TWI228944B - Self-oscillating electronic discharge lamp ballast with dimming control - Google Patents
Self-oscillating electronic discharge lamp ballast with dimming control Download PDFInfo
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Abstract
Description
12289441228944
Di-D4 :稽納二極體Di-D4: Zener diode
Dst :二極體Dst: Diode
Np :繞組Np: winding
Nsl :繞組Nsl: winding
Ri :電阻Ri: resistance
Rgl :閘極電阻 VB :直流電壓Rgl: Gate resistance VB: DC voltage
Dac :閘流體 Lm :激磁電感 Q1, Q2 :電晶體 ns2 :繞組 R2 :電阻 Rg2 :閘極電阻 VetH :夕卜部電壓源 柒、 本案若有化學式時,請揭示最能顯示發明特徵的化學 式: 參 捌、 聲明事項 □本案係舱專利法第二十條第一項□第一款但書或二款但書規 定之期間,其日期爲:_ 玖、 發明說明 (發明說明應敘明:發明所屬之技術領域、先前技術、內容、實施方式及圖式簡單說明) 發明所屬之技術領域 本發明係為一種可調整功率控制之自激式電源供應 器,尤指一種具有調光控制之自激式放電燈之電子安定器。 φ 先前技術 氣體放電燈管之白熱光源以螢光燈管為例,其效率之 增加始終為該技術領域研發之重點。該種氣體放電燈管之 光源一般而言其產生熱量較少並可具有較高之能源轉換效 率。該氣體放電燈管之整體效率可藉由減少熱消耗已增加 效率。然而,往昔主要討論之問題是在關於氣體放電燈管 之光頻譜及光源大小輸出控制。 然而,由於氣體放電燈管與螢光燈管之效率增益遠大 於白熾燈,使得氣體放電燈管與螢光燈管直接取代了白熾 6 1228944 燈在市場上與製造上的位置。 =复雜於白熾燈,且氣體放電燈;電子特 複雜與昂貴。 心σ同先控制電路相對 更具體而言’只有傳統氣體 (magnetic banast)可進行微 且广之-电感安定器 在現今主要應;且二子安,器 制’且具有體積小、重量輕、高發光效率、c 音等優點。調光或是亮度丄 照明糸統研發其重要考驗是在於省能 …b 超過50¾的省能效率。在商業 、,…先疋否能提供 對環境之需求控制光源之大小、,增加了 自行針 m譬如,可用來減少電腦工作站產 割與視覺上增加物體效果及空間特色。 。視見刀 I幸的是,電子安定器對於調光控制十分昂貴 ΐ及irm:主往被應用來盡可能減少控制的複雜 =本。然而,習知自激式電路之操作係藉 自然特性以及負載因素’因此其控制上相對因難, 負載、電路元件及線電壓變動的敏感度很高。其原 載、電路元件及線電壓變動會造成自激式頻率的改變,因 此改變放電燈管的功率。舉例而言’當線電壓具有i 變 動時’放電燈管功率變化率通常纟15%。這樣的變動通常 會超過± 10%放電燈管之功率限制並且縮短放電燈管的壽 命。這樣的問題不只侷限在放電燈管之控制上,同樣發: 在自激式電路配置之電源供應器或是電源轉換器 (convener ),包含降壓轉換器(buck c〇nvmer)、升壓轉換 器(boost C〇nverter )、降壓-升壓轉換器(buck b〇⑹ converter)、反驰式轉換器(F丨yback c〇nverter)、與順向式 1228944 轉換器(Forward C_erter)、推挽式轉換器(pud ! converter)、對稱式或是非對稱式半橋轉換電路以及全橋轉 換電路。 另一複雜因素為放電燈管電流峰質因素(current factor, CF ),其為放電燈管電流之峰值與電流方均根值之 t匕值。針對高頻率電子安定器(ba丨丨扣),電流峰質因素 上瞻⑽⑽1 faCt°r,CF)為電子安定器設計時重要之因 :二般而言’電流品質因素越高,放電燈管的壽命越短。 未經凋變純弦波訊號其電流峰質因素為丨4,三角波 流峰質因素為1.7。許多電子式安定琴 “ ,电 疋态像电何幫浦功率因素 校正(Charge-pump-power_fact〇r c〇rrecti〇n,⑽ 安定器係利用調變共振元件來達到功率 電流峰質因素一般皆韶禍丨7门 ’ …、而其 ,^ 、 (過·7。因此,頻率調變是最常用來 ^電流峰質因素’雖然其遭遇的困難.如同上變述…用來 職疋之故,本發明繁於習知技 之意念,發明出本案之『自激犬放”,及改良發明 控制』。 目,放式放电燈之電子安定器調光 發明内容 本發明之目的在於提供一 之電子式電源供應器、電源轉換器:°構間早,^格便宜 燈管之電子安定哭 原轉換益(c〇nverter)、或是放電 電流峰f S 供一具高效率以及較佳放電燈管 二;1:)電因 為改善電路::率】:^於提供一種高效率之技術及電路 一从、4 手U素(power fact〇0利用帝改由夕认 7C件以達到頻率調變+ ^ 一 為達到本幸夕a 4电路的電流峰質因素。 放電燈管之電子安」及構想’—電源供應器例如一氣體 女疋杰,包含一變頻器(inVerter)、一共振 1228944 匹配電路(resonant matching circuit)以及一轉換電路 —▲ erter circuit)。έ亥轉換電路(converter circuit)係用以決 2忒變頻器之切換頻率,使該切換頻率與該電源供應器之 ^載實質上無關。其中,該電源供應器係藉由該共振匹 配包路(1^〇別111 matching circuit)與該負載耦合連接。 本案得藉由以下列圖示與詳細說明,俾得一更深入之 了解。 圖示簡單說明 塊圖; 第一圖係纟案較佳實施例之電子安$器系统之電路方 犬雷:ί ί ί本案第一較佳實施例之M0SFE丁驅動之自激 式電=式電子安定器之電路示意圖: rgl · 圖, .第三圖⑷、⑻係第二圖之簡化等效電路及波形示意 塊 圖:弟四圖係本案較佳實施例之電子安定器之電路方 f五圖係第四圖之簡化等效電路示意圖; +题U⑷仏'可5周式比流^ ( current transf〇rmer)線圈 電壓等效電路示意圖; rner )、.·果圈 第七圖係本案第二 定器之電路示意圖; 弟六圖⑻係係第六圖⑷之較佳化實現之電路示意圖; 較佳實施例之自激式電子式電子安 弟八圖係本幸妨/土杏 立 系季又垃貝'把例之可應用在本案 護電路示意圖 之過電流保 第九圖(a)、(b)、(c)係本 極驅動電壓之波形示意目;以及不门-壓下切換電流及閘 第十圖(a) (b)、(c)係本案放士 壓之波形示意圖。 sw及閘極驅動電 1228944 圖示符號說明 1 0 0 ·父流電源 1 1 0 :功率因素校正交流/ 直流轉換電路 120 :直流連接電容 130 :變頻器 140 :電感 170 :該放電燈管 1 80 :内部電容 2 1 0 :金屬氧化半導體場效 電晶體 2 11 :金屬氧化半導體場效 電晶體 212 :高頻電容 214 :電感 215 :電容 310 :功率變頻器 320 :共振匹配電路 330 :閘極轉換電路 340 :電流感測器 400 :脈衝變壓器 81 1 :直流矽控管(SCR) α :相角 C 1,C 2 :電容 Θ :相角 iinj ·· 電流 iz :二極體電流 i $ ·反饋電流 i m a g ·激磁電流 cst :電容 CT :比流器 D1-D4·稽納二極體 Dae :閘流體 Dst :二極體 Lm :激磁電感 Np :繞組 Q1,Qz ·電晶體 Nsl :繞組 Ns2 :繞組 1 :電阻 R2 :電阻 Rgl :閘極電阻 Rg2 :閘極電阻 VB :直流電壓 Vctrl :外部電壓源 實施方式 請參閱第一圖,第一圖係本案較佳實施例之電子安定 器系統之電路方塊圖。如第一圖所示,電子安定器系統係 10 1228944Dac: Gate fluid Lm: Excitation inductance Q1, Q2: Transistor ns2: Winding R2: Resistor Rg2: Gate resistance VetH: Xibu Department voltage source 柒 If there is a chemical formula in this case, please disclose the chemical formula that best shows the characteristics of the invention:事项 、 Declaration items □ This case is the first paragraph of Article 20 of the Patent Law □ The period specified in paragraph 1 or paragraph 2 of the proviso, the date is: _ 玖 Description of the invention (the description of the invention shall state: (Technical field, prior art, content, implementation, and drawings are simply explained) Technical field to which the invention belongs The present invention is a self-excited power supply with adjustable power control, especially a self-excited type with dimming control Electronic ballast for discharge lamps. φ Previous technology The white light source of the gas discharge tube is a fluorescent tube as an example. The increase in efficiency has always been the focus of research and development