Case I Consider two particles of a system having masses m1 and m2 are moving with velocities v1 and v2, respectively. Then, total linear momentum of the system p=m1v1+m2v2=p1+p2
If F is the external force acting on the system, then according to Newton's second law of motion, F=dtdp
For an isolated system, F=0⇒dtdp=0 ⇒p= constant i.e. p1+p2= constant
Case II Consider two particles of masses m1 and m2 moving along a straight line in opposite direction collide to each other, if Δp1 and Δp2 be the changes in momenta produced in time Δt, then according to the law of conservation of momentum, if no external force (for isolated system) is applied on the system ⇒Δp1+Δp2=0 ⇒Δp2=−Δp1 ⇒ΔtΔp2=−ΔtΔp1 ⇒ Force on m2=− Force on m1 [∵F=dtdp] F2=−F1
So, in an isolated system, when total momentum of interacting particles is conserved, it follow both, Newton's second and third laws.
Hence, options (b) and (c) are correct.