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TWI351806B - High step-up isolated converter with two input pow - Google Patents

High step-up isolated converter with two input pow Download PDF

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Publication number
TWI351806B
TWI351806B TW97119988A TW97119988A TWI351806B TW I351806 B TWI351806 B TW I351806B TW 97119988 A TW97119988 A TW 97119988A TW 97119988 A TW97119988 A TW 97119988A TW I351806 B TWI351806 B TW I351806B
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switch
voltage
power
current
input
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TW97119988A
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TW200950288A (en
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Rong Jong Wai
Chung You Lin
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Univ Yuan Ze
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1351806 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/直流電力轉 換器及潔淨能源科技之範疇,雖然本發明所牽涉之技術領域廣 泛,但主要係發展「高昇壓式隔離型雙輸入電源轉換器」,可 將兩種不同電壓之低壓直流電源輸入,同時轉換為穩定高壓直 流電源輸出,並具有電源雙向傳遞之功能,提昇能源利用率及 φ 增加供電穩定度。 【先前技術】 近百年來,人類的科技一日千里,生產技術不斷進步,對 曰常生活有了顯著的改善,但全球人口的曰益增長,伴隨而來 的則是能源使用的問題。十九世紀期間石油是促進工業社會出 現的一種重要燃料,而於二十世紀初期,石油取代了煤成為近 代最重要的能源,然而世界上石油的產量幾乎被幾個主要產油 的國家所掌控,而於西元1973年及西元1979年爆發的二次石 油危機,對全球造成莫大的影響。近年來石油價格持續攀升且 現今石油的存量正在迅速減少中,專家預估半世紀後會出現供 應上的危機,未來幾年内,石油價格居高不下是可預見的,因 此價格低廉且蘊藏量豐富的煤又逐漸恢復其重要性。 目前,用煤量最多的是將燃料及煤用在發電廠,其次是將 原料煤煉焦成焦炭後用在鋼鐵業,此外,煤還可以用來生產汽 9 1351806 油、苯、瀝青及合成橡膠等重要產品或副產品。但煤與水混合 後將產生酸性物質,若滲入土壤將汙染附近的河川或湖泊,而 煤燃燒後產生的二氧化碳、二氧化硫及灰粒等,嚴重汙染空氣, 因此,環境汙染為使用煤礦所產生的主要缺點。針對二氧化碳 對全球造成的溫室效應影響,世界各國於西元1997年在日本京 都舉行的「第三次締約國大會」中簽署「京都議定書」,規範控 制人為排放之溫室氣體數量,且於西元2005年初正式生效。為 • 達成溫室氣體減量,國内初期研擬以核能發電來抑制二氧化碳 排放的主張,然而核能發電的安全顧慮及公害問題,使得其應 用存在著許多爭議。為改善非再生能源容量的逐漸減少及溫室 效應所反映出來的問題,除了減少現有能源使用的浪費外,新 -能源的開發是刻不容緩。 一般新能源對環境的衝擊不大,其所造成之空氣、水或廢 棄物等污染行為較不顯著,更重要的是此種能源開發更可重複 φ 使用,具有永續發展的特性,潔淨能源(Clean Energy)為新能源 中較受到重視永續利用的能源[1]-[2],然而部分潔淨能源發電 能量密度較低且易受季節變化或地理環境影響。電力電子與監 控技術關係到各式電氣產品性能及成本的競爭力與能源節約和 環保的兼顧,因此在國際上,被視為二十一世紀產業中僅次於 資訊技術之另一重要關鍵性技術。 潔淨能源由於發電特性導致輸出電壓並非固定,且易隨負 1351806 載變化而浮動,或是其發電量易受自然環境變化而有所限制, 對連續供電需求下而言,電源供電品質極不穩定,一般而言, 潔淨能源皆無法直接應用於一般電器產品,因此由電力電子領 域所發展之直流/直流電源轉換器[3],[4]為應用潔淨能源不可或 缺之電力裝置,此外大部分潔淨能源不具有能源儲存之功能, 當潔淨能源應用於分散式發電系統或是油電混合車輛動力系 統,一般皆以蓄電池或超電容作為電源儲存裝置[5],[6],以混 # 合式供電方式達成輸出電源連續穩定,但需利用額外之傳統電 源轉換器及充電器或是單一雙向轉換器[7] 一 [9]以滿足電源儲存 裝置之供電及充電需求,也同時額外增加系統架設成本。 除了運用傳統電源轉換器搭配充電器於電源儲存裝置外, 近年來許多專家學者投入雙向轉換器之研究,以期達成減少轉 換器裝置數目、簡化複雜供電系統及降低系統成本之目標一 般架構通常使用傳統昇壓式轉換器,並將與輸出高壓倒串聯之 •輸出二極體更換為功率半導體開關,即可視為雙向昇/降壓型轉 換器[7] ’參考文獻[8]並以此架構發展出具柔性切換機制之雙向 昇/降壓型轉換器’此架構雖可實現電源儲存裝置於雙向轉換器 昇壓模式時供電及降魔模式時充電之功能,但仍需額外增加一 轉換器裝置,且其不具有高昇/降壓比之特性,此外亦需將蓄電 池或是超電容串接至較高電壓之輸入,方可滿足高壓直流輸出 電壓之需求;為達成電源雙向傳遞之目的,亦有專家學者提出 1351806 將後級四顆整流二極體替換為功率半導體開關之全橋式轉換器 架構[9],配合驅動訊號之相位位移(Phase Shift)技術或是主動式 電壓箝制技術[1〇],[11],克服變壓器存在洩漏電感造成開關上 電壓突波問題,可達成開關零電壓及零電流柔性切換以降低切 換損失及進一步提升效率,並可藉由變壓器匝數比將直流輸出 電壓提升,達成高昇壓比、電氣隔離以及高壓側與低壓側開關 耐壓耐流匹配之效果,導通時降低開關之導通損失,但此作法 • 仍需額外增加一轉換器裝置。為減少元件使用,參考文獻[12] 中,僅以三個開關及耦合電感架構達成高昇壓比及高壓側與低 壓側開關耐壓耐流匹配,並可逹成高效率之電源轉換,但對潔 淨能源大功率應用場合,通常需將低壓侧與高壓側逕行電氣隔 離,以保護電源使用端,使用耦合電感架構並不具電氣隔離特 性,且於雙電源輸入情況下運用此架構亦需額外增加一組轉換 器。 # 為進一步簡化系統及降低系統設置成本,專家學者發展出 以單一電源轉換器同時滿足雙電源輸入及電源雙向傳遞功能之 轉換器架構[13],[14],參考文獻[13]中,以三繞組之耦合電感架 構達成雙電源輸入及電源雙向傳遞功能,且具有高昇壓比及高 效率轉換之特性,但其電源儲存裝置之充電能量僅能由另一輸 入電源提供,而不能由輸出高壓側反饋,且其不具電氣隔離特 性,無法應用於對電氣隔離需求場合下;參考文獻[14]基於雙 12 1351806 向昇/降壓型轉換器’所發展出對兩輸人電源電路串聯之雙向雙 電源輸入之電源轉換器,當兩電源同時供電狀態下,導通損失 可大幅降低,且兩電源之輸入電流連續,對於應用於輸入電源 為低電壓高電流之潔淨能源時,其架構可有效提升效率,但此 架構昇壓比受限於傳統雙向昇/降壓型轉換器架構,且不具電氣 隔離特性’此外所有開關均須承受輸入大電流和輸出高電壓, 對開關選輯麼耐流匹配上,無法選取低耐壓低導通電阻之功 籲率半導體開關,易導致額外導通損失。有鑑於此,本發明之高 昇壓式隔離型雙輸入電源轉換器,引入變壓器及主動式箱制電 路之架構’克服上述缺點,所發展之轉換器具有高昇壓比、電 氣隔離、雙輸入電源、電源儲存裝置充電能量來至另一電源或 是輸出電源反饋、高壓侧與低壓側開關耐壓耐流匹配以及主動 式電壓柑制之特性’對於應用於輸入電源為低電壓高電流之潔 淨能源及電源儲存裝置之混合式電源供應系統時,可有效提升 # 整體轉換效率’並可減小系統架設成本》 備註:參考文獻 [1] S. R. Bull, ^Renewable energy today and tomorrow,M Proc. IEEE, vol. 89, no. 8, pp. 1216-1226,2001.1351806 IX. INSTRUCTIONS OF THE INVENTION: TECHNICAL FIELD The technical field of the present invention includes the scope of power electronics, DC/DC power converters, and clean energy technologies, although the technical field involved in the present invention is extensive, but mainly The development of "high-boost isolated dual-input power converter" can input two low-voltage DC power supplies of different voltages, and simultaneously convert them into stable high-voltage DC power supply output, and has the function of two-way power transmission to improve energy utilization and increase φ Power supply stability. [Prior Art] In the past 100 years, human science and technology have been growing rapidly, and production technology has been continuously improved. It has significantly improved the daily life, but the growth of the global population has accompanied the problem of energy use. During the nineteenth century, oil was an important fuel for the emergence of industrial society. In the early twentieth century, oil replaced coal as the most important energy source in modern times. However, the world's oil production was controlled by several major oil-producing countries. The second oil crisis that erupted in 1973 and in 1979 has had a huge impact on the world. In recent years, oil prices have continued to rise and the stock of oil is rapidly declining. Experts estimate that there will be a supply crisis in the next half century. In the next few years, high oil prices are foreseeable, so the prices are low and abundant. The coal gradually recovered its importance. At present, the most used coal is fuel and coal used in power plants, followed by coking coal into coke for use in the steel industry. In addition, coal can also be used to produce steam 9 1351806 oil, benzene, asphalt and synthetic rubber. And other important products or by-products. However, when coal and water are mixed, acidic substances will be produced. If it penetrates into the soil, it will pollute nearby rivers or lakes. The carbon dioxide, sulfur dioxide and ash particles generated after coal combustion will seriously pollute the air. Therefore, environmental pollution is caused by the use of coal mines. The main drawback. In response to the global greenhouse effect of carbon dioxide, countries around the world signed the "Kyoto Protocol" in the Third Conference of States Parties held in Kyoto, Japan in 1997 to regulate the amount of greenhouse gases emitted by humans, and officially in early 2005. Effective. In order to achieve greenhouse gas reduction, the domestic initial research on nuclear power generation to curb carbon dioxide emissions, however, nuclear power generation safety concerns and pollution issues, there are many disputes in its application. In order to improve the gradual reduction of non-renewable energy capacity and the problems reflected by the greenhouse effect, in addition to reducing the waste of existing energy use, the development of new-energy is an urgent task. Generally, new energy has little impact on the environment, and the pollution caused by air, water or waste is less significant. More importantly, such energy development can be repeated. It has sustainable development characteristics and clean energy. (Clean Energy) is a new energy source that is valued for sustainable use [1]-[2]. However, some clean energy sources have low energy density and are susceptible to seasonal changes or geographical environment. Power electronics and monitoring technology are related to the competitiveness of various electrical products and cost, and the balance between energy conservation and environmental protection. Therefore, it is regarded as another important key to the 21st century industry after information technology. technology. Clean energy energy output characteristics are not fixed due to power generation characteristics, and it is easy to float with negative 1351806 load, or its power generation is subject to changes in natural environment. For continuous power supply demand, power supply quality is extremely unstable. In general, clean energy cannot be directly applied to general electrical products. Therefore, DC/DC power converters developed in the field of power electronics [3], [4] are indispensable power devices for applying clean energy. Some clean energy does not have the function of energy storage. When clean energy is applied to decentralized power generation systems or hybrid electric vehicle power systems, batteries or super capacitors are generally used as power storage devices [5], [6], to mix # The integrated power supply mode achieves continuous and stable output power supply, but needs to use additional traditional power converters and chargers or single bidirectional converters [7] one [9] to meet the power supply and charging requirements of the power storage device, and also add additional systems. Erection costs. In addition to the use of traditional power converters and chargers in power storage devices, in recent years, many experts and scholars have invested in the study of two-way converters in order to achieve the goal of reducing the number of converter devices, simplifying complex power supply systems and reducing system costs. A boost converter that replaces the output diode with the output high voltage in series with a power semiconductor switch can be considered as a bidirectional step-up/step-down converter [7] 'Reference [8] and develops with this architecture Bidirectional step-up/step-down converter with flexible switching mechanism. This architecture can realize the function of charging the power storage device in the power supply mode and the magic mode when the bidirectional converter is boosted, but an additional converter device is required. It does not have the characteristics of high rise/down ratio, and it also needs to connect the battery or super capacitor to the input of higher voltage to meet the demand of high voltage DC output voltage. For the purpose of achieving two-way transmission of power, there are also experts. Scholars proposed 1351806 to replace the latter four rectifier diodes with a full-bridge converter architecture for power semiconductor switches [9] With the phase shift (Phase Shift) technology of the drive signal or the active voltage clamp technology [1〇], [11], overcoming the voltage surge problem on the switch caused by the leakage inductance of the transformer, the switching zero voltage and zero current flexible switching can be achieved. In order to reduce switching loss and further improve efficiency, the DC output voltage can be increased by the transformer turns ratio to achieve high boost ratio, electrical isolation, and high voltage side and low side switch withstand voltage and current resistance matching. Turn-on loss, but this practice • An additional converter unit is still required. In order to reduce the use of components, reference [12] achieves high boost ratio and high-voltage side and low-side switch withstand voltage and current resistance matching with only three switches and coupled inductor architecture, and can be converted into high-efficiency power conversion, but In clean energy high-power applications, it is usually necessary to electrically isolate the low-voltage side from the high-voltage side to protect the power supply end. The coupled inductor structure does not have electrical isolation characteristics, and the use of this architecture in the case of dual power input requires an additional one. Group converter. # In order to further simplify the system and reduce the system setup cost, experts and scholars have developed a converter architecture that satisfies the dual power supply input and power supply bidirectional transmission function with a single power converter [13], [14], in reference [13], The three-winding coupled inductor architecture achieves dual power supply input and power supply bidirectional transmission, and has high boost ratio and high efficiency conversion characteristics, but the charging energy of the power storage device can only be provided by another input power source, but not by the output high voltage. Side feedback, and it does not have electrical isolation characteristics, can not be applied to the occasion of electrical isolation requirements; reference [14] based on the dual 12 1351806 to the step-up / step-down converter 'developed two-way power supply circuit in series two-way Dual power input power converter, when the two power supplies are simultaneously powered, the conduction loss can be greatly reduced, and the input current of the two power supplies is continuous. For the clean energy source applied to the input power supply with low voltage and high current, the architecture can be effectively improved. Efficiency, but this architecture boost ratio is limited by the traditional two-way up/down converter architecture and is not electrically isolated. In addition, all switches must withstand the input high current and output high voltage. For the current selection of the switch selection, it is impossible to select the low-voltage low-on-resistance semiconductor switch, which is easy to cause additional conduction loss. In view of the above, the high-boost isolated dual-input power converter of the present invention introduces a transformer and an active box circuit architecture to overcome the above disadvantages, and the developed converter has a high step-up ratio, electrical isolation, dual input power supply, The power storage device charges energy to another power supply or output power feedback, high-voltage side and low-voltage side switch withstand voltage and current resistance matching, and active voltage citrus characteristics. For the application of power supply for low voltage and high current clean energy and When the hybrid power supply system of the power storage device can effectively improve the overall conversion efficiency of 'and reduce the system installation cost'. Remarks: References [1] SR Bull, ^Renewable energy today and tomorrow, M Proc. IEEE, vol 89, no. 8, pp. 1216-1226, 2001.

[2] S. Rahman, uGreen power: what is it and where can we find it?/5 IEEE Power Energy Mag., vol. 1, no. 1, pp. 30-37,2003.[2] S. Rahman, uGreen power: what is it and where can we find it?/5 IEEE Power Energy Mag., vol. 1, no. 1, pp. 30-37, 2003.

[3] F. Blaabjerg, Z. Chen, and S. B. Kjaer,“Power electronics as efficient interface in dispersed power generation systems,5, IEEE Tram. Power Electron., vol. 19, no. 5, pp. 1184-1194,2004. 13 1351806 [4] R. J. Wai,C. Y. Lin,R. Υ· Duan,and Y. R. Chang,“High-efficiency dc-dc converter with high voltage gain and reduced switch stress,5, IEEE Trans. Ind. Electron., vol. 54, no. 1, pp. 354-364, 2007.[3] F. Blaabjerg, Z. Chen, and SB Kjaer, "Power electronics as efficient interface in dispersed power generation systems, 5, IEEE Tram. Power Electron., vol. 19, no. 5, pp. 1184-1194, 2004. 13 1351806 [4] RJ Wai, CY Lin, R. Du·Duan, and YR Chang, “High-efficiency dc-dc converter with high voltage gain and reduced switch stress,5, IEEE Trans. Ind. Electron., Vol. 54, no. 1, pp. 354-364, 2007.

[5] L. Solero, A. Lidozzi, and J. A. Pomilio,“Design of multiple-input power converter for hybrid vehicles,IEEE Trans. Power Electron., vol. 20, no. 5, pp. 1007-1016, 2005.[5] L. Solero, A. Lidozzi, and J. A. Pomilio, "Design of multiple-input power converter for hybrid vehicles, IEEE Trans. Power Electron., vol. 20, no. 5, pp. 1007-1016, 2005.

[6] J· S. Lai and D. J. Nelson, “Energy management power converters in hybrid electric and fuel cell vehicles,5, Proc. IEEE, vol. 95, no. 4, pp. 766-777, 2007.[6] J. S. Lai and D. J. Nelson, “Energy management power converters in hybrid electric and fuel cell vehicles, 5, Proc. IEEE, vol. 95, no. 4, pp. 766-777, 2007.

[7] J. Zhang, J. S. Lai, R. Y. Kim and W. Yu, “High-power density design of a soft-switching high-power bidirectional dc-dc converter,IEEE Trans. Power Electron.^ vol. 22, no. 4, pp. 1145-1153, 2007.[7] J. Zhang, JS Lai, RY Kim and W. Yu, “High-power density design of a soft-switching high-power bidirectional dc-dc converter, IEEE Trans. Power Electron.^ vol. 22, no. 4, pp. 1145-1153, 2007.

[8] E. Sanchis-Kilders, A. Ferreres, E. Maset, J. B. Ejea, V. Esteve, J. Jordan, A. Garrigos,and J. Calvente, “Soft switching bidirectional converter for battery discharging-charging,IEEE APEC Conf., 2006, pp. 603-609.[8] E. Sanchis-Kilders, A. Ferreres, E. Maset, JB Ejea, V. Esteve, J. Jordan, A. Garrigos, and J. Calvente, “Soft switching bidirectional converter for battery discharging-charging, IEEE APEC Conf., 2006, pp. 603-609.

[9] S. Inoue and H. Akagi, UA bidirectional isolated dc-dc converter as a core circuit of the next-generation medium-voltage power conversion system,IEEE Trans. Power Electron., vol. 22, no. 2, pp. 535-542, 2007.[9] S. Inoue and H. Akagi, UA bidirectional isolated dc-dc converter as a core circuit of the next-generation medium-voltage power conversion system, IEEE Trans. Power Electron., vol. 22, no. 2, pp 535-542, 2007.

[10] H. Tao, J. L. Duarte, and M. A. M. Hendrix, “Three-port triple-half-bridge bidirectional converter with zero-voltage switching,” IEEE Trans. Power Electron., vol. 23, no. 2, pp. 782-792,2008.[10] H. Tao, JL Duarte, and MAM Hendrix, “Three-port triple-half-bridge bidirectional converter with zero-voltage switching,” IEEE Trans. Power Electron., vol. 23, no. 2, pp. 782 -792, 2008.

[11] K. Wang, C. Y. Lin, L. Zhu, D. Qu, F. C. Lee, and J. S. Lai, ^Bidirectional dc to dc converters for fuel cell systems,M Proc. PET'98, 1998, pp. 47-51.[11] K. Wang, CY Lin, L. Zhu, D. Qu, FC Lee, and JS Lai, ^Bidirectional dc to dc converters for fuel cell systems, M Proc. PET'98, 1998, pp. 47-51 .

[12] R. J. Wai and R. Y. Duan,“High-efficiency bidirectional converter for power sources with great voltage diversity,5, IEEE Trans. Power[12] R. J. Wai and R. Y. Duan, “High-efficiency bidirectional converter for power sources with great voltage diversity, 5, IEEE Trans. Power

Electron., vol. 22, no. 5, pp. 1986-1996,2007.Electron., vol. 22, no. 5, pp. 1986-1996, 2007.

[13] R. J. Wai,C. Y· Lin, L. W· Liu, and Y. R. Chang, “High-efficiency 14 1351806 single-stage bidirectional converter witii multi-input power sources,M IETProc. Electric Power Appl., vol. 1, no. 5, pp. 763-777,2007.[13] RJ Wai, C. Y. Lin, L. W· Liu, and YR Chang, “High-efficiency 14 1351806 single-stage bidirectional converter witii multi-input power sources, M IETProc. Electric Power Appl., vol. 1, no. 5, pp. 763-777, 2007.

