JPS5960999A - Zero cross detector for dimming discharge lamp - Google Patents

Zero cross detector for dimming discharge lamp

Info

Publication number
JPS5960999A
JPS5960999A JP17221882A JP17221882A JPS5960999A JP S5960999 A JPS5960999 A JP S5960999A JP 17221882 A JP17221882 A JP 17221882A JP 17221882 A JP17221882 A JP 17221882A JP S5960999 A JPS5960999 A JP S5960999A
Authority
JP
Japan
Prior art keywords
zero
circuit
wave
discharge lamp
zero cross
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.)
Pending
Application number
JP17221882A
Other languages
Japanese (ja)
Inventor
徳永 重行
昭弘 柴田
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.)
Toshiba Electric Equipment Corp
Toshiba Denzai KK
Original Assignee
Toshiba Electric Equipment Corp
Toshiba Denzai KK
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 Toshiba Electric Equipment Corp, Toshiba Denzai KK filed Critical Toshiba Electric Equipment Corp
Priority to JP17221882A priority Critical patent/JPS5960999A/en
Publication of JPS5960999A publication Critical patent/JPS5960999A/en
Pending legal-status Critical Current

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  • Discharge-Lamp Control Circuits And Pulse- Feed Circuits (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明は放電灯調光用ゼロ・クロス検出装置に係るもの
である1゜ 放電灯による照明のコントロール/ステムにおいては、
ザイリスの位相角又は点弧角を変化させて瞬時電力量を
調製し、それにより照明を調節している。すなわち、電
源からの正弦波形の半ザイークル期間においてゼロ・ク
ロス点を基準として点弧角を定めて調光制御を行なって
いるが、ゼロ・クロス点の検出が電源からの正弦波形の
崩れ又はノイズ成分により精確に行なえないと点弧角を
定める基準点が浮動して瞬時電力量が変動し、そのため
放電灯の照明にチラッキが生じる。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a zero-cross detection device for dimming a discharge lamp.
The phase angle or firing angle of the Xyris is varied to adjust the instantaneous amount of power and thereby the illumination. In other words, dimming control is performed by determining the firing angle with the zero-crossing point as a reference during the half-cycle period of the sine waveform from the power supply, but the detection of the zero-crossing point is due to the collapse of the sine waveform from the power supply or noise. If this cannot be done accurately depending on the components, the reference point for determining the ignition angle will float, causing fluctuations in the instantaneous amount of electric power, which will cause flickering in the illumination of the discharge lamp.

本発明の目的は電源からの正弦波形の歪み又はノイズ混
入によるゼロ・クロス点の不精確な検出を排して究極的
には放電灯の照明のチラッキを解ンI月することにある
7、 すなわち、庫発明では電源からの正弦波形をP波して正
弦波からノイズ成分を除去してこれを整形し、ゼロ・ク
ロス点以外の点をゼロ・クロス点として検出する可能性
を排除し、同時に戸波による位相遅れを袖IT< L/
て電源からの正弦波形のセロ・クロス点に整形正弦波の
ゼロ・クロス点を精確に一致させ、そしてこの整形正弦
波からゼロ・クロス点を検知するのである。
The purpose of the present invention is to eliminate inaccurate detection of zero-crossing points due to distortion of the sine waveform from the power supply or noise contamination, and ultimately to eliminate flickering in the illumination of discharge lamps7. That is, in the storage invention, the sine waveform from the power supply is converted into a P wave, the noise component is removed from the sine wave, and this is shaped, eliminating the possibility of detecting a point other than the zero-crossing point as a zero-crossing point. At the same time, the phase delay caused by Tonami is removed by IT < L/
The zero-crossing point of the shaped sine wave is precisely matched with the zero-crossing point of the sine waveform from the power supply, and the zero-crossing point is detected from this shaped sine wave.

以下に添(”1図を参照して本発明の詳細な説明する。The present invention will be described in detail below with reference to Figure 1.

第1図において、入力端子2−2に変圧器4が接続され
、この変圧器4の二次側に調整抵抗r。
In FIG. 1, a transformer 4 is connected to the input terminal 2-2, and an adjustment resistor r is connected to the secondary side of the transformer 4.

固定抵抗R1,コンデンサC1から成る第1のCRP彼
回路が接続されている。この第1のr波回路にボ′ルテ
ージ・ホロアA1が→ゑ続される。このボルテ−ジ・ホ
ロアA1の出力に固定抵抗R2,コンデンサC2から成
る第2のCRP波回路が接続されている。
A first CRP circuit consisting of a fixed resistor R1 and a capacitor C1 is connected. A voltage follower A1 is connected to this first r-wave circuit. A second CRP wave circuit consisting of a fixed resistor R2 and a capacitor C2 is connected to the output of the voltage follower A1.

