Ocean Thermal Energy Conversion (OTEC)

Exploits the temperature difference between warm tropical surface seawater and cold deep seawater to drive a heat engine for electricity generation.

Fundamental Principle

Solar Energy Stored in Thermal Gradients

OTEC exploits the temperature difference between warm surface seawater and cold deep seawater to drive a heat engine. The ocean acts as an enormous solar collector: tropical surface waters absorb solar radiation and maintain temperatures of 24-29°C year-round, while water below 800-1000m remains at 4-6°C due to the global thermohaline circulation that brings cold polar water to tropical depths.

This thermal gradient represents stored solar energy of staggering scale. On an average day, tropical seas absorb solar radiation equivalent in heat content to approximately 250 billion barrels of oil. The global theoretical potential for OTEC has been estimated at 8-30 TW, with practical potential around 3-5 TW when accounting for geographic constraints and environmental limits. This exceeds current global electricity consumption (~3 TW average) and dwarfs other ocean energy sources (wave: ~0.5 TW practical, tidal: ~0.1 TW practical).

Geographic Distribution

The necessary thermal gradient (minimum ΔT ≈ 20°C between surface and 1000m depth) exists primarily between latitudes 20°N and 20°S. Within this tropical band:

  • 98 countries and territories have potential OTEC resources
  • Best resources: Caribbean, Pacific islands, Southeast Asia, East African coast, northern Australia
  • Ideal sites combine steep bathymetry (deep water close to shore) with consistently warm surface waters
  • Islands with short distances to 1000m depth are most economically favorable

The resource is remarkably stable compared to other renewables: the thermal gradient varies only ~20% seasonally (vs. 200-400% for solar/wind) and maintains 24/7, 365-day availability. El Niño/La Niña events can cause larger variations (up to 50%) in some Pacific locations.

Thermodynamic Constraint

OTEC operates as a heat engine between two reservoirs. The fundamental limit is the Carnot efficiency:

equation carnot_otec $$\eta_{Carnot} = \frac{T_H - T_C}{T_H} = \frac{\Delta T}{T_H}$$ :::

For typical OTEC conditions (T_H = 28°C = 301 K, T_C = 4°C = 277 K, ΔT = 24 K):

$$\eta_{Carnot} = \frac{24}{301} = 7.97%$$

This is the theoretical maximum. No OTEC system can exceed ~8% thermal efficiency regardless of engineering improvements. :::

Compare this to:

The low efficiency is not a flaw but an inherent consequence of the small temperature difference. However, the "fuel" (ocean thermal energy) is free, abundant, and renewable.

Conversion Mechanism

System Types

1. Closed-Cycle OTEC

The most common design, proposed by Jacques d'Arsonval in 1881.

Process:

  1. Warm surface seawater (~26-28°C) heats a working fluid with low boiling point
  2. Working fluid vaporizes in the evaporator
  3. Expanding vapor drives a turbine-generator
  4. Cold deep seawater (~4-6°C) condenses the vapor in the condenser
  5. Liquid working fluid returns to evaporator, repeating the cycle

Working fluids:

Advantages: Higher pressure operation allows smaller turbines; proven Rankine cycle technology Disadvantages: Requires large heat exchangers; working fluid handling

2. Open-Cycle OTEC

Proposed by Georges Claude in the 1920s; he built the first working plant in Cuba (1930).

Process:

  1. Warm surface seawater enters a vacuum chamber (pressure ~2-3 kPa)
  2. At this low pressure, seawater boils at ~22-26°C, producing steam
  3. Low-pressure steam drives a turbine-generator
  4. Cold deep seawater condenses the steam
  5. Condensate is pure fresh water (desalinated)

Advantages: Produces desalinated water as byproduct; no working fluid needed Disadvantages: Very large, low-pressure turbines required; lower power density

The 1993 NELHA open-cycle plant achieved 97% seawater-to-steam conversion efficiency and produced 7,000 gallons of fresh water per day alongside 80 kW net power.

3. Hybrid Cycle

Combines elements of both:

Key Components

Heat Exchangers

The critical cost driver, representing 25-50% of total plant capital cost. Requirements:

Materials: Titanium (excellent corrosion resistance, expensive), aluminum alloys (lower cost, shorter life), advanced composites.

A 100 MW plant would require approximately 200 heat exchanger units, each larger than a 20-foot shipping container.

Cold Water Pipe (CWP)

The engineering challenge that has historically limited OTEC development:

A 100 MW plant requires cold water flow of ~200-400 m³/s, necessitating massive pipes.

Recent advances: HDPE pipes now available up to 3m diameter; bundled pipe configurations for larger flows; improved deployment techniques from offshore oil/gas industry.

