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TW201332263A - Current balancing device - Google Patents

Current balancing device Download PDF

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Publication number
TW201332263A
TW201332263A TW101101586A TW101101586A TW201332263A TW 201332263 A TW201332263 A TW 201332263A TW 101101586 A TW101101586 A TW 101101586A TW 101101586 A TW101101586 A TW 101101586A TW 201332263 A TW201332263 A TW 201332263A
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Taiwan
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current
differential transformer
output
energy transfer
transformer
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TW101101586A
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Chinese (zh)
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Kuo-In Hwu
Wei-Cheng Tu
Ming-Jie Hong
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Univ Nat Taipei Technology
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Priority to TW101101586A priority Critical patent/TW201332263A/en
Publication of TW201332263A publication Critical patent/TW201332263A/en

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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02BCLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO BUILDINGS, e.g. HOUSING, HOUSE APPLIANCES OR RELATED END-USER APPLICATIONS
    • Y02B70/00Technologies for an efficient end-user side electric power management and consumption
    • Y02B70/10Technologies improving the efficiency by using switched-mode power supplies [SMPS], i.e. efficient power electronics conversion e.g. power factor correction or reduction of losses in power supplies or efficient standby modes

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Abstract

A current balancing device drives at least two sets of LED lamp to illuminate and includes a Zeta-type converter, a differential transformer and two sets of rectifier circuit. The technical characteristics of the present invention is that the equivalent leakage inductance of the differential transformer replaces the output inductance of the Zeta-type converter, and an energy transmission capacitor can demagnetize the differential transformer and recycle energy therefrom so as to avoid power loss and increase the overall efficiency.

Description

電流平衡裝置Current balancing device

本發明是有關於一種電流平衡電路,特別是指一種可回收激磁能量以避免功率損耗並提昇整體效率之電流平衡裝置。The present invention relates to a current balancing circuit, and more particularly to a current balancing device that recovers excitation energy to avoid power loss and improve overall efficiency.

現有LED驅動裝置是採用如圖1的定電壓源驅動,或是如圖2的定電流源驅動,介紹如下。The existing LED driving device is driven by a constant voltage source as shown in Fig. 1, or driven by a constant current source as shown in Fig. 2, as follows.

參閱圖1,一種定電壓的LED驅動裝置9是將LED~LEDn的各陰極端接地,LED~LEDn的各陽極端分別串聯一限流電阻(Ballast Resistor)後並聯於一總輸入端,並於該總輸入端加載一定電壓源Vin,但是當該定電壓源Vin的電壓或LED~LEDn的各順向電壓有變動時,流經LED~LEDn的電流也會隨之變動,因此其缺點是穩流能力差。Referring to Figure 1, LED with fixed-voltage driving device 9 is the LED - each cathode terminal grounded LED n of, LED ~ after each of the male terminal LED n are respectively connected in series a current limiting resistor (Ballast Resistor) in parallel with a total input terminal, and load the constant voltage source V in total to the input terminal, but when the constant voltage source V in voltage or a forward voltage of each LED ~ LED n are changes in the current flowing through the LED ~ LED n will also change Therefore, its shortcoming is that the flow stability is poor.

參閱圖2,一種定電流的LED驅動裝置8包括定電壓源Vin、輸入電容Cin、降壓轉換器、輸出電感Lo及輸出電容Co,最後輸出一恆定電流給一LED燈串,由於LED元件的亮度與電流成正比關係,因此使用多個LED元件彼此串聯,使每一LED元件的電流一致,避免電流不穩的問題。Referring to FIG. 2, a constant current LED driving device 8 includes a constant voltage source V in , an input capacitor C in , a buck converter, an output inductor L o , and an output capacitor C o , and finally outputs a constant current to an LED string. Since the brightness of the LED element is proportional to the current, a plurality of LED elements are connected in series to each other so that the current of each LED element is uniform, thereby avoiding the problem of current instability.

然而,多組並聯LED燈串就需更複雜的驅動電路,以電流平衡式的驅動裝置為例,當負載不平衡時造成驅動裝置的差動變壓器兩端的跨壓不為零,因此現有的作法是加入重置二極體作為去磁元件,亦有在去磁路徑加入去磁電阻或稽納二極體以完成去磁,但是會功率損耗而降低整體效率。However, multiple sets of parallel LED strings require more complicated driving circuits. Taking a current-balanced driving device as an example, when the load is unbalanced, the voltage across the differential transformer of the driving device is not zero, so the existing method is used. The reset diode is added as a demagnetization element, and a demagnetization resistor or a dipole is added to the demagnetization path to complete the demagnetization, but power loss is reduced to reduce the overall efficiency.

因此,本發明之目的,即在提供一種可回收激磁能量以避免功率損耗並提昇整體效率之電流平衡裝置。Accordingly, it is an object of the present invention to provide a current balancing device that recovers excitation energy to avoid power loss and improve overall efficiency.

於是,本發明的電流平衡裝置驅動至少二組發光二極體燈串發亮,該電流平衡裝置包含一差動變壓器及二組整流電路,該差動變壓器包括一輸入端、一變壓器本體及二輸出端,該輸入端接收一直流電源以使該變壓器本體產生激磁並於各該輸出端輸出一驅動電流,該差動變壓器具有一等效漏感;二組整流電路分別耦接該差動變壓器之各該輸出端並驅動各組發光二極體燈串發亮,各該整流電路包括一對於該差動變壓器去磁以對於該差動變壓器去磁的重置二極體,及一對於該驅動電流整流後供給各組發光二極體燈串的整流單元。Therefore, the current balancing device of the present invention drives at least two groups of light emitting diode strings to illuminate, the current balancing device comprises a differential transformer and two sets of rectifier circuits, the differential transformer comprising an input end, a transformer body and two An output end, the input end receives a DC power source to cause the transformer body to generate excitation and output a driving current at each of the output ends, the differential transformer has an equivalent leakage inductance; the two sets of rectifier circuits are respectively coupled to the differential transformer Each of the output terminals drives each group of light emitting diode strings to illuminate, and each of the rectifier circuits includes a reset diode for demagnetizing the differential transformer to demagnetize the differential transformer, and The rectifying unit that supplies the light-emitting diode strings of each group after the driving current is rectified.

