JPH0228307A - Power supply - Google Patents
Power supplyInfo
- Publication number
- JPH0228307A JPH0228307A JP1130073A JP13007389A JPH0228307A JP H0228307 A JPH0228307 A JP H0228307A JP 1130073 A JP1130073 A JP 1130073A JP 13007389 A JP13007389 A JP 13007389A JP H0228307 A JPH0228307 A JP H0228307A
- Authority
- JP
- Japan
- Prior art keywords
- capacitance
- less
- ceramic
- power supply
- dielectric
- 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.)
- Granted
Links
- 239000003985 ceramic capacitor Substances 0.000 claims abstract description 28
- VEALVRVVWBQVSL-UHFFFAOYSA-N strontium titanate Chemical compound [Sr+2].[O-][Ti]([O-])=O VEALVRVVWBQVSL-UHFFFAOYSA-N 0.000 claims abstract description 18
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 claims abstract description 7
- 230000005684 electric field Effects 0.000 claims abstract description 7
- 229910052746 lanthanum Inorganic materials 0.000 claims abstract description 5
- FZLIPJUXYLNCLC-UHFFFAOYSA-N lanthanum atom Chemical compound [La] FZLIPJUXYLNCLC-UHFFFAOYSA-N 0.000 claims abstract description 5
- JRPBQTZRNDNNOP-UHFFFAOYSA-N barium titanate Chemical compound [Ba+2].[Ba+2].[O-][Ti]([O-])([O-])[O-] JRPBQTZRNDNNOP-UHFFFAOYSA-N 0.000 claims description 11
- 229910002113 barium titanate Inorganic materials 0.000 claims description 11
- 238000010438 heat treatment Methods 0.000 claims description 9
- 230000006698 induction Effects 0.000 claims description 9
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 claims description 6
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims description 4
- 239000000654 additive Substances 0.000 claims description 4
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 claims description 3
- 230000000996 additive effect Effects 0.000 claims description 3
- 229910052804 chromium Inorganic materials 0.000 claims description 3
- 239000011651 chromium Substances 0.000 claims description 3
- 229910017052 cobalt Inorganic materials 0.000 claims description 3
- 239000010941 cobalt Substances 0.000 claims description 3
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 claims description 3
- WPBNNNQJVZRUHP-UHFFFAOYSA-L manganese(2+);methyl n-[[2-(methoxycarbonylcarbamothioylamino)phenyl]carbamothioyl]carbamate;n-[2-(sulfidocarbothioylamino)ethyl]carbamodithioate Chemical compound [Mn+2].[S-]C(=S)NCCNC([S-])=S.COC(=O)NC(=S)NC1=CC=CC=C1NC(=S)NC(=O)OC WPBNNNQJVZRUHP-UHFFFAOYSA-L 0.000 claims description 3
- 239000000463 material Substances 0.000 claims description 3
- 229910052751 metal Inorganic materials 0.000 claims description 3
- 239000002184 metal Substances 0.000 claims description 3
- 150000002739 metals Chemical class 0.000 claims description 3
- 229910052759 nickel Inorganic materials 0.000 claims description 3
- 229910052761 rare earth metal Inorganic materials 0.000 claims description 3
- 229910052742 iron Inorganic materials 0.000 claims description 2
- 229910052758 niobium Inorganic materials 0.000 claims description 2
- 239000010955 niobium Substances 0.000 claims description 2
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 claims description 2
- 239000000919 ceramic Substances 0.000 abstract description 34
- 230000005611 electricity Effects 0.000 abstract description 6
- 239000003989 dielectric material Substances 0.000 abstract description 2
- XBYNNYGGLWJASC-UHFFFAOYSA-N barium titanium Chemical compound [Ti].[Ba] XBYNNYGGLWJASC-UHFFFAOYSA-N 0.000 abstract 1
- 230000006866 deterioration Effects 0.000 abstract 1
- 230000007423 decrease Effects 0.000 description 8
- 239000003990 capacitor Substances 0.000 description 5
