1. Introduction
The rapid development of road transportation infrastructure causes a large amount of greenhouse gas emissions due to the consumption of materials, fuel, and energy during the processes of construction, maintenance, and service, and this exacerbates the problem of global warming. Studies regarding the utilization of recycled solid waste materials and road energy harvesting technology have been conducted to achieve the purposes of energy saving and emission reduction [
1,
2,
3]. Of these, solar energy, which is clean, renewable, and widely distributed along highways, illustrates great potential in the field of roadway clean energy harvesting to support the energy consumption of infrastructure and vehicles. Moreover, photovoltaic (PV) power generation is commonly used to convert solar energy into electricity [
4,
5].
Before their application in the road transportation field, PV modules were widely used in central PV power plants [
6], building roofs [
7,
8], the water surface areas of reservoirs, the idle land of airports, and the space outside cooling towers [
9,
10,
11,
12,
13] for solar power generation. In contrast, highway infrastructure possesses significant energy endowment due to the long route length and wide distribution area exposed to the sun, compensating for the disadvantage of requiring a large amount of land to arrange PV modules. PV power generation in road traffic is commonly realized by means of PV pavements, PV channels, roadside parking lot roofs, the slopes along highways, etc. [
14,
15,
16]. Considering the long routes, huge areas, and easy placement of PV modules, road slopes have gradually drawn more attention in road solar energy harvesting in recent decades [
17]. For instance, many engineering projects of PV power generation systems on highway slopes have been constructed and put into use in provinces such as Shandong and Henan in China. To facilitate the large-scale utilization of solar energy on highway slopes, it is necessary to provide practical calculation and assessment methods for the power generation potential in order to support the PV power generation system’s decision-making, planning, and design processes for project-level and network-level applications.
There are many studies on the PV power generation potential evaluation of countries, cities, blocks, building roofs, and certain objects, such as the cooling towers in thermal power plants [
7,
12,
18,
19,
20,
21]. However, different assessment methods have been adopted for different application scenarios since the affecting factors of the spatial distribution, the geometric boundary, and the solar radiation vary. In the field of solar power generation potential assessments of highways and highway slopes, Sharma et al. [
15] investigated the PV power generation potential of an Indian national expressway by constructing roof structures above the highways. Kim et al. [
16] introduced the site selection criteria for PV power generation projects on national highways in South Korea, and they illustrated examples of solar power generation systems installed on parking lot roofs in rest areas, highway slopes, and abandoned roads. Jung et al. [
17] proposed a method to evaluate the photovoltaic power generation potential of road slopes using publicly available digital maps for the site selection of PV panels. Rehman et al. [
22] evaluated the power generation potential of public bus routes by considering the shading impact of obstacles based on fisheye image processing results. Kim et al. [
23] put forward a two-stage assessment approach for the highway solar energy potential, which firstly identifies suitable solar energy utilization sites on a national highway network using low-resolution maps and then evaluates the PV power generation potential on the slopes of the selected sites using high-resolution maps.
Therefore, it can be observed that the existing research has mainly focused on the PV power generation potential assessment of in-service highways using digital maps or image processing techniques. The impacts of the highway orientation, the geometric characteristics of highway slopes, and the placement scheme of PV panels are not comprehensively considered during potential assessments. To address these problems, this study aims to establish an assessment method for the PV generation potential of highway slopes based on the design or measured geometric parameters of the slope, the highway orientation, and the optimum placement scheme of the PV panels. The assessment method could help with the estimation of the solar energy utilization potential of highway slopes and facilitate decision making and scheme selection in the planning and design stages of highway PV power generation system projects.
The remainder of this paper is organized as follows:
Section 2 outlines the procedures and critical parameter calculation methods of the proposed PV power generation potential assessment method.
Section 3 presents the determination method of the optimal PV array placement scheme for highway slopes in different directions.
Section 4 provides a case study where the PV power generation potential on the slope of a 1.97 km long highway section in Xi’an City, China, is assessed utilizing the proposed method. Finally,
Section 5 summarizes the primary research contents and the conclusions of this study.
