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Arhtur Hajaali, Prof T.Stoesser in collaboration with P.PĂŠpin (R&D GE Renewable Energy)
Assessment of Borda-Carnot losses on tidal power projects
coupling near-field and far-field CFD models.
Introduction
.
Why Tidal Power Energy?
• Department of Energy and Climate Change’s (DECC) UK aims at producing 20% of its energy from
renewables by 20201.
• The United-Kingdom and France possess 80% of the European tidal energy potential2.
• Predictable and reliable source of energy independent of the weather or seasons.
• Tidal water pumped into a secondary-basin, store and delay power generation to response to energy
grid demands.
Bulb Turbine:
• First developed in 1913 by Victor Kaplan.
• Low head turbine, most efficient with large flow rate.
• Designed and installed on first large-scale tidal power project3 (Rance, 1967, 240MW)
Project Aim
.
• Investigate the Borda-Carnot losses occurring between the mouth
of the draft-tube and the inlet of the bulb unit.
• Analyse the interaction between the outlet of the diffuser and the
estuary flow.
• Perform specific laboratory experiments to compare and validate
results from the CFD coding.
Methodology
.
Figure 2: Near-Field and Far-Field software configuration
Numerical analysis based on near-field and far-field CFD coupling:
Near-Field Model: (HYDRO3D)
• Use Large-Eddy Simulation (LES) method to model the complex swirls
and vortexes.
• Computationally demanding, hence coupled with a far-field model.
Far-Field Model: (FVCOM)
• Three-dimensional software based on RANS fundamental equations.
• Compute the estuary behaviour prior and subsequent to the bulb unit.
• Connect the sea behaviour (wave,secondary) as input for the near-field
model.
PhD Timeframe
Table 1: Gantt Chart
.
1. Study of near-field (FVCOM) and far-field (Hydro3D) CFD
software.
2. Define computational environment to assess the causes and the
behaviour of the Borda-Carnot losses.
3. Perform simulations and refine the CFD models of the Borda-
Carnot losses affecting the turbine efficiency.
4. Define specific laboratory experiences to collect results
regarding the Borda-Carnot losses affecting a real scaled bulb.
5. Study the eventual disparity and refine the CFD model.
(Scientific Paper #2)
6. Redaction of the PhD thesis.
References
.
1.Department of Energy and Climate Change (DECC). 2011. UK Renewable
Energy Roadmap.
2.De Laleu, V. (2009) La mer, nouvelle source d’énergies renouvelables ?
Available at: http://goo.gl/LnaHnb (Accessed: 12/06/2016)
3.Casacci, S. and Technique, D. (1973) ‘Les groupes bulbes Projets et
perspectives’, La Houille Blanche, doi: 10.1051/lhb/1973015.
Figure 1: Component of Bulb Unit

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WISE-CDT-Research-Poster-Template-A0-Size

  • 1. Arhtur Hajaali, Prof T.Stoesser in collaboration with P.PĂŠpin (R&D GE Renewable Energy) Assessment of Borda-Carnot losses on tidal power projects coupling near-field and far-field CFD models. Introduction . Why Tidal Power Energy? • Department of Energy and Climate Change’s (DECC) UK aims at producing 20% of its energy from renewables by 20201. • The United-Kingdom and France possess 80% of the European tidal energy potential2. • Predictable and reliable source of energy independent of the weather or seasons. • Tidal water pumped into a secondary-basin, store and delay power generation to response to energy grid demands. Bulb Turbine: • First developed in 1913 by Victor Kaplan. • Low head turbine, most efficient with large flow rate. • Designed and installed on first large-scale tidal power project3 (Rance, 1967, 240MW) Project Aim . • Investigate the Borda-Carnot losses occurring between the mouth of the draft-tube and the inlet of the bulb unit. • Analyse the interaction between the outlet of the diffuser and the estuary flow. • Perform specific laboratory experiments to compare and validate results from the CFD coding. Methodology . Figure 2: Near-Field and Far-Field software configuration Numerical analysis based on near-field and far-field CFD coupling: Near-Field Model: (HYDRO3D) • Use Large-Eddy Simulation (LES) method to model the complex swirls and vortexes. • Computationally demanding, hence coupled with a far-field model. Far-Field Model: (FVCOM) • Three-dimensional software based on RANS fundamental equations. • Compute the estuary behaviour prior and subsequent to the bulb unit. • Connect the sea behaviour (wave,secondary) as input for the near-field model. PhD Timeframe Table 1: Gantt Chart . 1. Study of near-field (FVCOM) and far-field (Hydro3D) CFD software. 2. Define computational environment to assess the causes and the behaviour of the Borda-Carnot losses. 3. Perform simulations and refine the CFD models of the Borda- Carnot losses affecting the turbine efficiency. 4. Define specific laboratory experiences to collect results regarding the Borda-Carnot losses affecting a real scaled bulb. 5. Study the eventual disparity and refine the CFD model. (Scientific Paper #2) 6. Redaction of the PhD thesis. References . 1.Department of Energy and Climate Change (DECC). 2011. UK Renewable Energy Roadmap. 2.De Laleu, V. (2009) La mer, nouvelle source d’énergies renouvelables ? Available at: http://goo.gl/LnaHnb (Accessed: 12/06/2016) 3.Casacci, S. and Technique, D. (1973) ‘Les groupes bulbes Projets et perspectives’, La Houille Blanche, doi: 10.1051/lhb/1973015. Figure 1: Component of Bulb Unit