TW201021384A - Efficient bidirectional conversion device - Google Patents
Efficient bidirectional conversion device Download PDFInfo
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- TW201021384A TW201021384A TW097145142A TW97145142A TW201021384A TW 201021384 A TW201021384 A TW 201021384A TW 097145142 A TW097145142 A TW 097145142A TW 97145142 A TW97145142 A TW 97145142A TW 201021384 A TW201021384 A TW 201021384A
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02B—CLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO BUILDINGS, e.g. HOUSING, HOUSE APPLIANCES OR RELATED END-USER APPLICATIONS
- Y02B70/00—Technologies for an efficient end-user side electric power management and consumption
- Y02B70/10—Technologies improving the efficiency by using switched-mode power supplies [SMPS], i.e. efficient power electronics conversion e.g. power factor correction or reduction of losses in power supplies or efficient standby modes
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201021384 九、發明說明: 【發明所屬之技術領域】 本,明是有關於-種轉換裝置,特別是指_種直流轉 直流的高效能雙向轉換裝置。 【先前技術】201021384 IX. Description of the invention: [Technical field to which the invention pertains] The present invention relates to a conversion device, and more particularly to a high-performance bidirectional conversion device for DC-DC. [Prior Art]
如圖1所示,美國專利號US 7382113 B2提出一種習知 的雙向轉換裝置,適用於設在一蓄電、池&和—電容g之 間’且可對能量進行雙向的轉換以使能量由蓄電池匕向電 容Q方向釋放或由電容。向蓄電池^方向釋放。當能量 釋放方向是由蓄電池匕往電容^時,此時蓄電池匕是作 為一,源,對料負載的電纟^進行充電;而當能量釋放 方向疋由電谷CV往蓄電池&時,此時電容c从是作為一電 源,對作為負載的蓄電池匕進行充電。 該雙向轉換裝置包含:一耦合電路i、一第一開關 、-第二開關102、一第三開關1〇3、一第一二極體⑴、 第極體112、一第三二極體113、一第一電容a!、 一第二電容122,及一電感13。 該鶴合電路1包括一第_繞組u,及一第二繞組Η。 且每一繞組11、12具有—極性點端和-非極性點端。該第 一繞組11之極性點端與該蓄電池^電連接。 該第開關101電連接於該第一繞組U之非極性點端 和地之間’且可在導通狀態和不導通狀態間切換。 該第-極體ln具有—電連接於該第—繞組U之非 極性點端的陽極,及一陰極。 5 201021384 該第-電容121電,接於該第一二極體u之陰極和地 之間。 、 該第三二極體113具有一電連接於該第一二極體ui之 陰極的陽極,及一陰極。 該第二電容122電連接於該第二繞組12之非極性點端 和該第三二極體113的陰極之間。 該第二二極體112具有一電連接於地的陽極,及一陰極 〇 该電感13電連接於該第一繞組u之極性點端和該第二 二極體112的陰極之間。 該第二開關1G2電連接於該該第二二極體112的陰極和 該第二—極體113的陰極m且可在導通狀態和不導通狀 態間切換。 該第三開關103可在導通狀態和不導通狀態間切換, 且具有-電連接於該第三二極體113的陰極的第—端和電連 接於該電容的第二端。 根據所需的能量釋放方向,此雙向轉換裝置會進行相 對應的切換,以使能量由蓄電池匕流向電容c似或是由電 容Ca/流向蓄電池^,而此雙向轉換裝置詳細的作動情形可 參考此專利案,在此不再贅述。簡言< ’此習知的雙向轉 換裝置具有以下缺點:需要額外的電感與多個二極體才能 完成雙向轉換的功能,尤其二極體導通損失多於具有同: 整流功能的每一開關,且所有開關之柔性切換效果不明顯 ,因此轉換效率有待進一步提升,又整個電路因外加電感 201021384 ,使成本較高且體積也較大。 【發明内容】 因此’本發明之目的’即在提供高轉換效率並能避免 上述習知缺失的高效能雙向轉換裝置。 該咼效能雙向轉換裝置’適用於設在一第一儲能單元 和一第二储能單元之間,且包括: 一耦合電路,包括一第一繞組,及一第二繞組,且每 一繞組具有一第一端和一第二端,該第一繞組之第一端電 連接於該第一儲能單元,而該第一繞組的第二端與該第二 繞組的第一端電連接; 一第一開關,具有一電連接於該第一繞組之第二端的 第端和一接地的第二端,且可在導通狀態和不導通狀態 間切換; 一第二開關,具有一電連接於該第一繞組之第二端的 第一端和一第二端,且可在導通狀態和不導通狀態間切換 9 一第三開關,具有一電連接於該第二開關之第二端的 第一端和一電連接於該第二繞組之第二端的第二端,且可 在導通狀態和不導通狀態間切換; 一第四開關,具有一電連接於該第三開關之第二端的 第一端和一電連接於該第二儲能單元的第二端,且可在導 通狀態和不導通狀態間切換;及 •—第-電容’電連接於該第二開關的第二端和地之間 201021384 透過該等開關的切換,可使該第一儲能單元的能量釋 放至該第二儲能單元或使該第二儲能單元的能量釋放至該 第一儲能單元。 本發明之功效在於僅使用四個功率半導體開關元件即 元成雙向電流之控制,而用電壓箝制、同步整流與零電壓 切換及零電流切換方式有效地降低開關之導通損失,且耗 合電路嚴格劃分高、低壓側之電流大小以充分使用元件規 格,使得本裝置具有低切換損失與低導通損失之特性,以 達到高轉換效率之目的。 【實施方式】 有關本發明之前述及其他技術内容、特點與功效,在 以下配合參考圖式之一個較佳實施例的詳細說明中將可 清楚的呈現。 如圖2所示,本發明高效能雙向轉換裝置之較佳實施 例適用於設在一第一儲能單元和一第二儲能單元之間,且 可對能量進行雙向的轉換以由第一储能單元向第二 儲能單元方向釋放或由第二儲能單元向第—儲能單元方向 釋放。當能量釋放方向是由第—儲能單元往第二儲能翠元 時’此時第-儲能單元是作為一電源,對作為負載的第二 铸能單元進行充電;而當能量釋放方向是由第二储能單Γ 在第-儲能單元時,此時第二儲能單元是作為―,: 作為負載的第一儲能單元進行充電。 ' 而在本實施例中,該第 且該電池包括蓄電池、 明 一儲能單元以一電池為例作說 燃料電池、太陽能電池等 ~ 而 201021384 該第-儲能單元也可為其他直流發電農置,且不以這些為 限。而在本實施例中,該第二儲能單元是以一輸出電容 為例作說明’但不以此為限。錄本實施例中該第一儲w 能單元相較於該第二儲能單元而言,是—低Μ㈣能元件 ,而該第二儲能單元可併入一高壓的匯流排中使用。 該雙向轉換裝置之較佳實施例包括:一耦合電路八、 -第-開I"…第二開關&、一第三開關&、一第四開 關&、一第—電容C;,及一第二電容As shown in Fig. 1, U.S. Patent No. 7,382,113 B2 proposes a conventional bidirectional conversion device suitable for being placed between a power storage, a pool & and a capacitor g and capable of bidirectionally converting energy to enable energy The battery is discharged toward the capacitor Q or by a capacitor. Release to the battery ^ direction. When the energy release direction is from the battery to the capacitor ^, then the battery 匕 is used as a source, the charge of the load is charged; and when the energy release direction is from the electricity valley CV to the battery & The capacitor c is used as a power source to charge the battery pack as a load. The bidirectional conversion device includes: a coupling circuit i, a first switch, a second switch 102, a third switch 1〇3, a first diode (1), a pole body 112, and a third diode 113. a first capacitor a!, a second capacitor 122, and an inductor 13. The crane circuit 1 includes a first winding u and a second winding 。. And each of the windings 11, 12 has a -polar point end and a - non-polar point end. The polarity end of the first winding 11 is electrically connected to the battery. The first switch 101 is electrically connected between the non-polar point end of the first winding U and the ground and is switchable between a conducting state and a non-conducting state. The first pole body ln has an anode electrically connected to a non-polar point end of the first winding U, and a cathode. 