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JPS6260804B2 - - Google Patents
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JPS6260804B2 - - Google Patents

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Publication number
JPS6260804B2
JPS6260804B2 JP58159582A JP15958283A JPS6260804B2 JP S6260804 B2 JPS6260804 B2 JP S6260804B2 JP 58159582 A JP58159582 A JP 58159582A JP 15958283 A JP15958283 A JP 15958283A JP S6260804 B2 JPS6260804 B2 JP S6260804B2
Authority
JP
Japan
Prior art keywords
capacitor element
pulse generator
terminal plate
pulse
discharge lamp
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.)
Expired
Application number
JP58159582A
Other languages
Japanese (ja)
Other versions
JPS6052007A (en
Inventor
Takenobu Iida
Jojiro Shiina
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Iwasaki Electric Co Ltd
Original Assignee
Iwasaki Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Iwasaki Electric Co Ltd filed Critical Iwasaki Electric Co Ltd
Priority to JP58159582A priority Critical patent/JPS6052007A/en
Publication of JPS6052007A publication Critical patent/JPS6052007A/en
Publication of JPS6260804B2 publication Critical patent/JPS6260804B2/ja
Granted legal-status Critical Current

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  • Circuit Arrangements For Discharge Lamps (AREA)
  • Ceramic Capacitors (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は、高圧ナトリウムランプのような高圧
金属蒸気放電灯を始動点灯させるのに用いられる
パルス発生器の改良に関する。 高圧ナトリウムランプのような高圧金属蒸気放
電灯は一般に始動電圧が高く、通常の商用電源電
圧で始動させることは困難であるため、例えば、
放電灯の内部にパルス発生器を組み込んで、該パ
ルス発生器により高電圧パルスを発生させ、これ
を電源電圧と共に放電灯に印加して始動点灯させ
ることが行われている。 第1図は上記のような高圧金属蒸気放電灯の回
路構成の一例を示すものである。この回路は、交
流電源1にチヨークコイルのごとき誘導性素子2
を介して発光管3を接続するとともに、該発光管
3と並列に、半導体スイツチング素子4及びダイ
オード5の並列回路と非線形コンデンサー素子6
と熱応動開閉器7とを直列に接続してなる始動回
路8を接続したものである。9は発光管3及び始
動回路8を収納した外球を示す。 かかる回路において、交流電源1を投入する
と、電源電圧周波の半サイクルにおいて非線形コ
ンデンサー素子6が充電され、次の半サイクルに
おいて半導体スイツチング素子4がブレークオー
バーし非線形コンデンサー素子6に充電された電
荷は誘導性素子2及びコンデンサー10を通して
急激に放電する。このとき非線形コンデンサー素
子6の非線形特性により圧電効果を伴う弛張発振
が生じ誘導性素子2の中に高電圧パルスが発生
し、これが電源電圧と共に発光管3に印加される
ため放電灯が始動する。放電灯が始動した後は始
動回路8には低電圧しか印加されずかつ熱応動開
閉器7も開くため高電圧パルスの発生は停止す
る。 前記動作から明らかなように、非線形コンデン
サー素子6は誘導性素子2とともにパルス発生器
を構成しているわけである。 ところで、上記のようなパルス発生器に使用す
る非線形コンデンサー素子として現在のところ最
も適当であると考えられるものは、チタン酸バリ
ウムを主体とした強誘電体セラミツクコンデンサ
ーであるが、これを放電灯に組み込んで使用する
場合には、コンデンサー基板の構成材料の選定の
みならず、コンデンサー基板に対するリード線の
接続構造及びコンデンサー素子の外装等、構造上
種々の工夫を施さなければ実用的なパルス発生器
は得られない。なぜなら、これらは、発生する高
電圧パルスの大きさ、コンデンサー素子の耐熱
性、耐圧性及び機械的強度等に大きな影響を及ぼ
すからである。 例えば、従来から一般の電子部品として用いら
れているセラミツクコンデンサーは、セラミツク
基板の両面に銀膜の電極を被着し、これにリード
線を鉛−錫合金半田で接続したうえ、全体を樹脂
でオーバーコートしたものが多い。ところが、こ
のような構造のものはせいぜい150℃程度の耐熱
性しかなく、とても高圧金属蒸気放電灯に組み込
んで使用することはできない。また、セラミツク
基板上の電極に直接にリード線を接続してあるの
で、コンデンサー素子の圧電効果に伴う振動を十
分に吸収しえず、その結果高電圧パルスの発生を
抑制してしまい、しかも機械的疲労も大きいとい
う難点があつた。 本発明は、以上の点に鑑みてなされたもので、
誘導性素子と非線形コンデンサー素子とからなる
パルス発生器において、非線形コンデンサー素子
の構造を改良・工夫することにより、高圧金属蒸
気放電灯を確実に始動させることができる高電圧
パルスを発生させることができる一方、耐熱性、
耐圧性及び機械的強度等も十分に大きく、従つて
放電灯に組み込んで実用に供しうるパルス発生器
を提供せんとするものである。 発明者等は、先ず、コンデンサー素子を構成す
るセラミツク基板に対するリード線の接続構造
が、高電圧パルスの高さ及び機械的強度等に対し
てとりわけ大きな関係があることに着目して次の
ような実験を行つた。強誘電体セラミツク基板の
材料として、チタン酸バリウム(BaTiO3)に数モ
ル%のジルコニウム酸バリウム(BaZrO3)及びチ
タン酸ストロンチウム(SrTiO3)と微量の希土類
金属酸化物とを添加してなる粉末にバインダーと
してポリビニルアルコールを加えて撹拌し、プレ
ス成形した後、1400℃の温度で2時間気中焼成を
行い、直径26mm、厚み0.5mmの円板状の基板を作
つた。この基板の両面に銀ペーストをスクリーン
印刷で直径25.7mmに塗布し、乾燥後750℃の温度
