TW561680B - Three-level soft-switched converters - Google Patents
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561680 A7 ______ B7 五、發明説明(1 ) 相關申請案之交互參考 此為2000年8月31日申請,序號〇9/652, 869,名稱為"軟 式切換全橋式轉換器π的專利申請案及2〇〇丨年2月5日申請 ,序號--,名稱為"軟式切換全橋轉換器"的專利申 請案之部分延續申請案(代理人文件編號36977:169122)3 發明背景 發明領域 本發明係有關於電源轉換器,且特別有關於高電壓電源 轉換器。 先前技藝說明 一般而言,因為開關的額定電壓係由轉換器的輸入及/ 或輸出電壓而決定,所以高電壓電源轉換應用裝置需具有 高額定電壓的切換元件。洌如,在習知中,分離的降低電 壓之變壓裔的轉換器’亦即,在轉換器中具有輸出電壓比 輸入電壓低的分離電Μ器’在主側切換元件上的電壓係由 輸入電壓及轉1奐器的拓撲(topology)而決定。在如半橋式 及全橋式轉換is之橋式拓撲中的主側開關會受到與輸入電 壓相等之最小電壓的影響。然而,在如單一切換的提前 (forward)及反驰(flyback)轉換器之單端拓撲中的開關電 壓會比輸入電壓高很多。 在南私堡應用裝置中’達成南效率為主要的設計挑戰, 其需要使經由仔細選擇的轉換Is拓撲及切換元件特性之傳 導及切換損失最佳化。顧名思義,如金氧半場效電晶體 (Metal Oxide Semiconductor Field Effect Transistor -4- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 561680561680 A7 ______ B7 V. Description of the Invention (1) Cross Reference to Related Applications This is an application filed on August 31, 2000, with serial number 0/9/652, 869, and named " soft-switching full-bridge converter π. Application and application dated February 5, 2000, serial number-, part of the continuation application for the patent application named "Soft Switching Full Bridge Converter" (Attorney Document No. 36977: 169122) 3 Background of the Invention FIELD OF THE INVENTION The present invention relates to power converters, and more particularly to high voltage power converters. Description of the prior art Generally speaking, because the rated voltage of the switch is determined by the input and / or output voltage of the converter, the high voltage power conversion application device needs a switching element with a high rated voltage. For example, in the prior art, the voltage of the main-side switching element of the separated voltage-reducing transformer converter 'that is, the converter having a separation voltage lower than the input voltage in the converter is determined by The input voltage and topology of the converter are determined. Main-side switches in bridge topologies such as half-bridge and full-bridge transitions are affected by a minimum voltage equal to the input voltage. However, switching voltages in single-ended topologies such as single-switched forward and flyback converters can be much higher than the input voltage. Achieving southern efficiency is a major design challenge in a Nanshuibao application device, which needs to optimize the conduction and switching loss of the characteristics of the switching Is topology and switching elements through careful selection. As the name suggests, such as metal oxide semiconductor field effect transistor (Metal Oxide Semiconductor Field Effect Transistor -4- This paper size applies to China National Standard (CNS) A4 specifications (210X 297 mm) 561680
,簡稱MOSFET)、絕緣閘極雙載子電晶Gate Bipolar Transistor ,簡稱iGBT)及雙載子接面電晶體 (Bipolar Junction Transistor,簡稱BJT)之較高額定電 壓的半導體開關與其相對應之具有較低額定電壓的開關比 孝父起來,會有較大的傳導損失。除此之外,在高電壓應用 裝a中切換知失也會增加。一般而言,切換損失可藉由 使用各種不同之共振或軟式切換的拓撲而降低及甚至消除 。然而,降低傳導損失的方法非常有限。事實上,一旦拓 撲及開關選擇了最低傳導損失所需的額定電壓,能進一步 降低傳導損失的唯一方法就是使用一種拓撲,其可利用具 有較低的額定電壓且因而具有較低的傳導損失之開關。因 為在熟知的多位準轉換器之階級的電路中,主側開關的操 作電壓比輸入電壓低,所以在高電壓應用裝置中,自然會 選擇多位準轉換器3到目前為止,很多種多位準直流/交流 及直流/直流轉換器已敘述於文獻之中。 如一個洌子,圖1會示的是三位準,零電壓切換 (zero-voltage-switched,簡稱ZVS)的直流/直流轉換器, 其敘述於1998年IEEE電力電子專家會議記錄第卜7頁,由(Referred to as MOSFET), Insulated Gate Bipolar Transistor Gate Bipolar Transistor (iGBT) and Bipolar Junction Transistor (BJT) have higher rated voltage semiconductor switches corresponding to them. A switch with a lower rated voltage will have a larger conduction loss than a filial father. In addition, switching knowledge will increase in high-voltage applications. In general, switching losses can be reduced and even eliminated by using a variety of different resonant or soft switching topologies. However, the methods for reducing conduction loss are very limited. In fact, once the topology and the switch have selected the rated voltage required for the lowest conduction loss, the only way to further reduce the conduction loss is to use a topology that can utilize a switch with a lower voltage rating and therefore a lower conduction loss . Because in the well-known multilevel converter circuit, the operating voltage of the main switch is lower than the input voltage, so in high-voltage applications, the multilevel converter 3 will naturally be selected. Level DC / AC and DC / DC converters have been described in the literature. As a bitch, Figure 1 shows a three-level, zero-voltage-switched (ZVS) DC / DC converter, which is described in the 1998 IEEE Power Electronics Experts' Conference Records, p. 7 ,by
Barb i等所發表的「高輸入電壓的直流/直流轉換器:具有 W2的峰笸電壓、電容性的關閉緩衝(snubbing)、以及零 電壓導通的四個開關」論文中。圖1中的轉換器提供了全部 四個主開關的ZVS導通,並且提供了將主開關的電壓限制於 W2 ’以派衝寬度調變(pulse-width-modulation,簡稱 PWM )控制來操作的恆定頻率。然而,因為圖1中的電路會依 -5- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐)Barbi et al. Published a paper entitled "High Input Voltage DC / DC Converters: Peak-to-Voltage with W2, Capacitive Snubbing, and Four Switches with Zero-Voltage Conduction". The converter in Figure 1 provides ZVS conduction for all four main switches, and provides a constant limit to the voltage of the main switch to W2 'to operate with pulse-width-modulation (PWM) control frequency. However, because the circuit in Figure 1 will conform to the Chinese National Standard (CNS) A4 specification (210X 297 mm) according to this paper size
