JPH0132647B2 - - Google Patents
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- Publication number
- JPH0132647B2 JPH0132647B2 JP5813981A JP5813981A JPH0132647B2 JP H0132647 B2 JPH0132647 B2 JP H0132647B2 JP 5813981 A JP5813981 A JP 5813981A JP 5813981 A JP5813981 A JP 5813981A JP H0132647 B2 JPH0132647 B2 JP H0132647B2
- Authority
- JP
- Japan
- Prior art keywords
- ceramic capacitor
- present
- pulse voltage
- voltage
- nonlinear
- 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
Links
- 239000003985 ceramic capacitor Substances 0.000 claims description 21
- 150000001339 alkali metal compounds Chemical class 0.000 claims description 6
- 239000000203 mixture Substances 0.000 claims description 6
- 229910052708 sodium Inorganic materials 0.000 claims description 2
- 229910018068 Li 2 O Inorganic materials 0.000 claims 1
- 229910052701 rubidium Inorganic materials 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 9
- 230000001939 inductive effect Effects 0.000 description 7
- 239000006104 solid solution Substances 0.000 description 7
- CSCPPACGZOOCGX-UHFFFAOYSA-N Acetone Chemical compound CC(C)=O CSCPPACGZOOCGX-UHFFFAOYSA-N 0.000 description 4
- JRPBQTZRNDNNOP-UHFFFAOYSA-N barium titanate Chemical compound [Ba+2].[Ba+2].[O-][Ti]([O-])([O-])[O-] JRPBQTZRNDNNOP-UHFFFAOYSA-N 0.000 description 4
- 229910002113 barium titanate Inorganic materials 0.000 description 4
- 229910052573 porcelain Inorganic materials 0.000 description 4
- 239000013078 crystal Substances 0.000 description 3
- ATUOYWHBWRKTHZ-UHFFFAOYSA-N Propane Chemical compound CCC ATUOYWHBWRKTHZ-UHFFFAOYSA-N 0.000 description 2
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 description 2
- 229910000288 alkali metal carbonate Inorganic materials 0.000 description 2
- 150000008041 alkali metal carbonates Chemical class 0.000 description 2
- 239000003990 capacitor Substances 0.000 description 2
- 239000000919 ceramic Substances 0.000 description 2
- 238000010304 firing Methods 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 239000002994 raw material Substances 0.000 description 2
- 239000007858 starting material Substances 0.000 description 2
- 229910052726 zirconium Inorganic materials 0.000 description 2
- DGAQECJNVWCQMB-PUAWFVPOSA-M Ilexoside XXIX Chemical compound C[C@@H]1CC[C@@]2(CC[C@@]3(C(=CC[C@H]4[C@]3(CC[C@@H]5[C@@]4(CC[C@@H](C5(C)C)OS(=O)(=O)[O-])C)C)[C@@H]2[C@]1(C)O)C)C(=O)O[C@H]6[C@@H]([C@H]([C@@H]([C@H](O6)CO)O)O)O.[Na+] DGAQECJNVWCQMB-PUAWFVPOSA-M 0.000 description 1
- 239000004698 Polyethylene Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- 229910010413 TiO 2 Inorganic materials 0.000 description 1
- 229910000272 alkali metal oxide Inorganic materials 0.000 description 1
- 239000011230 binding agent Substances 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- NKZSPGSOXYXWQA-UHFFFAOYSA-N dioxido(oxo)titanium;lead(2+) Chemical compound [Pb+2].[O-][Ti]([O-])=O NKZSPGSOXYXWQA-UHFFFAOYSA-N 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000008187 granular material Substances 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 1
- 229910052753 mercury Inorganic materials 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- -1 polyethylene Polymers 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 239000001294 propane Substances 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 239000011734 sodium Substances 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
Landscapes
- Ceramic Capacitors (AREA)
