2.5 Flashcards
Kirchhoff’s Law
- 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:
jν=αν Bν(T).
Interpretation of Kirchhoff’s Law
- 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
Maxwellian Velocity Distribution
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
Boltzmann Distribution Law
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
Saha Equation
- 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.
Planck’s Law for Radiation Energy Density
Uν dν = 8πh/c3 · ν3dν / (ehν/kBT-1).
- For hν > kBT
→ Wien-part behaves like:
Uν dν ≈ 8πh/c3 · ν3e-hν/kBT.
Summary of High Energy Drop-off (1+4)
- 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
Local Thermodynamic Equilibrium (LTE)
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