[14] M. Marchesoni and C. Vacca, <cNew dc-dc converter for energy storage system interfacing in fuel cell hybrid electric vehicles,IEEE Trans. Power Electron., vol. 22, no. 1, pp. 301-308, 2007. 【發明内容】 第一圖表示本發明所揭示高昇壓式隔離型雙輸入電源轉換 0 器之第一較佳實施例之電路架構,由第一電源電路101、第二 電源電路102、全橋式電路103、主動式箝制電路104以及直流 輸出電路105所組成,其中第一電源電路ιοί由第一輸入電壓 源β、第一電源開關、第一電容C,、第一電感L,以及第一開 關&所組成;第二直流電路1〇2由第二輸入電壓源&、第二電 源開關& 2、第二電容C2、第二電感L2以及第二開關&所組成; 全橋式電路103由第三開關&、第四開關、第五開關、第 φ 六開關&、第七開關*^7、第八開關&、第九開關叉、第十開關心 及隔離變壓器2:所組成,隔離變壓器7;包含隔離變壓器一次側 及隔離變壓器二次側,匝數比為1:«,耦合係數為& ;主 動式箝制電路104由箝制開關^及箝制電容(^所組成;直流輸 出電路105由直流輸出電容Q及直流輸出負載\所組成,直流 輸出電容C。上電壓為直流輸出電壓。本發明所揭示高昇壓式 隔離型雙輸入電源轉換器之輸入電源,即第一輸入電壓源^;以 及第二電壓源厂2,可由蓄電池、超電容 '燃料電也、太陽光電 15 1351806 池、直流風力發電機或交流風力發電機整流為直流電源作為直 流電源供應。 第一電源電路101及第二電源電路1〇2主要透過第一開關 &及第二開關A之切換,將第一輸入電壓源γ及第二輪入電壓 源C之電壓源形式之電能分別轉換為第一電感電流l及第二電 感電流,以電流源電能形式呈現,兩直流電源再經由全橋弋 電路103之開關切換以轉換為交流電流,透過隔離變壓器乃之 Φ 昇壓’分時序對直流輸出電路1〇5之直流輸出電容(:。充電並提 供能量給直流輸出負載及,當第一電感電流L或第二電感電流 b透過隔離變壓器7;昇壓過程中,因隔離變壓器乃存在洩漏電 感h,第一電感電流L或第二電感電流L無法即時傳遞至隔離 變壓器7;,因此會對第一開關$或第二開關&寄生電容充電, 一般開關之寄生電容值皆很小,導致開關截止時將產生電壓突 波,易對開關造成損壞,所以本轉換器加入主動式箝制電路ι〇4 •以解決此問題,第一開關、或第二開關&截止時,第一電感電 流y或第二電感電流L可透過箝制開關&寄生二極體對箝制電 容Cc充電,可有效箝制開關電壓以避免突波現象發生,之後再 將推制開關知導通,將儲存於箝制電容&之能量透過隔離變壓 器乃對直流輸出電路1〇5供電。 本發明所揭不高昇壓式隔離型雙輸入電源轉換器依供電情 形可刀為四種狀態.單輸入電源獨立供電、雙輸入電源同時供 1351806 電、雙輪入電源分別供電與充電以及輸出電源反饋。當第一輸 入電塵源W第二輸人電壓源[兩者其中之—發生故障,或是 電源管理系統因應不同輸出負載及節省能源之目的欲 -輸入電壓源γ或第二輸入電壓源n不輸出功率時,可將第一 電源開關〜或第二電源開關〜截止,其中第_電源開關〜及 第二電源開心2可使用訊號㈣之繼電〇以實現,完成電源 切離之目的。 本發明改善先前技術之原理及對照功效如下: 1·雙輸入電源雙向轉換器架構:本發明可同時達成雙輸入電 源轉換以及電能傳遞具雙向之功效,可節省額外需要電源 雙向傳遞之轉換器,或是節省額外雙電源輸入需求之轉換 器,因此非常適合應用於現今電源供應系統發展潮流中, 具電源儲存裝置之混合型電源供應系統。 2·具高昇壓比及電氣隔離之特性:採用隔離變壓器達成高昇 壓比及電氣隔離之特性,第一輸入電壓源γ及第二輸入電壓 源G之接地點分別與直流輸出電路105之直流輸出電壓卩 之接地點分隔’且可透過隔離變壓器7;匝數比為1:„將輸出 電壓大大提升,非常適合輸入電源為潔淨能源,轉換其直 流低壓至直流高壓以利後級電源應用。 3.高壓側及低壓側開關耐壓耐流匹配:透過全橋式電路105 中隔離變壓器7;將全橋式電路105分隔成所需低耐壓高耐 17 流開關之低壓側第三開關&、第四開關\、第五開關&及第 六開關&,以及所需高耐壓低耐流開關之高壓側第七開關 A、第八開關&、第九開關&及第十開關,可容易選擇 功率半導體開關以有效降低開關導通損失及切換損失,達 成高轉換效率之功效。 輸入電流連續:第一電感々及第二電感l2具電流連續特性, 可於輸入電源端擷取出較小漣波之輸入電流,當應用於潔 淨能源為輸入電源時,可有效濾除電流漣波及避免損害潔 淨能源裝置,延長潔淨能源裝置之使用壽命。 主動式電壓箝制:透過主動式箝制電路104之箝制開關知提 供電流路徑以及箝制電容Cc穩壓,將全橋式電路1〇5中低 壓側之第三開關s3'第四開關《s4、第五開關又及第六開關\ 截止時之開關電壓箝制於箝制電容電壓Fcc,且第一電源電 路101之第一開關A和第二電源電路102之第二開關^截止 時開關電壓亦箝制於箝制電容電壓Kcc,解決因隔離變壓器 乃存在洩漏電感4所造成之電壓突波,箝制電容Q可有效 吸收第一電感電流仏或第二電感電流L與洩漏電感電流心 之差,之後再將箝制開關&導通,將儲存於箝制電容cc之 月&量透過隔離變壓器乃再次對直流輸出電路1〇5供電。 導通損失大幅降低:當操作於雙輸入電源同時供電狀態 下,當第一開關5;導通且第二開關&截止時,第一開關電流 1351806 減少至第一電感電流l與第二電感電流z.i2之差,同理, 當第二開關<s2導通且第一開關&截止時,第二開關電流 減少至第二電感電流L與第一電感電流L之差,因此導通 損失可大幅降低,對於應用於輸入電源為低電壓高電流之 潔淨能源時,本發明之轉換器可成功減小導通損失,以進 一步提升轉換效率。 7.功率半導體開關所承受電壓與輸入電壓無關:功率半導體 # 開關所承受電壓僅與直流輸出電壓及隔離變壓器之匝數比 有關’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。 【實施方式】 本發明所揭示高昇壓式隔離型雙輸入電源轉換器之第一較 佳實施例之電路架構簡化後等效電路如圖二所示,並定義電壓 •及電流符號於圖二,隔離變壓器rr表示為理想變壓器厂及洩漏 電感A ’理想變壓器忑包含理想變壓器一次側%及理想變壓器 二次侧',假設直流輸出電容(^及箝制電容Cc夠大,直流輸出 電路105可等效為直流輸出電壓源箝制電容電壓Fcc為固定 值’並假设所有半導體元件均為理想元件,可忽略開關及二極 體之導通壓降’依本轉換器之供電情形可分為四種狀態:單輸 入電源獨立供電、雙輸入電源同時供電、雙輸入電源分別供電 與充電以及輸出電源反饋。 (金)單輪入電源獨立供電狀態 (一)第一輪入電壓源獨立供電 -第-輸人電壓源G發生故障時’或電源管理系統因應不 同輸出負栽及節省能源之目#’欲調節第二輸人電㈣匕不輸 出力率時,可將第二電源關&截止以完成電源切離之目的, 並使第二開關4持續導通,此時第—輸人電㈣J可於獨立供 電狀態下操作;第—輸人電虔源^於獨立供電狀態之電麼電流 時序波形如圓三所示,定義開關切換週期時間'、第—㈣責 任週期4以及㈣㈣責任職《,由於電輯作之對稱性, 在此分析前半個開關切換週期0.5&,而電路操作模式如圖四所 示。 1.模式一 [ί。〜當時間ί = ί。時,將第一開關&、第四開關& 及第五開關&截止,此時第二開關冬、第三開關冬及第六開 關*S6仍處於導通狀態;第一開關q、第四開關&及第五開關 &上電壓均箝制等同於箝制電容電壓,在此死區時間 内,第一電感電流L流經箝制開關5^寄生二極體,箝制開關 電流iDs,«:為負,對箝制電容Cc充電,第一電感電流l、理想 變壓器一次側電流、及箝制開關電流Zdwc可分別表示為 之1 ⑺= (’ii +0-5WT~(Kc)(i-io) (1) im(t) = Y^Vcc-~)(t-t〇) (2) 1351806 ZD5,ic(〇 = ^i(〇-itl(i) (3) =^c(4 +Ld~nV.L·- V.L. nLsh 其中L代表第-電感電流L平均值,A代表第一電感電流 漣波’其定義為第一電感電流最大值減去第一電感電流最小 值。由式(2)可得知理想變壓器一次側電流‘由零漸增此 電流可感應出理想變壓器二次側電流k,經第七開關&及 第十開關*S1()寄生二極體對直流輸出電壓源4供電。[14] M. Marchesoni and C. Vacca, <cNew dc-dc converter for energy storage system interfacing in fuel cell hybrid electric vehicles, IEEE Trans. Power Electron., vol. 22, no. 1, pp. 301-308 The first diagram shows the circuit architecture of the first preferred embodiment of the high-boosting isolated dual-input power converter 0 of the present invention, which is composed of a first power supply circuit 101 and a second power supply circuit 102. a full bridge circuit 103, an active clamp circuit 104, and a DC output circuit 105, wherein the first power circuit ιοί is composed of a first input voltage source β, a first power switch, a first capacitor C, a first inductor L, and The first DC switch 1 is composed of a second input voltage source & a second power switch &2; a second capacitor C2; a second inductor L2; and a second switch & The full bridge circuit 103 is composed of a third switch & a fourth switch, a fifth switch, a φ sixth switch & a seventh switch *^7, an eighth switch & a ninth switch fork, a tenth switch core, and Isolation transformer 2: composed of isolation transformer 7; package The primary side of the isolation transformer and the secondary side of the isolation transformer have a turns ratio of 1:«, and the coupling coefficient is &; the active clamp circuit 104 is composed of a clamp switch and a clamp capacitor (the DC output circuit 105 is composed of a DC output capacitor). Q and DC output load\, DC output capacitor C. The upper voltage is the DC output voltage. The input power of the high-boost isolated dual-input power converter disclosed in the present invention, that is, the first input voltage source ^; and the second The voltage source factory 2 can be rectified into a DC power supply by a battery, a super capacitor 'fuel electric power, a solar photovoltaic 15 1351806 pool, a direct current wind power generator or an alternating current wind power generator as a direct current power supply. The first power supply circuit 101 and the second power supply circuit 1 〇2 mainly converts the electric energy in the form of the voltage source of the first input voltage source γ and the second wheel-in voltage source C into the first inductor current l and the second inductor respectively through the switching of the first switch & and the second switch A The current is presented in the form of current source power, and the two DC power sources are switched by the switch of the full bridge circuit 103 to be converted into an alternating current, which is passed through the isolation transformer. Boost 'minute timing to DC output circuit 1〇5 DC output capacitor (:. charge and provide energy to the DC output load and when the first inductor current L or the second inductor current b passes through the isolation transformer 7; during the boosting process Because the isolation transformer has a leakage inductance h, the first inductor current L or the second inductor current L cannot be immediately transmitted to the isolation transformer 7; therefore, the first switch $ or the second switch & parasitic capacitance is charged, and the general switch The parasitic capacitance value is very small, which will cause voltage surge when the switch is turned off, which is easy to damage the switch. Therefore, the converter is added to the active clamp circuit ι〇4 to solve this problem, the first switch, or the second switch & When the cut-off, the first inductor current y or the second inductor current L can charge the clamp capacitor Cc through the clamp switch & parasitic diode, which can effectively clamp the switch voltage to avoid the occurrence of a surge phenomenon, and then the push switch is known. Turning on, the energy stored in the clamp capacitor & is passed through the isolation transformer to supply power to the DC output circuit 1〇5. The high-boosting isolated double-input power converter disclosed in the present invention can be used in four states according to the power supply situation. The single-input power supply is independently supplied, and the dual-input power supply simultaneously supplies power and charging of the 1351806 electric power supply and the dual-wheel power supply, and the output power supply. Feedback. When the first input electric dust source W is the second input voltage source [both of which are faulty, or the power management system is intended to respond to different output loads and save energy - input voltage source γ or second input voltage source n When the power is not output, the first power switch ~ or the second power switch may be turned off, wherein the _ power switch ~ and the second power supply happy 2 can use the relay of the signal (4) to achieve the purpose of power cut-off. The invention improves the principle and the control effect of the prior art as follows: 1. Double-input power bidirectional converter architecture: The invention can simultaneously achieve dual-input power conversion and power transmission with bidirectional effect, and can save additional converters requiring two-way power transmission. It is also a converter that saves the need for additional dual power input requirements, making it ideal for hybrid power supply systems with power storage devices in today's power supply systems. 2. High-boost ratio and electrical isolation: The isolation transformer is used to achieve high boost ratio and electrical isolation. The grounding point of the first input voltage source γ and the second input voltage source G and the DC output of the DC output circuit 105 are respectively The grounding point of the voltage 分隔 is separated and can pass through the isolating transformer 7; the turns ratio is 1: „The output voltage is greatly improved, which is very suitable for the input power supply to be clean energy, and convert its DC low voltage to DC high voltage for the later stage power application. High-voltage side and low-voltage side switch withstand voltage and current matching: through the isolation transformer 7 in the full-bridge circuit 105; the full-bridge circuit 105 is divided into the low-voltage side third switch of the required low-voltage high-resistance 17-flow switch & , the fourth switch \, the fifth switch & and the sixth switch &, and the high voltage side seventh switch A, the eighth switch & the ninth switch & The switch can easily select the power semiconductor switch to effectively reduce the switch conduction loss and switching loss, and achieve the effect of high conversion efficiency. The input current is continuous: the first inductor 々 and the second inductor l2 have continuous current The input current of the smaller chopping wave can be taken out at the input power terminal. When applied to the clean energy source as the input power source, it can effectively filter out the current chopping and avoid damage to the clean energy device, prolonging the service life of the clean energy device. Clamping: through the clamp switch of the active clamp circuit 104, the current path and the clamp capacitor Cc are regulated, and the third switch s3' of the full-bridge circuit 1〇5 is connected to the fourth switch “s4, the fifth switch and The switching voltage of the sixth switch \off is clamped to the clamp capacitor voltage Fcc, and the switch voltage is clamped to the clamp capacitor voltage Kcc when the first switch A of the first power supply circuit 101 and the second switch of the second power supply circuit 102 are turned off. Solving the voltage surge caused by the leakage transformer 4 in the isolation transformer, the clamping capacitor Q can effectively absorb the difference between the first inductor current 仏 or the second inductor current L and the leakage inductor current center, and then turn on the clamp switch & Passing the month & amount stored in the clamp capacitor cc through the isolation transformer again supplies power to the DC output circuit 1〇5. The conduction loss is greatly reduced: when operating In the simultaneous power supply state of the dual input power supply, when the first switch 5 is turned on and the second switch & is turned off, the first switch current 1351806 is reduced to the difference between the first inductor current 1 and the second inductor current z.i2, similarly When the second switch <s2 is turned on and the first switch & is off, the second switch current is reduced to the difference between the second inductor current L and the first inductor current L, so the conduction loss can be greatly reduced, and is applied to the input power source. For low-voltage, high-current clean energy, the converter of the present invention can successfully reduce the conduction loss to further improve the conversion efficiency. 7. The voltage of the power semiconductor switch is independent of the input voltage: the power semiconductor # switch is only subjected to the voltage The DC output voltage and the turns ratio of the isolation transformer are related to this application. This feature is more suitable for power conversion applications where the DC input voltage varies widely. [Embodiment] The circuit structure of the first preferred embodiment of the high-boost isolation type dual-input power converter disclosed in the present invention is simplified as shown in FIG. 2, and the voltage and current symbols are defined in FIG. Isolation transformer rr is expressed as an ideal transformer factory and leakage inductance A 'ideal transformer 忑 contains ideal transformer primary side % and ideal transformer secondary side', assuming DC output capacitance (^ and clamping capacitor Cc is large enough, DC output circuit 105 can be equivalent Capacitor capacitor voltage Fcc is fixed for the DC output voltage source 'and assumes that all semiconductor components are ideal components, and the turn-on voltage drop of the switch and the diode can be ignored. According to the power supply of the converter, it can be divided into four states: Input power supply independent power supply, dual input power supply at the same time, dual input power supply separately and charging and output power feedback. (Gold) single wheel input power supply independent power supply state (1) first round input voltage source independent power supply - first - input voltage When the source G fails, or the power management system responds to different output loads and saves energy. #'To adjust the second input power (4)匕When the force rate is output, the second power source can be turned off & off to complete the power cut-off, and the second switch 4 is continuously turned on. At this time, the first-to-be-powered (four) J can be operated under the independent power supply state; The power supply current source is in the state of independent power supply. The current timing waveform is as shown in circle 3. The switch switching cycle time is defined, the - (four) responsibility cycle 4 and (4) (four) responsibility. "Because of the symmetry of the electric series, here The first half of the switch switching cycle is 0.5& and the circuit operating mode is shown in Figure 4. 1. Mode one [ί.~ When time ί = ί., the first switch & the fourth switch & The five switches & off, at this time, the second switch winter, the third switch winter and the sixth switch *S6 are still in the on state; the first switch q, the fourth switch & and the fifth switch & Clamping the capacitor voltage, during this dead time, the first inductor current L flows through the clamp switch 5^ parasitic diode, clamps the switch current iDs, «: is negative, charges the clamp capacitor Cc, the first inductor current l, ideal Transformer primary current, and clamp switch current Zdw c can be expressed as 1 (7) = ('ii +0-5WT~(Kc)(i-io) (1) im(t) = Y^Vcc-~)(tt〇) (2) 1351806 ZD5,ic (〇= ^i(〇-itl(i) (3) =^c(4 +Ld~nV.L·- VL nLsh where L represents the average value of the first inductor current L and A represents the first inductor current ripple] It is defined as the maximum value of the first inductor current minus the minimum value of the first inductor current. It can be known from equation (2) that the primary current of the ideal transformer is increased by zero. This current can induce the secondary current k of the ideal transformer. The seventh switch & and the tenth switch *S1() parasitic diode supply power to the DC output voltage source 4.

2.模式二[(〜&]:模式二為箝制開關第七開關&及第十 開關&。導通期間,第七開關&及第十開關心零電壓導通並 且以同步整流方式取代寄生二極體之電流,可減小開關導通 損失’而箝制開關&零電壓導通且可提供箝制開關電流ζ·2. Mode 2 [(~&]: Mode 2 is the clamp switch seventh switch & and the tenth switch & during the conduction period, the seventh switch & and the tenth switch core zero voltage is turned on and replaced by synchronous rectification The current of the parasitic diode can reduce the switch conduction loss' while the clamp switch & zero voltage is turned on and can provide the clamp switch current ζ·

DS,SCDS, SC

正方向路徑,第一電感電流L、理想變壓器一次側電流^及 柑制開關電流zossc仍可表示如式(1)至式(3)所示,箝制開關 電么|(· zns,sc流經零點且其換相時間為ί = ί61,將心sc = 〇代入式 (3)可求得心如式(4)所示。 hx=t, + LxLk{ILX +〇.5A^)[Fcc(L, + 1,)-¾ -^ΑΓ1 (4) 當時間之後,箝制開關電流zDSSC為正,將原儲存於箝制 電容Cc之能量’與第一電感電流L一併匯集至理想變壓器 一次側%,理想變壓器一次側電流^持續漸增,感應出理 想變壓器二次侧電流k經第七開關《S7及第十開關&。對直流 輪出電壓源4供電β時間/ = 6時,理想變壓器一次側電流^ 21 1351806 最大值可表示為 ^)=*d*^)(w。) (5) 其中時間’2可表示為,2=,。+(05_05《_桃。模式一至模式 一期間’沒漏電感跨壓心與耦合係數灸關係式可表示為 (6) 根據柯希何夫電壓定律(Kirchh〇ff,s Current Law),迴路電壓 方程式表示如下:The positive direction path, the first inductor current L, the ideal transformer primary current ^ and the citrus switch current zossc can still be expressed as shown in equations (1) to (3), and the clamp switch is electrically | (· zns, sc flows through Zero point and its commutation time is ί = ί61, and the heart sc = 〇 is substituted into equation (3) to find the heart as shown in equation (4). hx=t, + LxLk{ILX +〇.5A^)[Fcc( L, + 1,) -3⁄4 -^ΑΓ1 (4) After the time, the clamp switch current zDSSC is positive, and the energy stored in the clamp capacitor Cc is collected together with the first inductor current L to the primary side of the ideal transformer. The ideal transformer primary side current ^ continues to increase, inducting the ideal transformer secondary side current k through the seventh switch "S7 and tenth switch & When the DC output voltage source 4 is supplied with β time / = 6, the ideal transformer primary current ^ 21 1351806 maximum value can be expressed as ^) = * d * ^) (w.) (5) where time '2 can be expressed as , 2=,. +(05_05 "_ peach. Mode 1 to mode 1" no leakage inductance across the core and coupling coefficient moxibustion can be expressed as (6) according to Kirchh〇ff, s Current Law, loop voltage The equation is expressed as follows:

Vcc~^Lk~vm=〇 ⑺ 其中理想變壓器-次側跨壓。將式⑹代入式⑺, 箝制電容電壓Fcc可改寫為Vcc~^Lk~vm=〇 (7) where the ideal transformer - the secondary side cross-pressure. Substituting equation (6) into equation (7), the clamp capacitor voltage Fcc can be rewritten as