- Inorganic Insulating Materials (AREA)
Description
本発明はチタン酸バリウムを主成分とした強誘
電性磁器組成物よりなる非線形セラミツクコンデ
ンサに関するもので、誘導性素子との結合により
高電圧パルスを発生させることを特徴としたもの
である。
従来からパルス発生器として誘導性素子とペロ
ブスカイト形構造を有する非線形コンデンサとか
らなる構造のものが知られている。このペロブス
カイト形誘電体素子はチタン酸バリウム、チタン
酸鉛などの多結晶固溶体が有効であることが知ら
れている。しかし高いパルス電圧が再現性よく得
られない。またパルス電圧のバラツキが大きいな
どの欠点を有しており、かつまた室温より少し温
度が高くなるとパルス電圧が急激に低下するなど
の致命的な欠点があり実用上問題があつた。
本発明は高いパルス電圧が再現性よく、またパ
ルス電圧のバラツキが少なく、かつ広い温度範囲
で高いパルス電圧を有する非線形セラミツクコン
デンサを提供するものである。
すなわち、ペロブスカイト形結晶構造を有する
チタン酸バリウム固溶体にジルコニウムを含有さ
せ、アルカリ金属の化合物を微量添加することに
より、広い温度範囲で高いパルス電圧を再現性よ
く得られることを見い出したものである。
以下、本発明を実施例に基づき詳細に説明す
る。
出発原料としてBaCO3、TiO2、ZrO2、アルカ
リ金属炭酸塩を第1表に示す配合比でもつて計量
し、アセトン、メノウ玉石と共にポリエチレンポ
ツトで約16時間湿式混合し、濾過、乾燥して調整
原料を得た。これを1120℃で2時間仮焼しアセト
ン中でボールミル粉砕を16時間行ない、濾過、乾
燥した原料に有機結合材を約3.0重量%添加して
顆粒状として、1ton/cm2の圧力にて直径16.0mm
φ、厚み0.65mmの円板状に成形する。次いで1400
℃にて2時間焼成して得られた磁器に12.0mmφの
銀電極を塗布し、800℃にて30分間焼付けして非
線形セラミツクコンデンサ用の素子を得る。この
ようにして得られたコンデンサ素子につき、誘電
率、tanδ、絶縁抵抗(IR)パルス電圧の各電気
特性を測定し、その結果を第1表に示した。
The present invention relates to a nonlinear ceramic capacitor made of a ferroelectric ceramic composition containing barium titanate as a main component, and is characterized in that it generates high voltage pulses by coupling with an inductive element. BACKGROUND ART Conventionally, pulse generators having a structure consisting of an inductive element and a nonlinear capacitor having a perovskite structure have been known. It is known that polycrystalline solid solutions such as barium titanate and lead titanate are effective for this perovskite dielectric element. However, high pulse voltage cannot be obtained with good reproducibility. In addition, it has the disadvantage that the pulse voltage varies widely, and it also has the fatal disadvantage that the pulse voltage drops rapidly when the temperature is slightly higher than room temperature, which poses a practical problem. The present invention provides a nonlinear ceramic capacitor that has high pulse voltage with good reproducibility, has little variation in pulse voltage, and has high pulse voltage over a wide temperature range. In other words, it was discovered that by incorporating zirconium into a barium titanate solid solution having a perovskite crystal structure and adding a trace amount of an alkali metal compound, a high pulse voltage can be obtained with good reproducibility over a wide temperature range. Hereinafter, the present invention will be explained in detail based on examples. As starting materials, BaCO 3 , TiO 2 , ZrO 2 , and alkali metal carbonate were weighed at the mixing ratio shown in Table 1, wet-mixed with acetone and agate stones in a polyethylene pot for about 16 hours, filtered, and dried. I got the raw material. This was calcined at 1120°C for 2 hours, ball-milled in acetone for 16 hours, filtered, and dried. Approximately 3.0% by weight of an organic binder was added to the raw material to make it into granules, which were then pulverized to a diameter of 1 ton/cm 2 under a pressure of 1 ton/cm 2. 16.0mm
Form into a disk shape with a diameter of 0.65 mm and a thickness of 0.65 mm. then 1400
A silver electrode of 12.0 mmφ is coated on the porcelain obtained by firing at 800°C for 2 hours, and an element for a nonlinear ceramic capacitor is obtained by baking at 800°C for 30 minutes. The electrical characteristics of the capacitor element thus obtained were measured, including dielectric constant, tan δ, insulation resistance (IR), and pulse voltage, and the results are shown in Table 1.
