JPS635876B2 - - Google Patents
Info
- Publication number
- JPS635876B2 JPS635876B2 JP11127583A JP11127583A JPS635876B2 JP S635876 B2 JPS635876 B2 JP S635876B2 JP 11127583 A JP11127583 A JP 11127583A JP 11127583 A JP11127583 A JP 11127583A JP S635876 B2 JPS635876 B2 JP S635876B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- semiconductor
- semiconductor switching
- induction heating
- switching element
- 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
- 239000004065 semiconductor Substances 0.000 claims description 36
- 238000010438 heat treatment Methods 0.000 claims description 35
- 239000003990 capacitor Substances 0.000 claims description 30
- 229910052751 metal Inorganic materials 0.000 claims description 18
- 239000002184 metal Substances 0.000 claims description 18
- 230000006698 induction Effects 0.000 claims description 17
- 230000000694 effects Effects 0.000 description 11
- 239000011347 resin Substances 0.000 description 11
- 229920005989 resin Polymers 0.000 description 11
- 239000004020 conductor Substances 0.000 description 8
- 238000010586 diagram Methods 0.000 description 8
- 238000001816 cooling Methods 0.000 description 7
- 230000005855 radiation Effects 0.000 description 5
- 230000007423 decrease Effects 0.000 description 4
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 3
- 238000010411 cooking Methods 0.000 description 3
- 230000005672 electromagnetic field Effects 0.000 description 3
- 230000002411 adverse Effects 0.000 description 2
- 229910052782 aluminium Inorganic materials 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 238000010292 electrical insulation Methods 0.000 description 2
- 230000005674 electromagnetic induction Effects 0.000 description 2
- 230000017525 heat dissipation Effects 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 230000004907 flux Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000004806 packaging method and process Methods 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、誘導加熱調理器に係り、特に内部の
高周波電力変換装置から外部に漏洩する電磁界、
特に、AMラジオ周波数帯域に於ける漏洩磁界を
低減する構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an induction heating cooker, and in particular to an electromagnetic field leaking to the outside from an internal high-frequency power converter.
In particular, it relates to a structure that reduces leakage magnetic fields in the AM radio frequency band.
従来例の構成とその問題点
従来、誘導加熱調理器は、高周波高磁束密度の
磁界を発生する加熱コイルと、その加熱コイルに
高周波大電流を供給する高周波電力変換装置を具
備しており、特に高周波電力変換装置の共振コン
デンサ、半導体スイツチング素子あるいは高周波
電源用フイルタコンデンサ等の高周波回路部品に
は、急峻な立ち上がり、下ち下がりをもつ大電流
が流れている。そのため高周波電力変換装置から
発生する漏洩磁界は、特にAMラジオの受信に防
害を与える。この漏洩磁界を低減するために、従
来、第1図に示すように、鍋載置板1の下に位置
する加熱コイル2を除いた高周波電力変換装置3
が配設されている導電材料でできた内部シヤーシ
4の上部全体をアルミ等の導電材料製のシールド
カバー5で覆うというような手段がとられてき
た。しかしこのような構造では、導電性シールド
カバー5に加熱コイル2の高密度高周波の磁界が
鎖交し、シールドカバー5に誘導電流が流れ、そ
こで熱損失が生じ、調理器の加熱効率を下げた
り、前記誘導電流が発する反磁界が加熱コイルの
等価インダクタンスを減じるため、加熱コイル巻
数をその分増やして補償することが、高周波電力
変換装置の設計上必要となつてくる。またシール
ドカバー5は導電体であるので、他の電気部品と
の電気絶縁を、確保するために、かなりの空間を
必要とする等の問題点があつた。これらの問題点
は、すべて、調理器の高さを低くする(薄型化を
はかる)際の深刻な制限項目となる。またシール
ドカバー5のように高周波電力変換装置全体を覆
う導電板を調理器内部に設けると、導電板が、加
熱コイル2や、負荷鍋底から受ける輻射熱によ
り、高温となり、機器内部の温度を上げてしま
い、半導体部品や、その他の電気部品の冷却に悪
影響を与えることとなり、それらの信頼性を損う
恐れがある。Conventional configuration and its problems Traditionally, induction heating cookers have been equipped with a heating coil that generates a magnetic field with high frequency and high magnetic flux density, and a high frequency power converter that supplies a high frequency large current to the heating coil. A large current with steep rises and drops flows through high-frequency circuit components such as resonant capacitors of high-frequency power converters, semiconductor switching elements, and filter capacitors for high-frequency power supplies. Therefore, the leakage magnetic field generated from the high-frequency power converter is particularly harmful to AM radio reception. In order to reduce this leakage magnetic field, conventionally, as shown in FIG.