で気中焼成して電極を形成した。そしてこの電極
部分に第2図に示すような、リード線11を備え
た端子板12を銀粉末と低融点ガラス粉末とから
なるペーストで接着し、約500℃の温度で気中焼
成を行つて固定した。リード線11には直径0.5
mmのニツケル線を用い、端子板は鉄―ニツケル―
コバルト―クロム合金を用い、厚みを0.3mmと
し、直径は1mm〜5mmの範囲で種々異るものを使
用した。このようなコンデンサー素子を第3図に
示すように、半導体スイツチング素子4とダイオ
ード5並びに抵抗体13の並列回路及び誘導性素
子2を介して交流電源1に接続したうえ、非線形
コンデンサー6の部分をフレオン液中に保持し、
交流200V、50Hzの入力を加えて、常温における
パルスピーク電圧を測定した。第1表に、このと
きのリード線端子板の直径とパルスピーク電圧の
関係を示す。
The present invention relates to improvements in pulse generators used to start high pressure metal vapor discharge lamps, such as high pressure sodium lamps. High-pressure metal vapor discharge lamps such as high-pressure sodium lamps generally have a high starting voltage and are difficult to start with normal commercial power supply voltage.
A pulse generator is installed inside a discharge lamp, and the pulse generator generates a high voltage pulse, which is applied together with a power supply voltage to the discharge lamp to start and light it. FIG. 1 shows an example of the circuit configuration of the above-described high-pressure metal vapor discharge lamp. This circuit consists of an AC power source 1 and an inductive element 2 such as a chiyoke coil.
A parallel circuit of a semiconductor switching element 4 and a diode 5 and a nonlinear capacitor element 6 are connected in parallel with the arc tube 3 through the arc tube 3.
A starting circuit 8 is connected in which a thermally responsive switch 7 and a starting circuit 8 are connected in series. Reference numeral 9 indicates an outer sphere housing the arc tube 3 and the starting circuit 8. In this circuit, when the AC power supply 1 is turned on, the nonlinear capacitor element 6 is charged in a half cycle of the power supply voltage frequency, and in the next half cycle, the semiconductor switching element 4 breaks over and the charge charged in the nonlinear capacitor element 6 is induced. A sudden discharge occurs through the magnetic element 2 and the capacitor 10. At this time, relaxation oscillation accompanied by a piezoelectric effect occurs due to the nonlinear characteristics of the nonlinear capacitor element 6, and a high voltage pulse is generated in the inductive element 2, which is applied to the arc tube 3 together with the power supply voltage, thereby starting the discharge lamp. After the discharge lamp is started, only a low voltage is applied to the starting circuit 8 and the thermally responsive switch 7 is also opened, so the generation of high voltage pulses is stopped. As is clear from the above operation, the nonlinear capacitor element 6 and the inductive element 2 constitute a pulse generator. By the way, the type of nonlinear capacitor element currently considered most suitable for use in the above-mentioned pulse generator is a ferroelectric ceramic capacitor mainly made of barium titanate. When used as a built-in device, a practical pulse generator is not possible unless various structural improvements are made, such as the selection of the constitutive material of the capacitor board, the connection structure of the lead wires to the capacitor board, and the exterior of the capacitor element. I can't get it. This is because these greatly affect the magnitude of the generated high voltage pulse, the heat resistance, pressure resistance, mechanical