In collisions, while some kinetic energy may convert to heat and transfer to individual particles, total linear momentum remains conserved and is solely represented by the momentum of the center of mass. The total kinetic energy of colliding objects is conserved, but it can shift between center-of-mass and internal degrees of freedom. Angular momentum, however, can be divided into orbital and spin components, with total angular momentum conserved despite potential transfers to internal angular momentum. If particles are lost during a collision, they can carry away momentum, but as long as the bulk mass remains intact, its momentum equals the sum of its constituent particles' momenta. Thus, momentum is not lost to internal degrees of freedom in a collision.