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Kepler’s Laws • What are the shapes and important properties of the planetary orbits? • How does the speed of a planet vary as it orbits the sun? • How does the period of a planet's orbit depend on its distance from the Sun? Kepler’s First Law • The orbits of the planets are elliptical (not circular) with the Sun at one focus of the ellipse. • 'a' = semi-major axis: Avg. distance between sun and planet Kepler’s Second Law Kepler determined that a planet moves faster when near the Sun, and slower when far from the Sun. Planet Faster Sun Slower Kepler's Second Law A line connecting the Sun and a planet sweeps out equal areas in equal times. slower faster Translation: planets move faster when closer to the Sun. Kepler's Third Law The square of a planet's orbital period is proportional to the cube of its semi-major axis. P2 is proportional to a3 or P2 (in Earth years) = a3 (in A.U.) 1 A.U. = 1.5 x 108 km Translation: The further the planet is from the sun, the longer the period. Correction to Kepler’s Third Law Earth and sun actually rotate about their common center of mass Corresponds to a point inside sun Used to detect extrasolar planets Why? Kepler’s Laws provided a complete kinematical description of planetary motion (including the motion of planetary satellites, like the Moon) - but why did the planets move like that? The Apple & the Moon Isaac Newton realized that the motion of a falling apple and the motion of the Moon were both actually the same motion, caused by the same force - the gravitational force. Universal Gravitation Newton’s idea was that gravity was a universal force acting between any two objects. Gravitational Field Strength To measure the strength of the gravitational field at any point, measure the gravitational force, F, exerted on any “test mass”, m. Gravitational Field Strength, g = F/m Gravitational Field Strength Near the surface of the Earth, g = F/m = 9.8 N/kg = 9.8 m/s2. In general, g = GM/r2, where M is the mass of the object creating the field, r is the distance from the object’s center, and G = 6.67 x10-11 Nm2/kg2. Gravitational Force If g is the strength of the gravitational field at some point, then the gravitational force on an object of mass m at that point is Fgrav = mg. If g is the gravitational field strength at some point (in N/kg), then the free fall acceleration at that point is also g (in m/s2). Gravitational Field Inside a Planet If you are located a distance r from the center of a planet: – all of the planet’s mass inside a sphere of radius r pulls you toward the center of the planet. – All of the planet’s mass outside a sphere of radius r exerts no net gravitational force on you. Gravitational Field Inside a Planet The blue-shaded part of the planet pulls you toward point C. The grey-shaded part of the planet does not pull you at all. Gravitational Field Inside a Planet Half way to the center of the planet, g has one-half of its surface value. At the center of the planet, g = 0 N/kg. Kepler’s Laws are just a special case of Newton’s Laws! Newton explained Kepler’s Laws by solving the law of Universal Gravitation and the law of Motion Ellipses are one possible solution, but there are others (parabolas and hyperbolas) Kepler’s Laws are just a special case of Newton’s Laws! Newton explained Kepler’s Laws by solving the law of Universal Gravitation and the law of Motion Ellipses are one possible solution, but there are others (parabolas and hyperbolas) Bound and Unbound Orbits Unbound (comet) Unbound (galaxy-galaxy) Bound (planets, binary stars) Understanding Kepler’s Laws: conservation of angular momentum L = mv x r = constant r larger distance smaller v planet moves slower smaller distance smaller r bigger v planet moves faster Understanding Kepler’s Third Law Newton’s generalization of Kepler’s Third Law is given by: 4p2 a3 p2 = G(M1 + M2) Mplanet << Msun, so 4p2 a3 p2 = GMsun This has two amazing implications: The orbital period of a planet depends only on its distance from the sun, and this is true whenever M1 << M2 An Astronaut and the Space Shuttle have the same orbit! Second Amazing Implication: If we know the period p and the average distance of the orbit a, we can calculate the mass of the sun!