Measures have been taken to cover the entire upper part of the internal chassis 4, which is made of a conductive material, on which the shielding material is disposed, with a shield cover 5 made of a conductive material such as aluminum. However, in such a structure, the high-density, high-frequency magnetic field of the heating coil 2 interlinks with the conductive shield cover 5, causing an induced current to flow in the shield cover 5, causing heat loss and reducing the heating efficiency of the cooker. Since the demagnetizing field generated by the induced current reduces the equivalent inductance of the heating coil, it becomes necessary to compensate by increasing the number of turns of the heating coil in the design of the high-frequency power converter. Further, since the shield cover 5 is a conductor, there are problems in that it requires a considerable amount of space in order to ensure electrical insulation from other electrical parts. All of these problems pose serious limitations when reducing the height (thinner profile) of the cooker. Furthermore, if a conductive plate like the shield cover 5 that covers the entire high-frequency power converter is installed inside the cooking device, the conductive plate will become hot due to the radiant heat received from the heating coil 2 and the bottom of the load pan, raising the temperature inside the device. This may adversely affect the cooling of semiconductor components and other electrical components, and may impair their reliability.
さらに、第1図に於て、内部シヤーシ4や、外
部筐体6を樹脂化した場合には、高周波電力変換
装置3から発生する磁界を、その上面を覆うシー
ルド板5だけでは十分な低減ができない。 Furthermore, in FIG. 1, when the internal chassis 4 and the external casing 6 are made of resin, the magnetic field generated from the high frequency power converter 3 cannot be sufficiently reduced by the shield plate 5 covering the top surface thereof. Can not.
即ち、樹脂部分から磁界が外部に漏洩してしま
うため少くとも内部シヤーシ4が導電体である
か、外部筐体6が導電体であり、磁気シールド効
果を、もつていなくてはならないということであ
る。筐体の樹脂化は、機器の軽量化あるいは製品
価格の低減のために非常に有利であるが、従来例
のように高周波電力変換装置全体を導電体で取り
囲むという従来の電磁遮蔽構造では、徹底的な筐
体の樹脂化は難しく、筐体の樹脂化の長所を十分
ひきだすことはできなかつた。そのため、最近で
は、高周波電力変換装置から出す輻射雑音に対す
る低減対策をせずに樹脂化するため、ラジオ周波
数帯域での輻射雑音によつて外部のラジオ放送受
信にかなりの防害を及ぼす場合があつた。 In other words, since the magnetic field leaks to the outside from the resin part, at least the internal chassis 4 or the external casing 6 must be a conductor and have a magnetic shielding effect. be. Making the case of resin is very advantageous for reducing the weight of the device and the product price, but the conventional electromagnetic shielding structure of surrounding the entire high frequency power converter with a conductive material is not completely effective. It was difficult to make the casing from resin, and the advantages of making the casing from resin could not be fully exploited. Therefore, recently, high-frequency power converters are made of resin without taking measures to reduce the radiated noise emitted from the equipment, which may cause considerable damage to external radio broadcast reception due to radiated noise in the radio frequency band. Ta.
発明の目的
本発明の目的は、上記従来の欠点を解消するも
ので、誘導加熱調理器の高周波電力変換装置から
外部に漏洩するラジオ周波数帯域に於ける電磁界
を、簡単な構成で低減するところにあり、さらに
はそれによつて、誘導加熱調理器の筐体の樹脂
化、薄型化、小型化を促進することにある。Purpose of the Invention The purpose of the present invention is to eliminate the above-mentioned conventional drawbacks, and to reduce the electromagnetic field in the radio frequency band leaking to the outside from the high frequency power converter of an induction heating cooker with a simple configuration. Furthermore, the purpose of the present invention is to promote the use of resin, thinness, and miniaturization of the housing of induction heating cookers.
