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Gravitation Flat Earth • Up to now we have parameterized the weight of an object as W mg • This is true for a flat earth assumption. • Is the earth flat? • What evidence is there that it is not? Gravitational Force • Central Force - Directed between the centers of mass for the two objects. • Inverse Square Law Force - Strength drops off as 1/r². m1m2 F21 G 2 rˆ r G 6.672 1011 Nm2 / kg 2 r m1 m2 Earth & the Moon • What is the gravitational force between the rm earth and the moon? M e 5.97 10 kg 24 mm 7.35 10 kg 22 rem 3.85 10 m 8 re 6.37 10 m 6 rm 1.74 10 m 6 re me rem mm Potential Energy • Calculate work needed to change height U W rf ri U rf ri F ( r )dr 1 1 GMm ˆ 2 r drrˆ GMm r rf ri If Ui=0 at ri=, GMm U r Kepler’s Laws • All planets move in elliptical orbits with the sun at one focal point. • Planets sweep out equal areas in equal time intervals. – Conservation of angular momentum • Square of the orbital period is proportional to the cube of the semi-major axis of the orbit. A1 A2 Orbital Motion • Assume only gravitational force and circular motion at constant speed. Newton’s 2nd Law T = orbital time period F ma GMm v2 m 2 r r GM 2 v r d 2 r v t T GM 2 r r T 2 v m r M 2 3 4 r 2 T GM Earth Satellites • Landsat-7 has an orbit altitude of 705 km. What is its acceleration, speed, and orbital period? re 6.37 10 m 6 M e 5.97 10 kg 24 Geostationary Satellites • One orbit = One Day • Types of Satellites – Weather – Communications Digital Globe - Quickbird • 2 foot resolution • Altitude of 280 mi q = 1.3 mrad Moon’s Orbit • What is the period of the moon’s orbit? 29.5 days Synodic (w.r.t. sun) 27.3 days Sidereal (w.r.t. stars) 0 days M e 5.97 10 24 kg rem 3.85 108 m 4 2 r 3 6 T 2.38 10 s GM e T = 27.5 days Escape Velocity • Escape velocity - Velocity a projectile needs to escape the gravitational force. Ki U i U f At rmax = , v M e 5.97 10 24 kg Re 6.37 10 6 m GMm GMm mv R rmax 2GM R 1 2 2 ve = 11.2 km/s Tides • Tides--rise and fall of ocean levels – 12-hour cycle – Interaction between the moon’s gravity and the earth’s centripetal acceleration. Gravitational Acceleration GM g 2 r Centripetal Acceleration a r 2 a>g a=g a<g