TWI262646B - High-efficiency bidirectional converter for power sources with great voltage diversity - Google Patents

High-efficiency bidirectional converter for power sources with great voltage diversity Download PDF

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TWI262646B
TWI262646B TW94123668A TW94123668A TWI262646B TW I262646 B TWI262646 B TW I262646B TW 94123668 A TW94123668 A TW 94123668A TW 94123668 A TW94123668 A TW 94123668A TW I262646 B TWI262646 B TW I262646B
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voltage
low
circuit
switch
inductor
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TW94123668A
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TW200703857A (en
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Rong-Jong Wai
Rou-Yong Duan
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Wai Zheng Zhong
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Abstract

The aim of this invention focuses on the development of a high-efficiency bidirectional converter for power sources with great voltage diversity. In traditional bidirectional converters, the circuit topology with transformer form is the common usual. Moreover, the soft-switching techniques including zero-voltage-switching (ZVS) or zero-current-switching (ZCS) are usually used for alleviating the corresponding switching losses. However, there are four and upward power semiconductor switches in these circuit schemes. By this way, it will result in the increase of production cost, and the degeneration of conversion efficiency. The coupled-inductor bidirectional scheme in the proposed converter only adopts three power semiconductor switches to accomplish the objective of bidirectional current control. Under the situation of non-isolation circuit topology, it still possesses the protection of electric safety for operators. Due to the characteristics of high step-up and step-down ratio, the battery module with low voltage could be injected into a high-voltage dc bus for the later utilization, e.g., high-voltage load, front-end of inverter. Since the techniques of voltage clamping, synchronous rectification and soft switching are manipulated in this circuit topology, and the corresponding device specifications are adequately performed, it can achieve the goal of high-efficiency bidirectional power conversion for power sources with great voltage diversity.

Description

1262646 九、發明說明: 【發明所屬之技術領域】本發明所涉及之技術領域包 含電力電子、直流/直流換流技術及能源科技之範疇,雖 然本發明料涉之技術領域廣泛,但其主要在於以蓄電池 作為辅助電源系統,將蓄電池電力昇壓至直流高壓電路系 統(或稱匯流排)’或是反向對#電池充t,以提供匯流排 緊急或容量調節所需之電力。 【先前技術】 a由於石油危機’引發能源不足問題,世界各地將潔淨 ^原開發為重要課題之—。應用潔淨能源發㈣統,一般 電池作為辅助電源系統’可有效降低潔淨能源之備 載合置,進而減少系統購置及供電成本。 ^灣電力供電穩定’停電機會少,傳統蓄電池的地位 電源’並不強調充電速度與效率。目前大樓設計, 至定度需求的場所,不斷電系統也只供應停電 人:油::”機併聯之短暫時間。然而新上市的油電混 大里銷售亚發揮運用其省油效果,將可暫時舒 用電池電力搭配引擎動Π;: =讀而快速地利 高效率雙向換流器為必備之電力;;壯〇取佳效率’因此 慣以串聯方式擴充蓄電二ί力=裂置。—般設計者習 戶 ’避免高昇壓比所面臨技術問題以及 ΓΪ重之缺點。電池串聯所產生的後遺症非常 夕取重要是各個電池的容量與壽命不-致’只要有-個 1262646 故障,勢必造成供電中斷。另一方面,為考量電池容量平 衡問題,必須全部串聯蓄電池同時更換,並且盡量使用同 一廠牌,俾使蓄電池容量可以匹配發揮。基本上,從蓄電 池的功率-電壓特性曲線上分析,並聯之蓄電池組並沒有 匹配問題,可以任意增加或減少數量,免除故障維修以及 電池管理問題。為此併聯組合之低壓電源,具高壓差比之 高效率雙向換流器更顯出其重要性。1262646 IX. Description of the Invention: TECHNICAL FIELD The technical field of the present invention includes the fields of power electronics, DC/DC converter technology, and energy technology. Although the present invention covers a wide range of technical fields, it mainly lies in The battery is used as an auxiliary power supply system to boost the battery power to a DC high voltage circuit system (or bus bar) or to reverse the # battery to provide the power required for bus emergency or capacity regulation. [Prior Art] a Due to the lack of energy caused by the oil crisis, cleanliness has been developed as an important issue in the world. The application of clean energy (four) systems and general batteries as auxiliary power systems can effectively reduce the backup and installation of clean energy, thereby reducing system acquisition and power supply costs. ^ Bay Power Supply Stable 'There will be fewer motor stops, and the status of conventional batteries' does not emphasize charging speed and efficiency. At present, the design of the building, to the location of the demand, the continuous power system is only available for power outages: oil:: "The short time of the machine parallel. However, the newly listed oil and electricity mixed sales in Asia to use its fuel-saving effect will be temporarily Use battery power to match the engine;: = read and quickly increase the efficiency of the two-way converter is the necessary power;; strong and good efficiency 'so it is used to expand the power storage in series 2 力 force = split. - General design The households 'avoid the technical problems and the disadvantages of the high boost ratio. The sequelae of the battery series is very important. The capacity and life of each battery are not - as long as there is a 1262646 failure, it will inevitably cause a power interruption. On the other hand, in order to consider the battery capacity balance problem, all series batteries must be replaced at the same time, and the same brand should be used as much as possible so that the battery capacity can be matched. Basically, from the power-voltage characteristic curve of the battery, parallel There is no matching problem with the battery pack, and the number can be increased or decreased arbitrarily, eliminating the problem of fault repair and battery management. This parallel combination of the low voltage power supply, high efficiency with high differential pressure than the bidirectional inverter its importance is even more evident.

習用雙向換流器如參考文獻[1]-[1〇],茲將其電壓規 格、容量、效率、電路架構及優缺點整理如表一所示。 表一、習用雙向換流器技術比較Conventional two-way converters, such as references [1]-[1〇], are listed in Table 1 for their voltage specifications, capacity, efficiency, circuit architecture, and advantages and disadvantages. Table 1, comparison of conventional two-way converter technology

參考 文獻 低壓 側 電壓 高壓 側 電壓 輸出 容量 最高轉換效 率 電路架構 優缺點比較 [1] [2] [3] [43 [5] [6] [7] [8] [9] [10]References Low Voltage Side Voltage High Voltage Side Voltage Output Capacity Maximum Conversion Efficiency Circuit Architecture Advantages and Disadvantages Comparison [1] [2] [3] [43 [5] [6] [7] [8] [9] [10]

24V24V

48V48V

100W 94% 半橋變壓器 優點 缺點100W 94% Half-Bridge Transformer Advantages Disadvantages

12V12V

5V5V

50V50V

36V36V

48V48V

24V24V

36V36V

10V10V

80V 50V80V 50V

380V380V

9V9V

360V360V

70V70V

72V72V

24V24V

340V340V

288V288V

100V100V

1.6kW1.6kW

20W20W

200W200W

120W120W

168W168W

60W60W

800W800W

1.6kW1.6kW

200W 92% 半橋變壓器 昇壓85% 降壓80% 優點 缺點 4昏 W.h 電容充電式缺k 輕載效率高 無法應用於重載 相移控制,具柔性切換 切換頻,漣浊高 架構簡單,不需電感 開關操作於作用區,效率 低 同步整流切換 昇壓91% 降壓87% 91% 電感+半橋 變壓器 電感+全橋 變壓器 不高 順向93% 逆向94%200W 92% Half-bridge transformer boost 85% step-down 80% Advantages and disadvantages 4 faint Wh Capacitor charging type lacking k Light load efficiency can not be applied to heavy-duty phase shift control, with flexible switching frequency, turbid high architecture is simple, no Inductor switch is required to operate in the active area, low efficiency, synchronous rectification, switching boost, 91%, step-down 87%, 91% inductance + half-bridge transformer inductance + full-bridge transformer, not high, 93%, reverse 94%

硯察表-所#技術比較,A部分_多為變壓器 ^62646 式,所使用功率半導體開關元件為四至九個,雖然部分使 用零電壓或零電流之柔性切換技術,然而電流流經太多開 關’將大幅提咼切換及導通之損失。另外一個問題是變壓 器並不適合接受大範圍變動之電壓,其原因為變動激磁電 流將易使鐵心飽和,以及變壓器需承受全部傳輸功率,必 須加大鐵心容量因應,倘若能夠克服上述問題,可望降低 成本以及提高轉換效率。 備註:參考文獻 [1] D. H. Xu? C. H. Zhao, and H. F. Fan, UA PWM plus phase-shift control bidirectional DC-DC converter;1 2 3 IEEE Trans. Power Electron., vol. 19? pp. 666-675, 2004.Inspect the table-to-the-technical comparison. Part A is mostly transformer type ^62646. The power semiconductor switching components used are four to nine. Although some use zero-voltage or zero-current flexible switching technology, the current flows through too many switches. 'The loss of switching and conduction will be greatly improved. Another problem is that the transformer is not suitable for accepting a wide range of voltage changes. The reason is that the variable excitation current will easily saturate the core, and the transformer must withstand the full transmission power. The core capacity must be increased. If the above problem can be overcome, it is expected to be reduced. Cost and increase conversion efficiency. Remarks: References [1] DH Xu? CH Zhao, and HF Fan, UA PWM plus phase-shift control bidirectional DC-DC converter; 1 2 3 IEEE Trans. Power Electron., vol. 19? pp. 666-675, 2004.

[2] F· Z· Peng, H. Li, G. J. Su,and J. S· Lawler,“A new ZVS bidirectional DC-DC converter for fuel cell and battery application;4 IEEE Trans, Power Electron,, vol. 19? pp. 54-65, 2004. 8 1 H. S. H. Chung,W. C· Chow,S· Y· R. Hui,and S. T· S· Lee,“Development of a switched-capacitor DC-DC converter with bidirectional power flow/5 6 IEEE Trans. Circuits Syst, vol. 47, pp. 1383-1389, 2000. 2 M. Jain,M· Daniele,and P. K· Jain,“A bidirectional DC-DC converter topology for low power application,” vol. 15, pp. 595-606, 2000. 3 H. L· Chan,K· W. E· Cheng,and D· Sutanto, “Bidirectional phase-shifted DC-DC converter,” Lei/m*·,vol. 35, pp. 523-524, 1999. 4 H. L. Chan,K· W. E. Cheng,and D· Sutanto, “ZCS-ZVS bi-directional phase-shifted DC-DC converter with extended load ranged IEE Proc. Electr. Power Appl, vol. 150, pp. 269-277, 2003. 5 G. Chen,Y· S· Lee,S. Y· R. Hui,D. H· Xu,and Y· S_ Wang,“Actively clamped bidirectional flyback converter?!>, IEEE Trans. Ind. Electron., vol. 47? pp. 770-779, 2000. 6 C. Y. Inaba,Y. Konishi,and M· Nakaoka,“High frequency PWM controlled step-up chopper type DC-DC power converters with reduced peak switch voltage stress;7 IEE Proc. Electr. Power Appl, vol. 151? pp. 47-52, 2004. 7 K. Wang,C. Y· Lin,L· Zhu,D. Qu,F. C. Lee,and J· S· Lai, “Bi-directional 1262646 DC to DC converters for fuel cell systems/5 in Proc. IEEE Workshop Power Electron. Transport, 1998, pp. 47-51.[2] F·Z· Peng, H. Li, GJ Su, and J. S. Lawler, “A new ZVS bidirectional DC-DC converter for fuel cell and battery application; 4 IEEE Trans, Power Electron,, vol. 19 Pp. 54-65, 2004. 8 1 HSH Chung, W. C. Chow, S. Y. R. Hui, and S. T. S. Lee, “Development of a switched-capacitor DC-DC converter with bidirectional Power flow/5 6 IEEE Trans. Circuits Syst, vol. 47, pp. 1383-1389, 2000. 2 M. Jain, M. Daniele, and P. K. Jain, “A bidirectional DC-DC converter topology for low power Application,” vol. 15, pp. 595-606, 2000. 3 H. L· Chan, K· W. E· Cheng, and D· Sutanto, “Bidirectional phase-shifted DC-DC converter,” Lei/m* ·, vol. 35, pp. 523-524, 1999. 4 HL Chan, K· WE Cheng, and D· Sutanto, “ZCS-ZVS bi-directional phase-shifted DC-DC converter with extended load ranged IEE Proc. Electr Power Appl, vol. 150, pp. 269-277, 2003. 5 G. Chen, Y·S· Lee, S. Y. R. Hui, D. H· Xu, and Y· S_ Wang, “Actively clamped Bidirectio Nal flyback converter?!>, IEEE Trans. Ind. Electron., vol. 47? pp. 770-779, 2000. 6 CY Inaba, Y. Konishi, and M. Nakaoka, "High frequency PWM controlled step-up chopper Type DC-DC power converters with reduced peak switch voltage stress;7 IEE Proc. Electr. Power Appl, vol. 151? pp. 47-52, 2004. 7 K. Wang, C. Y· Lin, L· Zhu, D Qu, FC Lee, and J. S. Lai, "Bi-directional 1262646 DC to DC converters for fuel cell systems/5 in Proc. IEEE Workshop Power Electron. Transport, 1998, pp. 47-51.

