Next Article in Journal
Securing Automatic Identification System Communications Using Physical-Layer Key Generation Protocol
Previous Article in Journal
A Dynamic Cloud Center of Gravity Model for Real-Time System-Level Health Status Assessment of Intelligent Ship
Previous Article in Special Issue
Research on the Response Characteristics of Excavation and Support in Circular Sand Soil Foundation Pit Based on Parameter Verification
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Experimental Study on Enhanced Serviceability for Human Activities of Floating Structures with Wave-Dissipating Modules

1
Department of Structural Engineering Research, Korea Institute of Civil Engineering and Building Technology, Goyang 10223, Republic of Korea
2
Department of Hydro Science and Engineering Research, Korea Institute of Civil Engineering and Building Technology, Goyang 10223, Republic of Korea
*
Author to whom correspondence should be addressed.
J. Mar. Sci. Eng. 2025, 13(2), 385; https://doi.org/10.3390/jmse13020385
Submission received: 8 January 2025 / Revised: 17 February 2025 / Accepted: 17 February 2025 / Published: 19 February 2025

Abstract

:
This study evaluates the serviceability of floating structures designed for marine cities by incorporating wave-dissipating modules. Small-scale model tests in a 2D wave flume were conducted to compare the serviceability of structures with and without these modules under different wave conditions (1-year and 100-year return period waves). The results showed that wave-dissipating modules significantly reduced vertical acceleration, with reductions of approximately 44~45% levels for 1-year return period waves and 54~57% levels for 100-year return period waves. When a topside building was included, the reductions were similarly pronounced, reaching 64% and 63~64% levels for 1-year and 100-year return period waves, respectively. The modules also mitigated inclination (angle), with reduction rates ranging from 55~77% levels, depending on wave conditions and the presence of a topside building. These findings suggest that incorporating wave-dissipating modules around the periphery of floating structures can enhance their serviceability by creating more comfortable and stable environments for human activities, while also improving the stability of the structures themselves. Future research should focus on scaling up the model tests and conducting field experiments to validate these findings under real conditions, as well as optimizing module designs for different wave conditions and structural configurations.

1. Introduction

Recently, there has been an increasing trend of interest and demand for floating offshore infrastructure in terms of environmentally friendly utilization of maritime space. Floating offshore infrastructure can be largely classified into industrial facilities such as industrial plants and ports, as well as those intended for human activities such as floating cities. Up until now, floating structures have been widely used for industrial facilities, such as ports for container loading and energy storage platforms for oil and LNG. Additionally, there is a growing trend to apply floating renewable energy hubs to renewable energy complexes, such as offshore wind farms, as part of projects like Denmark’s Net-zero race project, in order to compensate for the intermittency issues of renewable energy. The serviceability guidelines for floating infrastructure intended for industrial facilities primarily focus on inclination (angle), aiming to ensure the stable operation of topside by preventing equipment failures and malfunctions [1].
In addition to industrial facility uses, there has been a recent movement to construct floating marine cities, such as the Saudi Arabian NEOM city project. In floating marine cities, unlike industrial facility uses, continuous human activity and habitation take place, making the impact of floating structure motion on human comfort (such as seasickness and other discomforts) a major issue. Therefore, in floating structures focused on human activity, controlling the motion of the floating structure to a level that ensures human comfort is referred to as serviceability. To prevent physical discomfort experienced by humans, serviceability guidelines based on vertical acceleration due to the floating structure’s motion are provided [1,2]. These serviceability guidelines for human activity-focused floating structures are not only applied to floating marine cities but are also expanding into areas such as floating offshore wind farm and other maritime industrial facilities to ensure the health and safety of maintenance personnel [3,4].
To improve the serviceability of floating infrastructure, it is necessary to reduce the wave motion of the floating structures, and various studies have been conducted in this regard. Xiao et al. [5] reported that perforated walls have a significant impact on reducing the pitch behavior and wave run-up of floating structures through experimental studies on floating structures with perforated walls. Yao [6] reported that the hydro damping effect of perforations formed on the bottom surface of the floating body can reduce wave motion. Han and Wang [7] studied the reduction of wave energy by floating breakwaters with slitted openings, while Chen et al. [8] conducted a study on reducing the motion of pontoon type floating bodies by applying damping plates to reduce the size and weight of the floating bodies. In addition, many studies have been conducted on reducing the motion of floating offshore wind platforms (semi-submersibles) using damping plates [9,10,11,12].
Bi et al. [13] conducted an analytical study by installing a vertical tensioned sheet barrier at the front of the floating body to stabilize its motion. Gayathri et al. [14] researched the reduction of wave forces acting on a floating bridge by installing a vertical partial flexible barrier at the front of the floating bridge. Liu and Li [15] studied the hydrodynamic behavior characteristics of a double curtain-wall breakwater system composed of a seaward perforated wall and a shoreward impermeable wall.
In addition to mechanical methods based on the shape of the floating body (or secondary modules), there has been a growing interest and research in nature-based methods for wave dissipation [16,17,18]. Nature-based wave-dissipation methods using seaweed, shellfish farming, etc., around the floating body can be environmentally friendly and cost-effective. However, they may have limitations in terms of accessibility of ships and sustainability depending on the season (typhoon, seawater temperature changes). Therefore, nature-based damping methods are still being attempted for coastal protection and marine aquaculture farms in response to climate change, rather than for large floating infrastructures such as industrial facilities, floating cities, and ports.
This paper proposes a method to reduce wave motion by placing wave-dissipating modules on the outer edges of a floating structure designed for marine cities. The serviceability indexes with and without the wave-dissipating modules were evaluated and analyzed through a 2D wave flume test. The serviceability indexes focused on the vertical acceleration related to the discomfort of residents and the inclination for the stable operation of topside (buildings).