2. Methodology
This study aims to develop a method to estimate the PV power generation potential of slopes in road transport systems. Considering the geometric characteristics and structure composition of highway infrastructure, the technical approach of the potential assessment is proposed and illustrated in
Figure 1. The assessment starts with the segmentation of the highway alignment and a calculation of the available slope area, followed by an estimation of the inclined solar radiation. The factors causing the radiation and energy losses in the PV system are considered. The PV power generation potential of highway slopes can be determined after entering the highway geometric and radiation data and adopting the desirable placement scheme of the PV array.
2.1. Highway Segmentation and Slope Area Calculation
The effective solar radiation received on a highway slope is significantly affected by orientation. A slope facing due south is usually found to have the most exposure to solar radiation. However, the orientation of a highway slope surface changes constantly, as the shape and direction of the highway alignment varies along the road centerline. To facilitate the PV power generation potential evaluation, a highway alignment segmentation method is proposed, and a method for the calculation of the available slope area is established according to the spatial distribution characteristics of highway infrastructure.
2.1.1. Highway Slope Orientation Calculation
Generally, a highway alignment includes two primary types of sections, i.e., a straight-line section and a curve section. For straight-line sections or curves with small intersection angles (the angle between the tangents at the starting point and the ending point), the highway alignment direction can be determined using the coordinates of the starting and ending points. Subsequently, the slope orientation can be characterized by the azimuth of the slope (
γ), which can be calculated according to the alignment direction. The highway alignment distribution and the slope orientation calculation methods are presented in
Figure 2. The direction angle (
δ) of a highway alignment can be calculated using Equation (1):
where
and
are the
x-axis and
y-axis coordinates of the starting point of the
th alignment segment, respectively;
and
are the ending point coordinates of the
th segment or the starting point coordinates of the
)th segment, respectively.
Once the direction angle of the highway segment is obtained, the azimuth of the corresponding slope can be determined based on the relation between the highway alignment direction and the slope orientation, as shown in
Figure 2. The highway subgrade is normally classified into three types, i.e., the fill-type, cut-type, and fill-and-cut-type subgrades, which are presented in
Figure 3. The slopes of the fill-type and cut-type subgrades are usually symmetrical, indicating that the azimuth difference of the slopes on both sides is 180°. The PV power generation potential of a slope is significantly impacted by the type and orientation of the subgrade. Therefore, the slope orientation calculation method of the three kinds of subgrade was investigated to facilitate the potential assessment.
The slope azimuths of the fill-type subgrade in different directions were calculated, and they are presented in
Table 1. For highway segments with the cut-type subgrade, the azimuths of the left and right slopes were found to be the same as those of the right and left slopes of the fill-type subgrade, respectively. Fill-and-cut subgrade slopes are the combination of the previous two types of slopes, and the slope azimuth can be determined accordingly. It should be noted that only the part higher than 5 m of the cut slope is considered for PV installation to reduce the influence of glare and reflection on drivers caused by the PV panels.
2.1.2. Highway Alignment Segmentation
For curve sections of a highway alignment with large intersection angles, alignment segmentation should be conducted to consider the impact of slope orientation variation on the effective solar radiation received on the slope. The curve sections should be divided into segments that can be approximately treated as straight lines, i.e., obtaining small intersection angles. A typical alignment segmentation scheme and slope orientation calculation method are presented in
Figure 4. The highway direction determined by the starting and ending points of the divided segment and the corresponding slope azimuth shown in
Table 1 could be adopted as the representative highway direction and slope azimuth.
However, the number of divided segments will be too large if the intersection angle of each segment is too small. In contrast, the accuracy and reliability of the effective radiation calculation results will be significantly impacted if a curve segment with a large intersection angle is treated as a straight line. Therefore, it is necessary to determine the reasonable threshold of the intersection angle for the alignment segmentation. As the slope orientation is perpendicular to the highway direction, the intersection angle is equal to the change in the slope azimuth angle at the starting point and ending point. To determine the reasonable threshold, the influence of the slope azimuth variation on the power generation ability of the PV modules was analyzed utilizing the regression model between the PV array azimuth and the generated energy developed in the southern region of Slovakia by Bozikova et al. [
24]. The model is demonstrated in Equation (2) and
Figure 5.