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k 561680 A7 B7 五、發明説明(3 ) 賴諸存於變塵Is T R中的漏電感’以產生用於開關Q 2及Q 4的 Z V S之條件,所以開關Q 2及Q 4的Z V S只能在完全負載附近之非 常有限的負載範圍內達成,除非漏電感顯著增加,或增加 相當大的外部電感,與變壓器的主繞組串聯。應該要注意 的是’在圖1中,電感器L·的電感ί糸表不變屋Is的漏電感及 外部增加的電感(若有的話)之總和。增加與主繞組串聯的 電感 *會對電路的效能產生有害的影響9 因為這樣會降低 有效次(secondary)ί則的工作遇期’益且會產生嚴重的寄生 振龄(ringing),這是由於電感與不會傳導的次ί則整流Is之 接面電容的交互作用3 —般而言,次側工作週期的降低需 籍由降低變壓器的臣(turn)比來做補償,其會增加主倒上 的傳導損失,這是因為進入變塵is之主谢的反射負載電流 也會增加 3 為了降低寄生振龄’需要大的次倒緩衝Is (snubber),其會進一步降低轉換效率。 如另一個例子,圖2繪示的是三位準,軟式切換的直流/ 直流轉換is,其欽述於2 0 0 0年IE E E國際電ί言能源協會 (IN TELEC)的會議記錄第512-517頁’由Canales等人所發表 的"零電壓切換的三位準直流/直流轉換器”論文中。圖2中 的二位準轉換is也具有全部θ個電晶體Qi到Q4之ZVS導通的 特性。除此之外,藉由使甩π飛驰(flying)電容器"CB,其 也異有相位移位控制之怪定頻率操作的特徵。圖2中的電路 ί糸使用諸存於輸出〉慮波電感器的倉&量,以達成夕卜儐ί開關Q i 及Q 4的Z V S,亚且使两諸存於變墨is的漏電感,以達成内侧 開關Q2及Q3的ZVS。因此,外惻開關的ZVS可在寬廣的負載範 -6- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐)k 561680 A7 B7 V. Description of the invention (3) Relying on the leakage inductance 'is present in the dust-changing Is TR to generate the conditions for the ZVS of the switches Q 2 and Q 4, so the ZVS of the switches Q 2 and Q 4 can only be Achieved within a very limited load range near full load, unless the leakage inductance increases significantly or a considerable external inductance is added in series with the transformer's main winding. It should be noted that, in Figure 1, the inductance of the inductor L · represents the sum of the leakage inductance of the constant house Is and the externally added inductance (if any). Increasing the inductance in series with the main winding * will have a detrimental effect on the efficiency of the circuit 9 because this will reduce the effective secondary period, and will cause severe parasitic ringing, which is due to Interaction between inductance and non-conducting secondary rectifier Is interface capacitance 3-Generally speaking, the reduction of the secondary side duty cycle needs to be compensated by reducing the turn ratio of the transformer, which will increase the main trip This is because the reflected load current that enters into the duster is also increased. In order to reduce the parasitic vibration age, a large secondary back buffer Is (snubber) is required, which will further reduce the conversion efficiency. As another example, Figure 2 shows a three-level, soft-switched DC / DC conversion is, which is described in 2000 IE EE International Telecommunications Energy Association (IN TELEC) minutes 512 -517 page "Three-bit quasi-DC / DC converter with zero voltage switching" by Canales et al. The two-level converter is shown in Figure 2 also has all θ transistors Zi to Q4 ZVS Continuity characteristics. In addition, by using a π flying capacitor " CB, it also has the characteristic of strange frequency operation of phase shift control. The circuit in Figure 2 uses various storage In the output> the volume of the inductor is considered to achieve the ZVS of the switches Q i and Q 4 and the leakage inductances stored in the variable ink is to achieve the internal switches Q2 and Q3. ZVS. Therefore, the ZVS of the external switch can be used in a wide range of load -6- This paper size applies to China National Standard (CNS) A4 specifications (210X 297 mm)
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k 561680 A7 ____ B7__ 五、發明説明(4 ) 圍内達成,然而内側開關的ZVS範圍非常有限,除非渴電感 顯著增加,及/或增加大的外部電感,與主繞組事聯。如已 解釋的,漏電感增加及/或外部電容器的增加,對電路的效 能會產生有害的影響。 近來,一種軟式切換全橋式技衛,其實質上能達成具有 未損失的次側工作週期且具有最小傳遞能量之整個負裁戶 行範圍之主開關的ZVS,係敘述於2000年8月31日,由Jang 及Jo vano vie所申請之專利申請案序號09/652, 869。達成此 技術的一種方式係繪示於圖3中。圖3中的電路係使用赌存 於耦合電感器之磁化電感中的能量,以使電容所玫的電 何通過即將導通且因此能達成ZVS的開關。藉由適當地選擇 耦合電感器之磁化電感的值,圖3之轉換器中的主開關甚至 可在沒有負載的情況下,達成ZVS。因為在圖3的電路中, 在輕負載處,產生ZVS條件之所需的能量不需鍺存於漏電感 中’所以可以使變壓器的漏電感最小化。因此,次側上之 工作週期的損失可最小化,其能使變壓器的臣比最大化, 因此能使主侧傳導損失最小化。除此之外,變壓器的最小 漏電感可使由漏電感與整流器的接面電容之間的共振所產 生的次ί則振鈴顯著地降低,其可使經常用於降低振鈐的緩 衝器電路之功率消耗大大地降低。 在本發明中,達成圖3之轉換器之主開關的ZVS所使用的 觀念可擴展到三位準轉換器。 發明概要 社本發明中,所揭露的是許多三位準、I亙定頻率、軟式 本紙張尺度適用中國國家標準(CNS) Α4規格(210 X 297公釐) 561680 A7 B7 五、發明説明(5 ) 切換的分離轉換,其實質上可在負載電流及輸入電壓的 寬廣破圍内’達成主開關的零電壓導通。一般面言9 14些 轉換係使用分離變壓25之主谢上的電感Is 5以產生主開 關的ZVS條件。在一些具體實施例中,主側電感器為具有兩 繞組的搞合電感is ’面在其他的具體實施例令’電感器只 有一個繞組。電感器及變壓器會配置於電路中,以致於在 串接的四個開關之外倒及内倒對的開關之間的相位移位改 變會改變相反方向之變塵is的電感器及繞組的繞组上之電 壓秒積。特別而言’如果外倒及内倒對的開關之間的相位 移位改變,以致於變壓器的繞組上之電壓秒積降低,則電 感器的繞組上之電壓秒積會增加,而且反之亦然3 因為在本發明的電路中’當負載電流降低及/或輸入電壓 增加時’緒存於電感Is中之ZVS的可用能量會增加,所以本 發明的電路可在輸入電壓及負載電流的非常寬廣範圍内’ 包括沒有負載,達成ZVS。 除此之外,因為用來產生輕載處的ZVS條件之能量不是鍺 存於變壓is的漏電感中,所以變塵Is的漏電感可以最小化 ,其也會使變壓器之次惻上的工作週期損失最小化。因此 ’本發明的轉換is可以最大的工作週期來運作’因此可使 主開關的傳導損失及變壓器之次谢之組件上的電/堅最小化 ’其可以改善轉換效率。此外^因為漏電感已最小化’所 以由漏電感與整流器的接面電容之間的共振所產生的次谢 寄生振龄也會最小化^以致於通常用來降低振龄之所需之 緩衝s電路的功率消耗也會降低° -8- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 561680 A7 B7 五、發明説明(6 本發明的電路可實施為直流/直流轉換器或直流,/交流反 相泛之任一。如果實施為直流直流轉換器,可使用任何型 式的次ί射整流器’例如,具有中央分接的次繞組之全波整 流器、具由電流加倍的全波整流器、或全橋全波整流器。 圖式簡單說明 圖1繪示的是恆定頻率、pWM、ZVS、三位準的直流/直流 轉換器:(a)電源階段;(b)主開關的時序圖(先前技藝)3 圖2緣示的是恆定頻率、相位移位、zvs、三位準的直流/ 直流轉換器:(a)電源階段;(b)主開關的時序圖(先前技 藝)。 圖3输示的是使用耦合電感器之全橋轉換器,以達成輸入 電塵及輸出電流在寬廣範圍内之主開關的zvs(先前技藝)。 圖4綠示的是根據本發明之軟式切換直流/直流三位準轉 換器之較佳具體實施例之一。 圖5繪示的是圖4所繪示之軟式切換三位準直流/直流轉 換器之較佳具體實施例的簡化電路。 圖6(a)-(1)繪示的是在切換週期的期間,圖4中之軟式切 換三位準直流/直流轉換器的拓撲階段s 圖7(a)-(〇)繪示的是圖4中之軟式切換三位準直流/直流 轉換器的關鍵波形:(a)驅動開關Si的訊號·,(b)驅動開關 S·2的訊號;(c)驅動開關33的訊號;(d)驅動開關54的訊號; (e)通過開關\的電壓波形vsi ; (f )通過開關s2的電壓波形 vS2; (g)通過開關33的電壓波形Vs3; (h)通過開關54的電壓 波形vS4: (i)主電壓vP; (j)通過耦合電感器的電壓νλβ: 〇〇 -9- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)k 561680 A7 ____ B7__ 5. The description of the invention (4) is reached within the range, however, the ZVS range of the inner switch is very limited, unless the thirsty inductance increases significantly and / or a large external inductance is added to the main winding. As explained, an increase in leakage inductance and / or an increase in external capacitors can have a detrimental effect on the performance of the circuit. Recently, a soft-switching full-bridge technical guard, which can essentially achieve the ZVS main switch of the entire negative redeployment range with a non-lost secondary duty cycle and minimal transfer energy, is described on August 31, 2000 Date, patent application serial number 09/652, 869 filed by Jang and Jo vano vie. One way to achieve this technique is illustrated in FIG. The circuit in Figure 3 uses the energy stored in the magnetizing inductance of the coupled inductor so that the capacitor's current will pass through and thus achieve ZVS switching. By properly selecting the value of the magnetizing inductance of the coupled inductor, the main switch in the converter of Figure 3 can achieve ZVS