2. Serviceability of Floating Structures

2.1. Serviceavility Guideline and Evaluation

Germany’s Aachen University and the UK’s Cranfield University have analyzed various serviceability guidelines for the motion of marine structures (including ships) through the EU Horizon 2020 project, to establish guidelines for the impact of floating structures motion on human activities during maintenance of floating offshore wind platforms [3,4]. According to their research results, the requirements for serviceability guidelines applicable to human activities on floating offshore wind platforms are the following: first, they must include the frequency range of 0.1~0.5 Hz, which is the floating structure’s motion period; second, they must provide reference values for vertical motion (acceleration), which is a major component of human discomfort. It is also stated that the serviceability guidelines for the motion of ships [19] and fixed offshore structures are difficult to apply directly to floating structures.
Therefore, the guidelines applicable to the serviceability assessment related to floating structure motion with a focus on human activities during the maintenance of floating offshore wind platforms are approximately at the level of ISO 2631-1:1997 [20]. Although the Nordforsk [21] are aimed at ships, they are often referenced in various fields of research related to human operability on actual floating offshore platforms and are worth considering [3,22]. In addition, NR 636 [23] provides guidelines on habitability and comfort for humans on floating structures, but it reports limitations in that no reference values for vertical motion are provided and the frequency range is applicable only within 1 to 80 Hz.
(1)
RMS acceleration in vertical direction
ISO 2631-1:1997 [20] provides guidelines on the impact of all forms of vibration (motion) on the human body in the form of frequency-weighted RMS (Root Mean Square) acceleration. The frequency range for human health or comfort is specified as 0.5 to 80 Hz, and the frequency range for seasickness is specified as 0.1 to 0.5 Hz [20,24]. In general, vibrations (motions) that begin to make humans feel uncomfortable have an acceleration of approximately 0.315 to 0.63 m/s2 (see Table 1). The impact of vibrations on human health and comfort, depending on exposure time, is depicted and presented as the “health guidance caution zone” in Figure 1. According to this, at a vibration exposure time of 24 h, caution is required at an acceleration of 0.25 m/s2, and at an exposure time of 4 to 8 h, caution is required at an acceleration of approximately 0.5 m/s2 [25].
The frequency-weighted RMS acceleration reflects the frequency-dependent nature of the impact of vibrations (motions) on human comfort, and it is presented as an evaluation indicator in major guidelines such as ISO, ABS, and NR [3,4,24]. The frequency-weighted RMS acceleration is calculated using the frequency-weighting function [3,4,26] as shown in Equation (1), and the overall process for calculating the frequency-weighted RMS acceleration is shown in Figure 2 [3,4,27,28,29].
α w = 1 T 0 T [ α w t ] 2 d t 1 / 2
where, αw represents the frequency-weighted RMS acceleration, αw(t) represents the time-domain signal of frequency-weighted acceleration, which is the measured acceleration signal multiplied by the frequency-weighting function as presented in Figure 3 [20,26], and T represents the acceleration measurement time. Additionally, some guidelines, such as Nordforsk [21], use un-weighted RMS acceleration as an evaluation indicator.
(2)
Inclination (angle)
The serviceability criteria for the inclination of floating structures are partially presented. The Japanese Mega-Float project provides inclination criteria of 1.0° for offshore runways and 1.5° for offshore roads [30]. The Nordforsk project [21] presents RMS inclination criteria of 2.0~2.5° for human activities on the floating structure, such as cruise liners and transit passengers, and 3.0~6.0° for intellectual and manual work. Additionally, DNV [31] specifies an inclination criterion of 5° for floating offshore wind turbine. Considering these inclination criteria comprehensively, an inclination criterion of 1.5° is suitable for areas requiring the same level of flatness as land, 2.0° for human activities, and 3.0~6.0° for workability and the stable operation of topsides.

2.2. Enhanced Serviceability Using Wave-Dissipating Module

This paper proposes a method to improve serviceability by reducing the wave motion of the main floating structure by placing wave-dissipating modules on the outer edges of the main floating structure, as presented in Figure 4. The wave-dissipating module consists of external slits and internal buoyancy cells in Figure 4b; the slits are designed to dissipate wave energy, and the buoyancy cells are intended to ensure their self-buoyancy.
To increase wave energy dissipation efficiency, the slits apply 30% porosity, and the buoyancy cells have a cylindrical shape. Regarding the decision of porosity on the wall of wave-dissipating model, Korea applies a perforated wall with an approximate porosity of 30%, considering ease of construction and hydraulic characteristics [32]. KICT [32] presents the hydraulic characteristics of perforated walls based on various porosity combinations.
Previous studies aimed at reducing the wave-induced motion of floating bodies can be broadly classified into three groups: vertical barriers [13,14,15], heave plates [8,9,10,11,12], and perforated (porous) members [5,6,7]. The vertical barrier method has the disadvantage of the vertical barrier being difficult to secure, which is separate from the floating body, and is unfavorable in deep water. The heave plate method is an efficient method for reducing vertical motion (heave) in vertically-oriented floating bodies, such as spar and columns in semi-submersible types, but it is less effective for horizontally-oriented pontoon-type floating bodies, as in this study. The perforated (porous) member method is suitable for pontoon type floating bodies, but the perforated members do not have their self-buoyancy, affecting the freeboard and draft of the main floating body, necessitating a greater height for the main floating body. The wave-dissipating module in this study is an appropriate method for reducing motion in pontoon type floating bodies, as it possesses its self-buoyancy, which does not affect the freeboard and draft of the main floating body, allowing for optimal design of the main floating body.

