JPS6322039B2 - - Google Patents
Info
- Publication number
- JPS6322039B2 JPS6322039B2 JP4113781A JP4113781A JPS6322039B2 JP S6322039 B2 JPS6322039 B2 JP S6322039B2 JP 4113781 A JP4113781 A JP 4113781A JP 4113781 A JP4113781 A JP 4113781A JP S6322039 B2 JPS6322039 B2 JP S6322039B2
- Authority
- JP
- Japan
- Prior art keywords
- phase
- current
- lamp
- control element
- half cycle
- 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
Links
- 238000010586 diagram Methods 0.000 description 7
- DGAQECJNVWCQMB-PUAWFVPOSA-M Ilexoside XXIX Chemical compound C[C@@H]1CC[C@@]2(CC[C@@]3(C(=CC[C@H]4[C@]3(CC[C@@H]5[C@@]4(CC[C@@H](C5(C)C)OS(=O)(=O)[O-])C)C)[C@@H]2[C@]1(C)O)C)C(=O)O[C@H]6[C@@H]([C@H]([C@@H]([C@H](O6)CO)O)O)O.[Na+] DGAQECJNVWCQMB-PUAWFVPOSA-M 0.000 description 5
- 229910052708 sodium Inorganic materials 0.000 description 5
- 239000011734 sodium Substances 0.000 description 5
- 230000003111 delayed effect Effects 0.000 description 2
- 238000001514 detection method Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 1
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 1
- 229910052753 mercury Inorganic materials 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- 230000001960 triggered effect Effects 0.000 description 1
Landscapes
- Circuit Arrangements For Discharge Lamps (AREA)
Description
【発明の詳細な説明】
本発明は、放電灯の始動直後から定格点灯状態
に移行するまでの間において、放電灯の入力電流
を定格時の入力電流以下に制御することのできる
放電灯定入力点灯装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a constant input current for a discharge lamp that can control the input current of the discharge lamp to be below the input current at the rated time from immediately after the discharge lamp starts to when the discharge lamp shifts to the rated lighting state. It relates to a lighting device.
近年、点灯装置の小型、軽量及び省電力の要求
に応えるため、水銀灯や高圧ナトリウム灯のよう
に高圧蒸気圧の放電灯の点灯回路においても、放
電灯と直列に交流制御素子を接続し、この交流制
御素子の導通位相角を制御して限流インピーダン
スを小さくする、いわゆる位相制御方式が研究さ
れ、一部では実用化されている。第1図はその原
理的回路を示す図面であつて、図中1は商用電
源、2は限流インピーダンス素子、3は放電灯、
4は交流制御素子、5は交流制御素子4のオフ時
に限流インピーダンス素子2を補償する限流要素
である。第2図a及びbは放電灯3のランプ電流
Ilaと電源電圧Vsの位相関係を示し、同図aは始
動直後の状態を、同図bは定格時の状態を示す。 In recent years, in order to meet the demand for compact, lightweight, and power-saving lighting devices, AC control elements are connected in series with the discharge lamps, even in the lighting circuits of high-pressure vapor pressure discharge lamps such as mercury lamps and high-pressure sodium lamps. A so-called phase control method, which reduces current-limiting impedance by controlling the conduction phase angle of an AC control element, has been researched and has been put into practical use in some cases. Figure 1 is a diagram showing the principle circuit, in which 1 is a commercial power supply, 2 is a current-limiting impedance element, 3 is a discharge lamp,
4 is an AC control element, and 5 is a current limiting element that compensates for the current limiting impedance element 2 when the AC control element 4 is off. Figure 2 a and b show the lamp current of discharge lamp 3.
The phase relationship between I la and the power supply voltage Vs is shown. Figure a shows the state immediately after starting, and figure b shows the state at the rated time.
