JPH04188775A - Solar cell - Google Patents
Solar cellInfo
- Publication number
- JPH04188775A JPH04188775A JP2316193A JP31619390A JPH04188775A JP H04188775 A JPH04188775 A JP H04188775A JP 2316193 A JP2316193 A JP 2316193A JP 31619390 A JP31619390 A JP 31619390A JP H04188775 A JPH04188775 A JP H04188775A
- Authority
- JP
- Japan
- Prior art keywords
- solar cell
- angle
- diffraction
- diffraction gratings
- transmission type
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000011295 pitch Substances 0.000 claims abstract description 14
- 210000004027 cell Anatomy 0.000 abstract description 17
- 230000005540 biological transmission Effects 0.000 abstract description 10
- 210000005056 cell body Anatomy 0.000 abstract description 4
- 239000000758 substrate Substances 0.000 abstract description 3
- 239000011521 glass Substances 0.000 description 3
- 230000007246 mechanism Effects 0.000 description 3
- 230000008859 change Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 229920002120 photoresistant polymer Polymers 0.000 description 2
- 230000009471 action Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- NJPPVKZQTLUDBO-UHFFFAOYSA-N novaluron Chemical compound C1=C(Cl)C(OC(F)(F)C(OC(F)(F)F)F)=CC=C1NC(=O)NC(=O)C1=C(F)C=CC=C1F NJPPVKZQTLUDBO-UHFFFAOYSA-N 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000012780 transparent material Substances 0.000 description 1
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野コ
本発明は、居住用建物、オフィスビルなどの電力源とし
て使用するのに好適な太陽電池の改良に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to improvements in solar cells suitable for use as a power source for residential buildings, office buildings, and the like.
[従来の技術] 従来の太陽電池は7次のように構成されていた。[Conventional technology] Conventional solar cells were constructed as follows.
■太陽電池をそのまま屋根等の取付部に配置する。■Place the solar cell directly on the roof or other mounting area.
■取付部に架台を用い1南側へ所定角度傾けて設置する
。■Use a pedestal for the mounting part and install it at a specified angle to the south.
■太陽追尾機構を付属させ、太陽追尾を行いながら、集
光するように構成する。■A solar tracking mechanism is attached and configured to focus light while tracking the sun.
[発明が解決しようとする課題]
しかし、上述の従来技術のものでは1次の問題点があっ
た。[Problems to be Solved by the Invention] However, the above-mentioned prior art had the first problem.
即ち、前記■のものでは設置状態により効率が大きく変
化する。That is, in the case of the above item (2), the efficiency varies greatly depending on the installation condition.
また、■のものでは■のものに比較し、採光効率の点で
は大となるが、朝、夕の効率低下が大きい、更に、■の
ものでは効率的には非常に高く。In addition, the type ■ has a higher daylighting efficiency than the type ■, but the efficiency decreases greatly in the morning and evening, and furthermore, the efficiency of the type ■ is extremely high.
理想的な状態であるが、前記のように動力源と制御機構
により成る高価な追尾機槽を備える必要があった。Although this would be an ideal situation, it would be necessary to provide an expensive tracking aircraft tank consisting of a power source and a control mechanism as described above.
特に、大面積の太陽電池を用いる場合にはシステムが大
掛かりとなり、非常に高価となり多大のエネルギー(t
カ)を消費するという問題点(:i1題)があった。In particular, when using large-area solar cells, the system becomes large-scale, extremely expensive, and requires a large amount of energy (tons).
There was a problem (i1 problem) of consuming the amount of F).
本発明は従来のものの上記課題を解決するようにした太
陽電池を提供することを目的とする。An object of the present invention is to provide a solar cell that solves the above-mentioned problems of conventional solar cells.
[課題を解決するための手段]
本発明は太陽電池に太陽光の入射側に格子ピッチが異な
る多数の格子で形成された回折格子を備えるようにした
ものである。[Means for Solving the Problems] According to the present invention, a solar cell is provided with a diffraction grating formed of a large number of gratings with different grating pitches on the sunlight incident side.
[作用]
本発明では、太陽光の入射側に格子ピッチが異なる透過
型回折格子を備えることにより1時々刻々と変化する太
陽光線を常に一定方向の面に気中して導くことができる
ようにしたものであるから。[Function] In the present invention, by providing a transmission diffraction grating with a different grating pitch on the sunlight incident side, it is possible to always guide the ever-changing sunlight rays into the air in a fixed direction. Because that's what I did.
朝、夕でも太陽電池本体に対する採光効率は殆ど低下し
ない。Even in the morning and evening, the lighting efficiency for the solar cell body hardly decreases.