even without a load. In the circuit of Fig. 3, at light load, the energy required to generate the ZVS condition does not require germanium to be stored in the leakage inductance ', so the leakage inductance of the transformer can be minimized. Therefore, the loss of the duty cycle on the secondary side can be minimized, which can maximize the ratio of the transformer, and thus minimize the conduction loss on the primary side. In addition, the minimum leakage inductance of the transformer can significantly reduce the secondary ringing caused by the resonance between the leakage inductance and the interface capacitance of the rectifier, which can make the buffer circuit often used to reduce the vibration Power consumption is greatly reduced. In the present invention, the concept used in ZVS to achieve the main switch of the converter of Fig. 3 can be extended to a three-level converter. SUMMARY OF THE INVENTION In the present invention, many three-level standards, I fixed frequencies, and flexible paper sizes are applicable to the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 561680 A7 B7 V. Description of the invention (5 ) Switching and separation, which can achieve zero-voltage conduction of the main switch within a wide range of load current and input voltage. Generally speaking, some conversions use the inductor Is 5 on the main transformer of the separation transformer 25 to generate the ZVS condition of the main switch. In some specific embodiments, the main-side inductor is a two-winding inductive inductor is 'plane. In other specific embodiments, the' inductor has only one winding. Inductors and transformers will be arranged in the circuit, so that the phase shift between the switches that are reversed and inverted inside the four switches connected in series will change the windings of the inductors and windings in the opposite direction. Second product of voltage on the group. In particular, 'if the phase shift between the outer and inner pairs of switches changes such that the voltage second product on the windings of the transformer decreases, the voltage second product on the windings of the inductor will increase, and vice versa 3 Because the available energy of the ZVS stored in the inductor Is increases when the load current decreases and / or the input voltage increases in the circuit of the present invention, the circuit of the present invention can provide a very wide range of input voltage and load current. In scope 'includes no load to reach ZVS. In addition, because the energy used to generate the ZVS condition at light load is not germanium stored in the leakage inductance of the transformer is, the leakage inductance of the dust change Is can be minimized, which will also make the transformer Minimize work cycle losses. Therefore, ‘the conversion of the present invention can be operated with the maximum duty cycle’, thereby minimizing the conduction loss of the main switch and the electrical / hardness of the transformer ’s second most important component, which can improve the conversion efficiency. In addition, ^ Since the leakage inductance has been minimized ', the secondary parasitic vibration age caused by the resonance between the leakage inductance and the interface capacitance of the rectifier will also be minimized ^ so that the buffers usually used to reduce the vibration age The power consumption of the circuit will also be reduced ° -8- This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 561680 A7 B7 V. Description of the invention (6 The circuit of the invention can be implemented as DC / DC conversion Either a DC or AC / AC inverter. If implemented as a DC-DC converter, any type of secondary rectifier can be used. For example, a full-wave rectifier with a secondary winding with a central tap, Full-wave rectifier, or full-bridge full-wave rectifier. Brief description of the figure Figure 1 shows a constant-frequency, pWM, ZVS, three-level DC / DC converter: (a) power stage; (b) the main switch Timing diagram (previous technique) 3 Figure 2 shows a constant frequency, phase shift, zvs, three-level DC / DC converter: (a) power stage; (b) timing diagram of the main switch (previous technique) Figure 3 shows the use of coupling Inductor full-bridge converter to achieve the zvs (previous technique) of the main switch with input dust and output current in a wide range. Figure 4 green shows a soft switching DC / DC three-level converter according to the present invention One of the preferred embodiments. Fig. 5 shows a simplified circuit of the preferred embodiment of the soft switching three-bit quasi-DC / DC converter shown in Fig. 4. Figs. 6 (a)-(1) Shown during the switching cycle is the topology phase s of the soft-switching three-level quasi-DC / DC converter in Figure 4. Figures 7 (a)-(〇) show the soft-switching three-level quasi-levels in Figure 4. Key waveforms of DC / DC converters: (a) signal driving switch Si, (b) signal driving switch S · 2; (c) signal driving switch 33; (d) signal driving switch 54; (e) ) Voltage waveform vsi through switch \; (f) Voltage waveform vS2 through switch s2; (g) Voltage waveform Vs3 through switch 33; (h) Voltage waveform vS4 through switch 54: (i) Main voltage vP; ( j) The voltage νλβ through the coupled inductor: 〇〇-9- This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm)
