Collisions – Impulse and Momentum - 3 types of collisions physics

3 In the cases where ∆𝑡 is a really small interval, then ∆𝑡→𝑑𝑡 and the Impulse‐Momentum Theorem becomes; 𝐼 ±𝐹𝑑𝑡 For the above integral the force must be a function of time. For the trivial case where the force is constant, the solution to the integral is 𝐼 ................
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