Respuesta :
The Question is not complete and this is the complete question;
Part A
Find the relative speed u between Chuck and the ball after Chuck has thrown the ball.
Express the speed in terms ofv_c and v_b.
Part B
What is the speed v_b of the ball (relative to the ground) while it is in theair?
Express your answer in terms of m_ball, Image for Chuck and Jackie stand on separate carts, both of which can slide without friction. The combined mass of Chuck, and u.
Part C
What is Chuck's speed v_c (relative to the ground) after he throws theball?
Express your answer in terms ofm_ball, Image for Chuck and Jackie stand on separate carts, both of which canslide without friction. The combined mass of Chuck, and u.
Part D
Find Jackie's speed v_j (relative to the ground) after she catches the ball, in terms of v_b.
Express v_j in terms of m_ball, Image for Chuck and Jackie stand on separate carts, both of which canslide without friction. The combined mass of Chuck, and v_b.
Part E
Find Jackie's speed v_j (relative to the ground) after she catches theball, in terms of u.
Express v_j in terms of m_ball, Image for Chuck and Jackie stand on separate carts, both of which canslide without friction. The combined mass of Chuck, and u.
Answer:
A) u = Vc + Vb
B) Vb = m(cart)u/ [(mball) + m(cart)]
C) Vc = um(ball)/[(mball) + m(cart)]
D) Vj = m(ball)Vb/ [(mball) + m(cart)]
E) Vj = (m(ball) x um(cart)) / [(mball) + m(cart)]²
Explanation:
A) We want to find the relative speed between chuck and the ball after he has thrown the ball.
Now, chuck and the ball are opposite to each other , therefore the relative speed between them is equal to the sum of their speeds, so; u = chucks speed + ball's speed
u = Vc + Vb
B) From conservation of momentum, we know that;
Initial momentum = Final momentum.
Since balls are at rest, initial momentum(P1) is zero
Now, final momentum (P2) is;
P2 = - m(cart)Vc + m(ball)Vb
Now since P1 = P2 and P1 =0.thus,
- m(cart)Vc + m(ball)Vb = 0
Add - m(cart)Vc to both sides to obtain;
m(ball)Vb = m(cart)Vc
Vb = (m(cart)Vc) / m(ball)
From answer a above, Vc = u - Vb
So, Vb = [m(cart)(u - Vb] / m(ball)
Multiply both sides by m(ball) to get;
Vb(mball) = m(cart)u - m(cart)Vb
Add m(cart)Vb to both sides to get;
Vb(mball) + m(cart)Vb = m(cart)u
Vb[(mball) + m(cart)] = m(cart)u
So, Vb = m(cart)u/ [(mball) + m(cart)]
C) From above; Vc = u - Vb
So, Vc = u - m(cart)u/ [(mball) + m(cart)]
Vc = [u((mball) + m(cart))] - m(cart)u] / [(mball) + m(cart)]
So, Vc = um(ball)/[(mball) + m(cart)]
D) In this case initial momentum = m(ball)Vb while final momentum is [(mball) + m(cart)]Vj
Thus as stated in b above, in conservation of momentum,
Initial momentum = final momentum.
Hence ;
m(ball)Vb = [(mball) + m(cart)]Vj
So; Vj = m(ball)Vb/ [(mball) + m(cart)]
E) From earlier, we saw that;
Vb = m(cart)u/ [(mball) + m(cart)]
So putting that for Vb in D above to get;
Vj = [m(ball)/ [(mball) + m(cart)]] x [m(cart)u/ [(mball) + m(cart)]
= (m(ball) x um(cart)) / [(mball) + m(cart)]²