Inverters Dr John Fletcher.

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Presentation transcript:

Inverters Dr John Fletcher

Basics Inverters are DC to AC converters We can use inverters to generate A dc supply Single-phase AC supply Three-phase AC supply from a single dc source. The basic building block is the inverter ‘leg’. An inverter leg is shown. Vdc is the input, Vout the output.

Inverter switching T1 and T2 are NEVER turned on together. Why? T1 and T2 are switched using PWM in a complementary manner (T2 ON, T1 OFF) Vout is then a switched waveform, just like the basic step-down converter earlier.

Pulse-width Modulation T1,on T2,on

Current Paths Current path if T2 ON, or T1 and T2 OFF Two switches with freewheel diodes provides uni-directional voltage and bi-directional current control. Only when T1 is ON is energy supplied from the source. When T2 ON, a zero voltage loop is applied. With positive current flow → Current path if T2 ON, or T1 and T2 OFF Current path if T1 ON

Current Paths When T1 is ON (or T1 and T2 OFF) energy has to be absorbed by the source. When T2 ON, a zero voltage loop is applied. With negative current flow → Current path if T2 ON Current path if T1 ON, or T1 and T2 OFF

Bridge Leg V-I graph The basic bridge leg can operate in two quadrants of the VI graph. I V

Average Output Voltage A single inverter leg produces an average output voltage: Define a duty cycle or modulation index Hence m must be between 0 and 1. We can make m vary in time therefore we can produce any voltage and any frequency we desire (within the bounds fixed by the switching frequency and Vdc).

Switching Frequency Switch frequency (1/Ts) of the pulse-width modulated (PWM) signal is usually chosen as high as possible to reduce current ripple in the load. Max switching frequency is limited by losses and the ability to manage those device losses (remember lecture 2?) In low power circuits, switching frequency can be as high as ~1 MHz High power circuits (say >500kW) may use frequencies of 1kHz or less.

Single-phase H-bridge Two inverter legs connected in parallel.

Single-phase H-bridge From previous discussion on inverter legs So the average output voltage applied to the load For a sinusoidal output (ma-mb) must vary sinusoidally.

Single-phase H-bridge The modulation indices of both inverter legs vary sinusoidally in time with a modulation depth, m (0<m<0.5) and an offset. If we apply (2) and (3) to (1) we get That is, the modulation depth, m, sets the magnitude of the ac output voltage and ωt sets the frequency. Notice that the dc offset in the modulation indices is co-phasal and does not appear in the output voltage. We can control the magnitude and frequency.

H-Bridge V-I graph The H-bridge can operate in all four quadrants of the VI graph. It can generate both polarities of voltage and control both polarities of current. I V

PWM Generation Ts t1 t2 (t1-t2)/2 Ts/2 m1 m2 Vload Leg 1 output Leg 2 output Carrier waveform Modulation indices of each leg are compared with a triangular carrier waveform. Intersects define the turn-on and turn-off instant of each bridge leg. With this scheme load sees two output voltage pulses per switching cycle. Harmonic spectrum of the applied voltage has components around multiples of the switching frequency.

Three-phase inverters Now if:

Three-phase inverters Inserting modulation indices into (1-3) gives: Three-phase output voltages The circuit is a pulse-width modulated voltage source inverter (VSI).

Six-step Operation The previous section looked at pulse-width modulated VSIs. PWM VSIs can be used at all but very high power drives. For high-power drives, often the switches are turned ON and OFF once during one fundamental cycle rather than many 100s of times with PWM. The output voltage waveform is then ‘square wave’.

Six-step Line Voltages Line voltages are stepped Fourier analysis of output voltages gives and line voltages and phase voltage

Six-step Inverter Currents Inverter currents are obviously non-sinusoidal. (Note: this load is inductive) Result from the harmonic voltages in the output line voltage. Harmonic currents causes additional loss components. And also torque ripple if the load is a machine.