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JPS6144418B2 - - Google Patents
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JPS6144418B2 - - Google Patents

Info

Publication number
JPS6144418B2
JPS6144418B2 JP1738179A JP1738179A JPS6144418B2 JP S6144418 B2 JPS6144418 B2 JP S6144418B2 JP 1738179 A JP1738179 A JP 1738179A JP 1738179 A JP1738179 A JP 1738179A JP S6144418 B2 JPS6144418 B2 JP S6144418B2
Authority
JP
Japan
Prior art keywords
radio receiver
inductance
antenna
frequency
resonance
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
JP1738179A
Other languages
Japanese (ja)
Other versions
JPS55110438A (en
Inventor
Akira Okamoto
Hideo Shibuya
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 Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP1738179A priority Critical patent/JPS55110438A/en
Publication of JPS55110438A publication Critical patent/JPS55110438A/en
Publication of JPS6144418B2 publication Critical patent/JPS6144418B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B1/00Details of transmission systems, not covered by a single one of groups H04B3/00 - H04B13/00; Details of transmission systems not characterised by the medium used for transmission
    • H04B1/06Receivers
    • H04B1/16Circuits
    • H04B1/18Input circuits, e.g. for coupling to an antenna or a transmission line

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Details Of Aerials (AREA)
  • Input Circuits Of Receivers And Coupling Of Receivers And Audio Equipment (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は車載用アンテナに関するもので、アン
テナ特性の改善を図ることを目的とする。 バラクタダイオードを利用したC同調のラジオ
受信機を自動車に装着する場合、カーアンテナは
第1図に等価回路で示すように容量性のためトラ
ツキング等の問題が発生し、アンテナ回路を非同
調によらなければならない。なおR1,C1はアン
テナの輻射インピーダンス、C2はケーブルの容
量である。またこれにともないμ同調ラジオ受信
機に比べ実用感度(S/N)の悪化は避られな
い。 本発明はこの欠点を除去したものである。ま
ず、S/Nはラジオ受信機に供給される信号レベ
ル、ラジオ受信機より見た信号源インピーダンス
の平方根、およびラジオ受信機の雑音指数
(NF)によつて決まる。そこでNFが一定であれ
ばS/Nを改善するには
The present invention relates to an on-vehicle antenna, and an object of the present invention is to improve antenna characteristics. When installing a C-tuned radio receiver using a varactor diode in a car, problems such as tracking occur due to the car antenna's capacitive nature, as shown in the equivalent circuit in Figure 1, and the antenna circuit is untuned. There must be. Note that R 1 and C 1 are the radiation impedance of the antenna, and C 2 is the capacitance of the cable. In addition, as a result, practical sensitivity (S/N) will inevitably deteriorate compared to μ-tuned radio receivers. The present invention eliminates this drawback. First, S/N is determined by the signal level supplied to the radio receiver, the square root of the signal source impedance seen by the radio receiver, and the noise figure (NF) of the radio receiver. Therefore, if NF is constant, how to improve S/N

【表】 が大きくなるようにすればよい。 一方、第1図においてR1はC1に比べインピー
ダンスが充分低いので、ラジオ受信機の入力イン
ピーダンスが充分高ければラジオ受信機に供給さ
れる信号レベルは容量C1とC2の分割比によつて
決まる。またラジオ受信機より見た信号源インピ
ーダンスはC1+C2になり、この関係は第2図の
ようになる。 今、容量C1に対しインダクタンスL1を第3図
のように挿入すると、その共振周波数近傍では直
列共振により信号レベルの分割比が小さくなり、
ラジオ受信機に供給される信号レベルが大きくな
ると共にラジオ受信機から見た信号源インピーダ
ンスも低下し、S/Nの向上がはかれる。第4図
はその状態を示したものである。 ここでこの共振周波数を受信帯域より低い周波
数に設定すると共振周波数以上の周波数ではラジ
オ受信機に供給される信号レベルはL1とC2の分
割比になり、周波数の2乗に比例して悪化するた
め共振周波数は受信帯域より高い周波数に設定す
る方が有利である。 なおVHF帯を考慮した場合、L1に対し並列に
VHF帯信号を通過させる容量を設けておけば良
い。 ところで上記実施例では高い受信周波数に対し
ては有用であるが、低い受信周波数に対しては効
果が少い。第5図はその点を考慮した実施例であ
つて容量C2に対し並列にインダクタンスL2を設
け、第6図のように共振周波数の近傍では並列共
振によつて信号レベルの分割比を小さく、ラジオ
受信機に供給される信号レベルが大きくなるよう
にしている。なお、第5図において、L1はアン
テナの輻射インピーダンスに直列に接続されたイ
ンダクタンスである。 この場合、ラジオ受信機より見た信号源インピ
ーダンスも高くなり、S/Nが悪化するように思
われるが
[Table] should be made larger. On the other hand, in Figure 1, R 1 has a sufficiently low impedance compared to C 1 , so if the input impedance of the radio receiver is sufficiently high, the signal level supplied to the radio receiver will depend on the division ratio of capacitances C 1 and C 2 . It will be decided. Also, the signal source impedance seen from the radio receiver is C 1 +C 2 , and this relationship is as shown in FIG. Now, if an inductance L 1 is inserted into a capacitance C 1 as shown in Figure 3, the signal level division ratio will become smaller near the resonance frequency due to series resonance.
As the signal level supplied to the radio receiver increases, the signal source impedance seen from the radio receiver also decreases, improving the S/N ratio. FIG. 4 shows this state. If this resonant frequency is set to a frequency lower than the reception band, the signal level supplied to the radio receiver at frequencies above the resonant frequency will be the division ratio of L 1 and C 2 , and will deteriorate in proportion to the square of the frequency. Therefore, it is advantageous to set the resonance frequency to a higher frequency than the reception band. In addition, when considering the VHF band, in parallel to L 1
It is sufficient to provide a capacity for passing VHF band signals. By the way, although the above embodiment is useful for high reception frequencies, it is less effective for low reception frequencies. Figure 5 shows an embodiment that takes this point into consideration, where an inductance L 2 is provided in parallel to the capacitance C 2 , and as shown in Figure 6, the signal level division ratio is reduced by parallel resonance near the resonance frequency. , so that the signal level supplied to the radio receiver is increased. In addition, in FIG. 5, L1 is an inductance connected in series to the radiation impedance of the antenna. In this case, the signal source impedance seen by the radio receiver also increases, and the S/N seems to deteriorate.

