orbital motion = kepler explained “compromise”: planet moves in curved orbit planet wants to...

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Orbital Motion = Kepler Explained “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity Sun’s gravitationa l pull forces planet into orbit by changing direction of planets velocity

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Page 1: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Orbital Motion = Kepler Explained

“Compromise”: planet moves in curved orbit

Planet wants to move in a straight line of constant velocity (Newton 1)

Sun’s gravitational pull forces planet into orbit by changing direction of planets velocity

Page 2: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

It takes a stronger force to make a high speed planet move in an orbit

Page 3: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Cannon “Thought Experiment”

• http://www.phys.virginia.edu/classes/109N/more_stuff/Applets/newt/newtmtn.html

Page 4: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Applications

• From the distance r between two bodies and the gravitational acceleration a of one of the bodies, we can compute the mass M of the other

F = ma = G Mm/r2 (m cancels out)

– From the weight of objects (i.e., the force of gravity) near the surface of the Earth, and known radius of Earth RE = 6.4103 km, we find ME = 61024 kg

– Your weight on another planet is F = m GM/r2

• E.g., on the Moon your weight would be 1/6 of what it is on Earth

Page 5: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Applications (cont’d)

• The mass of the Sun can be deduced from the orbital velocity of the planets: MS = rOrbitvOrbit

2/G = 21030 kg – actually, Sun and planets orbit their common center of mass

• Orbital mechanics. A body in an elliptical orbit cannot escape the mass it's orbiting unless something increases its velocity to a certain value called the escape velocity– Escape velocity from Earth's surface is about 25,000 mph (7

mi/sec)

Page 6: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

From Newton to Einstein

• If we use Newton II and the law of universal gravity, we can calculate how a celestial object moves, i.e. figure out its acceleration, which leads to its velocity, which leads to its position as a function of time:

ma= F = GMm/r2

so its acceleration a= GM/r2 is independent of its mass!

• This prompted Einstein to formulate his gravitational theory as pure geometry.

Page 7: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Telescopes

From Galileo to Hubble: Telescopes use lenses and mirrors to focus and therefore collect light

Page 8: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Rain analogy: Collect light as you collect rain

Rain/light collected is proportional to area of umbrella/mirror, not its diameter

Page 9: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Light hits Matter: Refraction• Light travels at different speeds in vacuum, air,

and other substances• When light hits the material at an angle, part of it

slows down while the rest continues at the original speed – results in a change of direction– Different colors bend different amounts – prism,

rainbow

Page 10: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Application for Refraction

• Lenses use refraction to focus light to a single spot

Page 11: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Light hits Matter (II): Reflection• Light that hits a mirror is

reflected at the same angle it was incident from

• Proper design of a mirror (the shape of a parabola) can focus all rays incident on the mirror to a single place

Page 12: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Application for Reflection

• Curved mirrors use reflection to focus light to a single spot

Page 13: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Telescopes

• Light collectors

• Two types:– Reflectors

(Mirrors)– Refractors

(Lenses)

Page 14: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Refracting Telescopes

Page 15: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Reflecting Telescope

Page 16: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Problems with Refractors

• Different colors (wavelengths) bent by different amounts – chromatic aberration

• Other forms of aberration

• Deform under their own weight

• Absorption of light

• Have two surfaces that must be optically perfect

Page 17: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Telescope Size• A larger telescope gathers more light (more

collecting area)

• Angular resolution is limited by diffraction of light waves; this also improves with larger telescope size

Page 18: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Resolving Power of Telescopes

Page 19: Orbital Motion = Kepler Explained  “Compromise”: planet moves in curved orbit Planet wants to move in a straight line of constant velocity (Newton 1)

Atmospheric Limitations