in this technical field. The light source of such a gas discharge lamp generally generates less heat and has a higher energy conversion efficiency. The overall efficiency of the gas discharge lamp can be increased by reducing heat consumption. However, the main issues discussed in the past were the control of the light spectrum and light source output of gas discharge lamps. However, since the efficiency gains of gas discharge tubes and fluorescent tubes are much larger than those of incandescent lamps, gas discharge tubes and fluorescent tubes have directly replaced incandescent 6 1228944 lamps in the market and manufacturing positions. = Complex than incandescent and gas discharge lamps; electronics are extremely complex and expensive. The heart σ and the control circuit are relatively more specific. 'Only traditional gas (magnetic banast) can be micro and wide-inductive ballasts are mainly used today; and the two-child safety, device system' has a small size, light weight, high Luminous efficiency, c-tone and other advantages. The main test of dimming or brightness and lighting system development is energy saving ... b Energy saving efficiency over 50¾. In commerce, whether you can provide the need for the environment to control the size of the light source, and increase the self-needle m. For example, it can be used to reduce computer workstation production and visually increase the effect of objects and space characteristics. . Fortunately, fortunately, electronic ballasts are very expensive for dimming control. Ϊ́ and irm: mainly used to reduce the complexity of control as much as possible. However, the operation of the conventional self-excited circuit is based on natural characteristics and load factors, so its control is relatively difficult, and the sensitivity of the load, circuit components, and line voltage changes is very high. Variations in its original load, circuit components, and line voltage will cause the self-excited frequency to change, thus changing the power of the discharge lamp. For example, 'when the line voltage has a change in i', the power change rate of the discharge lamp is usually 纟 15%. Such changes will usually exceed the power limit of the ± 10% discharge lamp and shorten the life of the discharge lamp. Such problems are not limited to the control of discharge lamps, but they also occur: a power supply or a conventional converter configured in a self-excited circuit, including a buck converter (buck c0nvmer) and a boost converter Converter (boost C0nverter), buck-boost converter (buck b〇⑹ converter), flyback converter (F 丨 yback c〇nverter), and forward 1228944 converter (Forward C_erter), push Pud! Converter, symmetric or asymmetric half-bridge conversion circuit and full-bridge conversion circuit. Another complex factor is the peak current factor (CF) of the discharge lamp current, which is the value of the peak current and the root mean square value of the discharge lamp current. For high-frequency electronic ballasts (ba 丨 丨 buckle), the current peak quality factor is reviewed (1 faCt ° r, CF) is an important factor in the design of electronic ballasts: In general, the higher the current quality factor, the more discharge lamps The shorter the life span. For unsaturated pure sine wave signals, the current peak quality factor is 4 and the triangular wave current peak quality factor is 1.7. Many electronic ballasts are “Charge-pump-power_fact〇rc〇rrecti〇n,” the ballast state is like electricity and pump power factor correction. 7 gates ', and its, ^, (over · 7. Therefore, frequency modulation is the most commonly used to ^ current peak quality factor', although the difficulties encountered. As stated above ... used for professional purposes, the present invention Familiar with the idea of knowing the technology, he invented the "self-excited dog put" and improved invention control. "Purpose, the electronic ballast dimming of discharge type discharge lamp SUMMARY OF THE INVENTION The object of the present invention is to provide an electronic power supply. Power supply, power converter: ° Early between the structure, ^ grid cheap lamp electronic stability cry original conversion benefits (connverter), or discharge current peak f S for a high efficiency and better discharge lamp two; 1 :) Electricity because of improving the circuit :: rate]: ^ in providing a high-efficiency technology and circuit one, 4 