Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the...

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Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws

Transcript of Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the...

Page 1: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Chapter 2: The Copernican RevolutionThe Birth of Modern Science

•Ancient Astronomy

•Models of the Solar System

•Laws of Planetary Motion

•Newton’s Laws– Laws of Motion– Law of Gravitation

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The universe is full of magical things, patiently waiting for our wits to grow sharper.

Eden Philpotts

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Cosmology: study of the structure and evolution of the

universe

• Ancient civilizations universe = solar system + fixed stars

• Today universe = totality of all space, time,

matter and energy

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There are three principle means of acquiring knowledge…….

observation of nature,reflection, andexperimentation.

Observation collects facts;reflection combines them;experimentation verifies the result of that combination.

Denis Diderot (1713 - 1784)

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Scientific Method

Gather data

Form theory

Test theory

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Astronomy in Ancient Times

• Ancient people had a better, clearer chance to study the sky and see the patterns of stars (constellations) than we do today.

• Drew pictures of constellations; created stories to account for the figures being in the sky.

• Used stars and constellations for navigation.

• Noticed changes in Moon’s shape and position against the stars.

• Created accurate calendars of seasons.

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Ancient AstronomyStonehenge on the summer solstice.

As seen from the center of the stone circle,

the Sun rises directly over the "heel stone" on the longest day of the year.

The Big Horn Medicine Wheel in Wyoming,

built by the Plains Indians. Its spokes and rock piles are aligned with the rising and setting of the Sun and other

stars.

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Astronomy in Early Americas• Maya Indians developed

written language and number system.

• Recorded motions of Sun, Moon, and planets -- especially Venus.

• Fragments of astronomical observations recorded in picture books made of tree bark show that Mayans had learned to predict solar and lunar eclipses and the path of Venus.

• One Mayan calendar more accurate than those of Spanish.

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Ancient Contributions to Astronomy• Egyptians

– recorded interval of floods on Nile• every 365 days

– noted Sirius rose with Sun when floods due– invented sundials to measure time of day from

movement of the Sun.

• Babylonians– first people to make detailed records of movements

of Mercury, Venus, Mars, Jupiter, Saturn• only planets visible until telescope

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Greek Astronomy

• Probably based on knowledge from Babylonians.

• Thales predicted eclipse of Sun that occurred in 585 B.C.

• Around 550 B.C., Pythagoras noted that the Evening Star and Morning Star were really the same body (actually planet Venus).

• Some Greek astronomers thought the Earth might be in the shape of a ball and that moonlight was really reflected sunlight.

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Time Line• Ancient Greeks

– Pythagoras 6th century B.C.

– Aristotle 348-322 B.C.

– Aristarchus 310-230 B.C.

– Hipparchus ~130 B.C.

– Ptolemy ~A.D. 140

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Pythagorean Paradigm

• The Pythagorean Paradigm had three key points about the movements of celestial objects:

– the planets, Sun, Moon and stars move in perfectly circular orbits;

– the speed of the planets, Sun, Moon and stars in the circular orbits is perfectly uniform;

– the Earth is at the exact center of the motion of the celestial bodies.

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Aristotle’s Universe:A Geocentric Model

• Aristotle proposed that

–the heavens were literally composed of concentric, crystalline spheres

–to which the celestial objects were attached

–and which rotated at different velocities,

–with the Earth at the center (geocentric).

The figure illustrates the ordering of the spheres to which the Sun, Moon, and visible planets were attached.

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Planetary Motion• From Earth, planets appear to move wrt fixed stars and vary greatly in brightness.

• Most of the time, planets undergo direct motion - moving W to E relative to background stars.

• Occasionally, they change direction and temporarily undergo retrograde motion - motion from E to W -before looping back.

(retrograde-moveretrograde-move)

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Planetary Motion: Epicycles and Deferents

•Retrograde motion was first explained as follows:

•the planets were attached, not to the concentric spheres themselves, but to circles attached to the concentric spheres, as illustrated in the adjacent diagram.

•These circles were called "Epicycles",and the concentric spheres to which they were attached were termed the "Deferents".

• (epicycle-moveepicycle-move)

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Motions of Mercury and Venus• Mercury and Venus exhibit a special motion,

not observed in the other planets.

– They always remain close to the Sun, first moving away from it,then pausing, and then moving toward it.

– Venus and Mercury can be seen in the morning and evening skies, but never at midnight (except in polar latitudes).

