TW201001869A - Method and apparatus with negative resistance in wireless power transfers - Google Patents
Method and apparatus with negative resistance in wireless power transfers Download PDFInfo
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- TW201001869A TW201001869A TW98115922A TW98115922A TW201001869A TW 201001869 A TW201001869 A TW 201001869A TW 98115922 A TW98115922 A TW 98115922A TW 98115922 A TW98115922 A TW 98115922A TW 201001869 A TW201001869 A TW 201001869A
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Classifications
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- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
- G06K7/00—Methods or arrangements for sensing record carriers, e.g. for reading patterns
- G06K7/0008—General problems related to the reading of electronic memory record carriers, independent of its reading method, e.g. power transfer
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- G—PHYSICS
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- G06K19/00—Record carriers for use with machines and with at least a part designed to carry digital markings
- G06K19/06—Record carriers for use with machines and with at least a part designed to carry digital markings characterised by the kind of the digital marking, e.g. shape, nature, code
- G06K19/067—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components
- G06K19/07—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components with integrated circuit chips
- G06K19/0701—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components with integrated circuit chips at least one of the integrated circuit chips comprising an arrangement for power management
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- G—PHYSICS
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- G06K19/06—Record carriers for use with machines and with at least a part designed to carry digital markings characterised by the kind of the digital marking, e.g. shape, nature, code
- G06K19/067—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components
- G06K19/07—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components with integrated circuit chips
- G06K19/0701—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components with integrated circuit chips at least one of the integrated circuit chips comprising an arrangement for power management
- G06K19/0715—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components with integrated circuit chips at least one of the integrated circuit chips comprising an arrangement for power management the arrangement including means to regulate power transfer to the integrated circuit
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- G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
- G06K19/00—Record carriers for use with machines and with at least a part designed to carry digital markings
- G06K19/06—Record carriers for use with machines and with at least a part designed to carry digital markings characterised by the kind of the digital marking, e.g. shape, nature, code
- G06K19/067—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components
- G06K19/07—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components with integrated circuit chips
- G06K19/0723—Record carriers with conductive marks, printed circuits or semiconductor circuit elements, e.g. credit or identity cards also with resonating or responding marks without active components with integrated circuit chips the record carrier comprising an arrangement for non-contact communication, e.g. wireless communication circuits on transponder cards, non-contact smart cards or RFIDs
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- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
- G06K7/00—Methods or arrangements for sensing record carriers, e.g. for reading patterns
- G06K7/10—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation
- G06K7/10009—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation sensing by radiation using wavelengths larger than 0.1 mm, e.g. radio-waves or microwaves
- G06K7/10158—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation sensing by radiation using wavelengths larger than 0.1 mm, e.g. radio-waves or microwaves methods and means used by the interrogation device for reliably powering the wireless record carriers using an electromagnetic interrogation field
- G06K7/10178—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation sensing by radiation using wavelengths larger than 0.1 mm, e.g. radio-waves or microwaves methods and means used by the interrogation device for reliably powering the wireless record carriers using an electromagnetic interrogation field including auxiliary means for focusing, repeating or boosting the electromagnetic interrogation field
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F38/00—Adaptations of transformers or inductances for specific applications or functions
- H01F38/14—Inductive couplings
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/12—Supports; Mounting means
- H01Q1/22—Supports; Mounting means by structural association with other equipment or articles
- H01Q1/2208—Supports; Mounting means by structural association with other equipment or articles associated with components used in interrogation type services, i.e. in systems for information exchange between an interrogator/reader and a tag/transponder, e.g. in Radio Frequency Identification [RFID] systems
