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Available kinetic energy is possessed by a system of two or more bodies in virtue of the relative motion of its parts.
There is probably but little transformation of one form of kinetic energy into another in the plant.
The latter may be called the internal kinetic energy of the system.
If we assume that there is no loss of apparent kinetic energy we have also miuii +miuf2 = miui2 +mfuzi.
The increase of the kinetic energy of a rigid body in any interval of time is equal to the work done by the extraneous forces acting on the body.