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k 561680 A7 -___ B7 五、發明説明(7 ) 主電流波形iP,·(1)磁化電流波形iMC : (m)電流L ; (n)電流 h ; (〇)輸出濾波器Vs之輸入端的電壓。 圖8綠示的是本發明之另一具體實施例,其使用具有中央 分接的主繞組之變壓器。 圖9緣示的是本發明之又一具體實施例,其使用單一繞組 電感器。 圖10繪示的是本發明之一具體實施例,其具有用於電容 器CB1及CB2的預先充電電路。 發明詳細說明 圖4緣示的是根據本發明之軟式切換直流/直流三位準轉 換器之較佳具體實施例之一。圖4中的三位準轉換器包含串 聯連接的主開關Si到$4、分隔路線(rail-splitting)的電容 器Ccl及Cc2、”飛馳(f lying)電容器"(^及Cb2、分離變壓器TR 、以及耦合電容器Lc。在此具體實施例中,負载係經由連 接至變壓器之中央分接的(center —tapped)次側的全波整 流器而耦接至轉換器。除此之外,箝位(clamp)二極體t 及b會在開關關閉之後,分別用來箝位外侧開關&及&的 電壓到VIN/2,而如果最後會藉由寄生電路及開關的特徵與 時序訊號之不匹配而在變壓器繞組上產生次側的電壓不安 定的情形,會使用阻隔電容器CB來防止變壓器飽和。 應該要注意的是,在圖4的具體實施例中,次側輸出電路 係實施為具有中央分接的次繞組之全波整流器。然而,本 發明之直流/直ML轉換器實施裝置的次側輸出電路也可實 施為任意形式的整流器’例如’具有加倍電流的全波整流 •10- 本紙張尺度適用中國國家標準(CMS) A4規格(210 X 297公釐) -------- 561680 A7 B7 五、發明説明(8" 器,或全橋全波整流器。除此之外,本發明的轉換器也可 實施為直流/交流反相器,亦即,在變壓器的次繞組與負載 之間,沒有整流器電路。 為了便於解釋圖4中的電路之運作,圖5繪示的是其簡化 的電路圖。在此簡化的電路中,假設輸出濾波器LF的電感 足夠大,以至於在切換週期的期間,輪出濾波器可模型化 為具有與輸出電流1〇的大小相等之恆定電流源。再者,假 設電容器Ccl&CC2的電容(其來自於將電壓分成一半的電容 分壓器(divider))是大的,以致於電容器(:(:1及(:(:2可分別藉 由電壓源V^Vu/2及V2=V1N/2而模型化。同樣地,假設"飛馳 (flying)電容器"CB1&CB2的電容足夠大,以致於電容器可 分別模式化為恆定電壓源VCB1& VCB2。因為在切換週期的期 間,耦合電感器繞組及變壓器繞組的平均電壓為零,並且 因為當使用相位移位控制時,在每個橋接腳中的成對開關 係以50%的工作週期來運作,所以圖5中之電壓源VCB1&VCB2 的大小與V,N/4相等,亦即,VCB1 = VCB2= VlN/4。 為了更簡化圖4中之電路的運作分析,還假設導通的電晶 體開關之阻抗為零,而沒有導通的開關之電阻為無限大。 除此之外,會忽略變壓器TR及耦合電感器Lc兩者的漏電感 ’與變壓器TR的磁化電感,這是因為其對於電路運作的影 響不明顯。然而,在此分析中,不能忽略耦合電感器Lc的 磁化電感及主開關Crh的輸出電容,這是因為其在電路運 作中扮演主要的角色。因此,在圖5中,耦合電感器Lc會模 型化為具有匝比1^ = 1及具有通過串接的繞組AC及CB之平行 -11 · 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐)k 561680 A7 -___ B7 V. Description of the invention (7) Main current waveform iP, · (1) Magnetizing current waveform iMC: (m) current L; (n) current h; (〇) voltage of input terminal of output filter Vs . Fig. 8 shows another embodiment of the present invention in green, which uses a transformer having a main winding with a central tap. FIG. 9 illustrates another embodiment of the present invention, which uses a single winding inductor. FIG. 10 shows a specific embodiment of the present invention, which has a pre-charging circuit for the capacitors CB1 and CB2. Detailed description of the invention Fig. 4 shows one of the preferred embodiments of the soft switching DC / DC three-position quasi-converter according to the present invention. The three-level converter in FIG. 4 includes main switches Si to $ 4 connected in series, capacitors Ccl and Cc of a rail-splitting, "f lying capacitors" (^ and Cb2, separation transformer TR, And the coupling capacitor Lc. In this specific embodiment, the load is coupled to the converter via a center-tapped secondary-side full-wave rectifier connected to the transformer. In addition, the clamp ) Diodes t and b will be used to clamp the voltages of the outer switches & and & to VIN / 2 after the switch is turned off, and if the characteristics of the parasitic circuit and the switch do not match the timing signal at the end In the case of voltage instability on the secondary side of the transformer winding, a blocking capacitor CB is used to prevent the transformer from being saturated. It should be noted that in the specific embodiment of FIG. 4, the secondary side output circuit is implemented with a central branch. Full-wave rectifier connected to the secondary winding. However, the secondary-side output circuit of the DC / DC ML converter implementation device of the present invention can also be implemented as any form of rectifier 'for example' full-wave rectification with double current • 10- This paper size applies Chinese National Standard (CMS) A4 specification (210 X 297 mm) -------- 561680 A7 B7 V. Description of the invention (8 " or full-bridge full-wave rectifier. Except In addition, the converter of the present invention can also be implemented as a DC / AC inverter, that is, there is no rectifier circuit between the secondary winding of the transformer and the load. To facilitate the explanation of the operation of the circuit in FIG. 4, FIG. 5 The simplified circuit diagram is shown. In this simplified circuit, it is assumed that the inductance of the output filter LF is large enough that during the switching period, the wheel-out filter can be modeled to have a size equal to the output current 10. An equal constant current source. Furthermore, suppose that the capacitance of the capacitor Ccl & CC2 (which comes from a capacitor divider that divides the voltage in half) is so large that the capacitors (: (: 1 and (: (: 2 can be modeled by the voltage sources V ^ Vu / 2 and V2 = V1N / 2, respectively. Similarly, it is assumed that the capacitance of "flying capacitor" CB1 & CB2 is large enough that the capacitors can be individually patterned Is a constant voltage source VCB1 & VCB2. Because switching During this period, the average voltage of the coupled inductor winding and transformer winding is zero, and because the phase-shift control is used, the pairwise split relationship in each bridge pin operates at a 50% duty cycle, so Figure 5 The size of the voltage source VCB1 & VCB2 is equal to V, N / 4, that is, VCB1 = VCB2 = VlN / 4. In order to simplify the operation analysis of the circuit in Figure 4, it is also assumed that the impedance of the turned-on transistor switch is zero. , And the resistance of the non-conducting switch is infinite. In addition, the leakage inductance ′ of both the transformer TR and the coupled inductor Lc and the magnetizing inductance of the transformer TR are ignored, because the influence on the circuit operation is not obvious. However, in this analysis, the magnetizing inductance of the coupled inductor Lc and the output capacitance of the main switch Crh cannot be ignored because it plays a major role in circuit operation. Therefore, in Figure 5, the coupled inductor Lc will be modeled as a parallel with a winding ratio of 1 ^ = 1 and with windings AC and CB connected in series. -11 · This paper applies the Chinese National Standard (CNS) A4 specification ( 210X297 mm)
