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Lecture 2: Physical Processes In Lecture 2: Physical Processes In

Lecture 2: Physical Processes In - PowerPoint Presentation

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Lecture 2: Physical Processes In - PPT Presentation

Astrophysical and Laboratory Plasmas Lecture 1 TemperatureDensity regime Many physical processes Focus on AtomicPlasma interactions Atomic properties are intrinsic independent of external factors temp den etc ID: 242345

transfer radiative section fig radiative transfer fig section lines atomic coefficients equilibrium absorption radiation emissivity level lte collisional rate

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Slide1

Lecture 2: Physical Processes InAstrophysical and Laboratory Plasmas

Lecture 1: Temperature-Density regime

Many physical processes

Focus on

Atomic+Plasma

interactions

Atomic properties are

intrinsic

,

independent of external factors (temp, den, etc.)

Plasma interactions are treated as

extrinsic

Approximation:

Isolated atoms perturbed by environmentSlide2

Quantum Statistical Equilibrium

D

ivision between atomic and plasma physics

Calculation of

individual

atomic parameters –

Chs

. 2-7

Hartree-Fock

, Close-Coupling (R-Matrix), etc.

Radiative

and collisional properties

 Transition probabilities and cross sections

External

statistical

equilibrium of particles

Local-Thermodynamic-Equilibrium (LTE)

 characterized by local temperature-density

Saha

ionization balance, Boltzmann level population

 Boltzmann-

Saha

distribution

Non-LTE requires explicit particle-radiation coupling

 Collisional-

Radiative

model (simple) –

Ch. 8: Emission lines

 Multi-level

radiative

transfer model (complex) –

Ch. 9: AbsorptionSlide3

Collisional-Radiative (CR) Models

Section 8.2 and Fig. 8.7

Need excitation and

radiative

parameters,

viz.

 Electron impact cross sections (E): Ch. 5 – EIE

Maxwellian

averaged rate coefficients (T)

Eq. (5.31)

 A-values and oscillator strengths

 Ch. 4 –

Radiative

Transitions

Other processes such as fluorescent excitation by background radiation field may be

includedSlide4

Coupled CR Rate Equations

Level Populations, emissivity, line ratios

Section 8.1.3

Examples: [O II], [S II] forbidden lines

He-like X-ray lines:

Section 8.4, Fig. 8.7

General time-dependent rate equation

Eq. (8.41)

Transient emission spectra (e.g. black-hole accretion disk x-ray flares):

Fig. 8.13Slide5

Non-LTE Radiative Transfer Models

Ch. 9: Absorption lines and

radiative

transfer

Consider radiation-matter coupling explicitly

For each photon frequency, specify

monochromatic

source function S

monochromatic opacity and emissivity

Section 9.4:

Radiative

transferSlide6

Optical Depth Definition:

Fig. 9.9 and Eq. (9.118)

Basic

radiative

transfer equation: Eq. (9.119)

Absorption and emissivity coefficients

Source function:

Eq. (9.126)

S

 Einstein A,B coefficients