TWI223135B - Zero-current switching power factor corrector with energy recycling - Google Patents
Zero-current switching power factor corrector with energy recycling Download PDFInfo
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1223135 玖、發明說明: 【發明所屬之技術領域】 =明係關於一種具能量回收之零電流切換功因校正 二二一=:轉態時所產生逆向能量,經儲能、放 電4步驟予以再利用之零電流切換功因校正器。 【先前技術】 ”目前既有的交換式電源轉換器大致包括有—功因校正 益、:受前述功因校正器的升㈣換電路、—連接受控於 功因校正器之順向式輸出電路及一 ^ /、備獨立波寬調變功能 ㈣助電源電路。纟中:該功因校正控制器係用以控制前 述的升壓轉換電路及順向式輸出電路,配合輸出電 定電源輸出。 心 傳統的功因校正器乃藉由其開關的切換來將能量由輸 入端轉換至輸出端,而在理想上的開關切換瞬間其跨於開 關兩側的電壓為零(zvs)或流經開關兩側的電流為零(零電 抓切換卩達到無切換損並降低電磁干擾問||。傳統之 零電流切換轉換器雖能將開關切換損降至最低,但還是存 在能量損耗的問題。 如同一發明人所創作並提出申請獲准的公告第二七九 五一四號「功率調整器之零電流切換電路」新型專利案( 請參閱附件一所示),其創作背景對於傳統功率調整器( 功因杈正為、)提出檢討,如其第四圖所揭示的一種交換式 電源供應器,其優點在於使用元件數量少,生產成本較低 3 ,然而其改善效率約只在8 5 %左右,且因二極體(7 3 )之恢復電流相當大,將提高切換損失,所造成的電磁干 擾(EMI)亦十分可觀,又因其切換時有尖銳的逆向恢復電流 通過動悲元件,容易破壞元件,故其元件的可靠性最差。 又如其第五圖所示,係另種交換式電源供應器,其以 若干串接的蕭基二極體(74) (Sh〇ckley Di〇de)及電阻 、電容取代前述的二極體(73),此一構造仍具有前一 電路利用元件較少之優點,除此之外,因蕭基二極體(7 4 )之逆向恢復電流較小,故其可能引起之電磁干擾亦小 ’但其效率依'然較低,僅約8 7%,又因多個二極體串接 使順向壓降提高,造成切換損失大,其耐壓不容易平衡, 而易造成損壞’故其元件可靠性差,製造成本高。至於其 第六圖所示之零電壓切換式電源供應器,其效率可達9 = %,且因其逆向恢復電流經由零電壓切換電路回收,故電 磁I擾較小,然其零電壓切換電路將產生較大於輸入電流 的尖銳切換動作,故無法將電磁干擾減至最低,除此,此 種零電Μ切換式電源供應器所使用之零件數最乡,且因控 制複雜’ Φ有尖銳電流經過主動元件,故元件之可靠性較 由上述可知,有關交換式電源供應器在效率改善方面 有不;>、研九在讨論此問題,而前述專利案進一步提出 、早决方木’係利用耗能方式消除逆向恢復電流以改善電 :功率因素及提高用電效率,具體作法係於切換電路上設 -由電容、電感、飽和電感及電阻等組成之耗能迴路,藉 【223135 以吸收消耗觸發時產生之逆向恢復電流,#而避 擾及尖銳電流通過動態元件。 、前述專利案儘管大幅提升了功因校正器的工作效率, 並解決了逆向恢復電流所造成的電磁干擾及其對於動態元 :造成的損害’但所謂的逆向恢復電流事實上亦是—種能 量’如能回收予以再利用,將有助於功因校正 : 之進一步提升。 + 【發明内容】 因^本發明的主要目的即在提供一種可進一步將欲消 的月b量回收予以再利用之零電流切換功因校正器,使其 具有能源回收功能,以進—步改善其效率及減少能量損耗 0 。為達成前述目的採取的主要技術手段係令前述功因校 正益於-橋式整流器與一電源輸出端間分設有一濾波電容 、-儲能電感及-能量轉換電路;又有—功因校正控制器 之輸出端透過-金氧半場效電晶體連接於儲能電感與 轉換電路之間;其中: 該能量轉換電路係以一飽和電抗、一功率二極體串接 於前述儲能電感與電源輸出端間,又以一電感、一儲能電 容及數個二極體與前述飽和電抗、功率二極體及金氧半場 效電晶體連接,以構成數個電流迴路,而在不同時間工作 乂便回收觸七日夺產生的逆向恢復電流,再經儲能、放電等 步驟使其运至電源輪出端予以再利用,藉此以有效提升功 因校正器的工作效率。 前述能量轉換電路包括有· 一飽和電抗,係與一功 與電源輸出端間; 率二極體串接於前述儲能電感 此里回收電谷’係透過-電感、-二極體在飽和電 几/、力率一極體之間構成迴路;該二極體並透過又一二極 體連接至電源輸出端; 一消耗電阻,其-端連接前述電感,並透過—電容與 前述飽和電抗、電感構成迴路;該電容 接至電源輸出端; 二、、、端儲旎電容,係連接於電源輸出端與接地之間。 前述功因校正控帝J器係由一脈波寬度調變電路構成。 【實施方式】 一有關本發明一較佳實施例之具體電路構造,請參閱第 一圖:不’其令-功因校正器係於-橋式整流器、(10) ”电源輪出端Vc>Ut間分設有一濾波電容C!、一儲能電感 Li及-能量轉換電路(2㈧;又以一功因校正控:器二 3 〇 )之輪出端透過一金氧半場效電晶體Qi連接於儲能電 感,與能量轉換電路(2 〇 )之間;其中:該功因校:: 制裔(3 〇 )係由一脈波寬度調變電路構成。处曰 換電路(20)係包括: ^轉 一飽和電抗L2,係與一功率二極體Dl串接於前述 電感Li與電源輸出端; 此 1223135 一能量回收電容&,係透過一電 一 飽和電括 ί φ a # 1 一一極肢D2在1223135 发明 Description of the invention: [Technical field to which the invention belongs] = Ming is about a zero-current switching work factor correction with energy recovery 221 =: Reverse energy generated during the transition state, which can be reprocessed in 4 steps of energy storage and discharge Use zero current to switch the power factor corrector. [Previous technology] "The existing switching power converters currently include-power factor correction benefits: the circuit of the power factor correction by the aforementioned power factor corrector,-connection to the forward output controlled by the power factor corrector Circuit and a power supply circuit with independent wave width modulation function. Middle: The power factor correction controller is used to control the aforementioned boost conversion circuit and forward output circuit, and cooperate with the output electric constant power output. The traditional power factor corrector converts the energy from the input to the output by the switch of the switch. At the ideal moment of the switch, the voltage across the switch is zero (zvs) or flows through The current on both sides of the switch is zero (zero-electric-grip switching achieves no