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Chapter 3: Spectral lines in stars

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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Page 1: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Chapter 3: Spectral lines in stars

Page 2: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Emission and absorption of light

Emission line spectrumContinuous spectrum(thermal, blackbody)

Independent of composition

Dependent on composition

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

Each element has its own unique spectrum

Page 4: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Absorption lines in the Sun’s spectrum

Page 5: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Absorption Line Spectrum

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Gustav Kirchhoff (1824-1887)

Page 6: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

absorption lines of hydrogen

Page 7: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Emission Line Spectrum

• Produced by a low-density gas

• depends on composition and temperature

Page 8: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Emission lines

Page 9: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

The Balmer series for hydrogen: Visible light

electrons falling to n=2

Rydberg formula (Balmer for nf = 2) :1 / = R (1/nf

2 - 1/ni2)

R = Rydberg constant = 1.097 x 107 m-1

Page 10: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

The hydrogen atom

Page 11: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition
Page 12: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Energy levels and transitions of the many-electron atom: Sodium

Quantum states of the valence electron

Page 13: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

The Bohr Model

• Classical physics predicts that the electron should spiral into the nucleus

• Cannot explain emission spectra

Page 14: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

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

Page 15: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

From Coulomb’s law, the force between the proton and electron is

F = 1

40

q1 q2 r2

This is the centripetal force, mv2 / r

Where q1 = q2 = e for the hydrogen atom

Page 16: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Bohr radius a0 = 0h2 / me2 = 5.29 x 10-11 m

So when the electron is in any energy level n:

KE of the electron in the nth level: Kn = 1/2 mv2

-1

40

e2 r

PE of the electron in the nth level: Un =

Total energy En = Kn + Un = ??? Compare to Rydberg formula!

Page 17: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Reduced mass: the nucleus is not infinite in mass, Bohr model is off by 0.1%

mr = m1 + m2

m1 m2

isotopes

Page 18: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Ionized Helium is also a 1-electron atom

Page 19: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

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

Page 20: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Energy Level Transitions

AllowedNot Allowed

• Continuum• Ionization• Differences

between elements• isotopes

Page 21: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Stellar classification scheme

Page 22: 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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Page 23: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Is this star hotter or cooler than the Sun?

Page 24: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition
Page 25: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Spectrum of Arcturus

Page 26: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition
Page 27: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Temperature

Lu

min

osi

tyThe Hertzsprung-Russell diagram plots the luminosity vs. temperature of stars

Page 28: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

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

Page 29: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition
Page 30: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition
Page 31: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition
Page 32: Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition

Lines in a star’s spectrum correspond to a spectral type that reveals its temperature

(Hottest) O B A F G K M (Coolest)