How 3rd law of motion exceeded to law of conservation of momentum
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Derivation of Conservation of Momentum
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.A=m1(v1−u1) (change in momentum of particle A)
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.A=m1(v1−u1) (change in momentum of particle A)B=m2(v2−u2) (change in momentum of particle B)
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.A=m1(v1−u1) (change in momentum of particle A)B=m2(v2−u2) (change in momentum of particle B)FBA=−FAB (from third law of motion)
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.A=m1(v1−u1) (change in momentum of particle A)B=m2(v2−u2) (change in momentum of particle B)FBA=−FAB (from third law of motion)FBA=m2∗a2=m2(v2−u2)t
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.A=m1(v1−u1) (change in momentum of particle A)B=m2(v2−u2) (change in momentum of particle B)FBA=−FAB (from third law of motion)FBA=m2∗a2=m2(v2−u2)tFAB=m1∗a1=m1(v1−u1)t
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.A=m1(v1−u1) (change in momentum of particle A)B=m2(v2−u2) (change in momentum of particle B)FBA=−FAB (from third law of motion)FBA=m2∗a2=m2(v2−u2)tFAB=m1∗a1=m1(v1−u1)tm2(v2−u2)t=−m1(v1−u1)t
Derivation of Conservation of MomentumNewton’s third law states that for a force applied by an object A on object B, object B exerts back an equal force in magnitude, but opposite in direction. This idea was used by Newton to derive the law of conservation of momentum.Consider two colliding particles A and B whose masses are m1 and m2 with initial and final velocities as u1 and v1 of A and u2 and v2 of B. The time of contact between two particles is given as t.A=m1(v1−u1) (change in momentum of particle A)B=m2(v2−u2) (change in momentum of particle B)FBA=−FAB (from third law of motion)FBA=m2∗a2=m2(v2−u2)tFAB=m1∗a1=m1(v1−u1)tm2(v2−u2)t=−m1(v1−u1)tm1u1+m2u2=m1v1+
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