Law of Conservation of Linear Momentum:
According to Newton’s second law of motion the force acting on an isolated force is equal to rate of change of momentum i.e.,
\(\vec F = \frac{d\vec p}{dt}\)
If external force is absent i.e. \(\vec F\) = 0
\(\frac{d \vec p}{dt} = 0\)
or \(\vec p\) = constant (Because differentiation of constant with respect to any quantity is zero)
or p = mu = constant
or m1u1 = m2u2
i.e., in absence of external force the linear momentum of particle remains unchanged.
Proof of Newton’s Third Law by Newton’s Second Law:
Suppose there are two bodies A and B in an isolated system. When they collide, then at the time of collision, body A applies force \(\vec F_{21}\) on body Band body B applies force \(\vec F_{21}\) on body A These forces \(\vec F_{21}\) and \(\vec F _{12}\) are said action and reaction respectively. The time of contact of both particles is ∆t.
∵ Change in linear momentum = Force × time interval
∴ Change in momentum of particle A
\(\overrightarrow{\Delta p_1} = \overrightarrow{F_{12}}\times\Delta t\)
and that of particle B,
\(\overrightarrow{\Delta p_2} = \overrightarrow{F_{21}}\times\Delta t\)
∴ Total change in momentum of the system = \(\overrightarrow{\Delta p_1} + \overrightarrow{\Delta p_2}.\) If no external force is acting on the system, then according to law of conservation of momentum,

This is Newton's third law of motion.