CN104682856A - Spectral solar photovoltaic system - Google Patents
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- 230000003595 spectral effect Effects 0.000 title claims description 23
- 238000006243 chemical reaction Methods 0.000 claims abstract description 46
- 238000001228 spectrum Methods 0.000 claims description 118
- 230000005540 biological transmission Effects 0.000 claims description 29
- 239000000463 material Substances 0.000 claims description 22
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 4
- 229910021417 amorphous silicon Inorganic materials 0.000 claims description 4
- 229910021421 monocrystalline silicon Inorganic materials 0.000 claims description 4
- VTGARNNDLOTBET-UHFFFAOYSA-N gallium antimonide Chemical compound [Sb]#[Ga] VTGARNNDLOTBET-UHFFFAOYSA-N 0.000 claims description 3
- 238000002360 preparation method Methods 0.000 abstract description 17
- 230000003287 optical effect Effects 0.000 abstract description 13
- 238000005516 engineering process Methods 0.000 abstract description 9
- 230000020169 heat generation Effects 0.000 abstract description 4
- 239000010409 thin film Substances 0.000 description 29
- 238000010586 diagram Methods 0.000 description 11
- 238000004088 simulation Methods 0.000 description 6
- 238000000411 transmission spectrum Methods 0.000 description 6
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 4
- 239000010408 film Substances 0.000 description 4
- 239000010410 layer Substances 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 230000005622 photoelectricity Effects 0.000 description 4
- 230000005855 radiation Effects 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 230000028161 membrane depolarization Effects 0.000 description 3
- 238000012986 modification Methods 0.000 description 3
- 230000004048 modification Effects 0.000 description 3
- 238000005457 optimization Methods 0.000 description 3
- 230000010287 polarization Effects 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 3
- 238000009826 distribution Methods 0.000 description 2
- 229910005542 GaSb Inorganic materials 0.000 description 1
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 229910052787 antimony Inorganic materials 0.000 description 1
- WATWJIUSRGPENY-UHFFFAOYSA-N antimony atom Chemical compound [Sb] WATWJIUSRGPENY-UHFFFAOYSA-N 0.000 description 1
- 229910052733 gallium Inorganic materials 0.000 description 1
- 239000011229 interlayer Substances 0.000 description 1
- 230000008092 positive effect Effects 0.000 description 1
- 238000002834 transmittance Methods 0.000 description 1
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02S—GENERATION OF ELECTRIC POWER BY CONVERSION OF INFRARED RADIATION, VISIBLE LIGHT OR ULTRAVIOLET LIGHT, e.g. USING PHOTOVOLTAIC [PV] MODULES
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- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/40—Optical elements or arrangements
- H10F77/42—Optical elements or arrangements directly associated or integrated with photovoltaic cells, e.g. light-reflecting means or light-concentrating means
- H10F77/488—Reflecting light-concentrating means, e.g. parabolic mirrors or concentrators using total internal reflection
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- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
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- Y02E10/50—Photovoltaic [PV] energy
- Y02E10/52—PV systems with concentrators
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Abstract
本发明实施例公开了一种分光谱太阳能光伏系统,包括第一分光单元、第二分光单元、第三分光单元、第一电池组、第二电池组、第三电池组和第四电池组,由于第一电池组、第二电池组、第三电池组和第四电池组为制备工艺较为成熟、对相应波段的光电转换效率高、成本较低的四个不同带隙的单结光伏电池组,取代了制备工艺高、发热严重的叠层光伏电池,结构简单,易于实现,降低了宽谱光伏系统的制备成本,从而提高了宽谱光伏系统的应用范围,同时,光路简单,损耗较低,提高了宽谱光伏系统的光电转换效率。
The embodiment of the present invention discloses a spectrum-splitting solar photovoltaic system, including a first light-splitting unit, a second light-splitting unit, a third light-splitting unit, a first battery group, a second battery group, a third battery group and a fourth battery group, Since the first battery group, the second battery group, the third battery group and the fourth battery group are four single-junction photovoltaic battery groups with different band gaps with relatively mature preparation technology, high photoelectric conversion efficiency for the corresponding wave band, and low cost , instead of the tandem photovoltaic cells with high preparation process and severe heat generation, the structure is simple and easy to realize, which reduces the preparation cost of the broadband photovoltaic system, thus improving the application range of the broadband photovoltaic system. At the same time, the optical path is simple and the loss is low , improving the photoelectric conversion efficiency of broadband photovoltaic systems.
Description
技术领域technical field
本发明涉及光伏领域,尤其涉及一种分光谱太阳能光伏系统。The invention relates to the field of photovoltaics, in particular to a spectrum-split solar photovoltaic system.
背景技术Background technique
太阳能是地球上最丰富的可再生能源,实现对太阳能的高效利用对人类社会未来能源结构调整有着重大的意义。请参考图1,图1是太阳能辐射的光谱能量分布图,如图1所示,太阳能辐射光谱非常宽,地表上接收到的太阳能辐射光谱能量的90%位于280nm-2500nm的宽谱波段范围内。Solar energy is the most abundant renewable energy on the earth, and the realization of efficient utilization of solar energy is of great significance to the future energy structure adjustment of human society. Please refer to Figure 1, Figure 1 is the spectral energy distribution diagram of solar radiation, as shown in Figure 1, the solar radiation spectrum is very wide, and 90% of the solar radiation spectral energy received on the surface is located in the broad spectrum band range of 280nm-2500nm .
