JPS58209089A - Radio wave leakage preventing device - Google Patents

Radio wave leakage preventing device

Info

Publication number
JPS58209089A
JPS58209089A JP57089873A JP8987382A JPS58209089A JP S58209089 A JPS58209089 A JP S58209089A JP 57089873 A JP57089873 A JP 57089873A JP 8987382 A JP8987382 A JP 8987382A JP S58209089 A JPS58209089 A JP S58209089A
Authority
JP
Japan
Prior art keywords
choke
radio wave
wave leakage
cover
groove
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
Application number
JP57089873A
Other languages
Japanese (ja)
Other versions
JPS6235232B2 (en
Inventor
石野 健
康雄 橋本
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.)
TDK Corp
Original Assignee
TDK Corp
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 TDK Corp filed Critical TDK Corp
Priority to JP57089873A priority Critical patent/JPS58209089A/en
Priority to GB08230255A priority patent/GB2122059B/en
Priority to US06/438,256 priority patent/US4525614A/en
Priority to IT8268285A priority patent/IT1191223B/en
Priority to DE3242125A priority patent/DE3242125C2/en
Priority to FR8219333A priority patent/FR2527886A1/en
Publication of JPS58209089A publication Critical patent/JPS58209089A/en
Publication of JPS6235232B2 publication Critical patent/JPS6235232B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05BELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
    • H05B6/00Heating by electric, magnetic or electromagnetic fields
    • H05B6/64Heating using microwaves
    • H05B6/76Prevention of microwave leakage, e.g. door sealings
    • H05B6/763Microwave radiation seals for doors
    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05BELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
    • H05B6/00Heating by electric, magnetic or electromagnetic fields
    • H05B6/64Heating using microwaves
    • H05B6/6414Aspects relating to the door of the microwave heating apparatus

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) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 (技術分野) 本発明は、電子レンジ等のマイクロ波加熱装置におしl
″る電波漏洩防11.装置の改良に関する。
Detailed description of the invention (Technical field) The present invention provides
Regarding radio wave leakage prevention 11. Improvement of equipment.

(背景]支術) 従来、マイクロ波加熱装置(例えば電子レンジ)の本体
とJJ〔との隙間から電波が漏洩するのを防止ス乙)手
段、1−シて、ンールドバネによるメタルコンタクト方
式、及びチョーク結合方式あるいはゴムフェライト、カ
ーボンゴム等の電波吸収部材によるものが1ノ18案さ
れてい4)3゜ 第1図は従来の電波漏洩防止装置の断面図で、1はマイ
クロ波加熱装置の本体の壁、2は本体1のmll開開1
部に開閉口r1:に」IV、付けられた扉、3は庫内を
示す。)J〔2には本体1の前面開口部に対向する面の
周縁に金属仕りJ&4.5により庫内の励振電波の波長
の略1/4の長さに設定された電波減衰溝(以下チョー
ク溝という)6が設けられ、又このチョーク溝の外側に
ゴムフェライト、カーボンゴム等の電波吸収部材7が配
置され、前記チョーク溝6Vc塵埃等が溜まるのを防止
するためと前記電波吸収部」」7の押え付けを兼ね備え
たチョフカバー8か取イマ]けられている。このチョー
ク力・・−8はチョーク溝6内・\の%3’、 1lJ
tのJ11ヨ人を妨げl「いi’?lf材、例えはポリ
プロピレン等の低Rg ’jtq’、率(・」+・1に
より構成されている。9はプラスチック製の化粧ツノバ
ー、10はカラス板、1]は金網、12は取付子7.1
;(は本体1に把料げられたシールドバネて゛本体1と
罪2をメタルコンタクトにより市、波の漏洩をl>tt
 1.する。シールドバネの弾性劣化ある(・は金属酸
旧二物の被膜ができたような場合、又は本体と屏の間に
、ゴミのような絶縁物質が入り込んだ場合等にメタルコ
ンタクI・が不冗全となるときは、この隙間を通して電
波漏洩l〜ようとするh瓢この漏洩電波は前記チョーク
溝6によイ)′電気的抑制とTh:液吸収部材7による
電波吸収作用によって外部へ漏洩でろのを防止して(・
る。
(Background) Techniques) Conventionally, means for preventing radio waves from leaking from the gap between the main body of a microwave heating device (for example, a microwave oven) and a JJ are as follows: 1. A metal contact method using a rolled spring; There are 1 out of 18 proposals for the choke coupling method or those using radio wave absorbing materials such as rubber ferrite and carbon rubber.4) 3゜Figure 1 is a cross-sectional view of a conventional radio wave leakage prevention device, and 1 shows the main body of a microwave heating device. wall, 2 is the ml opening 1 of the main body 1
3 indicates the inside of the refrigerator. ) J [2 has a metal finish on the periphery of the surface facing the front opening of the main body 1. A radio wave attenuation groove (hereinafter referred to as choke Furthermore, a radio wave absorbing member 7 made of rubber ferrite, carbon rubber, etc. is arranged on the outside of this choke groove to prevent dust from accumulating in the choke groove 6Vc. The chop cover that combines the holding force of 7] is kicked. This choke force...-8 is %3' of choke groove 6, 1lJ
It is composed of a low Rg 'jtq' material such as polypropylene, and a rate (・'+1). 9 is a plastic decorative horn bar, and 10 is a plastic decorative horn bar. Glass plate, 1] is wire mesh, 12 is mount 7.1
(The shield spring held in body 1 connects body 1 and sin 2 with metal contact, and prevents wave leakage.
1. do. The elasticity of the shield spring has deteriorated (・ indicates that the metal contact I・ is not redundant due to the formation of a film of metallic acid, or when insulating material such as dust has entered between the main body and the screen. When this happens, radio waves will leak through this gap.The leaked radio waves will be leaked to the outside by the choke groove 6. To prevent (・
Ru.

