Conventional photovoltaic (PV) modules (exclude interdigitated back contact modules) with silicon or gallium arsenide PV cells often have significant inactive module surface area. This results from wafer cutting techniques and metal contacts that reduce the module’s collection area and the resultant power conversion efficiency. A holographic light collector (HLC) combining a low-cost holographic optical element and a diffuser into conventional PV modules is proposed and evaluated to collect the solar illumination over the inactive module area. The angular tolerance and extra annual energy yield (EY) of the HLC are analyzed. It is found that improvements in EY of 4.5%, 4.1%, and 3.8% can be obtained when PV panels are deployed with two-axis tracking systems, single-axis tracking systems, and without tracking systems, respectively. |
1.IntroductionDuring the past several decades, photovoltaic (PV) solar energy conversion has played an increasingly important role as a renewable energy source.^{1} The $\$/{\mathrm{W}}_{\mathrm{PV}}$ costs of PV modules have dropped dramatically, primarily due to improved manufacturing methods and increased solar cell efficiency.^{1}^{,}^{2} It has been reported that individual PV cell efficiencies are approaching 27%,^{3} and the best module power conversion efficiency is about 23%.^{4} However, the $\$/{\mathrm{W}}_{\mathrm{PV}}$ is not expected to decrease hugely due to the maturing wafer manufacturing industry and the small difference between the experimental efficiency and the theoretical efficiency limitation.^{5} Thus in order to increase the energy yield (EY) of a regular PV module, new light collection techniques with low component and manufacturing costs need to be employed.^{6} As efficient, lightweight, and low-cost methods, holographic solar concentration techniques such as holographic lens, planar holographic concentrator, and spectrum splitting have shown significant potential in increasing the EY of PV systems.^{7}^{–}^{16} Many types of PV cells used in modules are not perfectly square in shape.^{1}^{,}^{2} When assembled in modules, this results in a certain percentage of the module area not occupied by active PV cell material and solar illumination that is not collected for electrical conversion. Other factors, such as bus and finger contacts [exclude interdigitated back contact (IBC) cells] and the module package configuration, also contribute to inactive module surface area (IMSA) that does not contribute to PV solar energy conversion. Even the new half-cell modules designed to minimize the space between cells still have an IMSA ratio of $\sim 6\%$. Table 1 shows several commercial solar panels’ specifications with the IMSA ratio varying from 6% (half-cell module) to 11% (old module). The IMSA ratio is defined by $\mathrm{IMSAR}={A}_{\mathrm{HLC}}/{A}_{M}$. ${A}_{\mathrm{HLC}}$ and ${A}_{M}$ are the IMSA area and the whole PV module surface area, respectively. In this paper, a light management technique to capture the solar energy falling on the IMSA is described using a holographic light collector (HLC) consisting of a reflection type volume holographic element combined with a diffuser. The system is analyzed to determine the additional EY in a specific location (Tucson, Arizona) by considering the solar illumination’s varied incident angle at different times and seasons. The results show that 53% of the illumination falling onto the IMSA can be collected and converted into extra electricity when two-axis tracking systems are deployed together with the PV systems. This corresponds to an increase in EY of 4.5% when the IMSA is 8.25% of the entire PV panel surface area. In addition, EY improvements of 4.1% and 3.8% can be realized, respectively, with single-axis tracking and fixed solar arrays. In Sec. 2, the system design aspects, including the geometrical configurations, PV cell spectral responsivity (SR), and HOE properties, are discussed. The power collection efficiency of the HLC is evaluated as a function of Sun angle changes during a day at different seasons, and the resulting improvement in EY is presented in Sec. 3. The results for an experimental HOE are presented in Sec. 4. Section 5 summarizes the performance of the HLC and its potential to increase the power collection efficiency of regular PV systems. Table 1IMSA ratio of several commercial solar panels.
