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Kepler’s Laws of Planetary Motion © David Hoult 2009

Kepler’s Laws of Planetary Motion © David Hoult 2009

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

Kepler’s Laws of Planetary Motion

© David Hoult 2009

Page 2: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 3: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 4: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 5: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 6: Kepler’s Laws of Planetary Motion © David Hoult 2009

The eccentricity of an ellipse gives an indication of the difference between its major and minor axes

© David Hoult 2009

Page 7: Kepler’s Laws of Planetary Motion © David Hoult 2009

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

Page 8: Kepler’s Laws of Planetary Motion © David Hoult 2009

eccentricity = distance between foci / major axis

© David Hoult 2009

Page 9: Kepler’s Laws of Planetary Motion © David Hoult 2009

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

Page 10: Kepler’s Laws of Planetary Motion © David Hoult 2009

Law 1

Each planet orbits the sun in an elliptical path with the sun at one focus of the ellipse.

© David Hoult 2009

Page 11: Kepler’s Laws of Planetary Motion © David Hoult 2009

Mercury 0.206

© David Hoult 2009

Page 12: Kepler’s Laws of Planetary Motion © David Hoult 2009

Mercury 0.206 Venus 0.0068

© David Hoult 2009

Page 13: Kepler’s Laws of Planetary Motion © David Hoult 2009

Mercury 0.206 Venus 0.0068 Earth 0.0167

© David Hoult 2009

Page 14: Kepler’s Laws of Planetary Motion © David Hoult 2009

Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934

© David Hoult 2009

Page 15: Kepler’s Laws of Planetary Motion © David Hoult 2009

Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485

© David Hoult 2009

Page 16: Kepler’s Laws of Planetary Motion © David Hoult 2009

Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485 Saturn 0.0556

© David Hoult 2009

Page 17: Kepler’s Laws of Planetary Motion © David Hoult 2009

Mercury 0.206 Venus 0.0068 Earth 0.0167 Mars 0.0934 Jupiter 0.0485 Saturn 0.0556 Uranus 0.0472

© David Hoult 2009

Page 18: Kepler’s Laws of Planetary Motion © David Hoult 2009

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

Page 19: Kepler’s Laws of Planetary Motion © David Hoult 2009

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

Page 20: Kepler’s Laws of Planetary Motion © David Hoult 2009

...it can be shown that...

© David Hoult 2009

Page 21: Kepler’s Laws of Planetary Motion © David Hoult 2009

minor axismajor axis

= 1 - e2

where e is the eccentricity of the ellipse

© David Hoult 2009

Page 22: Kepler’s Laws of Planetary Motion © David Hoult 2009

minor axismajor axis

= 1 - e2

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

Page 23: Kepler’s Laws of Planetary Motion © David Hoult 2009

minor axismajor axis

= 1 - e2

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

Page 24: Kepler’s Laws of Planetary Motion © David Hoult 2009

In calculations we will consider the orbits to be circular

© David Hoult 2009

Page 25: Kepler’s Laws of Planetary Motion © David Hoult 2009

Eccentricity of ellipse much exaggerated© David Hoult 2009

Page 26: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 27: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 28: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 29: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 30: Kepler’s Laws of Planetary Motion © David Hoult 2009

© David Hoult 2009

Page 31: Kepler’s Laws of Planetary Motion © David Hoult 2009

Law 2

A line from the sun to a planet sweeps out equal areas in equal times.

© David Hoult 2009

Page 32: Kepler’s Laws of Planetary Motion © David Hoult 2009

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

Page 33: Kepler’s Laws of Planetary Motion © David Hoult 2009

T2

r3= a constant

© David Hoult 2009

Page 34: Kepler’s Laws of Planetary Motion © David Hoult 2009

F = Gr2

Mm

© David Hoult 2009

Page 35: Kepler’s Laws of Planetary Motion © David Hoult 2009

F = m r 2

F = Gr2

Mm

© David Hoult 2009

Page 36: Kepler’s Laws of Planetary Motion © David Hoult 2009

F = Gr2

Mm F = m r 2

© David Hoult 2009

Page 37: Kepler’s Laws of Planetary Motion © David Hoult 2009

F = Gr2

Mm F = m r 2

r2G M m m r 2

=

© David Hoult 2009

Page 38: Kepler’s Laws of Planetary Motion © David Hoult 2009

F = Gr2

Mm F = m r 2

= T

2

r2G M m m r 2

=

© David Hoult 2009

Page 39: Kepler’s Laws of Planetary Motion © David Hoult 2009

T2

r3= 42

GM

© David Hoult 2009

Page 40: Kepler’s Laws of Planetary Motion © David Hoult 2009

T2

r3= 42

GM

in which we see Kepler’s third law

© David Hoult 2009