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JPS5824929B2 - Inductance element of power line carrier blocking filter - Google Patents
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JPS5824929B2 - Inductance element of power line carrier blocking filter - Google Patents

Inductance element of power line carrier blocking filter

Info

Publication number
JPS5824929B2
JPS5824929B2 JP2146476A JP2146476A JPS5824929B2 JP S5824929 B2 JPS5824929 B2 JP S5824929B2 JP 2146476 A JP2146476 A JP 2146476A JP 2146476 A JP2146476 A JP 2146476A JP S5824929 B2 JPS5824929 B2 JP S5824929B2
Authority
JP
Japan
Prior art keywords
power line
inductance element
inductance
line carrier
impedance
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP2146476A
Other languages
Japanese (ja)
Other versions
JPS52104836A (en
Inventor
岡本晋典
北川文夫
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP2146476A priority Critical patent/JPS5824929B2/en
Publication of JPS52104836A publication Critical patent/JPS52104836A/en
Publication of JPS5824929B2 publication Critical patent/JPS5824929B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H7/00Multiple-port networks comprising only passive electrical elements as network components
    • H03H7/01Frequency selective two-port networks
    • H03H7/17Structural details of sub-circuits of frequency selective networks
    • H03H7/1741Comprising typical LC combinations, irrespective of presence and location of additional resistors
    • H03H7/1758Series LC in shunt or branch path
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H7/00Multiple-port networks comprising only passive electrical elements as network components
    • H03H7/01Frequency selective two-port networks
    • H03H7/09Filters comprising mutual inductance
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H7/00Multiple-port networks comprising only passive electrical elements as network components
    • H03H7/01Frequency selective two-port networks
    • H03H7/17Structural details of sub-circuits of frequency selective networks
    • H03H7/1741Comprising typical LC combinations, irrespective of presence and location of additional resistors
    • H03H7/1766Parallel LC in series path

Landscapes

  • Filters And Equalizers (AREA)
  • Cable Transmission Systems, Equalization Of Radio And Reduction Of Echo (AREA)
  • Coils Or Transformers For Communication (AREA)

Description

【発明の詳細な説明】 本発明は、同一の磁性材料1に複数組バイファラ巻きし
たコイル2,3,4,5,6,7を互いに直交するよう
に巻回し、各コイル2,3,4゜5.6,7を直列接続
して合成インダクタンスを取り出して成ることを特徴と
する電力線搬送波阻止用フィルタのインダクタンス要素
に係り、その目的とするところは小型で軽量に製作する
ことができる電力線搬送波阻止用フィルタのインダクタ
ンス要素を提供するにある。
DETAILED DESCRIPTION OF THE INVENTION In the present invention, a plurality of sets of coils 2, 3, 4, 5, 6, and 7 are wound perpendicularly to each other on the same magnetic material 1.゜It pertains to the inductance element of a filter for power line carrier wave blocking, which is characterized by connecting 5.6 and 7 in series and extracting the composite inductance, and its purpose is to reduce the power line carrier wave which can be made compact and lightweight. The present invention provides an inductance element for a blocking filter.

普通商用電源周波に高周波信号を重量させて通信を行な
う所謂電力線搬送通信においては、信号の伝送に必要な
伝路は予じめ電力線路として送受信機間に準備されてお
り、その伝送路たる電力線路を通して通報を信号に変換
し、信号を伝送している。
In so-called power line carrier communication, in which communication is carried out by adding high-frequency signals to the normal commercial power frequency, the path necessary for signal transmission is prepared in advance as a power line between the transmitter and receiver, and the transmission path, which is the power Converts notifications into signals and transmits them through railroad tracks.

従って信号の伝送には新たに専用の伝送路を設備する必
要がないという利点を有している。
Therefore, it has the advantage that there is no need to newly install a dedicated transmission line for signal transmission.

しかし電力線路が大地帰路方式であったり、信号の屋外
漏洩レベルが規定値以上である場合は関連の法規制を受
けるために電力線搬送通信の普及をさまたげていた。
However, if the power line is a return-to-ground type or if the outdoor signal leakage level exceeds a specified value, the related laws and regulations will be required, which has hindered the spread of power line carrier communications.

