Inclined porous medium convection at large Rayleigh number
High-Rayleigh-number ( $Ra$ ) convection in an inclined two-dimensional porous layer is investigated using direct numerical simulations (DNS) and stability and variational upper-bound analyses. When the inclination angle $\unicode[STIX]{x1D719}$ of the layer satisfies $0^{\circ }<\unicode[STIX]{x...
Saved in:
Published in | Journal of fluid mechanics Vol. 837; pp. 670 - 702 |
---|---|
Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Cambridge, UK
Cambridge University Press
25.02.2018
|
Subjects | |
Online Access | Get full text |
Cover
Loading…
Summary: | High-Rayleigh-number (
$Ra$
) convection in an inclined two-dimensional porous layer is investigated using direct numerical simulations (DNS) and stability and variational upper-bound analyses. When the inclination angle
$\unicode[STIX]{x1D719}$
of the layer satisfies
$0^{\circ }<\unicode[STIX]{x1D719}\lesssim 25^{\circ }$
, DNS confirm that the flow exhibits a three-region wall-normal asymptotic structure in accord with the strictly horizontal (
$\unicode[STIX]{x1D719}=0^{\circ }$
) case, except that as
$\unicode[STIX]{x1D719}$
is increased the time-mean spacing between neighbouring interior plumes also increases substantially. Both DNS and upper-bound analysis indicate that the heat transport enhancement factor (i.e. the Nusselt number)
$Nu\sim CRa$
with a
$\unicode[STIX]{x1D719}$
-dependent prefactor
$C$
. When
$\unicode[STIX]{x1D719}>\unicode[STIX]{x1D719}_{t}$
, however, where
$30^{\circ }<\unicode[STIX]{x1D719}_{t}<32^{\circ }$
independently of
$Ra$
, the columnar flow structure is completely broken down: the flow transitions to a large-scale travelling-wave convective roll state, and the heat transport is significantly reduced. To better understand the physics of inclined porous medium convection at large
$Ra$
and modest inclination angles, a spatial Floquet analysis is performed, yielding predictions of the linear stability of numerically computed, fully nonlinear steady convective states. The results show that there exist two types of instability when
$\unicode[STIX]{x1D719}\neq 0^{\circ }$
: a bulk-mode instability and a wall-mode instability, consistent with previous findings for
$\unicode[STIX]{x1D719}=0^{\circ }$
(Wen et al., J. Fluid Mech., vol. 772, 2015, pp. 197–224). The background flow induced by the inclination of the layer intensifies the bulk-mode instability during its subsequent nonlinear evolution, thereby favouring increased spacing between the interior plumes relative to that observed in convection in a horizontal porous layer. |
---|---|
Bibliography: | USDOE Office of Science (SC) SC0001114 |
ISSN: | 0022-1120 1469-7645 |
DOI: | 10.1017/jfm.2017.863 |