5 201021384 The first capacitor 121 is electrically connected between the cathode of the first diode u and the ground. The third diode 113 has an anode electrically connected to the cathode of the first diode ui, and a cathode. The second capacitor 122 is electrically connected between the non-polar dot end of the second winding 12 and the cathode of the third diode 113. The second diode 112 has an anode electrically connected to the ground, and a cathode 〇 electrically connected between the polarity end of the first winding u and the cathode of the second diode 112. The second switch 1G2 is electrically connected to the cathode of the second diode 112 and the cathode m of the second body 113 and is switchable between a conducting state and a non-conducting state. The third switch 103 is switchable between an on state and a non-conducting state, and has a first end electrically connected to the cathode of the third diode 113 and a second end electrically connected to the capacitor. According to the required energy release direction, the bidirectional conversion device performs corresponding switching so that the energy flows from the battery to the capacitor c or from the capacitor Ca/ to the battery, and the detailed operation of the bidirectional converter can be referred to. This patent case is not described here. Briefly < 'This conventional bidirectional conversion device has the following disadvantages: an additional inductance and multiple diodes are required to perform the bidirectional conversion function, especially the diode conduction loss is more than each switch having the same: rectification function The flexible switching effect of all switches is not obvious, so the conversion efficiency needs to be further improved, and the whole circuit is costly and bulky due to the external inductance 201021384. SUMMARY OF THE INVENTION Therefore, the object of the present invention is to provide a high-performance bidirectional conversion device which has high conversion efficiency and can avoid the above-mentioned conventional deficiencies. The 咼 performance bidirectional conversion device is adapted to be disposed between a first energy storage unit and a second energy storage unit, and includes: a coupling circuit including a first winding, and a second winding, and each winding Having a first end and a second end, the first end of the first winding is electrically connected to the first energy storage unit, and the second end of the first winding is electrically connected to the first end of the second winding; a first switch having a first end electrically connected to the second end of the first winding and a grounded second end, and switchable between a conductive state and a non-conductive state; a second switch having an electrical connection a first end and a second end of the second end of the first winding, and switchable between a conducting state and a non-conducting state, a third switch having a first end electrically connected to the second end of the second switch And a second end electrically connected to the second end of the second winding, and switchable between a conductive state and a non-conductive state; a fourth switch having a first end electrically connected to the second end of the third switch And electrically connected to the second end of the second energy storage unit, Switching between a conducting state and a non-conducting state; and - the first capacitor is electrically connected between the second end of the second switch and the ground 201021384 by switching the switches to enable the first energy storage unit The energy is released to the second energy storage unit or the energy of the second energy storage unit is released to the first energy storage unit. The invention has the effect of using only four power semiconductor switching elements, that is, the control of the bidirectional current, and the voltage clamping, the synchronous rectification and the zero voltage switching and the zero current switching manner effectively reduce the conduction loss of the switch, and the consumption circuit is strict. The currents of the high and low voltage sides are divided to fully utilize the component specifications, so that the device has the characteristics of low switching loss and low conduction loss to achieve high conversion efficiency. The above and other technical contents, features, and advantages of the present invention will be apparent from the following detailed description of the preferred embodiments. As shown in FIG. 2, the preferred embodiment of the high-performance bidirectional conversion device of the present invention is adapted to be disposed between a first energy storage unit and a second energy storage unit, and can perform bidirectional conversion of energy to be first. The energy storage unit is released toward the second energy storage unit or released by the second energy storage unit toward the first energy storage unit. When the energy release direction is from the first energy storage unit to the second energy storage Cuiyuan, the first energy storage unit acts as a power source to charge the second casting energy unit as a load; and when the energy release direction is When the second energy storage unit is in the first energy storage unit, the second energy storage unit is charged as the first energy storage unit as the load. In the present embodiment, the battery includes a battery, and the first energy storage unit uses a battery as an example for a fuel cell, a solar cell, etc. - and 201021384 the first energy storage unit can also be other DC power generation farms. Set, and not limited to these. In this embodiment, the second energy storage unit is an output capacitor as an example, but is not limited thereto. In the embodiment, the first energy storage unit is a low-lying (four) energy component compared to the second energy storage unit, and the second energy storage unit can be incorporated into a high-voltage busbar. The preferred embodiment of the bidirectional conversion device includes: a coupling circuit VIII, a first-open I" second switch & a third switch & a fourth switch & a first capacitor C; And a second capacitor
