Next Article in Journal
Monitoring of Defects of a Photovoltaic Power Plant Using a Drone
Next Article in Special Issue
A Study of the Hydrodynamic Performance of a Pitch-type Wave Energy Converter–Rotor
Previous Article in Journal
Heat Transfer at the Interface of Graphene Nanoribbons with Different Relative Orientations and Gaps
Previous Article in Special Issue
Integration of Marine Wave Energy Converters into Seaports: A Case Study in the Port of Valencia
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Characterization of Wave Energy Potential for the Baltic Sea with Focus on the Swedish Exclusive Economic Zone

1
Department of Earth Sciences, Uppsala University, Villavägen 16, SE-752 36 Uppsala, Sweden
2
Finnish Meteorological Institute, P.O. Box 503, FI-00101 Helsinki, Finland
3
Swedish Meteorological and Hydrological Institute, SE-601 76 Norrköping, Sweden
4
Geological Survey of Sweden, Box 670, SE-751 28 Uppsala, Sweden
5
Division of Electricity, Department of Engineering Sciences, Uppsala University, Box 534, SE-751 21 Uppsala, Sweden
*
Author to whom correspondence should be addressed.
Energies 2019, 12(5), 793; https://doi.org/10.3390/en12050793
Submission received: 8 January 2019 / Revised: 17 February 2019 / Accepted: 26 February 2019 / Published: 27 February 2019
(This article belongs to the Special Issue Wave Energy Conversion)

Abstract

:
In this study, a third-generation wave model is used to examine the wave power resource for the Baltic Sea region at an unprecedented one-kilometer-scale resolution for the years 1998 to 2013. Special focus is given to the evaluation and description of wave field characteristics for the Swedish Exclusive Economic Zone (SEEZ). It is carried out to provide a more detailed assessment of the potential of waves as a renewable energy resource for the region. The wave energy potential is largely controlled by the distance from the coast and the fetch associated with the prevailing dominant wave direction. The ice cover is also shown to significantly influence the wave power resource, especially in the most northern basins of the SEEZ. For the areas in focus here, the potential annual average wave energy flux reaches 45 MWh/m/year in the two sub-basins with the highest wave energies, but local variations are up to 65 MWh/m/year. The assessment provides the basis for a further detailed identification of potential sites for wave energy converters. An outlook is given for additional aspects studied within a broad multi-disciplinary project to assess the conditions for offshore wave energy conversion within the SEEZ.

1. Introduction

Renewables presently supply more than 20% of the world’s energy demand and represented almost two-thirds of the new net electricity capacity additions in 2016 [1]. The majority of the growth in renewables comes from solar power and photovoltaics grew faster than any other energy resource in 2016 [1]. To meet future energy demands and accelerate decarbonisation in all sectors in order to be on track to meet long-term climate goals, a diversified set of energy sources is needed. A significant part of global renewable energy resources is stored in oceans. Wave energy has attracted the attention of the scientific community and the energy industry especially since the 1970s, in connection to the oil crisis of 1973 [2], but the first patent for a device to convert wave energy into usable energy was filed in France as early as 1799 [2,3].
There are several potential advantages of utilizing wave energy for renewable electric power generation [4]. Through the years, technological breakthroughs in relevant disciplines have enabled wave energy device development to accelerate and testing has shown promising results [5]. However, costs to implement modern wave energy converters (WECs) are currently higher than those of other renewable energy technologies [6] and combined with the unproven status of the technologies this has hindered investors’ confidence in the sector. With a small absolute contribution, ocean power is expected to scale up from small- to medium-size demonstration projects over the coming years. The International Energy Agency [7] reports that detailed cost analysis for wave energy conducted for the US Department of Energy concluded that costs could decrease significantly as technology moves towards more commercial scale.
Before an implementation of WECs, a thorough assessment of the conditions should be conducted for the area of interest. A first step would be a spatio-temporal energy resource assessment and availability analysis. The wave power resource, or wave energy potential, has been assessed in many recent studies, e.g., for coastal ocean areas [8,9], for seas [10,11] and for lake Erie [12]. Additional references on wave energy resource assessments are also found listed by country or region in Chen et al. [13] and an overview of the global distribution of wave power resources is discussed in Kasiulis et al. [14].
The Baltic Sea is a relatively large semi-enclosed sea bounded by nine countries with an estimated combined area of about 435,000 km 2 . Overall, maps for the theoretical wave energy potential, or wave power, for such a large study area provide an excellent overall view of available wave resources for energy conversion. For the Baltic Sea region, several previous studies have also been conducted, some of which have neglected the influence from seasonal ice conditions [11,15] or have focused their studies on areas which are almost always ice-free [16,17,18]. The seasonal ice-cover is, however, known to influence the wave climate and Tuomi et al. [19] suggested ways to calculate different types of statistics taking the ice-time into account.
The Baltic Sea and the Swedish west coast are of high interest as the government of Sweden, together with a broad coalition of political parties, has set a target to have 100% renewable electricity production by 2040 [20]. It is clear from works such as [21,22,23,24] that a high horizontal resolution for the wave model is required to effectively capture the spatial variations of waves near coasts. Wave energy conversion sites generally benefit from being located closer rather than further away from suitable harbors in order to facilitate and reduce the costs of transportation to and from the site. Being close to the shore also reduces the cost of power transmission. Coarse numerical wave model results are therefore of limited use in assessing the near-shore wave energy resource. Existing wave energy converter test sites have so far been placed within 17 km from the shore in water depths less than 100 m (see Figure 14 in [6]), requiring fine detailed bathymetry data to make a joint analysis and identification of potentially interesting pilot sites for WECs. Future large-scale commercial wave energy park installations may very well be located further from the shore as well as in deeper waters, depending on several conditions at accessible and available sites, WEC and transmission technology, the possibility of using ROV (remotely operated underwater vehicle) robotics in sea operation and maintenance, among many other aspects including economy of scale and the price of electricity.
In a multi-disciplinary project, a high horizontal resolution of the wave field information can be useful as it can be combined with high-resolution topographic data, geotechnical information, environmental classifications and other types of information [22] relevant in site selection. The size of the proposed wave energy park installations may often range from around 250 by 250 m to 1 km 2 in size and here we report results from a high-resolution 16-year wave hindcast (at about 1 km 2 ) with the aim to provide estimates of the theoretical wave energy potential for the Baltic Sea and along the Swedish west coast. Previous studies for the region include Weisse et al. [25] with 5 times lower resolution, and Reistad et al. [26] with about 10 times lower resolution. Björkqvist et al. [24] is one of the most detailed studies of wave climate, over a long time period of 41 years, conducted for this region using a wave hindcast dataset that included modeled sea ice at about 1 nmi horizontal resolution (about 2 km), but no wave energy resource assessment was conducted. An extremely detailed 100 m horizontal resolution simulation, but for a much more limited domain, has been performed for the Lithuanian coast [27]. The dataset produced here also provides necessary statistical information for detailed calculations of technical wave energy potential in upcoming studies as this study is only one part of a larger project on marine energy conversion in the SEEZ [22]. The total wave energy resource of Sweden has no precise estimate [22,28] and further study is needed.
One of our aims is to introduce a partly new and innovative way to present the wave power resource using the distance from resolved land as a factor that is highly influential on the wave field, through its connection to processes that reduce wave energy near the coast. These include the fetch conditions, breaking wave effects (shoaling and refraction), bottom friction as well as shadowing effects from islands. The distance from the coast parameter provides the basis for a relative resource classification method introduced in this work. While new for the Baltic Sea, a similar method has been used in Nobre et al. [29] for some parts of the Portuguese coast. The results are illustrated and focused on the Swedish exclusive economic zone, but the classification could be carried out in a similar way for other basins around the world, or using national marine boundaries to facilitate assessment of the most promising wave energy resource areas in different countries. Another aim of this paper is to use high-resolution wave modeling to investigate the Baltic Sea area for its wave power resource. The results will be discussed both on a basin level and at a wave energy converter park level which is unique for the studied area. A detailed assessment is also carried out to characterize the directional dependence on the wave power resource and its effect on the temporal availability of the wave energy. This could be of great importance for fetch-limited seas at high latitudes as there is great seasonal and directional variability in the wave field parameters.
This paper is structured as follows: In Section 2, the numerical wave modeling and datasets are introduced. This is followed in Section 3 by an evaluation of the wave model results using wave buoy data. Then, results that characterize the wave power resource for Swedish conditions are presented and discussed in Section 4. Wave power estimates for the SEEZ are also compared and contrasted with results for the Baltic Sea and a relative resource classification and simple joint analysis is carried out on some other aspects such as water depth in Section 5. A brief outlook for more aspects to be studied for this region is given and results are discussed in Section 3, Section 4 and Section 5. Finally, a summary and conclusions on the main results are found in Section 6.