It can be observed in
Figure 5 that the energy generation changing rate reaches the maximum value at an azimuth angle of
. Therefore, to evaluate the influence of azimuth variation on PV power generation, the variation ratios of the energy generated by the PV array with azimuth angles close to
were calculated, and they are shown in
Figure 6. To ensure the accuracy and reliability of the power generation potential assessment, the energy generation variation ratio caused by the change in the slope azimuth in the divided segments should be controlled within certain levels based on the project requirements. If the variation ratio control level is set to 3%, the change in the azimuth angle should be less than 5° according to the results shown in
Figure 6; this was selected as the threshold of the intersection angle for the alignment segmentation in this study.
Furthermore, after the threshold of the intersection angle is adopted, the segmentation length for the curve alignment sections can be determined according to Equation (3):
where
is the radius of the circular section in the curve alignment section
m;
is the threshold of the intersection angle, which was adopted as
in this study.
In a typical highway alignment, the curve section is commonly composed of a transition curve and a circular curve. The average curvature of the transition curve is smaller than that of the circular curve, resulting in a larger radius of curvature. Therefore, the segmentation length calculated with the transition curve radius will be larger than that calculated with the circular curve radius. To simplify the alignment segmentation of large-scale highway networks, the r in Equation (3) was conservatively adopted as the radius of the circular curve for the curve section.
2.1.3. Available Slope Area for PV Installation
The length of the slope area available for PV installation can be adopted as the straight-line length or the curve segment length. The width of the available slope area can be determined according to the height and grade of the highway slope. The average of the slope width at the starting point and ending point of the alignment segment was adopted as the representative width of the slope area, shown as follows:
where
is the representative slope width of the
th highway segment;
and
are the slope width at the starting point and ending point of the
th highway segment, respectively, which can be calculated as follows:
where
and
are the slope height and slope grade at the starting point of the
th segment, respectively.
The available slope area for PV installation can be determined based on Equation (6) after the length and width are obtained:
where
is the available slope area of the
th highway segment for PV installation.
2.2. Solar Radiation Estimation on a Tilted Surface
The solar radiation received on a tilted surface is composed of three parts, i.e., the direct solar radiation, the sky-scattered radiation, and the ground-reflected radiation [
25,
26], which is shown as follows:
The direct solar radiation on a tilted surface
can be calculated as follows:
where
[
27] is the direct light enhancement coefficient, which can be calculated as follows:
where
and
are the solar incidence angle and solar elevation angle in degrees, respectively, which can be determined as follows:
where
A is the sun azimuth in degrees;
is the local latitude in degrees; and
can be expressed as follows:
where
is the time zone time in a 24 h clock;
is the model coefficient, which adopts 1 and −1 for the eastern and western hemispheres, respectively;
is the time zone center longitude in degrees;
is the local longitude in degrees; and
[
28] is the sun declination in degrees, which can be determined as follows:
where
is the order of days in a year ranging from 1 to 365.
The amount of scattered radiation on a tilted surface
can be determined based on the Hay model [
29], as shown in Equation (14):
where
is the solar radiation at the outer level of the atmosphere in
, which can be calculated as follows:
where
n,
ω,
φ, and
δ have the same meanings as illustrated above.
The amount of ground-reflected radiation on a tilted surface
[
30] can be determined using Equation (16):
where
is the average reflectivity of the ground, which is generally adopted as 0.15;
,
, and
have the same meanings as clarified above.
Therefore, the unit area solar radiation received on a tilted surface can be determined based on Equations (7)–(16) using geographic location data, such as longitude and latitude; solar radiation data on the horizontal plane, such as and ; and the inclination angle and the azimuth angle of the tilted surface.