switching loss and reduces electromagnetic interference problems. || Although the traditional zero-current switching converter can minimize the switching loss of the switch, it still has the problem of energy loss. As the same inventor created and filed an application for approval of the new patent case No. 2759514 "zero current switching circuit of power regulator" (see Annex I), its creative background for the The power regulator (work factor is correct) is proposed to be reviewed. As shown in its fourth figure, a switching power supply has the advantages of using a small number of components and lower production costs3, but its improvement efficiency is only about 8 5%, and because the recovery current of the diode (7 3) is quite large, it will increase the switching loss, and the electromagnetic interference (EMI) caused by it is also very considerable, and because of the sharp reverse recovery current through the switch during the switching The component is easy to damage, so its component reliability is the worst. As shown in the fifth figure, it is another switching power supply, which uses a number of serially connected Schottky diodes (74) (Shockley Diode) and resistors and capacitors instead of the aforementioned diode (73). This structure still has the advantage of using fewer components in the previous circuit. In addition, due to the reverse of the Schottky diode (7 4) The recovery current is small, so the electromagnetic interference it may cause is also small, but its efficiency is still low, only about 8 7%, and the forward voltage drop is increased due to the connection of multiple diodes, which causes a large switching loss. , Its pressure resistance is not easy to balance, but easy to cause damage. The components have poor reliability and high manufacturing costs. As for the zero-voltage switching power supply shown in the sixth figure, its efficiency can reach 9 =%, and because its reverse recovery current is recovered through the zero-voltage switching circuit, the electromagnetic interference is relatively low. It is small, but its zero voltage switching circuit will produce a sharp switching action larger than the input current, so it cannot reduce electromagnetic interference to a minimum. In addition, the number of parts used in this zero power M switching power supply is the most rural, and Because the control is complicated, there is a sharp current flowing through the active element, so the reliability of the element is better than the above. There is no improvement in the efficiency of the switching power supply; > Yanjiu is discussing this issue, and the aforementioned patent case further It is proposed that the early determination of Fangmu 'is to use energy consumption to eliminate reverse recovery current to improve electricity: power factor and improve electricity efficiency. The specific method is to set the switching circuit-the consumption of capacitors, inductors, saturated inductors and resistors. The energy circuit uses [223135] to absorb the reverse recovery current generated when the consumption is triggered, and # avoids interference and sharp current through the dynamic element. Although the aforementioned patent case has greatly improved the work efficiency of the power factor corrector, and solved the electromagnetic interference caused by the reverse recovery current and its damage to the dynamic element: 'the so-called reverse recovery current is actually a kind of energy 'If recycled and reused, it will help power factor correction: further improve. + [Content of the invention] Because the main