- H01Q1/2225—Supports; Mounting means by structural association with other equipment or articles associated with components used in interrogation type services, i.e. in systems for information exchange between an interrogator/reader and a tag/transponder, e.g. in Radio Frequency Identification [RFID] systems used in active tags, i.e. provided with its own power source or in passive tags, i.e. deriving power from RF signal
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/36—Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith
- H01Q1/38—Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith formed by a conductive layer on an insulating support
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q7/00—Loop antennas with a substantially uniform current distribution around the loop and having a directional radiation pattern in a plane perpendicular to the plane of the loop
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- H02J5/005—
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/005—Mechanical details of housing or structure aiming to accommodate the power transfer means, e.g. mechanical integration of coils, antennas or transducers into emitting or receiving devices
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/10—Circuit arrangements or systems for wireless supply or distribution of electric power using inductive coupling
- H02J50/12—Circuit arrangements or systems for wireless supply or distribution of electric power using inductive coupling of the resonant type
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/20—Circuit arrangements or systems for wireless supply or distribution of electric power using microwaves or radio frequency waves
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/40—Circuit arrangements or systems for wireless supply or distribution of electric power using two or more transmitting or receiving devices
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/50—Circuit arrangements or systems for wireless supply or distribution of electric power using additional energy repeaters between transmitting devices and receiving devices
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/80—Circuit arrangements or systems for wireless supply or distribution of electric power involving the exchange of data, concerning supply or distribution of electric power, between transmitting devices and receiving devices
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/90—Circuit arrangements or systems for wireless supply or distribution of electric power involving detection or optimisation of position, e.g. alignment
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- H02J7/025—
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- H04B5/48—
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- H04B5/72—
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- H04B5/79—
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/50—Circuit arrangements or systems for wireless supply or distribution of electric power using additional energy repeaters between transmitting devices and receiving devices
- H02J50/502—Circuit arrangements or systems for wireless supply or distribution of electric power using additional energy repeaters between transmitting devices and receiving devices the energy repeater being integrated together with the emitter or the receiver
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/60—Circuit arrangements or systems for wireless supply or distribution of electric power responsive to the presence of foreign objects, e.g. detection of living beings
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J7/00—Circuit arrangements for charging or depolarising batteries or for supplying loads from batteries
- H02J7/00032—Circuit arrangements for charging or depolarising batteries or for supplying loads from batteries characterised by data exchange
- H02J7/00034—Charger exchanging data with an electronic device, i.e. telephone, whose internal battery is under charge
Description
201001869 六、發明說明: 依據35 U.S.C. §119之優先權主張 本申請案依據35 U.S.C. §119(e)主張以下各案的優先 權: 於2008年6月11日申請之題為 「REVERSE LINK SIGNALING VIA RECEIVE ANTENNA IMPEDANCE MODULATION」的美國臨時專利申請案61/060,735 ; 於2008年6月11日申請之題為「SIGNALING CHARGING IN WIRELESS POWER ENVIRONMENT」的美國臨時專利 申請案 61/060,738 ; 於2008年5月13日申請之題為「ADAPTIVE TUNING MECHANISM FOR WIRELESS POWER TRANSFER」的美 國臨時專利申請案61/053,008 ; 於2008年5月13日申請之題為「EFFICIENT POWER MANAGEMENT SCHEME FOR WIRELESS POWER CHARGING SYSTEMS」的美國臨時專利申請案61/053,010 ; 於2008年6月11曰申請之題為「TRANSMIT POWER CONTROL FOR A WIRELESS CHARGING SYSTEM」的美 國臨時專利申請案61/060,741 ; 於2008年5月13曰申請之題為 「REPEATERS FOR ENHANCEMENT OF WIRELESS POWER TRANSFER」的 美國臨時專利申請案61/053,000 ; 於2008年5月13日申請之題為「WIRELESS POWER TRANSFER FOR APPLIANCES AND EQUIPMENTS」的美 140360.doc 201001869 國臨時專利申請案61/053,004 ; 於2008年7月16曰申請之題為「WIRELESS POWER TRANSFER USING NEGATIVE RESISTANCE」的美國臨 時專利申請案61/081,332 ; 於2008年5月13日申請之題為「EMBEDDED RECEIVE ANTENNA FOR WIRELESS POWER TRANSFER」的美國 臨時專利申請案61/053,012 ;及 於2008年5月13日申請之題為「PLANAR LARGE AREA WIRELESS CHARGING SYSTEM」的美國臨時專利申請案 61/053,015。 【先前技術】 通常,每一電池供電器件(諸如,無線電子器件)需要自 有充電器及電力源,其通常為交流(AC)電力出線座。在許 多器件需要充電時,此種有線組態變得難以使用。 