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線 561680 A7 B7 五、發明説明(9 的磁化電感La之理想變壓器,而變壓器只會藉由具有阻 比nTR的理想變壓器而模型化。應該要注意的是,電感器k 的磁化電感LCM之係表示端點C開路時,在端點a及B之間所量 測到的電感。 參考圖5 ’在電流之間可產生以下的關係。 iP = iPl + iP2 (1) h = h\ + ^MC (2) ’2 - ’/>2 AC, (3) 因為耦合電感器Lc之繞組AC及繞組CB的匝數相同 ,其一 定為 lP\ ~ lP2 (4) 將方程式(4)代入方程式(1)-(3)可得 (5) ’丨+ ‘c (6) h = (7) 從方程式(6)及(7)可知,電流1及i2係由兩種組件所組成 :主電流組件ip/2及磁化電流組件iMC。主電流組件係直接 取決於負載電流,而磁化電流不是直接取決於負載,而是 取決於通過磁化電感的電壓秒積。顧名思義,一旦改變外 側開關S4與個別的内側開關S2&S3之導通瞬間之間的 相位移位,會產生隨著負載電流改變而改變的磁化電流, 以保持輸出規定。通常,隨著負載改變之相位移位的改變 在輕負載處會較大,亦即,如同負載會朝著沒有負載降低 -12- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐)Line 561680 A7 B7 V. Description of the invention (9 ideal transformer of magnetizing inductance La, and the transformer will only be modeled by an ideal transformer with resistance ratio nTR. It should be noted that the magnetizing inductance LCM of the inductor k Represents the inductance measured between terminals a and B when terminal C is open. Refer to Figure 5 'The following relationship can be generated between currents. IP = iPl + iP2 (1) h = h \ + ^ MC (2) '2-' / > 2 AC, (3) Because the number of turns of the winding AC and winding CB of the coupled inductor Lc is the same, it must be lP \ ~ lP2 (4) Substitute equation (4) into the equation (1)-(3) can be obtained (5) '丨 +' c (6) h = (7) From equations (6) and (7), we can see that current 1 and i2 are composed of two components: the main current The component ip / 2 and the magnetizing current component iMC. The main current component directly depends on the load current, and the magnetizing current does not depend directly on the load, but depends on the voltage second product through the magnetizing inductance. As the name implies, once the outer switch S4 is changed with the individual The phase shift between the on-times of the inner switch S2 & S3 of the Changing the magnetizing current to maintain the output specification. Generally, the change in phase shift with load changes will be larger at light loads, that is, as the load will decrease toward no load -12- This paper size applies to China Standard (CNS) A4 (210X 297 mm)
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k 561680 A7 ______B7 五、發明説明(1〇 ) ’而不會朝著重載降低。因為在圖4的電路中,當負載接近 零時,相位移位會增加,所以LMC的電壓秒積也會增加,以 致於圖4中的電路會在沒有負載處,產生最大的磁化電流, 其可在沒有負載處,達成ZVS。 因為磁化電流i MC不會提供負載電流,如圖5所示,所以其 係表示傳遞電流。一般而言,此傳遞電流及其相對應的能 1應該最小化,以降低損失及使轉換效率最大化。由於 的電壓秒積係反相取決於負載電流,所以圖4中的電路在全 載處所傳遞的能量比在輕負載處為低,因此,其具有最小 傳遞電流之寬廣負載範圍内的ZVS之特徵。 還從圖5可知 VAB = VAC + VCB (8) 因為耦合電感Lc的兩個繞組具有相同的匝數,亦即,因 為Lc的匝比為nLC = i,其必定為 VAC = VCB ( 9 ) 或k 561680 A7 ______B7 V. Description of the Invention (1〇) ’without reducing towards heavy load. Because in the circuit of FIG. 4, the phase shift will increase when the load is close to zero, so the voltage second product of the LMC will also increase, so that the circuit in FIG. 4 will generate the maximum magnetizing current at no load. ZVS can be achieved without load. Because the magnetizing current i MC does not provide a load current, as shown in Fig. 5, it represents the transfer current. In general, this transfer current and its corresponding energy 1 should be minimized to reduce losses and maximize conversion efficiency. Because the voltage-second product system is inversely dependent on the load current, the circuit in Figure 4 transmits less energy at full load than at light load. Therefore, it has the characteristics of ZVS over a wide load range with the smallest transfer current. . It can also be seen from Figure 5 that VAB = VAC + VCB (8) because the two windings of the coupled inductor Lc have the same number of turns, that is, because the turns ratio of Lc is nLC = i, it must be VAC = VCB (9) or
一般對於恆定頻率的相位移位控制而言,電壓為方波 電壓,其包含大小V1N/2之變化的正及負脈衝,其藉由、尸q 的時間區間所區隔。根據方程式(1 〇)及參考圖5,在内側開 關S2及S4的任一個閉合及vAB = 0時的時間區間,主電屋大小 為V1N /4,而在V1N /2時的時間區間,主電壓大 小為 |vp| = 〇。 -13· 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 561680 A7 ____B7 五、發明説明(11 ) 為了更便於分析,圖6繪示的是在切換週期的期間,轉換 器的拓撲階段’而圖7繪示的是關鍵波形。 如圖7所繪不,因為在時間區間的期間,開關\及心 為閉合,而開關S3&S4為開路,電壓V1N /2,以致於 主電廢vP=0。除此之外,在拓撲階段的期間,其等效電路 係緣示於圖6(a)中,輸出電流丨。會流經輸出整流器Dq2及相 對應之變壓器的次側,以致於主電流ip= Iq/i1tr,其中h = NP/NS為變壓器的匝比,\為主繞組的匝數,而\為次繞組 的匝數。因為主電流為負,所以電流込及“也都為負,如圖 7(m)及7(n)所繪示。同時,由於正電壓Vab= yiN/2,所以磁 化電流iMC會以斜率V1N/(2LMC)線性地增加,其會使込增加, 而使i2降低。在這整個階段的期間,因為主電壓Vp為零,所 以在輸出濾波器的輸入端之電壓vs(其與電壓秒相等)為零 。當開關51關閉時,此階段會在結束。 在開關51於1:=1\關閉之後,流經開關Si的電晶體之電流會 轉向到開關的輸出電容器1,如圖6(b)所繪示。在此拓撲 階段中,因為通過電容器1及(:4的電壓總合等於恆定電壓 V!N/2,所以電流i2會同時對電容器C,充電,並且使電容器 C4放電。因此,通過開關的電壓會增加,而通過開關S4 的電壓會降低,如圖7(e)及(h)所繪示。除此之外,在此階 段的期間,點A的電位會降低,而使電壓vAB從νίΝ/2朝著零 降低,並且同時會使主電壓vP從零朝著VIN/4上升,如圖7(0 及(j)所繪示。正的主電壓會使輸出電流I。開始從整流器D02 轉換到整流器。因為忽略了變壓器TR的漏電感,所以此 -14- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 561680 A7 B7 五、發明説明(12 ) 轉換是瞬間的。然而,如果出現漏電感,電流從一個整流 器轉換到另一個整流器會花費時間。因為在此轉換時間的 期間,兩個整流器會導通,亦即,變壓器的次侧會短路, 所以電壓乂5為零,如圖7(0)所繪示。 在電容器C4Kt=T2完全放電之後,亦即,在電壓vS4到達 零之後,電流i2會繼續流經開關54的反平行二極體〇4及箝位 二極體DC1,而取代流經(^及(:4,如圖6(c)所繪示。由於正 電壓VIN/4會施加到主繞組,所以電流iP、込、以及i2會從負 往正的方向上升。為了達成開關54的ZVS,開關34需要在其 反平行二極體〇4正導通之時間區間的期間導通,如圖7所繪 示。當輸出電流10完全從整流器D02轉換到整流器DQ1時,亦 即,當主電流變成iP=Ia/nTi^,圖6(c)的階段會在t = T# 束。 在時間區間T3- T4的期間,電流(其流經閉合開關s2)的 供應係來自於電壓源VCB1,而電流i2(其流經閉合開關S4)的 供應係來自於電壓源V2,如圖6(d)所繪示。當開關S2關閉時 ,圖6(d)的階段會在t=T4結束。在開關S2關閉之後,流經開 關S2之電晶體的電流會轉向到輸出電容器C2,如圖6(e)所繪 示。在此拓撲階段中,因為通過電容器02及(:3的電壓總合等 於恆定電壓VCBl + VCB2 = VIN/2,所以電流i i會同時對電容器C2 充電,並且使電容器C3放電。因此,通過開關S2的電壓會增 加,而通過開關S3的電壓會降低,如圖7(f)及(g)所繪示。 同時,點A的電位會開始降低,而使電壓vAB從零朝著-νιΝ/2 降低,並且會使主電壓Vp&V1N/4朝著零降抵,如圖7(i)及 -15- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 561680 A7 ____ B7 ___ 五、發明説明(13 ) (j )所繪示。因為主電壓的降低會反射到次側,所以電壓Vs 也會朝著零降低,如圖7(〇)所繪示。當電容器(:3完全放電 及當電流I開始流經開關33的反平行二極體〇3時,此階段會 在t=T5結束,如圖6(f)所繪示。因為在t=T5之後,負電壓 VIN/2會施加到磁化電感lmc,所以磁化電流iMc會以常數斜率 V1N/(2LMC)開始朝著零線性地降低,如圖7(i)所繪示。在 於t=Te到達零之後,其會以負的方向繼續流動,如圖6(g) 所表示。當開關s4關閉時,圖6(g)的拓撲階段會在t = T7結束 ’並且轉換器會進入第二個切換週期的一半。在第二個切 換週期的一半之期間的運作,亦即,在時間區間八-了13之 期間的運作,係與在具有開關S1&S2與開關33及34交換的角 色之時間區間八-T7之期間的運作相同。 