[実施例]
次に本発明による太陽電池を第1図〜第2図に示す一実
施例に基づいて説明する。[Example] Next, a solar cell according to the present invention will be described based on an example shown in FIGS. 1 and 2.
第1図(イ)は1本発明の太陽電池の構成を示す縦断正
面図である。FIG. 1(a) is a longitudinal sectional front view showing the configuration of a solar cell according to the present invention.
同図において、1は太陽電池本体2の上に設けられる回
折格子、3は回折格子1上に配置される透明のカバーで
、このカバーは、たとえばガラス板で構成される。In the figure, 1 is a diffraction grating provided on a solar cell main body 2, and 3 is a transparent cover placed on the diffraction grating 1. This cover is made of, for example, a glass plate.
4はこれら1〜3を収納するケースである。4 is a case that stores these 1 to 3.
なお7回折格子lは、同図(ロ)、(ハ)に示すように
ガラス、フィルム等の透明材料より成る基板にの表面を
フォトレジスト(樹脂)で被覆した後、上方から照射し
て格子ピッチの異なる格子1 al+ 1 a2’ H
H及びlb、、、lb、、lb、、。As shown in Figures (B) and (C), the 7-diffraction grating 1 is made by coating the surface of a substrate made of a transparent material such as glass or film with photoresist (resin), and then irradiating the grating from above. Lattice with different pitch 1 al+ 1 a2' H
H and lb, , lb, , lb, .
・をエツチング加工して形成する。- Formed by etching.
この場合、フォトレジスト層の部分を同図(ロ)に示す
ように正弦波(sin−wave)状に形成したホログ
ラフィック回折格子の型とするほか、同図(ハ)に示す
ように矩形波に形成したラミナー回折格子とすることも
できる。In this case, the photoresist layer is formed into a holographic diffraction grating with a sinusoidal shape as shown in (b) of the same figure, or a rectangular wave as shown in (c) of the same figure. It can also be a laminar diffraction grating formed in
以上1〜4によって本発明の太陽を池旦が構成される。The sun of the present invention is constituted by 1 to 4 above.
次に本発明の原理について第2図を用いて説明する。Next, the principle of the present invention will be explained using FIG. 2.
同図に示すように格子ピッチの異なる透過型回折格子1
の上方から光が照射されるときは、その入射角を11回
折角をαとした場合
sin i +sin a=λ/P−(1)が成立す
る。Transmission type diffraction gratings 1 with different grating pitches as shown in the figure.
When light is irradiated from above, sin i + sin a = λ/P-(1) holds true, where the incident angle is 11 and the diffraction angle is α.
但し、λは光の波長、Pは格子ピッチである。However, λ is the wavelength of light and P is the grating pitch.
同図のように格子ピッチを設定したときに、太陽光線の
入射角が時間と共に、たとえばl l+ 12+1、
・・・i、と変化しても1回折角αは同図に示すように
一定値となる。When the grating pitch is set as shown in the figure, the incident angle of sunlight changes over time, for example, l l + 12 + 1,
...i, the single diffraction angle α remains constant as shown in the figure.
一方、格子ピッチPは一旦設定した後は、これらの値p
HP2+ P3・・・Plは一定となるためλ/P、〜
λ/P、も一定である。On the other hand, once the grating pitch P is set, these values p
HP2+ P3...Pl is constant, so λ/P, ~
λ/P is also constant.
従って、(1)式から回折角αがOとなるように各11
〜i、に対するPを予め設定するようにすれば、透過光
線は同図にQ、〜Q、で示すように透過型回折格子1の
基板に垂直となる回折角α=0となる光線へと変換する
ことができる。Therefore, from equation (1), each 11
By setting P for ~i in advance, the transmitted light ray becomes a light ray with a diffraction angle α = 0 that is perpendicular to the substrate of the transmission type diffraction grating 1, as shown by Q and ~Q in the figure. can be converted.
従って1本発明の太陽電池旦を建物の屋根等に配置した
場合、太陽の運行に伴う入射光線の角度の変化に拘わら
ず、太陽光線は回折格子1によって平行光線にされて、
効率良く太陽電池本体2に入射するよう導かれる。Therefore, when the solar cell panel of the present invention is placed on the roof of a building, etc., regardless of the change in the angle of the incident rays due to the movement of the sun, the sunlight rays are made into parallel rays by the diffraction grating 1.
The light is guided to efficiently enter the solar cell main body 2.
[発明の効果コ
本発明は上記のように構成したものであるから次のよう
な優れた効果を有する。[Effects of the Invention] Since the present invention is constructed as described above, it has the following excellent effects.
