Ch. 8 Universal Gravitation Part 1: Kepler`s Laws

advertisement
Ch. 8
Universal
Gravitation
Objectives: Section 8.1
Motion in the Heavens and on Earth
Part 1:
Kepler’s Laws
Johannes Kepler
Johannes Kepler (1571-1630) was an
assistant to the Danish astronomer Tycho
Brahe.
 Kepler was convinced that geometry and
mathematics could be used to explain the
motion of the planets. Unlike Brahe, he
used a heliocentric model.


Objectives
 Relate
Kepler’s laws of planetary motion to
Newton’s law of universal gravitation.
 Calculate the periods and speeds of orbiting
objects.
 Describe the method Cavendish used to
measure G and the results of knowing G.
Tycho
Brahe
I spent 26 years
making star charts
using this quadrant
and no telescope.
Kepler’s Laws
Johannes Kepler discovered 3 laws from the
motion of the planets as mapped by Tycho
Brahe
1.
2.
3.
I thought the sun
went around the
Earth and the
planets went
around the Sun.
Planetary orbits are elliptical not circular
Orbits sweep out equal areas in equal times
T2/r3 = k where k = “constant”
constant”
I used Tycho Brahe’s
data to come up with my
laws. It took him 20
years to collect it.
1
Kepler’s 1st Law
Kepler’s 1st Law
1. The orbits of the planets are ellipses, with
the sun at one focus.
(Law of Ellipses)
Orbits are ellipses
The Sun is at one
of the foci
The closer the planets
are to one another,
the more circular the
orbit.
Kepler’s 2nd Law
Kepler’s 2nd Law
2.
2. An imaginary line drawn from the center
of the sun to the center of the planet will
sweep out equal areas in equal intervals of
time.
(Law of Equal Areas)
Deals with speed…
faster when closer
to the sun.
Kepler’s 3rd Law
3. The ratio of the squares of the periods of
any two planets is equal to the ratio of the
cubes of their average distances from the
sun.
(Law of Harmonies)
Orbits sweep out equal areas in equal times
The Sun is at one
of the foci
Kepler’s 3rd Law
T2/r3 = k where k = “constant”
constant”
T = the period for 1 revolution
r = the average radius of the elliptical orbit
So for every orbiting body everywhere, this
ratio is true
(TA/TB)2 = (rA/rB)3
2
Universal Gravitation
Part 2:
Universal
Gravitation

Isaac Newton
 24yrs
old…
an apple fall to the ground made
him wonder if gravity extended beyond Earth
 Developed a theory of universal gravitation
 Attractive force between two objects
 Watching


Law of Universal Gravitation

The force of attraction between any two
masses is constant throughout the
universe
Sec. 8.2
Using the Law of Universal
Gravitation

m m 
F  G A 2 B 
 d 
problems involving orbital speed and
period
 Relate weightlessness to objects in free fall
 Distinguish between inertia mass and
gravitational mass
 Contrast Newton’s and Einstein’s views about
gravitation
6.67 x 10-11 N·m2/kg2

If a projectile moves fast enough, it falls at
the same rate that the Earth curves
Objectives
 Solve
G is a universal gravitational constant
between two masses
Satellite Motion
The apple was also attracting the Earth
Proposed Law of Universal Gravitation
How fast are satellites moving?

F = ma or F = mv2/r
(ac = v2/r)

F = G(mAmB/d2)
Solve for velocity? Set them equal to each
other
 G(mAmB/d2) = mv2/r
which gives you….

3
Period of a Satellite Circling Earth
r3
T  2
GmE
or if we know the velocity…
T
2 r
v
Universal Law of Gravitation
History Outline
1. Kepler used Brahe’
Brahe’s data to make Kepler’
Kepler’s
Laws
2. Newton derived the universal law using
Keplers Laws
3. Newton proved his law using the apple and
the moon
4. Cavendish measures the universal constant
Universal Law of Gravitation
Newton derived the universal law of gravity
He knew:
a) T2/r3 = k
b) v = 2
2r/T
c) F = mv2/r
Weightlessness
What is gravity in outer space?
 Where space shuttle orbits…g = 8.7m/s2
 How come astronauts
are “floating” then?