[10] Υ· M. Chen,Y· C. Liu,and F. Y· Wu,“Multi_input DC/DC converter based on the multiwinding transformer for renewable energy applications^ IEEE Trans. Ind. Appl, vol. 38? pp. 1096-1104, 2002. 本發明高效率高壓差比雙向換流器利用耦合電感之雙 向架構,僅使用三個開關即完成雙内電流之控制,加上本 架構有高昇、降壓比之特性,因此可使用低壓蓄電池即可 併入高壓匯流排,以利後級高壓負載或反流器前端使用。 換流器之切換技術,採用電壓箝制、同步整流與零電壓及 零電流方式,充分使用元件規格,使得本裝置具有高昇降 壓比、低切換損失與低導通損失之特點,可達到高效率高 壓差比雙向換流之目的。 【發明内容】 本發明所揭示之高效率高壓差比雙向換流器之架構, 如圖1所示,其中包含一低壓電路1〇1 :由一低壓開關&與 搞合電感7;—次側繞組心組成,藉由低壓開關&導通與截 止,儲存或釋放耦合電感乃一次側繞組b之能量;一中壓 電路102:由耦合電感卩二次側繞組心與一中壓電容^組 成’介於低壓電路101與高壓電路1〇4之間,主要是利用中 壓電容A提高昇壓比例或承受降壓時之部分電壓;一箝制 電路103 :由一箝制電感&、一箝制電容& 、一第一箝制 一極體、一第二箝制二極體/¾與一第三箝制二極體D3x 組成,主要是吸收耦合電感之漏感能量,保護低壓開關&, 1262646 並將吸收之此量釋放於輸出端;-高壓電路104 ··由-高 β硐關&、、且成,利用該開關提供路徑,達成高壓電路1〇4 ”低壓電路101雙向能量傳遞,此電壓一般又稱為高壓匯 流排;一降壓電路105:由一降壓開關&、一降壓電感心 及一降壓二極體乃2組成,負責釋放中壓電容&之放電回 路。 低疋電路1 〇 1與咼壓電路1 〇4分別代表兩種差距很大之 •直流電壓,雙向換流器之定義為兩者必為電源與負載且可 互換。換言之,若電源在高壓電路104,則負载為低壓電 路101忒負載可為直流設備或充電狀態之蓄電池。反之, ,電源在低壓電路101,代表昇壓後,將電源能量提升電位 至高壓電路104,提供至高壓直流匯流排負载,該低壓電 源可為蓄電池,亦或燃料電池、風力發電機與太陽能等潔 淨能源之直流發電裝置。總而言之,本裝置共有昇壓與降 • 壓兩種功能。身壓方面:低壓開關&導通時,低壓電路101 為電源,耦合電感一次侧繞組k為充電狀態,同時透過 耦合電感7;二次側繞組心,結合箝制電容〇1對中壓電容& 充電,當低壓開關截止時,耦合電感7;之漏感能量由箝 制電容q吸收;當漏感影響大幅減少後,耦合電感了兩側 . 繞組結合低壓電源電壓^以及中壓電容Q,經由高壓開關 供南壓電路104功率。降壓方面:高壓開關&導通時, 10 1262646 ,南墨電路1〇4為電源,高壓電路104對中麼電路102及低壓 電路101充電;高麼開關^截止時,柄合電仏能量全部 “由同V整*狀&之回路’由其—次側繞組&傳到低壓電 路101之負載,此時,中壓電容c2亦由低壓開關4與降壓 開關*S2提供回路,透過輕合電感(二次側繞組^與降壓電 感A對低壓電路101之負载供電。 ,、本·明之「鬲效率高壓差比雙向換流器」具有直流降 壓及直流昇壓兩種功能,因此共有兩組電路時序與工作模 式’以下將分為A、B兩部分詳述工作原理,為簡化電路 分析,所有開關元件及二極體導通壓降忽略不計。另外, 為使說明精簡易於瞭解,專有名詞不至於冗長,電路歸屬 圖號(如…電路1〇1)省略之,直接對照說明所屬圖式即可明 瞭。 A.降壓部分 南效率高壓差比雙向換流器降壓部分電路之工作原 理,如圖2所示之電路時序以及圖3電路工作模式,以下分 析將參照兩圖同時說明。將圖丨所示之高效率高壓差比雙 向換流器等效電路繪製如圖2(a)所示,由於此電路具有昇 壓及降壓兩種操作方式,為清楚標示電感電流之正極性流 向,將依據圖2(a)統一本發明所有圖說之電流正值與負值 之定義。此外,為便於說明電源及負載之應用,圖2高壓 11 1262646 - 侧並聯電容模擬電源或負載效應,低壓側使用蓄電池,兼 具電源與負載之功能。然而,因本裝置具備雙向能量傳遞 功能’其應用電源或負載種類不侷限於此。 模式一:時間[6〜高壓開關&導通一段時間 令間於〖=&時’高麼開關&導通一段時間,該開關 ‘通電流從南壓電路穿越中壓電路之中壓電容q及|馬合電 感7;二次侧繞組&,最後由低壓電路之耦合電感i 一次側 繞組Zp流出至低壓電路端。此時耦合f電感C一、二次側繞 組心及心相當於兩個電感串聯,並繞製於同一個鐵粉芯。 令搞合電感7;之一次側繞組b與二次側繞組心之匝數比為 # Λ^/Λ^,激磁電感為丄从以及漏電感為&,則搞合係數 介定義為 k = LMAh+LM) (1) 由於耦合電感採三明治疊繞方式,線圈耦合效果良好,而 且耦合電感之漏感能量對相對鐵粉芯容量小,只要做好電 壓箝制的功效,充分吸收漏感能量,對於系統電壓影響不 高,為簡化數學方料,便於理論分析,兹將麵合係數灸 定義為1。由於繞製同一鐵粉芯之電感與匝數平方成正比, 右Z紹及zM2分別代表耦合電感c之一、二次側繞組之激磁 電感,其關係式為LM1 ·· = M2 : W,因此,模式一中耦 合電感之激磁電感為兩電感串聯相加,可表示為 1262646 LM={l^N)2Lm={\ + \IN)2LM2 (2) 此模式激磁電流之平均值/ZMv與激磁電流爬升率分別為[10] Υ·M. Chen, Y·C. Liu, and F. Y· Wu, “Multi_input DC/DC converter based on the multiwinding transformer for renewable energy applications^ IEEE Trans. Ind. Appl, vol. 38? pp 1096-1104, 2002. The high efficiency high-voltage differential ratio bidirectional converter of the present invention utilizes a bidirectional architecture of coupled inductors to perform dual internal current control using only three switches, and the structure has high rise and fall ratio characteristics. Therefore, the high-voltage busbar can be incorporated into the high-voltage busbar for use in the high-voltage load of the rear stage or the front end of the inverter. The switching technology of the inverter is fully utilized by voltage clamping, synchronous rectification and zero voltage and zero current. The component specification makes the device have the characteristics of high buck-boost ratio, low switching loss and low conduction loss, and can achieve high efficiency and high-pressure difference ratio bidirectional commutation. [Invention] The high-efficiency high-pressure difference ratio bidirectional disclosed by the present invention The structure of the converter, as shown in Fig. 1, includes a low voltage circuit 1〇1: consisting of a low voltage switch & and an inductor 7; the secondary side winding core, with a low voltage switch & Passing through, storing or releasing the coupled inductor is the energy of the primary winding b; an intermediate voltage circuit 102: consisting of the coupled inductor 卩 secondary winding core and a medium voltage capacitor ^ between the low voltage circuit 101 and the high voltage circuit Between 1 and 4, mainly using medium voltage capacitor A to increase the boost ratio or to withstand a part of the voltage when stepping down; a clamping circuit 103: by a clamped inductor & a clamped capacitor & a first clamped one The pole body, a second clamp diode/3⁄4 and a third clamp diode D3x are mainly used to absorb the leakage inductance energy of the coupled inductor, protect the low voltage switch & 1262646 and release the absorbed amount to the output end. ; - high voltage circuit 104 · · by - high β & & , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , A step-down circuit 105 is composed of a step-down switch & a step-down inductor core and a step-down diode 2, and is responsible for discharging the discharge circuit of the medium voltage capacitor & The low-voltage circuit 1 〇 1 and the voltage-suppressing circuit 1 〇 4 represent two very large DC voltages, respectively, which are defined as power and load and are interchangeable. In other words, if the power source is in the high voltage circuit 104, the load is the low voltage circuit 101. The load can be a DC device or a state of charge battery. Conversely, after the low voltage circuit 101 represents the boosting, the power supply energy is boosted to the high voltage circuit 104 to provide a high voltage DC bus load, which may be a battery, or a fuel cell, a wind power generator, or a solar power source. DC power generation unit for clean energy. All in all, the unit has two functions: boost and drop. Body pressure: When the low-voltage switch & is turned on, the low-voltage circuit 101 is the power supply, and the coupled-inductor primary-side winding k is in a charged state, while passing through the coupled inductor 7; the secondary-side winding core, combined with the clamped capacitor 〇1 for the medium-voltage capacitor & Charging, when the low-voltage switch is turned off, the coupling inductance 7; the leakage inductance energy is absorbed by the clamp capacitor q; when the leakage inductance is greatly reduced, the coupling inductance is on both sides. The winding combines the low-voltage power supply voltage ^ and the medium-voltage capacitor Q, The power of the south voltage circuit 104 is supplied via a high voltage switch. Buck: high voltage switch & Turn on, 10 1262646, South ink circuit 1〇4 is the power supply, high voltage circuit 104 is connected to the circuit 102 and low voltage circuit 101; "The circuit of the same V-shape & is passed from its secondary winding & to the load of the low voltage circuit 101. At this time, the medium voltage capacitor c2 is also provided by the low voltage switch 4 and the buck switch *S2. Through the light-inductive inductance (secondary winding ^ and the step-down inductor A to supply the load of the low-voltage circuit 101. , Ben Ming's "鬲 efficiency high-voltage difference ratio bidirectional converter" has two functions of DC step-down and DC step-up. Therefore, there are two sets of circuit timing and working mode. 'The following will be divided into two parts, A and B. The working principle is detailed. To simplify the circuit analysis, all switching elements and diodes have a negated voltage drop. In addition, for the sake of simplicity Understand that the proper nouns are not too long, the circuit attribution figure number (such as ... circuit 1〇1) is omitted, and the direct description of the associated schema can be understood. A. The step-down part of the south efficiency high-pressure difference is lower than the bidirectional converter Working part of the voltage part circuit The circuit timing shown in Figure 2 and the circuit operation mode in Figure 3, the following analysis will be described with reference to the two figures. The high-efficiency high-voltage difference ratio bidirectional converter equivalent circuit shown in Figure 绘制 is shown in Figure 2 (a As shown in the figure, since the circuit has two operating modes of boosting and bucking, in order to clearly indicate the positive current flow of the inductor current, the definitions of positive and negative currents of all the figures of the present invention will be unified according to FIG. 2(a). In addition, for the convenience of power supply and load application, Figure 2 high voltage 11 1262646 - side shunt capacitor analog power supply or load effect, low voltage side battery, both power and load function. However, because the device has two-way energy transfer function ' The application power supply or load type is not limited to this. Mode 1: Time [6 ~ high voltage switch & turn on for a period of time between 〖=& when 'high' switch & turn on for a period of time, the switch 'pass current from south The voltage circuit passes through the medium voltage circuit, the voltage capacitor q and the | horse combined inductor 7; the secondary side winding &, and finally the low voltage circuit coupled inductor i primary side winding Zp flows out to the low voltage circuit end. The f-inductor C, the secondary side winding core and the heart are equivalent to two inductors connected in series, and wound in the same iron powder core. Let the inductance 7; the primary side winding b and the secondary side winding core The ratio is # Λ^/Λ^, the magnetizing inductance is 丄 and the leakage inductance is &, then the coupling factor is defined as k = LMAh+LM) (1) Since the coupled inductor adopts the sandwich winding method, the coil coupling effect is good. And the leakage inductance energy of the coupled inductor is small relative to the volume of the iron powder core. As long as the voltage clamping effect is achieved, the leakage energy is fully absorbed, and the influence on the system voltage is not high. In order to simplify the mathematical formula and facilitate the theoretical analysis, The coefficient of moxibustion is defined as 1. Since the inductance of the same iron powder core is proportional to the square of the turns, the right Z and zM2 represent the magnetizing inductance of one of the coupled inductors c and the secondary winding, respectively, and the relationship is LM1 ·· = M2 : W, so The magnetizing inductance of the coupled inductor in mode 1 is the series addition of the two inductors, which can be expressed as 1262646 LM={l^N)2Lm={\ + \IN)2LM2 (2) The average value of the excitation current in this mode/ZMv and excitation Current climb rate is

Ilmv 二 Pin IVh (3)Ilmv II Pin IVh (3)