正開發在傳送器與耦合至待充電之電子器件的接收器之 間使用空中或無線電力傳送的方法。此等方法通常落在兩 個類別中。一個類別係基於介於傳送天線與待充電之器件 上的接收天線之間的平面波輻射(亦被稱作遠場輻射)的耦 合。接收天線收集所輻射之電力且對其進行整流以供對電 池充電。天線通常具有諧振長度以便改良耦合效率。此方 法的缺點為電力耦合隨著天線之間的距離増加而快速衰 退。因此,跨越合理距離(例如,小於丨公尺至2公尺)來充 電變為困難的。另外,由於傳送系統輻射平面波,所以若 未經由濾波來進行適當控制,則無意之輻射可干擾其他系 140360.doc 201001869 統。 「無線能量傳送技術之其他方法係基於在嵌人於(例如) 「充電」墊或表面中的傳送天線與嵌入於待充電之主機電 子器件中的接收天線(加上整流電路)之間的電感熬合。此 種方法具有以下缺點1,傳送天線與接收天線之間的間 隔必㈣常接近(例如’在千分之幾公尺内)。儘管此種方 法確貫具有對相同區域中之多個器件同時充電的能力,但 此區域通常㈣小且要求使时將料n件準確地定位至 特疋區域。因此’需要提供—種適應傳送天線及接收天 線之靈活放置及定向的無線充電配置。 在無線電力傳送之情況下,需要用於調整天線之操作特 性使之適合不同環境及最佳化電力傳輸特性的系統及方 法。 【實施方式】 意謂「充當實例、例子或 」之任何實施例不必被理 詞語「例示性」在本文中用以 例示」。本文中描述為「例示性 解為比其他實施例較佳或有利。 在下文結合附圖陳述之詳細描述意欲作為對本發明之例 不性實施例的描述且不意欲表示可實踐本發明的唯一實施 例。在此描述各處所使用之術語「例示性」意謂「充當實 例、例子或例示」且將不必祐裡奶& 1 # ^ 个乂掖理解為比其他例示性實施例 較佳或有利。該詳細描述包括較細節以便達成提供對本 發明之例示性實施例之澈底理解的目的。熟習此項技術者 將明瞭可在無此料定細節之情況下實踐本發明之例示性 140360.doc 201001869 實施例。在一些情、τ —月况下,以方塊圖形式來展 器件以便避免使本文所s相— …、夫、〜構及 楚。 見之例不性貫施例的新穎性不清 舌司§吾「热線電力I力士士丄 在本文中用以意謂在不使用實體 導體之情況下自傳送哭你、¥ 、電磁 送。。傳送至接收器的與電場、磁場、 磁場或其他者相關聯的任何形式之能量。 圖1說明根據本發明之久 _ 〜 各種例不性貫施例的無線傳送或 充電系統1 〇〇。將蚣人带丄 ^ f 將輸入電力102提供至傳送器1〇4以供 用於提供能量傳輸之鲈鉍+θ , ^ ^ ^ 輻射%106。一接收器108耦合至輻射 場106且產生一輪屮雷士 11n 输出電力110以供耦合至輸出電力110之 件(未圖示)儲存或消耗。傳。 ° _ 寻k态1〇4與接收态108相隔距離 ? 2。。在一例示性實施例中’根據相互譜振關係來組態傳 运益1〇4及接收器1()8’且在接收器1()8之諧振頻率與傳送 器刚之譜振頻率完全相同時, 106之「近場」中時’傳送器104與接收器108之間的傳送 損失為最小的。 ' 傳送β 104進-步包括一傳送天線114,傳送天線…係 用於提供-用於能量傳送之構件的傳送天線ιΐ4,且接收 器⑽進-步包括-接收天線118,接收天線u8係用於提 供-用於能量接收之構件。根據應用及將與之相關聯之器 件來對傳送天線及接收天線定尺寸。如所陳述,藉由將傳 送天線之近場中的大部分能量轉合至接收天線而非以電磁 波形式將多數能量傳播至遠場來進行有效能量傳輸。當在 此近場中時,可在傳送天線114與接收天線ιι8之間形成柄 140360.doc 201001869 合模式。在Λ線114及118四周此近場耗合可發生的區域在 本文中被稱作耦合模式區。 圖2展示無線電力傳輸系統之簡化示意圖。傳送器104包 括一振盈|§122、一功率放女51194¾ 、泰、山 刀手放大β 124及一濾波及匹配電路 126。该振盪器經組態以在所要頻率下產生,γ回應於調 整信號123來調整該所要頻率。可藉由功率放大器丨二以二 回應於控制信號125之放大量來放大振盪器信號。濾波及 匹配電路126可經包括以濾出諧波或其他不想要之頻率且 將傳送器104之阻抗與傳送天線U4匹配。 接收器可包括一匹配電路i 3 2及一整流及切換電路以產 生-DC電力輸出以對電池136(如圖2所示)充電或對耦合至 接,器之器件(未圖示)供電。匹配電路132可經包括以將接 收态108之阻抗與接收天線丨丨8匹配。 圖3所說明,例示性實施例中所使用之 「環形」天線丨-,其在…亦可被稱作「磁性I 線。環形天線可經組態以包括一空心或實體心(諸如,肥 粒鐵心)。空心環形天線可更好地容許放置於該心附近之 外來實體器件。此外,—空心環形天線允許其他組件放置 於心區域内。另外’ 形可更易於使得能夠將接收 天、桌118(圖2)放置於傳送天線114(圖2)之平面内,在該平 面内’傳运天線114(圖2)之耗合模式區可更強大。 如所陳述, 近似匹配期間 量傳輸。然而 在傳送器1 0 4與接收器刚之間的諸振匹配或 ,發生傳送器104與接收器1〇8之間的有效能 ,即使當傳送器】〇4與接收器1〇8之間的諧振 140360.doc 201001869 不匹配時,亦可在較低效率下傳輸能量。藉由將來自傳送 天線之近場的能量福合至駐於建立了此近場之鄰域中的接 收天線而非將能量自傳送天線傳播至自由空間中來進行能 量傳輸。 / 環形或磁性天線之魏頻㈣基於電叙電容。環形天 線中之電感通常僅為由該環形天線產生之電感,而通常將 電容添加至環形天線之電感以在所要諸振頻率下產生―今皆 振結構。作為-非限制性實例,可將電容器152及電容器白 15 4添加至該天線以建立_產生譜振信號} $ 6的譜振電路。 因此,對於較大直徑之環形天線而言,誘發諧振所需之· 容的大小隨著環形天線之直徑或電感增加而減小。此外, 隨著環形天線或磁性天線之直徑增加,近場之有效能量傳 輸區域增加。當然,其他諧振電路為可能的。作為另—非 限制性實例’一電容器可並行地放置於環形天線之兩個端 子之間。另外’―般熟習此項技術者將認識到,對於傳送 天線,锴振信號156可為環形天線150之輸入。 、、 本發明之心性實施例包括在處於彼此之近場中的兩個 天線之間搞合電力。如所陳述’近場為在天線四周磁場存 在但不可傳播或轄射遠離該天線的區域。其通常限制於接 天’泉之貝肢體積的體積。在本發明之例示性實施例 中’磁性型天線(諸如,單E環形天線及多區環形天線)用 於傳送(Tx)及接收(Rx)天線系統兩者,因為與電型天 =偶極)之電近場相比’磁性型天線之磁近場振幅傾 °同。此允許該對天線之間的潛在較高耗合。此外, 140360.doc 201001869 亦涵蓋「電」天線(例如,偶極及單極)或磁性天線與電天 線之組合。 Τχ天線可在足夠低之頻率下及在天線大小足夠大之情況 下操作,以在顯著大於由早先所提及之遠場及電感方=允 許之距離的距離下達成至小Rx天線之良好耦合(例如 dB)。若對Tx天線正確地定尺寸,則在主機器件上之天 線放置於受驅動Τχ環形天線之耦合模式區(亦即,在近場 中)内時,可達成高耦合程度(例如,_2至-4 dB)。 圖4展示指示傳送天線與接收天線之間的耦合強度的模 擬結果。曲線170及172分別指示傳送天線及接收天線之電 力接受的量測。換言之,在大負數之情況下,存在非常緊 饴之阻抗匹配,且多數電力被接受且因此由傳送天線輻 射。相反,小負數指示多數電力被自天線反射回,因為在 給定頻率下不存在緊密阻抗匹配。在圖4中,調諧傳送天 線及接收天線以使之具有約13 _ 5 6 MHz之諧振頻率。 曲線170說明在各個頻率處之自傳送天線傳送之電力 1。因此,在對應於約13.528 MHz及13.593 MHz的點la及 3a處,多數電力被反射且不傳送到傳送天線外。然而,在 對應於約13.56 MHz之點2a處,可看到,大量電力被接受 且傳送到天線外。 類似地,曲線172說明在各個頻率處由接收天線接收之 电力里。因此,在對應於約13 528 MHz& 13 593 MHz的點 lb及讣處,多數電力被反射且不經由接收天線傳送及進入 接收器中。然而,在對應於約13·56 MHz之點孔處,可看 140360.doc 201001869 到’大!電力被接收天線接受幻專送至接收器中。 曲線174指示在經由傳送天線自傳送器發送 ' 經由接收 天線接收且傳送至接收器後在接收器處接收到的電力量。 =此’在對應於㈣·528 MHz及13 593 MHzmUc -,發迗出傳送器外之電力的多數在接收器處為不可用 的’因為⑴傳送天線拒絕自傳送器發送至其之多數電力及 ⑺傳送天線與接收天線之間㈣合隨著頻㈣離譜振頻率 而效率降低。然而,在對應於約13·56 MHZ之點2。處,可 看到,自傳送器發送之大量電力在接收器處為可用的,指 示傳送天線與接收天線之間的高耦合程度。 圖5A及圖5B展示根據本發明之例示性實施例的用於傳 送天線及接收天線之環形天線的佈局。可以許多不同方式 :組悲%形天線’在廣泛各種大小下具有單個環或多個 環。另外,該等環可呈許多不同形狀,諸如(僅舉例頂 形、橢圓形、正方形及矩形。圖5八說明大正方形環形傳送 天線114S及小正方形環形接收天線118,小正方形環形接 收天線118與傳送天線1148放置於相同平面中且接近於傳
送天線U4S之中心。圖5B說明大圓形環形傳送天線114C 及小正方形環形接收天線11 8,,小正方形環形接收天線 Π8與傳送天線丨丨化放置於相同平面中且接近於傳送天線 114C之中心。正方形環形傳送天線1148具有邊長「&」,而 圓形環形傳送天線114C具有直徑Γφ」。對於正方形環形 而言,可展示存在等效圓形環形,其直徑可界定為: =孝α/;Γ 0 140360.doc 201001869 圖6展示指示與圖4A及圖4B中所說明之正方形及圓形傳 送天線的各種周圍有關的在傳送天線與接收天線之間的耦 合強度的楔擬結果。因此,曲線丨8〇展示在圓形環形傳送 天線114C之各種周圍大小下圓形環形傳送天線114C與接收 天線118之間的耦合強度。類似地,曲線182展示在正方形 環形傳送天線114S之各種等效周圍大小下正方形環形傳送 天線114S與接收天線118,之間的耦合強度。 圖7展示指示與圖5A及圖5B中所說明之正方形及圓形傳 送天線的各種表面積有關的在傳$天線與接收天線之間的 耦合強度的模擬結|。因&,曲線19〇展示在圓形環形傳 送天線114C之各種表面積下圓形環形傳送天線i 14匸與接收 天線118之間的耦合強度。類似地,曲線192展示在正方形 %形傳达天線114S之各種表面積下正方形環形傳送天線 114S與接收天線118,之間的耦合強度。 圖S展示接收天線相對於傳送天線之各種放置點以說明 在共2及同軸放置下之耦合強度。如本文所使用,「共 面」忍s胃傳送天線與接收天線具有大體上對準之平面(亦 即,具有指向大體上相同之方向的表面法線)且傳送天線 與接收天線之平面之間不具有距離(或具有小距離)。如本 文所使用,「同軸」意謂傳送天線與接收天線具有大體上 對準^平面(亦即,具有指向大體上相同之方向的表面法 線)且該兩個平面之間的距離並非細小的’且此外,傳送 天線與接收天線之表面法線大體上沿著相同向量延伸,或 該兩個法線排成梯形。 一 140360.doc -12- 201001869 作為貫例,點P1、P2、p3及p7為接收天線相對於傳送天 線之所有共面放置點。作為另—實例,點似…為接收天 '、、手於傳送天線之同軸放置點。下表展示在圖8所說明 之各個放置點(P1至P7)處的耦合強度(S21)及耦合效率(表 不為自傳送天線傳送之到達接收天線的電力的百分比)。 表1 位置 — 距平面的距離 (cm) S21效率 (%) iicrxDctm^" 對RX DC電力輸出)