3. Small-Scale Tests

3.1. Test Models and Set-Up

To evaluate the wave motion of the floating structure and its serviceability, 2D wave flume test was conducted. The model tests were performed at Korea Institute of Civil Engineering and Building Technology (KICT) in Korea. The length, width, and height of the wave flume is 50 m, 0.8 m, and 1.5 m, respectively, and the active absorption type wave generator is installed in the wave flume. Figure 5 shows the schematic sketch of wave flume.
The test model was designed based on the floating marine city design shown in Figure 6, applying a Froude similarity ratio of 1/50. To investigate only the unidirectional motions of heave and pitch in the 2D wave flume test, only half the width of 1 unit was manufactured. The detailed specifications of the test model are shown in Table 2. The test model was categorized into four cases according to the combination of floating structure, topside, and wave-dissipating module, as shown in Table 3. The floating structure and wave-dissipating module were connected by steel rods.
The installation of the test model in the 2D wave flume is shown in Figure 5 and Figure 7. The main objective of this experiment is to measure the free-body motion of the floating structure. However, to minimize the surge motion of the floating structure due to wave loads, a mooring system using a wire rope connected to a weak spring was applied to allow semi-free body motion. The weak spring-wire mooring was connected to the four corners of the floating body, as shown in Figure 8. Consequently, the surge motion of the floating body was minimally restricted, while the heave and pitch motions, which are the main measurement items of this study, were allowed. This represents semi-free body motion. The influence of the weak spring-wire mooring used in this study on the heave and pitch motions of the floating body is considered to be minimal, and it is deemed an appropriate method to identify the influence of the wave-dissipation modules on the free body motion of the floating body. The floating structure’s motion was measured accurately using a motion capture system with ultraviolet cameras. Additionally, inclinometers were installed at the center and four accelerometers at the corners of the floating structure for further measurements.

3.2. Wave Conditions

Wave loads were based on the design conditions of 1-year return period wave loads and 100-year return period wave loads, as shown in Table 4. The serviceability criteria for floating structures are based on the recommendations of project authorities, and many projects or guidelines apply the assessment for a 1-year return period wave. Therefore, this paper reflects these guidelines and conducts a serviceability evaluation for a 1-year return period wave. Additionally, to identify the effectiveness of the wave-dissipation modules, a serviceability evaluation was also conducted for the extreme condition of a 100-year return period wave. Although various periods were tested based on the wave conditions in Table 4, this paper analyzes only the two design wave conditions. The floating structure’s response in regular waves was used only for analyzing floating structure fundamental motions, while the serviceability assessment analyzed irregular waves, representing actual sea conditions. The water depth used was 20 m, and it was scaled down to 0.4 m. In still water conditions, the freeboard and draft of the CASE 1 series are 0.126 m and 0.094 m, respectively, while the freeboard and draft of the CASE 2 series are 0.057 m and 0.163 m, respectively.
The free water surface was measured with the capacity type wave gauges. The separation of incident and reflected waves were performed at two locations (W.G. 1 and 2 and W.G. 3 and 4 in Figure 5) by Goda and Suzuki [33]. The transmitted wave was measured with the wave gauge 5 (W.G. 5). The irregular waves were generated with JONSWAP wave function.

3.3. Maximum Acceleration Position

To assess the serviceability regarding human comfort, it is recommended to use the acceleration values measured at the corners of the floating structure, where the most unfavorable acceleration values are typically observed, with a measurement duration of at least 2 min for low-frequency areas below 2 Hz [34]. Consequently, the maximum acceleration location was determined to evaluate the serviceability of the floating structure using the experimental results. The acceleration time history data for the bow and stern are shown in Figure 9.
Upon analysis, it was found that the bow exhibited slightly higher acceleration values overall; therefore, the bow was selected as the representative location for serviceability evaluation related to vertical acceleration. The absolute maximum acceleration for CASE 1-1 (floating structure) was 1.018 m/s2 for the 1-year return period wave load and 1.615 m/s2 for the 100-year return period wave load, respectively. For CASE 1-2 (floating structure combining with wave-dissipating module), the absolute maximum acceleration was 0.317 m/s2 for the 1-year return period wave load and 0.746 m/s2 for the 100-year return period wave load, respectively.