为了提高对太阳能能量的利用,人们在单结半导体材料的光伏电池的基础上研发了叠层式多结宽谱光伏系统,请参考图2,图2是现有技术中叠层式多结宽谱光伏系统的示意图,如图2所示,该光伏系统将太阳光谱分成几个连续的波段,用禁带宽度与这些波段有最佳匹配的多个半导体材料做成光伏电池,并按禁带宽度从大到小的顺序从外向里一层层叠合起来。让波长短、强度大的光被最外层的宽隙材料电池利用,波长较长的光能够透射进去让较窄禁带宽度的材料电池利用。这样就可以拓展光伏系统的光谱相应范围,最大限度的将光能转换为电能。In order to improve the utilization of solar energy, people have developed a stacked multi-junction wide-spectrum photovoltaic system on the basis of photovoltaic cells made of single-junction semiconductor materials. Please refer to Figure 2. The schematic diagram of the spectrum photovoltaic system, as shown in Figure 2, the photovoltaic system divides the solar spectrum into several continuous bands, and uses a plurality of semiconductor materials with the best match between the band gap and these bands to make photovoltaic cells, and according to the band gap The order of width from large to small is stacked layer by layer from the outside to the inside. Light with a short wavelength and high intensity is used by the outermost wide-gap material cell, and light with a longer wavelength can be transmitted in to be used by a material cell with a narrower band gap. In this way, the spectral response range of the photovoltaic system can be expanded, and the light energy can be converted into electrical energy to the maximum extent.
但是叠层式多结宽谱光伏系统由于各级器件链接、光能透射与电路连接复杂,产生的损耗很高,并且由于其叠层结构需要采用价格昂贵的高性能光伏材料,还需要考虑各层间电流与晶格结构的匹配问题,布置层数较多时热管理复杂,会导致昂贵的制备成本。However, the stacked multi-junction wide-spectrum photovoltaic system has a high loss due to the complex connection of devices at all levels, light energy transmission and circuit connection, and because its stacked structure needs to use expensive high-performance photovoltaic materials, it is also necessary to consider various The problem of matching the interlayer current and the lattice structure, and the complex thermal management when the number of layers is arranged, will lead to expensive preparation costs.
因此,现有技术中存在叠层式宽谱光伏系统的制备成本高和光电转换效率低的技术问题。Therefore, there are technical problems of high manufacturing cost and low photoelectric conversion efficiency of stacked wide-spectrum photovoltaic systems in the prior art.
发明内容Contents of the invention
本发明实施例通过提供一种分光谱太阳能光伏系统,用以解决现有技术中存在的叠层式宽谱光伏系统的制备成本高和光电转换效率低的技术问题。Embodiments of the present invention provide a split-spectrum solar photovoltaic system to solve the technical problems of high manufacturing cost and low photoelectric conversion efficiency of stacked wide-spectrum photovoltaic systems in the prior art.
本发明实施例提供了一种分光谱太阳能光伏系统,包括:An embodiment of the present invention provides a split-spectrum solar photovoltaic system, including:
第一分光单元,具有第一透射端与第一反射端,所述第一分光单元能够将入射的太阳能宽光谱分为反射的第一波段光谱与透射的第二波段光谱;The first light-splitting unit has a first transmission end and a first reflection end, and the first light-splitting unit can divide the incident solar broad spectrum into a reflected first band spectrum and a transmitted second band spectrum;
第二分光单元,设置于所述第一反射端,所述第二分光单元具有第二透射端与第二反射端,所述第二分光单元能够将所述第一波段光谱分为反射的第一子波段光谱与透射的第二子波段光谱;The second light splitting unit is arranged at the first reflection end, the second light splitting unit has a second transmission end and a second reflection end, and the second light splitting unit can split the first band spectrum into reflected second light splitting units. A sub-band spectrum and a transmitted second sub-band spectrum;
第三分光单元,设置于所述第一透射端,所述第三分光单元具有第三透射端与第三反射端,所述第三分光单元能够将所述第二波段光谱分为反射的第三子波段光谱与投射的第四子波段光谱;The third light-splitting unit is arranged at the first transmission end, the third light-splitting unit has a third transmission end and a third reflection end, and the third light-splitting unit can divide the second band spectrum into reflected first The third sub-band spectrum and the projected fourth sub-band spectrum;
第一电池组,设置于所述第二反射端,用于将所述第一子波段光谱的太阳能转换为电能,所述第一电池组的材料对所述第一子波段光谱的太阳能的光电转换效率超过第一预设值;The first battery group is arranged at the second reflective end, and is used to convert the solar energy of the first sub-band spectrum into electrical energy, and the material of the first battery group is suitable for the photoelectricity of the solar energy of the first sub-band spectrum. The conversion efficiency exceeds the first preset value;
