JP2012084545A - Light source device for solar simulator - Google Patents

Light source device for solar simulator Download PDF

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JP2012084545A
JP2012084545A JP2012009780A JP2012009780A JP2012084545A JP 2012084545 A JP2012084545 A JP 2012084545A JP 2012009780 A JP2012009780 A JP 2012009780A JP 2012009780 A JP2012009780 A JP 2012009780A JP 2012084545 A JP2012084545 A JP 2012084545A
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light source
source device
solar simulator
flash lamp
voltage power
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JP5229927B2 (en
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Shinichi Igari
真一 猪狩
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National Institute of Advanced Industrial Science and Technology AIST
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    • 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
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Abstract

PROBLEM TO BE SOLVED: To provide a light source device for a solar simulator in which light emission time of light emitted from a flash lamp is extended to about 10 ms by using a flash lamp as a light-emitting source from the solar simulator, the waveform can be made trapezoidal, and the crest can be flattened.SOLUTION: The light source device for a solar simulator comprises a DC high voltage power supply 1, a PFN2 where capacitors and reactors are connected in a shape of a distributed constant circuit with the DC high voltage power supply 1, and a flash lamp 3 connected with the output open end of the PFN2. Capacitance of at least one capacitor 22 out of the capacitors in the PFN2 close to the DC high voltage power supply 1 side is set larger than that of other capacitors.

Description

本発明は、ソーラシミュレータ用光源装置に係り、特に、太陽電池ＩＶ測定用ソーラシミュレータに用いられるソーラシミュレータ用光源装置に関する。   The present invention relates to a solar simulator light source device, and more particularly to a solar light source device used in a solar simulator for solar cell IV measurement.

図９は、従来技術に係るフラッシュランプ点灯装置におけるフラッシュランプの発光波形を示す図である。
同図に示すように、この発光波形は、発光幅が短く、また発光波形が台形でなく、そのパルス幅は約５００μｓと短く、形状は山形である。 FIG. 9 is a diagram showing a light emission waveform of the flash lamp in the flash lamp lighting device according to the prior art.
As shown in the figure, the emission waveform has a short emission width, the emission waveform is not trapezoidal, the pulse width is as short as about 500 μs, and the shape is a mountain shape.

パルスパワー工学の基礎と応用，京都ハイパワーテクノロジー研究会編，近代科学社Basics and applications of pulse power engineering, Kyoto High Power Technology Study Group, Modern Science 高電圧パルスパワー工学，原雅則・秋山秀典著，森北出版High voltage pulse power engineering, Masanori Hara, Hidenori Akiyama, Morikita Publishing Transientelectronics -Pulsed Circuit Technology Paul W．SmithWileyTransientelectronics -Pulsed Circuit Technology Paul W. SmithWiley 「ミドルパルス・マルチフラッシュによるＩ−Ｖ測定法の開発とその有効性」第３回次世代太陽光発電システムシンポジウム予稿集 日本学術振興会,p270-273,2006年7月"Development of IV measurement method by middle pulse multi flash and its effectiveness" Proceedings of the 3rd Next Generation Solar Power System Symposium Japan Society for the Promotion of Science, p270-273, July 2006

