wave energy

1- Introduction

  • Objective: discuss the potential contribution of ocean energy to overall energy supply and climate mitigation.

  • Renewable ocean energy originates from six distinct sources, each with different origins and requiring different conversion technologies:

    • Waves: energy from the wind transferred to the upper ocean surface; stores as potential energy (mass displacement from mean sea level) and kinetic energy (motion of water particles).

    • Tidal Range: rise and fall driven by Earth–Moon–Sun gravitation and rotational effects.

    • Tidal Currents: water flow resulting from tidal range (filling/emptying of coastal regions).

    • Ocean Currents: wind-driven and thermohaline circulation.

    • Ocean Thermal Energy Conversion (OTEC): energy from temperature differences between surface (solar-heated) water and colder water below ~1000 m.

    • Salinity Gradients (osmotic power): energy from salinity differences between freshwater and seawater at river mouths.

2- Ocean energy

A. Wave energy

  • Wave energy is the energy transferred from wind to the ocean.

  • Energy storage forms:

    • Potential energy: due to water mass displaced from the mean sea level.

    • Kinetic energy: due to motion of water particles.

  • Wave size and period depend on:

    • Wind speed

    • Duration of wind blowing (order of days)

    • Fetch: distance over which the wind blows across the ocean.

  • Waves efficiently transfer energy and can travel long distances as swells beyond storm regions.

  • Most energetic waves are generated between 30° and 60° latitudes by extratropical storms.

B. Tidal range

  • Tides are regular, predictable changes in ocean height due to gravitational and rotational forces among Earth, Moon, and Sun, plus centrifugal and inertial effects.

  • Common tidal patterns:

    • Semi-diurnal: roughly two high tides and two low tides per day.

    • Diurnal: only one high and one low tide per day.

  • Tidal day (lunar day): 24 h 50 min; this shifts the timing of successive high/low tides daily.

  • Diurnal and semi-diurnal tides occur at different times in different locations.

  • Tides vary in amplitude over the year due to relative Earth–Moon–Sun positions.

  • Spring tides: maximum tidal range when Sun, Moon, and Earth align (full moon and new moon).

  • Neap tides: minimum tidal range when Earth–Moon axis is at 90° to Earth–Sun axis.

  • Tide timing and magnitude depend on: global position, ocean bed shape, shoreline geometry, and Coriolis acceleration.

  • Amphidromic points: locations where tidal range is nearly zero, yet tidal currents may remain high due to differences in water surface levels on either side.

C. Tidal currents

  • Tidal currents are the horizontal water movements within tidal systems, driven by the rise and fall of tides.

  • Currents are generated by horizontal water movement and modulated by seabed bathymetry, especially near coasts or constrictions (e.g., islands).

  • Timing and magnitude of tidal currents are highly predictable and largely insensitive to climate change.

  • Near-shore currents exist; significant currents also occur in open ocean, with some regions (e.g., western boundary currents) offering sufficient velocities (~2 m/s) to drive present-day technologies.

D. Ocean currents

  • Ocean currents are continuous, directed water movements driven by multiple forces: wind, Coriolis effect, breaking waves, and temperature/salinity differences.

  • About 15% of the total solar input to the ocean is retained as thermal energy, concentrated at the surface and decreasing with depth due to low thermal conductivity.

  • Surface water temperatures can exceed +25°C in the tropics, while temperatures ~1,000 m depth range from +5°C to +10°C.

E. Ocean Thermal Energy Conversion (OTEC)

  • OTEC relies on temperature differences between surface warm water and colder deep water to generate electricity.

  • A minimum temperature difference of oxed{ riangle T 1 20^
    ing C } is generally required to operate an OTEC plant.

  • OTEC resources: an annual average temperature difference map shows tropical areas with potential greater than 20<br>ingC20^<br>ing C.

  • Characteristics:

    • OTEC provides continuously available (base-load) energy, albeit with low energy density compared with wave/tidal energy.

    • Seasonal variation exists (slight between seasons).

F. Salinity gradients (osmotic power)

  • Energy arises from mixing freshwater with seawater across a semi-permeable membrane, driven by chemical potential differences.

  • Two main concepts: Reversed Electro-Dialysis (RED) and Pressure-Retarded Osmosis (PRO).

  • RED: uses a stack of alternating anion and cation exchange membranes to generate voltage from chemical potential differences.

  • PRO: uses osmotic pressure difference as the driving force; seawater and freshwater have a tendency to mix; membranes permit selective water flow, generating pressure.

  • Osmotic pressure definition: oxed{ oxed{ 1 = i imes n imes R imes T } } where:

    • ii is the Van 't Hoff index, representing the number of particles formed per dissolved substance.

    • nn is molar concentration (mol/L).

    • RR is the ideal gas constant.

    • TT is temperature in Kelvin.