Vrr=~L.y CC nk dc (8) 亦即第一開關&、第四開關&及第五開關&電壓均箝制於 4/(从)’而第八開關\及第九開關&上電壓均箝制於匕。 3·模式二h〜g:當時間ί = 6時,將箝制開關&、第七開關矣 及第十開關心截止,致使箝制開關電流心尤降低至零以及 推制開關電流上升至箝制電容電壓厂,此時箝制開關 源極對第二輸入電壓源厂2之地點相對電壓為零伏特,且第 一開關電慶b、第四開關電壓及第五開關電壓V_降 低至零伏特,第一輸入電壓源γ對第一電感Α充電,由於存 在凜漏電感厶,箝制開關電流降低至零之速度較理想變 22 1351806 壓器一次側電流^降低至零之速度快,當箝制開關電流 降低至零時,第四開關&及第五開關&之寄生二極體以極小 電流導通以銜接理想變壓器一次側電流^與第一電感電流 y之差’理想變壓器一次側電流‘近乎等於第一電感電流 L,而洩漏電感A上迴路電壓方程式可表示為= 〇, 理想變壓器一次侧電流k以_Krfc/nLA之斜率遞減,洩漏電感 A之能量透過變壓器持續對直流輸出電壓源4供電。 4. 模式四[G〜^4]:當時間ί = ί3時,將第一開關&導通,此時第 二開關4、第三開關&及第六開關叉仍處於導通狀態,由於 第一開關5;導通前電壓已降至零伏特,第一開關&導通具零 電壓切換之特性,第一開關&導通後,第一輸入電壓源^持 續對第一電感4充電,第一電感電流L呈線性增加;模式四 中當理想變壓器電流已重置為零,理想變壓器上跨壓亦為 零’因此第七開關&、第八開關&、第九開關^及第十開關 \上電壓均箝制於^/2。 5. 模式五h〜當時間時,將第四開關&及第五開關& 導通,由於第四開關\及第五開關&導通前電壓已降低至零 伏特,第四開關\及第五開關&導通具零電壓切換之特性, 而第一電感A仍處於充電狀態,第一電感電流b根據流經路 徑之線上電阻,以分流方式流經第一開關$、第三開關&串 聯第四開關&及第五開關&串聯第六開關&等三條路徑。 23 依據伏秒平衡(voltage_second Balance)理論,開關切換周 期内第-電感A之平均電壓為零,其關係式可表示為 m + 2dd)Ts + (F, - vcc)(l -dx- 2dd)Ts = 0 (9a)Vrr=~Ly CC nk dc (8), that is, the first switch & the fourth switch & and the fifth switch & voltage are clamped to 4/(s) and the eighth switch and the ninth switch & The upper voltage is clamped to the crucible. 3. Mode 2h~g: When time ί = 6, the clamp switch & seventh switch 矣 and the tenth switch core are cut off, causing the clamp switch current to drop to zero and the push switch current to rise to the clamp capacitor. The voltage factory, at this time, the voltage of the clamp switch source to the second input voltage source factory 2 is zero volt, and the first switch electric b, the fourth switch voltage and the fifth switch voltage V_ are reduced to zero volts, An input voltage source γ charges the first inductor ,, because of the leakage inductance 厶, the clamp switch current is reduced to zero, and the speed is better than 22 1351806. The primary side current of the press is reduced to zero, and the clamp switch current is reduced. At zero o'clock, the parasitic diode of the fourth switch & and the fifth switch & is turned on with a very small current to connect the difference between the primary current of the ideal transformer and the first inductor current y 'the ideal transformer primary current' is almost equal to An inductor current L, and the loop voltage equation on the leakage inductor A can be expressed as = 〇, the primary transformer current k is decremented by the slope of _Krfc/nLA, and the energy of the leakage inductor A is continuously transmitted through the transformer. DC output supply voltage source 4. 4. Mode 4 [G~^4]: When the time ί = ί3, the first switch & is turned on, at this time, the second switch 4, the third switch & and the sixth switch fork are still in the on state, due to the a switch 5; the voltage before the conduction has dropped to zero volts, the first switch & conduction has a zero voltage switching characteristic, after the first switch & conduction, the first input voltage source ^ continues to charge the first inductor 4, first The inductor current L increases linearly; when the ideal transformer current has been reset to zero in mode 4, the ideal transformer crossover voltage is also zero', so the seventh switch & eighth switch & ninth switch ^ and tenth switch \Up voltage is clamped to ^/2. 5. Mode 5h~ When the time is up, the fourth switch & and the fifth switch & turn on, because the fourth switch \ and the fifth switch & before the conduction voltage has been reduced to zero volts, the fourth switch \ and The five-switch & conduction has the characteristic of zero voltage switching, and the first inductor A is still in a charging state, and the first inductor current b flows through the first switch $, the third switch & in a shunt manner according to the resistance on the line flowing through the path; Three paths of the fourth switch & and the fifth switch & series sixth switch & 23 According to the voltage_second balance theory, the average voltage of the first-inductor A is zero in the switching period, and the relationship can be expressed as m + 2dd)Ts + (F, - vcc)(l -dx- 2dd) Ts = 0 (9a)

Vcc =~~~--V l~d\~^dd (9b) 根據式⑻及式(9),並假設死區時时任週期《很〗、,第一輪入 電壓源與直流輸出電屋源匕關係可表示為 ^dc~~--nkV. l~dx 1 (10) 而第一電感電流漣波可表示為Vcc =~~~--V l~d\~^dd (9b) According to equations (8) and (9), and assume the dead zone time period "very", the first round of voltage source and DC output The relationship between the source and the source can be expressed as ^dc~~--nkV. l~dx 1 (10) and the first inductor current chopping can be expressed as

VATSVATS

(二)第二輸入電壓源獨立供電 當第一輸入電壓源K發生故障時,或電源管理系統因應不 同輸出負載及節省能源之目的,欲調節第一輸入電壓源K不輸 φ出功率時,可將第一電源開關心,截止以完成電源切離之目的, 並使第一開關g持續導通,此時第二輸入電壓源G可於獨立供 電狀態下操作;第二輸入電壓源匕於獨立供電狀態之電壓電流 時序波形如圖五所示,定義第二開關責任週期4,由於電路操 作之對稱性,在此分析前半個開關切換週期〇57^,而電路操作 模式如圖六所示。 模式一 [/。〜Μ :當時間ί =(。時,第一開關$、第三開關兄及 第六開關叉仍處於導通狀態,而第四開關&及第五開關<s5已 24 1351806 截止一段時間,此時將第二開關&載止;第二開關&、第四 開關\及第五開關叉上電壓均箝制等同於箝制電容電壓 tc,在此死區時間,第二電感電流ii2流經箝制開關& 寄生二極體,箝制開關電流為負,對箝制電容充電, 理想變壓器一次側電流^、第二電感電流及箝制開關電 流可分別表示為式(2)、式(12)及式(13)。 iL2(t) = (IL2 + 〇.5ML2) + ±(V2 - Vcc){t -1,) (12) ^Ds.scif) = ^i(0 ~ hii{) =[^^^^。)_队2+。5峋)(13) 其中L代表第二電感電流L平均值,代表第二電感電流 漣波,其定義為第二電感電流最大值減去第一電感電流最小 值。由式(2)可得知理想變壓器一次側電流‘由零漸增,此 電流可感應出理想變壓器二次側電流心2,經第七開關&及 φ 第十開關\寄生二極體對直流輸出電壓源匕c供電。 2.模式二[[〜模式二為箝制開關知、第七開關&及第十 開關A。導通期間’第七開料及第十關&零電壓導通並 且以同步整流方式取代寄生二極體之電流,可減小開關導通 損失㈣制開關知零電愿導通且可提供籍制開關電流^。 正方向路理想變壓器—次側電流、、第二電感電流^及 箝制開關電f歐仍可表示如式⑺、式⑴)及式⑴)所示, 箝制開關電流W夂流經零點且其換相時間為,=,62,將 25 1351806 sc =〇代入式(13)可求得如式(14)所示。 hi ~t〇 + LlLk{lL1 + 〇.5Aii2)[fcc(^* + A) -丨 (14) 當時間(之後’箱制開關電流1ds,sc為正,將原儲存於藉制 電容Cc之能量,與第二電感電流L 一併匯集至理想變壓器 一次側%,理想變壓器一次側電流/奶持續漸增,感應出理 想變壓器二次側電流心2經第七開關尽及第十開關心對直流 輸出電壓源匕c供電。時間i = G時,理想變壓器一次側電流k 最大值亦可表示如式(5)所示,時間(2可表示為 L=G + (〇.5-0·5《-毛凡。模式一至模式二期間,洩漏電感A 跨壓與耦合係數&關係式亦可表示如式(6)所示,根據柯希荷 夫電壓定律推導,箝制電容電壓Fcc可改寫如式(8)所示,亦 即第二開關4、第四開關\及第五開關冬電壓均箝制於 4/(甿)’而第八開關\及第九開關^上電壓均箝制於匕。 3.模式三h〜當時間i = q時,將箝制開關&、第七開關& 及第十開關心截止,致使箝制開關電流心尤降低至零以及 箝制開關電流Vsc上升至箝制電容電壓,此時箝制開關 &源極對第二輸入電壓源&之地點相對電壓為零伏特,且第 二開關電壓Vi2、第四開關電壓^及第五開關電壓⑹ 降低至零伏待’第二輸入電壓源&對第二電感々充電,由於 存在泡漏電感V箝制開關電流‘降低至零之速度較理想 變壓器A側電流^降低至零之速度快,當籍制開關電流 26 1351806 W降低至零時,第四開關&及第五開關&之寄生二極體以 極小電流導通以銜接理想變壓器一次側電〜與第二電感 電流L之差,理想變壓器一次側電流^近乎等於第二電感 電流L,而洩漏電感4上迴路電壓方程式可表示為 ,理想删一次側電流…匕〆峋之斜率遞 減,洩漏電“之能量透過變壓器持續對直流輸出電壓源 乙供電。 4_模式四[,广g:當時間^時,將第二開關&、第四開關& 及第五開關。導通,此時第-開關V第三開關&及第六開 ’仍處於導通狀態’由於第二開關&、第四開關&及第五 開關&導通前電Μ已降至零伏特’第二開關&、第四開關& 及第五開關4導通具零電壓切換之特性,第二開關&導通 後,第二輸入電壓源K持續對第二電感&充電,第二電感電 流L呈線性增加,第二電感電流G根據流經路徑之線上電 阻,以分流方式流經第二開關&、第三開關&串聯第四開關 &及第五開關&串聯第六開關&等三條路徑;模式四中當理 想變壓器電流已重置為零後’理想變壓器上跨壓亦為零,因 此第七開關S?、第八開關&、第九開關<s9及第十開關心上電 壓均箝制於匕,/2。 5.模式五1>4 :當時間ί = ί4時,將第三開關《S3及第六開關& 截止,第三開關A及第六開關&零電壓截止,而第二電感& 27 1351806 仍處於充電狀態’第二電感電流L以單—路徑流經第二開關 A。 依據伏秒平衡理論,開關切換周期内第二電感乓之平均電 壓為零,其關係式可表示為 V2{d2 + 2dd)Ts + (V2 — Vcc)(\ — d2— 2dd)Ts = 0 1(2) The second input voltage source is independently powered. When the first input voltage source K fails, or the power management system responds to different output loads and saves energy, if the first input voltage source K is to be output, the power is not output. The first power switch can be turned off to complete the power cut-off, and the first switch g is continuously turned on. At this time, the second input voltage source G can be operated in an independent power supply state; the second input voltage source is independent The voltage and current timing waveform of the power supply state is shown in Figure 5. The second switch duty cycle is defined. Due to the symmetry of the circuit operation, the first half of the switching cycle is analyzed 〇57^, and the circuit operation mode is as shown in Fig. 6. Mode one [/. ~Μ: When time ί = (., the first switch $, the third switch brother and the sixth switch fork are still in the on state, and the fourth switch & and the fifth switch <s5 has been 24 1351806 for a period of time, At this time, the second switch & the second switch &, the fourth switch \ and the fifth switch fork voltage clamp are equal to the clamp capacitor voltage tc, during this dead time, the second inductor current ii2 flows through Clamp switch & parasitic diode, clamp switch current is negative, charge the clamp capacitor, ideal transformer primary current ^, second inductor current and clamp switch current can be expressed as equation (2), formula (12) and (13) iL2(t) = (IL2 + 〇.5ML2) + ±(V2 - Vcc){t -1,) (12) ^Ds.scif) = ^i(0 ~ hii{) =[^^ ^^. )_ Team 2+. 5峋) (13) where L represents the average value of the second inductor current L, representing the second inductor current ripple, which is defined as the second inductor current maximum minus the first inductor current minimum. It can be known from equation (2) that the primary current of the ideal transformer 'increasing from zero, this current can induce the secondary side current core 2 of the ideal transformer, via the seventh switch & and φ the tenth switch\parasitic diode pair The DC output voltage source 匕c is powered. 2. Mode 2 [[~ Mode 2 is the clamp switch, the seventh switch & and the tenth switch A. During the conduction period, the 'seventh material and the tenth level & zero voltage conduction and replace the current of the parasitic diode by synchronous rectification, which can reduce the switch conduction loss (4), the switch knows that the electric power is turned on and can provide the switch current ^ . The positive direction transformer of the positive direction—the secondary current, the second inductor current ^, and the clamped switch power f can still be expressed as shown in equations (7), (1), and (1), and the clamped switch current W 夂 flows through the zero point and changes The phase time is, =, 62, and 25 1351806 sc = 〇 substituting into equation (13) can be obtained as shown in equation (14). Hi ~t〇+ LlLk{lL1 + 〇.5Aii2)[fcc(^* + A) -丨(14) When time (after 'box switching current 1ds, sc is positive, the original is stored in the borrowing capacitor Cc The energy is collected together with the second inductor current L to the primary side of the ideal transformer. The current of the ideal transformer is gradually increased. The current of the secondary side of the ideal transformer is induced by the seventh switch and the tenth switch. DC output voltage source 匕c power supply. When time i = G, the maximum value of the primary transformer current k can also be expressed as shown in equation (5), time (2 can be expressed as L = G + (〇.5-0· 5 "- Mao Fan. During mode 1 to mode 2, the leakage inductance A cross-over voltage and coupling coefficient & can also be expressed as shown in equation (6). According to Kirchoff's voltage law, the clamp capacitor voltage Fcc can be rewritten as shown. (8), that is, the second switch 4, the fourth switch \ and the fifth switch are both clamped to the voltage of 4/(氓)', and the voltages of the eighth switch and the ninth switch are clamped to the clamp. Mode 3 h~ When time i = q, the clamp switch & seventh switch & and the tenth switch core are turned off, causing the clamp switch The flow center is especially reduced to zero and the clamp switch current Vsc rises to the clamp capacitor voltage. At this time, the clamp switch & source is opposite to the second input voltage source & the relative voltage is zero volt, and the second switch voltage Vi2, fourth The switching voltage ^ and the fifth switching voltage (6) are reduced to zero volts to be 'the second input voltage source & charging the second inductor ,, due to the presence of the bubble leakage inductance V clamping the switching current 'lower to zero speed than the ideal transformer A side current ^The speed is reduced to zero. When the switch current 26 1351806 W is reduced to zero, the parasitic diodes of the fourth switch & and the fifth switch & are turned on with a very small current to connect the ideal transformer to the primary side. The difference between the second inductor current L, the ideal transformer primary current ^ is almost equal to the second inductor current L, and the loop voltage equation on the leakage inductor 4 can be expressed as, ideally, the slope of the primary side is reduced... The energy is continuously supplied to the DC output voltage source B through the transformer. 4_Mode 4 [, Wide g: When the time is ^, the second switch & the fourth switch & and the fifth switch. Pass, at this time, the first switch V third switch & and the sixth switch 'is still in the on state' because the second switch & the fourth switch & and the fifth switch & the pre-conduction power has been reduced to zero volts 'The second switch & the fourth switch & and the fifth switch 4 conduct the characteristic of zero voltage switching. After the second switch & is turned on, the second input voltage source K continues to charge the second inductor & The inductor current L increases linearly, and the second inductor current G flows through the second switch & the third switch & series fourth switch & and the fifth switch & series in accordance with the resistance of the line flowing through the path Three switches & three paths; in mode four, when the ideal transformer current has been reset to zero, the ideal transformer has zero crossover voltage, so the seventh switch S?, the eighth switch & the ninth switch <s9 And the voltage on the tenth switch core is clamped to 匕, /2. 5. Mode 5 1 > 4: When time ί = ί4, the third switch "S3 and sixth switch & cut off, the third switch A and the sixth switch & zero voltage cutoff, and the second inductance & 27 1351806 is still in a charging state 'The second inductor current L flows through the second switch A in a single-path. According to the volt-second balance theory, the average voltage of the second inductance ping in the switching period is zero, and the relationship can be expressed as V2{d2 + 2dd)Ts + (V2 - Vcc)(\ - d2 - 2dd)Ts = 0 1

(15a) (15b) 第二輸 V〇c 根據式(8)及式(15),並假設死區時間責任週期毛很小 入電壓源&與直流輸出電壓源ρς關係可表示為 d2 nkV2 (16) 而第二電感電流漣波△。可表示為 △/ 11 2L2(15a) (15b) The second output V〇c is based on equations (8) and (15), and assumes that the dead time period of the duty cycle is small. The voltage source & and the DC output voltage source ρ ς can be expressed as d2 nkV2 (16) The second inductor current is chopped by Δ. Can be expressed as △ / 11 2L2

VATS (17) (貳)雙輸入電源同時供電狀態VATS (17) (贰) dual input power supply simultaneously

第一輸入電壓源K及第二輸入電壓源ρς於雙輸入電源同時 供電狀態’電路分析建構於第-電感電流L大於第二電感電流 L之條件下,此時電壓電流時序波形如圖七所示,由於電路操 作之對稱性,在此分析前半個開關切換週期〇5J;,而電路操作 模式如圖八所示。 模式一 1Λ4]:當時間ί=/〇時,第一開關&、第三開關&及 第六開關5;仍處於導通狀態,而第四開關&及第五開關&已 截止一段時間,此時將第二開關&戴止;第二開關&、第四 28 1351806 開關及第五開關&上電壓均箝制等同於箝制電容電壓 Fcc,在此死區時間毛&内,根據柯希荷夫電流定律 (Kirchhoff’s C_nt !^)推導可得^。化,第一開關電 流心,S1可表示為,相較於第一電感電流Μ完全流經第 -開關V此特性可有效降低開關導通損失,由於第一電感 電流y大於第二電感電流匕2,因此第一開關電流/_為正, 而第二電感電流Q流經第一電源電路及箝制開關^寄生二 • 極體後’再流回第二電感A,此時箱制開關電流“c為負, 對箝制電容Cc充電,理想變壓器一次側電流心1、第二電感 電流b及箝制開關電流亦可分別表示為式(2)、式〇幻 及式(13)。由式(2)可得知理想變壓n _次側電流~丨由零漸 增,此電流可感應出理想變壓器二次側電流^,經第七開 關A及第十開關5^。寄生二極體對直流輸出電壓源匕供電。 2.模式二h〜?2]:模式二為第一段箝制開關知導通期間,在 • 此區間同時將第七開關S7及第十開關〜導通,第七開關… 及第十開關5;。零電壓導通並且以同步整流方式取代寄生二 極體之電流,可減小開關導通損失,而箝制開關&零電壓導 通且可乂供箝制開關電流^冗正方向路徑,理想變壓器一次 側電流V,、第二電感電流心及箝制開關電流&冗仍可表示如 式(2)、式(12)及式(13)所示,箝制開關電流^流經零點且 其換相時間為i = ,將= 〇代入式(丨3)可求得心如式(i 4) 29 所示。當時間/之後,箝制開關電流‘况為正,將原儲存 於箝制電容cc之能量,與第二電感電流L 一併匯集至理想 變壓器一次側Μ,理想變壓器一次側電流k持續漸增,感 應出理想變壓器二次側電流經第七開關\及第十開關心 對直流輸出電壓源4供電.時間i = G時,理想變壓器一次側 電流Μ於第一段箝制開關《sc導通其間最大值可表示如式(5) 所示,時間6可表示為6=心+ (0.5_0.5《_4)7^。模式一至模 式二期間,洩漏電感4跨壓與耦合係數女關係式亦可表示如 式(6)所示,根據柯希荷夫電壓定律推導,箝制電容電壓 可改寫如式(8)所示,亦即第二開關足、第四開關&及第五 開關&電壓均箝制於&/(„&),而第八開關&及第九開關& 上電壓均箝制於L。 模式三h〜y··當時間ί = ί2時,將箝制開關&、第七開關& 及第十開關心截止,致使箝制開關電流降低至零以及 箝制開關電壓1;取上升至箝制電容電壓。,此時箝制開關 &源極對第二輸入電壓源&之地點相對電壓為零伏特,且第 二開關電壓〜2、第四開關電壓”⑽及第五開關電壓⑹ 降低至零伏特,第二輸入電壓源G對第二電感尽充電,由於 存在浅漏電感V籍制開關電流,歡降低至零之速度較理想 變壓器-次側電流〜丨降低至零之速度快,當箝制開關電流 W降低至零時’第四開β! A及第五開關4之寄生二極體以 1351806 極小電流導通以銜接理想變壓器一次側電流^與第二電感 電流L之差,理想變壓器一次側電流k近乎等於第二電感 電流L ’而洩漏電感A上迴路電壓方程式可表示為 vu +〜1=0,理想變壓器一次側電流~丨以—匕/wZ^之斜率遞 減,洩漏電感4之能量透過變壓器持續對直流輸出電壓源 匕供電。The first input voltage source K and the second input voltage source ρ are connected to the dual input power supply at the same time. The circuit analysis is constructed under the condition that the first inductor current L is greater than the second inductor current L, and the voltage and current timing waveform is as shown in FIG. It is shown that due to the symmetry of the circuit operation, the first half of the switching cycle is 〇5J; and the circuit operation mode is as shown in FIG. Mode 1Λ4]: When time ί=/〇, the first switch & the third switch & and the sixth switch 5; are still in the on state, and the fourth switch & and the fifth switch & Time, at this time, the second switch & the second switch & the fourth 28 1351806 switch and the fifth switch & upper voltage clamp are equivalent to the clamp capacitor voltage Fcc, in this dead time hair & According to Kirchhoff's current law (Kirchhoff's C_nt !^) derivation can be obtained ^. The first switching current center, S1, can be expressed as compared with the first inductor current Μ completely flowing through the first switch V. This characteristic can effectively reduce the switch conduction loss, since the first inductor current y is greater than the second inductor current 匕2 Therefore, the first switch current /_ is positive, and the second inductor current Q flows through the first power supply circuit and clamps the switch to the parasitic diode, and then flows back to the second inductor A, and the box switch current "c" Negatively, charging the clamp capacitor Cc, the ideal transformer primary current core 1, the second inductor current b, and the clamp switch current can also be expressed as equation (2), equation, and equation (13), respectively. It can be known that the ideal transformer n _ secondary current ~ 渐 is gradually increased by zero, this current can induce the ideal transformer secondary current ^, through the seventh switch A and the tenth switch 5 ^. Parasitic diode pair DC output Voltage source 匕 power supply 2. Mode 2 h~?2]: Mode 2 is the first segment of the clamp switch. During the conduction period, the seventh switch S7 and the tenth switch are turned on, the seventh switch... and Ten switch 5; zero voltage conduction and replace the parasitic diode with synchronous rectification Current, which can reduce the switch conduction loss, while the clamp switch & zero voltage is turned on and can be used to clamp the switch current ^ redundant positive direction path, ideal transformer primary side current V, second inductor current core and clamp switch current & redundant It can still be expressed as shown in equations (2), (12) and (13), the clamp switch current ^ flows through the zero point and its commutation time is i = , and the = 〇 substitution type (丨3) can be obtained. As shown in equation (i 4) 29, when the time/after, the clamp switch current is positive, the energy stored in the clamp capacitor cc is combined with the second inductor current L to the primary side of the ideal transformer. The primary side current k of the transformer continues to increase, and the secondary current of the ideal transformer is induced to supply power to the DC output voltage source 4 through the seventh switch and the tenth switch core. When the time i = G, the primary current of the ideal transformer is first. The segment clamp switch "sc maximum value can be expressed as shown in equation (5), and time 6 can be expressed as 6 = heart + (0.5_0.5 "_4) 7^. During mode 1 to mode 2, leakage inductance 4 cross-voltage The female relationship with the coupling coefficient can also be expressed as shown in equation (6), according to Ke The Scheffer voltage law is derived, and the clamp capacitor voltage can be rewritten as shown in equation (8), that is, the second switch foot, the fourth switch & and the fifth switch & voltage are clamped to &/(„&) And the eighth switch & and the ninth switch & upper voltage are clamped to L. Mode three h~y·· When time ί = ί2, the clamp switch & seventh switch & and the tenth switch core are cut off, causing the clamp switch current to decrease to zero and the clamp switch voltage to be 1; take rise to the clamp capacitor Voltage. At this time, the clamp switch & source is opposite to the second input voltage source & the relative voltage is zero volt, and the second switching voltage 〜2, the fourth switching voltage ”, and the fifth switching voltage (6) are reduced to zero volts. The second input voltage source G charges the second inductor as much as possible. Because of the shallow leakage inductance V, the switch current is reduced to zero. The speed of the transformer is lower than the ideal transformer-secondary current ~ 丨 is reduced to zero, when the switch current is clamped. When W is reduced to zero, the fourth open β! A and the parasitic diode of the fifth switch 4 are turned on with a very small current of 1351806 to bridge the difference between the primary side current of the ideal transformer and the second inductor current L, and the ideal transformer primary current k It is almost equal to the second inductor current L' and the loop voltage equation on the leakage inductor A can be expressed as vu +~1=0. The slope of the ideal transformer primary current ~丨 decreases with the slope of -匕/wZ^, and the energy of the leakage inductor 4 passes through the transformer. Continuously supply power to the DC output voltage source.