しかし、応答速度が遅い、高効率太陽電池や薄膜太陽電池を、短い発光幅（５００μｓ）と山形波形の照射光で測定しようとすると、得られるＩＶ特性は過渡特性を示し、太陽電池の諸特性値に、過小もしくは過大な計算結果をもたらす懸念がある。また、放射照度に対する太陽電池出力の直線性からのずれや、基準太陽電池と被測定太陽電池の相対分光感度の違いにより生じるスペクトルミスマッチ誤差を生じるおそれがある。
このような電圧掃引時の過渡状態による誤差を抑えて、正しい太陽電池のＩＶ特性を得るためには、電気的に９５％と充分飽和した状態を与えるに十分な時間、すなわち応答時定数の4倍以上の時間に及ぶ平坦な照射光下で、ＩＶ特性を測定することが必要となる。そのためには発光波形の拡張が要求される。すなわち、ソーラシミュレータの光源の発光時間を１０ｍｓ程度まで拡張し、またその発光波形の台形化と波高部の平坦化を図る必要がある。 However, when measuring high-efficiency solar cells and thin-film solar cells with slow response speeds with a short emission width (500 μs) and chevron-shaped irradiation light, the IV characteristics obtained show transient characteristics, and various characteristics of solar cells There is concern that the value may lead to under- or over-calculated results. Further, there is a possibility that a spectral mismatch error caused by a deviation from the linearity of the solar cell output with respect to the irradiance or a difference in relative spectral sensitivity between the reference solar cell and the solar cell to be measured occurs.
In order to suppress the error due to the transient state at the time of the voltage sweep and to obtain the correct IV characteristic of the solar cell, a time sufficient to give a sufficiently saturated state of 95% electrically, that is, a response time constant of 4 It is necessary to measure the IV characteristics under flat irradiation light over a time more than doubled. For this purpose, it is necessary to expand the emission waveform. That is, it is necessary to extend the light emission time of the light source of the solar simulator to about 10 ms, and to make the light emission waveform trapezoidal and flatten the wave height.

本発明の目的は、上記の問題点に鑑み、ソーラシミュレータの発光源としてフラッシュランプを用い、フラッシュランプからの発光光の発光時間を１０ｍｓ程度まで拡張し、かつ波形の台形化と波高部の平坦化を可能にしたソーラシミュレータ用光源装置を提供することにある。   In view of the above problems, the object of the present invention is to use a flash lamp as the light source of the solar simulator, extend the light emission time of the light emitted from the flash lamp to about 10 ms, and make the waveform trapezoidal and flat in the wave height portion. It is an object to provide a solar simulator light source device that can be realized.

第１の手段は、ソーラシミュレータ用光源装置において、直流高圧電源と、該直流高圧電源にコンデンサとリアクトルとを分布定数回路状に接続されたＰＦＮと、該ＰＦＮの出力開放端に接続されたフラッシュランプとからなり、前記ＰＦＮの出力端に接続されるリアクトルと並列に抵抗を接続したことを特徴とするソーラシミュレータ用光源装置である。
第２の手段は、ソーラシミュレータ用光源装置において、直流高圧電源と、該直流高圧電源にコンデンサとリアクトルとを分布定数回路状に接続されたＰＦＮと、該ＰＦＮの出力開放端に接続されたフラッシュランプとからなり、前記ＰＦＮの出力端に接続されるリアクトルのインダクタンスを他のリアクトルのインダクタンスよりも大きくしたことを特徴とするソーラシミュレータ用光源装置である。
第３の手段は、ソーラシミュレータ用光源装置において、直流高圧電源と、該直流高圧電源にコンデンサとリアクトルとを分布定数回路状に接続されたＰＦＮと、該ＰＦＮの出力開放端に接続されたフラッシュランプとからなり、前記ＰＦＮの前記直流高圧電源側に近いコンデンサの少なくとも１つのコンデンサのキャパシタンスを他のコンデンサのキャパシタンスより大きくしたことを特徴とするソーラシミュレータ用光源装置である。 In a solar simulator light source device, a first means is a DC high-voltage power supply, a PFN in which a capacitor and a reactor are connected to the DC high-voltage power supply in a distributed constant circuit form, and a flash connected to the output open end of the PFN A solar simulator light source device comprising a lamp and having a resistor connected in parallel with a reactor connected to the output terminal of the PFN.
The second means is a solar simulator light source device, a DC high-voltage power supply, a PFN in which a capacitor and a reactor are connected to the DC high-voltage power supply in a distributed constant circuit form, and a flash connected to the output open end of the PFN A solar simulator light source device comprising a lamp and having an inductance of a reactor connected to an output terminal of the PFN made larger than an inductance of another reactor.
The third means is a solar simulator light source device, a direct current high voltage power source, a PFN in which a capacitor and a reactor are connected to the direct current high voltage power source in a distributed constant circuit form, and a flash connected to an output open end of the PFN A solar simulator light source device comprising a lamp and having a capacitance of at least one of the capacitors close to the DC high-voltage power supply side of the PFN larger than that of other capacitors.