発明の構成
上記目的を達するため、本発明の誘導加熱調理
器は、複数個の半導体スイツチング素子とそれに
逆並列に接続されたダンパーダイオードを具備
し、その半導体スイツチング素子の導通期間を制
御することにより出力電力を制御する高周波電力
変換装置に於て、前記半導体スイツチング素子の
遮断時に生起する急峻な立下がり波形及びそれに
伴う共振コンデンサの充電電流の急激な立上がり
波形等を含む高周波電流成分の形成する閉ループ
の開口部を選択的に最少にするように構成したも
のであり、特に本発明に於ては、前記高周波電流
成分の閉ループを構成する複数個の半導体スイツ
チング素子及びそれに接続される配電線の構成を
規定することにより、ラジオ周波数帯域の防害電
磁界低減を計つている。従来の誘導加熱調理器で
は、電流容量が不足で、同一半導体スイツチング
素子を並列にして使用する必要のある場合、第2
図のようにそれぞれの半導体スイツチング素子7
を別々の金属ベース8上に配し金属ベースを一方
の電極としてそれを冷却フイン9に接続固定し、
他の電極はそれぞれのパツケージングから出され
た端子10を導電金属棒11等で相互に接続し、
リード線12,13で共振コンデンサ14等の部
品に接続されているのが通常であつたが、本発明
は、複数組の同一半導体接合を同一金属ベース上
に配列し、その半導体接合の主電流の流れる一方
の電極は、前記金属ベースに接続され、他の電極
は、その半導体接続近傍で相互に接続され単一電
極として、他の部品と接続される構成であり、こ
のようにすることにより、複数個の半導体スイツ
チング素子を並列に接続して使用する場合、前述
の半導体スイツチング素子の遮断時の高周波電流
閉ループの開口面積を極めて小さくすることがで
き、そこから発生する磁界を低減できるという効
果を有する。この効果は、半導体スイツチング素
子に接続されるリード線を撚り合わせたり、束ね
たりすることによりさらに大きくなる。Structure of the Invention In order to achieve the above object, the induction heating cooker of the present invention includes a plurality of semiconductor switching elements and a damper diode connected in antiparallel to the semiconductor switching elements, and controls the conduction period of the semiconductor switching elements. In a high-frequency power conversion device that controls output power, a closed loop formed by high-frequency current components including a steep falling waveform that occurs when the semiconductor switching element is cut off and a sudden rising waveform of the charging current of a resonant capacitor accompanying the steep falling waveform. In particular, in the present invention, a plurality of semiconductor switching elements constituting a closed loop for the high frequency current component and a distribution line connected thereto are configured to selectively minimize the opening of the high frequency current component. By stipulating the above, it is intended to reduce the electromagnetic field to prevent damage in the radio frequency band. In conventional induction heating cookers, when the current capacity is insufficient and it is necessary to use the same semiconductor switching elements in parallel, the second
As shown in the figure, each semiconductor switching element 7
are arranged on separate metal bases 8, and the metal bases are used as one electrodes, which are connected and fixed to cooling fins 9.
For the other electrodes, the terminals 10 taken out from each packaging are connected to each other with a conductive metal rod 11 or the like.
Normally, the lead wires 12 and 13 are connected to components such as the resonant capacitor 14, but in the present invention, multiple sets of the same semiconductor junction are arranged on the same metal base, and the main current of the semiconductor junction is One electrode through which the current flows is connected to the metal base, and the other electrodes are connected to each other near the semiconductor connection and connected to other parts as a single electrode. When multiple semiconductor switching devices are connected in parallel, the opening area of the high-frequency current closed loop when the semiconductor switching devices are cut off can be made extremely small, and the magnetic field generated therefrom can be reduced. has. This effect is further enhanced by twisting or bundling the lead wires connected to the semiconductor switching element.
実施例の説明
以下、本発明の実施例について図面に基づいて
説明する。DESCRIPTION OF EMBODIMENTS Hereinafter, embodiments of the present invention will be described based on the drawings.
第3図は誘導加熱調理器の高周波電力変換装置
の一例で、トランジスタインバータの基本回路図
である。この第3図に於て、商用低周波電源15
は全波整流器17により全波整流されてフイルタ
コイル18を介して、高周波電源コンデンサ19
に接続されている。高周波電源コンデンサ19の
正極端子には、加熱コイル21が接続され、加熱
コイル21のもう一方の端子と高周波電源コンデ
ンサ19の負極側端子の間には、コレクタ−エミ
ツタ端子間に逆並列にダイオードが接続された
NPN逆導通トランジスタ22の2コ並列回路と、
共振コンデンサ23の並列回路が接続されてい
る。また逆導通スイツチングトランジスタ22の
ベースには制御回路ブロツク20から駆動信号が
供給され、制御回路ブロツク20は電源トランス
16から制御電源を供給されている。このインバ
ータ回路の動作を第4図により詳説する。第4図
aは逆導通スイツチングトランジスタ22の駆動
電流IBであり、時刻t1で順方向電流IB1が流れ始
め、第4図bのように逆導通スイツチングトラン
ジスタ22にダイオード電流IDが流れた後に、ス
イツチングトランジスタが導通し、加熱コイル2
1と負荷鍋との合成インピーダンスで決まる傾き
でコレクタ電流ICが増加する。所定の時間TON後
(時刻t2)に前記逆導通トランジスタ22の駆動
電流IB1の供給が停止され、逆導通トランジスタ
22は遮断し始め、コレクタ電流が急激に減少
し、下降時間Tf後(時刻t3)に完全に遮断し、コ
レクタ電流ICは零になる。一方逆導通トランジス
タ22が遮断し始め、コレクタ電流IC(TON期間中
は加熱コイル21に略等しい電流が流れる)が減
少し始めると同時に加熱コイル21に逆起電力が
発生し、共振コンデンサ23に充電電流を流す。
その立ち上がり時間は、逆導通トランジスタ22
の下降時間Tfと対応し、非常に急峻であり、そ
の後加熱コイル21と共振コンデンサ23の共振
電流が共振コンデンサ23に第4図dの如く流れ
る。逆導通トランジスタ22のコレクタ−エミツ
タ間には、第4図cに示すように、コレクタ電流
が減少し始めると同時に、加熱コイル21と共振
コンデンサ23の共振電圧が印加する。コレクタ
電圧の後縁が零点を切る点(時刻t4)にて再び逆
導通トランジスタ22のベースにドライブ電流IB
1を印加する。この後は、以上述べた動作が繰り
返される。なお、逆導通トランジスタ22のダイ
オードは、ダンパーダイオードである。また加熱
コイル21に流れる電流は、第4図eに示す如
く、逆導通トランジスタ22に流れる電流(同図
b)と共振コンデンサ23の電流(同図d)の和
であり、急峻な立上がり、立下がり波形はない。 FIG. 3 is an example of a high frequency power conversion device for an induction heating cooker, and is a basic circuit diagram of a transistor inverter. In this Figure 3, the commercial low frequency power supply 15
is full-wave rectified by a full-wave rectifier 17 and passed through a filter coil 18 to a high-frequency power supply capacitor 19.
