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Elimination of Dead-time in PWM Controlled Inverters Lihua Chen and Fang Z. Peng ECE department, Michigan State University, East Lansing, Michigan 48824 USA Abstract- A dead-time elimination method is presented in this paper for PWM controlled inverters. In comparison to using expensive current sensors, this method precisely determines the load current direction by detecting the operating conditions of active devices and their anti-parallel diodes. A low-cost diode- conducting detection circuit is developed to measure the operating status of the anti-parallel diode. In comparison with complicated compensators, this method features with simple logic and flexible implementation. This method significantly reduces the output distortion and regains the RMS value. The principle of proposed dead-time elimination method is described. Simulation and experimental results are given to demonstrate the validity and features of the dead-time elimination method. I. INTRODUCTION To avoid shoot-though in PWM controlled voltage source inverters (VSI), dead-time, a small interval during which both the upper and lower switches in a phase leg are off, is introduced into the control of the standard VSI phase leg. However, such a blanking time can cause problems such as output waveform distortion and fundamental voltage loss in VSIs. Fig. 1 shows the dead-time effect in a voltage source inverter. The output voltage error AV, shown in figure 1 (a), caused by dead-time is depicted as: AV = tA Vd, x sgn(i,) (1) current, as well as temperature, which makes the compensation less effective, especially at low output current, low frequency, and zero current crossing. [5] proposed a new switching strategy for PWM power converters. [6] presented an IGBT gate driver circuit to eliminate the dead-time effect. [7] proposed a phase leg configuration topology which prevented shoot through. However, an additional diode in series in the phase leg increases complexity and causes more loss in the inverter. Also, this phase leg configuration is not suitable for high power inverters because the upper device gate turn off voltage is reversely clamped by a diode turn on voltage. Such a low voltage, usually less than 2 V, is not enough to ensure that a device is in off state during the activation of its complement device. In this work, an effective dead-time elimination method is proposed, which can be easily implemented in the inverter PWM controller or gate driver. The principle will be discussed first and then simulation and experimental results are provided to demonstrate the validity and features of the proposed novel method. II. PRINCIPLE OF DEAD-TIME ELIMINATION To explain the principle of the proposed dead-time elimination method, we refer to a generic phase leg of VSIs, as shown in figure 2. where tA is the dead-time interval, and T, is the carrier switching period. As a result, the effect of the dead-time on the output voltage becomes severe when the modulation index is small. Fig 1 (b) shows the output voltage waveform distortion caused by dead-time effect. VO # No dead time io<0 - , ' - v f I - I ,AV . 1 NV U%,a vu 61111 . with dead time I 07 kOg) Vref io0 1 ( a ) ( b ) Fig. 1. Dead-time effect. To overcome dead-time effects, most solutions focus on dead-time compensation [1-4] by introducing complicated PWM controller and expensive current detection hardware. In practice, the dead-time varies with the devices and output Fig. 2. A generic phase leg of VSIs. Assuming the output current flows out of the phase leg, in each switching cycle, the current comes out from the upper device when Kp is on and freewheels through diode Dn when Kp is off. Here this current direction is defined as positive. Under this condition, the generic phase leg can be equivalently expressed as a P type switching cell shown in the left figure of Fig. 3. Similarly when load current flows into the phase leg, defined as negative, the current goes into the lower device when Kn is on and freewheels through diode Dp when Kn is off. Under this condition, the generic phase leg can be equivalently expressed as a N type switching cell shown in the right figure 1-4244-0714-1/07/$20.00 C 2007 IEEE. 306

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Page 1: [IEEE PEC 07 - Twenty-Second Annual IEEE Applied Power Electronics Conference and Exposition - Anaheim, CA, USA (2007.02.25-2007.03.1)] APEC 07 - Twenty-Second Annual IEEE Applied

Elimination of Dead-time in PWM ControlledInverters

Lihua Chen and Fang Z. PengECE department, Michigan State University, East Lansing, Michigan 48824 USA

Abstract- A dead-time elimination method is presented in thispaper for PWM controlled inverters. In comparison to usingexpensive current sensors, this method precisely determines theload current direction by detecting the operating conditions ofactive devices and their anti-parallel diodes. A low-cost diode-conducting detection circuit is developed to measure the operatingstatus of the anti-parallel diode. In comparison with complicatedcompensators, this method features with simple logic and flexibleimplementation. This method significantly reduces the outputdistortion and regains the RMS value. The principle of proposeddead-time elimination method is described. Simulation andexperimental results are given to demonstrate the validity andfeatures of the dead-time elimination method.