本發明的電流平衡裝置的技術特點在於:該電流平衡裝置還包括一在該電流平衡裝置前級的Zeta-type轉換器,其具有一功率開關、一儲能電感、一能量傳遞電容、一二極體元件及一輸出電感,該功率開關、該儲能電感及該能量傳遞電容各具有一第一端及一第二端,該功率開關的第一端接取一電源並控制電流導通/不導通地輸出於其第二端,該儲能電感的第一端與該能量傳遞電容的第一端連接於該功率開關的第二端,該能量傳遞電容的第一端連接於該儲能電感的第一端,該能量傳遞電容的第二端連接於該二極體元件的陰極端,該儲能電感的第二端及該二極體元件的陽極端接地,自該能量傳遞電容及該二極體元件之連接處輸出該直流電源至該差動變壓器之輸入端,藉由該差動變壓器的等效漏感替換原來Zeta-type轉換器之輸出電感,並配合該能量傳遞電容對於該差動變壓器之激磁電感去磁並回收能量。The technical feature of the current balancing device of the present invention is that the current balancing device further includes a Zeta-type converter in front of the current balancing device, which has a power switch, a storage inductor, an energy transfer capacitor, and a second a pole element and an output inductor, the power switch, the energy storage inductor and the energy transfer capacitor each have a first end and a second end, the first end of the power switch is connected to a power source and controls current conduction/non-conduction The first end of the energy storage inductor and the first end of the energy transfer capacitor are connected to the second end of the power switch, and the first end of the energy transfer capacitor is connected to the energy storage inductor. The first end of the energy transfer capacitor is connected to the cathode end of the diode element, the second end of the energy storage inductor and the anode end of the diode element are grounded, and the energy transfer capacitance and the The connection of the diode element outputs the DC power source to the input end of the differential transformer, and replaces the output inductance of the original Zeta-type converter by the equivalent leakage inductance of the differential transformer, and cooperates with the energy transfer capacitor The magnetizing inductance of the differential transformer is demagnetized and recovers energy.

本發明的電流平衡裝置之功效在於:藉由差動變壓器的等效漏感替換Zeta-type轉換器的輸出電感,並利用能量傳遞電容作為去磁元件對於差動變壓器之激磁電感去磁並回收能量,避免功率損耗並提昇整體效率與增加其電流均流準確性。The effect of the current balancing device of the present invention is that the output inductance of the Zeta-type converter is replaced by the equivalent leakage inductance of the differential transformer, and the energy transfer capacitance is used as the demagnetization element to demagnetize and recover the magnetizing inductance of the differential transformer. Energy, avoiding power loss and increasing overall efficiency and increasing its current sharing accuracy.

有關本發明之前述及其他技術內容、特點與功效,在以下配合參考圖式之較佳實施例的詳細說明中,將可清楚的呈現。The foregoing and other objects, features, and advantages of the invention are set forth in the <RTIgt;

在介紹本發明之前,需先說明的是,並非所有類型具有輸出電感的電源轉換器都適用於作為電流平衡裝置的前級電路,說明如下。Before the present invention is described, it should be noted that not all types of power converters having output inductors are suitable for use as a front stage circuit as a current balancing device, as explained below.

參閱圖3,一種Cuk轉換器71是利用電電感器L2當作能量轉移元件,但是Cuk轉換器71之所以無法應用於電流平衡裝置,其主要原因為Cuk轉換器71為負電壓輸出。Referring to Fig. 3, a Cuk converter 71 utilizes an electrical inductor L 2 as an energy transfer element, but the reason why the Cuk converter 71 cannot be applied to a current balancing device is that the Cuk converter 71 is a negative voltage output.

參閱圖4,一種單端初級電感轉換器(Sepic)72是利用電感器L2作為能量轉移元件,但由於Sepic轉換器之電感器L2直接接地,因此,也無法利用變壓器之等效漏感替換此電感器L2Referring to FIG. 4, a single-ended primary inductor converter (Sepic) 72 uses an inductor L2 as an energy transfer element, but since the inductor L 2 of the Sepic converter is directly grounded, it cannot be replaced by the equivalent leakage inductance of the transformer. This inductor L 2 .

由以上結果可知,排除了選用Cuk轉換器71或單端初級電感器72作為電流平衡裝置的前級電路的可能性。From the above results, it is understood that the possibility of using the Cuk converter 71 or the single-ended primary inductor 72 as the pre-stage circuit of the current balancing device is eliminated.

參閱圖5,與圖3及圖4具有類似元件的Zeta轉換器73,具有一功率開關S、一儲能電感L、一能量傳遞電容C、一二極體元件Dp及一輸出電感Lo,由於輸出電感Lo是正電壓輸出,因此,本發明即是利用變壓器5(如圖6)之等效漏感替換其輸出電感Lo,經測試獲得了與圖3及圖4具有類似元件的電源轉換器無法達成的功效。Referring to FIG. 5, a Zeta converter 73 having similar components to FIGS. 3 and 4 has a power switch S, a storage inductor L, an energy transfer capacitor C, a diode component D p and an output inductor L o . Since the output inductor L o is a positive voltage output, the present invention replaces the output inductance L o with the equivalent leakage inductance of the transformer 5 ( FIG. 6 ), and has obtained similar components as those of FIGS. 3 and 4 . The power converter can't achieve the effect.