第二电池组,设置于所述第二透射端,用于将所述第二子波段光谱的太阳能转换为电能,所述第二电池组的材料对所述第二子波段光谱的太阳能的光电转换效率超过第二预设值;The second battery group is arranged at the second transmission end, and is used to convert the solar energy of the second sub-band spectrum into electric energy, and the material of the second battery group is suitable for the photoelectricity of the solar energy of the second sub-band spectrum. the conversion efficiency exceeds the second preset value;
第三电池组,设置于所述第三反射端,用于将所述第三子波段光谱的太阳能转换为电能,所述第三电池组的材料对所述第三子波段光谱的太阳能的光电转换效率超过第三预设值;The third battery group is arranged at the third reflective end, and is used to convert the solar energy of the third sub-band spectrum into electric energy, and the material of the third battery group is suitable for the photoelectricity of the solar energy of the third sub-band spectrum. the conversion efficiency exceeds the third preset value;
第四电池组,设置于所述第三透射端,用于将所述第四子波段光谱的太阳能转换为电能,所述第四电池组的材料对所述第四子波段光谱的太阳能的光电转换效率超过第四预设值;The fourth battery group is arranged at the third transmission end, and is used to convert the solar energy of the fourth sub-band spectrum into electric energy, and the material of the fourth battery group has a positive effect on the photoelectricity of the solar energy of the fourth sub-band spectrum. the conversion efficiency exceeds the fourth preset value;
其中,所述第一电池组、第二电池组、第三电池组和第四电池组为单结电池组。Wherein, the first battery pack, the second battery pack, the third battery pack and the fourth battery pack are single-junction battery packs.
可选地,所述第一分光单元具体为第一长波通薄膜干涉截止滤光片,所述第一波段光谱为短波段350nm-800nm光谱,所述第二波段光谱为850nm-2000nm光谱。Optionally, the first light-splitting unit is specifically a first long-pass thin-film interference cut-off filter, the first band spectrum is a short-band spectrum of 350nm-800nm, and the second band spectrum is a spectrum of 850nm-2000nm.
可选地,所述第一长波通薄膜干涉截止滤光片与入射的太阳光的光路呈45°倾斜放置。Optionally, the first long-wave pass thin-film interference cut-off filter is placed at an angle of 45° to the optical path of the incident sunlight.
可选地,所述第二分光单元具体为第二长波通薄膜干涉截止滤光片,所述第一子波段光谱为350nm-500nm光谱,所述第二子波段光谱为500nm-800nm光谱。Optionally, the second light splitting unit is specifically a second long-wave pass thin-film interference cut-off filter, the first sub-band spectrum is a 350nm-500nm spectrum, and the second sub-band spectrum is a 500nm-800nm spectrum.
可选地,所述第一电池组为非晶硅光伏电池组,所述第二电池组为砷化镓光伏电池组。Optionally, the first battery group is an amorphous silicon photovoltaic battery group, and the second battery group is a gallium arsenide photovoltaic battery group.
可选地,所述第二长波通薄膜干涉截止滤光片与所述第一长波通薄膜干涉截止滤光片反射的太阳光的光路呈45°倾斜放置。Optionally, the optical path of the sunlight reflected by the second long-wave pass thin-film interference cut-off filter and the first long-wave pass thin-film interference cut-off filter is placed at an angle of 45°.
可选地,所述第三分光单元具体为第三长波通薄膜干涉截止滤光片,所述第三子波段光谱为850nm-1100nm光谱,第四子波段光谱为1200nm-2000nm。Optionally, the third light splitting unit is specifically a third long-wave pass thin-film interference cut-off filter, the third sub-band spectrum is 850nm-1100nm spectrum, and the fourth sub-band spectrum is 1200nm-2000nm.
可选地,所述第三电池组具体为单晶硅光伏电池组,所述第四电池组具体为锑化镓光伏电池组。Optionally, the third cell group is specifically a monocrystalline silicon photovoltaic cell group, and the fourth cell group is specifically a gallium antimonide photovoltaic cell group.
可选地,所述第三长波通薄膜干涉截止滤光片与所述第一长波通薄膜干涉截止滤光片透射的太阳光的光路呈45°倾斜放置。Optionally, the third long-wave pass thin-film interference cut-off filter is placed at an angle of 45° to the light path of sunlight transmitted by the first long-wave pass thin-film interference cut-off filter.
本发明实施例中提供的一个或多个技术方案,至少具有如下技术效果或优点:One or more technical solutions provided in the embodiments of the present invention have at least the following technical effects or advantages:
1、由于采用了制备工艺较为成熟、对相应波段的光电转换效率高、成本较低的四个不同带隙的单结光伏电池组,取代了制备工艺高、发热严重的叠层光伏电池,结构简单,易于实现,降低了宽谱光伏系统的制备成本,从而提高了宽谱光伏系统的应用范围,同时,光路简单,损耗较低,提高了宽谱光伏系统的光电转换效率。1. Due to the use of four single-junction photovoltaic cell groups with different band gaps with relatively mature preparation technology, high photoelectric conversion efficiency for the corresponding wave band, and low cost, it replaces the stacked photovoltaic cells with high preparation technology and serious heat generation. It is simple and easy to realize, and reduces the preparation cost of the broadband photovoltaic system, thus improving the application range of the broadband photovoltaic system. At the same time, the optical path is simple and the loss is low, and the photoelectric conversion efficiency of the broadband photovoltaic system is improved.
