JPS6343291A - Radio frequency heater - Google Patents

Radio frequency heater

Info

Publication number
JPS6343291A
JPS6343291A JP18552386A JP18552386A JPS6343291A JP S6343291 A JPS6343291 A JP S6343291A JP 18552386 A JP18552386 A JP 18552386A JP 18552386 A JP18552386 A JP 18552386A JP S6343291 A JPS6343291 A JP S6343291A
Authority
JP
Japan
Prior art keywords
flange
door
wall
radio wave
heating chamber
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.)
Pending
Application number
JP18552386A
Other languages
Japanese (ja)
Inventor
岩淵 康司
哲男 窪田
幸雄 田中
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.)
Hitachi Heating Appliances Co Ltd
Original Assignee
Hitachi Heating Appliances 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 Hitachi Heating Appliances Co Ltd filed Critical Hitachi Heating Appliances Co Ltd
Priority to JP18552386A priority Critical patent/JPS6343291A/en
Publication of JPS6343291A publication Critical patent/JPS6343291A/en
Pending legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Abstract] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は高周波加熱装置のドア構造の改良に関する。[Detailed description of the invention] Industrial applications The present invention relates to an improvement in the door structure of a high frequency heating device.

従来の技術 高周波加熱装置のドア周縁に特性インピーダンスの異な
る溝を深さ方向に設け、この溝の深さ方向の特性インピ
ーダンスを不連続にすることにより、実質的深さが使用
波長の4分の1より小さくしても、溝の入口でのインピ
ーダンスが最大となり、チョーク溝と同様に漏洩電波を
少なくすることができるという提案が特開昭60−25
190号公報にあるにの従来例では、溝の深さ方向に幅
の異なる溝を設けたり、溝の周壁の形状を深さ方向に変
形するなどかなり形状が複雑である。また、特性インピ
ーダンスの不連続部における反射防止を考慮する必要が
ある。
Conventional technology Grooves with different characteristic impedances are provided in the depth direction on the periphery of the door of a high-frequency heating device, and by making the characteristic impedance of the grooves discontinuous in the depth direction, the effective depth is reduced to a quarter of the wavelength used. A proposal was made in JP-A-60-25 that even if the value is smaller than 1, the impedance at the entrance of the groove is maximized, and leakage radio waves can be reduced in the same way as a choke groove.
In the conventional example disclosed in Japanese Patent No. 190, the shape is quite complicated, such as providing grooves with different widths in the depth direction of the groove and deforming the shape of the peripheral wall of the groove in the depth direction. Furthermore, it is necessary to consider reflection prevention at discontinuous portions of characteristic impedance.

発明が解決しようとする問題点 溝の深さ方向に、複雑な形状をした溝を設ける必要があ
り、また特性インピーダンスの不連続部における反射防
止に手間が掛かかる点である。
Problems to be Solved by the Invention It is necessary to provide grooves with complicated shapes in the depth direction of the grooves, and it takes time and effort to prevent reflections at discontinuous portions of characteristic impedance.

問題点を解決するための手段 本発明は、ドア周囲を取り囲む額縁状の電波減衰空胴の
最外周壁に当たる部分を複数の導体片とし、この導体片
の先端を電波減衰空胴の入口を狭めるように張り出し、
この張り出し面をテーパ付誘電体カバーで覆ったもので
ある。
Means for Solving the Problems The present invention uses a plurality of conductor pieces at the outermost peripheral wall of a frame-shaped radio wave attenuation cavity surrounding the door, and narrows the entrance of the radio wave attenuation cavity at the tips of these conductor pieces. It sticks out like this,
This projecting surface is covered with a tapered dielectric cover.

作用 上記のように構成することにより、導体片により漏洩し
ようとする電波はTEM波として電波減衰空胴に導かれ
る。電波減衰空胴を容量とインダクタンスの並列共振回
路とみなした場合、誘電体カバーによって電波減衰空胴
の入口での容量成分が大きくなり、その分だけインダク
タンス成分が小さくてよい、すなわち電波減衰空胴の深
さが自由空間波長の4分の1よりも小さい状態でチョー
ク溝として作用する。
Effect: With the above configuration, radio waves that are about to leak due to the conductor piece are guided to the radio wave attenuation cavity as TEM waves. When considering a radio wave attenuation cavity as a parallel resonant circuit of capacitance and inductance, the capacitance component at the entrance of the radio wave attenuation cavity becomes larger due to the dielectric cover, and the inductance component only needs to be smaller by that much, that is, the radio wave attenuation cavity acts as a choke groove with a depth of less than a quarter of the free space wavelength.

実施例 本発明の一実施例による高周波加熱装置の構成および作
用を図面とともに説明する。
Embodiment The structure and operation of a high-frequency heating device according to an embodiment of the present invention will be explained with reference to the drawings.