2. Numerical Wave Hindcast and Available Data

2.1. Numerical Modeling

Wave climate modelling was performed for the Baltic Sea, Skagerrak and Kattegat area using the WAM Cycle 4.5.1 model [30,31,32] with a high horizontal resolution of 0.01° latitude, 0.02° longitude (about 1.1 km) on a spherical grid for the time period 1998 to 2013. This is a higher horizontal resolution compared to previous wave hindcast studies for a domain of this size. The model domain spans from longitude 9.10° to 30.48° and latitude 53.55° in the south to 65.95° in the north. Although WAM was originally developed as a deep water model, it was later modified for finite depths [33]. It has been extensively validated in the Baltic Sea, including several coastal implementations (e.g., [19,23,34,35,36]). WAM was therefore chosen for this study, as it is an established model that is well suited to simulate the wave conditions in the entire study area.
The WAM model solves the transport equation for wave energy and includes processes for propagation, refraction and nonlinear interaction of the spectral components, as well as meteorological input and dissipation of wave energy. The spectral resolution in WAM was set to 24 directions (15 degrees) and 35 frequencies, which covers a logarithmically scaled frequency band from 0.042 Hz to 1.07 Hz, similar to Tuomi et al. [19].
The estimated computational time for the wave modeling was about 110,000 cpu-hours and the simulations were performed in terms of 32 runs, each of which was about 6 months long with a 3-day initial spin-up time period for the wave field. Spin-up periods were removed to form a uniform dataset from 1 January 1998 to 31 December 2013. Hourly output statistics for significant wave height, energy period, peak wave period, mean wave direction and some additional parameters were saved and processed. Wave parameters were evaluated against buoy measurements and further statistical calculations were carried out to characterize the wave power resource.

2.1.1. Bathymetric Data

The depth grid is a compilation of two publicly available datasets: the Baltic Sea Hydrographic Commission (BSHC) 500 m grid, published in 2013, see [37], and the European Marine Observation and Data Network (EMODNET) Bathymetry 1/8 × 1/8 arc minutes (ca 250 m) grid, published in 2016 [38]. The datasets were interpolated, resampled to a cell size of 250 × 250 m and geographically projected to the European Terrestrial Reference System 1989 (ETRS89) Lambert azimuthal equal-area (LAEA) projection coordinate reference system to be primarily used in marine spatial planning in Sweden. The bathymetry for the wave model was calculated from the high-resolution depth data by averaging nearby grid cells to an effective 1 km 2 grid, followed by an interpolation to the WAM grid locations in World Geodetic System 1984 (WGS84) coordinates.
An example of a zoomed in view of the bathymetric data around the island of Öland and part of Gotland is presented in Strömstedt et al. [22]. From this, it was clear that a great advantage of the present study is the ability to combine different types of information on a high-resolution grid. Areas around coastal zones and between mainland Sweden and the island of Öland could also be represented with wet(sea) points, which has not always been the case for previous more coarse resolution modeling studies.

2.1.2. Ice and Wind Data

Taking ice into account in wave modeling is very important in a basin with seasonal ice, such as the Baltic Sea, because it limits the amount of time where significant waves can be present and changes the fetch for surrounding areas. The ice product used is formed using the operational ice charts produced by the Swedish Ice Service at the Swedish Meteorological and Hydrological Institute (SMHI), based on a combination of satellite information and in situ observations. The software used for this is called IceMap, in which the operator manually draws a large number of polygons on a computer screen. Each polygon was assigned a number of ice attributes, such as level ice thickness and total ice concentration. As a result, the ice edge and ice extent in the IceMap dataset are both very reliable, whereas the ice properties within the ice pack can have large uncertainties. The resulting ice chart is digitized and saved on a 2D grid of about 4 km resolution. The availability of IceMap ice charts is about twice weekly before March 2005, and almost daily during the winter season from March 2005 and onwards. The IceMap ice product was compared with purely satellite-derived ice charts by Uiboupin et al. [39]. The available ice data from SMHI were interpolated to daily files and WAM was updated on a daily basis.
SMHI also provided wind speed and wind direction at the height of 10 m every 3 h from dynamical downscaling using the HIRLAM model (High Resolution Limited Area Model, [40]) which are more detailed than global reanalysis data. The atmospheric reanalysis dataset generated using HIRLAM, used in this project, is called EURO4M and is further described in Dahlgren et al. [41]. The winds were provided to the wave model using the interpolation routines attached to the WAM model developed by the Norwegian Meteorological Institute (met.no). Some small errors in coastal zones with missing ice might be present in the current modeling setup, because the ice data and wind data were of coarser resolution than the wave model grid. The interpolation routines may therefore not have considered all special cases with different land and sea-ice masks. This is likely to cause only very small errors in the actual wave power resource estimate because the wave resource close to the coast is smaller compared to off-shore areas.

2.2. Wave Buoy Data

In the evaluation of the wave modeling results, wave records available through an open database managed by SMHI (http://opendata-download-ocobs.smhi.se/explore/) are used as well as wave buoy measurements outside the island of Östergarnsholm east of Gotland managed by the Finnish Meteorological Institute (FMI). Distributions of significant wave height are shown in Figure 1. The names of the different wave records correspond to the names given in the SMHI database. Specifically, 17 wave records from 14 buoy locations located in or near the SEEZ with measurements ranging from a few thousand measured 30 min values to at most over 150,000 half-hour data are used. Hence, for some locations, available data span more than a decade of wave measurements and other data span only a few months. The SEEZ area was determined using the open database for georeferenced marine names and maritime boundaries [42]. Details of the locations, water depth and approximate distance to the coast are given in Table 1, and the locations are shown in Figure 2. Table 1 also contains an assessment of mean significant wave heights and 95th percentile both from all available measurements and from the 16-year wave hindcast results. Additional details, such as the number of available data, number of coinciding modeled and measured values and some evaluation statistics for the coinciding data are found in Table 2. These are further discussed in the evaluation section.

3. Model Evaluation

Overall, the measured and hindcast mean significant wave heights in Table 1 agree regarding the range of encountered values for the region. Measured values are between 0.37 m (close to coast at Oskarsgrundet) and 1.24 m (at Södra Östersjön wave buoy representing more open sea conditions). The corresponding modeled values calculated for the full 16 years of simulation were found to be 0.34 m and 1.21 m. Table 1 also shows estimates of the 95th percentile for significant wave height, which indicates that, in general, slightly higher values are estimated from the hindcast compared to the measurements. Nevertheless, the range of variations in the measurements—from 0.78 m at Oskarsgrundet to 3.04 m at Södra Östersjön—is well estimated by the hindcast values, which fall between 0.87 and 3.11 m. The differences observed in Table 1 can partly be explained by differences in time periods between measurements and model values, but a slight overestimation of the variability in the significant wave height will later be shown when the coinciding data are evaluated.
The distributions of the measured values of significant wave height in Figure 1 (a) and hindcast values in (b) also show a good agreement for many sites, but with some larger differences most obviously seen for Oskarsgrundet and Trubaduren locations (red full or dotted lines marked with squares). In this figure, only data from wave records with more than 15,000 half-hours are used to form the measured distributions. Only data up to 4.5 m are shown since larger significant wave heights are rare. Wave heights above 8 m occur in some basins [43], but extreme conditions for the Baltic Sea are not in focus here.
On the west coast of Sweden, some issues with either too short fetch conditions from the North Sea used in the modeling or missing wave–current interactions caused some underestimation of significant wave heights and wave periods when the evaluation of coinciding data was performed. Further testing with a wave–atmosphere–ocean-coupled model system for a short time period has indicated that wave–current interaction could be important (personal communication with Lichuan Wu at Uppsala University) and inclusion of boundary conditions from a North Sea wave model may have alleviated the issue.
A statistical post-processing correction was applied for the Swedish west coast based on a monthly wave index method, which is essentially identical to a geostrophic wind index method used in wind energy applications described further in Nilsson and Bergström [44]. Here, it was, however, applied to correct wave information (significant wave height and energy period) using a modeled wave dataset from Weisse et al. [25], which has taken into account the potentially long fetch conditions for the region by application of nested simulations covering the North Atlantic ocean, but performed the simulations at about 5 km horizontal resolution. All coinciding times with ice-free conditions in both datasets were used to form the monthly correction factors.
For the wave buoy Väderöarna WR which has the largest amount of coinciding measured and modeled data, the bias was reduced from −0.25 m down to −0.09 m. At the buoy Läsö Ost, the bias was also reduced from −0.16 m to −0.12 m, but at the wave buoy Trubaduren located closer to coast a small overestimation of significant wave height of 0.01 m was increased to 0.06 m after the correction was applied. The overall error statistics considering all available wave records from the Swedish west coast showed improvements by the procedure. The wave power resource estimate for the two datasets differed at most by about 10% when all coinciding data were used.
It is worth noting that the correction approach only used the two modeled datasets. No calibration using the measurements was applied, which could in future work be possible to use for further improved wave energy resource estimations for specific sites with available wave data. Such an assessment has, however, already been performed for the west coast of Sweden in the study by Waters et al. [45] with overall similar results to those presented here. Since the wave buoy measurements were not used for calibration, they can be used to evaluate the performance of the produced wave hindcast dataset, which is our aim here.
Table 2 lists the bias for all wave records that has coinciding measured and modeled data. This bias is also shown in Figure 2 next to the location name on a geographical map. There are 14 sites with measurements, of which three have two wave records for the same location in the SMHI database, making it, in total, 17 wave records used for the evaluation. Apart from the 14 wave measurement locations, three additional sites in Figure 2 are marked with red dots inside squares on the map and also marked with the names: KP Sundsvall, KP Ålands hav and KP Ystad. Seventeen selected grid point locations are marked in total where full two-dimensional directional wave spectra and additional wave statistics were saved on an hourly basis for testing and validation purposes. Wave buoy data from SMHI are available at http://opendata-download-ocobs.smhi.se/explore/ and for the wave buoy outside Östergarnsholm run by the Finnish Meteorological Institute (FMI) by contacting the author group. The bias varies between −0.12 m and 0.15 m for different wave records, with an overall bias of −0.06 m. No obvious systematic difference between geographical regions is present, which confirms that the dataset is suitable for a relative comparison between sub-basins within the SEEZ.
In Table 2, the centered root-mean-square error (CRMSE), linear correlation coefficient and standard deviation of the measurements are also listed. High correlations above 0.90 are shown in comparison to all wave records except at Oskarsgrundet which has 0.71. Oskarsgrundet is located closest to the coast and has the lowest observed standard deviation of all sites with 0.20 m, because of its relatively low wave climate. The root-mean square errors range from 0.17 m to 0.38 m with an overall average of 0.26 m, which is similar to reported error statistics of previous wave modeling efforts [19,21,24].
A good way to investigate model behavior and compare modeling errors at different sites is to scale the standard deviation of significant wave height from the model as well as the CRMSE with the measured standard deviation and display the result in a Taylor diagram [46], as shown in Figure 3. The evaluation metrics used are properly defined in Appendix A. The Taylor diagram uses the law of cosines to display how the normalized wave hindcast statistics (CRMSE/ σ b u o y , σ h i n d c a s t / σ b u o y and the linear correlation coefficient ρ ) compare at different sites and relative to the observed values.
Figure 3 reveals that all sites except site K (Trubaduren) and I (Oskarsgrundet) have a normalized CRMSE of less than 0.45 since each green dashed line away from the observed point A indicates a 0.1 times CRMSE/ σ b u o y increase. Site G (Ölands södra grund) has a standard deviation of about 19% larger than observed, which may be related to special topographic conditions in this area. Apart from the three above mentioned sites, the other locations all show standard deviations between 0% and 10% higher than the observed values. This is shown by their placement between the black line—indicating a ratio 1 for the standard deviations—and the first dashed black line on the right, indicating a ratio of 1.1. This can be considered as a good behavior for the hindcast dataset since the buoy locations are geographically spread out and a relative assessment for the SEEZ is one of our objectives.
The linear correlation coefficient is, as previously discussed, above 0.90 for all sites except Oskarsgrundet (I), which is close to coasts and islands from several directions. Trubaduren is also located relatively close to coast (8.4 km) and in a geographical location which is complex. There are some islands nearby and there is proximity to several coastlines, which may further increase the difficulty to obtain more accurate wave model results. At the Östergarnsholm site (F) in the Baltic Sea, the distance of 8.5 km to the island of Gotland is similar, and there is a smaller island named Östergarnsholm about 4 km from the buoy location. This island was too small to be resolved on the model grid, but otherwise the archipelago is less complicated on the east side of Gotland; overall, the wave model showed good error statistics at Östergarnsholm, with an overestimation of only about 3% for σ , a linear correlation of 0.95 and a CRMSE of 0.21 m. Nevertheless, it is likely that relative errors may be somewhat larger for locations closer to the coast, especially in certain regions within the SEEZ that has a complex archipelago. This is also consistent with conclusions from more focused wave modeling efforts in archipelagos and near-shore regions [23,36].