I. INTRODUCTION

To avoid shoot-though in PWM controlled voltage sourceinverters (VSI), dead-time, a small interval during which boththe upper and lower switches in a phase leg are off, isintroduced into the control of the standard VSI phase leg.However, such a blanking time can cause problems such asoutput waveform distortion and fundamental voltage loss inVSIs.

Fig. 1 shows the dead-time effect in a voltage source inverter.The output voltage error AV, shown in figure 1 (a), caused bydead-time is depicted as:

AV = tA Vd, x sgn(i,) (1)

current, as well as temperature, which makes the compensationless effective, especially at low output current, low frequency,and zero current crossing. [5] proposed a new switchingstrategy for PWM power converters. [6] presented an IGBTgate driver circuit to eliminate the dead-time effect. [7]proposed a phase leg configuration topology which preventedshoot through. However, an additional diode in series in thephase leg increases complexity and causes more loss in theinverter. Also, this phase leg configuration is not suitable forhigh power inverters because the upper device gate turn offvoltage is reversely clamped by a diode turn on voltage. Such alow voltage, usually less than 2 V, is not enough to ensure thata device is in off state during the activation of its complementdevice.

In this work, an effective dead-time elimination method isproposed, which can be easily implemented in the inverterPWM controller or gate driver. The principle will be discussedfirst and then simulation and experimental results are providedto demonstrate the validity and features of the proposed novelmethod.

II. PRINCIPLE OF DEAD-TIME ELIMINATION

To explain the principle of the proposed dead-timeelimination method, we refer to a generic phase leg of VSIs, asshown in figure 2.

where tA is the dead-time interval, and T, is the carrierswitching period. As a result, the effect of the dead-time on theoutput voltage becomes severe when the modulation index issmall. Fig 1 (b) shows the output voltage waveform distortioncaused by dead-time effect.

VO # No dead time

io<0

- , ' - v f I -I ,AV.

1NV U%,avu 61111

. with dead time

I 07

kOg)

Vref

io0 1

( a ) ( b )

Fig. 1. Dead-time effect.To overcome dead-time effects, most solutions focus on

dead-time compensation [1-4] by introducing complicatedPWM controller and expensive current detection hardware. Inpractice, the dead-time varies with the devices and output

Fig. 2. A generic phase leg of VSIs.

Assuming the output current flows out of the phase leg, ineach switching cycle, the current comes out from the upperdevice when Kp is on and freewheels through diode Dn whenKp is off. Here this current direction is defined as positive.Under this condition, the generic phase leg can be equivalentlyexpressed as a P type switching cell shown in the left figure ofFig. 3. Similarly when load current flows into the phase leg,defined as negative, the current goes into the lower devicewhen Kn is on and freewheels through diode Dp when Kn is off.Under this condition, the generic phase leg can be equivalentlyexpressed as a N type switching cell shown in the right figure

1-4244-0714-1/07/$20.00 C 2007 IEEE. 306

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of Fig. 3. Actually a generic phase leg is a combination of oneP switch cell and one N switch cell. There is no question thatdead-time is not required for either a P switch cell or a Nswitch cell because both cells are configured with acontrollable switch in series with a uncontrollable diode.

KpXZ Dp

iL iL

ZiDn KnX,

diode, DI, is on, in which V,e is negative, the comparator U1output is low. As a result, a current flows through the LED Doand causes it to light up. This signal will be level shifted ortransferred through optic-electrical interface circuit. On theother hand, when the anti-parallel diode is off, the LED Do willbe turned off.

Fig. 5. Diode-conducting detection circuit.P Switch Cell N Switch Cell

Fig. 3. Equivalent switch cells.

The control scheme for a generic phase leg can be illustratedin figure 4. Only one gate control signal is needed for eachphase leg. When the output current is positive, the gate controlsignal is selected to gate-on and gate-off upper device, Kp,only. When the output current is negative, the gate controlsignal will be inverted and used for manipulating lower device,Kn. The control scheme can be mathematically described aslogic functions as follows:

SP = S * sgn(iL)

Sn = s * sgn(iL)

S~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

Sgn (i0)

s~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~SIn

I'

ti!Fig. 4. Dead-time elimination control schemes.