It is connected to the. A heating coil 21 is connected to the positive terminal of the high-frequency power capacitor 19, and a diode is connected in antiparallel between the collector and emitter terminals between the other terminal of the heating coil 21 and the negative terminal of the high-frequency power capacitor 19. connected
Two parallel circuits of NPN reverse conduction transistors 22,
A parallel circuit of resonant capacitors 23 is connected. Further, a drive signal is supplied to the base of the reverse conduction switching transistor 22 from the control circuit block 20, and the control circuit block 20 is supplied with control power from the power transformer 16. The operation of this inverter circuit will be explained in detail with reference to FIG. FIG. 4a shows the drive current I B of the reverse conduction switching transistor 22. At time t 1 , the forward current I B1 starts flowing, and as shown in FIG. 4B, the diode current I D flows through the reverse conduction switching transistor 22. flows, the switching transistor becomes conductive, and the heating coil 2
Collector current I C increases with a slope determined by the combined impedance of 1 and the load pot. After a predetermined time T ON (time t 2 ), the supply of the drive current I B1 to the reverse conduction transistor 22 is stopped, the reverse conduction transistor 22 begins to shut off, the collector current decreases rapidly, and after a falling time T f (time t 3 ), the circuit is completely shut off and the collector current I C becomes zero. On the other hand, the reverse conduction transistor 22 begins to shut off, and at the same time the collector current I C (substantially equal current flows through the heating coil 21 during the T ON period) begins to decrease, a back electromotive force is generated in the heating coil 21, and the resonant capacitor 23 A charging current is applied to the
The rise time of the reverse conducting transistor 22
It corresponds to the falling time T f of , which is very steep, and then the resonant current of the heating coil 21 and the resonant capacitor 23 flows through the resonant capacitor 23 as shown in FIG. 4d. As shown in FIG. 4c, the resonant voltage of the heating coil 21 and the resonant capacitor 23 is applied between the collector and emitter of the reverse conducting transistor 22 at the same time as the collector current begins to decrease. At the point where the trailing edge of the collector voltage crosses zero (time t 4 ), the drive current I B flows again to the base of the reverse conduction transistor 22.
Apply 1 . After this, the operations described above are repeated. Note that the diode of the reverse conducting transistor 22 is a damper diode. Furthermore, as shown in Figure 4e, the current flowing through the heating coil 21 is the sum of the current flowing through the reverse conduction transistor 22 (b in the figure) and the current in the resonant capacitor 23 (d in the figure), and has a steep rise and rise. There is no falling waveform.
