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Solar Physics Course Lecture Art Poland. Modeling MHD equations And Spectroscopy. Why. What I am going to talk about should lead to our understanding of physical processes in outer solar atmosphere: Heating Energy transport Solar wind acceleration Magnetic field evolution. Overview.

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Solar physics course lecture art poland

Solar Physics CourseLectureArt Poland

Modeling MHD equations

And

Spectroscopy


Why

  • What I am going to talk about should lead to our understanding of physical processes in outer solar atmosphere:

    • Heating

    • Energy transport

    • Solar wind acceleration

    • Magnetic field evolution


Overview
Overview

  • Modeling features in the solar atmosphere involves solving the full MHD equations.

  • The solution of these equations needs initial conditions and boundary conditions.

  • To get realistic values, you need observations.

  • In this lecture I will first talk about how to get the observations, and then how they are used in the solution of the equations.


What features

Closed loops

Open magnetic field

What Features


What quantities do we need
What Quantities Do We Need?

  • The equations tell us we need to observe

    • Temperature

    • Density

    • Velocity

    • Magnetic field

  • To do time dependence we need each as a function of time.


Questions
Questions

  • How can we measure these quantities at the Sun?

  • Spectroscopic observations

  • What causes an absorbtion line? How is one formed?

  • Why are some lines in emission?



Comments
Comments

  • Equations derived from observations in the lab. of atomic spectra.

  • Quantum mechanics gives more precise description.

  • What I am showing helps visualize the structure.


Level splitting momentum
Level Splitting, Momentum

  • When there are multiple electrons in an atom, the n levels are split.

  • The split levels are referred to as s,p,d,f,

    • For n=1 there are only s levels

    • For n=2 there are s and p levels

    • For n=3 there are s,p,and d levels

    • etc


Spin

  • The other quantity is electron spin.

    • He for example has 2 electrons, both can occupy the n=1 level because one has a spin of +1/2 and the other a spin of -1/2

    • Transitions between spin level have a very low probability, and are referred to as forbidden transitions.

    • When they are opposite to each other they are referred to as singlets

    • When they are the same, triplets

    • Spin combined with momentum can also give doublets.


Sample energy diagram
Sample Energy Diagram

  • Allowed transitions

  • Forbidden transitions

  • Magnetic fields can split sub-levels (ie 22s into 2 levels).


Summary
Summary

  • Atomic structure - Spectral lines

  • Electron transitions

    • N levels

    • Momentum s,p,d,f

    • Spin

  • Momentum and spin splitting occurs in magnetic field – can use splitting to measure strength of field.


How to use spectra
How to Use Spectra

  • Velocity?

    • Doppler shift

    • Sometimes just an asymmetry in profile

  • What else?

  • Temperature – next topic

  • Density – next topic


Gas state
Gas State

  • 1) The basic observed equation is P=NkT, N=ρ/uMH

    • a. This is important: if you know two, you know the third.

    • b. Can make observations that yield T, and ρ so you can get P.

  • 2) Temperature and mean velocity – visualization again

    • a. Perfect box with perfect collisions: collision momentum with wall is 2mvx

    • b. Number of collisions vx/2L L is size of box

    • c. Total of all momentum is ΣΜvx2/L

    • d. Momentum is pressure so P=ML-3Σvx2

    • e. Define mean vx2=n-1Σvx2

    • f. vx2=vy2=vz2=1/3v2

    • g. P=n/3L3(Mv2)=1/3(NMv2)

    • h. So average energy ½ Mv2=3/2 kT This is important because it relates energy, velocity, to temperature. (not bulk velocity)


Get the t
Get The T

  • Velocity of atoms and electrons related to T was just shown.

  • What do we need to get the temperature of the gas? First assumption?

    • Assume a Maxwellian velocity distribution

  • What must be assumed for this to be valid?

    • Collisions (not so good at very low r)

  • f(v,T)= (M/2πkT)3/2v2e-(Mv2/2kT)

  • Maxwellian tail of distribution


Line profile emission
Line Profile Emission

  • Where to measure for T?

  • Can get T from line width.


Boltzmann distribution
Boltzmann Distribution

  • a. Ni/N=gi/ue-ε/kT ε=hν

  • b. Can use the ratio for 2 energy levels to get relative populations between two energy levels.

  • c. Measure two lines from same atom to get T

  • d. Ni/Nj=gi/gje-δε/kT


Saha equation
Saha Equation

  • a. equation of ionization state:

  • Ni/Nj(Ne)=(2πmkT)3/2/h3(2(ui(T)/uj(T))e-ε/kT

  • b. Used to determine gas temperature

FeIII FeIV

N

T


How to get lines
How to Get Lines

  • I is the intensity you observe

  • S is emission/cm3

  • t is optical depth n is frequency

  • How do you get an absorption line from this?

  • How do you get an emission line?


Other issues
Other issues

  • Non-LTE

  • A or f values

    • Line brightness

    • Collision prob.

  • Plank function

  • Differential emission measure

n

Log Ne2


Summary1
Summary

  • Spectra can give us:

    • T via line width, line ratios

    • Density via line ratios or diff. emission measure

    • Velocity via line shift





How to solve
How to Solve

  • Depends on the problem

    • Near the Sun small area, cartesian

    • Whole Sun or Heliosphere, spherical

  • Coupled differential equations.

  • The big problem is steep gradients.

    • Transition region (T gradient)

    • Flares (P gradients, shocks)

  • The boundary conditions you choose almost always dictate the solution.


Results
Results

  • The output of these programs are table of numbers, T(x,y,z,t), P(x,y,z,t),etc.

  • Need to visualize the results

  • Need to make visualizations something that you can compare with observations.


Variable grid mesh major breakthrough
Variable Grid MeshMajor Breakthrough

  • Paramesh

  • Steep T gradient in transition region.

  • Almost no gradient in corona.


Gridding changes as calculation progresses
Gridding Changes as Calculation progresses


Other issues1
Other Issues

  • Conduction

    • Isotropic

    • Anisotropic –along B field

  • Radiative losses

    • Optically thin - collisions

    • Non-LTE T(collision) T(radiation)

  • Heating

    • Constant

    • Alfven waves – a function of B

  • Make each of these a replaceable module in your program.


Conduction
Conduction

  • Conduction only along B field

    • How the grid is oriented with respect to B

Excess heating low down

Numerical diffusion makes it wider.



Model output
Model Output

All profiles from same T different v



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