4. Wave Power Resources

In Figure 4, the annually averaged wave power P is shown, calculated using the relationship:
P = 1 16 ρ g H s 2 c g ( T e , h ) ,
where H s is the significant wave height, ρ is the density of seawater, g is the acceleration of gravity, T e is the energy period and c g ( T e , h ) is the group velocity determined from the energy period and the water depth, h. See Appendix B for further details, references and a brief discussion on the results from a method comparison at two sites.
Wave power estimates for the Baltic Sea and SEEZ are based on the 16-year hourly wave hindcast values. Ice-time-included statistics are displayed, where the wave power P is set to zero when the ice concentration seen by the model is larger than 30%. Tuomi et al. [19] suggested similar ice-time-included statistics for mean significant wave height in basins with seasonal ice cover. The wave resource is about 8 kW/m in the outer parts of the SEEZ in the middle of the Baltic Sea and varies down to nearly no wave energy in sheltered areas close to land. On the west coast of Sweden, there is also a higher amount of wave energy closer to the coast in the northern part of the SEEZ, which is less sheltered by Denmark. Comparable wave power estimates can be seen along the western coastal areas in the Baltic Proper. This is related to the predominant wind directions from west and southwest which result in higher wave energy near the western shores than near the eastern shores (e.g., [19,24,27]). Similar results have previously been found also for the average annual wave energy density [17].

4.1. Wave Energy in Different Basins

For a further discussion on the wave power resource variations within the SEEZ, the SEEZ region is split into 11 smaller basins, as shown in Figure 5. The basins are named 1 to 11, starting from the most northern latitudes and continuing first within the Baltic Sea, and finally including two basins on the Swedish west coast. The dominant wave directions, water depth and wave power resource were considered when choosing the locations of the basins.
For a brief comparative overview of the mean behavior of the wave energy resource in different basins, a cumulative sum of P arranged from its highest to its lowest value is shown in Figure 6a with different colored lines corresponding to different basins. It can be seen that the summation to the annual mean wave energy resource in basin 8 and 11 is the highest and reaches 48 and 45 MWh/m/year, respectively. This is followed by basins 6 and 5 which have 41 and 34 MWh/m/year as an annually averaged theoretical wave energy potential. The two most northern basins 1 and 2 show the lowest wave energy potentials, on average 10 MWh/m/year, and all other basins group together with 19 to 22 MWh/m/year. The mean for all of the SEEZ is 28 MWh/m/year.
In Figure 6b, the same data are shown with a logarithmic x-axis to more easily identify how much of the wave energy comes from relatively short periods of time each year. The strongest storms each year for this region will, due to the synoptic weather conditions, bring with them a surge in wave energy that lasts only a few hours to a day or so. This is due to the relatively short fetch conditions, which result in the predominance of wind sea over swell systems. The summation of ordered wave power values P reveals this aspect of the wave hindcast data. For instance, it can be seen in (b) for basin 8 and 11 that 15 MWh/m is condensed to occur during a time period that amounts, in total, to only about 10 days per year.
To investigate and compare this behavior for different basins, it becomes natural to scale also the y-axis by normalizing with the annual average (Figure 6c). The two most northern basins have about 40% of their wave energy resource summed up in about 10 days, while the comparable percentage for basins 8 and 9 is closer to 30%. This behavior is more prominent for the most northern basins because of their more extensive ice-cover. Each year, the longer ice-time will cause low or no wave energy potential for several months that would otherwise frequently have high wind waves brought on by intense passing low pressure systems.

4.2. The Ice Cover

To investigate the effect of the ice-cover on the wave power potential, the difference between our ice-time-included wave power estimate and a so-called ice-free statistic from Tuomi et al. [19] was calculated, where averaging of P was done only for all the times when the model did not see ice. In this case, this corresponds to ice concentrations less than 30%. Figure 7 clearly shows that in the northern part of the Baltic Sea the wave power may have been reduced by up to 900 W/m, which can constitute even up to 50% of the wave power resource in some regions. Some minor effects on the wave resource between 0 and 150 W/m from the ice-cover can also be seen south of latitude 59 locally around some coastal areas, but most significantly it is basins 1 and 2 that are affected followed by basins 3, 4 and parts of basin 5.
Similar results discussing the influence of ice on the mean significant wave height as well as percentiles of significant wave heights were presented in Björkqvist et al. [24]. In [24], a clear effect in the Gulf of Riga was not seen but a couple of reasons differ between these studies. Here, interpolated ice-concentrations from observations were used; Björkqvist et al. [24] used an ice-model coupled to the wave modeling. The different studies also have different time periods. Björkqvist et al. [24] let the wave model see the ice at 50% ice concentration, whereas in the present work the ice is considered at 30% similar to the setup used in Tuomi et al. [19].

4.3. Directional Dependence

Different directions correspond to different fetch conditions and can therefore behave variably in terms of the available average wave power. Conditionally averaged wave power estimates for separate directional sectors are therefore useful in studying why the wave power resource varies between the basins, as displayed in Figure 4.
In Figure 8, the conditionally averaged wave power in four 90-degree mean wave directional sectors is shown. Waves from the southerly sector (a) correspond well to the overall average pattern of Figure 4, although most of the power potential for this sector is further to the north. This is an effect of the generally longer fetch for the northern parts of basins when the waves are from the south. For northerly waves, the most significant energy resources are located further to the south.
The conditionally averaged wave power is overall lower for wave directions from the north and the east, because the more frequent storm tracks for the region will be mainly from south and southwest. Nevertheless, for easterly waves, the long fetch conditions from the Gulf of Finland cause an interesting anomaly where the northern part of basin 5 has an average wave power of about 5 kW/m (Figure 8c). Such a region could potentially have a more evenly spread out wave power resource.
Finally, it is noticed that for mean wave directions from the west (d), some of the highest averages are in the middle of the southern Baltic Sea (or the Baltic Proper), and along the coasts of Latvia, Lithuania and northern Poland. These regions might have some of the highest wave power potentials in the Baltic Sea, which would be in line with previous modeling studies [17,19,24,47].
In terms of the SEEZ, it is clear that the west coast of Sweden and basin 11 display some of the highest conditionally averaged wave power both with waves from the south and west related to the long fetch conditions from the North Sea. For basin 8—which showed similar annual average wave power to basin 11—the resource is, in general, directionally more spread. In basin 8, the most energetic resources still refer to wave directions from the south and the west, but compared to other basins there is also some more wave power in situations with waves from the north and the east. It is only in the southern part of basin 8 that the highest wave power resource values are shown for the western directional sector. This implies that most of the wave power resource for basin 8 should be expected to come from situations with wave directions from the south and southwest.