– Venus never gets >48o from the Sun; Mercury more distant than 28o.

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Epicycles, Deferents, and the Orbits of Mercury and Venus

Special features of the orbits of Mercury and Venus modeled by requiring that the center of the epicycle of the planet be firmly attached to the line joining the Earth and Sun.

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Epicycle/Deferent ModificationsIn actual models, the center of the epicycle moved with uniform circular motion, not around the center of the deferent, but around a point that was displaced by some distance from the center of the deferent.

This modification predicted planetary motions that more closely matched the observed motions.

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Further Modifiations• In practice, even this was not

enough to account for the detailed motion of the planets on the celestial sphere!

• In more sophisticated epicycle models further "refinements" were introduced:

In some cases, epicycles were themselves placed on epicycles, as illustrated in the adjacent figure.

The full Ptolemaic model required 80 different circles!!

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Ptolemy• 127-151 A.D. in Alexandria

• Accomplishments– completion of a “geocentric” model of solar system

that accurately predicts motions of planets by using combinations of regular circular motions

– invented latitude and longitude (gave coordinates for 8000 places)

– first to orient maps with NORTH at top and EAST at right

– developed magnitude system to describe brightness of stars that is still used today

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Aristarchus• 310-230 B.C.

• Applied geometry to find – distance to Moon

• Directly measure angular diameter

• Calculate linear diameter using lunar eclipse

– relative distances and sizes of the Sun and Moon• ratio of distances to Sun and Moon by observing angle

between the Sun and Moon at first or third quarter Moon.

• Proposed that the Sun is stationary and that the Earth orbits the Sun and spins on its own axis once a day.

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Hipparchus• ~190-125 B.C.

• Often called “greatest astronomer of antiquity.”

• Contributions to astronomy– improved on Aristarchus’ method for calculating the

distances to the Sun and Moon,– improved determination of the length of the year,– extensive observations and theories of motions of the

Sun and Moon,– earliest systematic catalog of brighter stars ,– first estimate of precession shift in the vernal equinox.

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Time Line• Ancient Greeks

– Pythagoras 6th century B.C.

– Aristotle 348-322 B.C.

– Aristarchus 310-230 B.C.

– Hipparchus ~130 B.C.

– Ptolemy ~A.D. 140

• Dark Ages A.D. 5th - 10th century– Arabs translated books, planets positions

– China 1054 A.D. supernova; Crab Nebula

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Heliocentric Model - Copernicus• In 1543, Copernicus proposed

that: the Sun, not the Earth, is the center of the solar system.

• Such a model is called a heliocentric system.

• Ordering of planets known to Copernicus in this new system is illustrated in the figure.

• Represents modern ordering of planets.

• (copernican-move)

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Stellar Parallax• Stars should appear to

change their position with the respect to the other background stars as the Earth moved about its orbit.

• In Copernicus’ day, no stellar parallax was observed, so the Copernican model was considered to be only a convenient calculation tool for planetary motion.

• In 1838, Friedrich Wilhelm Bessel succeeded in measuring the parallax of the nearby, faint star 61 Cygni. ( penny at 4 miles)

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• Ancient Greeks Pythagoras 6th century B.C. Aristotle 348-322 B.C. Aristarchus 310-230 B.C. Ptolemy ~A.D. 140

• Dark Ages A.D. 5th - 10th century• Renaissance Copernicus

(1473-1543) Tycho Brahe Kepler Galileo (1546-1601) (1571-1630) (1564-1642)

Newton (1642-1727)

Time Line

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Galileo Galilei

• Galileo used his telescope to show that Venus went through a complete set of phases, just like the Moon.

• This observation was among the most important in human history, for it provided the first conclusive observational proof that was consistent with the Copernican system but not the Ptolemaic system.

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Galileo and Jupiter

• Galileo observed 4 points of light that changed their positions with time around the planet Jupiter.

• He concluded that these were objects in orbit around Jupiter.

• Galileo called them the Medicea Siderea-the “Medician Stars” in honor of Cosimo II de'Medici, who had become Grand Duke of Tuscany in 1609.

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Proof of the Heliocentric Hypothesis

• In 1729, James Bradley (British Astronomer Royal) discovered a phenomenon called aberration of starlight while trying to observe stellar parallax.

• In one year, noted 20’’ shift in a star’s observed position from its true position.

• Information yields value for the speed of Earth through space (18.6 miles/sec).

