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Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition.

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Presentation on theme: "Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition."— Presentation transcript:

1 Chapter 3: Spectral lines in stars

2 Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition Dependent on composition

3 Each element has its own unique spectrum

4 Absorption lines in the Sun’s spectrum

5 Absorption Line Spectrum Gustav Kirchhoff (1824-1887)

6 absorption lines of hydrogen

7 Emission Line Spectrum Produced by a low- density gas depends on composition and temperature

8 Emission lines

9 The Balmer series for hydrogen: Visible light electrons falling to n=2 Rydberg formula (Balmer for n f = 2) : 1 / = R (1/n f 2 - 1/n i 2 ) R = Rydberg constant = 1.097 x 10 7 m -1

10 The hydrogen atom

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12 Energy levels and transitions of the many-electron atom: Sodium Quantum states of the valence electron

13 The Bohr Model Classical physics predicts that the electron should spiral into the nucleus Cannot explain emission spectra

14 The Bohr model: The e- stays in certain stable orbits, emits no radiation unless it jumps to a lower level The angular momentum of the e- is quantized the attaction between p and e- provides the centripetal acceleration n = principal quantum number

15 From Coulomb’s law, the force between the proton and electron is F = 1 4  0 q 1 q 2 r2r2 This is the centripetal force, mv 2 / r Where q 1 = q 2 = e for the hydrogen atom

16 Bohr radius a 0 =  0 h 2 /  me 2 = 5.29 x 10 -11 m So when the electron is in any energy level n: KE of the electron in the nth level: K n = 1/2 mv 2 4  0 e 2 r PE of the electron in the nth level: U n = Total energy E n = K n + U n = ??? Compare to Rydberg formula!

17 Reduced mass: the nucleus is not infinite in mass, Bohr model is off by 0.1% m r = m 1 + m 2 m 1 m 2 isotopes

18 Ionized Helium is also a 1-electron atom

19 Why is the emission spectrum of ionized helium similar to that of hydrogen? 1.Because hydrogen and helium are similar chemically 2.Because several of the energy levels of hydrogen and helium are the same 3.Because hydrogen and helium have similar atomic masses 4.It is a total coincidence

20 Energy Level Transitions AllowedNot Allowed Continuum Ionization Differences between elements isotopes

21 Stellar classification scheme

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23 Is this star hotter or cooler than the Sun?

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25 Spectrum of Arcturus

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27 Temperature Luminosity The Hertzsprung- Russell diagram plots the luminosity vs. temperature of stars

28 B - V is a measure of color: the smaller B-V, the hotter the star (magnitudes, remember!)

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32 Lines in a star’s spectrum correspond to a spectral type that reveals its temperature (Hottest) O B A F G K M (Coolest)


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