  • Typical osmotic pressure ranges for seawater vs freshwater: around 2.42.6extMPa2.4-2.6 ext{ MPa} (24–26 bar).

  • Operational pre-pressurization: seawater is pressurized to about half the osmotic pressure, ~1.21.3extMPa1.2-1.3 ext{ MPa} (12–13 bar).

  • In membrane modules, freshwater migrates through the membrane into pressurized seawater, producing brackish water that is split into two streams.

  • Power production distribution in PRO: roughly one-third goes to a hydropower turbine, while the remainder passes through a pressure exchanger to pressurize incoming seawater.

  • Brackish water can be returned to river or sea, with mixing of sources over time.

3- Technology and applications of wave energy

  • Numerous wave energy technologies exist, with demonstrations across operation principles to convert wave energy.

  • Major variables in wave energy systems:

    • Mode of wave interaction with devices (heaving, surging, pitching).

    • Water depth (deep, intermediate, shallow).

    • Distance from shore (shoreline, nearshore, offshore).

  • A generic wave energy device scheme comprises three conversion stages:

    • Primary interface: fluid-mechanical processes that feed mechanical power to the next stage.

    • Secondary subsystem: can provide direct drive or short-term storage to facilitate power processing before electrical conversion.

    • Tertiary conversion: electromechanical and electrical processes.

  • Wave energy converters are categorized by location, size, and operating principle:

    • Location-based categories:

    • Shoreline devices: attached to/embedded in boundary; easier maintenance; shorter offshore cables but potentially weaker wave regimes.

    • Nearshore devices: suitable for moderate depths (10–25 m); example: a 2 MW device with a 1.5 MW wind turbine potential to be added; aims to maximize energy in close-to-shore areas; environmental considerations may limit large nearshore farms.

    • Offshore devices: target high-power waves (> 40 m depth) before energy dissipation devices.

  • Wave energy converters (WECs) types by geometry/orientation:

    • Point absorbers: small in diameter relative to wavelength; move to harvest energy from the wave motion in all directions, converting up/down pitching into rotary/oscillatory motion.

    • Attenuators: elongated structures aligned with the wave direction; consist of multiple cylindrical sections connected by hinges; sections move relative to each other.

    • Terminators: long devices perpendicular to the main wave direction; stationary or rotating to dissipate wave energy.

  • Other operating-principle categories:

    • Pressure differential devices: oscillating water columns (OWC) and Archimedes principle converters; typically shoreline-adjacent.

    • Overtopping devices: fluids collected above sea level and released through turbines; axial-flow turbines commonly used for low heads.

    • Impact/surge devices: flexible/ articulated structures that move water mass within a constrained chamber.

  • Wells turbine (example of pressure differential concept):

    • Self-rectifying air turbine with symmetric blades and no flow-direction-dependent twisting; rotates in the same direction regardless of airflow direction.

    • Advantages: no guide vane is required; simplification of design.

    • Drawbacks: noisy operation, narrow operating range, reduced torque at low flow; higher angle of attack causes flow separation and stall, reducing power extraction.

  • Wells turbine theory of operation and performance metrics (as given in the example):

    • General coefficients:

    • Torque coefficient: C_T = rac{T}{
      ho 1 ext{omega}^2 R^5}

    • Stagnation pressure drop coefficient: C{po} = rac{ riangle Po}{
      ho 1 ext{omega}^2 R^2}

    • Turbine efficiency: oxed{ oxed{ 1 = rac{T ext{omega} riangle P_o}{Q} } }

    • Flow coefficient: oxed{ oxed{ 1 = rac{C_x}{U} } }
      where:

    • C<em>xC<em>x = axial flow velocity, UU = rotor tip speed, TT = torque, hoho = density, extomegaext{omega} = angular velocity, RR = rotor tip radius, riangleP</em>oriangle P</em>o = total pressure drop, extQext{Q} = volume flow rate.

    • Example values (Wells turbine):

    • Tip diameter: DT=588extmm<br>ightarrowR=294extmmD_T = 588 ext{ mm} <br>ightarrow R = 294 ext{ mm}

    • Hub diameter: DH=400extmmD_H = 400 ext{ mm}

    • Tip clearance: t=1extmmt = 1 ext{ mm}

    • Rotational speed: N = 2000 ext{ rpm} \Rightarrow 1 = rac{2\u03c0 N}{60} = 209.33 ext{ rad/s}

    • Flow velocity at inlet: V=12.31extm/sV = 12.31 ext{ m/s}

    • Torque: T=12.79extNmT = 12.79 ext{ N·m}

    • Total pressure loss: rianglePo=2476extPariangle P_o = 2476 ext{ Pa}

    • Air density: <br>ho=1.225extkg/m3<br>ho = 1.225 ext{ kg/m}^3

    • Derived quantities (from the example):