參閱圖6,本發明之電流平衡裝置100之較佳實施例包含一在前級的Zeta-type轉換器10、一差動變壓器5及二組整流電路601、602,各整流電路601、602分別電性連接各發光二極體燈串LS1、LS2,整流電路601包括重置二極體Df1及整流單元61,整流電路602包括重置二極體Df2及整流單元62;電流平衡裝置100的各元件分別介紹如下。Referring to FIG. 6, a preferred embodiment of the current balancing device 100 of the present invention includes a Zeta-type converter 10 in the front stage, a differential transformer 5, and two sets of rectifier circuits 601 and 602. The rectifier circuits 601 and 602 respectively Electrically connecting each of the LED strings LS 1 and LS 2 , the rectifier circuit 601 includes a reset diode D f1 and a rectifying unit 61 , and the rectifying circuit 602 includes a reset diode D f2 and a rectifying unit 62 ; The components of the device 100 are described below.

Zeta-type轉換器10具有一功率開關S、一儲能電感L、一能量傳遞電容C及一二極體元件D,功率開關S、儲能電感L及能量傳遞電容C各具有一第一端11、21、31及一第二端12、22、32,功率開關S的第一端11接取一電源Vin並控制電流導通/不導通地輸出於其第二端12,該儲能電感L的第一端21與能量傳遞電容C的第一端31連接於功率開關S的第二端12,能量傳遞電容C的第一端31連接於儲能電感L的第一端21,能量傳遞電容C的第二端32連接於二極體元件D的陰極端41,儲能電感L的第二端22及二極體元件的陽極端42接地。The Zeta-type converter 10 has a power switch S, an energy storage inductor L, an energy transfer capacitor C and a diode element D. The power switch S, the energy storage inductor L and the energy transfer capacitor C each have a first end. 11, 21, 31 and a second end 12, 22, 32, the first end 11 of the power switch S is connected to a power source V in and controls the current conduction/non-conduction to be outputted to the second end 12 thereof, the energy storage inductor The first end 21 of the L and the first end 31 of the energy transfer capacitor C are connected to the second end 12 of the power switch S. The first end 31 of the energy transfer capacitor C is connected to the first end 21 of the energy storage inductor L, and the energy transfer The second end 32 of the capacitor C is connected to the cathode end 41 of the diode element D, the second end 22 of the storage inductor L and the anode end 42 of the diode element are grounded.

差動變壓器5包括一輸入端50、一變壓器本體500及二輸出端51、52,變壓器本體500具有一變壓器T及一、二次側繞組N1及N2,輸入端50接收一直流電源以使變壓器本體500產生激磁並於各輸出端51、52輸出一驅動電流Io1、Io2(如圖7),二組整流電路601、602分別耦接差動變壓器5之各輸出端50並驅動各組發光二極體燈串LS1、LS2發亮,重置二極體Df1、Df2對差動變壓器5去磁以重置差動變壓器5,各整流單元61、62對各驅動電流Io1、Io2整流後供給各組發光二極體燈串LS1、LS2,各整流單元61、62包括一二極體Do1、Do2及一電容Co1、Co2,感測電阻Rs可配合回授取樣電路用於偵測電流,由於非本發明重點,不在此贅述。The differential transformer 5 includes an input terminal 50, a transformer body 500 and two output terminals 51, 52. The transformer body 500 has a transformer T and primary and secondary windings N 1 and N 2 , and the input terminal 50 receives the DC power supply. The transformer body 500 is excited and outputs a driving current I o1 , I o2 (see FIG. 7 ) at each of the output terminals 51 , 52 . The two sets of rectifier circuits 601 and 602 are respectively coupled to the respective output ends 50 of the differential transformer 5 and driven. Each group of LED strings LS 1 and LS 2 is illuminated, and the reset diodes D f1 and D f2 demagnetize the differential transformer 5 to reset the differential transformer 5, and each of the rectifying units 61 and 62 is driven by each. The currents I o1 and I o2 are rectified and supplied to each group of LED strings LS 1 and LS 2 , and each of the rectifying units 61 and 62 includes a diode D o1 , D o2 and a capacitor C o1 , C o2 , and senses. The resistor R s can be used in conjunction with the feedback sampling circuit for detecting current, which is not described here because it is not the focus of the present invention.

理想的差動變壓器5不會有漏感,考慮到實際的差動變壓器5會產生漏感,因而,本發明電路設計上就是藉由差動變壓器5的等效漏感替換Zeta-type轉換器10的輸出電感,達到節省元件及提升效能之目的。The ideal differential transformer 5 does not have a leakage inductance. Considering that the actual differential transformer 5 generates a leakage inductance, the circuit of the present invention is designed to replace the Zeta-type converter by the equivalent leakage inductance of the differential transformer 5. 10 output inductors, to save components and improve performance.

