%0 Journal Article %1 Pier2017Linear %A Pier, Benoît %A Schmid, Peter J. %D 2017 %J Journal of Fluid Mechanics %K 76e05-parallel-shear-flows 76e30-hydrodynamic-stability-nonlinear-effects %P 435--480 %R 10.1017/jfm.2017.58 %T Linear and Nonlinear Dynamics of Pulsatile Channel Flow %U http://dx.doi.org/10.1017/jfm.2017.58 %V 815 %X he dynamics of small-amplitude perturbations, as well as the regime of fully developed nonlinear propagating waves, is investigated for pulsatile channel flows. The time-periodic base flows are known analytically and completely determined by the Reynolds number (based on the mean flow rate), the Womersley number (a dimensionless expression of the frequency) and the flow-rate waveform. This paper considers pulsatile flows with a single oscillating component and hence only three non-dimensional control parameters are present. Linear stability characteristics are obtained both by Floquet analyses and by linearized direct numerical simulations. In particular, the long-term growth or decay rates and the intracyclic modulation amplitudes are systematically computed. At large frequencies (mainly ), increasing the amplitude of the oscillating component is found to have a stabilizing effect, while it is destabilizing at lower frequencies; strongest destabilization is found for . Whether stable or unstable, perturbations may undergo large-amplitude intracyclic modulations; these intracyclic modulation amplitudes reach huge values at low pulsation frequencies. For linearly unstable configurations, the resulting saturated fully developed finite-amplitude solutions are computed by direct numerical simulations of the complete Navier–Stokes equations. Essentially two types of nonlinear dynamics have been identified: 'cruising' regimes for which nonlinearities are sustained throughout the entire pulsation cycle and which may be interpreted as modulated Tollmien–Schlichting waves, and 'ballistic' regimes that are propelled into a nonlinear phase before subsiding again to small amplitudes within every pulsation cycle. Cruising regimes are found to prevail for weak base-flow pulsation amplitudes, while ballistic regimes are selected at larger pulsation amplitudes; at larger pulsation frequencies, however, the ballistic regime may be bypassed due to the stabilizing effect of the base-flow pulsating component. By investigating extended regions of a multi-dimensional parameter space and considering both two-dimensional and three-dimensional perturbations, the linear and nonlinear dynamics are systematically explored and characterized.

@article{Pier2017Linear, abstract = {{he dynamics of small-amplitude perturbations, as well as the regime of fully developed nonlinear propagating waves, is investigated for pulsatile channel flows. The time-periodic base flows are known analytically and completely determined by the Reynolds number (based on the mean flow rate), the Womersley number (a dimensionless expression of the frequency) and the flow-rate waveform. This paper considers pulsatile flows with a single oscillating component and hence only three non-dimensional control parameters are present. Linear stability characteristics are obtained both by Floquet analyses and by linearized direct numerical simulations. In particular, the long-term growth or decay rates and the intracyclic modulation amplitudes are systematically computed. At large frequencies (mainly ), increasing the amplitude of the oscillating component is found to have a stabilizing effect, while it is destabilizing at lower frequencies; strongest destabilization is found for . Whether stable or unstable, perturbations may undergo large-amplitude intracyclic modulations; these intracyclic modulation amplitudes reach huge values at low pulsation frequencies. For linearly unstable configurations, the resulting saturated fully developed finite-amplitude solutions are computed by direct numerical simulations of the complete Navier–Stokes equations. Essentially two types of nonlinear dynamics have been identified: 'cruising' regimes for which nonlinearities are sustained throughout the entire pulsation cycle and which may be interpreted as modulated Tollmien–Schlichting waves, and 'ballistic' regimes that are propelled into a nonlinear phase before subsiding again to small amplitudes within every pulsation cycle. Cruising regimes are found to prevail for weak base-flow pulsation amplitudes, while ballistic regimes are selected at larger pulsation amplitudes; at larger pulsation frequencies, however, the ballistic regime may be bypassed due to the stabilizing effect of the base-flow pulsating component. By investigating extended regions of a multi-dimensional parameter space and considering both two-dimensional and three-dimensional perturbations, the linear and nonlinear dynamics are systematically explored and characterized.}}, added-at = {2019-03-01T00:11:50.000+0100}, author = {Pier, Beno\^{i}t and Schmid, Peter J.}, biburl = {https://www.bibsonomy.org/bibtex/2b4d9bda3fd9105b9c9337e52f4dd6ea7/gdmcbain}, citeulike-article-id = {14587233}, citeulike-linkout-0 = {http://dx.doi.org/10.1017/jfm.2017.58}, day = 21, doi = {10.1017/jfm.2017.58}, interhash = {08296cfe894f23a3edd29f9e6a6600a8}, intrahash = {b4d9bda3fd9105b9c9337e52f4dd6ea7}, issn = {0022-1120}, journal = {Journal of Fluid Mechanics}, keywords = {76e05-parallel-shear-flows 76e30-hydrodynamic-stability-nonlinear-effects}, month = feb, pages = {435--480}, posted-at = {2018-05-15 06:14:14}, priority = {5}, timestamp = {2019-03-01T00:11:50.000+0100}, title = {{Linear and Nonlinear Dynamics of Pulsatile Channel Flow}}, url = {http://dx.doi.org/10.1017/jfm.2017.58}, volume = 815, year = 2017 }