Lm^lm Idt-VH -vC2 - VL (4) 若耦合電感7;之耦合係數左為1,則1船=心且_/^2=4。 為高壓電路之電壓1¾所提供功率;ve2表示中壓電容6:2之 電壓,由於電容值很大,故可視為定電壓。當高壓電路輸 入端所提供功率為定值時,高壓開關流過平均電流同為 ’其與高壓電路之電壓厂//之積為尸π。考慮高壓差比及 忽略損失情況下,激磁平均值電流與低壓側平均電流 zZv之比值約等同於降壓比(匕/心),是故電流匕^遠小於電 流。此外,從方程式(2)得知,電感值與匝數平方成正 比,因此耦合電感兩繞組串聯激磁,其激磁電感值高 於任何一組。激磁電感^^的跨壓扣除電壓ve2及匕後,所 剩無幾,再加上激磁電感ZM放大輕合電感獨立繞組之激 磁電感值,所以壓抑之數值,此數值代表流經高壓 開關4電流漣波成分可以有效降低。因此低平均電流與低 漣波電流波形,所產生導通損失自然較少,例如MOSFET 之導通損失為。令及分別為耦合電感一、二 次侧繞組心及心之電壓,則兩者關係式為 (5)Lm^lm Idt-VH -vC2 - VL (4) If the coupling inductance 7; the coupling coefficient to the left is 1, then 1 ship = heart and _ / ^ 2 = 4. The power is supplied to the voltage of the high voltage circuit 13⁄4; ve2 represents the voltage of the medium voltage capacitor of 6:2, which can be regarded as a constant voltage because of the large capacitance value. When the power supplied from the input end of the high voltage circuit is constant, the high voltage switch flows through the average current as the product of the voltage plant of the high voltage circuit. Considering the high-pressure difference ratio and ignoring the loss, the ratio of the excitation average current to the low-voltage average current zZv is approximately equal to the step-down ratio (匕/heart), so the current 匕^ is much smaller than the current. In addition, it is known from equation (2) that the inductance value is proportional to the square of the number of turns, so that the two windings of the coupled inductor are excited in series, and the magnitude of the magnetizing inductance is higher than any one. After the voltage of the magnetizing inductance ^^ is deducted from the voltage ve2 and 匕, there is little left, plus the magnetizing inductance ZM amplifies the value of the magnetizing inductance of the independent winding of the light-inductive inductor, so the value of the suppression, which represents the current flowing through the high-voltage switch 4 The wave component can be effectively reduced. Therefore, the low average current and low chopping current waveforms naturally produce less conduction losses, such as the conduction loss of the MOSFET. Let and be the voltage of the coupled inductor first and second side windings and the heart, then the relationship between the two is (5)

VLS 丨 VLP 二 N 1262646 - 因此,高壓電路之電壓心可表示成 ’ V^^vls+Vlp+VlHN + 1)Vl^Vc2+Vl ⑹ 在此模式中,麵合電感7;-、二次側繞組心及々同時 激磁,兩繞組電流^與。,同方向相等(亦等於且持 續上昇,同時供應給低壓電路輸出端。此外降壓電路之電 流b由降壓電感Z2,透過降廢二極體A導通所提供回路, 放電給低壓電路之蓄電池,因此該電感之電愿%=匕,且 >蓄電池充電t流為f 。再者,觀察低壓開關^為截止 狀態,其跨壓為 VDSl^yL+yLP ⑺ 模式二:時間[W2];高壓開_觸發訊號截止瞬間 高壓開關&觸發訊號截止瞬間(叫),輕合電感^兩侧 繞組LP及心失去高壓開關4所提供激磁的動力,但由於 一、二次側繞組之漏感^與々2仍有能量釋放,其電流無 1法瞬間改變,以致二次側繞組v電流b透過降壓二極逢 /¾及IV疋開關&飛輪二極體路徑續流,但其值逐漸減少。 此時該開關兩端為零電壓,等待下一個模式零電壓切換 (Zero Voltage Switching,ZVS)。依據磁通不滅定律,由於 二次側繞組釋放電流路徑(高壓開關4)已中斷,儲存鐵粉 芯内的能量將只剩一次側繞組回路,其電流^透過低壓開 關&之飛輪二極體路徑,釋放給低壓側蓄電池並逐漸增 14 1262646 加。此時該開關兩端亦為零電壓,等待下一個模式同步整 流導通。 模式三:時間[纟2〜6];低壓開關及降壓開關&觸發訊號 導通瞬間 前一模式已經形成低壓開關&及降壓開關&之飛輪二 極體導通’本模式開始直接觸發導通,元件電流特性,保 持先前狀態持續改變。前者為同步整流,對低壓電路具高 流入電流而言,同步整流技術可大幅降低飛輪二極體之導 通損失’後者開關零電壓導通,無切換損失。本模式止於 耦合電感7;之二次側繞組電流。降為零。 模式四:時間1¾〜〖4];中壓電容(^放電至低壓電路 本模式始於激磁能量由耗合電感& 一次側繞組電流 心,全部釋放於低壓電路,二次側繞組電流。由零上昇 為正,表示中壓電容&開始放電,其路徑係經由降壓開關 &、降壓電感A到低壓電路對蓄電池充電,然後透過低壓 開關之飛輪一極體回到二次側繞組心的極性點端。此時 降壓電感A為儲能狀態,同時其電壓々2可表示為 VL2 =VC2 ⑻ 此時二次側繞組心電流b包括激磁電流以及來自高壓 側的感應電流^ ’經低壓開關\對低壓電路之蓄電池充電, 该電壓為,一次側繞組電流若忽略開關交越的空 1262646 白時間(Lockout Time),令高壓開關&責任週期伽以印⑹ 為4,且低壓開關&與降壓開關&責任週期同為則 1 3 (9) 降壓電感12電壓vZ2介於匕、〜及Vc2三電壓源之間,其存 在之意義為三電壓源必須串聯一電流源始成一回路,以承 X其中之壓差。由於模式一時,降壓電感A電壓々2等於 低壓電路之蓄電池電壓匕,依據伏_秒平衡(v〇it_sec〇nd Balance),可以得到模式四時電壓μ為 VL2=1Ld3^l (1()) 將方程式(1G)及二次側繞組電壓〜=7^之_代入方程 式(8)可以得到 vc2 = (#+i+d3/岣)fz ⑴) 本模式—人侧繞組心之電壓vLp等於低壓電路之蓄電池電 壓^,因此可以再依據伏·秒平衡(v〇lt_sec〇nd如丨⑽⑶), 反推可得模式一時之電壓化户為 VLP=VL^\i ^2) 將方程式(9)、方程式(11)及方程式幻代入方程式,且 令降壓比例定義為Gn,則其值可表示為 (13) 16 1 h N(l^d3) + \ 利用方程式(13)繪製不同匝數比#時,其降壓比例^^^與高 壓開關&責任週期4之關係曲線,如圖4所示。由責任週 1262646 期4可以瞭解,^固定情況下, ^ ^ , 取巧降壓比(代表低壓側 可經由調節輸出之最高電壓 5Gri/况3=〇的位置,其值可表示如下: 3 (max)VLS 丨VLP II N 1262646 - Therefore, the voltage core of the high voltage circuit can be expressed as 'V^^vls+Vlp+VlHN + 1)Vl^Vc2+Vl (6) In this mode, the face inductance 7;-, secondary side The winding core and the 々 are simultaneously excited, and the two winding currents are combined. The same direction is equal (also equal to and continues to rise, and is supplied to the output of the low-voltage circuit. In addition, the current b of the step-down circuit is provided by the step-down inductor Z2, which is supplied through the circuit of the reduced-discharge diode A, and discharged to the battery of the low-voltage circuit. Therefore, the electric current of the inductor is %=匕, and > the battery charging t flow is f. Furthermore, the low voltage switch ^ is observed to be in an off state, and its cross voltage is VDSl^yL+yLP (7) mode two: time [W2]; High voltage on_trigger signal cutoff moment high voltage switch & trigger signal cutoff instant (called), light combined inductance ^ both sides of the winding LP and the heart loses the excitation power provided by the high voltage switch 4, but due to the leakage inductance of the primary and secondary windings ^ and 々2 still have energy release, and the current does not change instantaneously in one method, so that the secondary side winding v current b passes through the buck diode/3⁄4 and IV疋 switch & flywheel diode path freewheel, but its value Gradually decrease. At this time, the switch has zero voltage at both ends, waiting for the next mode Zero Voltage Switching (ZVS). According to the law of flux incompetence, since the secondary side winding release current path (high voltage switch 4) has been interrupted, Storage of iron powder The energy in the core will only have one primary winding loop left, and its current will pass through the flywheel diode path of the low voltage switch & the release to the low side battery and gradually increase by 14 1262646. At this time, the switch is also zero voltage at both ends. Wait for the next mode to synchronously rectify conduction. Mode 3: Time [纟2~6]; Low-voltage switch and buck switch & Trigger signal turn-on moment The previous mode has formed a low-voltage switch & buck switch & flywheel diode Body conduction 'this mode starts to directly trigger conduction, component current characteristics, keep the previous state continuously changing. The former is synchronous rectification, and the high-inrush current for low-voltage circuits, the synchronous rectification technology can greatly reduce the conduction loss of the flywheel diode' The switch has zero voltage conduction and no switching loss. This mode stops at the coupled inductor 7; the secondary winding current is reduced to zero. Mode 4: Time 13⁄4~〖4]; Medium Voltage Capacitor (^ Discharge to Low Voltage Circuit This Mode Starting from the excitation energy by the inductor and the primary winding current, all released in the low-voltage circuit, the secondary winding current. From zero to positive, indicating medium voltage The capacitor & begins to discharge, the path is charged to the battery via the buck switch & buck inductor A to the low voltage circuit, and then returns to the polarity end of the secondary winding core through the flywheel of the low voltage switch. The step-down inductor A is in the state of energy storage, and its voltage 々2 can be expressed as VL2 = VC2 (8) At this time, the secondary side winding current b includes the excitation current and the induced current from the high voltage side ^ 'via the low voltage switch \ for the low voltage circuit When the battery is charged, the voltage is, if the primary winding current ignores the gap of the switch, the empty 1262646 white time (Lockout Time), so that the high voltage switch & duty cycle is printed with (6) 4, and the low voltage switch & and the buck switch & The duty cycle is the same as 1 3 (9) The step-down inductor 12 voltage vZ2 is between the three voltage sources of 匕, ~ and Vc2. The meaning of the existence is that the three voltage sources must be connected in series with a current source to form a loop. The pressure difference among them. Since the mode is low, the step-down inductor A voltage 々2 is equal to the battery voltage 低压 of the low-voltage circuit. According to the volt-second balance (v〇it_sec〇nd Balance), the mode four-time voltage μ can be obtained as VL2=1Ld3^l (1() Substituting the equation (1G) and the secondary winding voltage ~=7^ into equation (8) can be obtained vc2 = (#+i+d3/岣)fz (1)) This mode - the voltage of the human side winding vLp is equal to The battery voltage of the low-voltage circuit is ^, so it can be based on the volt-second balance (v〇lt_sec〇nd such as 丨(10)(3)), and the voltage of the available mode is VLP=VL^\i ^2). ), Equation (11) and the equation illusion into the equation, and let the step-down ratio be defined as Gn, then its value can be expressed as (13) 16 1 h N(l^d3) + \ Use equation (13) to draw different parameters When compared with #, its buck ratio ^^^ is related to the high voltage switch & duty cycle 4, as shown in Figure 4. It can be understood from Responsibility Week 1262646 Period 4, ^ ^, the deceleration ratio (representing the low voltage side can be adjusted by the highest voltage of the output 5Gri / condition 3 = 〇 position, the value can be expressed as follows: 3 (max )