■太陽の運行によって入射光線の角度、入射量が変化し
ても入射部に設けられた格子ピッチの異なる透過型回折
格子によって常に適正な同一角度で当該太陽電池(本体
)の一定面(入射面)へ導くことができるようにしたた
め、入射光線の量は日中においては略一定とすることが
でき。■Even if the angle and amount of incident light rays change due to the movement of the sun, the transmission diffraction gratings with different grating pitches provided at the entrance part will always maintain the same proper angle on a certain surface (the entrance surface) of the solar cell (main body). ), the amount of incident light can be kept approximately constant during the day.
採光効率を向上させることができる。Lighting efficiency can be improved.
■この場合、透過型回折格子はガラス、フィルム等の基
材より成るため、軽く、可撓性があり。■In this case, the transmission diffraction grating is made of a base material such as glass or film, so it is light and flexible.
加工、設置が容易である。Easy to process and install.
■しかも1本発明の場合、従来のような大掛かりな追尾
機構を備える必要がなく、平面状の採光窓材の上面に設
ける構成で良いため、極めて経済的で、実用性大である
。(1) Moreover, in the case of the present invention, there is no need to provide a large-scale tracking mechanism like the conventional one, and the structure can be provided on the top surface of a planar daylighting window material, so it is extremely economical and highly practical.
第1図(イ)は本発明を適用した太陽電池の全体の構成
を示す縦断正面図、同図(ロ)及び(ハ)は夫々格子ピ
ッチの異なる透過型回折格子の例としてのホログラフィ
ック回折格子とラミナー回折格子の拡大断面図である。
第2図は本発明の構成に使用する回折格子の作用を説明
するために描いた説明図である。
1:透過型回折格子
2:太陽電池本体
3:カバー
4:ケース
5二太陽電池
出願人 三洋電機株式会社
代理人 弁理士 斎藤春弥
はか1名
第1図
(イ)
(ロ)
(ハ)
1:透過型回折格子
2 太陽電池本体
6 カバー
4:ケース
5゛太陽電池FIG. 1(a) is a longitudinal sectional front view showing the overall configuration of a solar cell to which the present invention is applied, and FIG. 1(b) and (c) are examples of holographic diffraction gratings with different grating pitches FIG. 3 is an enlarged cross-sectional view of a grating and a laminar diffraction grating. FIG. 2 is an explanatory diagram drawn to explain the action of the diffraction grating used in the configuration of the present invention. 1: Transmission type diffraction grating 2: Solar cell body 3: Cover 4: Case 5 2. Solar cell applicant Sanyo Electric Co., Ltd. agent Patent attorney Haruya Saito (1 person) Figure 1 (A) (B) (C) 1: Transmission type diffraction grating 2 Solar cell body 6 Cover 4: Case 5゛Solar cell
Claims (1)
形成された回折格子を備えたことを特徴とする太陽電池
。1. A solar cell characterized by having a diffraction grating formed of a large number of gratings with different grating pitches on the sunlight incident side.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2316193A JPH04188775A (en) | 1990-11-22 | 1990-11-22 | Solar cell |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2316193A JPH04188775A (en) | 1990-11-22 | 1990-11-22 | Solar cell |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04188775A true JPH04188775A (en) | 1992-07-07 |
Family
ID=18074337
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2316193A Pending JPH04188775A (en) | 1990-11-22 | 1990-11-22 | Solar cell |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04188775A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2011102956A2 (en) * | 2010-02-22 | 2011-08-25 | University Of Delaware | Photonic crystal enhanced light trapping solar cell |
JP2013509707A (en) * | 2009-11-02 | 2013-03-14 | エルジー イノテック カンパニー リミテッド | Solar cell and manufacturing method thereof |
JP2013537004A (en) * | 2010-12-21 | 2013-09-26 | 財團法人工業技術研究院 | Multi-band concentrator / energy conversion module |
-
1990
- 1990-11-22 JP JP2316193A patent/JPH04188775A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013509707A (en) * | 2009-11-02 | 2013-03-14 | エルジー イノテック カンパニー リミテッド | Solar cell and manufacturing method thereof |
WO2011102956A2 (en) * | 2010-02-22 | 2011-08-25 | University Of Delaware | Photonic crystal enhanced light trapping solar cell |
WO2011102956A3 (en) * | 2010-02-22 | 2011-11-24 | University Of Delaware | Photonic crystal enhanced light trapping solar cell |
JP2013537004A (en) * | 2010-12-21 | 2013-09-26 | 財團法人工業技術研究院 | Multi-band concentrator / energy conversion module |
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