しかしなから、従来の電波漏洩防11−装置は、チョー
ク溝が体積に占める削合が太き(・にもかかわt−)ず
充分な性能が出ないことも経験上明らかであるし、又部
品点数が多いことからそのηノ刊作業性か悪い為、最近
、件部、価格、量産性の観点から伸′2の改良方法がな
されている。例えば、チョーク力・・−を電波吸収機・
能を自1:る月別で構成したとか、あイ)(・はチ、1
−り溝の内部に電波吸収作用な配置す4)方法の1jl
案がなされている。例えば特公昭”、++1−IQ2)
(、牛l饅〉昭51−31982、実公昭56−160
68(:目l′1′−来の技術の例−r;l;、る3、
これらの方法はチョーク機rff″、を著しく低−1・
させるし、チョーク溝内部は′市1/11−・(1舷J
’r ’J(11度か強いΔ−め′Nイ波吸収部利を焼
損さぜイ)惧ねか3(・・I)実用に供+、 #rtな
い。
However, it is clear from experience that the conventional radio wave leakage prevention device does not have sufficient performance because the choke groove occupies a large amount of the volume. Due to the large number of parts, its workability is poor, so improvements have been made recently from the viewpoints of construction, cost, and mass production. For example, the choke force...- can be converted into a radio wave absorber...
It is said that Noh was organized by month.
- 4) Method 1jl of arranging a radio wave absorbing function inside the groove
A plan is being made. For example, “Tokukosho”, ++1-IQ2)
(Beef L Buns) Showa 51-31982, Jikko Showa 56-160
68(:l'1'-Example of the previous technology-r;l;,ru3,
These methods reduce the choke machine rff'', significantly lower -1.
The inside of the choke groove is
'r'J (11 degrees or strong ∆-me'N wave absorbing part will be burned out) I'm afraid 3 (...I) Not available for practical use, #rt.

(発明θ)、i’、li :l’Q )本冗明は、電波
漏洩ljJ、市装置βの改良に係り、上述(7,)如く
1/C来の欠点を改良しなされたもので、チっ−ク()
)機能イ1損゛なわぜずにナヨーク結合の構造を小1(
11にし、広・112賊となし、且つ部品点数を減丁こ
とにより安価で電波漏洩の抑制効果の高い装置を持供−
!r 6 o斗町゛、明によろ装置のt時機は、開閉可
能プ、0]Aを、5、く入閉1: 1.−1!:造り)
本体を有し、本体と扇の間の電波漏洩通路か1゛)の箱
;波漏洩を防止する装置に[・9いて、市;θヅ漏洩通
路に面する側で、本体または届の少/、cくとも一力に
チョーク溝を設け、該チョーク溝の人]二1をチョーク
カバーにより塞ぐ構j<1!をイ1し、At前記チョー
クカバーは磁性体と絶縁体の混合物で複素誘電率の実数
項ε′カ・15以下であり、11つ損失項でル)る (1帽に目A料から+14成され、Ail記チョーク溝
の外側に!M”I MLチョークカバーと同一材質で一
体に形成された′CLi、波吸収部分を有するごとき電
波漏洩防止装置にある。
(Invention θ), i', li :l'Q) This statement relates to the improvement of radio wave leakage ljJ and city equipment β, and has been made to improve the drawbacks of 1/C as mentioned above (7,). , tick()
) The structure of the Nayoke coupling can be changed to a small one (
By making it 11 and 112 wide, and reducing the number of parts, we have a device that is inexpensive and highly effective in suppressing radio wave leakage.
! r 6 o Tomachi ゛, the t time of the device by the light can be opened and closed. -1! : construction)
A box with a main body and a radio wave leakage passage between the main body and the fan; a box with a device to prevent wave leakage; /、c At least a choke groove is provided in one direction, and the person in the choke groove 21 is covered with a choke cover j < 1! The choke cover is a mixture of a magnetic material and an insulator, and the real number term ε' of the complex dielectric constant is less than 15, and the loss term is 11. The electromagnetic wave leakage prevention device has a wave absorbing portion formed integrally with the choke cover and made of the same material as the choke cover.