2.System Design2.1.Design ConfigurationSolar illumination falling onto the IMSA can be redirected onto the PV cells either by a transmission or reflection HOE.^{7} An advantage of a reflective type HOE is that it can be encapsulated into existing PV module packages without deploying another cover glass needed by the transmission HOE.^{17} Also, light diffracted from an HOE can be designed to exceed the critical angle of the module’s glass cover (Fig. 1). This effectively extends the distance over which light can be collected and transferred to the module’s PV cell regions. A simplified diagram of the HLC is shown in Fig. 1. The thickness of the solar panel’s encapsulation glass is $H$, the width of the IMSA is $L$, and the refractive index of the glass cover is assumed to be 1.50. Holographic elements have both angular and spectral selectivity; therefore, as the angle and wavelength differ from the design values, the diffraction efficiency will decrease. A tracking system will keep the hologram at the design values resulting in a high collection efficiency. In contrast, a Lambertian diffuser has a relatively low sensitivity to the angle and wavelength variation of the incident solar illumination. Therefore, combining a holographic element with a diffuser can offer advantages for collecting solar illumination. In Fig. 1, the IMSA is covered with an HLC consisting of a reflection HOE constructed with wavelength selectivity matched to the PV cell’s SR and angles and a Lambertian diffuser surface. For this configuration, the solar illumination incident on the HOE surface is partly diffracted into an angle that is larger than the critical angle of the glass cover. The diffuser scatters the remaining light that is not diffracted by the HOE. Some of this scattered light exceeding the cover glass’s critical angle is reflected onto the PV cell surface and converted into electrical power and energy. Multiple interactions of light scattered by the diffuser and diffracted by the hologram that make it to the PV cell surface are also considered in the simulation. The HOE is designed to be symmetric about the center of the IMSA to increase the length of the effective light collection region. The left half of the HOE diffracts light to a PV cell on the left side of the IMSA, and the right half of the HOE diffracts light to a cell on the right. The effective length describing the propagation distance of the diffracted/diffused light in the horizontal direction is given by where ${\theta}_{d}$ is the diffraction angle and $H$ is the thickness of the encapsulation glass. The glass cover functions as a light waveguide to redirect light with angles larger than the glass cover’s critical angle onto the cells. ${n}_{g}$ is the refractive index of the glass. ${\theta}_{\mathrm{CA}}$ is the total internal reflection angle of the cover, which is around 41.8 deg for a glass with a refractive index of 1.50. Equation (1) indicates that the effective light collection area’s length is proportional to the cover glass’s thickness and the sinusoidal value of the redirected light’s angle. For the commercial PV panels shown in Table 1, the shortest effective collection length is 8.53 mm when the thickness of the cover glass is 3.2 mm. This means part of the diffracted light can interact with the HLC a second time when the length of the IMSA is longer than 8.53 mm.2.2.Current Responsivity of Silicon CellsThe SR characteristics vary significantly with different combinations of semiconductor materials such as GaAs, CIGS, and CdTe.^{1}^{,}^{2} To determine the appropriate peak wavelength of the HOE, the specific current responsivity (CR) of the PV cell needs to be evaluated by taking the product of the solar spectrum and the SR of the PV cells. The expression of the CR for a PV cell under the illumination with global standard AM1.5 spectrum is given by In this paper, the monocrystalline silicon cell is used as the target material for the HLC design. The standard AM1.5G spectrum is depicted in Fig. 2(a), and the SR of the silicon cells is shown in Fig. 2(b). The CR of a monocrystalline silicon PV cell is shown in Fig. 2(c) when illuminated with AM1.5G spectrum. It implies that the optimal spectral range for HOE design ranges from 600 to 800 nm. With proper multiplexing, index modulation profile, and thickness, an HOE can be designed to have a high DE with $>300\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{nm}$ of spectral bandwidth. A function for optimizing the spectral bandwidth of the HOE is given by Eq. (4)$$\mathrm{\Gamma}={\int}_{{\lambda}_{\mathrm{min}}}^{{\lambda}_{\mathrm{max}}}\mathrm{CR}(\lambda )\xb7\mathrm{DE}(\lambda )\xb7\mathrm{d}\lambda ,$$To illustrate the change in the hologram’s peak efficiency wavelength as a function of the DE spectral bandwidth, assume that the DE of the hologram has a rectangular characteristic with wavelength. Also assume that the HOE and PV cell are illuminated with an AM1.5G spectrum [Fig. 2(a)], the PV cell is silicon [Fig. 2(b)], and the DE is 100% within the spectral bandwidth, as shown in Fig. 2(c). These factors are then used to compute the optimal $\mathrm{\Gamma}$ as a function of the spectral bandwidth of the hologram and determine the design wavelength. Figure 2(d) shows the optimal design central wavelength of the HOE as the function of the HOE’s spectral bandwidth. The result indicates that the optimal design wavelength for the HOE should be shifted to a shorter wavelength as the spectral bandwidth of the hologram increases. 2.3.HOE DesignThere are two basic steps designing an HOE. The first is to determine the angles and wavelength of the construction and reconstruction conditions using Bragg matching conditions.^{18}^{–}^{21} The expression of the Bragg matching condition is given by Eq. (5)$$\overrightarrow{\mathbf{K}}={\overrightarrow{\mathbf{k}}}_{1,{\lambda}_{1}}-{\overrightarrow{\mathbf{k}}}_{2,{\lambda}_{1}}={\overrightarrow{\mathbf{k}}}_{1,{\lambda}_{2}}-{\overrightarrow{\mathbf{k}}}_{2,{\lambda}_{2}},$$Using the methodology of Sec. 2.2, a reflection hologram with a 200-nm spectral bandwidth will have an optimum $\mathrm{\Gamma}$ with a design wavelength of 600 nm. A diagram of the Bragg condition for constructing a hologram at ${\lambda}_{1}$ and reconstructing it at ${\lambda}_{2}$ inside the holographic material is shown in Fig. 3, where $d$ is the thickness of the HOE. Based on the Bragg matching condition, the grating period in $x$ and $z$ directions can be derived as Eq. (6)$${\mathrm{\Lambda}}_{x}=\frac{\lambda}{2{n}_{h}\text{\hspace{0.17em}}\mathrm{cos}\left(\frac{{\theta}_{2}+{\theta}_{1}}{2}\right)\mathrm{sin}\left(\frac{{\theta}_{2}-{\theta}_{1}}{2}\right)},\phantom{\rule[-0.0ex]{1em}{0.0ex}}{\mathrm{\Lambda}}_{z}=\frac{\lambda}{2{n}_{h}\text{\hspace{0.17em}}\mathrm{sin}\left(\frac{{\theta}_{2}+{\theta}_{1}}{2}\right)\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{sin}\left(\frac{{\theta}_{2}-{\theta}_{1}}{2}\right)},$$For an unslanted reflection HOE, the DE is given by where $\mathrm{\Delta}n$ is the index modulation, and $d$ is the thickness of the HOE. This expression indicates that the DE of a reflection HOE can be increased larger the thickness and index modulation; however, the diffraction efficiency starts to saturate.One method to achieve a large spectral and angular bandwidth of the hologram is to vary the grating period as a function of depth within the hologram.^{15}^{,}^{22} It is possible to achieve this effect in recording materials such as dichromated gelatin.^{15}^{–}^{17}^{,}^{22} Figure 4(a) and 4(b) show the grating profiles in the $x\text{\u2013}z$ plane within the hologram for the reflection hologram case described in Fig. 3. Figure 4(a) shows a uniform index modulation with depth, and Fig. 4(b) has a 20% exponential swelling index profile with hologram depth. The maximum refractive index modulation for both cases is 0.08, and the hologram thickness prior to the swelling process is $20\text{\hspace{0.17em}\hspace{0.17em}}\mu \mathrm{m}$. Figure 5 shows the diffraction efficiency as a function of wavelength and angle for the modulation profiles described in Figs. 4(a) and 4(b). The calculations were performed using rigorous coupled wave analysis, which allows consideration of the varied index modulation profile and the $x\text{\u2013}y$ plane angle evaluations. As shown in Fig. 5(a), the spectral bandwidth of the hologram with swelling increases significantly (over 200 nm) compared to the hologram with uniform refractive index modulation (50 nm) with the same prior-processing hologram thickness. The diffracted beam, in this case, exceeds the critical angle for wavelengths greater than the design wavelength. This allows the light to be guided to the location of PV cells and will increase the power collection efficiency and EY of the module. The coordinates used for describing the incident beam are illustrated in Fig. 5(b). The normalized propagation vector of the incident beam is given by Eq. (8)$$\overrightarrow{k}=[{k}_{x},{k}_{y},{k}_{z}]=[\mathrm{sin}(\theta )\mathrm{cos}(\varphi ),\text{\hspace{0.17em}}\mathrm{sin}(\theta )\mathrm{sin}(\varphi ),\text{\hspace{0.17em}}\mathrm{cos}(\theta )],$$Table 2Parameters of HOE.