效:可=广放置點〜及。3皆展示— P7亦為共面放置點’但在傳送環形天線外 叙八“放置點心具有高轉合效率,但很明顯存在—些 5且耦合模式區延伸超出傳送環形天線之周邊。 :置點p5與傳送天線同軸且展示相當大的耗合效率。放 r i. 而:之麵合效率不如共面放置點之輕合效率-樣高。缺 而,放置點P5之麵合效率為足夠高的, 置 之傳送天線與接收天線之間傳送大量電力。軸放置 2點P4處於傳送天線之周圍内但在傳送天線之平面上 午距離處之—位置中,其可被稱作偏移同轴玫置 140360.doc 201001869 (亦即,表面法線在大體上相同之方向上但處於不同位置 處)或偏移共面(亦即,表面法線在大體上相同之方向上_ 平面相對於彼此偏移)。自該表’可看到,在偏移距離為 2.5 cm%,放置點p4仍具有相對良好之耦合效率。 ,放置_說明在傳送天線之周圍外部且處於傳送天線之 平面上方相當大距離處的放置點。如可自該表看到,放置 點P7展示傳送天線與接收天線之間的很少叙合效率。 圖9展示指示在傳送天線與接收天線之間的各種距離下 同軸放置的福合強度的模擬結果。圖9之模擬係關於處於 同軸放置之正方形傳送天線及接收天線,其均具有約U 公尺之邊且處於1()顧2之傳送頻率下。可相,在距離小 於約0.5公尺時,搞合強度保持相當高且均一。 圖10為根據本發明之例示性實施例的傳送器的簡化方塊 圖。一傳送11200包括傳送電路2G2及—傳送天線2〇4。大 體上s傳;^電路2()2藉由提供—致使在傳送天線咖周圍產 生近場能量的振盪信號來將RF電力提供至傳送天線綱。 牛例而。傳送益2〇〇可在13 56則z ISM頻帶處操作。 —例不性傳达電路2〇2包括··一目定阻抗匹配電路鳩,固 疋I1抗匹配包路2〇6係用於將傳送電路之阻抗(例如, 5〇歐姆)匹配至傳送天線綱;及—低通濾波器(LpF卵, 低通遽波器(LPF)2〇8經組態以將譜波發射減少至防止麵合 至接收器1〇8(圖υ之器件的自干擾的位準。其他實施例可 包括不同遽波器拓撲(包括但不限於使特定頻率衰減而同 時使其他頻率通過的陷波遽波器)’且可包括一適應性阻 140360.doc -14- 201001869 抗匹配’其可基於 t ^ ^ , ... ^ ,、彳傳送量度(諸如,至天線之輸出 电刀4由功率放大考、、芬兩 進一牛七化 ^ <DC電流)來改變。傳送電路202 進步包括一經組態以驗私山, 功率放大器21〇。傳送 辰盈器212判定之RF信號的 代地’可包含整合 了匕3離散益件或電路’或替 RF雷*私山 〜成。—來自傳送天線204之例示性 RF電力輸出可為約25瓦。 傳送電路202進—牛勹化 ^ 夕匕括—處理器214’該處理器214用
於在特疋接收器之傳译贴e;w斗、 〇1, 得送^段(或工作循環)期間致能振盪器 212、用於調整該振堡 ^ 盈益之頻率,及用於調整用於實施通 ㈣…於經由相㈣件所附接之接收器與相鄰器件互 動)的輸出電力位準。 傳送電路2〇2可進-步包括:-負載感測電路216,負載 感測電路216係用於㈣在由傳送天線2 是否; 子在作用中之接收器。舉例而言,一負載感測電路 2161視流動至功率放大器21()之電流,其受在由傳送天線 204產生之近場附近的作用中之接收器的存在與否影響。 對功率放大益210上之負載改變的^貞測係由處理器214監 視八用於判疋是否致能振盪器212以傳送能量以與作用 中之接收器通信。 傳送天線204可貫施為天線條,其具有經選擇以使電阻 性損失保持為低的厚度、寬度及金屬類型。在習知實施 中,傳送八線204可通常經組態以與較大結構(諸如,桌 子、墊、燈或其他不便攜帶之組態)相關聯。因此,傳送 天線204通常將不需要「阻」以便為特定尺寸。傳送天線 140360.doc •15- 201001869 204之例示性實施可為「電學上小的」(亦即,波長之分數) 且經㈣以猎由使用電容器來界定譜振頻率來在較低之可 射貝率下諸振。在傳送天線2G4在直徑或邊長(若為正方形 環形)上相對於接收天線可為較墙如,〇.5G公尺)的例示 性應用中,傳送天線204將未必需要較大&數以獲得合理 電容。 圖11為根據本發明之實施例的接收器的方塊圖。—接收 器3〇0包括接收電路302及一接收天線304。接收器進一 步搞合至器件35〇以向其提供所接收之電力。請注意,將 接收器300說明為在器件35〇外部但可整合於器件別中。 通常,能量係無線地傳播至接收天線取且接著經由接收 電路3 02而耗合至器件350。 接收天線3 04經調譜以在與傳送天線2〇4(圖i 〇)相同之頻 率下或幾乎相同之頻率下譜振。接收天線3〇4可與傳送天 線204類似地^尺寸’或可基於相關聯器件350之尺寸來不 同地定尺寸。舉例而言,器件35〇可為具有小於傳送天線 204之直徑或長度的直徑或長度尺寸的攜帶型電子器件。 在此類實例中’接收天線304可實施為多®天線以便減少 調諧電容器(未圖示)之電容值且增加接收天線之阻抗。舉 例而言,接收天線304可放置於器件35〇之實質周圍四周: 以便最大化天線直徑及減少接收天線之環形姐(亦即,繞 組)之數目及繞組間電容。 接收電路302提供與接收天線3〇4的阻抗匹配。接收電路 3〇2包括用於將一所接收RF能量源轉換至供器件350使^之 140360.doc 16 201001869 充電電力的電力轉換電路306。電力轉換電路3〇6包括—汉开 至DC轉換器308且亦可包括一1)(:至1)(:轉換器31〇。虾至 DC轉換器308將接收天線3〇4處接收到之rf能量信號整流 至非父流電力,而DC至DC轉換器310將經整流之RF能量 信號轉換至可與器件350相容的能量勢(例如,電壓)。涵= 各種RF至DC轉換n,包括部分及全整流器、調節器 接器、倍加器以及線性及切換轉換器。 叫
收電路302可進—步包括用於將接收天線304連接至電 力轉換電路306或替代地用於將電力轉換電路撕斷開 換電路312。如下文更充分地解釋,將接收天線%植電力 轉換電路306斷開不僅暫時中止對器件别之充電, =^細(圖2)所「看到」之「負載」。如上文所揭示, 包括負載感測電路216,其制提供至傳送器功 於判心Γ之偏置電流的波動。因此,傳送器2〇°具有用 、a ③何時存在於傳送器之近場中的機制。 一:J個接收器300存在於傳送器之近場,時,可希望對 或夕個接收器之負载及卸載進 器能夠更有效地輕合至傳送器。亦可使其他接收 除至其他附近之 心純器以便消 載。接收器之此「卸载」在^ =附近傳送器:L之負 外,如下文更充分地解釋,由=冉為「覆盍」。此 偵測的卸載與負载之間的此切換 傳送器-的通信機制。另外二 =接收器腿 聯,該協定致能自接收器3 咖、該切換相關 得达态200的訊息發送。舉 140360.doc -J7- 201001869 例而言,切換速度可為約100微秒。 在一例示性實施例中’傳送器與接收器之間的通伊 益件感測及充電控制機制,而非習知雙向通信。, 傳送器使精料信號之通/_控來調整能量在以中 是否可用。接收器將此等能量變化解釋為來自傳送哭: 息。自接收器㈣’接收器使轉收天線之調譜及去譜來調 整正接受來自近場之多少電力。傳送器可侦測來自近場: 所使用電力的此差異且將此等變化解釋為來自接收器之訊 接收電路302可進—步包括用以識別接收到之能量波動 的發#號偵測器及信標電路314 ’該等能量波動可對應於 自傳送器至接收器之資訊性發信號。此外,發信號及^標 電路314亦可用則貞測減少之灯信號能量(亦即 號)的傳送及將該減少之職號能量整流成標稱電i = 於喚醒接收電路302内之未供電或耗盡電力之電路以便組 態接收電路3 0 2以進行無線充電。 接收電路302進一步包括用於協調本文所描述之接收器 3〇〇之處理(包括對本文所描述之切換電路的控制)的處 理器3!6。減器3()()之|蓋亦可在發生其他事件(包括偵 測到向器件350提供充電電力之外部有線充電源(例如,壁 式/USB電力))後發生。除了控制接收器之覆蓋外,處理器 3 16亦可監視彳$標電路3 14以判定一信標狀態及擷取自傳送 器發送之訊息。處理器316亦可調整〇(:至〇(:轉換器31〇以 獲得改良之效能。 140360.doc 201001869 、,圖12展示用於在傳送器與接收器之間進行訊息傳遞的傳 〉电路之部分的簡圖。在本發明之一些例示性實施例尹, 可在傳送器與接收器之間致能用於通信之構件。在圖12 功率放大器21 〇驅動傳送天線2〇4以產生輻射場。甴在 對於傳运天線2 〇 4為所要之頻率下振堡的載波信號⑽來驅 動 ic 口。 入斋。使用傳送調變信號224來控制功率放大 益2 1 〇之輪出。 傳路可藉由對功率放大器川使用一通/斷鍵控程序 來將^就發送至接收器。換言之,在岑證傳送調變信號 24日守功率放大器21G將在傳送天線⑽上驅動載波信號 220之頻率。在使傳送調變信號以失效時,功率放大器在 傳送天線204上將不驅動任何頻率。 垂圖12之傳送電路亦包括-負載感測電路216,負載感測 路216將電力供應至功率放大器21G且產生-接收信號 235輸^。在負載感測電路216中,跨電阻器&之電壓降形 成於Is ϊ虎226之電力盘jj. φ 也刀一功率放大器210之電源228之間。功 率放大器21 〇所消耗之雨士 & , 〇σ %力的任何變化將引起將由差動放 大器23 0放大的電壓降的變彳卜。木推、y _ 复化 备傳送天線與接收器(未展 不於圖12中)中之接收天線 σ 处%祸合杈式時,由功率玫大 器21 (h及取之電流量將改轡。始士 換s之,若傳送天線210不存 在耦合模式諧振,則驅動|S私 勃輻射場所需之電力將為第一量。 若存在搞合模式諧振’則功率 刀年放大益210所消耗之電力量 將上升,因為多數電力輕合至技& 1 & 至接收天線中。因此,如下文 所解釋,接收信號235可指干* 才日不耦合至傳送天線235之接忧天 140360.doc •19- 201001869 線的存在且亦可偵測自接收天線發送之信號。另外,接收 器電流汲取之變化可在傳送器之功率放大器電流没取中觀 測到,且如下文所解釋,此變化可用以偵測來自接收天線 之信號。 圖13A至圖13C展示在各種狀態下之接收電路的一部分 的簡圖以說明接收器與傳送器之間的訊息傳遞。圖13八至 圖13C皆展示相同電路元件’ +同之處為各個開關之狀 怨。接收天線304包括一特性電感L1,其驅動節點35〇。節 點350經由開關S1A選擇性地耦合至接地端。節點35〇亦經 由開關S1B選擇性地耦合至二極體⑴及整流器318。整流 器318將DC電力信號322供應至—接收器件(未圖示)以對該 接收器件供電、對電池充電,或其組合。二極體叫與電容 器C3及電阻器R1 —同耦合至傳送信號32〇 ,傳送信號 經濾波以移除諧波及不想要之頻率。因此,C3&R丨之 組合可在傳送信號320上產生一信號,其模仿由上文參看 圖12之傳送斋來論述的傳送調變信號224產生的傳送調 變〇 本迤明之例示性貫施例包括對接收器件之電流及取的調 變及對接收天線之阻抗的調變以實現反向鏈路發信號。參 看圖13 A及圖12兩者,在接收器件之電力汲取變化時,負 載感測電路216偵測傳送天線上之所得電力變化,且由此 等變化可產生接收信號235。 在圖13A至圖13C之實施例中,可藉由修改開關S1A及 S2A之狀態來改變經由傳送器之電流汲取。在圖l3A中, 140360.doc •20· 201001869 開關S1A及開關S2A均斷開而產生一「DC斷開狀態」且實 質上自傳送天線204移除負載。此減少傳送器所看到之電 流。 在圖13B中,開關S1A閉合且開關S2A斷開,從而產生接 收天線304之「DC短路狀態」。因此,可使用圖ub中之狀 態來增加在傳送器中所看到之電流。 在圖13C中,開關S1A斷開且開關S2A閉合而產生一正常 接收模式(在本文中亦被稱作「DC操作狀態」),其中電力 可由DC輸出信號322供應且可偵測到傳送信號32〇。在圖 13C所不之狀態下,接收器接收一正常電力量,因此消耗 比DC斷開狀態或DC短路狀態時多或少的來自傳送天線之 電力。 反向鏈路發信號可藉由DC操作狀態(圖13C)與DC短路狀 態(圖13B)之間的切換來實現。反向鏈路發信號亦可藉由 DC操作狀態(圖13C)與dc斷開狀態(圖13A)之間的切換來 實現。 圖14A至圖14C展示在各種狀態下之替代接收電路的一 部分的簡圖以說明接收器與傳送器之間的訊息傳遞。 圖14A至圖14C皆展示相同電路元件,+同之處為各個 開關之狀態。接收天線3〇4包括一特性電扣,特性電感 L1驅動節點350。節點mo經由電容器及開關仙來選擇 f也耦口至接地ir而。節點35〇亦經由電容器來叙合至 二極體D1及整流器318。二極體⑴與電容器^及電阻_ 一同耗合轉送信號32G’傳送信㈣〇經濾波以移除諸波 140360.doc -21 - 201001869 及不想要之頻率。因此,EH、C3& R1之組合可在傳送信號 32〇上產生一信號’其模仿由上文參看圖12之傳送器來論 述的傳送調變信號224產生的傳送調變。 整流器318連接至開關S2B,開關S2B串聯連接於電阻器 R2及接地端。整流器318亦連接至開關S3;^開關S3B之另 一側將D C電力信號3 2 2供應至一接收器件(未圖示)以對該 接收器件供電、對電池充電,或其組合。 在圖13A至圖l3C中,藉由經由開關S1B選擇性地將接收 天線304耦合至接地端來改變該接收天線之Dc阻抗。相對 照地,在圖!4A至圖14C之實施例中,可藉由修改開關 SIB、S2B及S3B之狀態以改變接收天線3〇42AC阻抗來修 改天線之阻抗以產生反向鏈路發信號。