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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.
It is much more probable that heat is really the kinetic energy of motion of the molecules, and is passed on from one to another by collisions.
If we assume that there is no loss of apparent kinetic energy we have also miuii +miuf2 = miui2 +mfuzi.