2.3. PV Power Generation Potential Assessment
Further analysis in the highway slope PV power generation potential assessment method can be conducted once the available slope area and solar radiation are obtained. However, the radiation loss of the PV modules and the energy loss in the PV array’s distributed microgrid system will significantly affect the PV power generation potential. Hence, related factors are considered in the assessment process and are discussed in this section.
2.3.1. Solar Radiation Received by PV Modules
Ideally, the calculation of the PV module’s received solar radiation mainly considers the azimuth and tilt angles of the module. However, a considerable solar radiation loss will be generated due to occlusion and light transmittance. Therefore, the near shading, far shading, and IAM losses should be accounted for when determining the PV module’s received solar radiation. The impacts of the three loss sources and the quantitative calculation method are demonstrated below.
- (1)
Near shading and Far shading
Near shading and far shading are mainly composed of remote near shading and far shading and close near shading and far shading. Remote occlusion generally considers nearby mountains or other distant but large objects. The solar radiation received by the photovoltaic arrays is reduced to a certain extent due to the huge volume and the relative geographical location to the slope. Close near shading and far shading include two aspects, i.e., the occlusion of the PV panel itself and the surrounding obstacles. To reduce close occlusion, a certain interval between the PV panels and a certain distance from the surrounding obstacles are required for the installation of the PV array system.
In this study, the remote occlusion reduction coefficient Kd was used to quantify the radiation loss caused by the occlusion of remote objects. In a flat terrain area, the remote occlusion effect is low, and Kd can be adopted as 1. In complex terrain or mountainous areas, the remote occlusion effects on the PV modules are complex, and it is advised to determine Kd based on local experience or onsite measurements using radiometers. The close occlusion reduction coefficient Kn was utilized to represent the shading effects of the PV panels and the highway slope. The PV array placement scheme and the cross-section type of the highway subgrade significantly affect the occlusion of PV modules. Therefore, the value of Kn is suggested to be determined by simulating the PV power generation under certain placement schemes in software such as PVsyst7.2.
- (2)
The IAM loss
The IAM loss refers to the process of reducing the actual total solar radiation received due to the reflection and scattering of the solar panel during the process of solar radiation entering the PV panel from the air. The radiation loss can be quantified via natural light reflectivity (
R), which is primarily related to the reflection ability of the optical material, the incidence angle, and the packaging glass material of the PV module. Common calculation models include Fresnel’s law, the ASHRAE model, and the Sandia model. Fresnel’s law [
31,
32] was used in this study, and the formula is as follows:
where
R is the reflectivity of natural light;
is the solar incidence angle in degrees; and
is the reflection angle of the incident light in degrees.
Generally, the sum of transmittance and reflectivity is 1, and the transmittance (
T) will significantly affect the absorption of direct solar radiation on a tilted PV panel (
). Therefore, the effective direct solar radiation (
) received by the PV panel can be determined using Equation (18):
where
T is the transmittance of natural light, which can be calculated as follows:
Accordingly, the effective solar radiation on tilted PV modules can be obtained by utilizing Equation (20):
where
is the effective solar radiation on tilted PV modules;
is the remote occlusion reduction coefficient; and
is the solar radiation received by tilted PV modules considering the IAM loss, which can be determined as follows:
where
is the sky-scattered radiation on a tilted surface;
is the ground-reflected radiation on a tilted surface.
2.3.2. Theoretical Power Generation of PV Module and Actual Power Generation of PV System
After obtaining the effective solar radiation received by an inclined PV module, the theoretical power generation can be determined by considering the photoelectric conversion efficiency of the PV module with the following equation:
where
is the theoretical power generation of tilted PV modules,
;
is the photoelectric conversion efficiency, which is adopted as 0.15 for conventional crystalline silicon photovoltaic modules.
PV array systems with many modules will have a power loss caused by temperature changes in the modules, the power loss in the inverters, and the PV module performance decay. The evaluation method for these factors is discussed and illustrated below.
Firstly, temperature changes in the PV modules will affect the photoelectric conversion efficiency [
33,
34], which can be evaluated using the temperature correction coefficient shown in the following equation:
where
is the temperature correction coefficient;
is the maximum power temperature coefficient of the PV module; and
is the temperature of the PV module.
