...

Physics 231 Topic 8: Gravitation Wade Fisher October 24-26 2012

by user

on
Category: Documents
16

views

Report

Comments

Transcript

Physics 231 Topic 8: Gravitation Wade Fisher October 24-26 2012
Physics 231
Topic 8: Gravitation
Wade Fisher
October
2012
MSU Physics24-26
231 Fall 2012
1
Clicker Quiz!
3 children are sitting on a rotating disc in a playground.
The disc starts to spin faster and faster.
Which of the three is most likely to start sliding first?
top view
A
B
a)
b)
c)
d)
child A
child B
child C
the same for all three
C
MSU Physics 231 Fall 2012
2
Key Concepts: Gravitation
Newton’s Law of Gravitation
Gravitational Acceleration
Planetary Motion
Kepler’s Laws
Gravitational Potential Energy
Conservation of ME
Artificial Satellites
Covers chapter 9 in Rex & Wolfson
MSU Physics 231 Fall 2012
3
The gravitational force, revisited
Newton:
m1 m2
F G 2
r
G=6.673·10-11 Nm2/kg2
The gravitational force works between every two massive
particles in the universe, yet is the least well understood
force known.
MSU Physics 231 Fall 2012
4
Gravitation between two objects
A
B
The gravitational force exerted by the spherical
object A on B can be calculated by assuming that all
of A’s mass would be concentrated in its center and
likewise for object B.
Conditions: B must be outside of A
A and B must be ‘homogeneous’
MSU Physics 231 Fall 2012
5
Gravitation between two objects
m1m2
F G 2
r
The gravitational force exerted by the spherical
object A on B can be calculated by assuming that all
of A’s mass would be concentrated in its center and
likewise for object B.
The force of the earth on the moon is equal and
opposite to the force of the moon on the earth!
MSU Physics 231 Fall 2012
6
Gravitation between two objects
m1m2
F G 2
r
MSU Physics 231 Fall 2012
7
Gravitational acceleration
m1mEARTH
F G
2
F=mg
r
g=GmEARTH/r2
Radius from Earth’s
Center (km)
Gravitational
Acceleration (m/s2)
Earth’s Surface
6366
9.81
Mount Everest
6366 + 8.85
9.78
Mariana Trench
6366 - 11.03
9.85
Polar Orbit Satellite
6366 + 1600
6.27
Geosynchronous
Satellite
6366 + 36000
0.22
MSU Physics 231 Fall 2012
8
Orbital Velocities
What does the word orbit mean?
An orbit is the gravitationally
curved path of an object around
a point in space.
To orbit the object, you need to
satisfy the kinematic conditions
of that type of orbit (more on
this shortly…)
MSU Physics 231 Fall 2012
9
launch
speed
4 km/s
6 km/s
MSU Physics 231 Fall 2012
8 km/s
10
Gravitational potential energy
So far, we used: PEgravity=mgh Only valid for h near
earth’s surface.
More general: PEgravity=-GMEarthm/r
PE=0 at infinite distance from the center of the earth (r=∞)
Earlier we noted that we could define the zero of
PEgravity anywhere we wanted. So the surface of
the earth is as good as anywhere!
PE1  G
R2
R1
mEARTH
m
R1
mEARTH
PE2  G
m
R2
MSU Physics 231 Fall 2012
R1<R2
Thus…
PE1 < PE2
11
Gravitational potential energy
So far, we used: PEgravity=mgh Only valid for h near
earth’s surface.
More general: PEgravity=-GMEarthm/r
PE=0 at infinite distance from the center of the earth (r=∞)
Earlier we noted that we could define the zero of
PEgravity anywhere we wanted. So the surface of
the earth is as good as anywhere!
R2=R1+h
R2
R1
PE2  PE1  G
mEARTH
m
m  (G EARTH m)
R2
R1
mEARTH
mEARTH
 G
m  (G
m)
( R1  h)
R1
 mEARTH
1
1
 mGmEARTH ( 
)  m G
2
R1 R1  h
R
1

