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Page 1: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 1 Intro to Stars

Kepler, Newton and

Gravitation

Page 2: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 2 Intro to Stars

Using the unit of distance

1 AU = Earth-Sun distance

PLANETS COPERNICUS MODERN

Mercury 0.38 0.387

Venus 0.72 0.723

Earth 1.00 1.00

Mars 1.52 1.52

Jupiter 5.22 5.20

Saturn 9.17 9.54

Page 3: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 3 Intro to Stars

Johannes Kepler - 1600 A.D.

• built on successes and failures

• demanded that his model’s predictions be

at least as accurate as the observations (1

arcmin error)

foundation for modern cosmological concepts

“I have discovered among the celestial movements

the full nature of harmony.”

Page 4: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 4 Intro to Stars

Kepler - the Ellipse

Page 5: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 5 Intro to Stars

Kepler - the Ellipse two focal points -

foci

focal distance

Page 6: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 6 Intro to Stars

Kepler - the Ellipse

minor axis

semi-minor axis - half the minor axis

Page 7: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 7 Intro to Stars

Kepler - the Ellipse

major axis

minor axis

semi-major axis - half the major axis (a)

semi-minor axis - half the minor axis

Page 8: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 8 Intro to Stars

Kepler - the Ellipse two focal points -

foci major axis

minor axis

focal distance

semi-major axis - half the major axis (a)

semi-minor axis - half the minor axis

eccentricity = focal distance

major axis

Page 9: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 9 Intro to Stars

Kepler - the Ellipse

major axis

focal distance

eccentricity = focal distance

major axis

e = 0 means ????

e = 1 means ????

Page 10: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 10 Intro to Stars

Kepler’s Three Laws

I. Law of Ellipses

Each planet’s orbit is an ellipse with

the Sun at one of the foci.

implication: distance of the planet to

the Sun varies

Page 11: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 11 Intro to Stars

Kepler’s Three Laws

II. Law of Equal Areas

A line drawn from a planet to the Sun

sweeps out equal areas in equal times.

implication: orbital speeds are non-uniform

yet vary in a regular way

Closer a planet is the the Sun, the faster

it moves in its orbit

(force ????)

Page 12: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 12 Intro to Stars

Kepler’s Three Laws

III. Harmonic Law

Planet p (Earth years) a (AU)

============================

Mercury 0.24 0.39

Venus 0.62 0.72

Earth 1.0 1.0

Mars 1.9 1.5

Jupiter 12 5.2

Saturn 29 9.5

Page 13: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 13 Intro to Stars

Kepler’s Three Laws

III. Harmonic Law

Square of the orbital period is proportional

to the cube of the average distance.

p2 = k a3

implication: planets with large orbits

move slowly

Proportion holds for all planets =>

A PHYSICAL CAUSE !!

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Kepler, Newton and Gravity 14 Intro to Stars

Kepler’s Third Law

p2 = k a3

k = proportionality constant

p (years)

a (AU’s)

=> k = 1

True for any body orbiting the Sun, even spacecraft!

“I contemplate its beauty with incredible

and ravishing delight.

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Kepler, Newton and Gravity 15 Intro to Stars

Kepler

made perhaps the greatest leap in scientific thinking

predictions were 10 times more accurate than either

Ptolemaic model (geocentric)

Copernican model (heliocentric)

gave birth to astronomy as a physical science

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Kepler, Newton and Gravity 16 Intro to Stars

Orbital Eccentricities

Planet Orbital Eccentricity

Mercury 0.206

Venus 0.007

Earth 0.017

Mars 0.094

Jupiter 0.048

Saturn 0.054

Uranus 0.048

Neptune 0.007

Pluto 0.253

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Kepler, Newton and Gravity 17 Intro to Stars

GALILEO, NEWTON,

and GRAVITY

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Kepler, Newton and Gravity 18 Intro to Stars

Mechanics: the study of falling bodies

speed: how fast you are going

velocity: how fast you are going

in a specific direction

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Kepler, Newton and Gravity 19 Intro to Stars

Albany to Portland:

speed = 100 km/hr

velocity =

Portland to Albany:

speed = 80 km/hr

velocity =

?????? 100 km/hr north

?????? 80 km/hr south

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Kepler, Newton and Gravity 20 Intro to Stars

• change in speed

• change in direction

• change in both speed and direction

velocity: speed and direction

acceleration: CHANGE in velocity

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Kepler, Newton and Gravity 21 Intro to Stars

• You are stopped at a red light.

