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Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine [email protected]

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Page 1: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Astronomy 101The Solar System

Tuesday, Thursday2:30-3:45 pmHasbrouck 20

Tom [email protected]

Page 2: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Course

• Course Website:– http://blogs.umass.edu/astron101-tburbine/

• Textbook:– Pathways to Astronomy (2nd Edition) by Stephen Schneider

and Thomas Arny.• You also will need a calculator.

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Office Hours

• Mine• Tuesday, Thursday - 1:15-2:15pm• Lederle Graduate Research Tower C 632

• Neil• Tuesday, Thursday - 11 am-noon • Lederle Graduate Research Tower B 619-O

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Homework

• We will use Spark• https://spark.oit.umass.edu/webct/logonDisplay.d

owebct• Homework will be due approximately twice a

week

Page 5: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Astronomy Information• Astronomy Help Desk• Mon-Thurs 7-9pm• Hasbrouck 205

•The Observatory should be open on clear Thursdays

• Students should check the observatory website at: http://www.astro.umass.edu/~orchardhill for updated information

• There's a map to the observatory on the website.

Page 6: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Final

• Monday - 12/14 • 4:00 pm• Hasbrouck 20

Page 7: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

HW #7

• Due today

Page 8: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

HW #8

• Due today

Page 9: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

HW #9

• Due October 27

Page 10: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Exam #2

• Next Thursday• Bring a calculator and a pencil• No cell phones, Blackberries, iPhones• Covers material from September 22 through

October 8 (Units 14-31)

Page 11: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Formulas you need to know• F = GMm/r2

• F = ma• a = GM/r2

• Escape velocity = sqrt(2GM/r)• T (K) = T (oC) + 273.15• c = f*λ• E = h*f• KE = 1/2mv2

• E = mc2

Page 12: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

More Formulas

• Power emitted per unit surface area = σT4

• λmax (nm) = (2,900,000 nm*K)/T• Apparent brightness = Luminosity

4π x (distance)2

Page 13: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

LCROSS Impact

• http://www.youtube.com/watch?v=VVYKjR1sJY4• http://dsc.discovery.com/videos/news-lcross-smashes-

into-the-moon.html

Page 14: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Solar System

• Sun• Eight Planets• Their moons• Dwarf Planets• Asteroids• Comets

Page 15: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Sun

Page 16: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Sun

• 74% H• 25% He• Traces of everything else

Page 17: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Mercury

Page 18: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Venus

Page 19: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Earth

Page 20: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Earth’s crust• 46.6% O• 27.7% Si• 8.1% Al • 5.0% Fe • 3.6% Ca• 2.8% Na• 2.6% K • 2.1% Mg

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Moon

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Comet

Page 23: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Mars

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Asteroid

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http://spaceguard.esa.int

Hiroshima

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Meteorites

chondrite

Pallasite – mixtures of olivine and metal Iron

Page 29: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Jupiter

Page 30: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Jupiter

• 90% H• 10% He• Traces of everything else

Page 31: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Io

Page 32: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Europa

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Saturn

Page 34: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Saturn

• 75% H• 25% He• Traces of everything else

Page 35: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Uranus

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Neptune

Page 37: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Pluto

Page 38: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the
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How do we determine what astronomical bodies are made of?

Page 40: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

How do we determine what astronomical bodies are made of?

• Measure how they emit or reflect light– Tells you about their surfaces

• Measure their physical properties– Tells you about their interiors

Page 41: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the
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Planetary densities

volumeweightdensity =

3

34 rvolume π=

But how do we determine mass?

mass

Units are g/cm3 or kg/m3

1 g/cm3 = 1,000 kg/m3

Page 43: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Use Newton’s Laws of motion…2

324pa

GM π

=

Where P is the period of a planet’s orbita is the distance from the planet to the SunG is Newton’s constantM is the mass of the Sun

This assumes that orbits are circles, and that the mass of a planet is tiny compared to the mass of the Sun.

Use this relation with P and a for the Earth, and you’ll get the mass of the Sun: MSun = 1.98892 x 1030 kg

Page 44: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

But we want to know the mass of a planet!