hands U prime (power fact0 0 using Di Gaiyou to identify 7C pieces to achieve frequency modulation + ^ one In order to reach the current peak quality factor of the 4 circuit "Electrical Safety of Discharge Lamps" and Conception'—A power supply such as a gas woman, includes a frequency converter (inVerter), a resonant 1228944 matching circuit (resonant matching circuit), and a conversion circuit (▲ erter circuit). The converter circuit is used to determine the switching frequency of the 2 忒 inverter, so that the switching frequency is essentially independent of the load of the power supply. The power supply is connected by the resonance matching circuit ( 1 ^ 〇 别 111 matching circuit) and the load coupling connection. This case can get a deeper understanding by the following diagrams and detailed description. The diagram briefly illustrates the block diagram; the first diagram is the preferred implementation of the case Example of the circuit of an electronic ballast system: ί ί ί The circuit diagram of the M0SFE D-driven self-excited electric ballast electronic ballast of the first preferred embodiment of the case: rgl 2. The simplified equivalent circuit and waveform schematic block diagram of the second diagram: the fourth diagram is the circuit diagram of the electronic ballast of the preferred embodiment of the case; the fifth diagram is the simplified equivalent circuit diagram of the fourth diagram; + question U仏 '5 cycles of equivalent current ^ (current transfomer) Coil voltage equivalent circuit diagram; rner) .. · Fruit circle The seventh diagram is the circuit diagram of the second stator of the case; the sixth figure is the sixth. The circuit diagram of the optimized implementation of Figure ;; the self-excited electronic electronic safety device of the preferred embodiment is shown in Figure 8. This is a good example / the soil is a good example of the circuit can be applied to this case protection circuit diagram The ninth diagram (a), (b), and (c) of the overcurrent protection are the schematic diagrams of the waveforms of the driving voltage of the pole; and the tenth diagram (a) (b), (c) of the gate-depressed switching current and gate ) Is a waveform diagram of depressor pressure in this case. SW and gate drive power 1228944 Symbol description 1 0 0 · Parent current power supply 1 1 0: Power factor correction AC / DC conversion circuit 120: DC connection capacitor 130: Inverter 140: Inductor 170: The discharge lamp 1 80 : Internal capacitor 2 1 0: Metal oxide semiconductor field effect transistor 2 11: Metal oxide semiconductor field effect transistor 212: High-frequency capacitor 214: Inductor 215: Capacitor 310: Power inverter 320: Resonant matching circuit 330: Gate switching Circuit 340: current sensor 400: pulse transformer 81 1: DC silicon controlled transistor (SCR) α: phase angle C 1, C 2: capacitance Θ: phase angle iinj · current iz: diode current i $ · feedback Current imag · Excitation current cst: Capacitance CT: Current transformer D1-D4 · Schneider diode Dae: Gate fluid Dst: Diode Lm: Excitation inductance Np: Winding Q1, Qz · Transistor Nsl: Winding Ns2: Winding 1: resistance R2: resistance Rgl: gate resistance Rg2: gate resistance VB: DC voltage Vctrl: external voltage source For implementation, please refer to the first figure, which is a circuit block of the electronic ballast system of the preferred embodiment of this case Illustration. As shown in the first figure, the electronic ballast system is 10 1228944
由' —父流包源1 Ο 〇來括/j£ dfl» JU 求徒供包力。然而,一般而言該電子安 疋器或nt供應電路是由一直流電源提供電力。因此, 該包子女疋杰系統需要包含一功率因素校正交流/直流 (PFC AC/DC)轉換電路11〇,該pFC ac/dc轉換電路n〇 二有功率口素k正以及交流/直流轉換功能。在該電子安定 器電路中通常包含-直流連接電容(DC Hnk以_加)12〇 與泫PFC AC/DC轉換電路11〇電連接。 現今所使用的放電燈管其電力來源為一交流電流,因 此在該電子安定器電路需包含一變頻器(inverter)i3〇以及 一串連連接的電感140。該變頻器130將該PFC AC/DC轉 換電路110所轉換輸出的直流電切換輸出之一近似方波電 壓訊輩’纟經由該電€ 140將該近似方波電壓i號轉換成 為一近似弦波訊號。而該電感丨40與該放電燈管170之内 部電容180組成一 LC或是LCC共振匹配電路以減少電 磁雜訊干擾(讀),用以加強波形調整,進而延長放電燈 管的壽命。 在這樣的電路配置中,具有三個最基本的可控制參數 以控制放電燈管之功率:(!)、直流電壓(DC Hnk …V) ( 2 )、占空比(duty rati〇 ) D,( 3 )、切換頻率,。當 定頻及固定占空比控制時且放電燈管之調光控制係自5麸: 3電燈管之電流來決定,因此放電燈管之功率係為該直 流電壓vB的函數。改變直流電壓(Dc nnk v〇h_) ^之 ^小即可達到直流電壓之控制。占空比之控制係改變變6頻 器之切換開關之導通時間,當切換週期固定時。調光控制 ^實現係藉由占空比之控制,當切換開關之導通時間減少 時,則由電源轉換至負載之能量亦會減少。頻率控制係改 變切換頻率之大小,當維持占空比為一定值時(亦即 5〇°/。)。藉由頻率控制實現之調光控制係改變切換頻率異於 共振電路140自然共振頻率,使較少能量耦合至該放電燈 1228944 :雜ΐ述之控制方法可分別合併使用,然而會造成實現的 直Α電壓調光控制一般較少使帛,目$並沒有 =之方法控制功率因素修正級之輸出電壓以 占空比控制係為一較佳之調光控制,然而在 殊情形下’亦即切換開關在占空比很小時,則無 ^ 電壓切換之操作且無法忍受嚴格之MOSFET之體一極俨: 反相^相關問題(reverse•⑽very_related㈣二)體之 省知自激式轉換器在四十五年前已經應用在各 ’且直二轉二”及及強電子安定器中。