Secondly, the inverter loss is mainly caused by the energy loss during the operation of the inverter, which is related to the technical parameters and operating conditions of the inverter itself and is evaluated with the inverter loss correction coefficient . For typical inverters with a nominal AC power of 60 , the number of MPPTs of 16, and the inverter capacity ratio is 1.27; according to our calculations in PVsyst, is generally adopted as 0.98.
Thirdly, the power generation ability of PV modules will decrease as the module performance decay accumulates with time, which can be evaluated with the PV module performance decay correction coefficient
. Generally, the average annual power attenuation rate of conventional crystalline silicon photovoltaic modules is in the range of 0.8~0.9%. Combining the above correction factors and the theoretical power generation of PV modules, the actual power generation of the PV system can be obtained with the following equation:
where
is the actual power generation of the PV system,
;
is the inverter loss correction coefficient; and
is the PV module performance decay correction coefficient.
Based on the above analysis, the actual power generation of the PV system can be calculated based on the solar radiation data on the horizontal plane and the placement conditions. The comprehensive formula is as follows:
where all symbols used in the above formula have the same meanings as illustrated above.
2.3.3. Assessment of Total Solar Power Generation Potential
By integrating the above key steps of the solar power generation evaluation, a basic assessment method for the PV power generation potential of highway slopes can be proposed as follows: (1) segment the alignment of highways in the system; (2) calculate the available slope area for the PV array placement of each highway segment; (3) calculate the effective radiation received by the tilted PV arrays on the slopes of each highway segment considering the radiation loss caused by the PV module; (4) calculate the effective power generation of the PV array on the slope of each highway segment considering the energy loss generated in the PV system; and (5) calculate the total solar power generation potential of the highway slope in the transport system.
Therefore, the total solar power generation potential of a highway slope can be determined based on Equation (26) as follows:
where
is the total solar power generation potential on highway slopes,
;
and
are the total solar power generation potential on the left and right highway slopes, respectively,
;
i and
j are the left slope ID and right slope ID of different highway segments, respectively;
is the unit area actual power generation on the slope,
;
is the available slope area of different highway segments,
;
is the solar radiation received by a tilted PV module considering the IAM loss;
is the remote occlusion reduction coefficient;
is the close occlusion reduction coefficient;
is the photoelectric conversion efficiency;
is the temperature correction coefficient;
is the inverter loss correction coefficient; and
is the PV module performance decay correction coefficient.
4. Case Study of PV Power Generation Potential Assessment
- (1)
Collection of geographic and climate information
In this case study, the slope solar power generation potential of a highway in Chang’an District, Xi’an City, China, was calculated. The research site is located near 108.93° E and 34.17° N, and the typical annual horizontal radiation of Xi’an was selected as the horizontal solar radiation data for this example, which is presented in
Table 9.
- (2)
Highway alignment geometric data collection and segmentation
For the convenience of explanation, this paper only took a 1.97 km long section of the expressway as an example to illustrate the calculation method of the solar power generation potential of highway slopes. The horizontal alignment design of the selected highway section is shown in
Figure 14. There are four transition curves and two circular curves in the horizontal alignment. The length of the transition curves, the radius of the circular curves, the stake number, and the coordinates could be obtained from the design documents. The length of each transition curve is 90 m, and the radii of the circular curves are 520 m and 580 m.
Based on the alignment geometric data, highway segmentation can be conducted according to the method presented in
Section 2.1.2. It is a straight line from the starting point to station K0 + 536.97 of this highway section, which was set as the first segment. The first transition curve and circular curve follow after station K0 + 536.97. According to the principle that the intersection angle of the segmented curve should be less than
, the segmentation length was determined to be 50.61 m for the first circular curve. Similarly, the segment length of the second circular curve was calculated as 45.37 m. Accordingly, the selected highway section could be divided into 27 segments, and the geometric data are shown in
Table A2. Furthermore, the highway direction and the slope azimuth angles could be determined based on Equation (1) and
Table 1, which are presented in
Table A2.
