22.10.2014 Views

CERFACS CERFACS Scientific Activity Report Jan. 2010 – Dec. 2011

CERFACS CERFACS Scientific Activity Report Jan. 2010 – Dec. 2011

CERFACS CERFACS Scientific Activity Report Jan. 2010 – Dec. 2011

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

TURBOMACHINERY<br />

3.2.4 Compressor flows : simulation of turbulent flow patterns<br />

(A. Gomar, T. Leonard, G. Dufour, N. Gourdain)<br />

Flows in turbomachines are very complex : turbulence, relative motion between rotating and non rotating<br />

parts, 3D blade geometry and technological effects are among the difficulties encountered by flow solvers.<br />

While the overall performance of turbomachinery elements in nominal conditions is usually well estimated<br />

(efficiency, pressure ratio, etc.) by classical RANS simulations, it is no longer true when an accurate<br />

description of the flow unsteadiness is necessary, especially at off-design conditions. In that context, LES<br />

could give a better understanding of the flow and thus allow considerable breakthrough in the machine<br />

design. LES has thus been performed with elsA on a whole 3D passage of a single transonic rotor of an<br />

axial compressor (the so-called NASA rotor 37 [26]). This test case is close to an industrial configuration<br />

(high Reynolds number 5 × 10 6 , supersonic tip Mach number, etc.). The results obtained with different<br />

”classical” numerical schemes (both upwind and centered schemes, second and third order) have been<br />

compared. A mesh convergence has also been conducted, considering from 10 to 100M cells to represent<br />

the blade passage. Results shows that a 3 rd order upwind scheme on a 100M cells mesh is necessary to<br />

obtain a correct description of the flow unsteadiness, such as the interaction between the boundary layer<br />

and the shock at the leading edge, Fig. 3.6(a). Moreover, the prediction of the efficiency by LES (that<br />

remains challenging in this configuration) is largely influenced by the grid density, Fig. 3.6(b).<br />

(a)<br />

(b)<br />

FIG. 3.6: LES results with elsA in NASA rotor 37 : (a) Instantaneous flow field shaded with the density<br />

gradient and (b) comparison of efficiency curves (grid 1 : 10M cells, grid 2 : 25M cells, grid 3 : 100M<br />

cells).<br />

The understanding of the route leading to unstable behaviors in centrifugal compressors is also of primary<br />

interest. Since most RANS flow solvers usually exhibit poor predictive capability at near stall conditions<br />

(especially regarding the physical phenomena that lead to surge), a study is currently under progress to apply<br />

and compare different approaches in elsA in a centrifugal compressor. The configuration is a high-pressure<br />

single stage compressor (Pi9), experimentally investigated at Ecole Centrale Lyon, which is representative<br />

of the SAFRAN Turbomeca engines.<br />

(U)RANS and hybrid RANS-LES (DDES type) have been tested on a centrifugal compressor complex flow.<br />

RANS simulations were performed using various turbulence model (Smith, Spalart and EARSM) on two<br />

grids of different refinement levels. The comparison with experiments shows a good agreement on a large<br />

range of mass flow, but some discrepancies appear on the prediction of the surge line position. DDES are<br />

currently investigated on the isolated rotor to study the effect of turbulence and secondary flows (such as<br />

the tip clearance flow) on the compressor stability.<br />

152 <strong>Jan</strong>. <strong>2010</strong> – <strong>Dec</strong>. <strong>2011</strong>

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!