astr 1102-002 2008 fall semester

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ASTR 1102-002 2008 Fall Semester Joel E. Tohline, Alumni Professor Office: 247 Nicholson Hall [Slides from Lecture23]

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ASTR 1102-002 2008 Fall Semester. Joel E. Tohline, Alumni Professor Office: 247 Nicholson Hall [Slides from Lecture23]. Chapter 26 : Cosmology and Chapter 27: Exploring the Universe. Implications of Big Bang. Era of “recombination” and “Cosmic Microwave Background (CMB)” - PowerPoint PPT Presentation

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Page 1: ASTR 1102-002 2008 Fall Semester

ASTR 1102-0022008 Fall Semester

Joel E. Tohline, Alumni ProfessorOffice: 247 Nicholson Hall

[Slides from Lecture23]

Page 2: ASTR 1102-002 2008 Fall Semester

Chapter 26: Cosmologyand

Chapter 27: Exploring the Universe

Page 3: ASTR 1102-002 2008 Fall Semester

Implications of Big Bang

• Era of “recombination” and “Cosmic Microwave Background (CMB)”

• Origin of the Elements

• Non-uniformities in the Early Universe and the Origin of Galaxies

Page 4: ASTR 1102-002 2008 Fall Semester
Page 5: ASTR 1102-002 2008 Fall Semester
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At the time of recombination, the temperature wasa few thousand degreeseverywhere!

But from our point ofview “now,” this radiation has been significantly redshifted(due to expansion ofthe universe) so the spectrum should looklike a “black-body” ofa much cooler temperature.

Page 9: ASTR 1102-002 2008 Fall Semester

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Page 10: ASTR 1102-002 2008 Fall Semester

At the time of recombination, the temperature wasa few thousand degreeseverywhere!

But from our point ofview “now,” this radiation has been significantly redshifted(due to expansion ofthe universe) so the spectrum should looklike a “black-body” ofa much cooler temperature.

From Einstein’s theory,Dicke & Peebles (Princeton University)predict T = 3 K.

Page 11: ASTR 1102-002 2008 Fall Semester

At the time of recombination, the temperature wasa few thousand degreeseverywhere!

But from our point ofview “now,” this radiation has been significantly redshifted(due to expansion ofthe universe) so the spectrum should looklike a “black-body” ofa much cooler temperature.

From Einstein’s theory,Dicke & Peebles (Princeton University)predict T = 3 K.

Page 12: ASTR 1102-002 2008 Fall Semester

Rem

embe

r “B

lack

bod

y sp

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from

Cha

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What would a 3 K spectrum look like?

Page 13: ASTR 1102-002 2008 Fall Semester

Penzias & Wilson discover CMB radiation; awarded 1978 Nobel Prize

Page 14: ASTR 1102-002 2008 Fall Semester
Page 15: ASTR 1102-002 2008 Fall Semester
Page 16: ASTR 1102-002 2008 Fall Semester

Uniformity of CMB• COBE satellite measurements (which

improved on discovery of Penzias & Wilson) show …– CMB temperature is 2.725 K

– Exactly the same temperature no matter which direction you look in the sky! at the time of recombination, the universe was extremely uniform

– Slight Doppler shift due to Earth’s motion through space

– Otherwise, only very tiny fluctuations; smaller than 200 micro-Kelvin (K)

Page 17: ASTR 1102-002 2008 Fall Semester

Uniformity of CMB• COBE satellite measurements (which

improved on discovery of Penzias & Wilson) show …– CMB temperature is 2.725 K

– Exactly the same temperature no matter which direction you look in the sky! at the time of recombination, the universe was extremely uniform

– Slight Doppler shift due to Earth’s motion through space

– Otherwise, only very tiny fluctuations; smaller than 200 micro-Kelvin (K)

Page 18: ASTR 1102-002 2008 Fall Semester
Page 19: ASTR 1102-002 2008 Fall Semester

Uniformity of CMB• COBE satellite measurements (which

improved on discovery of Penzias & Wilson) show …– CMB temperature is 2.725 K

– Exactly the same temperature no matter which direction you look in the sky! at the time of recombination, the universe was extremely uniform

– Slight Doppler shift due to Earth’s motion through space

– Otherwise, only very tiny fluctuations; smaller than 200 micro-Kelvin (K)