4.4. Dependence on the Distance from the Coastline

The previous maps (Figure 4 and Figure 8) show that the distance to the nearest coastline plays an important role in controlling the wave power potential. When the wind is from the coast, the fetch limits the growth of the near-shore waves. For other wind directions, wave energy is smaller than in the open sea because of the sheltering of the shoreline and islands as well as because of the dissipation due to bottom friction and depth-induced wave breaking when the waves approach from open sea to the shallow coastal waters. The influence of these factors on the wave energy is different (see Figure 8), but there is an overall dependence on the geometrical situation, which to some extent can be quantified by the distance to the nearest coast. For two points given in latitude and longitude, the distance between them can be effectively approximated using a Haversine formula [48]. This was done for each sea point and all land points on the computational grid.
Figure 9 displays the variation of annual average wave power at different distances from land for the SEEZ in (a) and compares it to the Baltic Sea as a whole in (b). A largely similar pattern can be seen for the wave power, with an increase close to the square-root of the distance from land for at least the first 40 km from the coast.
Figure 9 shows that the wave power resource can vary greatly at the same distance from the coast. The near-shore variation (less than 5 km from the coast) in wave power ranged from nearly zero to about 6.3 kW/m within the SEEZ. At about 30 km from the coast, variations up to about 7.5 kW/m occurred but very few places had less than 1 kW/m wave power as the annual mean. Such variation needs to be further investigated when areas more or less suitable for placement of wave energy converters are to be identified. A mapping using a relative classification for each grid cell could be useful for further investigation including other aspects.

5. Relative Wave Power Resource Classification

It is reasonable to assume that the costs involved in off-shore projects make it useful to find locations that are relatively close to the coast but also have a reasonably high wave power resource [49]. In a relative classification for the SEEZ, the locations of which are more promising than others with regards to these aspects can be identified. Five classes are defined based on a conditional mean value and its standard deviation of the wave power at different 1 km distance from coast intervals. In a notation with P ¯ S E E Z denoting the mean annual wave power at a given distance interval from the coast and σ S E E Z denoting the corresponding standard deviation (see Figure 9), the annual average wave power P is classified for each grid cell using five classes, where 5 is the best.
Class 1 if the wave power resource is low relative to typical at its distance from the coast:
P P ¯ S E E Z σ S E E Z .
Class 2 if the wave power resource is lower than average relative to its distance, but not as low as the lowest class:
P ¯ S E E Z σ S E E Z < P P ¯ S E E Z .
Class 3 if the wave power resource is greater than average, but not above one added standard deviation:
P ¯ S E E Z < P P ¯ S E E Z + σ S E E Z .
Class 4 if the wave power resource is greater than one added standard deviation, but not two standard deviations:
P ¯ S E E Z + σ S E E Z < P P ¯ S E E Z + 2 σ S E E Z .
Class 5 if the wave power resource is greater than two added standard deviations above the mean for the SEEZ:
P > P ¯ S E E Z + 2 σ S E E Z .
In Figure 10, a map of the result of this classification is presented. It is noticeable how the lower than average wave power resource classes in blue dominate the results above latitude 60. The main area for class 5 is located on the west coast of Sweden (area 11 in Figure 5). Other basins show a more diverse range of results.

5.1. Discussion on Additional Aspects

As mentioned in the introduction, locating the best potential wave energy converter sites requires investigations into several aspects. To illustrate the influence of some of these aspects, the 5-class relative resource classification of the previous section is combined with choices regarding water depth, absolute amount of annual mean wave power resource and distance from the coast, and subsequently also a temporal availability aspect.
In Figure 11a, a red iso-line for a water depth of 100 m is overlaid on top of the relative wave resource classification and it is noticed that several relatively large areas of the SEEZ have depth conditions that exceed 100 m. This is especially true in the outer parts of basins 6, 8 and 11, which are the basins with the highest average wave energy estimates (see Figure 6). The isoline of 100 m was chosen based on literature about the typical water depth of wave energy converter sites in Europe today [6], but is not to be interpreted as a limit for commercial installations in the future. The water depth can also affect the efficiency of the WEC if it is bottom mounted and the availability of the site, including the associated costs for divers during placement, operations and maintenance of wave park equipment [50]. The depth conditions therefore need to be taken into account in a discussion of suitability of potential WEC sites.
The question of choosing a specific amount of wave energy resource that is high enough for a wave energy conversion project to be profitable is a difficult one, as it depends on multiple factors and costs [49]. In Figure 11b, a red iso-line for 3.2 kW/m, as a mean value for the SEEZ, has been plotted to illustrate that areas close to coasts within the SEEZ mostly would not have this much wave power resource in the Baltic Sea, but some coastal areas in basin 11 on the west coast of Sweden do. A site near the island of Sicily with an annual average wave power potential of about 3.3 kW/m was discussed in Iuppa et al. [21] to “… not generate sufficient energy to ensure an economic payback over a reasonable period of time”, but no single wave resource parameter is enough to draw a general conclusion on this. It can, however, be instructive to choose a mid-range value to illustrate a method that can be used to identify interesting areas even if economical concerns and other aspects require additional study.
From the review of Magagna and Uihlein [6], pilot sites for wave energy converters are typically placed within a distance of about 17 km from the coast. To illustrate the effect of such a choice, a red iso-line corresponding to 20 km distance to resolved land is plotted on top of the relative classification in Figure 11c. Since wave climate in the Baltic Sea is milder compared to other European coastal regions, a different value might turn out to be appropriate and for commercial wave energy converter sites different choices will likely be applicable. The maps in Figure 11 should not be considered as final results, but as an illustration of the method. The maximum distance to the shoreline that can be allowed in the Baltic Sea will be determined in upcoming studies, and the maps in Figure 11 could then be redrawn using this evidence-based value. A strong dependence on distance from the coast exists for the energy losses due to transmission, number of weather windows for O&M (operations and maintenance) activities as well as the presence of extreme significant wave heights. Further study is needed for the Baltic Sea region to determine an appropriate choice for the maximum distance from the shoreline. This will likely also depend on the type of wave energy converter.
Different choices for the different aspects will of course decide how inclusive the identification of potentially interesting sites for wave energy conversion becomes. In Figure 11d, areas are identified that fulfil the choice of more than 3.2 kW/m as the annual mean wave power and at the same time are located within 20 km of the coastline, and have a water depth of less than 100 m. This identification should be recognized as an interesting case study, but does not imply that other areas could not be of interest, especially for commercial wave energy converter sites.
The regions identified include a large area in basin 11 on the west coast (marked A on the map), which is natural to assume to be one of the best places given its relatively high wave power resource related to long fetch from the North Sea. Some other smaller identified regions include an area south of the island of Öland and southeast of the Blekinge coast near Karlskrona (marked B). There are also regions around the coasts of Gotland (C) and Gotska Sandön (D) as well as a band outside the Stockholm archipelago ranging from close to Sandhamn in the north to Landsort in the south (E) and some minor areas in basin 9.
It should be recognized that some of these locations might not be possible places for offshore infrastructure due to other aspects not discussed here, such as shipping lines, environmental factors and geotechnical assessment of sea floor conditions. As discussed, less strict choices than those made here would give a more inclusive result, which may be considered advantageous since additional aspects will be considered at a later stage. A more inclusive result could, however, also be discussed to identify areas that do not have much wave energy resource, or that are further from the coast, or in deeper water than any existing European WEC project, considering the review by Magagna and Uihlein [6] from 2015. The relative classification method will also be useful for an inclusive approach, since it will determine whether the locations under consideration have a higher or lower than average wave power resource for their given distance from the coast—a reasonably fair and objective way to find favorable locations for a specific region.
Because choices related to a specific case study can always be discussed in terms of how appropriate they are for a given region, a brief sensitivity analysis in Appendix C is performed. This includes results for a choice of 150 m water depth and investigations varying the annual wave energy potential between 1.2, 3.2 and 5.2 kW/m, as well as exploring three different choices of distance from the coast at 20, 50 and 100 km.

5.2. Temporal Availability

One topic touched upon in Section 4.1 is the temporal availability aspect or uneven temporal distribution of the wave energy resource. At these latitudes, the wave energy is largely governed by passing low-pressure systems and associated high wind events may give very high wave energy potentials for short time periods, followed by other times with much lower amounts of wave resource. However, compared to wind, waves generally offer a less intermittent source over time with more predictable forecasting and a higher degree of utility for electric power production [5,51,52].
The cumulative sum of ordered wave power estimates in Figure 6 showed, however, that a large part of the annual theoretical wave energy potential can come during an amount of time that constitutes only 10 days or a couple of weeks at a basin level. Figure 12a,b illustrate the same issue but at a kilometer-scale level (or wave energy converter park level) to be able to combine this availability aspect with the other aspects presented. From (a), it is recognized that, for many places, between 40 and 60% of the annual wave energy resource constitute a total time-span of less than 3 weeks per year during the most intense wave events. In (b), similarly, between 70 and close to 100% of the wave energy resource occur during a time-span of less than 3 months, implying long time periods with a low wave energy resource in this region every year. In (c), the relative resource classification is shown with a red overlaid iso-line if 50% of the annual wave energy resource is available during a shorter summed up time than 3 weeks. This shows that, in particular, many coastal regions experience reduced temporal availability (or uneven temporal distribution of the wave energy resource), when significant parts of the year experience low wave resource values.
In the case of wave energy, however, it is also important to mention that fewer occurrences and shorter durations of extreme wave conditions are beneficial for wave energy plant survivability, but these aspects are not studied here. Wave energy converters are also generally designed to generate electricity at the most energetic sea state with regard to the yearly production capability. This will be further covered in an upcoming study within the same Swedish national wave energy resource assessment project [22].
In Figure 12d, a zoomed-in view is presented of the southern part of the SEEZ that includes all areas that have passed the introduced criteria in terms of the temporal availability of the wave energy resource, water depth, distance from the coast and amount of wave power resource. The effect added by including the availability aspect was quite small for the previously identified interesting areas in the Baltic Sea (compare Figure 11d), but had a larger impact for the region denoted A in basin 11 around the coasts and in the northern part. This was interpreted to be related to the wave directional dependence in the northern part of basin 11 where wave energy resource was highest mainly from the southern sector and not as high in the case of waves from the western sector. This implied that although the annual averaged wave power was estimated higher than the average for the SEEZ (3.2 kW/m), this was achieved mainly from high wave power resources associated with a specific directional sector. The wave energy hence became less well distributed over time in parts of basin 11 in comparison to, for instance, in basin 8.
This study presents one approach to account for the temporal availability of the wave energy resource, which is an important consideration when identifying potential WEC sites. Other possible methods to achieve this same goal might include quantifying the seasonal dependence of the wave energy resource [27]. This aspect will also be covered more extensively in future technical wave energy resource assessments being conducted for the region.

