2014 IEEE International Symposium on Circuits and Systems (ISCAS) 2014
DOI: 10.1109/iscas.2014.6865078
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Analytical design procedure for resonant inductively coupled wireless power transfer system with class-E<sup>2</sup> DC-DC converter

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Cited by 12 publications
(6 citation statements)
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“…As the airgap of the ICT is great, the coupling is weak. Consequently, to achieve the demanded transmitted power, important reactive power need to be directed, so the usage of resonant elements [37][38][39][40][41][42][43] in both sides of the ICT is essential as compensation to ensure good efficiency. Furthermore, the output parameters at the load part should be monitored in order to supervise the charging profile of the battery and to assure its protection.…”
Section: Static Battery Chargingmentioning
confidence: 99%
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“…As the airgap of the ICT is great, the coupling is weak. Consequently, to achieve the demanded transmitted power, important reactive power need to be directed, so the usage of resonant elements [37][38][39][40][41][42][43] in both sides of the ICT is essential as compensation to ensure good efficiency. Furthermore, the output parameters at the load part should be monitored in order to supervise the charging profile of the battery and to assure its protection.…”
Section: Static Battery Chargingmentioning
confidence: 99%
“…The setting in place of dynamic IPT schemes in the road infrastructure will eliminate the necessity for charging halts and could result in a noteworthy reduction in the size of the on-board battery [38][39][40][41][42][43]. The fruitful illustration of the practicality of this technology may point out a tangible media to increase the reception of electric mobility and to deal with the furthermost critical features of the use of EV.…”
Section: Ipt In Ev On Roadmentioning
confidence: 99%
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“…Once the limitations on the coil geometry and coupled impedances are fully defined, the matching network could be optimized to minimize loss. Alternatively, the network could be removed altogether, as recent work [24], [25] has shown that if the coil geometry can be fixed, providing a constant coupling coefficient, then the power amplifier and rectifier can also be optimized and made independent of resistive changes to the load resistance on the rectifier.…”
Section: E Controllable Impedance Matching Systemmentioning
confidence: 99%
“…When the switch is off, the DC power source will charge the LC resonator and the load; when the switch is on, the energy stored in the LC resonator releases the power to the C 1 , and since the resonant frequency is different between the LC resonator and the L, C, C 1 series network, the parameters of the circuit should be designed to make sure that the voltage of C 1 will be exactly zero at the end of the switch-off mode, resulting in a ZVS action. Reference [57] presents an example of a Class E amplifier application for a Reference [58] applied the Class E technique in both the transmitter and the receiver. The simulation results showed that the circuit could achieve ZVS/ZDS conditions for both sides with an output power of 5 W and an overall efficiency of 65.9%.…”
Section: Frequency Splittingmentioning
confidence: 99%