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Like the actual Leibniz, they allow absolute quantities of motion, but claim that space and time themselves are nothing but the relations between bodies.
And if relative distances and times exhaust the spatiotemporal in this way, then shouldn't all quantities of motion be defined in terms of those relations?
It is of course arguable whether any of these three proposals are successful; (even) stripped of Leibniz's Aristotelian packaging, can absolute quantities of motion 'stand on their own feet'?
According to this view, the only quantities of motion are relative quantities, relative velocity, acceleration and so on, and all relative motions are equal, so there is no true sense of motion.
A theory that satisfies all the goals of Mach-heavy would appear to be ideal for the vindication of strict relationism and the elimination of absolute quantities of motion from mechanics.
At very least, there are quantities of motion implicit in Leibniz's mechanics — change in force and true speed — that are not merely relative; the folk reading is committed to Leibniz simply missing this obvious fact.
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Its quantity of motion = 1 m/s × 4lbs = 4 units.
First, he argues that Descartes's quantity of motion is not an adequate measure of force.
It is merely a quantity of motion calculable in another substance.
Descartes conserves the joint quantity of motion by equipping the stationary object C with a resisting force sufficient to deflect the moving body B, a solution that does uphold the quantity of motion in cases where C is at rest.
In his Principles of Philosophy, Descartes had argued that the quantity of motion in the world remains constant, where the quantity of motion of a body is determined by its speed times its size.
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