3.Energy Yield Evaluation3.1.Incident Solar Illumination AngleThe hologram diffraction efficiency and the EY are highly dependent on the angle of incident solar illumination relative to the normal of the hologram surface. The Sun’s angle relative to a surface normal, in turn, depends on the geographical location, time of the day, and the season of the year. The zenith ${\theta}_{S,\mathrm{ZE}}$ and azimuth ${\phi}_{S,\mathrm{AZ}}$ angles of the Sun can be readily obtained from well-known Sun position algorithms.^{23} Sun position values can be combined with parameters for the geographical location and system deployment method (i.e., dual-axis tracking, single-axis tracking, or fixed angle arrays) to determine the angle of incidence and irradiance at the module surface. To simplify the EY calculation process for evaluating the hologram collection efficiency, the incident solar spectrum is assumed to be the AM1.5G spectrum with a total input irradiance of $1000\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{W}/{\mathrm{m}}^{2}$. The solar angle can be described by the elevation angle (${\theta}_{S,\mathrm{EL}}=90\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{deg}-{\theta}_{S,\mathrm{ZE}}$) and azimuth angle (${\theta}_{S,\mathrm{AZ}}$) that are given by the following equations: Eq. (9)$${\theta}_{S,\mathrm{EL}}({t}_{d},{t}_{h})={\mathrm{sin}}^{-1}\{\mathrm{sin}[\delta ({t}_{d})]\mathrm{sin}(\varphi )+\mathrm{cos}[\delta ({t}_{d})]\mathrm{cos}(\varphi )\mathrm{cos}[\mathrm{HRA}({t}_{h})]\},$$Eq. (10)$${\phi}_{S,\mathrm{AZ}}({t}_{d},{\mathrm{t}}_{h})={\mathrm{cos}}^{-1}\left\{\frac{\mathrm{sin}[\mathrm{cos}(\varphi )]-\mathrm{cos}[\delta ({t}_{d})]\mathrm{sin}\text{\hspace{0.17em}}d(\varphi )\mathrm{cos}[\mathrm{HRA}({t}_{h})]}{\mathrm{cos}({\theta}_{S,\mathrm{EL}})}\right\},$$Eq. (11)$$\mathrm{sin}(\delta )=\mathrm{sin}(-23.45\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{deg})\text{\hspace{0.17em}}\mathrm{cos}[\frac{360}{365}({t}_{d}+10)].$$Eq. (12)$$\mathrm{HRA}({t}_{h})=15\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{deg}[\mathrm{LST}({t}_{h})-12].$$Eq. (13)$${\overrightarrow{\mathbf{k}}}_{\text{solar}}=[\mathrm{cos}({\theta}_{S,\mathrm{EL}})\mathrm{sin}({\phi}_{S,\mathrm{AZ}}),\mathrm{cos}({\theta}_{S,\mathrm{EL}})\mathrm{cos}({\phi}_{S,\mathrm{AZ}}),\mathrm{sin}({\theta}_{S,\mathrm{EL}})].$$Moreover, when the PV module’s surface normal is not perpendicular to the ground surface, in other words, it has a zenith angle and azimuth angle described by (${\theta}_{M,\mathrm{ZE}}$, ${\phi}_{M,\mathrm{AZ}}$), the angle of the solar illumination relative to the module’s surface normal is then given by Eq. (14)$$\gamma ={\mathrm{cos}}^{-1}[\mathrm{cos}({\theta}_{M,\mathrm{EL}})\mathrm{cos}({\theta}_{S,\mathrm{EL}})\mathrm{cos}({\phi}_{M,\mathrm{AZ}}-{\phi}_{S,\mathrm{AZ}})+\mathrm{sin}({\theta}_{M,\mathrm{EL}})\mathrm{sin}({\theta}_{S,\mathrm{EL}})],$$3.2.Performance