Impulse-Momentum Theorem. Impulse (\(\vec{J = \int \vec{F dt\)) equals the change in momentum (\(\Delta \vec{p = m\vec{v_f - m\vec{v_i\)). Force is the rate of change of momentum.
Impulse (\(\vec{J}\)) is defined as the integral of force (\(\vec{F}\)) over the time interval (\(\Delta t\)) during which it acts:
$$ \vec{J} = \int_{t_1}^{t_2} \vec{F} dt $$
According to Newton's second law, force is the rate of change of momentum (\(\vec{p}\)): \( \vec{F} = \frac{d\vec{p}}{dt} \).
Substituting this into the impulse integral:
$$ \vec{J} = \int_{t_1}^{t_2} \frac{d\vec{p}}{dt} dt = \int_{p_1}^{p_2} d\vec{p} = \vec{p}_2 - \vec{p}_1 = \Delta \vec{p} $$
This is the Impulse-Momentum Theorem, which states that the impulse applied to an object is equal to the change in its momentum. Option (1) correctly defines impulse as the change in momentum. Option (2) defines force. Option (3) relates to work. Option (4) relates to power or energy transfer rate.