在圖14A至圖 中,可藉由電容器C2來調諧接收天線3〇4之諧振頻率。因 此,可藉由使用開關S1B經由電容器C1來選擇性地耦合接 收天線304(基本上將諧振電路改變至將在與傳送天線最佳 耦合的範圍外的不同頻率)來改變接收天線^々的八匚阻抗。 若接收天線304之諧振頻率接近於傳送天線之諧振頻率, 且接收天線304處於傳送天線之近場中,則可形成一耦合 模式’其中接收器可自輕射場1 〇6汲取顯著電力。 在圓14A中,開關S1B閉合,此將天線去諧且產生一 「AC覆蓋狀態」,該「Ac覆蓋狀態」基本上「覆蓋」接收 天線304使之免於被傳送天線2〇4偵測到,因為接收天線不 在傳送天線之頻率處諧振。由於接收天線將不處於耦合模 式下,所以開關S2B及S3B之狀態對於本論述而言並非特 140360.doc -22- 201001869 別重要。 在圖14Β中,開關S1B斷開,開關S2B閉合,且開關㈣ 斷開,從而產生接收天線304之「經調諧假負載狀態」。因 為開關S輯開,所以電容器〇不影響譜振電路,且與電 容器C2組合之接收天線304將處於可與傳送天線之譜振頻 率匹配的一譜振頻率下。開關S3B斷開與開關S2B閉合之 組合為整流器產生一相對高電流假負載,其將經由接收天 f κ 線304沒取更多電力,此可由傳送天線感測到。另外,可 债測到傳送信號320,因為接收天線處於自傳送天線接收 電力的狀態下。 在圖14C中,開關S1B斷開,開關S2B斷開,且開關㈣ 閉合,從而產生接收天線3〇4之「經調諧操作狀態」。因為 開關s1B斷開,所以電容器C1不影㈣振電路,且與電容 HC2組合之接收天線3〇4將處於可與傳送天線之諧振頻率 匹配的-諧振頻率下。開關S2B斷開與開關_閉合之組 合產生-正常操作狀態,其中電力可咖輸出信號職 應且可偵測到一傳送信號32〇。 反向鏈路發信號可藉由經㈣操作狀態(圖Μ)績覆 =狀態⑽UA)之間的切換來實現。反向鏈路發信號亦可 精由經调諧假負載狀態(圖14顺Ac覆蓋狀態⑷从)之間 的切換來貫現。反向鏈路發信號亦可藉由經調譜操作狀態 (圖叫與經調_載狀態(圖_之間的切換來實現, 因為接收咨所消紅夕·蕾士曰jJt /丄 以耗之電力1將存在差異,此可由傳送器中 之負載感測電路偵測到。 140360.doc 23· 201001869 將認識到,可使用開關 立覆蓋、產生反向鏈路發 當然,一般熟習此項技術者 S!B、S2B及S3B之其他組合來建 件°另外,可將開關S〗A及 路以建立其他可能組合以進 電力供應至接收器件。 如上文參看圖12所論述, 信號及將電力供應至接收器 S1B添加至圖14A至圖〗4C之電 行覆蓋、反向鏈路發信號及將 因此,在處於耦合模式下時 可將信號自傳送器發送至接收器。另彳,在處㈣合模式 下寺如上文參看圖13入至圖13C及圖〗4A至圖14C所論 述,可將fg號自接收器發送至傳送器。 圖15A至圖15C為說明用於使用上述發信號技術在傳送 器與接收器之間通信的訊息傳遞協定的時序圖。在一種例 =方法中’自傳送器至接收器的信號在本文中被稱作 *則向鏈路」且使用正常振盪與無振盪之間的簡單AM調 變。亦涵蓋其他調變技術。作為非限制性實例,信號存在 可解釋為1,且無信號存在可解釋為〇。 精由對接收器件所汲取之電力的調變來提供反向鏈路發 信號,該電力汲取可藉由傳送器中之負載感測電路债= 到。作為非限制性實例,較高電力狀態可解釋為丨,且較 低電力狀態可解釋為〇。請注意,傳送器必須開啟以便接 收器能夠執行反向鏈路發信號。另外,在前向鏈路發信號 期間接收器應不執行反向鏈路發信號。此外,若兩個接收 益件試圖同時執行反向鏈路發信號,則衝突可發生,此將 使傳送器難以(若非不可能)解碼適當反向鏈路信號。 在本文所描述之例示性實施例中,發信號類似於具有 140360.doc •24- 201001869 開始位元、-資料位元組、一同位位元及一停止位元的通 用非同步接收傳送(UART)串列通信協定。當然:,任何串 列通信協定可適於進行本文所描述的本發明之例示性實施 例。為便於描述且並非限^,將描述訊息料協定,使得 用於傳達每一位元組傳送之週期為約1〇 ms。 圖15A說明訊息傳遞協定之最簡單且最低電力的形式。 將在每個循環週期410(在例示性實施例中為約一秒)重複同 步脈衝420。作為非限制性實例,同步脈衝工作時間可為 ㈣Μ。在傳送器開啟時,具有至少—同步脈衝42〇之循 環週期41G可無限地重複。請注意,「同步脈衝」有些許用 岡不當,因為如由「白」脈衝42G,所說明,同步脈衝別可 為在脈衝週期期間的穩態頻率。同步脈衝微亦可包括藉 由上述之通/斷鍵控且如「陰影」脈衝42〇所說明在諧振頻 率處發信號。圖15A說明一最小電力狀態,其中譜振頻率 處之電力係在同步脈衝42〇期間供應的且傳送天線在電力 週期45〇期間為關閉的。允許所有接收器件在同步脈衝携 期間接收電力。 、圖⑽況明具有同步脈衝42〇、反向鏈路週期彻及電力 週期45G,之循環週期彻,其中傳送天線開啟且藉由在谐振 /率处振逢且不執行任何發信號來供應全電力。上時序圖 說明整個循環週期410,且下時序圖說明同步脈衝㈣及反 =鏈路週期430之分解圖。如下文所解釋,電力週期4训可 分成用於多個接收器件之不同週期。圖1SB展示用於三個 不同接收器件之三個電力區段pdl、pd2及pdn。 I40360.doc -25- 201001869 在前向鏈路發信號發生時,同步脈衝420可包括暖機週 期422、前向鏈路週期424及監聽週期426 〇監聽週期426可 包括一交遞週期427及一開始反向鏈路週期428。在同步脈 衝420期間,傳送器可在前向鏈路週期424(由「陰影」部 分指示)期間發出一前向鏈路訊息且在監聽週期426期間等 待來自接收器之答覆。在圖15B中,無接收器答覆,此由 監聽週期426期間之「白」部分指示。 圖1 5C類似於圖1 5B,不同在於如由「交叉影線」部分 所指示,接收器在開始反向鏈路週期428及反向鏈路週期 43 0期間答覆。在圖15中,在同步脈衝420期間,傳送器在 前向鏈路週期424期間發出一前向鏈路訊息且在監聽週期 426期間等待來自接收器之答覆。將要進行答覆之任何接 收器在交遞週期427結束之前、在開始反向鏈路週期428期 間及可能在反向鏈路週期430期間開始其答覆。 作為非限制性實例,表2展示可由傳送器及接收器發送 之一些可能訊息。 表2 TX命令 TX訊息 RX答覆 RX訊息 空 NDQ(新器件查詢) NDR(新器件回應) DD TT PP rr cc DQ(器件查詢) DD DS(器件狀態) DD TT PP cc ACK(根據先前DS確 認器件XX) SA(時槽指派) DD NN MM cc RES(重設所有電力時 槽指派) 140360.doc -26- 201001869 其中: 空=無傳送命令; DD=器件編號; TT=器件類型; ΡΡ =所請求電力; rr=一隨機數; cc=總和檢查碼; NN=時槽之開始;及 MM=時槽結束。 在解釋表1的程序中,空命令意謂在前向鏈路週期424期 間傳送器不發送訊息。在第2行中,由傳送器發送一新器 件查詢(NDQ)。若接收器件回應,則其用新器件回應 (NDR)以及器件編號(對於新器件而言其應為零,直至傳送 器指派器件編號為止)、電力請求、隨機數及接收答覆中 之所有資料位元的總和檢查碼來作出回應。 在第3行中,由傳送器發送一新器件查詢(DQ)以及一器 件編號。由該DQ定址之接收器件用一器件狀態(DS)以及 器件編號、器件類型、所請求電力量及接收答覆中之所有 資料位元的總和檢查碼來進行答覆。 在第4行中,傳送器將一確認(ACK)發出至對先前DQ作 答覆之接收器。無接收器對ACK作出回應。 在第5行中,傳送器發出時槽指派(SA)以及器件編號、 電力週期450'内之開始時間、電力週期450’内之結束時間 及接收答覆中之所有資料位元的總和檢查碼。無接收器對 140360.doc •27· 201001869 SA作出回應。 在第6行中’傳送器發出一指示所有接收器應停止使用 其所分配之時槽的重設(RES)。無接收器對RES作出回 應。 當然’ 一般熟習此項技術者將認識到’該等命令及回應 為例示性的,且涵蓋於本發明之範疇内的各種實施例可使 用此等命令及回應之變體,且在本發明之範疇内,可想出 額外命令及回應。 為了進一步說明通信如何發生,將論述五種不同情況。 在第一種情況中,最初無接收器件在傳送器之耦合模式區 内,且一個接收器件進入該耦合模式區。在無器件存在於 該耦合模式區中時,傳送器將保持在低電力狀態下(如圖 15A所說明)且在每個循環週期41〇重複同步脈衝42〇。同步 脈衝420在前向鏈路週期424期間將包括—NDq,且傳送器 在監聽週期426期間將監聽答覆。若未接收到答覆,則傳 送器停機,直至用於下一個循環週期41〇之同步脈衝42〇的 時間為止。 在將新接收器件引入至該耦合模式區時,該接收器件最 初開啟且監聽一同步脈衝420。該新接收器件可將同步脈 衝420用於電力,但在電力週期45〇,期間應進入一覆蓋或非 電力接收模式(本文中被稱作「下匯流排」)。另外,該新 接收器件監聽傳送命令且忽略除了 NDQ外之所有傳送命 令。在一新接收器件接收到NDQ時,其在交遞週期427、 開始反向鏈路週期428及可能在反向鏈路週期43〇期間保持 140360.doc -28- 201001869 2啟。在前向鏈路週期424之後且在交遞週期427結束之 前’匕接收器件用馳、為零之器件ID(新器件ID將由傳送 器指派)、電力量請求、隨機數及總和檢查碼來作出回 應。新接收器件接著在電力週期45(),期間下匯流排。 若傳送器正確地接收到該職,則其在下—個同步脈衝 ㈣上用-用於新接收器件之時槽指派(s A)來作出回應。 /匕括用於新接收器件之器件ID、開始時間、結束時 門及、和;^查碼。用於此SA之開始時間及結束時間將為 零,指示新接收器件在電力週期45〇,期間之任何時間週期 内不應上匯流排。在新接收器件可上匯流排時,新接收器 牛將接收浪特疋電力區段pdn的具有實際開始時間及 結束時間的隨後SA。若新接收器件未接收到一適當總和檢 查碼三則其保持於新器件模式且再次回應於一卿。 在第二種情況中,無接收器件在傳送器之福合模式區 内且個以上接收器件進入該雜合模式區。在此模式 I ’在將兩個新接㈣件引人至料合模式㈣,其最初 :直在匯流排上。該等新接收器件可將同步脈衝420用於 包力’但-旦已接收到同步脈衝,便應在電力週期彻I 期間下匯流排。另外,該等新接收器件監聽傳送命令且忽 =除了 NDQ外之所有傳送命令。在新接收器件接收仙〇 T其在父遞週期427、開始反向鏈路週期428及可能在反 向鏈路週期43G期間保持開啟。在前向鏈路週期似之後且 在交遞週期427結束之前,接收器件用職、為零之器件 叫新器件卿由傳送器指派)、電力量請求、隨機數及總 140360.doc -29- 201001869 和檢查碼來作出回應。 。=而’由於兩個或兩個以上接收器件同時進行回應,且 可月b具有不同隨機數及總和檢查碼,所以傳送器所接收到 之訊息將被混淆,且傳送器中之總和檢查碼將不精確。結 果,傳送器將不在隨後同步脈衝420上發出SA。 田在NDR後未出現一緊鄰从時,該等接收器件中之每一 者在用NDR作出回應之前等待隨機數目之隨後仙心舉例 而言’兩個器件均回應於第-個NDQ,所以無隨後_ ,。益件1決定在回應於另一個NDQ之前等待四個NDQ。 叩件2决疋在回應於另—個ndq之前等待兩個仙〇。結 果’在傳送器發出下一個NDQ時,無器件用職來作出回 應。在傳达器發出下一個NDQ時,僅器件2用聰來作出 口應’傳送S成功地接收到該NDR且發出_用於哭件2之 ::。在下-個NDQ時,器件2不回應,因為其不再為新器 ’且$件1不回應’因為其隨機等待週期尚未過去。在 傳送器發出下—個NDQ時,僅器们用職來作出回岸, 傳运器成功地接收㈣NDR且發出—用於器件丨之从。 在第三種情況中,至少—接收器件處於福合模式區中, 且一新接收器件進入兮知人y 4- r-. °亥耦合杈式區。在此模式下,將該新 接收器件引入至該耦合模 . ^亥新 镆式&且其取初一直在匯流排上。 _收器件可將同步脈衝420用於電力,但—旦已接收到 同步脈衝420 ’便應在電力週期45q,期間下匯流排。另外, ㈣收器件監聽傳送命令且㈣除了 NDQ外之所有傳 令。週期性地,傳详哭脸& , 辱达益將發出一 NDQ以查看是否有任何新 I40360.doc -30- 201001869 器件已進人該叙合模式區。新器件將接著用贿來答覆。 在隨後同步脈衝420時,傳送器將發m新器件之不 指派電力時槽的从。傳送器接著重新計算該耗合模式區中 之所:器件的電力分配且為每一器件產生新从,所以不存 在重叠電力區段Pdn。在每—器件接收到其新从後,其僅 在其新Pdn期間開始上匯流排。 、在第四種情況下,正常電力輸送操作繼續,無接收器件 進入或離開麵合模式區。在此種情況期間,傳送器將週期 性㈣由-器件查詢(DQ)來探查(ping)每一器件。所查詢 之·«件用器件狀態(DS)來作出回應。若該Ds指示一不同 電力請f,則傳送器可將電力分配重新分配給㈣合模式 品中之每器件。如上文關於第三種情況來解釋的,傳送 盗亦將週期性地發出Ndq。 、 「在第五種情況中’將一器件自該耦合模式區移除。此 、二私除」狀態可為在實體上自該耦合模式區移除該器 件:該器件停機,或該器件覆蓋自身(可能因為其不再需 要電力)。如早先所規定,傳送器週期性地發出—用於該 輕合模式區中之所有器件的D Q。^至-特定器件之兩個 ,續DQ:傳回—有效DS,_送器將該器件自其所分配 器件之β單移除且將電力週期450,重新分配給剩餘器件。 傳达益亦將給缺失之器件指派零時間之電力分配,以防其 Α句傳送部仍進行接收。若錯誤地將一器件自電力分配 '、、丨其了藉由用一適當NDR回應於NDQ來重新獲得電 力分配。 Λ 140360.doc •31 · 201001869 表3說明一非限制性命令及答覆序列以說明通信協定如 何操作。 表3