^ ^ 7 發生在責任週期 d (Η) _亦代表高㈣關^最高責任週期。觀察圖4,小於 ‘)之責任週期區域,責任週期越大,低壓電路之輸出 電壓將會升高’但若超過‘叫部分,低壓電路之輸出電 β、反ik之下&因此超過&_)部份之責任週期將無法調 節控制低壓電路之輸出電壓。 將方程式⑼代人方程式⑺可以得到低壓開關⑯端 所承受之跨壓以及箝制電容ς電壓Vci VDS\ - VC1 - /(15) 依據方程式(15)分析,是圖4⑷降壓比例〜曲線的 斜率。當降壓開關.¾電流㈣始大於降壓電感電流^時, 降壓二極體A截止以及第二箝制二極體Α導通釋放箝制 電容q之電流/C1,此時高壓開關4兩端之電壓由^降至 4 -vL2+Fl。 模式五:時間[~〜匕];低壓開關&及降壓開關&觸發訊號 同時截止 此時原先流過降壓開關&的電流會對該開關之寄生電 容充電’由於v仍3+v如+Vd2=^之電壓關係,電壓^幻上 17 1262646 幵’另外兩 流〖L2導通, 降壓電感12為持續電 依據方程式(12)可以 ’另外兩者電壓勢必下降。首先, k導通,降壓二極體必須導通。 求出降壓二極體A兩端在模式一截 截止時的跨壓為 、 (16) VD2 ~ 依據方程式(14)已經限制責任週期a之最大值,將該最大 值代入方程式(16),即可設計降壓二極體a之耐壓規格。 依據圖4所*,大部分介於ορό·?之間,目此該降壓 •二極體Ζ)2承受最高電愿約為三倍蓄電池電壓,因此可使用 低£低‘通彳貝失之蕭基二極體。其次,二次側繞組漏感 ‘ Ζ*2以及箝制電感勾皆必須保持續流,其導通路徑必須強 迫高壓開關&之飛輪二極體導通,由於降壓二極體A為快 速‘通之蕭基一極體,此時與高壓開關&兩者跨壓電壓互 相箝制,一長一消,當降壓開關&截止時,高壓開關&之 爪輪一極體亦九成導通,此時箝制電感A釋放電壓為高壓 之汾=匕-VC1,因此該電流k迅速下降。由於漏感 仍有殘存爿b里持續釋放,耦合電感4兩侧繞組之感應電流 A及Ϊ·2無法立即截止,但快速下降。 模式六:時間[匕〜(6];高壓開關&觸發訊號導通 當咼壓開關4之飛輪二極體導通時,開關兩端跨壓降 為零,此時觸發訊號導通,其波形具有零電壓切換之效果。 由於雨一模式各元件電流續流模式已經到末段,加上高塵 開關4給予耦合電感7;激磁路徑,二次側繞組心將再接受 18 1262646 激磁,一次側繞組電流b將逐漸減少。因受二次側繞組 心激磁影響,一次側繞組非極性點電壓為正,低壓開關& 之飛輪二極體截止,一次側繞組電流^開始對低壓開關& 之寄生電容充電。由於低壓開關&之寄生電容比一般高壓 開關大,因此兩端跨壓上昇時,所需充電電流較高,其充 電電流包括h、匕况2及G。箝制電感勾釋放電流完畢後, 第二箝制二極體&截止,其逆向恢復電流將反向流至箝制 電感A,後續會造成兩者電壓震盪,因此加入第三箝制二 極體Dk可以有效限制第二箝制二極體乃3之電壓。當低壓 開關A電壓等於箝制電容q之電壓Μ時,本模式結 束。 模式七:時間h〜第一箝制二極體乃丨導通 低壓開關\電壓高於箝制電容q之電壓Μ時,第一箝 制一極體Α導通,將先前充電至寄生電容之電流導入箝制 電奋q,由於該電容設計容量很大,因此電壓斤1幾乎無 連波,低壓開關&跨壓因此得以限制,並於模式四所提供 路控將能量傳給低壓電路,其電壓如方程式(ls)所示,該 方私式電壓與責任週期4有比例關係,因此可以採用低 I低導通知失之MOSFET開關。當漏感能量釋放完畢時, 第、箝制一極體Q截止,表示感應電流纟1與丨2降為零,耦合 電感2;、一次側繞組心與心同樣串聯接受高壓電路之相 19 1262646 Β·昇壓部分 回效率问壓差比雙向換流器昇壓部分電路之工作原 :里,如圖5及圖6所示之電路時序以及工作模式。雙向換流 為在處理昇壓功能時,降壓電路元件不需工作,如降壓電 感12、降壓二極體句及降壓開關&,圖6電路工作模式將 降壓電路部分以虛線表示。以下分析將參照兩圖同時說 明。 杈式一:時間〜6];低壓開關4導通一段時間 時間於時,低壓開關4已導通一段時間,耦合電 感7;—次側繞組心從低壓電路之蓄電池抽出電流激磁,其 一次側繞組心之電流ζ·Ιρ為一次側感應電流&及激磁電流 所組成。一次側感應電流4來自理想變壓器感應至二 次側繞組4之二次側感應電流ζ·2 ;而激磁電流匕^丨為激磁 電感Ζ紹所產生,主要於低壓開關Α導通時儲存能量,當 低壓開關&截止後再傳遞給二次側繞組心。此時,上述二 者電流46全部流經低壓開關A,其中二次側繞組 As感應極性點為正電壓,串聯箝制電容〇1之電壓v ,經 由掛制電感4 ’以及低壓開關4及弟二籍制二極體形成 20 1262646 ‘ι回路,對中壓電容q充電。前面的降壓部分對耦合係 數b已、域明内容並令其值為1,㈣箝制電感Ζι刻意設 計小電感,其電流t等於二次側繞組電流‘屬於小電流, 更因二次侧繞組漏感心2影響,限制電流變化率,因此二 次側繞組電壓义2幾乎可以忽略不計,是故中壓電容之電 壓VC2可計算出^ ^ 7 occurs in the responsibility cycle d (Η) _ also represents high (four) off ^ maximum responsibility cycle. Observe Figure 4, less than the responsibility cycle area of '), the greater the duty cycle, the output voltage of the low-voltage circuit will rise 'but if it exceeds the 'called part, the output voltage of the low-voltage circuit is below β, anti-ik under & therefore exceed &The;_) part of the duty cycle will not be able to regulate the output voltage of the low voltage circuit. Equation (9) can be obtained by equation (7) to obtain the voltage across the end of the low-voltage switch 16 and the clamp capacitor ς voltage Vci VDS\ - VC1 - /(15) According to equation (15), it is the slope of the step-down ratio curve of Figure 4(4). . When the buck switch .3⁄4 current (4) is greater than the buck inductor current ^, the buck diode A is turned off and the second clamp diode is turned on to release the current of the clamp capacitor q / C1, at which time the high voltage switch 4 is The voltage is reduced from ^ to 4 -vL2+Fl. Mode 5: Time [~~匕]; Low-voltage switch & buck switch & trigger signal simultaneously cut off the current flowing through the buck switch & the current will charge the parasitic capacitance of the switch 'because v is still 3+ v, such as the voltage relationship of +Vd2=^, voltage ^ illusion on 17 1262646 幵 'the other two flows 〖L2 conduction, the step-down inductor 12 is continuous power according to equation (12) can be 'other voltages are bound to fall. First, k is turned on and the step-down diode must be turned on. Find the voltage across the two ends of the step-down diode A at the end of the mode cutoff, (16) VD2 ~ The maximum value of the duty cycle a has been limited according to equation (14), and the maximum value is substituted into equation (16). The pressure specification of the step-down diode a can be designed. According to Figure 4, most of them are between ορό·?, so the buck•diodeΖ2 can withstand the highest battery voltage of about three times the battery voltage, so it can be used low and low The Xiaoji diode. Secondly, the secondary side winding leakage inductance 'Ζ*2 and the clamped inductance hook must be kept continuous, and the conduction path must force the high-voltage switch & flywheel diode to conduct, because the step-down diode A is fast Xiaoji one pole, at this time with the high voltage switch & both voltage across the voltage clamped each other, a long cut, when the buck switch & cut off, the high voltage switch & claw wheel one pole is also turned on, At this time, the clamping inductor A releases the voltage to the high voltage 汾=匕-VC1, so the current k drops rapidly. Since the leakage inductance remains in the residual 爿b, the induced currents A and Ϊ·2 of the windings on both sides of the coupled inductor 4 cannot be cut off immediately, but fall rapidly. Mode 6: Time [匕~(6]; High-voltage switch & trigger signal conduction When the flywheel diode of the pressure switch 4 is turned on, the voltage across the switch is zero, and the trigger signal is turned on, and the waveform has zero. The effect of voltage switching. Since the current freewheeling mode of each component of the rain mode has reached the end, plus the high dust switch 4 gives the coupled inductor 7; the excitation path, the secondary winding core will accept 18 1262646 excitation, primary winding current b will gradually decrease. Due to the influence of the secondary side winding core excitation, the primary side winding non-polar point voltage is positive, the low side switch & flywheel diode is cut off, the primary side winding current ^ starts to the low voltage switch & parasitic capacitance Charging. Since the parasitic capacitance of the low-voltage switch & is larger than that of the general high-voltage switch, the required charging current is higher when the voltage across the two terminals rises, and the charging current includes h, condition 2, and G. After the current is released by the clamped inductor hook , the second clamp diode & cutoff, its reverse recovery current will flow back to the clamp inductor A, which will cause the voltage oscillation of the two, so the addition of the third clamp diode Dk can be effective The second clamp diode is the voltage of 3. When the voltage of the low voltage switch A is equal to the voltage of the clamp capacitor q, the mode ends. Mode 7: Time h~ The first clamp diode is the low voltage switch and the voltage is high. When the voltage of the capacitor q is clamped, the first clamped one pole is turned on, and the current previously charged to the parasitic capacitor is introduced into the clamped electric power. Since the capacitor has a large design capacity, the voltage has almost no wave, low voltage. The switch & cross-voltage is thus limited, and the path provided in mode 4 transmits energy to the low-voltage circuit. The voltage is as shown in equation (ls), and the private voltage is proportional to the duty cycle 4, so it can be used. The low I low-conductance notification loses the MOSFET switch. When the leakage inductance energy is released, the first clamping body Q is turned off, indicating that the induced currents 纟1 and 丨2 are reduced to zero, the coupled inductor 2; the primary side winding core and the heart The phase of the high-voltage circuit is also connected in series. 19 1262646 Β · Boost part of the efficiency of the voltage difference than the bi-directional converter step-up part of the circuit: in, as shown in Figure 5 and Figure 6 circuit timing and mode of operation. When the flow is processed, the step-down circuit components do not need to work, such as the buck inductor 12, the buck diode sentence, and the buck switch & the circuit operation mode of Fig. 6 shows the step-down circuit portion as a broken line. The following analysis will be explained with reference to the two figures. 杈 Type 1: Time ~ 6]; Low-voltage switch 4 is turned on for a period of time, the low-voltage switch 4 has been turned on for a period of time, coupled with the inductor 7; - the secondary side winding from the battery of the low-voltage circuit The current is excited, and the current ζ·Ιρ of the primary winding core is composed of the primary side induced current & and the exciting current. The primary side induced current 4 is derived from the secondary transformer induced current of the secondary transformer 4 from the ideal transformer. 2; and the excitation current 匕^丨 is generated by the excitation inductance, mainly stored when the low-voltage switch Α is turned on, and then transmitted to the secondary winding core when the low-voltage switch & At this time, the currents 46 of the two currents all flow through the low voltage switch A, wherein the secondary side winding As senses the polarity point to be a positive voltage, and the voltage v of the capacitor 〇1 is clamped in series, via the hanging inductor 4' and the low voltage switch 4 and the second The system diode forms 20 1262646 'ι loop, charging the medium voltage capacitor q. The front step-down part has a coupling coefficient b, the domain content and its value is 1. (4) The clamp inductor Ζι deliberately designs a small inductor whose current t is equal to the secondary side winding current 'belongs to a small current, and more because of the secondary winding The leakage sensation 2 affects and limits the current change rate, so the secondary side winding voltage 2 is almost negligible, so the voltage of the medium voltage capacitor VC2 can be calculated.