該耦合電路rr包括二個繞於一鐵蕊(圖 ,分別是-第-繞一及一第二一其中,二 1·Ν。且每—繞組以具有一第一端(為極性點端)及一第二端 (為非極性點端)。該第—繞組之極性點端與該電池電連 接’而該第—繞組4的非極性點端與該第二繞組h的極 性點端電連接。 山該第—開關&具有一電連接於該第一繞組z尸之非極性 點端的第_端和一接地的第二端,且可在導通狀態和不導 通狀態間切換。 § 開關&具有一電連接於該第一繞組之非極性 點端的第一Λ* 和一第二端,且可在導通狀態和不導通狀態 間切換。 I第一開關&具有一電連接於該第二開關&之第二端 的第·^端知 —第二端’且可在導通狀態和不導通狀態間切 換。 第四開關&具有一電連接於該第三開關&之第二端 201021384 的第一端和一電連接於該輸出電容的第二端,且可在導 通狀態和不導通狀態間切換。 該第一電容電幻連接於該第二開關&的第二端和地之 間。 該第二電容C"2電連接於該第三開關&的第二端和第二 繞組b的非極性點端之間。 根據所需的能量釋放方向,此高效能雙向轉換裝置會 進行相對應的切換,以使能量由輸出電容c"流向電池或是 由電池流向輸出電容當能量由輪出電容流向電池時 〇 ’經由南效能雙向轉換裝置在能量傳輸的過程將輸出電容 之電壓匕降低後提供給電池,使電池得到一低於輸出電 容的電壓,簡稱此時為降壓模式。而當能量由電池流向 輸出電容時,經由高效能雙向轉換裝置昇壓在能量傳輸 的過程將電池之電壓厂L提高後提供給輸出電容Ch,使輸出 電容得到一高於電池的電壓,以下簡稱此時為昇壓模式 〇 在執行降壓模式時,主要藉由第四開關&導通與截止 © ’控制錯存或釋放耦合電路7;之能量’以調節該電池的電 壓厂ί。其餘三個開關&、5^及&搭配第四開關*SV切換,時 序操作為當第四開關&先導通,隨之第二開關&再導通, 且當第四開關心和第二開關&皆不導通之後’第—開關& 和第三開關&再同時導通。 在執行昇壓模式時,主要藉由第〆開關A之導通與截 止’控制儲存或釋放耦合電路八之能量’以調整該輸出電 10 201021384 容的電壓4。其餘三個開關&、&及&搭配第一開關 &切換,時序操作為當第一開關&先導通,隨之第三開關 A再導通,且當第一開關&和第三開關&皆不導通之後, 第二開關&和第四開關&再同時導通。以下即針對降壓 方面、昇壓方面這二種情形來對整個電路的運作分別 說明。 A·降壓方面: 參閲圖3,依據該四開關&、&、&、&的切換,此高 效月b雙向轉換裝置會在七種模式下作動,以下圖4~i〇分別 針對每-模式進行說明,且值得注意的是,為了方便說明 ,模式® 4〜1〇巾的第一儲能單元直接用電池來表示,而該 第二儲能單元直接用輸出電$ G表示。且圖3和圖^中 的^、匕4參數分別代表第一開關&、第二開關 &第一開關&、第四開關心之控制端的電壓,心、。別 代表流過該第-繞組的電流、流過該第二繞組&的電流 ,&、參數分別代表流過該第一開關&的電流、該第一 開關&之兩端的電壓Ά參數分別代表流過第二開關 &的電流、該第二開關&之兩端的電壓參數分別 代表抓過第三開關&的電流、該第三開關&之兩端的電壓 Ά參數分別代表流過第四„ ^的電流、該第四開 關A之兩端的電壓。 模式一(時間:: 參閱圖4,在此模式一下,該第二開關&和第四開關 心已導通—段時間而其餘開關不導通。且圖4中標示出在 11 201021384 此模式一下,電流路徑的走向。且以下為了方便說明,不 導通的開關(在_此模式為:第一開關心和第三開關d以虛 線表示。 電池進行充電: 輸出電谷C"提供一電流先依序經由第四'開關、第二 電容匸2及該第一繞組’然後分成兩路徑電流,其_電流 經由第一繞組1/>對電池充電。 第一電容c7進行充電:The coupling circuit rr includes two windings (Fig., respectively - first-to-one and one second, two and one), and each winding has a first end (which is a polarity end) And a second end (which is a non-polar point end). The polarity end of the first winding is electrically connected to the battery, and the non-polar point end of the first winding 4 is electrically connected to the polarity end of the second winding h The first switch-ample has a first end electrically connected to the non-polar end of the first winding z and a grounded second end, and is switchable between a conducting state and a non-conducting state. § Switch & Having a first Λ* and a second end electrically connected to the non-polar point end of the first winding, and switchable between an on state and a non-conduction state. The first switch & has an electrical connection to the The second end of the second switch & the second end 'and the second end' can be switched between the on state and the non-conducting state. The fourth switch & has an electrical connection to the second end of the third switch & The first end of 201021384 and an electrical connection are connected to the second end of the output capacitor, and can be in a conducting state and not conducting Inter-state switching. The first capacitor is electrically connected between the second end of the second switch & ground. The second capacitor C" 2 is electrically connected to the second end of the third switch & Between the non-polar end of winding b. According to the required energy release direction, the high-efficiency bidirectional converter will perform the corresponding switching so that the energy flows from the output capacitor c" to the battery or from the battery to the output capacitor. When the capacitor is discharged from the capacitor to the battery, the voltage of the output capacitor is reduced in the process of energy transmission through the south-efficiency bidirectional conversion device, and then the battery is supplied to the battery, so that the battery obtains a voltage lower than the output capacitor. When the energy flows from the battery to the output capacitor, the voltage is boosted by the high-efficiency bidirectional conversion device to increase the voltage of the battery L to the output capacitor Ch, so that the output capacitor obtains a voltage higher than the battery. Referred to as the boost mode at this time, when the buck mode is executed, the fourth switch & turn-on and turn-off © 'control error or release coupling circuit 7; The quantity 'to adjust the voltage of the battery factory ί. The other three switches &, 5^ & with the fourth switch * SV switch, the timing operation is when the fourth switch & first turn on, followed by the second switch & Re-conducting, and when the fourth switch core and the second switch & are not turned on, the 'first switch' and the third switch & are simultaneously turned on. When the boost mode is executed, mainly by the third switch A Turn on and off 'control storage or release the energy of the coupling circuit eight' to adjust the voltage of the output power 10 201021384. The remaining three switches &, & && with the first switch & switching, timing operation is The first switch & is turned on first, and then the third switch A is turned on again, and after the first switch & and the third switch & are not turned on, the second switch & and the fourth switch & The following is a description of the operation of the entire circuit for both the buck and boost aspects. A·Bucking aspect: Referring to Figure 3, according to the switching of the four switches &amper &, &, &, &, the high efficiency monthly b bidirectional