EvaluationThe HLC consisting of an HOE and a diffuser is in combination of the PV cells shown in Fig. 6. The PV cell has a dimension of ${W}_{\mathrm{PV}}\times {W}_{\mathrm{PV}}$, the reflectivity of the white diffuser is ${R}_{D}$, and the IMSA has a width of $L$. Figure 6(b) shows a single PV module where ${A}_{\mathrm{HLC}}$ and ${A}_{M}$ are the surface areas of the IMSA and PV cells, respectively, and they are given by Eq. (15)$${A}_{M}={({W}_{\mathrm{PV}}+L)}^{2},\phantom{\rule[-0.0ex]{1em}{0.0ex}}{A}_{\mathrm{HLC}}=2\xb7({W}_{\mathrm{PV}}+L)\xb7L-{L}^{2}\text{\hspace{0.17em}\hspace{0.17em}}/2.$$Eq. (16)$${P}_{\text{cell}}({t}_{s})={A}_{M}\xb7{\int}_{{\lambda}_{\mathrm{min}}}^{{\lambda}_{\mathrm{max}}}{E}_{\mathrm{AM}1.5}(\lambda ,{t}_{s})\xb7\mathrm{SR}(\lambda )\xb7\mathrm{FF}\xb7{V}_{\mathrm{OC}}\xb7\mathrm{d}\lambda \phantom{\rule{0ex}{0ex}}={A}_{M}\xb7\mathrm{FF}\xb7{V}_{\mathrm{OC}}\xb7{\int}_{{\lambda}_{\mathrm{min}}}^{{\lambda}_{\mathrm{max}}}{E}_{\mathrm{AM}1.5}(\lambda ,{t}_{s})\xb7\mathrm{SR}(\lambda )\xb7\mathrm{d}\lambda .$$Eq. (17)$${P}_{\mathrm{HLC}}({t}_{i})={A}_{\mathrm{HLC}}\xb7\mathrm{FF}\xb7{V}_{\mathrm{OC}}\xb7{\int}_{{\lambda}_{\mathrm{min}}}^{{\lambda}_{\mathrm{max}}}{E}_{\mathrm{AM}1.5}(\lambda ,{t}_{s})\xb7\mathrm{SR}(\lambda )\xb7\mathrm{OCE}(\lambda ,{t}_{s})\xb7\mathrm{d}\lambda ,$$Eq. (18)$$\mathrm{NCPR}({t}_{s})=\frac{{P}_{\mathrm{HLC}}({t}_{s})}{{P}_{\text{cell}}({t}_{s})}=\frac{{A}_{\mathrm{HLC}}}{{A}_{M}-{A}_{\mathrm{HLC}}}\frac{{\int}_{{\lambda}_{\mathrm{min}}}^{{\lambda}_{\mathrm{max}}}{E}_{\mathrm{AM}1.5}(\lambda ,{t}_{s})\xb7\mathrm{SR}(\lambda )\xb7\mathrm{OCE}(\lambda ,{t}_{s})\xb7\mathrm{d}\lambda}{{\int}_{{\lambda}_{\mathrm{min}}}^{{\lambda}_{\mathrm{max}}}{E}_{\mathrm{AM}1.5}(\lambda ,{t}_{s})\xb7\mathrm{SR}(\lambda )\xb7\mathrm{d}\lambda}.$$Eq. (19)$$\mathrm{AEYI}=\frac{{\mathrm{EY}}_{\mathrm{HLC}}}{{\mathrm{EY}}_{\text{cell}}}=\frac{\sum {P}_{\mathrm{HLC}}({t}_{s})\xb7\mathrm{\Delta}t}{\sum {P}_{\text{cell}}({t}_{s})\xb7\mathrm{\Delta}t}=\frac{\sum {P}_{\mathrm{HLC}}({t}_{s})}{\sum {P}_{\text{cell}}({t}_{s})},$$3.3.Influence of Thickness of the Cover GlassEquation (1) indicates that the effective light collection length $l$ is proportional to the thickness of the encapsulation glass ($H$) (i.e., a thicker cover glass results in a longer collection length). The NCPR performance as a function of the cover glass thickness ($H$) for an HLC consists only a diffuser and one with only an HOE. The illumination considered for this aspect is on the IMSA only. Table 3 gives the other parameters used for calculation. Figure 7(a) illustrated the distribution of the rays absorbed by the PV cells when light is normally incident on the IMSA, and it indicates that most rays are absorbed near the edges of PV cells. Table 3Specifications used for the simulation.
