Title: COMPLEXITY IN SOLAR ACTIVE REGIONS
1COMPLEXITY IN SOLAR ACTIVE REGIONS
- Loukas Vlahos
- Department of Physics
- University of Thessaloniki, Greece
2Active regions are open, non-linear dynamical
systems
- Energy enters and escape from all boundaries but
the most important boundary is the photosphere... - The statistical properties of the formation and
evolution of active regions at the photosphere
are of importance for the flare energy release
3SMALL SCALE VS LARGE SCALE ORGANIZATION
- AR are formed and developed gradually till they
disappear - Follow well defined statistical laws
- Size distribution of AR, fractal dimension have
been studied - AR made by N-mutually interacting loops, which
are never stable and represent the eddy patterns
of turbulence in the convection zone
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5Introduction(a few well accepted facts)
- The flux tubes during their buoyant rise to the
surface are influenced by several physical
effects e.g. Coriolis force, magnetic tension,
drag and most importantly the convection motion.
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8THE CORONAL PART OF ACTIVE REGIONS RESPOND TO
THE EVOLUTION OF THEIR PHOTOSPHERIC BOUNDARY
9Active region formation
10Key observations to constrain the models
- Size distribution of active regions
- 1.9ltklt2.1 (see Howard 1996)
11Active regions form fractal structures
- The geometrical characteristics of the active
regions can be represented with a single
characteristic correlation dimension - See Meunier 1999 and references sited in this
article
12Statistics of the explosive events
- Peak intensity distribution of explosive events
in the low chromosphere follow also a power law
with index (see for example Ellerman bombs,
Georgoulis et al. 2002)
13Question?
- Are the sub-photospheric / photospheric /
chromospheric/coronal characteristics of the
magnetic field evolution independent? - Basic working assumption The Complexity of the
magnetic field in active region suggest that all
solar phenomena are interdependent and the well
known say for the evolution of non-linear systems
(attributed to Lorentz) the sensitivity to the
initial conditions in non-liner systems is such
that the flopping of the winds of a butterfly in
Brazil will influence the weather in New York
apply to all solar phenomena.
14Sub-photospheric evolution
- Let us assume that the convection zone is
penetrated with flux tubes (fibrils) with
different size and magnetic strength all moving
with different speeds towards the surface. - Can we cut the 3-D box with a surface and
consider that each magnetic tube is represented
with a circle with diameter R. - Almost 20 years ago Tom Bogdan in his Ph.D pose
this question and try to develop the statistical
evolution of the dilute gas consisted of 2-D
fibrils
15Statistics of sub-photospheric evolution of
magnetic fields
- See Bogdan and Lerche (1985)
- There is considerable
- work published on the
- filamentary MHD
16Vortex attraction and formation of active regions
- The magnetic field emerging through the surface
of the sun are individually encircled by one or
more subsurface vortex rings, providing an
important part of the observed clustering of
magnetic fibrils.. Parker (1992)
17A model based on transport on fractal support and
percolation(Model-1)
- Carl Schrijver and collaborators (1992/1997)
presented a model were magnetic field robes are
filling a point in this lattice with probability
p and then executing random walks on a
structured lattice. The flux robe diffuse on a
network already structured.
18A Cellular Automaton Model based on
percolation(models 2/3)
- See Wentzel and Seiden (1992), Seiden and Wenrzel
(1996)
19The basic rules for Model-4(Vlahos, et al, ApJ
Letters, 2002)
- We use a 200x1000 square grid with no magnetic
flux (0) - We star by filling 0.5 (1)positive magnetic
flux a 0.5 (-1) negative. - Stimulation probability P Any active point for
one time step stimulate the emergence of new flux
in the neighborhood. Newly emerged flux appear in
dipoles. - Diffusion due to unrestricted random walk
Dm(mobility) free motion on the grid. - Diffusion due to submergence Dd (submergence of
flux) Fast disappearance if the neighboring
points are non-active. - Spontaneous generation of new flux E (its value
is not important) To keep the process going
20The basic rules for Model-4(Vlahos, et al., ApJ
Letters, 2002)
- Comment These models are based on two universal
principals on the development of complex systems.
(A) The continuous fight tendencies Emergence
vs diffusion and (B) Percolation - The results are generic and independent on the
exact values of the free parameters but the
observations constrain their values to a subset
of the available 3-D space (PxDmxDd
(0-1)X(0-1)x(0-1)
21Results
- The evolution of active points
- Are the values of P,D,E unique?
22A basic portrait
23Size distribution
24Fractal correlation dimension
- See also Meunier 1999 for similar results using a
variant of Wentzel and Seiden model.
25Energy release
- Cancellation of flux due to collisions of
opposite flux releases energy
26Peak flux frequency distribution
27Waiting Time Distribution
28Is the statistics of the size distribution
correlated to the energy release statistics?
29A movie on the active region evolution and
magnetic field cancellation
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31The standard SOC model for flares
- Loading phase-very important
- Rule-1 Instability threshold (criticality)
- Rule-2 Redistribution and energy release
- Reloading - Either continuous or after relaxation
32Magnetic field evolution in the corona(A 3-D MHD
simulation)
- Ake Nordlund and Klaus Galsgaard (1996)
33Similar results from the SOC theory
- Vlahos, Georgoulis, Isliker, Anastasiadis see
also review by Charbonneau et al. (2001)
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35Connection of CA to MHD
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40A movie from the SOC and TRACE
- ..\..\..\movie_flare.mpg
- A TRACE movie
41Fractal properties of the unstable current regions
- McIntosh et al (2002) (DF?1.8-2.0)
42Wave propagation in a structured active region
(filled with intermittent current sheets sitting
on a fractal in 3-D space)
- Wave propagation reinforces the current sheet and
the absorption coefficient of the waves is
enhanced by several orders of magnitude
43Old paradigm
- Let us leave behind these nice historic cartoons
and search for a new one to replace them
44The new paradigm
- A new model for the energy release seems to be
suggested - This model has different characteristics from the
old cartoons - The current sheets are driven from the evolution
of magnetic fields at the convection
zone/photosphere level. - Many characteristics of this sub-photospheric/phot
ospheric evolution are imprinted on the evolving
and changing current sheet in all levels of the
corona
45My favorite cartoon(it is time for change of
paradigm) although here we must be careful on the
same problems I have just mention.
- Vlahos(1992/1993), Vlahos and Anastasiadis
(1991-92)
46Levy flights in velocityan anomalous diffusion
in velocity space
47Combine magnetic turbulence and E-field
- Magnetic turbulence are trapping the particles
for Energies EltEc - Electric fields heat the particles up to Ec and
freely accelerate them above Ec
48Velocity Distribution above cut off
49Summary
- The turbulent convection zone, through the
magnetic fields drives the entire solar
atmosphere. - The complexity of our system (convection
zone/photosphere/chromosphere/corona) is such
that only statistical analysis and statistical
models can capture its dynamical evolution - There is strong correlation between the evolution
of photosphere patterns and chromospheric/coronal
effects (this is indicated by my k-a dependence)
50Summary
- We need a series of 3-D MHD studies to understand
deeper the physical meaning of the free
parameters of our CA models and restrict the
rules further - I believe that we need to start building global
solar models using more techniques borrowed from
complexity theory. - We will make considerable progress only if we
understand deeper the interconnection of the
elements of our system, this new global
understanding has to be reflected even on the
drawing of new cartoons