參閱圖7,本較佳實施例的Zeta-type轉換器10自能量傳遞電容C及二極體元件D之連接處輸出直流電源vD至差動變壓器5,輸出電感L配合能量傳遞電容C對於差動變壓器5去磁並回收能量;另外,流經功率開關S之電流以iin表示,流經儲能電感L之電流以iL表示及電壓以vL表示,能量傳遞電容C之跨壓以vC表示,流經能量傳輸二極體D之電流以iD表示;本較佳實施例的差動變壓器5中,一、二次側繞組N1及N2之跨壓以v1、v2表示,變壓器T之激磁電感以Lm表示,變壓器T之一、二次側漏感Lr1、Lr2跨壓以vLr1、vLr2表示,流經變壓器T之一、二次側漏感Lr1、Lr2之電流以iLr1、iLr2表示;流經重置二極體Df1及Df2之電流以iDf1、iDf2表示;經各整流單元61、62整流後的電壓以Vo1、Vo2表示。Referring to FIG. 7, the Zeta-type converter 10 of the preferred embodiment outputs a DC power source v D to the differential transformer 5 from the junction of the energy transfer capacitor C and the diode element D, and the output inductor L cooperates with the energy transfer capacitor C. The differential transformer 5 demagnetizes and recovers energy; in addition, the current flowing through the power switch S is represented by i in , the current flowing through the storage inductor L is represented by i L , and the voltage is represented by v L , and the voltage transfer capacitor C is cross-voltage In the case of v C , the current flowing through the energy transfer diode D is represented by i D ; in the differential transformer 5 of the preferred embodiment, the cross-pressure of the primary and secondary windings N 1 and N 2 is v 1 , v 2 indicates that the magnetizing inductance of the transformer T is expressed by L m , and one of the transformers T and the secondary side leakage inductances L r1 and L r2 are represented by v Lr1 and v Lr2 across the transformer, and flow through one of the transformers T and the secondary side leakage. The currents of the senses L r1 and L r2 are represented by i Lr1 , i Lr2 ; the currents flowing through the reset diodes D f1 and D f2 are represented by i Df1 , i Df2 ; the voltages rectified by the respective rectifying units 61 , 62 are V o1 and V o2 are indicated.

為了方便分析,首先進行下列幾點假設:功率開關S與能量傳輸二極體D均視為理想元件,即功率開關S之切換時間、導通電阻和能量傳輸二極體D順向導通壓降與反向恢復時間均忽略不計;儲能電感L與能量傳遞電容C皆不考慮寄生電阻;將每一發光二極體燈串LS1、LS2等效為一理想二極體、膝點電壓及內阻之串聯;主電路架構操作於不連續導通模式下;變壓器T之一、二次側匝數比為1:1且漏感均相等。In order to facilitate the analysis, the following assumptions are made: the power switch S and the energy transfer diode D are both regarded as ideal components, that is, the switching time of the power switch S, the on-resistance and the energy transfer diode D are in turn. The reverse recovery time is negligible; the energy storage inductor L and the energy transfer capacitor C do not consider parasitic resistance; each LED string LS 1 and LS 2 is equivalent to an ideal diode, knee voltage and The series connection of internal resistance; the main circuit architecture operates in discontinuous conduction mode; the turns ratio of one of the transformer T and the secondary side is 1:1 and the leakage inductance is equal.

以下配合圖8至圖13將本較佳實施例的各操作模式介紹如下,主要是依據功率開關與二極體之導通與截止情形及變壓器T與儲能元件之不同狀態,可將本發明之電流平衡裝置100在一週期T s 內分為六個模式[t 0 t t 1]、[t 1 t t 2]、[t 2 t t 3]、[t 3 t t 4]、[t 4 t t 5]、[t 5 t t 0+T s ]來進行電路分析,其元件標號代表意義可參考如圖7的說明內容。The following modes of operation of the preferred embodiment are described below with reference to FIG. 8 to FIG. 13 , which are mainly based on the conduction and cut-off of the power switch and the diode and the different states of the transformer T and the energy storage component, and the present invention can be The current balancing device 100 is divided into six modes in a period T s [ t 0 t t 1 ], [ t 1 t t 2 ], [ t 2 t t 3 ], [ t 3 t t 4 ], [ t 4 t t 5 ], [ t 5 t t 0 + T s ] is used for circuit analysis, and the component numbers represent the meanings as shown in the description of FIG. 7 .

模式一:參閱圖8,功率開關S導通,輸出二極體D o 1D o 2導通,輸入電源V in 對儲能電感L激磁,故i L 直線上升;同時,輸入電源V in 與能量傳遞電容C將能量提供至負載端,因此能量傳遞電容C為放電狀態。因每一顆LED發光元件的製程因素不同,即使在相同的電流驅動下,其每一顆LED發光元件的工作電壓依然會有些許不同,在此假設V o 1<V o 2,變壓器T被啟動,激磁電感等效至一次側,激磁電流由打點流入。由於變壓器T之正向傳遞電流遠大於激磁電流,故流經差動變壓器T之一、二次側電流值極為相近,即跨壓v Lr 1 跨壓v Lr 2,故可假設跨壓v Lr 1=跨壓v Lr 2,由克希荷夫電壓定律可得知下列表示式: Mode 1: Referring to Figure 8, power switch S is turned on, the output diode D o 1 and D o 2 is turned on, the input power supply V in L magnetizing of the inductor, so the rise i L linearly; Meanwhile, the input power supply V in the energy The transfer capacitor C supplies energy to the load terminal, so the energy transfer capacitor C is in a discharged state. Due to the different process factors of each LED light-emitting component, even under the same current drive, the operating voltage of each LED light-emitting component will be slightly different. It is assumed that V o 1 < V o 2 , the transformer T is Startup, the magnetizing inductance is equivalent to the primary side, and the exciting current flows in by the dot. Since the forward current of the transformer T is much larger than the excitation current, the current value flowing through one of the differential transformers T and the secondary side are very similar, that is, the voltage across the voltage v Lr 1 Cross-pressure v Lr 2 , so it can be assumed that the trans-voltage v Lr 1 = the trans-voltage v Lr 2 , the following expression can be known from the Khr-Hoff voltage law:

V in +v C =v Lr 1+v 1+V o 1=v Lr 2-v 2+V o 2 公式1 V in + v C = v Lr 1 + v 1 + V o 1 = v Lr 2 - v 2 + V o 2 Equation 1