【表】 で明らかのようにS/Nはラジオ受信機の信号源
インピーダンスの平方根に比例するので分割比が
小さくなることによるS/N向上分の方が大き
く、全体としてS/N向上につながる。 なお、この共振周波数は受信帯域より高い周波
数に設定すると共振周波数以下の周波数ではラジ
オ受信機に供給される信号レベルはC1とL2の分
割になり周波数の2乗に反比例して悪化するため
共振周波数は受信帯域より低い周波数に設定する
方が有利である。またL2はラジオ受信機内部に
あつてもよい。 さらにアンテナ、ボデー間の容量C3を考慮し
た場合、L1はC1,C3の総和に対し直列共振、L2
はC1+C2+C3に並列共振と考えれば良い。 上記実施例より明らかなように本発明によれば
S/Nよく信号を受信することができ、またその
ために追加する部分点数はわずかでよい。
As is clear from the table, the S/N is proportional to the square root of the signal source impedance of the radio receiver, so the S/N improvement due to a smaller division ratio is greater, leading to an overall S/N improvement. . Note that if this resonant frequency is set to a frequency higher than the receiving band, the signal level supplied to the radio receiver at frequencies below the resonant frequency will be divided into C1 and L2 , and will deteriorate in inverse proportion to the square of the frequency. It is advantageous to set the resonance frequency to a frequency lower than the reception band. Also, L2 may be located inside the radio receiver. Furthermore, when considering the capacitance C 3 between the antenna and the body, L 1 is series resonance with respect to the sum of C 1 and C 3 , and L 2
can be thought of as parallel resonance with C 1 + C 2 + C 3 . As is clear from the above embodiments, according to the present invention, signals can be received with a good S/N ratio, and only a small number of partial points are added for this purpose.

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

第1図は従来のアンテナの等価回路図、第2図
はその特性図、第3図は本発明の一実施例におけ
るアンテナの等価回路図、第4図は同特性図、第
5図は他の実施例の等価回路図、第6図は同特性
図である。 R1,C1……アンテナの輻射インピーダンス、
C2……ケーブルの容量、L1……インダクタン
ス。
Figure 1 is an equivalent circuit diagram of a conventional antenna, Figure 2 is its characteristic diagram, Figure 3 is an equivalent circuit diagram of an antenna according to an embodiment of the present invention, Figure 4 is the same characteristic diagram, and Figure 5 is another diagram. FIG. 6 is an equivalent circuit diagram of the embodiment, and FIG. 6 is a characteristic diagram thereof. R 1 , C 1 ...radiation impedance of antenna,
C 2 ... Cable capacity, L 1 ... Inductance.

Claims (1)

【特許請求の範囲】 1 アンテナ本体と給電線との間に第1のインダ
クタンスを設け、受信帯域以上の周波数で共振点
を選ぶと共に、ケーブル容量、ラジオ受信機入力
容量に対し並列に第2のインダクタンスを設け、
同容量とインピーダンスとの共振を受信帯域以下
に選んだことを特徴とする車載用アンテナ。 2 第1のインダクタンスは並列にVHF帯信号
通過用容量を設けたものを用いることを特徴とす
る特許請求の範囲第1項記載の車載用アンテナ。
[Claims] 1. A first inductance is provided between the antenna body and the feed line, a resonance point is selected at a frequency above the reception band, and a second inductance is provided in parallel with the cable capacity and radio receiver input capacity. Provide an inductance,
An in-vehicle antenna characterized by having resonance between the same capacitance and impedance below the reception band. 2. The vehicle-mounted antenna according to claim 1, wherein the first inductance is provided with a VHF band signal passing capacity in parallel.
JP1738179A 1979-02-16 1979-02-16 Antenna for car mounting Granted JPS55110438A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1738179A JPS55110438A (en) 1979-02-16 1979-02-16 Antenna for car mounting

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1738179A JPS55110438A (en) 1979-02-16 1979-02-16 Antenna for car mounting

Publications (2)

Publication Number Publication Date
JPS55110438A JPS55110438A (en) 1980-08-25
JPS6144418B2 true JPS6144418B2 (en) 1986-10-02

Family

ID=11942421

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1738179A Granted JPS55110438A (en) 1979-02-16 1979-02-16 Antenna for car mounting

Country Status (1)

Country Link
JP (1) JPS55110438A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58141036A (en) * 1982-02-16 1983-08-22 Sony Corp Antenna circuit
JPH0611673Y2 (en) * 1987-07-14 1994-03-23 日本板硝子株式会社 Car receiver

Also Published As

Publication number Publication date
JPS55110438A (en) 1980-08-25

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