Article(id=1243249292404703817, tenantId=1146029695717560320, journalId=1240685776644648972, issueId=1243249291226104389, articleNumber=null, orderNo=null, doi=10.3969/j.issn.1007-7294.2025.06.005, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1734105600000, receivedDateStr=2024-12-14, revisedDate=null, revisedDateStr=null, acceptedDate=null, acceptedDateStr=null, onlineDate=1774343329763, onlineDateStr=2026-03-24, pubDate=1750348800000, pubDateStr=2025-06-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1774343329763, onlineIssueDateStr=2026-03-24, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1774343329763, creator=13701087609, updateTime=1774343329763, updator=13701087609, issue=Issue{id=1243249291226104389, tenantId=1146029695717560320, journalId=1240685776644648972, year='2025', volume='29', issue='6', pageStart='849', pageEnd='1012', issueExtLink='null', onlineDate='null', pubDate='null', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1774343329483, creator=13701087609, updateTime=1774501488873, updator=13701087609, preIssue=null, nextIssue=null, ext={EN=IssueExt(id=1243912659851133780, tenantId=1146029695717560320, journalId=1240685776644648972, issueId=1243249291226104389, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1243912659851133781, tenantId=1146029695717560320, journalId=1240685776644648972, issueId=1243249291226104389, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null}, startPage=901, endPage=911, ext={EN=ArticleExt(id=1243262369929999130, articleId=1243249292404703817, tenantId=1146029695717560320, journalId=1240685776644648972, language=EN, title=Energy Efficiency Operating Indicator Forecasting and Speed Design Optimization for Polar Ice Class Merchant Vessels, columnId=1241023037940748650, journalTitle=Journal of Ship Mechanics, columnName=Hydrodynamics, runingTitle=null, highlight=null, articleAbstract=

In order to accurately forecast the main engine fuel consumption and reduce the Energy Efficiency Operational Indicator (EEOI) of merchant ships in polar ice areas, the energy transfer relationship between ship-machine-propeller is studied by analyzing the complex force situation during ship navigation and building a MATLAB/Simulink simulation platform based on multi-environmental resistance, propeller efficiency, main engine power, fuel consumption, fuel consumption rate and EEOI calculation module. Considering the environmental factors of wind, wave and ice, the route is divided into sections, the calculation of main engine power, main engine fuel consumption and EEOI for each section is completed, and the speed design is optimized based on the simulation model for each section. Under the requirements of the voyage plan, the optimization results show that the energy efficiency operation index of the whole route is reduced by 3.114% and the fuel consumption is reduced by 9.17 t.

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LU Yu (1988-), male, Ph.D., associate professor

LIU She-wen(1966-), male, Ph.D., professor, corresponding author, E-mail: .

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为准确预报冰区商船的主机油耗以及降低营运能效指数(Energy Efficiency Operational Indicator,EEOI),通过分析航行过程中的受力情况、船-机-桨的能量传递关系,采用Simulink构建多环境阻力、螺旋桨效率、主机功率、油耗、燃油消耗率和EEOI计算模块。考虑风、浪、冰的影响对航线进行航段划分,完成各航段主机功率、油耗和EEOI计算并进行航速设计优化。优化结果表明,在满足航行计划的要求下,船舶能效营运指数可降低3.114%,油耗减少9.17吨。

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卢雨(1988-),男,博士,大连海事大学副教授

刘社文(1966-),男,博士,大连海事大学教授。

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optimization, figureFileSmall=N33bbWLOCUAZGXrENNsBfQ==, figureFileBig=2/QYvypCR+SEmjMnCZcOpw==, tableContent=null), ArticleFig(id=1243893801668948050, tenantId=1146029695717560320, journalId=1240685776644648972, articleId=1243249292404703817, language=EN, label=null, caption=null, figureFileSmall=null, figureFileBig=null, tableContent=
Marine fuel typesMDOLFOHFO
Ccarbon%4560.860.85
CFi7893.151 043.114 40
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CO2 emission factors

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Marine fuel typesMDOLFOHFO
Ccarbon%4560.860.85
CFi7893.151 043.114 40
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LPP/mB/mDraft/mD/mDesign speed/(m·s−1)
186.428.515.81114.8
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Main parameters of the target vessel

