Hybrid Offshore Wind and Wave Energy Systems: A Review
Abstract
1. Introduction
2. Research Progress on OWT Foundations and Wave Energy Devices
2.1. Research Progress on OWT Foundations
2.2. Research Progress on WECs
- (1)
- (2)
- Enhancing the performance of power take-off (PTO) systems [84,85,86,87] and innovating control strategies are central to improving overall power generation efficiency. Beyond conventional damping control, recent research has expanded toward advanced approaches such as model predictive control [62], optimal control [63], and machine-learning-based adaptive control [64]. These strategies aim to achieve efficient broadband energy capture while ensuring stable system operation. In particular, they show strong potential for coping with complex and highly variable sea states.
- (3)
- The application of multi-degree-of-freedom energy absorption mechanisms [83] is also increasing. By jointly harvesting wave energy from multiple directions [78,79,80] and optimizing motion trajectories through coordinated control strategies, these systems significantly enhance energy conversion performance under broad-spectrum wave conditions.
- (4)
- At the system level, development is shifting from single devices toward array-based and integrated configurations. This trend is especially evident in WWHSs, where coupling with offshore wind farms introduces new interaction effects among devices that influence both energy capture and platform stability. As a result, array-level coordinated control and energy dispatch have emerged as key research topics in recent years.
3. Research Progress of WWHSs
3.1. Co-Located Systems
3.2. Island Systems
3.3. Hybrid Systems
3.3.1. Bottom-Fixed Hybrid Systems
3.3.2. Floating Hybrid Systems
4. Optimization of Hybrid Wind–Wave Energy Systems: Technologies and Layouts
4.1. Technological Optimization
4.1.1. Integrated Design of Foundations and WECs
4.1.2. Power Conversion and Performance Enhancement
4.1.3. Innovative Designs of Hybrid Foundation Concepts
4.2. Layout Optimization
4.2.1. Key Layout Parameters of Hybrid Wind–Wave Arrays
4.2.2. Layout Optimization Algorithms and Simulation Tools
4.2.3. Platform Type Adaptation Layout Strategy
5. Discussion
5.1. System-Level Performance Analysis
5.2. Technological Trends and Methodological Innovations
5.3. Research Gaps and Challenges
6. Conclusions and Suggestions for Future Research
6.1. Conclusions
6.2. Future Research
Funding
Data Availability Statement
Conflicts of Interest
Abbreviations
| WWHS | Wind–wave hybrid system |
| OWT | Offshore wind turbine |
| FOWT | Floating offshore wind turbine |
| CBF | Composite bucket foundation |
| OB | Oscillating buoy |
| PTO | Power take-off |
| WEC | Wave energy converter |
| RAO | Response amplitude operator |
| UN-SDG | United nations sustainable development goal |
| TLP | Tension-leg platform |
| OWC | Oscillating water column |
| PDA | Peripherally distributed array |
| UDA | Uniformly distributed array |
| NDA | Non-uniformly distributed array |
| OSPREY | Ocean surge-driven renewable energy |
| OWCD | Oscillating water column device |
| BEM | Boundary element method |
| HOREHS | Hybrid offshore renewable energy harvesting system |
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| WECs | Oscillating Bodies | Oscillating Water Column | Overtopping |
|---|---|---|---|
| Working principle | Utilizing reciprocating body motion of waves | Air turbine driven by air compressed by wave energy | Hydro, air, or hydraulic type turbine driven by wave energy |
| Name | Wind Turbine Type | Wind Turbine Power Capacity (MW) | WEC Type | WEC Power Capacity (MW) | Status | Location |
|---|---|---|---|---|---|---|
| Poseidon P37 [140] | Semi-sub | 3 × 0.011 | Heaving | 10 × 0.003 | Sea test in 2012–2013 | Denmark |
| P80 [141] | Semi-sub | 4–10 | Heaving | 2–3.6 | 1:30 scale tested in 2022 | Denmark |
| DualSub [142] | Semi-sub | 2 | Heaving | 0.5 | N/A | N/A |
| InSPIRE [143] | Semi-sub | 8–12 | Pressure | 4/6 | Scaled testing in 2022 | University of Edinburgh |
| W2Power [144] | Semi-sub | 2 × 3.6 | Heaving | 18 × 0.1 | 1:3 scale tested in 2008 | Spain |
| NoviOcean [145] | Barge | 3 × 0.05 | Heaving | 0.65 | 1:5 scale tested in 2022 | Stockholm archipelago |
| No. | Wind Turbine | WEC | Main Content | Reference |
|---|---|---|---|---|