4·模式四[G〜Q]:當時間ί = ί3時,第一開關$丨、第三開關&及 第六開關&仍處於導通狀態,此時將第二開關&、第四開關 \及第五開關&導通,由於第二開關&、第四開關&及第五 開關&導通前電壓已降至零伏特,第二開關&、第四開關& 及第五開關&導通具零電壓切換之特性,第二開關&導通 後,第二輸入電壓源F2持續對第二電感尽充電,此時第一電 感A仍處於充電狀態,第一電感電流一及第二電感電流ii2呈 線性增加,上升斜率分別為γ/々及& ,且第一電感電流L 及第二電感電流L流經路徑,係根據最小之線上電阻分流方 式分佈;模式四中當理想變壓器電流降低為零後,理想變壓 器二次側電壓亦為零,第七開關尽、第八開關&、第九開關 &及第十開關&。上電壓均為匕/2。由於第一開關驅動訊號 2;及第二開關驅動訊號Γ2之對稱切換方式,第一開關驅動訊 號忑及第二開關驅動訊號5重疊為均勻分佈,模式四所經時 間可表示為 ί4 - ί3 = 0.25« + c/2 -1)[。。 31 1351806 5.模式五[q〜ί5]:當時間(=/4時,第二開關&、第四開關&及 第五開關^仍處於導通狀態,此時將第一開關&、第三開關 &及第六開關叉截止;第一開關&、第三開關&及第六開關 &上電壓均箝制等同於箝制電容電壓,在此死區時間 内’根據柯希荷夫電流定律推導可,第二開 關電流iDS_52可表示為Zi2 -Ζ·£1,相較於第二電感電流々2完全流 經第二開關&,此特性可有效降低開關導通損失,由於第一 電感電流Ζ·£|大於第二電感電流L,因此第二開關電流為 負,而第一電感電流L流經箝制開關^寄生二極體及第二電 源電路後,再流回第一電感马,此時箝制開關電流為 負,對箝制電容Cc充電,理想變壓器第一電感電流t、一 次側電流k及箝制開關電流zowc可分別表示為 (18)4. Mode 4 [G~Q]: When time ί = ί3, the first switch $丨, the third switch & and the sixth switch & are still in the on state, and the second switch & The switch \ and the fifth switch & turn on, since the second switch & the fourth switch & and the fifth switch & the voltage before the conduction has dropped to zero volts, the second switch & the fourth switch & The fifth switch & conduction has the characteristic of zero voltage switching. After the second switch & is turned on, the second input voltage source F2 continues to charge the second inductor. At this time, the first inductor A is still in the charging state, and the first inductor current is one. And the second inductor current ii2 increases linearly, and the rising slopes are γ/々 and & respectively, and the first inductor current L and the second inductor current L flow through the path according to the minimum on-line resistance shunting mode; When the ideal transformer current is reduced to zero, the secondary side voltage of the ideal transformer is also zero, the seventh switch, the eighth switch & the ninth switch & and the tenth switch & The upper voltage is 匕/2. Due to the symmetric switching mode of the first switch driving signal 2 and the second switch driving signal Γ2, the first switch driving signal 忑 and the second switch driving signal 5 are evenly distributed, and the mode 4 elapsed time can be expressed as ί4 - ί3 = 0.25« + c/2 -1) [. . 31 1351806 5. Mode 5 [q~ί5]: When time (=/4, the second switch & the fourth switch & and the fifth switch ^ are still in the on state, the first switch & The third switch & and the sixth switch fork are turned off; the first switch & the third switch & and the sixth switch & upper voltage clamp are equivalent to the clamp capacitor voltage, in this dead time period, according to the Kirchhof current The law derivation can be, the second switch current iDS_52 can be expressed as Zi2 - Ζ · £1, compared to the second inductor current 々 2 completely through the second switch &, this characteristic can effectively reduce the switch conduction loss, due to the first inductance The current Ζ·£| is greater than the second inductor current L, so the second switch current is negative, and the first inductor current L flows through the clamp switch parasitic diode and the second power circuit, and then flows back to the first inductor horse. At this time, the clamp switch current is negative, and the clamp capacitor Cc is charged. The ideal transformer first inductor current t, the primary side current k, and the clamp switch current zowc can be expressed as (18), respectively.

lLi(t) = (/„ + 0.5Δ/,!) + ~~(yy _ vcc^t _QlLi(t) = (/„ + 0.5Δ/,!) + ~~(yy _ vcc^t _Q

~1(0 = 一»4) (19) nLiLk +0·5Δζιι) (20) 其中時間q又可表示為G = ί〇+025(1+ΚΚ。由式〇9)可得 去理想變壓器一次側電流〜丨由零漸減,此電流可感應出理想 變壓器二次側電流〜2 ’經第八開關&及第九開關&寄生二極 體對直流輸出電壓源4供電。 32 1351806 6.模式六[is〜g:模式六為第二段箝制開關知導通期間,在 此區間同時將第八開關&及第九開關\導通,第八開關&及 第九開關&零電壓導通並且以同步整流方式取代寄生二極 體之電流,可減小開關導通損失,而箝制開關&零電壓導通 且可提供箝制開關電流心况正方向路徑,第一電感電流L、 理想變壓器一次側電流^及箝制開關電流仍可表示如 式(18)、式(19)及式(20)所示,箝制開關電流心wc流經零點且 其換相時間為ί = ί«,將k,iC=〇代入式(20)可求得如式(21) 所示β = ^4 + 〇.5Δ^)[^(Ζ4 -/,)-¾ +^ΑΓ' (21) 當時間之後,箝制開關電流為正,將原儲存於箝制 電谷Cc之能量,與第一電感電流L 一併匯集至理想變壓器 一次側Μ,理想變壓器一次側電流k為負且持續漸減,感 應出理想變壓器二次側電流心2經第八開關\及第九開關& 對直流輸出電壓源4供電。時間ί=ί6時,理想變壓器一次側 電流k於第二段箝制開關^導通期間最小值可表示如 α’6) = 士 (22) 其中時間匕可表示為㈡4 + (〇.5_〇.5KFs。模式五至模式 六中’茂漏電感矣跨壓與耦合係數灸關係式亦可表示為 (23) v,=~(l-Wc 33 1351806 根據柯希荷夫電壓定律,迴路電壓方程式表示如下:~1(0 = a »4) (19) nLiLk +0·5Δζιι) (20) where time q can be expressed as G = ί〇+025 (1+ΚΚ. From equation 〇9), the ideal transformer can be obtained once. The side current ~ 渐 is gradually reduced by zero, this current can induce the ideal transformer secondary side current ~ 2 ' via the eighth switch & and the ninth switch & parasitic diode to the DC output voltage source 4 power. 32 1351806 6. Mode 6 [is~g: Mode 6 is the second segment of the clamp switch. During the conduction period, the eighth switch & and the ninth switch are turned on, the eighth switch & and the ninth switch & Zero voltage is turned on and the current of the parasitic diode is replaced by synchronous rectification, which can reduce the switch conduction loss, while the clamp switch & zero voltage is turned on and can provide the positive direction path of the clamp switch current state, the first inductor current L, The ideal transformer primary current ^ and the clamp switch current can still be expressed as shown in equations (18), (19) and (20), the clamped switch current center wc flows through the zero point and its commutation time is ί = ί«, Substituting k, iC=〇 into equation (20) can be obtained as shown in equation (21) β = ^4 + 〇.5Δ^)[^(Ζ4 -/,)-3⁄4 +^ΑΓ' (21) When time After that, the clamp switch current is positive, and the energy stored in the clamped electric valley Cc is collected together with the first inductor current L to the primary side of the ideal transformer. The current side k of the ideal transformer is negative and continuously decreases, and the ideal is induced. The secondary side current core of the transformer is supplied to the DC output voltage source 4 via the eighth switch and the ninth switch & . When time ί=ί6, the minimum value of the primary transformer current k of the ideal transformer in the second stage clamp switch can be expressed as α'6) = ± (22) where time 匕 can be expressed as (2) 4 + (〇.5_〇. 5KFs. Mode 5 to Mode 6 'The leakage inductance, cross-pressure and coupling coefficient moxibustion can also be expressed as (23) v,=~(l-Wc 33 1351806 According to Kirchoff's voltage law, the loop voltage equation is expressed as follows:

Vcc+^Lk+vm=〇 其中理想變壓器一次側跨壓%1=_匕/„ (24),箝制電容電壓rcc亦可改寫如式(8)所示,亦即第一開 關$、第三開關&及第六開關怂電壓均箝制於&/(虓),而第 七開關尽及第十開關\上電壓均箝制於4。Vcc+^Lk+vm=〇The ideal transformer primary side span voltage%1=_匕/„ (24), the clamp capacitor voltage rcc can also be rewritten as shown in equation (8), that is, the first switch $, the third switch Both the & and the sixth switch 怂 voltage are clamped to &/(虓), and the seventh switch is clamped to 4 at the tenth switch and the upper voltage.

模式七hy :當時間ί = &時,將箝制開關知、第八開關& 及第九開關&截止,致使箝制開關電流心况降低至零以及箝 制開關電壓v0iS5c上升至箝制電容電壓,此時箝制開關^ 源極對第二輸入電壓源&之地點相對電壓為零伏特,且第一 開關電壓、第三開關電壓v〇以3及第六開關電壓降低 至零伏特,第一輸入電壓源γ對第一電感Α充電,由於存在 漏電感1¾,抽制開關電流降低至零之速度較理想變壓Mode sevenhy: When time ί = &, the clamp switch is known, the eighth switch & and the ninth switch & cut off, causing the clamp switch current state to fall to zero and the clamp switch voltage v0iS5c to rise to the clamp capacitor voltage, At this time, the clamp switch ^ source is opposite to the second input voltage source & the relative voltage is zero volt, and the first switching voltage, the third switching voltage v 〇 is reduced to zero and the sixth switching voltage to zero volts, the first input The voltage source γ charges the first inductor ,, and because of the leakage inductance 13⁄4, the pumping switch current is reduced to zero.

(24) 將式(23)代入式 器一次側電流心1增加至零之速度快,當箝制開關電流心冗降 低至零時,第三開關4及第六開關&之寄生二極體以極小電 流導通以銜接理想變壓器一次側電流、與第一電感電流L 之差,理想變壓器一次側電流k近乎等於第一電感電流L, 而洩漏電感A上迴路電壓方程式可表示為Vu+v〃i=〇,理想 變壓1§ 一次側電流k以匕c / 之斜率遞增’浪漏電感4之能 量透過變壓器持續對直流輸出電壓源Krfc供電。 8.模式八A〜g:當時間/ = 〇時,第土開關&、第四開關\及 34 1351806 第五開關&仍處於導通狀態,此時將第一開關乂導通,由於 第一開關*^導通前電壓已降至零伏特,第一開關&導通具零 電壓切換之特性,第一開關$導通後,第一輸入電壓源K持 續對第一電感4充電,此時第二電感心仍處於充電狀態,第 一電感電流k及第二電感電流zi2呈線性增加,上升斜率分別 為γ/Α及;模式八中當理想變壓器電流為零後,理想 變壓器二次側電壓亦為零,第七開關&、第八開關乂、第九 開關S9及第十開關&上電壓均為&/2。 依據伏秒平衡理論,開關切換周期内第一電感及及第二電 感八之平均電壓為零,其關係式可表示為式(9)及式(15),根據 式(8)、式(9)及式(15) ’並假設死區時間責任週期毛很小,第一 輸入電壓源K、第二輸入電壓源κ及直流輸出電壓源&關係可 表不為(24) The speed at which the current side of the primary side of the equation (23) is increased to zero is fast, and when the current of the clamped switch is reduced to zero, the parasitic diodes of the third switch 4 and the sixth switch & The minimum current is turned on to connect the current of the ideal transformer to the first inductor current L. The ideal transformer primary current k is almost equal to the first inductor current L, and the loop voltage equation on the leakage inductor A can be expressed as Vu+v〃i. =〇, ideal transformer 1§ The primary current k is incremented by the slope of 匕c / 'The energy of the leakage inductance 4 continues to supply the DC output voltage source Krfc through the transformer. 8. Mode 8A~g: When time / = 〇, the earth switch &, the fourth switch \ and 34 1351806 The fifth switch & is still in the on state, at this time the first switch 乂 is turned on, due to the first The voltage of the switch *^ has been reduced to zero volts before the conduction, the first switch & conduction has zero voltage switching characteristics, after the first switch $ is turned on, the first input voltage source K continues to charge the first inductor 4, at this time the second The inductor core is still in a state of charge, and the first inductor current k and the second inductor current zi2 linearly increase, and the rising slopes are respectively γ/Α; and in the eighth mode, when the ideal transformer current is zero, the ideal transformer secondary side voltage is also The voltages of zero, seventh switch & eighth switch 乂, ninth switch S9 and tenth switch & are both & /2. According to the volt-second balance theory, the average voltage of the first inductor and the second inductor eight is zero in the switching period, and the relationship can be expressed as equations (9) and (15) according to equations (8) and (9). And equation (15) 'and assume that the duty cycle of the dead time is small, the first input voltage source K, the second input voltage source κ and the DC output voltage source & relationship can be expressed as

Vdc=T^nkVi=TZJ;n^ (25) 而第一電感電流漣波及第二電感電流漣波aq亦可表示如 式(11)及式(17)所示。 (參)雙輸入電源分別供電與充電狀態 現今電源供應系統發展潮流中,混合型電源供應系統通常 至少具一電源儲存裝置如蓄電池或超電容,提供當另一電源故 障時之持續電力輸出,或是當另一電源啟動暫態時間内之主要 電力輸出’因此電源供應系統需要具有雙向電能傳遞之功能, 35 1351806 使電源儲存裝置具充電及供電迴路❶在此供電狀態分析下·,假 設第二輸入電壓源G為電源儲存裝置,可對其充電,當第一輸 入電壓源K於供電狀態及第二輸入電壓源K於充電狀態,第— 電感電流L為正,第一電感電流L為負,電路分析建構於第一 電感電流L絕對值大於第二電感電流L絕對值之條件下,此時 電壓電流時序波形如圖九所示’由於電路操作之對稱性,在此 分析前半個開關切換週期0.5&,而電路操作模式如圖十所示。 • L模式一[(。〜U :當時間ί = ί❶時,第一開關\、第三開關晃及 第六開關怂仍處於導通狀態,而第四開關\及第五開關冬已 截止一段時間,此時將第二開關&截止,致使第二開關&寄 生二極體自然導通,第二電感電流L流經第二開關&寄生二 極體;第三開關&、第四開關\、第五開關&及第六開關& 上電壓均為零’第七開關尽、第八開關&、第九開關&及第 十開關5;。上電壓均為4/2,在此死區時間毛&内,第一電 ^ 感马及第二電感A分別處於充電狀態及放電狀態,第一電感 電流Zil及第二電感電流L之斜率分別為F, /勾及Κ2 /12。 2.模式二〜模式二為第一段箝制開關^導通期間,在 此區間同時將第七開關&及第十開關心導通,箝制電容電 壓Fcc對第二電感矣及第二電壓源&充電,並透過理想變壓 器對直流輸出電壓源匕供電,其中第二電感電流L為負並 且流經第一開關\ ’而第一電感1,仍處於充電狀態,在模式 36 1351806 二時間内,根據柯希荷夫電流定律推導可得, 第一開關電流可表示為L -zu,第二電感電流ii2、理想 變壓器一次側電流k及箝制開關電流則可表示為 z£2(0 = ihi + °·5Δ/Ι2) + -~{V2 - Vcc){t -ί,) (26) (27)Vdc = T^nkVi = TZJ; n^ (25) The first inductor current chopping and the second inductor current chopping aq can also be expressed as shown in equations (11) and (17). (Parameter) Dual Input Power Supply Power Supply and Charging Status In today's power supply system development trend, hybrid power supply systems usually have at least one power storage device such as a battery or a super capacitor to provide continuous power output when another power failure occurs, or Is the main power output during the transient time of another power supply' so the power supply system needs to have the function of two-way power transmission, 35 1351806 enables the power storage device to have charging and power supply circuit ❶ under this power supply state analysis, assuming the second The input voltage source G is a power storage device, and can be charged. When the first input voltage source K is in the power supply state and the second input voltage source K is in the charging state, the first inductor current L is positive, and the first inductor current L is negative. The circuit analysis is constructed under the condition that the absolute value of the first inductor current L is greater than the absolute value of the second inductor current L. At this time, the voltage and current timing waveform is as shown in FIG. 9 'Because of the symmetry of the circuit operation, the first half of the switch is analyzed here. The cycle is 0.5 & while the circuit operation mode is shown in Figure 10. • L mode one [(.~U: When time ί = ί❶, the first switch \, the third switch sway and the sixth switch 怂 are still in the on state, and the fourth switch \ and the fifth switch have been closed for a while. At this time, the second switch & is turned off, causing the second switch & parasitic diode to be naturally turned on, the second inductor current L flowing through the second switch & parasitic diode; the third switch & \, the fifth switch & and the sixth switch & the upper voltage is zero 'the seventh switch, the eighth switch & the ninth switch & and the tenth switch 5; the upper voltage is 4/2, In the dead time, the first electric sensor and the second inductor A are respectively in a charging state and a discharging state, and the slopes of the first inductor current Zil and the second inductor current L are respectively F, /hook and Κ2 /12. 2. Mode 2 to Mode 2 is the first clamp switch. During the conduction period, the seventh switch & and the tenth switch core are simultaneously turned on in this interval, and the capacitor voltage Fcc is clamped to the second inductor and the second voltage. Source & charge, and supply power to the DC output voltage source through an ideal transformer, where the second inductor The flow L is negative and flows through the first switch \ ' and the first inductance 1 is still in a state of charge. In the mode 36 1351806, according to the Kirchhoff current law, the first switch current can be expressed as L -zu. , the second inductor current ii2, the ideal transformer primary side current k and the clamp switch current can be expressed as z£2 (0 = ihi + °·5Δ/Ι2) + -~{V2 - Vcc){t -ί,) ( 26) (27)