strength, etc. of the capacitor element. For example, ceramic capacitors, which have traditionally been used as general electronic components, have silver film electrodes coated on both sides of a ceramic substrate, lead wires connected to these with lead-tin alloy solder, and the entire body made of resin. Many have overcoats. However, this type of structure has a heat resistance of only about 150 degrees Celsius at most, so it cannot be used in a high-pressure metal vapor discharge lamp. In addition, since the lead wires are connected directly to the electrodes on the ceramic substrate, vibrations caused by the piezoelectric effect of the capacitor element cannot be sufficiently absorbed, and as a result, the generation of high voltage pulses is suppressed. The problem was that it was very tiring. The present invention has been made in view of the above points, and
In a pulse generator consisting of an inductive element and a nonlinear capacitor element, by improving and devising the structure of the nonlinear capacitor element, it is possible to generate a high voltage pulse that can reliably start a high pressure metal vapor discharge lamp. On the other hand, heat resistance,
It is an object of the present invention to provide a pulse generator which has sufficiently high pressure resistance and mechanical strength, and which can be incorporated into a discharge lamp for practical use. The inventors first focused on the fact that the connection structure of the lead wire to the ceramic substrate constituting the capacitor element has a particularly large relationship with the height of the high voltage pulse, mechanical strength, etc., and developed the following method. I conducted an experiment. A powder made by adding several mol% of barium zirconate (BaZrO 3 ) and strontium titanate (SrTiO 3 ) to barium titanate (BaTiO 3 ) and a trace amount of rare earth metal oxide as a material for ferroelectric ceramic substrates. Polyvinyl alcohol was added as a binder, stirred, and press-molded, followed by baking in the air at a temperature of 1400°C for 2 hours to produce a disc-shaped substrate with a diameter of 26 mm and a thickness of 0.5 mm. Silver paste was applied to both sides of this substrate by screen printing to a diameter of 25.7 mm, and after drying, it was baked in air at a temperature of 750°C to form electrodes. Then, a terminal plate 12 equipped with a lead wire 11 as shown in Fig. 2 was adhered to this electrode part with a paste made of silver powder and low melting point glass powder, and fired in the air at a temperature of about 500°C. Fixed. Lead wire 11 has a diameter of 0.5
mm nickel wire is used, and the terminal board is iron - nickel -
A cobalt-chromium alloy was used, with a thickness of 0.3 mm, and various diameters ranging from 1 mm to 5 mm. As shown in FIG. 3, such a capacitor element is connected to an AC power source 1 via a parallel circuit of a semiconductor switching element 4, a diode 5, a resistor 13, and an inductive element 2, and the nonlinear capacitor 6 is held in Freon liquid,
The pulse peak voltage at room temperature was measured by applying AC 200V, 50Hz input. Table 1 shows the relationship between the diameter of the lead wire terminal plate and the pulse peak voltage at this time.