2、由于整个光电转换过程不需要利用制备工艺复杂的叠层光伏电池,结构简单,易于实现,同时整个光伏系统的光路简单,并且太阳能宽光谱占据90%以上能量的350nm-2000nm中每个波段均能够由对应的光电转换效率高的光伏电池组进行转换,对太阳能进行光电转换的光谱范围广,光电转换的利用率高。2. Since the entire photoelectric conversion process does not require the use of laminated photovoltaic cells with complex preparation processes, the structure is simple and easy to implement. At the same time, the optical path of the entire photovoltaic system is simple, and the wide spectrum of solar energy occupies more than 90% of the energy in each band of 350nm-2000nm All of them can be converted by the corresponding photovoltaic cells with high photoelectric conversion efficiency, and the photoelectric conversion of solar energy has a wide spectral range, and the utilization rate of photoelectric conversion is high.
附图说明Description of drawings
图1为太阳能辐射的光谱能量分布图;Fig. 1 is the spectral energy distribution diagram of solar radiation;
图2为现有技术中叠层式多结宽谱光伏系统的示意图;2 is a schematic diagram of a stacked multi-junction broadband photovoltaic system in the prior art;
图3为本发明实施例提供的分光谱太阳能光伏系统的示意图;3 is a schematic diagram of a split-spectrum solar photovoltaic system provided by an embodiment of the present invention;
图4为本发明实施例提供的分光谱太阳能光伏系统的实例图;Figure 4 is an example diagram of a split-spectrum solar photovoltaic system provided by an embodiment of the present invention;
图5A为本发明实施例提供的第一长波通薄膜干涉截止滤光片透射光谱的仿真结果示意图;5A is a schematic diagram of the simulation results of the transmission spectrum of the first long-wave pass thin-film interference cut-off filter provided by the embodiment of the present invention;
图5B为本发明实施例提供的第二长波通薄膜干涉截止滤光片透射光谱的仿真结果示意图;5B is a schematic diagram of the simulation results of the transmission spectrum of the second long-wave pass thin-film interference cut-off filter provided by the embodiment of the present invention;
图5C为本发明实施例提供的第三长波通薄膜干涉截止滤光片透射光谱的仿真结果示意图。FIG. 5C is a schematic diagram of simulation results of the transmission spectrum of the third long-wave pass thin-film interference cut-off filter provided by the embodiment of the present invention.
具体实施方式Detailed ways
本发明实施例通过提供一种分光谱太阳能光伏系统,用以解决现有技术中存在的叠层式宽谱光伏系统的制备成本高和光电转换效率低的技术问题。Embodiments of the present invention provide a split-spectrum solar photovoltaic system to solve the technical problems of high manufacturing cost and low photoelectric conversion efficiency of stacked wide-spectrum photovoltaic systems in the prior art.
请参考图3,图3为本发明实施例提供的一种分光谱太阳能光伏系统的示意图,如图3所示,该分光谱太阳能光伏系统包括:Please refer to FIG. 3. FIG. 3 is a schematic diagram of a split-spectrum solar photovoltaic system provided by an embodiment of the present invention. As shown in FIG. 3, the split-spectrum solar photovoltaic system includes:
第一分光单元,具有第一透射端与第一反射端,第一分光单元能够将入射的太阳能宽光谱分为反射的第一波段光谱与透射的第二波段光谱;The first light-splitting unit has a first transmission end and a first reflection end, and the first light-splitting unit can divide the incident solar broad spectrum into a reflected first band spectrum and a transmitted second band spectrum;
第二分光单元,设置于第一反射端,第二分光单元具有第二透射端与第二反射端,第二分光单元能够将第一波段光谱分为反射的第一子波段光谱与透射的第二子波段光谱;The second light-splitting unit is arranged at the first reflection end, the second light-splitting unit has a second transmission end and a second reflection end, and the second light-splitting unit can divide the first band spectrum into a reflected first sub-band spectrum and a transmitted first sub-band spectrum Two sub-band spectra;
第三分光单元,设置于第一透射端,第三分光单元具有第三透射端与第三反射端,第三分光单元能够将第二波段光谱分为反射的第三子波段光谱与投射的第四子波段光谱;The third light-splitting unit is arranged at the first transmission end, the third light-splitting unit has a third transmission end and a third reflection end, and the third light-splitting unit can divide the second band spectrum into a reflected third sub-band spectrum and a projected third sub-band spectrum Four sub-band spectra;
第一电池组,设置于第二反射端,用于将第一子波段光谱的太阳能转换为电能,在实际应用中,为保证光电转换效率,可以将第一电池组的材料设置为对第一子波段光谱的太阳能的光电转换效率超过第一预设值的材料,当然,第一预设值可以根据实际情况进行具体设置,例如为20%等等,以满足实际情况的需要,在此不做限制;The first battery group is arranged at the second reflective end, and is used to convert the solar energy of the first sub-band spectrum into electric energy. In practical applications, in order to ensure the photoelectric conversion efficiency, the material of the first battery group can be set to the Materials whose photoelectric conversion efficiency of solar energy in the sub-band spectrum exceeds the first preset value. Of course, the first preset value can be specifically set according to the actual situation, such as 20%, etc., to meet the needs of the actual situation. make restrictions;