converter will operate in seven modes, as shown in Figure 4 below. Explain separately for each mode, and it is worth noting that, for convenience of explanation, the first energy storage unit of the mode® 4~1 wipe is directly represented by a battery, and the second energy storage unit directly uses the output power $G. Said. The parameters of ^ and 匕4 in Fig. 3 and Fig. 2 respectively represent the voltage, heart, and the control terminals of the first switch & second switch & first switch & Do not represent the current flowing through the first winding, the current flowing through the second winding & the parameters represent the current flowing through the first switch & the voltage across the first switch & The parameters respectively represent the current flowing through the second switch & the voltage parameters at the two ends of the second switch & respectively represent the current drawn through the third switch & the voltage Ά parameter at the two ends of the third switch & The current flowing through the fourth „ ^, the voltage across the fourth switch A. Mode 1 (Time:: Refer to Figure 4, in this mode, the second switch & and the fourth switch is turned on – time The remaining switches are not turned on. And in Figure 4, the current path is shown in this mode at 11 201021384. And for the sake of convenience, the non-conducting switch (in this mode is: the first switch and the third switch d) The battery is charged. The battery is charged: the output electric current C" provides a current through the fourth 'switch, the second capacitor 匸2 and the first winding' and then splits into two path currents, and the current flows through the first winding 1 />for battery The electrical charge of the first capacitor c7:
另一電流經由第二開關&對第一電容。進行充電,且Another current is passed to the first capacitor via the second switch & Charging, and
Vzj*及參數分別為第一繞組〇的電壓和第二繞組k的電壓 ,兩者關係式為 因此’輸出電容之電壓6可表示成 V»=VC2+Vls+vlp+Vl=(<N + 1)Vu>+Vci^Vl ⑺ 又第一 vsi =VL + 開關&為不導通狀態,其跨壓為 〜=vcl (3) 模式二(時間 W2):Vzj* and the parameters are the voltage of the first winding 〇 and the voltage of the second winding k, respectively. The relationship between the two is such that the voltage 6 of the output capacitor can be expressed as V»=VC2+Vls+vlp+Vl=(<N + 1) Vu>+Vci^Vl (7) The first vsi = VL + switch & is non-conducting, and its voltage across is ~=vcl (3) mode two (time W2):
所示,在模式一下,該第二開關&和第四開關 =已導通—段時間而其餘開關不導通。圖5中標示出在此 模式—下,電流路徑的走向。 签it電容C;開始經由第一繞組〇放電至電池,使流經 ^ _ 2之電流轉向,其餘路徑維持前一模式運作。 模式三(時間:W3): 如圖6献- 所不’在此模式三下,所有開關皆不導通,且 12 201021384 圖6中標示出在此模式下,電流路徑的走向。 漏感能量釋放: 當第四開關心剛不導通時,因為第一繞組、第二繞 組Zs之漏感與&的能量必須釋放’所以第一繞組I?之電 流心流經第一開關&的基體二極體續流,且第二繞組^^之 電流L則經由第一電容ς及第三開關&的基體二極體路徑 續流,導致第一開關&及第三開關&之兩端為零電壓,以 在下一個模式進行零電壓切換。As shown, in the mode, the second switch & and the fourth switch = have been turned on for a period of time while the remaining switches are not conducting. The direction of the current path in this mode is indicated in Figure 5. The it capacitor C is marked; it begins to discharge to the battery via the first winding, and the current flowing through ^ _ 2 is turned, and the remaining paths maintain the previous mode operation. Mode 3 (Time: W3): As shown in Figure 6 - No. In this mode, all switches are not conducting, and 12 201021384 Figure 6 shows the direction of the current path in this mode. Leakage energy release: When the fourth switch core is not conducting, because the leakage inductance of the first winding and the second winding Zs and the energy of the & must be released, the current of the first winding I? flows through the first switch & The base diode is freewheeling, and the current L of the second winding is freewheeled through the first capacitor ς and the base diode path of the third switch & the first switch & and the third switch & The two ends are zero voltage to switch to zero voltage in the next mode.
模式四(時間:r3〜r4): 如圖7所示,在此模式下,該第一開關&和第三開關 &開始導通而其餘開關不導通。且圖7中標示出在此模式 下’電流路徑的走向。 因為在前一模式時,第一開關&及第三開關&之基體 二極體已經導通,本模式開始時使該二開Μ A、&導通, 成為具低導通損失之同步整流(synchr〇n〇us代…狀 態。. 當第二繞組之漏感能量釋放完時,經由第三開關& 之電流轉向,且第三開關&為零電廢導通,因此無切換損 失。同時’第二電容c2進行放電至第二繞組,藉由磁路 感應方式感應至第-繞組ο且將能量釋放至電池。 令第四開關&之導通責任週期(Duty Cycle)為4 ,且勿、 略交越之暫態時間,目,丨d & 〜 之關係式為 4與^導通責任週期^ 4 + 名=1 (4) 13 201021384 此時第一繞組之電壓Vip等於電池之電壓&,依據伏_ 秒平衡(V〇lt-Second Balance),可得模式一中之第一繞組〇 的電壓L為 VLP = ^x[(l-i/4)M] (5) 將上式代入方程式(3),可得第一電容C;之電壓Vci為 vci=^+vi/)=Fi/ii4=vsl (6) 第一電容C/之電壓vcl也等同於第一開關&之跨壓〜, 利用上式可以計算第二電容q之電壓%為 VC2=V„-VC1 =^ + 1/^) (7) ❹ 將方程式(5)及(7)代入方程式(2)可求出降壓比%為 ^=VjVH=dJ{N^2) (8) 再將上式代入方程式(6)可得到 ^sl=K/(JV + 2) = vS2 (9) 當匝數比N固定時,第一開關&和第二開關&之跨壓 VS1 與輸出電容之電壓4有關,與第四開關&之責任 週期4及電池之電壓無關’所以可使用低壓低導通損的金屬 氧化物半導趙場效電晶體(MOSFET)作為開關。 〇 模式五(時間:ί4〜ί5): 如圖8所示,在此模式下,每—開關皆不導通。且圖8 中標示出在此模式下,電流路徑的走向。 备第一開關Α和第三開關&剛不導通時,因為第一繞 k、第二繞組心之漏感4]與心仍有能量釋放,因此第一 繞紐Ο之電流k流經第一開關&之基體二極體續流,且第 二繞組L之電流匕則經由第二電容q和第四開關&之基艎 14 201021384 二極體的絡徑續流至輸出電容,導致該第四開關心兩端 為零電壓’等待下一個模式以進行零電壓切換。 模式六(時間:匕): 如圖9所示,在此模式六下,第四開關心導通且其餘 開關不導通。且圖9中標示出在此模式下,電流路徑的走 向0 因為第四開關&之基體二極體導通,所以使第四開關 &導通時具有零電壓切換特性。當第一繞組“、第二繞級 L之漏感能量釋放完成時,兩繞組電流反向’分別對第— 開關&之寄生電容進行充電與使第二開關&之寄生電容 行放電。 模式七(時間ί6~ί。): 、如圖10所示,在此模式七下,第四開關&繼續導通而 於模式七期間内再將第二開^ &導通,且其餘開關不導通 〇 經由耦合電路7;的電流操作如前一模式,其他差別在 於: 當第一開關&之兩端電壓〜高於第一電容Q之電壓〜 時,第二開關&之基體二極體導通,此時使第二開關&導1 通具有零電流切換特性和同步整流功效。 *第一繞組b之電流k反向時’則回到模式一。 Β·昇壓方面: 古▲,閱圖11,依據該四開關&、&、&、&的切換,該 馬效能雙向轉換裝置會在七種模式下作動,以下圖12〜18 15 201021384 分別針對每一模式進行說明。且同樣,為了方便說明,模 式圖中的第一儲能單元直接以電池組表示,而該第二儲能 單元直接以輸出電容c"表示。 模式一(時間:: 參閱圖12,在此模式一下,該第一開關&和第三開關 &已導通一段時間而其餘開關不導通。且圖12中標示出在 此模式一下,電流路徑的走向。