2014 IEEE 36th International Telecommunications Energy Conference (INTELEC) 2014
DOI: 10.1109/intlec.2014.6972179
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Steady-state analysis of the bidirectional CLLLC resonant converter in time domain

Abstract: In this paper, the operating modes of the bidirectional CLLLC resonant converter are analyzed in time domain to determine the steady-state operating point. The operating mode boundaries, mode transitions and mode distribution are discussed and the dependencies of modes on voltage transfer ratio, inductor ratio and switching frequency are illustrated. Based on the mode analysis results, normalized equations and characteristics for the resonant tank currents and voltages are presented, which support the designer… Show more

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Cited by 15 publications
(7 citation statements)
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References 16 publications
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“…For obtaining the voltage gain and its relationship with respect to frequency, the fundamental harmonic approximation method (FHA) [19] was used to build the equivalent circuit model of the forward charging mode as illustrated in Figure 7 [20]. Here, V DC_Grid_FHA is the fundamental component of the square voltage waveform at the primary side.…”
Section: Equivalent Circuit and Mathematic Formulationmentioning
confidence: 99%
“…For obtaining the voltage gain and its relationship with respect to frequency, the fundamental harmonic approximation method (FHA) [19] was used to build the equivalent circuit model of the forward charging mode as illustrated in Figure 7 [20]. Here, V DC_Grid_FHA is the fundamental component of the square voltage waveform at the primary side.…”
Section: Equivalent Circuit and Mathematic Formulationmentioning
confidence: 99%
“…4) as this will be important for the following discussion. For a more detailed description please refer to [16] for the LLC and to [17] for the CLLLC topology. Within one C add =0pF…”
Section: A Subintervals and Operating Modesmentioning
confidence: 99%
“…The step-up operation mode at f sw = 85 kHz for the SiC SBD in Fig. 5(a) starts with the power transferring subinterval P at t = t 0 and is followed by subinterval N at t = t 1 , in which the power transfer to the secondary side diminishes and energy is stored in the resonant tank [17]. The rising edge of v sec is very steep due to the very small diode junction capacitance and thus the state of the output rectifier abruptly changes.…”
Section: B New Subinterval D In Step-up Operation Modementioning
confidence: 99%
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