由於變壓器T之一、二次側匝數比為1:1且漏感均相等,因此跨壓v 1=跨壓v 2且跨壓v Lr 1=跨壓v Lr 2,故可將公式1簡化後可得由公式2可知變壓器T的一次側繞組N 1之跨壓為(V o 2-V o 1)/2,此電壓為正值,因此激磁電感L m 進行激磁動作且變壓器T之一、二次側之漏感L r 1L r 2為激磁狀態。當功率開關S截止時,此模式結束。Since one of the transformers T and the secondary side have a ratio of turns of 1:1 and the leakage inductance is equal, the crossover voltage v 1 = the voltage across the pressure v 2 and the voltage across the pressure v Lr 1 = the voltage across the pressure v Lr 2 , so Equation 1 can be used. After simplification, it can be seen from Equation 2 that the voltage across the primary winding N 1 of the transformer T is ( V o 2 - V o 1 )/2, and this voltage is positive, so the exciting inductance L m is excited and the transformer T The leakage inductances L r 1 and L r 2 of the primary and secondary sides are in an excited state. This mode ends when the power switch S is turned off.

v 1=v 2=(V o 2-V o1 )/2 公式2 v 1 = v 2 =( V o 2 - V o1 )/2 Equation 2

模式二:參閱圖9,功率開關S截止,二極體D導通,電感L將儲存能量釋放至能量傳遞電容C上,故i L 呈線性下降,此時能量傳遞電容C為充電狀態;同時,變壓器T的一、二次側之漏感L r 1L r 2將上一狀態之激磁能量釋放至負載端,故漏感L r 1L r 2為去磁狀態。根據克希荷夫電壓定律可得知下列表示式: Mode 2: Referring to FIG. 9, the power switch S is turned off, the diode D is turned on, and the inductor L releases the stored energy to the energy transfer capacitor C, so i L decreases linearly, and the energy transfer capacitor C is in a charged state; The leakage inductances L r 1 and L r 2 of the primary and secondary sides of the transformer T release the excitation energy of the previous state to the load terminal, so the leakage inductances L r 1 and L r 2 are demagnetized. According to Kirchhoff's voltage law, the following expressions can be known:

v Lr 1+v 1+V o 1=v Lr 2-v 2+V o 2 公式3 v Lr 1 + v 1 + V o 1 = v Lr 2 - v 2 + V o 2 Equation 3

將公式3簡化後可得:Simplify formula 3 to get:

v 1=v 2=(V o 2-V o1 )/2 公式4 v 1 = v 2 =( V o 2 - V o1 )/2 Equation 4

由於V o 2>V o 1且由公式4可得知變壓器T的一次側繞組N 1之跨壓仍為正值,故L m 仍進行激磁狀態。因此,當變壓器T的一、二次側之漏感L r 1L r 2去磁至零時,此模式結束。Since V o 2 > V o 1 and it can be known from Equation 4 that the voltage across the primary winding N 1 of the transformer T is still positive, L m is still excited. Therefore, when the leakage inductances L r 1 and L r 2 of the primary and secondary sides of the transformer T are demagnetized to zero, this mode ends.

模式三:參閱圖10,功率開關S仍處於截止,二極體D導通,電感L仍持續將能量釋放於能量傳遞電容C上,輸出二極體D o 1D o 2截止且負載端能量由輸出電容C o 1C o 2所提供。因此,變壓器T之一次側無續流路徑且變壓器T之激磁電流必須續流,且其續流方向為打點流入,故激磁電感L m 藉由匝數平方正比之關係將其等效至二次側為L m ',因此激磁電流由二次側打點流入做續流動作。由於二極體D、重置二極體Df1及Df2導通,因此變壓器T兩端跨壓為零,故電感電流i L 往二極體D、重置二極體Df1及Df2做分流,此時,變壓器Ti m '為一定值,故激磁的磁通為一定值。此時,由於變壓器T之一、二次側負向傳遞電流較先前之正向傳遞電流來的小,故不得忽略激磁電流,由於重置二極體電流i Df 2只比i Df 1多了一定值的i m '成份,故i Df 1i Df 2兩者電流斜率相等且i Df 2i Df 1較慢下降至零。由克希荷夫電壓定律可得知下列表示式: Mode 3: Referring to Figure 10, the power switch S is still off, the diode D is turned on, the inductor L continues to release energy on the energy transfer capacitor C, the output diodes D o 1 and D o 2 are cut off and the load end energy Provided by output capacitors C o 1 and C o 2 . Therefore, the primary side of the transformer T has no freewheeling path and the excitation current of the transformer T must be freewheeling, and its freewheeling direction is the inflow of the dot, so the magnetizing inductance L m is equivalent to the second by the relationship of the square of the turns. The side is L m ' , so the excitation current flows from the secondary side to make a freewheeling action. Since the diode D and the reset diodes D f1 and D f2 are turned on, the voltage across the transformer T is zero, so the inductor current i L is made to the diode D , the reset diodes D f1 and D f2 Dividing, at this time, the i m ' of the transformer T is a certain value, so the magnetic flux of the excitation is a certain value. At this time, since the negative current transfer current of one of the transformers T and the secondary side is smaller than the previous forward current, the excitation current should not be ignored, since the reset diode current i Df 2 is only more than i Df 1 A certain value of i m ' component, so i Df 1 and i Df 2 both have equal current slopes and i Df 2 falls slower to zero than i Df 1 . The following expressions can be known from Kirchhoff's voltage law:

v C +v L =v D =0 公式5 v C + v L = v D =0 Equation 5

於此階段中,由於電感L仍持續將能量釋放於能量傳遞電容C上,因此電容電壓v C 將緩緩的上升,且由公式5可得知當v C +v L >0時,二極體D會被截止,此模式結束。In this stage, since the inductor L continues to release energy to the energy transfer capacitor C, the capacitor voltage v C will rise slowly, and Equation 5 shows that when v C + v L >0, the pole Body D will be cut off and this mode ends.