このためラインフィルタを使用して関連法規制の障害を
解決しようとしたが、従来の平衡型ラインフィルタに使
用されているコイルはコイルのインダクタンスを大きく
且つ形状を小さくするために巻線を別々に磁性材料に巻
回していた。
For this reason, attempts have been made to use line filters to solve the related legal and regulatory obstacles, but the coils used in conventional balanced line filters have separate windings to increase the inductance and reduce the size of the coil. It was wrapped in magnetic material.

そのため電流容量によって形状、重量が大きくなって、
装置の取付場所を困難とするという欠点があった。
Therefore, the shape and weight increase depending on the current capacity,
This has the disadvantage that the installation location of the device is difficult.

本発明は上述の欠点に鑑みて提供したもので、以下実施
例により詳述する。
The present invention has been provided in view of the above-mentioned drawbacks, and will be described in detail below with reference to Examples.

1は略直方体のフェライトコアのような磁性材料であっ
てこの磁性材料1には前後方向、左右方向及び側周に夫
々2組のコイル2,3.4,5.6.7をバイファイラ
に巻回して、各バイファイラ巻きしたコイル2,3.4
.5.6.7組を互いの磁束方向が直交するようにしで
ある。
Reference numeral 1 denotes a magnetic material such as a substantially rectangular ferrite core, and two sets of coils 2, 3.4, 5, 6. Turn each bifilar wound coil 2, 3.4
.. 5.6.7 pairs are arranged so that their magnetic flux directions are perpendicular to each other.

各コイル2,3.4,5.6,7の端子8〜19は各コ
イル2乃至7のインダクタンスの出力端子とする。
Terminals 8 to 19 of each coil 2, 3.4, 5.6, and 7 are used as inductance output terminals of each coil 2 to 7.

第2図a、bはフィルタ回路の基本型を示すもので、第
2図aは所謂り型、第2図すはπ型の構成をなすもので
ある。
Figures 2a and 2b show the basic types of filter circuits, with Figure 2a having a so-called type and Figure 2 having a π type configuration.

第2図a、bにあっては4端子A乃至りの各端子間に接
続されたインピーダンス辺20,21.22゜23は第
3図aに示すようにインダクタンス素子り或いは第3図
すに示すインダクタンス素子りとキャパシタンス素子C
8との並列回路によって構成され、またインピーダンス
辺24,25.26は第3図Cに示すキャパシタンス素
子C8或いは第3図dに示すインダクタンス素子りとキ
ャパシタンス素子C6との直列回路によって構成される
In Figures 2a and 2b, the impedance sides 20, 21, 22° 23 connected between the four terminals A to 4 are inductance elements as shown in Figure 3a, or as shown in Figure 3. Inductance element and capacitance element C shown
The impedance sides 24, 25, and 26 are constructed by a series circuit of a capacitance element C8 shown in FIG. 3C or an inductance element shown in FIG. 3D and a capacitance element C6.

第4図は第2図aのL型フィルタを用いた所謂帯域阻止
型フィルタ回路を示すもので、かかる回路を構成するに
当っては、第1図実施例の互いに直交配列されたコイル
2と4とを直列的に接続して合成インダクタンス素子り
、を形成し、この合成インダクタンス素子L1の両端に
キャパシタンス素子C1を並列に接続して第2図aにお
けるインピーダンス辺20を構成する。
FIG. 4 shows a so-called band rejection filter circuit using the L-type filter shown in FIG. 4 are connected in series to form a composite inductance element L1, and a capacitance element C1 is connected in parallel to both ends of this composite inductance element L1 to constitute the impedance side 20 in FIG. 2a.

更に上記同様にコイル3と5とを直列接続して合成イン
ダクタンス素子L2を形成し、この合成インダクタンス
素子L2にキャパシタンス素子C2を並列に接続して第
2図aにおけるインピーダンス辺21を構成する。
Further, in the same manner as described above, coils 3 and 5 are connected in series to form a composite inductance element L2, and a capacitance element C2 is connected in parallel to this composite inductance element L2 to constitute the impedance side 21 in FIG. 2a.

インダクタンス素子L1L2はその相互誘導係数Mによ
って磁気的に結合される。
The inductance elements L1L2 are magnetically coupled by their mutual induction coefficient M.