vC2=NVl+vci (17) U此期間’低壓開關&電流‘等於㈤·+ζ·2,由於激磁 電仙為電感儲存能量,電流由小逐漸上升,波形斜率 為正1關導通瞬間,中壓電容c2充電電流匕為一週期之 峰值,並隨該電容電壓逐漸上升而下降,電流丨2為一次侧 感應電流^所產生,其關係式為/1=外,電流4波形斜率為 負。因此一次侧繞組之電流‘為^與!·说丨兩者之和,又 兩波形斜率互補,造成低壓開關&導通期間,電流b趨近 方波,同理一次侧繞組電流k加上二次側感應電流Μ高壓 小電流)等於低壓開關&電流,其波形亦接近方波。方 波之電抓波开> 代表思義有兩點··第一點,流經低壓開關^ 電流波形之漣波成分低,而開關導通損失與電流平方成正 比,假設在相同平均電流下,方波電流之平方和小於三角 波電流平方和,因此方波電流所造成低壓開關 '之導通損 失遠低於高漣波電流。第二點,電流^與電流兩者波 21 1262646 形斜率相反’可以接受更低之激磁電感,代表輕合電 感7;—次側繞組b匝數及鐵心容量可大幅減少,_次側妗 組高電流所造成之銅損及鐵心損亦同步降低。 模式二··時間Ui〜Q];低壓開關觸發訊號戴止 低壓開關&觸發訊號於ί = ^時截止,受限於耦合電感了 一二次側繞組之漏感能量釋放影響,耦合電咸一 _ ^ ^ 繞組電流Lp與b ’續流並向低壓開關之寄生電容充電, 鲁 ϋ此開關兩端電壓¥决速上昇,截止中的高麈開關^兩 端電壓V瓜3亦開始下降。當低壓開關&兩端電壓ν^ι等於 痛制電容G電壓VC1時,本模式結束。 杈式二··時間[G〜耦合電感二次側繞組電流一轉向 低壓開關&兩端電壓1;瓜1高於箝制電容q電壓化1時, 第一箝制二極體/^導通,對箝制電容q充電,吸收一次側 鲁繞組Z〆漏感&所釋放能量,由於該電容為—具高頻響 f佳之高容量電容,藉以快速導引前述電流“至箝制; 谷q 口此其電壓vcl可視為一穩定之低漣波直流電壓, 以確保開關承受電愿之最大值。此外,第-箝制二極體A :、貝為f夬速$通_極體,其耐壓規格同於低壓開關^,所 以二低/肖耗功率與低導通電壓之蕭基二極體為最佳選擇。 ’ 〃+觀祭此核式的電路特性,如果激磁磁通於連續,箝制 .電谷Cl即疋傳統昇壓轉換器(Boost Converter)之輸出電 1262646 壓,因此箝制電容電壓vcl與低壓電路之電壓&關係為 VC1 =^L +VLP =VDSl (18) 由於二次侧繞組心僅有高壓感應電流&,遠小於一次 侧繞組電流ζ·ΖΡ,因此在二次側繞組漏感能量較一次側 繞組釋放快速’一次侧繞組漏感k則因存在高電流,釋 放速度較慢,,加上補充箝制電容ς於模式一下降之電壓, 續流時間較長。高容量之箝制電容ς可以充分吸收一次側 繞組漏感之能量’从汉丹电澄Uj以在模式丨卩、/主叫哪 導通時,釋放給中壓電容c2,是以可以箝制漏感能量並义 入昇壓。二次側繞組電流b於時間6時降為零,一次側爲 磁電流/^^釋放能量,透過磁路至二次側,電流L緩慢」 昇流出非極性點。二次側繞組電流L,將迫使^開關! 寄生電容電壓、,放電至高壓電路,逐漸降至零並導由 高壓開關4之飛輪二極體。 模式::.時叫〜,4];高壓開關4觸發訊號導通 咼壓開關&之飛輪二極體導诵主 遐令通¥,施以觸發訊號,今 成同步整流以降低導通損失。,士 心谓大此日寸畜電池電壓、- 、%〇組電壓VLP、一次侧繞組電壓 _ 电與中壓電容電壓” 聯,以低電流型式對高壓電容C奋 c //充電。激磁能量則Λ 磁通不滅定律,在漏感能量耗 饥士 k俊輕合電感7;仍會习vC2=NVl+vci (17) U During this period, 'low-voltage switch & current' is equal to (5)·+ζ·2. Since the excitation charge stores energy for the inductor, the current gradually rises from small to small, and the slope of the waveform is positive 1 turn-on instant. The charging current c2 of the medium voltage capacitor c is the peak value of one cycle, and decreases as the capacitor voltage gradually rises. The current 丨2 is generated by the primary side induced current ^, and the relationship is /1=external, and the slope of the current 4 waveform is negative. Therefore, the current of the primary winding is 'the sum of the two and the sum of the two, and the slopes of the two waveforms are complementary, causing the low-voltage switch & during the conduction period, the current b approaches the square wave, and the primary winding current k plus two The secondary side induced current Μ high voltage small current) is equal to the low voltage switch & current, and its waveform is also close to the square wave. The square wave's electric grab wave opens > represents two points. · The first point, flowing through the low voltage switch ^ The current waveform has a low chopping component, and the switch conduction loss is proportional to the square of the current, assuming the same average current. The square sum of the square wave current is smaller than the square sum of the triangular wave currents, so the conduction loss of the low voltage switch caused by the square wave current is much lower than the high chopping current. The second point, the current ^ and the current both wave 21 1262646 shape slope is opposite 'can accept a lower magnetizing inductance, representing the light coupling inductance 7; the number of secondary windings b and the core capacity can be greatly reduced, _ secondary side group The copper loss and core loss caused by high current are also reduced simultaneously. Mode 2··Time Ui~Q]; low-voltage switch trigger signal wear-stop low-voltage switch & trigger signal is off at ί = ^, limited by the coupling inductance of a secondary side winding leakage energy release effect, coupling electric salt A _ ^ ^ winding current Lp and b ' freewheeling and charging the parasitic capacitance of the low-voltage switch, the voltage across the switch is ramped up, and the voltage across the high-turn switch ^ V is also starting to drop. This mode ends when the low voltage switch & voltage ν^ι is equal to the painful capacitor G voltage VC1.杈式二··Time [G~coupled inductor secondary winding current one turns to low voltage switch & voltage at both ends 1; melon 1 is higher than clamp capacitor q voltage, 1 first clamp diode / ^ conduction, right The clamp capacitor q is charged, absorbing the leakage energy of the primary side winding and the leakage energy. Since the capacitor is a high-capacity capacitor with high frequency, the current is quickly guided to the clamp. The voltage vcl can be regarded as a stable low chopping DC voltage to ensure that the switch can withstand the maximum value of the switch. In addition, the first clamp diode A:, the shell is f idle, the pass_pole body, and the withstand voltage specifications are the same. For low-voltage switch ^, so the low-shear / Xiao power consumption and low-on-voltage of the Xiaoji diode is the best choice. ' 〃 + view the nuclear circuit characteristics, if the magnetic flux is continuous, clamped. Cl is the output of the traditional boost converter (Boost Converter), which is 1262646, so the voltage of the clamp capacitor voltage vcl and the low voltage circuit is & VC1 = ^L + VLP = VDSl (18) due to the secondary winding core only There is a high-voltage induced current &, which is much smaller than the primary winding current ζ·ΖΡ, The leakage inductance energy of the secondary side winding is faster than that of the primary side winding. The leakage inductance of the primary side winding is due to the presence of a high current, and the release speed is slow, and the voltage of the complementary clamp capacitor is reduced by the mode one, the freewheeling time. Longer. The high-capacity clamp capacitor ς can fully absorb the energy of the leakage inductance of the primary winding. 'From Handan Electric Cheng Uj, when the mode is 丨卩, / when the caller is turned on, it is released to the medium voltage capacitor c2. The leakage inductance energy is clamped and boosted. The secondary side winding current b drops to zero at time 6 and the primary side is magnetic current / ^ ^ release energy, through the magnetic circuit to the secondary side, the current L slowly rises and flows out Polar point. The secondary side winding current L will force the ^ switch! The parasitic capacitance voltage, discharged to the high voltage circuit, gradually drops to zero and is guided by the flywheel diode of the high voltage switch 4. Mode::.called ~, 4]; high voltage switch 4 trigger signal conduction 咼 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关 开关, the heart of the heart is said that the battery voltage of the day, -, % 〇 group voltage VLP, primary side winding voltage _ electric and medium voltage capacitor voltage", with low current type on the high voltage capacitor C f / c. The energy is Λ the law of magnetic flux immortality, the energy consumption in the leakage sense is k-kun light and inductance 7; still will learn

段時間之持續在一、-々伽婊4 A —側繞組電路提供電流,-⑸ 1262646 1箝制電合q充電,二次側繞組則對高壓電路釋放電 流。於模式四中期,中壓電容c2電壓〜2因持續放電下降, 同時箝制電容Cl電壓長期充電而上昇,第一箝制二極 體A逆偏截止。此時,—次側繞組電流仏等於二次側繞組 電流b,同時結束本模式。 模式五日守間[心〜纟d ,麵合電感7;兩侧繞組相等電流對高 壓電路放電The duration of the period is one, - 々 婊 4 A - the side winding circuit provides current, - (5) 1262646 1 clamps the electric charge q charge, and the secondary side winding discharges current to the high voltage circuit. In the middle of mode four, the medium voltage capacitor c2 voltage ~2 drops due to continuous discharge, while the clamp capacitor C1 voltage rises for a long time, and the first clamped diode A reverses off. At this time, the secondary side winding current 仏 is equal to the secondary side winding current b, and this mode is ended. Mode five-day custodial [heart ~ 纟d, face inductance 7; equal winding on both sides of the current discharge to the high voltage circuit

麵合電感7;兩側繞組電流以於電流l時,儲存於鐵 米刀心的能I均勾於兩繞組釋放,此時執合電感(二次側繞 組心在非極性點處,電壓為正,其值為 VLS = Nvlp = dxNVL /(1 ~dx) (i 9) 此時電壓Fz、v〆vC2及vZtS四者,對高壓電路放電,利 用方程式(17)至方程式(19),高壓電路之電壓^可計算如 下:Face inductance 7; when the winding currents on both sides are at current l, the energy I stored in the iron core is released in the two windings. At this time, the inductance is applied (the secondary winding core is at the non-polar point, the voltage is Positive, its value is VLS = Nvlp = dxNVL / (1 ~ dx) (i 9) At this time, the voltages Fz, v〆vC2 and vZtS are discharged to the high voltage circuit, using equations (17) to (19), high voltage The voltage of the circuit ^ can be calculated as follows:

= + VLP + VC2= + VLP + VC2

+ V+ V

LS (20)LS (20)

Gv2--ViGv2--Vi

VL 2 + N \-dx (21) 依據方程式(21)繪出如圖7所示,於不同匝數比y,昇壓比 例與低壓開關&責任週期4之關係曲線,並與習用耦 合電感電路之電壓增益作一比較[附註—習用耦合電感電路 24 1262646 . 之參考文獻:Q· Zhao, and F. C· Lee,“High-efficiency,high step-up DC-DC converters/5 IEEE Tran. Power Electronics, vol. 18, pp. 65-73, 2003]。如再將方程式(18)代入方程式(20) 可以得到低壓開關&之跨壓 VDS\ - + 2) (22) 觀察方程式(22),將高壓電路之電壓心及匝數比TV固定, 低壓開關&所承受電壓與低壓電路之電壓^及責任週期4 > 無關,因此可以確保功率半導體開關元件之所承受最高電 壓為定值。只要輸入電壓不高於低壓開關&耐壓,依據方 程式(22)所設計之換流器,配合原本高電壓增益比之特 性,低壓電路可接受高、低電壓大範圍變動之電壓。高壓 開關&觸發訊號可於低壓開關&導通前,提早截止,停止 同步整流模式。 模式六:時間[G〜(〇];低壓開關&觸發訊號導通瞬間 | 低壓開關5\於纟=(5時導通,由於第一箝制二極體Α為 低壓蕭基二極體,低壓開關&導通瞬間立即逆偏。耦合電 感7; —次侧繞組漏感4限制電流心上昇斜率,以及流至 二次側繞組漏感之電流b需要時間降至零,兩漏感電流相 互箝制’以及第一箝制二極體马逆偏無逆向恢復電流,開 關無法自低壓電路、中壓電路與第一箝制二極體q等三路 • 控波取任何電流,自然形成零電流切換(Zer〇 Current 25 1262646VL 2 + N \-dx (21) According to equation (21), as shown in Figure 7, the relationship between the boost ratio and the low-voltage switch & duty cycle 4 is shown in different turns ratios y, and with the conventional coupled inductor A comparison of the voltage gain of the circuit [Note - Conventional Coupled Inductor Circuit 24 1262646 . References: Q· Zhao, and F. C· Lee, “High-efficiency, high step-up DC-DC converters/5 IEEE Tran. Power Electronics, vol. 18, pp. 65-73, 2003]. If we substitute equation (18) into equation (20), we can get the low voltage switch & cross voltage VDS\ - + 2) (22) Observe the equation (22) ), the voltage core and the turns ratio of the high voltage circuit are fixed to the TV, and the voltage of the low voltage switch & is independent of the voltage of the low voltage circuit and the duty cycle 4 > therefore, the maximum voltage of the power semiconductor switching element can be ensured. As long as the input voltage is not higher than the low voltage switch & withstand voltage, the converter designed according to equation (22), combined with the original high voltage gain ratio characteristics, the low voltage circuit can accept high and low voltage wide range of varying voltage. High voltage switch & trigger signal can be Before the voltage switch & turn on, stop early and stop the synchronous rectification mode. Mode 6: Time [G~(〇]; Low-voltage switch & Trigger signal conduction moment | Low-voltage switch 5\纟纟=(5° conduction, due to the first The clamped diode is a low-voltage Schottky diode, and the low-voltage switch & turns on immediately and reverses. The coupled inductor 7; - the secondary winding leakage inductance 4 limits the current core rise slope, and flows to the secondary side winding leakage inductance The current b needs time to fall to zero, the two leakage currents are mutually clamped' and the first clamped diode is reversed without reverse recovery current, and the switch cannot be self-voltage circuit, medium voltage circuit and first clamp diode q, etc. Road • Controlling any current, naturally forming a zero current switch (Zer〇Current 25 1262646