(発明のWlr成および作用) 図面は、本発明に係り、第2図はWltJ −2導彼管
21θ)−巨廣の一部にスリットをあけ、長さ1/4波
長のチョーク溝22(ギャビティ)を形成し、かりマイ
クロ波加熱装置の本体と屏の狭い電波A7i洩lll1
路を人為的に構成てろためにステップ変換器2;3を用
いた測定装置の断面図である。CIは、電波漏洩’、i
ff路に相当する通路24のキャンプ厚てあり、22′
はチョーク溝入[1を示す。又チョーク溝の長さを調整
出来ろように可変短絡板25を内装している。
(Wlr structure and operation of the invention) The drawings relate to the present invention, and FIG. This creates a narrow radio wave leakage between the main body and the screen of the microwave heating device.
3 is a sectional view of a measuring device using step transducers 2; 3 for artificially structuring the path; FIG. CI is radio wave leakage', i
The camp of the passage 24 corresponding to the ff road is thick and 22'
indicates chalk grooving [1]. Also, a variable shorting plate 25 is installed inside so that the length of the choke groove can be adjusted.

第3図は、1(i、θグik+i洩通路21内にあって
チョーク溝22の入1122’を塞ぐ部(g’ 2(i
 0) I(S、伺状態を示l〜、平板状γ′1ILI
材2+’+ (1!7み2.Fimm 、 長さ+5+
++m、 )は通路24内にル)−′)て人112Σ−
′な塞ぐどJl、:l;、漏洩電波方向に若干伸び、電
波吸収r?+X4gの役割もはた丁ようになっている。
FIG. 3 shows a portion (g' 2(i
0) I(S, indicates the open state l~, tabular γ′1ILI
Material 2+'+ (1!7 み2.Fimm, Length+5+
++m, ) is in the passage 24 (le)-') person 112Σ-
'Nagudo Jl, :l;, slightly elongated in the direction of leakage radio waves, radio wave absorption r? The role of +X4g is also similar.

ΔI/板状都旧として、表1に示すε′を変えた利料を
用いた。
The interest rates shown in Table 1 with different values of ε' were used as ΔI/plate-like capital.

表1にお見・て試料Nn1〜;3は、比較的誘電率が小
さく、磁気損失が大きいイ」刺Ni−M、−Zo系フェ
ライトの粉末とクロロブレンゴムとの混合物からなるゴ
ムフェライトで′A;)す、試料1’!′14〜7は誘
電率か大きく磁気損失が大きい利料Mn−Zn系フェラ
イトの粉末クロロプレンゴムとの混合物から7’:Cl
)コノ2フエライトでk)イ)。
As shown in Table 1, samples Nn1 to 3 are rubber ferrites made of a mixture of Ni-M, -Zo-based ferrite powder and chloroprene rubber, which have relatively low dielectric constants and large magnetic losses. 'A;) Sample 1'! '14 to 7 are from a mixture of Mn-Zn ferrite with high dielectric constant and large magnetic loss and powdered chloroprene rubber.7':Cl
) Kono2 ferrite k) b).

表1に示ゴー各神試4:l NIL I〜NIL7から
なるチョークカバーをチョーク人1−12:’に把料け
た場合の透過性1ノ1.な比較し評価する。測定力法は
、周波数2200〜2fifi(l M I I zの
範囲をスイープさせて、出力レベルをl・ng変換し、
較11゛シた後波形をオシロスコープで観測し、その波
彩:16よひ値がらその特性を評価した。
Table 1 shows the transparency when the chalk cover consisting of NIL I to NIL7 is grasped into the chalk person 1-12:'. Compare and evaluate. The measurement force method sweeps the frequency range of 2200 to 2fifi (l M I I z, converts the output level into l ng,
After the comparison, the waveform was observed with an oscilloscope, and its characteristics were evaluated based on the wave color: 16 value.

