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Kepler’s Laws of Planetary Motion © David Hoult 2009.

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Presentation on theme: "Kepler’s Laws of Planetary Motion © David Hoult 2009."— Presentation transcript:

1 Kepler’s Laws of Planetary Motion © David Hoult 2009

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6 The eccentricity of an ellipse gives an indication of the difference between its major and minor axes © David Hoult 2009

7 The eccentricity depends on the distance between the two points, f (compared with the length of the piece of string) The eccentricity of an ellipse gives an indication of the difference between its major and minor axes © David Hoult 2009

8 eccentricity = distance between foci / major axis © David Hoult 2009

9 The eccentricity of the orbits of the planets is low; their orbits are very nearly circular orbits. eccentricity = distance between foci / major axis © David Hoult 2009

10 Law 1 Each planet orbits the sun in an elliptical path with the sun at one focus of the ellipse. © David Hoult 2009

11 Mercury 0.206 © David Hoult 2009

12 Mercury 0.206 Venus 0.0068 © David Hoult 2009

13 Mercury 0.206 Venus 0.0068 Earth 0.0167 © David Hoult 2009

14 Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 © David Hoult 2009

15 Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485 © David Hoult 2009

16 Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485 Saturn 0.0556 © David Hoult 2009

17 Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485 Saturn 0.0556 Uranus 0.0472 © David Hoult 2009

18 Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485 Saturn 0.0556 Uranus 0.0472 Neptune 0.0086 © David Hoult 2009

19 Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485 Saturn 0.0556 Uranus 0.0472 Neptune 0.0086 Pluto 0.25 © David Hoult 2009

20 ...it can be shown that... © David Hoult 2009

21 minor axis major axis = 1 - e 2 where e is the eccentricity of the ellipse © David Hoult 2009

22 minor axis major axis = 1 - e 2 where e is the eccentricity of the ellipse which means that even for the planet (?) with the most eccentric orbit, the ratio of minor to major axis is only about: © David Hoult 2009

23 minor axis major axis = 1 - e 2 where e is the eccentricity of the ellipse which means that even for the planet (?) with the most eccentric orbit, the ratio of minor to major axes is only about: 0.97 © David Hoult 2009

24 In calculations we will consider the orbits to be circular © David Hoult 2009

25 Eccentricity of ellipse much exaggerated © David Hoult 2009

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31 Law 2 A line from the sun to a planet sweeps out equal areas in equal times. © David Hoult 2009

32 Law 3 The square of the time period of a planet’s orbit is directly proportional to the cube of its mean distance from the sun. © David Hoult 2009

33 T2T2 r3r3 = a constant © David Hoult 2009

34 F = G r2r2 Mm © David Hoult 2009

35 F = m r 2m r 2 F = G r2r2 Mm © David Hoult 2009

36 F = G r2r2 Mm F = m r 2m r 2 © David Hoult 2009

37 F = G r2r2 Mm F = m r 2m r 2 r2r2 G M mG M m m r 2m r 2 = © David Hoult 2009

38 F = G r2r2 Mm F = m r 2m r 2  = T 2 2  r2r2 G M mG M m m r 2m r 2 = © David Hoult 2009

39 T2T2 r3r3 = 4242 GM © David Hoult 2009

40 T2T2 r3r3 = 4242 GM in which we see Kepler’s third law © David Hoult 2009


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