purpose of the present invention is to provide a zero-current switching power factor corrector that can further recover the monthly amount of b to be consumed, so that it has an energy recovery function to further improve Its efficiency and reduced energy loss are 0%. The main technical means adopted to achieve the foregoing purpose is to make the aforementioned power factor correction benefit-a bridge capacitor and a power output terminal are provided with a filter capacitor, an energy storage inductor, and an energy conversion circuit; and there is a power factor correction control The output end of the device is connected between the energy storage inductor and the conversion circuit through a metal-oxide half field effect transistor; wherein: the energy conversion circuit is connected in series with a saturated reactance and a power diode to the aforementioned energy storage inductor and power output Between the terminals, an inductor, an energy storage capacitor, and several diodes are connected to the aforementioned saturated reactance, power diode, and metal-oxide half field effect transistor to form several current loops, and it is convenient to work at different times. Recycling the reverse recovery current generated by the seventh-day capture, and then transporting it to the output of the power wheel for reuse through steps such as energy storage and discharge, thereby effectively improving the work efficiency of the power factor corrector. The aforementioned energy conversion circuit includes a saturated reactance between the first power and the power output terminal; a rate diode is connected in series with the energy storage inductor, and the recovery valley is transmitted through the inductor and the diode in the saturated capacitor. A circuit is formed between the first and second poles of the power rate; the second pole is connected to the power output terminal through another second pole; a consumption resistor whose-terminal is connected to the aforementioned inductor, and through the capacitor and the aforementioned saturated reactance, The inductor forms a loop; the capacitor is connected to the power output terminal; the storage capacitors at the terminals 2, and are connected between the power output terminal and ground. The aforementioned power factor correction control J device is composed of a pulse width modulation circuit. [Embodiment] For a specific circuit structure of a preferred embodiment of the present invention, please refer to the first figure: "It's not made-the power factor corrector is connected to a-bridge rectifier, (10)" power wheel output Vc > Ut is provided with a filter capacitor C !, an energy storage inductor Li, and an energy conversion circuit (2㈧; and a power factor correction control device: device 2 30) is connected through a gold-oxygen half field effect transistor Qi. Between the energy storage inductor and the energy conversion circuit (20); of which: the power factor school :: The system (30) is composed of a pulse width modulation circuit. The circuit for switching (20) is Including: ^ turn a saturated reactance L2, which is connected in series with a power diode Dl between the aforementioned inductor Li and the power output; the 1223135 energy recovery capacitor & One pole limb D2 in
他不电抗L2與功率二極體D 並禮過又… 體D)之間構成迴路;該二極體D2 :,° —極體D3連接至電源輸出端; 々r t二、 八鈿連接刖述電感L3,並透過一電 谷C3與前述餘和電抗l 電感L3構成迴路,·該電容C3又 !由一 一極體1)4連接至電源輸出端; 一終端儲能電容G,係連接於雷%认,He does not form a loop between the reactance L2 and the power diode D, and the body D); the diode D2 :, °-the pole body D3 is connected to the power output terminal; The inductor L3 forms a loop with the aforementioned Yuhe reactance L3 through an electric valley C3. The capacitor C3 is again connected to the power output terminal by a pole body 1) 4; a terminal energy storage capacitor G is connected to Ray% recognized,