(7) 第4図は、チョーク入口を金属版で塞いだときすなわら
チョークなしとl〜だ場合の特性(曲線の)、チョーク
のみの」シin−、H−なわ(シ〕チョークの特性(曲
線中) ) %よO・第2図に示−・1−如(、試料直
1〜7の材料2(i (’、fig状がIIFさ2.5
v11n電波進行方向の寸法丁なわち長さl!’im+
++ )θ)゛旧友j影状のチョークカバーでチョーク
入(Iを塞いだ場合の!+、!l性(曲線■〜■)を示
した。、試本・1陥1〜7の(4旧は、誘電率ε′を4
5から・11.・1土て゛変化さぜたイ、の−C′ある
。チョークなしの場合、曲#j((〜のように’+N 
、1li41t(t、 、はとんど一定でO(出基準と
した。チョークのみの場合、曲線■のように2450 
MIIZで411を出θ)透1尚胤どなり漏洩電波は、
この周θシ数で゛火部分減良[7、チョークなしの透過
損の] / I 0O(10の電力しかJ’14過(ρ
111洩)していな(・1、−Jミ、−り人11を電波
吸収7111H材試料%1〜7で塞いだ場合の4!1l
l1曲線(1)〜(7)から、ε′が比較的小さい15
以下の陽1〜陥・1によ、5いて特性はピーク値をもち
、チョークのみθ) !l’、’r性と比較して広帯域
と15[ろ。但I〜、最小1ffQ過111゛の値は若
干大きくなると共に、そのときの周波数は2450MI
IZから低い(8) 方に推移1〜で(・ろことかわかる。又、ε′が大きく
20以上のlNn、 5〜Nα7において特性は、はと
んどピーク値がみられな(チョークの影響による多少の
減衰はみられろが、はとんど平坦な減衰を示している。
(7) Figure 4 shows the characteristics (curves) when the choke inlet is closed with a metal plate, that is, when there is no choke and when there is a choke. Characteristics (in the curve) ) % 0 ・ Shown in Figure 2 - 1 - As (, Samples 1 to 7 Material 2 (i (', fig shape is IIF 2.5
v11n Dimensions in the direction of radio wave propagation, that is, length l! 'im+
++ ) θ) ゛Old friend j The shadow-shaped chalk cover shows the !+, !l characteristics (curves ■ to ■) when I is blocked. Previously, the dielectric constant ε' was set to 4
5 to 11.・There is -C' in 1. Without choke, song #j (('+N like ~
, 1li41t (t, , is almost constant and O (output standard). In case of only choke, 2450 as shown in curve ■
MIIZ outputs 411 θ) Toru 1 Naotane roaring leaked radio waves are
At this number of cycles θ, the fire part decreases [7, transmission loss without choke] / I 0O (only 10 power exceeds J'14 (ρ
111 leak) (・1, -Jmi, -rihito 11 is blocked with radio wave absorbing 7111H material sample %1~7) 4!1l
From l1 curves (1) to (7), ε' is relatively small15
According to positive 1 to negative 1 below, the characteristic 5 has a peak value, and only choke θ)! Broadband and 15[ro] compared to l','r characteristics. However, the value of minimum 1ffQ over 111゛ becomes slightly larger, and the frequency at that time becomes 2450MI.
It can be seen that there is a transition from IZ to low (8) at 1~(・low). Also, when ε' is large and 20 or more, lNn, 5~Nα7, the characteristic hardly shows a peak value (choke). Although there is some attenuation due to the influence, the attenuation is mostly flat.

特に、材料]東7ε’ = 41.4  の材料におい
ては、チョークの影響は7よ<磁性体1東7の透過減衰
のみの特性となっている。このことは、ε′が大きい場
合試料自体からの反射が太き(、チョーク内部に電波が
入り込まないためと考えられろ。
In particular, in the material of [Material] East7ε' = 41.4, the influence of the choke is characterized only by the transmission attenuation of 7<magnetic material 1 East7. This is thought to be because when ε' is large, the reflection from the sample itself is thick (and the radio waves do not enter the inside of the choke).

次に、第4図に示す如く材料により最小透過量点が低周
波の方にずれているが、チョークの長さを短か(すれば
、チョークによる周波数特性はその状態にもとて事がで
き、2450MTfzで最小の透過量−を得られろと推
定され第2図の可変旬絡叛25によりチョーク寸法を調
整(チョーク寸法を小さく1−ろ)することにより中心
周波数2450MI−Tzに最小の透過量点を移動させ
て(0,5mm〜](1mm程度移動)チョーク入口に
磁性体を配置したときの特性を測ボした。その結果、第
5図の特性が得られた。第5図から分るように、ε′が
約15JJ、下の試料Nn1〜4に:1dいてチー1−
りの機能が生かされ、かつチョークのみの%1’lと比
べ広帯域な特性を得ることが出来ろことが判明した。尚
、ε′が20以上の試料NC,,5〜7におし・ては、
やはり反射が大きくチョークの内(flISに充分市1
波が人らjcいためチョーク特性が生かされず、充分小
さな透過量を得ることが出来な(1゜ 第5図の結果によりε′の影響が大きいことが分った為
、試料N11〜7のε′値と、最小の透過量および透過
ij1ンJ’2(blll 、J、り少ない領域(帯域
中)と、利1・1がもつ透過減衰]11111′lを表
2にまとめた。又、ε′と特性値の関係を第6図、第7
図に示す。第6図は、ε′と最小減衰[11値の関係で
あり、87図は、ε′と帯j火中の関f糸でル)ろ。こ
のことより、ε′がほぼ15」ソ、下の場合、チョーク
のみの最小透過量より多少悪()、【ろが、実用的に充
分な特性である2、5 dB」ン、上の712を性が得
られ且つ帯域[1〕も240MITzす、上の光分な’
l!l”性が111られろ。第6図、第7図よりε′が
15伺近を境として急激な!14′性劣化を示すことが
分イ)。
Next, as shown in Figure 4, the point of minimum transmission is shifted toward lower frequencies depending on the material, but if the length of the choke is shortened (if this is done, the frequency characteristics due to the choke will change significantly in that state as well). It is estimated that the minimum transmission amount can be obtained at 2450 MTfz, and by adjusting the choke size (by reducing the choke size by 1-) using the variable frequency filter 25 shown in Fig. 2, the minimum transmission amount can be obtained at the center frequency of 2450 MTfz. We measured the characteristics when the magnetic material was placed at the choke inlet by moving the permeation point (from 0.5 mm to 1 mm).As a result, the characteristics shown in Figure 5 were obtained.Figure 5 As can be seen, ε' is about 15JJ, and the samples Nn1 to 4 below have 1d and Q1-
It has been found that the new function of the choke is utilized, and that it is possible to obtain a broadband characteristic compared to the choke only. In addition, for samples NC, 5 to 7, where ε′ is 20 or more,
After all, the reflection is large inside the chalk (sufficient city 1 for flIS)
Because the waves were small, the choke characteristics were not utilized, and a sufficiently small amount of transmission could not be obtained (1°). ' value, minimum transmission amount, transmission ij1-J'2 (bll, J, less area (in the band), and transmission attenuation of gain 1.1)11111'l are summarized in Table 2. Also, The relationship between ε′ and characteristic values is shown in Figures 6 and 7.
As shown in the figure. Figure 6 shows the relationship between ε' and the minimum attenuation [11 value], and Figure 87 shows the relationship between ε' and the relationship between ε' and the band j. From this, it can be seen that when ε' is approximately 15" or lower, it is slightly worse than the minimum transmission amount of only a choke (2.5 dB"), which is a practically sufficient characteristic (712). , and the band [1] is also 240 MITz.
l! It can be seen from Figures 6 and 7 that ε' shows a rapid deterioration of !14' as it approaches 15 degrees.