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LPP/mB/mDraft/mD/mDesign speed/(m·s−1)
186.428.515.81114.8
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TypeNumberPowermaxr/minmax
RT-flex50D110 470124
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Main engine parameters

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TypeNumberPowermaxr/minmax
RT-flex50D110 470124
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Scale223344
DirectionSmooth windTop windTop windSmooth windTop windSmooth wind
Distance/n mile85261676159711881627
Scale455566
DirectionCross windTop windSmooth windCross windTop windCross wind
Distance/n mile515242641222426626
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Wind information in routes

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Scale223344
DirectionSmooth windTop windTop windSmooth windTop windSmooth wind
Distance/n mile85261676159711881627
Scale455566
DirectionCross windTop windSmooth windCross windTop windCross wind
Distance/n mile515242641222426626
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Hwave/m2.2723.3446.355Hice/m0.30.50.71
Twave/s22.2335.46Cice(%)10%50%30%40%
Weight (%)14.719.725.210.418.211.5Distance/n mile85300228100
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Wave information and ice information in routes

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Hwave/m2.2723.3446.355Hice/m0.30.50.71
Twave/s22.2335.46Cice(%)10%50%30%40%
Weight (%)14.719.725.210.418.211.5Distance/n mile85300228100
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Section No.Navigation areaSea conditionsVoyage/n mileSpeed/kn
1Wind class 226113
2Wind class 357613.5
3Top wind and wave zoneWind class 4108812.2
4Wind class 524211.2
5Wind class 641611.6
6Wind class 438711.8
7Cross wind zoneWind class 522213.5
8Wind class 662613.2
9Wind class 3139714.3
10Smooth wind and wave zoneWind class 4162714.3
11Wind class 554114.3
12Ice zoneHice 0.3 m, Cice 10%, Wind class 2, top wind8511
13Hice 0.5 m,Cice 50%, Wind class 2, top wind3008
14Hice 0.7 m, Cice 30%, Wind class 4, top wind2288.5
15Hice 1 m, Cice 40%, Wind class 5, smooth wind1006
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Segmented route data

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Section No.Navigation areaSea conditionsVoyage/n mileSpeed/kn
1Wind class 226113
2Wind class 357613.5
3Top wind and wave zoneWind class 4108812.2
4Wind class 524211.2
5Wind class 641611.6
6Wind class 438711.8
7Cross wind zoneWind class 522213.5
8Wind class 662613.2
9Wind class 3139714.3
10Smooth wind and wave zoneWind class 4162714.3
11Wind class 554114.3
12Ice zoneHice 0.3 m, Cice 10%, Wind class 2, top wind8511
13Hice 0.5 m,Cice 50%, Wind class 2, top wind3008
14Hice 0.7 m, Cice 30%, Wind class 4, top wind2288.5
15Hice 1 m, Cice 40%, Wind class 5, smooth wind1006
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冰级商船营运能效指数预报及航速优化研究
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卢雨 1 , 李辰然 1 , 朱向杭 2 , 李世桉 1 , 顾朱浩 1 , 刘社文 1
船舶力学 | 流体力学 2025,29(6): 901-911
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船舶力学 | 流体力学 2025, 29(6): 901-911
冰级商船营运能效指数预报及航速优化研究
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卢雨1, 李辰然1, 朱向杭2, 李世桉1, 顾朱浩1, 刘社文1
作者信息
  • 1.大连海事大学,辽宁 大连 116026
  • 2.中国特种飞行器研究所,湖北 荆门 448001
  • 卢雨(1988-),男,博士,大连海事大学副教授

    刘社文(1966-),男,博士,大连海事大学教授。

通讯作者:

corresponding author, E-mail:
Energy Efficiency Operating Indicator Forecasting and Speed Design Optimization for Polar Ice Class Merchant Vessels
Yu LU1, Chen-ran LI1, Xiang-hang ZHU2, Shi-an LI1, Zhu-hao GU1, She-wen LIU1
Affiliations
  • 1.Dalian Maritime University, Dalian 116026, China
  • 2.AVIC Special Vehicle Research Institute, Jingmen 448001, China
出版时间: 2025-06-20 doi: 10.3969/j.issn.1007-7294.2025.06.005
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为准确预报冰区商船的主机油耗以及降低营运能效指数(Energy Efficiency Operational Indicator,EEOI),通过分析航行过程中的受力情况、船-机-桨的能量传递关系,采用Simulink构建多环境阻力、螺旋桨效率、主机功率、油耗、燃油消耗率和EEOI计算模块。考虑风、浪、冰的影响对航线进行航段划分,完成各航段主机功率、油耗和EEOI计算并进行航速设计优化。优化结果表明,在满足航行计划的要求下,船舶能效营运指数可降低3.114%,油耗减少9.17吨。

