2.5 Flashcards

1
Q

Kirchhoff’s Law

A
  • valid for optically thick objects in a cavity
  • cavity in thermodynamic equilibrium
  • the emission through a small hole equals black body radiation
    Iν=Bν(T)
  • In thermodynamic equilibrium:
    Sν=Bν(T)
    Sν=jν / αν
  • leading to Kirchhoff’s law:
    jνν Bν(T).
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2
Q

Interpretation of Kirchhoff’s Law

A
  • For atomic, molecular gases, and many solid particles: jν and αν have strong peaks
    → Optically thin emission has strong emission lines
    → absorbing gas has strong absorption lines
  • In thermodynamic equilibrium, peaks in jν and αν must compensate each other
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3
Q

Maxwellian Velocity Distribution

A

dnv = 4π n (m/2πkBT)3/2 v2 exp(-mv2 / 2kBT) dv
- Describes the distribution of particle velocities at temperature T.
- nv = number of particles
- n = number of particles per unit volume
- v = velocity and m = particle mass

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4
Q

Boltzmann Distribution Law

A

ne/n0 = exp(-Ee / kB T)
- Describes the population of excited states (ne) of an atom or molecule relative to the ground state (n0)
- E = Energy of excited state above ground state

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5
Q

Saha Equation

A
  • Describes ionization state of the gas.
  • x: fraction of atoms ionized:

x2/(1-x)=(2πme)3/2/h3(kBT)5/2/P e-χ/kBT

  • me: electron mass,
  • P: pressure
  • χ: ionization potential.
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6
Q

Planck’s Law for Radiation Energy Density

A

Uν dν = 8πh/c3 · ν3dν / (ehν/kBT-1).

  • For hν > kBT
    → Wien-part behaves like:

Uν dν ≈ 8πh/c3 · ν3e-hν/kBT.

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7
Q

Summary of High Energy Drop-off (1+4)

A
  • All formulae have an exponential drop-off for high energies

∝e-E/kBT

where E is:

  • kinetic energy mv2 / 2
  • excitation energy Ee
  • ionization energy χ
  • photon energy hν
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8
Q

Local Thermodynamic Equilibrium (LTE)

A

LTE is valid for an isolated box filled with gas.

  • All walls at T
  • gas at T
  • Planck radiation field Uν(T)

LTE conditions for a volume in a star with diameter d for gas:

  • T=const for gas (same velocity distribution in entire volume)
  • d>Λp = mean free path of particles

for radiation:

  • isotropic Planck radiation field in equilibrium with gas
  • d>Λr = mean free path of photons between emission and absorption
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