一般に、高圧放電灯は始動直後、ランプコンダ
クタンスが定格時に比べて非常に大きいため、交
流制御素子4の導通位相θを、第2図に示す如く
定格時に比べて適当に遅らせる必要がある。この
ような位相制御を行なえば、定格に移行するまで
の期間(以下始動期間という)、入力電流を定格
時の入力電流以下に抑えることができ、定入力始
動が可能であり、更に本願出願人は先に、商用電
源1に交流制御素子4、限流インピーダンス素子
2及び放電灯3を直列に接続し、商用電源電圧
Vsのゼロクロス位相よりランプ電流Ilaが転流す
るまでのランプ電流転流位相角Tに対応して上記
交流制御素子4の導通位相θを、商用電源の半サ
イクル毎に制御する制御回路を有する放電灯定入
力点灯装置において、制御すべき現半サイクルの
直前のランプ電流転流位相角Ti-1に対応して、
該現半サイクルの交流制御素子4の導通位相θiを
制御する制御回路を設けたことを特徴とする放電
灯定入力点灯装置を出願したが、かかる点灯装置
においては、始動過程において発生するランプ電
流波形の正負非対称の問題は改善されているが、
グロー放電時におけるランプ電流Ilaの急増現象
は改善されていない。 Generally, immediately after starting a high-pressure discharge lamp, the lamp conductance is much larger than at the rated time, so it is necessary to appropriately delay the conduction phase θ of the AC control element 4 compared to the rated time, as shown in FIG. If such phase control is performed, the input current can be suppressed to less than the input current at the rated value during the period until the transition to the rated value (hereinafter referred to as the starting period), and constant input starting is possible. First, connect the AC control element 4, current limiting impedance element 2, and discharge lamp 3 in series to the commercial power supply 1, and set the commercial power supply voltage.
A lamp having a control circuit that controls the conduction phase θ of the AC control element 4 every half cycle of the commercial power supply in accordance with the lamp current commutation phase angle T from the zero cross phase of Vs to the commutation of the lamp current Ila. In a lamp constant input lighting device, corresponding to the lamp current commutation phase angle Ti -1 immediately before the current half cycle to be controlled,
The application has been filed for a constant input lighting device for a discharge lamp characterized in that it is equipped with a control circuit that controls the conduction phase θi of the AC control element 4 during the current half cycle. Although the problem of positive and negative asymmetry of the waveform has been improved,
The sudden increase in lamp current Ila during glow discharge has not been improved.
このランプ電流Ilaの急増現象について説明す
ると、第3図においては電源電圧Vsの(i+2)
半サイクルに大電流が流れるが、この現象の生じ
る条件は半波点灯である。グロー放電時、ランプ
内部の放電破壊が不完全なための当然半波点灯も
ある。この状況が(i+1)半サイクルで生じた
時どうなるかを第3図は示している。すなわち、
i半サイクルにおいて、ランプ電流転流位相Ti
が大きく遅れたとする。この場合、(i−1)半
サイクルでは大電流がランプに流れている。する
と(i−1)半サイクルにおけるランプ電流転流
位相角Ti-1は小さいから、i半サイクルにおけ
る交流制御素子4のオフ期間△Tiも小さくなる。
従つて、交流制御素子4の導通位相θi(=Ti+△
Ti)は遅れるため、i半サイクルから(i+1)
半サイクルに亘るランプ電流Ilaは小さくなる。
そして、(i+1)半サイクルで半波点灯したと
するとTi+1が小さくなり△Ti+1は大きくな
る。この時、半波点灯しているためランプ電流
Ilaは小さく、(i+2)半サイクルにおいて大電
流が流れる。 To explain this rapid increase in lamp current Ila, in Fig. 3, (i+2) of power supply voltage Vs
A large current flows during a half cycle, and the condition for this phenomenon is half-wave lighting. During glow discharge, there is naturally half-wave lighting because the discharge breakdown inside the lamp is incomplete. Figure 3 shows what happens when this situation occurs in (i+1) half cycles. That is,
In the i half cycle, the lamp current commutation phase Ti
Suppose that there is a large delay. In this case, a large current flows through the lamp during the (i-1) half cycle. Then, since the lamp current commutation phase angle Ti -1 in the (i-1) half cycle is small, the off period ΔTi of the AC control element 4 in the i half cycle also becomes small.
Therefore, the conduction phase θi (=Ti+△
Ti) is delayed, so from i half cycle to (i+1)
The lamp current Ila over a half cycle is small.
If half-wave lighting is performed for (i+1) half cycles, Ti+1 becomes smaller and ΔTi+1 becomes larger. At this time, the lamp current is
Ila is small, and a large current flows in (i+2) half cycles.
