The present invention generally relates to systems for optimizing wireless power transfer utilizing a single tuned resonator circuit.
Wireless power transfer (WPT) involves the use of time-varying magnetic fields to wireles sly transfer power from a source to a device. Faraday's law of magnetic induction provides that if a time-varying current is applied to one coil (e.g., a transmitter coil) a voltage will be induced in a nearby second coil (e.g., a receiver coil). The voltage induced in the receiver coil can then be rectified and filtered to generate a stable DC voltage for powering an electronic device or charging a battery. The receiver coil and associated circuitry for generating a DC voltage can be connected to or included within the electronic device itself such as a smartphone or other portable device.
The Wireless Power Consortium (WPC) was established in 2008 to develop the Qi inductive power standard for charging and powering electronic devices. Powermat is another well-known standard for WPT developed by the Power Matters Alliance (PMA). There also have been some market consolidation efforts to unite into larger organizations, such as the AirFuel Alliance consisting of PMA and the Rezence standard from the Alliance For Wireless Power (A4WP).
Earlier versions of both the Qi and Powermat standards fixed the peak resonant frequency of the wireless power transfer process at 100 kHz for Qi and 277 kHz for Powermat. These fixed values are based on the nominal values of the primary inductance of the transmitter coil and the primary capacitance of the associated transmitter-side resonant capacitor in series with the transmitter coil. The operating frequency for transmitters called for in these standards is based on these assumed fixed resonant frequencies. In actual wireless power transmitters the peak resonant frequency is not fixed but is rather a function of the nominal inductance and capacitance values of the transmitter coil and capacitor and other factors such as component variations, load, and leakage. Different wireless power receivers may put different loads on a particular wireless power transmitter, and power leakage varies depending on how well-aligned a wireless power receiver's coil is to the transmitter coil. The entire behavior of the wireless power transfer system is affected by variations in the actual resonant frequency of a wireless power transmitter.
Later versions of these standards allow for slight variations in the operating frequency away from the assumed fixed resonant frequency, but these variations still rely on the basic assumption that the resonant frequency of the transmitter is a known, fixed value based on the nominal inductance of the transmitter coil (measured without being magnetically coupled to a receiver coil) and the nominal capacitance of the resonant capacitor. The Qi standard still requires that the receiver is tuned to a fixed frequency, the fixed frequency being tuned to the assumed fixed resonant frequency of the transmitter, i.e., 100 KHz. The assumed resonant frequency is determined from the measurement of the receiver coil inductance without being in proximity to a transmitter coil and the receiver resonant capacitor. In actual operating Qi systems, while the transmitter and receiver are magnetically coupled, variable resonant frequencies are generated, which is not just unpredictable but adversely affects the ability to deliver more power.
As maximum power transfer in a wireless power system occurs when the operating frequency is close to or at the resonant frequency, an incorrect assumption about the resonant frequency affects the ability of the system to deliver close to maximum power. The incorrect assumption about the resonant frequency also creates anomalies in the control loop. For example, in the Qi and PowerMat systems, when the receiver requests an increase in power, the Qi and Powermat systems lower the operating frequency of the transmitter to be closer to the assumed fixed resonant frequency. As the actual (and varying) resonant frequency was often higher than the assumed resonant frequency, the delivered power would decrease instead and the transmitter would turn off due to this anomaly, sometimes referred to as “control inversion.” For example, if the actual resonant frequency of a wireless power transfer system is 150 kHz but the assumed resonant frequency is 100 kHz, the system may adjust the operating frequency closer to 100 kHz in an attempt to increase the delivered power but may actually be lowering the delivered power by moving too far away from the actual resonant frequency. An operating frequency that is too far from the actual resonant frequency can also cause large unanticipated voltage peaks in the resonant components in both the receiver and the transmitter. The reliability of the wireless power transfer system thus can also be affected by assuming an incorrect fixed resonant frequency.
Thus, there is a long felt need for a wireless power transfer system in which the variability of system performance at resonance is clearly understood so as to optimized the system performance for maximum power transfer.
According to an embodiment of the present disclosure there is provided a wireless power transfer system comprising a wireless power receiver comprising a receiver coil configured to couple with a magnetic field emitted by a wireless power transmitter, wherein a time-varying current is induced in the receiver coil by the magnetic field, and the wireless power receiver does not comprise a resonant capacitor.