MSU Physics 231 Fall 2012

h  mgh

12
Gravitational potential energy
So far, we used: PEgravity=mgh Only valid for h near
earth’s surface.
More general: PEgravity=-GMEarthm/r
PE=0 at infinite distance from the center of the earth (r=∞)
Example: escape speed (a.k.a. second cosmic speed )
what should the minimum initial velocity of a rocket be if
we want to make sure it will not fall back to earth?
MSU Physics 231 Fall 2012
13
Some definitions
First cosmic speed: speed of a satellite on a low-lying circular orbit
(rsatellite ≈ rplanet):
Msg = Msv2/r so v1 =(gr) where g = Gmplanet/rp2
For earth:
g=9.81 m/s2 r=6.366x106 m
v1=7.91x103 m/s
Second cosmic speed: speed needed to break free from a planet:
v1 =(2GMp/Rp) = (2gr)
For earth:
g=9.81 m/s2 r=6.366x106 m
v2=1.12x104 m/s
Synchronous orbit of a satellite: rotation period of satellite is the same
as rotation period of the planet
For earth: period T = 24 hours
Angular speed
 = 2/(243600) = 7.27x10-5 rad/s
For earth what is its radius?
Use Fg=mac so Gmearthmsat/r2 = msat2r (note rrearth !)
So r3=Gme/2
r=(Gme/2)1/3 = 3.54x107 = 35400 km
MSU Physics 231 Fall 2012
14
launch speed = 10 km/s
MSU Physics 231 Fall 2012
15
Clicker Quiz! Earth and Moon
a) one quarter
If the distance to the Moon were
b) one half
doubled, then the force of attraction
c) the same
between Earth and the Moon would be:
d) two times
e) four times
MSU Physics 231 Fall 2012
16
Kepler’s laws
Johannes Kepler
(1571-1630)
MSU Physics 231 Fall 2012
17
Kepler’s First law
Eccentricity: e
c
b
e   1  
a
a
2
An object A bound to another object B by a force that goes
with 1/r2 moves in an elliptical orbit around B, with B being
in one of the focus point of the ellipse.
MSU Physics 231 Fall 2012
18
Kepler’s First law
p+q = constant
An object A bound to another object B by a force that goes
with 1/r2 moves in an elliptical orbit around B, with B being
in one of the focus point of the ellipse.
MSU Physics 231 Fall 2012
19
PEgravity=-GMEarthm/r
Kepler’s second law
Area(D-C-SUN)=Area(B-A-SUN)
Potential energy is maximal,
Kinetic energy is minimal
Potential energy is close to
0 here, but still negative
Potential energy is minimal, kinetic energy is maximal
(potential energy is very negative here)
A line drawn from the sun to the elliptical orbit of a planet
sweeps out equal areas in equal time intervals.
MSU Physics 231 Fall 2012
20
Kepler’s third law
Consider a planet in circular motion around the sun:
G
M sun M planet
r
2

M planet v 2planet
r
s 2r
v

t
T
 4 2  3
2
r  K s r 3
T  
 GM sun 
T2
 Ks
3
r
K s  2.97 10 19 s 2 / m 3
r3
C
2
T
C  3.36 1018 m 3 / s 2
MSU Physics 231 Fall 2012
21
Kepler’s third law
Consider a planet in circular motion
around the sun:
r3
r3
C
2
T
C  3.36 1018 m3 / s 2
T2
r3=C T2
r3=constantT2
T: period-time it takes to make
one revolution
If the orbit is an ellipse, replace r with a, the semi-major axis.
a=(half the sum of the smallest and greatest distance from the sun)
MSU Physics 231 Fall 2012
22
An Example
star
A
Two planets are orbiting a star.
B The orbit of A has a radius of 108 km.
The distance of closest approach of B
to the star is 5x107 km and its
maximum distance from the star is 109
km. If A has a rotational period of 1
year, what is the rotational period of
B?
MSU Physics 231 Fall 2012
23
An Example
star
A
Two planets are orbiting a star. The
B orbit of A has a radius of 108 km. The
distance of closest approach of B to
the star is 5x107 km and its maximum
distance from the star is 109 km. If A
has a rotational period of 1 year, what
is the rotational period of B?
MSU Physics 231 Fall 2012
24
Clicker Quiz! Averting Disaster
a) it’s in Earth’s gravitational field
The Moon does
b) the net force on it is zero
not crash into
c) it is beyond the main pull of Earth’s gravity
Earth because:
d) it’s being pulled by the Sun as well as by
Earth
e) its velocity is large enough to stay in orbit
MSU Physics 231 Fall 2012
25
For Next Week
Chapter 10:
Solids and Fluids
Homework Set 8
Due Wednesday Nov 2!
MSU Physics 231 Fall 2012
26
Fly UP