模式四:參閱圖11,功率開關S與二極體D截止,儲能電感L之去磁路徑乃經由重置二極體D f 1D f 2中兩路徑做去磁,能量傳遞電容C為充電狀態,此時負載端能量仍由輸出電容所提供。由克希荷夫電壓定律可得知下列表示式: Mode 4: Referring to FIG. 11, the power switch S and the diode D are cut off, and the demagnetization path of the energy storage inductor L is demagnetized by resetting the two paths of the diodes D f 1 and D f 2 , and the energy transfer capacitor C In the state of charge, the load end energy is still provided by the output capacitor. The following expressions can be known from Kirchhoff's voltage law:

v Lr 1+v 1=v Lr 2-v 2 公式6 v Lr 1 + v 1 = v Lr 2 - v 2 Equation 6

因變壓器T之一、二次側匝數比為1:1且漏感均相等,因此v 1=v 2v Lr 1=v Lr 2,故v 1=v 2=0,變壓器T之兩端跨壓為零,激磁電感電流依然做續流動作,故激磁之磁通為一定值。Since one of the transformers T and the secondary side have a ratio of turns of 1:1 and the leakage inductance is equal, v 1 = v 2 and v Lr 1 = v Lr 2 , so v 1 = v 2 =0, two of the transformers T The end-span voltage is zero, and the magnetizing inductor current still performs the freewheeling action, so the magnetic flux of the exciting magnet is a certain value.

模式五:參閱圖12,功率開關S與二極體D截止,此階段電感L已將能量釋放完畢,重置二極體D f 1截止,負載端能量仍由輸出電容C ο 1C ο 2所提供。此時,由於重置二極體D f 1截止,故變壓器T的一、二次側無傳遞電流,而流經二次側電流為激磁電流,故變壓器TL m '則經由重置二極體D f 2進行去磁,於去磁迴路上,由於激磁電感L m '遠大於電感L與漏感L r 2,因此電容電壓v C 將大部份跨於激磁電感L m '上。此時,激磁電感L m '將橫跨電容電壓v C 將能量釋放於能量傳遞電容C上,能量傳遞電容C為充電狀態,重置二極體D f 2導通,其中,電感電流i L 上仍有電流成份,此仍為激磁電感之去磁電流。當L m '將能量釋放完畢時,重置二極體D f 2截止,則進入下一模式。 Mode 5: Referring to Figure 12, the power switch S and the diode D are turned off. At this stage, the inductor L has released the energy, the reset diode D f 1 is turned off, and the load end energy is still output capacitors C ο 1 and C ο 2 provided. At this time, since the reset diode D f 1 is turned off, no current is transmitted on the primary and secondary sides of the transformer T , and the current flowing through the secondary side is the exciting current, so the L m ' of the transformer T is reset via The polar body D f 2 is demagnetized. On the demagnetization circuit, since the magnetizing inductance L m ' is much larger than the inductance L and the leakage inductance L r 2 , the capacitance voltage v C will mostly straddle the exciting inductance L m '. At this time, the magnetizing inductance L m ' will release energy to the energy transfer capacitor C across the capacitor voltage v C , the energy transfer capacitor C is in a state of charge, and the reset diode D f 2 is turned on, wherein the inductor current i L is There is still a current component, which is still the demagnetizing current of the magnetizing inductance. When L m ' is released, the reset diode D f 2 is turned off, and the next mode is entered.

模式六:參閱圖13,功率開關S、二極體D與重置二極體D f 1截止,負載端能量仍由輸出電容C o 1C o 2所提供;此時變壓器TL m '於上個模式已將能量釋放完畢,故重置二極體D f 2截止;當功率開關S再次導通時此模式結束,下個模式即又回到模式一的狀態。 Model 6: Referring to Figure 13, a power switch S, diode D and a reset diode D f 1 is turned off, the energy load terminal of the output capacitor C o 1 still and C o 2 provided; in this case the transformer T m L ' In the last mode, the energy has been released, so the reset diode D f 2 is turned off; when the power switch S is turned on again, the mode ends, and the next mode returns to the mode one state.

為了驗證實際的情況,實驗時設定兩組相同/不同內阻的發光二極體燈串LS 1LS 2,不同內阻的情況是在發光二極體燈串LS 2增加3Ω的內阻,再經由本發明的電流平衡裝置100的作用後觀察其均流效果。In order to verify the actual situation, two sets of light-emitting diode strings LS 1 and LS 2 with the same/different internal resistance are set in the experiment. The different internal resistance is to increase the internal resistance of the light-emitting diode string LS 2 by 3Ω. Further, the current sharing effect is observed after the action of the current balancing device 100 of the present invention.

如表1-1及表1-2為兩組相同內阻的發光二極體燈串LS 1LS 2,模擬在輸入電壓為24伏且負載為20%(輕載)及100%(滿載)在不增加3Ω的內阻的測試結果,參閱圖14為輸出電壓及輸出電流的相關波形。Table 1-1 and Table 1-2 show two groups of LEDs with the same internal resistance, LS 1 and LS 2 , with an input voltage of 24 volts and a load of 20% (light load) and 100% (full load). In the test results without increasing the internal resistance of 3Ω, refer to Figure 14 for the relevant waveforms of output voltage and output current.