    • Flow area: A = rac{1}{4}igl(DC^2 - DH^2igr) = rac{1}{4} igl( (DT + 2t)^2 - DH^2 igr) = 0.147 ext{ m}^2

    • Volume flow rate: Q=CxA=12.31imes0.147=1.81extm3/extsQ = C_x A = 12.31 imes 0.147 = 1.81 ext{ m}^3/ ext{s}

    • Rotor tip speed: U = 1 imes R = 209.33 imes 0.294 = 61.54 ext{ m/s}

    • Torque coefficient: C_T = rac{T}{
      ho 1^2 R^5} = rac{12.79}{1.225 imes 209.33^2 imes 0.294^5} \approx 0.1084

    • Stagnation pressure drop coefficient: C{po} = rac{ riangle Po}{
      ho 1^2 R^2} = rac{2476}{1.225 imes 209.33^2 imes 0.294^2} \approx 0.053

    • Efficiency: 1 = rac{T ext{omega} riangle P_o}{Q} = rac{12.79 imes 209.33 imes 2476}{1.81} \approx 60.24 ext{%}

    • Flow coefficient: 1 = rac{C_x}{U} = rac{12.31}{61.54} \approx 0.20

  • Research trends in Wells turbine (examples and references): near blade tip and casing groove, near blade tip and casing endplate design, near blade trailing edge Gurney flap, static extended trailing edge, and radiused edge blade tips.

    • References (examples):

    • Halder et al. (2015): High-performance ocean energy harvesting turbine design – casing treatment scheme. Energy, 86, 219–231. doi:10.1016/j.energy.2015.03.131

    • Madhan Kumar et al. (2021): Combined casing groove and blade tip treatment for wave energy harvesting turbine.

    • Das et al. (2022): Performance improvement of a Wells turbine through automated optimization technique. Energy Conversion and Management: X, 16, 100285. doi:10.1016/j.ecmx.2022.100285

    • Kotb et al. (2021): Potential of performance improvement of a modified Wells turbine using passive control for wave energy conversion. Ocean Engineering, 242, 110178. doi:10.1016/j.oceaneng.2021.110178

    • Kumar et al. (2019): Performance enhancement of Wells turbine: Combined radiused edge blade tip, static extended trailing edge, and variable thickness modifications. Ocean Engineering, 185, 47–58. doi:10.1016/j.oceaneng.2019.05.041

  • Example recap: Wells turbine specs and computed performance metrics illustrate how design choices affect efficiency, pressure loss, and energy capture.

4- Technology and applications of tidal range

  • Tidal range development has historically focused on estuarine sites using a barrage to enclose an estuary and drive conventional low-head hydro turbines; a barrage can operate in both directions to generate electricity from incoming and outgoing tides.

  • Barrages create a reservoir (basin) with turbines between the inlet and the basin.

  • Alternative barrage configurations include multi-basin operations where basins fill and empty at different times; turbines are located between basins; such schemes can provide more flexible, near-continuous power generation.

  • The latest advances focus on offshore basins, i.e., tidal lagoons—single or multiple lagoons located away from estuaries.

  • A tidal lagoon is formed by installing a retaining wall across a bay or extending from the coast, creating ponds of water that are discharged through turbines at low tide.

  • The conversion mechanism most widely used for tidal range electricity is the bulb-turbine.

  • Typical capacity factor for tidal power stations is estimated to vary from 25 ext{% to }35 ext{%}.

5- Technology and applications of tidal and ocean currents

  • Technologies to extract kinetic energy from tidal, river, and ocean currents are under development; tidal energy converters are the most mature to date.

  • Key difference: river/ocean currents are generally unidirectional, while tidal currents reverse between ebb and flood; thus tidal turbines are designed to generate in both directions.

  • Turbines are classified by principle of operation: axial-flow, cross-flow, and reciprocating devices.

  • On a single device, multiple turbines may be used (examples often show multiple rotors).

  • Design considerations include:

    • Reversing flow (tidal) needs bidirectional or reversible designs.

    • Cavitation and harsh underwater conditions (salt water, debris, fouling).

    • Axial-flow turbines can reverse nacelle direction with each tide or use fixed nacelle with blades that tolerate bidirectional flow.

    • Rotor shrouds (cowlings/ducts) can improve hydrodynamic performance by increasing rotor velocity and reducing tip losses.

    • Economic balance: the energy gained by shrouds must offset the additional cost over the device life.

    • Turbine siting is crucial due to wake effects and to optimize array deployments (akin to wind farms).

6- Technology and applications of ocean thermal energy conversion (OTEC)

  • OTEC plants can use three conversion schemes: open cycle, closed cycle, and hybrid.

  • Open cycle: water serves as the working fluid.

    • Surface seawater is pumped into a low-pressure chamber where evaporation occurs.