表    2 尚、電波吸収特性も、この場合活用されており、表1に
示すように、透過減衰量2dB/mす、」−の特性を試
料陥1〜7の材料は有しているため減衰効果も十分生か
され帯域中も広くなっている。
Table 2 The radio wave absorption characteristics are also utilized in this case, and as shown in Table 1, the transmission attenuation is 2 dB/m. The effect is fully utilized and the band is widened.

又、第2図の寸法dが大きくなってチョーク機能が劣化
したとしても材料の減衰特性により電波漏洩防止効果を
発揮する。表1の試料歯3と崗4のl;ma2.を比較
同ソ)と、171)と0.70であり透過減衰量ど;て
g、42+lll/c+nど7.27+llt/Cmで
大きな差がある。、−(’f、cわちフェライト利質に
よって透過減衰量が大きな変化な示すが、J光過減衰計
に大きく寄与’f 7;)l;ma、、 (7+“/μ
′)は、(l(1の試料1東]のtanδ1が0118
のどき透過減衰111α(C出/cm )は2.37d
B/mであることから少l、[くとも半分以上の電波が
減衰する3rlllを得るには、はぼ05以」二を必要
とする。チョークツノバー形状は、電波漏洩通路に面し
た表面を平面となし、チョークl’J rfBに向って
突出するようにしたことによって一4→]iのアンテナ
効果により電波のチョーク内部への進入が良くなり、そ
のチョーク機能を損なわず特性を改善できるとも云える
Further, even if the choke function deteriorates due to the increase in the dimension d in FIG. 2, the radio wave leakage prevention effect is still exhibited due to the attenuation characteristics of the material. l of sample tooth 3 and grout 4 in Table 1; ma2. The transmission attenuation amount is 7.27+llt/Cm, which is 0.70, and there is a large difference in transmission attenuation. , -('f,c, the transmission attenuation varies greatly depending on the ferrite quality, but it greatly contributes to the J optical overattenuation meter'f 7;)l;ma,, (7+"/μ
') is (l(sample 1 east of 1) tan δ1 is 0118
Throat transmission attenuation 111α (C output/cm ) is 2.37d
B/m, so to obtain 3rllll, which attenuates at least half of the radio waves, requires at least 05"2. The shape of the choke horn bar is such that the surface facing the radio wave leakage path is flat and protrudes toward the choke l'J rfB, thereby preventing radio waves from entering the choke due to the antenna effect of 14→]i. It can be said that the characteristics can be improved without impairing the choke function.

試料1寛3を用い、T4′l、8図(イj仲)C→に示
した如く第2図のギートビティ22の入1−122/を
塞ぐ取付は状態を変えた場合の特性を第9図に示す。第
8図(イ)は平板であり、第8図(ロ)は凸状で、第8
図e・)はさらに凸を太き(チョークギャビティ内に突
出した形状である。いずれも、チョーク特性をあまり損
なゎ(11) ず、広い帯域が得られている。
Using sample 1-3, as shown in T4'l, Figure 8 (Ij-naka) C→, the installation that closes the entrance 1-122/ of Geetbitty 22 in Figure 2 shows the characteristics when changing the condition. As shown in the figure. Figure 8 (a) is a flat plate, Figure 8 (b) is a convex shape, and
In Figure e), the convexity is even thicker (it has a shape that protrudes into the choke gap).In both cases, the choke characteristics are not significantly impaired (11), and a wide band is obtained.