4. Evaluation of Serviceability

4.1. Evaluation of Serviceability for Prototype Without Wave-Dissipating Module

(1)
RMS accelerations
For the CASE 1-1 test model (only the floating structure), the vertical acceleration time history and the corresponding RMS acceleration analysis for a wave load with a 1-year return period are shown in Figure 10 and Table 5. The serviceability evaluation for vertical acceleration indicated that RMS acceleration A (which means frequency un-weighted) was approximately 0.224 m/s2, and RMS acceleration B (which means frequency-weighted by ISO2631-1: 1997) was approximately 0.212 m/s2. The ratio of the RMS value to the mean value was approximately 1.29~1.30, and RMS acceleration B was about 95% of RMS acceleration A. The vertical acceleration time history and the serviceability evaluation results for a wave load with a 100-year return period are shown in Figure 11 and Table 5. The serviceability evaluation results for vertical acceleration indicated that RMS acceleration A was approximately 0.352 m/s2, and RMS acceleration B was approximately 0.315 m/s2. The ratio of the RMS value to the mean value was about 1.24~1.25, and RMS acceleration B was about 90% of RMS acceleration A.
For the CASE 2-1 test model (floating structure combining with topside (building)), the vertical acceleration time history and RMS acceleration analysis results for a wave load with a 1-year return period are shown in Figure 12 and Table 5. The serviceability evaluation results for vertical acceleration indicated that RMS acceleration A was approximately 0.119 m/s2, and RMS acceleration B was approximately 0.107 m/s2. The ratio of the RMS value to the mean value was about 1.27, and RMS acceleration B was about 90% of RMS acceleration A. The vertical acceleration time history and the serviceability evaluation results for a wave load with a 100-year return period are shown in Figure 13 and Table 5. The serviceability evaluation results for vertical acceleration indicated that RMS acceleration A was approximately 0.271 m/s2, and RMS acceleration B was approximately 0.217 m/s2. The ratio of the RMS value to the mean value was about 1.24, and RMS acceleration B was about 80% of RMS acceleration A.
(2)
Inclination (angle)
For the CASE 1-1 test model, the time history of the inclination measured at the center of the test model for wave loads with 1-year and 100-year return periods is shown in Figure 14a and Table 6. For the 1-year return period wave load, the absolute maximum inclination was approximately 4.571°, and the RMS inclination was approximately 0.901°. For the 100-year return period wave load, the absolute maximum inclination was approximately 5.597°, and the RMS inclination was approximately 1.479°.
For the CASE 2-1 test model, the time history of the inclination measured at the center of the test model for wave loads with 1-year and 100-year return periods is shown in Figure 14b and Table 6. For the 1-year return period wave load, the absolute maximum inclination was approximately 3.353°, and the RMS inclination was approximately 0.950°. For the 100-year return period wave load, the absolute maximum inclination was approximately 7.770°, and the RMS inclination was approximately 2.348°.

4.2. Enhanced Serviceability of Wave-Dissipating Modules

(1)
RMS accelerations
The RMS accelerations of the floating structure with the wave-dissipating module were calculated in the same method as the prototype. The influence of the wave-dissipating module on the RMS acceleration of the floating structure was analyzed for wave loads with 1-year and 100-year return periods, and the results are presented in Table 7 and Table 8, respectively. The analysis results for the RMS accelerations for the 1-year return period wave load indicated that, with the wave-dissipating module, CASE 1 series (only floating structure) showed approximately 44~45% levels of the prototype’s RMS acceleration, and CASE 2 series (floating structure with topside) showed approximately 64% level. For the 100-year return period wave load, the RMS acceleration with the wave-dissipating module for CASE 1 series was approximately 54~57% levels of the prototype, and for CASE 2 series, it was approximately 63~64% levels.
This is clearly distinguishable in the response spectrum (irregular wave) of the vertical acceleration of the floating structure shown in Figure 15 and the response time history (regular waves) shown in Figure 16. The effect of reducing RMS acceleration results in improved serviceability concerning the vertical acceleration of the prototype of floating structure.
(2)
Inclination (angle)
The RMS inclinations of the floating structure with the wave-dissipating module were calculated in the same method as the prototype. The influence of the wave-dissipating module on the RMS inclination of the floating structure was analyzed for wave loads with 1-year and 100-year return periods, and the results are presented in Figure 17 and Table 9. The analysis results for the RMS inclinations for the 1-year return period wave load indicated that, with the wave-dissipating module, CASE 1 series showed approximately 55% level of the prototype’s RMS inclination, and CASE 2 series showed approximately 66% level. For the 100-year return period wave load, the RMS inclination with the wave-dissipating module for CASE 1 series was approximately 77% level of the prototype, and for CASE 2 series, it was approximately 67% level.
(3)
Topside (additional weight) effects
The serviceability evaluation was conducted at the bow (front). In the case of regular waves, as shown in Figure 16, the heave displacement at the bow of the CASE 2 series was smaller than that of the CASE 1 series. This is considered to be due to the heavier weight effect of the CASE 2 series, resulting in reduced motion. However, in the case of irregular waves, as shown in Figure 17, the pitch angle of the CASE 2 series was larger than that of the CASE 1 series. This is because the bow receives the impact force of peak waves directly, and in the case of irregular waves, the dynamic inertial force effect due to the heavier weight and higher center of gravity of the CASE 2 series is significant.
In terms of the floating body’s motion period, as shown in Figure 15, the period (s.) of the CASE 2 series in irregular waves was slightly longer (the frequency (Hz) was shorter) due to the weight effect compared to the CASE 1 series. Therefore, even though the pitch angle (heave displacement) of the CASE 2 series increases, the acceleration is more sensitive to the period (s.) change (m/s2), and the increased period (s.) results in a tendency for the acceleration to decrease compared to the CASE 1 series.