如表2-1及表2-2為輸入電壓24伏且負載為20%(輕載)及100%(滿載)下在其中一組發光二極體燈串LS 2增加3Ω的內阻的測試結果,由表2可知輕載時的電流誤差率為+0.57%,-0.57%,滿載時的電流誤差率為+0.42%,-0.42%,參閱圖15為輸出電壓及輸出電流的相關波形,可驗證本發明確實具有良好的均流效果。Table 2-1 and Table 2-2 show the internal resistance of a group of LED strings LS 2 with an input voltage of 24 volts and a load of 20% (light load) and 100% (full load). As a result, Table 2 shows that the current error rate at light load is +0.57%, -0.57%, and the current error rate at full load is +0.42%, -0.42%. See Figure 15 for the waveforms of output voltage and output current. It can be verified that the present invention does have a good current sharing effect.

除了雙通道的電流平衡裝置100,熟知本領域技術人士當知,只要是雙數的多通道(如:四通道)的電流平衡裝置都適用於本發明的電路架構,當不以雙通道的電流平衡裝置100為限制。In addition to the dual-channel current balancing device 100, it is well known to those skilled in the art that as long as a multi-channel (eg, four-channel) current balancing device is suitable for the circuit architecture of the present invention, when the current is not balanced by two channels Device 100 is a limitation.

綜上所述,本發明的電流平衡裝置100之功效在於:將差動變壓器5的等效漏感設計為Zeta-type轉換器10的輸出電感,並利用能量傳遞電容C作為去磁元件對於差動變壓器5去磁並回收能量,避免功率損耗而提昇整體效率與增加其電流均流準確性,故確實能達成本發明之目的。In summary, the current balancing device 100 of the present invention is effective in that the equivalent leakage inductance of the differential transformer 5 is designed as the output inductance of the Zeta-type converter 10, and the energy transfer capacitor C is used as the demagnetization element for the difference. The dynamic transformer 5 demagnetizes and recovers energy, avoids power loss, improves overall efficiency, and increases its current sharing accuracy, so that the object of the present invention can be achieved.

惟以上所述者,僅為本發明之較佳實施例而已,當不能以此限定本發明實施之範圍,即大凡依本發明申請專利範圍及發明說明內容所作之簡單的等效變化與修飾,皆仍屬本發明專利涵蓋之範圍內。The above is only the preferred embodiment of the present invention, and the scope of the invention is not limited thereto, that is, the simple equivalent changes and modifications made by the scope of the invention and the description of the invention are All remain within the scope of the invention patent.

[習知][知知]

9...定電壓的LED驅動裝置9. . . Constant voltage LED driver

8...定電流的LED驅動裝置8. . . Constant current LED driver

[本創作][This creation]

100...電流平衡裝置100. . . Current balancing device

10...Zeta-type轉換器10. . . Zeta-type converter

11、21、31...第一端11, 21, 31. . . First end

12、22、32...第二端12, 22, 32. . . Second end

41...陰極端41. . . Cathode end

42...陽極端42. . . Anode end

5...差動變壓器5. . . Differential transformer

50...輸入端50. . . Input

500...變壓器本體500. . . Transformer body

51、52...輸出端51, 52. . . Output

61、62...整流單元61, 62. . . Rectifier unit

601、602...整流電路601, 602. . . Rectifier circuit

71...Cuk轉換器71. . . Cuk converter

72...單端初級電感器72. . . Single-ended primary inductor

73...Zeta轉換器73. . . Zeta converter

C...能量傳遞電容C. . . Energy transfer capacitor

Co1、Co2...電容C o1 , C o2 . . . capacitance

D...二極體元件D. . . Diode component

Df1、Df2...重置二極體D f1 , D f2 . . . Reset diode

Do1、Do2...二極體D o1 , D o2 . . . Dipole

L...儲能電感L. . . Energy storage inductor

LS1、LS2...發光二極體燈串LS 1 , LS 2 . . . Light-emitting diode string

N1、N2...一、二次側繞組N 1 , N 2 . . . First and second side winding

Rs...感測電阻R s . . . Sense resistor

S...功率開關S. . . Power switch

T...變壓器T. . . transformer

Vin...電源V in . . . power supply

圖1是說明一種定電壓的LED驅動裝置的電路圖;1 is a circuit diagram illustrating a constant voltage LED driving device;

圖2是說明一種定電流的LED驅動裝置的電路圖;2 is a circuit diagram illustrating a constant current LED driving device;

圖3是說明一種Cuk轉換器的電路圖;Figure 3 is a circuit diagram illustrating a Cuk converter;

圖4是說明一種單端初級電感轉換器的電路圖;4 is a circuit diagram illustrating a single-ended primary inductor converter;

圖5是說明一種Zeta-type轉換器的電路圖;Figure 5 is a circuit diagram illustrating a Zeta-type converter;

圖6是說明本發明之電流平衡裝置之較佳實施例的電路圖;Figure 6 is a circuit diagram showing a preferred embodiment of the current balancing device of the present invention;

圖7是說明本發明之電流平衡裝置之較佳實施例的各元件及其電流及電壓的電路圖;Figure 7 is a circuit diagram showing the components of the preferred embodiment of the current balancing device of the present invention and their current and voltage;

圖8是說明本發明之較佳實施例處於模式一的電路圖;Figure 8 is a circuit diagram showing a preferred embodiment of the present invention in mode one;

圖9是說明本發明之較佳實施例處於模式二的電路圖;Figure 9 is a circuit diagram showing the second embodiment of the preferred embodiment of the present invention;

圖10是說明本發明之較佳實施例處於模式三的電路圖;Figure 10 is a circuit diagram showing the preferred embodiment of the present invention in mode three;

圖11是說明本發明之較佳實施例處於模式四的電路圖;Figure 11 is a circuit diagram showing the fourth embodiment of the preferred embodiment of the present invention;

圖12是說明本發明之較佳實施例處於模式五的電路圖;Figure 12 is a circuit diagram showing the fifth embodiment of the preferred embodiment of the present invention;

圖13是說明本發明之較佳實施例處於模式六的電路圖;Figure 13 is a circuit diagram showing the mode of the preferred embodiment of the present invention;

圖14是兩組相同內阻的發光二極體燈串的輸出電壓及輸出電流的相關波形圖;及Figure 14 is a waveform diagram showing the output voltage and output current of two sets of light-emitting diode strings of the same internal resistance;

圖15是兩組不同內阻的發光二極體燈串的輸出電壓及輸出電流的相關波形圖。Fig. 15 is a waveform diagram showing the output voltage and output current of two sets of light-emitting diode strings of different internal resistances.