Page 20: ASTR 1102-002 2008 Fall Semester

Uniformity of CMB• COBE satellite measurements (which

improved on discovery of Penzias & Wilson) show …– CMB temperature is 2.725 K

– Exactly the same temperature no matter which direction you look in the sky! at the time of recombination, the universe was extremely uniform

– Slight Doppler shift due to Earth’s motion through space

– Otherwise, only very tiny fluctuations; smaller than 200 micro-Kelvin (K)

Page 21: ASTR 1102-002 2008 Fall Semester
Page 22: ASTR 1102-002 2008 Fall Semester
Page 23: ASTR 1102-002 2008 Fall Semester
Page 24: ASTR 1102-002 2008 Fall Semester

Uniformity of CMB• COBE satellite measurements (which

improved on discovery of Penzias & Wilson) show …– CMB temperature is 2.725 K– Exactly the same temperature no matter which

direction you look in the sky! at the time of recombination, the universe was extremely uniform

– Slight Doppler shift due to Earth’s motion through space

– Otherwise, only very tiny fluctuations; smaller than 200 micro-Kelvin (K) – confirmed by WMAP spacecraft

Page 25: ASTR 1102-002 2008 Fall Semester
Page 26: ASTR 1102-002 2008 Fall Semester
Page 27: ASTR 1102-002 2008 Fall Semester

Implications of Big Bang

• Era of “recombination” and “Cosmic Microwave Background (CMB)”

• Origin of the Elements

• Non-uniformities in the Early Universe and the Origin of Galaxies

Page 28: ASTR 1102-002 2008 Fall Semester
Page 29: ASTR 1102-002 2008 Fall Semester
Page 30: ASTR 1102-002 2008 Fall Semester
Page 31: ASTR 1102-002 2008 Fall Semester
Page 32: ASTR 1102-002 2008 Fall Semester

Implications of Big Bang

• Era of “recombination” and “Cosmic Microwave Background (CMB)”

• Origin of the Elements

• Non-uniformities in the Early Universe and the Origin of Galaxies

Page 33: ASTR 1102-002 2008 Fall Semester

Origin of the Elements

• Looking back even further in time – before recombination – the universe was even hotter

• At a sufficiently early epoch it was too hot for any atomic nuclei heavier than Hydrogen to have existed!

• When did the first elements form; and which ones were able to form? ANS: In the “first 3 minutes”; and only Helium!

Page 34: ASTR 1102-002 2008 Fall Semester
Page 35: ASTR 1102-002 2008 Fall Semester
Page 36: ASTR 1102-002 2008 Fall Semester

Origin of the Elements

• Looking back even further in time – before recombination – the universe was even hotter

• At a sufficiently early epoch it was too hot for any atomic nuclei heavier than Hydrogen to have existed!

• When did the first elements form; and which ones were able to form? ANS: In the “first 3 minutes”; and only Helium!

Page 37: ASTR 1102-002 2008 Fall Semester
Page 38: ASTR 1102-002 2008 Fall Semester

Origin of the Elements

• Looking back even further in time – before recombination – the universe was even hotter

• At a sufficiently early epoch it was too hot for any atomic nuclei heavier than Hydrogen to have existed!

• When did the first elements form; and which ones were able to form?

Page 39: ASTR 1102-002 2008 Fall Semester
Page 40: ASTR 1102-002 2008 Fall Semester
Page 41: ASTR 1102-002 2008 Fall Semester

Origin of the Elements

• Looking back even further in time – before recombination – the universe was even hotter

• At a sufficiently early epoch it was too hot for any atomic nuclei heavier than Hydrogen to have existed!

• When did the first elements form; and which ones were able to form? ANS: In the “first 3 minutes”; and only Helium!

Page 42: ASTR 1102-002 2008 Fall Semester
Page 43: ASTR 1102-002 2008 Fall Semester
Page 44: ASTR 1102-002 2008 Fall Semester

How Do We Measure 0 ?

• Measure (count up) all the matter density in the universe (0) and compare the value to c.

• Measure distances and redshifts of even more distant galaxies and look for deviations in the Hubble diagram.

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Modern Hubble Law implies:

0 = m +

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Page 51: ASTR 1102-002 2008 Fall Semester