’as,sc (’) = ’μ ⑺ _ ’i2 (0 —XnULk + L2) - nV2Lk - V浴Lf nL2Lk ]{t-tx)~{IL2+Q.SML2) (28) 其中時間A又可表示為A =i。。由式(27)可得知理想變壓 器一次側電流由零漸增,此電流可感應出理想變壓器二次 側電流^,經第七開關&及第十開關心對直流輸出電壓源 C供電。模式二期間,洩漏電感A跨壓與耦合係數灸關係式 亦可表示如式(6)所示,根據柯希荷夫電壓定律推導,箝制 電容電壓可改寫如式⑻所示,亦即第二開關&、第四開 關\及第五開關&電壓均箱制於〇,而第八開關&及 第九開關5;上電壓均箝制於匕。 3.模式二匕〜^]:當時間/ = ?2時,將箝制開關知、第七開關& 及第十開關心截止,致使箝制開關電流‘降低至零,第 二瞻2寄生二極體自然導通承受第二電感電流。第二電 感乙2釋出能量對第二電壓鮮2充電,在第二開關&寄生二極 導L後為漏電感々上電壓瞬間反相,迴路電壓方程式可 37 1351806 表示為Vw =〇,理想變壓器一次側電流^以之斜 率遞減’並致使第四開關及第五開關寄生二極體導通,將泡 漏電感L*上所儲存之能量透過變壓器傳遞至直流輸出電壓 源匕。 4. 模式四h〜Μ:當時間i = G時,第一開關4、第三開關&及 第六開關叉仍處於導通狀態,此時將第二開關&、第四開關 &及第五開關&導通,第二開關&零電壓導通並且以同步整 流方式取代寄生二極體之電流,而第一電感A仍處於充電狀 態,第一電感電流心及第二電感電流L流經路徑,係根據最 小之線上電阻分流方式分佈;模式四中當理想變壓器電流重 置為零後,理想變壓器二次側電壓亦為零,第七開關&、第 八開關\、第九開關叉及第十開關心上電壓均為匕/ 2。 5. 模式五h〜y:當時間ί = &時,第二開關&、第四開關&及 第五開關&仍處於導通狀態,此時將第—開關《、第三開關 *S3及第六開關&截止;第—開關&、第三開關&及第六開關 怂上電壓均箝制等同於箝制電容電壓&C,在此死區時間 内,根據柯希荷夫電流定律推導可得,第二開 關電流可表示為,而第一電感電流^流經箱制開 關*SC寄生二極體及第二電源電路後,再流回第—電感々,此 時符制開關電流為負,對箱制電容&充電,理想變麼 器第-電感電流匕丨、-次側電流^丨及箝制開關電流“可分 38 1351806 別表示為式(18)、式(19)及式(20)。由式(19)可得知理想變壓 器一次側電流^由零漸減,此電流可感應出理想變壓器二次 側電流,經第八開關及第九開關\寄生二極體對直流輸 出電壓源匕供電》 6. 模式六[ί5~ίό]:模式六為第二段箝制開關&導通期間,在 此區間同時將第八開關<S8及第九開關<S9導通,第八開關&、 第九開關&及箝制開關<SC零電壓導通並且以同步整流方式 取代寄生二極體之電流,可減小開關導通損失,第一電感電 流心、理想變壓器一次側電流^及箝制開關電流“π仍可表 示如式(18)、式(19)及式(20)所示。 7. 模式七[L〜.當時間ί =匕時’將箝制開關&、第八開關& 及第九開關\截止,致使箝制開關寄生二極體自然導通以 及理想變壓器二次側電流k流經第八開關、及第九開關~ 寄生二極體,在此死區時間内,第一電感電流。持續對 箝制電容充電,並透過變壓器對直流輸出電壓源匕供電。 模式五至模式七中,洩漏電感A跨壓與耦合係數&關係式亦 可表示如式(23)所示,根據柯希荷夫電壓定律推導,箝制電 容電壓匕c可改寫如式(8)所示,亦即第一開關&、第三開關& 及第六開關S6電壓均箝制鮮rfc/(咐,而第七開關&及第十 開關\。上電壓均箝制於乙。 8·模式八[W8]:當時間叫時,第二開關第四開關&及 39 !3518〇6 第五開關&仍處於導通狀態,此時將第一開關&導通,洩漏 電感4上電壓瞬間反相,迴路電壓方程式可表示為 vu+vm = 〇,理想變壓器一次側電流以匕/„4之斜率遞增 至零,將洩漏電感Α上所儲存之能量透過變壓器傳遞至直流 輸出電壓源4 ,當第一開關&導通後,第一輸入電壓源γ對 第一電感'充電,此時第二電感/^仍處於放電狀態,第一電 感電流h及第二電感電流L呈線性增加,上升斜率分別為 卩/马及6/12;模式八中,當理想變壓器電流重置為零後’ 理想變壓器二次側電壓亦為零,第七開關尽、第八開關&、 第九開關&及第十開關\。上電壓均為匕c / 2。 依據伏秒平衡理論,開關切換周期内第一電感勾及第二電 感尤2之平均電壓為零,其關係式可表示為式(29)及式(3〇)所示。'as,sc (') = 'μ (7) _ 'i2 (0 —XnULk + L2) - nV2Lk - V bath Lf nL2Lk ]{t-tx)~{IL2+Q.SML2) (28) where time A is again Expressed as A = i. . It can be known from equation (27) that the primary side current of the ideal transformer is gradually increased from zero, and this current can induce the secondary current of the ideal transformer, and the power supply to the DC output voltage source C is supplied through the seventh switch & During mode 2, the leakage inductance A cross-pressure and coupling coefficient moxibustion relationship can also be expressed as shown in equation (6). According to the Kirchoff voltage law, the clamp capacitor voltage can be rewritten as shown in equation (8), that is, the second switch &;, the fourth switch \ and the fifth switch & voltage are boxed in the 〇, and the eighth switch & and the ninth switch 5; the upper voltage is clamped to 匕. 3. Mode 2匕~^]: When time / = ?2, the clamp switch is known, the seventh switch & and the tenth switch core is cut off, causing the clamp switch current to 'decrease to zero, the second view 2 parasitic pole The body is naturally conducting to withstand the second inductor current. The second inductor B2 releases energy to charge the second voltage, and after the second switch & parasitic diode conductance L, the voltage is instantaneously inverted for the leakage inductance, and the loop voltage equation can be expressed as Vw = 〇, 37 1351806, The slope of the ideal transformer primary side is decremented by 'and the fourth switch and the fifth switch parasitic diode are turned on, and the energy stored on the bubble leakage inductance L* is transmitted to the DC output voltage source 透过 through the transformer. 4. Mode 4h~Μ: When time i = G, the first switch 4, the third switch & and the sixth switch fork are still in the on state, and the second switch & the fourth switch & The fifth switch & is turned on, the second switch & zero voltage is turned on and the current of the parasitic diode is replaced by synchronous rectification, and the first inductor A is still in a charging state, the first inductor current core and the second inductor current L flow The path is distributed according to the minimum line resistance shunting mode; when the ideal transformer current is reset to zero in mode 4, the secondary side voltage of the ideal transformer is also zero, the seventh switch & the eighth switch \, the ninth switch The voltage on both the fork and the tenth switch is 匕 / 2. 5. Mode 5h~y: When time ί = &, the second switch & the fourth switch & and the fifth switch & are still in the on state, at this time the first switch ", the third switch * S3 and the sixth switch &cutoff; the first switch & the third switch & and the sixth switch 电压 voltage clamp are equal to the clamp capacitor voltage & C, in this dead time, according to Kirchhof current law The derivation can be obtained, the second switch current can be expressed as, and the first inductor current flows through the box switch *SC parasitic diode and the second power circuit, and then flows back to the first inductor 々, at this time, the switch current Negative, for the box capacitor & charging, the ideal inductor - inductor current 匕丨, - secondary current ^ 丨 and clamp switch current " can be divided into 38 1351806 is not expressed as equation (18), formula (19) and Equation (20). It can be known from equation (19) that the primary side current of the ideal transformer is gradually reduced by zero. This current can induce the secondary side current of the ideal transformer. After the eighth switch and the ninth switch\parasitic diode pair DC Output Voltage Source 匕 Power Supply 6. 6. Mode 6 [ί5~ίό]: Mode 6 is the second stage clamp switch & During the conduction period, the eighth switch <S8 and the ninth switch <S9 are turned on at the same time in this interval, and the eighth switch & ninth switch & and clamp switch <SC zero voltage is turned on and replaced by synchronous rectification The current of the parasitic diode can reduce the switch conduction loss. The first inductor current center, the ideal transformer primary current ^ and the clamp switch current "π can still be expressed as equations (18), (19) and (20). Shown. 7. Mode seven [L~. When time ί =匕" will clamp switch & eighth switch & and ninth switch \ cutoff, causing the clamp switch parasitic diode to conduct naturally and the ideal transformer secondary current k Flow through the eighth switch, and the ninth switch ~ parasitic diode, the first inductor current during this dead time. The clamp capacitor is continuously charged and the DC output voltage source 匕 is supplied through the transformer. In mode 5 to mode 7, the leakage inductance A cross-over and coupling coefficient & can also be expressed as shown in equation (23). According to Kirchhoff's voltage law, the clamped capacitor voltage 匕c can be rewritten as in equation (8). That is, the first switch & the third switch & and the sixth switch S6 voltage are clamped fresh rfc / (咐, and the seventh switch & and the tenth switch \. The upper voltage is clamped to B. 8· Mode 8 [W8]: When the time is called, the second switch, the fourth switch & and the 39 !3518〇6 fifth switch & are still in the on state, at this time, the first switch & is turned on, and the voltage on the leakage inductor 4 is turned on. Instantaneous inversion, the loop voltage equation can be expressed as vu+vm = 〇, the ideal transformer primary current increases to zero with a slope of 匕/„4, and the energy stored in the leakage inductance 透过 is transmitted through the transformer to the DC output voltage source 4 After the first switch & is turned on, the first input voltage source γ charges the first inductor, and at this time, the second inductor/^ is still in a discharging state, and the first inductor current h and the second inductor current L linearly increase. The rising slopes are 卩/马 and 6/12; in mode eight, when ideal After the voltage of the voltage is reset to zero, the voltage on the secondary side of the ideal transformer is also zero. The seventh switch, the eighth switch & the ninth switch & and the tenth switch are all 匕c / 2. According to the volt-second balance theory, the average voltage of the first inductor hook and the second inductor 2 in the switching period is zero, and the relationship can be expressed by equations (29) and (3).

VxdxTs + {V{-Vcc){\~dx)Ts^ (29a)VxdxTs + {V{-Vcc){\~dx)Ts^ (29a)

Vcc~\-dxVi (29b) V2(d2 + 4dd)Ts + (V2 - Fcc)(l -d2~ 4dd)Ts = 0 (3〇a)Vcc~\-dxVi (29b) V2(d2 + 4dd)Ts + (V2 - Fcc)(l -d2~ 4dd)Ts = 0 (3〇a)

Vcc 一 i-d2-4ddVl (30b) 根據式(8)、式(29)及式(30),並假設死區時間責任週期毛很小, 第一輸入電壓源γ、第二輸入電壓源G及直流輸出電壓源4關 係可表示為式(25)所示。而第—電感電流漣波⑷及第二電感電 流漣波Δζ〗2亦可表示如式(U)及式(17)所示。 丄乃1806 (肆)輸出電琢反饋狀態 當直流輸出電壓源4發生電壓異常升高,或電源管理系統 因應不同輸出負載及節省能源之目的,欲調節第—輪人電壓源 β不輸出功率,直流輸出電壓源匕對電源儲存裝置之第二電壓 源Κ充電時,可將第一電源開關〜截止以完成電源切離之目 的’並使第-開關\持續導通,此時第二輸入電壓源G可於輸 出電源反館狀H下操作,為方便分析直流輸出電壓源匕對第二 電壓源Κ充電’將洩漏電感4等效至理想變壓器二次側%處, 以二次側洩漏電感心表示,其感值大小等於,此時等效電 路可表示如圖十-所示,而電壓電流時序波形如圖十二所示, 由於電路操作之對稱性,在此分析前半個開關切換週期〇5&, 而電路操作模式如圖十三所示。 1,模式一 [/。〜當時間ί = ί。時,第一開關$、第三開關&及 第六開關叉仍處於導通狀態,而第四開關&及第五開關&已 截止一段時間,此時將第二開關&截止,致使第二開關&寄 生二極體自然導通,第二電感電流L流經第二開關&寄生二 極體’第二開關4、第四開關Α、第五開關4及第六開關& 上電壓均為零’第七開關*v第八開關v第九開關&及第 十開關5;。上電壓均為4/2,在此死區時間内,第二電 感A處於放電狀態,第二電感電流L之斜率為矣,對第 二電壓源K2充電。 1351806 2·模式二h〜模式二為箝制開關第七開關&及第十 開關心導通期間,箝制電容電壓rcc對第二電感&及第二輸 入電壓源f2充電,而直流輸出電壓源&則透過理想變壓器一 同對第二電感12及第二輸入電壓源y2充電,此時理想變壓器 一次側電壓%等於箝制電容電壓匕c,第二電感電流L、理 想變壓器一次侧電流^及箝制開關電流奴冗可分別表示為 式(26)、式(31)及式(32) »Vcc-i-d2-4ddVl (30b) according to equations (8), (29) and (30), and assumes that the duty cycle of the dead time period is small, the first input voltage source γ, the second input voltage source G The relationship between the DC output voltage source 4 and the DC output voltage source 4 can be expressed as Equation (25). The first-inductance current chopping (4) and the second inductive current chopping Δζ2 can also be expressed as shown in the equations (U) and (17).丄乃1806 (肆) output power feedback state When the DC output voltage source 4 voltage rises abnormally, or the power management system responds to different output loads and saves energy, it is necessary to adjust the first-wheel voltage source β to output power. When the DC output voltage source Κ charges the second voltage source 电源 of the power storage device, the first power switch can be turned off to complete the power cut-off purpose and the first switch is continuously turned on, and the second input voltage source is at this time. G can be operated under the output power supply anti-column H, in order to facilitate analysis of the DC output voltage source Κ charging the second voltage source ' 'The leakage inductance 4 is equivalent to the ideal transformer secondary side %, to the secondary side leakage inductance core It means that the magnitude of the sense is equal to, the equivalent circuit can be represented as shown in Figure 10-, and the voltage and current timing waveform is shown in Figure 12. Due to the symmetry of the circuit operation, the first half of the switching cycle is analyzed here. 5&, and the circuit operation mode is shown in Figure 13. 1, mode one [/. ~ When time ί = ί. The first switch $, the third switch & and the sixth switch fork are still in an on state, and the fourth switch & and the fifth switch & have been turned off for a period of time, at which time the second switch & The second switch & parasitic diode is naturally turned on, and the second inductor current L flows through the second switch & parasitic diode 'second switch 4, fourth switch Α, fifth switch 4 and sixth switch & The voltage is zero 'the seventh switch * v the eighth switch v the ninth switch & and the tenth switch 5; The upper voltage is 4/2. During this dead time, the second inductor A is in a discharging state, and the slope of the second inductor current L is 矣, and the second voltage source K2 is charged. 1351806 2·Mode 2h~Mode 2 is the clamp switch seventh switch & and the tenth switch core is turned on, the clamp capacitor voltage rcc charges the second inductor & and the second input voltage source f2, and the DC output voltage source & The second inductor 12 and the second input voltage source y2 are charged together by the ideal transformer. At this time, the ideal transformer primary side voltage % is equal to the clamp capacitor voltage 匕c, the second inductor current L, the ideal transformer primary side current ^ and the clamp switch Current slave redundancy can be expressed as equation (26), equation (31), and equation (32), respectively.

(31) ^Νΐ(0 ~ —{nVQC ~ Kk)(f ~〇 Lkl bs,sc (Ο ~ (0 ~ hi ) FCC(^2I2+ LiLn ·](卜 〇-(,ι2+〇·5Δ。) (32) 由式(31)可得知理想變壓器—次側電流^由零漸減,當籍制 開關電流心,《:流經零點且其換相時間為ί = ίΜ,將心冗=〇代 入式(32)可求付如式(33)所示。(31) ^Νΐ(0 ~ -{nVQC ~ Kk)(f ~〇Lkl bs,sc (Ο ~ (0 ~ hi ) FCC(^2I2+ LiLn ·](卜〇-(,ι2+〇·5Δ.) ( 32) It can be known from equation (31) that the ideal transformer—the secondary current ^ is gradually reduced by zero. When the current is switched, the current is flowing through the zero point and its commutation time is ί = ίΜ, and the heart is redundant = 〇 (32) The payable is as shown in equation (33).

-f +__L2Lk2(IL1+0.5ML7) 64 1 Vcc{n2L2+Lk2)~VdcnL2-V2Lk2 (33) 當時間叫4之後’箝制開關電流w為負,直流輸出電壓源 4則透過理想變壓器同時對箝制電容q及第二電感尤充 電。時間i = i2af ’理想變壓器—次侧電流、最小值亦可表示 (34) 跨壓與輕合係數㈣係式可 Ζ·ΛΠ (’2 ) = "7 — (W^CC ~ ~ 〇-f +__L2Lk2(IL1+0.5ML7) 64 1 Vcc{n2L2+Lk2)~VdcnL2-V2Lk2 (33) When the time is called 4, the clamp current w is negative, and the DC output voltage source 4 is clamped through the ideal transformer. The capacitor q and the second inductor are particularly charged. Time i = i2af ‘ideal transformer—secondary current and minimum value can also be expressed (34) Trans-pressure and light-combination coefficient (4) can be Ζ·ΛΠ (’2 ) = "7 — (W^CC ~ ~ 〇

Hi 模式二期間’二次側洩漏電感 42 1351806 表不為 vLki=(}-k)Vdc (35) 根據柯希荷夫電壓定律,迴路電壓方程式表示如下:During the Hi mode two period 'secondary leakage inductance 42 1351806 is not expressed as vLki=(}-k)Vdc (35) According to Kirchoff's voltage law, the loop voltage equation is expressed as follows:

Vdc~VN2~VLk2=0 (36) 其中理想變壓器二次側跨壓〜2 =„FCC。將式(35)代入式 (36),箝制電容電壓?^可改寫為 (37)Vdc~VN2~VLk2=0 (36) where the ideal transformer secondary side voltage is ~2 =„FCC. Substituting equation (35) into equation (36), clamp capacitor voltage?^ can be rewritten as (37)