Seawater Pumps

Pumping represents the largest parasitic load:

One Lockheed Martin design: 49.8 MW net from a system consuming 19.55 MW for pumping alone.

Turbine-Generator

Efficiency Chain

Starting from Carnot maximum (~8%):

Stage Efficiency Factor Running Total
Carnot limit (ΔT = 24°C) 8.0% 8.0%
Heat exchanger irreversibilities ×0.7-0.8 5.6-6.4%
Turbine efficiency ×0.85-0.90 4.8-5.8%
Generator efficiency ×0.95-0.98 4.6-5.7%
Pump parasitic load ×0.6-0.8 2.8-4.5%
Other auxiliaries ×0.9-0.95 2.5-4.3%

Net thermal efficiency: 2.5-4.5% typical, up to 5.4% in optimized designs

Early OTEC systems achieved only 1-3% efficiency. Modern designs approach 3-5%.

Theoretical Limits

Fundamental Carnot Constraint

The Carnot efficiency sets an absolute ceiling that no engineering can overcome:

$$\eta_{max} = \frac{T_H - T_C}{T_H}$$

For OTEC with ΔT = 20-25°C and T_H ≈ 300 K:

Temperature Difference Carnot Efficiency
18°C 6.0%
20°C 6.7%
22°C 7.3%
24°C 8.0%
26°C 8.6%

Increasing the temperature difference offers the only path to higher theoretical efficiency. Approaches include:

Hybrid solar-OTEC systems can theoretically achieve higher efficiencies by boosting T_H.

Practical Efficiency Limits

Real systems face additional constraints:

Finite heat transfer rates: Heat exchangers cannot achieve infinite heat transfer; some temperature difference is "lost" across exchanger surfaces.

Pumping requirements: Large seawater volumes must be pumped, consuming 20-40% of gross output.

Irreversibilities: Friction, turbulence, non-ideal expansion all reduce efficiency below Carnot.

Best demonstrated net efficiency: ~3% (various pilot plants) Theoretical optimized designs: ~5-5.4% (not yet demonstrated at scale) Ultimate practical ceiling: ~6% (half of Carnot, if all components optimized)

Resource Extraction Limits

Even with unlimited OTEC deployment, there are environmental limits:

A University of Hawaii study estimated 15,000 plants of 1 GW each, spaced 30 km apart within 100 km of land, could sustainably generate >2 TW without large-scale disruption.

Practical Limitations

Engineering Challenges

Cold water pipe: The single greatest technical barrier. Deploying and maintaining a 1000m pipe in open ocean conditions remains difficult and expensive. Pipe failures have ended several early projects.

Heat exchanger size and cost: Low ΔT requires enormous heat transfer surface area. Heat exchangers represent 25-50% of plant cost.

Biofouling: Marine organisms colonize heat exchanger surfaces, degrading performance. Continuous cleaning systems required.

Corrosion: Seawater is highly corrosive. Titanium resists corrosion but costs 5-10× more than steel.

Scale: Small pilot plants (<1 MW) cannot demonstrate economic viability. Commercial plants need to be 10-100 MW, but no one has built at this scale.

Economic Barriers

Capital cost: Current estimates range widely:

Compare to: Solar PV ~7001,000/kW,onshorewindTILDE700-1,000/kW, onshore wind ~1,000-1,500/kW, offshore wind ~$2,500-4,000/kW.

LCOE (Levelized Cost of Energy):

For comparison: Onshore wind 0.030.05/kWh,solarPV0.03-0.05/kWh, solar PV0.03-0.06/kWh, diesel generation on islands $0.20-0.40/kWh.

Financing: High capital cost, unproven technology at scale, and long payback periods deter commercial lenders. Most projects require government or development bank support.

Operational Challenges

Maintenance: Offshore or coastal marine environments are hostile. Access for repairs is weather-dependent and expensive.

Reliability: Limited operational experience means reliability is unproven at commercial scale.

Grid integration: On small island grids, a single large OTEC plant could represent a major fraction of total capacity, creating stability challenges if it trips offline.

Scaling Characteristics

Scale Economics

OTEC exhibits strong economies of scale:

- Capital cost per kW decreases approximately 20% for each doubling of plant size - Operating costs per kWh decrease with size - Minimum economic scale: likely 10-50 MW for islands, 100+ MW for grid-connected
Plant Size Estimated Capital Cost LCOE (Concessionary Financing)
1 MW 15,00025,000/kW15,000-25,000/kW 0.40-0.60/kWh
10 MW 8,00012,000/kW8,000-12,000/kW 0.20-0.35/kWh
50 MW 5,0008,000/kW5,000-8,000/kW 0.15-0.25/kWh
100 MW 4,0006,000/kW4,000-6,000/kW 0.09-0.18/kWh

Japanese studies project 30% capital cost reduction for offshore OTEC as structures are optimized, potentially reaching $0.26/kWh LCOE for 50 MW plantships with concessionary loans.