由圖6的波形(m)及(η)可知,全部四個主開關\到\在關 閉瞬間’流經開關的電流之大小相同,亦即,Generally, for a constant frequency phase shift control, the voltage is a square wave voltage, which includes positive and negative pulses with a change of magnitude V1N / 2, which are separated by the time interval of the corpse q. According to equation (10) and referring to FIG. 5, in the time interval when any of the inner switches S2 and S4 are closed and vAB = 0, the size of the main electric house is V1N / 4, and in the time interval when V1N / 2, the main The magnitude of the voltage is | vp | = 〇. -13 · This paper size is in accordance with Chinese National Standard (CNS) A4 (210 X 297 mm) 561680 A7 ____B7 V. Description of the invention (11) For easier analysis, Figure 6 shows the conversion during the switching cycle. Topological stage of the processor 'while Figure 7 shows the key waveforms. As shown in Fig. 7, during the time interval, the switch \ and the core are closed, and the switch S3 & S4 is open and the voltage V1N / 2, so that the main electrical waste vP = 0. In addition, during the topology phase, its equivalent circuit is shown in Fig. 6 (a), and the output current 丨. Will flow through the output rectifier Dq2 and the secondary side of the corresponding transformer, so that the main current ip = Iq / i1tr, where h = NP / NS is the turns ratio of the transformer, \ is the number of turns of the primary winding, and \ is the secondary winding Number of turns. Because the main current is negative, the currents 込 and "are also negative, as shown in Figs. 7 (m) and 7 (n). At the same time, because the positive voltage Vab = yiN / 2, the magnetizing current iMC will have a slope V1N / (2LMC) increases linearly, which will increase 込 and decrease i2. During this whole period, because the main voltage Vp is zero, the voltage vs (which is equal to the voltage seconds) at the input of the output filter ) Is zero. When the switch 51 is closed, this phase will end. After the switch 51 is closed at 1: = 1 \, the current flowing through the transistor Si will be turned to the output capacitor 1 of the switch, as shown in Figure 6 ( b). In this topology stage, because the voltages through capacitors 1 and (: 4 are equal to the constant voltage V! N / 2, the current i2 will charge capacitor C, and discharge capacitor C4 at the same time. Therefore, the voltage through the switch will increase, while the voltage through the switch S4 will decrease, as shown in Figures 7 (e) and (h). In addition, during this stage, the potential at point A will decrease, The voltage vAB decreases from νίΝ / 2 toward zero, and at the same time, the main voltage vP increases from zero toward VIN / 4, such as 7 (0 and (j). Positive main voltage will cause output current I. Begin to switch from rectifier D02 to rectifier. Because the leakage inductance of transformer TR is ignored, this -14- This paper size applies to Chinese national standards (CNS) A4 specification (210 X 297 mm) 561680 A7 B7 V. Description of the invention (12) The conversion is instantaneous. However, if leakage inductance occurs, it will take time to switch the current from one rectifier to another. Because here During the conversion time, the two rectifiers will be turned on, that is, the secondary side of the transformer will be short-circuited, so the voltage 乂 5 is zero, as shown in Figure 7 (0). After the capacitor C4Kt = T2 is completely discharged, that is, After the voltage vS4 reaches zero, the current i2 will continue to flow through the anti-parallel diode 04 and the clamp diode DC1 of the switch 54 instead of flowing through (^ and (: 4, as shown in Figure 6 (c)). As the positive voltage VIN / 4 is applied to the main winding, the currents iP, 込, and i2 rise from the negative to the positive direction. In order to achieve the ZVS of the switch 54, the switch 34 needs to be at its antiparallel diode. 4 During the positive conduction time interval, the conduction is shown in Figure 7 When the output current 10 is completely switched from the rectifier D02 to the rectifier DQ1, that is, when the main current becomes iP = Ia / nTi ^, the stage of FIG. 6 (c) will be bundled at t = T #. In the time interval T3- T4 During this period, the supply of current (which flows through the closed switch s2) is from the voltage source VCB1, and the supply of current i2 (which flows through the closed switch S4) is from the voltage source V2, as shown in Figure 6 (d) When the switch S2 is closed, the phase of Fig. 6 (d) will end at t = T4. After the switch S2 is closed, the current flowing through the transistor of the switch S2 will be diverted to the output capacitor C2, as shown in Fig. 6 (e). Draw. In this topology stage, because the voltages through capacitors 02 and (: 3 are equal to the constant voltage VCBl + VCB2 = VIN / 2, the current ii will simultaneously charge capacitor C2 and discharge capacitor C3. Therefore, through switch S2 The voltage will increase and the voltage through switch S3 will decrease, as shown in Figures 7 (f) and (g). At the same time, the potential at point A will start to decrease, so that the voltage vAB will go from zero toward -νιN / 2 Decrease and reduce the main voltage Vp & V1N / 4 towards zero, as shown in Figure 7 (i) and -15- This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 561680 A7 ____ B7 ___ 5. It is shown in the description of the invention (13) (j). Because the decrease of the main voltage will be reflected to the secondary side, the voltage Vs will also decrease towards zero, as shown in Fig. 7 (〇). When the capacitor ( : 3 is fully discharged and when the current I begins to flow through the antiparallel diode 03 of the switch 33, this stage will end at t = T5, as shown in Figure 6 (f). Because after t = T5, the negative The voltage VIN / 2 is applied to the magnetizing inductance lmc, so the magnetizing current iMc starts to decrease linearly toward zero with a constant slope V1N / (2LMC), As shown in Figure 7 (i), after t = Te reaches zero, it will continue to flow in a negative direction, as shown in Figure 6 (g). When the switch s4 is closed, the topology stage of Figure 6 (g) Will end at t = T7 'and the converter will enter half of the second switching cycle. Operation during half of the second switching cycle, that is, operation during time interval eight to 13 is related to The operation is the same during the time interval eight-T7 with the roles of switches S1 & S2 and switches 33 and 34. From the waveforms (m) and (η) of Fig. 6, it can be seen that all four main switches \ to \ are closed The instantaneous' current flowing through the switch is the same, that is,