第二电池组,设置于第二透射端,用于将第二子波段光谱的太阳能转换为电能,在实际应用中,为保证光电转换效率,可以将第二电池组的材料设置为对第二子波段光谱的太阳能的光电转换效率超过第二预设值的材料,当然,第二预设值可以根据实际情况进行具体设置,例如为20%等等,以满足实际情况的需要,在此不做限制;The second battery group is arranged at the second transmission end, and is used to convert the solar energy of the second sub-band spectrum into electric energy. In practical applications, in order to ensure the photoelectric conversion efficiency, the material of the second battery group can be set to the second Materials whose photoelectric conversion efficiency of solar energy in the sub-band spectrum exceeds the second preset value. Of course, the second preset value can be specifically set according to the actual situation, such as 20%, etc., to meet the needs of the actual situation. make restrictions;
第三电池组,设置于第三反射端,用于将第三子波段光谱的太阳能转换为电能,在实际应用中,为保证光电转换效率,可以将第三电池组的材料设置为对第三子波段光谱的太阳能的光电转换效率超过第三预设值的材料,当然,第三预设值可以根据实际情况进行具体设置,例如为20%等等,以满足实际情况的需要,在此不做限制;The third battery group is arranged at the third reflective end, and is used to convert the solar energy of the third sub-band spectrum into electric energy. In practical applications, in order to ensure the photoelectric conversion efficiency, the material of the third battery group can be set to the Materials whose photoelectric conversion efficiency of solar energy in the sub-band spectrum exceeds the third preset value. Of course, the third preset value can be specifically set according to the actual situation, such as 20%, etc., to meet the needs of the actual situation. make restrictions;
第四电池组,设置于第三透射端,用于将第四子波段光谱的太阳能转换为电能,在实际应用中,为保证光电转换效率,可以将第四电池组的材料设置为对第四子波段光谱的太阳能的光电转换效率超过第四预设值的材料,当然,第四预设值可以根据实际情况进行具体设置,例如为20%等等,以满足实际情况的需要,在此不做限制;The fourth battery group is arranged at the third transmission end, and is used to convert the solar energy of the fourth sub-band spectrum into electric energy. In practical applications, in order to ensure the photoelectric conversion efficiency, the material of the fourth battery group can be set to the fourth Materials whose photoelectric conversion efficiency of solar energy in the sub-band spectrum exceeds the fourth preset value. Of course, the fourth preset value can be specifically set according to the actual situation, such as 20%, etc., to meet the needs of the actual situation. make restrictions;
其中,第一电池组、第二电池组、第三电池组和第四电池组均为制备工艺较为成熟、对相应波段的光电转换效率高、成本较低的单结电池组。Among them, the first battery group, the second battery group, the third battery group and the fourth battery group are all single-junction battery groups with relatively mature preparation technology, high photoelectric conversion efficiency for corresponding wavelength bands, and low cost.
通过上述部分可以看出,由于采用了制备工艺较为成熟、对相应波段的光电转换效率高、成本较低的四个不同带隙的单结光伏电池组,取代了制备工艺高、发热严重的叠层光伏电池,结构简单,易于实现,降低了宽谱光伏系统的制备成本,从而提高了宽谱光伏系统的应用范围,同时,光路简单,损耗较低,提高了宽谱光伏系统的光电转换效率。It can be seen from the above part that due to the use of four single-junction photovoltaic cell groups with different band gaps, which have relatively mature preparation technology, high photoelectric conversion efficiency for the corresponding wave band, and low cost, it has replaced the stacked solar cells with high preparation technology and serious heat generation. The multi-layer photovoltaic cell has a simple structure and is easy to realize, which reduces the preparation cost of the broadband photovoltaic system, thus improving the application range of the broadband photovoltaic system. At the same time, the optical path is simple and the loss is low, which improves the photoelectric conversion efficiency of the broadband photovoltaic system .
请继续参考图4,图4是本发明实施例提供的分光谱太阳能光伏系统的实例图,在接下来的部分中,如图4所示,将以第一分光单元具体为第一长波通薄膜干涉截止滤光片、第二分光单元具体为第二长波通薄膜干涉截止滤光片、第三分光单元具体为第一长波通薄膜干涉截止滤光片为例,来进行详细的举例描述。当然,在其他实施例中,本领域所属的技术人员能够根据实际情况,将分光单元采用其他合适的装置或者部件,例如透镜或者多个透镜的组合等等,以实现本实施例中长波通薄膜干涉截止滤光片的功能,在此就不再赘述了。Please continue to refer to Figure 4, Figure 4 is an example diagram of the split-spectrum solar photovoltaic system provided by the embodiment of the present invention, in the next part, as shown in Figure 4, the first light-splitting unit will be specifically referred to as the first long-wave pass film The interference cut-off filter, the second light-splitting unit being specifically the second long-wave pass thin-film interference cut-off filter, and the third light-splitting unit being specifically the first long-wave pass thin-film interference cut-off filter are taken as examples for detailed description. Of course, in other embodiments, those skilled in the art can use other suitable devices or components for the light splitting unit according to the actual situation, such as a lens or a combination of multiple lenses, etc., so as to realize the long-wave pass film in this embodiment. The function of the interference cut-off filter will not be repeated here.
