JPS6133616Y2 - - Google Patents

Info

Publication number
JPS6133616Y2
JPS6133616Y2 JP12925178U JP12925178U JPS6133616Y2 JP S6133616 Y2 JPS6133616 Y2 JP S6133616Y2 JP 12925178 U JP12925178 U JP 12925178U JP 12925178 U JP12925178 U JP 12925178U JP S6133616 Y2 JPS6133616 Y2 JP S6133616Y2
Authority
JP
Japan
Prior art keywords
transformer
winding
balanced
unbalanced
load
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
JP12925178U
Other languages
Japanese (ja)
Other versions
JPS5545289U (en
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 filed Critical
Priority to JP12925178U priority Critical patent/JPS6133616Y2/ja
Publication of JPS5545289U publication Critical patent/JPS5545289U/ja
Application granted granted Critical
Publication of JPS6133616Y2 publication Critical patent/JPS6133616Y2/ja
Expired legal-status Critical Current

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  • Cable Transmission Systems, Equalization Of Radio And Reduction Of Echo (AREA)

Description

【考案の詳細な説明】 本考案は少くとも2個以浄の変成器を有する平
衡不平衡変換変成器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a balanced unbalanced conversion transformer having at least two or more transformers.

従来の平衡不平衡変換変成器100は、第1図
に示すように、ペア線22を磁心1に1:1で巻
装した2条線路型変成器2と、一次巻線3および
二次巻線4がそれぞれ磁心5に巻装された絶縁型
変成器6とから構成され、2条線路型変成器2を
平衡負荷側7に接続し、絶縁型変成器6を不平衡
負荷側8に接続している。このような平衡不平衡
変換変成器100において良好な伝送特性を得る
には、2条線路型変成器2の特性インピーダンス
Wb(Ω)の値が平衡負荷7の値に十分近いこと
が必要である。しかしながら、平衡負荷7のイン
ピーダンスが高い場合、例えば300Ωにおいて
は、300ΩのWbを有する2条線路型変成器2を実
現する事は非常に困難であるため、伝送特性が大
幅に劣化する。
As shown in FIG. 1, a conventional balanced-unbalanced transformer 100 includes a two-line type transformer 2 in which paired wires 22 are wound around a magnetic core 1 at a ratio of 1:1, a primary winding 3 and a secondary winding. The wires 4 are each composed of an insulated transformer 6 wound around a magnetic core 5, and the double line transformer 2 is connected to a balanced load side 7, and the insulated transformer 6 is connected to an unbalanced load side 8. are doing. In order to obtain good transmission characteristics in such a balanced unbalanced conversion transformer 100, the characteristic impedance of the double line type transformer 2 is
It is necessary that the value of Wb (Ω) be sufficiently close to the value of the balanced load 7. However, when the impedance of the balanced load 7 is high, for example 300Ω, it is very difficult to realize a double line transformer 2 having a Wb of 300Ω, and the transmission characteristics are significantly deteriorated.

本考案の目的は上述の欠点を除去した平衡不平
衡変換変成器を提供することにある。
The object of the present invention is to provide a balanced-unbalanced conversion transformer which eliminates the above-mentioned drawbacks.

次に図面を参照して本考案を詳細に説明する。
第2図は本考案の一実施例を示す回路図である。
図において、本考案の変成器は第1巻線9と第2
巻線10との巻数比が1:1の関係にある2条線
路型変成器11と、一次巻線12と二次巻線13
および静電遮蔽14を有する絶縁型変成器15と
から構成され、絶縁型変成器15は平衡負荷16
に接続され、2条線路型変成器11は不平衡負荷
17に接続され、さらに静電遮蔽14は第2巻線
10の巻終り18に接続されその巻始め19は接
地されている。
Next, the present invention will be explained in detail with reference to the drawings.
FIG. 2 is a circuit diagram showing an embodiment of the present invention.
In the figure, the transformer of the present invention has a first winding 9 and a second winding 9.
A two-line transformer 11 having a turns ratio of 1:1 with the winding 10, a primary winding 12, and a secondary winding 13.
and an isolated transformer 15 having an electrostatic shield 14, and the isolated transformer 15 has a balanced load 16.
The two-line transformer 11 is connected to an unbalanced load 17, and the electrostatic shield 14 is connected to the end 18 of the second winding 10, and the beginning 19 of the second winding 10 is grounded.