【表】 第1表から明らかなように、端子板の直径が2
mmを越えると、パルスピーク電圧は急激に低下す
る傾向が見られる。これは、端子板と導電性ガラ
ス接着剤が強誘電体セラミツク板の直径方向の振
動を抑制するためであると考えられ、かかる理由
からリード線の端子板の面積はできるだけ小さく
することが望ましい。しかしながら、端子板の面
積を小さくすることは強誘電体セラミツク板及び
電極に対するリード線の接続強度が小さくなるこ
とにつながる。放電灯への組み込みを考慮した場
合、前記端子板の直径は少なくとも3mm以上にす
る必要がある。前記実験において端子板の直径を
3mmとした場合、第1表から明らかなようにパル
スピーク値は2000Vであり、高圧ナトリウムラン
プを始動させることは可能である。 ところが、かかる端子板を具えたコンデンサー
素子を実際に放電灯の外球内部に組み込んで使用
したところ、フレオン液中の動作ではみられなか
つた不都合な現象が発生した。すなわち、基板の
両面に接着した端子板間で耐圧不良によるスパー
クが頻発した。この原因は、強誘電体セラミツク
コンデンサーの基板自体の機械的振動の抵抗とな
る媒体がないため、振動を抑える端子板接着部に
応力が集中して、その部分にクラツクが入り、そ
こにスパークが生ずるものと考えられる。また、
コンデンサー素子を組み込む外球の内部が真空で
あると、コンデンサー素子の縁面に放電が生じた
り、放電灯の点灯に伴う高温によりコンデンサー
基体中の酸素がうばわれてコンデンサー素子の固
有抵抗が低下する等の不都合も生ずる。 そこで、発明者等はコンデンサー素子の構造を
以下のように工夫してみた。 先ず、前記実験と同様に、チタン酸バリウムを
主体とする材料で、直径26mm、厚み0.5mmの基体
を形成した。次にこの基体の両面に銀ペーストを
スクリーン印刷で直径25.7mmに塗布し、750℃の
温度で気中焼成して電極を形成した。次いで第4
図に示すように、基体14及び電極15a,15
bの周囲を電極15a,15bの中心部の直径2
mmだけを除いて、低融点ガラスペースト16で完
全にオーバーコートし、乾燥させた後、550℃の
温度で気中焼成を行つて基体の周囲を無機質ガラ
スで被覆した。次に、第5図に示すように、無機
質ガラスの非被覆部分の外側に該非被覆部分の面
積より大きい面積を有する第2図に示すごとき構
造の端子板12a,12bを当てがい、これを導
電性ガラスペースト17a,17bによつて電極
15a,15bに接着したうえ、約500℃の温度
で気中焼成を行つて固定した。 このように構成したコンデンサー素子を前記実
験と同様に第3図に示すような回路に接続し、フ
レオン液中で交流200V、50Hzの入力を加えて、
常温におけるパルスピーク電圧を測定した。第2
表はそのときのリード線端子板の直径とパルスピ
ーク電圧の関係を示すものである。
[Table] As is clear from Table 1, the diameter of the terminal plate is 2
When it exceeds mm, the pulse peak voltage tends to decrease rapidly. This is thought to be because the terminal plate and the conductive glass adhesive suppress vibrations in the diametrical direction of the ferroelectric ceramic plate, and for this reason it is desirable to make the area of the lead wire terminal plate as small as possible. However, reducing the area of the terminal plate leads to a reduction in the connection strength of the lead wires to the ferroelectric ceramic plate and the electrodes. When considering incorporation into a discharge lamp, the diameter of the terminal plate needs to be at least 3 mm or more. In the above experiment, when the diameter of the terminal plate was 3 mm, the pulse peak value was 2000 V, as is clear from Table 1, and it was possible to start the high pressure sodium lamp. However, when a capacitor element equipped with such a terminal plate was actually incorporated into the outer bulb of a discharge lamp and used, an inconvenient phenomenon occurred that was not observed when operating in Freon liquid. That is, sparks frequently occurred between the terminal plates bonded to both sides of the board due to poor voltage resistance. The reason for this is that the ferroelectric ceramic capacitor substrate itself does not have a medium to resist mechanical vibrations, so stress concentrates on the bonded area of the terminal board that suppresses vibrations, causing cracks in that area and sparks. This is considered to occur. Also,
If the inside of the outer bulb in which the capacitor element is installed is in a vacuum, discharge will occur on the edge of the capacitor element, and the high temperatures associated with lighting a discharge lamp will eat away the oxygen in the capacitor base, reducing the specific resistance of the capacitor element. Other inconveniences may also occur. Therefore, the inventors devised the structure of the capacitor element as follows. First, similarly to the experiment described above, a substrate having a diameter of 26 mm and a thickness of 0.5 mm was formed from a material mainly consisting of barium titanate. Next, silver paste was applied to both sides of this substrate by screen printing to a diameter of 25.7 mm, and then baked in air at a temperature of 750°C to form electrodes. Then the fourth
As shown in the figure, the base 14 and electrodes 15a, 15
The circumference of b is the diameter 2 of the center of electrodes 15a and 15b.
The substrate was completely overcoated with the low melting point glass paste 16, except for only the mm, and after drying, baking was performed in air at a temperature of 550° C. to cover the periphery of the substrate with inorganic glass. Next, as shown in FIG. 5, terminal plates 12a and 12b having a structure as shown in FIG. 2 and having an area larger than the area of the non-coated portion of the inorganic glass are placed on the outside of the non-coated portion of the inorganic glass, and this is made conductive. The electrodes 15a and 15b were adhered to each other using glass pastes 17a and 17b, and then baked in air at a temperature of about 500° C. to fix them. The capacitor element constructed in this way was connected to the circuit shown in Figure 3 in the same way as in the previous experiment, and an input of AC 200 V and 50 Hz was applied in Freon liquid.
Pulse peak voltage was measured at room temperature. Second
The table shows the relationship between the diameter of the lead wire terminal plate and the pulse peak voltage at that time.