Switching,ZCS)特性。此時電路電流仍然維持輸出側流 向,但逐漸遞減中,因此本電路導通時具柔性切換特性, 有效減輕切換損失。 本模式末期漏感能量釋放後,耦合電感C之二次側繞 ’、、電饥w轉向,流入低壓開關&,以小電流對高壓開關夕 之飛輪二極體,施以逆向恢復電流。由於箱制電感^無法3 =提供電流於二次側繞組電流L,因此迫使第 =箝制二極體A與第三箝制二極體化同時導通,截止狀 ㈣射3跨心朋等於高㈣路之電壓6。當箝制 !電流/£1等於二次側繞組電心時,第三箝制二極體 化截止瞬間(4),開關4跨壓、回到kvcl,完成一 切換週期(Switching Cycle),接來 —的情形。 接下以作㈣則回到模式 本發明时㈣騎壓_工作方式,若制於 :::作方ί’部分元件可取:代或省略,仍可购 整流楔::獨使用降壓方式,低壓開關X僅操作於同步 獨使用導通損之蕭基二極體替代。若單 屢開關w/作 賴提可省略降壓電路外,由於高 代。3作於同步整流模式,可使用—般二極體取 1月係針對國内外文獻及習用電路改善先前技術之 26 1262646 原理及對照功效如下: 1. 開關少且架構簡單。本發明之高效率高壓差比雙向換流 器,僅使用三個開關即可達成雙向能量傳遞之功能,與 先前技術至少需要四個以上開關而言,不僅架構簡單, 且元件少,成本低廉。 2. 具高壓差比,低壓電源選擇性高。本發4之換流器,可 以接受兩端高差距之電壓。實務應用上,高壓電路可以 提供交流電器負載所需反流器之前端高壓直流電源,低 壓電路則採用12V高容量電池即可使用,不需多組電 池串聯,直接改為並聯,以避免電池串聯故障所產生電 源管理問題。 3. 具電壓箝制與柔性切換,轉換效率高。本發明之換流器 充分導入高壓侧小電流與低壓側大電流之特性,並箝制 開關元件之最高電壓,因此得以將元件效益充分利用, 包括開關利用率、低導通損失與成本。此外,本發明之 換流器,運用漏感之特性,達成零電壓切換,降低高頻 '之切換損失。因此,減少開關數量並抑制導通與切換之 損失,轉換效率自然提高。 4. 所有開關及二極體皆可達成電壓箝制功能。本發明之換 流器,無開關導通時之短路電流及二極體逆向高恢復電 流之問題,且無需加裝緩震電路。 5. 昇壓功能中,開關所需承受電壓與輸入電壓無關。本發 明之換流器,操作於昇壓工作方式時,功率半導體開關 所承受電壓僅與直流輸出電壓及耦合電感之匝數比有 27 1262646 關,此特點更適合直流輸入電壓大範圍變動之電源轉換 裝置應用,然而必要條件為直流輸入電壓源不可高過功 率半導體開關财壓。 6·雖無電氣隔離,但仍具電氣安全之特性。根據說明書中 昇降壓電路理論分析,低壓電路既使在開路狀態,也不 會有發生高電壓之情形。倘若發生不可抗之因素,如元 件故障,低壓侧因此發生高電壓狀況,但由於選擇低壓 具低額定電壓之特性,必先導致該開關v仍過壓 擊穿,產生短路電流,此時會將降低人體比較容易接觸 之低壓電路相關元件電壓,其短路電流足以將保險絲快 速熔斷,同時隔離高電壓傳導至低壓電路之路徑,確保 操作人員接觸低壓電路時,不會發生感電事故。 【實施方式】 ^本發明高效率高壓差比雙向換流器設計之規範為高壓 電路電墨F^OOV以及低壓電路電塵匕=24γ為基礎作實 :二列之驗證’其考量為交流11〇v反流器之前端電源一般 "又计為直流200V,備用電源兼具負載則以蓄電池為首要 之應=,而兩組直流12V電池組串聯為業界常用之裝置。 電路設計之第一步驟,先決定輕合電感之阻數比與開關元 ^之規格。依據電壓規格可知,%2=1/巧广8.33,是故高 壓,關&之責任週期名必須依照方程式(14)設計,同時必 須符合昇降壓雙向電壓增益之電壓調整要求,因此利用圖 4及圖7 乂又比對,可以決定匝數比# = 先前昇、降壓 兩種工作方式皆已說明箝制電容〇1可以吸收耦合電感之漏 28 1262646 ~ 感能量,其能量又可以透過其他路徑提供給輸出端,因此 漏感大小比例,可影響電壓增益之範圍有限,是以本發明 所使用之耦合電感可以接受高漏感變壓器,不侷限使用高 耦合係數之三明治疊繞方式,運用習用兩繞組分開繞法即 可完成。本貫施例之搞合電感’為一具南氣隙之南激磁電 流雙繞組變壓器,利用該變壓器匝數比不同,區隔電壓與 電流範圍,低壓侧匝數少電流大,高壓側反之。將匝數比 代入圖8所示之降壓部分電路,設計當高壓電路電壓 > ^=20〇ν,於不同匝數#時,其低壓開關電壓1/^、低 壓電路電壓^與高壓開關&責任週期4之關係曲線。依據 此圖計算,當低壓電路之電壓為零時,低壓開關4承受最 高為65V之電壓,因此可以選擇額定電壓為80V之 MOSFET元件。至於降壓開關&與高壓開關&之最高電壓 等於高壓電路電壓200V,因此可以選擇額定電壓為250V 之MOSFET元件。二極體方面,第二箝制二極體乃3耐壓 與高壓電路電壓200V相同,可選擇額定電壓為250V之 i | 快速二極體,其餘二極體皆因電壓箝制之功效,小於或等 於箝制電容之電壓να,因此可使用低導通電壓與低逆 向恢復之蕭基(Schottky)二極體。本實施例切換頻率為 100kHz,詳細之規格條列如下:Switching, ZCS) features. At this time, the circuit current still maintains the output side flow, but gradually decreases, so the circuit has a flexible switching characteristic when it is turned on, effectively reducing the switching loss. After the leakage energy is released at the end of this mode, the secondary side of the coupled inductor C is turned around, and the electric hunger w turns into the low-voltage switch & the small current is applied to the flywheel diode of the high-voltage switch, and the reverse recovery current is applied. Since the box inductance ^ cannot 3 = supply current to the secondary side winding current L, forcing the first clamped diode A and the third clamped diode to be simultaneously turned on, and the cutoff (four) shot 3 cross-hearted is equal to the high (four) way The voltage is 6. When clamping! Current / £1 is equal to the secondary winding core, the third clamping diode is turned off (4), switch 4 crosses the pressure, returns to kvcl, completes a switching cycle (Switching Cycle), and then - The situation. Next, it is used as (4) to return to the mode. In the present invention (4) riding pressure _ working mode, if:::: square ί' part of the component can be taken: generation or omission, still available rectifier wedge:: use the buck mode alone, The low-voltage switch X is only operated in the synchronous replacement of the Schottky diode of the conduction loss. If the single switch w/ is used, the step-down circuit can be omitted, due to the high generation. 3 In the synchronous rectification mode, the general diode can be used. January is to improve the prior art for domestic and foreign literature and custom circuits. 26 1262646 Principles and comparisons are as follows: 1. Less switches and simple structure. The high efficiency high-voltage difference ratio bidirectional converter of the present invention can realize the bidirectional energy transfer function by using only three switches, and the prior art requires at least four switches, which is not only simple in structure, but also has few components and low cost. 2. With high pressure difference ratio, low voltage power supply has high selectivity. The inverter of the present invention 4 can accept a voltage with a high difference between the two ends. In practice, the high-voltage circuit can provide the high-voltage DC power supply of the front-end of the inverter required for the AC electrical load, and the low-voltage circuit can be used with the 12V high-capacity battery. It is not necessary to connect multiple batteries in series, and directly change to parallel to avoid battery connection. Power management issues caused by the failure. 3. With voltage clamping and flexible switching, the conversion efficiency is high. The inverter of the present invention sufficiently introduces the characteristics of the low current on the high voltage side and the large current on the low voltage side, and clamps the highest voltage of the switching element, thereby making full use of the component benefits, including switching utilization, low conduction loss, and cost. Further, the inverter of the present invention uses the characteristics of the leakage inductance to achieve zero voltage switching and reduces the switching loss of the high frequency. Therefore, the number of switches is reduced and the loss of conduction and switching is suppressed, and the conversion efficiency is naturally improved. 4. All switches and diodes can achieve voltage clamping. The converter of the present invention has no problem of short-circuit current when the switch is turned on and the reverse high recovery current of the diode, and does not need to be equipped with a cushioning circuit. 5. In the boost function, the required voltage of the switch is independent of the input voltage. When the converter of the present invention is operated in the boosting mode, the voltage of the power semiconductor switch is only 27 1262646 with the ratio of the DC output voltage and the coupled inductor. This feature is more suitable for the power supply with a wide range of DC input voltage. The conversion device is applied, however, the necessary condition is that the DC input voltage source cannot be higher than the power semiconductor switch. 6. Although there is no electrical isolation, it still has electrical safety characteristics. According to the theoretical analysis of the buck-boost circuit in the manual, the low-voltage circuit is in an open state and there is no high voltage. In the event of a force-to-force factor, such as a component failure, a low-voltage condition occurs on the low-voltage side. However, due to the low-voltage characteristic of the low-voltage device, the switch v must be over-voltage breakdown and short-circuit current. It reduces the voltage of the low-voltage circuit-related components that the human body is relatively easy to contact. The short-circuit current is enough to quickly blow the fuse, and isolates the path of high-voltage conduction to the low-voltage circuit to ensure that the operator does not experience a power-sensitive accident when it contacts the low-voltage circuit. [Embodiment] ^ The specification of the high efficiency high-voltage difference ratio bidirectional converter design of the present invention is based on the high-voltage circuit ink F^OOV and the low-voltage circuit electric dust 匕=24γ: the verification of the two columns' consideration is AC 11 The front-end power supply of the 〇v inverter is generally calculated as DC 200V, and the standby power supply has the load as the primary battery =, and the two sets of DC 12V battery packs are commonly used in the industry. In the first step of the circuit design, the resistance ratio of the light-inductive inductor and the specification of the switching element are first determined. According to the voltage specification, %2=1/Qiaoguang 8.33 is the high voltage, the duty cycle name must be designed according to equation (14), and must meet the voltage regulation requirements of buck-boost bi-directional voltage gain, so use Figure 4 And Figure 7 乂 and compare, you can determine the turns ratio # = previous rise and fall two working methods have shown that the clamp capacitor 〇1 can absorb the leakage of the coupled inductor 28 1262646 ~ sense energy, its energy can pass through other paths Provided to the output, so the leakage inductance ratio can affect the range of voltage gain is limited. The coupled inductor used in the present invention can accept a high leakage inductance transformer, and is not limited to the use of a high coupling coefficient sandwich stacking method, using the conventional two Winding can be done separately. The coupling inductance of the present embodiment is a south-excited current double-winding transformer with a south air gap. The turns ratio is different, the voltage and current range are different, the number of turns on the low-voltage side is small, and the high-voltage side is opposite. Substituting the turns ratio into the step-down circuit shown in Figure 8, designing the high-voltage circuit voltage > ^=20〇ν, at different turns#, its low-voltage switching voltage 1/^, low-voltage circuit voltage ^ and high-voltage switch & responsibility cycle 4 relationship curve. According to this figure, when the voltage of the low-voltage circuit is zero, the low-voltage switch 4 is subjected to a voltage of up to 65V, so that a MOSFET component with a rated voltage of 80V can be selected. As for the buck switch & and the high voltage switch & the highest voltage is equal to the high voltage circuit voltage of 200V, so you can choose a MOSFET component with a rated voltage of 250V. In terms of diodes, the second clamp diode is the same as the voltage of 200V and the high voltage circuit voltage is 200V. The fast voltage diode with a rated voltage of 250V can be selected. The other two diodes are less than or equal to the voltage clamp effect. The voltage να of the capacitor is clamped, so a Schottky diode with low turn-on voltage and low reverse recovery can be used. The switching frequency of this embodiment is 100 kHz, and the detailed specifications are as follows:

VH : 200V VL : 24V 7; : Αν·#2=3Τ:6Τ ; ZP=14//H ; 4=52"Η ;灸= 0.98 ; . core : EE-55 29 1262646 ^ : FQI90N08 ^ 80V/71A ^5(〇N)=12mQ ^ I2PAK &及& ·· IRFP264N,250V/44A,㈣=60mQ,TO-247VH : 200V VL : 24V 7; : Αν·#2=3Τ:6Τ ; ZP=14//H; 4=52"Η; moxibustion = 0.98 ; . core : EE-55 29 1262646 ^ : FQI90N08 ^ 80V/71A ^5(〇N)=12mQ ^ I2PAK &&& ·· IRFP264N, 250V/44A, (4)=60mQ, TO-247