能效营运指数  /  冰级船  /  航段划分  /  优化设计

In order to accurately forecast the main engine fuel consumption and reduce the Energy Efficiency Operational Indicator (EEOI) of merchant ships in polar ice areas, the energy transfer relationship between ship-machine-propeller is studied by analyzing the complex force situation during ship navigation and building a MATLAB/Simulink simulation platform based on multi-environmental resistance, propeller efficiency, main engine power, fuel consumption, fuel consumption rate and EEOI calculation module. Considering the environmental factors of wind, wave and ice, the route is divided into sections, the calculation of main engine power, main engine fuel consumption and EEOI for each section is completed, and the speed design is optimized based on the simulation model for each section. Under the requirements of the voyage plan, the optimization results show that the energy efficiency operation index of the whole route is reduced by 3.114% and the fuel consumption is reduced by 9.17 t.

Energy Efficiency Operational Indicator  /  ice-class ships  /  segment division  /  design optimization
卢雨, 李辰然, 朱向杭, 李世桉, 顾朱浩, 刘社文. 冰级商船营运能效指数预报及航速优化研究. 船舶力学, 2025 , 29 (6) : 901 -911 . DOI: 10.3969/j.issn.1007-7294.2025.06.005
Yu LU, Chen-ran LI, Xiang-hang ZHU, Shi-an LI, Zhu-hao GU, She-wen LIU. Energy Efficiency Operating Indicator Forecasting and Speed Design Optimization for Polar Ice Class Merchant Vessels[J]. Journal of Ship Mechanics, 2025 , 29 (6) : 901 -911 . DOI: 10.3969/j.issn.1007-7294.2025.06.005
The International Maritime Organization (IMO) officially implemented the Ship Energy Efficiency Operational Indicator (EEOI) in 2011, which has promoted the development of green shipping. From the perspective of ship operation, the main engine speed is directly related to the ship's speed, which is closely linked to energy efficiency indicators such as resistance during navigation and fuel consumption. Therefore, finding the optimal speed for a given route is an important way to reduce the EEOI and achieve energy savings and emissions reduction.
A considerable amount of analysis and research has already been conducted on the energy efficiency of ships operating in conventional waterways. Liu[1] established an interference model of navigational environment, and derived the relationship between EEOI and sea state conditions, characteristic wave height, loading rate, cargo capacity, main engine speed, etc. Fan[2] utilized the ship-engine-propeller relationship to establish the main engine energy consumption model based on Simulink, and compared the main engine energy efficiency with that of the ship's actual voyage through the real ship algorithm. Ni[3] analyzed the EEOI and made a sensitivity analysis of the ship EEOI with the sailing speed, berthing time, full load rate factor, ship type factor, etc.. Huo[4] studied the energy saving of the ship during sailing by optimizing the ship's section and subsection speeds in order to determine the lowest total fuel consumption. Most of the researches have focused on the energy efficiency of ships operating in conventional waters, but not much work has been done on the energy efficiency of ships navigating in ice. Finland-Sweden proposed a formula in the ice-class specification guidelines to calculate the minimum power for ice-class ships[5], with this formula additionally defining a minimum speed for Finnish-Swedish ice-class ships in specific channel ice conditions. By comparing the empirical formula method for forecasting the minimum main engine power of ice-class vessels in the Finnish-Swedish ice-class specification guidelines, Ni et al[6] proposed the discrete element method to calculate the ice resistance and establish the resistance-velocity curve, through which the main engine power forecasting method for ice-class vessels was established. Hou et al[7] applied uncertainty analysis and optimization theory to solve the minimum speed optimization model, using the main engine speed of ice-class ships as the design variable, validating the EEOI as an effective reference index for energy efficiency optimization in ice-class ships.
Simulink is used in this paper to establish a prediction model for the main engine EEOI of low-ice-class ships. Considering environmental factors, the route is divided into several segments, with fixed distance ranges for each segment. The average speed is used to predict the main engine fuel consumption and optimize the overall route, aiming to obtain the optimal speed profile. This approach minimizes the EEOI while ensuring fuel consumption not to increase.