第1図および第2図において、1は加熱室で。In Figures 1 and 2, 1 is a heating chamber.

2は加熱室1の開口部を取り囲むフランジで、3は外箱
である。4は加熱室1内をのぞくためにドア5の中央部
にできるだけ広範囲に設けた小穴群である。6はこの小
穴群4の周囲を取り囲む段部で、この段部6は小穴群4
の内面に接着した透光性のドア内カバー15の端部が清
掃の際などにはがれるのを防ぐと共に、ドア5閉成時に
フランジ2と平面接触する封口面7の平面度を良くする
ものである。8は封口面7の端部よりフランジ2に対し
て略直角に折り曲げた第1の壁面である。9は第1の壁
面8の端部よりフランジ2に対して略平行に延長した第
2の壁面である。10は第2の壁面9の端部よりフラン
ジ2に向かって略直角に折り曲げた多数の導体片で、こ
の導体片10の先端には加熱室1開口部側に向かって張
り出した張出面11を設けている。小穴群4、段部6.
封口面7、第1の壁面8、第2の壁面9、導体片10お
よび張出面11は1枚の金属板から一体成形している。
2 is a flange surrounding the opening of the heating chamber 1, and 3 is an outer box. Reference numeral 4 designates a group of small holes provided in the center of the door 5 as wide as possible to allow viewing into the heating chamber 1. Reference numeral 6 denotes a step surrounding the small hole group 4;
This prevents the end of the translucent door inner cover 15 adhered to the inner surface of the door from peeling off during cleaning, etc., and improves the flatness of the sealing surface 7 that makes plane contact with the flange 2 when the door 5 is closed. be. Reference numeral 8 denotes a first wall surface bent from the end of the sealing surface 7 at a substantially right angle to the flange 2. Reference numeral 9 denotes a second wall surface extending substantially parallel to the flange 2 from the end of the first wall surface 8. Numerous conductor pieces 10 are bent at a substantially right angle from the end of the second wall surface 9 toward the flange 2, and each of the conductor pieces 10 has a projecting surface 11 extending toward the opening of the heating chamber 1 at the tip thereof. It is set up. Small hole group 4, stepped portion 6.
The sealing surface 7, the first wall surface 8, the second wall surface 9, the conductor piece 10, and the projecting surface 11 are integrally formed from a single metal plate.

第1の壁面8.第2の壁面9、導体片10および張出面
11により電波減衰空胴12を形成する。この電波減衰
空胴12の入口をふさぐ不透明の誘電体カバー13から
突き出した突起片14は張出面11に設けた貫通穴23
を介して導体片10に設けた取付穴18に引っ掛かるよ
うになっている。ドア5の外側を覆う透光性のドア外カ
バー16から突き出した突起片17は導体片10の根元
を互いに連結する連結面2oの端部に引っ掛かるように
なっている。誘電体カバー13の最外周裏面には外方に
向って薄くなるテーパ24を設けて取り付けの際にドア
外カバー16の端部に乗り上げ゛ないようにしている。
First wall 8. A radio wave attenuation cavity 12 is formed by the second wall surface 9, the conductor piece 10, and the projecting surface 11. The projection piece 14 protruding from the opaque dielectric cover 13 that blocks the entrance of the radio wave attenuation cavity 12 is connected to a through hole 23 provided in the projecting surface 11.
It is adapted to be hooked into a mounting hole 18 provided in the conductor piece 10 via the conductor piece 10. A protruding piece 17 protruding from a translucent door outer cover 16 covering the outside of the door 5 is hooked onto an end of a connecting surface 2o that connects the bases of the conductor pieces 10 to each other. A taper 24 that becomes thinner toward the outside is provided on the back surface of the outermost periphery of the dielectric cover 13 to prevent it from riding on the edge of the door outer cover 16 during installation.

誘電体カバー13の電波減衰空Jljl12の入口に当
たる裏側には、電波減衰空胴12の内部に向かって突き
出たインピーダンス調整部25を設けている。また、導
体片10に対向して不透明シート19がドア外カバー1
6の内面に設けられ、外部より導体片10の間隙が見え
ないようになっている。
An impedance adjustment portion 25 protruding toward the inside of the radio wave attenuation cavity 12 is provided on the back side of the dielectric cover 13 corresponding to the entrance of the radio wave attenuation cavity Jljl12. Further, an opaque sheet 19 is placed on the door outer cover 1 facing the conductor piece 10.
6, so that the gap between the conductor pieces 10 is not visible from the outside.

次に上記のように構成した実施例の作用効果を説明する
。加熱室1開口部を取り囲むフランジ2と封口面7との
平面接触部に向かう入射電波に対して、第3図のような
簡易等価回路によって定性的に電波シール効果を説明す
る。21はフランジ2と封口面7との平面接触部に対応
する容量で、一種のバイパスコンデンサとして作用する
。平面接触部は平行板線路と考えられ、この線路の容量
は平行板のギャップに比例するので容量21は上記平面
接触部のギャップが小さいほど大きくなり、電波シール
効果が増す。第1の壁面8と導体片10とはTEM波を
伝搬する平行板線路を形成し、終端が第2の壁面9によ
って短絡されたものとみなすことができる。この場合、
張出面11が無ければ第5図のように電界が分布し、平
行板線路の長さQ、すなわち電波減衰空胴12の深さは
自由空間波長λの約4分の1で並列共振を起こし、イン
ピーダンスが最大となる。電波減衰空J5i12の周壁
の厚さは実用上、自由空間波長λに比べて十分水さいの
で無視して説明している。簡易等価回路を示す第3図で
は容量とインダクタンスを並列にした並列共振回路22
として表わせる。
Next, the effects of the embodiment configured as described above will be explained. The radio wave sealing effect will be qualitatively explained using a simple equivalent circuit as shown in FIG. 3 with respect to the incident radio waves directed toward the planar contact portion between the flange 2 surrounding the opening of the heating chamber 1 and the sealing surface 7. 21 is a capacitor corresponding to the planar contact portion between the flange 2 and the sealing surface 7, and acts as a type of bypass capacitor. The planar contact portion is considered to be a parallel plate line, and the capacitance of this line is proportional to the gap between the parallel plates, so the capacitance 21 becomes larger as the gap of the planar contact portion is smaller, and the radio wave sealing effect increases. The first wall surface 8 and the conductor piece 10 form a parallel plate line for propagating TEM waves, and it can be considered that the terminal end is short-circuited by the second wall surface 9. in this case,
If there is no overhanging surface 11, the electric field will be distributed as shown in Figure 5, and the length Q of the parallel plate line, that is, the depth of the radio wave attenuation cavity 12, will cause parallel resonance at about one-fourth of the free space wavelength λ. , the impedance is maximum. In practical terms, the thickness of the peripheral wall of the radio wave attenuating space J5i12 is sufficiently smaller than the free space wavelength λ, so it is ignored in the explanation. Figure 3, which shows a simple equivalent circuit, shows a parallel resonant circuit 22 in which capacitance and inductance are connected in parallel.
It can be expressed as

本発明のように、電波減衰空胴12の最外周壁に当たる
導体片10の先端を電波減衰空Jlq12の入口を狭め
るように折り曲げて張出面11を形成した場合、第4図
のような電界分布となる。この場合、張出面11の端部
と第1の壁面8との間の電気力線は、第5図に比べては
るかに密集し易い。
When, as in the present invention, the tip of the conductor piece 10 that is the outermost peripheral wall of the radio wave attenuation cavity 12 is bent to narrow the entrance of the radio wave attenuation cavity Jlq12 to form the overhanging surface 11, the electric field distribution as shown in FIG. 4 is obtained. becomes. In this case, the lines of electric force between the end of the projecting surface 11 and the first wall surface 8 are much more likely to be concentrated than in FIG. 5.

これは第4図の電波減衰空胴12の入口における容量成
分が大きくなり、その分だけインダクタンス成分を小さ
くしても、特定の周波数に共振させることができること
を意味する。すなわち、電波減衰空胴12の深さQを自
由空間波長λの4分の1より小さくしてもインピーダン
ス最大が得られ、漏洩電波を小さく抑えることができる
This means that the capacitance component at the entrance of the radio wave attenuation cavity 12 shown in FIG. 4 becomes large, and even if the inductance component is reduced by that much, resonance can be achieved at a specific frequency. That is, even if the depth Q of the radio wave attenuation cavity 12 is made smaller than one quarter of the free space wavelength λ, the maximum impedance can be obtained and leakage radio waves can be suppressed to a small level.

なお、インピーダンス調整部25は、電波減衰空胴12
の入口における容量成分をさらに増す効果があり、電波
減衰空胴12の深さ悲を一層小さくするものである。
Note that the impedance adjustment section 25 is a radio wave attenuation cavity 12
This has the effect of further increasing the capacitive component at the entrance of the radio wave attenuating cavity 12, and further reducing the depth of the radio wave attenuation cavity 12.