命令 描述 答覆 描述 註釋 DQ1 查詢器件1 DS1 IFFcc 器件1為類型 1,想要最大 電力 電池電量低之蜂 式電話 DQ2 查詢器件2 DS 2 1 84 cc 器件2為類型 3,想要減少 電力時槽 具有幾乎充滿電 之電池的PDA SA2 84 FF 時槽指派器 件2 減少器件2之電力 時槽(首先減少, 接著增加) SA1 00 83 時槽指派器 件1 增加器件1之電力 時才曹 NDQ 新器件查詢 NDR 00 04 FF rr cc 發現新器件 電池電量低、電 力最大之滑鼠 SA3 00 00 時槽指派器 件3 在NDQ後立即答 覆意謂其係用於 新器件。器件ID 為3。初始電力時 槽為0。 SA 1 00 40 時槽指派器 件1 給器件1重新指派 1/4電力 SA2 41 80 時槽指派器 件2 給器件2重新指派 1/4電力 SA3 81FF 時槽指派器 件2 給器件3重新指派 1/4電力 NDQ 新器件查詢 無答覆,所以没 發現新器件 空 DQ1 DQ2 DQ3 NDQ 140360.doc •32- 201001869 庄思’用於新器件之第_時槽指派不分配時槽。认每一 現存器件分配-新的非重疊時槽,接著最後給新器:分配 一時槽以用於接收電力。 在一例示性實施例中’―無線充電器件可向使用者領示 一可視信號(諸如,燈光),指示其已成功地進入充電區且 使其自身向本端傳送器註冊。此將給予使用者肯定反饋, 即’器件確實準備好充電。 、 在本發明之其他例示性實施例中,接收器及傳送器可在 如圖I示之獨立通信頻道i i 9(例如,藍芽、、蜂巢 式’寺等)上通信。在一獨立通信頻道之情況下,循環週 期無需包括任何通信週期且整個時間可專用於電力週期 柳。傳送器仍可糾槽分配給每—接收Μ(經由該獨立 通信頻這來通信)且每-接收器件僅在其所分配之電力區 段Pdn期間上匯流排。 ,上述之經時間多工的電力分配可為用於將電力供應給傳 达益之_合模式區内之多個接收器件的最有效方法。铁 而’在本發明之其他實施例中,可使用其他電力分配方 案。 圖16A至圖16D為說明用於在傳送器與—或多個接從器 之間傳送電力的信標電力模式的簡化方塊圖。圖Μ說明 ,信標耗合模式區51〇中不存在接收器件時具有低電力 j標」信號525的傳送器52Q。作為非限制性實例,信標 ^虎525可諸如在〜1〇至〜2〇 rf之範圍中。當一待充電 之器件放置於該耦合模式區中時,此信號可足以將初始電 140360.doc -33- 201001869 力提供給該器件。 圖16B說明放置於傳送信標信號525之傳送器52〇的信標 耦合模式區510内之接收器件53〇。若接收器件53〇開啟且 與傳送器形成一耦合,則其將產生一反向鏈路耦合, 其貫際上只是接收器接受來自信標信號525之電力。此額 外電力可由傳送器之負載感測電路216(圖12)感測到。結 果,傳送器可進入高電力模式。 圖16CI兒明傳送器520產生高電力信號525,,導致高電力 耦合模式區510,。只要接收器件53〇正接受電力且結果產生 反向鏈路叙合535,傳送器便將保持於高電力狀態。雖然 僅說明一個接收器件530,但耦合模式區510中可存在多個 接收器件530。若存在多個接收器件53〇,則其將基於每一 f收器件530耦合之良好程度來共用由傳送器傳送之電力 量。舉例而言,如上文參看圖8及圖9來解釋的,對於每一 接收器件530而言,搞合效率可取決於器件放置於稱合模 式區510内之何處而為不同的。 圖1 6 D說明即使在接收器件5 3 〇處於信標搞合模式區别 中時仍產生信標信號525的傳送器52〇。此狀態可發生於接 收σ。件53(HT機時,或器件覆蓋其自身時(可能因為其不再 需要電力)。 如R時間多卫模式—樣,接收器及傳送器可在獨立通信 頻道(例如’藍芽、zigbee等等)上通信。在―獨立通信頻 道之情況下’傳送器可基於輕合模式區51〇中之接收器件 的數目及其各別電力要求來判定何時在信標模式與高電力 I40360.doc -34· 201001869 模式之間切換或產生多個電力位準。 本發明之例示性實施例包括在兩個天線之間的近場電力 傳輸中經由將額外天線引人絲合天線之㈣中來增強相 對大傳送天線與小接收天線之間的輕合,該等額外天線將 充當轉發器且將增強自傳送天線朝著接收天線之電力流。 在-例示性實施例中,使_合至系統中之傳送天線及 接收天線的-或多個另外天線。此等另外天線包含轉發器 天線(諸如,主動或被動天線)。被動天線可僅包括天線環 形及用於㈣天線之諧振頻率的電容性元件。♦了天線環 形及一或多個調諧電容器外,—主動元件可包括用於增加 一經轉發近場輻射之強度的放大器。 電力傳輸系統中之傳送天線與轉發器天線之組合可經最 佳化’使得基於諸如終端貞冑、調魅件、魏頻率及轉 發器天線相對於傳送天線之放置的因素來增強至非常小接 收天線的電力耗合。 一單一傳送天線展示一有限近場耦合模式區。因此,經 由在傳达天線之近場耦合模式區中之接收器來充電的器件 之使用者可需要一相當大之使用者存取空間,此將為代價 過於高以至少不方便的。此外,該輕合模式區可隨著接 收天線遠離傳送天線而快速地減小。 一轉發器天線可重聚焦及重塑來自—傳送天線之福合模 式區以在轉發器天線周圍產生一第二耦合模式區,其可更 適於將能量耦合至一接收天線。 圖17八說明大傳送天線710A,及與傳送天線71〇A共面地 140360.doc -35- 201001869 安置且安置於傳送天線710A之周邊内的較小轉發器天線 72〇A。傳送天線710A及轉發器天線72〇A均形成於桌74〇 上。包括一接收天線730A之一器件放置於轉發器天線 720A之周邊内。在非常大天線之情況下,傳送天線7i〇A 中心附近可存在相對弱之轉合模式區的區域。在試_合 至非常小接收天線730A之情況下,此弱區之存在可尤其顯
而易見的。與傳送天線710A共面放置但具有較小大小之轉 發器天線720A可能夠將由傳送天線71〇A 區重聚焦成轉發器天線蘭周圍的更小且更強二= 合杈式區。結果’一相對強之經轉發近場輻射可用於接收 天線73 0A。 圖㈣說明傳送天線7剛,及相對於傳送天線侧同4 放置之較大轉發器天線72〇B。包括一接收天線7则之_ 器件放置於轉發器天線7細之周邊内。傳送天線胸月 成於燈罩742下邊緣周圍四周,而轉發器天線胸安置方 桌740上。應記得在同軸放置之情況下,近場輕射可相费 於距天線之平面的距離增加而相對快速地減小。結果,相 對於傳送天線71〇B放置成同轴放置的小接收天線7卿可 處於㈣合模式區中。然而,與傳送天線_同轴地放置 之大轉發器天線膽可能夠將傳送天線鳩之耗合模式 區重塑成在轉發器天線四周之不同地方中的另 Γ式區。結果,—相對強之_發近料时詩與轉^ 态天線72〇B共面放置之接收天線730B。 圖18A說明大傳送天線_連同三個較小轉發器天線 140360.doc •36- 201001869 72〇C ’该二個較小轉發器天線72〇匸與傳送天線7i〇c共面 地安置且安置於傳送天線710C之周邊内。傳送天線710C 及轉叙态天線720C形成於桌740上。包括接收天線730C之 各種器件放置於傳送天線7丨〇c及轉發器天線72〇c内之各 個位置處。如同圖17A所說明之實施例一樣,圖18A之實 鉍例可忐夠將由傳送天線71〇c產生之耦合模式區重聚焦成 在轉發器天線720C中之每一者四周的更小且更強之經轉發 耦合模式區。結果,一相對強之經轉發近場輻射可用於接 收天線73OC °接收天線中之某些放置於任何轉發器天線 720C外部。應記得耦合模式區可稍微延伸出天線之周邊 外。因此,接收天線730C可能狗接收來自傳送天線 以及任何附近轉發器天線720C之近場輻射的電力。結果, 放置於任何轉發器天線72叱外部之接收天線仍可能夠接收 來自傳送天線710C以及任何附近轉發器天線72〇c之近場 輕射的電力。 圖18B說明大傳送天線710〇,及相對於傳送天線71〇〇有 偏移地同軸放置及有偏移地共面放置的較小轉發器天線 720D。包括-接收天線頂〇之_器件放置於轉發器天線 72〇D中之一者之周邊内。作為非限制性實例,傳送天線 7iOD可安置於天花板746上,而轉發器天線72〇1)可安置於 桌740上。如同圖17B之實施例一樣,處於偏移同軸放置之 轉發器天線7 2 0 D可能夠將來自傳送器天線7丨〇 d之近場輻 射重塑及增強成轉發器天線720D四周之經轉發近場輻射。胃 結果,一相對強之經轉發近場輻射可用於與轉發器天線 140360.doc -37- 201001869 720D共面放置之接收天線730D。 雖然各種傳送天線及轉發器天線已大體上展示為在表面 上,但此等天線亦可安置於表面下(例如,在桌下、在地 板下、在牆壁後面,或在天花板後面)、或在表面内(例 如,桌面、牆壁、地板或天花板)。 圖19展示指示傳送天線、轉發器天線及接收天線之間的 搞合強度的模擬結果。調譜傳送天線、轉發器天線及接收 天線以使之具有約1 3 _ 5 6 MHz之譜振頻率。 曲線810說明在各個頻率處在饋入至傳送天線之總電力 中自傳送天線傳送之電力量的量測。類似地,曲線82〇說 明在各個頻率處在接收H天線之料附近可用的總電力中 由接收天線經由轉發器天線接收到之電力量的量測。最 後,曲線830說明在各個頻率處在傳送天線與接收天線之 間經由轉發器天線實際耦合且進入接收天線中的電力量。 在對應於約13.56 MHz的曲線830之峰值處,可看到,自 傳送器發送之大量電力在接收器處為可料,指示傳送天 線、轉發器天線及接收天線之組合之間的高柄合程度。 圖篇展示指示在不具有轉發器天線之情況下在傳送天 線與相對於傳送天線安置成同軸放置的接收天線之間的搞 合強度的模擬結果。調譜傳送天線及接收天線以使之具有 約職Hz之諧振頻率。在此模財,傳送天線在一邊上為 、勺1.3 A尺,且接收天線為在一邊上為約毫米之多環形 天線。接收天線放置於距傳送天線之平面約2公尺處。曲 線81〇A說明在各個頻率處在饋人至傳送天線之端子的總電 140360.doc •38· 201001869 力中自傳送天線傳送之電力量的量測。類似地,曲線刚 說月在口個頻率處在接收天線之端子附近可用的總電力中 由接收天、.泉接收到之電力量的量測。最後,曲線㈣a說明 在各個頻率處在傳送天線與接收天線之間實際搞合的電力 量。 圖20B展示才曰不在轉發器天線包括於系、统中時圖的 傳送天線與接收天線之間的耦合強度的模擬結果。傳送天 線及接收天線具有與圖2从中之大小及放置相同的大小及 « °轉發在_邊上為約28 em且與接收天線共面 地放置(亦即,距傳送天線之平面約〇.丨公尺)。在圖2〇b 中,曲線81〇B說明在各個頻率處在饋入至傳送天線之端子 的、、.i包力中自傳送天線傳送之電力量的量測。曲線Μ⑽說 明在各個冑率處在接收天線之端子附近可用的總電力中由 接收天線經由轉發器天線接收到之電力量。最後,曲線 830B說明在各個頻率處在傳送天線與接收天線之間經由轉 發益天線貫際耦合且進入接收天線中的電力量。 虽將來自圖20A及圖20B之耦合電力(830A及830B)進行 比較時,可看到,在不具有轉發器天線之情況下,耦合電 力830A峰值為約-36 dB。而在具有轉發器天線之情況下, 耦合電力830B峰值為約_5 dB。因此,在諧振頻率附近, 可用於接收天線之電力量歸因於對轉發器天線之包括而顯 著增加。 本發明之例示性實施例包括在所涉及天線(諸如,傳送 天、、泉接收天線及轉發裔天線)中之一或多者之電路尹產 140360.doc -39· 201001869 生負電阻。此負電阻可減少 容器之等效串聯電阻(ESR) 負電阻反相器。 天線導體之正電阻(損失)及電 ’在例示性實施例中,使用一 在例不性貫施例中,將—負電阻施加至經耦合之傳送天 線、接收:線、轉發器天線或其組合,其在彼此之近場中 操作以將電力自遠接$楂工^ 運接至傳达天収源無線地傳輸至連接至 接收天線之負載。6番— & 戰負電阻之作用為補償天線之 調諧電容器之有限0。A彻__ ω _ 兮豆楨失及 ’限Q。在例不性實施例中,天線 在天線電路中之招生古品益 .. 失方面特性較接近於理想天線及電容 裔’ ¥致無線電力傳輸之較高總效率。儘管產生一負勺且 之電力’但對總拓撲之適當設計將改良系統之端 在例讀實施财,對所達成效率之改良愈天 線配條件相當,此亦導致較高效率。可藉由絲 几件來執仃此使用負電阻之匹配程序。 圖21說明構成負電阻產生器910之具有正及 示性運算放大器電路。貞電阻產生m及負反饋的例 二、一連接於運算放大器輸出與負輸入之間的第一反 饋電阻器922、一連接於運管 乐汉 第_ W ㈣於^放大讀出與正輪人之間的 弟-反饋電阻_,及,至正輸入的 920。負電阻產生器91〇建立且 山 屯阻口口 子929之門&耸1自+ 〃有在弟一碥子928與第二端 之間的專效負電阻930的電路。 其可被展示:
/ =— Μ 1^2 ) U/J
V 140360.doc -40· 201001869 條件為-β£5α,<ν<βΕία, 其中Rf為第一反饋電阻器922、R!為第二反饋電阻器 924,且R2為輸入電阻器926 ;且 其中±Esat為關於將運算放大器驅動至飽和區的一給定範 圍之差動輸入的該運算放大器之輸出電壓。 此電路之輸入電阻基於其IV特性而等效於一負電阻。 由-RN用符號展示之負電阻可置於天線電路中以抵銷來自 天線電路之其他組件的電阻。 圖22A至圖22C分別說明包括用於傳送天線、轉發器天 線及接收器天線之負電阻的例示性天線電路。在圖22A 中,一無線電力傳送電路940包括與一電容元件944耦合之 一傳送天線942,該電容元件944具有一等效串聯電阻 (ESR)946。該電容元件串聯耦合於負電阻產生器910A。一 信號產生器950耦合於傳送天線942與負電阻產生器910A之 間。該信號產生器提供一振盪電力信號,用於在諧振頻率 處驅動該無線電力傳送電路940以產生具有近場輻射之耦 合模式區。 在圖22B中,一無線電力轉發器電路960包括與電容元件 964耦合之一轉發器天線962,電容元件964具有ESR 966。 該電容元件串聯耦合於負電阻產生器910B。如早先所解 釋,無線電力轉發器電路960在諧振頻率處振盪以將具有 近場輻射之耦合模式區修改成一經修改之耦合模式區。 在圖22C中,一無線電力接收電路980包括與電容元件 140360.doc -41 - 201001869 984耦合之一接收天線982,電容元件984具有ESR 986。該 電容元件串聯耦合於負電阻產生器910C。一負載990耦合 於接收天線982與負電阻產生器91 0C之間。無線電力接收 電路980在諧振頻率處振盪以接收來自一耦合模式區或一 經轉發耦合模式區之能量且將該能量供應至負載990,其 表示跨越接收天線982之端子的負載(例如,電池及充電電 路)的阻抗。 圖22B說明將具有用於負電阻產生器910B之電源(未圖 示)的轉發器。當然,轉發器電路960可與具有負載990之 接收電路980類似地加以組態。在彼種情況下,負載990可 經組態以用於產生、儲存或產生與儲存用於負電阻產生器 910B之電力。 在圖22A至圖22C中,隨天線(942、962及982)展示之Rc 符號表示歸因於形成天線之金屬的有限導電性的損失。 Rrad符號表示天線之輻射電阻。ESR(946、966及986)為對 有限Q值負責的電容器之等效串聯電阻。電容元件(944、 964及984)為理想調諧電容值。-RN(910A、910B及910C) 為用於抵銷電路中之損失的負電阻。 在所展示之例示性耦合天線中,可利用一全波解決方 案。負電阻對此系統中電力傳輸之效率的影響可展示如 下: _ _R!oad_ "R,〇ad + Σ (-^) + Σ (Rrad +RC+ ESR) 對於一例示性穩定系統,滿足以下條件: 140360.doc -42- 201001869 ^ioad + Σ rad + + ESR) >| ^ (~RN) j 大體上’可選擇負f阻以抵銷天線電路中之多數損失。 然而’負電阻可設計成欠補償的’使得天線系統保 定。 心 f 熟習此項技術者將理解,可❹各種不同技術及技藝中 之任-者來表示資訊及信號。舉例而言,可藉由電麼、電 流、電磁波、磁場或磁粒子、光場或光粒子或其任何組合 來表不可在上文之描述中提及的資料、指令、命令、資 訊、信號、位元、符號及碼片。 、 熟習此項技術者應進一步瞭解,結合本文所揭示之實施 例描述的各種說明性邏輯區塊、模組、電路及演算法Η 可貫施為電子硬體、電腦軟體或其兩者之組合。為清楚地 說明硬體愈敕體夕+ = 軟體之此互換性,已在上文大體上在功能性方 面描述各種說明性组侔、 、仵區塊、模組、電路及步驟。此功 此性是實施為硬體或是軟體取決於特定應用及外加於整個 系A上之5又s十約束。熟習此項技術者可針對每一特定應用 以不同方式來實施所描述之魏性,但此等實施決策不^ 被解釋為造成偏離本發明之例示性實㈣的範- 可藉由通用處理器'數位信號處理器 積體電路(ASIC)、妒可和』 竹殊應用 。 琢了耘式化閘陣列(FPGA)或其他可裡式 ~輯益件_散閘或電晶體邏輯、離散硬體組件,或1 ^計以執行本文所述功能的任何組合來實施或執行結^ 本文所揭示實施例來彳+ 、U來“述的各種說明性邏輯區塊、模組及 电路 通用處理哭可或他老to -了為微處理器,但在替代實施例中,處 140360.doc -43- 201001869 理器可為任何習知處理器、护制 益衩釗态、微控制器或狀態機。 處理器亦可實施為計算写件之卸人 /1 , σ〇 态忏之組合,例如,DSP與微處理 益之組合、複數個微處理芎、紝人 心王亞、,,〇 口 DSP核心的一或多個微 處理器,或任何其他此種組態。 、-、°合本文所揭示之實施例所描述的方法或演算法之步驟 可直接以硬體、由處理器執行之軟體模組或以兩者之組合 來貫知。軟體模組可駐於隨機存取記憶體(RAM)、快閃記 It體、唯讀記憶體(R〇M)、電可程式化R〇M(EpR〇M)、電 可抹除可程式化ROM(EEPROM)、暫存器、硬碟、抽取式 碟片、CD-ROM,或此項技術中已知之任何其他形式的儲 存媒體中。例示性儲存媒體耦合至處理器,使得處理器可 自錄存媒體讀取資訊並將資訊寫入至儲存媒體。在替代實 施例中,儲存媒體可與處理器整合。處理器及儲存媒體可 駐於ASIC中。八810可駐於使用者終端機中。在替代實施 中處理器及儲存媒體可作為離散組件而駐於使用者終 端機中。 ~ 在—或多個例示性實施例中,可以硬體、軟體、勤體或 八任何組合來實施所描述之功能。若以軟體來實施,則功 能可作為一或多個指令或程式碼而儲存於電腦可讀媒體上 或經由電腦可讀媒體來傳送。電腦可讀媒體包括電腦錯存 媒體及通信媒體,通信媒體包括促進將電腦程式自一處傳 輸至另一處的任何媒體。儲存媒體可為可由電腦存取之 何可用媒體。舉例而言且不限制,此電腦可讀媒體可包含 RAM、R〇M、EEPR〇m、CD-ROM或其他光碟儲存、罐釋 140360.doc -44- 201001869 儲存或其他磁性儲存器件,或可㈣載運或儲存呈指令或 貧料結構之形式的所要程式碼且可由電腦存取的任何其他 媒體X將任何連接適當地稱作電腦可讀媒體。舉例而 言’若使用同軸電€、光纖電境、雙絞線、數位用戶線 (D叫或諸如紅外線、無線電及微波之無線技術自網站、 祠服器或其他遠線调值&磁 '、,达軟肢,則該同軸電纟覽、光纖電 纜又、,又線DSL ’或諸如紅外線、無線電及微波之益線 技術係包括於媒體之定義中。如本文中使用,磁碟及光碟 包括光碟(CD)、雷射光碟、光學光碟、數位影音光碟 (DVD)、軟性磁碟及藍光光碟,其中磁碟通常用磁性方式 來重現資才斗,而光碟用雷射以光學方式來重現資料。上述 各者之組合亦應包括於電腦可讀媒體之範疇内。
提供對所揭示例示性實施例之先前描述以使任何熟習此 項技術者能夠製造或使用本發明。熟習此項技術者將易於 見對此等例不性貫施例之各種修改,且在不脫離本發明 精神或範可的情況下,本文所界^之通用原理可應用於 其他實施例。因此,本發明不意欲限於本文所示之實施 例,而疋符合與本文所揭示之原理及新穎特徵一致的最廣 範疇。 ” 【圖式簡單說明】 圖1展示無線電力傳輸系統之簡化方塊圖。 圖2展不無線電力傳輸系統之簡化示意圖。 圖3展示用於本發明之例示性實施例中的環形天線的示 意圖。 140360.doc •45- 201001869 圖4展示指示傳送天線與接收天線之間㈣合強度的模 擬結果。 圖5A及圖5B展示根據本發明之例示性實施例的用於傳 送天線及接收天線之環形天線的佈局。 圖6展示指示與圖5A及圖5B中所說明之正方形及圓形傳 送天線的各種腳大小有關的在傳送天線與接&天線之間 的耦合強度的模擬結果。 圖7展不指不與圖5a及圖5B中所說明之正方形及圓形傳 送天線的各種表面積有關的在傳送天線與接收天線之間的 耦合強度的模擬結果。 圖8展示接收天線相對於傳送天線之各種放置點以說明 在共面及同軸放置下之耦合強度。 圖9展不指不在傳送天線與接收天線之間的各種距離下 同軸放置的耦合強度的模擬結果。 圖10為根據本發明之例示性實施例的傳送器的簡化方塊 圖。 圖11為根據本發明之例示性實施例的接收器的簡化方塊 圖。 圖1 2展示用於在傳送器與接收器之間進行訊息傳遞的傳 送電路之部分的簡圖。 圖13A至圖i3C展示在各種狀態下之接收電路的一部分 的簡圖以說明接收器與傳送器之間的訊息傳遞。 圖14A至圖i4C展示在各種狀態下之替代接收電路的一 部分的簡圖以說明接收器與傳送器之間的訊息傳遞。 140360.doc -46- 201001869 圖15A至圖15C為說明用於傳送器與接收器之間的通信 的訊息傳遞協定的時序圖。 圖16A至® 16D為說明用於在傳送器與接收器之間傳送 電力的信標電力模式的簡化方塊圖。 圖A „兒月大傳送天線,及與該傳送天線共面及同轴地 安置之較小轉發器天線。 圖1 7B D兒明傳送天線,及相對於該傳送天線同軸放置之 較大轉發器天線。 /18A說明大傳送天線,及與該傳送天線共面地安置且 文置於傳达天線之周邊内的三個不同之較小轉發器天線。 圖1 8B β兄明大傳送天線’及相對於傳送天線有偏移地同 軸放置及有偏移地共面放置的較小轉發器天線。 圖19展示指示傳送天線、轉發器天線及接收天線之間的 耗合強度的模擬結果。 圖2〇Α展示指示在不具有轉發器天線之情況下傳送天線 與接收天線之間的耦合強度的模擬結果。 圖20Β展示扎示在具有轉發器天線之情況下傳送天線與 接收天線之間的耦合強度的模擬結果。 圖21說明構成負電阻轉換器之具有正及負反饋的例示性 運算放大器。 圖22Α至圖22C分別說明包括用於傳送天線、轉發器天 線及接收器天線之負電阻的例示性天線電路。 【主要元件符號說明】 1 a-3a 140360.doc -47- 201001869 lb-3b 點 1 c-3c 點 100 無線傳送或充電系統 102 輸入電力 104 傳送器 106 幸虽射场 108 接收器 110 輸出電力 112 距離 114 傳送天線 114C 大圓形環形傳送天線 114S 正方形環形傳送天線 118 接收天線 118' 接收天線 119 獨立通信頻道 122 振盪器 123 調整信號 124 功率放大器 125 控制信號 126 濾波及匹配電路 132 匹配電路 136 電池 150 「環形」天線 152 電容器 140360.doc -48- 201001869 154 電容器 156 諧振信號 170 曲線 172 曲線 174 曲線 180 曲線 182 曲線 190 曲線 200 傳送器 202 傳送電路 204 傳送天線 206 固定阻抗匹配電路 208 低通渡波器 210 功率放大器 212 振盪器 214 處理器 216 負載感測電路 220 載波信號 224 傳送調變信號 226 信號 228 電源 230 差動放大器 235 接收信號 300 接收器 140360.doc •49- 201001869 302 接收電路 304 接收天線 306 電力轉換電路 308 RF至DC轉換器 310 DC至DC轉換器 312 切換電路 314 發信號偵測器及信標電路 3 16 處理器 3 18 整流器 320 傳送信號 322 DC電力信號 350 器件/節點 410 循環週期 420 同步脈衝 420' 「白」脈衝 422 暖機週期 424 前向鍵路週期 426 監聽週期 427 交遞週期 428 開始反向鍵路週期 430 反向鏈路週期 450 電力週期 450' 電力週期 510 信標耦合模式區 140360.doc -50- 201001869 510' 高電力耦合模式區 520 傳送器 525 信標信號 525' 局電力信號 530 接收器件 535 反向鏈路麵合 710A 傳送天線 710B 傳送天線 、 710C 傳送天線 710C 傳送天線 710D 傳送天線 720A 較小轉發器天線 720B 較大轉發器天線 720C 轉發器天線 720D 轉發器天線 730A i. 接收天線 730B 接收天線 730C 接收天線 730D 接收天線 740 台 742 燈罩 746 天花板 810 曲線 810A 曲線 140360.doc •51 - 201001869