你逑接於電源輪出端與接地 之間。 /、牧L 又如第二圖所示,為本發明工作電壓電流在不同時序 下,波形。其具體電路工作原理將配合第三圖加以說明, 在第三圖中將全部時序由Τ0〜Τ6分成七段來逐一說明。第 四圖為飽和電A L2在不同時序下之理論磁滞曲線,藉由飽 和電抗L2在不同時序的特性來達到零電流切換⑽)及能 源回收的目的。首先’請參閱第三圖所示各時序下的電路 特性: TO : TO是接續Tfi &办 ,^ ^ 只ib而來,由於此動作已處於穩定狀態 ,所以此時電容C3維持原來的放電狀態,且飽和感抗L2進 入飽和狀態呈現短路的特性,金氧半場效電晶豸Q1尚未開 啟,所以輸入能量藉由橋式整流器(i 〇 )之電流^經由 儲能電感Li、飽和感抗Lz、二極體Di對輸出提供所需之能 量。而在T6時’流經電容&的電流㈣因為飽和感抗^ 的飽和而消失H c3消耗電流l2經由飽和感抗L2、電感 L3持續將能量消耗在電阻Ri上,為下-次充電做準備。心 T1 :在此狀態下,金氡半場效電晶體Qi正準備要開啟 1223135 ,在此瞬間因為電流l2仍維持原方向流動,且飽和感抗L2 處於放電狀態’所以電》l2、l4與電流“之電流方向相抵 4,金氧半場效電晶體Ql達到零電流切換工作的目的,用 以減少切換損。在此時飽和感抗L2產生電流h經二極體仏 流至輸出端,所以飽和咸叔T y A才几L2將由飽和狀態趨向主動狀態 。而電容C3仍保持原來放電狀態。 T2:在此狀態下,金氧半場效電晶體Qi已開啟,此時 飽和感抗L2已放電完畢並進入主動區呈現高阻抗狀態,而 二極體D,正處於逆向恢復狀態所以會有電流h、i6等二個 $向電流產生,且大部分逆向流經h電流路徑到地,僅微 里電流經過Is電流路徑。而流經電感u、電阻I、電容〇 :到地的電流會將二極體仏逆向能量健存於電感W,以 為能量回收做準備。 T3:在此狀態下,二極體Dl的逆向能量已釋放完畢, 所以此時電感l3極性會反轉過來而產生卜和18兩路電流 路為電流I 7 ’其流經二極體對電容C2充電,而將二 極體Di逆向能量健存於電容C2上達到能量回收的目的;另 :路為電流I8,其;^經電感L3、電阻Ri、電容㈣飽和感 U充電,將飽和感机L2從主動區再推至飽和區而呈現低 阻抗狀態。如第四圖之T3箭頭所示,是從第三象限推向 第一象限。 _ T4 ·在此時電感L3已將能量完全釋放給電容c2,而能 量將轉換成電壓形式保存於電容C2等待再利用。而電容C3 保持放電以產生電流以持續將飽和感抗L2推向飽和狀 1223135 丁5 ··在此狀態下,金氧半場效電晶體Qi正準備要關閉 斤以儲旎電感Li開始釋放其保存的能量。因為電容&本 身π有負電壓差使得二極體h兩端呈逆向電壓而不會導通 =二極體D3呈順向電壓導通,故電流IiQ由儲能電感^流 、二已飽和的飽和感抗U、電容&、二極體d3到電壓輸出端 V〇ut p思之將電容ο上之能量回收至輸出端。此動作達成再 利用電谷C2回收能篁的目的。此時電容Cs仍維持放電,其You are connected between the output of the power wheel and the ground. /, Mu L As shown in the second figure, it is the waveform of the working voltage and current of the present invention at different timings. The specific circuit working principle will be described in conjunction with the third figure, in which all timings are divided into seven segments from TO to T6 to explain one by one. The fourth graph is the theoretical hysteresis curve of the saturated electric current A L2 at different timings. The characteristics of the saturated reactance L2 at different timings are used to achieve zero current switching ⑽) and energy recovery. First, please refer to the circuit characteristics at each timing shown in the third figure: TO: TO is connected to Tfi & ^ ^ only from ib, because this action is already in a stable state, the capacitor C3 at this time maintains the original discharge State, and the saturation inductance L2 enters the saturation state and exhibits a short-circuit characteristic. The metal-oxide half-field effect transistor Q1 has not been turned on, so the input energy is passed through the current of the bridge rectifier (i 〇) ^ via the energy storage inductor Li and the saturation inductance Lz, diode Di provide the required energy to the output. At T6, the current flowing through the capacitor & disappears due to the saturation of the saturation inductance ^ H c3 The consumption current l2 continuously consumes energy on the resistor Ri via the saturation inductance L2 and the inductance L3, which is used for the next charge ready. Heart T1: In this state, Jin Qi's half-field effect transistor Qi is preparing to turn on 1223135. At this moment, because the current l2 still flows in the original direction, and the saturation inductance L2 is in the discharging state, so the electricity is l2, l4 and the current. "The current direction is offset by 4. The metal-oxide half-field effect transistor Ql achieves the purpose of zero-current switching operation to reduce the switching loss. At this time, the current h generated by