| 1 | Monopile | OWC | PTO damping significantly affects hydrodynamic efficiency, with each wave condition having an optimal PTO damping value that maximizes the CWR. The optimal opening ratio is approximately 1.25%, resulting in a maximum CWR of 0.63. | [95] |
| 2 | Monopile | OWC | The damping coefficient is the primary factor affecting the capture width ratio. Run-up is higher on the OWC chamber face than on the monopile and increases with both wave steepness and damping coefficient. Under irregular waves, maximum run-ups are 1.5–2 times larger than in regular waves and show a stronger dependence on wave steepness. | [96] |
| 3 | Monopile | OWC | The inclusion of an internal cylinder produces broad peaks in the capture factor at higher frequencies. The optimal skirt opening angle for maximizing power extraction is the symmetric configuration (θ1 = 2π/3; θ2 = π/2). | [97] |
| 4 | Monopile | OWC | The presence of the OWC chamber reduces both the horizontal force and overturning moment on the monopile. | [98] |
| 5 | Monopile | OWC | In certain wave conditions, the wave forces on the OWC and the monopile mutually balance, resulting in a near-zero net force on the integrated system. | [99] |
| 6 | Monopile | OWC | The hybrid device reflects 5–66% and transmits 3–45% of incident wave power. Optimal performance occurs with a turbine damping corresponding to a 0.5% orifice, with a second peak at 1.0%. Resonance peaks appear at T = 6 s and T = 9 s, with a broad high-performance region between T = 8 s and 11 s. | [146] |
| 7 | Monopile | OWC | Peak efficiency occurs during piston-mode resonance of the water column. When the OWC cross-section width equals the monopile radius (B = R) and its draft is 1.5R, the device absorbs over 80% of the incident wave energy across a width of 2B. | [147] |
| 8 | Jacket | OWC | The maximum value of CWR is about 13%, with average values between 4% and 7%. | [100] |
| 9 | Monopile | Semi-immersed buoy | Compared to an isolated WEC array without a monopile, the integration with a monopile enhances the overall power absorption of the hybrid array across a broad frequency range. Specifically, the two front WECs show a 15% increase in power, while the two rear WECs experience an 8% reduction due to shielding. Additionally, the buoy reduces wave loads and overturning moments on the monopile by 25% and 32%, respectively. However, the total horizontal wave force on the combined hybrid system exceeds that on a standalone monopile. | [104] |
| 10 | Monopile | Hollow annular buoy | The buoy reduces wave loads and overturning moments on the monopile by 25% and 32%, respectively, while the monopile also reduces horizontal loading on the WEC. However, the total horizontal wave force on the integrated system exceeds that on a standalone monopile foundation. | [27] |
| 11 | Monopile | Hollow annular buoy | In the MWWC system, the WEC performs optimally at a wave period of approximately 10 s, while the NREL 5-MW wind turbine contributes the dominant share of the total power output. | [102] |
| 12 | Monopile | Segmented buoy | A segmented buoy integrated with a monopile absorbs about 1.3 times more power than an annular buoy under a Coulomb-type PTO and shows superior performance at shorter wave periods; this advantage remains for certain PTO coefficients under a linear PTO model. | [107] |
| 13 | Monopile | Segmented buoy | By adding WECs to monopile, the hybrid system can produce 26.44% more renewable energy than the monopile offshore wind turbine. | [105] |
| 14 | CBF | Cylindrical buoy | Compared with the single CBF, the CBF-OB WWHS can reduce the wave run-up by about 0–60% and the wave pressure by about 0–40% at the position of 0–135°. At 135–180°, the wave run-up can increase by about 0–40%, and the wave pressure can increase by about 0–50%. The CBF-OB WWHS can significantly improve the absorption efficiency of the buoy, which is about 1.5 to 4.0 times higher than that of the single buoy. | [109] |
| 15 | Jacket | Cone bottom cylindrical buoy | Compared to the heave-type WEC integrated with a jacket, the swing-type WEC exhibits higher motion velocities, greater support reaction forces, and larger connection loads, thereby exerting a more significant influence on the jacket structure. Additionally, in terms of power capture, the swing-type WEC demonstrates clearly superior average hourly power generation. | [108] |
