Impulse equals Change in Momentum

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Theorem

Let a force $\mathbf F$ be applied to a particle $P$.

Then the impulse $\mathbf J$ imparted to $P$ is equal to the change of momentum of $P$.


Proof

\(\ds \mathbf F\) \(=\) \(\ds \dfrac {\d \mathbf p} {\d t}\) Newton's Second Law of Motion: $\mathbf p$ is the (linear) momentum of $P$
\(\ds \leadsto \ \ \) \(\ds \int_{t_1}^{t_2} \mathbf F \rd t\) \(=\) \(\ds \int_{t_1}^{t_2} \dfrac {\d \mathbf p} {\d t}\) integrating $\mathbf F$ with respect to time between limits $t_1$ to $t_2$
\(\ds \leadsto \ \ \) \(\ds \mathbf J\) \(=\) \(\ds \bigintlimits {\mathbf p} {t \mathop = t_1} {t \mathop = t_2}\) Definition of Impulse, and Fundamental Theorem of Calculus
\(\ds \) \(=\) \(\ds \mathbf p_{t_2} - \mathbf p_{t_1}\)

Hence the impulse $\mathbf J$ equals the change of (linear) momentum between $t_1$ and $t_2$, as required.

$\blacksquare$


Sources