III. SIMULATION RESULTS

To validate the proposed dead-time elimination method, anH-bridge inverter shown in Fig. 6 has been simulated usingSaber software. The load is composed of an 8 mH inductor anda 2.4 ohm resistor. Vd, is set to 250 V and the inverter iscontrolled by unipolar sinusoidal PWM with switchingfrequency 10 kHz. The fundamental frequency of the outputvoltage is set to 60 Hz.

(2)

(3)

As analyzed above, the determination of load currentdirection is key for dead-time elimination. Contrary to using anexpensive current sensor, the load current direction can beprecisely determined by the operating status of switches andtheir anti-parallel diodes. For example, in a generic phase leg,if switch Kp is on or diode Dn is on, the load current flows outfrom phase leg. Analogously the load current flows into phaseleg if either switch Kn or diode Dp is on. In implementation, theoperating status of a switch can be easily determined bymeasuring its gate signal level if its activation delay isnegligible. A diode-conducting detection (DCD) circuit shownin figure 5 is used to determine the anti-parallel diodeoperating status. As shown in Fig. 5, when the anti-parallel

Db,

Fig. 6. H-bridge voltage source inverter.

Fig. 7 shows the output current waveforms when themodulation index is 0.2. The dark brown curve is the outputcurrent with a dead-time of 2 usec, and the blue curve is theoutput current with the proposed dead-time elimination method.The dark brown curve shows a notable distortion, however, theblue curve is pure sinusoidal. It shows that the dead-time effecthas been minimized when the proposed method is used. TheRMS value of output current is only 8.82 A when there is a 2usec dead-time. However, after the dead-time elimination, theoutput current RMS value increases to 6.99 A.Table 1 gives a comparison of output current RMS value and

THD for case 1: with 2 usec dead-time, and case 2: with theproposed dead-time elimination method. The results show that,in case 2, the output current THD has been significantlyreduced, and the desired RMS value has been achieved.

307

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20

;~0

RMS.888236

With dead-time No dead-time

70 75 80 85 90 95Time [ins]

Fig. 7. Simulated output current waveforms with MI=0.2

Table 1. Comparison of output current for case 1: 2 usec dead-time, and case 2:

with proposed method.

Modulation '0 (RMS) (A) I 0 (%THD)Index 2 usec Dead time 2 usec Dead time

dead eliminated dead eliminatedtime time

0.1 2.0 4.24 20.5% 1.8%

0.2 6.94 8.83 6.16% 1.03%

0.4 16.33 18 2.66% 0.63%

0.8 34.8 36.3 1.26% 0.32%

1.0 43.95 45.5 0.99% 0.23%

IV. IMPLEMENTATION METHODS AND TEST RESULTS

To validate the proposed dead-time elimination method, anH-bridge inverter, shown in figure 6, and its gate drivers havebeen built and tested. Two Powerex IGBT modules(CM300DY-1 2H) have been chosen to configure this H-bridgeinverter, and the load is composed of an 8 mH inductor and a2.4 ohms resistor, which are exactly the values used forsimulation in section 2.

POS

PWMWith nodeadtime

-Sb P

NEG

Fig. 8. Test circuit block diagram.

Fig. 8 shows the test circuit configuration. Four DCDcircuits are employed to detect the anti-parallel diodes, Dap, Dan,Dbp, and Dbn, operating condition, and their output signals, Cap,Can, Cbp, and Cbn, are fed back to a complex programmable

logic device (CPLD). The digital signal processor (DSP),TMS320LF2407A, only sends two PWM signals, Sa and Sb, tothe CPLD; The control logic is implemented within the CPLDwith hardware description language (HDL). The level shift forDCD circuit outputs and gate signals are achieved by anelectrical-optic-electrical method implemented with opticalfibers.The test conditions are the same as those used for simulation.

