160 likes | 170 Views
Discover the genius of Isaac Newton's three laws of motion and law of universal gravitation, which explain the fundamental principles behind how objects move and interact. Learn how Newton's laws revolutionized physics and led to important advancements in calculus. Explore applications of his laws in various fields, from celestial mechanics to measuring weight on different planets. From Newton to Einstein, uncover the evolution of our understanding of the forces that shape the universe.
E N D
Isaac Newton – The Theorist Key question: Why are things happening? Invented calculus and physics while on vacation from college His three Laws of Motion, together with the Law of Universal Gravitation, explain all of Kepler’s Laws (and more!) Isaac Newton (1642–1727)
Isaac Newton (1642–1727) Major Works: Principia (1687) [Full title: Philosophiae naturalis principia mathematica] Opticks [sic!](1704) Later in life he was Master of the Mint, dabbled in alchemy, and spent a great deal of effort trying to make his enemies miserable
Newton’s first Law In the absence of a net external force, a body either is at rest or moves with constant velocity. Contrary to Aristotle, motion at constant velocity (may be zero) is thus the natural state of objects, not being at rest. Change of velocity needs to be explained; why a body is moving steadily does not.
Mass & Weight Mass is the property of an object Weight is a force, e.g. the force an object of certain mass may exert on a scale
Newton’s second Law The net external force on a body is equal to the mass of that body times its acceleration F = ma. Or: the mass of that body times its acceleration is equal to the net force exerted on it ma = F Or: a=F/m Or: m=F/a
Newton’s 3rd law For every action, there is an equal and opposite reaction Does not sound like much, but that’s where all forces come from!
Newton’s Laws of Motion (Axioms) Every body continues in a state of rest or in a state of uniform motion in a straight line unless it is compelled to change that state by forces acting on it (law of inertia) The change of motion is proportional to the motive force impressed (i.e. if the mass is constant, F = ma) For every action, there is an equal and opposite reaction (That’s where forces come from!)
Newton’s Laws a) No force: particle at rest b) Force: particle starts moving c) Two forces: particle changes movement Gravity pulls baseball back to earth by continuously changing its velocity (and thereby its position) Always the same constant pull
Law of Universal Gravitation Force = G Mearth Mman/ R2 Mman MEarth R
Orbital Motion = Kepler Explained “Compromise”: planet moves in curved orbit Sun’s gravitational pull forces planet into orbit by changing direction of planets velocity Planet wants to move in a straight line of constant velocity (Newton 1)
It takes a stronger force to make a high speed planet move in an orbit
Cannon “Thought Experiment” http://www.phys.virginia.edu/classes/109N/more_stuff/Applets/newt/newtmtn.html
Applications • From the distance r between two bodies and the gravitational acceleration a of one of the bodies, we can compute the mass M of the other F = ma = G Mm/r2 (m cancels out) • From the weight of objects (i.e., the force of gravity) near the surface of the Earth, and known radius of Earth RE = 6.4103 km, we find ME = 61024 kg • Your weight on another planet is F = m GM/r2 • E.g., on the Moon your weight would be 1/6 of what it is on Earth
Applications (cont’d) • The mass of the Sun can be deduced from the orbital velocity of the planets: MS= rOrbitvOrbit2/G = 21030 kg • actually, Sun and planets orbit their common center of mass • Orbital mechanics. A body in an elliptical orbit cannot escape the mass it's orbiting unless something increases its velocity to a certain value called the escape velocity • Escape velocity from Earth's surface is about 25,000 mph (7 mi/sec)
From Newton to Einstein If we use Newton II and the law of universal gravity, we can calculate how a celestial object moves, i.e. figure out its acceleration, which leads to its velocity, which leads to its position as a function of time: ma= F = GMm/r2 so its acceleration a= GM/r2is independent of its mass! This prompted Einstein to formulate his gravitational theory as pure geometry.