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Aberration of Starlight

Page 31: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• Ancient Greeks Pythagoras 6th century B.C. Aristotle 348-322 B.C. Aristarchus 310-230 B.C. Ptolemy ~A.D. 140

• Dark Ages A.D. 5th - 10th century• Renaissance Copernicus

(1473-1543) Tycho Brahe Kepler Galileo (1546-1601) (1571-1630) (1564-1642)

Newton (1642-1727)

Time Line

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Tycho Brahe

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Tycho Brahe• Danish astronomer• Studied a bright new star in sky

that faded over time.• In 1577, studied a comet

– in trying to determine its distance from Earth by observing from different locations, noted that there was no change in apparent position

– proposed comet must be farther from Earth than the Moon.

• Built instrument to measure positions of planets and stars to within one arc minute (1’).

Quadrant Sextant

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Johannes Kepler:Laws of Planetary Motion

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Kepler’s Firsts• First to investigate the formation of pictures with a pin hole camera; • First to explain the process of vision by refraction within the eye; • First to formulate eyeglass designing for nearsightedness and farsightedness; • First to explain the use of both eyes for depth perception. • First to describe: real, virtual, upright and inverted images and magnification; • First to explain the principles of how a telescope works; • First to discover and describe the properties of total internal reflection. • His book Stereometrica Doliorum formed the basis of integral calculus. • First to explain that the tides are caused by the Moon. • Tried to use stellar parallax caused by the Earth's orbit to measure the distance to

the stars; the same principle as depth perception. Today this branch of research is called astrometry.

• First to suggest that the Sun rotates about its axis in Astronomia Nova.• First to derive the birth year of Christ, that is now universally accepted. • First to derive logarithms purely based on mathematics, independent of Napier's

tables published in 1614. • He coined the word "satellite" in his pamphlet Narratio de Observatis a se quatuor

Iovis sattelitibus erronibus

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Kepler: Elliptical orbitsThe amount of "flattening" of the ellipse is the

eccentricity. In the following figure the ellipses become more eccentric from left to right.

A circle may be viewed as a special case of an ellipse with zero eccentricity, while as the ellipse becomes

more flattened the eccentricity approaches one.

(eccentricity-anim)

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• Some orbits in the Solar System cannot be approximated at all well by circles

Elliptical Orbits and Kepler’s Laws

- for example, Pluto’s separation from the Sun varies by about 50% during its orbit!

According to Kepler’s First Law, closed orbits arounda central object under gravity are ellipses.

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F’ FC

r

As a planet moves in an elliptical orbit, the Sun is at one focus (F or F’) of the ellipse.

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F’ FC

r

vperihelion

As a planet moves in an elliptical orbit, the Sun is at one focus (F or F’) of the ellipse

The line that connects the planet’s point of closest approachto the Sun, the perihelion ...

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F’ FC

r

v

aphelion

perihelion

As a planet moves in an elliptical orbit, the Sun is at one focus (F or F’) of the ellipse

… and its point of greatest separation from the Sun, the aphelion

is called the major axis of the ellipse.

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F’ FC

r

v

The only other thing we need to know about ellipses is howto identify the length of the “semi-major axis”, because that determines the period of the orbit.

a a

“Semi” means half, and so the semi-major axis a is half thelength of the major axis:

Page 42: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Kepler’s 1st Law:

The orbits of the planets are ellipses, with the Sun at one focus of the ellipse.

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Kepler’s 2nd Law

• The line joining the planet to the Sun sweeps out equal areas in equal times as the planet travels around the ellipse.

Orbit-anim

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An object in a highly elliptical orbit travels very slowlywhen it is far out in the Solar System,

… but speeds up as it passes the Sun.

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According to Kepler’s Second Law,

… the line joining the object and the Sun ...

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… sweeps out equal areas in equal intervals of time.

equal areas

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That is, Kepler’s Second Law states that

The line joining a planet and the Sun sweeps outequal areas in equal intervals of time.

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v

m

M

r

For circular orbits around one particular mass - e.g. the Sun - we know that the period of the orbit (the time for one completerevolution) depended only on the radius r

r

- this is Kepler’s 3rd Law:

the orbital period squared is proportional to the orbital radius cubed.