You step on the gas.

Your speed changes from 0 to 15 km/hr.

Are you accelerating?

speed: measured in km/hr

velocity: measured in km/hr in a direction

acceleration: measured in km/hr

unit of time

Three Cases

Yes, it is your speed that is changing.

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Kepler, Newton and Gravity 22 Intro to Stars

• You are driving in a circle around a racetrack

at a constant 20 km/hr.

Are you accelerating?

Yes. Your direction is changing.

• You are braking from 25 km/hr to 15 km/hr.

Are you accelerating?

Yes. Your speed is changing.

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Kepler, Newton and Gravity 23 Intro to Stars

Galileo and Motion

downward motion:

gravity pulling downward

forced motion

attractive force

horizontal motion:

would continue forever if no forces acted

natural motion

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Kepler, Newton and Gravity 24 Intro to Stars

Galileo’s Experiment

inclined plane, perfectly smooth

perfectly smooth ball

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Kepler, Newton and Gravity 25 Intro to Stars

Galileo’s Experiment

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Kepler, Newton and Gravity 26 Intro to Stars

Galileo’s Experiment

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Kepler, Newton and Gravity 27 Intro to Stars

Galileo’s Experiment

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Kepler, Newton and Gravity 28 Intro to Stars

Galileo

inertia: natural tendency for a body in motion

to remain in motion or natural tendency

for a body at rest to remain at rest

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Kepler, Newton and Gravity 29 Intro to Stars

acceleration due to gravity

• constant

• velocity changes at a constant rate

• at earth’s surface g = 9.8 m/s

Galileo also experimented with falling bodies

falling is NOT a natural motion

motion due to the force of gravity

s

We can use 10 m/s/s

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Kepler, Newton and Gravity 30 Intro to Stars

DROPPED ROCK

How fast is it going after

5 seconds of falling?

10 m/s

30 m/s

Starts at

0 m/s

How fast is it going after

1 second of falling?

How fast is it going after

3 seconds of falling?

50 m/s

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Kepler, Newton and Gravity 31 Intro to Stars

PARACHUTIST

How fast is she going after

5 seconds of falling?

10 m/s

30 m/s

Starts at

0 m/s

How fast is she going after

1 second of falling?

How fast is she going after

3 seconds of falling?

50 m/s

Ignore air resistance

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Kepler, Newton and Gravity 32 Intro to Stars

ALL falling bodies

fall with the

SAME acceleration !!

Page 33: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 33 Intro to Stars

Newton 1600 A.D.

Principia - Physics of motion

and Concept of Gravitation

Concept of Force

force produces an acceleration

acceleration is in the same direction

as the force

Page 34: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 34 Intro to Stars

Increase the force

=> greater acceleration

=> object reaches a greater velocity

What kind of relationship is this?

ACCELERATION

is directly proportional to

FORCE

Page 35: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 35 Intro to Stars

Increase the MASS

apply the original force

=> less acceleration

What kind of relationship is this?

ACCELERATION

is inversely proportional to

MASS

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Kepler, Newton and Gravity 36 Intro to Stars

Can you come up with a Pot O’ Gold type

relationship for acceleration, force & mass?

a = F

m

Forces have direction (same direction

as the acceleration)

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Kepler, Newton and Gravity 37 Intro to Stars

Newton clarified these definitions:

• mass : the measure of an object’s resistance

to a change in motion

• velocity : how fast an object moves in a

particular direction

• acceleration : how much the velocity (or

direction) changes with time

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Kepler, Newton and Gravity 38 Intro to Stars

Newton’s Three Laws of Motion

• INERTIAL LAW

A body at rest remains at rest unless

acted on by an outside force.

