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JP4257987B2 - Portable wireless device - Google Patents
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JP4257987B2 - Portable wireless device - Google Patents

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Publication number
JP4257987B2
JP4257987B2 JP33701299A JP33701299A JP4257987B2 JP 4257987 B2 JP4257987 B2 JP 4257987B2 JP 33701299 A JP33701299 A JP 33701299A JP 33701299 A JP33701299 A JP 33701299A JP 4257987 B2 JP4257987 B2 JP 4257987B2
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Japan
Prior art keywords
shield case
antenna
substrate
magnetic film
film
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JP33701299A
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Japanese (ja)
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JP2001156484A (en
Inventor
信二 田邉
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Mitsubishi Electric Corp
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Mitsubishi Electric Corp
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Description

【0001】
【発明の属する技術分野】
本発明は、携帯電話などの移動体携帯無線機の、電磁シールド技術に関する。
【0002】
【従来の技術】
携帯電話などの移動体無線機は、一般に送信のためのRF(高周波)回路と、受信のためのデジタル回路からなる。送受信が同時に行われるタイプの無線機では、受信部と送信部の相互干渉、受信部デジタル制御回路からのEMI(Electromagnetic Interference 電磁干渉)抑制のため、電磁シールドが必要となる。また、現在日本の携帯電話の主流であるPDC(Personal Digital Communications)方式のように、送受信が同時に行われないタイプの無線機においても、送信波が、RF回路内の変調回路のPLL(Phase Locked Loop)などに回り込むことによる変調度の劣化を防ぐため、電磁シールドが必要となる。また、変調回路は、その性格上長い伝送路を用いることができないため、アンテナのできるだけ近くに配置するため、シールドに要求される仕様も、より厳しいものとなっている。
【0003】
図6は従来の携帯無線装置としての携帯電話の内部を示す概略図であり、1はシールドケース、2は送信回路や受信回路が組み込まれた基板、3は回路基板上に設けられた接地パターン、4はシールドケース1から引き出されたアンテナ、5は電気接触子である。
【0004】
シールドケース1は、板金、または、ABS(アクリロニトリル ブタジエン スチレン)材のようなプラスチックに、Cu、Niなどの金属膜を無電解メッキ、蒸着などで積んだ「箱形」に形成され、このシールドケース1を基板2の送信回路等の高周波RF回路がある部分を覆うようにかぶせて用いている。この場合、ただかぶせただけでは、シールドケース1は、フローティングで浮いた形となり、シールドとして動作しない。電磁シールドとしては、RF部ののっている基板の縁にある接地パターン3と電気的接触を取り、回路を覆うようにする必要がある。一般に、シールドケースに用いる薄い板金や、金属膜を均一に基板の導電部と接触させることは不可能であり、突起やバネなどの電気接触子5を用いて、定点で確実に電気接続を採る方法が用いられている。その中でも、バネを用いて接触をとる方法は、最も確実な方法として、多くの携帯機で用いられている。また、電気接触子5の配置は、図6に示すように、従来は、アンテナの近くはより密に、アンテナから遠い部分は疎に配置している。1
【0005】
【発明が解決しようとする課題】
電磁シールドをするためには、シールドケースと下の基板との電気的な接続を何カ所かとり、隙間から電磁波が漏れないようにする必要がある。従来は、シールド金属に流れる誘導電流の方向を考えずに、闇雲に、ほぼ等間隔に、あるいは、アンテナに近い部分を集中的に電気接触子を配置して電気接触をとっていた。特にアンテナから遠い下端では、電気接触子を減らしていた。このため、シールド効果が弱くなることもあった。
【0006】
また、シールドケースをプラスチックに金属薄膜をコーティングしたものを用いる場合、金属膜として、センダスト(FeAlSi)磁性粉体などを塗布した例はあるが、これらの磁性体は、現在の携帯電話が用いている1GHz近傍もしくはそれ以上の高周波では、比透磁率はほとんど1であり、効果を発揮しない。
【0007】
この発明は上記のようなシールドに関する問題点を解決するために行われたもので、確実なシールドを簡単な構成で得ることを目的とする。
【0008】
【課題を解決するための手段】
この発明に係る携帯無線装置においては、アンテナから電波を放射する時にシールドケースに誘起される高周波誘起電流のうち、シールドケースから上記基板の接地パターンに流れる電流成分の電流密度が高い部分で上記電気接触子の配置密度を高くしたものである。
【0009】
また、アンテナがシールドケースから引き出される位置の近傍、およびアンテナがシールドケースから引き出される位置から遠い部分で上記電気接触子の配置密度を高くしたものである。
0010
さらに、シールドケースは樹脂表面に導電性膜を形成した部材で構成され、導電性膜上にさらに異方性磁性膜を積層し、この異方性磁性膜の磁化容易軸方向をアンテナに流れる電流と同じ方向にしたものである。
0011
また、異方性磁性膜を異方性グラニュラー膜としたものである。
0012
【発明の実施の形態】
実施の形態1.