The energy efficiency model of ice-class ships is constructed by analyzing the force during sailing and the energy transfer relationship between ship, engine and propeller. The resistance of a ship is calculated through the speed and sea state information, and the energy efficiency of the ship is finally obtained by matching the open water characteristics of the propeller and the characteristics of the main engine.
The energy efficiency of ship operations is used to describe the relationship between a ship's CO2 emissions and the amount of cargo it carries. According to the Guidelines for Voluntary Use of the Ship EEOI[8], if a single voyage is segmented, the overall EEOI can be obtained from the EEOI on the different segments. The energy efficiency operational indicator is defined as:
where i is the fuel type; FCi is the fuel consumption of the ship during the voyage; CFi is the CO2 emission factor, i.e., CO2 emissions per ton of fuel consumed; mcargo is the ship's cargo mass; and D is the voyage distance. The CO2 emission factors for commonly used marine fuels are shown in Tab. 1.
The resistance components of ice-class 1A ships sailing through sea ice are more complex than those of ordinary merchant ships. In addition to hydrostatic resistance, wave resistance, and wind resistance, ice resistance in the sea ice area must also be considered. Based on empirical formulas, a resistance calculation model is developed using Simulink.
The hydrostatic resistance to which a ship is subjected while sailing consists of the frictional resistance Rf, the residual resistance Rr and the attached resistance Rap as shown in Eq. (2). Frictional resistance is related to hull surface roughness, wet surface area and speed.
where Cf is the frictional drag coefficient, ΔCf is the roughness compensation factor, V is the speed, S is the wet surface area of the ship, and ρ is the seawater density.
The frictional resistance coefficient is calculated using the method proposed by ITTC. According to the assumption, the relationship between frictional resistance coefficient and the residual resistance of the ship are shown in Eq. (3):
The appendage resistance can be calculated as Rap=KA(Rf+Rr), in which KA is a percentage of the appendage resistance in the hull resistance.
The ship's wave resistance is calculated as per the formula proposed by Daidola et al[11] to solve the axial average wave force, the formula[9] is as follows:
where ρ represents the density of seawater, g is the gravitational acceleration, L denotes the ship length, h signifies the wave height, and χ indicates the wave direction angle. The coefficients Cxi and Cyi correspond to the wave-induced resistance coefficients in the axial and transverse directions, respectively, while CNi represents the wave-induced moment coefficient, and λ is the wavelength.
The part of hull above the waterline, and the superstructure as well, will be affected by the sea wind. Isherwood[12], through the waterline on the hull of the lateral projection area, the length of the ship, and other parameters for variables of the multivariate linear regression, got the wind load coefficient and the wind moment coefficient of the numerical expression for the wind calculation as shown in the following formula[10]:
where Cx, Cy, CN denote the wind load coefficients in each axial direction of the ship; vw is the relative wind speed; AT is the forward projected area of the ship hull above the waterline; AL is the side projected area of the ship hull above the waterline; LOA is the ship's length, B is the ship's breadth; S is the perimeter of the hull's side projection area above the waterline; C is the distance of the side projection surface's centroid from the ship's bow; M is the number of pillars on the side projection centerline surface; ASS is the superstructure's side projection area; a0-a6, b0-b6 and c0-c6 are regression coefficients.
The empirical estimation method, based on extensive experimental data, has become a widely-used approach for predicting ice resistance. This method relies on continuous refinement and the generalized ice-floating resistance formula derived by Huang et al[13] from experimental data of KCS, JCS, AIV, and Araon:
where ρice is the density of broken ice taken as 900 kg/m3, h is the thickness of sea ice, D is the diameter of the upper surface of sea ice, v is the speed of navigation, C is the density of ice, and Fr is the Froude number.