本発明の実施例を以上述べたインバータ回路を
例にとつて述べる。第5図及び第6図は本発明の
一実施例であつて、第3図のインバータ回路図に
於て、逆導通トランジスタ22と共振コンデンサ
23とその配線からなる一点鎖線で囲んだブロツ
クAの構成図を第5図に示し、並列に接続された
2個の逆導通トランジスタ22の断面構成図を第
6図に示している。第6図に於て、逆導通NPN
トランジスタを構成する2個の同一シリコンチツ
プ22が一枚の金属ベース25の上に配列され、
金属ベース25がコレクタと同電位になるよう接
続されている。一方2つのエミツタ電極はシリコ
ンチツプ近傍で、導電体のリードで相互に接線さ
れ、エミツタ端子27に接続され、同様に、2個
のベース電極もシリコンチツプ近傍で相互に接続
されベース端子28に接続されており、これらは
樹脂ケース26と、注入された樹脂29により一
体成型され一部品となつている。一方第5図にお
いて、第6図の構造をもつ逆導通NPNトランジ
スタが冷却フイン24の上にビスで取りつけられ
エミツタ端子27及び金属ベース25(コレクタ
端子)に接続されたリード線31,30は、撚り
合わされ、他の端子は共振コンデンサ32の接続
端子33に接続されている。そして、共振コンデ
ンサ32及びその接続端子33付近のリード線
は、アルミ板等の導電体34で周囲を取り囲まれ
ている。 Embodiments of the present invention will be described using the inverter circuit described above as an example. 5 and 6 show an embodiment of the present invention, and in the inverter circuit diagram of FIG. 3, a block A surrounded by a dashed line consisting of a reverse conduction transistor 22, a resonant capacitor 23, and their wiring is shown. A block diagram is shown in FIG. 5, and a cross-sectional block diagram of two reverse conducting transistors 22 connected in parallel is shown in FIG. In Figure 6, reverse conduction NPN
Two identical silicon chips 22 constituting a transistor are arranged on one metal base 25,
The metal base 25 is connected to the collector so as to have the same potential. On the other hand, the two emitter electrodes are connected to each other near the silicon chip by conductive leads and connected to the emitter terminal 27, and similarly, the two base electrodes are also connected to each other near the silicon chip and connected to the base terminal 28. These are integrally molded with the resin case 26 and the injected resin 29 to form a single component. On the other hand, in FIG. 5, a reverse conduction NPN transistor having the structure shown in FIG. 6 is mounted on the cooling fin 24 with screws, and the lead wires 31 and 30 are connected to the emitter terminal 27 and the metal base 25 (collector terminal). The other terminal is connected to a connecting terminal 33 of a resonant capacitor 32. The resonant capacitor 32 and its lead wire near the connection terminal 33 are surrounded by a conductor 34 such as an aluminum plate.
以下、上記構成に於ける作用について説明す
る。上記インバータに於て、前述のように加熱コ
イル21には第4図eに示す略連続な電流が流れ
急激な電流変化はない。一方、逆導通トランジス
タ22には第4図bに示す電流が流れ、そして共
振コンデンサ23には第4図dに示す電流が流
れ、これらの波形には特に時刻t2からt3にかけて
急激な電流変化が生起する。この波形を分析する
ため逆導通トランジスタ22と共振コンデンサ2
3からなる閉回路をとりだし、第7図に示す。そ
して第8図には各素子を流れる電流波形を示す。
電流の向きは第7図に矢印で示す方向を正として
いる。前述した時刻t2からt3にかけての急峻な電
流変化は等価的に第8図cに示す高周波パルス電
流が、第7図の閉回路を矢印で示す向きに流れる
とみてよい。時刻t2とt3の時間間隔はスイツチン
グトランジスタのコレクタ電流の下降時間に対応
し、インバータの出力電力が約1.2KWの場合、
コレクタ電流のピーク電流は約50A程度であり、
時刻t2とt3の間隔は、1μsec前後である。そのた
め、このトランジスタ遮断時の高周波電流成分の
周波数スペクトルは500KHzから2MHzのものが
支配的である。一方、前記トランジスタ遮断時の
高周波電流成分による磁界の強さは前述の第7図
で示す遮断時の高周波電流成分の閉ループの取囲
む面積(斜線部)に比例して増減する。そこで本
実施例は、第5図に示すように前記トランジスタ
遮断時の高周波電流成分の流れる閉回路の作る面
積を最小にすべく逆導通トランジスタ22のコレ
クタ及びエミツタから共振コンデンサ32の端子
33を結ぶ配線30及び31を撚り合せ、そして
共振コンデンサ32の素子と、接続端子30,3
1付近の配線で生じる前記高周波電流閉ループの
開口部を導電性材料でできたシールド板34によ
つて取り囲み、さらに、逆導通トランジスタのエ
ミツタどうしを接続する導電金属棒11と逆導通
トランジスタと放熱フイン24で構成される閉ル
ープを第5図、第6図に示すように、同一金属ベ
ース上に半導体チツプを並べることにより極めて
小さくするものであり、第9図に従来例と本実施
例に於ける前記トランジスタ遮断時の高周波電流
成分の形成する閉回路の開口面積の差を示してい
る。第9図aは従来例、同図bは本実施例の構成
例である。本実施例による高周波低減効果は、例
えば誘導加熱調理器から約3m離れた場所に於
て、測定した場合、周波数500KHz〜2MHzに於
て約10〜15dB輻射雑音を低減できる。 The effects of the above configuration will be explained below. In the above inverter, as described above, a substantially continuous current as shown in FIG. 4e flows through the heating coil 21, and there is no sudden change in current. On the other hand, the current shown in FIG. 4b flows through the reverse conduction transistor 22, and the current shown in FIG . Change occurs. In order to analyze this waveform, a reverse conducting transistor 22 and a resonant capacitor 2 are used.