在本实施例中,由于所需利用的太阳能光谱范围较宽,因此对于长波段的分光谱需要对截止滤光片进行多级基本膜系级联,以拓展高反射区域和达到高截止度的光谱。同时本系统拟采用分光路结构将截止滤光片组分光谱后的窄谱段聚焦到对应波段的光伏电池上,因此在光路设计上要求这些不同膜系结构的截止滤光片处于45°倾斜入射状态。而在大角度倾斜入射的情况下,薄膜滤光片的光谱特性会受到偏振效应的影响,截止边带会向短波方向移动,S偏振分量的反射带会展宽,P偏振分量的反射带会减小。由此会导致滤光片在透射带出现透射率下降,反射带出现反射次峰,边带截止度降低。同时选用的不同半导体材料的相邻吸收波段之间的间隔很窄小于50nm,对设计的干涉截止滤光片在大角度倾斜入射时的光谱特性要求较高,应具有良好的截止边带特性。In this embodiment, due to the wide range of solar energy spectrum to be utilized, it is necessary to cascade the cut-off filter with multi-level basic film systems to expand the high reflection area and achieve high cut-off for the long-wavelength spectrum. spectrum. At the same time, this system intends to use the split light path structure to focus the narrow spectrum of the cut-off filter components on the photovoltaic cells of the corresponding band, so the cut-off filters of these different film structures are required to be at a 45° tilt incident state. In the case of oblique incidence at a large angle, the spectral characteristics of the thin-film filter will be affected by the polarization effect, the cut-off sideband will move to the short-wave direction, the reflection band of the S polarization component will widen, and the reflection band of the P polarization component will decrease. Small. This will lead to a decrease in the transmittance of the filter in the transmission band, a reflection sub-peak in the reflection band, and a decrease in the sideband cut-off. At the same time, the interval between adjacent absorption bands of different semiconductor materials is very narrow and less than 50nm. The spectral characteristics of the designed interference cut-off filter are high when it is obliquely incident at a large angle, and it should have good cut-off sideband characteristics.
对于第一长波通薄膜干涉截止滤光片,经过消偏振优化设计后,其在45°倾斜入射时的分光谱范围为:850nm-2000nm为高透射区,350nm-800nm为高反射区。截止边带小于50nm。其透射光谱的仿真结果如图5A所示。For the first long-wave pass thin-film interference cut-off filter, after depolarization optimization design, its spectral range at 45° oblique incidence is: 850nm-2000nm is a high transmission area, and 350nm-800nm is a high reflection area. The cut-off sideband is less than 50nm. The simulation result of its transmission spectrum is shown in Fig. 5A.
对于第二长波通薄膜干涉截止滤光片,经过消偏振优化设计后,其在45°倾斜入射时的分光谱范围为:550nm-800nm为高透射区,350nm-500nm为高反射区,截止边带小于50nm。其透射光谱的仿真结果如图5B所示。For the second long-wave pass thin-film interference cut-off filter, after depolarization optimization design, its spectral range at 45° oblique incidence is: 550nm-800nm is the high transmission area, 350nm-500nm is the high reflection area, and the cut-off edge The band is less than 50nm. The simulation results of its transmission spectrum are shown in Fig. 5B.
对于第三长波通薄膜干涉截止滤光片,经过消偏振优化设计后,其在45°倾斜入射时的分光谱范围为:1200nm-2000nm为高透射区,850nm-1100nm为高反射区,截止边带小于100nm。其透射光谱的仿真结果如图5C所示。For the third long-wave pass thin-film interference cut-off filter, after depolarization optimization design, its spectral range at 45° oblique incidence is: 1200nm-2000nm is the high transmission area, 850nm-1100nm is the high reflection area, and the cut-off edge The band is less than 100nm. The simulation result of its transmission spectrum is shown in Fig. 5C.