| 16 | Monopile | Cone bottom cylindrical buoy | When monopile is combined with large dense arrays of WECs to form a WWHS, it will have a destructive impact on the overall energy extraction. Such effects are more negative under high-frequency waves. | [110] |
| 17 | Spar | OWC | Compared to a standalone 5 MW FWT, the power of the hybrid system has increased by 9%. By eliminating the independent WEC mooring lines and infrastructure costs, the WEC levelized cost of energy is reduced by 14% and the equivalent tower root stress of the FWT during its lifetime is reduced by 23%. | [111] |
| 18 | Spar | OWC | The large number of OWC WECs increases the generated power, and reduces the dynamic response of the spar platform. | [112] |
| 19 | Barge-based floating platform | OWC | The barge platform with an OWC effectively reduces pitch and fore-aft tower-top oscillations under regular waves with periods between 6.4 s and 12.25 s. In contrast, a single barge platform performs better for wave periods of 12.25 s to 20 s. For the remaining wave periods, there is no significant difference in performance between the two platforms. | [114] |
| 20 | Barge-based floating platform | OWC | The barge equipped with OWC performs better than a single barge. With the period of 10 s, the barge with OWC significantly reduced the pitch angle by 30.8% and fore-aft displacement by 25% compared to the single barge system. | [115] |
| 21 | Semi-sub | OWC | The platform exhibits a lower response in fully or partially open chambers. When the chamber is open or partially open, the influence of the PTO on the platform’s dynamic response is limited, indicating that the normal operation of the OWC has a limited impact on the platform’s dynamics. | [116] |
| 22 | Semi-sub | OWC | A semisubmersible is usually designed with a small motion to prevent the wind turbine from becoming much more rigid in strength. However, the high efficiency of wave energy conversion requires a large motion of the platform. Instead of pursuing the wave energy conversion efficiency, an increase in damping effect or help in reducing the wave exciting force on semisubmersible would be the primary consideration of the integration. | [117] |
| 23 | Semi-sub | OWC | The introduction of the oscillating water column can not only capture wave energy but also reduce the heave, roll and pitch responses, especially for long waves kh ≤ 2.0, kh ≤ 1.4 and kh ≤ 1.76, respectively. The maximum reduction in heave, roll and pitch are 35%, 55.4% and 13.8%, respectively. | [118] |
| 24 | Spar | Hollow annular buoy | As the damping increases, the surge, pitch, mooring rope line remain unaffected, while spar heave and torus heave motions tend to be more similar, the relative heave motion weakens, and the average absorbed wave power does not significantly increase. Compared with the situation without wind, the wind causes larger deviations in the average wave surge and pitch motions. The influence of wind on wave energy absorption can be ignored. | [23] |
| 25 | Spar | Hollow annular buoy | The presence of WECs and tidal turbines will reduce the bending moments of the tower base fore-aft but increase the mooring tension. | [119] |
| 26 | Spar | Hollow annular buoy | In the rated operating condition, the pitch amplitude of the combined concept is 31.5% less than that of the FOWT. At the same time, the torus-shaped WECs hardly affect the power performance of the wind turbine. The combined concept provides an additional contribution of wave energy, which is about 11.4% of the annual power production in the rated operating case. | [162] |
| 27 | Spar | Cone bottom cylindrical buoy | The smaller the distance between the spar and the WECS, the smaller the power generated, attributed to the strong fluidic interaction effect. If a large number of WECs are used, the distance between the spar and the WECs should be increased to avoid the negative impact of the interaction effect on the output power. | [120] |
| 28 | TLP | Hollow annular buoy | In coupled wind–wave conditions, wind loads dominate the mean surge response, while wave loads govern the standard deviation and peak responses. Under rated wind conditions, power output is mainly from the wind turbine and no WEC water exit or entry occurs. Under maximum operational seas, water exit and entry of the WEC floater may occur when the significant wave height reaches 6 m. | [122] |