For objects orbiting a common central body (e.g. the Sun)in approximately circular orbits,

Page 49: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

F’ FC

r

v

a a

For elliptical orbits,the period dependsnot on r, but on thesemi-major axisa instead.

a a

Let’s see what determines the period for an elliptical orbit:

Page 50: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

For objects orbiting a common central body (e.g. the Sun)

It turns out that Kepler’s 3rd Law applies to all ellipticalorbits, not just circles, if we replace “orbital radius”by “semi major axis”:

the orbital period squared is proportional to the orbital radius cubed.the orbital period squared is proportional to the semi major axis cubed.

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a aa a

So as all of these elliptical orbits have the same semi-majoraxis a, so they have the same period.

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So if each of these orbits is around the same massiveobject (e.g. the Sun),

Page 53: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

So if each of these orbits is around the same massiveobject (e.g. the Sun),

then as they all have the same semi-major axis length a,

Page 54: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

So if each of these orbits is around the same massiveobject (e.g. the Sun),

then as they all have the same semi-major axis length a,

then, by Kepler’sThird Law,they have the sameorbital period.

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Ellipses and Orbits

Ellipse animation

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Kepler’s 3rd Law

The ratio of the squares of the

revolution periods (P) for two planets is

equal to the ratio of the cubes of their

semi-major axes (a).

P2 = a3 or P2/a3 = 1 where

P is the planet’s sidereal orbital period

(in Earth years)

and

a is the length of the semi-major axis

(in astronomical units)

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Astronomical Unit

• One astronomical unit is the semi-major axis of the Earth’s orbit around the Sun, essentially the average distance between Earth and the Sun.

• abbreviation: A.U.

• one A.U. ~ 150 x 106 km

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Kepler’s 3rd Law for the Planets

Planet a (A.U.) P(Earth years) P*P/a*a*a eccentricityMercury 0.387 0.241 0.98 0.206Venus 0.723 0.615 0.99 0.007Earth 1 1 1.00 0.017Mars 1.524 1.881 0.99 0.093

Jupiter 5.203 11.86 0.99 0.048Saturn 9.537 29.42 0.99 0.054Uranus 19.19 83.75 0.99 0.047

Neptune 30.07 163.7 0.99 0.009Pluto 39.48 248 0.99 0.249

P2 = a3 or P2/a3 = 1

Page 59: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Planetary Motions• The planets’ orbits (except Mercury and

Pluto) are nearly circular.• The further a planet is from the Sun, the

greater its orbital period.• Although derived for the six innermost

planets known at the time, Kepler’s Laws apply to all currently known planets.

• Do Kepler’s laws apply to comets orbiting the Sun?Do they apply to the moons of Jupiter?

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Chapter 2 Homework•Text, page 58.•Problem # 1 - accuracy of Tycho Brahe’s observations

–Use equation on page 26 relating unknown diameter (uncertainty in position) to angular diameter (1’ = 1 arc minute), and distance to object (distance to Moon, Sun, Saturn from Earth).

–distance to Moon - p. 198–distance to Sun - 1 A.U.–distance from Sun to Saturn at perihelion

p. A-5, Table 3A

•Problem # 6 - elliptical orbit of Halley’s comet

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Kepler’s Laws• 1st Law: Each planet moves around the

Sun in an orbit that is an ellipse, with the Sun at one focus of the ellipse.

• 2nd Law: The straight line joining a planet and the Sun sweeps out equal areas in equal intervals of time.

• 3rd Law: The squares of the periods of revolution of the planets are in direct proportion to the cubes of the semi-major axes of their orbits.

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What’s important so far?• Through history, people have used the scientific method:

– observe and gather data,

– form theory to explain observations and predict behavior

– test theory’s predictions.

• Greeks produced first surviving, recorded models of universe:

– geocentric (Earth at center of universe),

– other celestial objects in circular orbits about Earth, and

– move with constant speed in those orbits.

• Geocentric models require complicated combinations of deferents and epicycles to explain observed motion of planets. Ptolemaic model required 80 such combinations.

• Copernicus revived heliocentric model of solar system, but kept circular, constant speed orbits.

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What’s important so far? continued• Without use of a telescope, Tycho Brahe made very accurate

measurements of the positions of celestial objects.• Johannes Kepler inherited Brahe’s data and determined three

empirical laws governing the motion of orbiting celestial objects.– 1st Law: Each planet moves around the Sun in an orbit that is

an ellipse, with the Sun at one focus of the ellipse.– 2nd Law: The straight line joining a planet and the Sun

sweeps out equal areas in equal intervals of time.– 3rd Law: The squares of the periods of revolution of the

planets are in direct proportion to the cubes of the semi-major axes of their orbits.