図1は本発明の実施の形態1を示す概略図である。図5の従来のものと、構成はほぼ同じであり、1はシールドケース、2は送信回路、受信回路や論理回路等が組み込まれた基板、3は基板2上に設けられた接地パターン、4はシールドケース1から引き出されたアンテナ、5は電気接触子である。ここで、電気接触子5はアンテナに近い上部と、アンテナから遠い下部でその配置密度を高く配置している。このように配置する理由は、発明者らが電磁波解析した結果、アンテナの鏡像電流の流れる方向である上下端に重点的に、シールドケース1から電気接触子5を通じて接地パターン3へ流れる電流が阻止されないように電気接触をとることで、内部回路への送信波の回り込みを減少できることがわかったためである。アンテナに近い上端だけでなく、従来は電気接触の強化を図っていなかったアンテナと反対側である下端でも、電気接触を良くする手段をとることで、脇からの電磁回り込みを減少させる。
0013
電気接触子5をこのように配置することで、電気接触子5の数を従来のものと同じにしても、シールド効果が高いものが得られる。また、電気接触子5の数を減らしても従来と同じシールド効果が得られることになる。なお、ここでは側方には電気接触子5を設けないものを示しているが、もちろん側方にも少量の電気接触子を設けても良く、特にアンテナに近い側方上部に設けるのは効果があるのは言うまでもない。
0014
図2は電気接触子5の例を示すものである。電気接触子として、バネ性の金属5を基板2の接地パターン3にハンダ51等で電気接触を確実にして固着したもので、シールドケース1を基板2にネジ(図示しない)等で基板側に押し付けるようにして、電気接触子であるバネ性の金属5をシールドケース1の金属膜1aと確実に接触させる。このようにして確実に電気接触を確保するが、ここで、電気接触子5の数は少ないほど重量が軽くなり、組立て工程も単純となり、コストも低減できる。携帯電話等の携帯無線装置にあっては、少しでも重量を軽く、コストを安く、という要求が強く、これらの効果は非常に大きい。本発明によれば、シールド効果の高い部分に重点的に電気接触子5を配置することで、より少ない数の電気接触子でより大きなシールド効果が得られるものである。なお、電気接触子5としてここではバネ性の金属のものを示したが、これに限られるものではなく、接地パターン上に金属の突起を設けたようなものでも良く、接地パターン3とシールドケースの金属部分とが良好に電気接触する手段を設けたものであれば良い。
0015
以上の効果を、解析結果を用いて説明する。図3はシールドケースと基板の電気接触状態を3種類変えて、シールドケース内部の基板2上での電界強度分布を3次元有限要素法電磁界解析で計算したものである。図3(a)は、シールドケースを基板に載せただけで、基板との電気接触がとれていない場合、(b)は、シールドボックスの左右の側方のみ電気接触を取った場合、(C)は、上下部分も電気接触を取った場合を示しており、斜線部分は、電界強度の値がある値よりも高い領域を示す。図3(b)は図3(a)と比較して、斜線部の面積はほとんど変わっていない、すなわち側方での電気接触はほとんど効いていないことがわかる。これに対し、図3(c)では斜線部分の面積が大幅に減少しており、上下方向の電気接続は極めて良く効いていることがわかる。
0016
以上は、アンテナからの送信波により誘起されるシールドケースの表面電流(高周波誘起電流)は、主にアンテナの電流が流れる方向、すなわち、シールドケースの上下方向に流れるよう誘起されるためであり、アンテナから遠い、シールドケース下端でもシールドケースから接地パターンに流れるように、すなわち接触部を横切るように高周波誘起電流が流れており、この部分に重点的に電気接触を取れば、シールド効果が高くなるからと考えられる。またシールドケース側方では接触部を横切る高周波誘起電流は少ないため、電気接触はシールドにほとんど影響せず、電気接触を良くする手段を多く設ける必要はない。このように、シールド効果を上げるためには、高周波誘起電流と直交する方向に接触面がある場合、この部分が細くて長いスリットにならないよう電気接触を良くする手段を設けることがシールド効果向上に不可欠である。
0017
実施の形態2.