- FYYHWMGAXLPEAU-UHFFFAOYSA-N Magnesium Chemical compound [Mg] FYYHWMGAXLPEAU-UHFFFAOYSA-N 0.000 description 3
- GWEVSGVZZGPLCZ-UHFFFAOYSA-N Titan oxide Chemical compound O=[Ti]=O GWEVSGVZZGPLCZ-UHFFFAOYSA-N 0.000 description 3
- AOWKSNWVBZGMTJ-UHFFFAOYSA-N calcium titanate Chemical compound [Ca+2].[O-][Ti]([O-])=O AOWKSNWVBZGMTJ-UHFFFAOYSA-N 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 229910052839 forsterite Inorganic materials 0.000 description 3
- 229910052749 magnesium Inorganic materials 0.000 description 3
- 239000011777 magnesium Substances 0.000 description 3
- HCWCAKKEBCNQJP-UHFFFAOYSA-N magnesium orthosilicate Chemical compound [Mg+2].[Mg+2].[O-][Si]([O-])([O-])[O-] HCWCAKKEBCNQJP-UHFFFAOYSA-N 0.000 description 3
- OGIDPMRJRNCKJF-UHFFFAOYSA-N titanium oxide Inorganic materials [Ti]=O OGIDPMRJRNCKJF-UHFFFAOYSA-N 0.000 description 3
- 229910000831 Steel Inorganic materials 0.000 description 2
- MRELNEQAGSRDBK-UHFFFAOYSA-N lanthanum(3+);oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[La+3].[La+3] MRELNEQAGSRDBK-UHFFFAOYSA-N 0.000 description 2
- 230000008018 melting Effects 0.000 description 2
- 238000002844 melting Methods 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 238000009958 sewing Methods 0.000 description 2
- 239000010959 steel Substances 0.000 description 2
- 239000011230 binding agent Substances 0.000 description 1
- 229910000420 cerium oxide Inorganic materials 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000004927 clay Substances 0.000 description 1
- 229910052570 clay Inorganic materials 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
- 238000001035 drying Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000003822 epoxy resin Substances 0.000 description 1
- 230000005621 ferroelectricity Effects 0.000 description 1
- 238000010304 firing Methods 0.000 description 1
- 235000013305 food Nutrition 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- UQSXHKLRYXJYBZ-UHFFFAOYSA-N iron oxide Inorganic materials [Fe]=O UQSXHKLRYXJYBZ-UHFFFAOYSA-N 0.000 description 1
- 235000013980 iron oxide Nutrition 0.000 description 1
- VBMVTYDPPZVILR-UHFFFAOYSA-N iron(2+);oxygen(2-) Chemical class [O-2].[Fe+2] VBMVTYDPPZVILR-UHFFFAOYSA-N 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- BMMGVYCKOGBVEV-UHFFFAOYSA-N oxo(oxoceriooxy)cerium Chemical compound [Ce]=O.O=[Ce]=O BMMGVYCKOGBVEV-UHFFFAOYSA-N 0.000 description 1
- 239000003973 paint Substances 0.000 description 1
- 229920000647 polyepoxide Polymers 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 238000005476 soldering Methods 0.000 description 1
- -1 steatite Chemical compound 0.000 description 1
- 229910052712 strontium Inorganic materials 0.000 description 1
- CIOAGBVUUVVLOB-UHFFFAOYSA-N strontium atom Chemical compound [Sr] CIOAGBVUUVVLOB-UHFFFAOYSA-N 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 229920003002 synthetic resin Polymers 0.000 description 1
- 239000000057 synthetic resin Substances 0.000 description 1
- 238000003466 welding Methods 0.000 description 1
- 239000002023 wood Substances 0.000 description 1
Landscapes
- General Induction Heating (AREA)
- Control Of High-Frequency Heating Circuits (AREA)
- Compositions Of Oxide Ceramics (AREA)
- Ceramic Capacitors (AREA)
- Inorganic Insulating Materials (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、電源装置に関するもの、さらに詳しくいえば
、高周波の発振、共振または結合の電気回路の部材にチ
タン酸ストロンチウム系セラミックコンデンサを用いた
電源装置に関するものである。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a power supply device, and more specifically, to a power supply device using a strontium titanate ceramic capacitor as a member of an electric circuit for high frequency oscillation, resonance or coupling. This relates to power supplies.