g = F/m
Universal Law of Gravitation
History Outline
1. Kepler used Brahe’
Brahe’s data to make Kepler’
Kepler’s
Laws
a) Measured the motion of the
stars and planets
b) Planets move from year to
year but stars stay put
c) Kepler developed laws to
explain the motion of the
planets
Universal Law of Gravitation
Newton derived the universal law of gravity
He knew:
a) T2/r3 = k
b) v = 2r/T
c) F = m( v )2
r
4
Universal Law of Gravitation
Newton derived the universal law of gravity
He knew:
F = m42r
a) T2/r3 = k
T2
b) v =
F = m42r
c) F = m (2r/T )2
r3k
r
F=
m42r2
F = 42 m
T 2r
k
Universal Law of Gravitation
Newton derived the universal law of gravity
He knew:
F = 42 m
k
But once he got to this part, he
realized that every action had
an equal and opposite reaction
so, he had to add another “m”
r2
F=G
r2
m1
m2
r2
Universal Law of Gravitation
F = Gm1m2
r2
F = the force of gravity between 2 objects
Universal Law of Gravitation
“G” was not known but the equation was still
proven by the comparison of an apple and the
Moon.
m1 = mass of object #1
m2 = mass of object #2
Newton thought that maybe the
Moon moved through the heavens
for the same reason apples fell to
the ground
r = distance between their centers of mass
G = Universal Gravitational Constant
Universal Law of Gravitation
If F = Gm1m2
r2
Then if F = ma then
m1a = Gm1m2
r2
So,
a = Gm2
r2
a = Gme
r2
This equation works for
any mass attracted to
the Earth
Universal Law of Gravitation
60re
a = Gme
r2
a=
9.81m/s2
re
for an apple
Since the Moon is 60x further away
rmoon = 60re
So, a = Gme
(60re )2
amoon = Gme amoon = aapple
3600
3600re 2
5
Universal Law of Gravitation
Universal Law of Gravitation
amoon = .0027m/s2 according to the formula
a = v2
The real acceleration of the Moon can be
measured:
a = v2
v = 2
2r/T
T = 28.5days = 28.5x24x60x60 = 2462400s
r = 60re = 60x 6.4x106m = 384000000m
re = 6.4x106m
r
v = 2
2r/T
T = 28.5days
r = 60re
Universal Law of Gravitation
r
Universal Law of Gravitation
a = v2
a = v2 = (980m/s)2/384000000m = .0025m/s2
v = 2
2r/T
v = 2
384000000m) / (2462400s) =980m/s
2384000000m)
v = 2
2r/T
v = 2
384000000m) / (2462400s) =980m/s
2384000000m)
T = 28.5days = 28.5x24x60x60 = 2462400s
r = 60re = 60x 6.4x106m = 384000000m
re = 6.4x106m
T = 28.5days = 28.5x24x60x60 = 2462400s
r = 60re = 60x 6.4x106m = 384000000m
re = 6.4x106m
r
Universal Law of Gravitation
a = v2 = (980m/s)2/384000000m = .0025m/s2
r
The real acceleration of the Moon = .0025m/s2
The theoretical acceleration
= .0027m/s2
r
Universal Law of Gravitation
1. Cavendish measures the universal constant
A. “G” was still unknown for 100years
B. Cavendish figured it out using a Torsion Balance
This was so close that this became well accepted
and Newton went down in history as the one
who “discovered”
discovered” gravity
6
Universal Law of Gravitation
Torsion Balance
1. Imagine twisting the thread
around 100 times
Universal Law of Gravitation
Torsion Balance
2. Then let go
2. Then let go
3. The system would spin in
the opposite direction
3. The system would spin in
the opposite direction
Universal Law of Gravitation
Torsion Balance
1. Now imagine the force that
pulls the bar back
Universal Law of Gravitation
Torsion Balance
2. The force of a twisted wire
is called torsion
3. Attach a spring scale to the
bar and measure this torsion
force
F
Universal Law of Gravitation
Torsion Balance
F
1. Imagine twisting the thread
around 100 times
7. The force of a twist of 1/60th
of a degree =
.0144N / (100)(360)(60) =
0.00000000667N
F
4. The force he measured was
.0144N
5. Now he has to figure out
how much torsion a tiny
fraction of a twist would
make.
6. If he twisted the string 1/60th
of 1 degree, the force on the
scale would be 100times
360 times 60 times smaller.
Universal Law of Gravitation
8.
He used a mirror
attached to the string to
reflect a beam of light
onto a far away wall.
9.
He used this to measure
the angle the string had
twisted
Each marking measured 1/60th
of a degree
7
Universal Law of Gravitation
10.
11.
Universal Law of Gravitation
He then placed a 1 kg
ball at each end of the
bar
Next, he placed 1kg
masses on the table
near the masses on the
bar
12.
13.
14.
15.
Universal Law of Gravitation
He let go.
The force of gravity
twisted the string
2/60th’s of a degree.
The masses stopped
moving.
The force of gravity
between the masses =
the torsion in the string
Universal Law of Gravitation
Top View
12.
13.
14.
15.
He let go.
The force of gravity
twisted the string
2/60th’s of a degree.
The masses stopped
moving.
The force of gravity
between the masses =
the torsion in the string
Torsion Force
Fg
16.
There were 2 forces from
the two sets of balls
17.
Total Torsion Force = 2Fg
18.
The total angle it twisted
was 2/60th’s of a degree
Fg
Torsion Force
Universal Law of Gravitation
Top View
16. Torsion Force =
Universal Law of Gravitation
Top View
22. m1
=
=
=
24. r
25. Fg =
0.00000000667N x 2 =
0.00000001334N
23. m2
Torsion Force
20. 2Fg = 0.00000001334N
m1 = 1.0kg
Fg
21. Fg = 0.00000000667N
7x1
r = .10m
Fg =
6.6
Fg
0 -9 N
Torsion Force
m2 = 1.0kg
1.0kg
1.0kg
.10m
0.00000000667N
26. Fg
= Gm1m2
r2
27. G =
Fg r2
m1m2
G = 6.67 x 10-11 Nm2
kg2
8
Universal Law of Gravitation
F = Gm1m2
r2
F = the force of gravity between 2 objects
m1 = mass of object #1
m2 = mass of object #2
Here’s a sketch of the
Experiment from
Cavendish’s time
r = distance between their centers of mass
G = Universal Gravitational Constant
G = 6.67 x 10-11 Nm2
kg2
Sample Problems
1.
No matter how much you say you don’
don’t find
someone attractive, the fact is, that all people
are at least gravitationally attractive. If you
have a mass of 70kg and the other person has
a mass of 80kg, what is the force of
gravitational attraction between you both
when you are sitting .50m apart?
Sample Problem