5. Conclusions

This paper presents an experimental evaluation of the serviceability of floating structures designed for marine cities. The authors propose enhancing serviceability by incorporating wave-dissipating modules on the structure’s periphery to reduce motion. The study uses small-scale model tests in a wave flume to compare the serviceability of structures with and without these modules under different wave conditions (1-year and 100-year return period waves). Serviceability is assessed using two key indicators: vertical acceleration (related to human comfort) and inclination (angle) (related to the stability of topside building).
The results of this study show that wave-dissipating modules significantly reduce vertical acceleration. The modules effectively dampen wave motion, leading to a substantial decrease in vertical acceleration. The reduction was approximately 44~45% levels for the prototype of the floating structure under 1-year return period waves and 54~57% levels for the 100-year return period waves. The reduction was similarly pronounced when the topside building was included, reaching 64% and 63~64% levels reduction under 1-year and 100-year return period waves, respectively. The wave-dissipating modules also mitigated inclination (angle), although the improvement was less dramatic than the reduction in vertical acceleration. Reduction rates ranged from 55~77% levels depending on the wave conditions and whether a topside building was present.
The experimental results demonstrate that incorporating wave-dissipating modules around the periphery of floating structures is an effective method for enhancing their serviceability. The significant reduction in vertical acceleration and improvement in inclination (angle) strongly suggest that these modules can create more comfortable and stable environments for human activities on floating offshore structures, while also enhancing the stability of the structure itself. The fundamental concept of the wave-dissipation modules of this study is to be attached to multi-sides of the floating body to respond to the multi-directionality of waves. However, in this experimental study, to primarily verify the unidirectional behavior of the floating body with the wave-dissipation modules, the modules were attached only to the bow (front) and stern (rear) sides of the floating body to suit the 2D wave flume test. Therefore, it is expected that the behavior of the actual floating body with the modules installed on multi-sides will differ, and this will be verified through additional experiments in the near future. Also, further research might focus on scaling up the model tests and conducting field experiments to validate these findings under real conditions. Optimization of module design for different wave conditions and structural configurations is also a potential area for future study.

Author Contributions

Conceptualization, Y.-J.J.; methodology, Y.-J.J. and J.K.; validation, Y.-J.J. and J.K.; formal analysis, Y.-J.J.; investigation, M.-S.P. and Y.-T.K.; resources, M.-S.P. and Y.-T.K.; data curation, M.-S.P. and Y.-T.K.; writing—original draft preparation, Y.-J.J.; writing—review and editing, Y.-J.J.; visualization, Y.-J.J.; supervision, Y.-J.J.; project administration, Y.-J.J.; funding acquisition, Y.-J.J. All authors have read and agreed to the published version of the manuscript.

Funding

This work is supported by the Korea Agency for Infrastructure Technology Advancement (KAIA) grant funded by the Ministry of Land, Infrastructure, and Transport (Grant RS-2023-00250727) through the Korea Floating Infrastructure Research Center at Seoul National University.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author.

Conflicts of Interest

The authors declare no conflicts of interest.