Lx : 7/iH L2 : 60//H Q : 22//F/100V C2 : 10//F/200VLx : 7/iH L2 : 60//H Q : 22//F/100V C2 : 10//F/200V

ZV 及 D3x : STPS20H100CT,100V/2* 10A (Schottky), TO-220AB /¾ : SF1005G,300V/16A,TO-220A 為使更進一步暸解本發明之内容,以下實施例之實驗波 形,電路元件之電壓及電流之代號,敬請參閱圖3(a) ° 本發明高效率高壓差比雙向換流器降壓部分電路之實 施例如圖9所示,當高壓電路電壓4=200V與低壓電路電 壓匕=24¥,輸出功率為300W時,各元件之實驗波形。圖 9(a)為低壓開關於同步整流控制時之電壓電流波形’’其 開關電壓VMr50V,符合理論分析。圖9(b)與圖9(c)分別 顯示降壓開關&與高壓開關&之電壓電流波形,依圖所 示,兩開關導通時具零電壓切換特性,且截止時,電壓粉 制約在200V。圖9(d)呈現耦合電感兩侧繞組k與心電流 變化之波形。 圖10為本發明高效率高壓差比雙向換流器弈麇部分 電路之實施例,當高壓電路電壓^=200及低壓電路電壓 Kz^24V,輸出功率為300W時,各元件之實驗波形。圖1〇⑻ 30 1262646 . 為低壓開關&電壓電流波形,其開關電壓,近似 方程式(22)之理論分析,導通時電流具零電流切換特性且 接近低漣波之方波。圖10(b)顯示高壓開關&於同步整流 控制時之電壓電流波形,電壓箝制小於200V。圖10(c)呈 現耦合電感兩侧繞組k與4電流變化之波形。 本發明高效率高壓差比雙向換^流器昇壓與降壓電路之 實測轉換效率如圖11所示,最高降壓轉換效率約在 95.5%,昇壓最高轉換效率則超過在96%。輕載效率昇壓 ⑩ 高於降壓係因降壓電路之零電壓切換具有較高環流,而重 載區域昇壓效率較差在於大部分能量傳遞靠低壓開關之 運作,導通損失急遽上昇所致。 圖12為本發明高效率高壓差比雙向換流器,第二較 佳實施例之方塊圖。該架構與前面所提第一較佳實施例比 較,工作原理相仿,但箝制電路123比箝制電路103之元 件,減少箝制電感A與第三箝制二極體D3;c。依據第一較 佳實施例之規範,在同樣的功率輸出條件,模擬之結果如 — 圖13所示第二較佳實施例之降壓電路模擬波形響應,以 及圖14之第二較佳實施例之昇壓電路模擬波形響應。對 照圖13與圖9,圖13(c)之高壓開關&之截止電壓為 匕-να,小於圖9(c)之相同開關,可以進一步選擇較低額 定電壓之開關。然而圖13(b)之降壓開關&導通前之電壓 提高成為vα,只能達成接近零電壓柔性切換,因此在降 、 壓方面,兩較佳實施例各有所長。再比較圖14與圖10之 . 昇壓部分性能,圖14(a)及圖14(b)之低壓開關&與高壓開 1262646 關&之箝制電壓效果優於圖10(a)及圖10(b),此乃少了第 二較佳實施例中第三箝制二極體與箝制電感A,因此 籍制電容電壓%可以釋放更快,並可以支撐高壓開 止時之部分電壓。 雖:、、、;本餐明已以如述較佳實施例揭示,然其並非用以 限,本發明,任何熟習此技藝者,再不脫離本發明之_神 $範圍内,當可作各種之變動與修改,因此本發明之保護 fe圍當視後附之申請專利範圍所界定者為準。 【圖式簡單說明】 圖1本發明高效率高壓差比雙向換流器,第一較佳實施 例之電路架構。 ^ 圖2本發明局效率高壓差比雙向換流器之降壓部分電路 時序。 圖 圖4 圖 本發明高效率高壓差比雙向換流器之降壓部分 工作模式。 本發明高效率高壓差比雙向換流器之降壓部分電 路’於不同e數比料,降壓比例Gn與 &責任週期4之關係曲線。 本發明局效率高壓差比雙向換流器之昇壓部分 時序。 圖6本發明局效率高壓差比雙向換流器之昇壓 工作模式。 电塔 圖7本發明尚效率高壓差比雙向換流器之昇壓部分電 路,於不同®數比斤時,昇壓比例〜與低壓^關 1262646 &責任週期4之關係曲線,並與習用耦合電感電路 之電壓增益作一比較。 圖8 本發明高效率高壓差比雙向換流器之降壓部分電 路,設計高壓電路電壓4二200V,於不同匝數比I 時,低壓開關電壓、低壓電路電壓^與高壓開 關&責任週期4之關係曲線。 圖9 本發明高效率高壓差比雙向換流器降壓部分電路之 實施例,當高壓電路電壓^=200¥、低壓電路電壓 ί^=24ν以及輸出功率為300W時,各元件實驗波 形。 圖10本發明高效率高壓差比雙向換流器昇壓部分電路之 實施例,當高壓電路電壓4=20〇ν、低壓電路電壓 ^=24ν以及輸出功率為300W時,各元件實驗波 形。 圖11本發明高效率高壓差比雙向換流器昇壓與降壓電路 之實測轉換效率。 圖12本發明高效率高壓差比雙向換流器,第二較佳實施 例之電路架構。 圖13本發明高效率高壓差比雙向換流器,第二較佳實施 例之降壓電路模擬波形響應。 圖14本發明高效率高壓差比雙向換流器,第二較佳實施 例之昇壓電路模擬波形響應。 【主要元件符號說明】 101 :低壓電路 1262646 102 :中壓電路 103 :箝制電路 104 :高壓電路 105 :降壓電路 123 :箝制電路 ^ :高壓電路電壓 匕:低壓電路電壓 A :低壓功_率半導體開關(簡稱低壓開關) & :降壓功率半導體開關(簡稱降壓開關) 5^ :南壓功率半導體開關(簡稱南壓開關) 7;:具高激磁電流之變壓器(簡稱耦合電感) 免:耦合電感7;之耦合係數 :耦合電感一次側繞組 As :耦合電感二次侧繞組ZV and D3x: STPS20H100CT, 100V/2* 10A (Schottky), TO-220AB /3⁄4 : SF1005G, 300V/16A, TO-220A In order to further understand the contents of the present invention, the experimental waveforms of the following embodiments, circuit components For the voltage and current codes, please refer to Figure 3(a). The high-efficiency high-voltage ratio bidirectional converter step-down part of the circuit is implemented as shown in Figure 9. When the high-voltage circuit voltage is 4=200V and the low-voltage circuit voltage匕=24¥, the experimental waveform of each component when the output power is 300W. Figure 9(a) shows the voltage-current waveform '' of the low-voltage switch during synchronous rectification control's switching voltage VMr50V, which is in line with theoretical analysis. Figure 9(b) and Figure 9(c) show the voltage and current waveforms of the buck switch & and the high-voltage switch & respectively, as shown in the figure, when the two switches are turned on with zero voltage switching characteristics, and when turned off, the voltage powder is restricted. At 200V. Figure 9(d) shows the waveform of the variation of the winding k and the heart current on both sides of the coupled inductor. Fig. 10 is a view showing an embodiment of a high-efficiency high-voltage differential ratio bidirectional converter circuit of the present invention. When the high-voltage circuit voltage is ^=200 and the low-voltage circuit voltage is Kz^24V, and the output power is 300W, the experimental waveform of each component. Fig. 1〇(8) 30 1262646. For the low-voltage switch & voltage and current waveform, its switching voltage, approximating the theoretical analysis of equation (22), the current has a zero-current switching characteristic and is close to a low-chopper square wave. Figure 10(b) shows the voltage and current waveforms of the high-voltage switch & during synchronous rectification control, with voltage clamping less than 200V. Figure 10(c) shows the waveform of the current changes in the windings k and 4 on both sides of the coupled inductor. The measured efficiency of the high-efficiency high-voltage difference ratio bidirectional converter step-up and step-down circuit of the present invention is shown in Fig. 11. The highest step-down conversion efficiency is about 95.5%, and the maximum boosting conversion efficiency is over 96%. The light load efficiency boost 10 is higher than the buck system because the zero voltage switching of the buck circuit has a higher circulating current, while the boosting efficiency of the heavy load region is poor. Most of the energy transfer is caused by the operation of the low voltage switch, and the conduction loss is rapidly increased. Figure 12 is a block diagram of a second preferred embodiment of the high efficiency high voltage differential ratio bidirectional converter of the present invention. The architecture is similar to the first preferred embodiment described above, and the operating principle is similar, but the clamping circuit 123 reduces the clamping inductance A and the third clamping diode D3; c than the components of the clamping circuit 103. According to the specification of the first preferred embodiment, in the same power output condition, the result of the simulation is as follows: the step-down circuit analog waveform response of the second preferred embodiment shown in FIG. 13, and the second preferred embodiment of FIG. The boost circuit simulates the waveform response. Referring to Fig. 13 and Fig. 9, the cut-off voltage of the high voltage switch & of Fig. 13(c) is 匕-να, which is smaller than the same switch of Fig. 9(c), and the switch of the lower rated voltage can be further selected. However, the voltage of the step-down switch of Fig. 13(b) is increased to vα, and only a near-zero voltage flexible switching can be achieved, so that the two preferred embodiments have their respective advantages in terms of down-and-down. Comparing Fig. 14 and Fig. 10, the boosting part performance, the low voltage switch & and the high voltage opening 1262646 of Fig. 14(a) and Fig. 14(b) are better than the Fig. 10(a) and Fig. 10(b), this is the third clamped diode and the clamped inductor A in the second preferred embodiment, so that the capacitor voltage % can be released faster and can support a part of the voltage when the high voltage is turned on. The present invention has been disclosed in the preferred embodiments as described above, but it is not intended to limit the scope of the invention, and any person skilled in the art can make various kinds without departing from the scope of the present invention. The invention is subject to change and modification, and therefore the protection of the present invention is defined by the scope of the patent application. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a circuit diagram of a high-efficiency high-voltage differential ratio bidirectional converter of the first preferred embodiment of the present invention. ^ Figure 2 shows the efficiency of the high voltage difference ratio of the bidirectional converter of the invention. Figure 4 is a diagram showing the step-down operation mode of the high efficiency high voltage difference ratio bidirectional converter of the present invention. The high-efficiency high-voltage difference of the present invention is based on the relationship between the step-down ratio of the step-down ratio Gn and the duty cycle 4 of the step-down portion of the bidirectional converter. The efficiency difference of the present invention is higher than that of the boosting portion of the bidirectional converter. Fig. 6 shows the boosting mode of the efficiency of the high voltage difference ratio bidirectional converter of the present invention. Electric tower Figure 7 The present invention is also a high-voltage difference ratio bi-directional converter boosting part of the circuit, in different о-numbers, the boost ratio ~ and low-voltage ^ off 1262646 & duty cycle 4 relationship, and with the use The voltage gain of the coupled inductor circuit is compared. Figure 8 is a high-efficiency high-voltage differential ratio bidirectional converter step-down circuit of the present invention, designed high-voltage circuit voltage 4 2 200V, at different turns ratio I, low-voltage switching voltage, low-voltage circuit voltage ^ and high-voltage switch & duty cycle 4 relationship curve. Fig. 9 shows an embodiment of the high-efficiency high-voltage difference ratio bidirectional converter step-down circuit of the present invention. When the high-voltage circuit voltage is ^=200¥, the low-voltage circuit voltage ί^=24ν, and the output power is 300W, the components are experimentally shaped. Fig. 10 shows an embodiment of the high-efficiency high-voltage difference ratio bidirectional converter boosting section circuit of the present invention. When the high-voltage circuit voltage is 4 = 20 〇 ν, the low-voltage circuit voltage is ^ = 24 ν, and the output power is 300 W, the components are experimentally shaped. Figure 11 shows the measured conversion efficiency of the high efficiency high voltage difference ratio bidirectional converter step-up and step-down circuit of the present invention. Figure 12 is a circuit diagram showing a high efficiency high voltage difference ratio bidirectional converter of the present invention, a second preferred embodiment. Figure 13 is a high efficiency high voltage difference ratio bidirectional converter of the present invention, and the buck circuit of the second preferred embodiment simulates a waveform response. Figure 14 is a high efficiency high voltage difference ratio bidirectional converter of the present invention, and the booster circuit of the second preferred embodiment simulates a waveform response. [Main component symbol description] 101: Low voltage circuit 1262646 102: Medium voltage circuit 103: Clamp circuit 104: High voltage circuit 105: Step-down circuit 123: Clamp circuit ^: High voltage circuit voltage 匕: Low voltage circuit voltage A: Low voltage work _ rate Semiconductor switch (referred to as low voltage switch) & : Buck power semiconductor switch (referred to as buck switch) 5^: South voltage power semiconductor switch (referred to as South voltage switch) 7;: transformer with high excitation current (referred to as coupled inductor) : Coupling inductor 7; coupling coefficient: coupled inductor primary winding As: coupled inductor secondary winding

Lk\ :摩馬合電感一次側繞組之漏感 Lja :耦合電感二次側繞組之漏感 Lml :耦合電感一次側繞組之激磁 電感 ^m2 :耦合電感二次側繞組之激磁 電感 A 箝制電感 l2 降壓電感 Q 箝制電容 c2 中壓電容 A 第一箝制二極體 d2 降壓二極體 34 1262646 A:第二箝制二極體 :第三箝制二極體Lk\ : Leakage inductance of the primary winding of Momma inductor Lja: Leakage inductance of the secondary winding of the coupled inductor Lml : Magnetizing inductance of the primary winding of the coupled inductor ^m2 : Magnetizing inductance of the secondary winding of the coupled inductor A Clamping inductor l2 Buck inductor Q clamp capacitor c2 medium voltage capacitor A first clamp diode d2 step-down diode 34 1262646 A: second clamp diode: third clamp diode