次にこの様な構成の変成器の動作を説明する。
一般に、不衡平負荷17のインピーダンスは50Ω
又は75Ωであるためこの時の2条線路型変成器1
1の特性インピーダンスWbは50Ω又は75Ωで良
い。この特性インピーダンスは第1および第2巻
線および9,10を一般に市販されている線材を
トロイダル磁心にバイフアイラ巻きすることによ
り得られる。
Next, the operation of the transformer having such a configuration will be explained.
Generally, the impedance of unbalanced load 17 is 50Ω
Or since it is 75Ω, the double line type transformer 1 in this case
The characteristic impedance Wb of 1 may be 50Ω or 75Ω. This characteristic impedance is obtained by bifilar winding the first and second windings and 9, 10 using commercially available wires around a toroidal magnetic core.

次に縦電流減衰量(20logE1/E2)について説
明する。第2図において、平衡負荷の中点20よ
り流入した縦電流は二次巻線13と静電遮へい1
4の静電容量C2Sを介して第2巻線10の巻終り
18に印刷される。このことから第2図の縦電流
に対する等価回路は第3図のように書ける。第3
図において、i1およびi2は図に示すように閉ルー
プをとつたときの各ループの電流である。ここ
で、第1巻線9と第2巻線10が密結合すなわち
第1および第2巻線9,10のインダクタンスL
と第1および第2巻線9,10間の相互インダク
タンスMが等しいとすると、i2により負荷17お
よび抵抗23に生ずる電圧VRおよびV23は大きさ
が同じで方向が互いに逆の関係を有している。一
方、2条線路型変成器9は入力電圧をそのまま出
力する性質を有するため、抵抗23の両端の電圧
V23は負荷17にそのまま出力される。従つて、
負荷17には、電圧VRとこれと極性の異なる電
圧V23が与えられるため、その合成電圧は零とな
る。すなわち、負荷17を流れる電流i2は零とな
り、その縦電流減衰量は無限大となる。しかし、
実際には浮遊容量や、結合係数(M/L)が1で
ないため有限値となる。
Next, the amount of longitudinal current attenuation (20logE 1 /E 2 ) will be explained. In Fig. 2, the longitudinal current flowing from the midpoint 20 of the balanced load flows through the secondary winding 13 and the electrostatic shield 1.
It is printed on the end winding 18 of the second winding 10 via a capacitance C 2S of 4. From this, the equivalent circuit for the longitudinal current in FIG. 2 can be written as shown in FIG. 3. Third
In the figure, i 1 and i 2 are the currents in each loop when a closed loop is taken as shown in the figure. Here, the first winding 9 and the second winding 10 are tightly coupled, that is, the inductance L of the first and second windings 9 and 10 is
Assuming that the mutual inductance M between the first and second windings 9 and 10 is equal, the voltages V R and V 23 generated in the load 17 and the resistor 23 due to i 2 have the same magnitude and opposite directions. have. On the other hand, since the double line type transformer 9 has the property of outputting the input voltage as it is, the voltage across the resistor 23 is
V 23 is output to the load 17 as is. Therefore,
Since the load 17 is applied with the voltage V R and the voltage V 23 with a different polarity from this, the combined voltage is zero. That is, the current i 2 flowing through the load 17 becomes zero, and its longitudinal current attenuation becomes infinite. but,
Actually, since the stray capacitance and the coupling coefficient (M/L) are not 1, they are finite values.

第4図は本考案の変成器と従来のそれとの特性
の比較をインピーダンス比75Ω(変成器11の特
性インピーダンス):300Ω(平衡負荷16のイ
ンピーダンス)の変成器を例にとり示したもの
で、曲線Bに示されるように、本考案の変成器で
は不整合減衰量が大巾に改善されている。また、
曲線Aに示されるように縦電流減衰も改善されて
いる。
Figure 4 shows a comparison of the characteristics of the transformer of the present invention and that of a conventional one, taking as an example a transformer with an impedance ratio of 75Ω (characteristic impedance of transformer 11):300Ω (impedance of balanced load 16). As shown in Fig. B, the mismatch attenuation is greatly improved in the transformer of the present invention. Also,
The longitudinal current decay is also improved as shown in curve A.

ここで変成器の各エレメントに如何なる特性を
有するものを使用するかについて説明する。2条
線路型変成器11の特性インピーダンスWbは75
Ωであればよく、容易に実現できる。変成器15
の巻線13は、この場合、平衡負荷インピーダン
スが300Ωであるから、300Ωに近くなるよう巻線
仕様内容を定る。同様に巻線12は特性インピー
ダンス75Ωに近づくよう巻線仕様を定めている。
Here, the characteristics of each element of the transformer will be explained. The characteristic impedance Wb of the double line type transformer 11 is 75
Ω, and can be easily realized. Transformer 15
In this case, the balanced load impedance of the winding 13 is 300Ω, so the winding specifications are determined to be close to 300Ω. Similarly, the winding specifications for the winding 12 are set so that the characteristic impedance approaches 75Ω.

