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594 MEDIEVAL ENGLAND<br />

place to another as a process requiring the continuous action of<br />

a motive agent, a<br />

conception precisely opposite to the seven^<br />

teenth/century conception of inertia. So long as the external<br />

motive agent continued to operate, the Aristotelian theory held<br />

that velocity would be directly proportional to the motive<br />

power and inversely proportional to the resistance of the<br />

medium; remove the external agent, and the motion would<br />

stop. Many everyday phenomena supported these judgements,<br />

5<br />

but three did not. First, according to this Aristotelian law ,<br />

there should be a finite<br />

velocity with any finite values ofpower and resistance, yet in fact ifthe power is smaller than the resis^<br />

tance it may fail to move the body at all. To escape this diffi'<br />

culty, Bradwardine used a modification ofthe 'law* according<br />

to which velocity was proportional to the excess of power over<br />

resistance, and he tried to<br />

express by means of an algebraic<br />

function how change in<br />

velocity was related, as a dependent<br />

variable, to the<br />

independent variables, power and resistance.<br />

Bradwardine's use of mathematical functions seems to have<br />

inspired the attempt made by the French physicist, Jean<br />

Buridan, to deal with the other two phenomena that provided<br />

difficulties for Aristotle's conception ofmotion, the motion of<br />

a projectile after leaving the projector, and the acceleration ofa<br />

freely falling body. What was the motive power that kept the<br />

projectile going? This question had worried physicists since<br />

Aristotle himself. Buridan introduced a quantitative notion<br />

of impetus, analogous to Newton's momentum, imparted by the<br />

projector; this impetus maintained the projectile's velocity and<br />

enabled it to impart velocity to other bodies with which it col'<br />

lided. The acceleration of freely falling bodies Buridan attri'<br />

buted to successive increments of impetus added by gravity.<br />

Work relevant to both problems was taken up again in Ox'<br />

ford. William of in<br />

^Ockham, accordance with his general<br />

principles of inquiry, reduced motion to the fact that from inx<br />

stant to instant a is body observed to change its<br />

spatial relations<br />

with other bodies. He rejected Buridan's impetus as an unx<br />

necessary complication. Science, he declared in effect, should,<br />

in the interests of economy, confine itself to the description of

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