図4は、本発明の実施の形態2を説明する携帯無線装置の内部概略図である。図4において、シールドケース1aは、CuやAlなどの導電性金属シールド膜上に、Niなどの磁性膜を積層し、しかも図中6の矢印で示すように、磁性膜の磁化容易軸方向を上下方向、すなわち高周波誘起電流と同じ方向にしている。このようにすることで、横方向での高周波透磁率を高く保つことができ、電波の反射係数を大きくする、すなわち高いシールド効果が得られる。
0018
ここで、Niのように一般によく用いられる磁性膜は、携帯電話で使用されている数100MHz〜数GHzといった高い周波数では透磁率が低くなり、上記効果が小さくなる。このような膜であっても、異方性を付加すれば、その磁化困難軸方向では高周波領域での透磁率の低下が小さくなり、上記効果が得られる。また、異方性FeAlOグラニュラー系軟磁性膜(異方性グラニュラー膜)のような異方性磁性膜であれば、磁化困難軸(磁化容易軸と直交方向)の透磁率は、1GHz以上でも、高い透磁率が得られる。すなわち、異方性グラニュラー膜であれば、磁化容易軸方向を高周波誘起電流と同じ方向にすることで、携帯電話で使用されている、数100MHz〜数GHzといった高い周波数でも良好な磁性膜として用いることができ、本実施の形態による効果が顕著となる。
0019
図5は、磁性による3次元有限要素法電磁界解析を用い、CuやAlなどの導電性金属シールド膜上に、比透磁率100の磁性膜を100オングストロームの厚さで積層した場合について、周波数940MHzの高周波において、アンテナ電流の値を0dBとして、基板上の長さ10mmのマイクロストリップ線路に対し、−80dBのアイソレーションがとれる領域がどれだけ広がるかを計算したものである。ここでは、基板がシールドされている部分が、より実際の携帯無線装置に近い形状で計算している。図4(a)は磁性膜がない場合、図4(b)は磁性膜がある場合の計算結果を示す。図の斜線部分が、アイソレーションが−80dBよりも低い領域を示す。磁性膜が有る場合には斜線部はほとんどなく、本発明により、シールド特性は格段に向上することが明らかにされた。このように、わずか100オングストロームの磁性膜でもシールド効果としては非常に大きな効果があることが、本発明者らにより明らかにされた。
0020
なお、ここで異方性の磁性膜にあっては、その膜厚が磁化困難軸方向の透磁率を考慮した磁性膜固有の高周波の表皮深さの、50分の1以上、より好ましくは20分の1以上あれば、シールド効果を示すと考えられる。
0021
【発明の効果】
この発明に係る携帯無線装置においては、アンテナから電波を放射する時にシールドケースに誘起される高周波誘起電流のうち、シールドケースから上記基板の接地パターンに流れる電流成分の電流密度が高い部分における電気接触が、他の部分の電気接触よりも良くなる手段を設けたので、確実に電磁シールド効果を高めることができる。
0022
また、アンテナがシールドケースから引き出される位置の近傍、およびアンテナがシールドケースから引き出される位置から遠い部分で電気接触が良くなる手段を設けたので、より簡単な構造で電磁シールド効果の高いものが得られる。
0023
また、電気接触を複数の電気接触子により形成し、高周波誘起電流の、シールドケースから基板の接地パターンに流れる電流成分の電流密度が高い部分で、電気接触子の配置密度を大きくしたので、電気接触子の数が少なくても、電磁シールド効果の高いものが得られる。
0024
さらに、シールドケースは樹脂表面に導電性膜を形成した部材で構成され、導電性膜上にさらに異方性磁性膜を積層し、この異方性磁性膜の磁化容易軸方向をアンテナに流れる電流と同じ方向にしたので、薄い磁性膜でも電磁シールド効果の高いものが得られる。
0025
また、異方性磁性膜を異方性グラニュラー膜としたので、より高い電磁シールド効果が得られる。
【図面の簡単な説明】
0026
【図1】 この発明の実施の形態1の携帯無線装置の内部を示す概略図である。
【図2】 電気接触子の一例を示す断面図である。
【図3】 この発明の実施の形態1の効果を説明する図である。
【図4】 この発明の実施の形態2の携帯無線装置の内部を示す概略図である。
【図5】 この発明の実施の形態2の効果を説明する図である。
【図6】 従来の携帯無線装置の内部を示す概略図である。
【符号の説明】
0027
1 シールドケース
2 基板
3 接地パターン
4 アンテナ
5 電気接触子
6 磁性膜の磁化容易軸方向
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to an electromagnetic shielding technique for a mobile mobile radio such as a mobile phone.