如图4所示,第一长波通薄膜干涉截止滤光片401401与入射的太阳光的光路呈45°倾斜放置,从而能够将入射的太阳能宽光谱分为反射的第一波段光谱与透射的第二波段光谱,其中,第一波段光谱为短波段350nm-800nm光谱,第二波段光谱为850nm-2000nm光谱。需要说明的是,在其他实施例中,第一波段光谱与第二波段光谱的划分可以为其他段,如第一波段光谱可以为350nm-1200nm,第二波段光谱可以为1200-2000nm等等,在此不做限制,当然,若第一波段光谱和第二波段光谱的范围均发生变化,则后续的第二分光单元、第三分光单元和对应的电池组也需要进行相应的调整,以尽量提高分光谱太阳能光伏系统的光电转换效率,在此就不再赘述了了。As shown in Figure 4, the first long-wave pass thin-film interference cut-off filter 401401 is placed at an angle of 45° to the optical path of the incident sunlight, so that the wide spectrum of the incident solar energy can be divided into the reflected first band spectrum and the transmitted second band spectrum. Two-band spectrum, wherein, the first-band spectrum is a short-wavelength 350nm-800nm spectrum, and the second-band spectrum is a 850nm-2000nm spectrum. It should be noted that, in other embodiments, the spectrum of the first band and the spectrum of the second band can be divided into other segments, such as the spectrum of the first band can be 350nm-1200nm, the spectrum of the second band can be 1200-2000nm, etc. There is no limitation here. Of course, if the ranges of the first band spectrum and the second band spectrum are changed, the subsequent second light splitting unit, third light splitting unit and corresponding battery packs also need to be adjusted accordingly to try to Improving the photoelectric conversion efficiency of the split-spectrum solar photovoltaic system will not be repeated here.
请继续参考图4,第二长波通薄膜干涉截止滤光片402与第一长波通薄膜干涉截止滤光片401反射的太阳光的光路呈45°倾斜放置,第一子波段光谱为350nm-500nm光谱,第二子波段光谱为500nm-800nm光谱。Please continue to refer to FIG. 4, the optical path of the sunlight reflected by the second long-wave pass thin-film interference cut-off filter 402 and the first long-wave pass thin-film interference cut-off filter 401 is placed at a 45° inclination, and the first sub-band spectrum is 350nm-500nm Spectrum, the second sub-band spectrum is 500nm-800nm spectrum.
在本实施例中,第一电池组为对350nm-500nm波段的光电转换效率高的非晶硅光伏电池组404,第二电池组为对550nm-800nm波段的光电转换效率高的砷化镓(GaAs)光伏电池组405。In this embodiment, the first battery pack is an amorphous silicon photovoltaic battery pack 404 with high photoelectric conversion efficiency in the 350nm-500nm band, and the second battery pack is gallium arsenide (GaAs) with high photoelectric conversion efficiency in the 550nm-800nm band. GaAs) photovoltaic cells 405.
请继续参考图4,第三长波通薄膜干涉截止滤光片403与第一长波通薄膜干涉截止滤光片401透射的太阳光的光路呈45°倾斜放置,第三子波段光谱为850nm-1100nm光谱,第四子波段光谱为1200nm-2000nm。Please continue to refer to FIG. 4, the optical path of the sunlight transmitted by the third long-wave pass thin-film interference cut-off filter 403 and the first long-wave pass thin-film interference cut-off filter 401 is placed at an angle of 45°, and the third sub-band spectrum is 850nm-1100nm Spectrum, the fourth sub-band spectrum is 1200nm-2000nm.
在本实施例中,第三电池组具体为对850nm-1100nm波段的光电转换效率高的单晶硅光伏电池组406,第四电池组具体为对1200nm-1800nm波段的光电转换效率高的锑化镓(GaSb)光伏电池组407。In this embodiment, the third battery pack is specifically a monocrystalline silicon photovoltaic battery pack 406 with high photoelectric conversion efficiency in the 850nm-1100nm band, and the fourth battery pack is specifically an antimony photovoltaic battery pack 406 with high photoelectric conversion efficiency in the 1200nm-1800nm band. Gallium (GaSb) photovoltaic cells 407 .
可以上述实施例看出,当外部入射的宽光谱太阳光(350nm-2000nm)照射到与输入光路呈45°倾斜放置的第一长波通薄膜干涉截止滤光片时,第一长波通薄膜干涉截止滤光片将350nm-800nm的短波段光谱经由反射端输出到第二长波通薄膜干涉截止滤光片,同时第一长波通薄膜干涉截止滤光片将850nm-2000nm的长波段光谱经由透射端输出到第三长波通薄膜干涉截止滤光片;第二长波通薄膜干涉截止滤光片将入射的350nm-800nm波段分成350nm-500nm的反射波段和550nm-800nm的透射波段分别聚焦到非晶硅光伏电池组和砷化镓光伏电池组上;第三长波通薄膜干涉截止滤光片将入射的850nm-2000nm波段分成850nm-1100nm的反射波段和1200nm-2000nm的透射波段,分别聚焦到单晶硅光伏电池组和锑化镓光伏电池组上。整个光电转换过程不需要利用制备工艺复杂的叠层光伏电池,结构简单,易于实现,同时整个光伏系统的光路简单,并且太阳能宽光谱占据90%以上能量的350nm-2000nm中每个波段均能够由对应的光电转换效率高的光伏电池组进行转换,对太阳能进行光电转换的光谱范围广,光电转换的利用率高。It can be seen from the foregoing embodiments that when the external incident broad-spectrum sunlight (350nm-2000nm) irradiates the first long-wave pass thin-film interference cut-off filter placed at an angle of 45° to the input optical path, the first long-wave pass thin-film interference cut-off filter The filter outputs the short-band spectrum of 350nm-800nm to the second long-wave pass thin-film interference cut-off filter through the reflection end, and the first long-wave pass thin-film interference cut-off filter outputs the long-wave band spectrum of 850nm-2000nm through the transmission end to the third long-wave pass thin-film interference cut-off filter; the second long-wave pass thin-film interference cut-off filter divides the incident 350nm-800nm waveband into a reflection waveband of 350nm-500nm and a transmission waveband of 550nm-800nm to focus on the amorphous silicon photovoltaic On the battery pack and gallium arsenide photovoltaic cell pack; the third long-wave pass thin-film interference cut-off filter divides the incident 850nm-2000nm band into a reflection band of 850nm-1100nm and a transmission band of 1200nm-2000nm, which are respectively focused on the monocrystalline silicon photovoltaic battery pack and gallium antimonide photovoltaic cell pack. The entire photoelectric conversion process does not require the use of stacked photovoltaic cells with complex preparation processes. The structure is simple and easy to implement. At the same time, the optical path of the entire photovoltaic system is simple, and each band in the 350nm-2000nm, which occupies more than 90% of the energy of the solar broad spectrum, can be controlled by Corresponding photovoltaic cells with high photoelectric conversion efficiency are used for conversion, and the photoelectric conversion of solar energy has a wide spectral range, and the utilization rate of photoelectric conversion is high.