自激式轉換器其主要優: 電子:定Γ Λ ust)操作的優點,特別是應用在 堪缺 其為—種最為簡單及便宜有效率的電路社 構。然而,如前所述,自激式共振電路之操作頻 = 作時之然頻率,相依於該貞載且極難控制、=^ 簡單電路時。對於習知特定電路元件之組合二 電路結構以及其頻率控制之燈光調節控制是極其複 =該放電燈管的照明效率不可能是最佳化之控制。-故些問題,纟案電力控制方法係利用讀文磁 樂 改變切換頻率使得放電燈管功率更容易調節政 虱體=電燈管之燈光調節控制電路結構十分簡單。。Included by '— father stream package source 1 〇 〇 / j £ dfl »JU Apprenticeship for the package. However, in general, the electronic amplifier or the nt supply circuit is powered by a DC power source. Therefore, the packaged child system needs to include a power factor corrected AC / DC (PFC AC / DC) conversion circuit 11o. The pFC ac / dc conversion circuit n0 has a power factor k positive and AC / DC conversion functions. . The electronic ballast circuit usually includes a DC link capacitor (DC Hnk plus or minus) 12 and is electrically connected to the PFC AC / DC conversion circuit 11. The power source of the discharge lamp used today is an AC current, so the electronic ballast circuit needs to include an inverter i30 and a series connected inductor 140. The inverter 130 converts one of the DC power switching outputs converted by the PFC AC / DC conversion circuit 110 into an approximate square wave voltage signal, and converts the approximate square wave voltage i into an approximate sine wave signal through the electricity 140. . The inductor 40 and the internal capacitor 180 of the discharge lamp 170 form an LC or LCC resonance matching circuit to reduce electromagnetic noise interference (reading), which is used to strengthen the waveform adjustment and extend the life of the discharge lamp. In such a circuit configuration, there are three most basic controllable parameters to control the power of the discharge lamp: (!), DC voltage (DC Hnk… V) (2), duty ratio (duty rati〇) D, (3) Switching frequency. When the fixed frequency and fixed duty cycle are controlled and the dimming control of the discharge lamp is determined from the current of the 5 bulbs: 3 electric lamps, the power of the discharge lamp is a function of the DC voltage vB. The DC voltage can be controlled by changing the DC voltage (Dc nnk v〇h_). The duty cycle is controlled by changing the on-time of the 6-frequency switch. When the switching period is fixed. The dimming control ^ is realized by controlling the duty cycle. When the on-time of the switch is reduced, the energy transferred from the power supply to the load will also be reduced. The frequency control changes the size of the switching frequency when the duty cycle is maintained at a certain value (that is, 50 ° /.). The dimming control implemented by frequency control changes the switching frequency different from the natural resonance frequency of the resonance circuit 140, so that less energy is coupled to the discharge lamp 1228944: the control methods described in the description can be combined and used separately, but it will cause the direct Α Voltage dimming control is generally less effective. There is no way to control the output voltage of the power factor correction stage. The duty cycle control system is a better dimming control. When the duty cycle is very small, there is no ^ voltage switching operation and can not tolerate the strict MOSFET body. 俨: Reverse 相关 related problem (reverse • ⑽very_related㈣ 二) The provincial self-excited converter is in forty-five It has been applied to the "two straight to two" and strong electronic ballasts years ago. The main advantages of self-excited converters are: the advantages of electronic: fixed Γ Λ ust) operation, especially in applications where it is lacking— This is the simplest, cheapest and most efficient circuit architecture. However, as mentioned earlier, the operating frequency of a self-excited resonant circuit = the frequency at which it operates, which depends on the load and is extremely difficult to control. The combination of the circuit structure and the frequency adjustment of the light control of the conventional specific circuit element is extremely complicated = the lighting efficiency of the discharge tube cannot be the optimal control.-For these reasons, the power control method Using reading magnetic music to change the switching frequency makes it easier to adjust the power of the discharge lamp. The structure of the light adjustment control circuit of the electric lamp body is very simple.