- (3)
Calculation of available slope area of the highway segments
Taking the first highway segment as an example, it is necessary to consider the length, the width, and the proportion of the slope that are required for the PV array placement. Since there is a 180 m long retaining wall installed along the left slope of the first segment based on the design document, this part of the slope was considered for solar energy utilization in this study. As the slope widths at the two ends of the first segment are 2.93 m and 15.42 m, the average slope width could be determined to be 10.35 m according to Equation (4). The length of the slope could be calculated as the station number difference between the two ends of the segment, and it was 536.97 m. By subtracting the length of the retaining wall, the effective slope length should be 356.97 m. Accordingly, the available slope area could be calculated based on Equation (5), and it was 3694.64
. Therefore, the available slope area of all segments could be determined, and they are illustrated in
Table A3.
- (4)
The optimal placement scheme and area of the PV array for highway segments
The optimal placement schemes of the highway segments with different slope orientations could be selected based on the recommended schemes presented in
Table 9. Taking the first segment, for instance, the azimuth of the right slope is 23.69° (as shown in
Table A2), which is between 0° and 45°. Therefore, the power generation was simulated with the placement schemes “① + 26°” and “① + 20°”. The simulation results show that the scheme “① + 26°” had a higher power generation, and this was selected as the desirable placement scheme for the right slope of the first segment. Subsequently, the area of the PV array that could be placed on the slope could be determined according to the effective slope area utilization ratio of the corresponding installation scheme shown in
Table 9. Accordingly, the optimal placement scheme and area of the PV array for slopes of different highway segments were determined, and they are documented in
Table A4.
- (5)
The theoretical and actual solar radiation received by per unit PV panel area
The theoretical unit area solar radiation on the tilted PV array surface could be calculated based on the location of the project, the placement scheme of the PV array, and the solar-radiation-related coefficients according to the method illustrated in
Section 2.2. Thereafter, the actual solar radiation received by the PV panel could be obtained by subtracting the near shading, far shading, and IAM losses according to the method presented in
Section 2.3.1. As the selected section of the highway is in the flat terrain area, the remote occlusion effect
Kd was adopted as 1. The close occlusion reduction coefficient
Kn and the transmittance of natural light on the PV modules were determined by simulating the PV power generation under the selected placement schemes in PVsyst7.2. Accordingly, the values of the theoretical and actual solar radiation received by per unit PV panel area on the slopes of different highway segments were calculated, and they are presented in
Table A5.
- (6)
Calculation of the actual power generation of the PV array on highway slopes
The theoretical power generation of the tilted PV modules could be determined according to Equation (13), utilizing the actual unit area solar radiation results shown in
Table A5, and the photoelectric conversion efficiency was adopted as 0.15 in this study. Afterwards, the actual power generation of the PV system could be calculated using Equation (15). As the temperature of the PV module varies with time during the year, the yearly average value of the temperature correction coefficient
was determined by simulating the power generation of the 27 highway segments and calculating the temperature loss in PVsyst7.2. Therefore,
was adopted as 0.95 in this study. The inverter loss correction coefficient
was adopted as 0.98 to represent general application conditions, while the PV module performance decay correction coefficient was not considered since the long-term power generation potential was not the main focus of this case study. Therefore, the theoretical and actual power generation potentials of the PV system on the slopes of the selected highway section could be determined, and they are shown in
Table A6.
- (7)
Assessment of the solar power generation potential of the selected highway section
After a comprehensive analysis and calculations of the case study, the available slope area for the PV array installation, the actual unit area solar radiation received on the tilted PV panels, and the actual unit area power generation of the PV array on the slopes of the 27 highway segments were obtained. Therefore, the actual annual power generation potential of the selected highway section could be further determined according to Equation (17). The assessment results of the solar power generation on the slopes of different highway segments are illustrated in
Table A7, and the overall solar power generation potential of the studied highway section was found to be 3,896,061.68 kWh in total.