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lecture16 - 7.2 Conservation of Linear Momentum We talked...

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7.2 Conservation of Linear Momentum We talked last time how Newton’s Laws naturally show up in our discussions of momentum. It turns out we can write all of Newton’s Laws in terms of momentum: 1. Law of Inertia : A body at rest will remain at rest, and a body in motion will continue in straight line motion unless acted upon by some external force. constant = p v v 2. a m F v v = t p F Δ Δ = v Force equals the rate of change of momentum. 3. Action Equals Reaction: 21 12 F F - = t p t p Δ Δ - = Δ Δ 2 1 2 1 p p Δ - = Δ *Changes in the momentum are of equal magnitude and in opposite directions! What are the consequences of this???
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Such a system will consist of two particles, m 1 and m 2 , interacting with each other. m 1 m 2 Assume for now that the two particles form an isolated system from the rest of the universe, and the only forces they experience are their mutual forces. In other words, there are no external forces. Let the net force on particle 1 by 2 be F . F Then by Newton’s 3 rd Law, we know that the net force on particle 2 is –F . -F By Newton’s 2 nd Law. t p F Δ Δ = 1 t p F Δ Δ = - 2 Now let’s add these two equations together. t p t p F F Δ Δ + Δ Δ = - + 2 1 ) ( 0 = 0 ) ( 2 1 = Δ + Δ t p p , 0 = Δ Δ t P where , the total momentum . 2
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This note was uploaded on 08/04/2009 for the course PHYS 2001 taught by Professor Sprunger during the Fall '08 term at LSU.

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lecture16 - 7.2 Conservation of Linear Momentum We talked...

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