亦即第二開關&、第四開關S4及第五開關叉電壓均箝制於 灸4/«,而第八開關&及第九開關&上電壓均箝制於匕。 3.模式二[q〜:當時間(=&時’將箝制開關&、第七開關& 及第十開關&。截止,致使箝制開關電流Lx降低至零以及 箝制開關電流上升至箝制電容電壓pcc,此時箝制開關 源極對第二輸入電壓源厂a之地點相對電壓為零伏特,理想 變壓器電壓降低至零伏特,二次側洩漏電感心2上電壓瞬間 反相’二次側洩漏電感矣2上電流連續致使第八開關&及第 九開關叉之寄生二極體導通,導通迴路電壓方程式可表示為 να2+ν"2 + ίς = 〇 ’理想變壓器二次側電流k以之斜率 在極短暫時間内遞增至零,將二次側洩漏電感/^上所儲存 之能量釋放至直流輸出電壓源匕c,而第二開關&寄生二極 體則自然導通承受第二電感電流L,在此死區時間元rs内, 第二電感与處於放電狀態,第二電感電濟^之斜率為 43 1351806 尽,對第二電壓源K充電》 4. 模式四h〜g:當時間/ =匕時,第一開關$、第三開關&及 第六開關&仍處於導通狀態,此時將第二開關&、第四開關 \及第五開關&導通,第二開關\零電壓導通並且以同步整 流方式取代寄生二極體之電流,第二電感電流^2流經路徑根 據流經路徑之線上電阻,以分流方式流經第二開關&、第三 開關*串聯第四開關&及第五開關&串聯第六開關&等三 條路徑。 5. 模式五當時間ί = ~時,第二開關&、第四開關&及 第五開關冬仍處於導通狀態,此時將第三開關&及第六開關 \截止;第三開關冬及第六開關&零電壓截止,而第二電感 尽仍處於充電狀態,第二電感電流l以單一路徑流經第二開 關*^。模式三至模式五期間,當理想變壓器電流已重置為 零’理想變壓器上跨壓亦為零,因此第七開關v第八開關 &、第九開關&及第十開關心上電壓均箝制於匕/2。 依據伏秒平衡理論,開關切換周期内.第二電感以平均電 壓為零’其關係式可表示為式⑽所示,根據式(37)及式(3〇), 並假設死區時間責任週期《很小,第二輸入電壓源G及直流輸 出電壓源匕關係可表示為式⑽所示,而第二電感電流漣波岣 亦可表示如式(17)所示。 本發明所揭示高昇壓式隔離型雙輸入電源轉換器之第一較 1351806 佳實施例技術特徵為:第一點,具雙輸入電源雙向轉換機制, 可予許不同電氣特性之電壓源作為輸入端,共同提昇電壓位 準,簡化多組轉換器昇壓再併聯供電之架構;第二點,具高昇 壓比及電氣隔離特性,利用隔離變壓器匝數比與責任週期控 制,即可獲得高電壓增益;第三點,轉換效率高,在輸入輸出 電壓隔離架構下,嚴謹區分低壓側大電流,高壓側低電流特性, 分別可選用適合電壓範圍之低成本高效率功率元件;第四點, • 主動式電壓箝制技術解決因隔離變壓器存在洩漏電感所造成之 電壓突波問題,並將洩漏電感能量有效輸出至直流輸出電路; 第五點,具導通損失大幅降低特性,兩輸入電源電路以串聯方 式連接,當轉換器操作於雙輸入電源同時供電狀態時,導通損 失可大幅降低,對於應用於輸入電源為低電壓高電流之潔淨能 源時,成功減小導通損失並可大幅提升轉換效率;第六點,雙 輸入電源端之輸入電流連續,輸入電源以直流電流源電能形式 # 呈現,並可於電源端擷取出較小漣波之輸入電流,當應用於潔 淨能源為輸入電源時,可有效濾除電流漣波及避免損害潔淨能 源裝置,延長潔淨能源裝置之使用壽命;第七點,功率半導體 開關所承受電壓僅與直流輸出電壓及隔離變壓器之匝數比有 關,此特點更適合直流輸入電壓大範圍變動之電源轉換裝置應 用。 當本發明所揭示之高昇壓式隔離型雙輸入電源轉換器輸入 45 1351806 電源均為潔淨能源,或是輸出直流電源已具保護機制,不需輸 出電源反饋路徑時,本發明之高昇壓式隔離型雙輸入電源轉換 器可簡化為如圖十四所示之第二較佳實施例之電路架構。與第 一較佳實施例之差別在於第一圖之全橋式電路1〇3與第十四圖 之單向全橋式電路1403,將第一較佳實施例中第七開關&、第 八開關\、第九開關&及第十開關$。,替換為第一二極體q、 第二二極體A、第三二極體A及第四二極體,並且減少使用 ® 四組開關驅動訊號。本發明所揭示高昇壓式隔離型雙輸入電源 轉換器之第二較佳實施例中,第一輸入電壓源γ以及第二電壓 源厂2,可由蓄電池'超電容、燃料電池、太陽光電池、直流風 力發電機或交流風力發電機整流為直流電源作為直流電源供 應。當雙輸入電源均為不具電源儲存特性之能源時,供電情形 可分為二種狀態:單輸入電源獨立供電及雙輸入電源同時供 電,此二種供電狀態之其操作模式分別與第一較佳實施例之供 ®電狀態相同,並可簡化系統架構以及架設成本》當雙輸入電源 分別為不具電源儲存特性之能源及電源儲存裝置時,供電情形 可分為三種狀態:單輸入電源獨立供電、雙輸入電源同時供電 以及雙輸入電源分別供電與充電,此三種供電狀態之其操作模 式分別與第一較佳實施例之供電狀態相同,並可簡化系統架構 以及表β又成本本發明所揭示南昇麼式隔離型雙輸入電源轉換 器之第二較佳實施例技術特徵為:第一點,具雙輸入電源機制 46 1351806 及電源儲存裝置充電機制,可予許不同電氣特性之電壓源作為 輸入端,共同提昇電壓位準,簡化多組轉換器昇壓再併聯供電 之架構,並且依電源管理需求及供電情形可分為.三種狀態:單 輸入電源獨立供電、雙輸入電源同時供電以及雙輸入電源分別 供電與充電,第二點,具高昇壓比及電氣隔離特性,利用隔離 變壓器匝數比與責任週期控制,即可獲得高電壓増益;第三點, 轉換效率高,在輸入輸出電壓隔離架構下,嚴謹區分低壓側大 ® 電流,高壓側低電流特性,分別可選用適合電壓範圍之低成本 高效率功率元件;第四點,主動式電壓箝制技術解決因隔離變 壓器存在洩漏電感所造成之電壓突波問題,並將洩漏電感能量 有效輸出至直流輸出電路;第五點,具導通損失大幅降低特性, 兩輸入電源電路以串聯方式連接,當轉換器操作於雙輸入電源 同時供電狀態時,導通損失可大幅降低,對於應用於輸入電源 為低電壓尚電流之潔淨能源時,成功減小導通損失並可大幅提 ® 升轉換效率;第六點,雙輸入電源端之輸入電流連續,輸入電 源以直流電流源電能形式呈現,並可於電源端棟取出較小漣波 之輸入電流,當應用於潔淨能源為輸入電源時,可有效濾除電 流漣波及避免損害潔淨能源裝置,延長潔淨能源裝置之使用壽 命;第七點’功率半導體開關所承受電壓僅與直流輸出電壓及 隔離變壓器之匝數比有關,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;第八點,單向全橋式電路架構簡單, 1351806 單向全橋式電路僅使用四顆開關及四顆二極體,即具對電源儲 存裝置充電迴路之機制。 為使進一步瞭解本發明之内容,以下實施例之模擬波形, 元件之電壓及電流之代號,敬請參閱第二圖;本實施例採用電 路模擬軟體ISPICE予以驗證本發明所揭示高昇壓式隔離型雙 輸入電源轉換器之可行性,其中第一輸入電壓源)^採28伏特低 壓能源、第二輸入電壓源F2則採用24伏特之蓄電池作為電源儲 存裝置,配合直流輸出電路105輸出400伏特直流電壓,適當 選取本發明所揭示高昇壓式隔離型雙輸入電源轉換器元件,第 一開關&、第二開關<S2、第三開關<S3、第四開關\、第五開關&、 第六開關&以及箝制開關&等低壓側開關選用型號IRFP260之 MOSFET功率開關,而高壓側之第七開關<S7、第八開關&、第 九開關<S9、第十開關心採用型號IRFM460之MOSFET功率開 關,高昇壓式隔離型雙輸入電源轉換器之操作頻率設定為 10kHz,第一開關$及第二開關叉切換頻率則為20KHz,本實 施例詳細之規格如下: L, : 400 μ Η L2 : 200 μ Η 4 : 2.4 η · 6.5That is, the second switch & the fourth switch S4 and the fifth switch fork voltage are both clamped to the moxibustion 4/«, and the eighth switch & and the ninth switch & 3. Mode 2 [q~: When time (=&' will clamp switch & seventh switch & and tenth switch & cutoff, causing clamp switch current Lx to decrease to zero and clamp switch current to rise to Clamping the capacitor voltage pcc, at this time, the voltage of the clamped switch source to the second input voltage source factory a is zero volts, the ideal transformer voltage is reduced to zero volts, and the voltage on the secondary side leakage inductor core 2 is instantaneously inverted 'secondary The current on the side leakage inductance 矣2 continuously causes the parasitic diode of the eighth switch & and the ninth switch fork to be turned on, and the conduction loop voltage equation can be expressed as να2+ν"2 + ς ς 〇 'ideal transformer secondary side current k The slope is incremented to zero in a very short time, and the stored energy on the secondary leakage inductance / ^ is released to the DC output voltage source 匕c, while the second switch & parasitic diode is naturally conducted to withstand the second Inductor current L, in this dead time rs, the second inductance is in the discharge state, the slope of the second inductor is 43 1351806, and the second voltage source K is charged. 4. Mode four h~g: When time / = ,, The first switch $, the third switch & and the sixth switch & are still in an on state, at this time, the second switch & the fourth switch \ and the fifth switch & are turned on, and the second switch \ zero voltage is turned on and The current of the parasitic diode is replaced by a synchronous rectification method, and the second inductor current ^2 flows through the second switch & the third switch * series fourth switch & And the fifth switch & series sixth switch & three paths. 5. mode five when time ί = ~, the second switch & fourth switch & and the fifth switch is still in the on state, at this time The third switch & and the sixth switch are turned off; the third switch winter and the sixth switch & zero voltage are turned off, while the second inductor is still in the charging state, and the second inductor current l flows through the second switch in a single path. *^. During mode 3 to mode 5, when the ideal transformer current has been reset to zero 'the ideal transformer is also zero across the transformer, so the seventh switch v eighth switch & ninth switch & The upper voltage is clamped to 匕/2. Balance according to volt-seconds Theory, during the switching cycle. The second inductor has an average voltage of zero'. The relationship can be expressed as equation (10), according to equations (37) and (3〇), and assumes that the dead time duty cycle is small. The relationship between the second input voltage source G and the DC output voltage source 可 can be expressed as Equation (10), and the second inductor current 涟 岣 can also be expressed as shown in Equation (17). The high-boost isolation type disclosed in the present invention The first embodiment of the input power converter is 1351806. The technical feature of the preferred embodiment is: the first point has a two-input power bidirectional conversion mechanism, and a voltage source with different electrical characteristics can be used as an input terminal to jointly raise the voltage level and simplify multiple groups. The converter boosts and parallels the power supply architecture; the second point, with high boost ratio and electrical isolation characteristics, using the isolation transformer turns ratio and duty cycle control, can obtain high voltage gain; third, the conversion efficiency is high, Under the input-output voltage isolation architecture, the high-voltage side high-current and high-voltage side low-current characteristics are strictly distinguished, and low-cost high-efficiency power components suitable for the voltage range can be selected respectively. Fourth point, • Active power The pressure clamp technology solves the voltage surge problem caused by the leakage inductance of the isolation transformer, and effectively outputs the leakage inductance energy to the DC output circuit. The fifth point has the characteristic that the conduction loss is greatly reduced, and the two input power supply circuits are connected in series. When the converter is operated in a dual-input power supply state, the conduction loss can be greatly reduced. When applied to a clean energy source where the input power source is low voltage and high current, the conduction loss is successfully reduced and the conversion efficiency can be greatly improved; The input current of the dual input power supply is continuous, and the input power is presented in the form of DC current source energy, and the input current of the smaller chopping wave can be taken out at the power supply end. When applied to the clean power source as the input power source, the current can be effectively filtered. Chopping and avoiding damage to clean energy devices and prolonging the service life of clean energy devices; seventh, the voltage of the power semiconductor switch is only related to the DC output voltage and the turns ratio of the isolation transformer. This feature is more suitable for large-scale changes of DC input voltage. Power conversion device application. The high-boost isolation type of the high-boost isolated dual-input power converter input 45 1351806 is clean energy, or the output DC power supply has a protection mechanism, and the power supply feedback path is not required, the high-boost isolation of the present invention The type of dual input power converter can be simplified to the circuit architecture of the second preferred embodiment as shown in FIG. The difference from the first preferred embodiment is the full bridge circuit 1〇3 of the first figure and the unidirectional full bridge circuit 1403 of the fourteenth embodiment, and the seventh switch & Eight switches \, ninth switch & and tenth switch $. Replace with the first diode q, the second diode A, the third diode A, and the fourth diode, and reduce the use of four sets of switch drive signals. In a second preferred embodiment of the high-boost isolated dual-input power converter disclosed in the present invention, the first input voltage source γ and the second voltage source factory 2 can be used by the battery 'supercapacitor, fuel cell, solar cell, DC The wind turbine or AC wind turbine is rectified to a DC power source as a DC power source. When the dual input power supply is an energy source without power storage characteristics, the power supply situation can be divided into two states: single input power supply independent power supply and dual input power supply simultaneously, and the operation modes of the two power supply states are respectively the first and the better. The power supply status of the embodiment is the same, and the system architecture and the erection cost can be simplified. When the dual input power supply is an energy and power storage device that does not have the power storage characteristics, the power supply situation can be divided into three states: single input power supply, independent power supply, The dual input power supply is simultaneously powered and the dual input power supply is respectively powered and charged. The operating modes of the three power supply states are the same as the power supply states of the first preferred embodiment, respectively, and the system architecture and the table β are further simplified. The second preferred embodiment of the dual-input dual-input power converter is characterized in that: the first point has a dual input power mechanism 46 1351806 and a power storage device charging mechanism, and a voltage source of different electrical characteristics can be used as an input. End, jointly raise the voltage level, simplify the structure of multiple sets of converters and then parallel supply, According to the power management requirements and power supply situation, it can be divided into three states: single input power supply independent power supply, dual input power supply and power supply and charging for dual input power supply, and second point, high boost ratio and electrical isolation, use isolation The transformer turns ratio and duty cycle control can obtain high voltage benefits. Thirdly, the conversion efficiency is high. Under the input and output voltage isolation architecture, the low voltage side large current and the high voltage side low current characteristics can be distinguished. The low-cost and high-efficiency power components in the voltage range; the fourth point, the active voltage clamping technology solves the voltage surge problem caused by the leakage inductance of the isolation transformer, and effectively outputs the leakage inductance energy to the DC output circuit; The conduction loss is greatly reduced. The two input power circuits are connected in series. When the converter is operated in the dual-input power supply state, the conduction loss can be greatly reduced. For the clean energy source when the input power source is low voltage and current, Successfully reduce conduction losses and significantly increase conversion efficiency The sixth point is that the input current of the dual input power terminal is continuous, the input power source is presented in the form of DC current source power, and the input current of the smaller chopping wave can be taken out at the power terminal end, which can be effectively applied when the clean energy source is the input power source. Filter out current ripple and avoid damage to clean energy devices, and extend the service life of clean energy devices. The power point of the seventh point 'power semiconductor switch is only related to the DC output voltage and the turns ratio of the isolation transformer. This feature is more suitable for DC input voltage. The application of the power conversion device with a wide range of changes; the eighth point, the one-way full-bridge circuit structure is simple, the 1351806 one-way full-bridge circuit uses only four switches and four diodes, that is, the charging circuit for the power storage device mechanism. In order to further understand the contents of the present invention, the analog waveforms of the following embodiments, the voltage and current codes of the components, please refer to the second figure; this embodiment uses the circuit simulation software ISPICE to verify the high-boost isolation type disclosed in the present invention. The feasibility of the dual input power converter, wherein the first input voltage source is 28 volts low voltage energy, and the second input voltage source F2 uses a 24 volt battery as the power storage device, and the DC output circuit 105 outputs 400 volts DC voltage. The high-boost isolated dual-input power converter component disclosed in the present invention is appropriately selected, the first switch & the second switch < S2, the third switch < S3, the fourth switch, the fifth switch & The sixth switch & and the clamp switch & low voltage side switch selects the MOSFET power switch of the model IRFP260, and the seventh switch of the high voltage side <S7, the eighth switch & the ninth switch <S9, the tenth switch core Using the IGBT power switch of the model IRFM460, the operating frequency of the high-boost isolated dual-input power converter is set to 10 kHz, the first switch $ and the second switch fork Compared with the frequency 20KHz, the detailed implementation of the embodiment of the present specification is as follows: L,: 400 μ Η L2: 200 μ Η 4: 2.4 η · 6.5