以上の如(、本発明によると、チョークの機能をそれほ
ど損わせずに、かつチョークの構造を小型にでき、かつ
チョーク内部への塵埃の進入阻止と共に電波吸収機能を
兼ね備えさせたことにより、電波漏洩防止の効果をより
一層増大させろことができろ。又、部品点数を減すこと
により安価な装置を提供出来る。
As described above (according to the present invention), the structure of the choke can be made compact without significantly impairing the function of the choke, and it also has a function of absorbing radio waves while preventing dust from entering the inside of the choke. It is possible to further increase the leakage prevention effect.Also, by reducing the number of parts, an inexpensive device can be provided.

以下に、本発明の実施例を示す。Examples of the present invention are shown below.

(実施例1) 第10図に、実施例1の電波漏洩防止装置の断面図を示
−J’−o符号は第1図と同一であるので、同一符号部
分の説明は省略する。14は、チョークカバーで、フェ
ライト粉末とゴム又はプラスチック等の絶縁物との混合
物試料歯3からなり、その一端L4aは、金属仕切板2
5と係合するようにカギ形に形成され、他端14bはチ
ョーク溝の入口を塞いで外方に延長し、化粧カバー9の
端部で固定されて(・る。すなわち、チョークカバーは
その表面が本俸10対向壁1′に対し、はぼ平行平面と
され、チ(12) ヨーク溝の入1’−’l :i6よび隣室6′の入口部
分を塞ぐように取イζjけられている1、 (実施例2) 第11図(A+及び(11)に、実施例2の電波漏洩防
止装置の断面図を示す。IIIはチョークカバーで、フ
ェライト粉末とゴム又はプラスチック等の絶縁体との混
合物からなり、その一端は金属仕切板5と保合−「るよ
うにツyギ形に形成され、他端はチョーク溝の入1■1
を塞いで外方に延長し、化粧カバー9の端部で固定され
ている。チョークカバーの表面は、本体1の対向壁1′
に対l〜でほぼ平行平面とされ、裏面にはチョーク7)
/f6の内方に突出する突出部141が一体に形成され
ている。突出部は第11図(Blのごとく、適当な間隔
でドアの周辺部に複数個もうけられろ。この突出部はア
ンテナとして作用し電波をチョーク溝内に放出するので
電波吸収特性が向上同一る。
(Example 1) FIG. 10 shows a cross-sectional view of the radio wave leakage prevention device of Example 1. Since the symbols -J'-o are the same as those in FIG. 1, explanation of the parts with the same symbols will be omitted. Reference numeral 14 denotes a chalk cover, which consists of a mixture sample tooth 3 of ferrite powder and an insulating material such as rubber or plastic, and one end L4a of which is connected to a metal partition plate 2.
5, and the other end 14b extends outward to close the entrance of the choke groove, and is fixed at the end of the decorative cover 9. In other words, the choke cover The surface is made almost parallel to the main wall 10 and the opposite wall 1', and the yoke groove 1'-'l is set so as to close the entrance part of i6 and the adjacent chamber 6'. (Example 2) Figure 11 (A+ and (11) shows a cross-sectional view of the radio wave leakage prevention device of Example 2. III is a choke cover, which is made of ferrite powder and an insulator such as rubber or plastic One end is formed into a cylindrical shape to fit with the metal partition plate 5, and the other end is formed with a chalk groove.
It closes and extends outward, and is fixed at the end of the decorative cover 9. The surface of the choke cover is the opposite wall 1' of the main body 1.
It is considered to be a nearly parallel plane with l ~, and there is a chalk on the back side 7)
A protrusion 141 that protrudes inward at /f6 is integrally formed. As shown in Figure 11 (Bl), a plurality of protrusions should be provided around the door at appropriate intervals.These protrusions act as antennas and emit radio waves into the choke groove, improving the radio wave absorption characteristics. .

(実施例3) 第12図は実施例3の電波漏洩防止装置の断面図である
1、14はチー1−フカバーで、フェライト粉末とゴノ
、又はプラスチック等の絶縁体との混合物から1cす、
チョークツノバーの表面は本体1の対向壁1′に対して
平行平面とされ裏面には、チョーク溝6の外側にあって
、金属仕切板4と15で囲まれた狭い空室内に挿入され
た電波吸収体142が一体に形成されている。この電波
吸収体142は第12図(B)のごとくドアのほぼ全周
にもうけられる。
(Example 3) Figure 12 is a cross-sectional view of the radio wave leakage prevention device of Example 3. Reference numerals 1 and 14 are chief covers, and 1 c is made from a mixture of ferrite powder and an insulator such as gono or plastic. ,
The front surface of the choke horn bar is a plane parallel to the opposing wall 1' of the main body 1, and the back surface is inserted into a narrow cavity surrounded by metal partition plates 4 and 15, which is located outside the choke groove 6. A radio wave absorber 142 is integrally formed. This radio wave absorber 142 is provided almost all around the door as shown in FIG. 12(B).