2 In TR 其中’ I 〇為負載電流’ nTR為變磨器的匝比,而I ^為磁化 電流i mc的大小。 根據方程式(11),在關閉的開關之電容正在充電(通過開 關的電壓正上升)與即將導通的開關之電容正在放電(通過 開關的電壓正下降)的期間,開關的轉換會藉由主電流“及 磁化電流iMe所儲存的能量而完成。當磁化電流L所提供的 轉換能量總是儲存於耦合電感器Lc的磁化電感L中時,電 流iP所提供的轉換能量會儲存於次側輸出電路的濾波器電 感(未繪示於圖5中),或變壓器TR及耦合電感器。的漏電感2 In TR where ‘I 〇 is the load current’ nTR is the turns ratio of the transformer and I is the magnitude of the magnetizing current i mc. According to equation (11), during the period when the capacitor of the closed switch is being charged (the voltage through the switch is rising) and the capacitor of the switch to be turned on is being discharged (the voltage is falling through the switch), the switch is switched by the main current "And the energy stored in the magnetizing current iMe. When the conversion energy provided by the magnetizing current L is always stored in the magnetizing inductance L of the coupled inductor Lc, the conversion energy provided by the current iP is stored in the secondary output circuit Filter inductance (not shown in Figure 5), or the leakage inductance of the transformer TR and the coupled inductor.
561680561680
(未㈣於® 5中)之任-種之中。特別是對於内側開關^及 S3而s,lp所提供的轉換能量係儲存於輸出濾波電感器^ 之中’而對於外侧開關\及s4而言,其係儲存於變壓器的漏 電感之中。因為希望最小化變壓器1的漏電感,以使次側 的寄生振鈴最小化,所以儲存於漏電感中的能量相當小, 亦即,比儲存於輸出濾波電感器中的能量更小。因此,在 圖4的電路中,可輕易達成在整個負載範圍内之内侧開關心 及S3的ZVS,而外側開關\及\的2”需要適當大小的磁化電 感LMC,這是因為在輕負載處,需要產生外侧開關心及&之 ZVS條件的幾乎全部能量係儲存於磁化電感之中。 如200 1年2月5日申請之專利申請案序號__所解 釋’在具有搞合電感器及分離變壓器的全橋電路中,電感 器及變壓器可互換角色。特別而言,藉由增加次繞組於耦 合電感器中,耦合電感器可用來當作變壓器,以將電源傳 送到連接次側的輸出電路,而變壓器的磁化電感可用來當 作電感器’以儲存ZVS的能量。圖8及9緣示的是兩個這樣的 具體實施例。一般而言,圖8及9中之電路的運作與圖4中之 電路的運作相同。主要的差異是,在圖4的電路中,當成對 的外側及内側開關之間的相位移位為180度時,會得到最大 輸出電壓(電壓秒積),而當相位移位為零時,圖8及9的電 路會產生最大輸出電壓(電壓秒積)β因為都需要使簡單的 控制訊號於電壓控制迴路中反相,以得到所希望的控制迴 路特性,所以不同具體實施例之控制特徵的差異會對控制 迴路設計產生微小的影響。 -17- 本紙張尺度適用中國國家標準(CNS) Α4規格(210 X 297公釐) 561680 A7 ___B7 五、發明説明(15 ) 如已解釋的,在本發明的電路中,達成外部對的開關之 ZVS比内部對的開關較為困難,這是因為在此兩對開關中, 可達到產生ZVS條件的能量不相同。一般而言,為了達成zvs ’此能量必須至少等於使即將導通的開關之電容放電且同 時對已關閉的開關之電容充電所需的能量。在重載電流處 ,ZVS主要可糟由儲存於變壓器TR的漏電感來達成。當負載 電流降低時,儲存於漏電感中的能量也會降低,而儲存於 電感器Lc中的能量會增加,以至於在輕載處,Lc可用來增加 ZVS所需之能量的負擔。事實上,在沒有負載處,此Lc會提 供產生ZVS條件所需的全部能量。因此,如果選擇Lc的值, 以致於在沒有負載且最大輸入電壓,達成zvs, zvs 可在整個負載及輸入電壓範圍内達成。 如果忽略變壓器之繞組的電容,達成圖4之實施裝置中之 外侧開關的ZVS所需的磁化電感lmc為 L^c-ik~r 〇2) 然而’達成圖8及9之實施裝置中之内側開關的zvs所需的 電感Le為(Not in ® 5) of any-among the species. Especially for the inner switches ^ and S3 and s, lp, the conversion energy provided is stored in the output filter inductor ^ and for the outer switches \ and s4, it is stored in the leakage inductance of the transformer. Since it is desirable to minimize the leakage inductance of the transformer 1 to minimize the parasitic ringing on the secondary side, the energy stored in the leakage inductance is relatively small, that is, less than the energy stored in the output filter inductor. Therefore, in the circuit of Fig. 4, the ZVS of the inner switch core and S3 can be easily achieved in the entire load range, and the outer switch \ and \ 2 "needs a magnetizing inductor LMC of an appropriate size because it is at a light load. Almost all the energy needed to generate the outer switching core and the ZVS condition of & is stored in the magnetized inductor. As explained in the patent application serial number filed on February 5, 2001 __ In a full-bridge circuit of a split transformer, the inductors and transformers have interchangeable roles. In particular, by adding a secondary winding to the coupled inductor, the coupled inductor can be used as a transformer to transfer power to the output connected to the secondary side. Circuit, and the magnetizing inductance of the transformer can be used as an inductor to store ZVS energy. Figures 8 and 9 show two such specific embodiments. Generally speaking, the operation of the circuit in Figures 8 and 9 is similar to The operation of the circuit in Figure 4 is the same. The main difference is that in the circuit of Figure 4, when the phase shift between the pair of outer and inner switches is 180 degrees, the maximum output voltage (voltage second product) is obtained When the phase shift is zero, the circuits in Figures 8 and 9 will produce the maximum output voltage (voltage second product) β because both need to invert the simple control signal in the voltage control loop to get the desired control loop. Characteristics, so the difference in the control characteristics of different specific embodiments will have a slight impact on the design of the control circuit. -17- This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 561680 A7 ___B7 V. Invention Explanation (15) As explained, in the circuit of the present invention, it is more difficult to achieve the ZVS of the switches of the external pair than the switches of the internal pair, because the energy that can achieve the ZVS condition is different in the two pairs of switches In general, in order to achieve zvs' this energy must be at least equal to the energy required to discharge the capacitor of the switch that is about to turn on and at the same time charge the capacitor of the switch that is turned off. At heavy load current, ZVS can mainly be stored in This is achieved by the leakage inductance of the transformer TR. When the load current decreases, the energy stored in the leakage inductance will also decrease, and the energy stored in the inductor Lc will increase. As for light load, Lc can be used to increase the load of the energy required for ZVS. In fact, where there is no load, this Lc will provide all the energy required to generate ZVS conditions. Therefore, if the value of Lc is chosen, With no load and maximum input voltage, zvs can be achieved, and zvs can be achieved over the entire load and input voltage range. If the capacitance of the transformer winding is ignored, the magnetizing inductance lmc required to achieve ZVS of the external switch in the implementation device of Figure 4 is L ^ c-ik ~ r 〇2) However, the inductance Le required to achieve the zvs of the inner switch in the implementation device of FIGS. 8 and 9 is