Cc : 220 β¥ C, : 660 ^ F C2 · 660 β F C0 : 100 β¥ 48 1351806 第十五圖表示本發明所揭示高昇壓式隔離型雙輸入電源 轉換器輸出功率400瓦特時,第一輪入電壓源γ於獨立供電狀 態之模擬波形響應:(a)表示各開關驅動訊號電壓波形,與第三 圖波形時序給定之各開關驅動訊號電壓波形相符;(b)表示第一 電感電流L、第一開關電壓vDwi、第一開關電流心&、第三開 關電壓以及第三開關電流心幻,由圖中顯示出第一電感電 流b連續,第一輸入電壓源%穩定輸出功率416瓦特,此外, • 第一開關Α導通前,第一開關電壓先降至零伏特,因此第 一開關導通具零電壓切換之特性,而第一開關&及第三開關& 截止時電壓均箝制於箝制電容電壓厂⑦,有效改善變壓器漏感所 造成開關電壓突波現象;(C)表示箝制電容電壓^^、箝制開關電 壓VDS,《:、箝制開關電流心况以及理想變壓器一次側電流^,箝 制電容電壓Fcc為定值,且所有低壓側開關截止時均箝制於此電 壓值,箝制開關電流/取冗於開關導通前為負,電流流經其寄生 •二極體’箝制開關<SC導通時具零電壓切換之特性,而理想變壓 器一次側電流^為正值時通過第三開關&及第六開關&,電流 為負值時通過第四開關&及第五開關&,經變壓器升壓後,再 整流對直流輸出電路105供電;(d)表示直流輸出電壓匕、第七 開關電壓、第七開關電流以及理想變壓器二次側電流 圖中直流輸出電壓Κ穩定輸出400伏特,而第七開關電學 於理想變壓器二次側電流降低至零時產生電壓震盪之 49 1351806 現象’這是由於當第一開關&導通致使變壓器電流降低至零, 此時再將第七開關《s7與第十開關&。截止,或是第八開關&與第 九開關4截止,開關上寄生二極體之反向恢復電流所造成洩漏 電感與開關寄生電容諧振現象。 第十六圖表示本發明所揭示高昇壓式隔離型雙輸入電源轉 換器輸出功率200瓦特時,第二輸入電壓源厂2於獨立供電狀態 之模擬波形響應:(a)表示各開關驅動訊號電壓波形,與第五圖 • 波形時序給定之各開關驅動訊號電壓波形相符;(b)表示第二電 感電流L、第二開關電壓vm52、第二開關電流心^2、第三開關 電壓%〜?3以及第三開關電流zDSS3,由圖中顯示出第二電感電流 L連續,第二輸入電壓源G穩定輸出功率212瓦特,此外,第 二開關&導通前,第二開關電壓心^先降至零伏特,因此第二 開關具零電壓導通之特性,而第二開關&及第三開關&截止時 電壓均箝制於箝制電容電壓pcc,有效改善變壓器漏感所造成開 •關電壓突波現象,與第-輸入電壓源^於獨立供電狀態之模擬 波形響應圖十五(b)相比較,不同的是時序上電感電流分流之時 間區段,但均可有效減低開關上之導通損失;(c)表示箝制電容 電壓厂CC、箱制開關電麼艾、箱·制開關電流/仿尤以及理想變壓 器-人側電流W,箝制電容電壓Fcc為定值,且所有低壓側開關 截止時均箝制於此電壓值,箝制開關電流‘於開關導通前為 負,電流流經其寄生二極體,箝制開關\導通時具零電壓切換 1351806 之特性,而理想變壓器一次側電流k為正值時通過第三開關4 及第’、開關\ ’電流為負值時通過第四關&及第五開關&, 經變麼器升壓後’再整流對直流輸出電路1G5供電;⑷表示直 流輸出電壓F。、第七開關電壓v⑽7、第七開關電流‘7以及理 想變壓器二次側電流心2,圖中直流輸出電壓穩定輸出400伏 特,而第七開關電壓v〇ss7於理想變壓器二次側電流^降低至零 時產生電壓震盪之現象,這是由於當第一開關$導通致使變壓 器電流降低至零,此時再將第七開關&與第十開關 '。截止,或 疋第八開關\與第九開關A截止’開關上寄生二極體之反向恢 復電流所造成洩漏電感與開關寄生電容諧振現象。 第十七圓表示本發明所揭示高昇壓式隔離型雙輸入電源轉 換器輸出功率600瓦特時,第一輸入電壓源^及第二輸入電壓 源匕於同時供電狀態之模擬波形響應:(a)表示各開關驅動訊號 電壓波形,與第七圖波形時序給定之各開關驅動訊號電壓波形 相符;(b)表示第一電感電流l、第二電感電流t、第一開關電 壓νω,·?ι、第一開關電流心幻、第二開關電壓s2以及第二開關 電流心为,由圖中顯示出第一電感電流k及第二電感電流匕均 連續,第一輸入電壓源γ及第二輸入電壓源κ同時穩定輸出功 率,此時第一輸入電壓源G輸出功率為4〇5瓦特,第二輸入電 壓源Κ輸出功率為220瓦特,此外,第一開關及第二開關在此 操作模式下導通均具零電壓切換之特性,且第一開關&及第二 51 1351806 開關&截止時電壓均箝制於箝制電容電壓fcc,有效改善變壓器 漏感所造成開關電壓突波現象,當模式四第二開關《s2導通時, 第二開關電流«仍為零,第一開關電流降低,可成功降 低開關之導通損失;表示箝制電容電壓rcc、箝制開關電壓 VI«.SC、箝制開關電流ksc以及理想變壓器一次側電流^ ,箝制 電容電壓Kcc為定值,且所有低壓側開關截止時均箝制於此電壓 值,箝制開關電流於開關導通前為負,電流流經其寄生二 •極體,箝制開關&導通時具零電壓切換之特性,而理想變壓器 一次側電流‘為正值時通過第三開關&及第六開關&,電流為 負值時通過第四開關\及第五開關&,經變壓器升壓後,再整 流對直流輸出電路1〇5供電;(句表示直流輸出電壓乙、第七開 關電壓π、第七開關電流以及理想變壓器二次側電流 心2 ’圖中直流輸出電壓穩定輸出400伏特,而第七開關電壓 va$,·?7於理想變壓器二次側電流k降低至零時產生電壓震盪之 ♦現象,這是由於當第一開關^或第二開關^導通,致使變屋器 電流降低至零,此時再將第七開關从第十開關^截止,或是 第八開關\與第九開關S9截止,開關上寄生二極體之反向恢復 電流所造成茂漏電感與開關寄生電容諧振現象;⑷表示第三開 關電壓〜、第三開關電流“、第四開關電壓S以及第四 開關電流“(’由圖中顯示出第三開關電流一 3及第四開關電 流以時序區分,透過變麼器對直流輸出電路105供電,並 52 1351806 且電感電流可在第三開關<s3、第四開關<s4、第五開關<s5及第六 開關<s6同時導通時,以分流形式減低導通損失,而第三開關及 第四開關截止時電壓均箝制於箝制電容電壓。 第十八圖表示本發明所揭示高昇壓式隔離型雙輸入電源轉 換器輸出功率400瓦特時,第一輸入電壓源γ於供電狀態及第 二輸入電壓源F2於充電狀態之模擬波形響應:(a)表示各開關驅 動訊號電壓波形’與第九圖波形時序給定之各開關驅動訊號電 • 壓波形相符;(b)表示第一電感電流L、第二電感電流、第一 開關電壓”取51、第一開關電流、第二開關電壓Vd^2以及第 二開關電流心,52 ’由圖中顯示出第一電感電流L為正,第二電 感電流L為負’且兩者均為連續電流,第一輸入電壓源γ穩定 輸出功率,而第二輸入電壓源。之蓄電池以定電流穩定充電, 此時第一輸入電壓源6輸出功率為658瓦特,第二輸入電壓源& 充電功率為201瓦特,第一開關&及第二開關&截止時電壓均 •箝制於箝制電容電壓,有效改善變壓器漏感所造成開關電壓 突波現象’在此操作狀態巾,第二開關&以同步整流方式減低 開關導通損失,開關導通時具零電壓切換特性;(c)表示箝制電 容電壓Fcc、箝制開關電壓v取疋、箝制開關電流以及理想變 壓器一次側電流^,箝制電容電壓Fcc為定值,且所有低壓側開 關截止時均箝制於此電壓值,在模式二中籍制開關電流‘為 正’籍制電gCc能量透過變壓器對直流輸出電路ι〇5供電,而 53 1351806 在模式五箝制開關電流W於開關導通前為負,電流流經其寄 生二極體,箝制開關知導通時具零電壓切換特性,且於模式五 至模式七中,箝制開關電流匕均為負,此區間内第一電感電 流h對箝制電容cc充電;⑷表示直流輸出電磨匕、第七開關電 壓心以7、第七開關電流以及理想變壓器二次側電流^,圖 中直流輸出電壓匕穩定輸出400伏特,而第七開關術卿於 理想變壓器二次側電流k降低至零時產生電壓震盪之現象這 籲疋由於當第一開關*^或第二開關\導通,致使變壓器電流降低 至零,此時再將第七開關&與第十開關&截止,或是第八開關 \與第九開關&戴止,開關上寄生二極體之反向恢復電流所造 成洩漏電感與開關寄生電容諧振現象;(e)表示第三開關電壓 VDS,S3、第二開關電流/现幻、第四開關電壓別以及第四開關電 流心以4,由圖中顯示出第三開關電流心力及第四開關電流心”4 以時序區分,透過變壓器升壓對直流輸出電路1〇5供電,並且 •電感電流可在第三開關<s3、第四開關、第五開關<s5及第六開 關&同時導通時,以分流形式減低導通損失,而第三開關&及 第四開關\截止時電壓均箝制於箝制電容電壓厂。 第十九圖表示本發明所揭示高昇壓式隔離型雙輸入電源 轉換器充電功率200瓦特時’第二輸入電壓源&於輸出電源反 鎖狀態之模擬波形響應:(a)表示各開關驅動訊號電壓波形,與 第十二圖波形時序給定之各開關驅動訊號電壓波形相符;(b)表 54 1351806 示第二電感電流b、第二開關電壓V0ii2、第二開關電流、 第三開關電壓以及第三開關電流,由圖中顯示第二電 感電流為負,第二輸入電壓源G之蓄電池以定電流穩定充 電,在此操作狀態中,第二開關4以同步整流方式減低開關導 通損失,開關導通時具零電壓切換特性,而第一開關S及第三 開關$截止時電壓均箝制於箝制電容電壓Fcc,有效改善變壓器 漏感所造成開關電虔突波現象;(c)表示箝制電容電愿厂cc、籍制 Φ 開關電壓v取sc、箝制開關電流bs,sc以及理想變壓器一次側電流 W,箝制電容電壓rcc為定值,且所有低壓側開關截止時均箝制 於此電壓值,當箝制開關\導通時,箝制電容Q先對第二電感 A及第二輸入電壓源G供電,此時箝制開關電流b尤為正,之 後箝制開關電流^為負,由輸出電源反饋能量對箝制電容Cc 充電’而理想變壓器-次側電流^為正值時通過第四開關&及 第五開關&,電流為負值時通過第三開關^及第六開關^ ,輸 電源反饋能量經變壓器降壓後,對第二電感^及第二輸入電 壓源匕供電,(d)表示直流輸出電壓匕、第七開關電壓⑹、第 七開關電抓以及理想變壓器二次側電流〜2,圖中直流輸出 電壓匕反饋時之電壓為铜伏特,直流輸出電鮮。反饋功率為 212瓦特’而第七開關電壓、”於理想變壓器二次側電流^降 低至零時產生電壓震蓋之現象,這是由於當第一開關^導通致 使變壓器電机降低至零,此時再將第七開關^與第十開關〜截 55 1351806 止,或是第八開關&與第九開關&載止,開關上寄生二極體之 反向恢復電流所造成茂漏電感與開關寄生電容諧振現象。 第二十圖表示高昇壓式隔離型雙輪入電源轉換器,各個操 作狀態下之電路模擬轉換效率:⑷表示第一輸人電 立供電狀態下之⑽轉倾率,第—輪人電壓㈣使用28伏特 低壓電源,而直流輸出電壓[為伏特,於此操作狀態下最 ㈣換Μ可㈣96%;_示第二輪人電壓源Κ2於獨立供電 狀態下之電源轉換效率’第二輪入電壓源以用24伏特蓄電 池’而直流輸出電壓匕為400伏特,於此操作狀態下最高轉換 效率可问於94Λ,⑷表不第—輪人電廢源^及第二輸入電壓源 ^於同時供電狀態下之電源轉換效率,第—輸人電壓Μ使用 28伏特低壓電源’第—輸人電愿源[使用μ伏特蓄電池並固 定其輸出功率為200瓦特,而直流輸出電壓匕為_伏特於 此操作狀態下最高熟效率村高於规;⑷以[輪入電 壓源!、供電狀態及第二輸人電壓源[於充電狀態下之電源轉 換效率,第-輪入《源㈣28伏特低壓電源,第二輸入電 壓源F2使用24伐胜苷你 池並固定其充電功率為200瓦特,而直 :電壓K為侧伏特,於此操作狀態下最高轉換效率可高 繼=)表示第二輪入電麼㈣於輸出電源反饋狀態下之電 源轉換效率,第 出電μ於電岐使用24伏特蓄電池'而直流輸 原反饋時為楊伏特,於此操作狀態下最高轉換 56 1351806 效率可高於94% ;由電路模擬結果顯示電源轉換效率於各操作 模式下最高點皆可高於91%,可驗證本發明所揭示之高昇壓式 隔離型雙輸入電源轉換器具有高電源轉換效率之特性。 雖然本發明已前述較佳實施例揭示,然其並非用以限定本 發明,任何熟習此技藝者,再不脫離本發明之精神和範圍内, 當可作各種之變動與修改,因此本發明之保護範圍當視後附之 申請專利範圍所界定者為準。 【圖式簡單說明】 第一圖表示高昇壓式隔離型雙輸入電源轉換器,第一較佳實施 例之電路架構 第二圖表示高昇壓式隔離型雙輸入電源轉換器等效電路 第三圖表示第一輸入電壓源P;於獨立供電狀態之電壓電流時 序波形 第四圖表示第一輸入電壓源^於獨立供電狀態之電路操作模 式 第五圖表示第二輸入電壓源G於獨立供電狀態之電壓電流時 序波形 第六圖表示第二輸入電壓源匕於獨立供電狀態之電路操作模 式 第七圖表示第一輸入電壓源Κ及第二輸入電壓源匕於同時供 電狀態之電壓電流時序波形 57 I351806 第八圓表示第一輸入電壓源γ及第二輸入電壓源匕於同時供 電狀態之電路操作模式 第九圖表示第一輸入電壓源厂 ,於供電狀態及第二輸入電壓源 於充電狀態之電壓電流時序波形 第十圖表示第一輸入電壓源γ於供電狀態及第二輸入電壓源 κ2於充電狀態之電路操作模式 第十一圖表示輸出電源反饋狀態之高昇壓式隔離型雙輸入電 源轉換器等效電路 第十二圖表示第二輸入電壓源匕於輸出電源反饋狀態之電壓 電流時序波形 第十三圖表示第二輸入電壓源&於輸出電源反饋狀態之電路 操作模式 第十四圖表示高昇壓式隔離型雙輸入電源轉換器,第二較佳實 施例之電路架構 • 第十五圖表示高昇壓式隔離型雙輸入電源轉換器,第一輸入電 壓源F;於獨立供電狀態之模擬波形響應 第十六圖表示高昇壓式隔離型雙輸入電源轉換器,第二輸入電 壓源G於獨立供電狀態之模擬波形響應 第十七圖表示高昇壓式隔離型雙輸入電源轉換器,第一輸入電 壓源K及第二輸入電壓源匕於同時供電狀態之模擬 波形響應 58 1351806 第十八圖表示高昇壓式隔離型雙輸入電源轉換器,第一輸入電 壓源γ於供電狀態及第二輸入電壓源κ2於充電狀態 之模擬波形響應 第十九圖表示高昇壓式隔離型雙輸入電源轉換器,第二輸入電 壓源匕於輸出電源反饋狀態之模擬波形響應 第二十圖表示高昇壓式隔離型雙輸入電源轉換器,各個操作狀 態下之電路模擬轉換效率 【主要元件符號說明】 101:第一電源電路 102:第二電源電路 103:全橋式電路 104:主動式箝制電路 105:直流輸出電路 1403:單向全橋式電路 F1:第一輸入電壓源 F2:第二輸入電壓源 匕:直流輸出電壓 A:第一電感 4:第二電感 •s1:第一開關 59 1351806 第二開關 第三開關 第四開關 第五開關 第六開關 第七開關 «V第八開關 第九開關 s1Q:第十開關 箝制開關 心1:第一電源開關 \2:第二電源開關 7;:第一開關驅動訊號 Γ2:第二開關驅動訊號 Γ3:第三開關驅動訊號 Γ4:第四開關驅動訊號 7;:第五開關驅動訊號 7;:第六開關驅動訊號 Γ7:第七開關驅動訊號 Γ8:第八開關驅動訊號 7;:第九開關驅動訊號 1351806 7;。:第十開關驅動訊號 I:箝制開關驅動訊號 7^:第一電源開關觸發訊號 尽2:第二電源開關觸發訊號 7;:隔離變壓器 隔離變壓器一次側 :隔離變壓器二次侧 «:隔離變壓器匝數比率 Ce:箝制電容 ς:第一電容 C2:第二電容 C。:直流輸出電容 Λ。:直流輸出負載 A:第一二極體 d2:第二二極體 d3:第三二極體 d4:第四二極體 61Cc : 220 β¥ C, : 660 ^ F C2 · 660 β F C0 : 100 β ¥ 48 1351806 The fifteenth figure shows that the high-boost isolated dual-input power converter disclosed in the present invention has an output power of 400 watts, the first The analog waveform response of the wheeled voltage source γ in the independent power supply state: (a) indicates the waveform of each switch driving signal voltage, which is consistent with the voltage of each switch driving signal given in the waveform of the third figure; (b) represents the first inductor current L The first switching voltage vDwi, the first switching current center &, the third switching voltage, and the third switching current heart illusion, wherein the first inductor current b is continuous, and the first input voltage source has a stable output power of 416 watts. In addition, • before the first switch Α is turned on, the first switching voltage first drops to zero volts, so the first switch conducts the characteristic of zero voltage switching, and the first switch & and the third switch & In the clamp capacitor voltage factory 7, effectively improve the switching voltage surge caused by the leakage inductance of the transformer; (C) shows the clamp capacitor voltage ^^, clamp switch voltage VDS, ":, clamp switch current state And the ideal transformer primary current ^, the clamp capacitor voltage Fcc is fixed, and all low-voltage side switches are clamped to this voltage value when the switch is turned off, the clamp switch current / take redundant before the switch is turned on, the current flows through its parasitic The pole body 'clamp switch' has the characteristic of zero voltage switching when the SC is turned on, and the third switch & and the sixth switch & when the primary side current of the ideal transformer is positive, the fourth switch is passed when the current is negative. & and the fifth switch & after boosting by the transformer, rectifying and supplying power to the DC output circuit 105; (d) indicating the DC output voltage 匕, the seventh switching voltage, the seventh switching current, and the secondary current diagram of the ideal transformer The medium-to-DC output voltage Κ stabilizes the output of 400 volts, and the seventh switch is electrically generated when the secondary side current of the ideal transformer is reduced to zero. 49 1351806 Phenomenon 'This is because the first switch & conduction causes the transformer current to drop to zero. At this time, the seventh switch "s7" and the tenth switch & The cutoff, or the eighth switch & and the ninth switch 4 are turned off, and the reverse recovery current of the parasitic diode on the switch causes the leakage inductance and the parasitic capacitance of the switch to resonate. Figure 16 is a diagram showing the analog waveform response of the second input voltage source factory 2 in an independent power supply state when the output power of the high-boost isolated dual-input power converter of the present invention is 200 watts: (a) indicates the drive signal voltage of each switch The waveform is consistent with the waveforms of the respective switch drive signals given by the waveforms of the fifth figure; (b) represents the second inductor current L, the second switch voltage vm52, the second switch current core^2, and the third switch voltage %~? 3 and the third switching current zDSS3, the second inductor current L is continuous, and the second input voltage source G stabilizes the output power by 212 watts. In addition, before the second switch & conduction, the second switching voltage is lowered first. Up to zero volts, so the second switch has zero voltage conduction characteristics, and the second switch & and the third switch & off voltage are clamped to the clamp capacitor voltage pcc, effectively improving the leakage inductance caused by the leakage inductance of the transformer The wave phenomenon is compared with the analog waveform response of the first-input voltage source in the independent power supply state. Figure 15 (b), the difference is the time period of the inductor current shunt on the timing, but there are Effectively reduce the conduction loss on the switch; (c) indicates the clamp capacitor voltage factory CC, the box switch electric switch, the box switch current / analog and the ideal transformer - the human side current W, the clamp capacitor voltage Fcc is fixed, And all the low-voltage side switches are clamped to this voltage value when the switch is turned off. The clamp switch current 'is negative before the switch is turned on, the current flows through its parasitic diode, and the clamp switch\ turns on with the characteristic of zero voltage switching 1351806, and the ideal transformer When the primary side current k is positive, the third switch 4 and the ', switch' current are negative, and the fourth switch & and the fifth switch & The output circuit 1G5 supplies power; (4) represents the DC output voltage F. The seventh switching voltage v(10)7, the seventh switching current '7 and the secondary side current core 2 of the ideal transformer, the DC output voltage is stably outputted at 400 volts, and the seventh switching voltage v〇ss7 is reduced at the secondary side of the ideal transformer. The phenomenon of voltage oscillation occurs at zero time, because when the first switch $ is turned on, the transformer current is reduced to zero, and then the seventh switch & and the tenth switch '. The leakage inductance and the parasitic capacitance resonance phenomenon caused by the reverse recovery current of the parasitic diode on the switch of the eighth switch \ and the ninth switch A are turned off. The seventeenth circle shows the analog waveform response of the first input voltage source and the second input voltage source in the simultaneous power supply state when the output power of the high-boost isolated dual-input power converter disclosed in the present invention is 600 watts: (a) The waveforms of the drive signal voltages of the switches are matched with the waveforms of the respective switch drive signals given by the waveforms of the seventh waveform; (b) the first inductor current l, the second inductor current t, the first switch voltage νω, ·? The first switching current, the second switching voltage s2, and the second switching current are, wherein the first inductor current k and the second inductor current are continuous, the first input voltage source γ and the second input voltage are continuous The source κ simultaneously stabilizes the output power. At this time, the output power of the first input voltage source G is 4 〇 5 watts, and the output power of the second input voltage source 220 is 220 watts. In addition, the first switch and the second switch are turned on in this operation mode. Each has the characteristics of zero voltage switching, and the first switch & and the second 51 1351806 switch & cut-off voltage are clamped to the clamp capacitor voltage fcc, effectively improving the switch caused by the leakage inductance of the transformer Voltage surge phenomenon, when the second switch "s2" of mode 4, the second switch current « is still zero, the first switch current is reduced, the conduction loss of the switch can be successfully reduced; the clamp capacitor voltage rcc, the clamp switch voltage VI« .SC, clamp switch current ksc and ideal transformer primary current ^, clamp capacitor voltage Kcc is fixed value, and all low-voltage side switches are clamped to this voltage value when cut off, clamp switch current is negative before switch is turned on, current flows through Its parasitic diode, clamp switch & switch with zero voltage switching characteristics, and the ideal transformer primary current 'is a positive value through the third switch & and the sixth switch & The fourth switch \ and the fifth switch &, after being boosted by the transformer, rectify and supply power to the DC output circuit 1〇5; (the sentence indicates the DC output voltage B, the seventh switching voltage π, the seventh switching current, and the ideal transformer II) The secondary current core 2' shows that the DC output voltage is stable at 400 volts, and the seventh switching voltage va$, ·7 is generated when the secondary side current k of the ideal transformer is reduced to zero. The phenomenon of oscillating oscillating, this is because when the first switch ^ or the second switch ^ is turned on, the current of the transformer is reduced to zero, and then the seventh switch is turned off from the tenth switch ^, or the eighth switch\ And the ninth switch S9 is cut off, the reverse recovery current of the parasitic diode on the switch causes the leakage inductance and the switching parasitic capacitance to resonate; (4) represents the third switching voltage ~, the third switching current ", the fourth switching voltage S and The fourth switch current "(' is shown by the third switch current 3 and the fourth switch current is divided by timing, the DC output circuit 105 is powered by the converter, and 52 1351806 and the inductor current can be in the third switch <; s3, the fourth switch < s4, the fifth switch < s5 and the sixth switch < s6 simultaneously turn on, reduce the conduction loss in the form of shunt, and the voltage of the third switch and the fourth switch are clamped to the clamp capacitor Voltage. Figure 18 is a diagram showing the analog waveform response of the first input voltage source γ to the power supply state and the second input voltage source F2 to the state of charge when the output power of the high-boost isolated dual-input power converter of the present invention is 400 watts: ( a) indicating that each switch driving signal voltage waveform 'conforms with each switch driving signal electric pressure waveform given by the ninth waveform waveform timing; (b) indicates that the first inductor current L, the second inductor current, and the first switching voltage are taken 51 The first switching current, the second switching voltage Vd^2, and the second switching current center, 52' are shown by the figure that the first inductor current L is positive, the second inductor current L is negative 'and both are continuous currents The first input voltage source γ stabilizes the output power, and the second input voltage source stores the battery stably at a constant current. At this time, the first input voltage source 6 has an output power of 658 watts, and the second input voltage source & charging power is 201 watts, the first switch & and the second switch & cut-off voltage are all clamped to the clamp capacitor voltage, effectively improving the switching voltage surge caused by the transformer leakage inductance 'in this operating state The second switch & reduces the conduction loss of the switch by synchronous rectification, and has a zero voltage switching characteristic when the switch is turned on; (c) indicates the clamp capacitor voltage Fcc, the clamp switch voltage v, the clamp switch current, and the ideal transformer primary current. ^, the clamp capacitor voltage Fcc is fixed, and all low-voltage side switches are clamped to this voltage value when turned off. In mode 2, the switch current is 'positive'. Power gCc energy is transmitted through the transformer to the DC output circuit 〇5 Power supply, and 53 1351806 in the mode five clamp switch current W is negative before the switch is turned on, the current flows through its parasitic diode, the clamp switch knows that there is zero voltage switching when turned on, and in mode five to mode seven, the clamp switch The current 匕 is negative, and the first inductor current h charges the clamp capacitor cc in this interval; (4) represents the DC output electric grind, the seventh switch voltage core 7, the seventh switch current, and the ideal transformer secondary current ^, The medium-DC output voltage 匕 stabilizes the output of 400 volts, and the seventh switch sings the voltage oscillation when the secondary side current k of the ideal transformer decreases to zero. Because the first switch *^ or the second switch \ is turned on, causing the transformer current to drop to zero, then the seventh switch & and the tenth switch & cut off, or the eighth switch \ and the ninth switch & wear, the reverse recovery current of the parasitic diode on the switch causes the leakage inductance and the switching parasitic capacitance resonance phenomenon; (e) represents the third switching voltage VDS, S3, the second switching current / the current, the fourth switch The voltage and the fourth switch current core are 4, and the third switch current core force and the fourth switch current core are shown in the figure to be separated by timing. The DC output circuit 1〇5 is supplied through the transformer boost, and • the inductor current When the third switch <s3, the fourth switch, the fifth switch <s5, and the sixth switch & are simultaneously turned on, the conduction loss is reduced in a shunt manner, and the third switch & and the fourth switch \off voltage Both are clamped to the clamp capacitor voltage plant. Figure 19 is a diagram showing the analog waveform response of the second input voltage source & in the output power reverse lock state of the high-boost isolated dual-input power converter with a charging power of 200 watts as shown in the present invention: (a) indicating the respective switch driving signals The voltage waveform is consistent with each of the switch drive signal voltage waveforms given by the waveform timing of the twelfth figure; (b) Table 54 1351806 shows the second inductor current b, the second switch voltage V0ii2, the second switch current, the third switch voltage, and the The three-switch current is shown by the figure that the second inductor current is negative, and the battery of the second input voltage source G is stably charged with a constant current. In this operating state, the second switch 4 reduces the switch conduction loss by synchronous rectification, and the switch is turned on. The zero-voltage switching characteristic is adopted, and the voltages of the first switch S and the third switch $ are clamped to the clamp capacitor voltage Fcc, which effectively improves the switching power surge phenomenon caused by the leakage inductance of the transformer; (c) represents the clamped capacitor electric wish Factory cc, system Φ switch voltage v take sc, clamp switch current bs, sc and ideal transformer primary side current W, clamp capacitor voltage rcc is fixed, and All low-voltage side switches are clamped to this voltage value when the switch is turned off. When the clamp switch is turned on, the clamp capacitor Q first supplies power to the second inductor A and the second input voltage source G. At this time, the clamp switch current b is particularly positive, and then the clamp switch is turned on. The current ^ is negative, the output power supply feedback energy charges the clamp capacitor Cc', and the ideal transformer-secondary current ^ is positive value through the fourth switch & and the fifth switch & the current is negative when passing the third switch ^ and the sixth switch ^, the power supply feedback energy is stepped down by the transformer, the second inductor ^ and the second input voltage source 匕 power, (d) represents the DC output voltage 匕, the seventh switching voltage (6), the seventh switch Grab and the ideal transformer secondary side current ~ 2, the DC output voltage 图 feedback voltage is copper volts, DC output is fresh. The feedback power is 212 watts' and the seventh switching voltage, "the phenomenon of voltage shock is generated when the current of the secondary side of the ideal transformer is reduced to zero. This is because when the first switch is turned on, the transformer motor is reduced to zero. Then, the seventh switch ^ and the tenth switch ~ cut 55 1351806, or the eighth switch & and the ninth switch & the reverse recovery current caused by the reverse parasitic diode on the switch Switching parasitic capacitance resonance phenomenon. Figure 20 shows the high-boost isolated two-wheel-in power converter, the circuit simulation conversion efficiency under various operating conditions: (4) indicates the (10) turn rate under the first input power supply state, The first-wheel voltage (four) uses a 28 volt low-voltage power supply, and the DC output voltage [for volts, the most (four) change in this operating state can be (four) 96%; _ shows the second round of human voltage source Κ 2 in the independent power supply state of the power conversion Efficiency 'The second round-in voltage source uses a 24 volt battery' and the DC output voltage 匕 is 400 volts. The maximum conversion efficiency in this operating state can be 94 Λ, (4) the first-round human waste source and the second Input The voltage source is the power conversion efficiency under the simultaneous power supply state, the first input voltage is 28 28 volts low voltage power supply 'the first input power source [use the μ volt battery and fix its output power is 200 watts, and the DC output voltage匕 is _ volt in this operating state, the highest efficiency village is higher than the regulation; (4) with [wheeling voltage source!, power supply state and the second input voltage source [power conversion efficiency under charge state, the first round" Source (four) 28 volt low-voltage power supply, the second input voltage source F2 uses 24 volts glycosides your pool and fixed its charging power is 200 watts, and straight: voltage K is side volts, the highest conversion efficiency can be high in this operating state =) Indicates the second round of power-in (4) power conversion efficiency in the output power supply feedback state, the first power-off μ is used in the power supply 24 volt battery 'and the DC input original feedback is Yang Volt, the highest conversion 56 1351806 efficiency in this operating state It can be higher than 94%; the circuit simulation results show that the power conversion efficiency can be higher than 91% in each operation mode, which can verify the high-boost isolated dual-input power converter disclosed by the present invention. The invention has the characteristics of high power conversion efficiency. Although the present invention has been disclosed in the foregoing preferred embodiments, it is not intended to limit the invention, and various modifications may be made without departing from the spirit and scope of the invention. The scope of protection of the present invention is defined by the scope of the appended claims. [First Description of the Drawings] The first figure shows a high-boost isolated dual-input power converter, a first preferred embodiment The second diagram of the circuit architecture shows the equivalent circuit of the high-boost isolated dual-input power converter. The third diagram shows the first input voltage source P. The voltage-current timing waveform in the independent power supply state shows the first input voltage source. Circuit Operation Mode in Independent Power Supply State The fifth diagram shows the voltage current timing waveform of the second input voltage source G in the independent power supply state. The sixth diagram shows the circuit operation mode of the second input voltage source in the independent power supply state. An input voltage source Κ and a second input voltage source 匕 in a simultaneous power supply state voltage and current timing waveform 57 I351806 eighth round table The first input voltage source γ and the second input voltage source are in a simultaneous power supply state. The ninth diagram shows the first input voltage source factory, and the voltage and current timing waveforms in the power supply state and the second input voltage source in the charging state. Figure 10 shows the circuit operation mode of the first input voltage source γ in the power supply state and the second input voltage source κ2 in the charging state. Figure 11 shows the equivalent circuit of the high-boost isolated dual-input power converter with the output power feedback state. Figure 12 shows the voltage and current timing waveform of the second input voltage source 输出 in the output power supply feedback state. Figure 13 shows the second input voltage source & circuit operation mode in the output power supply feedback state. Figure 14 shows high boost isolation. Type Dual Input Power Converter, Circuit Architecture of Second Preferred Embodiment • Figure 15 shows a high boost isolated dual input power converter, a first input voltage source F; an analog waveform response in an independent power supply state. The six figures show the high-boost isolated dual-input power converter, and the second input voltage source G is in the independent power supply. In response to the seventeenth diagram, the high-boost isolated dual-input power converter, the first input voltage source K and the second input voltage source are in the simultaneous power supply state of the analog waveform response 58 1351806. Figure 18 shows the high-boost isolation type. The dual input power converter, the first input voltage source γ is in the power supply state, and the second input voltage source κ2 is in the charging state. The analog waveform response is shown in FIG. 19 to represent the high-boost isolated dual-input power converter and the second input voltage source. The analog waveform response in the output power feedback state is shown in the twentieth diagram. The high-boost isolated dual-input power converter has a circuit analog conversion efficiency under various operating conditions. [Main component symbol description] 101: First power supply circuit 102: Two power supply circuit 103: full bridge circuit 104: active clamp circuit 105: DC output circuit 1403: one-way full bridge circuit F1: first input voltage source F2: second input voltage source 匕: DC output voltage A: An inductor 4: a second inductor • s1: a first switch 59 1351806 a second switch a third switch a fourth switch a fifth switch a sixth switch a seventh switch «V eighth Switch ninth switch s1Q: tenth switch clamp switch heart 1: first power switch \2: second power switch 7;: first switch drive signal Γ 2: second switch drive signal Γ 3: third switch drive signal Γ 4: Four switch drive signal 7;: fifth switch drive signal 7;: sixth switch drive signal Γ7: seventh switch drive signal Γ8: eighth switch drive signal 7; ninth switch drive signal 1351806 7; : Tenth switch drive signal I: clamp switch drive signal 7^: first power switch trigger signal 2: second power switch trigger signal 7;: isolation transformer isolation transformer primary side: isolation transformer secondary side «: isolation transformer匝Number ratio Ce: clamp capacitor ς: first capacitor C2: second capacitor C. : DC output capacitor Λ. : DC output load A: first diode d2: second diode d3: third diode d4: fourth diode 61