6. Summary and Conclusions

A 16-year wave hindcast dataset at one-kilometer-scale horizontal resolution for the Baltic Sea and Swedish Exclusive Economic Zone was produced using a third-generation wave model, which took seasonal ice-cover into account. This provided the basis for a wave energy resource assessment at a wave energy converter park level, with a typical size of between about 250 by 250 m and 1 km 2 . This study also provided the first detailed assessment of the wave power resource for the Baltic Sea region.
The wave hindcast dataset was evaluated against wave buoy measurements within or near the SEEZ and showed a good general agreement with the observations. An overall bias of −0.06 m, centered root-mean-square difference of about 0.26 m and linear correlation coefficient of about 0.92 were found (see Table 2), which are comparable to other recent third-generation wave modeling efforts. The dataset was noted to have a slightly too large variability for significant wave height, with standard deviation of the significant wave height being between 1 and 10% larger than the observed values for most places.
The theoretical wave power potential was calculated and analyzed for its dependence on aspects such as fetch related to mean wave directional sectors, water depth and distance to coast, presence of sea-ice and temporal availability. Important variations were shown to occur between different geographical basins of the SEEZ, as well as on more local wave energy park scale. When it comes to the temporal availability study of wave power, an important conclusion was that wave energy became less well distributed over time in basin 11 on the Swedish west coast in comparison to basin 8 (in the Baltic proper). These were the two basins showing the highest wave power potentials within the SEEZ and the study shows the importance of considering the directional dependence of wave power in fetch-limited areas. For these areas, the potential annual average wave energy flux reaches about 45 MWh/m/year, but local variations are up to 65 MWh/m/year.
A method to introduce a 5-class relative classification of the wave power resource for the SEEZ region was presented and illustrated using the wave hindcast data. The method effectively compares the amount of wave power resource at a site to other locations at similar distances to the coast, which helps to identify regions that could—from a wave resource perspective—be interesting for further study. The method could be applied to other basins in different parts of the world and contribute at a national level to identify areas for potential WEC sites.
The relative classification was used together with additional aspects such as water depth, distance from the coast and temporal availability of the wave energy resource in a case study to identify some regions that may be of interest for further study as near-shore potential WEC sites. Related work is ongoing within a broad multi-disciplinary project for marine energy conversion that will cover aspects such as environmental factors (including both ecosystem components and nature conservation areas), geotechnical information (e.g., excavation capacity and bearing capacity of the seafloor), variations in sea-level conditions and technical wave energy resource assessment. The identification of potentially interesting sites is illustrated to heavily depend on choices taken for different aspects and this may be best determined at a project level, since economical concerns are also of interest. The datasets and methods introduced here are, however, stepping stones that can be used to pursue overarching goals that are common for wave energy assessments: combining different types of data for identifying and classifying suitable offshore wave energy pilot sites.

Author Contributions

Conceptualization, E.N., A.R., J.-V.B., H.P. and E.S.; methodology, E.N., J.-V.B., H.P., A.D. and A.R.; software, E.N., A.D., J.-V.B. and H.P.; validation, E.N., J.-V.B. and H.P.; formal analysis, E.N., J.-V.B., H.P. and A.D.; investigation, E.N., J.-V.B., H.P. and A.D.; resources, E.N., A.R., A.D., L.A. and J.N.; data curation, E.N. and A.D.; writing—original draft preparation, E.N.; writing—review and editing, E.N., A.R., A.D., J.-V.B., H.P., L.A., J.N. and E.S.; visualization, E.N.; project administration, E.N., A.R. and E.S.; funding acquisition, E.S., A.R. and E.N.

Funding

The authors thank the Swedish Energy Agency for financing this project (Project No. 42256-1) within the national Swedish research program for marine energy conversion. E.N. and A.R. were partly funded by Swedish Research Council (Grant No. 2015-06020), FORMAS (Grant No. 2018-01784) and by Finn-Malmgrens scholarship.

Acknowledgments

The wave modeling was mostly performed on resources provided by SNIC through Uppsala Multidisciplinary Center for Advanced Computational Science (UPPMAX) under Project SNIC 2017/1-222, High-resolution atmospheric and wave modeling for the Baltic Sea. The Östergarnsholm wave measurements are part of the research infrastructure facilities provided by FINMARI (Finnish Marine Research Infrastructure network). The project is also supported by the Swedish STandUP for Energy research alliance, a collaboration initiative financed by the Swedish gorvernment. StandUP for Energy is acknowledged for providing a research infrastructure.

Conflicts of Interest

The authors declare no conflict of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results.

Appendix A. Evaluation Metrics

Let us consider two variables, f n and r n , defined at N discrete points (in time and or space). For us, f can represent the hindcast values and the reference field values; r can represent the wave buoy observations. The correlation coefficient R between f and r is defined as
R = 1 N n = 1 N ( f n f ¯ ) ( r n r ¯ ) σ f σ r ,
where f ¯ and r ¯ are the mean values and σ f and σ r are the standard deviations of f and r, respectively.
A commonly used statistic to quantify differences in two fields is the RMS difference E, which for fields f and r is defined as
E = 1 N n = 1 N ( f n r n ) 2 1 / 2 .
To separate the differences in the patterns from the differences in the mean values of the two fields, E can be resolved into two components. The overall bias is defined as
E ¯ = f ¯ r ¯
and the centered pattern RMS difference or error (CRMSE) is defined by
E = 1 N n = 1 N ( f n f ¯ ) ( r n r ¯ ) 2 1 / 2 .
Because the correlation R, centered root-mean-square error E and standard deviations of the test field σ f and reference field σ r are related through the relationship
E 2 = σ f 2 + σ r 2 2 σ f σ r R ,
and the law of cosines is similarly given by
c 2 = a 2 + b 2 2 a b c o s ϕ ,
where a, b, and c are the lengths of the sides of a triangle and ϕ is the angle opposite side c. These evaluation metrics can be presented effectively using a Taylor diagram [46].

Appendix B. Wave Power Potential Estimates

Computation of the wave power estimates is based on the energy flux per unit crest length relationship for random waves that is defined as:
P = ρ g E ( f ) c g ( f , h ) d f ,
where ρ is the density of seawater (1008 kgm−3 was used as a representative value for the surface water in the Baltic Sea), g is the acceleration of gravity (9.82 ms−2), f is the frequency, E is the variance density spectrum, and c g is the group velocity.
Most integrated wave parameters are defined using spectral moments. The n-th moment is defined as
m n = f n E ( f ) d f .
Since the moment m 0 is simply the variance of the wave field, the significant wave height H s can be defined as
H s = H m 0 = 4 m 0 .
The energy period T e , which is also called the mean wave period, is defined as:
T e = m 1 m 0 .
We can now determine an approximation for the wave energy flux in terms of these two variables:
P = 1 16 ρ g H s 2 c g ( T e , h ) .
The group velocity c g is approximated from the energy period T e and water depth h. Since this choice of group velocity is independent of f, the above equation follows directly from the integral in Equation (A7). All calculations are based on this formula, which is given as Equation (1) in the main text.
A simple approximation is used to iterate and find the group velocity using the water depth, h, and wave energy period, T e , similar to that which has been applied in previous work [11,15]. Here, however, the energy period is used (instead of the peak period which is sometimes used due to availability reasons) because Equation (A11) gives the exact value of the wave energy flux if the water depth is deep.
The method was compared on field measurements from the Östergarnsholm buoy in 39 m water depth and a small difference of −2% was found (not shown here) to the full wave spectrum calculation, which is more accurate. A smaller dataset of high-frequency wave measurements from the Väderöarna WR buoy was also used for testing and in 79 m water depth there was no difference in the results from the two methods.