References

  1. Jeong, Y.J.; Kim, J.; Park, J.H.; Kim, Y.T.; Park, M.S. A study on serviceability recommendations for human activity-oriented floating structures. In Proceedings of the KSCE 2023 Convention, Yeosu, Republic of Korea, 18–20 October 2023. [Google Scholar]
  2. Kim, J.; Jeong, Y.J.; Kim, Y.T. Frequency-domain analysis for motion of floating structures with perforated wall. J. Korean Soc. Coast. Ocean Eng. 2024, 36, 1–10. [Google Scholar] [CrossRef]
  3. Schwarzkopf, M.A.; Scheu, M.N.; Altay, O.; Kolios, A. Whole body vibration on offshore structures: An evaluation of existing guidelines for assessing low frequency motions. In Proceedings of the 28th International Ocean and Polar Engineering Conference (ISOPE 2018), Sapporo, Japan, 10–15 June 2018; Available online: http://dspace.lib.cranfield.ac.uk/handle/1826/13617 (accessed on 7 January 2025).
  4. Scheu, M.; Matha, D.; Schwarzkopf, M.; Kolios, A. Human exposure to motion during maintenance on floating offshore wind turbines. Ocean Eng. 2018, 165, 293–306. [Google Scholar] [CrossRef]
  5. Xiao, L.; Kou, Y.; Tao, L.; Yang, L. Comparative study of hydrodynamic performances of breakwaters with double-layered perforated walls attached to ring-shaped very large floating structures. Ocean Eng. 2016, 111, 279–291. [Google Scholar] [CrossRef]
  6. Yao, Z. Very large Floating Container Terminal and Optimal Layout of Gill Cells. Ph.D. Thesis, National University of Singapore, Singapore, 2007. [Google Scholar]
  7. Han, M.; Wang, C.M. Modelling wide perforated breakwater with horizontal slits using Hybrid-BEM method. Ocean Eng. 2021, 222, 108630. [Google Scholar] [CrossRef]
  8. Chen, Z.; Wang, Y.; Dong, H.; Zheng, B. Time-domain hydrodynamic analysis of pontoon-plate floating breakwater. Water Sci. Eng. 2012, 5, 291–303. [Google Scholar] [CrossRef]
  9. Sudhakar, S.; Nallayarasu, S. Hydrodynamic responses of spar hull with single and double heave plates in random waves. Int. J. Ocean Syst. Eng. 2014, 4, 1–18. [Google Scholar] [CrossRef]
  10. Carlos, L.-P.; Antonio, S.-I. Hydrodynamic coefficients and pressure loads on heave plates for semi-submersible floating offshore wind turbines: A comparative analysis using large scale models. Renew. Energy 2015, 81, 864–881. [Google Scholar] [CrossRef]
  11. Ana, B.-B.; Sergio, F.-R.; Adolfo, M.-L.; Enrique, M.-F.; Francisco, M.-B.; Julio, O.-E.; Jose, R.-T.; Cristina, S.-G.; Alvaro, V.-P.; Carlos, L.-P.; et al. Scale effects on heave plates for semi submersible floating offshore wind turbines: Case study with a solid plain plate. J. Offshore Mech. Arct. Eng. 2020, 142, 1–9. [Google Scholar] [CrossRef]
  12. Xu, J.; Wang, C.; Li, J.; Tang, G.; Yang, Y. Influence of damping plate size on pitch motion response of floating offshore wind turbine. J. Mar. Sci. Eng. 2024, 12, 1600. [Google Scholar] [CrossRef]
  13. Bi, C.; Wu, M.S.; Law, A.W.-K. Stabilisation of compliant floating platforms with sheet barriers under wave action. Ocean Eng. 2021, 240, 109933. [Google Scholar] [CrossRef]
  14. Gayathri, R.; Kar, P.; Behera, H.; Sahoo, T. Oblique wave scattering by a floating bridge in the presence of a vertical permeable flexible barrier. J. Offshore Mech. Arct. Eng. ASME 2021, 143, 021701. [Google Scholar] [CrossRef]
  15. Liu, Y.; Li, Y.-C. Wave interaction with a wave absorbing double curtain-wall breakwater. Ocean Eng. 2011, 38, 1237–1245. [Google Scholar] [CrossRef]
  16. Zhu, L.; Huguenard, K.; Zou, Q.-P.; Fredriksson, D.W.; Xie, D. Aquaculture farms as nature-based coastal protection: Random wave attenuation by suspended and submerged canopies. Coast. Eng. 2020, 160, 103737. [Google Scholar] [CrossRef]
  17. Marino, M.; Nasca, S.; Alkharoubi, A.I.; Cavallaro, L.; Foti, E. Efficacy of nature-based solutions for coastal protection under a changing climate: A modelling approach. Coast. Eng. 2025, 198, 104700. [Google Scholar] [CrossRef]
  18. Landmann, J.; Hammer, T.C.; Gunther, H.; Hildebrandt, A. Large-scale investigation of wave dampening characteristics of organic, artificial floating islands. Ecol. Eng. 2022, 181, 106691. [Google Scholar] [CrossRef]
  19. ISO 6954:2000; Mechanical Vibration-Guidelines for the Measurement, Reporting and Evaluation of Vibration with Regard to Habitability on Passenger and Merchant Ships. International Organization for Standardization: Geneva, Switzerland, 2000.
  20. ISO 2631-1:1997; Mechanical Vibration and Shock Evaluation of Human Exposure to Whole Body Vibration Part 1: General Requirement. International Organization for Standardization: Geneva, Switzerland, 1997.
  21. Nordforsk. Assessment of Ship Performance in a Seaway, The Nordic Co-Operative Project: Seakeeping Performance of Ships. Nordic Co-operative Organization for Applied Research; Nordforsk: Oslo, Norway, 1987. [Google Scholar]
  22. Sindre, M. Design Criteria for Offshore Feed Barge. Master’s Thesis, Norwegian University of Science and Technology, Trondheim, Norway, 2012. [Google Scholar]
  23. Bureau Veritas. Rule Note NR 636: Comfort and Health On-Board Offshore Units; Bureau Veritas: Neuilly sur Seine Cedex, France, 2016. [Google Scholar]
  24. Saha, G.K.; Mahdi, M.A.; Kona, A.A. A study on motion sickness incidence at several positions of a ship in irregular waves. In Proceedings of the Internation Shipping Conference, Kolkata, India, 26 November 2020. [Google Scholar]