Mode 4 (time: r3~r4): As shown in Fig. 7, in this mode, the first switch & and the third switch & start to conduct and the remaining switches are not turned on. And the direction of the current path in this mode is indicated in Figure 7. Because in the former mode, the base diodes of the first switch & and the third switch & have been turned on, this mode starts to turn on the two openings A, & to become synchronous rectification with low conduction loss ( Synchr〇n〇us generation... state. When the leakage inductance energy of the second winding is released, the current through the third switch & and the third switch & zero electrical waste is turned on, so there is no switching loss. 'The second capacitor c2 is discharged to the second winding, induced to the first winding by magnetic path induction and releases energy to the battery. Let the duty cycle of the fourth switch & 4 be 4 , the transient time of the crossover, the target, 丨d & 〜 relationship is 4 and ^ conduction responsibility cycle ^ 4 + name = 1 (4) 13 201021384 The voltage of the first winding Vip is equal to the voltage of the battery &;, according to V 〇 lt-Second Balance, the voltage L of the first winding 模式 in mode one is VLP = ^x[(li/4)M] (5) Substituting the above formula into the equation (3), the first capacitor C is obtained; the voltage Vci is vci=^+vi/)=Fi/ii4=vsl (6) The first capacitor C/the voltage vcl is also Same as the first switch & cross voltage ~, using the above formula, the voltage % of the second capacitor q can be calculated as VC2 = V „ - VC1 = ^ + 1 / ^) (7) ❹ Equations (5) and (7) Substituting equation (2) can find the step-down ratio % is ^=VjVH=dJ{N^2) (8) Substituting the above formula into equation (6) can obtain ^sl=K/(JV + 2) = vS2 (9) When the turns ratio is fixed to N, the voltage across the first switch & and the second switch & VS1 is related to the voltage 4 of the output capacitor, regardless of the duty cycle 4 of the fourth switch & Therefore, a low-voltage low-conductance metal oxide semi-conducting field effect transistor (MOSFET) can be used as the switch. 〇 mode five (time: ί4~ί5): As shown in Fig. 8, in this mode, each switch It is not conductive, and the direction of the current path in this mode is marked in Figure 8. When the first switch Α and the third switch & are not conducting, because of the leakage inductance of the first winding k and the second winding core 4] There is still energy release from the heart, so the first winding current k flows through the base diode of the first switch & and the current 匕 of the second winding L passes through the second capacitor q and the fourth switch &; Based on 14 201021384 diodes continue to flow to the output capacitor, causing the fourth switch to zero voltage across the 'wait for the next mode for zero voltage switching. Mode six (time: 匕): as shown in Figure 9. It is shown that in this mode, the fourth switch core is turned on and the remaining switches are not turned on. And in Fig. 9, it is indicated that in this mode, the current path is shifted to 0 because the base diode of the fourth switch & is turned on, so that the fourth switch & turns on with zero voltage switching characteristics. When the first winding ", the leakage inductance energy release of the second winding L is completed, the two winding currents reverse" respectively charge the parasitic capacitance of the first switch & and discharge the parasitic capacitance of the second switch & Mode 7 (time ί6~ί.): As shown in Figure 10, in this mode, the fourth switch & continues to conduct and the second switch is turned on during the mode seven, and the remaining switches are not The current flowing through the coupling circuit 7 is as in the previous mode, and the other difference is: when the voltage across the first switch & is higher than the voltage of the first capacitor Q, the base of the second switch & The body is turned on, and at this time, the second switch & conduction has a zero current switching characteristic and a synchronous rectification function. * When the current k of the first winding b is reversed, it returns to mode 1. Β·boost: ancient ▲ According to the switching of the four switches &, &, &, &, the horse performance bidirectional conversion device will operate in seven modes, as shown in the following Figures 12~18 15 201021384 for each mode Description, and again, for convenience of explanation, mode The first energy storage unit is directly represented by a battery pack, and the second energy storage unit is directly represented by an output capacitor c" mode one (time:: see Fig. 12, in this mode, the first switch & The third switch & has been turned on for a while and the remaining switches are not turned on. And in Figure 12, the direction of the current path is indicated in this mode.
第開關&之電流h來自兩路徑,其一從電池流至第 繞組之電、流,該電流^包括第一繞址之感應電流和 激磁電流。另外-個電流從第—電容,經由第三開關^ 、第二繞組U第二電容C2進行充電,因此該第二電容 C2之電壓VC2表示為vC2=A^+vcl 〇〇) 模式二(時間:: 參閱圖13,在此模式二下,所有開關皆不導通。且 13中標示出在此模式二下’電流路徑的走向。The current h of the switch & is from two paths, one of which flows from the battery to the first winding, and the current includes the first sensed induced current and the exciting current. In addition, a current is charged from the first capacitor through the third switch ^, the second winding U and the second capacitor C2, so the voltage VC2 of the second capacitor C2 is expressed as vC2=A^+vcl 〇〇) mode 2 (time) :: Refer to Figure 13. In this mode 2, all switches are not conducting, and 13 is marked with the trend of the current path in this mode.
