
(a)
The change in momentum of m1 during collision along x and y directions.
(a)

Answer to Problem 63P
The change in momentum of m1 during collision along x and y directions are −m1vi and 0.751m1vi respectively.
Explanation of Solution
Using the conservation of linear momentum along x direction,
Δp1,x=m2(v2,x,i−v2,x,f)=m2(v2,x,i−14vicosθ)
Using the conservation of linear momentum along y direction,
Δp1,y=m2(v2,y,i−v2,y,f)=m2(v2,y,i−14visinθ)
Conclusion:
Substitute 0 m/s for v2,x,i, 5m1 for m2, −36.9° for θ to get Δp1,x.
Δp1,x=(5m1)(0−14vicos(−36.9°))=−0.9997m1vi≈−m1vi
Substitute 0 m/s for v2,y,i, 5m1 for m2, −36.9° for θ to get Δp1,y.
Δp1,x=(5m1)(0−14visin(−36.9°))=0.751m1vi
Therefore, change in momentum of m1 during collision along x and y directions are −m1vi and 0.751m1vi respectively.
(b)
The change in momentum of m2 during collision along x and y directions.
(b)

Answer to Problem 63P
The change in momentum of m2 during collision along x and y directions are m1vi and −0.751m1vi respectively.
Explanation of Solution
Using the conservation of linear momentum along x direction,
Δp2,x=m1(v1,x,i−v1,x,f)=m1(vi−v1,x,f)
Using the conservation of linear momentum along y direction,
Δp2,y=m1(v1,y,i−v1,y,f)=m1(v1,y,i−v1)
Conclusion:
Substitute 0 m/s for v1,x,f to get Δp2,x.
Δp2,x=m1(vi−0)=m1vi
Substitute 0 m/s for v1,y,i and 0.751vi for v1 to get Δp2,y.
Δp2,y=m1(0−0.751vi)=−0.751m1vi
Therefore, change in momentum of m2 during collision along x and y directions are m1vi and −0.751m1vi respectively. The momentum changes in (a) and (b) are equal in magnitude and opposite in direction.
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Chapter 7 Solutions
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