NNMREC Arshiya Hoseyni Chime University of Washington Northwest National Marine Renewable Energy Center MSME Thesis Defense December 10 th, 2013.

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Presentation transcript:

NNMREC Arshiya Hoseyni Chime University of Washington Northwest National Marine Renewable Energy Center MSME Thesis Defense December 10 th, 2013

NNMREC US Water Resources & Usage 2 Water Resources Water Usage

NNMREC US Water Usage & Distribution 3

NNMREC US Water Usage & Distribution 4 Washington

NNMREC Columbia Basin Project US Bureau of Reclamation manages more than 47,000 miles of canals, drainages, and tunnels Columbia Basin Project 6,000 miles of channels 671,000 acres of farmlands 300 miles of main channel High flow rate capacity 5

NNMREC Flow Control High Hills Gates Courtesy of Professor Malte Tainter Gates 6

NNMREC Open Channel Flow Analysis Conservation of energy Fr 2 >1 => Supercritical Flow => Hydraulic Jump Conservation of Momentum 7 CV1 CV2

NNMREC Motivation Opportunity: Hydrokinetic turbines for flow control and power generation 8

NNMREC Motivation Pros Unidirectional Flow Cheaper than traditional hydropower (Dams) Easier permitting than tidal turbines Cons Small-scale power generation Farmers may not like the change from traditional control to new control 9

NNMREC Approach 1-D theoretical modeling 3-D CFD modeling  Turbines Actuator Disc Model Virtual Blade Model Comparison between models 10

NNMREC Approach 1-D theoretical modeling 3-D CFD modeling  Turbines Actuator Disc Model Virtual Blade Model Comparison between models 11

NNMREC 1-D Theory- Linear Momentum Theory Unconstrained Channel Power Coefficient 12 Betz limit

NNMREC 1-D Theory-Linear Momentum with blockage effects Constrained Channel Blockage Ratio Top View 13

NNMREC Constrained Channel Assumptions: No wake rotation No drag force No friction loss Uniform water depth at 3,4 and 5 4 Equations, 4 Unknowns (u 3, u 4, h 3, h 5 ) 14 1-D Theory-Linear Momentum with blockage effects

NNMREC Constrained Channel Assumptions: No wake rotation No drag force No friction loss Uniform water depth at 3,4 and 5 4 Equations, 4 Unknowns (u 3, u 4, h 3, h 5 ) 15 1-D Theory-Linear Momentum with blockage effects

NNMREC 1-D Theory- Channel Constriction Flow rate is constant Blockage Ratio is increased 5.1 m 5 m m 16 m 21 m 26 m 4m 16 BR=0.36 BR=0.48 4m

NNMREC Effect of Channel Constriction on Water Depth 17

NNMREC Effect of Channel Constriction on Power Generation 18

NNMREC Approach 1-D theoretical modeling 3-D CFD modeling  Turbines Actuator Disc Model Virtual Blade Model Comparison between models 19

NNMREC CFD- ADM, VBM ANSYS Fluent14.0 RANS Equations SST turbulence model Coupled Pseudo-Transient Solver Volume of Fluid Model Free surface is at VF=0.5 20

NNMREC CFD-Meshing Number of cells 16m wide channel3.3 million 21m wide channel4.2 million 21

NNMREC CFD-Boundary Conditions Mass flow inlet Pressure outlet No slip at walls D=4 m t= 0.2 m water air 30 m60 m 5 m 2.5 m 132,850 kg/s 50 kg/s 2.5 m 3 turbines(4m diameter) Turbulence BC: 22

NNMREC Approach 1-D theoretical modeling 3-D CFD modeling  Turbines Actuator Disc Model Virtual Blade Model Comparison between models 23

NNMREC CFD-Actuator Disc Model Porous Media Model C2 is inertial resistance of the porous media  P is based on 1-D theory at a given induction factor 24

NNMREC ADM- Velocity Contours BR=0.36 Fr=0.18 BR=0.48 Fr=

NNMREC ADM- Normalized Velocity BR=0.36 Fr=0.18 BR=0.48 Fr= Normalized Velocity Normalized water depth

NNMREC ADM- Dynamic Pressure BR=0.36 Fr=0.18 BR=0.48 Fr=

NNMREC Free Surface Elevation-Subcritical 28 Channel Length [m] Normalized Surface Elevation

NNMREC Supercritical(16m) Induction factor=0.6 Outlet depth and Inertial Resistance from 1-D theory 29 Velocity [m/s]

NNMREC 1-D theoretical modeling 3-D CFD modeling  Turbines Actuator Disc Model Virtual Blade Model Comparison between models Approach 30

NNMREC CFD-Virtual Blade Model Blade Element Theory VBM Input: Tip effect=96% 31

NNMREC VBM- Blade Design 32 Bahaj, 2004 c=50cm c=40cm Chord Distribution

NNMREC VBM-Cavitation Analysis Cavitation occurs when local pressure is lower than vapor pressure 33

NNMREC VBM- Cavitation Analysis 34

NNMREC VBM- Cavitation Analysis Cavitation number Cavitation occurs 35

NNMREC Cavitation- Pitching limit 36 Cavitation Number at the tip TSR=5

NNMREC Operating Condition TSR=5 Pitch the blades from -5 to 10 as long as AOA <8 4 Blades 37 Hub (D=80cm)

NNMREC VBM-Results BR=0.48 Fr=

NNMREC VBM- Power Coefficient kw 75 kw

NNMREC VBM- Dissipation Coefficient 360kw 270 kw 40 Useful power extraction by the turbines Mixing Wake rotation

NNMREC Replacing Gates by Turbines 41 15D Goal: Dissipate 1 MW

NNMREC 1-D theoretical modeling 3-D CFD modeling  Turbines Actuator Disc Model Virtual Blade Model Comparison between models Approach 42

NNMREC Comparison between models 43 Computation Time Turbine Inputs 1-D TheoryInstanta ADM6 hoursC 2 =f(a, ∆p) VBM2 days TSR, θ p,0

NNMREC Comparison to VBM 44 ADM a,Δp VBM 1-D theory a BR=0.48

NNMREC Conclusion At higher BRs, higher power extraction by turbines and higher power dissipation of the flow Turbines must be designed for the specific channel geometry to be optimized Cavitation Analysis is important to find out operating limits of the turbines 4 arrays of turbines are required to replace an array of gates At high BRs, 1-D theory and ADM over predict extracted power and under predicts the dissipated power 45

NNMREC Acknowledgement Professor Malte Professor Riley Dr. Novosselov Megan Karalus and Shazib Vijlee Northwest National Marine Renewable Energy Center Department of Energy 46