Tokamaks exhibit several types of relaxation oscillations such as sawteeth,
fishbones and Edge Localized Modes (ELMs) under appropriate conditions. Se
veral authors have introduced model nonlinear dynamic systems with a small
number of degrees of freedom which can illustrate the generic characteristi
cs of such oscillations. In these models, one focuses on physically "releva
nt'' degrees of freedom, without attempting to simulate all the myriad deta
ils of the fundamentally nonlinear tokamak phenomena. Such degrees of freed
om often involve the plasma macroscopic quantities such as pressure or dens
ity and also some measure of the plasma turbulence, which is thought to con
trol transport. In addition, "coherent'' modes may be involved in the dynam
ics of relaxation, as well as radial electric fields, sheared flows, etc. I
n the present work, an extension of an earlier sawtooth model (which involv
ed only two degrees of freedom) due to the authors is presented. The dynami
cal consequences of a pressure-driven "coherent'' mode, which interacts wit
h the turbulence in a specific manner, are investigated. Varying only the t
wo parameters related to the coherent mode, the bifurcation properties of t
he system have been studied. These turn out to be remarkably rich and varie
d and qualitatively similar to the behavior found experimentally in actual
tokamaks. The dynamic model presented involves only continuous nonlineariti
es and is the simplest known to the authors that can yield features such as
sawteeth, "compound sawteeth'' with partial crashes, "monster'' sawteeth,
metastability, intermittency, chaos, periodic and "grassy'' ELMing in appro
priate regions of parameter space. The results suggest that linear stabilit
y analysis of systems, while useful in elucidating instability drives, can
be misleading in understanding the dynamics of nonlinear systems over time
scales much longer than linear growth times and states far from stable equi
libria. [S1070-664X(99)00506-6].