Ship propulsion system is an energy conversion system composed of hull, host and propeller. The effective thrust generated by the propeller overcomes the drag force on the ship. The propulsion system and the relationship between the different efficiencies and powers of the ship propulsion system are shown in Figs. 1-2, where ηg, ηS, ηR, η0, ηH are the gearbox efficiency, shaft efficiency, relative rotational efficiency, propeller efficiency and hull efficiency, respectively, and PB, PS, PD, PT, PE are the braking power, shaft power, transmission power, propulsive power and effective power, respectively.
For an ordinary single-propeller seagoing vessel, the Tylor's formula is used to calculate the wake fraction ω=0.5CB−0.05, the Hankschel's formula is used to calculate the thrust dedution fraction t=0.5CP−0.12, ηS=0.96, the hull efficiency ηH=(1-t)/(1-ω), and the relative rotational efficiency ηR=0.9922+0.074 27×(CP−0.0225lcb)−0.059 08A0. The joint speed coefficient and thrust coefficient eliminate the rotational speed N to get Eq. (7). From Eq. (7), a linear relationship exists between the ratio of the thrust coefficient to the square of the advance coefficient and the ratio of the ship's drag to the square of the speed. By drawing the relationship curve between KT/J2 and J, the output power of the main engine is ultimately obtained by Eq (8) and the fuel consumption of the main engine is calculated:
where J is the advance coefficient, KT is the thrust coefficient, Va is the propeller advance speed, Va=(1 -ω)v, N is the main engine speed, D is the propeller diameter, T is the propeller thrust, ρ is the seawater density, A is a constant, ω is the wake fraction, v is ship speed, ge is the main engine fuel consumption rate, Ps is the main engine output power, and t is the sailing time.
The fuel consumption rate can be obtained through the fuel consumption rate curve of the main engine. The model sets speed limits between 30% and 108% of the maximum continuous speed, with power limits ranging from 10% to 25% of maximum continuous power. The maximum power limit for the target ship's main engine is defined as shown in Eq. (9). The integrated model of the simulation optimization system comprises three main components: navigational meteorological data, resistance model and propulsion system[15]. The Simulink simulation model is shown in Fig. 3.
where NMCR represents the maximum continuous speed, MCR denotes the maximum continuous power, and C, C1, and C2 are the relevant coefficients[16].
Ice-class ships operate in ice-covered areas, making it essential to assess their performance under high ice resistance. A Finnish-Swedish 1A ice-class ship (shown in Fig. 4) embarked from Lianyungang, navigating through the Yellow Sea, Korea Strait, Sea of Japan, Soya Strait, and the Sea of Okhotsk before entering the Arctic Ocean via the Bering Strait. The route (shown in Fig. 5) continued through the Chukchi Sea, East Siberian Sea, Laptev Sea, Kara Sea, Barents Sea, and Norwegian Sea. Covering a total distance of 8,096 n mile, the voyage included 713 n mile in ice channels and 7,383 n mile in open water, with no port calls en route. Equipped with low-speed diesel engine produced by Hudong Heavy Machinery Co. Ltd., the main parameters of the vessel and its main engine are shown in Tab. 2. and Tab. 3.
According to KT/J2-J curve obtained from propeller open water characteristic curve[6], ship's mainframe generally run in 75%-95% power range for a long time, and the mainframe fuel consumption rate can be determined by the corresponding curve between the power and the fuel consumption rate, as shown in Fig. 6.
The rated power and rotational speed of the target ship under the service speed was 6806.0 kW×107.4 r/min. The simulation model speed was set to 14.8 kn, the draught was 11 m, the water temperature was 5 ℃, then the model forecast value obtained was 6540.9 kW×106.6 r/min. The wind condition data of the target route is shown in Tab. 4 and percentage of wave and the sea state in the ice area is shown in Tab. 5.
The speed of the target vessel was maintained at around 13 kn most of the time, and accelerated slightly to around 14 kn in good sea conditions with a fair wind and waves. When entering the ice area, the ship sailed in the water with about 30% ice. The speed was less than 8 kn in the sea with an ice thickness of 0.8-1.5 m[14]. Based on the sea state data, the route was divided into 5 sections of top wind and wave area, 3 sections of cross wind and wave area, 3 sections of smooth wind and wave area and 4 sections of ice area, as shown in Tab. 6.
The mathematical simulation model based on Simulink was used to forecast the rotational speed, power, fuel consumption, fuel consumption rate, and ship energy efficiency operational indicator at different constant speeds for each cruise section. The results in the top wind and top wave area are shown in Fig. 7 and those in the cross wind area are shown in Fig. 8.