The NCPR for the HOE-only and the diffuser-only cases as a function of the thickness of the cover glass are shown in Fig. 7(b). As shown, NCPR increases for both cases when the cover glass gets thicker. The NCPR of the diffuser-only case is higher than the NCPR of the HOE-only case due to its broader spectral bandwidth; however, the NCPR of the HOE-only case approaches the saturation point much faster than the NCPR of the diffuser-only case resulting from the HOE’s higher angle selectivity. Thus for a solar panel with a thin ($<3.2\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{mm}$) encapsulation glass, the combination of the HOE and diffuser can provide a better light redirecting than the HOE-only or diffuser-only case. Although a higher NCPR is expected when a thicker glass cover is used, the cover glass thickness is chosen to be 3.2 mm since this corresponds to the value for most commercial PV modules (Table 1). 3.4.AEYI for Dual-Axis and Single-Axis Tracking Systems with HLCAccording to Sec. 3.1, the Sun’s angle at a specific location can be calculated using the corresponding latitude and longitude coordinates and the local time and season values. For this example, the coordinates (32.2226° N, 110.9747° W) for Tucson, Arizona, are used. The solar angle is then expressed in the k-space described by ${k}_{x}$ and ${k}_{y}$ given in Eq. (13). The east–west direction corresponds to the ${k}_{x}$ direction and the south–north direction corresponds to the ${k}_{y}$ direction. A dual-axis tracking system can dynamically track the Sun’s position and always ensure ${k}_{x}={k}_{y}=0$ to maintain the highest light collection efficiency. When employed with a dual-axis tracking system, the HLC keeps its highest NCPR (4.5%) at all times and seasons, resulting in an AEYI of 4.5% when the PV module has an IMSAR of 8.25%. This implies that for a system like that described in Table 3 which generates $100\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{kWh}/\text{year}$, an extra $4.5\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{kWh}/\text{year}$ can be achieved when an HLC and a dual-axis-tracking are used. Single-axis tracking systems are less expensive but do not compensate for seasonal changes in the Sun angle. Figure 8 shows the variation in solar angle in Tucson, Arizona, as a function of ${k}_{x}$ and ${k}_{y}$. In this case, with the conditions given in Table 3, the NCPR has a maximum value of 4.5% when ${k}_{x}={k}_{y}=0$ (normal incident), and the corresponding AEYI is 4.1%. This implies that for a system like that described in Table 3 which generates $100\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{kWh}/\text{year}$, an extra $4.1\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{kWh}/\text{year}$ can be achieved when an HLC and single-axis tracking are used. 3.5.AEYI for Fixed Arrays with HLCFinally, considering a fixed array PV system with HLC module parameters as given in Table 3, if it is deployed in Tucson at a tilt angle of 32 deg, the highest NCPR is again 4.5% when the solar illumination is normally incident (${k}_{x}={k}_{y}=0$) and decreases for other Sun angles (shown in Fig. 9). This gives an AEYI of 3.8% and implies an extra $3.8\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{kWh}/\text{year}$ can be attained when an HLC is used with a fixed angle PV module array, compared to the same fixed module array without an HLC that produces $100\text{\hspace{0.17em}\hspace{0.17em}}\mathrm{kWh}/\text{year}$. This AEYI is very close to the diffuser-only case with an NCPR of 3.5% [see Fig. 7(b)] since the holographic element contributes less to the total power collection efficiency while the incident angle deviates from the PV module’s surface normal significantly. Thus a dual-tracking system is needed to make the HLC achieve the highest collection efficiency. The AEYIs of the HLC deployed with fixed arrays, single-axis tracking, and dual-axis tracking systems are summarized in Table 4, where the AEYIs considering the diffuse light that contributes to 20% of the total illumination are also given. Table 4AEYI of the HLC employed with different systems.