本発明によれば、ソーラシミュレータ用光源装置として基本ＰＦＮを改良したＰＦＮを用いることにより、発光パルス幅が大きく波高部が平坦なフラッシュ光を実現することができ、ソーラシミュレータの光源として好適なソーラシミュレータ用光源装置が得られる。   According to the present invention, by using a PFN improved from the basic PFN as a light source device for a solar simulator, it is possible to realize flash light having a large light emission pulse width and a flat crest portion, which is suitable as a light source for a solar simulator. A simulator light source device is obtained.

ＰＦＮを用いたソーラシミュレータ用光源装置の構成を示す回路図である。It is a circuit diagram which shows the structure of the light source device for solar simulators using PFN. 図１に示したフラッシュランプの発光波形を示す図である。It is a figure which shows the light emission waveform of the flash lamp shown in FIG. 第１の実施形態本の発明に係るソーラシミュレータ用光源装置の構成を示す回路図である。1 is a circuit diagram showing a configuration of a light source device for a solar simulator according to the present invention. 図３に示したフラッシュランプの発光波形を示す図である。It is a figure which shows the light emission waveform of the flash lamp shown in FIG. 第２の実施形態の発明に係るソーラシミュレータ用光源装置の構成を示す回路図である。It is a circuit diagram which shows the structure of the light source device for solar simulators concerning invention of 2nd Embodiment. 図５に示したフラッシュランプの発光波形を示す図である。It is a figure which shows the light emission waveform of the flash lamp shown in FIG. 第３の実施形態の発明に係るソーラシミュレータ用光源装置の構成を示す回路図である。It is a circuit diagram which shows the structure of the light source device for solar simulators concerning invention of 3rd Embodiment. 図７に示したフラッシュランプの発光波形を示す図である。It is a figure which shows the light emission waveform of the flash lamp shown in FIG. 従来技術に係るフラッシュランプ点灯装置におけるフラッシュランプの発光波形を示す図である。It is a figure which shows the light emission waveform of the flash lamp in the flash lamp lighting device which concerns on a prior art.

本発明は、ソーラシミュレータ用光源装置の光源としてフラッシュランプを用い、フラッシュランプから放射される発光光の発光波形の台形化と波高部の平坦化を図るために、直流高圧電源とフラッシュランプとの間に、直列接続されたリアクトルと並列接続されたコンデンサからなるＬＣ回路を多段に接続したＰＦＮ（pulse forming network）を挿入したものである。   The present invention uses a flash lamp as a light source of a light source device for a solar simulator, and in order to make the emission waveform of emitted light emitted from the flash lamp trapezoidal and flatten the wave height portion, A PFN (pulse forming network) in which LC circuits composed of series-connected reactors and capacitors connected in parallel are connected in multiple stages is inserted between them.