In some implementations, a frequency response of the wireless power transfer system comprises a single significant peak. In other implementations, the receiver coil comprises any combination of single spiral coils, multiple spiral coils, longitudinal coils, or coils having any polarity structure. In certain implementations, the wireless power receiver may further comprise at least one auxiliary non-resonant capacitor. In further implementations, the auxiliary capacitor does not does not contribute to or affect an existing resonant frequency of the wireless power transfer system. In some implementations, the auxiliary capacitor does not create another peak in the frequency response of the wireless power system. In other implementations, the auxiliary capacitor is greater than about 470 nF. In certain implementations, a single significant resonant frequency of the system is configured to be less than about 400 kHz.
According to another embodiment of the present disclosure there is provided a wireless power transfer system comprising a wireless power transmitter comprising a transmitter coil configured to receive a time-varying current that flows in the transmitter coil to produce a transmitter magnetic field. The wireless power transfer system also comprises wireless power receiver comprising a receiver coil, and a resonant capacitor. In the wireless power transfer system, the transmitter magnetic field is configured to couple the wireless power transmitter with the wireless power receiver to induce a time-varying current to flow in the receiver coil of the wireless power receiver. In addition, the resonant capacitor in the wireless power transfer system is coupled to the wireless power transmitter and not the wireless power receiver.
In certain implementations, the resonant capacitor is configured to set a resonant frequency of the wireless power transmitter when the wireless power receiver is unloaded. In some implementations, the resonant capacitor is physically located in the wireless power transmitter and not the wireless power receiver. In other implementations, a frequency response of the wireless power transfer system comprises a single significant peak. In other implementations, the wireless power transmitter and/or the wireless power receiver may further comprise at least one auxiliary non-resonant capacitor. In further implementations, the auxiliary capacitor does not contribute to or affect an existing resonant frequency of the wireless power transfer system. In some implementations, the auxiliary capacitor does not create another peak in the frequency response of the wireless power system. In certain implementations, the auxiliary capacitor is greater than 470 nF. In other implementations, the transmitter and receiver coils comprise any combination of single spiral coils, multiple spiral coils, longitudinal coils, or coils having any polarity structure. In some implementations, a single significant resonant frequency of the system is configured to be less than about 400 kHz.
According to another embodiment of the present disclosure there is provided a wireless power transfer system comprising a wireless power transmitter comprising a transmitter coil configured to receive a time-varying current that flows in the transmitter coil to produce a transmitter magnetic field. The wireless power transfer system also comprises a wireless power receiver comprising a receiver coil, and a resonant capacitor. In the wireless power transfer system, the transmitter magnetic field is configured to couple the wireless power transmitter with the wireless power receiver to induce a time-varying current to flow in the receiver coil of the wireless power receiver. In addition, the resonant capacitor is only coupled to either the wireless power transmitter or the wireless power receiver, but not both.
In some implementations, the resonant capacitor is only coupled to the wireless power transmitter and not the wireless power receiver. In other implementations, the resonant capacitor is only coupled to the wireless power receiver and not the wireless power transmitter. In further implementations, the resonant capacitor is configured to set a resonant frequency of the wireless power transmitter when the resonant capacitor is only coupled to the wireless power transmitter and the wireless power receiver is unloaded. In certain implementations, the resonant capacitor is configured to set a resonant frequency of the wireless power receiver when the resonant capacitor is only coupled to the wireless power receiver and the wireless power receiver is unloaded.
In other implementations, the resonant capacitor is physically located in the wireless power transmitter and not the wireless power receiver. In further implementations, the resonant capacitor is physically located in the wireless power receiver and not the wireless power transmitter. In some implementations, a frequency response of the wireless power transfer system comprises a single significant peak. In certain implementations, the wireless power transmitter and/or the wireless power receiver may further comprise at least one auxiliary non-resonant capacitor. In other implementations, the auxiliary capacitor does not contribute to or affect an existing resonant frequency of the wireless power transfer system. In further implementations, the auxiliary capacitor does not create another peak in the frequency response of the wireless power system. In some implementations, the auxiliary capacitor is greater than 470 nF.
In some implementations, the transmitter and receiver coils comprise any combination of single spiral coils, multiple spiral coils, longitudinal coils, or coils having any polarity structure. In certain implementations, a resonant frequency of the system is configured to be less than about 400 kHz. In other implementations, a resonant frequency of the system is configured to be between about 80 kHz and 100 kHz. In further implementations, a resonant frequency of the system is configured to be about 85 kHz.