このように、定入力制御条件Ti-1−△Tiの関
係は交流制御素子4の導通位相θの収束効果はあ
るが、このままだと導通位相θが異常に前に進む
現象をグロー放電期間中は防ぐことができず、グ
ロー放電期間の数秒間は交流制御素子4の信頼性
を低下させる。 In this way, the constant input control condition Ti -1 −△Ti has the effect of converging the conduction phase θ of the AC control element 4, but if it continues as it is, the conduction phase θ will abnormally advance during the glow discharge period. This cannot be prevented and reduces the reliability of the AC control element 4 for several seconds during the glow discharge period.
本発明はかかる点に鑑みなされたもので、その
目的とするところは、グロー放電時における交流
制御素子の導通位相が異常に前に進むの防止する
ことにより、交流制御素子の信頼性を向上させる
にある。 The present invention has been made in view of the above, and its purpose is to improve the reliability of the AC control element by preventing the conduction phase of the AC control element from abnormally advancing during glow discharge. It is in.
高圧ナトリウム灯の場合、電源投入直後よりヒ
ータ抵抗に十分なヒータ電流を流す必要があるた
め、交流制御素子4のオフ期間△Tiをランプ始
動直後に制御すべきオフ期間△Tiよりかなり小
さくする必要がある。また、電源投入直後はラン
プ電流転流位相Ti-1はヒータが高抵抗であるた
め、ランプ始動直後よりかなり前に進む。この様
子を示したものが第4図で、図中イ点は高圧ナト
リウム灯を一般に始動させるに十分な予熱電流
0.8Aを得る位相条件を示している。そして、こ
のヒータ電流位相は、第5図に示す主チヨークコ
イル2のインダクタンスとヒータ抵抗だけで決る
定常位相となり、ヒータ予熱時は一定である。従
つて、ヒータ予熱期間においては、上記予め設定
した交流制御素子4の導通位相の上限を、1半サ
イクルもこえることなくイ点に固定されることに
なる。そして、ヒータスイツチが開路し、ランプ
が始動し始めグロー放電に入るとランプ電流転流
位相Tが乱れるため、上記導通位相の上限をこえ
ることがある。本発明はこの上限位相をこえた時
は、その上限位相を交流制御素子の導通位相とし
たものである。 In the case of high-pressure sodium lamps, a sufficient heater current must flow through the heater resistor immediately after the power is turned on, so the off-period △Ti of the AC control element 4 needs to be much smaller than the off-period △Ti that should be controlled immediately after the lamp starts. There is. In addition, immediately after the power is turned on, the lamp current commutation phase Ti -1 advances much earlier than immediately after the lamp is started, because the heater has a high resistance. This situation is shown in Figure 4, where point A indicates the preheating current sufficient to generally start a high-pressure sodium lamp.
The phase conditions for obtaining 0.8A are shown. This heater current phase becomes a steady phase determined only by the inductance of the main choke coil 2 and the heater resistance shown in FIG. 5, and is constant during heater preheating. Therefore, during the heater preheating period, the preset upper limit of the conduction phase of the AC control element 4 is fixed at point A without exceeding one and a half cycles. Then, when the heater switch is opened and the lamp starts to start and enters a glow discharge, the lamp current commutation phase T is disturbed and may exceed the upper limit of the conduction phase. In the present invention, when this upper limit phase is exceeded, the upper limit phase is made the conduction phase of the AC control element.
第6図は本発明を実現する回路の働きを示すブ
ロツク図で、第7図は同上の各部のタイミングチ
ヤートである。第4図における現半サイクルの直
前のランプ電流転流位相Ti-1は第1クロツク1
0の加算カウント期間で検出し、現半サイクルの
交流制御素子4のオフ期間△Tiは、上記第1ク
ロツク10の加算カウント数と同数の第2クロツ
ク11のクロツクパルスを減算して減算カウンタ
12の内容が現半サイクルのランプ電流転流位相
Ti以降よりゼロとなるまでの期間としている。
尚、加算カウンタ13の初期値N0は第4図の△
T0に相当する第2クロツクカウント数である。 FIG. 6 is a block diagram showing the function of a circuit implementing the present invention, and FIG. 7 is a timing chart of each part of the same. The lamp current commutation phase Ti -1 immediately before the current half cycle in FIG.