• Galileo used a telescope to observe the Moon and planets. The observed phases of Venus validated the heliocentric model proposed by Copernicus. Also discovered 4 moons orbiting Jupiter, Saturn’s rings, named lunar surface features, studied sunspots, noted visible disk of planets (stars - point sources).

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Why do the planets move

according to Kepler’s laws?

Or, more generally,

why do objects move as they do?

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How do you describe motion?• A piece of paper and a rubber ball are dropped from the

same height, at the same time. • Predict which will hit the ground first.• The piece of paper is crushed into a ball, approximately

the same size as the rubber ball. The paper ball and the rubber ball are dropped from the same height, at the same time.

• Predict which will hit the ground first.• A wooden block and piece of paper have the same area.

They are dropped at the same time from the same height.

• Describe the motion of the block and of the paper.

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Historical Views of Motion

• Aristotle: two types of motion

– natural motion

– violent motion

• Galileo– discredited Aristotelian

view of motion

Animations: Air resistance Free-fall

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Galileo: Why do objects move as they do?

Slope down, Slope up, No slope, speed increases. speed decreases. does speed

change?

Without friction, NO, the speed is

constant!

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What is a “natural” state of motion for an object?

At rest? Moving with constant velocity?

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Inertia and Mass

Inertia:

a body’s resistance to a change in its motion.

Mass:

a measure of an object’s inertia or, loosely, a measure of the total amount of matter contained within an object.

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Page 71: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Newton’s First Law

• Called the law of inertia.

• Since time of Aristotle, it was assumed that a body required some continual action on it to remain in motion, unless that motion were a part of natural motion of object.

• Newton’s first law simplifies concept of motion.

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Animation: collision-1st-law

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FORCES and MOTION• An object will remain

• (a) at rest or

• (b) moving in a straight line at constant speed until

• (c) some net external force acts on it.

Page 74: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

What if there is an outside influence?

To answer this question, Newton invoked the concept of a FORCE acting on a body to cause a change in the motion of the body.

Page 75: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Forces can act instantaneously

(baseball bat making contact with the baseball),

through contact

or

at a distance.

or

continuously

(gravity keeping the baseball from flying into space).

Page 76: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Velocity and Acceleration

Velocity: describes the change in position of a body divided by the time interval over which that change occurs.

Acceleration: The rate of change of the velocity of a body,

any change in the body’s velocity:speeding up, slowing down, changing direction.

Velocity is a vector quantity, requiring both the speed of the body and its direction.

Animation: circularmotion

Page 77: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Newton’s Second Law:

F = ma

• Relates – net external force F applied to

object of mass m – to resulting change in motion of object,

acceleration a.

Page 78: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –
Page 79: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

For a given mass,

greater force

yields

greater acceleration.

F = m a

For a given force,

greater mass (greater inertia),

yields

smaller acceleration.

F = m a

F = m asmaller mass,

yields

greater acceleration.F = m a

smaller force,

yields

smaller acceleration.

F = m a

If there is a NET FORCE on an object,how much will the object accelerate?

Page 80: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –
Page 81: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Questions - Newton’s Laws of Motion

• Consider a game of kick-the-can played with two cans --- one empty and one filled with concrete.

• Which can has greater mass?

• If someone came along and kicked the two cans with exactly the same force, which can would have a greater acceleration?

Explain in terms of Newton’s laws of motion.

• What does Newton’s 3rd law predict about the effect on the foot that kicks the two cans?

Page 82: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

How’s That?

• Newton’s Laws of Motion

– Inertia• penny/cup/paper

– F = ma• chair/empty/person

– Action/reaction• hand-to-hand

Page 83: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Newton and Gravitation• Newton’s three laws of motion enable

calculation of the acceleration of a body and its motion, BUT must first calculate the forces.

• Celestial bodies do not touch ------ do not exert forces on each other directly.

• Newton proposed that celestial bodies exert an attractive force on each other at a distance, across empty space.

• He called this force “gravitation.”

Page 84: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• Isaac Newton discovered that two bodies share a gravitational attraction, where the force of attraction depends on both their masses:

Page 85: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• Both bodies feel the same force, but in opposite directions.

Page 86: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

This is worth thinking about - for example, drop a pen to the floor. Newton’s laws say that the force with which the pen is attracting the Earth is equal and opposite to the force with which the Earth is attracting the pen, even though the pen is much lighter than the Earth!