作肩考+第二圖、第三圖(a)、(b),自激式轉換器其工 作原理敘述如下:第二圖係本案第一較佳 I MOSFE:駆動之自激式電子式電子安定器之電路示之 一金屬氧化半導體場效電晶體(MOSFETs) 21〇,,丨〗二^ =2:器輸出-方波電壓。高頻電容212以及電或2「4 匕二Ϊ匹配電路以改變輸出電壓訊號之波形,提佴適 田之啟動电壓並穩定穩態時放電燈管之電流。電 ,匕為一阻滯電容(blocking capacitor ) II以隍滯直冷: 壓直接跨壓在電感214±。自激式驅動電路包含; 12 1228944Take the shoulder test + the second and third pictures (a) and (b). The working principle of the self-excited converter is described as follows: The second picture is the first best I MOSFE: automatic self-excited electronic electronics in this case. The circuit of the stabilizer is shown as one of metal oxide semiconductor field effect transistors (MOSFETs) 21 ,,, and ^ = 2: device output-square wave voltage. The high-frequency capacitor 212 and the electric or 2 ″ 4 Ϊ Ϊ matching circuit to change the waveform of the output voltage signal, improve the starting voltage of Shida and stabilize the current of the discharge lamp when the steady state. Electric, 匕 is a blocking capacitor ( blocking capacitor) II with hysteresis and direct cooling: the voltage is directly across the inductor 214 ±. The self-excited driving circuit contains; 12 1228944
該比流器CT具有三個繞組Np, Rg2及背接稽納二極體 )D「D4。共振電感電流經由該 路所提供。該啟動電路包含電阻Ri 以及閘流體Dac。其中VaS|,V,,, ^流态CT被反饋且轉換成互補式電壓以驅動金屬氧化半 $體%效電晶體2 1 0, 2 1 1。初始閘極脈衝訊號係由啟動電 各电阻R丨,R2、電容Cst、二極體 vgsi,Vgs2分別代表開關元件210, 2 11閘極與源極之跨電壓。 第二圖(a)係第二圖之簡化等效電路示意圖。如第三圖 U)所不,戎比流器CT被模式化為一電流控制電流源並聯 一激磁電感Lm。一理想化之變壓器耦合二金屬氧化半導體 場效電晶體之閘極端。請參閱第三圖(b)係第二圖之簡化等 效電路波形不意圖。在任一參考時間,金屬氧化半導體 場效電晶體2 1 0戴止,金屬氧化半導體場效電晶體2丨丨導 通。因此激磁電流imag低於該反饋電流丨s,使得二極體電 流iz為一正值。對於理想之稽納稽納二極體(zener di〇des ) s施加於開關21 〇之閘極電壓為負值,則施加於開關2 η 之閘極電壓為正值,使得開關2丨1維持導通,開關2丨〇維 持載止。由於繞組電流為正值,當反饋電流在共振狀態中 改變其狀態時,如第三圖(b)所示標號220, 221,激磁電流 線性增加。最後,在時間tl,激磁電流imag高於該反饋電 流is,使得二極體電流為一負值,使得二極體電壓改變 極性,導致開關2 1 1裁止,開關2丨〇導通。並開啟下一個 對稱半週期。圖中ip代表比流器CT 一次側線圈電流,l 代表比流器ct二次側線圈電流,其中is=: ip/N N代表比 流器CT之匝數比。 由上所述,可知激磁電流imag與該反饋電流is之相對 大小扮演了決定操作頻率的關鍵因素。假設α為激磁電流 imag與該反饋電流is之一相角,且Θ為變頻器輸出電流與2 13 1228944 應共振電流之一相角, aM./2)-e 弟二圖(b)所示,因此 (1) (2)The current transformer CT has three windings Np, Rg2 and a back-connected diode (D4). The resonant inductor current is provided via this circuit. The starting circuit includes a resistor Ri and a gate fluid Dac. Among them VaS |, V The fluid CT is fed back and converted into a complementary voltage to drive the metal oxide half-efficiency transistor 2 1 0, 2 1 1. The initial gate pulse signal is generated by the starting resistors R 丨, R2. The capacitor Cst, the diodes vgsi, and Vgs2 respectively represent the voltage across the gate and source of the switching elements 210, 2 11. The second diagram (a) is a simplified equivalent circuit diagram of the second diagram. As shown in the third diagram U) No, the Ronby CT is modeled as a current-controlled current source in parallel with a magnetizing inductance Lm. An ideal transformer is coupled to the gate end of a two-metal oxide semiconductor field-effect transistor. See Figure 3 (b) for the first The simplified equivalent circuit waveform of the second figure is not intended. At any reference time, the metal oxide semiconductor field effect transistor 2 1 0 is worn, and the metal oxide semiconductor field effect transistor 2 is turned on. Therefore, the exciting current imag is lower than the feedback current.丨 s, so that the diode current iz is a positive value. Ideal zener diodes s The gate voltage applied to switch 21 〇 is a negative value, and the gate voltage applied to switch 2 η is a positive value, so that switch 2 丨 1 maintains conduction The switch 2 is maintained at a load. Because the winding current is a positive value, when the feedback current changes its state in the resonance state, as shown in the third figure (b), 220, 221, the exciting current increases linearly. Finally, in At time t1, the exciting current imag is higher than the feedback current is, so that the diode current becomes a negative value, which causes the diode voltage to change polarity, which causes the switch 2 1 1 to be disabled and the switch 2 丨 0 to be turned on. The next symmetry is turned on. Half cycle. In