本发明实施例中提供的一个或多个技术方案,至少具有如下技术效果或优点:One or more technical solutions provided in the embodiments of the present invention have at least the following technical effects or advantages:
1、由于采用了制备工艺较为成熟、对相应波段的光电转换效率高、成本较低的四个不同带隙的单结光伏电池组,取代了制备工艺高、发热严重的叠层光伏电池,结构简单,易于实现,降低了宽谱光伏系统的制备成本,从而提高了宽谱光伏系统的应用范围,同时,光路简单,损耗较低,提高了宽谱光伏系统的光电转换效率。1. Due to the use of four single-junction photovoltaic cell groups with different band gaps with relatively mature preparation technology, high photoelectric conversion efficiency for the corresponding wave band, and low cost, it replaces the stacked photovoltaic cells with high preparation technology and serious heat generation. It is simple and easy to realize, and reduces the preparation cost of the broadband photovoltaic system, thus improving the application range of the broadband photovoltaic system. At the same time, the optical path is simple and the loss is low, and the photoelectric conversion efficiency of the broadband photovoltaic system is improved.
2、由于整个光电转换过程不需要利用制备工艺复杂的叠层光伏电池,结构简单,易于实现,同时整个光伏系统的光路简单,并且太阳能宽光谱占据90%以上能量的350nm-2000nm中每个波段均能够由对应的光电转换效率高的光伏电池组进行转换,对太阳能进行光电转换的光谱范围广,光电转换的利用率高。2. Since the entire photoelectric conversion process does not require the use of laminated photovoltaic cells with complex preparation processes, the structure is simple and easy to implement. At the same time, the optical path of the entire photovoltaic system is simple, and the wide spectrum of solar energy occupies more than 90% of the energy in each band of 350nm-2000nm All of them can be converted by the corresponding photovoltaic cells with high photoelectric conversion efficiency, and the photoelectric conversion of solar energy has a wide spectral range, and the utilization rate of photoelectric conversion is high.
显然,本领域的技术人员可以对本发明进行各种改动和变型而不脱离本发明的精神和范围。这样,倘若本发明的这些修改和变型属于本发明权利要求及其等同技术的范围之内,则本发明也意图包含这些改动和变型在内。Obviously, those skilled in the art can make various changes and modifications to the present invention without departing from the spirit and scope of the present invention. Thus, if these modifications and variations of the present invention fall within the scope of the claims of the present invention and their equivalent technologies, the present invention also intends to include these modifications and variations.
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CN109167567A (en) * | 2018-08-21 | 2019-01-08 | 河海大学常州校区 | It is a kind of based on filter plate light splitting solar energy highly effective utilize device |
CN109289727A (en) * | 2018-08-20 | 2019-02-01 | 昆明理工大学 | A split spectroscopic solar photocatalytic reaction system |
CN110190147A (en) * | 2019-06-24 | 2019-08-30 | 北京大学深圳研究生院 | A Concentrating Photovoltaic System Based on Spectroscopic Elements |
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2015
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CN105932953A (en) * | 2016-06-14 | 2016-09-07 | 北京信息科技大学 | Photovoltaic module based on spectrums |
CN106887997A (en) * | 2017-03-29 | 2017-06-23 | 浙江晶科能源有限公司 | A kind of dispersion photovoltaic generating system |
CN109289727A (en) * | 2018-08-20 | 2019-02-01 | 昆明理工大学 | A split spectroscopic solar photocatalytic reaction system |
CN109167567A (en) * | 2018-08-21 | 2019-01-08 | 河海大学常州校区 | It is a kind of based on filter plate light splitting solar energy highly effective utilize device |
CN110190147A (en) * | 2019-06-24 | 2019-08-30 | 北京大学深圳研究生院 | A Concentrating Photovoltaic System Based on Spectroscopic Elements |
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