A body in motion at a constant velocity

along a straight line remains in motion

unless acted on by an outside force.

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Kepler, Newton and Gravity 39 Intro to Stars

Newton’s Three Laws of Motion

INERTIAL LAW

Implication:

If we see an acceleration, we know

there’s a net force acting on the

body in question (that is, change

in speed direction, or both)

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Kepler, Newton and Gravity 40 Intro to Stars

Newton’s Three Laws of Motion

• FORCE LAW

rate of change in a body’s velocity,

due to an applied force (in other words,

a body’s acceleration) is

– in the same direction as the force

– proportional to the force

– inversely proportional to its mass

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Kepler, Newton and Gravity 41 Intro to Stars

Newton’s Three Laws of Motion

FORCE LAW

Implication: can apply a force, measure

acceleration and infer the mass

of an object

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Kepler, Newton and Gravity 42 Intro to Stars

Newton’s Three Laws of Motion

• REACTION LAW

For every applied force, a force of

equal size by opposite direction arises.

Implication: forces act in pairs

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Kepler, Newton and Gravity 43 Intro to Stars

AN EXAMPLE

You are an astronaut out in space.

You push on your space capsule.

What is the equal and opposite force?

Since the forces are the SAME,

exactly what is different?

Spaceship pushes back on you.

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Kepler, Newton and Gravity 44 Intro to Stars

You Spaceship

F F

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Kepler, Newton and Gravity 45 Intro to Stars

You Spaceship

F F

m M

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Kepler, Newton and Gravity 46 Intro to Stars

You Spaceship

F F

m M

A a

Page 47: Kepler, Newton and Gravitationcf.linnbenton.edu/.../physci/rajabza/upload/6_Gravity.pdfIntro to Stars Kepler, Newton and Gravity 40 Newton’s Three Laws of Motion •FORCE LAW rate

Kepler, Newton and Gravity 47 Intro to Stars

You Spaceship

F F

m M

A a

Which has the greater velocity?

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Kepler, Newton and Gravity 48 Intro to Stars

NEWTON’S GREAT INSIGHT

Gravitation is an interaction

between two (or more)

bodies, such as the Sun and

the planets.

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Kepler, Newton and Gravity 49 Intro to Stars

Newton’s Law of Gravitation

• What direction does the force

of gravity act? (nature of the force)

• What is the amount of force?

(physical properties that determine

the strength of the force)

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Kepler, Newton and Gravity 50 Intro to Stars

LAWS OF MOTION

+

Kepler’s Planetary Laws

Law of Universal Gravitation

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Kepler, Newton and Gravity 51 Intro to Stars

GRAVITATION

• central force : type of force that causes

elliptical orbits; force directed towards

the center of motion

• planets moving in orbits under the influence

of a central force followed Kepler’s

Second Law (Law of Areas)

• from the geometric properties of ellipses,

force is described by a specific type of

force law => re-derived Kepler’s Third

Law using this force law

Newton’s Laws and Kepler’s Laws were in

total agreement

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Kepler, Newton and Gravity 52 Intro to Stars

• Direction - changing? or not?

Consider the moon in orbit:

curved path => changing

Newton’s First Law:

direction is changing

there is an acceleration

Therefore, there is a force acting

on the moon

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Kepler, Newton and Gravity 53 Intro to Stars

Force is directed towards the center

of the Earth. We call a center-directed

force a centripetal force.

At every point in its orbit, a centripetal

force acts on the moon to keep it

bound to Earth.