この第2のCRP波回路に振rlJ補償のだめの非反転
増巾器A2を接続する。この増巾器A2の利得は帰遷回
路r1とr2の比によって定まる。増巾器A2の出力に
抵抗R3,コンデンサC3から成る第5のcRP波回路
が接続され、そしてこのp波回路にボルテージホロアA
3が接続゛される1、最後に、ボルテージホロアA3の
出力にゼロ・クロス検知回路6が接続される。8−8は
出力端子である。セロ・クロス検知回路としては正弦波
を矩形波に変換してこれを微分してゼロ・クロス点を決
定するもの、人力信号を零電位と比較し零より大きい振
巾に対して出力してこの出力波形からゼロ・クロス点を
決定するものなどがある。
A non-inverting amplifier A2 for vibration rlJ compensation is connected to this second CRP wave circuit. The gain of this amplifier A2 is determined by the ratio of the transition circuits r1 and r2. A fifth cRP wave circuit consisting of a resistor R3 and a capacitor C3 is connected to the output of the amplifier A2, and a voltage follower A is connected to this p wave circuit.
Finally, a zero cross detection circuit 6 is connected to the output of the voltage follower A3. 8-8 is an output terminal. The zero cross detection circuit converts a sine wave into a rectangular wave and differentiates it to determine the zero cross point, and compares a human signal with zero potential and outputs it for an amplitude larger than zero. There are methods that determine the zero-crossing point from the output waveform.

入力端子2−2に加えられた電源からの人力信号(ノイ
ズを含む正弦波信号)は変圧器4により適当な振巾とさ
れ第1のCRP波回路に加えられてノイズ成分を除去さ
れる。単一のCR回路では90度の移相は不可能であり
、180度の移相には少なくとも6個のC11=”波回
路を必要とする。第1、第2.第6のcR−p波回路は
ノイズ成分の除去と180度の移相とを行うだめのもの
である。具体的には、各p波回路のCRの値を適宜調整
して6段のP波で180度だけ移相を遅らせるようにす
るのであり、特に第1段のp波回路の調整抵抗rは精確
に遅れを180度とするため沖波調整を行うものである
A human input signal (a sine wave signal containing noise) from the power supply applied to the input terminal 2-2 is made into an appropriate amplitude by the transformer 4, and is applied to the first CRP wave circuit to remove the noise component. A 90 degree phase shift is not possible with a single CR circuit, and a 180 degree phase shift requires at least 6 C11 = "wave circuits. 1st, 2nd, 6th cR-p The wave circuit is designed to remove noise components and shift the phase by 180 degrees.Specifically, the CR value of each p-wave circuit is adjusted appropriately to shift the P-wave by 180 degrees in six stages. The phase is delayed, and in particular, the adjustment resistor r of the first stage p-wave circuit performs offshore adjustment to accurately set the delay to 180 degrees.

第1段と第2段のp波回路の間にあるボルテージホロア
A1と第6段のp波回路とゼロ・クロス検知回路6との
間のボルテージホロアA3はいずれも同相同賑巾で人力
信号を出力側へ伝達するが、なお減衰補償のため第2段
と第6段のp波回路の間に非ノ9′転増11」回路A2
が挿入されている3、入力インピーダンスが非常に大き
いボルテージホロアは隣接回路間の隔離又は相互独立性
を保証するだめのものである。
The voltage follower A1 between the first and second stage p-wave circuits and the voltage follower A3 between the sixth stage p-wave circuit and zero-cross detection circuit 6 are both in-phase and in-phase. Transmits the human power signal to the output side, but also has a non-circuit 9' inverted 11'' circuit A2 between the second and sixth stage p-wave circuits to compensate for the attenuation.
3, the voltage follower with a very large input impedance is used to ensure isolation or mutual independence between adjacent circuits.

第2図に第1図の構成回路の各入出力部の波形を示す。FIG. 2 shows waveforms at each input/output section of the circuit shown in FIG. 1.

第2図(a)は電源から入力端子2−2に加えられるノ
イズ成分を含む正弦波である。第2図(b)、 (c)
FIG. 2(a) shows a sine wave including noise components applied from the power supply to the input terminal 2-2. Figure 2 (b), (c)
.

(d)は6段の1lFi’lk回路によりノイズ成分を
除去され、180度移相を遅らされる様子を示す各p波
回路の出力端子に現われる波形である。第2図(e)は
ゼロ・クロス点検出回路6が発生ずるゼロ・クロス点に
おける検出パルスを示す。
(d) is a waveform appearing at the output terminal of each p-wave circuit showing how the noise component is removed by the 6-stage 1lFi'lk circuit and the phase shift is delayed by 180 degrees. FIG. 2(e) shows a detection pulse generated by the zero-crossing point detection circuit 6 at the zero-crossing point.