コイル6又は7はキャパシタンス素子C3を直列に接続
して第2図aのインピーダンス辺24を構成する。
The coil 6 or 7 constitutes the impedance side 24 of FIG. 2a by connecting the capacitance element C3 in series.

第5図は本発明の別の実施例を示すもので、磁性材料1
は直方体部1cの両側上端面及び下端面に凹状の突出片
1aを一体突設するとともに、側周部に溝1bを周設し
た形状のものから構成せられ、溝1b内にコイル6を巻
回するとともにこのコイル6に対して直交するように直
方体部1cの上端面及び下端面及び前後面に沿うように
コイル2.3を前後方向にバイファイラにて巻回し、こ
れらのコイル2,3に対して直交するように更に突出片
1aの凹平面と直方体部1cの両側面とに沿うように左
右方向にコイル4,5をバイアイラにて巻回し、コイル
2,3,4,5.6が互いに接触しないように夫々間隙
を形成してあり、各コイル2,3,4.5を上記と同様
に接続して合成インダクタンス素子L1.L2を構成し
て、キャパシタンス素子C1C2を各合成インダクタン
ス素子り、 L2に並列接続し、コイル6にキャパシタ
ンス素子C3を直列接続しである。
FIG. 5 shows another embodiment of the present invention, in which the magnetic material 1
The rectangular parallelepiped part 1c has concave projecting pieces 1a integrally protruding from both upper and lower end faces, and a groove 1b around the side periphery, and the coil 6 is wound in the groove 1b. At the same time, the coils 2 and 3 are wound with a bifilar in the front-rear direction so as to be perpendicular to the coil 6 and along the upper and lower end surfaces and the front and rear surfaces of the rectangular parallelepiped part 1c. Further, the coils 4 and 5 are wound in the left-right direction using a biairer so as to be perpendicular to the concave plane of the protruding piece 1a and both side surfaces of the rectangular parallelepiped part 1c. A gap is formed between the coils 2, 3, and 4.5 so that they do not come into contact with each other, and the coils 2, 3, and 4.5 are connected in the same manner as described above to form a composite inductance element L1. The capacitance element C1C2 is connected in parallel to L2 as each composite inductance element, and the capacitance element C3 is connected in series to the coil 6.

しかして夫々によって構成せるインピーダンス辺20
,24.21に接続して第4図の帯域阻止型フィルタ回
路を構成する。
Therefore, the impedance side 20 configured by each
, 24 and 21 to form the band-elimination filter circuit shown in FIG.

さて一般に電磁結合係数をRとすれば自己インダクタン
スLと相互誘導係数Mとの関係はR二MO≦R≦1とな
る。
Now, in general, if the electromagnetic coupling coefficient is R, the relationship between the self-inductance L and the mutual induction coefficient M is R2MO≦R≦1.

従って第4図において合成インダクタンス素子L1L2
は互い直交した状態で巻線配置されたバイファイラ巻き
のコイル2,3,4,5を使用しであるからR≦となり
、合成インダクタンスは大きくなって、各インピーダン
ス辺20.21のインピーダンスが大きくなる。
Therefore, in FIG. 4, the composite inductance element L1L2
uses bifilar-wound coils 2, 3, 4, and 5 whose windings are arranged orthogonal to each other, so R≦, and the combined inductance becomes large and the impedance of each impedance side 20.21 becomes large. .

さて第4図回路において一般に直列及び並列共振回路の
共振周波数はf=−1−一であられさ2aJロー れる。
Now, in the circuit shown in FIG. 4, the resonant frequency of the series and parallel resonant circuits is generally f=-1-1, which is 2aJ low.

従って各回路の高周波信号に対する共振周波数を一致さ
せておくと、A、B端子間、及びC2D端子間のインピ
ーダンスは最大値を示し、またA、C端子間のインピー
ダンスは最小値を示す。
Therefore, if the resonant frequencies for the high-frequency signals of each circuit are matched, the impedance between the A and B terminals and between the C2D terminal will exhibit a maximum value, and the impedance between the A and C terminals will exhibit a minimum value.