the saturation inductance L2 flows through the diode to the output terminal, so it is saturated. Uncle Xian T y A L2 will go from saturation to active state. Capacitor C3 will still maintain the original discharge state. T2: In this state, the gold-oxygen half field effect transistor Qi has been turned on, and the saturation inductance L2 has been discharged at this time. It enters the active area and presents a high-impedance state, while diode D is in a reverse recovery state, so two $ -direction currents, such as current h and i6, are generated, and most of them flow through the current path of h to ground in the reverse direction, only a few miles The current passes through the Is current path. The current flowing through the inductor u, the resistor I, and the capacitor 0: the current to the ground will store the reverse energy of the diode 仏 in the inductor W in preparation for energy recovery. T3: In this state, two Polar body D1 reverse The quantity has been released, so at this time, the polarity of the inductor l3 will be reversed to generate two currents I and 18. The current I 7 'flows through the diode to charge the capacitor C2, and the diode Di is stored in reverse energy. The capacitor C2 achieves the purpose of energy recovery; the other is the current I8, which is charged by the inductor L3, the resistor Ri, and the capacitor ㈣ saturation sense U, and the saturation sensor L2 is pushed from the active area to the saturation area to show a low Impedance state. As shown by the arrow T3 in the fourth figure, it is pushed from the third quadrant to the first quadrant. _ T4 · At this time, the inductor L3 has completely released the energy to the capacitor c2, and the energy will be converted into a voltage and stored in Capacitor C2 is waiting to be reused. Capacitor C3 keeps discharging to generate current to continuously push the saturation inductance L2 to saturation. 1223135 Ding 5 ·· In this state, the metal-oxide half-field effect transistor Qi is preparing to shut down the jack to store 旎The inductor Li begins to release its stored energy. Because the capacitor & itself has a negative voltage difference, the reverse voltage across the diode h will not be conducted = the diode D3 conducts forward voltage, so the current IiQ is stored by energy Inductance current, two saturated saturation inductance U The capacitor & diode d3 to the voltage output terminal Vout will recover the energy from the capacitor ο to the output terminal. This action achieves the purpose of reusing energy valley C2 to recover energy. At this time, the capacitor Cs still maintains discharge. ,its
放電路梭上的電流Is持續將飽和感抗b推向飽和狀態,但 此時能量已非常微小。 T6 ·在此狀態下,電容C2能量已完全釋放,所以原本 帶有的電壓差已歸為零,所以此時二極體D3不導通,而二 極體/因達順向偏壓而導通,故電流h。將經由飽和感抗 L2、二極體Di到V〇ut。同時雷交h夬、日丨曰> 』于mu左測昇高於電壓輸出端 v〇ut,則電流Is因二極體D順向 、 贤同偈經而形成。電流19經儲 能電感Li、電容C3、二極體d4 5雷、、眉认, U4至寬/原輪出端且對電容The current Is on the shuttle continues to push the saturation inductance b to a saturated state, but at this time the energy is very small. T6 · In this state, the energy of the capacitor C2 has been completely released, so the voltage difference originally brought to it has returned to zero, so the diode D3 is not conducting at this time, and the diode / conducting is due to the forward bias, So the current h. Will pass the saturation sensor L2, diodes Di to Vout. At the same time, the lightning current h 夬, 丨, 曰, &, &, 于, and mu are measured at the left of the mu and rise to the voltage output terminal v0ut, then the current Is is formed by the diode D in the forward direction and the same path. The current 19 passes through the energy storage inductor Li, capacitor C3, diode d4, 5 thunder, and eyebrows, U4 to wide / outside of the original wheel and the capacitor