Plant Configurations

Land-based (onshore):

Shelf-mounted:

Floating (offshore):

Modular Approaches

Recent development trend: smaller, modular units rather than giant plants.

Global OTEC's "OTEC Power Module": 500 kW per unit, designed for:

This mirrors the successful scaling approach of solar PV and wind: many small units rather than few large ones.

Current Status

Historical Development

1881: Jacques d'Arsonval proposes closed-cycle OTEC concept 1930: Georges Claude demonstrates first working OTEC plant (Cuba), 22 kW 1979: Mini-OTEC (Hawaii) produces first net positive output: 50 kW gross, 10 kW net 1980: OTEC-1 (Hawaii) tests 1 MW heat exchangers on converted tanker 1993-1998: NELHA open-cycle plant operates, 210 kW gross, 80 kW net, produces fresh water 2013: NIOT (India) deploys 200 kW pilot plant (subsequently lost due to pipe failure) 2015: Makai 105 kW closed-cycle plant connected to Hawaii grid (first US grid-connected OTEC)

Operational Plants (2024)

Global installed OTEC capacity: <1 MW total

Makai Ocean Engineering (Hawaii):

Kumejima (Japan):

No commercial-scale (>1 MW) OTEC plants currently operate anywhere in the world.

Projects in Development

Global OTEC (UK):

KRISO (South Korea):

Japan (Okinawa/Kumejima):

Xenesys/Japan:

Other announced projects (status uncertain):

Technology Readiness

OTEC is rated at Technology Readiness Level (TRL) 6-7:

Key remaining challenges:

  1. Large-scale cold water pipe deployment and reliability
  2. Cost-effective heat exchanger manufacturing at scale
  3. Financing and risk mitigation for first commercial plants

Co-Products and Applications

OTEC's value proposition improves when co-products are considered:

Desalinated water: Open-cycle and hybrid plants produce fresh water. The 1993 NELHA plant produced 7,000 gallons/day. A 100 MW open-cycle plant could produce millions of gallons daily.

Seawater Air Conditioning (SWAC): Cold deep water can provide building cooling at 10% of the energy cost of conventional air conditioning. Already operational in some locations (e.g., Bora Bora, Honolulu) without OTEC power generation.

Aquaculture: Cold, nutrient-rich deep water supports cold-water species (salmon, lobster) and microalgae cultivation. NELHA hosts aquaculture companies generating ~$40 million annually from deep seawater resources.

Hydrogen/Ammonia production: OTEC electricity could power electrolysis for green hydrogen or ammonia production, particularly attractive for remote ocean locations.

Mineral extraction: Deep seawater contains valuable trace elements including lithium.

These byproducts can significantly improve project economics, potentially reducing effective LCOE by 20-40%.

Costs Summary

Parameter Current Projected (Mature)
Capital cost 8,00025,000/kW8,000-25,000/kW 4,000-6,000/kW
LCOE 0.200.50/kWh0.20-0.50/kWh 0.09-0.18/kWh
Capacity factor 90-95% 90-95%
Plant lifetime 20-30 years 30-40 years
O&M cost 2-4% of CAPEX/year 1.5-2.5% of CAPEX/year

OTEC's high capacity factor (90-95%) is a significant advantage over intermittent renewables (solar 15-25%, wind 25-45%). This partially compensates for higher capital costs when comparing total energy delivered.

Market Outlook

OTEC is not competitive with solar, wind, or conventional generation in most markets. However, it may find niches:

Most promising markets:

  1. Remote tropical islands with expensive diesel generation ($0.20-0.40/kWh)
  2. Island nations seeking energy independence
  3. Military bases requiring resilient, fuel-independent power
  4. Locations valuing co-products (water, cooling, aquaculture)

Development pathway:

Key enablers needed:

Realistic assessment: OTEC will likely remain a niche technology for tropical islands and specialized applications rather than a major contributor to global electricity supply. Its value lies in providing baseload renewable power where alternatives are limited, and in enabling integrated ocean resource utilization (power + water + cooling + aquaculture).

The technology works. The physics is proven. The question is whether costs can decline sufficiently for OTEC to compete economically at meaningful scale, or whether solar + storage will prove a more cost-effective path even for tropical island nations.