810B 820
820B 830
830A
830B 840 910
910A、910B、910C 920 922 924 926 928 929 930 940 942 944 946 950 960 962 964 曲線 曲線 曲線 曲線 曲線 曲線 曲線 負電阻產生器 負電阻產生器 運算放大器 第一反饋電阻器 第二反饋電阻器 輸入電阻器 第一端子 第二端子 等效負電阻 無線電力傳送電路 傳送天線 電容元件 等效串聯電阻 信號產生器 無線電力轉發器電路 轉發器天線 電容元件 140360.doc -52- 201001869 966 等 效 串 聯 電 阻 980 接 收 電 路 982 接 收 天 線 984 電 容 元 件 986 等 效 串 聯 電 阻 990 負 載 C1-C3 電 容 器 D1 二 極 體 ESR 等 效 串 聯 電 阻 LI 特 性 電 感 P1-P7 放 置 點 Pdl ' Pd2 > Pdn 電 力 區 段 R1、R2 電 阻 器 R〇 損 失 Rrad 天 線 之 輻 射 電阻 Rs 電 阻 器 S1A、SIB、S2A、S2B、S3B 開 關 -RN 負 電 阻 140360.doc -53-
Claims (1)
- 201001869 七、申請專利範圍·· 1. 一種無線電力接收電路,其包含: 一接收天線,其用於在一諧振頻率處耦合於一近場輻 射; 人=電^元件,其可操作地串聯耦合於該接收天線且包 s 一電谷值及一等效串聯電阻值; -負電阻產生器,其可操作地串聯耦合於該電容元件 且包含—負電阻值;及 負載,其可刼作地串聯耦合於該負電阻產生器且用 於在該無線電力接收電路大體上在《振頻率附近振盪 時汲取來自該近場輕射之電力。 2. 如請求们之無線電力接收電路,其中該負電阻產生器 係用於產生該負電阻值以抵銷該等效串聯電阻值、該接 收天線之歐姆電阻或其一組合中之至少一些。 3. 如請求们之無線電力接收電路,其中該負電阻產生器 包含: 一運算放大器’其包含—放大器輸出、—正輸入及— 負輸入,該負輸入可操作地耦合至該負電阻產生器之— 第一端子; 第反饋電阻器,其可操作地耦合於該放大器輪出 與該負輸入之間; 一第二反饋電阻器,其可操作地耦合於該放大器輪出 與該正輸入之間;及 —輸入電阻器,其可操作地耦合於該負電阻產生器之 140360.doc 201001869 一第二端子與該正輪入之間。 4·二請^们之無線電力接收電路,其中該第—反饋電阻 益。玄第二反饋電阻器及該輸入電阻器經 負電阻值以抵銷該等效串聯電阻值:… 電阻或其-組合中之至卜^ 請收天線之歐姆 5· 種無線電力傳送電路,其包含: 射; 傳送天線,其用於在-譜振頻率處產生一近場幸畐 人―:容元件’其可操作地串聯轉合於該傳送天線且包 含-電容值及-等效串聯電阻值; ’ —負電阻產生器,i掉 a ^ ^ A 耜作地串聯耦合於該電容元件 且包含一負電阻值;及 合兀忏 —信號產生芎,计 - °其可操作地串聯耦合於該負4 态’且用於將—传噃兩 必貝*€阻產生 。嬈電力施加至該盔t 使得該無線電力傳…、線電力傳送電路, 盪。 X %振頻率附近振 6. 如請求項5之無線雷^ “力傳送電路,其中+ 係用於產生該負電阳#、 甲。亥負電阻產生器 值以抵銷該等效串 送天線之歐姆電阻洸 外电阻值、該傳 次其一組合中之至少〜 7. ^青求項5之無線電力傳送電路,二。 包含: °亥負電阻產生器 —運算放大器, .^ 其包含—放大器輸出、_ τ # 負輪入,該負輪入可 正輪入及一 第一端子; 貝ι阻產生器之一 140360.doc 201001869 反饋電阻器,其可操作地耦合於.该放大器輸出 與該負輸入之間; 第 饋電阻器,其可操作地耦合於該放大器輸出 與該正輸入之間;及 一輸入電阻器’其可操作地耦合於該負電阻產生器之 一第二端子與該正輸入之間。 8.如請求項7之無線電力傳送電路,其中該第一反饋電阻 益、该第二反饋電阻器及該輸入電阻器經選擇以產生該 負電阻值以抵銷該等效串聯電阻值、該傳送天線之歐姆 電阻或其一組合中之至少一些。 9. 種無線電力轉發器電路,其包含: 模天線/於在―㈣頻率處麵合於在一鋼合 吴…之-近場輻射’且產生不同於 -經轉發耦合模式區; 祸“果式£之 i.. :電容元件’其可操作地串聯轉合 包含-電容值及一等效串聯電阻值;及 H泉且 負电阻產生器’其可操作地串聯耦人 且包含-負電阻值。 如轉合於該電容元件 10.如請求項9之無線電力轉發器電路 益係用於產生該負電阻值以抵鐵:中该負電阻產生 轉發器天線之歐姆電阻或並—組 > 串聯電阻值、該 器包含: 運算放大器,其包含-放大 丨1.—之無線電力轉發器電 S亥負電阻產生 140360.doc 器輪出、1輪入及 201001869 負輸入,該負輸入可操作地耦合至該負電阻產生器之 第一端子; 一第一反饋電阻器,其可操作地耦合於該放大器輪出 與該負輸入之間; 一第二反饋電阻器,其可操作地耦合於該放大器輪出 與該正輸入之間;及 輪入電阻器,其可操作地耦合於該負電阻產生器之 一第二端子與該正輸入之間。 12. 如請求項此無線電力轉發器電路,其中該第一反镇電 阻态、㈣二反饋電P且器及該輸入電p且器經選擇以產生 "亥負電阻值以抵銷該等效串聯電阻值、該轉發器天線之 歐姆電阻或其一組合中之至少一些。 、 13. —種方法,其包含·· 、、,在—傳送天線之—證振頻率處產生-電磁場以在該傳 送天線之一近場内建立一耦合模式區;及 、 藉由安置於該叙合模式區内的一接收天線接收來㈣ 稱合模式區之電力,J1中·^玄接收蝻 ^ 率附近諧振; 貝 其中該產生該電磁#包括設定該傳送天線之—傳送 件的-負電阻值以抵鎖該傳送天線之其他傳送組件 等效串聯電阻值中之至少一些。 、 14·^求項13之方法,其中該接收來自料合模式區之 匕括定該接收天線之-接收組件的一 抵鎖該接收天線之其他接收組件的 寻妓甲聯電阻值 I40360.doc 201001869 之至少一些。 15. —種方法,其包含: 在一傳送天線之—諧振 送天線之一近場内建立^處產生—電磁場以在該傳 叫遷立—耦合模式區;及 藉由安置於該輕合模式區内的 耦合模式區之電力,農 彡收天線接收來自該 率附近諧振; …接收天線大體上在該譜振頻 其中該接收來自該輕合 ^ , Λ <电刀包括設定該接收 天線之一接收組件的—泰彳 他接收組件的一等效…以抵鎖該接收天線之其 寺放串聯電阻值中之至少一此。 16. 如請求項15之方法,其中該產生 :〜 傳送天線之-傳送組件的一每、·设定該 之其他傳送組件的—等效了 以抵銷該傳送天線 寻效串聯電阻值中之至少一此。 1 7 · —種方法,其包含: 一 在一傳送天線之—諧拒 、頻率處產生一電磁場以在該傳 送:線之-近場内建立—耦合模式區,· 藉由一轉發器天線轉發恭 m广 料π亥包磁~以建立不同於該轉合 槙式區之一經轉發耦合模式區;及 ::安置於該搞合模式區内的一接收天線接收來自該 赉耦口模式區之電力’其令該接收天線大體上在該 &振頻率附近諧振; 其中該產生該電磁場包括設定該傳送天線之一傳送組 件的-負電阻值以抵銷該傳送天線之其他傳送組件的一 荨效串聯電阻值中之至少一歧。 140360.doc 201001869 18.如請求項17之方法’其中該接收來自該輪合模式… 力包括:歧該接收天線之-接收級件的—負電阻值: 抵銷該接收天線之其他接收組件的聯電阻 之至少一些。 τ 19·如請求項17之方法’其中該轉發該電磁場包括:設定今 轉發器天線之一轉發器組件的一負f " 哭工城 J貝冤阻值以抵銷該轉發 益天、.泉之其他轉發器組件的一等效串聯電 一些。 王y 20. 如請求項19之方法,其中 ,,, Λ按收术自该耦合模式區之電 力包括:設定該接收天線之一接收組件 ^ 4ϊ!ί J-Λ 1/ 2. 貝電阻值以 之至:一:其他接收組件的-等效串聯電阻值中 21. —種無線電力傳輸系統,其包含: 用於在-傳达天線之―㈣ 在該傳送天線之-近場内建立紅人座生電磁场以 _立一耦合模式區的構件;及 用於错由安置於該耦人措斗.广^ 來自該•合模式區之電二接收天線接收 上在該諧振頻率附近譜振; 〃錢收天線大體 ^該用於產生該電磁場之構件包括—用於設定該傳 送天線之一傳送組件的— - 值.、,,# 員電阻值以抵銷該傳送天線之 件。 甲如電阻值中之至少一些的構 1如請求項21之系統,其中該 之電力的構件包括:要收來自_合板式區 於3又夂該接收天線之一接收組 140360.doc 201001869 件的-負電阻值以抵銷該接收天線之其他接收組件的一 等效串聯電阻值中之至少一些的構件。 23. —種無線電力傳輸系統,其包含: -用於在-傳送天線之—諸振頻率處產生—電磁場以 二傳达天線之-近場内建立—輕合模式區的構件;及 ^用於藉由安置於該叙合模式區内的_接收天線接收 …… 7扪構件,其中該接收天線大體 上在该谐振頻率附近諧振; 其中該用於接收來自該耦入 一 + 口杈式£之電力的構件包括 一用於5又疋該接收天線之一接 ^ ^ 女队、、見仵的一負電阻值以抵 銷忒接收天線之其他接收組 至少一些的構件。 彳效串聯電阻值t之 -如請求項23之系統,其中該用於產 括:―用於設㈣傳送天線之—傳送件包 以抵銷該傳送天線之其他傳送…件的負電阻值 中之至少-些的構件。 Μ电阻值 25. —種無線電力傳輸系統,其包含·· 一用於在一傳送天線之一諧振頻率 + 在該傳送天線之一近場内建 生—笔磁場以 m 建立一耦合模式區的構件. 一用於藉由一轉發夭绐 ’ 寻啜态天線轉發該電磁場 該耗合模式區之一經轉發輕合模式區的構件及不同於 一用於藉㈣置料經轉發衫 線接收來自該經轉發稱合 内的-接收天 供八(he之電力的構 接收天線大體上在該諧振頻率附近譜振; 、該 I40360.doc 201001869 其中該用於產生該電日 送天線之一傳送組件的一構件包括一用於設定該傳 其他傳送組件的一等坪、電阻值以抵銷該傳送天線之 件。 J串聯電阻值中之至少一些的構 26.如請求項25之系統,其 之電力的構件包括:二用二接收來自該輕合模式區 件的1電阻值則該接收天線之—接收組 等效串聯電阻值中接收天線之其他接收組件的-&如電阻財之至少-些的構件。 括.— 其中㈣於轉發該電磁場之構件包 、用於設定該轉發器天線之一轉發器組件恭 阻值以抵鐵該轉發器天線之其他轉發器 文: 聯;阻㈣t 4效串 28·:ί:項27之系統,其中該用於接收來自該輕合模式區 “—Γ!件包括:一用於設定該接收天線之-接收組 、%阻值以抵銷該接收天線之其他接收組件的 等攻串聯電阻值中之至少一些的構件。 、 140360.doc
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TW98115924A TW201004091A (en) | 2008-05-13 | 2009-05-13 | Method and apparatus for an enlarged wireless charging area |
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