C3充電。最後回到TO時序反覆動作。 藉由上述說明可瞭解本發明功因1 赞a力LM又正器的電路構造與 工作原理,至於一具能量回收之焚雷、、4 叹< 茶私流功因校正器較佳的 具體規格可如以下所列,而主要开杜 王要70件額定值選取方法程序 將如下所示: 輸入輸出電壓電流規tC3 charges. Finally, it returns to the TO sequence repeatedly. With the above description, the circuit structure and working principle of the power factor of the present invention can be understood. As for an energy recovery thunderbolt, 4 sigh < tea private flow power factor corrector is better specific The specifications can be listed as follows, and the main Kaidu King needs 70 pieces of ratings. The selection procedure will be as follows: Input and output voltage and current gauge t
輸入電壓vin 90V/60HZInput voltage vin 90V / 60HZ
輸出電壓V〇ut 400V 9 1223135 最大輸出功率Pout 1 000W 工作頻率fs 100kHz 盤和電抗: 由工作波形中看到飽和感抗Lz需符合以下條件: 1 ·為了達到零電流切換的目的飽和感抗b漏感的能量 釋放時間I大於電晶冑Ql的爬昇時間n,波形如第五圖二 示其上2 0 n s時間即為其零電流切換時間; 2·在Τ2中看到飽和感抗u必須容納二極體Di的逆向 恢復電荷Qrr而不產生飽和;見象。㈣元件廠商提供之規 格表已知金氧半場效電晶體Q丨的爬昇時間約2〇ns,二極體 ⑴的逆向恢復電荷為45A/n電容C (L3=1〇〇uH ; T=1〇〇(>c ) 二以經由峰值電流Ip公式⑴與伏秒平衡公式(2)可 求得 Ιρ=16· 76A,飽和感抗 l2 = 〇· 48uH。 (1) L2 - ^Output voltage V〇ut 400V 9 1223135 Maximum output power Pout 1 000W Working frequency fs 100kHz Disk and reactance: From the working waveform, the saturation inductance Lz must meet the following conditions: 1 · To achieve the purpose of zero current switching, the saturation inductance b The energy release time I of the leakage inductance is greater than the climb time n of the transistor Q1, and the waveform is shown in Figure 5. The 20 ns time above is the zero-current switching time; 2. You must see the saturation inductance u in T2 The reverse of charge Di, which holds the diode Di, does not produce saturation; see phenomenon. The specification table provided by the component manufacturer knows that the climb time of the metal-oxide half-field-effect transistor Q 丨 is about 20ns, and the reverse recovery charge of the diode ⑴ is 45A / n capacitor C (L3 = 1OOuH; T = 1 〇〇 (&c; c) Second, the peak current Ip formula ⑴ and the volt-second balance formula (2) can be obtained ρ = 16.76A, saturation inductance 12 = 〇. 48uH. (1) L2-^
在此需再驗證飽和感抗L2是否飽和,公式⑺為I 電流斜率,代人得到值4A/US再將此結果代人(4)移項求3 得時間為15〇nS,戶斤以求得伏秒乘積為麵xi5〇ns = 6〇n伏 秒。最後代入磁通變量公式(5)求得勝5 97κ高斯因 飽和感抗L2規格表如=51(高斯,a/?/OD〆 μ 人 ^ △力<2如所以Qrr不會使產 生飽和感抗L2產生飽和現象。 (3) (4) (5) dL =尸 dt JL3 M(S),2 M = —Here it is necessary to verify whether the saturation inductance L2 is saturated. The formula ⑺ is the slope of the I current. Substitute the value to 4A / US. Then substitute this result for (4) and find 3. The time is 15nS. The volt-second product is the plane xi50ns = 60n volt-seconds. Finally, substitute the magnetic flux variable formula (5) to get the victory. 5 97 κ Gaussian L2 specification table for saturation sensibility is = 51 (Gauss, a /? / OD〆μ person ^ △ force < 2 if Qrr does not cause saturation Anti-L2 produces saturation. (3) (4) (5) dL = corpse dt JL3 M (S), 2 M = —
NxAexlO 10 1223135 能量回收用雷夂C2 : 由於電容C2跨壓Vc2必須低於 ^ m /¾ 輸出電壓避免二極體D!誤動作,所以Vu應低於6〇〇v — 400V=200V,在此選用跨壓為120V計算使用。而由於能量 回收時La的能量會完全釋放到電容ο上,所以經由公式( 6)移項求得電容C2 = 2500pF。NxAexlO 10 1223135 Thunderbolt C2 for energy recovery: Because the voltage Cc2 of the capacitor C2 must be lower than ^ m / ¾ to prevent the diode D! From malfunctioning, Vu should be lower than 600v — 400V = 200V, select here The calculation of the span voltage is 120V. Since La's energy is completely released to the capacitor ο during energy recovery, the capacitance C2 = 2500pF is obtained by shifting the term of formula (6).