當第-開關和第三開關^剛不導通時,為確保第 、組Ls之電流續流路後’因 此弟—開關&之基體二極體 此時,第一繞組心的電流“口第二繞組l的電 ,對第—開關&之寄生電容進行充 的兩端電壓v快速上昇,n昧 開關 端電壓^ 第二_&之寄生電容 端電壓VSZ進行釋放,直到當 -電客;兩端電壓'等於 電谷G的電壓v〇時,本模式結束。 模式三(時間:Ί): 參閱圖14,在此模式三下,所有開關皆不導通。且 16 201021384 14中標示出在此模式三下,電流路徑的走向。 當第一開關&之兩端電壓〜高於第一 時,第二開…基體二極趙導通以提供電流路;= 一繞組I,之漏感釋放至第一電容q以進行充電。 ,則第一 電容ς之電壓 令名為第一開關之責任週期 vcl與電池之電壓關係為 vn=VL+vLP=vsx=VLl{\-dx). YS2 (11)When the first switch and the third switch ^ are not conducting, in order to ensure the current of the first group and the group Ls, the current body of the first winding core is at the same time. The voltage of the two windings l, the voltage v across the charging of the parasitic capacitance of the first switch &ample rises rapidly, and the voltage of the n昧 switch terminal ^the second _& the parasitic capacitance terminal voltage VSZ is released until the electric passenger When the voltage at both ends is equal to the voltage v〇 of the valley G, this mode ends. Mode 3 (Time: Ί): Refer to Figure 14, in this mode, all switches are not conducting. And 16 201021384 14 In this mode three, the direction of the current path. When the voltage at the two ends of the first switch & is higher than the first, the second opening ... the base diode is turned on to provide a current path; = the leakage inductance of a winding I Released to the first capacitor q for charging. The voltage of the first capacitor 令 causes the duty cycle vcl of the first switch to be related to the voltage of the battery as vn=VL+vLP=vsx=VLl{\-dx). YS2 (11)
同時’第二繞組L之電流L之轉向,使第三開關&之 寄生電容進行充電’而第四開關m生電容進行放電且 相互箝制,該一開關&、5^之最高跨壓等於 VS3=VS4 = VH-VCI (12) 模式四(時間:i3〜f4): 參閱圖15,在此模式四下,該第二開關^和第四_ &導通而其餘開關不導通。且圖15中標示出在此模式四下 ,電流路徑的走向。 當該二開關&及\之基體二極體已導通時,將該二開關 &、&導通以完成同步整流且降低導通損失。此時第二繞組 4之電壓在非極性點處為正,其值為 =^ = ^,/(1-^) (13) 電池之電壓G、第一繞組〇之電壓心、第二繞組l之 電壓心與第二電容C2之電壓vcz四項電壓串聯,以低電流型 式流至輸出電容CV,從方程式(1〇)、(11)及(13)可得輸出電 容Ch之電壓FH如下:.At the same time, 'the steering of the current L of the second winding L causes the parasitic capacitance of the third switch & to be charged' and the fourth switch m generates the capacitor for discharge and clamps each other. The highest crossover voltage of the switch & VS3=VS4 = VH-VCI (12) Mode 4 (Time: i3~f4): Referring to Figure 15, in this mode, the second switch ^ and the fourth _ & are turned on and the remaining switches are not turned on. And in Figure 15, the course of the current path is shown in this mode. When the two switches & and the base diode are turned on, the two switches &, & are turned on to complete synchronous rectification and reduce conduction loss. At this time, the voltage of the second winding 4 is positive at the non-polar point, and its value is =^ = ^, /(1-^) (13) The voltage of the battery G, the voltage center of the first winding 、, the second winding The voltage core is connected in series with the voltage vcz of the second capacitor C2, and flows to the output capacitor CV in a low current mode. The voltage FH of the output capacitor Ch can be obtained from the equations (1〇), (11) and (13) as follows: .
Vh=Vl+vlp+ vC2 + νω = (2 + N)Vl /(1 - dx) (14) 17 201021384 其昇屢比例為Vh=Vl+vlp+ vC2 + νω = (2 + N)Vl /(1 - dx) (14) 17 201021384
Gy2=VH/VL=(2 + N)/(i^di) 〇 5) 將方程式(11)代入方葙— 程式(15)可得第一開關&之跨壓 vsi=Vh/(N + 2) = vm (16) 從方程式(16)與方程式(9)可知輸出電容G之電壓匕及 ^ Μ ’該二開關& 4之兩端跨壓,與電池之電堡 彳主要控制之責任週期…無關,因此該二開_ 之兩端的最高電壓為定值。 ❹ 該二開關A、&兩端之跨壓等於匕”。,而第一電容q 之電壓VCI又等同於該二開關u2之電壓,因此該二開關 &、&之兩端的最高電遷為定值,並小於輸出電容c"。所 u四開關^& ϋ於降麗、昇壓兩種操作,皆有電 壓箝制效能。 當第—繞組〇之電流l等於第二繞組l之電流 進入下一模式。 模式五(時間:Ws): 參閱圖16,在此模式五下,該第二開目&和第四開關❹ 4繼續導通,但於此模式期間内切換成不導通 不導心且圖16中標示出在此模式五下,電流路徑的2 . 當第一繞組之電流L等於第二繞組心之電流f時, 儲存於兩繞組的能量經由第四開關心釋放至輪出電容C , 此時其餘開關Α ϋ均無電流穿越。 模式六(時間: 18 201021384 參閲圖 開關不導通 走向。 备第一開關&導通時,第一繞έ ,A ^ r 現、·^心之漏感4,限制第一 繞組4之電“的上昇斜率,域至第二繞組! 電流匕需要時間降至零,因為、、5$之 兩漏感電流相互箝制,自鈇來 成零電流切換特性,錢第四開M &之基體二極體導通^Gy2=VH/VL=(2 + N)/(i^di) 〇5) Substituting equation (11) into the square—the program (15) can obtain the first switch & cross voltage vsi=Vh/(N + 2) = vm (16) From equations (16) and (9), the voltage of the output capacitor G 匕 and ^ Μ 'the two ends of the two switches & 4 cross-voltage, and the responsibility of the battery's main control The period... is irrelevant, so the highest voltage at both ends of the two open_ is a fixed value.跨 The voltage across the two switches A, & is equal to 匕". The voltage VCI of the first capacitor q is equal to the voltage of the two switches u2, so the highest voltage of the two switches &, & Moved to a fixed value, and is smaller than the output capacitor c". The four switches ^& ϋ 降 降 、 、 、 升压 升压 升压 、 、 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降 降The current enters the next mode. Mode 5 (Time: Ws): Referring to Figure 16, in this mode 5, the second opening & and the fourth switch ❹ 4 continue to conduct, but switch to non-conduction during this mode. Not guiding and shown in Figure 16 in this mode, the current path is 2. When the current L of the first winding is equal to the current f of the second winding, the energy stored in the two windings is released via the fourth switching center to When the capacitor C is turned on, the other switches Α 无 have no current crossing. Mode 6 (Time: 18 201021384 Refer to the diagram switch for non-conduction. When the first switch & is turned on, the first winding, A ^ r is now · The leakage inductance of the heart 4 limits the rising slope of the electric current of the first winding 4, the domain to the ! Dagger winding current takes time to zero, since the two $ 5 ,, the leakage inductance current clamp each other, to be self-Fu zero current switching characteristic, the fourth on the money M & of the base body diode conduction ^
