Section 2
Six step inverter → switching action occurs every 60°.
180° Conduction → each switch conduct for 180°.
Three switches (not on the same leg) are “on” at the same time, so the input
3
resistance with respect to supply is always R.
2
Vdc 2Vdc
Idc = = (supply/ input current)
3R⁄2 3R
Output:
2π
1 2
▪ VL = √ ∫03 vdc
2
dωt = √ vdc
π 3
VL √2
▪ Vph = = Vdc
√3 3
Vph √2
▪ IL = Iph = = vdc (star connected load)
R 3R
2 2V2dc
▪ Po = 3 Iph R=
3R
Switches ratings:
It works the same way for the other switches: when the switch is on, the current from
the connected phase flows through it and is positive. When it is off, the voltage across
it matches the supply voltage.
▪ Peak Inverse Voltage (PIV) = Vdc
Iph Vdc
▪ ISW,(rms) = =
√2 3R
1 π vdc 2 vdc vdc 2 vdc
▪ ISW,(avg) = ( + + )=
2π 6 3R 3R 3R 9R
vdc vdc 2 vdc
▪ ISW,(max) = Idc = = 3 =
Rin R 3R
2
Fourier expression:
Voltage:
4 vdc π π
▪ Vab = ∑∞
n ( cos (n )) sin (n(wt + ))
nπ 6 6
n=1,5,7,11 …etc.
Odd non triple-n harmonics. Then the LOH is 5th.
4 vdc π
▪ Van = ∑∞
n ( cos (n )) sin(nwt)
nπ√ 3 6
√V2L,rms −V21,rms
Vharmonics
▪ THD = =
V1,rms V1,rms
2 4 Vdc π √6
∵ VL.rms = √ Vdc , VL1,rms = ( cos ( )) = Vdc
3 π √ 2 6 π
2
2
VL.rms 2
− VL1,rms (√ vdc )2
3
∴ THD𝑣 = √ 2 =√ − 1 = 𝟑𝟏%
VL1,rms √6
( π vdc )2
Current
4 vdc π
i o = ∑∞
n ( cos (n )) sin(n(wt − θn ))
n π√3 Zn 6
where: - Zn = √R2 + (nωL)2 the load impedance at harmonic (n)
nωL
θn = tan−1 ( ).
R
√ ∑∞
n (Io n,rms )
2
THDi =
Io1,rms