Fig. 9 through Fig. 11I show the test results with the modulationindex of 0.2. In all three figures, ch4 is the output currentwaveform with 5AIdiv. logic signal AO though A7 are Cap, Ca,,Cbp, Cbn, Sap~San, Sbp~Sbn, respectively. It should be noted herethat all logic levels are negative, in which logic low means theanti-parallel diode is conducting or the switch is gated on.Figure 9 is the test results with the proposed dead-timeelimination method. It clearly shows that the output current isvery close to a sinusoidal waveform. The anti-parallel diodeoperating conditions are effectively detected as shown in AOthrough A3. When io is positive, switches Kan and Kbp are alwayoff. Switches Kap and Kbn are always off if io is negative. As acomparison, standard PWM control with 2 usec dead-time isalso tested and the results are shown in figure 10. It is obviousthat the output current has a reduced RMS value and notabledistortion.

; mrn"alzown/ s A;iso

/.,5AIdilv

Fig. 9. Experimental waveform using the proposed method.

Figure I1I shows the waveforms at a small time scale whenthe output current crosses zero. When i, is negative, diodes,Dap and Dbn, conduct current in each switching cycle. Logicsignals, A0 and A3, are the measurement results of the operatingstatus of diodes Dap and Dbn. Logic signals, A5 and A6, are gatesignals to control switches Kan and Kbp, respectively. Theswitches Kap and Kbn are always forced off. Analogoussituation applied to the condition when output current isnegative. Fig . I1I shows that during the process of load currentdirection change, the gate control signals, Sap, San, Sbp, and Sbn,divert smoothly.

In practice, the DCD circuit has a measurement dead zone.When the load current is extremely small, the operatingcondition of both anti-parallel diodes in a phase leg can not be

308

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Page 4: [IEEE PEC 07 - Twenty-Second Annual IEEE Applied Power Electronics Conference and Exposition - Anaheim, CA, USA (2007.02.25-2007.03.1)] APEC 07 - Twenty-Second Annual IEEE Applied

effectively detected. During which, a very limited delay (0.8usec) is applied to the gate signals. This delay has a negligibleeffect on the output waveforms, and that is confirmed as shownin the output current waveform in figure 9.

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Fig. 1u. Experimental waveform with dead-time effect.

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ipha ele ge t d w th n aCL.The lride po nedit will-t be

detected and fed to both upper and lower gate drivers. The

control scheme will be implemented within gate driver logic

circuit. In addition, the dead-time elimination method can be

implemented within a PWM controller, contained in the DSP

software.

In this paper, a method was proposed to eliminate dead-

time in the PWM controlled inverters. Compared to the

conventional PWM control with dead-time, this method

significantly reduces the output distortion and regains the RMS

value. Compared to using expensive current sensors and

complicated compensators, the low-cost DCD circuit, simple

logic and flexible implementation make it an attractive option

for VSI applications.

REFERENCES

[1]. L. Ben-Brahim, "On the compensation of dead time and zero-current

crossing for a PWM-inverter-controlled AC servo drive" IEEE

Transaction on Industrial Electronics, Volume 51, Issue 5, Oct. 2004

Page(s):1II13 -1118.

[2]. A. Cichowski, J. Nieznanski, "Self-tuning dead-time compensation

method for voltage-source inverters", IEEE Power Electronics Letters,

Volume 3, Issue 2, June 2005 Page(s):72 -75.

[3]. Y. Lai; F. Shyu, "Optimal common-mode Voltage reduction PWM

technique for inverter control with consideration of the dead-time effects-

part I: basic development", IEEE Transactions on Industry Applications,

Volume 40, Issue 6, Nov.-Dec. 2004 Page(s):1605- 1612.

[4]. A. R. Munoz, T.A. Lipo, "On-line dead-time compensation technique for

open-loop PWM-VSI drives", IEEE Transactions on Power Electronics,

Volume 14, Issue 4, July 1999 Page(s):683- 689.[5]. K. M. Cho; W. S. OH; C. G. In, "A new switching strategy for PWM

power converters" Power Electronics Specialists Conference, 23-27 June

2002 Page(s):221- 225 vol.1

[6]. B. Zhang; A.Q. Huang; B. Chen, "A novel IGBT gate driver to eliminate

the dead-time effect", Fourtieth IAS Annual Meeting, 2-6 Oct. 2005,

Page(s):913 -917 Vol. 2.

[7]. S. Park, T.M. Jahns, "A novel dead-time elimination methiod using

single-input enhanced phase-leg configuration", 38th IAS Annual

Meeting, 12 16 Oct. 2003 Page(s):2033- 2040 vol.3.

309

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