木材、樹脂、塗料1食品、衣類などの高周波乾燥や衣類
の高周波ミシンなどの誘電加熱、あるいは、鉄鋼の高周
波焼入れ、金属、ガラスなどの高周波熔融、または高周
波熔融などの誘導加熱の用途に対しては、その電源の回
路に一部セラミックコンデンサが使用されている。For use in induction heating for wood, resin, paint 1, high frequency drying of foods, clothing, etc., high frequency sewing machines for clothing, induction heating for steel, induction hardening of steel, high frequency melting of metals, glass, etc. uses some ceramic capacitors in its power supply circuit.
セラミックコンデンサは、熱的、化学的に安定である、
小形化し得る等の他に、コンデンサの構造が極めて簡単
なため、高周波で使い易い。Ceramic capacitors are thermally and chemically stable;
In addition to being compact, the structure of the capacitor is extremely simple, making it easy to use at high frequencies.
通常、セラミックコンデンサとしてはフォルステライト
系、ステアタイト系、チタン酸マグネシウム系、酸化チ
タン系、チタン酸カルシウム系などのセラミックスが用
いられているが、これらのセラミックスは誘電率が小さ
いためにある程度の電源出力を確保する上にあっては電
源装置が大形化せざるを得ない。Ceramic capacitors usually use forsterite-based, steatite-based, magnesium titanate-based, titanium oxide-based, calcium titanate-based ceramics, etc., but these ceramics have a low dielectric constant, so they can be used as a power source to some extent. In order to secure the output, the power supply device has to be larger.
近年、前記の各種用途の電源に関し、できるだけ大出力
化もしくは小形化が要望されて来ている。In recent years, there has been a demand for power supplies for the various uses mentioned above to be as large in output as possible or as compact as possible.
この要望に応えるために、高誘電率の例えばチタン酸バ
リウム系のセラミックスを誘電体とするセラミックコン
デンサを、前記各種用途の電源の回路部材として使用す
ることを検討して来た。その結果は、従来の高誘電率系
のセラミックスでは、使用中の温度上昇がはげしく、ま
たは課電時の電源出力が計算通りにとれないなどの問題
点があり、高周波の小電力の範囲に限定して使用せざる
を得なかった。本発明者らは、この原因は、これら従来
の高誘電率系のセラミックスが強誘電性であることによ
ることを突き止め、これを常誘電性又は程度の低い強誘
電性のものに置き換えることによってその問題点を克服
しうろことを見いだし、この知見に基づいて本発明をな
すに至った。In order to meet this demand, studies have been conducted on the use of ceramic capacitors whose dielectric material is a ceramic having a high dielectric constant, such as barium titanate, as a circuit member of a power source for the various uses mentioned above. As a result, conventional high-permittivity ceramics have problems such as rapid temperature rise during use or inability to obtain power output as calculated when applying electricity, and are limited to high-frequency, low-power ranges. I had no choice but to use it. The present inventors discovered that the cause of this is that these conventional high-permittivity ceramics are ferroelectric, and by replacing them with paraelectric or less ferroelectric materials. We have found a way to overcome these problems, and based on this knowledge, we have accomplished the present invention.
〔発明が解決しようとする課題〕
すなわち、本発明は、セラミックコンデンサとしてチタ
ン酸ストロンチウム系セラミックスを用いた、セラミッ
クコンデンサを前記回路の部材とする高周波誘電または
高周波誘導を用途とする電源装置を堤供するものである
0本発明において、チタン酸ストロンチウム系セラミッ
クスを用いたことにより上述した問題点である、使用中
の温度上昇を小さくするとともに、課電時の電源出力も
計算通りに近くとれ、さらに前記各種の電源の大出力も
しくは小形化を達成することができた。これらについて
、次に遂次、説明したい。[Problems to be Solved by the Invention] That is, the present invention provides a power supply device using strontium titanate ceramics as a ceramic capacitor and using the ceramic capacitor as a member of the circuit for high-frequency dielectric or high-frequency induction. In the present invention, by using strontium titanate ceramics, the temperature rise during use, which is the problem mentioned above, can be reduced, and the power output when applying electricity can be obtained close to the calculated value. We were able to achieve high output or miniaturization of various power supplies. I would like to explain these in turn.
セラミックコンデンサの使用中の温度上昇はセラミック
スの高周波誘電体損失が小さいほど低く押さえられる。The temperature rise during use of a ceramic capacitor can be suppressed as the high frequency dielectric loss of the ceramic is smaller.