【表】【table】
【表】
第1表において、試料番号11〜13、15、17〜
19、21〜23、25〜27、29〜38は本発明の範囲内を
示し、試料番号1〜10、14、16、20、24、28、
39、40は本発明の範囲外を示した。
なお、第1表に示した電気特性の測定に際し、
容量(誘電率)、tanδは周波数1KHz、1Vrmsで測
定し、絶縁抵抗(IR)は100VDCを30秒間印加後
の値である。またパルス電圧は第4図の回路によ
り測定したものである。
実施例において、出発原料にアルカリ金属の炭
酸塩を用いたが、アルカリ金属の他の化合物であ
つても同様の結果を期待することができ、アルカ
リ金属の酸化物の添加量は0.5重量%を越えると
パルス電圧が低く、パルス電圧は螢光灯点灯装置
の最良条件下で約400Vあれば点灯が可能であり、
特許請求の範囲の限定条件とした。またアルカリ
金属化合物を添加しない組成物においても0.01<
x<0.14の範囲でZrを固溶する系は良好な特性を
得られるが、アルカリ金属化合物を添加すること
により、さらに安定で良好な特性の磁器が得られ
る。
チタン酸バリウム固溶体(ABO3)において
A/B比が1.0近傍が最もパルス電圧が高く望ま
しいが、B過剰の場合焼成温度を低下できるのは
通常のセラミツクコンデンサと同様であり、逆に
A過剰の場合磁器体の結晶粒径は少し小さくなり
磁器体の機械的強度を増大させることができる。
本発明は上述のようにA/B比は1.0に限定す
るものではない。本発明の特徴はジルコニウムを
1〜14モル%固溶させた組成にアルカリ金属の化
合物を添加することにより、その優れた温度特性
を損うことなく、パルス電圧を増大させる点にあ
る。
本発明はBa(Ti1−x、Zrx)O3の多結晶固溶
体について説明したが、ペロブスカイト形結晶構
造を有する本組成においては、Baの一部にPb、
Sr、Caなど、またZrの一部にSnなどの固溶体成
分を置換しても同様な効果が期待できることは明
白である。
このようにして製作された本発明の非線形セラ
ミツクコンデンサを第1図のように誘導性素子1
と直列結合すると、第2図ロに示すようにパルス
波形が観測される。2は負荷抵抗、4は商用周波
数電源で、第2図イは商用周波数電圧波形図であ
る。
すなわち、本発明に係る非線形セラミツクコン
デンサは第3図に示すごとく良好な角形ヒステリ
シスを有し、電圧E0,−E0近傍で自発分極量であ
るD0の電荷が急変して充電電流が流れるが、電
圧がE0を越えてEsになると電荷量は飽和し、充
電電流は流れなくなる。この充電電流のスイツチ
ング作用のために誘導性素子より逆起電力に相応
する第2図ロのごとくパルス電圧が得られる。
第4図は本発明の非線形セラミツクコンデンサ
を用いた螢光灯の無接点起動用パルス発生器の回
路の実施例を示し、1は誘導性素子、3は本発明
に係る非線形セラミツク、4は商用周波数電源、
5は螢光灯、51,52は螢光灯フイラメント、6
はスイツチング回路で、スイツチング回路6によ
り第5図イに示すように非線形セラミツクコンデ
ンサに印加される電圧を調整すると、第5図ロに
示すように極めて高いパルス電圧を誘起し得るも
のである。
交流波形において、第5図イのEsのa点にて
スイツチング回路6はOFFとなり、−Esの電圧に
なる前にb点にてスイツチング回路6はONにな
るようにすると、第4図の誘導性素子1と非線形
セラミツクコンデンサによる誘起電圧(Ldi/dt)
は第5図ロに示すように極めて高いパルス電圧を
発生させ得る。
第5図イにおいてC点でスイツチング回路を
ONした場合、負方向にパルスを発生するため、
b点にてONする必要がある。また第5図ロの波
形が第4図の螢光灯の回路に印加された場合、破
線部分(b−a間)は誘導性素子1と螢光灯5の
フイラメント51,52のインピーダンスとなり、
螢光灯5のフイラメント51,52が加熱され、第
5図ロのa点のパルスにて放電が誘起され点灯す
るものである。
なお、パルス電圧および誘電率の温度特性は第
6図、第7図に示すごとく、従来の非線形セラミ
ツクコンデンサは高温度領域において高いパルス
電圧が得られず、また上限温度が30℃までと使用
温度範囲が狭く実用に耐えないものであつた。本
発明はこの上限温度を60〜80℃と拡大したもの
で、著しく使用用途の拡大ができるものである。
本発明に係る磁器組成を有する非線形セラミツ
クコンデンサは、従来から用いられている螢光灯
の点灯用に限らず、高圧パルスを必要とする、た
とえば都市ガス、プロパンガスの点火装置、水銀
灯、ナトリウムランプなどの放電灯の点灯起動回
路およびその他パルス発生器などの広い用途が考
えられ有益なものである。[Table] In Table 1, sample numbers 11-13, 15, 17-
19, 21-23, 25-27, 29-38 are within the scope of the present invention, sample numbers 1-10, 14, 16, 20, 24, 28,
Nos. 39 and 40 were outside the scope of the present invention. In addition, when measuring the electrical characteristics shown in Table 1,
Capacitance (permittivity) and tan δ are measured at a frequency of 1 KHz and 1 Vrms, and insulation resistance (IR) is the value after applying 100 VDC for 30 seconds. Further, the pulse voltage was measured using the circuit shown in FIG. In the examples, an alkali metal carbonate was used as the starting material, but similar results can be expected with other alkali metal compounds, and the amount of alkali metal oxide added was 0.5% by weight. If it exceeds this, the pulse voltage will be low, and under the best conditions for a fluorescent lamp lighting device, lighting can be achieved with a pulse voltage of about 400 V.
