JPH01103162A - Waveform controller - Google Patents
Waveform controllerInfo
- Publication number
- JPH01103162A JPH01103162A JP25953587A JP25953587A JPH01103162A JP H01103162 A JPH01103162 A JP H01103162A JP 25953587 A JP25953587 A JP 25953587A JP 25953587 A JP25953587 A JP 25953587A JP H01103162 A JPH01103162 A JP H01103162A
- Authority
- JP
- Japan
- Prior art keywords
- transformer
- peak voltage
- voltage
- generation
- peak
- 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.)
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Links
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- Ac-Ac Conversion (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、波形制御装置、特に最大値を近似的に維持し
ながら実効値を低下させる波形制御装置に関するもので
ある。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a waveform control device, and particularly to a waveform control device that reduces an effective value while approximately maintaining a maximum value.
電力需要家において、その電力需要量(電力消費it)
を抑制して電力料金の低減を図ることは経済的な面から
切火な問題である。For electricity consumers, their electricity demand (power consumption it)
It is an urgent problem from an economic point of view to try to reduce electricity charges by suppressing electricity consumption.
電力需要量を抑制するには受電点の電圧の実効値を低下
させることによって、その目的をはたすことができる。In order to suppress the power demand, the purpose can be achieved by lowering the effective value of the voltage at the receiving point.
しかしながら、蛍光灯や、水銀灯等の放電灯、またはマ
グネットスイッチ等のように、成る値以下に電圧が低下
すると、その機能かはたせなくなる電気機器がある。し
たがって、単に電圧の実効値を低下させるだけでは、成
る電気機器について動作しなくなる可能性があるので実
用的ではない。However, there are some electrical devices, such as fluorescent lamps, discharge lamps such as mercury lamps, and magnetic switches, which lose their functionality if the voltage drops below this value. Therefore, simply reducing the effective value of the voltage is not practical because the electrical equipment may stop working.
本発明の目的は、最大値を近似的に維持しながら、波形
分割方式によって実効値を低下させる波形制御装置を提
供することにある。An object of the present invention is to provide a waveform control device that reduces the effective value using a waveform division method while approximately maintaining the maximum value.
c問題点を解決するための手段〕
本発明の波形制御装置は、
正弦波交流電圧からピーク電圧を発生するピーク電圧発
生用変圧器と、
発生されたピーク電圧を、前記正弦波交流電圧に対して
逆極性で注入するピーク電圧逆注入用変圧器とを備え、
最大値を近似的に維持しながら実効値を低下させるごと
を特徴としている。Means for Solving Problem c] The waveform control device of the present invention includes: a peak voltage generation transformer that generates a peak voltage from a sine wave AC voltage; and a transformer for generating a peak voltage from a sine wave AC voltage; It is equipped with a peak voltage reverse injection transformer that injects with reverse polarity, and is characterized by reducing the effective value while approximately maintaining the maximum value.
第1図は、本発明の波形制御装置の基本回路図である。 FIG. 1 is a basic circuit diagram of a waveform control device of the present invention.
この波形制御装置は、ピーク電圧発生用変圧器11と、
ピーク電圧逆注入用変圧器12とから構成されている。This waveform control device includes a peak voltage generation transformer 11,
It is composed of a peak voltage reverse injection transformer 12.
ピーク電圧発生用変圧器11の2次巻線はピーク電圧逆
注入用変圧器12の1次巻線に、ピーク電圧が逆極性で
注入されるように接続されている。The secondary winding of the peak voltage generation transformer 11 is connected to the primary winding of the peak voltage reverse injection transformer 12 so that the peak voltage is injected with opposite polarity.
第2図は、ピーク電圧発生用変圧器11の一例を示す。FIG. 2 shows an example of the peak voltage generating transformer 11.
このピーク電圧発生用変圧器は、外鉄型変圧器鉄心21
の中央の脚に1次巻vA22が巻かれ、上方の継鉄部に
2次巻線23が巻かれている。継鉄部は断面を小さくす
る。このピーク電圧発生用変圧器の原理を、第3図を参
照しながら簡単に説明しておく。1次巻線による磁束Φ
、は、2つの継鉄部の磁束Φ2に分かれる。1次巻線2
2に加えられる電圧E0は正弦波電圧であり、1次巻、
122はEoより90°位相の遅れた磁束Φうを発生す
る。Φ。This peak voltage generation transformer has an outer iron type transformer core 21.
A primary winding vA22 is wound around the central leg of the yoke, and a secondary winding 23 is wound around the upper yoke. Make the cross section of the yoke smaller. The principle of this peak voltage generating transformer will be briefly explained with reference to FIG. Magnetic flux Φ due to primary winding
, is divided into two magnetic fluxes Φ2 of the yoke parts. Primary winding 2
The voltage E0 applied to 2 is a sine wave voltage, and the primary winding,
122 generates a magnetic flux Φ whose phase is delayed by 90 degrees from Eo. Φ.
は正弦波であるが、Φ2は成る磁束密度以上では急に飽
和して一定値となり、dΦ、/dt=0、従って2次起
電力は0になる。すなわち継鉄部が未飽和の期間だけ磁
束Φ2が変化し、その結果2次起電力eはピーク波とな
る。このピーク波の発生位相は、正弦波交流電圧E0の
最大値発生位相に一致している。is a sine wave, but above the magnetic flux density of Φ2, it suddenly saturates and becomes a constant value, dΦ,/dt=0, and therefore the secondary electromotive force becomes 0. That is, the magnetic flux Φ2 changes only during the period when the yoke is unsaturated, and as a result, the secondary electromotive force e becomes a peak wave. The generation phase of this peak wave coincides with the maximum value generation phase of the sinusoidal AC voltage E0.