此時電流路徑㈣維持前—模式,但逐漸遞減中,因此第 -開關A導通時具柔性切換特性,有效減輕切換損失。 模式七(時間:,6〜(。): /閱圖18 ’在此模式七下,該第一開關&繼續導通和 第二開關&於此模式期間中切換成導通,而其餘開關不導 通。且圖18中標示出在此模式七下,電流路徑的走向。 當漏感能量釋放後,第二繞組。之電“轉向並流入 第-開關使第三開關&之寄生電容進行放電和第四開 關^之寄生電容進行充電,且相互箝制。當第三開關&之基 體極體導通時,將第三開關&導通,可推得第四開關& 之兩端電壓如方程式(12)心〜此時完成一切換週期,4 工作模式回到模式一 ^ 實驗結果: 如圖19〜23所示,當輸出電容C开之電壓4=200V與電 池之電壓Fi=24V,輸出功率為500W時,本發明之較佳實施 例·於降壓操作的各元件之電壓和電流波形。 如圖I9所示,為兩側繞組马與尽之電流波形,第一繞 19 201021384 組4之電流h幾乎為負向之充電電流,第二繞組4之電流k 則為雙向流動。 如圖20所不,為第一開關&於同步整流控制時之電壓 和電流波形,其第一開關&之電壓%約等於50V ,符合理 論分析。 如圖21所示,為第二開關&之電壓和電流波形,具有 同步整流與零電壓切換特性,其電壓箝制與第一開關&相 同。 如圖22和23所示,分別顯示第三開關&與第四開關& ❹ 之電壓和電流波形,該二開關&、&導通時具零電壓切換特 性,不導通時電壓箝制約在i 5〇v,符合理論計算。 如圖24〜28所示,當輸出電容之電壓~=2〇〇v與電 池之電壓C=24V,輸出功率為5〇〇w時,本發明之較佳實施 例於昇壓方面的各元件之電壓和電流波形。 如圖24所示,為兩繞組電流之波形,第一繞組。之電 流I全部為正向之電池放電電流,第二繞組。之電流L則 為雙向流動。 ⑩ 如圖25所不,為第一開關&之電壓和電流波形,其電 流波形接近方波,有較低導通損失,同時具有零電流切換 效果,其第一開關&之電壓vsl約等於50V。 一如圖26所示,為第二開關&之電壓和電流波形,具有 同步整流與零電麗切換特性,電壓籍制值與第一開關&相 同。 如圖27和圖28所示,分別顯示第三開關&與第四開關 20 201021384 \之電壓和電流波形,該一開關χ、&導通時具零電壓切換 與同步整流特性,不導通時電壓箝制約在l5〇V。 如圖29所示’最高的降壓轉換效率約在95%,最高的 昇壓轉換效率則約在96%。 综上所述’本發明之較佳實施例具有以下優點: (一)相較於習知的雙向轉換裝置(如圖1},不需要額外 的電感和多個二極體,因此體積可減小以利於攜帶,且成 本也可降低。At this time, the current path (4) maintains the pre-mode, but gradually decreases, so the first switch A has a flexible switching characteristic when turned on, effectively reducing the switching loss. Mode seven (time:, 6~(.): / read Figure 18' In this mode, the first switch & continue to conduct and the second switch & switch to conduction during this mode, while the remaining switches are not Turning on. And in Figure 18, the direction of the current path is shown in this mode. When the leakage inductance energy is released, the second winding of the electric "turns and flows into the first switch to discharge the parasitic capacitance of the third switch & Charging with the parasitic capacitance of the fourth switch ^ and clamping each other. When the base body of the third switch & is turned on, the third switch & is turned on, and the voltage across the fourth switch & (12) Heart~ At this time, a switching cycle is completed, and 4 working mode returns to mode. ^ Experimental result: As shown in Fig. 19~23, when the output capacitor C is turned on at a voltage of 4=200V and the battery voltage is Fi=24V, the output is When the power is 500 W, the preferred embodiment of the present invention is the voltage and current waveform of each component of the step-down operation. As shown in Fig. I9, the current waveforms of the windings on both sides are the first winding 19 201021384 group 4 The current h is almost a negative charging current, the second winding The current k of 4 is a bidirectional flow. As shown in Fig. 20, the voltage and current waveform of the first switch & during the synchronous rectification control, the voltage of the first switch & is approximately equal to 50V, which is in accordance with the theoretical analysis. Figure 21 shows the voltage and current waveforms of the second switch & with synchronous rectification and zero voltage switching characteristics, the voltage clamping is the same as the first switch & as shown in Figures 22 and 23, the third switch is respectively shown. & and the fourth switch & ❹ voltage and current waveform, the two switches &, & turn on zero voltage switching characteristics, when the voltage is not on, the voltage clamp is limited to i 5〇v, in line with theoretical calculations. As shown in FIG. 28, when the voltage of the output capacitor is ~=2〇〇v and the voltage of the battery is C=24V, and the output power is 5〇〇w, the voltage of each component in the boosting embodiment of the preferred embodiment of the present invention is Current waveform: As shown in Figure 24, the waveform of the two winding currents, the first winding, the current I is all positive battery discharge current, and the second winding. The current L is bidirectional flow. , for the voltage and current waveform of the first switch & The current waveform is close to the square wave, has a low conduction loss, and has a zero current switching effect, and the voltage of the first switch & the frequency vsl is approximately equal to 50 V. As shown in Fig. 26, the voltage and current waveform of the second switch & With synchronous rectification and zero-electric switching characteristics, the voltage value is the same as that of the first switch & As shown in Fig. 27 and Fig. 28, the voltage and current of the third switch & and the fourth switch 20 201021384 are respectively displayed. The waveform, the one switch χ, & when turned on with zero voltage switching and synchronous rectification characteristics, the voltage clamp is limited to l5 〇 V when not conducting. As shown in Figure 29, the highest buck conversion efficiency is about 95%, and the highest boost conversion efficiency is about 96%. In summary, the preferred embodiment of the present invention has the following advantages: (1) Compared with the conventional bidirectional conversion device (Fig. 1), no additional inductance and multiple diodes are required, so the volume can be reduced. Small to facilitate carrying, and the cost can be reduced.