これまでのフォルステライト系ステアタイト系5チタン
酸マグネシウム系、酸化チタン系、チタン酸カルシウム
系などのセラミックスの高周波誘電体損失は何れも0.
1%以下のものが上記各種用途の電源の回路部材として
実用化されている。一方、電源の大出力化もしくは小形
化のためにはセラミックスは誘電率が高いことが必要で
あるが、この高誘電率系セラミックスの中で高周波誘電
損失を0.1%以下のもので上記各種セラミックス並み
のものを見い出すことはむずかしく、現状では前述した
ように従来の高周波誘電体損失が大きい高誘電率系のセ
ラミックスを使用する限定した高周波の小電力の範囲に
留まざるを得ない、一方、本発明者らは、これまでチタ
ン酸ストロンチウム系セラミックスを研究して来たが、
このセラミックスが最近ではその高周波誘電体損失が0
.1%以下であるものが可能であり、このセラミックス
を使用することによって、はじめて上記各種用途の使用
中の温度上昇を低く押えることに成功した。なお、この
セラミックスは、高周波誘電体損失は、0.1%以下、
また組成を適当に選択すれば0.03%以下にまで小さ
(することができる、また、高周波誘電体損失は、その
コンデンサの使用寿命に大きく関係し、できるだけ小さ
いことがのぞましいので、この点でも有利である。The high-frequency dielectric loss of conventional ceramics such as forsterite, steatite, magnesium pentatitanate, titanium oxide, and calcium titanate is 0.
Those with a content of 1% or less have been put into practical use as circuit members for power supplies for the various uses mentioned above. On the other hand, ceramics need to have a high dielectric constant in order to increase the output power or downsize the power supply. It is difficult to find something comparable to ceramics, and at present, as mentioned above, we have no choice but to limit ourselves to the limited high-frequency, low-power range using high-permittivity ceramics, which have a large high-frequency dielectric loss. The present inventors have been researching strontium titanate ceramics, but
Recently, this ceramic has been developed with a high frequency dielectric loss of 0.
.. 1% or less, and by using this ceramic, we have succeeded for the first time in suppressing the temperature rise during use in the various applications mentioned above. In addition, this ceramic has a high frequency dielectric loss of 0.1% or less.
In addition, if the composition is appropriately selected, it can be reduced to 0.03% or less. Also, high-frequency dielectric loss is greatly related to the service life of the capacitor, and it is desirable that it be as small as possible. It's advantageous.
次に、課電時の電源出力について説明したい。Next, I would like to explain the power output when charging.
上記各種用途の電源の出力は使用するセラミックコンデ
ンサに課電される電圧の自乗とその課電時の静電容量の
積に比例する。従って、電源出力を大きくするには、f
f1ift圧を大きくすることがまず必要である。しか
るに、従来の高誘電率系セラミックスは課電時の静電容
量が著しく低下するという欠点があり、この欠点からも
、従来の高誘電率系セラミックスを使用すると、限定し
た高周波の小電力の範囲に留まらざろを得ない、近年、
前記の各種電源に関し、できるだけ電源出力の電圧を高
(することが要望され、回路設計の都合上、コンデンサ
の能力の最上限まで電圧を印加することが、しばしば必
要とされるようになったため、上記の欠点の改善がこの
分野の重要な課題となってきている0本発明者らは、こ
の欠点の原因が、従来の高誘電率系セラミックスが強誘
電性であることによるとみて、この場合も常誘電性また
は程度の低い強誘電性のチタン酸ストロンチウム系セラ
ミックスであれば解決できることを見い出した。The output of the power supply for the above various uses is proportional to the product of the square of the voltage applied to the ceramic capacitor used and the capacitance at the time of application. Therefore, in order to increase the power output, f
It is first necessary to increase the f1ift pressure. However, conventional high-permittivity ceramics have the disadvantage of a significant decrease in capacitance when electricity is applied, and due to this disadvantage, when conventional high-permittivity ceramics are used, they cannot be used within a limited high-frequency, low-power range. In recent years, it has become difficult to stay in
Regarding the various power supplies mentioned above, there is a demand for the power output voltage to be as high as possible, and due to circuit design considerations, it is often necessary to apply a voltage up to the maximum capacity of the capacitor. Improvement of the above-mentioned drawbacks has become an important issue in this field.The present inventors believe that the cause of this drawback is that conventional high dielectric constant ceramics are ferroelectric. We have found that this problem can be solved by using strontium titanate ceramics that are paraelectric or have a low degree of ferroelectricity.
