TY - JOUR
T1 - Sequence of bifurcations of natural convection of air in a laterally heated cube with perfectly insulated horizontal and spanwise boundaries
AU - Gelfgat, Alexander
N1 - Publisher Copyright:
© 2023 American Physical Society.
PY - 2023/4
Y1 - 2023/4
N2 - A sequence of three steady-oscillatory transitions of buoyancy convection of air in a laterally heated cube with perfectly thermally insulated horizontal and spanwise boundaries is studied. The problem is treated by Newton and Arnoldi methods based on Krylov subspace iteration. The finite volume grid is gradually refined from 1003 to 2563 finite volumes. It is shown that the primary instability is characterized by two competing eigenmodes, whose temporal development results in two different oscillatory states that differ by their symmetries. Bifurcations due to both modes are subcritical. These modes develop into different oscillatory and then chaotic flow states which, at larger Grashof number, stabilize and arrive to single stable steady flow. With further increase of the Grashof number, this flow loses its stability again. It is argued that, in all the three transitions, the instability onsets as well as reinstatement of stability take place owing to an interaction between a destabilizing centrifugal mechanism and stabilizing effect of thermal stratification.
AB - A sequence of three steady-oscillatory transitions of buoyancy convection of air in a laterally heated cube with perfectly thermally insulated horizontal and spanwise boundaries is studied. The problem is treated by Newton and Arnoldi methods based on Krylov subspace iteration. The finite volume grid is gradually refined from 1003 to 2563 finite volumes. It is shown that the primary instability is characterized by two competing eigenmodes, whose temporal development results in two different oscillatory states that differ by their symmetries. Bifurcations due to both modes are subcritical. These modes develop into different oscillatory and then chaotic flow states which, at larger Grashof number, stabilize and arrive to single stable steady flow. With further increase of the Grashof number, this flow loses its stability again. It is argued that, in all the three transitions, the instability onsets as well as reinstatement of stability take place owing to an interaction between a destabilizing centrifugal mechanism and stabilizing effect of thermal stratification.
UR - http://www.scopus.com/inward/record.url?scp=85153855922&partnerID=8YFLogxK
U2 - 10.1103/PhysRevFluids.8.043902
DO - 10.1103/PhysRevFluids.8.043902
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AN - SCOPUS:85153855922
SN - 2469-990X
VL - 8
JO - Physical Review Fluids
JF - Physical Review Fluids
IS - 4
M1 - 043902
ER -