100...電流平衡裝置100. . . Current balancing device

10...Zeta-type轉換器10. . . Zeta-type converter

11、21、31...第一端11, 21, 31. . . First end

12、22、32...第二端12, 22, 32. . . Second end

41...陰極端41. . . Cathode end

42...陽極端42. . . Anode end

5...差動變壓器5. . . Differential transformer

50...輸入端50. . . Input

500...變壓器本體500. . . Transformer body

51、52...輸出端51, 52. . . Output

61、62...整流單元61, 62. . . Rectifier unit

601、602...整流電路601, 602. . . Rectifier circuit

C...能量傳遞電容C. . . Energy transfer capacitor

Co1、Co2...電容C o1 , C o2 . . . capacitance

D...二極體元件D. . . Diode component

Df1、Df2...重置二極體D f1 , D f2 . . . Reset diode

Do1、Do2...二極體D o1 , D o2 . . . Dipole

L...儲能電感L. . . Energy storage inductor

LS1、LS2...發光二極體燈串LS 1 , LS 2 . . . Light-emitting diode string

N1、N2...一、二次側繞組N 1 , N 2 . . . First and second side winding

Rs...感測電阻R s . . . Sense resistor

S...功率開關S. . . Power switch

T...變壓器T. . . transformer

Vin...電源V in . . . power supply

Claims (2)

一種電流平衡裝置,驅動至少二組發光二極體燈串發亮,該電流平衡裝置包含一差動變壓器及二組整流電路,該差動變壓器包括一輸入端、一變壓器本體及二輸出端,該輸入端接收一直流電源以使該變壓器本體產生激磁並於各該輸出端輸出一驅動電流,該差動變壓器具有一等效漏感;二組整流電路分別耦接該差動變壓器之各該輸出端並驅動各組發光二極體燈串發亮,各該整流電路包括一對於該差動變壓器去磁以對於該差動變壓器去磁的重置二極體,及一對於該驅動電流整流後供給各組發光二極體燈串的整流單元;其特徵在於:該電流平衡裝置還包括一在該電流平衡裝置前級的Zeta-type轉換器,該Zeta-type轉換器具有一功率開關、一儲能電感、一能量傳遞電容、一二極體元件及一輸出電感,該功率開關、該儲能電感及該能量傳遞電容各具有一第一端及一第二端,該功率開關的第一端接取一電源並控制電流導通/不導通地輸出於其第二端,該儲能電感的第一端與該能量傳遞電容的第一端連接於該功率開關的第二端,該能量傳遞電容的第一端連接於該儲能電感的第一端,該能量傳遞電容的第二端連接於該二極體元件的陰極端,該儲能電感的第二端及該二極體元件的陽極端接地,自該能量傳遞電容及該二極體元件之連接處輸出該直流電源至該差動變壓器之輸入端,藉由該差動變壓器的等效漏感替換該輸出電感,並配合該能量傳遞電容對於該差動變壓器去磁並回收能量。A current balancing device for driving at least two groups of light emitting diode strings to emit light, the current balancing device comprising a differential transformer and two sets of rectifier circuits, the differential transformer comprising an input end, a transformer body and two output ends, The input end receives a DC power source to cause the transformer body to generate excitation and output a driving current at each of the output ends, the differential transformer has an equivalent leakage inductance; the two sets of rectifier circuits are respectively coupled to the differential transformer The output terminal drives each group of light emitting diode strings to illuminate, and each of the rectifier circuits includes a reset diode for demagnetizing the differential transformer to demagnetize the differential transformer, and a rectifying current for the driving current a rectifying unit for supplying each group of light emitting diode strings; wherein the current balancing device further comprises a Zeta-type converter in front of the current balancing device, the Zeta-type converter having a power switch, An energy storage inductor, an energy transfer capacitor, a diode component, and an output inductor, the power switch, the energy storage inductor, and the energy transfer capacitor each have a first end and a The first end of the power switch is connected to a power source and controls the current conduction/non-conduction to be outputted to the second end thereof, and the first end of the energy storage inductor and the first end of the energy transfer capacitor are connected to the power a second end of the switch, the first end of the energy transfer capacitor is connected to the first end of the energy storage inductor, and the second end of the energy transfer capacitor is connected to the cathode end of the diode element, and the energy storage inductor is The two ends and the anode end of the diode element are grounded, and the DC power source is output from the connection of the energy transfer capacitor and the diode element to the input end of the differential transformer, and the equivalent leakage of the differential transformer The sense replaces the output inductor and cooperates with the energy transfer capacitor to demagnetize the differential transformer and recover energy. 依據申請專利範圍第1項所述之電流平衡裝置,其中,該整流單元包括一二極體及一電容。The current balancing device of claim 1, wherein the rectifying unit comprises a diode and a capacitor.
TW101101586A 2012-01-16 2012-01-16 Current balancing device TW201332263A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI869055B (en) * 2023-11-17 2025-01-01 義守大學 Driving circuit for driving electronic element

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI869055B (en) * 2023-11-17 2025-01-01 義守大學 Driving circuit for driving electronic element
US12395086B2 (en) 2023-11-17 2025-08-19 I-Shou University Driving circuit for driving electronic element

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