2017 IEEE Transportation Electrification Conference and Expo, Asia-Pacific (ITEC Asia-Pacific) 2017
DOI: 10.1109/itec-ap.2017.8080829
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Analysis and design of an LCC/S compensated resonant converter for inductively coupled power transfer

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Cited by 26 publications
(11 citation statements)
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“…In the LCC network, the compensation form is mostly T‐shaped network in order to generate a constant current I L 1 which contributes to the stabilization of secondary induced voltage; moreover, pure resistance of the input impedance can be achieved. The relationship between the resonance parameters of its components is shown as follows [30]: ωLf1badbreak=1ωCf1goodbreak=ωL1goodbreak−1ωC1$$\begin{equation}\omega {L}_{f1} = \frac{1}{{\omega {C}_{f1}}} = \omega {L}_1 - \frac{1}{{\omega {C}_1}}\end{equation}$$Furthermore, the secondary impedance Z r , the reflected impedance and the input impedance of the primary side Z in can be expressed as ZS=jωL2+1/jωC2+jXeq+ReqZR=ω2M2ZSZIN=jωLf1+1/jωCf1+1/jωL1+1/jωC1+Zr$$\begin{equation} \def\eqcellsep{&}\begin{array}{l} {Z}_S = j\omega {L}_2 + 1/j\omega {C}_2 + j{X}_{eq} + {R}_{eq}\\[9pt] {Z}_R = \dfrac{{{\omega }^2{M}^2}}{{{Z}_S}}\\[9pt] {Z}_{IN} = j\omega {L}_{f1} + 1/\left( {j\omega {C}_{f1} + 1/\left( {j\omega {L}_1 + 1/j\omega {C}_1 + {Z}_r} \right)} \right) \end{array} \end{equation}$$Substituting () into (), Z IN can be simplified as ZINbadbreak=ω2Lf12ZRgoodbreak=Lf12ZSM2$$...…”
Section: Control Scheme For Constant Voltage Chargementioning
confidence: 99%
“…In the LCC network, the compensation form is mostly T‐shaped network in order to generate a constant current I L 1 which contributes to the stabilization of secondary induced voltage; moreover, pure resistance of the input impedance can be achieved. The relationship between the resonance parameters of its components is shown as follows [30]: ωLf1badbreak=1ωCf1goodbreak=ωL1goodbreak−1ωC1$$\begin{equation}\omega {L}_{f1} = \frac{1}{{\omega {C}_{f1}}} = \omega {L}_1 - \frac{1}{{\omega {C}_1}}\end{equation}$$Furthermore, the secondary impedance Z r , the reflected impedance and the input impedance of the primary side Z in can be expressed as ZS=jωL2+1/jωC2+jXeq+ReqZR=ω2M2ZSZIN=jωLf1+1/jωCf1+1/jωL1+1/jωC1+Zr$$\begin{equation} \def\eqcellsep{&}\begin{array}{l} {Z}_S = j\omega {L}_2 + 1/j\omega {C}_2 + j{X}_{eq} + {R}_{eq}\\[9pt] {Z}_R = \dfrac{{{\omega }^2{M}^2}}{{{Z}_S}}\\[9pt] {Z}_{IN} = j\omega {L}_{f1} + 1/\left( {j\omega {C}_{f1} + 1/\left( {j\omega {L}_1 + 1/j\omega {C}_1 + {Z}_r} \right)} \right) \end{array} \end{equation}$$Substituting () into (), Z IN can be simplified as ZINbadbreak=ω2Lf12ZRgoodbreak=Lf12ZSM2$$...…”
Section: Control Scheme For Constant Voltage Chargementioning
confidence: 99%
“…As shown in [27], in the condition of 1 2 3 = =-Z Z Z , the input impedance is purely resistive when the load is resistor. Obviously in CV mode, the secondary side reflection This article has been accepted for publication in a future issue of this journal, but has not been fully edited.…”
Section: E Implementation Of Zpa In CC and Cv Modesmentioning
confidence: 99%
“…Nevertheless, the additional compensation capacitance and inductance introduced on the receiving side will inevitably increase the complexity and reduce the portability of the receiving side, which has the same shortcomings as the first method. To adapt to the principle of lightweight in the receiving side as well as fit the transfer characteristic, the authors of [27][28][29] realize the transformation of CC or CV mode by analyzing the characteristics of LCC-S by circuit equivalence. Analogously, the work by Lu et al [30][31] analyzes the features of high order topologies and summarizes some of the topologies that can implement CC and CV mode.…”
Section: Introductionmentioning
confidence: 99%
“…Thus, their resonant frequencies are irrelevant to the coupling coefficient [11]. For example, LCL, LCC-S, S-CLC, LC-S and double-sided LCC are compensation structures presented in previous articles [11][12][13][14][15]. Although all these compensations are tuned to zero voltage switching (ZVS), the coupling coil size limits the parameter of compensation elements.…”
Section: Introductionmentioning
confidence: 99%