TIDUFB1 December 2024
Input inductor (Li) filters out the switching frequency harmonics. Inductor design, amongst other factors, depends on calculation of the current ripple and choosing a material for the core that can tolerate the calculated current ripple. Figure 2-7 shows one switching cycle waveform of the inverter output voltage vi with respect to the inductor current.
Figure 2-7 Current Ripple
CalculationThe voltage across the inductor is given by V = Li(di/dt). For the Vienna rectifier, see Equation 7.
where
For control design, D is assumed to be the voltage at the other terminal of the inductor and is related to D’ by D’ = 1 – D. Rearranging the current ripple at any instant in the AC waveform is given as Equation 8.
Now assuming modulation index to be ma the duty cycle can be given as D' = ma*sin(ωt) and assuming that Vin = D' × (Vbus/2), Equation 9 can be derived.
From Equation 9, it is clear that the peak ripple is a factor where the input AC is in the sinusoidal waveform.
To get the maximum value differentiating the equation with respect to time, use Equation 10.
Which gives the maximum ripple exists at sin(ωt)=1/(2 × ma), Substituting this value, Equation 11 is derived.
With these values in mind, an appropriate core can be selected along with an inductor designed to meet this inductance value.