Page 87: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• Newton also worked out that if you keep the masses of the two bodies constant, the force of gravitational attraction depends on the distance between their centers:

mutual force of attraction

Page 88: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• For any two particular masses, the gravitational force between them depends on their separation as:

distance between the masses increasing

magnitude of the

gravitational force

between 2 fixed

masses

as the separation between the masses is increased, the gravitational force of attractionbetween them decreases quickly.

Page 89: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –
Page 90: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –
Page 91: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Gravity and Weight

• The weight of an object is a measure of the gravitational force the object feels in the presence of another object.

• For example on Earth, two objects with different masses will have different weights.

• Fg = m(GmEarth/rEarth2) = mg

• What is the weight of the Earth on us?

Page 92: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Mass and Weight• Mass

A measure of the total amount of matter contained within an object; a measure of an object’s inertia.

• Weight The force due to gravity on an object.

• Weight and mass are proportional.

• Fg = mg where m = mass of the object and g = acceleration of gravity

acting on the object

Page 93: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Free Fall• If the only force acting on an object is force of

gravity (weight), object is said to be in a state of free fall.

• A heavier body is attracted to the Earth with more force than a light body.

• Does the heavier object free fall faster?

• NO, the acceleration of the body depends on both

– the force applied to it and– the mass of the object, resisting the motion.

• g = F/m = F/m

Page 94: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• We call the force which keeps the Moon in its orbit around the Earth gravity.

Sir Isaac Newton’s conceptual leap in understandingof the effects of gravity largely involved his realizationthat the same force governs the motion of a falling objecton Earth - for example, an apple - and the motion of the Moon in its orbit around the Earth.

Newton’s Law of Gravitation

Page 95: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• Your pen dropping to the floor and a satellite in orbit around the Earth have something in common - they are both in freefall.

Page 96: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Planets, Apples, and the Moon• Some type of force must act on planet;

otherwise it would move in a straight line.• Newton analyzed Kepler’s 2nd Law and saw that

the Sun was the source of this force.• From Kepler’s 3rd Law, Newton deduced that

the force varied as 1/r2.• The force must act through a distance,

and Newton knew of such a force - the one that makes an apple accelerate downward from the tree to the Earth as the apple falls.

• Could this force extend all the way to the Moon?

Page 97: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

To see this, let’s review Newton’s thought experiment

Is it possible to throw an object into orbit around the Earth?

Page 98: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

On all these trajectories,the projectile is in free fall

under gravity.(If it were not, it would travel

in a straight line - that’s Newton’s

First Law of Motion.)

Page 99: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

If the ball is not given enough “sideways” velocity, its trajectory intercepts the Earth ...

that is, it falls to Earth eventually.

Page 100: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

On all these trajectories, the projectile is in free fall.On all these trajectories, the projectile is in free fall.On the trajectories which make complete orbits, the projectile is travelling “sideways” fast enough ...

Page 101: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

On all these trajectories, the projectile is in free fall.… that as it falls, the Earth curves away underneathit, and the projectile completes entire orbits without ever hitting the Earth.

Page 102: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Gravity and OrbitsThe Sun’s inward pull of gravity on the planet

competes with the planet’s tendency to continue moving in a straight line.

Page 103: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

“One had to be Newton to see that the Moon is falling,

when every one sees that it doesn’t.”Paul Valery

French poet and philosopher, 1871-1945

Page 104: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Navigating in Space•Newton's law of universal gravitation combined with Kepler's three laws explain planetary orbits.

•They also suggested the possibility of placing artificial satellites in orbit around the Earth or sending space probes to the planets.

•According to Newton's laws of motion and gravitation, if an object moves fast enough, its path will match the curvature of the Earth, and it will never hit the ground. It goes into orbit.

– Circular orbital velocity for a low Earth orbit is ~ 5 miles/sec.– If the object's velocity is > 5 miles/sec, but < 7 miles/sec,

its orbit will be an ellipse. – Velocities >7 miles/sec reach escape velocity, and the object

moves in a curved path that does not return to Earth.

Page 105: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

The effect of launch speed on the trajectory of a satellite.

• Required launch speed for Earth satellites is:

– ~8 km/s (17,500 mph) for circular orbit just above atmosphere,

– ~11 km/s (25,000 mph) to escape from Earth.