    • The low-pressure steam drives a turbine; evaporated steam can be discharged into the ocean or condensed with seawater to produce desalinated water.

  • Closed cycle: uses a working fluid such as ammonia or freon in a low-temperature Rankine cycle.

    • Surface seawater passes through an evaporator to vaporize the working fluid.

    • The vapor drives a turbine; the vapor is condensed by cold seawater typically from depths below 1000 m.

  • Hybrid cycle: combines attributes of closed and open cycles; after heating, seawater enters a flash evaporator, with partial desalination.

  • Challenges of OTEC include maintaining vacuums, biofouling and corrosion in heat exchangers, and reliable long-term operation.

7- Technology and applications of salinity gradients

  • Energy arises from mixing freshwater and seawater; the heat effect is small.

  • RED and PRO are the main concepts for converting this chemical potential into electricity.

  • Reversed electro dialysis (RED): uses an array of anion/cation exchange membranes to generate a voltage from chemical potential differences between concentrated salt solutions and freshwater.

    • The chemical potential difference generates voltage across membranes; the total system potential is the sum of membrane voltages.

  • Pressure-retarded osmosis (PRO): uses osmosis (osmotic pressure difference) as the driving force; the difference in salt concentration creates a driving force for water flux through semipermeable membranes.

  • Osmotic pressure formula (Van 't Hoff): oxed{ 1 = i imes n imes R imes T }

    • i = Van 't Hoff index (number of particles per dissolved substance).

    • n = molar concentration (mol/L).

    • R = 0.08206 L·atm·mol⁻¹·K⁻¹.

    • T = temperature in Kelvin.

  • For seawater and freshwater, typical osmotic pressure differences are about 2.42.6extMPa2.4-2.6 ext{ MPa} (24–26 bar).

  • Pre-pressurization: seawater is pressurized to about half the osmotic pressure, approx. 1.21.3extMPa1.2-1.3 ext{ MPa} (12–13 bar).

  • In PRO membranes, freshwater migrates into pressurized seawater, producing a brackish stream; the brackish water can be split into streams for power generation and pressurization.

8- Summary of practical considerations and connections

  • Ocean energy sources offer complementary options for a diversified renewable energy portfolio: waves provide high energy density but spatially variable; tides and currents offer predictable resources; OTEC and salinity gradient technologies provide base-load potential in suitable regions.

  • Technological maturity varies by resource: tidal range and salinity gradients have seen practical deployments, while many ocean current and osmotic concepts are still under development.

  • Environmental, economic, and grid integration considerations drive device siting, scale, and combination with other renewables.

  • Research and development focus areas include: improving device efficiency, reducing costs (e.g., through loss reduction, array optimization, and passive flow-control strategies), and addressing reliability and maintenance challenges underwater.

9- Quick reference: Key values and concepts from the material

  • Global theoretical wave energy potential: 32,000extTWh/yr32{,}000 ext{ TWh/yr} (roughly twice the 2008 global electricity supply of 16,800extTWh/yr16{,}800 ext{ TWh/yr}).

  • Latitude range associated with the most energetic ocean winds (30°–60°).

  • Open-cycle OTEC concept uses surface water as working fluid; closed-cycle uses ammonia or Freon; hybrid combines both.

  • Tidal lagoon capacity factor: 25 ext{%}–35 ext{%}.

  • Shallow to intermediate water depths (10–25 m) are typical for nearshore wave devices; offshore devices target deeper waters (>40 m).

  • Tidal current speeds around 2extm/s2 ext{ m/s} in favorable regions.

  • Example Wells turbine (numerical):

    • Tip diameter: D<em>T=588extmmD<em>T = 588 ext{ mm}; hub diameter: D</em>H=400extmmD</em>H = 400 ext{ mm}; tip clearance: t=1extmmt = 1 ext{ mm}.

    • Rotation: N=2000extrpmN = 2000 ext{ rpm}; wind speed: V=12.31extm/sV = 12.31 ext{ m/s}; torque: T=12.79extNmT = 12.79 ext{ N·m};

    • Pressure loss: rianglePo=2476extPariangle P_o = 2476 ext{ Pa}; density: <br>ho=1.225extkg/m3<br>ho = 1.225 ext{ kg/m}^3.

  • Wells turbine derived coefficients (example):

    • CText(torquecoefficient)0.1084C_T ext{ (torque coefficient)} \approx 0.1084

    • Cpoext(stagnationpressuredropcoefficient)0.053C_{po} ext{ (stagnation pressure drop coefficient)} \approx 0.053

    • 1 ext{ (efficiency)} \approx 60.24 ext{%}

    • 1 ext{ (flow coefficient)} \approx 0.20

  • Osmotic pressure example: for a 2.0 M NaCl solution at 30°C and 200 L water, 1 \approx 0.497 ext{ atm} (illustrative calculation shown in the source).