This is a limiting condition for the scope of the claims. In addition, even in compositions without adding alkali metal compounds, 0.01<
A system in which Zr is dissolved as a solid solution in the range of x<0.14 can obtain good properties, but by adding an alkali metal compound, porcelain with even more stable and good properties can be obtained. In barium titanate solid solution (ABO 3 ), the highest pulse voltage is desirable when the A/B ratio is around 1.0, but if there is an excess of B, the firing temperature can be lowered, just as in a normal ceramic capacitor; In this case, the crystal grain size of the porcelain body becomes slightly smaller and the mechanical strength of the porcelain body can be increased. In the present invention, the A/B ratio is not limited to 1.0 as described above. The feature of the present invention is that by adding an alkali metal compound to a composition containing 1 to 14 mol% of zirconium as a solid solution, the pulse voltage can be increased without impairing its excellent temperature characteristics. In the present invention, a polycrystalline solid solution of Ba(Ti 1 −x, Zrx)O 3 has been described, but in this composition having a perovskite crystal structure, a part of Ba contains Pb,
It is clear that similar effects can be expected by substituting Sr, Ca, etc., or a solid solution component such as Sn for a part of Zr. The nonlinear ceramic capacitor of the present invention manufactured in this way has an inductive element 1 as shown in FIG.
When connected in series, a pulse waveform as shown in FIG. 2B is observed. 2 is a load resistor, 4 is a commercial frequency power source, and FIG. 2A is a commercial frequency voltage waveform diagram. In other words, the nonlinear ceramic capacitor according to the present invention has good square hysteresis as shown in Fig. 3, and near the voltages E0 and -E0 , the charge of D0 , which is the amount of spontaneous polarization, changes suddenly and a charging current flows. However, when the voltage exceeds E 0 and reaches Es, the amount of charge is saturated and charging current no longer flows. Due to this switching action of the charging current, a pulse voltage is obtained from the inductive element as shown in FIG. 2B, which corresponds to the back electromotive force. FIG. 4 shows an embodiment of a pulse generator circuit for non-contact starting of a fluorescent lamp using the nonlinear ceramic capacitor of the present invention, in which 1 is an inductive element, 3 is a nonlinear ceramic capacitor according to the present invention, and 4 is a commercially available pulse generator. frequency power supply,
5 is a fluorescent lamp, 5 1 , 5 2 is a fluorescent lamp filament, 6
is a switching circuit which, when the switching circuit 6 adjusts the voltage applied to the nonlinear ceramic capacitor as shown in FIG. 5A, can induce an extremely high pulse voltage as shown in FIG. 5B. In the AC waveform, the switching circuit 6 is turned OFF at point a of Es in Figure 5A, and the switching circuit 6 is turned ON at point b before the voltage reaches -Es, resulting in the induction shown in Figure 4. The induced voltage (Ldi/dt) due to the magnetic element 1 and the nonlinear ceramic capacitor can generate an extremely high pulse voltage as shown in FIG. 5B. In Figure 5 A, connect the switching circuit at point C.