発明の効果 以上のように本発明によると、特性インピーダンスの異
なる複数の平行板線路(溝)を設けなくても、電波減衰
空胴の最外周壁に当たる導体片の先端に張出面を設け、
かつ電波減衰空胴の深さを自由空間波長の4分の1より
小さくできるので、ドアの薄形化が図れ、簡単な構造の
高周波加熱装置を提供できる。また、テーパ付の誘電体
カバーを設けたので、ドアの薄形化とともにドア外カバ
ーとの契合性がよくなるという効果がある。
Effects of the Invention As described above, according to the present invention, an overhanging surface is provided at the tip of the conductor piece that contacts the outermost peripheral wall of the radio wave attenuation cavity, without the need to provide a plurality of parallel plate lines (grooves) having different characteristic impedances.
In addition, since the depth of the radio wave attenuation cavity can be made smaller than one quarter of the free space wavelength, the door can be made thinner and a high frequency heating device with a simple structure can be provided. Furthermore, since the tapered dielectric cover is provided, the door can be made thinner and fit better with the door outer cover.

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

第1図は本発明の一実施例による高周波加熱装置のドア
5の金属部だけを示す要部斜視図、第2図は同ドア周囲
の電波シール部を示す要部断面図、第3図は同ドア5の
電波シール部の簡易等価回路図、第4図は同電波シール
部の電界分布図、第5図は同終端を短絡した平行板線路
の電界分布図である。 1・・・加熱室  2・・・フランジ 4・・・小穴群
5・・・ドア   6・・・段部   7・・・封口面
8・・・第1の壁面   9・・・第2の壁面10・・
・導体片    11・・・張出面13・・・誘電体カ
バー 16・・・ドア外カバー24・・・テーパ
FIG. 1 is a perspective view of a main part showing only the metal part of a door 5 of a high-frequency heating device according to an embodiment of the present invention, FIG. 2 is a cross-sectional view of a main part showing a radio wave seal around the door, and FIG. FIG. 4 is a simplified equivalent circuit diagram of the radio wave seal portion of the door 5, FIG. 4 is an electric field distribution diagram of the radio wave seal portion, and FIG. 5 is an electric field distribution diagram of the parallel plate line with the terminal ends short-circuited. DESCRIPTION OF SYMBOLS 1... Heating chamber 2... Flange 4... Small hole group 5... Door 6... Step part 7... Sealing surface 8... First wall surface 9... Second wall surface 10...
・Conductor piece 11...Protruding surface 13...Dielectric cover 16...Door outer cover 24...Taper

Claims (1)

【特許請求の範囲】[Claims] 加熱室(1)開口部を開閉するドア(5)の周縁に位置
しドア(5)閉成時には加熱室(1)開口部のフランジ
(2)に平面接触する封口面(7)と、この封口面(7
)の端部よりフランジ(2)に対して略直角の第1の壁
面(8)と、この第1の壁面(8)の端部よりフランジ
(2)に対して略平行に延長した第2の壁面(9)と、
この第2の壁面(9)の端部よりフランジ(2)に向か
って略直角の多数の導体片(10)と、この導体片(1
0)の先端から加熱室(1)開口部側に向って張り出し
た張出面(11)とを備え、かつ張出面(11)を覆う
誘電体カバー(13)を設け、このカバー(13)の最
外周裏面を外方に向かって薄くなるテーパ(24)状と
し、このテーパ(24)の先端でドア外カバー(16)
に契合したことを特徴とする高周波加熱装置。
A sealing surface (7) located at the periphery of the door (5) that opens and closes the opening of the heating chamber (1) and in planar contact with the flange (2) of the opening of the heating chamber (1) when the door (5) is closed; Sealing side (7
) and a second wall (8) extending substantially perpendicularly to the flange (2) from the end of the first wall (8), and a second wall extending substantially parallel to the flange (2) from the end of the first wall (8). The wall surface (9) of
A large number of conductor pieces (10) extending from the end of the second wall surface (9) to the flange (2) are substantially perpendicular to the flange (2).
A dielectric cover (13) is provided, which has a projecting surface (11) projecting from the tip of the heating chamber (1) toward the opening side of the heating chamber (1), and covers the projecting surface (11). The back surface of the outermost periphery is tapered (24) that becomes thinner toward the outside, and at the tip of this taper (24), the door outer cover (16) is formed.
A high frequency heating device characterized by being integrated with.
JP18552386A 1986-08-07 1986-08-07 Radio frequency heater Pending JPS6343291A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18552386A JPS6343291A (en) 1986-08-07 1986-08-07 Radio frequency heater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18552386A JPS6343291A (en) 1986-08-07 1986-08-07 Radio frequency heater

Publications (1)

Publication Number Publication Date
JPS6343291A true JPS6343291A (en) 1988-02-24

Family

ID=16172285

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18552386A Pending JPS6343291A (en) 1986-08-07 1986-08-07 Radio frequency heater

Country Status (1)

Country Link
JP (1) JPS6343291A (en)

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