Where F is the gravitational forceG is the constant of proportionalityM and m are the two masses exerting forcesr is the radius of the planeta is its acceleration due to gravity

2rGmMF = and F = ma

mar

GmMF == 2

Page 45: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

ar

GM=2

Solve for M, the mass of the Earth, by usinga = 9.8 m/sec2

r = 6.4 x 106 mG = 6.67 x 10-11 m3/(kg sec2)

GarM

2

=Re-arrange to get

MEarth = 5.9736 x 1024 kgVEarth = 1.0832 x 1021 m3

DEarth = 5515 kg/m3 = 5.515 g/cm3

Page 46: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Volume

• If you assume a planet is a sphere:• Volume = 4/3πr3

Page 47: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Density = ρ = Mass/VolumeρEarth = 5.515 g/cm3

Density (g/cm3)Metallic iron 7.87Basalt 3.3Water 1.0Water Ice 0.9Liquid Hydrogen 0.07

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Density of water

• Density of water is 1 g/cm3

• Density of water is 1,000 kg/m3

Page 49: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Density (g/cm3)

Iron 7.87

Basalt 3.3

Water 1.0

Cold ices 0.07-0.09

DensityWhat do these densities tell us?

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How big is the Solar System?One boundary

• Some scientists think that the furthest influence of the Solar System extends out to 125,000 astronomical units (2 light years).

• Since the nearest star is 4.22 light-years away, the Solar System size could extend almost half-way to the nearest star.

• Astronomers think that the Sun's gravitational field dominates the gravitational forces of the other stars in the Solar System out to this distance.

Page 55: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

What is out there?• The Oort Cloud (the source of long period comets)

extends out to a distance of 50,000 AU, and maybe even out to 100,000 AU.

• The Oort Cloud has never been seen directly. • Appears to exist because comets with extremely long

orbits sometimes pass near the Sun and then head back out again.

• The Oort cloud could have a trillion icy objects.

Page 56: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the
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Another possible boundary- Heliopause• Heliopause is the region of space where the sun's solar

wind meets the interstellar medium. Solar wind's strength is no longer great enough to push back against the interstellar medium.– Solar wind – charged particles ejected from the Sun– Interstellar medium – gas and dust between stars

• Heliosphere is a bubble in space "blown" into the interstellar medium

• It is a fluctuating boundary that is estimated to be ~80-100 AU away

Page 58: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the
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• Termination shock - the point where the solar wind slows down.

• Bow shock - the point where the interstellar medium, travelling in the opposite direction, slows down as it collides with the heliosphere.

Page 61: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the
Page 62: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

To learn how the Solar System formed

• Important to study the bodies that were the building blocks of the planets– Asteroids

• meteorites are almost all samples of asteroids– Comets

Page 63: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

What’s the difference?

• Asteroids• Comets• Meteorites

Page 64: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

What’s the difference?

• Asteroids - small, solid objects in the Solar System• Comets - small bodies in the Solar System that (at

least occasionally) exhibit a coma (or atmosphere) and/or a tail

• Meteorites - small extraterrestrial body that reaches the Earth's surface

Page 65: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

How do we know the age of the solar system

Page 66: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Radioactive dating

Page 67: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

What do we date?

Page 68: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Meteorites

Page 69: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

How old is the solar system?

• ~4.6 billion years• All meteorites tend to have these ages• Except:

Page 70: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

How old is the solar system?

• ~4.6 billion years• All meteorites tend to have these ages• Except:

– Martian meteorites– Lunar meteorites

Page 72: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

How do you determine this age?

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Dating a planetary surface

• Radioactive Dating – Need sample• Crater counting – Need image of surface

Page 74: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Radioactivity

• The spontaneous emission of radiation (light and/or particles) from the nucleus of an atom

Page 75: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Radioactivity

http://wps.prenhall.com/wps/media/tmp/labeling/2130796_dyn.jpg

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Half-Life

• The time required for half of a given sample of a radioactive isotope (parent) to decay to its daughter isotope.

Page 77: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

Radioactive Dating• You are dating when a rock crystallized

http://faculty.weber.edu/bdattilo/images/tim_rock.gif

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Radioactive Datingn = no(1/2)(t/half-life)

no = original amountn = amount left after decay

Also can write the formula asn = noe-λt

λ is the decay constantdecay constant is the fraction of a number of atoms of a

radioactive nuclide that disintegrates in a unit of timeHalf life = (ln 2)/λ = 0.693/λ

Page 79: Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 ...web.mit.edu/thb/www/Astronomy101.oct15.pdf · Use Newton’s Laws of motion… 2. 4 2 3. p a G M. π = Where. P. is the

• where e = 2.718 281 828 459 045 …

• Limit (1 + 1/n)n = en→∞

• For example if you have n = 1,000• The limit would be 2.716924

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http://www.gpc.edu/~pgore/myart/radgraph.gif

Exponential decay is where the rate of decayis directly proportional to the amount present.

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Any Questions?