Ju =~-^3 x/l32 =~C2 xF〇22 2 2 (6) 提升飽和電抗用電容G: 由於電容C2能量回收後電容C2上瞬間最大能量會等於 飽和感抗L2上飽和狀態能量,第五圖上T6時間為此時電 流波形,所以經由公式(7)可求出I飽和感抗u上最大 漏電電流ILK為8· 7A,在此假設〜3工作電壓為9V代入公 式(8)可求出電流建立時間T6為〇.43us,再將此值代 入公式(9)求得電容c3的值為〇· 19uF。 /lk = [2xJC2 (7) (8) (9) V u T* _ (’P — ) x 上2 %--Vc,~~ C3,且」仏一’LK)Xr6 VC3 2 VC3 由於電阻R丨是用來消耗電容C3將飽和感抗L2推向飽 :區用之電阻,所以必須能夠承受電容匕所流經消耗之能 量。且也要估算其可承受瓦特數,所以經由式(ι〇)求出 電阻值為51Q,由式(η)可估管 田八〈i i ^ j估异其取大消耗瓦特數p 阻 Ri 為 0· 78W。 η _ 厂C3 ^ Tperiod ^ ^C3 Λΐ'7α=2(/;^〇χ7; (10)Ju = ~-^ 3 x / l32 = ~ C2 xF〇22 2 2 (6) Capacitor G for increasing the saturation reactance: Since the energy of capacitor C2 is recovered, the maximum instantaneous energy on capacitor C2 will be equal to the saturation state energy on saturation inductance L2, The T6 time on the fifth figure is the current waveform at this time, so the maximum leakage current ILK on the saturation saturation reactance u can be calculated by formula (7) as 8 · 7A. Here we assume that ~ 3 working voltage is 9V and substituted into formula (8) It can be found that the current settling time T6 is 0.43us, and then this value is substituted into the formula (9) to obtain the value of the capacitance c3 of 19uF. / lk = [2xJC2 (7) (8) (9) V u T * _ ('P —) x 2%-Vc, ~~ C3, and "仏 一' LK) Xr6 VC3 2 VC3 due to resistance R丨 is used to dissipate capacitor C3 to push the saturation inductance L2 towards the saturation: resistance, so it must be able to withstand the energy consumed by the capacitor. And it is necessary to estimate the wattage that it can withstand, so the resistance value is 51Q through formula (ι〇). According to formula (η), Guantian eight <ii ^ j estimates that it takes a large consumption wattage p resistance Ri 0 · 78W. η _ Factory C3 ^ Tperiod ^ ^ C3 Λΐ'7α = 2 (/; ^ 〇χ7; (10)
Pr! =^C3(mis) 為了驗證所提出具能量回收改 = 的交換式電源供應器,盆電功因校正器 於在電路貝作時元件的選擇會對整由 影響,有別於以往實驗只單彳率產生-定的 本發明之能源回收電路主要是=^件做效率比較’由於 和此里,所以在本發明將各 攻门免 二極體ff卷栌4^ 對一種㊆用之不同材料係數 ㈣對整體效率的影響來 響,附件二為此實驗之主要電=2的差異所照成的影 同功率二極體規格表。 〜用於比季父的三種不 又在附件三的表列資料中 本發明後之能量損失差異,在附切換方式與加入 量回收之零電流切換電路 ^ 7顯看出加入具能 果選用材料係數較差之功率 旱、力“的效果’如 效果會更明顯。 丨-極體’此電路對效率提昇的 第六圖為輸入電壓盥雷 功率因數幾乎為UU9、);在 切換波形,在此量測到切換電壓;=軸的零電流 已大* 6A沾丨、沒 ^電机父越時間幾乎為零, 下各主要:切換損失。第八至十-圖為單-週期 ,:且二明:換電昼電流波形用來與理論波形相互比較 已八肢5且明本發明電路的可 下之效率曲線圖,在此可明领看出J十二圖為不同負載 對整體效率的差異愈加入本;2輸出功率二極體的選擇 入本發明電路所能提升之效率差別 12 . 叩至p< 令皂流切換功 因校正器可對傳統功因校正器效率達到改善的效果。立中 電路對金氧半場效電晶體產生幾乎無能量指耗 的效果,功因;^ t l _ 杈正益對其功率因數產生幾乎為1的效果, 2統之功因校正器輪出二極體逆向飽和能量的問題皆可 =本發:提出之電路予以改善解決。且經由此具能量回 之零電刀換功因校正器的電路實驗中發 可減少10多瓦的招生^ 此电路 甚至比材料係數最好的功率二極 體可以卽省更多能量,由此 工你4处、 此j °且明本發明具有相當良好的 乍效月b。進而本發明已具備 ^ 八侑頜者的進步性,並符合發明 專利要件,茇依法提起申請。 【圖式簡單說明】 (一)圖式部分 第一圖 第二圖 第三圖 第四圖 曲線圖。 係本發明之電路圖。 係本發明在不同時序 係本發明在不同時序 係本發明飽和電抗在 下之工作波形圖。 下的電路特性示意圖。 不同時序下之理論磁滯 第五圖 形圖 π π卜的 第六圖 第七圖 係本發明輸入電壓電流波形 係本發明金氧半場效電晶體 圖。 之零電壓切換波 13 1223135 形圖。 第八圖·係本發明飽和電抗之電壓電流波形圖。 第九圖:係本發明金氧半場效電晶體Vds對電感^、 電容C3之電流波形圖。 第十圖:係本發明金氧半場效電晶體Vds對功率二極 體D!、二極體D4之電流波形圖。 第十一圖:係本發明金氧半場效電晶體Vds對功率二 極體D!、電容C2之電流波形圖。 第十二圖:係本發明之整體效率曲線比較圖。 器電圖··係本發明-可行實施例之交換式電源供應 公告第二七九五一四號專利公報影本。 係本發明之主要電路元件規袼表。 傳統切換方式與零電流切 極體切換方式之實料換方式與使用蕭特 、之只測整體效率比較表。 (一)元件代表符號 (3 0 )=整(2 〇 )能量轉換電路 (d U )功因校正控制器 附件一 附件 附件 基 14Pr! = ^ C3 (mis) In order to verify the proposed switching power supply with energy recovery, the power factor correction of the basin power factor corrector will affect the reasoning during circuit operation, which is different from previous experiments. The energy recovery circuit of the present invention which only generates and sets a single rate is mainly used to compare the efficiency of the parts. 'Because of this, the present invention will be used to prevent each diode from being used. The influence of different material coefficients 整体 on the overall efficiency is greatly affected. Attachment II shows the same power diode specification table as the difference between the main electricity = 2 of this experiment. ~ The difference in energy loss after the invention in the three listed materials in Appendix III is not used in the comparison with Ji Father. The zero-current switching circuit with the switching method and the recovery of the added amount ^ 7 shows that the selected material can be added. The "effect" of power and force with poor coefficients will be more pronounced as the effect. 