Appendix C. Exploring the Effects of Different Choices when Identifying Areas of Wave Power Potential

Figure A1 shows the relative wave power resource classification when the choice for water depth is 150 m and for mean wave power 1.2 kW/m. Three different constraints on the distance from the shore are shown in Figure A1b–d. For more inclusive choices, larger areas will be identified and many of them will, by the relative resource classification, be recognized to have less than average theoretical wave power potential (blue colors) compared to sites at similar distances from the coast.
Figure A2 presents an investigation of how three different choices of mean annual wave power will affect which areas of the SEEZ remain for the case of a water depth limit of 150 m and distance from the coast limit of 100 km, which is recognized as being very inclusive. For a limit of 1.2 kW/m on the chosen wave power, most areas of the SEEZ would remain and for choices of 3.2 kW/m or 5.2 kW/m the area of interest is significantly reduced for this part of the world with relatively sheltered coastal regions.
Figure A1. In (a), the 5-class relative wave power resource classification is shown together with a red iso-line for the SEEZ region, indicating 150 m water depth. In (b), the relative classification is shown only for the areas that have less than 150 m water depth, more than 1.2 kW/m as annual wave power resource and are located within 100 km of land. (c) is the same as (b) but with a limit of 50 km distance from land. (d) is the same as (b) but with a limit of 20 km distance from land.
Figure A1. In (a), the 5-class relative wave power resource classification is shown together with a red iso-line for the SEEZ region, indicating 150 m water depth. In (b), the relative classification is shown only for the areas that have less than 150 m water depth, more than 1.2 kW/m as annual wave power resource and are located within 100 km of land. (c) is the same as (b) but with a limit of 50 km distance from land. (d) is the same as (b) but with a limit of 20 km distance from land.
Energies 12 00793 g0a1
Figure A2. In (a), the 5-class relative wave power resource classification is shown together with a red iso-line for the SEEZ region, indicating 150 m water depth. In (b), the relative classification is shown only for the areas that have less than 150 m water depth, more than 1.2 kW/m as annual wave power resource and are located within 100 km of land. (c) is the same as (b) but with a wave resource larger than 3.2 kW/m. (d) is the same as (b) but with a wave resource larger than 5.2 kW/m.
Figure A2. In (a), the 5-class relative wave power resource classification is shown together with a red iso-line for the SEEZ region, indicating 150 m water depth. In (b), the relative classification is shown only for the areas that have less than 150 m water depth, more than 1.2 kW/m as annual wave power resource and are located within 100 km of land. (c) is the same as (b) but with a wave resource larger than 3.2 kW/m. (d) is the same as (b) but with a wave resource larger than 5.2 kW/m.
Energies 12 00793 g0a2