[0002]
[Prior art]
A mobile radio device such as a cellular phone generally includes an RF (high frequency) circuit for transmission and a digital circuit for reception. In a radio device in which transmission and reception are performed at the same time, an electromagnetic shield is required to suppress mutual interference between the reception unit and the transmission unit and EMI (Electromagnetic Interference) from the reception unit digital control circuit. In addition, even in a radio device that does not transmit and receive simultaneously, as in the PDC (Personal Digital Communications) system, which is currently the mainstream of Japanese mobile phones, the transmitted wave is transmitted to the PLL (Phase Locked) of the modulation circuit in the RF circuit. In order to prevent deterioration of the modulation factor due to wrapping around the loop), an electromagnetic shield is required. In addition, since the modulation circuit cannot use a long transmission line due to its nature, the specifications required for the shield are stricter because the modulation circuit is arranged as close as possible to the antenna.
[0003]
FIG. 6 is a schematic diagram showing the inside of a mobile phone as a conventional portable radio apparatus, wherein 1 is a shield case, 2 is a substrate in which a transmission circuit and a reception circuit are incorporated, and 3 is a ground pattern provided on the circuit substrate. , 4 is an antenna pulled out from the shield case 1, and 5 is an electrical contact.
[0004]
The shield case 1 is formed in a “box” shape, in which a metal film such as Cu or Ni is stacked by electroless plating or vapor deposition on a plastic such as sheet metal or ABS (acrylonitrile butadiene styrene). 1 is used so as to cover a portion of the substrate 2 where a high-frequency RF circuit such as a transmission circuit is located. In this case, the shield case 1 is in a floating and floating shape only by being covered, and does not operate as a shield. As an electromagnetic shield, it is necessary to make electrical contact with the ground pattern 3 on the edge of the substrate on which the RF part is placed so as to cover the circuit. In general, it is impossible to uniformly contact a thin metal plate or metal film used for a shield case with a conductive portion of a substrate, and an electrical contact 5 such as a protrusion or a spring is used to reliably establish electrical connection at a fixed point. The method is used. Among them, the method of making contact using a spring is used in many portable devices as the most reliable method. In addition, as shown in FIG. 6, the electrical contacts 5 are conventionally arranged more densely near the antenna and sparsely located at a portion far from the antenna. 1
[0005]
[Problems to be solved by the invention]
In order to shield the electromagnetic wave, it is necessary to make several electrical connections between the shield case and the lower substrate so that the electromagnetic wave does not leak from the gap. Conventionally, without considering the direction of the induced current flowing through the shield metal, electrical contacts are arranged in the dark clouds at almost equal intervals or at a portion close to the antenna in a concentrated manner to make electrical contact. In particular, the electrical contacts were reduced at the lower end far from the antenna. For this reason, the shielding effect may be weakened.
[0006]
In addition, when using a shield case made of plastic coated with a metal thin film, there is an example in which Sendust (FeAlSi) magnetic powder is applied as a metal film, but these magnetic materials are used by current mobile phones. At high frequencies near 1 GHz or higher, the relative permeability is almost 1, which is not effective.
[0007]
The present invention has been made to solve the above-described problems relating to the shield, and an object thereof is to obtain a reliable shield with a simple configuration.
[0008]
[Means for Solving the Problems]
In the portable radio apparatus according to the present invention, the electric current is generated at a portion where the current density of the current component flowing from the shield case to the ground pattern of the substrate is high among the high-frequency induced current induced in the shield case when radio waves are emitted from the antenna. The arrangement density of the contacts is increased .