丨 -Polar body The sixth picture of the efficiency improvement of this circuit is that the input voltage and lightning power factor are almost UU9,); when switching waveforms, here The switching voltage was measured; = the zero current of the shaft is already large * 6A is not high, and the motor's time is almost zero. The following main: switching losses. The eighth to tenth-the picture is a single-cycle, and two Ming: The day-to-day electric current waveform is used to compare with the theoretical waveform. It is clear that the efficiency curve of the circuit of the present invention can be lowered. It can be clearly seen that the figure 12 is the difference between the overall efficiency of different loads. Add more to this; 2 the choice of the output power diode into the efficiency difference that the circuit of the present invention can improve 12. 12 to p < make soap flow switching power factor corrector can achieve the effect of improving the efficiency of the traditional power factor corrector. Metal Oxide Half Field Effect Transistor Produces almost no energy consumption effect, work factor; ^ tl _ _ Zheng Yi has an effect of almost 1 on its power factor, the power factor corrector of the 2 systems can reverse the problem of reverse saturation energy of the diode. Development: The proposed circuit is improved and solved. And through this circuit experiment with the energy returning zero electric knife power factor correction device, the enrollment can reduce more than 10 watts of enrollment ^ This circuit is even a power diode with the best material coefficient You can save more energy, so you can work in four places, and this invention has a very good first-better month b. Furthermore, the invention has the progress of ^ eight jaws, and meets the requirements of the invention patent,申请 File the application according to the law. [Simplified description of the drawings] (A) The first part of the second part of the drawing, the third picture, the fourth picture, and the fourth diagram. It is the circuit diagram of the present invention. The present invention is at different timings. It is the working waveform diagram of the saturated reactance of the present invention. The schematic diagram of the circuit characteristics below. Theoretical hysteresis at different timings. The fifth graph is π π. The sixth graph is the seventh graph. Figure of a metal-oxide-semiconductor half-field-effect transistor. Figure of zero-voltage switching wave 13 1223135. Figure 8 shows the voltage and current waveforms of the saturated reactance of the present invention. ^, Current waveform diagram of capacitor C3. Tenth diagram: the current waveform diagram of the metal-oxide half field effect transistor Vds of the present invention to the power diode D !, diode D4. The eleventh figure: the metal-oxide of the present invention Current waveform diagram of half field effect transistor Vds to power diode D! And capacitor C2. Figure 12: Comparison chart of the overall efficiency curve of the present invention. Electrical diagram of the present invention-the exchangeable form of a feasible embodiment Copy of Power Supply Announcement Patent No. 2795-14. It is the specification table of the main circuit components of the present invention. The actual switching method of the traditional switching method and the zero-current cut-off switching method and the use of Xiao Te, only test Comparison table of overall efficiency. (1) Symbols of component (3 0) = whole (2 0) energy conversion circuit (d U) power factor correction controller Annex 1 Annex Annex 14
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