(一)所有開關於昇壓與降壓兩個情況下,具有與 ZCS特性,而開關兩端的承受電壓固定到、於系統的最高 電壓’且不隨七刀換模式與責任週期的調I而改變,使開關 兩端的電壓充分抑制。 (―)以同步整流技術有效地降低開關之導通損失,且同 時具有高昇降壓比和高轉換效率。 (四)利用輕合電路[的電磁特性’嚴格劃分高、低壓 ’以充分使用元件規格。 准乂上所述者,僅為本發明之較佳實施例而已 能以此限定本發明音 田个 r m ^ ^ 實施之範圍,即大凡依本發明申請專利 範圍及發明說明内 f〜 M A .. 所乍之簡早的等效變化與修飾,皆仍 屬本發明專利涵蓋之範圍内。 【圖式簡單說明】 圖1是習4α _ , 雙向轉換裝置的電路圖; 圖2是本發明古^ 電路圖; 阿政能雙向轉換裝置之一較佳實施例的 21 201021384 圖3是該較佳實施例於降壓操作的時序圖; 圖4是該較佳實施例於降壓操作的電路圖, 式一下的操作; 圖5是該較佳實施例於降壓操作的電路圖, 式二下的操作; 圖6是該較佳實施例於降壓操作的電路圖, 式三下的操作; 圖7是該較佳實施例於降壓操作的電路圖, 式四下的操作; 囷8是該較佳實施例於降壓操作的電路圖, 式五下的操作; 圖9是該較佳實施例於降壓操作的電路圖, 式六下的操作; 圖10是該較佳實施例於降壓操作的電路圖 式七下的操作; 圖11是該較佳實施例於昇壓操作的時序圖; 圖12是該較佳實施例於昇壓操作的電路圖 式—下的操作; 圖13是該較佳實施例於昇壓.操作的電路圖 式二下的操作; 圖14是該較佳實施例於昇壓操作的電路圖 式三下的操作; 阖15是該較佳實施例於昇壓操作的電路圖 式四下的操作; 說明在模 說明在模 說明在模 說明在模 說明在模 說明在模 ’說明在模 ’說明在模 ’說明在模 ’說明在模 ’說明在模 201021384 圖16是該較佳實施例於昇壓操作的電路圖,說明在 式五下的操作; ° 模 圖17是該較佳實施例於昇壓操作的電路圖,說明在模 式六下的操作; 、 圖18是該較佳實施例於昇壓操作的電路圖,說明在模 式七下的操作; 、 圖19是該較佳實施例於降壓操作的實驗量測圖,說明 第一繞組和第二繞組之電流波形; 圖20是該較佳實施例於降壓操作的實驗量測圖,說明 該第一開關之電壓和電流波形; 圖21是該較佳實施例於降壓操作的實驗量測圖,說明 該第二開關之電壓和電流波形; 圖22是該較佳實施例於降壓操作的實驗量測圖,說明 該第三開關之電壓和電流波形; 圖23是該較佳實施例於降壓操作的實驗量測圖,說明 該第四開關之電壓和電流波形; 圖24是該較佳實施例於昇壓操作的實驗量測圖,說明 第一繞組和第二繞組之電流波形; 圖25是該較佳實施例於昇壓操作的實驗量測圖,說明 該第一開關之電壓和電流波形; 圖26是該較佳實施例於昇壓操作的實驗量測圖,說明 該第二開關之電壓和電流波形; 圖27是該較佳實施例於昇壓操作的實驗量測圖,說明 該第三開關之電壓和電流波形; 23 201021384 圖28是該較佳實施例於昇壓操作的實驗量測圖,說明 該第四開關之電壓和電流波形,及 圖29是該較佳實施例的實驗量測圖,說明在降壓操作 和昇壓操作的轉換效率。(1) All switches have the characteristics of ZCS in both boost and buck conditions, and the withstand voltage at both ends of the switch is fixed to the highest voltage of the system' and does not follow the seven-knife change mode and the duty cycle. Change to make the voltage across the switch fully suppressed. (―) The synchronous rectification technology effectively reduces the conduction loss of the switch, and at the same time has a high buck-boost ratio and high conversion efficiency. (4) Strictly dividing the high and low voltages by using the electromagnetic characteristics of the light-emitting circuit to fully utilize the component specifications. The above description is only for the preferred embodiment of the present invention, and can be used to limit the scope of the present invention to the rm ^ ^ implementation of the present invention, that is, the scope of the patent application and the description of the invention within the invention f ~ MA .. The short-term equivalent changes and modifications of the present invention are still within the scope of the present invention. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a circuit diagram of a conventional 4α _ , bidirectional conversion device; FIG. 2 is a circuit diagram of the present invention; a preferred embodiment of a political energy bidirectional conversion device 21 201021384 FIG. 3 is a preferred embodiment FIG. 4 is a circuit diagram of the buck operation of the preferred embodiment, and FIG. 5 is a circuit diagram of the buck operation of the preferred embodiment, and the operation of the second embodiment; 6 is a circuit diagram of the step-down operation of the preferred embodiment, and the operation of Equation 3; FIG. 7 is a circuit diagram of the step-down operation of the preferred embodiment, and operation of Equation 4; FIG. 8 is the preferred embodiment. FIG. 9 is a circuit diagram of the buck operation of the preferred embodiment, and operation of the sixth embodiment; FIG. 10 is a circuit diagram of the buck operation of the preferred embodiment. Figure 11 is a timing diagram of the boosting operation of the preferred embodiment; Figure 12 is a circuit diagram of the preferred embodiment of the boosting operation; Figure 13 is a preferred embodiment of the boosting operation Pressure. Operation of the circuit diagram 2 operation; Figure 14 is the comparison The preferred embodiment is the operation of the circuit diagram of the boosting operation; 阖15 is the operation of the circuit diagram of the preferred embodiment in the boosting operation; Illustrated in the modulo 'description in the modulo' description in the modulo 'description' in the modulo 'description' in the modulo' description in the modulo 201021384 Figure 16 is a circuit diagram of the preferred embodiment of the boosting operation, illustrating the operation under Equation 5; ° 17 is a circuit diagram of the boosting operation of the preferred embodiment, illustrating operation in mode six; and FIG. 18 is a circuit diagram of the boosting operation of the preferred embodiment, illustrating operation in mode seven; The preferred embodiment is an experimental measurement diagram of the step-down operation, illustrating the current waveforms of the first winding and the second winding; FIG. 20 is an experimental measurement diagram of the step-down operation of the preferred embodiment, illustrating the first switch FIG. 21 is an experimental measurement diagram of the step-down operation of the preferred embodiment, illustrating voltage and current waveforms of the second switch; FIG. 22 is an experimental amount of the step-down operation of the preferred embodiment. Mapping FIG. 23 is an experimental measurement diagram of the step-down operation of the preferred embodiment, illustrating voltage and current waveforms of the fourth switch; FIG. 24 is a boosting operation of the preferred embodiment. The experimental measurement chart illustrates the current waveforms of the first winding and the second winding; FIG. 25 is an experimental measurement diagram of the boosting operation of the preferred embodiment, illustrating the voltage and current waveforms of the first switch; The preferred embodiment is an experimental measurement diagram of the boosting operation, illustrating the voltage and current waveforms of the second switch; FIG. 27 is an experimental measurement diagram of the boosting operation of the preferred embodiment, illustrating the third switch Voltage and current waveforms; 23 201021384 FIG. 28 is an experimental measurement diagram of the boosting operation of the preferred embodiment, illustrating voltage and current waveforms of the fourth switch, and FIG. 29 is an experimental measurement diagram of the preferred embodiment. , indicating conversion efficiency in buck operation and boost operation.
24 201021384 【主要元件符號說明】24 201021384 [Main component symbol description]
Tr.....•…輛合電路Tr.....•...
Ch .......輸出電容 C1........-第一電容 C! ......第二電容 S1 •…第一開關 52 .........第二開關 53 .........第三開關 s4.........第四開關 LP.........第一繞組 Ls.........第二繞組Ch .......output capacitor C1........-first capacitor C!...second capacitor S1 •...first switch 52 ......... The second switch 53 ... the third switch s4 ... ... the fourth switch LP ... ... the first winding Ls. ..second winding
2525
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