[0009]
Further, the arrangement density of the electric contacts is increased in the vicinity of the position where the antenna is pulled out from the shield case and in the portion far from the position where the antenna is pulled out from the shield case.
[ 0010 ]
Furthermore, the shield case is composed of a member having a conductive film formed on the resin surface, and an anisotropic magnetic film is further laminated on the conductive film, and the current flowing through the antenna in the direction of the easy axis of magnetization of the anisotropic magnetic film. In the same direction.
[ 0011 ]
The anisotropic magnetic film is an anisotropic granular film.
[ 0012 ]
DETAILED DESCRIPTION OF THE INVENTION
Embodiment 1 FIG.
FIG. 1 is a schematic diagram showing Embodiment 1 of the present invention. The configuration is almost the same as the conventional one of FIG. 5, 1 is a shield case, 2 is a transmission circuit, a substrate on which a reception circuit and a logic circuit are incorporated, 3 is a ground pattern provided on the substrate 2, 4 Is an antenna drawn out from the shield case 1, and 5 is an electrical contact. Here, the electrical contacts 5 are arranged with a high arrangement density in the upper part close to the antenna and in the lower part far from the antenna. The reason for this arrangement is that, as a result of the electromagnetic wave analysis by the inventors, the current flowing from the shield case 1 to the ground pattern 3 through the electric contact 5 is blocked, focusing on the upper and lower ends in the direction in which the mirror image current flows. This is because it has been found that the wraparound of the transmission wave to the internal circuit can be reduced by making electrical contact so as not to occur. In addition to the upper end close to the antenna, the electromagnetic wraparound from the side is reduced by taking a means for improving the electric contact at the lower end opposite to the antenna, which has not been improved in electrical contact.
[ 0013 ]
By arranging the electric contacts 5 in this way, even if the number of the electric contacts 5 is the same as that of the conventional one, a high shielding effect can be obtained. Moreover, even if the number of electrical contacts 5 is reduced, the same shielding effect as that of the prior art can be obtained. In this example, the electric contact 5 is not provided on the side, but a small amount of electric contact may be provided on the side, and it is particularly effective to provide the electric contact 5 on the side near the antenna. It goes without saying that there is.
[ 0014 ]
FIG. 2 shows an example of the electric contact 5. As an electrical contact, a spring metal 5 is securely fixed to the ground pattern 3 of the substrate 2 with solder 51 or the like, and the shield case 1 is attached to the substrate 2 with screws (not shown) or the like on the substrate side. The spring metal 5 as an electrical contact is reliably brought into contact with the metal film 1a of the shield case 1 by pressing. In this way, electrical contact is reliably ensured. Here, the smaller the number of electrical contacts 5, the lighter the weight, the simpler the assembly process, and the lower the cost. In portable wireless devices such as mobile phones, there is a strong demand for light weight and low cost, and these effects are very large. According to the present invention, it is possible to obtain a larger shielding effect with a smaller number of electrical contacts by placing the electrical contacts 5 in a concentrated manner at a portion having a high shielding effect. In addition, although the thing of a spring metal was shown here as the electric contactor 5, it is not restricted to this, The thing which provided the metal protrusion on the grounding pattern may be sufficient, and the grounding pattern 3 and the shield case Any means may be used as long as a means for making good electrical contact with the metal portion is provided.
[ 0015 ]
The above effect is demonstrated using an analysis result. FIG. 3 shows three-dimensional finite element method electromagnetic field analysis of the electric field intensity distribution on the substrate 2 inside the shield case by changing three kinds of electrical contact states between the shield case and the substrate. FIG. 3A shows a case where the shield case is simply placed on the substrate and no electrical contact is made with the substrate. FIG. 3B shows a case where electrical contact is made only on the left and right sides of the shield box. ) Shows a case where the upper and lower portions are also in electrical contact, and the shaded portion shows a region where the electric field strength value is higher than a certain value. FIG. 3B shows that the area of the hatched portion is almost unchanged compared to FIG. 3A, that is, the electrical contact on the side is hardly effective. On the other hand, in FIG. 3C, the area of the shaded portion is greatly reduced, and it can be seen that the electrical connection in the vertical direction works extremely well.