  25. Ahn, S.J. Measurement and Evaluation of Whole Body Vibration-ISO 2631. Sound Vib. 2014, 24, 46–50. [Google Scholar]
  26. Estibaliz, A.; Jon, G.Z.; Oscar, M.C.; Jon, A.R.; Ines, C. Analysis of the motion sickness and the lack of comfort in car passengers. Appl. Sci. 2022, 2022, 3717. [Google Scholar] [CrossRef]
  27. Marjanen, Y. Validation and Improvement of the ISO 2631-1(1997) Standard Method for Evaluating Discomfort from Whole-Body Vibration in Multi-Axis Environment. Ph.D. Thesis, Loughborough University, Loughborough, UK, 2010. [Google Scholar]
  28. Choi, H.S.; Jung, D.J.; Kim, S.D.; Cheung, J.H. The vibration comfort evaluation of the shaking table mass foundation. J. Earthq. Eng. Soc. Korea 2011, 15, 53–60. [Google Scholar] [CrossRef]
  29. Kim, J.; Welcome, D.E.; Dong, R.G.; Song, W.J.; Hayden, C. Time-frequency characterization of hand-transmitted, impulsive vibration using analytic wavelet transform. J. Sound Vib. 2007, 308, 98–111. [Google Scholar] [CrossRef]
  30. Japan Shipbuilding Society. Structural Design of Very Large Floating Structure; Japan Shipbuilding Society: Tokyo, Japan, 2004. [Google Scholar]
  31. DNV-OS-J101; Design of Offshore Wind Turbine Structures. Det Norske Vertas: Oslo, Norway, 2010.
  32. Korea Institute of Construction Technology (KICT). Wave Reflection of Perforated-Wall Caisson Breakwaters; Korea Institute of Construction Technology: Goyang, Republic of Korea, 2000. (In Korean) [Google Scholar]
  33. Goda, Y.; Suzuki, Y. Estimation of incident and reflected waves. In Proceedings of the 15th Conference on Coastal Engineering, ASCE, Honolulu, HI, USA, 29 January 1976; pp. 828–845. [Google Scholar]
  34. KR. Noise and Vibration Guidelines; Korean Register: Busan, Republic of Korea, 2020. [Google Scholar]
Figure 1. Health guidance caution zone.
Figure 1. Health guidance caution zone.
Jmse 13 00385 g001
Figure 2. Evaluation process of frequency-weighted RMS acceleration [3,4,27,28,29].
Figure 2. Evaluation process of frequency-weighted RMS acceleration [3,4,27,28,29].
Jmse 13 00385 g002
Figure 3. Frequency-weighted functions.
Figure 3. Frequency-weighted functions.
Jmse 13 00385 g003
Figure 4. Floating structure with wave-dissipating module: (a) Concept model; (b) Wave-dissipating module detail; (c) Side view; (d) Front and plan view.
Figure 4. Floating structure with wave-dissipating module: (a) Concept model; (b) Wave-dissipating module detail; (c) Side view; (d) Front and plan view.
Jmse 13 00385 g004
Figure 5. Wave flume schematic sketch.
Figure 5. Wave flume schematic sketch.
Jmse 13 00385 g005
Figure 6. Test model: (a) Bird view; (b) Plan view; (c) Test model fabrication.
Figure 6. Test model: (a) Bird view; (b) Plan view; (c) Test model fabrication.
Jmse 13 00385 g006
Figure 7. Test model set-up: (a) Test model set-up; (b) Sensors installation.
Figure 7. Test model set-up: (a) Test model set-up; (b) Sensors installation.
Jmse 13 00385 g007
Figure 8. Weak spring-wire mooring system.
Figure 8. Weak spring-wire mooring system.
Jmse 13 00385 g008
Figure 9. Measured accelerations: (a) CASE 1-1 (1 yr.); (b) CASE 1-1 (100 yr.); (c) CASE 1-2 (1 yr.); (d) CASE 1-2 (100 yr.).
Figure 9. Measured accelerations: (a) CASE 1-1 (1 yr.); (b) CASE 1-1 (100 yr.); (c) CASE 1-2 (1 yr.); (d) CASE 1-2 (100 yr.).
Jmse 13 00385 g009
Figure 10. RMS acceleration of CASE 1-1 (1 yr.: Hs = 1.3 m, Tp = 6.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Figure 10. RMS acceleration of CASE 1-1 (1 yr.: Hs = 1.3 m, Tp = 6.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Jmse 13 00385 g010
Figure 11. RMS acceleration of CASE 1-1 (100 yr.: Hs = 2.1 m, Tp = 8.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Figure 11. RMS acceleration of CASE 1-1 (100 yr.: Hs = 2.1 m, Tp = 8.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Jmse 13 00385 g011
Figure 12. RMS acceleration of CASE 2-1 (1 yr.: Hs = 1.3 m, Tp = 6.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Figure 12. RMS acceleration of CASE 2-1 (1 yr.: Hs = 1.3 m, Tp = 6.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Jmse 13 00385 g012
Figure 13. RMS acceleration of CASE 2-1(100 yr.: Hs = 2.1 m, Tp = 8.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Figure 13. RMS acceleration of CASE 2-1(100 yr.: Hs = 2.1 m, Tp = 8.0 s.): (a) Measured acceleration (blue line); (b) Response spectrum; (c) Frequency-weighted acceleration (red line).
Jmse 13 00385 g013
Figure 14. RMS inclination (angle): (a) CASE 1-1; (b) CASE 2-1.
Figure 14. RMS inclination (angle): (a) CASE 1-1; (b) CASE 2-1.
Jmse 13 00385 g014
Figure 15. Response spectrums due to wave-dissipating module under irregular wave: (a) CASE 1 series (1 yr.); (b) CASE 1 series (100 yr.); (c) CASE 2 series (1 yr.); (d) CASE 2 series (100 yr.).
Figure 15. Response spectrums due to wave-dissipating module under irregular wave: (a) CASE 1 series (1 yr.); (b) CASE 1 series (100 yr.); (c) CASE 2 series (1 yr.); (d) CASE 2 series (100 yr.).
Jmse 13 00385 g015
Figure 16. Response time history due to wave-dissipating module under regular wave: (a) CASE 1 series (100 yr.); (b) CASE 2 series (100 yr.).
