}(0)=0y1(0)=0, initial velocity v0v_0v0.
Its position is
y1(t)=v0t−12gt2.y_1(t)=v_0t-\tfrac{1}{2}gt^2.y1(t)=v0t−21gt2.
- Ball 2 (dropped from height hhh):
Initial position y2(0)=hy_{2}(0)=hy2(0)=h, initial velocity 000.
Its position is
y2(t)=h−12gt2.y_2(t)=h-\tfrac{1}{2}gt^2.y2(t)=h−21gt2.
Time of collision
At collision, they are at the same height, so y1(t)=y2(t)y_1(t)=y_2(t)y1(t)=y2(t).
v0t−12gt2=h−12gt2v_0t-\tfrac{1}{2}gt^2=h-\tfrac{1}{2}gt^2v0t−21gt2=h−21gt2
The −12gt2-\tfrac{1}{2}gt^2−21gt2 terms cancel, leaving:
v0t=h⇒t=hv0.v_0t=h\quad \Rightarrow \quad t=\frac{h}{v_0}.v0t=h⇒t=v0h.
So the collision time is
tcollision=hv0.t_{\text{collision}}=\frac{h}{v_0}.tcollision=v0h.
Height of collision
Substitute t=hv0t=\dfrac{h}{v_0}t=v0h into either position equation, say y2(t)y_2(t)y2(t):
ycollision=h−12g(hv0)2=h−gh22v02.y_{\text{collision}} =h-\tfrac{1}{2}g\left(\frac{h}{v_0}\right)^2 =h-\frac{gh^2}{2v_0^2}.ycollision=h−21g(v0h)2=h−2v02gh2.
Or into y1(t)y_1(t)y1(t):
ycollision=v0(hv0)−12g(hv0)2=h−gh22v02,y_{\text{collision}} =v_0\left(\frac{h}{v_0}\right)-\tfrac{1}{2}g\left(\frac{h}{v_0}\right)^2 =h-\frac{gh^2}{2v_0^2},ycollision=v0(v0h)−21g(v0h)2=h−2v02gh2,
which matches, as it must.
This can be rewritten in a symmetric form if one relates hhh and v0v_0v0 for particular problems, but the key results for this setup are:
- Time when they collide: t=hv0t=\dfrac{h}{v_0}t=v0h.
- Height where they collide: y=h−gh22v02y=h-\dfrac{gh^2}{2v_0^2}y=h−2v02gh2.
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