When turned on, pulses are generated in the negative direction, so
It is necessary to turn it on at point b. Furthermore, when the waveform shown in FIG. 5B is applied to the circuit of the fluorescent lamp shown in FIG . Then,
The filaments 5 1 and 5 2 of the fluorescent lamp 5 are heated, and a discharge is induced by the pulse at point a in FIG. 5B, causing the lamp to turn on. The temperature characteristics of pulse voltage and dielectric constant are shown in Figures 6 and 7. Conventional nonlinear ceramic capacitors cannot obtain high pulse voltage in the high temperature range, and the upper limit temperature is 30°C, which is the operating temperature. The range was too narrow to be practical. The present invention expands this upper limit temperature to 60 to 80°C, and can significantly expand the range of uses. The nonlinear ceramic capacitor having a ceramic composition according to the present invention is useful not only for lighting conventionally used fluorescent lamps, but also for lighting devices that require high-pressure pulses, such as city gas, propane gas igniters, mercury lamps, and sodium lamps. The present invention is useful for a wide range of applications, such as lighting starting circuits for discharge lamps such as the above, and other pulse generators.
第1図は本発明の非線形セラミツクコンデンサ
のパルス波形測定回路、第2図は第1図における
波形図を示し、イは商用周波数電圧波形図、ロは
本発明の非線形セラミツクコンデンサの両端にか
かる電圧波形図、第3図は本発明の非線形セラミ
ツクコンデンサのヒステリシス特性図、第4図は
本発明の非線形セラミツクコンデンサを用いた螢
光灯の無接点起動用パルス発生器の一実施例の回
路図、第5図は第4図の回路により印加されるパ
ルス電圧波形図で、イは本発明の非線形セラミツ
クコンデンサに印加される電圧波形、ロは誘導性
素子により誘起された電圧波形、第6図は誘導性
素子により誘起された非線形セラミツクコンデン
サのパルス電圧の温度特性図、第7図は非線形セ
ラミツクコンデンサの誘電率の温度特性図であ
る。
Figure 1 shows a pulse waveform measurement circuit for the nonlinear ceramic capacitor of the present invention, Figure 2 shows the waveform diagram in Figure 1, A is a commercial frequency voltage waveform diagram, and B is the voltage applied across the nonlinear ceramic capacitor of the present invention. A waveform diagram, FIG. 3 is a hysteresis characteristic diagram of the nonlinear ceramic capacitor of the present invention, and FIG. 4 is a circuit diagram of an embodiment of a pulse generator for non-contact starting of a fluorescent lamp using the nonlinear ceramic capacitor of the present invention. 5 is a pulse voltage waveform diagram applied by the circuit of FIG. 4, A is a voltage waveform applied to the nonlinear ceramic capacitor of the present invention, B is a voltage waveform induced by an inductive element, and FIG. FIG. 7 is a temperature characteristic diagram of the pulse voltage of a nonlinear ceramic capacitor induced by an inductive element, and FIG. 7 is a temperature characteristic diagram of the dielectric constant of the nonlinear ceramic capacitor.
Claims (1)
Zrx)O3にアルカリ金属化合物のうち少なくとも
一種を酸化物(Li2O、Na2O、K2O、Rb2O、
Cs2O)に換算して0.5重量%以下を含有してなる
ことを特徴とする非線形セラミツクコンデンサ。 ただし、x=0.01〜0.14 2 パルス発生器の起動用素子として用いること
を特徴とする特許請求の範囲第1項記載の非線形
セラミツクコンデンサ。[Claims] 1. Consists of a polycrystalline body whose composition is Ba(Ti 1 -x,
Zrx) O 3 with at least one alkali metal compound oxide (Li 2 O, Na 2 O, K 2 O, Rb 2 O,
A nonlinear ceramic capacitor characterized by containing 0.5% by weight or less of Cs 2 O). However, x=0.01 to 0.14 2 The nonlinear ceramic capacitor according to claim 1, which is used as a starting element of a pulse generator.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5813981A JPS57172716A (en) | 1981-04-16 | 1981-04-16 | Nonlinear ceramic capacitor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5813981A JPS57172716A (en) | 1981-04-16 | 1981-04-16 | Nonlinear ceramic capacitor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57172716A JPS57172716A (en) | 1982-10-23 |
| JPH0132647B2 true JPH0132647B2 (en) | 1989-07-10 |
Family
ID=13075649
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5813981A Granted JPS57172716A (en) | 1981-04-16 | 1981-04-16 | Nonlinear ceramic capacitor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57172716A (en) |
-
1981
- 1981-04-16 JP JP5813981A patent/JPS57172716A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57172716A (en) | 1982-10-23 |
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