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Kepler, Newton and Gravity 54 Intro to Stars

Billiard Ball Analogy

• Ball makes a

collision with

side

• Ball changes

direction

• Ball accelerates

from applied

force of the

wall

Force is

directed towards

the center of the

table

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Kepler, Newton and Gravity 55 Intro to Stars

Pentagonal

Table

Force still

points to

the center Angle of strike and rebound

is smaller

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Kepler, Newton and Gravity 56 Intro to Stars

Hexagonal

Table

Force still

points to

the center Angle of strike and rebound

is even smaller

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Kepler, Newton and Gravity 57 Intro to Stars

Circular

Table

Infinite number

of sides, angle

of strike and

rebound is

zero

Force points to

center at every

point

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Kepler, Newton and Gravity 58 Intro to Stars

Moon in its ‘circular’ orbit: at every

point in its orbit, a centripetal force

acts on the moon to keep it bound to

Earth.

GRAVITY !!

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Kepler, Newton and Gravity 59 Intro to Stars

Law of Gravitation

Every body in the Universe attracts

every other body with a gravitational

force.

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Kepler, Newton and Gravity 60 Intro to Stars

Consider two objects only

• amount of gravitational force depends DIRECTLY

on the amount of material each object has (mass)

What would happen if you doubled the mass

of one of the objects?

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Kepler, Newton and Gravity 61 Intro to Stars

The force between them was F.

After the pink object doubles, the gravitational

force is 2 times F or 2F

TWICE AS MUCH

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Kepler, Newton and Gravity 62 Intro to Stars

The force between them was 2F

After the purple object doubles, the gravitational

force is 2 times 2F or 4F

4 TIMES the original

amount of force

Now what happens

if we double the mass

of the other object?

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Kepler, Newton and Gravity 63 Intro to Stars

To express that in algebra:

Fg is directly proportional to

mpurple x masspink

or

Fg m1 x m2

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Kepler, Newton and Gravity 64 Intro to Stars

• objects at greater separations have less gravitational

force between them than those closer together

Decrease of force with

distance happens in a

special way

Force is inversely

proportional to the

square of the distance.

1 m

When the distance

is 1 meter, the force

between them is F.

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Kepler, Newton and Gravity 65 Intro to Stars

1 m

Start with the objects

1 meter apart.

What happens if we move

them to 2 meters apart? (that is,

we double the distance)

2 m

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Kepler, Newton and Gravity 66 Intro to Stars

2 m

The force, when they were 1 meter apart, was

F - now at 2 meters, the force is

Less is it 1/2 as much?

is it 1/4 as much?

Force is proportional to 1

(distance) 2 Force is as much as it was. 1 4

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Kepler, Newton and Gravity 67 Intro to Stars

1 m 3 m

What happens to the force if we move

them 3 meters apart?

Force is then 1/9 as much as it was

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Kepler, Newton and Gravity 68 Intro to Stars

F is proportional to m1

F is proportional to m2

Force is proportional to 1

(distance) 2

Force m1 m2

(distance) 2 or

m1 m2

R 2

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Kepler, Newton and Gravity 69 Intro to Stars

Constant of proportionality is

G - Universal Gravitational Constant

G = 6.67 x 10-11

Force (newtons)

masses (kgs)

R (meters)

m1 m2

R 2

Force = G

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Kepler, Newton and Gravity 70 Intro to Stars

Law of Gravitation

Fgravity = G m1m2

R2

Interpretation:

Force due to gravity is directly

proportional to the masses of

the objects involved.

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Kepler, Newton and Gravity 71 Intro to Stars

Law of Gravitation

Fgravity = G m1m2

R2

Interpretation:

Force due to gravity is inversely

proportional to the distance

between them squared.

1 over

R2 Law

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Kepler, Newton and Gravity 72 Intro to Stars

Newton worked this out mathematically

(it’s a model) - how did he test this?

1 Re

60 Re Moon is 60 times

farther from the center

of the Earth than the

apple is.

How much less gravitational

force is felt at the location of

the Moon ?

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Kepler, Newton and Gravity 73 Intro to Stars

Force at Moon is 1

(60)2

= 1

3600

Newton’s mathematical model predicted

the force (acceleration) should be

3600 times less.