すなわち、これまでのフォルステライト系、ステアタイ
ト系、チタン酸マグネシウム系、酸化チタン系、チタン
酸カルシウム系などのセラミックスは、課電時の静電容
量の低下は無視できる程度であるが、本発明のチタン酸
ストロンチウム系セラミックスの課電時の静電容量の低
下、すなわち、静電容量の電圧の電圧依存率はIKV/
am誘電体厚さ当り0.5%以下に押えられ、温かに大
きい低下率を示すチタン酸バリウム系などの高誘電率系
セラミックスに比べ非常に優れていることが云える。In other words, with conventional forsterite-based, steatite-based, magnesium titanate-based, titanium oxide-based, and calcium titanate-based ceramics, the decrease in capacitance when electricity is applied is negligible, but the present invention The decrease in capacitance of strontium titanate ceramics when a voltage is applied, that is, the voltage dependence of the capacitance voltage is IKV/
It can be said that the dielectric constant is suppressed to 0.5% or less per am dielectric thickness, and is extremely superior to high dielectric constant ceramics such as barium titanate ceramics, which exhibit a large reduction rate in warm temperatures.
また、温度特性は、20℃における静電容量に対する8
5℃における静電容量の減少率を37%以下にすること
ができ、さらに、誘電率(または静電容量)の経時変化
が殆どなく優れている。従来の例えばチタン酸バリウム
系などの高誘電率系のセラミックスはこの経時変化が甚
だ大きく、上記各種用途の回路部材として適していない
ことが良く分る。In addition, the temperature characteristics are 8 for capacitance at 20°C.
The rate of decrease in capacitance at 5° C. can be made 37% or less, and furthermore, there is almost no change in dielectric constant (or capacitance) over time, which is excellent. It is well understood that conventional high dielectric constant ceramics such as barium titanate type ceramics exhibit extremely large changes over time and are not suitable as circuit members for the various uses mentioned above.
したがって、本発明の電源装置においては、比誘電率5
1O〜820、誘電体損失0.02%以下、静電容量の
電圧依存率IKV/m誘電体厚さの電界当り0.5%以
下を有し、かつ20℃における静電容量に対する85℃
における静電容量の減少率が37%以下であるチタン酸
ストロンチウム系セラミンクコンデンサを用いるもので
ある。Therefore, in the power supply device of the present invention, the dielectric constant is 5
1O~820, dielectric loss 0.02% or less, voltage dependence of capacitance IKV/m dielectric thickness per electric field 0.5% or less, and 85℃ for capacitance at 20℃
A strontium titanate-based ceramic capacitor with a capacitance reduction rate of 37% or less is used.
この発明は、チタン酸ストロンチウム20〜35モル%
とチタン酸ランタン5モル%とチタン酸バリウム60〜
75モル%とから成り、マンガン、ニオブ、クロム、ニ
ッケル、コバルト及び鉄の中から選ばれた金属の酸化物
と粘土質物と希土類元素酸化物の中から選ばれた少なく
とも1種の添加成分を含有し、比誘電率510〜820
.誘電体損失0.02%以下、静電容量の電圧依存率I
KV/w誘電体厚さの電界当り0.5%以下を有し、か
つ20℃における静電容量に対する85℃における静電
容量の減少率が37%以下であるチタン酸ストロンチウ
ム系セラミックコンデンサを用いた誘電または誘導加熱
用の電源装置である。This invention uses 20 to 35 mol% of strontium titanate.
and lanthanum titanate 5 mol% and barium titanate 60~
75 mol%, and contains at least one additive component selected from oxides of metals selected from manganese, niobium, chromium, nickel, cobalt, and iron, clayey materials, and oxides of rare earth elements. and relative dielectric constant 510~820
.. Dielectric loss 0.02% or less, voltage dependence ratio of capacitance I
Use a strontium titanate ceramic capacitor that has a KV/w dielectric thickness per electric field of 0.5% or less and a capacitance reduction rate of 37% or less at 85°C relative to the capacitance at 20°C. It is a power supply device for dielectric or induction heating.