[ 0016 ]
The above is because the surface current (high-frequency induced current) of the shield case induced by the transmission wave from the antenna is induced to flow mainly in the direction in which the antenna current flows, that is, in the vertical direction of the shield case. A high-frequency induced current flows so as to flow from the shield case to the ground pattern even at the lower end of the shield case, that is, far from the antenna, that is, across the contact portion. It is thought from. Further, since the high-frequency induced current crossing the contact portion is small on the side of the shield case, the electrical contact hardly affects the shield, and it is not necessary to provide many means for improving the electrical contact. Thus, in order to increase the shielding effect, when there is a contact surface in a direction orthogonal to the high frequency induced current, it is necessary to provide means for improving the electrical contact so that this portion is not thin and becomes a long slit, in order to improve the shielding effect. It is essential.
[ 0017 ]
Embodiment 2. FIG.
FIG. 4 is an internal schematic diagram of the portable radio apparatus for explaining the second embodiment of the present invention. In FIG. 4, a shield case 1a is formed by laminating a magnetic film such as Ni on a conductive metal shield film such as Cu or Al, and the direction of easy magnetization of the magnetic film is set as indicated by an arrow 6 in the figure. The vertical direction is the same as the high-frequency induced current. By doing so, the high-frequency magnetic permeability in the lateral direction can be kept high, and the reflection coefficient of radio waves is increased, that is, a high shielding effect is obtained.
[ 0018 ]
Here, a magnetic film generally used like Ni has a low magnetic permeability at a high frequency such as several hundred MHz to several GHz used in a mobile phone, and the above effect is reduced. Even in such a film, if anisotropy is added, the decrease in the magnetic permeability in the high-frequency region is reduced in the direction of the hard axis, and the above effect can be obtained. Further, if the anisotropic magnetic film such as an anisotropic FeAlO granular soft magnetic film (anisotropic granular film), the permeability of the hard axis (direction perpendicular to the easy axis) is 1 GHz or more, High permeability can be obtained. That is, if it is an anisotropic granular film, it is used as a good magnetic film even at a high frequency of several hundred MHz to several GHz, which is used in a cellular phone, by making the easy axis direction the same as the high frequency induced current. Therefore, the effect of the present embodiment is remarkable.
[ 0019 ]
FIG. 5 shows a case where a magnetic film having a relative permeability of 100 is laminated on a conductive metal shield film such as Cu or Al with a thickness of 100 angstroms using a three-dimensional finite element method electromagnetic field analysis by magnetism. This is a calculation of how much a region where isolation of −80 dB can be taken with respect to a microstrip line having a length of 10 mm on a substrate at an antenna current value of 0 dB at a high frequency of 940 MHz. Here, the portion where the substrate is shielded is calculated in a shape closer to an actual portable wireless device. FIG. 4A shows a calculation result when there is no magnetic film, and FIG. 4B shows a calculation result when there is a magnetic film. The hatched portion in the figure indicates a region where the isolation is lower than −80 dB. When the magnetic film is present, there is almost no hatched portion, and it has been clarified that the shield characteristics are remarkably improved by the present invention. Thus, the present inventors have revealed that a magnetic film having a thickness of only 100 angstroms has a very great shielding effect.
[ 0020 ]
Here, in the case of the anisotropic magnetic film, the film thickness is 1/50 or more of the high-frequency skin depth inherent in the magnetic film considering the permeability in the hard axis direction, more preferably 20 If it is more than 1 / min, it is considered that the shielding effect is exhibited.
[ 0021 ]
【The invention's effect】
In the portable wireless device according to the present invention, of the high-frequency induced current induced in the shield case when radiating radio waves from the antenna, the electrical contact in the portion where the current density of the current component flowing from the shield case to the ground pattern of the substrate is high However, since the means for improving the electrical contact of other parts is provided, the electromagnetic shielding effect can be surely enhanced.
[ 0022 ]
In addition, since a means for improving electrical contact is provided in the vicinity of the position where the antenna is pulled out from the shield case and in the part far from the position where the antenna is pulled out from the shield case, a simple structure with high electromagnetic shielding effect can be obtained. It is done.
[ 0023 ]
In addition, since the electrical contact is formed by a plurality of electrical contacts, the arrangement density of the electrical contacts is increased in the portion where the current density of the current component flowing from the shield case to the ground pattern of the substrate is high, and the electrical contact is increased. Even if the number of contacts is small, a high electromagnetic shielding effect can be obtained.