The foregoing and other objects and advantages will be apparent upon consideration of the following detailed description, taken in conjunction with the accompanying drawings, in which like reference characters refer to like parts throughout, and in which:
To provide an overall understanding of the devices described herein, certain illustrative embodiments will be described. Although the embodiments and features described herein are specifically described for use in wireless power transfer systems, it will be understood that all the components and other features outlined below may be combined with one another in any suitable manner and may be adapted and applied to other types power transfer systems desiring optimized power transfer to a receiver circuit coupled to a load.
Coils 102 and 110 may be magnetically coupled together by placing both coils in close proximity to each other and/or by placing both coils 102, 110 on a magnetic layer. The magnetic layer can be ferrite or any other magnetic layer known in the art. Coils 102 and 110 may comprise coils of any topology, such as, for example, single spirals, double spirals, longitudinal coils, etc. Coils 102 and 110 are preferably identical coils with the same number of turns, the same area, and wound in the same direction (i.e., clockwise or counter-clockwise). The power circuit 108 generates an AC signal of a defined voltage magnitude. The generated AC signal can be, but is not limited to, a square wave, a sinusoidal wave, a triangular wave, or a sawtooth wave. The AC signal causes time-varying current to flow from power circuit 108 through the rectifying circuit 106 to primary coil 102. The flow of current through coil 102 of the transmitter circuit Tx generates a magnetic field.
The magnetic field magnetically couples to the secondary coil 110 and induces a time-varying current that flows through the secondary coil 110 to the secondary capacitor 112 and the rectifying circuit 114. Faraday's law provides that the time-varying current that flows in the secondary coil 110 will oppose the magnetic field generated by the primary coil 102. The voltage generated as a result of the coupling of the primary coil 102 with the secondary coil 110 with the generated magnetic field is provided to the load 116, which may be a rechargeable battery or power a device (e.g., a smart phone, laptop or any other electronic device).
The wireless power transfer system 100 in
Such tuning between a primary coil of a transmitter and a secondary coil of a receiver is known in the art and is likened to the analogy of tuning forks in sympathetic resonance, or opera singers supposedly breaking wine glasses by matching the transmitter frequency to a receiver frequency. This frequency tuning or matching shall be referred to as a “double resonator” approach and is based on the transformer model. A more detailed and accurate understanding of the transformer model is explained in U.S. patent application Ser. No. 16/287,660, filed on Feb. 27, 2019, and entitled “SYSTEMS AND METHODS FOR HIGH-POWER WIRELESS POWER TRANSFER WITH DUAL-QI COMPATABILITY,” the contents of which are hereby incorporated by reference in its entirety. However neither the Qi standards body nor the SAE recognized the significant effect to the resonant profile during operation, which the present disclosure seeks to document and adapt to. The “double resonator” approach is invalid in a closely coupled system as there is a significant shift of the resonant peak in the frequency response of the system as a result of reflected impedances in the closed system.
Nonetheless, the wireless power transfer system as shown in
In the circuit of
The present disclosure therefore only has one resonant capacitor present in a wireless power transfer system, as shown in
Similarly, according to an embodiment of the present disclosure, the wireless power system 130 as shown in
In wireless power system 120 shown in
The wireless power systems 120 and 130 may comprise at least one auxiliary capacitor that does not contribute to, or affect an existing resonant frequency of the wireless power transfer system. Additionally, the at least one auxiliary capacitor does not create another significant or noticeable resonant peak in the frequency response of the system. In some implementations, the auxiliary capacitor is at least 470 nF. This ensures that the auxiliary capacitor does not create another significant or noticeable resonant peak in the frequency response of the system. In general, the contribution of the auxiliary capacitor in the wireless power system to the frequency response of the wireless power system is considered to be insignificant if the resonant frequency of the open-circuit receiver with the auxiliary capacitor connected is three times lower than the resonant frequency of the open-circuit transmitter. Here the open-circuit receiver refers to the non-operating inductance of the receiver coil combined with the remaining receiver circuit elements (e.g. the auxiliary capacitor and the secondary capacitor), with the transmitter coil in its vicinity or not. Similarly, the open-circuit transmitter refers to the non-operating inductance of the transmitter coil combined with the remaining transmitter circuit elements (e.g. the primary capacitor), with the receiver coil in its vicinity or not.
