In thermodynamics, motive power, or "puissance motive", in French, refers to the work associated with lifting a weight through a height, done cyclically; hence "work per unit time" or "force moving an object per unit distance per unit time"; or moving power.
Overview
In 1690, Denis Papin, in his “A New Method to Obtain Very Great Motive Powers at Small Cost”, in reference to his new theoretical heat engine (see: Papin engine), was employing the term "motive power" in reference to the ability of fire to raise weight, cyclically. [1]
In 1824, Sadi Carnot, in his On the Motive Power of Fire, employed the term as follows: [2]
“We use here the expression ‘motive power’ to express the useful effect that a motor is capable of producing. This effect can always be likened to the elevation of a weight to a certain height. It has, as we know, a measure, the product of the weight multiplied by the height to which it is raised.”
“Heat is nothing but motive power, or rather motion, which has changed form. It is motion of the particles of bodies. Whenever motive power is destroyed, there is a simultaneous production of an amount of heat exactly proportional to the motive power that is destroyed. Conversely, whenever there is destruction of heat, motive power is produced. Hence, we may state, as a general proposition, that the quantity of motive power in nature is fixed, and that, strictly speaking, motive power is neither produced nor destroyed. It is true that it changes its form, that is, it sometimes produces one kind of motion, sometimes another. But it is never annihilated.”— Sadi Carnot (c.1827), manuscript III (F° 7 recto); posthumously deposited to the French Academy of Sciences by M.H. Carnot in 1878; Robert Fox (1986) translation [3]