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Universal Gravitation Chapter 9 - Gravity • • • • • • • • • Universal Law of Gravity Universal Gravitational Constant, G Gravity and Distance – Inverse Square Laws Weight and Weightlessness Ocean Tides Gravitational Fields Einstein's Theory of Gravitation Black Holes Universal Gravitation Physics 1100 – Spring 2012 2 Newton’s Law of Universal Gravitation • From the Orbits of the planets, Newton deduced inverse square law of attraction. Gm m Gm 1 F ~ M M 1/rm22 FF 22 dd 1 2 2 Physics 1100 – Spring 2012 3 Cavendish Measurement of Gravity Physics 1100 – Spring 2012 4 Calculation of G F = GM1M2/r2 Newton’s Law of Universal Gravitation G = 6.67410-11 m3/(kg·s2) Earth: M = 5.9761024 kg; r = 6,378,000 m a = 9.80 m/s2 a1 = F/M1 = GM2/r2 acceleration of mass #1 due to mass #2 Physics 1100 – Spring 2012 5 Inverse Square Laws Physics 1100 – Spring 2012 6 Gravity as Inverse Square Law Physics 1100 – Spring 2012 7 Weight and Weightlessness • Weight • the force due to gravity on an object • Weight = Mass Acceleration of Gravity • W=mg • Weightlessness - a conditions wherein gravitational pull appears to be lacking – Examples: • Astronauts • Falling in an Elevator • Skydiving • Underwater Physics 1100 – Spring 2012 8 Weight and Weightlessness Physics 1100 – Spring 2012 9 Gravity Questions • Did the Moon exert a gravitational force on the Apollo astronauts? • What kind of objects can exert a gravitational force on other objects? • The constant G is a rather small number. What kind of objects can exert strong gravitational forces? Physics 1100 – Spring 2012 10 Gravity Questions • If the distance between two objects in space is doubled, then what happens to the gravitational force between them? • • What is the distance is tripled? …is quadrupled? • • • What if the mass of one of the object is doubled? …tripled? …quadrupled? Physics 1100 – Spring 2012 11 Tidal forces (Moon & Sun) Physics 1100 – Spring 2012 12 Gravity Fields Physics 1100 – Spring 2012 13 Class Problem • If the sun suddenly collapsed to become a black hole, the earth would a) leave the solar system in a straight-line path spiral b) spiral into the black hole c) undergo a major increase in tidal forces d) continue to circle in its usual orbit Physics 1100 – Spring 2012 14 General Relativity Einstein Upsets the Applecart Einstein’s Theory of Gravitation • Einstein perceived a gravitational field as a geometrical warping of 4-D space and time. Physics 1100 – Spring 2012 16 Mattress Example • Imagine 2 bowling balls on a mattress, ignore for the moment the “gravitational” interaction between them • As they roll around on the mattress, they make dimples in its surface • If they get close to each other, they sense these dimples and are “attracted” to each other Physics 1100 – Spring 2012 17 Bowling Balls on a Mattress Physics 1100 – Spring 2012 18 The 3 “Classic” Tests of General Relativity • Precession of Mercury’s orbit • Deflection of starlight (gravitational lensing) • Gravitational Redshift - Clocks run slower and slower in more and more intense grativational fields. Physics 1100 – Spring 2012 19 Black Holes Copyright – A. Hobart BLACK HOLES • If a massive star shrinks enough so that the escape velocity is equal to or greater than the speed of light, then it has become a black hole. • Light cannot escape from a black hole. Physics 1100 – Spring 2012 21