Physics 681: Solar Physics and Instrumentation – Lecture 10 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.

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Physics 681: Solar Physics and Instrumentation – Lecture 10 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research

October 4, 2005Center for Solar-Terrestrial Research The Atmosphere  Radiative Transfer – LTE Equation of Transfer Equlibria Absorption Lines in LTE  Radiative Transfer – Statistical Equilibrium (SE) Model Assumptions Line Radiation and Einstein Coefficients Continuum Radiation Collisions Source Function Equations of Statistical Equilibrium

October 4, 2005Center for Solar-Terrestrial Research Equation of Transfer  Optical depth  Radiative transfer equation  Formal solution  Total emergent intensity  How can we derive the source function from the absolute intensity? Inversion!

October 4, 2005Center for Solar-Terrestrial Research Equilibria  Thermodynamic equilibrium A single temperature T describes the state of the atmosphere everywhere Maxwellian velocity distribution Ionization and excitation according to the Saha and Boltzmann equations Homogeneous and isotropic black-body radiation field No temperature gradient!  Local thermodynamic equilibrium (LTE) Locally, a single temperature T describes the atmosphere Important simplification: S ν = B ν (T ) Thermalization length has to be shorter than the distance over which the temperature changes LTE might not apply to all species of particles Good approximation for visible and IR continua, line wings, and weak line profiles  Non-LTE (a single temperature T is insufficient) Radiative interactions are too rare Thermalization length is too long

October 4, 2005Center for Solar-Terrestrial Research Absorption Lines in LTE  Continuum and line absorption coefficients  Intensity at disk center  Doppler and collisional line broadening (Voigt profile)

October 4, 2005Center for Solar-Terrestrial Research Radiative Transfer – SE  Statistical Equlibrium (SE) Electrons are still described by a Maxwell distribution (single electron temperature T e ) However, population depends on radiative processes  Einstein coefficients  Spontaneous emission  Induced emission  Absorption

October 4, 2005Center for Solar-Terrestrial Research Continuum Radiation and Collisions  Photoionization  Radiative recombination  Collisional transitions between two bound states  Collisional transition from and to the continuum