なお商用電源周波数に対してはA、B端子間及びC,D
端子間のインピーダンスは小さく、またA。
In addition, for commercial power frequency, between A and B terminals and between C and D
The impedance between the terminals is small and A.

B端子のインピーダンスは大きくなる。The impedance of the B terminal increases.

故に今B。D端子間に商用電源周波に高周波信号(共振
周波数)を重量したものを印加すればA、C端子間にお
いては高周波信号が並列共振回路のインピーダンスと直
列共振回路のインピーダンスの比に応じて減裏を受ける
ため商用周波数のみが通過することになる。
Therefore, now B. If a commercial power supply frequency plus a high frequency signal (resonant frequency) is applied between the D terminals, the high frequency signal will be attenuated between the A and C terminals according to the ratio of the impedance of the parallel resonant circuit to the impedance of the series resonant circuit. Therefore, only commercial frequencies will pass through.

なお第4図の各インピーダンス辺の共振周波数を若干ず
らして回路を構成すれば共振周波数を一致させた場合に
比較し、帯域幅を広くとることが可能である。
Note that if the circuit is constructed by slightly shifting the resonant frequencies of each impedance side in FIG. 4, it is possible to obtain a wider bandwidth than when the resonant frequencies are matched.

本発明は同一磁性材料上に複数組のバイファイラ巻きし
たコイルを互いに直交するように巻回し、各コイルを交
互に直列接続して合成インダクタンスを取り出しである
から少ない巻数で大きなインダクタンスを独立的に取り
出すことができるもので、別個に巻回したインダクタン
スを用いたフィルタより小型軽量で且つ部品構成が少な
くて済むという効果を奏するものである。
In the present invention, multiple sets of bifilar-wound coils are wound on the same magnetic material so as to be orthogonal to each other, and each coil is connected in series alternately to extract a composite inductance. Therefore, a large inductance can be independently extracted with a small number of turns. This has the advantage that it is smaller and lighter than a filter using a separately wound inductance, and requires fewer parts.

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

第1図は本発明一実施例の斜視図、第2図a。 bはフィルタ回路の構成図、第3図a、b、c。 dはフィルタ回路のインピーダンス辺の素子構成図、第
4図は本発明の一実施例を用いた回路図、第5図は本発
明の他の実施例の斜視図であり、1は磁性材料、2,3
,4,5,6,7はコイルである。
FIG. 1 is a perspective view of an embodiment of the present invention, and FIG. 2a is a perspective view of an embodiment of the present invention. b is a block diagram of the filter circuit; FIGS. 3a, b, and c. d is an element configuration diagram on the impedance side of the filter circuit, FIG. 4 is a circuit diagram using one embodiment of the present invention, and FIG. 5 is a perspective view of another embodiment of the present invention. 2,3
, 4, 5, 6, and 7 are coils.

Claims (1)

【特許請求の範囲】[Claims] 1 同一の磁性材料に複数組のバイファイラ巻きしたコ
イルを互いに直交するように巻回し、各コイルを交互に
直列接続して合成インダクタンスを取り出して成ること
を特徴とする電力線搬送波阻止用フィルタのインダクタ
ンス要素。
1. An inductance element for a power line carrier blocking filter, characterized in that a plurality of sets of bifilar-wound coils are wound on the same magnetic material so as to be orthogonal to each other, and each coil is alternately connected in series to extract a composite inductance. .
JP2146476A 1976-02-28 1976-02-28 Inductance element of power line carrier blocking filter Expired JPS5824929B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2146476A JPS5824929B2 (en) 1976-02-28 1976-02-28 Inductance element of power line carrier blocking filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2146476A JPS5824929B2 (en) 1976-02-28 1976-02-28 Inductance element of power line carrier blocking filter

Publications (2)

Publication Number Publication Date
JPS52104836A JPS52104836A (en) 1977-09-02
JPS5824929B2 true JPS5824929B2 (en) 1983-05-24

Family

ID=12055693

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2146476A Expired JPS5824929B2 (en) 1976-02-28 1976-02-28 Inductance element of power line carrier blocking filter

Country Status (1)

Country Link
JP (1) JPS5824929B2 (en)

Also Published As

Publication number Publication date
JPS52104836A (en) 1977-09-02

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