CERFACS CERFACS Scientific Activity Report Jan. 2010 â Dec. 2011
CERFACS CERFACS Scientific Activity Report Jan. 2010 â Dec. 2011
CERFACS CERFACS Scientific Activity Report Jan. 2010 â Dec. 2011
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TURBOMACHINERY<br />
of each component, the flow is not necessarily solved with the same numerical method in the whole<br />
system. For example, previous works indicate that LES is a very efficient method for predicting reactive<br />
flows in a combustion chamber while RANS based approaches are more convenient for turbomachines.<br />
Based on a literature review, the first step towards integrated simulations is to develop a framework to<br />
exchange information between the combustion chamber (LES with the unstructured code AVBP) and the<br />
high-pressure turbine (RANS with the structured code elsA). The coupling between AVBP and elsA has<br />
been developed using the Open-PALM code coupling tool. The technique is based on the exchange of the<br />
conservative variables from AVBP to elsA with a method similar to the Chimera approach while elsA sends<br />
the pressure information to define the outlet non-reflective boundary condition of AVBP. This coupling<br />
process is done at each iteration of the flow solver until convergence is achieved. It was validated in a<br />
simple test case : a laminar Poiseuille channel flow. The technique needs now to be validated and tested<br />
with more complex test cases.<br />
3.1.4 Code coupling methods : application to elsA / elsA (F. Crevel, M. Montagnac)<br />
For some specific applications the use of different time steps can be helpful to reduce the cost of an unsteady<br />
flow simulation. For example, to describe a surge cycle in a gas turbine, it is mandatory to simulate both high<br />
frequencies (generated by the blade passing frequency, o(10,000)Hz) and low frequencies (due to the surge<br />
phenomenon, o(1)Hz). A simulation with a unique time step would need very large computing resources to<br />
describe the low frequency phenomenon. In that context, a simulation that uses a large time step in parts<br />
where only the description of low-frequency is important, coupled with a simulation that uses small time<br />
steps (where high-frequencies must be computed) is an attractive approach. This method has been tested<br />
by coupling two elsA simulations (considering two different time steps) with the Open-PALM coupling tool.<br />
The coupling developed here is based on the exchange of conservative fields on an interface defined by<br />
the user. The simulations are time accurate, which means that if N is the ratio between the time steps<br />
used in the two simulations, the large-time-scale simulation does one time step while the small-time-step<br />
simulation does N time steps. The small-time-step simulation sends to Open-PALM N fields while the<br />
large-time-step simulation only sends one. Open-PALM allows to exchange fields after calculating a<br />
moving average in order to smooth the solution over a coupling period. The application was tested on a<br />
turbulent channel. The channel is split in two parts and a wake is injected in the upstream part. As shown<br />
in Fig. 3.2, the wake is well transmitted in the downstream channel by the coupling method.<br />
FIG. 3.2: Coupling of two elsA simulations with the code coupling tool Open-PALM. The fields, colored<br />
with the density, show that the wake generated at the inlet of the upstream channel (up) is transmitted to the<br />
downstream one (bottom).<br />
148 <strong>Jan</strong>. <strong>2010</strong> – <strong>Dec</strong>. <strong>2011</strong>