TY - JOUR
T1 - Subcritical transition of Taylor - Couette - Poiseuille flow at high radius ratio
AU - Matsukawa, Yuki
AU - Tsukahara, Takahiro
N1 - Publisher Copyright:
© 2022 Author(s).
PY - 2022/7/1
Y1 - 2022/7/1
N2 - We performed direct numerical simulations of Taylor-Couette-Poiseuille flows within an annular channel with a radius ratio of 0.883. A parametric study was conducted on subcritical transition processes of the wall-bounded combined shear flow with a torsional base-flow profile with three control parameters of F(P) representing the axial mean pressure gradient and two Reynolds numbers R e in and R e out, based on the inner cylinder and outer cylinder rotational velocities, respectively. In the set (R e in, R e out) = (400, - 1000), the laminar flow becomes turbulent via finite-length and infinite-length turbulent bands, called one-way helical turbulence, as F(P) increases. Two-way helical turbulence appeared in the counterpart of the annular Poiseuille flow without cylindrical rotations, suggesting that the azimuthal Couette flow broke the symmetry of the helical turbulence of the axial Poiseuille flow. In the set of (R e in, R e out) = (800, - 2000) and (1200, - 3000), we found a ring-shaped localized turbulence at F(P) that provided an axial friction Reynolds number comparable to the azimuthal one. The flow states were mapped in parameter space spanned by the axial and azimuthal friction Reynolds numbers. Eight different flow regimes, including the laminar state, were identified based on turbulent statistics during these flow visualizations.
AB - We performed direct numerical simulations of Taylor-Couette-Poiseuille flows within an annular channel with a radius ratio of 0.883. A parametric study was conducted on subcritical transition processes of the wall-bounded combined shear flow with a torsional base-flow profile with three control parameters of F(P) representing the axial mean pressure gradient and two Reynolds numbers R e in and R e out, based on the inner cylinder and outer cylinder rotational velocities, respectively. In the set (R e in, R e out) = (400, - 1000), the laminar flow becomes turbulent via finite-length and infinite-length turbulent bands, called one-way helical turbulence, as F(P) increases. Two-way helical turbulence appeared in the counterpart of the annular Poiseuille flow without cylindrical rotations, suggesting that the azimuthal Couette flow broke the symmetry of the helical turbulence of the axial Poiseuille flow. In the set of (R e in, R e out) = (800, - 2000) and (1200, - 3000), we found a ring-shaped localized turbulence at F(P) that provided an axial friction Reynolds number comparable to the azimuthal one. The flow states were mapped in parameter space spanned by the axial and azimuthal friction Reynolds numbers. Eight different flow regimes, including the laminar state, were identified based on turbulent statistics during these flow visualizations.
UR - http://www.scopus.com/inward/record.url?scp=85133967880&partnerID=8YFLogxK
U2 - 10.1063/5.0096676
DO - 10.1063/5.0096676
M3 - Article
AN - SCOPUS:85133967880
SN - 1070-6631
VL - 34
JO - Physics of Fluids
JF - Physics of Fluids
IS - 7
M1 - 074109
ER -