Claims (1)

1262646 十、申請專利範圍: 1. -種高效率高壓差比雙向換流器,其中々八 -低壓電路:由一低壓開關與耦合電感 = 成,藉由低屢開關導通與截止組組 一次側繞組之能量; 切放輕合電感 一中壓電路:由耦合電减一,伽植 ⑽一一人侧繞組與—中麗電容组 成^丨難㈣路與“轉之間,主要是利用中屢 電各提高昇壓比例或承受降壓時之部分電壓; -箝制電路:由一箝制電感、一箝制電容、一第一箝 制二極體、一第二箝制二極體與一第三箝制二極體: 成’主要是吸收轉合電感之漏感能量,保護低塵開關, 並將吸收之能量釋放於輸出端; 1壓笔路:由一高壓開關組成,利用該開關提供路 徑,達成高壓電路與低壓電路雙向能量傳遞; -降壓電路:由一降壓開關、一降壓電感及一降壓二 極體組成,負責釋放中壓電容之放電回路; 裝置共有昇壓與降壓兩種功能;昇壓方面:定義低 壓電路為電源’高壓電路為負載;低壓開關導通時, 耦合電感一次側繞組為充電狀態,同時透過耦合電感 一次侧繞組’結合箝制電容對中壓電容充電;當低壓 開關截止時’ |馬合電感之漏感能量由箝制電容吸收; 當漏感影響大幅減少後,耦合電感兩側繞組結合低壓 電源電壓以及中壓電容,經由高壓開關提供高壓電路 1262646 功率;降壓方面:定義高壓電路為電源,低壓電路為 負載;高壓開關導通時,高壓電路對中壓電路及低壓 電路充電;高壓開關截止時,耦合電感能量全部經由 同步整流狀態之回路,由其一次側繞組傳到低壓電路 之負载’此時,中壓電容亦由低壓開關與降壓開關提 供回路,透過耦合電感二次側繞組與降壓電感對低壓 電路之負載供電; • 其特徵為僅使用三個開關即完成雙向電流之控制,加 上本架構有咼昇、降壓比之特性,因此可使用低壓蓄 電池即可併入高壓匯流排,以利後級高壓負載或反流 态刖端使用;換流器之切換技術,採用電壓箝制、同 V 1與令電壓零電流方式,充分使用元件規格,因 此本裝置具有高昇降壓比、低切換損失與低導通損失 之功效。 ' 2· ^申請專利範圍第丨項所述之高效率高壓差比雙向換 ^ ^ ’其中低壓電路與中壓電路之#合電感,為-具 回氣隙之高激磁電流雙繞組變壓器;利用該變壓器匝 數比不同,區隔電壓與電流範圍,低壓側匝數少電流 大’南愿側反之。 *申》月專利範圍第1項所述之高效率高壓差比雙向換 流器,其中箝制電路除可以吸收耦合電感一次側繞組 之漏感能量,其吸收能量可再用於昇壓或降壓;是以 本衣置所使用之耦合電感可以接受高漏感變壓器,不 侷限使用高轉合係數之三明治疊繞方式,運用習用兩 !262646 4· 繞紙分開繞法即可完成。 1高效率高壓差比雙向換流器, 八 7壓電路:由一低壓開嶋合電感 猎由低堡開關導通與截止,將儲存或釋放轉 感〜次側繞組之能量; 电 :中壓電路:由執合電感二次側繞組與-中壓電容組 ^介於低壓電路與高壓電路之間,主錢利用中壓 電容提高昇壓比例或承受降壓時之部分電壓; :箝制電路:由-箝制電容、—第—箝制二極體與一 :二箝制二極體組成,主要是吸收輕合電感之漏感能 里,保護低壓開關,並將吸收之能量釋放於輸出端,· 阿壓電路·由一高壓開關組成,利用該開關提供路 杈,達成高壓電路與低壓電路雙向能量傳遞; 降壓電路:由一降壓開關、一降壓電感及一降壓二 極體組成,負責釋放中壓電容之放電回路; 本ι置共有昇壓與降壓兩種功能;昇壓方面:定義低 壓電路為電源,高壓電路為負載;低壓開關導通時, 耦合電感一次側繞組為充電狀態,同時透過耦合電感 二次侧繞組,結合箝制電容對中壓電容充電;當低壓 開關截止時,輕合電感之漏感能量由箝制電容吸收; 當漏感影響大幅減少後,耦合電感兩側繞組結合低壓 電源電壓以及中壓電容,經由高壓開關提供高壓電路 功率「降壓方面:定義高壓電路為電源,低壓電路為 38 1262646 - 負载;高壓開關導通時,高壓電路對中壓電路及低壓 電路充電,南壓開關截止時,耦合電感能量全部經由 5 V t抓狀怨之回路,由其一次侧繞組傳到低壓電路 :負載’此時,中壓電容亦由低壓開關與降壓開關提 ί、回路,透過耦合電感二次側繞組與降壓電感對低壓 電路之負載供電; /、特欲為僅使用三個開關即完成雙向電流之控制,加 修上本架構有向昇、降壓比之特性,因此可使用低壓蓄 ,士即可併入高壓匯流排,以利後級高壓負載或反流 為則端使用;換流器之切換技術,採用電壓箝制、同 步整流與零電壓零電流方式,充分使用元件規格,因 此本衣置具有尚昇降壓比'低切換損失與低導通損失 之功效。 5·=請專利範圍帛4帛所述之高a率高壓差比雙向換 j裔,其中低壓電路與中壓電路之耦合電感,為一具 • 回氣隙之局激磁電流雙繞組變壓器;利用該變壓器匝 數比不同’區隔電壓與電流範圍,低壓側匝數少電流 大’高壓侧反之。 6· t申請專利範圍第4項所述之高效率高壓差比雙向換 流杰’其中箝制電路除可以吸收耦合電感一次側繞組 之漏感能量,其吸收能量可再用於昇壓或降壓;是以 、 本裝置所使用之耦合電感可以接受高漏感變壓器,不 侷限使用高耦合係數之三明治疊繞方式,運用習用兩 繞組分開繞法即可完成。1262646 X. Patent application scope: 1. A high-efficiency high-voltage differential ratio bidirectional converter, in which the 々8-low-voltage circuit: consists of a low-voltage switch and a coupled inductor = with a low-frequency switch-on and turn-off group primary side The energy of the winding; the light-inductance of the light-cutting inductor: a medium-voltage circuit: the coupling is reduced by one, the gamma is implanted (10), the one-side winding and the middle-capacitor capacitor are composed of ^ 丨 ( (four) road and "turn between, mainly in use Each of the voltage increases the boost ratio or withstands a part of the voltage during the step-down; - the clamp circuit: consists of a clamped inductor, a clamped capacitor, a first clamped diode, a second clamped diode, and a third clamped Polar body: into 'mainly absorbs the leakage inductance energy of the turn-in inductance, protects the low-dust switch, and releases the absorbed energy to the output end; 1press pen path: consists of a high-voltage switch, which provides the path to achieve high voltage Bidirectional energy transfer between circuit and low voltage circuit; - Buck circuit: consists of a step-down switch, a step-down inductor and a step-down diode, which is responsible for discharging the discharge circuit of the medium voltage capacitor; Kind of work Boost aspect: Define the low-voltage circuit as the power supply 'the high-voltage circuit is the load; when the low-voltage switch is turned on, the primary winding of the coupled inductor is in the charging state, and the medium-side capacitor is charged through the coupled inductor primary-side winding' combined with the clamped capacitor; When the switch is turned off, the leakage inductance energy of the horse-inductor is absorbed by the clamp capacitor; when the leakage inductance is greatly reduced, the windings on both sides of the coupled inductor combine the low-voltage power supply voltage and the medium-voltage capacitor to provide the high-voltage circuit 1262646 power through the high-voltage switch; Pressure: Define the high voltage circuit as the power supply, the low voltage circuit as the load; when the high voltage switch is turned on, the high voltage circuit charges the medium voltage circuit and the low voltage circuit; when the high voltage switch is turned off, the coupled inductor energy is all looped through the synchronous rectification state. The side winding is transmitted to the load of the low voltage circuit. At this time, the medium voltage capacitor is also provided by the low voltage switch and the step-down switch, and is supplied to the load of the low voltage circuit through the secondary winding of the coupled inductor and the buck inductor; Use two switches to complete the bidirectional current control, plus this architecture has The characteristics of the rising and lowering ratios can be used to integrate the high-voltage busbars with low-voltage batteries to facilitate the use of high-voltage loads or reverse-flow terminals. The switching technology of the inverters uses voltage clamping and V 1 The voltage zero current mode is used to fully utilize the component specifications, so the device has the advantages of high buck-boost ratio, low switching loss and low conduction loss. ' 2· ^ Patent Application Scope Item 高 High Efficiency High Pressure Difference Ratio Bidirectional Change ^ ^ 'The low-voltage circuit and the medium-voltage circuit are combined with the inductor, which is a high-excitation current double-winding transformer with a return air gap; the transformer turns ratio is different, the voltage and current range are separated, and the number of turns on the low-voltage side is small. The current is large, and the south side is opposite. The high-efficiency high-voltage difference ratio bidirectional converter described in the first paragraph of the patent scope of the patent, wherein the clamp circuit can absorb the leakage energy of the primary winding of the coupled inductor, and the absorbed energy can be It is used for boosting or stepping down. It is a coupling inductor used in this clothing. It can accept high leakage inductance transformers. It is not limited to the use of sandwich winding method with high conversion coefficient. ! 2626464-around paper separately around the law to complete. 1 high efficiency high voltage difference than bidirectional converter, eight 7 voltage circuit: by a low voltage open and close inductance switch by the low barrier switch conduction and cutoff, will store or release the energy of the transduction ~ secondary winding; electricity: medium voltage Circuit: The secondary side winding and the medium voltage capacitor group of the inductor are connected between the low voltage circuit and the high voltage circuit, and the main money utilizes the medium voltage capacitor to increase the boost ratio or to withstand some voltage during the step-down; Clamping circuit: consisting of - clamping capacitor, - first clamping diode and one: two clamping diode, mainly to absorb the leakage inductance of the light coupling inductance, protect the low voltage switch, and release the absorbed energy at the output end , · A pressure circuit · consists of a high voltage switch, using the switch to provide a roller to achieve two-way energy transfer between the high voltage circuit and the low voltage circuit; buck circuit: a buck switch, a buck inductor and a buck diode The body composition is responsible for releasing the discharge circuit of the medium voltage capacitor; the ι has a total of two functions of boosting and stepping; the boosting aspect: defining the low voltage circuit as the power source, the high voltage circuit as the load; when the low voltage switch is conducting, the coupling inductor is on the primary side Winding is In the state of charge, the secondary winding of the coupled inductor is combined with the clamp capacitor to charge the medium voltage capacitor; when the low voltage switch is turned off, the leakage inductance energy of the light coupling inductor is absorbed by the clamp capacitor; when the leakage inductance is greatly reduced, the coupled inductor The two sides of the winding combined with the low-voltage power supply voltage and the medium-voltage capacitor provide the high-voltage circuit power through the high-voltage switch. "Buck-proof aspect: the high-voltage circuit is defined as the power supply, the low-voltage circuit is 38 1262646 - the load; when the high-voltage switch is turned on, the high-voltage circuit is connected to the medium-voltage The circuit and the low-voltage circuit are charged. When the south-voltage switch is turned off, the coupled inductor energy is all passed through the loop of 5 V t, and the primary winding is transmitted to the low-voltage circuit: load 'At this time, the medium-voltage capacitor is also controlled by the low-voltage switch. The buck switch raises the loop and supplies power to the load of the low-voltage circuit through the secondary winding of the coupled inductor and the buck inductor; /, specifically, the control of the bidirectional current is completed by using only three switches, and the structure is modified. The characteristics of the rising and lowering ratios, so the low-pressure storage can be used to integrate the high-pressure busbars to facilitate the post-stage high-voltage load or reverse flow. The end uses; the converter switching technology uses voltage clamping, synchronous rectification and zero voltage zero current mode to fully use the component specifications, so the clothing has the effect of lowering the voltage drop ratio 'low switching loss and low conduction loss. 5 ·=Please refer to the patent range 帛4帛 for the high a-rate high-voltage difference than the bi-directional change, where the coupling inductance of the low-voltage circuit and the medium-voltage circuit is a localized excitation current double-winding transformer with a return air gap; The transformer turns ratio is different from the 'divided voltage and current range, the low voltage side turns less current and the high voltage side is the opposite. 6 · t patent application scope item 4 of the high efficiency high pressure difference ratio bidirectional commutation In addition to absorbing the leakage inductance energy of the primary winding of the coupled inductor, the absorbed energy can be used for boosting or stepping down. Therefore, the coupled inductor used in the device can accept a high leakage inductance transformer, and is not limited to using a high coupling coefficient. The sandwich winding method can be completed by using a conventional two-winding winding method.
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