以上のように、本考案の変成器では2条線路型
変成器を不平衡側に設け、静電遮へいを有する絶
縁型変成器を平衡側に設けるとともに縦電流が2
条線路型変成器の接地された巻線側に加わるよう
構成されているため、不整合減衰量および縦電流
減衰量がともに改善される。
As described above, in the transformer of the present invention, a double line type transformer is installed on the unbalanced side, an insulation type transformer with electrostatic shielding is installed on the balanced side, and the longitudinal current is
Since it is configured to be applied to the grounded winding side of the strip line type transformer, both mismatch attenuation and longitudinal current attenuation are improved.

なお、本考案は上述の実施例に限定されること
なく絶縁型変成器の巻数比および磁心形状は任意
に変えられ、第5図に示すように、絶縁型変成器
15と平衡負荷16との間に更に2条線路型変成
器21を接続する構成にしてもよい。
Note that the present invention is not limited to the above-described embodiments, and the turns ratio and magnetic core shape of the insulation type transformer can be changed arbitrarily, and as shown in FIG. A configuration may also be adopted in which a double line type transformer 21 is further connected between them.

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

第1図は従来の平衡不平衡変換変成器を示す回
路図、第2図は本考案の一実施例を示す回路図、
第3図は第2図の縦電流に対する特価回路、第4
図は本考案の変成器と従来のそれとの特性の比較
を示す図および第5図は本考案の他の実施例を示
す回路図である。第1図〜第5図において、 1,5……磁心、2,9,21……2条線路型
変成器、3,12……一次巻線、4,13……二
次巻線、6,15……絶縁型変成器、7,16…
…平衡負荷、8,17……不平衡平負荷、9……
第1巻線、10……第2巻線、14……静電遮へ
い、18……巻終り、19……巻始め、20……
中点。
FIG. 1 is a circuit diagram showing a conventional balanced/unbalanced conversion transformer, and FIG. 2 is a circuit diagram showing an embodiment of the present invention.
Figure 3 shows the special price circuit for the longitudinal current in Figure 2, and Figure 4.
The figure shows a comparison of characteristics between the transformer of the present invention and a conventional one, and FIG. 5 is a circuit diagram showing another embodiment of the present invention. In Figs. 1 to 5, 1, 5...Magnetic core, 2,9,21...Double line type transformer, 3,12...Primary winding, 4,13...Secondary winding, 6 , 15...Insulated transformer, 7, 16...
...Balanced load, 8,17...Unbalanced flat load, 9...
1st winding, 10...2nd winding, 14...static shielding, 18...end of winding, 19...beginning of winding, 20...
Midpoint.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 2条線路型変成器を不平衡側に設けこの変成器
と磁気結合していない絶縁型変成器を平衡側に設
けた平衡不平衡変換変成器であつて、前記2条線
路型変成器の第1巻線の巻始めを不平衡負荷に接
続し、前記2条線路型変成器の第2巻線の巻始め
を接地し、前記第1巻線の巻終りを前記絶縁型変
成器の一次巻線の一端に接続し、前記第2巻線の
巻終りを前記一次巻線の他端に接続し、前記絶縁
型変成器の一次および二次巻線間に静電遮蔽を行
う手段を設けるとともに前記静電遮蔽手段を前記
第2巻線の巻終りに接続したことを特徴とする平
衡不平衡変換変成器。
A balanced-unbalanced conversion transformer in which a two-line type transformer is provided on the unbalanced side and an insulating type transformer that is not magnetically coupled to this transformer is provided on the balanced side, the second line of the two-line type transformer being The beginning of the first winding is connected to an unbalanced load, the beginning of the second winding of the two-line transformer is grounded, and the end of the first winding is connected to the primary winding of the isolated transformer. and connecting the end of the second winding to the other end of the primary winding to provide electrostatic shielding between the primary and secondary windings of the isolated transformer; A balanced/unbalanced conversion transformer, characterized in that the electrostatic shielding means is connected to the end of the second winding.
JP12925178U 1978-09-19 1978-09-19 Expired JPS6133616Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12925178U JPS6133616Y2 (en) 1978-09-19 1978-09-19

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12925178U JPS6133616Y2 (en) 1978-09-19 1978-09-19

Publications (2)

Publication Number Publication Date
JPS5545289U JPS5545289U (en) 1980-03-25
JPS6133616Y2 true JPS6133616Y2 (en) 1986-10-01

Family

ID=29093722

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12925178U Expired JPS6133616Y2 (en) 1978-09-19 1978-09-19

Country Status (1)

Country Link
JP (1) JPS6133616Y2 (en)

Also Published As

Publication number Publication date
JPS5545289U (en) 1980-03-25

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