Lc^ 128C// (13) 其中C為相對應的開關對中之通過主開關的全部電容(寄 生及外部電容,若有的話)。 由圖5可知’流經磁化電感lmc的電流l會導致圖4之實施 裝置中之内部及外部對的開關之間的非對稱電流。顧名思 義,因為在此電(可由方程式(6)及(7)得到)中 -18- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公董) 561680 A7 _____— Β7 五、發明説明(16 ) ,所以内側開關S2及Ss所攜帶的電流總是高於外侧開關Si 及S4。可知在内部及外部對的開關之間的非對稱電流也會 出現在圖8及9的具體實施例中。此外,如果圖4、8以及9 之電路中的電流不安定是顯著的,以致於流經外侧開關& 及S4的電流丨2與流經内側開關\及\的電流L顯著不同時, 此兩對開關會選擇不同尺寸的開關,其會降低實施裝置的 成本,而不會犧牲電路效能。 應該要注意的是’在本發明的電路中,因為這些電路不 需要增加變壓器的漏電感,或大的外部電感,以儲存zvs 所需的能量,所以次側上的寄生振鈴會顯著降低。因為在 本發明的電路中之變壓器能以小的漏電感來完成,所以在 變壓器的漏電感與整流器的接面電容之間的次側振鈴可大 為降低。任何殘餘的寄生振鈴可藉由小(低電源)緩衝器電 路而降低。 最後,因為圖5中的電壓源VCB1= VIN/4及VCB2= VIN/4係分別 以電容CB1及CB2來實施,如圖4、8以及9所緣示,所以在開 始的瞬間之前,需要將這些電容到預先充電到Vin/4。顧名 思義’未預先充電之電容的電壓為零,其會在開始的期間 ’在變壓器的繞組上使電壓秒產生不安定的情形。此電壓 秒不安定會導致變壓器的飽和,其會在主側中產生損壞開 關的過多電流。圖1 〇繪示的是預先充電電路的一個例子。 圖10中的預先充電電路係以電阻RG1-RU來實施。應該要注 意的是’很多其他的預先充電電路之實施裝置可用於本發 明的任何電路。 •19- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 561680 A7 B7 五、發明説明(17 ) 應該要注意的是,以上詳細的敘述係用來說明本發明的 特定具體實施例,而不是侷限於此。在本發明的範圍内, 可做許多變化及修飾。此外,本發明不侷限於直流/直流轉 換器,而且也可應用到多位準直流/交流反相器。 -20- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)Lc ^ 128C // (13) where C is the total capacitance (parasitic and external capacitance, if any) of the corresponding switch pair through the main switch. It can be seen from Fig. 5 that the current l flowing through the magnetizing inductance lmc will cause an asymmetric current between the switches of the internal and external pairs in the implementation device of Fig. 4. As the name suggests, because in this electricity (available from equations (6) and (7)) -18- this paper size applies Chinese National Standard (CNS) A4 specifications (210 X 297 public directors) 561680 A7 _____ — Β7 V. Description of the invention (16), so the currents carried by the inner switches S2 and Ss are always higher than those of the outer switches Si and S4. It can be seen that asymmetric currents between the switches of the internal and external pairs also appear in the specific embodiments of Figs. In addition, if the current instability in the circuits of Figs. 4, 8 and 9 is so significant that the current flowing through the outer switches & and S4 is significantly different from the current L flowing through the inner switches \ and \, this The two pairs of switches will choose switches of different sizes, which will reduce the cost of implementing the device without sacrificing circuit performance. It should be noted that 'in the circuits of the present invention, since these circuits do not need to increase the leakage inductance of the transformer, or a large external inductance to store the energy required for zvs, the parasitic ringing on the secondary side is significantly reduced. Since the transformer in the circuit of the present invention can be completed with a small leakage inductance, the secondary ringing between the leakage inductance of the transformer and the interface capacitance of the rectifier can be greatly reduced. Any residual parasitic ringing can be reduced by small (low power) snubber circuits. Finally, because the voltage sources VCB1 = VIN / 4 and VCB2 = VIN / 4 in Figure 5 are implemented with capacitors CB1 and CB2, respectively, as shown in Figures 4, 8 and 9, you need to change the These capacitors are pre-charged to Vin / 4. As the name implies, the voltage of the capacitor which is not pre-charged is zero, which will cause the voltage to be unstable on the winding of the transformer during the initial period. This second-second instability can cause the transformer to saturate, which can cause excessive current in the primary side to damage the switch. Figure 10 shows an example of a pre-charge circuit. The pre-charging circuit in FIG. 10 is implemented with resistors RG1-RU. It should be noted that 'many other implementations of pre-charged circuits can be used with any circuit of the invention. • 19- This paper size is in accordance with Chinese National Standard (CNS) A4 (210X 297 mm) 561680 A7 B7 V. Description of the invention (17) It should be noted that the above detailed description is used to illustrate the specific and specific aspects of the present invention. The embodiment is not limited thereto. Many changes and modifications can be made within the scope of the invention. In addition, the present invention is not limited to a DC / DC converter, but can also be applied to a multi-bit quasi DC / AC inverter. -20- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
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US09/819,699 US6353547B1 (en) | 2000-08-31 | 2001-03-29 | Three-level soft-switched converters |
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Cited By (2)
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TWI551017B (en) * | 2013-04-19 | 2016-09-21 | 中心微電子德累斯頓股份公司 | System and method for regulating operation of non-symmetric boost based front end stage of rectifier with power factor correction, and system and method for reducing volume and losses of boost inductor in pfc rectifier |
TWI749933B (en) * | 2019-12-03 | 2021-12-11 | 萬國半導體國際有限合夥公司 | Switch circuit with reduced switch node ringing |
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2002
- 2002-03-15 TW TW91104924A patent/TW561680B/en not_active IP Right Cessation
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TWI551017B (en) * | 2013-04-19 | 2016-09-21 | 中心微電子德累斯頓股份公司 | System and method for regulating operation of non-symmetric boost based front end stage of rectifier with power factor correction, and system and method for reducing volume and losses of boost inductor in pfc rectifier |
TWI749933B (en) * | 2019-12-03 | 2021-12-11 | 萬國半導體國際有限合夥公司 | Switch circuit with reduced switch node ringing |
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