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Switch states of three-phase VSI, 180° mode

Short answer

In 180° conduction, three switches are on at any time and firing order is S1,S2,...,S6 every 60°. The phase voltage is a six-step wave with levels Vdc/3, 2Vdc/3, -Vdc/3, -2Vdc/3; each switch conducts 180°.

Obtain the switch states for three phase VSI of 180 degree conduction mode. Draw the waveform of output phase voltages of same inverter showing suitable modes of operation.

In a three-phase VSI with 180° conduction, each switch conducts for half a cycle, the two switches of a leg are complementary, and three switches (one per leg) are ON at any time. Gate signals are given in the order S1, S2, …, S6 every 60°, giving six switch states (modes) per cycle.

Circuit

     +-----+--------+--------+
     |     |        |        |
     |    S1 D1    S3 D3    S5 D5
    Vdc    |        |        |
     |     +--a     +--b     +--c
     |     |        |        |
     |    S4 D4    S6 D6    S2 D2
     |     |        |        |
     +-----+--------+--------+
      a, b, c -> star load (R per phase)

Switch states

Let the switching function of a leg be 1 when its upper switch is ON (phase on +Vdc+V_{dc}) and 0 when its lower switch is ON.

Modeωt\omega tON switchesState (a b c)vanv_{an}vbnv_{bn}vcnv_{cn}
10–60°S5, S6, S11 0 1V/3V/3−2V/3-2V/3V/3V/3
260–120°S6, S1, S21 0 02V/32V/3−V/3-V/3−V/3-V/3
3120–180°S1, S2, S31 1 0V/3V/3V/3V/3−2V/3-2V/3
4180–240°S2, S3, S40 1 0−V/3-V/32V/32V/3−V/3-V/3
5240–300°S3, S4, S50 1 1−2V/3-2V/3V/3V/3V/3V/3
6300–360°S4, S5, S60 0 1−V/3-V/3−V/3-V/32V/32V/3

(V=VdcV = V_{dc}.) The states 000 and 111 (zero states) are not used in six-step operation.

Phase voltage in a mode (star resistive load)

Mode 1: a and c are connected to +V+V, and b to the negative bus. Equivalent circuit: R∥R=R/2R\parallel R = R/2 in series with RR:

ib=VR/2+R=2V3R,vbn=−ibR=−2V3,van=vcn=V3i_b = \frac{V}{R/2 + R} = \frac{2V}{3R}, \quad v_{bn} = -i_bR = -\frac{2V}{3}, \quad v_{an} = v_{cn} = \frac{V}{3}

Mode 2: only a is on the positive bus; b and c are in parallel on the negative bus, giving van=2V/3v_{an} = 2V/3, vbn=vcn=−V/3v_{bn} = v_{cn} = -V/3. The other modes follow in the same way. In general, using the pole voltages vaOv_{aO}, vbOv_{bO}, vcOv_{cO} (±V/2\pm V/2):

van=2vaO−vbO−vcO3v_{an} = \frac{2v_{aO} - v_{bO} - v_{cO}}{3}

Phase voltage waveforms

 mode       1    2    3    4    5    6
 wt       0    60   120  180  240  300  360
 van 2V/3       ____
      V/3 _____|    |____
        0                |
     -V/3                |____      ____
    -2V/3                     |____|
 vbn 2V/3                 ____
      V/3            ____|    |____
        0           |              |
     -V/3       ____|              |____
    -2V/3 _____|
 vcn 2V/3                           ____
      V/3 _____                ____|
        0      |              |
     -V/3      |____      ____|
    -2V/3           |____|

Each phase voltage is a six-step wave (V/3V/3, 2V/32V/3, V/3V/3, −V/3-V/3, −2V/3-2V/3, −V/3-V/3), and vbnv_{bn} and vcnv_{cn} lag vanv_{an} by 120° and 240°.

Results: Vph,rms=23Vdc=0.471VdcV_{ph,rms} = \frac{\sqrt2}{3}V_{dc} = 0.471V_{dc}; fundamental peak =2Vdcπ= \frac{2V_{dc}}{\pi}; no triplen harmonics.

✓ Answer checked by Claude Opus 5.5 (high effort)

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