
Arturo O. answered 12/05/16
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(a)
You are correct.
vx = (4.33 x 105 m/s) cos(65°) ≅ 1.83 x 105 m/s
vy = (4.33 x 105 m/s) sin(65°) ≅ 3.92 x 105 m/s
(b)
Note the speeds are low enough to ignore relativistic effects. Apply conservation of linear momentum.
v1 = initial neutron speed (assumed to be along x)
vx = final neutron speed along x
vy = final neutron speed along y
wx = final alpha particle speed along x
wy = final alpha particle speed along y
Conservation along x-direction:
uv1 = uvx + (4u)wx ⇒ wx = (v1 - vx)/4 = (5 - 1.83)/4 x 105 m/s ≅ 0.793 x 105 m/s
Conservation along y-direction:
0 = uvy + (4u)wy ⇒ wy = -vy/4 = -(3.92 x 105 m/s) / 4 ≅ -9.80 x 104 m/s
0 = uvy + (4u)wy ⇒ wy = -vy/4 = -(3.92 x 105 m/s) / 4 ≅ -9.80 x 104 m/s
w = √(wx2 + wy2) =√[(0.793 x 105)2 + (-9.80 x 104)2] = 1.26 x 105 m/s
θ = tan-1(wy/wx) = tan-1(-9.8 x 104 / 0.793 x 105) = (360 - 51.0)° = 309°
I got the same speed as you for the alpha particle, but a different direction. Note the alpha particle moves in the +x and -y directions, which puts its velocity vector direction between 270° and 360°, so I think you put the angle in the wrong quadrant. Check my math and let me know what you think.

Arturo O.
You are welcome. That was a fun problem to work.
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12/06/16
Ian G.
12/06/16