About me
Born |
15 February 1564 |
---|---|
Died |
8 January 1642 (aged 77) |
Residence |
Grand Duchy of Tuscany, Italy |
Nationality |
Italian |
Fields |
Astronomy, physics and mathematics |
Institutions |
University of Pisa |
Patrons |
Cardinal del Monte |
Alma mater |
University of Pisa |
Academic advisors |
Ostilio Ricci[1] |
Notable students |
Benedetto Castelli |
Known for |
Kinematics |
Signature |
A biography by Galileo's pupil Vincenzo Viviani stated that Galileo had dropped balls of the same material, but different masses, from the Leaning Tower of Pisa to demonstrate that their time of descent was independent of their mass.This was contrary to what Aristotle had taught: that heavy objects fall faster than lighter ones, in direct proportion to weight.[128] While this story has been retold in popular accounts, there is no account by Galileo himself of such an experiment, and it is generally accepted by historians that it was at most a thought experiment which did not actually take place.An exception is Drake,argues that the experiment did take place, more or less as Viviani described it. The experiment described was actually performed by Simon Stevin (commonly known as Stevinus),[although the building used was actually the church tower in Delft in 1586.However most of his experiments with falling bodies were carried out using inclined planes where both the issues of timing and wind resistance were much reduced.
In his 1638 Discorsi, Galileo's character Salviati, widely regarded as Galileo's spokesman, held that all unequal weights would fall with the same finite speed in a vacuum. But this had previously been proposed by Lucretius and Simon Stevin.Cristiano Banti's Salviati also held it could be experimentally demonstrated by the comparison of pendulum motions in air with bobs of lead and of cork which had different weight but which were otherwise similar.
Galileo proposed that a falling body would fall with a uniform acceleration, as long as the resistance of the medium through which it was falling remained negligible, or in the limiting case of its falling through a vacuum. He also derived the correct kinematical law for the distance travelled during a uniform acceleration starting from rest—namely, that it is proportional to the square of the elapsed time ( d ∝ t 2 ).Prior to Galileo, Nicole Oresme, in the 14th century, had derived the times-squared law for uniformly accelerated change,[and Domingo de Soto had suggested in the 16th century that bodies falling through a homogeneous medium would be uniformly accelerated. expressed the time-squared law using geometrical constructions and mathematically precise words, adhering to the standards of the day. (It remained for others to re-express the law in algebraic terms).
He also concluded that objects retain their velocity unless a force—often friction—acts upon them, refuting the generally accepted Aristotelian hypothesis that objects "naturally" slow down and stop unless a force acts upon them. Philosophical ideas relating to inertia had been proposed by John Philoponus centuries earlier, as had Jean Buridan, and according to Joseph Needham, Mo Tzu had proposed it centuries before either of them; nevertheless, Galileo was the first to express it mathematically, verify it experimentally, and introduce the idea of frictional force, the key breakthrough in validating the concept. Galileo's Principle of Inertia stated: "A body moving on a level surface will continue in the same direction at constant speed unless disturbed." This principle was incorporated into Newton's laws of motion (first law)