4.Experimental ResultsIn order to verify some of the simulation results, experimental reflection holograms were formed in a commercial photopolymer recording material (Covestro HF200). This material has a thickness of $16\text{\hspace{0.17em}\hspace{0.17em}}\mu \mathrm{m}$ and a maximum refractive index modulation of 0.03. Reflection holograms were designed using the method described in Sec. 2.3. The experimental setup is shown in Fig. 10 for forming the hologram with light from a 532-nm laser and maximum diffraction efficiency at normal incidence with a reconstruction wavelength of 600 nm. The reconstruction angles are determined as 0 deg and 135 deg and the corresponding construction angles are 12.5 deg and 122.5 deg, and this results in a maximum diffraction efficiency at 600 nm. The holographic photopolymer is sandwiched between two right-angle prisms used for in- and out-coupling the two construction beams. The spectral diffraction efficiency of the recorded HOE is measured using an Ocean Optics USB 2000 spectrometer and indicates that the peak diffraction efficiency occurs at a wavelength of 600 nm. Figure 11 shows a plot of the measured and theoretical diffraction efficiency as a function of the reconstruction wavelength computed using ACWA. It indicates a shift of the spectra when the angle of incident illumination varies. The comparison has a best-fit refractive index modulation of 0.017. The upwelling of the sidelobes is an indication of the low collimation degree of the broadband testing illumination. In this case, the spectral bandwidth of the HOE is limited to 14 nm resulting from a low-index modulation amplitude, and the corresponding HLC’s AEYI is decreased to 3.7% when this HOE is combined into the HLC and deployed with a PV system specified in Table 3 (with dual-axis tracking). It has been shown that with the proper recording methods and warm processing techniques, the spectral bandwidth of the HOE made in DCG ranges from 10 to 350 nm.^{22} For an HOE formed in dichromated gelatin with the parameters given in Table 2 (with a prior-processing thickness of 20 m, an index modulation of 0.08, and an exponentially swelling coefficient of 0.2), the spectral bandwidth can approach 250 nm [Fig. 5(a)] and provide an AEYI of 4.5% when it is combined into the HLC and PV systems with parameters given in Table 3. 5.ConclusionsIn this paper, an HLC system consisting of a holographic optical element and a diffuser used to capture solar illumination falling onto the IMSA is proposed and analyzed. HLC configurations are formulated in the FRED optical simulation program and used to evaluate the power collection efficiency and AEYI. The annual EY analysis is computed for Tucson, Arizona, with dual-axis and single-axis tracking and a fixed non-tracking PV system. The corresponding improvements to the annual EY for a system with modules that have an IMSA of 8.25% are, respectively, 4.5%, 4.1%, and 3.8% with direct illumination. With direct and diffuse solar illumination, the corresponding AEYIs are, respectively, 4.3%, 4.0%, and 3.6%. Notice that the IMSA ratio of a commercial module might be smaller than the value used in this analysis, resulting in a smaller gain. The IMSA distribution has been assumed to be uniform for simplification purposes, but it is not uniformly distributed for standard modules. Future work will focus on the experimental evaluation of HLCs formed in materials with optimized thickness and refractive index modulation profiles such as dichromated gelatin. AcknowledgmentsThis material is based upon work primarily supported by the National Science Foundation (NSF) and Department of Energy (DOE) funded QESST Engineering Research Center (No. EEC-1041895). Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect those of the NSF or DOE. ReferencesM. A. Woodhouse et al.,
“Crystalline silicon photovoltaic module manufacturing costs and sustainable pricing: 1H 2018 Benchmark and Cost Reduction Road Map,”
Golden, Colorado
(2019). Google Scholar
E. Lorenzo,
“Energy collected and delivered by PV modules,”
Handbook of Photovoltaic Science and Engineering, 906
–930 Wiley(2002). Google Scholar
National Renewable Energy Laboratory, Best Research-Cell Efficiency Chart.,