It is detected during the addition count period of 0, and the off period ΔTi of the AC control element 4 in the current half cycle is calculated by subtracting the same number of clock pulses from the second clock 11 as the number of addition counts from the first clock 10. The content is the lamp current commutation phase of the current half cycle.
The period is defined as the period after Ti until it becomes zero.
Note that the initial value N0 of the addition counter 13 is △ in FIG.
This is the second clock count corresponding to T0 .
次に動作を説明する。電源電圧ゼロクロス検出
回路14で電源電圧Vsのゼロクロス位相を検出
すると、第4図におけるT0の期間、加算カウン
タ13の内容を初期値N0でプリセツトする。そ
して、時間T0経過後、加算カウンタは第1クロ
ツクパルスを加算カウントしランプ電流Ilaが転
流する迄カウントしつづける。一方、減算カウン
タ12は電源電圧Vsのゼロクロス検出後よりラ
ンプ電流Ilaが転流する迄、遅延回路15(ラツ
チ回路)の出力をプリセツトしている。ランプ電
流Ilaが転流すると同時に加算カウンタ12の内
容が遅延回路15に入力されると同時に、減算カ
ウンタ12は、第2クロツク11のクロツクパル
スを減算開始する。従つて減算カウンタ12は直
前の半サイクルでのランプ電流Ilaの転流位相角
Ti-1に相当する第1クロツクパルス数を減算す
ることになる。そしてゼロ比較回路16で減算カ
ウンタ12の内容がゼロになつた時刻に第7図の
Cに示すパルスを出力する。このパルスCは前記
定入力始動の制御条件Ti-1−△Tiで求まつた交
流制御素子4の導通位相角θで発生することにな
る。第7図のbは基準パルス発生回路17により
発生する基準パルスで、正の期間が交流制御素子
4の導通位相θの禁止位相である。 Next, the operation will be explained. When the power supply voltage zero cross detection circuit 14 detects the zero cross phase of the power supply voltage Vs, the contents of the addition counter 13 are preset to the initial value N0 during the period T0 in FIG. Then, after the time T0 has elapsed, the addition counter adds and counts the first clock pulse and continues counting until the lamp current Ila commutates. On the other hand, the subtraction counter 12 presets the output of the delay circuit 15 (latch circuit) from after the zero crossing of the power supply voltage Vs is detected until the lamp current Ila commutates. At the same time as the lamp current Ila commutates and the contents of the addition counter 12 are input to the delay circuit 15, the subtraction counter 12 starts subtracting the clock pulses of the second clock 11. Therefore, the subtraction counter 12 calculates the commutation phase angle of the lamp current Ila in the previous half cycle.
The number of first clock pulses corresponding to Ti -1 will be subtracted. Then, the zero comparator circuit 16 outputs a pulse shown at C in FIG. 7 at the time when the content of the subtraction counter 12 becomes zero. This pulse C is generated at the conduction phase angle θ of the AC control element 4 determined by the constant input starting control condition Ti −1 −ΔTi. 7b is a reference pulse generated by the reference pulse generation circuit 17, and the positive period is the prohibited phase of the conduction phase θ of the AC control element 4.
而して、基準パルスbとフリツプ・フロツプ1
8の出力dとのANDゲート19を介した出力e
は、ゼロ比較回路16で出力されるパルスCが基
準パルスbの正区間に入つたとき発生する。言い
換えれば、eの正パルスが発生した時が、交流制
御素子4の制限位相をこえた時であり、そして、
出力eと出力cとのORゲート20を介した出力
fの正パルスで交流制御素子4をトリガする。
尚、第6図において21はランプ電流転流位相検
出回路であり、図中a〜fの符号はそれぞれ第7
図のa〜fの信号出力を示す。 Therefore, reference pulse b and flip-flop 1
Output e via AND gate 19 with output d of 8
occurs when the pulse C output from the zero comparison circuit 16 enters the positive interval of the reference pulse b. In other words, the time when the positive pulse e is generated is the time when the phase limit of the AC control element 4 is exceeded, and
The AC control element 4 is triggered by a positive pulse of the output f via the OR gate 20 of the outputs e and c.
In addition, in FIG. 6, 21 is a lamp current commutation phase detection circuit, and the symbols a to f in the figure are the seventh
The signal outputs a to f in the figure are shown.