A closed circuit consisting of 3 is taken out and shown in Fig. 7. FIG. 8 shows the waveform of the current flowing through each element.
The direction of the current is defined as the direction shown by the arrow in FIG. 7 as positive. The steep current change from time t 2 to t 3 described above can be equivalently considered as the high-frequency pulse current shown in FIG. 8c flowing in the closed circuit in FIG. 7 in the direction shown by the arrow. The time interval between times t 2 and t 3 corresponds to the falling time of the collector current of the switching transistor, and when the output power of the inverter is about 1.2KW,
The peak current of the collector current is about 50A,
The interval between times t 2 and t 3 is approximately 1 μsec. Therefore, the frequency spectrum of the high-frequency current component when this transistor is cut off is predominantly from 500 KHz to 2 MHz. On the other hand, the strength of the magnetic field due to the high frequency current component when the transistor is cut off increases or decreases in proportion to the area (shaded area) surrounded by the closed loop of the high frequency current component when the transistor is cut off as shown in FIG. Therefore, in this embodiment, as shown in FIG. 5, the terminal 33 of the resonant capacitor 32 is connected from the collector and emitter of the reverse conducting transistor 22 in order to minimize the area created by the closed circuit through which the high frequency current component flows when the transistor is cut off. The wirings 30 and 31 are twisted together, and the element of the resonant capacitor 32 and the connection terminals 30, 3 are connected.
A shield plate 34 made of a conductive material surrounds the opening of the high-frequency current closed loop generated in the wiring near 1, and further includes a conductive metal rod 11 connecting the emitters of the reverse conduction transistors, a reverse conduction transistor, and a heat dissipation fin. As shown in FIGS. 5 and 6, the closed loop consisting of 24 is made extremely small by arranging semiconductor chips on the same metal base. It shows the difference in the opening area of the closed circuit formed by the high-frequency current component when the transistor is cut off. FIG. 9a shows a conventional example, and FIG. 9b shows an example of the configuration of this embodiment. The high frequency reduction effect according to this embodiment can reduce radiation noise by about 10 to 15 dB at a frequency of 500 KHz to 2 MHz, for example, when measured at a location about 3 m away from the induction heating cooker.
このように本実施例によれば、誘導加熱調理器
から発生するラジオ周波数帯域の輻射雑音を簡単
な構成で、他の部品配置や、冷却構成にほとんど
影響を与えることなく低減できるという効果を有
する。すなわち、本実施例は、複数個のスイツチ
ング素子を有するトランジスタ周辺から、発生す
るラジオ周波数帯域の輻射雑音を遮蔽板などによ
りスイツチング素子の周囲を取囲んで遮蔽する手
段をとることなく低減でき、大電流が流れ高電圧
が印加し、高損失の発生するトランジスタの冷却
に悪影響を与えず、高電圧の印加する放熱フイン
と遮蔽板との電気絶縁、遮蔽板と他の高圧充電部
間との電気絶縁を考慮するという必要もなく誘導
加熱調理器の薄型化、小型化に大きく寄与するも
のである。 As described above, this embodiment has the effect that the radiation noise in the radio frequency band generated from the induction heating cooker can be reduced with a simple configuration and with almost no effect on the arrangement of other parts or the cooling configuration. . In other words, in this embodiment, the radiation noise in the radio frequency band generated from around a transistor having a plurality of switching elements can be reduced without using a shielding plate or the like to surround and shield the switching elements. It does not adversely affect the cooling of transistors where current flows and high voltage is applied and high losses occur, and electrical insulation between the heat dissipation fins to which high voltage is applied and the shield plate, and between the shield plate and other high voltage live parts. There is no need to consider insulation, and this greatly contributes to making the induction heating cooker thinner and smaller.
なお複数個の半導体スイツチング素子の他の構
成例を第10図a及びbに示す。第10図bは同
一接合を有する半導体接合を二個近接して同一金
属ベース上に配列したものであるが、第10図a
は同一半導体チツプに複数の同一接合を有するト
ランジスタ接合を構成し、ダンパーダイオード3
7を別のチツプで作り、同一金属ベース上に近接
配置したものであり、第10図bは複数のスイツ
チングトランジスタ36及び、ダイオード接合を
同一半導体チツプ35に構成した例である。なお
以上の実施例に於てダンパーダイオードをスイツ
チングダイオード接合の近傍に配置しているの
は、ダンパーダイオードにも第8図の時刻t1に於
て、大きな急峻な電流変化が生ずる場合が負荷に
より出てくるからである。これは、特に無負荷に
近い場合ダイオード電流が増大するためである。 Other configuration examples of a plurality of semiconductor switching elements are shown in FIGS. 10a and 10b. Figure 10b shows two semiconductor junctions having the same junction arranged close together on the same metal base, while Figure 10a
constitutes a transistor junction having a plurality of identical junctions on the same semiconductor chip, and a damper diode 3
7 are made of separate chips and placed close to each other on the same metal base, and FIG. 10b shows an example in which a plurality of switching transistors 36 and diode junctions are formed on the same semiconductor chip 35. In the above embodiment, the damper diode is placed near the switching diode junction because the damper diode is also loaded when a large and steep current change occurs at time t1 in FIG. This is because it comes out due to This is because the diode current increases especially when near no load.
