2015 IEEE International Conference on Industrial Technology (ICIT) 2015
DOI: 10.1109/icit.2015.7125236
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Input voltage sliding mode control of the versatile buck-boost converter for photovoltaic applications

Abstract: The versatile buck-boost c interesting features, such as continuous i currents and ease of control in both step-u models. This paper addresses its use in low v applications where the nonlinear current sou characteristic of the PV module requires the in capacitor in the original power stage structure regulation of this additional input capacitor v considering a linear combination of the capa voltage error, and the integral of the volt switching function. The performance of the d that has been tested by simulati… Show more

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Cited by 6 publications
(4 citation statements)
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“…From management structure of (8), the acquisition port is (u T y) [8]. Using evaluating the rate of change energy and version of Kalman-Yakubovich-Popov lemma [21][22][23][24][25][26], we easily see that PCH model is passive because:…”
Section: Fig 2 Current and Power Versus Voltage Characteristicsmentioning
confidence: 99%
“…From management structure of (8), the acquisition port is (u T y) [8]. Using evaluating the rate of change energy and version of Kalman-Yakubovich-Popov lemma [21][22][23][24][25][26], we easily see that PCH model is passive because:…”
Section: Fig 2 Current and Power Versus Voltage Characteristicsmentioning
confidence: 99%
“…Coupled inductors can be defined and constructed in different ways. In the photovoltaic application reported in [24], the coupling coefficient is defined as k = M / L 1 L 2, where M is the mutual inductance, and L 1 and L 2 are the self‐inductances of the primary and the secondary coils, respectively. In both [24, 12], a 1:1 transformer was constructed with a pair of tightly coupled inductors of turns ratio N 1 / N 2 = 1 and a magnetising inductance L m.…”
Section: Non‐inverting Buck–boost Convertermentioning
confidence: 99%
“…In the photovoltaic application reported in [24], the coupling coefficient is defined as k = M / L 1 L 2, where M is the mutual inductance, and L 1 and L 2 are the self‐inductances of the primary and the secondary coils, respectively. In both [24, 12], a 1:1 transformer was constructed with a pair of tightly coupled inductors of turns ratio N 1 / N 2 = 1 and a magnetising inductance L m. Two identical non‐coupled inductors L a = L b were connected in series with the primary and the secondary of the transformer, where L m = M, L 1 = L a + M and L 2 = L b + M, and therefore L 1 = L 2.…”
Section: Non‐inverting Buck–boost Convertermentioning
confidence: 99%
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