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Models of the Solar System

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Models of the Solar System Positions of planets change, whereas stars appear relatively fixed Greeks held on to the Geocentric model because they could not ... – PowerPoint PPT presentation

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Title: Models of the Solar System


1
Models of the Solar System
  • Positions of planets change, whereas stars
    appear relatively fixed
  • Greeks held on to the Geocentric model because
    they could not observe stars to change their
    positions, and therefore thought that the earth
    must be stationary
  • Ptolemy, Aristotle and others refined the
    geocentric model
  • But there were problems.such as the path
    reversal by Mars ? Retrograde motion

2
Retrograde motion of Mars(path reversal seen in
the Sky)
3
Epicycles Ptolemic Geocentric Model
4
How do we know the Earth is spherical ?
  • Stars differ from place to place
  • Northern and southern hemispheres
  • What kind of an object always has a round shadow ?

5
Earth Shadow during Lunar Eclipse
Multiple Exposure Photograph
6
Cyrene
Syene
Tropic of Cancer
7
The Spherical Earth
  • The ancient Greeks had deduced not only that the
    Earth is spherical but also measured its
    circumference !

8
Eratostheness method to measure the
circumference of the earth

At noon on summer solstice day the Sun is
directly overhead at Syene, but at an angle of 7o
at Alexandria
  • Distance (Alexandria - Syene)
  • -- ---------------------------------------
  • 360 Circumference of the Earth

Sunlight
Alexandria
Answer 40,000 stadia 25,000 mi !
Syene
Earth
9
Earth-Moon-Sun GeometryAristarchuss
determination of distances(Closer the S-E-M
angle to 90, the farther the Sun)
If we replace the moon with a planet, then can
determine relative distances, as done by
Copernicus
10
Copernicus
11
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12
Copernican ModelInferior and Superior
Planets(orbits inside or outside the Earths
orbit)

13
Configurations of Inferior Planets, Earth, and
the Sun
Earth
14
Configurations of Superior Planets, Earth, and
the Sun
Opposition
Conjunction
Earth
Synodic (apparent) period one conjunction to
next (or one opposition to next)
15
Synodic and Sidereal Orbital Periods
  • Inferior planets are never at opposition
    superior planets can not be at inferior
    conjunction
  • Copernican model of orbital periods
  • Synodic period is the apparent orbital period of
    a planet, viewed from the earth, when the
    earth-planet-sun are in successive conjunction or
    opposition
  • Sidereal (with respect to stars) period is the
    real orbital period around the Sun
  • Synodic periods of outer planets (except Mars)
    are just over one year

16
Apparent (Synodic) and true (Sidereal with
respect to stars) orbital periods of planets
differ due to Earths relative motion
Synodic periods of all outer planets (except
mars) are just over 1 year because their Sidereal
periods are very long and they are in opposition
again soon after an earth-year
17
Earth-Venus-Sun
Inferior planets appear farthest away from the
Sun at greatest elongation
18
Measurements of Distances to Planets
Angle of max elongation
P-E-S
P
90 deg
Earth
P-E-S
E
S
Sin (P-E-S) PS / ES ES 1 AU
19
Copernicus first determined the relative
distances of planets
20
Copernican Heliocentric Model(Retrograde motion
of Mars seen when Earth overtakes Mars
periodically)
Earth is closer to the Sun, therefore moves
faster than Mars
21
Tycho The most accurate pre-telescopic observer
Tycho charted very accurately the movement of
Mars in the Sky, but still believed In the
Geocentric Universe
22
Kepler Tychos assistant(used Tychos data to
derive Keplers Laws)
23
Planetary Orbits
  • The Copernican heliocentric model is essentially
    correct
  • But it consisted of circular orbits which did not
    exactly fit observations of planetary positions
  • Kepler realized, based on Tychos data of the
    orbit of Mars, that orbits are elliptical ?
    Keplers First Law
  • However, the difference for Mars is tiny, to
    within the accuracy of drawing a circle with a
    thick pen !

24
Keplers First LawAll planetary orbits are
elliptical, with the Sun at one focus
25
Eccentricity ee distance between foci/major
axis AB / ab
a
A
B
b
A circle has e 0, and a straight line has e
1.0
26
Keplers Second LawPlanetary radius sweeps
equal area triangles in equal time
It follows that the velocity of the planet must
vary according to distance from the Sun --
fastest at Perihelion and slowest at Aphelion
27
Keplers Third Law P2 a3P Orbital Period, a
semi-major axis
What is the size a of the orbit of a comet with
the period P of 8 years?
28
Keplers Laws
  • Empirically derived from observational data
    largely from Tycho (e.g. observations of the
    positions of Mars in its orbit around the Sun)
  • Theoretical explanation had to await Newtons
    discovery of the Law of Gravitation
  • Universally valid for all gravitationally
    orbiting objects (e.g. stars around black holes
    before falling in)

29
Galileo
30
Galileos Discoveries With Telescope
  • Phases of Venus
  • - Venus displays phases like the Moon as it
    revolves around the Sun
  • Mountains and seas on the Moon
  • - Other objects in the sky are like the
    Earth (not therefore special)
  • Milky Way is made of stars like the Sun
  • Sunspots
  • - Imperfections or blemishes in
    otherwise perfect heavenly objects
  • 4 Galilean satellites of Jupiter
  • - Objects in the sky revolve around other
    objects, not the Earth (i.e. other moons)
  • All of these supported the Copernican System
  • Galileo also conducted experiments on
    gravity
  • Regardless of mass or weight objects fall at
    the same rate