Comparing to measured observations of

the Moon in its orbit, this was

‘pretty nearly’ the same.

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Kepler, Newton and Gravity 74 Intro to Stars

Newton’s Concept Extension

• Earth’s gravity keeps the moon

swinging around the Earth

• Sun’s gravity keeps the planets

swinging around the Sun

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Kepler, Newton and Gravity 75 Intro to Stars

Newton Revised

Kepler’s Third Law

p2 = k a3

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Kepler, Newton and Gravity 76 Intro to Stars

Newton Revised

Kepler’s Third Law

p2 = k a3

p2 = 4 2

G(Msun + mplanet)

a3

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Kepler, Newton and Gravity 77 Intro to Stars

Kepler’s Third Law Revised

p2 = 4 2

G(Msun + mplanet)

a3

TREMENDOUSLY

IMPORTANT !!

Can use this to find the

mass of the Sun !!

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Kepler, Newton and Gravity 78 Intro to Stars

p2 = 4 2

G(Msun + mplanet)

a3

• measure the period of the Earth’s orbit

• measure the average distance from the Sun

• approximate

Msun + mearth » Msun

• look up the value of G

• calculate the mass of the Sun !!

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Kepler, Newton and Gravity 79 Intro to Stars

We can find the mass of the

Sun using any body orbiting

the Sun.

We can find the mass of the

Earth using any body orbiting

the Earth.

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Kepler, Newton and Gravity 80 Intro to Stars

What would you do to find

the mass of a planet that

has no orbiting body?

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Kepler, Newton and Gravity 81 Intro to Stars

Center of Mass

center of mass : balance point of a group of objects

Where’s the balance point?

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Kepler, Newton and Gravity 82 Intro to Stars

1 AU (150 million km)

What’s your best

guess as to the location

of the center of mass

between the Earth

and the Sun ?

Earth

A mere 500 km

from the center of

the Sun !!!

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Kepler, Newton and Gravity 83 Intro to Stars

5 AU (750 million km)

What’s your best

guess as to the location

of the center of mass

between Jupiter and

the Sun ?

Jupiter

Just barely

outside the

surface of the Sun

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Kepler, Newton and Gravity 84 Intro to Stars

Newton’s Successful Predictions

• return of Halley’s comet

• discovery of planet Neptune

• binary star systems follow Kepler’s

Laws

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Kepler, Newton and Gravity 85 Intro to Stars

Newton’s Accomplishments

• found the physical interaction between

the Sun and the planets

• revised Kepler’s Third Law so that it

became a tool for calculating masses of

distant objects

• answered the question of how planets move

• made predictions far more accurate than any

before

• physical support for the heliocentric model

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Kepler, Newton and Gravity 86 Intro to Stars

Newton’s Law of Gravitation

Finally, a universal law, that is,

one that is the same for the

heavens and the Earth.

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Kepler, Newton and Gravity 87 Intro to Stars

Escape Speed:

minimum speed an object

must have to break free of

gravity

11 km/sec escape speed from

Earth

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Kepler, Newton and Gravity 88 Intro to Stars

Mass and radius of planet

determines the escape speed.

vescape = 2 Gm

R

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Kepler, Newton and Gravity 89 Intro to Stars

Newton’s Cosmology

cosmology : study of the origin, the nature and

the evolution of the Universe

Universe is infinite in extent

If it were not infinite, but finite, gravitation would

eventually pull all the matter in the Universe back

together => one large mass !

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Kepler, Newton and Gravity 90 Intro to Stars

In an infinite universe, there would be

an infinite number of small blobs of matter.

=> exactly the universe we see !

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Kepler, Newton and Gravity 91 Intro to Stars

One Small Teeny, Tiny Problem

Orbit of Mercury had an unexplained ‘wobble’

41 arcsec per century

Could not be explained with Newton’s physics

Hypothesis of a planet, hidden behind the Sun,

never proved to be true (Vulcan)