本発明は比較的比誘電率が小さくても、高周波誘電体損
失も小さいため、使用中の温度上昇を極端に少なくする
ことができ、また課電時の静電容量の低下が小さいもの
である。Even though the present invention has a relatively small dielectric constant, the high-frequency dielectric loss is also small, so the temperature rise during use can be extremely reduced, and the capacitance decreases when electricity is applied. .
次に実施例によって、本発明をさらに詳細に説明する。 Next, the present invention will be explained in more detail with reference to Examples.
第1表に示すモル比でチタン酸ストロンチウム。Strontium titanate in the molar ratios shown in Table 1.
チタン酸ランタン、チタン酸バリウム及び必要な添加成
分を混合し、適当量のバインダーを加え、直径16.5
m、厚さ1fiの円板に加圧成形したのち約1200℃
で2時間焼成してセラミックスを得た。Mix lanthanum titanate, barium titanate, and necessary additives, add an appropriate amount of binder, and make a powder with a diameter of 16.5 mm.
1200℃ after pressure forming into a disc with a thickness of 1fi.
Ceramics were obtained by firing for 2 hours.
添加成分中の希土類元素酸化物は、誘電体損失をさらに
少なくするために添加されるものであり、例えば酸化セ
リウム、酸化ランタンなどが用いられる。この添加量は
、通常0.01〜10重量%の範囲内で選ばれる。The rare earth element oxide in the additive component is added to further reduce dielectric loss, and for example, cerium oxide, lanthanum oxide, etc. are used. The amount added is usually selected within the range of 0.01 to 10% by weight.
また、マンガン、二オフ、クロム、ニッケル。Also manganese, diopter, chromium, and nickel.
コバルト及び鉄の酸化物と粘度質物は、ち密な組織の焼
結体を形成させるために鉱化剤として添加されるもので
ありその添加量は、通常0.1〜0.5重量%の範囲内
で選ばれる。Cobalt and iron oxides and clay substances are added as mineralizers to form a sintered body with a dense structure, and the amount added is usually in the range of 0.1 to 0.5% by weight. selected within.
これらのセラミックスは、例えば第1図、第2図に示す
構造のセラミックコンデンサとして使用される。第1図
においてセラミックスlの両面にはそれぞれ端子2.2
′が電極3,3′を介してはんだ付等の手段で固着され
、その周囲全面にわたってエポキシ樹脂等の合成樹脂5
で被覆されている。4は連結具である。These ceramics are used, for example, as a ceramic capacitor having the structure shown in FIGS. 1 and 2. In Fig. 1, terminals 2 and 2 are provided on both sides of the ceramic l.
' is fixed by means such as soldering via the electrodes 3, 3', and a synthetic resin 5 such as epoxy resin is applied over the entire surrounding area.
covered with. 4 is a connector.
第1図に示す形状のセラミックコンデンサに加工し、そ
の特性を測定し、その結果を第1表に示す。A ceramic capacitor having the shape shown in FIG. 1 was processed and its characteristics were measured. The results are shown in Table 1.
第1表
なお、コンデンサ特性の数値は以下のようにして求めた
ものである。Table 1 Note that the numerical values of the capacitor characteristics were determined as follows.
(イ)比誘電率tan δは20℃、1MHzの条件下
で測定した値を示した。(a) The relative dielectric constant tan δ is a value measured under the conditions of 20° C. and 1 MHz.
(D) 1度特性は20℃における静電容量に対する8
5℃における静電容量の減少率として示した。(D) 1 degree characteristic is 8 for capacitance at 20℃
It is shown as the rate of decrease in capacitance at 5°C.
(ハ)電圧依存率は誘電体の厚さ1鶴について印加され
た電圧1にVの電界当りの静電容量の以下の割合として
示した。(c) The voltage dependence ratio is expressed as the following ratio of capacitance per electric field of 1 to 1 V applied to a dielectric thickness of 1.
この表から明らかなように、いずれも比誘電率510〜
820、誘電体損失0.02%以下、静電容量の電圧依
存率IKV/m誘電体厚さの電界当り0.5%以下、温
度特性37%以下である。As is clear from this table, the dielectric constant is 510~
820, dielectric loss is 0.02% or less, voltage dependence ratio of capacitance IKV/m per electric field of dielectric thickness is 0.5% or less, and temperature characteristic is 37% or less.