Page 106: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Navigating in Space: Transfer Orbits• To send a spacecraft to another planet, it is launched into a

transfer orbit around the Sun that touches both the Earth's orbit and the orbit of the planet.

• Once the spacecraft is in the transfer orbit, it coasts to the planet. The gravitational force of the Sun takes over and this part of the ride is free.

• But transfer orbits put constraints on space travel. – The launch must occur when the planet and the Earth are in

the correct relative positions in their orbits. – This span of time is called a launch opportunity. – During each launch opportunity, which can be a few weeks in

duration, the spacecraft must be launched during a specific time of the day - launch window.

• If the spacecraft is headed for an inner planet (Mercury or Venus), the launch window occurs in the morning.

• For outer planets (Mars and beyond), the launch window occurs in the early evening.

Page 107: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Navigating in Space: Gravity Assist

• Another technique used by space navigators is called gravity assist.

• When a spacecraft passes very close to a planet, it can use the strong gravitational field of the planet to gain speed and change its direction of motion.

• According to Newton's laws of motion, the planet looses and equal amount of energy in the process, but because the mass of the planet is so much greater than the mass of the spacecraft, only the spacecraft is noticeably affected.

Page 108: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

This astronaut on a space walk is alsoin free fall.

The astronaut’s “sideways” velocityis sufficient to keephim or her in orbitaround the Earth.

Apparent Weightlessness in Orbit

Page 109: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• Why do astronauts in the Space Shuttle in Earth orbit feel weightless?

Let’s take a little time to answer the following question:

Page 110: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

• Some common misconceptions which become apparent in answers to this question are:

(a) there is no gravity in space,(b) there is no gravity outside the Earth’s atmosphere, or(c) at the Shuttle’s altitude, the force of gravity is very small.

Page 111: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

On all these trajectories, the projectile is in free fall.

In spacecraft (like the Shuttle) in Earth orbit, astronauts are in free fall, at the same rate as their spaceships.

That is why they experience weightlessness: just as a platform diver feels while diving down towards a pool, or a sky diver feels while in free fall.

Page 112: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Newton’s Form of Kepler’s 3rd Law• Newton generalized Kepler’s 3rd Law to include

sum of masses of the two objects in orbit about each other (in terms of the mass of the Sun).

– (M1 + M2) P2 = a3

– Observe orbital period and separation of a planet’s satellite, can compute the mass of the planet.

– Observe size of a double stars orbit and its orbital period, deduce the masses of stars in binary system.

• Planet and Sun orbit the common center of mass of the two bodies. – The Sun is not in precise center of orbit.

Page 113: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Mass of Planets, Stars, and Galaxies• By combining Newton’s Laws of Motion and

Gravitation Law, the masses of astronomical objects can be calculated.

• a = v2/r , for circular orbit of radius r

• F = ma = mv2/r

• mv2/r = Fg = GMm/ r2

• v = (GM/r)1/2

• P = 2r/v = 2 (r3/GM)1/2

• M = rv2/G• If the distance to an object and the orbital period of the

object are known, the mass can be calculated.

Page 114: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

What’s important in the last half?• Definitions and examples:

– inertia– mass– acceleration– force– gravity– weight– free fall– orbits

• Newton’s Laws of Motion and how they relate to one another and to objects.

• Newton’s Law of Gravitation

Page 115: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Review1. Briefly describe the geocentric model of the universe. Who

developed the model? What are the model’s basic flaws?

2. What is the Copernican model of the solar system? Flaws in the Copernican model?

3. What discoveries of Galileo helped confirm views of Copernicus?

4. Briefly describe Kepler’s three laws of orbital motion. List two modifications made by Newton to Kepler’s laws.

5. What are Newton’s three laws of motion?

6. What is Newton’s law of gravity? What is gravity? How does the gravitational force vary with the mass of the two objects? with distance between centers?

7. Discuss orbiting objects and free-fall.

8. What is escape speed?

Page 116: Chapter 2: The Copernican Revolution The Birth of Modern Science Ancient Astronomy Models of the Solar System Laws of Planetary Motion Newton’s Laws –

Exploring the Solar SystemSolar System

ObjectFlyby Orbit Probe Lander

Sample Return

Human

Mercury *

Venus * * * *

Moon * * * * * *

Mars * * * *

Jupiter * * *

Saturn * * *

Uranus *

Neptune *

Pluto

Asteroid * * ? ?

Comet * *