Domingo de Soto, early dynamics theorist

concept. Be that as it may, the example remained in the literature for scholars of that time to consider (eight editions of de Soto’s Quaestiones super octo libros physicorum Aristotelis were published between 1551 and 1613), and it is likely to have been known to Galileo, who mentions de Soto in his Tractatus de Elementis and who attended classes by some of de Soto’s intellectual descendants2 at the Roman College (now the Pontifical Gregorian University) in Rome. Furthermore, it was accompanied by an explicit indication that because of the uniformly accelerated nature of its motion, the distance traveled by a freely falling body can be calculated using the mean velocity theorem that had been stated and proved in the 14th century by the Oxford Calculators: for in seeking an appropriate global measure of the velocity of a uniformly accelerating object such as a falling heavy body, de Soto notes that “if the moving object A keeps increasing its velocity from 0 to 8, it covers just as much space as [another object] B moving with a uniform velocity of 4 in the same period of time.”1 He was thus the first to apply mathematics successfully to this physical problem— without experimental verification, but in a way that, because it was mathematically precise and physical, constituted an exceptionally clear invitation to experimental verification for such inquisitive minds as were prepared to recognize it. If de Soto’s writings did influence Galileo, as seems quite probable, they may have influenced his thinking on dynamics as well as on kinematics. According to Juan José Pérez Camacho and Ignacio Sols Lucía, de Soto’s concept of the resistentia interna of a body foreshadows Galileo’s resistenza interna in being intrinsic to the body itself rather than to its medium, and proportional to the weight of the body.3 What is less tenable is Pérez Camacho and Sols Lucía’s thesis that de Soto considered the velocity v of a moving body to be proportional to the motive force f and inversely proportional to its resistentia interna r—which would be correct in the case of a body accelerated from rest by a constant force, with time as the constant of proportionality and inertial mass as resistentia interna. On the contrary, it seems clear that de Soto’s understanding of the relationship among these quantities corresponded not to the formula v f/r but rather to the formula v log(f/r), first proposed by Bradwardine.4 The road from Aristotle to Galileo was long and tortuous, and those who advanced in one dimension often remained stationary or receded in others; de Soto’s contribution, though modest, may have been vital.