References

  1. IEA. Renewables 2017, Analysis and Forecasts to 2022 EXECUTIVE SUMMARY; Market Report Series; International Energy Agency: Paris, France, 2017; pp. 1–12. Available online: https://www.iea.org/media/publications/mtrmr/Renewables2017ExecutiveSummary.PDF (accessed on 20 August 2018).
  2. De, O.; Falcao, A. Wave energy utilization: A review of the technologies. Renew. Sustain. Energy Rev. 2010, 14, 899–918. [Google Scholar]
  3. Ross, D. Power from Sea Waves; Oxford University Press: Oxford, UK, 1995. [Google Scholar]
  4. Drew, B.; Plummer, A.R.; Sahinkaya, M.N. A review of wave energy converter technology. Proc. Inst. Mech. Eng. Part A J. Power Energy 2009, 223, 887–902. [Google Scholar] [CrossRef] [Green Version]
  5. Rusu, E.; Onea, F. A review of the technologies for wave energy extraction. Clean Energy 2018, 2, 10–19. [Google Scholar] [CrossRef] [Green Version]
  6. Magagna, D.; Uihlein, A. Ocean energy development in Europe: Current status and future perspectives. Int. J. Mar. Energy 2015, 11, 84–104. [Google Scholar] [CrossRef] [Green Version]
  7. IEA. Renewable Energy Medium-Term Market Report 2014, Market Analysis and Forecasts to 2020; Market Report Series; International Energy Agency: Paris, France, 2014; pp. 1–260. Available online: http://www.iea.org/publications/freepublications/publication/MTRMR2014.pdf (accessed on 20 August 2018).
  8. Morim, J.; Cartwright, N.; Etemad-Shahidi, A.; Strauss, D.; Hemer, M. Wave energy resource assessment along the Southeast coast of Australia on the basis of a 31-year hindcast. Appl. Energy 2016, 184, 276–297. [Google Scholar] [CrossRef]
  9. Bernardino, M.; Rusu, L.; Soares, C.G. Evaluation of the wave energy resources in the Cape Verde Islands. Renew. Energy 2017, 101, 316–326. [Google Scholar] [CrossRef]
  10. Akpınar, A.; Bingölbali, B.; Vledder, G.P.V. Long-term analysis of wave power potential in the Black Sea, based on 31-year SWAN simulations. Ocean Eng. 2017, 130, 482–497. [Google Scholar] [CrossRef]
  11. Kovaleva, O.; Eelsalu, M.; Soomere, T. Hot-spots of large wave energy resources in relatively sheltered sections of the Baltic Sea coast. Renew. Sustain. Energy Rev. 2017, 74, 424–437. [Google Scholar] [CrossRef]
  12. Farhadzadeh, A.; Hashemi, M.R.; Neill, S. Characterizing the Great Lakes hydrokinetic renewable energy resource: Lake Erie wave, surge and seiche characteristics. Energy 2017, 128, 661–675. [Google Scholar] [CrossRef]
  13. Chen, X.; Wang, K.; Zhang, Z.; Zeng, Y.; Zhang, Y.; O’Driscoll, K. An assessment of wind and wave climate as potential sources of renewable energy in the nearshore Shenzhen coastal zone of the South China Sea. Energy 2017, 134, 789–801. [Google Scholar] [CrossRef] [Green Version]
  14. Kasiulis, E.; Kofoed, J.P.; Povilaitis, A.; Radzevičius, A. Spatial Distribution of the Baltic Sea Near-Shore Wave Power Potential along the Coast of Klaipėda, Lithuania. Energies 2017, 10, 2170. [Google Scholar] [CrossRef]
  15. Soomere, T.; Eelsalu, M. On the wave energy potential along the eastern Baltic Sea coast. Renew. Energy 2014, 71, 221–233. [Google Scholar] [CrossRef]
  16. Bernhoff, H.; Sjöstedt, E.; Leijon, M. Wave energy resources in sheltered sea areas: A case study of the Baltic Sea. Renew. Energy 2006, 31, 2164–2170. [Google Scholar] [CrossRef]
  17. Henfridsson, U.; Neimane, V.; Strand, K.; Kapper, R.; Bernhoff, H.; Danielsson, O.; Leijon, M.; Sundberg, J.; Thorburn, K.; Ericsson, E.; et al. Wave energy potential in the Baltic Sea and the Danish part of the North Sea, with reflections on the Skagerrak. Renew. Energy 2007, 32, 2069–2084. [Google Scholar] [CrossRef]
  18. Kasiulis, E.; Punys, P.; Kofoed, J.P. Assessment of theoretical near-shore wave power potential along the Lithuanian coast of the Baltic Sea. Renew. Sustain. Energy Rev. 2015, 41, 134–142. [Google Scholar] [CrossRef]
  19. Tuomi, L.; Kahma, K.; Pettersson, H. Wave hindcast statistics in the seasonally ice-covered Baltic Sea. Boreal Environ. Res. 2011, 16, 451–472. [Google Scholar]
  20. Framework Agreement between the Swedish Social Democratic Party, the Moderate Party, the Swedish Green Party, the Centre Party and the Christian Democrats. 2016. Available online: https://www.government.se/49d8c1/contentassets/8239ed8e9517442580aac9bcb00197cc/ek-ok-eng.pdf (accessed on 20 August 2018).
  21. Iuppa, C.; Cavallaro, L.; Vicinanza, D.; Foti, E. Investigation of suitable sites for wave energy converters around Sicily (Italy). Ocean Sci. 2015, 11, 543–557. [Google Scholar] [CrossRef] [Green Version]
  22. Strömstedt, E.; Haikonen, K.; Engström, J.; Götman, M.; Sundberg, J.; Nyberg, J.; Zillén-Snowball, L.; Nilsson, E.; Dingwell, A.; Rutgersson, A. On Defining Wave Energy Pilot Sites in Swedish Seawaters. In Proceedings of the 12th European Wave and Tidal Energy Conference (EWTEC), Cork, Ireland, 27 August–1 September 2017. [Google Scholar]
  23. Björkqvist, J.V.; Tuomi, L.; Fortelius, C.; Pettersson, H.; Tikka, K.; Kahma, K.K. Improved estimates of nearshore wave conditions in the Gulf of Finland. J. Mar. Syst. 2017, 171, 43–53. [Google Scholar] [CrossRef]
  24. Björkqvist, J.V.; Lukas, I.; Alari, V.; van Vledder, G.P.; Hulst, S.; Pettersson, H.; Behrens, A.; Männik, A. Comparing a 41-year model hindcast with decades of wave measurements from the Baltic Sea. Ocean Eng. 2018, 152, 57–71. [Google Scholar] [CrossRef] [Green Version]
  25. Weisse, R.; von Storch, H.; Callies, U.; Chrastansky, A.; Feser, F.; Grabemann, I.; Günther, H.; Pluess, A.; Stoye, T.; Tellkamp, J.; et al. Regional Meteorological-Marine Reanalyses and Climate Change Projections. Bull. Am. Meteorol. Soc. 2009, 90, 849–860. [Google Scholar] [CrossRef]
  26. Reistad, M.; Breivik, Ø.; Haakenstad, H.; Aarnes, O.; Furevik, B. A High-Resolution Hindcast of Wind and Waves for The North Sea, The Norwegian Sea and The Barents Sea; Technical Report; Norwegian Meteorological Institute Research Report No. 2009/14; Norwegian Meteorological Institute: Oslo, Norway, 2009. [Google Scholar]
  27. Jakimavičius, D.; Kriaučiūnienė, J.; Šarauskienė, D. Assessment of wave climate and energy resources in the Baltic Sea nearshore (Lithuanian territorial water). Oceanologia 2018, 60, 207–218. [Google Scholar] [CrossRef]
  28. Holmberg, P.; Andersson, M.; Bolund, B.; Strandanger, K. Wave Power, Surveillance study of the development. Elforsk Rapport 2011, 11, 1–66. [Google Scholar]
  29. Nobre, A.; Pacheco, M.; Jorge, R.; Lopes, M.; Gato, L. Geo-spatial multi-criteria analysis for wave energy conversion system deployment. Renew. Energy 2009, 34, 97–111. [Google Scholar] [CrossRef]
  30. The Wamdi Group. The WAM Model-A Third Generation Ocean Wave Prediction Model. J. Phys. Oceanogr. 1988, 18, 1775–1810. [Google Scholar] [CrossRef]
  31. Komen, G.J.; Cavaleri, L.; Donelan, M.; Hasselmann, K.; Hasselmann, S.; Janssen, P.A.E.M. Dynamics and Modelling Ocean Waves; Cambridge University Press: Cambridge, UK, 1994. [Google Scholar]
  32. Guenther, H.; Hasselmann, S.; Janssen, P. The WAM Model Cycle 4; Technical Report; Deutsches KlimaRechenZentrum: Hamburg, Germany, 1992. [Google Scholar]
  33. Monbaliu, J.; Padilla-Hernández, R.; Hagreaves, J.C.; Albiach, J.C.C.; Luo, W.; Sclavo, M.; Günter, H. The spectral wave model, WAM, adapted for applications with high spatial resolution. Coast. Eng. 2000, 41, 41–62. [Google Scholar] [CrossRef]
  34. Räämet, A.; Soomere, T. The wave climate and its seasonal variability in the northeastern Baltic Sea. Estonian J. Earth Sci. 2010, 59, 100–113. [Google Scholar] [CrossRef]
  35. Soomere, T.; Weisse, R.; Behrens, A. Wave climate in the Arkona Basin, the Baltic Sea. Ocean Sci. 2012, 8, 287–300. [Google Scholar] [CrossRef] [Green Version]
  36. Tuomi, L.; Pettersson, H.; Fortelius, C.; Tikka, K.; Björkqvist, J.V.; Kahma, K.K. Wave modelling in archipelagos. Coast. Eng. 2014, 83, 205–220. [Google Scholar] [CrossRef]
  37. Baltic Sea Hydrographic Commission. Baltic Sea Bathymetry Database Version 0.9.3; BSHC: Helsinki, Finland, 2013; Available online: http://data.bshc.pro/ (accessed on 20 January 2016).
  38. Marine Information Service. EMODnet Digital Bathymetry (DTM); Marine Information Service: Alimos, Greece, 2016; Available online: http://www.emodnet-bathymetry.eu/ (accessed on 1 January 2017).
  39. Uiboupin, R.; Axell, L.; Raudsepp, U.; Sipelgas, L. Comparison of operational ice charts with satellite based ice concentration products in the Baltic Sea. In Proceedings of the 2010 IEEE/OES Baltic International Symposium (BALTIC), Riga, Latvia, 24–27 August 2010; pp. 1–8. [Google Scholar]
  40. Undén, P.; Rontu, L.; Järvinen, H.; Lynch, P.; Calvo, J.; Cats, G.; Cuaxart, J.; Eerola, K.; Fortelius, C.; Garcia-Moya, J.; et al. HIRLAM-5 Scientific Documentation; Technical Report; HIRLAM-5 Project; Swedish Meteorological and Hydrological Institute: Norrköping, Sweden, 2002.
  41. Dahlgren, P.; Kållberg, P.; Landelius, T.; Undén, P. EURO4M Project Report, D 2.9 Comparison of the Regional Reanalyses Products with Newly Developed and Existing State-of-the Art Systems; Technical Report; EURO4M Project; Swedish Meteorological and Hydrological Institute: Norrköping, Sweden, 2014.
  42. Claus, S.; Hauwere, N.D.; Vanhoorne, B.; Dias, F.S.; García, P.O.; Schepers, L.; Hernandez, F.; Mees, J. Marineregions.org Towards a Standard for Georeferenced Marine Names; Flanders Marine Institute: Ostend, Belgium, 2018; Available online: http://marineregions.org/ (accessed on 1 January 2018).
  43. Björkqvist, J.V.; Tuomi, L.; Tollman, N.; Kangas, A.; Pettersson, H.; Marjamaa, R.; Jokinen, H.; Fortelius, C. Brief communication: Characteristic properties of extreme wave events observed in the northern Baltic Proper, Baltic Sea. Nat. Hazards Earth Syst. Sci. 2017, 17, 1653–1658. [Google Scholar] [CrossRef] [Green Version]
  44. Nilsson, E.; Bergström, H. Från mätt vind till vindklimat, Normalårskorrigering. Elforsk Rapport 2009, 9, 1–39. [Google Scholar]
  45. Waters, R.; Engström, J.; Isberg, J.; Leijon, M. Wave climate off the Swedish west coast. Renew. Energy 2009, 34, 1600–1606. [Google Scholar] [CrossRef]
  46. Taylor, K.E. Summarizing multiple aspects of model performance in a single diagram. J. Geophys. Res. Atmos. 2001, 106, 7183–7192. [Google Scholar] [CrossRef] [Green Version]
  47. Jönsson, A.; Broman, B.; Rahm, L. Variations in the Baltic Sea wave fields. Ocean Eng. 2003, 30, 107–126. [Google Scholar] [CrossRef]
  48. Veness, C. Calculate Distance, Bearing and More between Latitude/Longitude Points. Available online: http://www.movable-type.co.uk (accessed on 1 January 2018).
  49. Astariz, S.; Iglesias, G. The economics of wave energy: A review. Renew. Sustain. Energy Rev. 2015, 45, 397–408. [Google Scholar] [CrossRef]
  50. Guanche, R.; de Andrés, A.; Losada, I.; Vidal, C. A global analysis of the operation and maintenance role on the placing of wave energy farms. Energy Convers. Manag. 2015, 106, 440–456. [Google Scholar] [CrossRef]
  51. Leijon, M.; Skoglund, A.; Waters, R.; Rehn, A.; Lindahl, M. On the physics of power, energy and economics of renewable electric energy sources—Part I. Renew. Energy 2010, 35, 1729–1734. [Google Scholar] [CrossRef]
  52. Skoglund, A.; Leijon, M.; Rehn, A.; Lindahl, M.; Waters, R. On the physics of power, energy and economics of renewable electric energy sources—Part II. Renew. Energy 2010, 35, 1735–1740. [Google Scholar] [CrossRef]
Figure 1. In (a), measured wave buoy distributions of significant wave height are shown for 13 locations with a varying number of available data, but always more than 15,000 half-hours of data, as indicated by the legend. In (b), the distributions of significant wave height for the 13 locations are shown based on 16 years of hourly output in the generated wave hindcast dataset. Different colors correspond to the subdivision of the SEEZ into 11 regional zones.
Figure 1. In (a), measured wave buoy distributions of significant wave height are shown for 13 locations with a varying number of available data, but always more than 15,000 half-hours of data, as indicated by the legend. In (b), the distributions of significant wave height for the 13 locations are shown based on 16 years of hourly output in the generated wave hindcast dataset. Different colors correspond to the subdivision of the SEEZ into 11 regional zones.
Energies 12 00793 g001