【表】 第2表から明らかなように、第5図に示すよう
な構造にすると、リード線端子板の直径が2.5mm
〜5mmの範囲ではパルスピーク電圧の値が極めて
安定しており、しかも端子板を直接コンデンサー
基体に接着した場合に比較して、端子板直径を大
きくしても高いパルスピーク値が得られる。この
ことは、パルスピーク値を下げることなくリード
線の接続強度を高め得ることを意味している。因
みに、上記構造によると、放電灯への組み込みを
考慮してリード線端子板の直径を3mmとした場合
のパルスピーク値は2500Vであり、この値は、高
圧ナトリウムランプを確実に始動させるのに十分
な値である。また、上記構造によるとコンデンサ
ー素子の基体は無機質ガラスで完全に被覆された
形となつているので、これを放電灯の外球の中に
組み込んだ場合にも、耐熱性は大きく、縁面放電
も生じにくく、さらにはコンデンサー基体中の酸
素がうばわれて固有抵抗が低下するといつた現象
も防ぐことができる。 前記のような構成の非線形コンデンサー素子を
有するパルス発生器を360Wの高圧ナトリウムラ
ンプに実施して点滅テストを行つたが、5000回以
上の始動において、ランプは確実に始動し、しか
もコンデンサー素子の接続端子部に放電破壊が生
ずることなく、耐振性も十分であつた。 以上の説明から明らかなように、本発明は、誘
導性素子と非線形コンデンサー素子とからなるパ
ルス発生器において、前記非線形コンデンサー素
子として、強誘電体セラミツク基板の表面に電極
を被着し、これら全体を前記電極に対する通電部
を除いて無機質ガラスで完全に被覆するととも
に、前記無機質ガラスの非被覆部分に該非被覆部
分の面積より大きい面積を有する端子板を設置し
てこれを導電性ガラスにより電極に接着したう
え、端子板にリード線を接続した構造のものを使
用することを特徴としており、これにより、先に
述べたような種々の効果を得ることができるもの
である。
[Table] As is clear from Table 2, if the structure shown in Figure 5 is used, the diameter of the lead wire terminal plate will be 2.5 mm.
In the range of ~5 mm, the value of the pulse peak voltage is extremely stable, and even if the terminal plate diameter is increased, a higher pulse peak value can be obtained compared to when the terminal plate is directly bonded to the capacitor substrate. This means that the connection strength of the lead wires can be increased without reducing the pulse peak value. Incidentally, according to the above structure, the pulse peak value is 2500V when the diameter of the lead wire terminal plate is 3 mm in consideration of incorporation into a discharge lamp, and this value is sufficient to reliably start a high-pressure sodium lamp. It is a sufficient value. In addition, according to the above structure, the base of the capacitor element is completely covered with inorganic glass, so even when it is incorporated into the outer bulb of a discharge lamp, it has great heat resistance, and the edge surface discharge Furthermore, it is possible to prevent the occurrence of oxygen in the capacitor substrate and a decrease in specific resistance. A pulse generator with a nonlinear capacitor element configured as described above was used in a 360W high-pressure sodium lamp to perform a flashing test, and the lamp started reliably after more than 5,000 starts, and the connection of the capacitor element was No discharge damage occurred in the terminal portion, and the vibration resistance was sufficient. As is clear from the above description, the present invention provides a pulse generator comprising an inductive element and a nonlinear capacitor element, in which an electrode is adhered to the surface of a ferroelectric ceramic substrate as the nonlinear capacitor element, and is completely covered with inorganic glass except for the current-carrying part to the electrode, and a terminal plate having an area larger than the area of the non-covered part is installed in the non-covered part of the inorganic glass, and this is connected to the electrode with conductive glass. It is characterized by the use of a structure in which lead wires are connected to the terminal board in addition to bonding, and thereby the various effects described above can be obtained.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本発明に係るパルス発生器を具備し
た高圧金属蒸気放電灯の回路図、第2図はパルス
発生器のコンデンサー素子に使用するリード線端
子板の斜視図、第3図はパルス発生器の試験回路
図、第4図は本発明に係るパルス発生器に用いる
コンデンサー素子の完成途中の断面図、第5図は
同じく完成後の断面図である。
Fig. 1 is a circuit diagram of a high-pressure metal vapor discharge lamp equipped with a pulse generator according to the present invention, Fig. 2 is a perspective view of a lead wire terminal plate used for a capacitor element of the pulse generator, and Fig. 3 is a circuit diagram of a high-pressure metal vapor discharge lamp equipped with a pulse generator according to the present invention. A test circuit diagram of the generator, FIG. 4 is a cross-sectional view of a capacitor element used in the pulse generator according to the present invention during completion, and FIG. 5 is a cross-sectional view of the capacitor element after completion.