the figure, ip represents the current of the primary coil of the current transformer CT, and l represents the current of the secondary coil of the current transformer ct, where is =: ip / NN represents the turns ratio of the current transformer CT. As mentioned above, It can be seen that the relative magnitude of the exciting current imag and the feedback current is a key factor determining the operating frequency. Assume α is a phase angle between the exciting current imag and the feedback current is, and Θ is the inverter output current and 2 13 1228944 should be resonant Phase angle of current, aM./2)-e FIG two (b), and therefore (1) (2)
IpSinG/jvJ rz τIpSinG / jvJ rz τ
一 mag, t〇 = V7Ts / 4L 其中,IP,N,VZ分別為共振 比以及稽納電壓。$藉_ + 的峰值、比流器C丁的匝數 就品質上來$,+ 月對背二極體之跨壓降。 隨之增加。既麸激磁%,激磁電流斜率將會 疋…、激磁電流和稽納雷、、亡θ 期將合縮輛Q + U Ρ W疋互補的,故切換週 功竹θ縮短且切換頻率將會 響因辛且合坆疋切換頻率的主要影 Β ^ I且曰到負载變動而有影燮。 考慮電感公式 3One mag, t〇 = V7Ts / 4L, where IP, N, VZ are the resonance ratio and the acceptance voltage, respectively. The peak value of $ borrow_ + and the number of turns of the current transformer C are up to $, and the monthly pressure drop across the back diode. With it increased. With the excitation percentage of bran, the slope of the exciting current will be…, the exciting current and the zener, and the dead θ period will be complementary Q + U ρ W 疋, so the switching Zhou Gongzhu θ shortens and the switching frequency will respond In addition, the main effect of combining switching frequencies is B ^ I, and there is an effect when the load changes. Consider inductance formula 3
Lm = μΑ^ρ2 / le (3) 有二:改匕,,le分別為鐵心導磁係數,有效戴面以及 有效磁通路後長度。 NP = UeV2Ts Ns / (μΑ0)2 (4 lpsin Θ) )1 3 ⑷ 因此簡化電路的設計步驟是十分直接的。典型設計 f驟係對於給定之匯流排電壓及切換頻率,設計共振元件 ^14及2丨1之大小。因此,共振電流1P及相位θ可設定在額 定放電燈官功率。從鐵心及磁通密度Β〇ρ之選取,比流器之 二次側線圈匝數為:Lm = μΑ ^ ρ2 / le (3) There are two: change the dagger, and le is the magnetic permeability of the core, the effective wearing surface and the length after the effective magnetic path. NP = UeV2Ts Ns / (μΑ0) 2 (4 lpsin Θ)) 1 3 ⑷ Therefore, it is very straightforward to simplify the design steps of the circuit. The typical design f is designed for the given bus voltage and switching frequency, the size of the resonant element ^ 14 and 2 丨 1. Therefore, the resonance current 1P and the phase θ can be set at the rated discharge lamp power. From the selection of the iron core and the magnetic flux density B〇ρ, the number of turns of the secondary coil of the current transformer is:
Ns - VxTs / 2AeBop (5) 其中,一次側線圈匝數可根據方程式(4)計算可得。上 述之分析及設計係根據簡化之模型,更詳盡之分析可參考 Tao et al·之論文 A Self-Oscillating Drive for Single-Stage Charge-Pump Power-Factor-Correction Electronic Ballast with Frequency Modulation”,Industry Applications Conference, 2 000; Conference Record of the IEEE,Volume 5, 2000; pp.3367-3373。 然而,如第四圖,所示根據簡化模型,自激式共振電 1228944 路可視為—系統,該系八一 31 〇係提供一方波電壓訊號3二^固子系統:一功率變頻器 該方波電壓訊號為_ : : ?振巴配電路320係轉換 330轉換由電壓或電流感測nu及—閘極轉換電路 或電流為—適當之 驅° =所偵測得到的反饋電壓 體。這三個子系統形成動變頻器之切換電晶 實質上相依於該負載:=车係由該電路的參數決定,且 為達到頻率控制之烟土 定迴路是必要的。一較佳方’夺^入控制電壓進入該獨立穩 之論文中。如前ς /去:去’係揭露於Tao 頻率因而增加。當注入電流二繞時,切換 這技術已經成功改善了電路效能換=因而降低。 -〇0、線電流譜波值(linecu ent=•㈣因素(― 田备n v harm〇nicS)、電流峰值 因素(lamp erest fact()r)以及放電燈管功率對線電壓變動之 敏感度。唯一缺點是注入比流器之電流偏差。 為克服自激式頻率改變之技術問題討論如下:請參閱 第五圖,係第四圖之簡化等效電路示意圖。如上所稽 納(zener )二極體電流ιζ之極性決定了閘極驅動電璧的極 性。因此,改變稽納二極體電流iz之極性即改變切換頻率。 稽納二極體電流丨z為反饋電流與激磁電流得差值,如下面 公式所示。 {ζ — is - imag = ( ip / N)- Imag (6) 由上面公式可知,適當之反饋電流可以獲得較佳之效 能。如第五圖虛線所示,一可控制電流丨⑷係被注入以調變 在稽納二極體電流^的零交越點。因此,可藉由控制激磁 電流以控制該稽納二極體電流1 z。然而’該切換頻率可調 15 1228944 變之範圍是有限的。改變比流器之跨璧可以有效控制激磁 電流之改變。幸運的是,比流器支線圈電壓係由第二電路 所決定。 因此’根據本案係利用控制稽納二極體電流^以控制 激磁電流。如第六圖所示,一可控制電壓之電壓源取代作 為比流器CT之負載之稽納(zener )二極體。不同於稽納 二極體箝制,比流器CT線圈之跨壓係由一外部電壓源Vc… 所控,,其中脈衝變壓器400係提供二閘極驅動電壓之C隔 離保護。第六圖(b)所示,一可控制電壓之電壓源包含一電 容c,,c2電壓分璧器。第七圖係係本㈣二較佳實絶例之 自激式電子式電子安定器之電路示意圖。 、 離傳Γ激式電路’問極驅動電路與比流器係分 小訊號電晶體Q,,q2用以放大閘 路基極-集極接面電晶體對藉制電… 電壓等於箝制電容電壓加上基極-集 極接面包曰曰㈣壓箝制電容電壓 及兩個放電電阻Rl及R,來 了由外。「-电壓vctr丨 電壓大小加以控制。以第七工切換頻率因此可由控制 定電壓5〜15伏特,,考慮M〇SFET閘極額 ^ ^ f : 11"0 " 功率調光可藉由電壓調變來 &供負載一平滑且連續 得如第四圖所示之榻古々、1。值得注意的電流注入使 簡單獨立之直流電源所:動以及外部控制電壓源可以被- 第七圖所不電路圖之另一 方式以增加燈管的|命美、優點是可提供較佳之啟動 包含兩個步驟一 上’較佳啟動方式一般而言 式之中,係加熱燈管之燈緣式丄—是啟動模式。