| 29 | STLP | Cone bottom cylindrical buoy | By arranging 8 WECs in a circular and concentric manner around the STLP, the motion of the WECs will be minimally hindered. At this time, the proportion change range of the hydrodynamic coefficient is the smallest, the power output is relatively stable, and it can absorb the maximum wave energy. | [124] |
| 30 | Semi-sub | Hollow annular buoy | With the increase in the number of WECs, the added mass of surge and pitch of the semisubmersible will be larger. The effect of the number of WECs on radiation damping surge and pitch of the semisubmersible is significant in the high frequency range. Radiation damping of pitch motion of the semisubmersible with three WECs has the largest value. | [132] |
| 31 | Semi-sub | Cylindrical buoy | The addition of WECs reduced the maximum horizontal force and pitch moment on the platform, whereas the maximum vertical force increased due to the increasing power take-off force, especially at low frequencies. | [126] |
| 32 | Semi-sub | Cylindrical buoy | When the platform and WEC are in synchronous mode, the power of a single WEC can be increased by up to 41.4%, and the total power can be raised to 26.7%. The heave motion of the platform also increases. Out of the vicinity of the synchronized mode frequency, the WECs have a small impact on the surge motion and pitch motion of the platform, whereas reducing its resonant heave motion at the natural frequency. | [133] |
| 33 | Semi-sub | Cylindrical buoy | Compared to the wind turbine, the amplitude of heave and pitch motions of the combined concept is reduced due to the generated damping from the WECs. An increase in motion amplitude of the WECs causes an increment in the extraction of energy from ocean waves. | [134] |
| 34 | Semi-sub | Cone bottom cylindrical buoy | Compared with a single floater, the array undertakes higher efficiency at low wave periods. Because the tested wave period is far away from resonance period of the platform, pith, heave and surge are almost increased at all periods. | [127] |
| 35 | Semi-sub | Cone bottom cylindrical buoy | The experimental results reveal overall that the addition of WECs on the floating platform may have desirable or undesirable effects; thus, there are contradicting effects on heave and pitch motions in the operational and survival modes. | [128] |
| 36 | Semi-sub | Hemispherical bottom buoy | Reactive control generally worsen the platform motion responses, while spring–damping control is able to mitigate the pitch motion to certain extent. Regarding power output, reactive control leads to the highest wave power generation, almost twice as much as that of spring–damping. | [129] |
| 37 | Semi-sub | Hemispherical bottom buoy | Adding wave absorbers to the 5-MW braceless semi-submersible FOWT leaves surge motion nearly unchanged, while significantly reducing heave and pitch responses. Although individual wave absorbers generally produce less power than a standalone device, WS1 exceeds the single-WS power at wave periods above 8 s due to diffraction effects from the platform side columns. | [130] |
| 38 | Semi-sub | Cylindrical buoy and Hemispherical bottom buoy | The hybrid system, incorporating 12 inner OBWECs and 15 outer Wavestars, achieves an optimal layout with notable reductions in surge, pitch, and heave motions compared to the standalone DeepCwind platform. The integration of diverse WEC types increases mean mooring loads, though these remain within acceptable and predictable limits. | [160] |
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Song, H.; Yu, T.; Tong, X.; Zhao, X.; Zhang, Z.; Lun, Z.; Wang, L.; Wang, Z. Hybrid Offshore Wind and Wave Energy Systems: A Review. Energies 2026, 19, 739. https://doi.org/10.3390/en19030739
Song H, Yu T, Tong X, Zhao X, Zhang Z, Lun Z, Wang L, Wang Z. Hybrid Offshore Wind and Wave Energy Systems: A Review. Energies. 2026; 19(3):739. https://doi.org/10.3390/en19030739
Chicago/Turabian StyleSong, Haoyang, Tongshun Yu, Xin Tong, Xuewen Zhao, Zhenyu Zhang, Zhixin Lun, Li Wang, and Zeke Wang. 2026. "Hybrid Offshore Wind and Wave Energy Systems: A Review" Energies 19, no. 3: 739. https://doi.org/10.3390/en19030739
APA StyleSong, H., Yu, T., Tong, X., Zhao, X., Zhang, Z., Lun, Z., Wang, L., & Wang, Z. (2026). Hybrid Offshore Wind and Wave Energy Systems: A Review. Energies, 19(3), 739. https://doi.org/10.3390/en19030739