Claims (1)

【特許請求の範囲】[Claims] 1 誘導性素子と非線形コンデンサー素子とから
なるパルス発生器において、前記非線形コンデン
サー素子は、強誘電体セラミツク基板の両面に金
属膜からなる電極を被着し、これら全体を前記電
極に対する通電部を除いて無機質ガラスで完全に
被覆するとともに、前記無機質ガラスの非被覆部
分の外側に該非被覆部分の面積より大きい面積を
有する端子板を設置してこれを導電性ガラスによ
り電極に接着したうえ、該端子板にリード線を接
続した構成であることを特徴とするパルス発生
器。
1. In a pulse generator consisting of an inductive element and a nonlinear capacitor element, the nonlinear capacitor element has electrodes made of a metal film adhered to both sides of a ferroelectric ceramic substrate, and the entire structure is made of a ferroelectric ceramic substrate, except for the current-carrying part to the electrode. At the same time, a terminal plate having an area larger than the area of the uncoated part is installed outside the uncoated part of the inorganic glass, and this is adhered to the electrode with conductive glass. A pulse generator characterized by having a structure in which a lead wire is connected to a plate.
JP58159582A 1983-08-31 1983-08-31 pulse generator Granted JPS6052007A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58159582A JPS6052007A (en) 1983-08-31 1983-08-31 pulse generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58159582A JPS6052007A (en) 1983-08-31 1983-08-31 pulse generator

Publications (2)

Publication Number Publication Date
JPS6052007A JPS6052007A (en) 1985-03-23
JPS6260804B2 true JPS6260804B2 (en) 1987-12-18

Family

ID=15696858

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58159582A Granted JPS6052007A (en) 1983-08-31 1983-08-31 pulse generator

Country Status (1)

Country Link
JP (1) JPS6052007A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63296209A (en) * 1987-05-28 1988-12-02 Iwasaki Electric Co Ltd Nonlinear capacitor for generation of high-voltage pulse
JPH03134997A (en) * 1989-10-20 1991-06-07 Iwasaki Electric Co Ltd metal vapor discharge lamp

Also Published As

Publication number Publication date
JPS6052007A (en) 1985-03-23

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