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Transcript of 1 DLES, Ercoftac Workshop, Trieste, 8-10 September 2008 LES of turbulent flow through a heated rod...
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DLES, Ercoftac Workshop, Trieste, 8-10 September 2008
LES of turbulent flow through a heated rod bundle arranged in a
triangular array.
S. Rolfo, J C Uribe and D. Laurence
The University of Manchester, M60 1QD, UKSchool of Mechanical, Aerospace & Civil Engineering.
CFD group
The
Uni
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of M
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Summary
Introduction:
• Code_Saturne
• RANS/LES coupling
• Rod Bundle test case
Results:
• Flow pulsations
• Average field
Conclusions
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Code_Saturne
Code developed by EdF and now open source downloadable from:
http://rd.edf.com/code_saturne
Unstructured
Co-located, Finite Volume Formulation
Different turbulent models (both RANS and LES)
Incompressible or expandable flows with or without heat transfer
Different modules: radiative heat transfer, combustion, magneto-hydrodynamics, compressible flows, two-phase flows
Possible coupling with Code_Aster for structural analysis and with Syrthes for thermal analysis.
Parallel code coupling capabilities (awarded the Gold medal on HPCx)
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RANS-LES coupling (1)
The Hybrid RANS-LES method is following a usual LES decomposition in large scale and sub-grid part:
The anisotropic part of the residual stress tensor and residual heat flux can be decomposed following a Schumann decomposition:
Sub- grid viscosity
RANS viscosity computed from the mean velocity field
For the eddy conductivity a simply turbulent Prandtl number analogy is used
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RANS-LES coupling (2)
The merging between the two velocity fields is done through a blending function to obtain a smooth transition
Turbulent RANS length scale computed with a relaxation model based on
Filter widthEmpirical constants computed in order to match the stress profile for channel flow @ Re = 395
Under-resolved standard LES
Hybrid results with meshSize ~ 0.1 mil cell
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Rod Bundle arranged in a triangular array• Experimental work:
I. Secondary flow : Vonka “Measurement of secondary vortices in Rod Bundle” Nuclear Engineering and Design, Volume 106, Issue 2, 2 February 1988, Pages 191-207
II. Flow pulsations: Krauss, Meyer “Experimental investigation of turbulent transport of momentum and energy in a heated rod bundle”, Nuclear Engineering and Design, Volume 180, Issue 3, April 1998, Pages 185-206
• CFD work (URANS):
1. E. Merzari, H. Ninokata, E. Baglietto “Numerical simulation of flows in tight-lattice fuel bundles Nuclear Engineering and Design”, Volume 238, Issue 7, July 2008, Pages 1703-1719 .
2. D. Chang, S. Tavoularis “Simulations of turbulence, heat transfer and mixing across narrow gaps between rod-bundle sub-channels” Nuclear Engineering and Design, Volume 238, Issue 1, January 2008, Pages 109-123
13 @Re 60000.93
112 @Re 39000Gap
f HzfDSt
f HzU
From II
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Rod Bundle: Cases definitionTwo different geometrical configuration
1. P/D = 1.06I. LES @ Re = 6000 Mesh size ~ 1.6 Million cells with Heat transfer.
– 0.75<Δr+<1.06 – 7.5<rΔθ+<11 – 16<Δx+<22.5
II. Hybrid @ Re = 6000 Mesh size ~ 0.35 Million cells with Heat transfer – 0.8<Δr+<1.3 – 15<rΔθ+<20 – 40<Δx+<60
III. Hybrid @ Re = 39000 Mesh size ~ 0.9 Million cells no Heat transfer – 0.8<Δr+<1.2 – 20<rΔθ+<25 – 50<Δx+<70
2. P/D = 1.15 I. LES @ Re = 6000 Mesh size ~ 1.4 Million cells no Heat transfer
– 0.8<Δr+<1.1 – 6.5<rΔθ+<10 – 16<Δx+<22.5
All the domains have a stream-wise length equal to 12 times the hydraulic diameter
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Results: Flow Pulsation in the mid-plane
Hybid @ Re = 6000LES P/D=1.15 @ Re = 6000
LES @ Re = 6000
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Conclusions and future work LES
Flow Fluctuations detected, Presence of a second dominant frequency has to be verified with bigger domain.
Hybrid Flow pulsations detected and dominant frequency in according with LES Problem in the near wall region. Possible reason blending function Same problem for the heat transfer
Future work Calibration of the wall function for the Rod Bundle (in progress) Improvement heat transfer with a dynamic turbulent Prandtl number LES computations with bigger cross section to verify the dominant frequencies Improved geometry with addition of wire wrapped around the pin (SFR reactor).
AcknowledgementsAcknowledgements This work was carried out as part of the TSEC programme KNOO and as such we are
grateful to the EPSRC for funding under grant EP/C549465/1.