この検出パルス(図では負のパルス)は入力正弦波のゼ
ロ・クロス点に正確に一致しており、そしてこれを基準
として位相角を決定して、各半サイクルの瞬時電力を一
定に制御して放電灯に供給する。
This detection pulse (negative pulse in the figure) exactly coincides with the zero crossing point of the input sine wave, and the phase angle is determined using this as a reference to control the instantaneous power in each half cycle to be constant. and supplies it to the discharge lamp.

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

第1図は本発明による放電灯調光用ゼロ・クロス検出装
置の回路を示す。 第2図は第1図のゼロ・クロス検出装置の各構成回路の
入出力端子に現われる波形を示す図であり、第2図(a
)は電源から入力端子へ加えられる正弦波信号、第2図
<b) (c) <d)はそれぞれ第1段、第2段、第
6段のp波回路の出力に現われる波形、第2図(e)は
ゼロ・クロス検出回路の出力波形、そして第2図(f)
は瞬時電力を調整された電源からの正弦波形を示す11 .2・・・入力端子、4・・変圧器、6・・・ゼロ・ク
ロス検出回路、8・・・出力端子、C,、C,、、C3
・・・コンデンサ、R,、R2、R3、rl 、 r2
・・固定抵抗、r ”’可変抵抗。、 特許出願人  東芝電材株式会社 代 理 人  弁理士 伊 東辰雄 代理人 弁理士伊東哲也
FIG. 1 shows a circuit of a zero-cross detection device for dimming a discharge lamp according to the present invention. FIG. 2 is a diagram showing waveforms appearing at the input/output terminals of each component circuit of the zero-cross detection device in FIG.
) are the sine wave signals applied from the power supply to the input terminal, Figure 2 <b) (c) <d) are the waveforms appearing at the outputs of the first, second and sixth stage p-wave circuits, respectively, and the second Figure (e) shows the output waveform of the zero-cross detection circuit, and Figure 2 (f)
11. shows a sinusoidal waveform from a regulated power supply with instantaneous power. 2...Input terminal, 4...Transformer, 6...Zero cross detection circuit, 8...Output terminal, C,,C,,,C3
...Capacitor, R,, R2, R3, rl, r2
・・Fixed resistance, r ''Variable resistance., Patent applicant: Toshiba Electric Materials Co., Ltd. Agent: Patent attorney: Tatsuo Ito, Patent attorney: Tetsuya Ito

Claims (1)

【特許請求の範囲】[Claims] 入力信号の位相をnπ(nは整数)たけ遅らせる少なく
とも6つのCT1戸波回路の直列1g:続とnπ遅らさ
れた信号のゼロ・クロスを検出する回路とを備えた放電
灯’−’j、′+l光用ゼロ・クロス検出装置、
A discharge lamp '-'j, comprising a series of at least six CT1 Tonami circuits that delay the phase of the input signal by nπ (n is an integer) and a circuit for detecting the zero crossing of the signal delayed by nπ, '+l zero cross detection device,
JP17221882A 1982-09-30 1982-09-30 Zero cross detector for dimming discharge lamp Pending JPS5960999A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17221882A JPS5960999A (en) 1982-09-30 1982-09-30 Zero cross detector for dimming discharge lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17221882A JPS5960999A (en) 1982-09-30 1982-09-30 Zero cross detector for dimming discharge lamp

Publications (1)

Publication Number Publication Date
JPS5960999A true JPS5960999A (en) 1984-04-07

Family

ID=15937778

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17221882A Pending JPS5960999A (en) 1982-09-30 1982-09-30 Zero cross detector for dimming discharge lamp

Country Status (1)

Country Link
JP (1) JPS5960999A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2012081350A1 (en) * 2010-12-14 2012-06-21 株式会社エルム Highly stable dimming device
WO2013187166A1 (en) * 2012-06-11 2013-12-19 株式会社エルム High-stability dimming device

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2012081350A1 (en) * 2010-12-14 2012-06-21 株式会社エルム Highly stable dimming device
JP5070587B2 (en) * 2010-12-14 2012-11-14 株式会社エルム Highly stable dimmer
US8618743B2 (en) 2010-12-14 2013-12-31 Elm Inc. High stability dimmer
WO2013187166A1 (en) * 2012-06-11 2013-12-19 株式会社エルム High-stability dimming device
JP5458457B1 (en) * 2012-06-11 2014-04-02 株式会社エルム Highly stable dimmer
US9220144B2 (en) 2012-06-11 2015-12-22 Elm Inc. High-stability dimmer

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