(2021) https://www.nrel.gov/pv/cell-efficiency.html April ). 2021). Google Scholar
National Renewable Energy Laboratory, Best Research-Cell Efficiency Chart.,
(2021) https://www.nrel.gov/pv/module-efficiency.html April ). 2021). Google Scholar
F. Schindler et al.,
“Towards the efficiency limits of multicrystalline silicon solar cells,”
Solar Energy Mater. Solar Cells, 185 198
–204
(2018). https://doi.org/10.1016/j.solmat.2018.05.006 SOCLD4 0379-6787 Google Scholar
A. Luque, Solar Cells and Optics for Photovoltaic Concentration, 305
–355 Institute of Physics(1989). Google Scholar
J. E. Ludman,
“Holographic solar concentrator,”
Appl. Opt., 21
(17), 3057
–3058
(1982). https://doi.org/10.1364/AO.21.003057 APOPAI 0003-6935 Google Scholar
Y. W. Zhang et al.,
“Photovoltaic concentrator using a holographic optical element,”
Appl. Opt., 27
(16), 3556
–3560
(1988). https://doi.org/10.1364/AO.27.003556 APOPAI 0003-6935 Google Scholar
C. Bainier, C. Hernandez and D. Courjon,
“Solar concentrating systems using holographic lenses,”
Solar Wind Technol., 5 395
–404
(1988). https://doi.org/10.1016/0741-983X(88)90006-9 Google Scholar
J. Ludman and J. Riccobon,
“Holographic solar concentrator for terrestrial photovoltaics,”
in Conf. Rec. of the 1994 IEEE First World Conf. Photovoltaic Energy Convers,
(1994). https://doi.org/10.1109/WCPEC.1994.520181 Google Scholar
R. K. Kostuk, J. Castro and D. Zhang,
“Holographic low concentration ratio solar concentrators,”
in Front. Opt.,
(2009). Google Scholar
D. Zhang et al.,
“Ultra light-trapping filters with broadband reflection holograms,”
Opt. Express, 20
(13), 14260
–14271
(2012). https://doi.org/10.1364/OE.20.014260 OPEXFF 1094-4087 Google Scholar
J. Zhao et al.,
“Improved solar illumination collection using holographic light management techniques,”
Proc. SPIE, 11120 111200L
(2019). https://doi.org/10.1117/12.2529868 PSISDG 0277-786X Google Scholar
A. G. Imenes and D. R. Mills,
“Spectral beam splitting technology for increased conversion efficiency in solar concentrating systems: a review,”
Solar Energy Mater. Solar Cells, 84
(1–4), 19
–69
(2004). https://doi.org/10.1016/j.solmat.2004.01.038 SOCLD4 0379-6787 Google Scholar
J. M. Russo et al.,
“Spectrum splitting metrics and effect of filter characteristics on photovoltaic system performance,”
Opt. Express, 22
(S2), A528
–A541
(2014). https://doi.org/10.1364/OE.22.00A528 OPEXFF 1094-4087 Google Scholar
B. D. Chrysler et al.,
“Spectrum-splitting photovoltaic system using bifacial cells for high energy yield,”
Proc. SPIE, 11121 111210B
(2019). https://doi.org/10.1117/12.2528049 PSISDG 0277-786X Google Scholar
J. Russo et al.,
“Characterization of diffuse anisotropic illumination effects to the output of bifacial and holographic planar concentrating photovoltaic panel configurations,”
in 38th IEEE Photovoltaic Specialists Conf.,
(2012). https://doi.org/10.1109/PVSC.2012.6317842 Google Scholar
C. G. Stojanoff,
“Review of the technology for the manufacturing of large-format DCG holograms for technical applications,”
Proc. SPIE, 3011 267
–278
(1997). https://doi.org/10.1117/12.328538 PSISDG 0277-786X Google Scholar
J. Goodman, Introduction to Fourier Optics, 297
–393 McGraw-Hill(1998). Google Scholar
H. Kogelnik,
“Coupled wave theory for thick hologram gratings,”
Bell Syst. Technol. J., 48 2909
–2947
(1969). https://doi.org/10.1002/j.1538-7305.1969.tb01198.x Google Scholar
M. G. Moharam and T. K. Gaylord,
“Three-dimensional vector coupled-wave analysis of planar-grating diffraction,”
J. Opt. Soc. Am., 73 1105
–1112
(1983). https://doi.org/10.1364/JOSA.73.001105 JOSAAH 0030-3941 Google Scholar
L. Solymar and D. J. Cooke, Volume Holography and Volume Gratings, Academic(1981). Google Scholar
I. Reda and A. Andreas,
“SPA: solar position algorithm,”
(2015). Google Scholar
BiographyJianbo Zhao received his BS degree in physics from Nankai University and his MS degree in optics from James C. Wyant College of Optical Sciences in 2015 and 2018. He is a PhD student at the University of Arizona. He is working on improving solar and AR systems performance by designing volume holographic elements under the supervision of Dr. Raymond K. Kostuk. |