次に、本実施例の動作を、第4図の波形図を参照しなが
ら説明する。Next, the operation of this embodiment will be explained with reference to the waveform diagram of FIG. 4.
受電した第4図(a)の正弦波交流電圧E0は、波形制
御装置のピーク電圧発生用変圧器11に供給され、第4
図(b)のピーク電圧eが形成される。The received sinusoidal AC voltage E0 of FIG. 4(a) is supplied to the peak voltage generation transformer 11 of the waveform control device, and the fourth
A peak voltage e as shown in FIG. 3(b) is formed.
このピーク電圧の発生位相は、前述したように、正弦波
交流電圧E、の最大値発生位相に一致している。ピーク
電圧eは、ピーク電圧逆注入用変圧器12を介して、正
弦波交流電圧E0に逆極性で重畳されて、第4図(c)
のように波形が分割された電圧E、が出力される。The generation phase of this peak voltage coincides with the maximum value generation phase of the sinusoidal AC voltage E, as described above. The peak voltage e is superimposed on the sinusoidal AC voltage E0 with the opposite polarity via the peak voltage reverse injection transformer 12, as shown in FIG. 4(c).
A voltage E whose waveform is divided as follows is output.
この電圧E+は、その最大値が正弦波交流電圧E、の最
大値に近似的に維持され、かつ、その実効値は低下して
いる。The maximum value of this voltage E+ is maintained approximately at the maximum value of the sinusoidal AC voltage E, and its effective value is decreasing.
したがって、このような分割波形の電圧により、蛍光灯
や、水銀灯等の放電灯、またはマグネットスイッチ等の
ように、成る値以上の電圧を必要とする機器の機能を保
持しながら、電力消費量の低減を図ることが可能となる
。Therefore, by using the voltage of such a divided waveform, the power consumption can be reduced while maintaining the functionality of devices that require a voltage higher than that value, such as fluorescent lamps, discharge lamps such as mercury lamps, and magnetic switches. It becomes possible to aim at reduction.
以上説明したように本発明によれば、波形分割方式によ
って最大値を近位的に維持しながら、実効値を低下させ
る簡単な構成の波形制御装置が得られる。As described above, according to the present invention, it is possible to obtain a waveform control device with a simple configuration that reduces the effective value while maintaining the maximum value proximally using the waveform division method.
第1図は、本発明の一実施例である波形制御装置の構成
図、
第2図は、第1図のピーク電圧発生用変圧器の一例を示
す図、
第3図は、第2図のピーク電圧発生用変圧器の動作を説
明するための波形図、
第4図は、第1図の実施例の動作を説明するための波形
図である。
11・・・・・ピーク電圧発生用変圧器12・・・・・
ピーク電圧逆注入用変圧器21・・・・・外鉄型変圧器
鉄心
22・・・・・1次巻線
23・・・・・2次巻線
代理人 弁理士 岩 佐 義 幸
第1図
e
第2図
第3図FIG. 1 is a block diagram of a waveform control device that is an embodiment of the present invention, FIG. 2 is a diagram showing an example of the peak voltage generation transformer shown in FIG. 1, and FIG. 3 is a diagram showing an example of the peak voltage generation transformer shown in FIG. FIG. 4 is a waveform diagram for explaining the operation of the peak voltage generating transformer. FIG. 4 is a waveform diagram for explaining the operation of the embodiment shown in FIG. 11...Transformer for peak voltage generation 12...
Peak voltage reverse injection transformer 21...External iron type transformer core 22...Primary winding 23...Secondary winding Agent Patent attorney Yoshiyuki Iwasa Figure 1 e Figure 2 Figure 3
Claims (1)
電圧発生用変圧器と、 発生されたピーク電圧を、前記正弦波交流電圧に対して
逆極性で注入するピーク電圧逆注入用変圧器とを備え、 最大値を近似的に維持しながら実効値を低下させる波形
制御装置。(1) A peak voltage generation transformer that generates a peak voltage from a sine wave AC voltage, and a peak voltage reverse injection transformer that injects the generated peak voltage with the opposite polarity to the sine wave AC voltage. A waveform control device that reduces the effective value while approximately maintaining the maximum value.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62259535A JP2695417B2 (en) | 1987-10-16 | 1987-10-16 | Waveform control device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62259535A JP2695417B2 (en) | 1987-10-16 | 1987-10-16 | Waveform control device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01103162A true JPH01103162A (en) | 1989-04-20 |
| JP2695417B2 JP2695417B2 (en) | 1997-12-24 |
Family
ID=17335456
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62259535A Expired - Lifetime JP2695417B2 (en) | 1987-10-16 | 1987-10-16 | Waveform control device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2695417B2 (en) |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5395227A (en) * | 1977-02-01 | 1978-08-21 | Tdk Corp | Voltage controlling transformer |
| JPS5647938U (en) * | 1980-09-02 | 1981-04-28 |
-
1987
- 1987-10-16 JP JP62259535A patent/JP2695417B2/en not_active Expired - Lifetime
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5395227A (en) * | 1977-02-01 | 1978-08-21 | Tdk Corp | Voltage controlling transformer |
| JPS5647938U (en) * | 1980-09-02 | 1981-04-28 |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2695417B2 (en) | 1997-12-24 |
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