Tidal Energy Extraction in an Idealized Ocean- Fjord Tidal Model with Astronomical Forcing EWTEC 2013, Aalborg, Denmark, September 2012 Mitsuhiro Kawase.

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Tidal Energy Extraction in an Idealized Ocean- Fjord Tidal Model with Astronomical Forcing EWTEC 2013, Aalborg, Denmark, September 2012 Mitsuhiro Kawase and Marisa Gedney Northwest National Marine Renewable Energy Center / School of Oceanography University of Washington Seattle WA United States

Acknowledgment Funding for this project was provided by U.S. Department of Energy Award Number DE-FG36- 08GO18179 Sandia National Laboratory

Contents Introduction / Motivation Model: Set-up, output and diagnosis Energetics of tidal energy extraction Subdomain model experiments Summary / Take-home points

Munk and Wunsch (1998) Global Ocean Energy Schematic Tide is a Source of Energy for Oceanic and Coastal Processes: Divert to Tidal Energy Generation

Tidal energy is globally harvested from gravity of sun and moon and transported by wave process: Regional hydrodynamic models receive tides from boundary conditions, and are often heavily “tuned” to reproduce tides as observed. R. Ray, GSFC Kawase and Thyng, 2010

Questions Addressed by This Study How does tidal energy extraction look like in the context of regional / global tidal energetics? What useful things might we learn from such a perspective? What are significant limitations (if any) of studying tidal energy extraction with a regional model? What are the uncertainties in energy extraction estimates made using regional models?

Approach: Construct an idealized numerical model of an ocean-estuary tidal system Ocean with 4000m-deep basin and 200m-deep, 500km-wide continental shelf Tide is forced astronomically by tide-generating force (TGF, lunar tide, 20° declination) 10km-wide silled “fjord” is appended at the northeastern corner. Normal case (200km long) Resonant case (400km long) Tidal energy is extracted over the sill (locally enhanced quadratic drag). The model serves boundary conditions to subdomain models: Regional model Coastal model

Model Tidal Response: Non-resonant Fjord

Energy Balance Equation For any model subdomain, Influx at the BoundaryNatural Dissipation Energy ExtractionGain from TGF C N = C E = Varied

Energy Balance Equation For equilibrium, average over tidal period, Influx at the BoundaryNatural Dissipation Energy ExtractionGain from TGF

Energy Extraction and Tidal Range Change Energy Extraction Tidal Range Extraction Coeff. C E MW meters

Energy Extraction vs. Tidal Range Energy Extraction (MW) Tidal Range (meters)

274MW 163MW Energetics of the Fjord: Non-resonant Case Energy Flux Natural Dissipation Change in Ocean Energy Flux MW W/m 2

There is no clearly defined outer boundary to the region from which the extracted energy is drawn – response to energy extraction is global. r Mechanical Energy Flux Feeding Energy Extraction

Why should we care about reduction in natural dissipation due to tidal energy development? Simpson, et al. (1990) Entrainment of dense water by tidal stirring (Potential energy creation) (Simpson and Bowers 1981) Partially / Fully Mixed Estuaries Always sufficient estuary length / kinetic energy available  exchange insensitive to reduction in u T ? (Stommel and Farmer 1953; MacCready and Geyer 2010) However, other estuarine characteristics (e.g. salt intrusion length) might be strongly affected. Fjords Exchange always limited by the amount of entrainment that can occur within a basin of fixed size (Knudsen 1900; Proudman 1953)  exchange highly sensitive?

958MW 1.57GW Energetics of the Fjord: Resonant Case Energy Flux Natural Dissipation Change in Ocean Energy Flux MW W/m 2

Subdomain Model Experiments

Full Domain ModelSubdomain Models Energy Extraction Experiments Boundary condition Intercomparison Subdomain Model Experiments

Energy Extraction vs. Tidal Range: Normalized

Energy Extraction vs. Tidal Range: Unscaled 298MW 247MW 182MW 562MW 657MW 679MW

Full Domain (MW) Regional Model (MW)Coastal Model (MW) Dirichlet Dirichlet, TGF CFCF, TGF DirichletDirichlet, TGF CFCF, TGF Non-resonant (-26%) 201 (-17%) 145 (-43%) 235 (-5%) 298 (+21%) 296 (+20%) 246 (<+1%) 244 (+1%) Resonant (-14%) 589 (-10%) 538 (-18%) 754 (+15%) 679 (+3%) 657 (0%) 698 (+6%) 689 (+5%) CF = Chapman – Flather boundary condition Effect of Tide-Generating Force and Boundary Conditions on Maximum Extractable Energy

Summary Energy is extracted from a tidal estuary in part at the expense of natural energy flux into estuarine processes Regional hydrodynamic models used for tidal energy applications should have its natural energetics validated Limited-domain representation does not fundamentally change the physics of the energy extraction processes Introduces uncertainty of up to ~25% in the carrying capacity of the estuary With judicious choice of domain and boundary conditions, this could possibly be reduced down to ~10% (further research needed)