図１は、ＰＦＮを用いたソーラシミュレータ用光源装置の構成を示す回路図、図２はフラッシュランプの発光波形を示す図である。
図１において、１は直流高圧電源、２はＰＦＮ、２１−１、２１−２・・・２１−ｎはリアクトル、２２−１、２２−２・・・２２−ｎはコンデンサ、３はフラッシュランプ、４はトリガートランス、５はトリガー電極であり、ＰＦＮ２は、各リアクトル２１−１、２１−２・・・２１−ｎのインダクタンスが、例えば、５ｍＨ、各コンデンサ２２−１、２２−２・・・２２−ｎのキャパシタンスが、例えば、５０μＦからなるＬＣ回路を、例えば、１０段接続して構成したものである。このソーラシミュレータ用光源装置によれば、フラッシュランプ３から、図２に示すように、発光パルス幅約１０.１ｍｓの発光光が得られるが、オーバーシュート、リンギング（波高部リップル＝１２.２％）が見られるため、ソーラシミュレータ用光源装置として用いるためには更なる改良が必要である。 FIG. 1 is a circuit diagram showing a configuration of a solar simulator light source device using PFN, and FIG. 2 is a diagram showing a light emission waveform of a flash lamp.
In FIG. 1, 1 is a DC high voltage power source, 2 is a PFN, 21-1, 21-2... 21-n is a reactor, 22-1, 22-2. 4 is a trigger transformer, 5 is a trigger electrode, and the PFN 2 has an inductance of each reactor 21-1, 21-2,..., 21-n, for example, 5 mH, each capacitor 22-1, 22-2,. An LC circuit having a capacitance of 22-n, for example, 50 μF, is configured by connecting, for example, 10 stages. According to this solar simulator light source device, emitted light having a light emission pulse width of about 10.1 ms can be obtained from the flash lamp 3 as shown in FIG. 2, but overshoot and ringing (wave height ripple = 12.2%). In order to use as a light source device for a solar simulator, further improvement is necessary.

本発明の第１の実施形態を図３および図４を用いて説明する。
図３は、本実施形態の発明に係るソーラシミュレータ用光源装置の構成を示す回路図、図４はフラッシュランプの発光波形を示す図である。
図３において、２３はＰＦＮ２の出力端に接続されるリアクトル２１−１と並列に接続された抵抗であり、抵抗２３の抵抗値は、例えば、２０Ωである。なお、その他の構成は図１に示した同符号の構成に対応する。図４に示すように、フラッシュランプ３からは、発光パルス幅１０.１ｍｓの発光光が得られ、立ち上がり部分のオーバーシュートとリンギング（波高部リップル８.５％）は、ほぼ無くなるが、全体として立ち上がり、立ち下がりが、なだらかに丸みを帯び、ソーラシミュレータ用光源装置として好適である。 A first embodiment of the present invention will be described with reference to FIGS.
FIG. 3 is a circuit diagram showing a configuration of a light source device for a solar simulator according to the invention of this embodiment, and FIG. 4 is a diagram showing a light emission waveform of a flash lamp.
In FIG. 3, reference numeral 23 denotes a resistor connected in parallel with the reactor 21-1 connected to the output terminal of the PFN 2, and the resistance value of the resistor 23 is 20Ω, for example. Other configurations correspond to the configurations of the same reference numerals shown in FIG. As shown in FIG. 4, emitted light having a light emission pulse width of 10.1 ms is obtained from the flash lamp 3, and overshoot and ringing (wave height ripple 8.5%) at the rising portion are almost eliminated, but as a whole The rising and falling edges are gently rounded, making it suitable as a solar simulator light source device.

本発明の第２の実施形態を図５および図６を用いて説明する。
図５は、本実施形態の発明に係るソーラシミュレータ用光源装置の構成を示す回路図、図６はフラッシュランプの発光波形を示す図である。
図５において、２１はＰＦＮ２の出力端に接続されるリアクトル２１−１と直列に付加的に接続されたリアクトルであり、リアクトル２１のインダクタンスは、例えば、５ｍＨである。なお、その他の構成は図１に示した同符号の構成に対応する。
図６に示すように、フラッシュランプ３からは、発光パルス幅９.１８ｍｓの発光光が得られ、その立ち上がり部分のオーバーシュート、リンギングは無くなるが、波高部平坦部の右下がりが大きくなるため、波高部リップルは９.６％となり、図４に示した第１の実施形態の場合比べて若干増加するが、ソーラシミュレータ用光源装置として好適である。 A second embodiment of the present invention will be described with reference to FIGS.
FIG. 5 is a circuit diagram showing the configuration of the solar simulator light source device according to the invention of this embodiment, and FIG. 6 is a diagram showing the light emission waveform of the flash lamp.
In FIG. 5, reference numeral 21 denotes a reactor additionally connected in series with a reactor 21-1 connected to the output end of the PFN 2, and the inductance of the reactor 21 is, for example, 5 mH. Other configurations correspond to the configurations of the same reference numerals shown in FIG.
As shown in FIG. 6, emitted light having a light emission pulse width of 9.18 ms is obtained from the flash lamp 3, and there is no overshoot or ringing at the rising portion, but the lowering of the right portion of the crest portion is increased. The crest ripple is 9.6%, which is slightly increased as compared with the first embodiment shown in FIG. 4, but is suitable as a light source device for a solar simulator.

