Abstract
Two semi-implicit six-stage Runge–Kutta algorithms are developed for the simulation of wall-bounded flows. Using these schemes, time integration is implicit in the wall-normal direction, and explicit in the other directions, to relax the time step constraint due to the fine mesh near the wall. The explicit subscheme is a six-stage fourth-order low-storage Runge–Kutta scheme. Based on analysis in Fourier space and results obtained for propagation test cases, the semi-implicit schemes are shown to be of order 3 and, for waves discretized by a number of points per period between 4 and 16, to be as accurate as, or more accurate than, the standard explicit fourth-order Runge–Kutta algorithm in terms of dissipation and dispersion. The large-eddy simulation of a compressible turbulent channel flow at a friction Reynolds number of 360 and a Mach number of 0.1 is then carried out with one of the proposed algorithms. The computational time is reduced by a factor 1.33 with respect to a large-eddy simulation using the explicit subscheme in all directions. Wall-pressure and velocity spectra from the large-eddy simulation are presented to give insights into the flow turbulent structures. In particular, wave number–frequency spectra are calculated. Acoustic components appear to be identified in these spectra.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.