この例の中の試料−2により第2図の形状の高周波尖頭
値25にV、静電容flooOPFのセラミックコンデ
ンサを作成し、これを回路部材として高周波加熱電源を
作成した。A ceramic capacitor with a high frequency peak value of 25 V and a capacitance flooOPF having a shape shown in FIG. 2 was prepared using sample 2 in this example, and a high frequency heating power source was prepared using this as a circuit member.
周囲温度50℃において、上記コンデンサに90KVA
の電力を加え、その温度上昇率を測定した。At an ambient temperature of 50℃, the above capacitor has 90KVA.
electric power was applied, and the rate of temperature rise was measured.
その結果約2℃であった。As a result, the temperature was about 2°C.
次に、本発明のチタン酸ストロンチウム系セラミックコ
ンデンサの一例と、従来の高誘電率系の例えばチタン酸
バリウム系セラミックコンデンサとの特性の相違を添付
図面に従って説明する。Next, the difference in characteristics between an example of the strontium titanate ceramic capacitor of the present invention and a conventional high dielectric constant ceramic capacitor, such as a barium titanate ceramic capacitor, will be explained with reference to the accompanying drawings.
第3図は、電圧依存率すなわち印加電圧(Vkν)を誘
電体の厚さ(dm■)で除した数を横軸とし、静電容!
(C)を縦軸として両者の関係をプロットしたグラフ
であるが、これから明らかように、V/d=1において
比較すると、本発明のストロンチウム系セラミックコン
デンサ(A)の静電容量の低下率は従来の高誘電率系の
チタン酸バリウム系セラミックコンデンサ(B)に比べ
て著しく小さくなっている。In Figure 3, the horizontal axis is the voltage dependence ratio, that is, the number obtained by dividing the applied voltage (Vkν) by the thickness of the dielectric (dm■), and the capacitance!
This is a graph plotting the relationship between the two with (C) as the vertical axis.As is clear from this graph, when compared at V/d=1, the rate of decrease in capacitance of the strontium-based ceramic capacitor (A) of the present invention is It is significantly smaller than the conventional high dielectric constant barium titanate ceramic capacitor (B).
また、第4図は温度特性を、20℃における静電容量に
対する85℃における静電容量の変化率(減少率)とし
て示したものである。従来のチタン酸バリウム系セラミ
ックコンデンサ(B)はこれが55%と大きいのに対し
、本発明のチタン酸ストロンチウム系セラミックコンデ
ンサでは15%程度である。Further, FIG. 4 shows the temperature characteristics as a rate of change (rate of decrease) in capacitance at 85° C. with respect to capacitance at 20° C. While this is as high as 55% for the conventional barium titanate ceramic capacitor (B), it is about 15% for the strontium titanate ceramic capacitor of the present invention.
さらに、第5図は静電容量の経時片を示すグラフである
が、これによると本発明のチタン酸ストロンチウム系セ
ラミックコンデンサ(A)の経時変化が従来のチタン酸
バリウム系セラミックコンデンサ(B)よりも著しく少
ないことが分る。Furthermore, FIG. 5 is a graph showing the capacitance over time, and it shows that the change over time of the strontium titanate ceramic capacitor (A) of the present invention is greater than that of the conventional barium titanate ceramic capacitor (B). It can be seen that there are significantly fewer
このように、本発明においては、電源としてより大きい
電源出力を得ることが可能であり、かつ長期間にわたっ
て安定した出力を得ることができる。As described above, in the present invention, it is possible to obtain a larger power output as a power supply, and stable output can be obtained over a long period of time.
本発明に係る電源装置はセラミックコンデンサとしてチ
タン酸ストロンチウム、チタン酸ランタン、チタン酸バ
リウム系セラミックスを用い、比誘電率510〜820
、誘電体損失0.02%以下、静電容量の電圧依存率I
XV/m誘電体厚さの電界当り0.5%以下を有し、か
つ20℃における静電容量に対する85℃における静電
容量の減少率が37%以下のセラミックスを用いた電源
装置を特徴とする為に、高周波感応や高周波ミシン等の
誘導加熱あるいは高周波波焼入れ、高周波熔融、高周波
溶接等の誘導加熱用の電源装置として、電源の大出力化
及び小形化が可能となったもので工業上の利益に多大な
ものがある。The power supply device according to the present invention uses strontium titanate, lanthanum titanate, and barium titanate ceramics as a ceramic capacitor, and has a dielectric constant of 510 to 820.