このように、導通位相が異常に遅れないように
しておけば、第3図における(i+2)半サイク
ルの現象は発生せず、また、前記Ti-1−△Tiの
制御条件による収束効果で導通位相は収束するこ
とになる。 In this way, if the conduction phase is prevented from being abnormally delayed, the (i+2) half-cycle phenomenon in Figure 3 will not occur, and the convergence effect due to the control condition of Ti -1 -△Ti will cause conduction. The phase will converge.
従つて、従来のように電源投入後、強制的にタ
イマーで交流制御素子の導通位相を固定しないの
で、高圧ナトリウム灯をも確実に始動でき、しか
もグロー放電時に、導通位相は上限位相より遅れ
ることがないので交流制御素子への突入電流が抑
制でき、該素子の信頼性の向上が図れ、予熱時に
電源回路にノイズが入つてもそれによつて導通位
相が固定されることがないのでより確実な始動が
可能となる。 Therefore, since the conduction phase of the AC control element is not forcibly fixed by a timer after the power is turned on as in the past, high-pressure sodium lamps can be started reliably, and moreover, the conduction phase lags behind the upper limit phase during glow discharge. Since there is no noise, the inrush current to the AC control element can be suppressed, improving the reliability of the element, and even if noise enters the power supply circuit during preheating, the conduction phase will not be fixed due to it, making it more reliable. It is now possible to start.
第1図は放電灯定入力点灯装置の原理的回路
図、第2図a及びbは同上の放電灯のランプ電流
と電源電圧の波形図で、aは始動直後の状態を、
bは定格時の状態を示す。第3図はグロー放電時
における従来のランプ電流及び電源電圧の波形
図、第4図は本発明に係る高圧ナトリウム灯の始
動に必要な制御条件を示す説明図、第5図は本発
明の原理的回路図、第6図は本発明の制御回路の
働きを示すブロツク図、第7図は同上の各部のタ
イムチヤートである。
Fig. 1 is a principle circuit diagram of a discharge lamp constant input lighting device, Fig. 2 a and b are waveform diagrams of the lamp current and power supply voltage of the same discharge lamp, and a shows the state immediately after starting.
b indicates the rated state. Fig. 3 is a waveform diagram of the conventional lamp current and power supply voltage during glow discharge, Fig. 4 is an explanatory diagram showing the control conditions necessary for starting the high-pressure sodium lamp according to the present invention, and Fig. 5 is the principle of the present invention. FIG. 6 is a block diagram showing the function of the control circuit of the present invention, and FIG. 7 is a time chart of each part of the same.
Claims (1)
ス素子及び放電灯を直列に接続し、商用電源電圧
のゼロクロス位相よりランプ電流が転流するまで
のランプ電流転流位相角に対応して上記交流制御
素子の導通位相を、商用電源の半サイクル毎に制
御する制御回路を有する放電灯定入力点灯装置に
おいて、制御すべき現半サイクルの直前のランプ
電流転流位相角に対応して、該現半サイクルの交
流制御素子の導通位相を制御する制御回路を設け
ると共に、上記導通位相が半サイクル毎の一定位
相より遅れた時、その一定位相を前記交流制御素
子の導通位相としたことを特徴とする放電灯定入
力点灯装置。1. An AC control element, a current limiting impedance element, and a discharge lamp are connected in series to a commercial power supply, and the AC control element In a discharge lamp constant input lighting device having a control circuit that controls the conduction phase of the current half cycle for each half cycle of the commercial power supply, the current half cycle A control circuit for controlling the conduction phase of the AC control element is provided, and when the conduction phase lags behind a constant phase for each half cycle, the constant phase is set as the conduction phase of the AC control element. Electric light constant input lighting device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4113781A JPS57154798A (en) | 1981-03-20 | 1981-03-20 | Discharge lamp constant input firing device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4113781A JPS57154798A (en) | 1981-03-20 | 1981-03-20 | Discharge lamp constant input firing device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57154798A JPS57154798A (en) | 1982-09-24 |
| JPS6322039B2 true JPS6322039B2 (en) | 1988-05-10 |
Family
ID=12600039
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4113781A Granted JPS57154798A (en) | 1981-03-20 | 1981-03-20 | Discharge lamp constant input firing device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57154798A (en) |
-
1981
- 1981-03-20 JP JP4113781A patent/JPS57154798A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57154798A (en) | 1982-09-24 |
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