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

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

2 Chapter 26: Cosmology and Chapter 27: Exploring the Universe

3 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

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8 At the time of recombination, the temperature was a few thousand degrees everywhere! But from our point of view “now,” this radiation has been significantly redshifted (due to expansion of the universe) so the spectrum should look like a “black-body” of a much cooler temperature.

9 Remember “Black body spectrum” from Chapter 5

10 At the time of recombination, the temperature was a few thousand degrees everywhere! But from our point of view “now,” this radiation has been significantly redshifted (due to expansion of the universe) so the spectrum should look like a “black-body” of a much cooler temperature. From Einstein’s theory, Dicke & Peebles (Princeton University) predict T = 3 K.

11 At the time of recombination, the temperature was a few thousand degrees everywhere! But from our point of view “now,” this radiation has been significantly redshifted (due to expansion of the universe) so the spectrum should look like a “black-body” of a much cooler temperature. From Einstein’s theory, Dicke & Peebles (Princeton University) predict T = 3 K.

12 Remember “Black body spectrum” from Chapter 5 What would a 3 K spectrum look like?

13 Penzias & Wilson discover CMB radiation; awarded 1978 Nobel Prize

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16 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)

17 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)

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19 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)

20 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)

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24 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

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27 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

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32 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

33 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!

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36 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!

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38 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?

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41 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!

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44 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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49 Modern Hubble Law implies:  0 =  m +  

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