, dielectric loss 0.02% or less, voltage dependence ratio of capacitance I
A power supply device using ceramics having an electric field of XV/m dielectric thickness of 0.5% or less and a reduction rate of capacitance at 85°C relative to capacitance at 20°C of 37% or less. In order to do this, it has become possible to increase the power output and make the power supply smaller, and it is used as a power supply device for induction heating such as high-frequency sensing and high-frequency sewing machines, or induction heating for high-frequency hardening, high-frequency melting, high-frequency welding, etc. There are huge profits.
第1図及び第2図は従来及び本発明に使用される高周波
誘電加熱、誘導加熱用セラミックコンデンサの断面図で
示す。
第3図は本発明の実施例で印加電圧に対する電圧依存率
の関係を示す図である
第4図は同じく本発明の実施例で温度に対する静電容量
変化りつ示す図である。
第5図は同じく本発明の実施例で静電容量の経時変化を
示す図である。
特許出願人 ティーデイ−ケイ株式会社代理人
弁理士 薬 師 稔0発
0発
東京都中f
式会社内
東京都中f
式会社内
処区日本橋1丁目13番1号
ティーデイ−ケイ株
処区日本橋1丁目13番1号
ティーデイ−ケイ株1 and 2 are cross-sectional views of ceramic capacitors for high frequency dielectric heating and induction heating used conventionally and in the present invention. FIG. 3 is a diagram showing the relationship between the voltage dependence ratio and the applied voltage in an embodiment of the present invention. FIG. 4 is a diagram showing the change in capacitance with respect to temperature in the same embodiment of the present invention. FIG. 5 is a diagram showing the change in capacitance over time in the same example of the present invention. Patent Applicant: TDC Co., Ltd. Agent
Patent Attorney Pharmacist Minoru 0 shots 0 Tokyo Chuo F. Shikisha Kaisha Chuo F. 1-13-1 Nihonbashi, Nihonbashi 1-chome, T.D.-K Co., Ltd.
Claims (1)
タン酸ランタン5モル%とチタン酸バリウム60〜75
モル%とから成り、マンガン,ニオブ,クロム,ニッケ
ル,コバルト及び鉄の中から選ぼれた金属の酸化物と粘
土質物と希土類元素酸化物の中から選ばれた少なくとも
1種の添加成分を含有し、比誘電率510〜820、誘
電体損失0.02%以下、静電容量の電圧依存率1KV
/mm誘電体厚さの電界当り0.5%以下を有し、かつ
20℃における静電容量に対する85℃における静電容
量の減少率が37%以下であるチタン酸ストロンチウム
系セラミックコンデンサを用いた誘電または誘導加熱用
の電源装置。(1) Strontium titanate 20-35 mol%, lanthanum titanate 5 mol%, barium titanate 60-75 mol%
mol%, and contains at least one additive component selected from oxides of metals selected from manganese, niobium, chromium, nickel, cobalt, and iron, clayey materials, and oxides of rare earth elements. , relative dielectric constant 510-820, dielectric loss 0.02% or less, voltage dependence of capacitance 1KV
A strontium titanate-based ceramic capacitor was used, which has a dielectric thickness of 0.5% or less per electric field and a reduction rate of capacitance at 85°C relative to capacitance at 20°C of 37% or less. Power supplies for dielectric or induction heating.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1130073A JPH0228307A (en) | 1989-05-25 | 1989-05-25 | Power supply |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1130073A JPH0228307A (en) | 1989-05-25 | 1989-05-25 | Power supply |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10645281A Division JPS589315A (en) | 1981-07-08 | 1981-07-08 | Power source |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0228307A true JPH0228307A (en) | 1990-01-30 |
| JPH0376773B2 JPH0376773B2 (en) | 1991-12-06 |
Family
ID=15025348
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1130073A Granted JPH0228307A (en) | 1989-05-25 | 1989-05-25 | Power supply |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0228307A (en) |
-
1989
- 1989-05-25 JP JP1130073A patent/JPH0228307A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0376773B2 (en) | 1991-12-06 |
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