発明の効果
以上のように本発明によれば、複数個の半導体
スイツチング接合を有し、急峻な遮断電流波形を
有する高周波電力変換装置に於て、導電材料でで
きた遮蔽板等で半導体スイツチング素子あるいは
高周波電力変換装置全体を覆つたりすることな
く、配線を工夫することによりラジオ周波数帯域
の輻射雑音を低減できるため、次のような効果を
有する。Effects of the Invention As described above, according to the present invention, in a high frequency power converter having a plurality of semiconductor switching junctions and a steep breaking current waveform, the semiconductor switching element is Alternatively, radiation noise in the radio frequency band can be reduced by devising the wiring without covering the entire high frequency power converter, resulting in the following effects.
(1) スイツチング素子の冷却条件を含め誘導加熱
調理器内部の冷却条件をほとんど悪化させな
い。(1) The cooling conditions inside the induction heating cooker, including the cooling conditions of the switching element, are hardly deteriorated.
(2) 少くとも高電圧の印加するスイツチング素子
あるいはダンパーダイオードの周囲に導電体の
遮蔽板が不必要なため、遮蔽板と部品との絶縁
距離を考慮する必要がなく、他の部品配置がや
りやすくなり、誘導加熱調理器全体の部品配置
が極めてコンパクトにでき、機器の小型化、薄
型化が計れる。(2) Since there is no need for a conductive shielding plate around at least the switching element or damper diode to which high voltage is applied, there is no need to consider the insulation distance between the shielding plate and the components, and other component placement is easy. The parts arrangement of the entire induction heating cooker can be made extremely compact, and the device can be made smaller and thinner.
(3) 前記スイツチングトランジスタ遮断時の高周
波電流成分の流れる閉回路を構成する部品及び
配線でスイツチングトランジスタ以外の共振コ
ンデンサ等の部品及び配線を選択的に電磁シー
ルドすることにより、本発明に於ける輻射雑音
低減効果はさらに高くなり、筐体が樹脂であつ
ても金属であつてもほぼ同等の雑音低減効果が
得られる。そのため、筐体の樹脂化が行いやす
く、このことは誘導加熱調理器の軽量化、組立
性の改善を促進する効果がある。(3) In the present invention, by selectively electromagnetically shielding components and wiring other than the switching transistor, such as a resonant capacitor, among the components and wiring that constitute the closed circuit through which the high-frequency current component flows when the switching transistor is cut off. The radiation noise reduction effect is even higher, and almost the same noise reduction effect can be obtained whether the housing is made of resin or metal. Therefore, the casing can be easily made of resin, which has the effect of reducing the weight of the induction heating cooker and improving its ease of assembly.
第1図は従来の電磁誘導加熱調理器の断面図、
第2図は従来の高周波電力変換装置に於ける共振
コンデンサと逆導通トランジスタとその配電線の
関係を示す要部斜視図、第3図は本発明の一実施
例を示す電磁誘導加熱調理器の高周波電力変換装
置の回路図、第4図は同要部の信号波形図、第5
図は同高周波電力変換装置に於ける共振コンデン
サと半導体スイツチング素子とその配電線の関係
を示す要部斜視図、第6図は同高周波電力変換装
置の半導体スイツチング素子の断面図、第7図は
同半導体スイツチング素子と共振コンデンサとそ
の配電線からなる閉ループの電気回路図、第8図
は同電気回路における要部の信号波形図、第9図
aは従来例における閉ループを示す要部正面図、
第9図bは本実施例に於ける閉ループを示す要部
正面図、第10図aおよび第10図bはそれぞれ
本発明の他の実施例における半導体スイツチング
素子の断面図である。
19…高周波電源コンデンサ、21…加熱コイ
ル、22…逆導通トランジスタ、23…共振コン
デンサ、25…金属ベース、30,31…リード
線、32…共振コンデンサ、34…導電体。
Figure 1 is a cross-sectional view of a conventional electromagnetic induction cooking device.
