Simple bifurcation scenario.
Bifurcation Analysis
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A second set of ideas from this toolkit relates to
multiscale bifurcation analysis. Consider the following highly
simplified problem, in which the turbulent heat flux in some system
is a function of a single parameter, the temperature gradient, and
for which a sequence of turbulence simulations which fully resolve
the turbulent dynamics produces the figure above. One expects to
find a bifurcation in the corresponding macroscopic system. That
is, as one slowly increases the heat flux from near zero, the
temperature gradient that one observes rises from a threshold value
of R/LT ~ 2.5 to R/LT ~ 4.5.
Around this point, further increase of the heat flux results in a
rapid doubling of the temperature gradient. (There is hysteresis in
such a system as well, indicated by the lower arrow.) To find the
critical heat flux, beyond which the temperature gradient suddenly
increases, one must presently ``design'' the numerical experiment
represented above by hand, and then analyze the results for regions
of macroscopic instability. Although tedious, this approach is
straightforward. However, realistic transport barrier bifurcation
scenarios involve several fluxes (electron and ion heat, parallel
and perpendicular momentum, particles, etc.) and a large
number of control parameters. It is not realistic to expect to find
critical points by hand in these circumstances.
Bifurcation analysis of similarly complicated systems is a
well-developed subject in engineering and applied math. Sophisticated
solvers exist for finding the critical parameters in such systems in
the presence of nonlinearity and noise. The central idea of the
multiscale bifurcation analysis is to embed the microscale solver —
the turbulence code — within existing engineering solvers. Together
with the averaging and restart techniques pioneered by Kevrekidis,
this approach allows the computer to ``design'' and carry out the
numerical experiments directly. We propose to adapt these techniques
for plasma physics, with specific application to the problem of
directly calculating the key aspects of transport barrier formation.
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