Figure 2. Map of the SEEZ with 17 selected grid points (marked in red) with saved full two-dimensional wave spectral information. The numbers at the 14 buoy locations denote the bias (Table 2). Locations marked with red squares (KP Sundsvall, KP Ålands hav, KP Ystad) had no wave buoy measurements but the two-dimensional wave spectra were saved. A dark blue line is included to indicate the extent of the SEEZ.
Figure 2. Map of the SEEZ with 17 selected grid points (marked in red) with saved full two-dimensional wave spectral information. The numbers at the 14 buoy locations denote the bias (Table 2). Locations marked with red squares (KP Sundsvall, KP Ålands hav, KP Ystad) had no wave buoy measurements but the two-dimensional wave spectra were saved. A dark blue line is included to indicate the extent of the SEEZ.
Energies 12 00793 g002
Figure 3. Taylor diagram for 11 observational wave records (red dots) with overlapping modeled and measured significant wave height. The red point marked A corresponds to the observational truth, whereas other letters correspond to different wave records, see Table 2. Blue dash-dotted lines indicate linear correlation. Green dashed lines correspond to centered root mean square difference normalized with the observational standard deviation. Black dotted lines indicate the ratio of modeled and observed standard deviation. A full black line for the value 1 corresponds to the observed normalized standard deviation.
Figure 3. Taylor diagram for 11 observational wave records (red dots) with overlapping modeled and measured significant wave height. The red point marked A corresponds to the observational truth, whereas other letters correspond to different wave records, see Table 2. Blue dash-dotted lines indicate linear correlation. Green dashed lines correspond to centered root mean square difference normalized with the observational standard deviation. Black dotted lines indicate the ratio of modeled and observed standard deviation. A full black line for the value 1 corresponds to the observed normalized standard deviation.
Energies 12 00793 g003
Figure 4. Map of the estimated annual mean wave power P for the Baltic Sea region including also the west coast region of the Swedish Exclusive Economic Zone. A black line is included to indicate the extent of the SEEZ.
Figure 4. Map of the estimated annual mean wave power P for the Baltic Sea region including also the west coast region of the Swedish Exclusive Economic Zone. A black line is included to indicate the extent of the SEEZ.
Energies 12 00793 g004
Figure 5. Subdivision of Swedish Exclusive Economic Zone into 11 smaller basins indicated by number and different colors.
Figure 5. Subdivision of Swedish Exclusive Economic Zone into 11 smaller basins indicated by number and different colors.
Energies 12 00793 g005
Figure 6. Cumulative sum of sorted wave power P (from highest to lowest) shown as a function of number of days summed for the 11 basins of the Swedish Exclusive Economic Zone in (a). In (b), a logarithmic x-axis is used and in (c) the cumulative sum of wave power P has been normalized with the annually summed value for each basin.
Figure 6. Cumulative sum of sorted wave power P (from highest to lowest) shown as a function of number of days summed for the 11 basins of the Swedish Exclusive Economic Zone in (a). In (b), a logarithmic x-axis is used and in (c) the cumulative sum of wave power P has been normalized with the annually summed value for each basin.
Energies 12 00793 g006
Figure 7. Difference in annual mean wave power estimates for ice-free conditions and ice-time-included statistics, illustrating a reduction of the wave power resource in the northern basins and along some coastal regions due to the presence of sea-ice. A black line is included to indicate the extent of the SEEZ.
Figure 7. Difference in annual mean wave power estimates for ice-free conditions and ice-time-included statistics, illustrating a reduction of the wave power resource in the northern basins and along some coastal regions due to the presence of sea-ice. A black line is included to indicate the extent of the SEEZ.
Energies 12 00793 g007
Figure 8. Map of the mean ice-free theoretical wave power potential conditionally averaged for four directional 90 degree sectors: in (a) if the mean wave direction is from the south, (b) if from north, (c) if from east and (d) if waves are from the west.
Figure 8. Map of the mean ice-free theoretical wave power potential conditionally averaged for four directional 90 degree sectors: in (a) if the mean wave direction is from the south, (b) if from north, (c) if from east and (d) if waves are from the west.
Energies 12 00793 g008
Figure 9. Annual mean wave power as a function of the distance to the nearest resolved land is shown for the SEEZ (a) in comparison to the Baltic Sea as a whole (in b). The white line with error bars shows the mean and 1 standard deviation of the data for a 1 km distance interval bin. The red line indicates the maximum value of each 1 kilometer bin. The color scale indicates the amount of total area in different combined 3 kilometer distance and 500 W/m wave power interval bins. Note the different scales in color bars.
Figure 9. Annual mean wave power as a function of the distance to the nearest resolved land is shown for the SEEZ (a) in comparison to the Baltic Sea as a whole (in b). The white line with error bars shows the mean and 1 standard deviation of the data for a 1 km distance interval bin. The red line indicates the maximum value of each 1 kilometer bin. The color scale indicates the amount of total area in different combined 3 kilometer distance and 500 W/m wave power interval bins. Note the different scales in color bars.
Energies 12 00793 g009
Figure 10. A relative classification of the wave power resource in five categories comparing the wave power at sites relative to typical annual mean values for its given distance from the coast, as presented in Figure 9.
Figure 10. A relative classification of the wave power resource in five categories comparing the wave power at sites relative to typical annual mean values for its given distance from the coast, as presented in Figure 9.
Energies 12 00793 g010
Figure 11. In (a), the relative wave power resource classification is shown together with a red iso-line for the SEEZ region indicating 100 m water depth. In (b), the red iso-line indicates a wave power of 3.2 kW/m. In (c), the red iso-line is drawn for the 20 km distance to the resolved land contour. In (d), the relative classification is shown only for the areas that have lower than 100 m water depth, more than 3.2 kW/m as annual mean wave power and are located less than 20 km from land (including the islands of Öland, Gotland and Gotska Sandön).
Figure 11. In (a), the relative wave power resource classification is shown together with a red iso-line for the SEEZ region indicating 100 m water depth. In (b), the red iso-line indicates a wave power of 3.2 kW/m. In (c), the red iso-line is drawn for the 20 km distance to the resolved land contour. In (d), the relative classification is shown only for the areas that have lower than 100 m water depth, more than 3.2 kW/m as annual mean wave power and are located less than 20 km from land (including the islands of Öland, Gotland and Gotska Sandön).
Energies 12 00793 g011
Figure 12. Map of the percentage of the annual wave resource available during the 3 weeks with the highest estimated wave power in (a) and for the 3 months with the highest estimated wave power in (b). In (c), the relative resource classification is shown with an added red isoline indicating whether 50% of the annual mean wave energy resource is available during a shorter summed up period of time than 3 weeks. In (d), the relative resource classification is shown only for the areas that have lower than 100 m water depth, more than 3.2 kW/m annual mean wave power, are located within 20 km of land and have a more spread out wave resource over time using the iso-line criteria displayed in (c).
Figure 12. Map of the percentage of the annual wave resource available during the 3 weeks with the highest estimated wave power in (a) and for the 3 months with the highest estimated wave power in (b). In (c), the relative resource classification is shown with an added red isoline indicating whether 50% of the annual mean wave energy resource is available during a shorter summed up period of time than 3 weeks. In (d), the relative resource classification is shown only for the areas that have lower than 100 m water depth, more than 3.2 kW/m annual mean wave power, are located within 20 km of land and have a more spread out wave resource over time using the iso-line criteria displayed in (c).
Energies 12 00793 g012
Table 1. Descriptive site and wave information on locations with wave buoys in or near the SEEZ. Latitude and longitude are given in WGS84. Also shown are water depth, approximate distance to nearest coast, mean significant wave height and 95th percentile of the significant wave height determined from measurements and closest gridpoint hindcast data.
Table 1. Descriptive site and wave information on locations with wave buoys in or near the SEEZ. Latitude and longitude are given in WGS84. Also shown are water depth, approximate distance to nearest coast, mean significant wave height and 95th percentile of the significant wave height determined from measurements and closest gridpoint hindcast data.
Name(Lat, Lon)DepthDistance H s ¯ ( Buoy ) H s ¯ P 95 ( Buoy ) P 95
Unit-[m][km][m][m][m][m]
Finngrundet(60.9000, 18.6167)70.143.90.860.822.032.07
Svenska Björn(59.4667, 20.3500)50.544.01.121.072.632.80
Almagrundet(59.1500, 19.1333)46.819.10.920.962.372.46
Huvudskär Ost(58.9333, 19.1667)98.838.70.941.002.192.58
Huvudskär Ost WR(58.9333, 19.1667)98.838.71.211.002.712.58
Gustav Dahlen(58.6000, 17.4667)65.412.30.690.711.711.85
Knolls grund(57.5167, 17.6167)93.329.90.950.892.202.25
Östergarnsholm(57.4167, 19.0533)28.08.50.890.822.032.10
Ölands södra grund(56.0667, 16.6833)37.922.31.031.042.412.62
Södra Östersjön(55.9167, 18.7833)112.4116.41.241.213.043.11
Karlskrona(55.9333, 15.3167)46.120.80.950.821.902.12
Oskarsgrundet(55.6000, 12.8500)8.34.20.370.340.780.87
Läsö Ost(57.2167, 11.5667)61.124.30.810.831.772.17
Läsö Ost WR(57.2167, 11.5667)61.124.30.770.831.662.17
Trubaduren(57.6000, 11.6333)36.28.40.740.791.852.18
Väderöarna(58.4833, 10.9333)72.018.31.021.022.512.89
Väderöarna WR(58.4833, 10.9333)72.018.31.131.022.832.89
Table 2. Wave buoy evaluation statistics and information on available data.
Table 2. Wave buoy evaluation statistics and information on available data.
NameLetterNr. DataCoincidingBiasCRMSECorrelation σ buoy
Unit---[m][m]-[m]
FinngrundetB68,75750,986−0.010.240.930.63
Svenska Björn-15,4760----
Alma grundetC130,00423,5150.040.290.910.67
Huvudskär OstD49,70945,602−0.030.240.940.65
Huvudskär Ost WR-36233623−0.070.210.960.75
Gustav Dahlen-24,3990----
Knolls grundE41,86517,065−0.030.230.950.65
ÖstergarnsholmF69,33823,315−0.090.210.950.61
Ölands södra grundG140,70234,1940.050.300.930.67
Södra ÖstersjönH33,94633,946−0.080.250.960.89
Karlskrona-13880----
OskarsgrundetI98,1448611−0.020.170.710.20
Läsö OstJ33,01233,012−0.120.270.920.50
Läsö Ost WR-24292429−0.060.220.900.49
TrubadurenK150,88827,1900.060.280.930.51
Väderöarna-56426020.150.380.950.80
Väderöarna WRL85,05267,488−0.090.380.920.87

Share and Cite

MDPI and ACS Style

Nilsson, E.; Rutgersson, A.; Dingwell, A.; Björkqvist, J.-V.; Pettersson, H.; Axell, L.; Nyberg, J.; Strömstedt, E. Characterization of Wave Energy Potential for the Baltic Sea with Focus on the Swedish Exclusive Economic Zone. Energies 2019, 12, 793. https://doi.org/10.3390/en12050793

AMA Style

Nilsson E, Rutgersson A, Dingwell A, Björkqvist J-V, Pettersson H, Axell L, Nyberg J, Strömstedt E. Characterization of Wave Energy Potential for the Baltic Sea with Focus on the Swedish Exclusive Economic Zone. Energies. 2019; 12(5):793. https://doi.org/10.3390/en12050793

Chicago/Turabian Style

Nilsson, Erik, Anna Rutgersson, Adam Dingwell, Jan-Victor Björkqvist, Heidi Pettersson, Lars Axell, Johan Nyberg, and Erland Strömstedt. 2019. "Characterization of Wave Energy Potential for the Baltic Sea with Focus on the Swedish Exclusive Economic Zone" Energies 12, no. 5: 793. https://doi.org/10.3390/en12050793

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