Fig. 2 is a perspective view of a main part showing the relationship between a resonant capacitor, a reverse conduction transistor, and its distribution line in a conventional high-frequency power converter, and Fig. 3 is an illustration of an electromagnetic induction cooking device showing an embodiment of the present invention. A circuit diagram of the high frequency power converter, Figure 4 is a signal waveform diagram of the same main part, Figure 5
The figure is a perspective view of the main parts showing the relationship between the resonant capacitor, the semiconductor switching element, and its distribution line in the same high-frequency power converter, FIG. 6 is a cross-sectional view of the semiconductor switching element of the same high-frequency power converter, and FIG. An electric circuit diagram of a closed loop consisting of the semiconductor switching element, a resonant capacitor, and its distribution line, FIG. 8 is a signal waveform diagram of the main part of the electric circuit, and FIG. 9a is a front view of the main part showing the closed loop in the conventional example.
FIG. 9b is a front view of essential parts showing a closed loop in this embodiment, and FIGS. 10a and 10b are sectional views of semiconductor switching elements in other embodiments of the present invention, respectively. 19... High frequency power supply capacitor, 21... Heating coil, 22... Reverse conducting transistor, 23... Resonant capacitor, 25... Metal base, 30, 31... Lead wire, 32... Resonant capacitor, 34... Conductor.
Claims (1)
電源用フイルタコンデンサとダンパーダイオード
が逆並列に接続された半導体スイツチング素子
と、該半導体スイツチング素子の導通時間を制御
することにより出力電力を制御する高周波発振制
御手段を有する高周波電力変換装置を備え、前記
半導体スイツチング素子は複数組の同一半導体接
合を有し、それらは同一金属ベース上に配列さ
れ、この半導体接合の主電流の流れる一方の電極
は前記金属ベースに接続され、他の電極は半導体
接合近傍で相互に接続され単一電極として他の部
品と接続した誘導加熱調理器。 2 ダンパーダイオードの半導体接合は金属ベー
ス上に配列され、半導体スイツチング素子の半導
体接合にその近傍で接続した特許請求の範囲第1
項記載の誘導加熱調理器。 3 半導体スイツチング素子に接続された主電流
の流れる配電線は、撚り合わせ、または、束ねら
れ相互に近接されてなる特許請求の範囲第1項記
載の誘導加熱調理器。 4 共振用コンデンサあるいは電源コンデンサは
接続される配電線の一部とともに周囲を導電金属
板にて遮蔽されてなる特許請求の範囲第1項記載
の誘導加熱調理器。[Claims] 1. A semiconductor switching element in which a heating coil, a resonance capacitor, a high frequency power supply filter capacitor, and a damper diode are connected in antiparallel, and output power by controlling the conduction time of the semiconductor switching element. The semiconductor switching element has a plurality of sets of the same semiconductor junction, which are arranged on the same metal base, and one of the semiconductor junctions through which the main current flows. An induction heating cooker in which the electrodes are connected to the metal base, and the other electrodes are connected to each other near the semiconductor junction to form a single electrode connected to other parts. 2. The semiconductor junction of the damper diode is arranged on a metal base and connected in its vicinity to the semiconductor junction of the semiconductor switching element.
Induction heating cooker as described in section. 3. The induction heating cooker according to claim 1, wherein the distribution lines connected to the semiconductor switching elements and through which the main current flows are twisted or bundled and placed close to each other. 4. The induction heating cooker according to claim 1, wherein the resonance capacitor or the power supply capacitor is surrounded by a conductive metal plate together with a part of the power distribution line to which it is connected.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58111275A JPS603889A (en) | 1983-06-20 | 1983-06-20 | induction heating cooker |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58111275A JPS603889A (en) | 1983-06-20 | 1983-06-20 | induction heating cooker |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS603889A JPS603889A (en) | 1985-01-10 |
| JPS635876B2 true JPS635876B2 (en) | 1988-02-05 |
Family
ID=14557088
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58111275A Granted JPS603889A (en) | 1983-06-20 | 1983-06-20 | induction heating cooker |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS603889A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9119624B2 (en) | 2006-04-24 | 2015-09-01 | Covidien Ag | ARC based adaptive control system for an electrosurgical unit |
| US10603098B2 (en) | 2013-05-31 | 2020-03-31 | Covidien Lp | Gain compensation for a full bridge inverter |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2722756B2 (en) * | 1990-03-12 | 1998-03-09 | 松下電器産業株式会社 | Induction heating cooker |
-
1983
- 1983-06-20 JP JP58111275A patent/JPS603889A/en active Granted
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9119624B2 (en) | 2006-04-24 | 2015-09-01 | Covidien Ag | ARC based adaptive control system for an electrosurgical unit |
| US10603098B2 (en) | 2013-05-31 | 2020-03-31 | Covidien Lp | Gain compensation for a full bridge inverter |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS603889A (en) | 1985-01-10 |
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