本発明の第３の実施形態を図７および図８を用いて説明する。
図７は、本実施形態の発明に係るソーラシミュレータ用光源装置の構成を示す回路図、図８はフラッシュランプの発光波形を示す図である。
図７において、２２はＰＦＮ２の直流高圧電源１側に近いコンデンサ、例えば、コンデンサ２１−ｎ−１と並列に付加的に接続されたコンデンサであり、このコンデンサ２２のキャパシタンスは、例えば、１２μＦである。なお、その他の構成は図５に示した同符号の構成に対応する。
図８に示すように、フラッシュランプ３からは、発光パルス幅９.３８ｍｓの発光光が得られ、付加されたコンデンサ２２がフラッシュランプ３から遠い位置にあるため、その効果が遅く効いてくるため、直流高圧電源１からの放電比率が、図５に示したものに比べて増える結果、波形の右下がりが緩和され、波高部リップル３.８％となり最も小さくなり、ソーラシミュレータ用光源装置として極めて好適である。 A third embodiment of the present invention will be described with reference to FIGS.
FIG. 7 is a circuit diagram showing the configuration of the light source device for solar simulator according to the invention of this embodiment, and FIG. 8 is a diagram showing the light emission waveform of the flash lamp.
In FIG. 7, 22 is a capacitor close to the DC high-voltage power supply 1 side of PFN2, for example, a capacitor additionally connected in parallel with capacitor 21-n-1, and the capacitance of this capacitor 22 is, for example, 12 μF. . Other configurations correspond to the configurations of the same reference numerals shown in FIG.
As shown in FIG. 8, since the flash lamp 3 emits light having a light emission pulse width of 9.38 ms, and the added capacitor 22 is located far from the flash lamp 3, the effect is effective. As a result, the discharge ratio from the DC high-voltage power supply 1 is increased as compared with that shown in FIG. 5. As a result, the lowering of the waveform to the right is alleviated and the peak height ripple is 3.8%, which is the smallest. Is preferred.

１ 直流高圧電源
２ ＰＦＮ
２１、２１−１、２１−２・・・２１−ｎ リアクトル
２２、２２−１、２２−２・・・２２−ｎ コンデンサ
２３ 抵抗
３ フラッシュランプ
４ トリガートランス
５ トリガー電極 1 DC high voltage power supply 2 PFN
21, 21-1, 21-2... 21 -n Reactors 22, 22-1, 22-2... 22 -n Capacitor 23 Resistance
3 Flash lamp 4 Trigger transformer 5 Trigger electrode

Claims (1)

ソーラシミュレータ用光源装置において、直流高圧電源と、該直流高圧電源にコンデンサとリアクトルとを分布定数回路状に接続されたＰＦＮと、該ＰＦＮの出力開放端に接続されたフラッシュランプとからなり、前記ＰＦＮの前記直流高圧電源側に近いコンデンサの少なくとも１つのコンデンサのキャパシタンスを他のコンデンサのキャパシタンスより大きくしたことを特徴とするソーラシミュレータ用光源装置。   In a solar simulator light source device, comprising: a direct-current high-voltage power supply; a PFN in which a capacitor and a reactor are connected to the direct-current high-voltage power supply in a distributed constant circuit; and a flash lamp connected to an output open end of the PFN, A light source device for a solar simulator, wherein the capacitance of at least one of the capacitors close to the DC high-voltage power supply side of PFN is made larger than the capacitances of the other capacitors.
JP2012009780A 2007-04-24 2012-01-20 Light source device for solar simulator Expired - Fee Related JP5229927B2 (en)

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