[ 0024 ]
Furthermore, the shield case is composed of a member having a conductive film formed on the resin surface, and an anisotropic magnetic film is further laminated on the conductive film, and the current flowing through the antenna in the direction of the easy axis of magnetization of the anisotropic magnetic film. Therefore, a thin magnetic film having a high electromagnetic shielding effect can be obtained.
[ 0025 ]
Further, since the anisotropic magnetic film is an anisotropic granular film, a higher electromagnetic shielding effect can be obtained.
[Brief description of the drawings]
[ 0026 ]
FIG. 1 is a schematic diagram showing the inside of a portable radio apparatus according to a first embodiment of the present invention.
FIG. 2 is a cross-sectional view showing an example of an electrical contact.
FIG. 3 is a diagram for explaining the effect of the first embodiment of the present invention.
FIG. 4 is a schematic diagram showing the inside of a portable radio apparatus according to a second embodiment of the present invention.
FIG. 5 is a diagram for explaining the effect of the second embodiment of the present invention.
FIG. 6 is a schematic diagram showing the inside of a conventional portable wireless device.
[Explanation of symbols]
[ 0027 ]
DESCRIPTION OF SYMBOLS 1 Shield case 2 Board | substrate 3 Grounding pattern 4 Antenna 5 Electric contact 6 The magnetization easy axis direction of a magnetic film

Claims (4)

基板上の少なくとも送信回路が構成された部分を覆うシールドケースが上記基板の接地パターンと電気接触するよう設けられ、上記シールドケースの外部に上記送信回路からの電波を放射するためのアンテナを備えた携帯無線装置において、上記アンテナから電波を放射する時に上記シールドケースに誘起される高周波誘起電流のうち、上記シールドケースから上記基板の接地パターンに流れる電流成分の電流密度が高い部分で上記電気接触子の配置密度を高くしたことを特徴とする携帯無線装置。A shield case covering at least a portion where the transmission circuit is configured on the substrate is provided so as to be in electrical contact with the ground pattern of the substrate, and an antenna for radiating radio waves from the transmission circuit is provided outside the shield case. In the portable radio device, the electric contact in a portion where a current density of a current component flowing from the shield case to the ground pattern of the substrate is high in a high frequency induced current induced in the shield case when radio waves are radiated from the antenna. A portable radio apparatus characterized by having a higher arrangement density . 上記アンテナが上記シールドケースから引き出される位置の近傍、および上記アンテナが上記シールドケースから引き出される位置から遠い部分で上記電気接触子の配置密度を高くしたことを特徴とする請求項1記載の携帯無線装置。2. The portable radio according to claim 1, wherein the arrangement density of the electric contacts is increased in a vicinity of a position where the antenna is pulled out from the shield case and a portion far from a position where the antenna is pulled out from the shield case. apparatus. 基板上の少なくとも送信回路が構成された部分を覆うシールドケースを設け、このシールドケースの外部に上記送信回路からの電波を放射するためのアンテナを備えた携帯無線装置において、上記シールドケースは樹脂表面に導電性膜を形成した部材で構成され、上記導電性膜上にさらに異方性磁性膜を積層し、この異方性磁性膜の磁化容易軸方向を上記アンテナに流れる電流と同じ方向にしたことを特徴とする請求項1または2に記載の携帯無線装置。In a portable wireless device provided with a shield case covering at least a portion where a transmission circuit is configured on a substrate, and having an antenna for radiating radio waves from the transmission circuit outside the shield case, the shield case has a resin surface An anisotropic magnetic film is further laminated on the conductive film, and the magnetization easy axis direction of the anisotropic magnetic film is set to the same direction as the current flowing through the antenna. The portable radio apparatus according to claim 1 or 2, wherein 上記異方性磁性膜を異方性グラニュラー膜としたことを特徴とする請求項記載の携帯無線装置。4. The portable radio apparatus according to claim 3, wherein the anisotropic magnetic film is an anisotropic granular film.
JP33701299A 1999-11-29 1999-11-29 Portable wireless device Expired - Fee Related JP4257987B2 (en)

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JP4762125B2 (en) * 2006-12-15 2011-08-31 株式会社東芝 Antenna device and radio device
JP4922003B2 (en) 2007-02-13 2012-04-25 株式会社東芝 ANTENNA DEVICE AND RADIO DEVICE
WO2020250823A1 (en) * 2019-06-13 2020-12-17 株式会社村田製作所 Module

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