The forecast results for each section in the smooth wind and smooth wave areas are shown in Fig. 9 and those for each section of the ice area are shown in Fig. 10.
The performance analysis of the target ship along a complete route aims to reduce the total voyage EEOI without increasing fuel consumption or altering the total voyage time.
where S is the voyage distance, T is the sailing time, and T0 is the voyage period. By keeping limits on maximum sustained power and rotational speed while meeting navigation plan requirements, the safety of the ship and the main engine's own condition setting constraints are considered. The goal is to determine the optimal speeds for each voyage section, aiming for minimum EEOI for the voyage.
Due to varying sea conditions across different sections, the mapping relationship between speed and the energy efficiency operational indicator (EEOI) differs in each section. Therefore, the speeds are coordinated and optimized using the T-search algorithm for directed optimization. A fast convergence rate is exhibited, as shown in Fig. 11. The results of engine speed and RPM for each segment are shown in Fig. 12. The comparisons of fuel consumption and EEOI before and after optimization are illustrated in Figs. 13 and 14, respectively. The results show that the fuel consumption of the main engine of the target ship is reduced by 9.17 t, and the EEOI of the whole route is reduced by 3.114%.
Adopting empirical formulas to build the simulation model can clearly reflect the relationship between each part of resistance, main engine power, rotational speed and fuel consumption, which is helpful to analyze the trend of fuel consumption and EEOI at a constant speed. The main conclusions of this paper are as follows.
(1) In head wind and head wave conditions, rotational speed and power increase linearly with speed, with minimum fuel consumption at 12-14.8 kn. Below 6 kn, speed changes significantly affect EEOI. In cross wind conditions, fuel consumption peaks around 8 kn, with minimal EEOI fluctuations at higher speeds. Following wind and waves can provide thrust, with significant EEOI variability at speeds below 10 kn.
(2) When the ship is navigating in the ice area, the target ship can easily reach the maximum sustained power and the maximum sustained RPM due to the high ice resistance generated by the floating broken ice. Ice thickness and ice density have a significant effect on the fuel consumption and EEOI of the target ship, and different ice segments have their own minimum fuel consumption rate and EEOI variation rate.
(3) Adjusting speeds for open water and ice segments reduces fuel consumption by 9.17 t and EEOI by 3.114%. Higher speeds in open water and lower speeds in ice improve efficiency. There are open water and ice areas in the target ship route, and the EEOI of the target ship in the ice area is of a higher magnitude than that in the open water area, and the ice area segments have a greater impact on the overall EEOI.
The final results show that in order to reduce the EEOI of the total voyage, adopting segmented speed strategies that maximize speed in open waters while ensuring safety and time margins in ice areas reduces overall EEOI. This approach is vital for green navigation and economic operations of low ice-class vessels.
  • 国家自然科学基金面上项目(52171293)
  • 大连市支持高层次人才创新创业项目(2020RQ009)
  • 大连市科技创新基金重点学科重大课题子课题项目(2020J25CY016)
  • 中央高校基本科研业务费专项资金项目(3132023516)
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2025年第29卷第6期
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doi: 10.3969/j.issn.1007-7294.2025.06.005
  • 接收时间:2024-12-14
  • 首发时间:2026-03-24
  • 出版时间:2025-06-20
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  • 收稿日期:2024-12-14
基金
National Natural Science Foundation of China General Program Project(52171293)
国家自然科学基金面上项目(52171293)
High-level Talent Innovation Support Program of Dalian(2020RQ009)
大连市支持高层次人才创新创业项目(2020RQ009)
Key Discipline Project of Dalian Science and Technology Innovation Fund(2020J25CY016)
大连市科技创新基金重点学科重大课题子课题项目(2020J25CY016)
Fundamental Research Funds for the Central Universities(3132023516)
中央高校基本科研业务费专项资金项目(3132023516)
作者信息
    1.大连海事大学,辽宁 大连 116026
    2.中国特种飞行器研究所,湖北 荆门 448001

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2种不同金属材料的力学参数

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鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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