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Lecture 6: Gravity and Motion

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Page 1: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Lecture 6: Gravity and Motion

Page 2: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Review from Last Lecture…

Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of

Newton’s Laws bound and unbound orbits tides and tidal friction

Page 3: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Kepler or Newton?

find the mass of the Earth using the fact that the Moon’s orbit has a period of 29 ½ days

find the average orbital distance for an asteroid that orbits the Sun with a period of 8 years

find the period of a binary star system with a mean orbital distance of 10 pc

Page 4: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Tides

Page 5: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

The Moon’s Tidal Forces on the Earth

Page 6: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound
Page 7: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound
Page 8: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound
Page 9: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound
Page 10: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound
Page 11: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Galactic Tidal Forces

Page 12: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound
Page 13: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Tidal Friction

Page 14: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Synchronous Rotation

Page 15: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Tidal friction and the Moon

Tidal friction from the Moon acting on the Earth causes the Earth’s rotation to slow down.

As a result, the Moon also moves further and further away from Earth (due to conservation of angular momentum).

Page 16: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Implications…

was the Moon’s angular size larger or smaller in the past?

was the length of a lunar month longer or shorter in the past?

were eclipses (both solar and lunar) more or less frequent in the past?

Page 17: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

The acceleration of gravity

the universal law of gravitation allows us to understand why the acceleration due to gravity is independent of the mass of the object

and why our weight is different on other planets

Page 18: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Why g is independent of mass

Imagine dropping a rock near the surface of the Earth. The force on the rock is:

Fg = G MEarth Mrock / d2 = G MEarth Mrock / (REarth)2

Newton’s Second Law of Motion says that the force is also:

Fg = Mrock arock = G MEarth Mrock / (REarth)2

arock = g = G MEarth / (REarth)2

Page 19: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Finding the value of g

g = G MEarth / (REarth)2

g = (6.67 x 10-11 m3/(kg s2) ) x 6.0 x 1024 kg / (6.4 x 106 m)2

Mearth = 6.0 x 1024 kg Rearth = 6.4 x 106 m

= 9.8 m/s2

Page 20: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

What about on the Moon?

g = G MMoon / (RMoon)2

g = (6.67 x 10-11 m3/(kg s2) ) x 7.4 x 1022 kg / (1.7 x 106 m)2

MMoon = 7.4 x 1022 kg RMoon = 1.7 x 106 m

= 1.7 m/s2

gravity is weaker on the Moon…therefore things gravity is weaker on the Moon…therefore things weighweigh less! less!

Page 21: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Matter and Energy

Page 22: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Energy is what makes matter move

kinetic energy = energy of motion potential energy = stored energy

gravitational chemical electrical

radiative energy = light

Page 23: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Units of Energy

calories kilowatt-hours BTU Joules

1 Joule = 0.00024 Calories

Page 24: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Quantifying Energy

kinetic energy = ½ m v2

where m = mass (in kg)and v = velocity (in m/s)

answer will be in Joules (1 J = kg x m2/s2)

Page 25: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Gravitational Potential Energy

the amount of gravitational potential energy is proportional to the mass, the force of gravity, and the distance

for example, for an object suspended above the earth, the gravitational potential energy is W = G m MEarth/r = m x g x r

Page 26: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Conservation of Energy

the total amount of energy in the Universe remains the same

energy can change forms but cannot be created or destroyed

Page 27: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

Orbital Energy

moving faster largerkinetic energy

moving slower smallerkinetic energy

Page 28: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

bound vs. unbound orbits

bound orbits gravitational potential energy balances kinetic energy

unbound orbits kinetic energy greaterthan gravitational potential

Page 29: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

gravitational encounters

Page 30: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

escape velocity

We can now derive the escape velocity by setting the kinetic energy equal to the gravitational potential energy:

½ m v2 = Gm MEarth/REarth

vescape = (2GMEarth / REarth)½

Page 31: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

The Escape Velocity from Earth

vescape = (2GMEarth / REarth)½

= (2 x 6.67x10-11 m3/(kg s2) x 6.0x1024 kg/6.4x106m)½

vescape = 11 km/s

Page 32: Lecture 6: Gravity and Motion Review from Last Lecture… Newton’s Universal Law of Gravitation Kepler’s Laws are special cases of Newton’s Laws bound

The End