[Note 48\3: I have, in the History, applied to Descartes the character which Bacon gives to Aristotle, 'Audax simul et pavidus:' though he was bold enough to enunciate the laws of motion without knowing them aright, he had not the courage to leave the planets to describe their orbits by the agency of those laws, without the machinery of contact.] {282} 4. When at last mathematicians, following Newton, had ventured to consider the motion of each planet as a mechanical problem not different in its nature from the motion of a stone cast from the hand; and when the solution of this problem and its immense consequences had become matters of general notoriety and interest; the new views introduced, as is usual, new terms, which soon became extensively current. We meet with such phrases as 'flying off in the tangent,' and 'deflexion from the tangent;' with antitheses between 'centripetal' and 'centrifugal force,' or between 'projectile' and 'central force.' 'Centers of force,' 'disturbing forces,' 'perturbations,' and 'perturbations of higher orders,' are not unfrequently spoken of: and the expression 'to gravitate,' and the term 'universal gravitation,' acquired a permanent place in the language. Yet for a long time, and even up to the present day, we find many indications that false and confused apprehensions on such subjects are by no means extirpated. Arguments are urged against the mechanical system of the universe, implying in the opponents an absence of all clear mechanical notions. Many of this class of writers retrograde to Kepler's point of view. This is, for example, the case with Lord Monboddo, who, arguing on the assumption that force is requisite to maintain, as well as to deflect motion, produced a series of attacks upon the Newtonian philosophy; which he inserted in his _Ancient Metaphysics_, published in 1779 and the succeeding years. This writer (like Kepler), measures force by the velocity which the body _has_[49\3], not by that which it _gains_. Such a use of language would prevent our obtaining any laws of motion at all. Accordingly, the author, in the very next page to that which I have just quoted, abandons this measure of force, and, in curvilinear motion, measures {283} force by 'the fall from the extremity of the arc.' Again; in his objections to the received theory, he denies that curvilinear motion is compounded, although his own mode of considering such motion assumes this composition in the only way in which it was ever intended by mathematicians. Many more instances might be adduced to show that a want of cultivation of the mechanical ideas rendered this philosopher incapable of judging of a mechanical system. [Note 49\3: _Anc. Met._ vol. ii. b. v. c. vi. p. 413.]