(実施例4) 第13図は囚及び(B)、実施例4の電波漏洩防止装置
の断面図である。14はチョークカバーで、フェライ]
・粉末とゴム又はプラスチック等の絶縁体との混合物か
らなりチョークカバーの表面は、本体1の対向壁1′に
対して平行平面とされ裏面にはチョーク溝6の内方に突
出する突出部141とチョーク溝6の外側]にあって金
属仕切板4と15で囲まれた狭い空室内に挿入された電
波吸収部材142とが一体に形成されている(第13図
(B))。実施例1〜4共に、ドア周辺に額縁状に取り
つけられてもよいし、数本の棒状のものでドア周辺を囲
むように取りつけられてもよい。
(Example 4) FIG. 13 is a cross-sectional view of the radio wave leakage prevention device of Example 4. 14 is a choke cover, Ferai]
- The surface of the choke cover made of a mixture of powder and an insulator such as rubber or plastic is a plane parallel to the opposing wall 1' of the main body 1, and the back surface has a protrusion 141 that protrudes inward of the choke groove 6. and a radio wave absorbing member 142 inserted into a narrow cavity surrounded by the metal partition plates 4 and 15 outside the choke groove 6 are integrally formed (FIG. 13(B)). In all of Examples 1 to 4, it may be attached to the periphery of the door in a frame-like manner, or it may be attached so as to surround the periphery of the door using several rod-shaped objects.

」−記谷実施例の変形も1.(は修飾は種々可能である
。第11図に1)及び(1))はチョークカバー14の
固定構造の例で、(21)は化むレノバーりの端部でチ
ョークカバー1−+を押えろものでル)ろ。このとき電
波吸収部イ]1・12か右在する実施例ではこの部材を
空室の壁でおさえ乙)ことにより支」\〜してもよい。
”-Variations of the Kiriya example are also 1. (1) and (1) in Fig. 11 are examples of the fixing structure of the choke cover 14, and (21) is an example of the fixing structure of the choke cover 14. It's erotic. At this time, in embodiments in which the radio wave absorbing parts 1 and 12 are located on the right side, this member may be supported by holding it against the wall of the empty room.

第14図(blは支切板5にスナップ動作のピン5aを
立て、チョークツノバート1にこれに対応する孔をもう
け、該ピンによりチョークカバー14を固定する構造を
示す。なおピンをチョークカバーにもうけ、支切板にも
うけた孔に、Vリスナツプ動作で固定させてもよい。第
1・1図(C)は空室を除去した構造で第10図、及び
第11図の場合には空室を除去l〜でもさしつかえない
。第14図(d)4:r、 第’ l 1図(A+ 、
 (川及び第13図囚。
Figure 14 (bl shows a structure in which a snap-action pin 5a is set up on the dividing plate 5, a corresponding hole is made in the choke horn bar 1, and the choke cover 14 is fixed with the pin.The pin is attached to the choke cover It may also be fixed in a hole made in the dividing plate using a V-resnap operation. Figures 1 and 1 (C) have a structure in which the empty space has been removed. It is okay to remove the empty room l~.Figure 14(d) 4:r,
(River and Figure 13 Prisoner.

(Blにおけろ突起11、の;tつの形状(台形、円柱
、正角錐)を示¥。又チョークツノバーの材質はフェラ
イトとゴムの混合物の他、ノJライトと合成樹脂の混合
物とすることイ)可能であ4)。なおチョークカバーは
細長の4辺により構成されろ長方形の額縁状であり、4
辺を一体構成と−[ることも可能であり、又は4辺を別
々に構成してチョーク溝の壁に固定することも可能であ
る。
(In Bl, the protrusion 11 has three shapes (trapezoid, cylinder, and square pyramid).The material of the choke horn bar is a mixture of ferrite and rubber, as well as a mixture of ferrite and synthetic resin. It is possible (a) and (4). The chalk cover is shaped like a rectangular picture frame and consists of four long and narrow sides.
It is also possible for the sides to be of integral construction, or for the four sides to be constructed separately and fixed to the wall of the choke groove.

(発明の効果) 以」二説明したごと(、本発明によるとチョークカバー
を磁性材で構成することにより広帯域で構造が単純で吸
収特性の優れた電波漏洩防止装置が借られろ。
(Effects of the Invention) As explained above, according to the present invention, by constructing the choke cover with a magnetic material, a radio wave leakage prevention device with a wide band, simple structure, and excellent absorption characteristics can be obtained.