31
Phases of Venus
Venus is never too far from the Sun, therefore
can not be in opposition like the Moon. Changing
phases of Venus demonstrate that it orbits the
Sun like the Earth.
32
Orbits and Motions
  • Orbits can not be circular since objects do NOT
    revolve around each other, but around their
    common center-of-mass
  • The Earth and the Moon both revolve around each
    other
  • This motion is in addition to Earths Rotation,
    Revolution, Precession

33
The Earth-Moon Barycenter
  • The earth and the moon both revolve around a
    common center of mass called the Barycenter
  • The barycenter of Sun-planet systems lies inside
    the Sun
  • As the earth is much more massive, the barycenter
    lies 1700 Km inside the earth
  • Calculate its position O from
  • M(E) x EO M (M) x MO

M
E
O
34
Gravity
  • Galileos observations on gravity led to Newtons
    Law of Gravitation and the three Laws of Motion
  • Objects fall at the same rate regardless of mass
    because more massive objects have more inertia or
    resistance to motion
  • Fgrav G (m1 x m2) / r2
  • Force of gravity between two masses is
    proportional to the product of masses divided by
    distance squared ? inverse square law

35
Newton Three Laws of Motion
  1. Inertia
  2. F ma
  3. Action Reaction

36
Newtons Laws of Motion
  • Law of Inertia A body continues in state of
    rest or motion unless acted on by an external
    force Mass is a measure of inertia
  • Law of Acceleration For a given mass m, the
    acceleration is proportional to the force applied
  • F m a
  • Law of Action equals Reaction For every action
    there is an equal and opposite reaction momemtum
    (mass x velocity) is conserved

37
Velocity, Speed, Acceleration
  • Velocity implies both speed and direction speed
    may be constant but direction could be changing,
    and hence accelerating
  • Acceleration implies change in speed or
    direction or both
  • For example, stone on a string being whirled
    around at constant speed direction is constantly
    changing therefore requires force

38
Ball Swung around on a String
Same Speed, (in uniform circular motion) Changing
Direction (swinging around the circle)
39
Donut Swung around on a String
40
Conservation of momemtumaction equal reaction
  • The momemtum (mv) is conserved before and after
    an event
  • Rocket and ignited gases
  • M(rocket) x V(rocket) m(gases) x v(gases)
  • Two billiard balls
  • m1 v1 m2 v2 m1 v1 m2 v2
  • v1,v2 velocities before collision
  • v1,v2 velocities after collision
  • Example you and your friend (twice as heavy)
    on ice!

41
Action Reaction
Equal and Opposite Force from the Table
Net Force is Zero, No Net Motion
42
Acceleration due to gravity
  • Acceleration is rate of change of velocity,
    speed or direction of motion, with time ? a v/t
  • Acceleration due to Earths gravity a ? g
  • g 9.8 m per second per second, or 32 ft/sec2
  • Speed in free-fall
  • T (sec) v (m/sec) v
    (ft/sec)
  • 0 0
    0
  • 1 9.8
    32
  • 2 19.6
    64
  • 3 29.4
    96
  • 60 mi/hr 88 ft/sec (between 2 and 3
    seconds)

43
Galileos experiment revisited
  • What is your weight and mass ?
  • Weight W is the force of gravity acting on a
    mass m causing acceleration g
  • Using F m a, and the Law of Gravitation
  • W m g G (m MEarth) /R2
  • (R Radius of the Earth)
  • The mass m of the falling object cancels out
    and does not matter therefore all objects fall
    at the same rate or acceleration
  • g GM / R2
  • i.e. constant acceleration due to gravity
    9.8 m/sec2

44
Galileos experiment on gravity
  • Galileo surmised that time differences between
    freely falling objects may be too small for human
    eye to discern
  • Therefore he used inclined planes to slow down
    the acceleration due to gravity and monitor the
    time more accurately

v
Changing the angle of the incline changes the
velocity v
45
g on the Moon
  • g(Moon) G M(Moon) / R(Moon)2
  • G 6.67 x 10-11 newton-meter2/kg2
  • M(Moon) 7.349 x 1022 Kg
  • R(Moon) 1738 Km
  • g (Moon) 1.62 m/sec/sec
  • About 1/6 of g(Earth) objects on the Moon
    fall at a rate six times slower than on the Earth

46
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47
Escape Velocity and Energy
  • To escape earths gravity an object must have
    (kinetic) energy equal to the gravitational
    (potential) energy of the earth
  • Kinetic energy due to motion
  • K.E. ½ m v2
  • Potential energy due to position and force
  • P.E. G m M(Earth) / R
  • (note the similarity with the Law of
    Gravitation)
  • Minimum energy needed for escape K.E. P.E.
  • ½ m v2 G m M / R
  • Note that the mass m cancels out, and
  • v (esc) 11 km/sec 7 mi/sec 25000 mi/hr
  • The escape velocity is the same for all
    objects of mass m

48
Object in orbit ? Continuous fall !
Object falls towards the earth at the same rate
as the earth curves away from it
49
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50
Angular Momentum
Conservation of angular momentum says that
product of radius r and momentum mv must be
constant ? radius times rotation rate (number of
rotations per second) is constant
51
Angular Momentum
  • All rotating objects have angular momentum
  • L mvr acts perpendicular to the plane of
    rotation
  • Examples helicopter rotor, ice skater, spinning
    top or wheel (experiment)
  • Gyroscope (to stabilize spacecrafts) is basically
    a spinning wheel whose axis maintains its
    direction slow precession like the Earths axis
    along the Circle of Precession

52
Conservation of Angular Momentum
  • Very important in physical phenomena observed in
    daily life as well as throughout the Universe.
    For example,
  • Varying speeds of planets in elliptical orbits
    around a star
  • Jets of extremely high velocity particles, as
    matter spirals into an accretion disc and falls
    into a black hole

53
Relativistic1 Jet From Black Hole
1. Relativistic velocities are close to the
speed of light
54
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