It should be noted that the embodiments of the present disclosure as shown in
Exemplary topologies for transmitter and receiver coils of the present disclosure, and associated drive circuitry, are described in the following patents and/or patent applications, the contents of which are hereby incorporated by reference in entirety: U.S. patent application Ser. No. 15/028,725 (now U.S. Pat. No. 10,581,276), filed on Mar. 28, 2016, and entitled “TUNED RESONANT MICROCELL-BASED ARRAY FOR WIRELESS POWER TRANSFER”; U.S. patent application Ser. No. 15/082,533 (now U.S. Pat. No. 10,374,459), filed on Mar. 28, 2016 and U.S. patent application Ser. No. 16/532,168, filed on Aug. 5, 2019, both entitled “WIRELESS POWER TRANSFER USING MULTIPLE COIL ARRAYS”; U.S. patent application Ser. No. 15/082,672 (now U.S. Pat. No. 10,263,471), filed on Mar. 28, 2016, and U.S. patent application Ser. No. 16/384,555, filed on Apr. 15, 2019, both entitled “MULTIPLE INTERLEAVED COIL STRUCTURES FOR WIRELESS POWER TRANSFER”; U.S. patent application Ser. No. 15/448,196, filed on Mar. 2, 2017, and entitled “RECEIVER COIL ARRANGEMENTS FOR INDUCTIVE WIRELESS POWER TRANSFER FOR PORTABLE DEVICES”; U.S. patent application Ser. No. 15/635,495 (now U.S. Pat. No. 10,312,745), filed on Jun. 28, 2017, and entitled “WIRELESS POWER TRANSFER SYSTEM WITH AUTOMATIC FOREIGN OBJECT REJECTION”; U.S. patent application Ser. No. 15/693,201, filed on Aug. 31, 2017, and entitled “SEGMENTED AND LONGITUDINAL RECEIVER COIL ARRANGEMENTS FOR WIRELESS POWER TRANSFER”; U.S. patent application Ser. No. 15/708,426, filed on Sep. 19, 2017, and entitled “BENT COIL STRUCTURE FOR WIRELESS POWER TRANSFER”; U.S. patent application Ser. No. 15/375,499, filed on Dec. 12, 2016, and entitled “SYSTEM FOR INDUCTIVE WIRELESS POWER TRANSFER FOR PORTABLE DEVICES”; U.S. patent application Ser. No. 15/613,538, filed on Jun. 5, 2017, and entitled “COIL STRUCTURES FOR ALIGNMENT AND INDUCTIVE WIRELESS POWER TRANSFER”, U.S. patent application Ser. No. 15/866,786 (now allowed), filed on Jan. 10, 2018, and entitled “WHEEL COILS AND CENTER-TAPPED LONGITUDINAL COILS FOR WIRELESS POWER TRANSFER”; U.S. patent application Ser. No. 15/882,147, filed on Jan. 29, 2018, and entitled “SYSTEM AND METHOD FOR FREQUENCY CONTROL AND FOREIGN OBJECT DETECTION IN WIRELESS POWER TRANSFER”; and U.S. patent application Ser. No. 16/287,660, filed on Feb. 27, 2019, and entitled “SYSTEMS AND METHODS FOR HIGH-POWER WIRELESS POWER TRANSFER WITH DUAL-QI COMPATABILITY.”
It should be noted that the term “directly connected to” indicates that the components are connected to each other without anything else connected between the components. It should also be noted that the term “about” or “approximately” indicates a range of ±20% of the stated value. Further, all the necessary electronic components of the transmitter circuit Tx and the receiver circuit Rx may not be described in the foregoing for brevity, however such electronic components are within the scope of the person of ordinary skill in the art and are hereby included in this disclosure.
Other objects, advantages and embodiments of the various aspects of the present invention will be apparent to those who are skilled in the field of the invention and are within the scope of the description and the accompanying Figures. For example, but without limitation, structural or functional elements might be rearranged consistent with the present invention. Similarly, principles according to the present invention could be applied to other examples, which, even if not specifically described here in detail, would nevertheless be within the scope of the present invention.
This application claims priority to and the benefit of U.S. Provisional Patent Application No. 62/873,985, filed on Jul. 15, 2019, entitled “TRUE OPTIMIZABLE WIRELESS POWER SYSTEMS”, the subject matter of which is hereby incorporated by reference in its entirety.
Number | Date | Country | |
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62873985 | Jul 2019 | US |