Claims (1)

1351806 十、申請專利範園:1351806 X. Applying for a patent garden: -種高昇壓式隔離型雙輸入電源轉換器,其中包含 -第-電琢電路:此電路由一個第一輸入電壓源、一個 電源開關、-個第一電容、一個第一電感以及一個 所構成’連接方式為第一輸入電壓源串接第一電源開關,再 串接第-電容,第-電容兩端再串接第—電感及第—開關; 第一電源電路主要功能係透過第—開關之切換,將第入 電壓源電能轉換為第—電感電流,以電流源電能形式呈現; 第一電源電路·此電路由一個第二輸入電壓源、—個 電源開關、-個第二電容、—個第二電感以及—個第二開關 所構成,連接方式為第二輸人電壓源串接第二電源開關,再 串接第一電容’第二電容兩端再串接第二電感及第二開關; 第-電源電路主要功能係透過第二開關之切換,將第二輸入 電壓源電能轉換為第二電感電流,以電流源電能形式呈現; 全橋式電路:此電路由一個第三開關、-個第四開關、一 個第五開關、—個第六開關、—個第七開關、-個第八開關、 個第九開關、-個第十開關以及一個隔離變壓器所構成; 隔離I壓器包含隔離變壓器—次側及隔離變壓器二次側;連 接方式為一般全橋式架構; 主動式籍制電路:此電路由一個箝制開關及-個箝制電容 所構成,連接方式為箝制開關串接箝制電容; 直流輸出電路.此電路由直流輸出電容及直流輪出負載所 構成’係為直流高難流排;連接方式為直流輸出電容並聯 直流輸出負載; 62 1351806 本轉換器之特徵為:第一點,具雙輸入電源雙向轉換機制, 可予許不同電氣特性之電壓源作為輸入端,共同提昇電壓位 準,簡化多組轉換器昇壓再併聯供電之架構,並且依電源管 理而求及供電情形可分為四種狀態:單輸入電源獨立供電、 雙輸入電源同時供電、雙輸入電源分別供電與充電以及輸出 電源反饋,第二點,具高昇壓比及電氣隔離特性,利用隔離 變壓器匝數比與責任週期控制,即可獲得高電壓增益;第三 點,轉換效率高,在輸入輸出電壓隔離架構下,嚴謹區分低 壓側大電流,高壓側低電流特性,分別可選用適合電壓範圍 之低成本高效率功率元件;第四點,主動式電壓箝制技術解 決因隔離變壓器存在洩漏電感所造成之電壓突波問題,並將 洩漏電感能量有效輸出至直流輸出電路;第五點,具導通損 失大幅降低特性,兩輸入電源電路以串聯方式連接,當轉換 器操作於雙輸入電源同時供電狀態時,導通損失可大幅降 低’對於應用於輸入電源為低電壓高電流之潔淨能源時,成 功減小導通損失並可大幅提升轉換效率;第六點,雙輸入電 源端之輸入電流連續,輸入電源以直流電流源電能形式呈 現’並可於電源端擷取出較小漣波之輸入電流,當應用於潔 淨能源為輸入電源時,可有效濾除電流漣波及避免損害潔淨 能源裝置,延長潔淨能源裝置之使用壽命;第七點,功率半 導體開關所承受電壓僅與直流輸出電壓及隔離變壓器之匝 數比有關,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。 2.如申請專利範圍第丨項所述之高昇壓式隔離型雙輸入電源 63 轉換器,其中第一電源開關及第二電源開關之功能為依電源 管理需求,完成第一輸入電壓源或第二輸入電壓源供應或切 離之目的。 如申請專利範圍第1項所述之高昇壓式隔離型雙輸入電源 轉換器,其中第一輸入電壓源以及第二電壓源,可由蓄電 池、超電容、燃料電池、太陽光電池、直流風力發電機或交 流風力發電機整流為直流電源,作為直流電源供應^ 如申請專利範圍第1項所述之高昇壓式隔離型雙輸入電源 轉換器’其中全橋式電路之功能為透過全橋式電路之開關切 換及隔離變壓器匝數比,依照不同之供電狀態,可將第一輸 入電壓源或第二輸入電壓源之能量,分時序對直流輸出電路 之直流輸出電容充電並提供能量給直流輸出負載,或是將輸 出直流電路電能反饋之能量,對具電源儲存特性之輸入電源 充電。 如申請專利範圍第1項所述之高昇壓式隔離型雙輸入電源 轉換器,其中主動式箝制電路之功能為當第一開關或第二開 關戴止瞬間,吸收第一電感電流或第二電感電流與理想變壓 器一次側電流之差,可有效箝制開關電壓以避免突波現象發 生,解決理想變壓器存在洩漏電感之問題。 一種高昇壓式隔離型雙輸入電源轉換器,其中包含 一第一電源電路·此電路由一個第一輸入電壓源、一個第一 電源開關、-個第-電容、一個第一電感以及一個第一開關 所構成;連接方式為第一輸入電壓源串接第一電源開關,再 串接第-電容’第-電容兩端再串接第—電感及第一開關; 1351806 第-電源電路主要功能係透過第—關之㈣,將第一輸入 電塵源電能轉換為第―電感電流,以電流源電能形式呈現; 第-電源電路:此電路由一個第二輸入電壓源、一個第二 電源開關、-個第二電容一個第二電感以及—個第二開關A high-boost isolated two-input power converter comprising a -first-electrode circuit: the circuit consists of a first input voltage source, a power switch, a first capacitor, a first inductor, and a The connection mode is that the first input voltage source is connected in series with the first power switch, and then the first capacitor is connected in series, and the first capacitor is connected in series with the first inductor and the first switch; the main function of the first power circuit is through the first switch Switching, converting the first input voltage source energy into the first inductor current, which is presented in the form of current source power; the first power circuit · the circuit consists of a second input voltage source, a power switch, a second capacitor, The second inductor and the second switch are formed by connecting the second input voltage source to the second power switch, and then connecting the first capacitor in series, and the second capacitor is connected in series with the second inductor and the second The main function of the first power supply circuit is to convert the second input voltage source electric energy into the second inductor current through the switching of the second switch, and present it as a current source electric energy; the full bridge circuit: the circuit is composed of one Three switches, a fourth switch, a fifth switch, a sixth switch, a seventh switch, an eighth switch, a ninth switch, a tenth switch, and an isolation transformer; The I voltage transformer includes an isolation transformer—the secondary side and the secondary side of the isolation transformer; the connection mode is a general full bridge structure; the active system circuit: the circuit is composed of a clamp switch and a clamp capacitor, and the connection mode is a clamp switch. Serial connection clamp capacitor; DC output circuit. This circuit consists of DC output capacitor and DC wheel load. It is a DC high-impedance flow line; the connection method is DC output capacitor parallel DC output load; 62 1351806 This converter is characterized by : The first point is a two-input power bidirectional conversion mechanism. The voltage source with different electrical characteristics can be used as an input terminal to jointly raise the voltage level, simplify the structure of multiple sets of converters and then parallel supply, and according to power management. The power supply situation can be divided into four states: single input power supply, independent power supply, dual input power supply, and dual input power supply. With the charging and output power feedback, the second point, with high boost ratio and electrical isolation characteristics, using the isolation transformer turns ratio and duty cycle control, can obtain high voltage gain; the third point, high conversion efficiency, at the input and output voltage Under the isolation structure, the high-voltage side high-current and high-voltage side low-current characteristics are strictly distinguished, and low-cost high-efficiency power components suitable for the voltage range can be selected respectively. Fourthly, the active voltage clamping technology solves the leakage inductance caused by the isolation transformer. Voltage surge problem, and the leakage inductance energy is effectively output to the DC output circuit; the fifth point has a significant reduction in conduction loss, and the two input power circuits are connected in series, when the converter operates on the dual input power supply simultaneously, The conduction loss can be greatly reduced. 'When applied to clean power with low voltage and high current for input power, the conduction loss is successfully reduced and the conversion efficiency can be greatly improved. The sixth point is that the input current of the dual input power supply is continuous, and the input power is DC. The current source is in the form of electric energy and can be taken out at the power supply The input current of Xiaobo wave can effectively filter out current ripple and avoid damage to clean energy devices and extend the service life of clean energy devices when applied to clean energy input power. The seventh point is that the voltage of the power semiconductor switch is only affected. The DC output voltage is related to the turns ratio of the isolation transformer. This feature is more suitable for power conversion applications where the DC input voltage varies widely. 2. The high-boost isolated dual-input power 63 converter as described in the scope of claim 2, wherein the first power switch and the second power switch function to complete the first input voltage source or the first according to power management requirements Two input voltage sources are supplied or cut away. The high-boost isolated dual-input power converter according to claim 1, wherein the first input voltage source and the second voltage source are a battery, a super capacitor, a fuel cell, a solar cell, a DC wind generator, or The AC wind turbine is rectified to a DC power supply as a DC power supply. ^ The high-boost isolated double-input power converter as described in the first application of the patent scope. The function of the full-bridge circuit is to switch through the full-bridge circuit. Switching and isolating the transformer turns ratio, according to different power supply states, the energy of the first input voltage source or the second input voltage source may be charged, and the DC output capacitor of the DC output circuit is charged and supplied with energy to the DC output load, or It is the energy that outputs the DC circuit power feedback, and charges the input power with the power storage characteristics. The high-boosting isolated dual-input power converter according to claim 1, wherein the active clamping circuit functions to absorb the first inductor current or the second inductor when the first switch or the second switch is worn. The difference between the current and the primary current of the ideal transformer can effectively clamp the switching voltage to avoid the occurrence of a surge phenomenon, and solve the problem of leakage inductance of the ideal transformer. A high-boost isolated two-input power converter includes a first power circuit. The circuit includes a first input voltage source, a first power switch, a first capacitor, a first inductor, and a first The switch comprises: the first input voltage source is connected in series with the first power switch, and then the first capacitor is connected in series with the first capacitor and the first inductor is connected in series; 1351806 main function of the first power circuit Through the first-off (four), the first input electric dust source electric energy is converted into the first “inductance current, which is presented in the form of current source electric energy; the first power supply circuit: the circuit is composed of a second input voltage source and a second power switch, a second capacitor, a second inductor, and a second switch 所構成;連接方式為第二輸人電麼源串接第二電源開關,再 串接第二電容’第二電容兩端再串接第二電感及第二開關; 第二電源電路主要功能係透過第二開關之切換,將第二輸入 電虔源電能轉換為第二電感電流,以電流源電能形式呈現; -單向全橋式電路:此電路由—個第三開關、—個第四開 關、-個第五開關、一個第六開關、一個第一二極體、一個 第二二極體、一個第三二極體、 一個第四二極體以及一個隔 離變壓器所構成,隔離變壓器包含隔離變壓卜次側及隔離 變壓器二次側;連接方式為一般全橋式架構; -主動式箝制電路:此電路由—個箝制開關及—個箝制電容 所構成;連接方式為箝制開關串接箝制電容; -直流輸出電路:此電路由直流輸出電容及直流輸出負載所 構成’係為直流高壓匯流排;連接方式為直流輸出電容並聯 直流輸出負載; 本轉換器之特徵為:第-點’具雙輪人電源機制及電源儲存 裝置充電機制’可予許不同電氣特性之電壓源作為輸入端, 共同提昇電壓位準’簡化多組轉換器昇壓再併聯供電之架 構’並且依電源管理需求及供電情形可分為三種狀態:單輸 入電源獨立供電、雙輸人電關時供f以及雙輸人電源分別 供電與充電;第二點’具高昇壓比及電氣隔離特性,利用隔 65 1351806 離變壓器匝數比與責任週期控制,即可獲得高電壓增益;第 三點’轉換效率高’在輸入輸出電壓隔離架構下,嚴謹區分 低壓側大電流,高壓側低電流特性,分別可選用適合電壓範 圍之低成本高效率功率元件;第四點,主動式電壓箝制技術 解決因隔離變壓器存在洩漏電感所造成之電壓突波問題,並 將洩漏電感能量有效輸出至直流輸出電路;第五點,具導通 損失大幅降低特性,兩輸入電源電路以串聯方式連接,當轉 換器操作於雙輸入電源同時供電狀態時,導通損失可大幅降 低,對於應用於輸入電源為低電壓高電流之潔淨能源時,成 功減小導通損失並可大幅提升轉換效率;第六點,雙輸入電 源端之輸入電流連續,輸入電源以直流電流源電能形式呈 現,並可於電源端擷取出較小漣波之輸入電流,當應用於潔 淨能源為輸入電源時,可有效濾除電流漣波及避免損害潔淨 能源裝置,延長潔淨能源裝置之使用壽命;第七點,功率半 導體開關所承受電壓僅與直流輸出電壓及隔離變壓器之阻 數比有關,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;第八點,單向全橋式電路架構簡單,單向全橋 式電路僅使用四顆開關及四顆二極體,即具對電源儲存裝置 充電迴路之機制。 .如申請專利範圍第6項所述之高昇壓式隔離型雙輸入電源 轉換器,其中第一電源開關及第二電源開關之功能為依電源 s理需求,完成第一輸入電壓源或第二輸入電壓源供應或切 離之目的》 8_如中請專利範圍第6項所述之高昇壓式隔離型雙輸入電源 66 1351806 轉換器彡中第一輸入電壓源以及第二電壓源可由蓄電 池超電各、燃料電池、太陽光電池、直流風力發電機或交 流風力發電機整流為直流電源,作為直流電源供應。 9. 如申請專利範圍第6項所述之高昇壓式隔離型雙輸入電源 轉換器其中全橋式電路之功能為透過全橋式電路之開關切 換及隔離變壓器®•數比,依照不同之供電狀態’可將第-輸 入電壓源或第二輸人電壓源之能量,分時序對直流輸出電路 之直流輪出電容充電並提供能量給直流輸出負載。 10. 如申請專利範圍第ό項所述之高昇壓式隔離型雙輸入電源 轉換器,其中主動式箝制電路之功能為當第—開關或第二開 關截止瞬間’吸收第一電感電流或第二電感電流與理想變壓 器一次側電流之差,可有效箝制開關電壓以避免突波現象發 生,解決理想變壓器存在洩漏電感之問題》 67The second power switch is connected in series with the second power switch, and the second capacitor is connected in series. The second capacitor is connected in series with the second inductor and the second switch. The main function of the second power circuit is Through the switching of the second switch, the second input electric source energy is converted into the second inductor current, which is presented in the form of current source electric energy; - one-way full bridge circuit: the circuit is composed of a third switch, a fourth The switch, the fifth switch, the sixth switch, a first diode, a second diode, a third diode, a fourth diode, and an isolation transformer, the isolation transformer includes Isolation transformer side and isolation transformer secondary side; connection mode is general full bridge structure; - active clamp circuit: this circuit is composed of a clamp switch and a clamp capacitor; the connection mode is clamp switch series Clamping capacitor; - DC output circuit: This circuit consists of DC output capacitor and DC output load 'as DC high voltage bus; connection mode is DC output capacitor parallel DC output negative The characteristics of this converter are: the first point 'with two-wheeled person power mechanism and the power storage device charging mechanism' can be used as a voltage source with different electrical characteristics as the input terminal to jointly raise the voltage level 'simplified multi-group converter The structure of voltage and parallel power supply can be divided into three states according to power management requirements and power supply conditions: single input power supply independent power supply, dual input power supply off supply f and dual input power supply separately supply and charge; High boost ratio and electrical isolation characteristics, high voltage gain can be obtained by using the transformer ratio and duty cycle control of 65 1351806. The third point is 'high conversion efficiency'. Under the input and output voltage isolation architecture, the low voltage side is strictly distinguished. Current, high-voltage side low-current characteristics, respectively, can choose low-cost high-efficiency power components suitable for voltage range; Fourth, active voltage clamping technology solves the voltage surge problem caused by leakage inductance of isolation transformer, and will leak inductance Energy is effectively output to the DC output circuit; the fifth point has a significant reduction in conduction loss characteristics, two inputs The source circuits are connected in series. When the converter is operated in a dual-input power supply state, the conduction loss can be greatly reduced. When applied to a clean energy source with low voltage and high current input power, the conduction loss is successfully reduced and can be greatly improved. Conversion efficiency; sixth point, the input current of the dual input power supply is continuous, the input power is presented in the form of DC current source power, and the input current of the smaller chopping wave can be taken out at the power supply end, when applied to the clean energy source as the input power source It can effectively filter out current ripple and avoid damage to clean energy devices and prolong the service life of clean energy devices. The seventh point is that the voltage of the power semiconductor switch is only related to the DC output voltage and the resistance ratio of the isolation transformer. This feature is more suitable. The application of the power conversion device with a wide range of DC input voltage variation; the eighth point, the one-way full-bridge circuit structure is simple, and the one-way full-bridge circuit uses only four switches and four diodes, that is, the power storage device is charged. The mechanism of the loop. The high-boosting isolated dual-input power converter according to claim 6, wherein the first power switch and the second power switch function to complete the first input voltage source or the second according to the power supply requirement The purpose of the input voltage source is to supply or cut off. 8_ The high-boost isolated dual-input power supply 66 1351806 as described in the patent scope, the first input voltage source and the second voltage source can be super-accumulated by the battery. Electricity, fuel cells, solar cells, DC wind turbines or AC wind turbines are rectified into DC power supplies as DC power supplies. 9. The high-boost isolated dual-input power converter as described in claim 6 wherein the function of the full-bridge circuit is to switch the switching and isolation transformers of the full-bridge circuit. The state 'characterizes the energy of the first input voltage source or the second input voltage source, and sequentially charges the DC output capacitor of the DC output circuit and supplies energy to the DC output load. 10. The high-boost isolated dual-input power converter as described in the scope of the patent application, wherein the function of the active clamping circuit is to absorb the first inductor current or the second when the first switch or the second switch is turned off. The difference between the inductor current and the primary current of the ideal transformer can effectively clamp the switching voltage to avoid the occurrence of glitch and solve the problem of leakage inductance of the ideal transformer.
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