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

第1図は従来の電波漏洩防止装置の断面図、第2図は測
定装置の要部断面図、第3図はチョークカバーを装着し
た状態図、第4図と第5図はチョークカバー試料N[l
l〜陥7を用いたときのチョークありとチョークなしの
ときの周波数特性図、第6図と第7図はε′の違いによ
る透過量および帯域11]特性図、第8図(イ)(ロ)
e・)は、裡々形状のチョークカバーを装着した状態図
、第9図は第8図(イ)(ロ)e・)の形状にした試料
Nn3を用いたときの周波数特性図、第10図、第11
図(A)及び(Bl、第12図(A)及び(Bl、及び
第13図(A)及び(Blは、本発明による構造例、第
1・1図(a)〜(djは本発明の各種修飾例である。 (17)A11 (9−1−弓の説、明;り−12図(A))6;チョー
ク溝 14;チョークツノバー 1112;′III波吸収j%B分 特許出願人 東京電気化学工業株式会社 特許出願代理人 弁理± 111  本 恵 − (18) 罠6図 第57 図 誘電竿と′ 早、8 図 (イ) (ロン (ハ) 乳70図 為l1図(A) 罠//図(Bう 底13図(A> 奉13図(8) 與14閉((L)     底74図ζb)襄14(2
)(リ シ
Fig. 1 is a cross-sectional view of a conventional radio wave leakage prevention device, Fig. 2 is a cross-sectional view of the main part of the measuring device, Fig. 3 is a state diagram with a choke cover attached, and Figs. 4 and 5 are choke cover sample N. [l
Figures 6 and 7 show the transmission amount and band 11] characteristic diagram depending on the difference in ε', and Figure 8 (a) ( B)
Fig. 9 is a frequency characteristic diagram when using sample Nn3 with the shape shown in Fig. 8 (a), (b), and e). Figure, 11th
Figures (A) and (Bl), Figures 12 (A) and (Bl), and Figures 13 (A) and (Bl) are structural examples according to the present invention, and Figures 1 and 1 (a) to (dj are structural examples according to the present invention). (17) A11 (9-1-Explanation of the bow, clear; Ri-12 (A)) 6; Choke groove 14; Choke horn bar 1112; 'III wave absorption j%B patent Applicant Tokyo Denki Kagaku Kogyo Co., Ltd. Patent Application Attorney ± 111 Megumi Moto - (18) Trap 6 Figure 57 Dielectric rod and ' Early, 8 Figure (A) (Ron (C) Breast 70 Figure 1 ( A) Trap//Figure (B bottom 13 figure (A> Bō 13 figure (8) 與 14 close ((L) bottom 74 figure ζb) 襄 14 (2
) (Rishi

Claims (1)

【特許請求の範囲】 開閉5f能な扇をふくみ閉じた構造の本体を有し、本体
と用の間の電波漏洩通路からの電波漏洩を防止する装置
において、電波漏洩通路に面する側で、本体または扇の
少なくとも一方にチョーク溝を設け、該チョーク溝の人
口をチョークカバーにより塞ぐ構造を有し、前記チョー
クカバーは磁性体と絶縁体の混合物で複素誘電率の実数
項ε′が15以下であり、且つ損失項である る磁性材料から構成され、前記チョーク溝の外側に前記
チョークカバーと同一材質で一体に形成された電波吸収
部分を有することを特徴とする電波漏洩防止装置。
[Claims] In a device for preventing radio wave leakage from a radio wave leakage path between the main body and the device, the device has a body having a closed structure including a fan that can be opened and closed by 5 f, on the side facing the radio wave leakage path, It has a structure in which a choke groove is provided in at least one of the main body or the fan, and the choke groove is closed by a choke cover, and the choke cover is a mixture of a magnetic material and an insulator, and the real number term ε' of the complex dielectric constant is 15 or less. A radio wave leakage prevention device comprising a magnetic material which is a loss component, and having a radio wave absorbing portion integrally formed of the same material as the choke cover on the outside of the choke groove.
JP57089873A 1982-05-28 1982-05-28 Radio wave leakage preventing device Granted JPS58209089A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP57089873A JPS58209089A (en) 1982-05-28 1982-05-28 Radio wave leakage preventing device
GB08230255A GB2122059B (en) 1982-05-28 1982-10-22 An absorber device for microwave leakage
US06/438,256 US4525614A (en) 1982-05-28 1982-11-01 Absorber device for microwave leakage
IT8268285A IT1191223B (en) 1982-05-28 1982-11-04 ELECTROMAGNETIC WAVES ABSORBING DEVICE TO PREVENT MICROWAVE DISPERSIONS
DE3242125A DE3242125C2 (en) 1982-05-28 1982-11-13 Wave absorber for a microwave oven
FR8219333A FR2527886A1 (en) 1982-05-28 1982-11-18 ABSORBING DEVICE FOR MICROWAVE LEAKS

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57089873A JPS58209089A (en) 1982-05-28 1982-05-28 Radio wave leakage preventing device

Publications (2)

Publication Number Publication Date
JPS58209089A true JPS58209089A (en) 1983-12-05
JPS6235232B2 JPS6235232B2 (en) 1987-07-31

Family

ID=13982881

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57089873A Granted JPS58209089A (en) 1982-05-28 1982-05-28 Radio wave leakage preventing device

Country Status (1)

Country Link
JP (1) JPS58209089A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0338799Y2 (en) * 1987-11-24 1991-08-15

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5040255A (en) * 1973-08-16 1975-04-12
JPS511556U (en) * 1974-06-21 1976-01-08

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5040255A (en) * 1973-08-16 1975-04-12
JPS511556U (en) * 1974-06-21 1976-01-08

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0338799Y2 (en) * 1987-11-24 1991-08-15

Also Published As

Publication number Publication date
JPS6235232B2 (en) 1987-07-31

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