Determining the Absorption Coefficient

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Presentation transcript:

Determining the Absorption Coefficient It would be Good to know how to determine the coefficients of the Equation of Transfer!

The Absorption Coefficient Occupation Numbers N = Total Number of an Element Ni,I = Number in the proper state (excitation and ionization) Thermal Properties of the Gas (State Variables: Pg, T, Ne) Atomic/Molecular Parameters: Excitation and Ionization Energies, Transition Probabilities, Broadening Parameters Absorption Coefficient

Absorption Coefficient Bohr Theory The One Electron Case e = Electron Charge (ESU) Z = Atomic number of the nucleus m = reduced mass of the nucleus mnucleus*me/(mnucleus+me) ~ me N = principal quantum number rn = effective orbital radius vn = speed in orbit Absorption Coefficient

Absorption Coefficient Bohr Model b-b b-f 3 2 4 1 f-f ∞ Total Energy (TE) = Kinetic Energy(KE) + Potential Energy(PE) PE is Negative For a bound state TE< 0 Therefore: |KE| < |PE| n = Excitation “stage” i = Ionization Stage: I = neutral, II=first ionized Absorption Coefficient

Absorption Coefficient Continuing ... Combine the Energy and Radial Force Equations Energy: Force: Substituting mv2 Absorption Coefficient

Absorption Coefficient Bohr Postulates Angular Momentum is Quantitized Now put v into the force equation: Now put r into the energy equation: Absorption Coefficient

Absorption Coefficient Hydrogen Atomic Parameters Z = 1 m = 1836.1 (1) / 1837.1 = 0.99946 me = 9.1033(10-28) gm e = electron charge = 4.803(10-10) esu h = 6.6252(10-27) erg s k = 1.380622(10-16) erg K Ei,n = -2.178617(10-11) / n2 ergs = -13.5985 / n2 eV 1 eV = 1.6021(10-12) erg For n = 1: Ei,1 = -13.5985 eV = -109678 cm-1 1 eV = 8065.465 cm-1 Ei,n = -109678 / n2 cm-1 Absorption Coefficient

Absorption Coefficient Continuing Note that all the energies are negative and increasing n =  ==> Ei, = 0 The lowest energy state has the largest negative energy For hydrogen-like atoms the energies can be deduced by multiplying by Z2 and the proper m. Li++ (Li III): 32(-13.60) = -122.4 eV hν = 122.4 eV = 122.4(1.6021(10-12) ergs) = 1.96(10-10) ergs ν = 2.9598(1016) Hz ==> λ = 101 Å What is the temperature? hν = kT ==> T = 1.4(106) K Absorption Coefficient

Absorption Coefficient Specifying Energies Energies are usually quoted WRT the ground state (n=1) Excitation Potential: χi,n ≡ Ei,n - Ei,1 For an arbitrary n it is the absolute energy difference between the nth state and the ground state (n=1). This means χi,1 = 0 and that χi, = -Ei,1 χi, ≡ Ionization Energy (Potential) = Energy needed to lift an electron from the ground state into the continuum (minimum condition) χi, = Ei, - Ei,1 Absorption Coefficient

Absorption Coefficient Ionization Energy Requirement: Em = χi, + ε ε goes into the thermal pool of the particles (absorption process) One can ionize from any bound state Energy required is: Ei,n = χi, - χi,n Energy of the electron will be: hν - Ei,n Absorption Coefficient

Absorption Coefficient A Free “Orbit” Consider the quantum number n which yields a positive energy n = a positive value The solution for the orbit yields a hyperbola Absorption Coefficient

Absorption Coefficient Bound Transitions Consider a transition between two bound states (a,b) => (na,nb) [n’s are the quantum numbers] m and Z for H Absorption Coefficient

Absorption Coefficient Hydrogen Lines Absorption Coefficient

Absorption Coefficient Balmer Series of H The lower level is n = 2  na = 2 First line (Hα) is the transition (absorption): 2 → 3. For absorption: lower → upper na → nb For emission: upper → lower nb → na The “observed” wavelength is 6562.3 The Rydberg formula gives vacuum wavelengths We need to account for the index of refraction of air: Edlen’s Formula Absorption Coefficient

Absorption Coefficient Edlen’s Formula Computes the Index of Refraction of Air νλair = c/n or λVacuum = nλAir Where σ = vacuum wavenumber in inverse microns. For Hα: λVac = 0.6564038 microns σ = 1.52345 n = 1.000276237 λAir = 6562.225 (calculated) Absorption Coefficient

Absorption Coefficient Series Limits λ = -911.672 (1/2 - 1/na2)-1 n Limit Name 1 912 Lyman 2 3646 Balmer 3 8204 Paschen 4 14590 Brackett 5 22790 Pfund For na = 2 one gets λ = 3646.668 Å Any photon which has λ < 3646.668 Å can move an electron from n = 2 to the continuum Series Limits are defined as n =  to nLower Absorption Coefficient