No matter how much you say you don’
don’t find someone attractive, the fact is, that all
people are at least gravitationally attractive. If you have a mass
mass of 70kg and the
other person has a mass of 80kg, what is the force of gravitational
gravitational attraction
between you both when you are sitting .50m apart?
Fg = ?
m1 = 70kg
m2 = 80kg
Fg
r = .50m
G = 6.67 x 10-11 Nm2
kg2
9
Homework
How the stars and planets move
 Pg 242 # 11-3
 Pg 247 #3a,c, 5
North Pole
Stars move in a circle as the
Earth rotates on its axis every
night.
How the stars and planets move
How the stars and planets move
Also, the stars move from
season to season through
the year
 So to explain the motion of the stars, Moon
and Sun you need to measure their positions at
a certain time of day or night
10am
9am
11am
12am
1pm
Night
2pm
Day
8am
3pm
7am
4pm
Summer night sky
6am
Winter night sky
5pm
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
10
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Every year, at the same
time, on the same day, the
stars are in the same
position they were last
year.
Night
Summer night sky
Winter night sky
12am 1/22/07
Day
Winter night sky
11
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
How the stars and planets move
Summer night sky
Winter night sky
12
How the stars and planets move
How the stars and planets move
Mars
Summer night sky
Winter night sky
How the stars and planets move
12am 1/22/08
Winter night sky
How the stars and planets move
There are celestial objects
that don’t stay in the same
place – they wander.
These are called
“wanderers”, or in Greek,
“Planets”.
12am 2/5/08
Winter night sky
Winter night sky
How the stars and planets move
There are celestial objects
that don’t stay in the same
place – they wander.
These are called
“wanderers”, or in Greek,
“Planets”.
12am 2/12/08
Winter night sky
How the stars and planets move
There are celestial objects
that don’t stay in the same
place – they wander.
These are called
“wanderers”, or in Greek,
“Planets”.
12am 1/29/08
There are celestial objects
that don’t stay in the same
place – they wander.
These are called
“wanderers”, or in Greek,
“Planets”.
There are celestial objects
that don’t stay in the same
place – they wander.
These are called
“wanderers”, or in Greek,
“Planets”.
12am 2/19/08
Winter night sky
13
How the stars and planets move
How the stars and planets move
There are celestial objects
that don’t stay in the same
place – they wander.
These are called
“wanderers”, or in Greek,
“Planets”.
Astronomers tried to
explain the moving objects.
At first, they thought these
planets were like the Sun
and the Moon.
They thought the planets
orbited around the Earth in
a circle
12am 2/26/08
Winter night sky
12am 3/5/08
Winter night sky
14
Download