Conservation of momentum in the x-direction:
mBv + 0 = mAvAx + 0
mAvAx = mBv Eqn 1
In the y-direction:
0 + 0 = mAvAy - mB(v/5)
mAvAy = mBv/5 Eqn 2
Divide Eqn 2 by Eqn 1, and you'll get:
vAy/vAx = 1/5 = 0.2
The angle of the final velocity vector is found from tan θ = vy/vx
θ = tan-10.2 = 11.3 degrees
Momentum is conserved during collisions. It is also a vector. I'll be using the notation (x, y) for vectors.
Ball B has mass = m1 and initial momentum PB
Ball A has mass = m2 and initial momentum PA
First calculate the total initial momentum:
1) Pinitial = PB + PA
PB = (m1*v, 0)
PA = (0, 0)
So:
2) Pinitial = (m1*v, 0)Now calculate the final momentum, Pfinal. We know the initial momentum and the final momentum of Ball B.
Ball B now has final momentum PBF.
Ball A has final momentum PAF.
Knowing that Pfinal = Pinitial, eqn. 1) can be rearranged to solve for the final momentum of Ball A:
3) PAF = Pinitial - PBF
4) PBF = (0, m1*-(1/5)v) as given in the problem
Now combine eqns. 2), 3), and 4) to solve for the momentum vector for Ball A, PAF.
Recall that vectors add like so: (a, b) + (c, d) = (a+c, b+d)
There is going to be an x and y component to this vector. Using Newton's Third Law you may be able to write this vector without any vector operations, but if not, you may use the above equations to determine it.Now to calculate the angle between Ball A's momentum vector, PAF, and the x-axis.
You have calculated a vector for PAF in the form (x1, y1) (these may be positive or negative values). It may help to draw out the vectors on a 2-d graph. Draw the x1 component along the x-axis, then starting the at the tip of this x1 vector component, draw the y1 component. These will be the sides of the triangle used to calculate the angle to the x-axis in the equation below.
Using this equation:
So:
θ = tan-1(y1/x1)
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