Figure 16. Response time history due to wave-dissipating module under regular wave: (a) CASE 1 series (100 yr.); (b) CASE 2 series (100 yr.).
Jmse 13 00385 g016
Figure 17. RMS inclination (angle) due to wave-dissipating module: (a) CASE 1 series (1 yr.); (b) CASE 1 series (100 yr.); (c) CASE 2 series (1 yr.); (d) CASE 2 series (100 yr.).
Figure 17. RMS inclination (angle) due to wave-dissipating module: (a) CASE 1 series (1 yr.); (b) CASE 1 series (100 yr.); (c) CASE 2 series (1 yr.); (d) CASE 2 series (100 yr.).
Jmse 13 00385 g017
Table 1. Reactions to vibration magnitudes.
Table 1. Reactions to vibration magnitudes.
AccelerationHuman Comfort Level
<0.315 m/s2not uncomfortable
0.315~0.63 m/s2a little uncomfortable
0.50~1.0 m/s2fairly uncomfortable
0.8~1.6 m/s2uncomfortable
1.25~2.5 m/s2very uncomfortable
>2 m/s2extremely uncomfortable
Table 2. Dimension of test models.
Table 2. Dimension of test models.
ItemsDimension (m)
(L × W × H)
Weight
(kg)
Etc.
1. Floating structure1.20 × 0.60 × 0.2264.80 -
2. Topside0.96 × 0.60 × 0.4050.46-
3. Wave-dissipating modules0.60 × 0.10 × 0.221.881EA/end side
4. Buoyancy cell D0.05
Table 3. Test model cases.
Table 3. Test model cases.
CasesTest Models
Floating StructureTopside BuildingWave-Dissipating Module
CASE 1-1--
CASE 1-2-
CASE 2-1-
CASE 2-2
Table 4. Wave condition (Irregular wave: JONSWAP γ = 3.3).
Table 4. Wave condition (Irregular wave: JONSWAP γ = 3.3).
No.Tp (s.)
Small (Real)
Hs (cm)
Small (Real)
L (cm)
Small (Real)
H/LReturn Period
R10.85 (6.0)2.6 (130)110 (5500)0.0236Regular
R21.13 (8.0)4.2 (210)177 (8850)0.0237Regular
IR10.85 (6.0)2.6 (130)110 (5500)0.0236Irregular (1 yr.)
IR21.13 (8.0)4.2 (210)177 (8850)0.0237Irregular (100 yr.)
Table 5. Summary of RMS accelerations for prototype.
Table 5. Summary of RMS accelerations for prototype.
Items1 yr. (Hs = 1.3 m, Tp = 6.0 s.)100 yr. (Hs = 2.1 m, Tp = 8.0 s.)
RMS acc. ARMS acc. BRMS acc. ARMS acc. B
CASE
1-1
CASE
2-1
CASE
1-1
CASE
2-1
CASE
1-1
CASE
2-1
CASE
1-1
CASE
2-1
MAX1.0180.4280.8350.3611.6151.4911.0860.729
RMS0.224
-
0.119
-
0.212
(0.95)
0.107
(0.90)
0.352
-
0.271
-
0.315
(0.90)
0.217
(0.80)
AVG0.1720.0940.1640.0840.2820.2190.2530.175
RMS/AVG1.301.271.291.271.251.241.241.24
Table 6. Summary of RMS inclinations (angle) for prototype.
Table 6. Summary of RMS inclinations (angle) for prototype.
Items1 yr. (Hs = 1.3 m, Tp = 6.0 s.)100 yr. (Hs = 2.1 m, Tp = 8.0 s.)Etc.
CASE1-1CASE2-1CASE1-1CASE2-1
MAX4.5713.3535.5977.770
RMS0.9010.9501.4792.348
AVG0.6840.7641.1581.920
RMS/AVG1.321.241.281.22
Table 7. Reduction of RMS acceleration due to wave-dissipating module: 1 yr.
Table 7. Reduction of RMS acceleration due to wave-dissipating module: 1 yr.
ItemsCASE 1 SeriesCASE 2 Series
RMS acc. ARMS acc. BRMS acc. ARMS acc. B
CASE
1-1
CASE
1-2
CASE
1-1
CASE
1-2
CASE
2-1
CASE
2-2
CASE
2-1
CASE
2-2
MAX1.0180.3170.8350.2820.4280.2690.3610.220
RMS0.224
-
0.101
(0.45)
0.212
-
0.093
(0.44)
0.119
-
0.076
(0.64)
0.107
-
0.068
(0.64)
AVG0.1720.0790.1640.0730.0940.0610.0840.055
RMS/AVG1.301.271.291.261.271.251.271.25
Table 8. Reduction of RMS acceleration due to wave-dissipating module: 100 yr.
Table 8. Reduction of RMS acceleration due to wave-dissipating module: 100 yr.
ItemsCASE 1 SeriesCASE 2 Series
RMS Acc. ARMS Acc. BRMS Acc. ARMS Acc. B
CASE
1-1
CASE
1-2
CASE
1-1
CASE
1-2
CASE
2-1
CASE
2-2
CASE
2-1
CASE
2-2
MAX1.6150.7461.0860.5131.4910.5780.7290.424
RMS0.352
-
0.202
(0.57)
0.315
-
0.169
(0.54)
0.271
-
0.172
(0.64)
0.217
-
0.136
(0.63)
AVG0.2820.1650.2530.1390.2190.1400.1750.110
RMS/AVG1.251.221.241.221.241.231.241.23
Table 9. Reduction of RMS inclination (angle) due to wave-dissipating module.
Table 9. Reduction of RMS inclination (angle) due to wave-dissipating module.
ItemsCASE 1 SeriesCASE 2 Series
1 yr.100 yr.1 yr.100 yr.
CASE
1-1
CASE
1-2
CASE
1-1
CASE
1-2
CASE
2-1
CASE
2-2
CASE
2-1
CASE
2-2
MAX4.5711.7285.5973.3863.3531.8777.7705.438
RMS0.901
-
0.496
(0.55)
1.479
-
1.138
(0.77)
0.950
-
0.624
(0.66)
2.348
-
1.580
(0.67)
AVG0.6840.3711.1580.9340.7640.4951.9201.320
RMS/AVG1.321.341.281.221.241.261.221.20
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Jeong, Y.-J.; Park, M.-S.; Kim, Y.-T.; Kim, J. Experimental Study on Enhanced Serviceability for Human Activities of Floating Structures with Wave-Dissipating Modules. J. Mar. Sci. Eng. 2025, 13, 385. https://doi.org/10.3390/jmse13020385

AMA Style

Jeong Y-J, Park M-S, Kim Y-T, Kim J. Experimental Study on Enhanced Serviceability for Human Activities of Floating Structures with Wave-Dissipating Modules. Journal of Marine Science and Engineering. 2025; 13(2):385. https://doi.org/10.3390/jmse13020385

Chicago/Turabian Style

Jeong, Youn-Ju, Min-Su Park, Young-Taek Kim, and Jeongsoo Kim. 2025. "Experimental Study on Enhanced Serviceability for Human Activities of Floating Structures with Wave-Dissipating Modules" Journal of Marine Science and Engineering 13, no. 2: 385. https://doi.org/10.3390/jmse13020385

APA Style

Jeong, Y.-J., Park, M.-S., Kim, Y.-T., & Kim, J. (2025). Experimental Study on Enhanced Serviceability for Human Activities of Floating Structures with Wave-Dissipating Modules. Journal of Marine Science and Engineering, 13(2), 385. https://doi.org/10.3390/jmse13020385

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop