JPS6372094A - Radio frequency heater - Google Patents

Radio frequency heater

Info

Publication number
JPS6372094A
JPS6372094A JP21537086A JP21537086A JPS6372094A JP S6372094 A JPS6372094 A JP S6372094A JP 21537086 A JP21537086 A JP 21537086A JP 21537086 A JP21537086 A JP 21537086A JP S6372094 A JPS6372094 A JP S6372094A
Authority
JP
Japan
Prior art keywords
wall surface
door
radio wave
flange
wave attenuation
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
JP21537086A
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 JP21537086A priority Critical patent/JPS6372094A/en
Publication of JPS6372094A publication Critical patent/JPS6372094A/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。
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 can be reduced to one-fourth of the wavelength used. Even if it is made smaller, the impedance at the entrance of the groove is maximum.

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60−25190号公報にある。こ
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シ形状
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。
There is a proposal in Japanese Patent Laid-Open No. 60-25190 that it is possible to reduce leakage radio waves in the same way as choke grooves. In this conventional example, the shape of the groove is complicated, such as by 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. It is also necessary to consider reflection prevention at discontinuities in 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、ドア周囲を取シ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、
張り出し面を覆う誘電体カバーを設け、その裏面の突起
片を導体片、張り出し面の貫通穴、取付穴にはめ込んで
固着し、又電波減衰空胴を構成する部分を一枚の金属板
から成形したものである。
Means for Solving the Problems The present invention provides a frame-shaped radio wave attenuation cavity surrounding the door with a plurality of conductor pieces at the outermost peripheral wall, and the tips of the conductor pieces are connected to the entrance of the radio wave attenuation cavity. Extend it out so as to narrow it,
A dielectric cover is provided to cover the projecting surface, and the projecting piece on the back side is fitted and fixed into the conductor piece, the through hole on the projecting surface, and the mounting hole, and the part that constitutes the radio wave attenuation cavity is molded from a single metal plate. This is what I did.

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、インピーダンス調整部によって電波
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よりも小さくでき
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 the radio wave attenuation cavity is regarded as a parallel resonant circuit of capacitance and inductance, the impedance adjustment section increases the capacitance component at the entrance of the radio wave attenuation cavity, and the inductance component may be reduced accordingly. That is, the depth of the radio wave attenuation cavity can be made smaller than one 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。Example 1 shows the configuration of a high-frequency heating device according to an embodiment of the present invention.

2よび作用を図面とともに説明する。第1図および第2
図において、1は加熱室で、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。
2 and its operation will be explained with reference to the drawings. Figures 1 and 2
In the figure, 1 is a heating chamber, 2 is a flange surrounding the opening of the heating chamber 1, and 3 is an outer box.

4は加熱室1内を覗くだめにドア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
折り曲げだ第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だ多数の導体片で、この導体片1
0の先端には加熱室1開口部+14’1に向かって張り
出した張出面11を設けている。小穴群41段部6.封
ロ面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。第
1の壁面8.第2の壁面9.導体片10および張出面1
1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26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20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ー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。誘
電体カバー13の電波減衰空胴12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16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。
Reference numeral 4 designates a group of small holes provided as wide as possible in the center of the door 5 in order to look into the inside of the heating chamber 1. Reference numeral 6 denotes a stepped portion surrounding the small hole group 4, and this stepped portion 6 prevents the end portion of the translucent door inner cover 15 adhered to the inner surface of the small hole group 4 from peeling off during cleaning, etc. Flange 2 when door 5 is closed
This improves the flatness of the sealing surface 7 that makes plane contact with the sealing surface 7. Reference numeral 8 denotes a first wall surface which is 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. Numeral conductor pieces 10 are bent at a substantially right angle from the end of the second wall surface 9 toward the flange 2.
0 is provided with an overhanging surface 11 that overhangs toward the heating chamber 1 opening +14'1. Small hole group 41 step part 6. Seal surface7. First wall 8. Second wall9. The conductor piece 10 and the projecting surface 11 are integrally formed from a single metal plate. First wall 8. Second wall9. Conductor piece 10 and overhanging surface 1
1 forms a radio wave attenuation cavity 12. The projection piece 14 protruding from the opaque dielectric cover 13 that blocks the entrance of the radio wave attenuation cavity 12 is hooked into the attachment hole 18 formed in the conductor piece 10 via the through hole 26 formed in the projecting surface 11. There is. A protruding piece 17 protruding from a translucent door outer cover 16 covering the outside of the door 5 is adapted to be caught on the end of a connecting surface 20 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. An impedance adjustment portion 25 that protrudes 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 12 . In addition, the conductor piece 10
An opaque sheet 19 is provided on the inner surface of the door outer cover 16 so as to face the door outer cover 16, 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.開口部を取シ囲むフランジ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ろ図のような
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
は平行板のキャン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
行板線路の長さ犯。
Next, the effects of the embodiment configured as described above will be explained. Heating chamber 1. The radio wave sealing effect will be qualitatively explained using a simple equivalent circuit as shown in FIG. 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 capacity of this line is proportional to the camp of the parallel plates, so the capacitance 21 becomes larger as the gap of the planar contact portion becomes 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 were no overhanging surface 11, the electric field would be distributed as shown in Figure 5, and the length of the parallel plate line would be affected.

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。電波減衰空胴12の周壁の厚さは実用上、自由空
間波長λに比べて十分小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。
That is, the depth of the radio wave attenuation cavity 12 causes parallel resonance at approximately one quarter of the free space wavelength λ, and the impedance becomes maximum. In practice, the thickness of the peripheral wall of the radio wave attenuation cavity 12 is sufficiently smaller than the free space wavelength λ, so it will be ignored in the description. In FIG. 3, which shows a simple equivalent circuit, it can be expressed as a parallel resonant circuit 22 in which a capacitance and an inductance are connected in parallel.

本実施例のように、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胴12の入口を狭める
ように折シ曲げて張出面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。
As in this embodiment, when the tip of the conductor piece 10 that is on the outermost peripheral wall of the radio wave attenuation cavity 12 is bent to narrow the entrance of the radio wave attenuation cavity 12 to form the projecting surface 11, as shown in FIG. The electric field distribution will be as follows. in this case.

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。これは第4図の電
波減衰空胴12人口における容量成分が犬きくなシ、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2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。
The lines of electric force between the end of the overhanging surface 11 and the first wall surface 8 are as follows:
It is much easier to crowd than in Figure 5. This means that even if the capacitance component in the radio wave attenuation cavity 12 shown in FIG. 4 is small, even if the inductance component is reduced by that much, resonance can be achieved at a specific frequency. That is, even if the depth 2 of the radio wave attenuation cavity 12 is made smaller than one-fourth of the free space wavelength λ, the maximum impedance can be obtained and leakage radio waves can be kept small.

なお、インピーダンス調整部25は、その誘電率の大き
さに比例して電波減衰空胴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lを
一層小さくするものである。
Note that the impedance adjustment section 25 has the effect of further increasing the capacitance component at the entrance of the radio wave attenuation cavity 12 in proportion to its dielectric constant, and further reduces the depth l of the radio wave attenuation cavity 12. be.

さらに、インピーダンス調整部25の断面形状として張
出面11の先端から第1の壁面8に近付くほど厚くして
いる。すなわち第4図のように電気力線の疎密に対応し
てインピーダンス調整部25の断面形状を選定し、少々
い材料で容量成分を増す効果を犬にしている。
Furthermore, the cross-sectional shape of the impedance adjustment portion 25 is made thicker as it approaches the first wall surface 8 from the tip of the projecting surface 11. That is, as shown in FIG. 4, the cross-sectional shape of the impedance adjustment part 25 is selected in accordance with the density of the electric lines of force, and the effect of increasing the capacitance component with a slightly thicker material is achieved.

