Finite-dimensional description of non-newtonian vortex flows
ESAIM. Proceedings, Tome 1 (1996), pp. 241-253
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The application of finite-dimensional dynamical systems theory to non-Newtonian vortex flow indicates the presence of complex temporal dynamics that is attributed to shear thinning and normal stress (giving rise to the so-called Weissenberg rod climbing phenomenon). These aspects are examined for Rayleigh-Benard thermal convection and Taylor-Couette rotational flow, in an attempt to elucidate on the mechanisms behind the onset and destabilization of secondary vortex flow common to these and possibly other non-Newtonian flows in the transition regime. Three transition scenarios are particularly explored, namely, the transition to chaos via intermittency, quasiperiodicity and period doubling.
@article{EP_1996_1_a16,
author = {Roger E. Khayat},
title = {Finite-dimensional description of non-newtonian vortex flows},
journal = {ESAIM. Proceedings},
pages = {241--253},
year = {1996},
volume = {1},
doi = {10.1051/proc:1996015},
language = {en},
url = {http://geodesic.mathdoc.fr/articles/10.1051/proc:1996015/}
}
Roger E. Khayat. Finite-dimensional description of non-newtonian vortex flows. ESAIM. Proceedings, Tome 1 (1996), pp. 241-253. doi: 10.1051/proc:1996015
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