Absorption Coefficient Excitation Move an Electron Between Bound States Ni,x = Number of ions (atoms) that have been ionized to state i and excited to level x Ni,x depends upon the number of ways an electron can enter level x Most levels have sublevels E from the “main” energy level If there are gx of these levels then there are gx ways of entering the level gx is called the statistical weight of the level (state) Each of the sublevels has a complete set of quantum numbers (n,l,ml,ms) or (n,l,j,mj) Absorption Coefficient

Absorption Coefficient Quantum Numbers n: Principal Quantum Number : orbital angular momentum quantum number L = (h/2π) 0    (n – 1) m : -   m < +  ms: ±½ j: j = l + s => j = l ± s s = ½ mj: -j  mj  +j Absorption Coefficient

Hydrogen Quantum Numbers n=1: (n = 1, l = 0, ml = 0, ms = ±½) n=2: (n = 2, l = 0, ml = 0, ms = ±½) (n = 2, l = 1, ml = -1, ms = ±½) (n = 2, l = 1, ml = 0, ms = ±½) (n = 2, l = 1, ml = 1, ms = ±½) Therefore for n=1 g=2 and for n=2 g = 8 For any H-like ion: gn = 2n2 For any atom having level J (alternate set quantum number) with sublevels -J,...0,...+J the statistical weight is gJ = 2J + 1 J is not necessarily an integer Absorption Coefficient

Absorption Coefficient Notation 2S+1LJ 2S+1: Multiplicity (Spin) S = ∑si L: Azimuthal Quantum Number L = ∑i J: L+S = total angular momentum vector Absorption Coefficient

Absorption Coefficient Boltzmann Equation We shall start with the state-ratio form of the equation The E’s are with respect to the continuum. χ is the excitation potential of the state pi is the probability that the state exists Absorption Coefficient

The Partition Function Note that pi depends on electron pressure and essentially quantifies perturbations of the electronic states. We define the partition function U as These numbers are tabulated for each element as a function of ionization stage, temperature, and “pressure.” The latter is expressed as a lowering of the ionization potential. Absorption Coefficient

Rewrite the Boltzman Equation Number in state X WRT ground state Sum Ni,x Substitute Absorption Coefficient

Absorption Coefficient Example What is the fraction of H that can undergo a Balmer transition at 5700K? We need g2, UI(5700), and χ2 g2 = 8 (n=2) UI(T) = 2 χ2 = 82259.0 cm-1 = 10.20 eV = 1.634(10-11) ergs N2/NI = 8/2 e-(χ/kT) = 4 e-20.76 = 3.842(10-9) Absorption Coefficient

Absorption Coefficient Ionization The Saha Equation This is the Saha equation. It gives the ratio of ground state populations for adjoining ionization stages. What one really wants is the number in the entire stage rather than just the ground state. Remember that χi,0 = 0. Absorption Coefficient

Rewrite The Saha Equation Note that m = me Absorption Coefficient

Computing Stage Populations Note that the Saha Equation does not tell you the populations but: NT = NI + NII + NIII + NIV +... Divide by NI NT/NI = 1 + NII/NI + (NIII/NII)(NII/NI) + (NIV/NIII)(NIII/NII)(NII/NI) + ... Each of the ratios is computable and NT is known. Absorption Coefficient

Absorption Coefficient Example What is the degree of ionization of H at τ = 2/3 in the Sun? T = 6035K and Pe = 26.5 dynes/cm2 Pe NII/NI = 0.3334 T5/2 (2UII/UI) e-13.598*CF/kT UII = 1: Partition function for a bare nucleus = 1 UI = 2 Pe NII/NI = 9.4332(108) e-26.15 = 4.162(10-3) NII/NI = 1.57(10-4) Absorption Coefficient

Absorption Coefficient Another Example The Same for Neutral and First Ionized Fe. T = 6035K and Pe = 26.5 dynes/cm2 Pe NII/NI = 0.3334 T5/2 (2UII/UI) e-7.87*CF/kT UII = 47.4 UI = 31.7 Pe NII/NI = 2.82(109) 2.68(10-7) NII/NI = 28.5 Absorption Coefficient

Absorption Coefficient Data Sources Atomic Energy Levels: NBS Monograph 35 and subsequent updates (NIST) Line Lists Compute from AEL MIT Wavelength Tables RMT - Charlotte Moore Kurucz Line Lists Literature for Specific Elements Partition Functions Drawin and Felenbok Bolton in ApJ Kurucz ATLAS Code Literature (Physica Scripta) Absorption Coefficient