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Gravitation and the Waltz of the Planets
Chapter Four
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Guiding Questions
1. How did ancient astronomers explain the motions ofthe planets?
2. Why did Copernicus think that the Earth and the otherplanets go around the Sun?
3. How did Tycho Brahe attempt to test the ideas of
Copernicus?4. What paths do the planets follow as they move aroundthe Sun?
5. What did Galileo see in his telescope that confirmedthat the planets orbit the Sun?
6. What fundamental laws of nature explain the motionsof objects on Earth as well as the motions of theplanets?
7. Why dont the planets fall into the Sun?
8. What keeps the same face of the Moon always pointed
toward the Earth ?
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Ancient astronomers invented geocentric models
to explain planetary motions
Like the Sun and Moon, the planets move on the celestial spherewith respect to the background of stars
Most of the time a planet moves eastward in direct motion, in thesame direction as the Sun and the Moon, but from time to time it
moves westward in retrograde motion
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Ancient astronomers believed the Earth to be at the centerof the universe
They invented a complex system of epicycles and deferentsto explain the direct and retrograde motions of the planets
on the celestial sphere
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Nicolaus Copernicus devised a
comprehensive heliocentric model
Copernicuss heliocentric(Sun-centered) theorysimplified the generalexplanation of planetarymotions
In a heliocentric system,the Earth is one of theplanets orbiting the Sun
The sidereal period of aplanet, its true orbitalperiod, is measured withrespect to the stars
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A planet undergoes retrograde motion as seen
from Earth when the Earth and the planet pass
each other
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A planets synodic period is measured with respect
to the Earth and the Sun (for example, from one
opposition to the next)
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Tycho Brahes astronomical observations provided
evidence for another model of the solar system
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Parallaxapparent difference in position of object
viewed from two different locations
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Johannes Kepler proposed elliptical paths
for the planets about the Sun
Using data collected by TychoBrahe, Kepler deduced three
laws of planetary motion:
the orbits are ellipses
With Sun at one focus
Equal areas in equal times
a planets speed varies as
it moves around its
elliptical orbit
The period squared equalsthe semi-major axis cubed
the orbital period of a
planet is related to the
size of its orbit
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Keplers First Law
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Keplers Second Law
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Keplers Third Law
P2= a3
P = planets sidereal period, in years
a = planets semimajor axis, in AU
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Galileos discoveries with a telescope strongly
supported a heliocentric model
Galileos observationsreported in 1610 the phases of Venus*
the motions of themoons of Jupiter*
mountains on theMoon
Sunspots on the Sun
*observations supportingheliocentric model
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One of Galileos most important discoveries with the telescope was
that Venus exhibits phases like those of the Moon Galileo also noticed that the apparent size of Venus as seen through
his telescope was related to the planets phase
Venus appears small at gibbous phase and largest at crescentphase
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There is a correlation between the phases of Venus and
the planets angular distance from the Sun
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24 15 10
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Geocentric Model Issues
To explain why Venus is neverseen very far from the Sun,the Ptolemaic model had toassume that the deferents ofVenus and of the Sun movetogether in lockstep, with theepicycle of Venus centered ona straight line between theEarth and the Sun
In this model, Venus wasnever on the opposite side ofthe Sun from the Earth, and soit could never have shown thegibbous phases that Galileoobserved
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In 1610 Galileo
discovered four
moons of Jupiter,
also called theGalilean moons or
satellites
This is a page from
his published workin 1610
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Telescope Photograph of Jupiter & the Galilean Moons
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Isaac Newton formulated three laws that describe
fundamental properties of physical reality
Called Newtons Laws ofMotion, they apply to themotions of objects on Earth aswell as in space a body remains at rest, or moves
in a straight line at a constantspeed, unless acted upon by anoutside force the law of inertia
the force on an object is directlyproportional to its mass and
acceleration F = mxa the principle of action and
reaction whenever one body exerts a
force on a second body, thesecond body exerts an equal andopposite force on the first body
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Newtons Law of Universal Gravitation
F = gravitational force between two objectsm1= mass of first object
m2= mass of second object
r = distance between objects
G = universal constant of gravitation
If the masses are measured in kilograms and the distance betweenthem in meters, then the force is measured in Newtons
Laboratory experiments have yielded a value for G of
G = 6.67 1011Newton m2/kg2
Newtons description of gravity accounts for Keplers
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Newton s description of gravity accounts for Kepler s
laws and explains the motions of the planets and
other orbiting bodies
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Orbital Motion
The law of universalgravitation accounts forplanets not falling into theSun nor the Moon crashing
into the Earth Paths A, B, and C do nothave enough horizontalvelocity to escape Earthssurface whereas Paths D,
E, and F do. Path E is where the
horizontal velocity is exactlywhat is needed so its orbitmatches the circular curve
of the Earth
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Orbits follow any one of the family of curves
called conic sections
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A Comet: An Example of Orbital Motion
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Gravitational forces between two objects
produce tides in distant regions of the universe
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Understanding Tidal Forces
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K W d
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Key Words acceleration
aphelion
conic section
conjunction
deferent
direct motion
eccentricity
ellipse
elongation
epicycle
focus force
geocentric model
gravitational force
gravity
greatest eastern and western elongation
heliocentric model
hyperbola inferior conjunction
inferior planet
Keplers laws
law of equal areas
law of inertia
major axis
mass
Neap and spring tides
Newtonian mechanics
Newtons laws of motion
Newtons form of Keplers third law
Occams razor
opposition
parabola
parallax
perihelion period (of a planet)
Ptolemaic system
retrograde motion
semimajor axis
sidereal period
speed
superior conjunction superior planet
synodic period
tidal forces
universal constant of gravitation
velocity