TY - JOUR
T1 - Direct Numerical Simulation of Flow over Periodic Hills up to Re H= 10 , 595
AU - Krank, Benjamin
AU - Kronbichler, Martin
AU - Wall, Wolfgang A.
N1 - Publisher Copyright:
© 2018, Springer Science+Business Media B.V., part of Springer Nature.
PY - 2018/9/1
Y1 - 2018/9/1
N2 - We present fully resolved computations of flow over periodic hills at the hill-Reynolds numbers Re H= 5 , 600 and Re H= 10 , 595 with the highest fidelity to date. The calculations are performed using spectral incompressible discontinuous Galerkin schemes of 8 th and 7 th order spatial accuracy, 3 rd order temporal accuracy, as well as 34 and 180 million grid points, respectively. We show that the remaining discretization error is small by comparing the results to h- and p-coarsened simulations. We quantify the statistical averaging error of the reattachment length, as this quantity is widely used as an ‘error norm’ in comparing numerical schemes. The results exhibit good agreement with the experimental and numerical reference data, but the reattachment length at Re H= 10 , 595 is predicted slightly shorter than in the most widely used LES references. In the second part of this paper, we show the broad range of capabilities of the numerical method by assessing the scheme for underresolved simulations (implicit large-eddy simulation) of the higher Reynolds number in a detailed h/p convergence study.
AB - We present fully resolved computations of flow over periodic hills at the hill-Reynolds numbers Re H= 5 , 600 and Re H= 10 , 595 with the highest fidelity to date. The calculations are performed using spectral incompressible discontinuous Galerkin schemes of 8 th and 7 th order spatial accuracy, 3 rd order temporal accuracy, as well as 34 and 180 million grid points, respectively. We show that the remaining discretization error is small by comparing the results to h- and p-coarsened simulations. We quantify the statistical averaging error of the reattachment length, as this quantity is widely used as an ‘error norm’ in comparing numerical schemes. The results exhibit good agreement with the experimental and numerical reference data, but the reattachment length at Re H= 10 , 595 is predicted slightly shorter than in the most widely used LES references. In the second part of this paper, we show the broad range of capabilities of the numerical method by assessing the scheme for underresolved simulations (implicit large-eddy simulation) of the higher Reynolds number in a detailed h/p convergence study.
KW - Direct numerical simulation
KW - High-order discontinuous Galerkin
KW - Incompressible Navier–Stokes equations
KW - Large-eddy simulation
KW - Periodic hill flow
UR - http://www.scopus.com/inward/record.url?scp=85048869668&partnerID=8YFLogxK
U2 - 10.1007/s10494-018-9941-3
DO - 10.1007/s10494-018-9941-3
M3 - Article
AN - SCOPUS:85048869668
SN - 1386-6184
VL - 101
SP - 521
EP - 551
JO - Flow, Turbulence and Combustion
JF - Flow, Turbulence and Combustion
IS - 2
ER -