在預熱模 放電之最低電壓前,以^ ^至一適當之溫度,在達到氣體 動模式之中’係加熱營1陰$之錢射及燈管變黑。在啟 且 乳體敌電狀態。然而此種方式 16 1228944 預熱器來實現。根據本發明,該 之預熱切換頻率。二亥二:—初始控制高電壓以達到預期 以達到足夠之預埶狀::換頻率一般而言-秒之内可 容(Rc)電路.素: 而時間控制可藉由-簡單電阻電 燈管電壓使該燈管發=預熱切換頻率因此可以無須使用高 為使該電路且古Φ & 保護電路心ί管在本案設計中提供-案較佳實施例之;常工作狀況。第八圖係本 當該電路係偵測該共振口路示意圖。 ::Γ旦過電流發生時直二二 過電 源轉換器不會被觸發動作。徑“scR)8丨丨¥通,使電 第九圖、第十圖係根據第 伏特、Lr=丨.56mH、c_5:2七圖毛路圖在直流電壓300 ⑽之鐵心丄單·6:?條件下與應用-工業用TDK 側線圈以及45瓦之;:::之一次側線圈與75 E之二次 以及2N2907A,晶體 U t標準之加222a 雙L η 杜心屯于女疋态實驗結果。 ^ ㈤、第十圖係在全載、70%負載盥60。/自哉 同電壓下切換電流、問極驅動電壓及放tc下不 分別對應控制電璧為llv、W4V - = 159.2¾ 及頻率之關係為—非線性關係,且頻梓加起^電燈管 值時,放電燈管之功率會急速下降。、 過某—特定 综合上述,本案可提供一種簡單電子 其提供-簡單之放電燈管調光控制技 ::’ 或是電源轉換器之中。 心在各式电源供應器 耵甲明寻利靶圍所欲保護者。 17Ns-VxTs / 2AeBop (5) where the number of turns of the primary coil can be calculated according to equation (4). The above analysis and design are based on a simplified model. For a more detailed analysis, please refer to the paper by Tao et al. A Self-Oscillating Drive for Single-Stage Charge-Pump Power-Factor-Correction Electronic Ballast with Frequency Modulation ", Industry Applications Conference , 2 000; Conference Record of the IEEE, Volume 5, 2000; pp.3367-3373. However, as shown in the fourth figure, according to the simplified model, the self-excited resonance circuit 1228944 can be regarded as a system, which is Bayi 31 〇 provides a square wave voltage signal 3 ^ solid subsystem: a power inverter, the square wave voltage signal is _::?? Zhenba with circuit 320 series conversion 330 conversion by voltage or current sensing nu and-gate conversion The circuit or current is-the proper drive ° = the detected feedback voltage body. These three subsystems form the switching transistor of the inverter and are essentially dependent on the load: = The car system is determined by the parameters of the circuit and is It is necessary to achieve the frequency control loop of the soil. A better method is to capture the control voltage and enter the independent stable paper. As before, // Go: Go 'is disclosed at the Tao frequency. As a result, when the injection current is wound, the switching technology has successfully improved the circuit efficiency and thus reduced. -〇0, line current spectral wave value (linecu ent = • ㈣factor (― 田 备 nv harm〇nicS), The current peak factor (lamp erest fact () r) and the sensitivity of the discharge lamp power to line voltage changes. The only disadvantage is the current deviation injected into the current transformer. The technical issues to overcome the self-excited frequency change are discussed below: see The fifth diagram is a simplified equivalent circuit diagram of the fourth diagram. As described above, the polarity of the zener diode current ιζ determines the polarity of the gate drive voltage. Therefore, the zener diode current iz is changed. The polarity changes the switching frequency. The diode current 丨 z is the difference between the feedback current and the exciting current, as shown in the following formula. {Ζ — is-imag = (ip / N)-Imag (6) From the above formula It can be known that a proper feedback current can obtain better performance. As shown by the dotted line in the fifth figure, a controllable current is injected to modulate the zero-crossing point of the diode current ^. Field current Control the audit diode current 1 z. However, 'the switching frequency is adjustable 15 1228944 The range of the change is limited. Changing the current span of the current transformer can effectively control the change of the exciting current. Fortunately, the current transformer branch line The coil voltage is determined by the second circuit. Therefore, according to the present case, the control audit diode current ^ is used to control the exciting current. As shown in the sixth figure, a voltage source with controllable voltage replaces the zener diode as the load of the current transformer CT. Unlike Zener diode clamping, the cross voltage of the CT coil of the current transformer is controlled by an external voltage source Vc ..., of which the pulse transformer 400 series provides C isolation protection for the driving voltage of the two gates. As shown in the sixth figure (b), a voltage source with controllable voltage includes a capacitor c ,, c2 voltage divider. The seventh diagram is a circuit diagram of the self-excited electronic electronic ballast which is the best example in this second example. The off-pass Γ-excited circuit 'question pole drive circuit and current transformer are divided into small signal transistors Q ,, q2 are used to amplify the gate base-collector junction transistor to borrow electricity ... The voltage is equal to the clamping capacitor voltage plus The upper base-collector is connected to the breadth to clamp the capacitor voltage and the two discharge resistors Rl and R from the outside. "-Voltage vctr 丨 The voltage is controlled. The switching frequency can be controlled at a voltage of 5 to 15 volts at the seventh stage. Consider the MoSFET gate limit ^ ^ f: 11 " 0 " Power dimming can be controlled by voltage The modulation comes from & the load is smooth and continuous as shown in Figure 4 and Figure 1. The noteworthy current injection makes simple and independent DC power supply: power and external control voltage source can be-Figure 7 The other way of the circuit diagram is to increase the lamp's life. The beauty, the advantage is that it can provide a better start. There are two steps. One is the "better start mode. In general, it is the lamp edge type of the heating lamp." —Is the start-up mode. Before the minimum voltage of the preheating mode discharge, at ^ ^ to an appropriate temperature, when the gas dynamic mode is reached, it is the heating camp and the lamp is blackened. The state of the enemy's electricity in the milk. However, this method is implemented by the 16 1228944 preheater. According to the present invention, the preheating switching frequency. 22:-Initially control the high voltage to achieve the expected to achieve sufficient preheating :: Change frequency in general-within seconds Capacitor (Rc) circuit. The time control can be achieved by-simple resistance of the lamp voltage to make the lamp = preheat switching frequency, so you do not need to use the circuit to protect the circuit Provided in the design of this case-one of the preferred embodiments of the case; normal operating conditions. The eighth figure is a schematic diagram of the circuit when the circuit detects the resonance port. :: Γ Once the overcurrent occurs, the two-to-two power converter does not It will be triggered. The path "scR) 8 丨 丨 ¥ is turned on, so that the ninth and tenth pictures of the electricity are based on the volt, Lr = .56mH, c_5: 2, and the seven-slot hair diagram is at a core voltage of 300 直流.丄 Single · 6 :? conditions and applications-industrial TDK side coil and 45 watts: ::: one primary side coil with 75 E secondary and 2N2907A, crystal U t standard plus 222a double L η Du Xintun Based on the results of the son-in-law experiment. ^ ㈤, the tenth picture is at full load, 70% load 60. / The switching current under the same voltage, the drive voltage of the interrogator and the corresponding control voltage under the tc are not llv, W4V-= 159.2¾, and the relationship between the frequency is a non-linear relationship, and the frequency is increased ^ Value, the power of the discharge lamp will drop rapidly. According to the above-specification, based on the above, this case can provide a simple electronic which provides-simple dimming control technology of discharge lamp: ’or power converter. Focus on all kinds of power supplies. Bie Jiaming seeks to protect the target. 17
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| CN102892246B (en) | 2011-07-18 | 2016-01-27 | 台达电子企业管理(上海)有限公司 | Discharge lamp system and control method thereof |
| TWI502868B (en) * | 2013-07-01 | 2015-10-01 | Univ Nat Formosa | Self-oscillating and single stage high power factor driver circuit |
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