さらに又、誘電体カバー13は突起片14と貫通穴23
、取付穴18との作用により確実に固着される。
Furthermore, the dielectric cover 13 has a projection piece 14 and a through hole 23.
, and are securely fixed by the action of the mounting hole 18.

発明の効果 以上のように1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る導体片の先端に張出面を設け、
更に張出面を覆う誘電体カバーを設け、その突起片を貫
通穴、取付穴にはめ込んだので、簡単な手段で電波減衰
空胴の深さを自由空間波長の4分の1より小さくでき、
ドアの薄形化が図れ、コンパクトな高周波加熱装置を提
供できる。
Effects of the Invention As described above, according to the present invention, an overhanging surface can be provided at the tip of the conductor piece that contacts the outermost peripheral wall of the radio wave attenuation cavity without providing a plurality of parallel plate lines (grooves) with different characteristic impedances. ,
Furthermore, a dielectric cover was provided to cover the protruding surface, and the protruding pieces were fitted into the through holes and mounting holes, so the depth of the radio wave attenuation cavity could be reduced to less than one-fourth of the free space wavelength by simple means.
The door can be made thinner, and a compact high-frequency heating device can be provided.

また、ドアを一枚の金属板から一体成形できる構成であ
シ1組立工数が低減でき、経済的波及効果も犬なるもの
がある。
Further, since the door can be integrally molded from a single metal plate, the number of assembly steps can be reduced, and the economic ripple effect is also significant.

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

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6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・・・フラノン。 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。 16・・・誘電体カバー、25・・・インピーダンス調
整部。
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, and FIG. 2 is a sectional view of a main part showing a radio wave seal part around the door. FIG. 6 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 its terminal ends short-circuited. 1... Heating chamber, 2... Furanone. 4... Small hole group, 5... Door. 6... Stepped portion, 7... Sealing surface. 8...First wall surface, 9...Second wall surface. 10... Conductor piece, 11... Projection surface. 16... Dielectric cover, 25... Impedance adjustment section.

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(
10)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、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)に誘電体カバー(13)の裏面に設けた突起片
(14)を引っ掛けることにより誘電カバー(13)を
ドア(5)に固着し、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)を一枚の金属板から成
形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 a door (5) that opens and closes the opening of the heating chamber (1), and which makes plane contact with the flange (2) of the opening of the heating chamber (1) when the door (5) is closed; This sealing surface (
A first wall surface (8) extends from the end of the first wall surface (8) substantially perpendicular to the flange (2), and a first wall surface (8) extends substantially parallel to the flange (2) from the end of the first wall surface (8). 2 wall surface (9), a large number of conductor pieces (10) approximately perpendicular to the flange (2) from the end of this second wall surface (9), and this conductor piece (
10) is provided with an overhanging surface (11) that overhangs from the tip of the heating chamber (1) toward the opening side, and is provided in the conductor piece (10) through a through hole (23) provided in the overhanging surface (11). The dielectric cover (13) is fixed to the door (5) by hooking the projection piece (14) provided on the back side of the dielectric cover (13) into the mounting hole (18), 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 formed from a single metal plate. High frequency heating device.
JP21537086A 1986-09-12 1986-09-12 Radio frequency heater Pending JPS6372094A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21537086A JPS6372094A (en) 1986-09-12 1986-09-12 Radio frequency heater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21537086A JPS6372094A (en) 1986-09-12 1986-09-12 Radio frequency heater

Publications (1)

Publication Number Publication Date
JPS6372094A true JPS6372094A (en) 1988-04-01

Family

ID=16671169

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21537086A Pending JPS6372094A (en) 1986-09-12 1986-09-12 Radio frequency heater

Country Status (1)

Country Link
JP (1) JPS6372094A (en)

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