Three-phase Transformerless Grid Connected Quasi Z-Source Inverter for Solar Photovoltaic Systems with Minimal Leakage Current Yam P. Siwakoti (PhD Student) Supervisor: Prof. Graham E. Town Department of Electronic Engineering, Macquarie University, NSW 2109 Australia 1 Overview Introduction of Grid Connected Inverter Transformerless System-Pros & Cons Modulation Technique Transformerless Quasi Z-Source Inverter Analysis of Common Mode Voltage Result and Discussion 2 Introduction: Grid Connected Inverter for PV Power Generated by the PV panel (1) is connected to the grid (4) via the grid connected inverter (2) and an energy meter (3). Grid Connected PV system should comply with the specific standards which are regulated by electrical utility. Total Harmonic Distortion (THD) of current Power Factor (PF) Leakage current and DC current injection Voltage/Phase/Frequency Islanding Operation Grounding Different International Standards: IEEE1547, VDE-0126-1-1, IEC61727, AS4777.2 Fig: Grid Connected Solar PV System 3 Introduction: Classification of GCI Grid Connected Inverters are classified into two catagories based on the electrical isolation between the PV panels and the utility grid Grid Connected Inverter Galvanic Isolation Without Galvanic Isolation With Transformer Transformerless Low Frequency Transformer High Frequency Transformer Fig: Classification of GCI 4 Introduction: Pros &Cons of Transformerless system Increase Efficiency (+2%) Reduced Size Advantages Reduced Weight Reduce Cost The galvanic isolation between the PV generator and the grid is lost. Leakage currents (common-mode currents) through the stray capacitance (Cp) between the PV array and the ground. Disadvantages Inverter could inject direct current (DC) to the grid saturate distribution transformer. Corrosion in the underground equipment Malfunction of CT and PT due to saturation 5 Introduction: Parasitic Capacitance and Leakage Current Electrical Grid Parasitic Capacitance formed between panels and metallic frame (50nF/kW-150nF/kW). Parasitic capacitance depends on: Surface area of PV array and ground frame Dust, humidity and salt cover Atmospheric conditions Transformerless Inverter Cpg Leakage Circulating Current Fig: Leakage current path Series resonant circuit consisting of Cpg, the PV generator, filtering elements and ground resistance (Rg). If the switching frequency of the inverter is close to the resonant frequency of the series circuit then large leakage current flows through the ground. Leakage current cause severe EMI (conducted and radiated), grid current distortion, and additional losses in the system and potential hazard to humans. The amplitude of the leakage current must be limited to within safe limits when connected to grid. 6 Leakage Current and Common Mode Voltage The value of leakage current depends on the amplitude and frequency content of the voltage fluctuations and Cpg. The modulation technique used in the inverter is the most dominant factor in determining the common mode voltage and leakage currents. The common mode voltage for three phase system is defined as: VRO P vCMV R = v vYN v BN RN 3 VYO Y 3 ̴ VBO O B N Grid Fig: Common mode voltage of 3-ph System 7 Leakage Current and Common Mode Voltage German national standard VDE DIN 0126-1-1 is taken into consideration because it is the most comprehensive standard in the field of solar electricity. Leakage Current <300mA for fire safety & <30mA for human safety Leakage currents should never be greater than 300 mA. German Standard VDE0126-1-1 In case of leakage currents higher than 300 mA, the system should shut-off in 0.3 seconds. Residual Current Monitoring Unit (RCMU) is used to detect the abnormal current. Table: An instantaneous current and disconnection time RMS Leakage Current Jump Value [mA] Disconnection Time [s] 30 0.3 60 0.15 100 0.04 8 Space Vector Pulse Width Modulation Technique SVPWM is a modulation technique for 3-Ф inverters. Total eight switching state: 6-Active States & 2-Zero states Duty-cycles of switch are computed from the selected switching state vectors out of eight possible switching vectors. The main advantage of SVPWM is the flexibility to choose space vectors and their placement in the switching cycle to achieve required performance specifications for the inverter with minimum switching transitions. Vq V3 (010) V1 (100) V2 (110) Vref V4 (011) V0 (000) V7 (111) V5 (001) α° V1 (100) R Vd Y B V6 (101) SVPWM V1 application 9 Transformerless Quasi Z-Source Inverter Quasi Z-Source Inverter is suitable for grid connected generation, specially Solar PV distributed Buck-Boost capability (Changing the modulation index (m) and shoot-through time period Tst) Single stage power conversion improve power conversion efficiency and reliability Continuous and constant current drawn from source Less stress on switching components C2 P + Cp L1 = L2 Grid D1 S1 Rg PV Array S3 R Uin Y C1 Rg Cp S5 S2 _ N S4 B S6 Filter VRO Lf VYO Lf VBO O Lf Ileakage Fig: 3-Ф transformerless Quasi Z-Source Inverter for grid connected PV System. Potential leakage current paths are shown as dotted lines. 10 Common Mode Voltage Analysis … R Common Mode Voltage Analysis during (T1-Tst/3)/2 (T3-Tst/3)/2 (T5-Tst/3)/2 For Even Vector (V2,V4,V6): e.g. for V2(110) v v vBN BU in BU in 0 2 BU in RN YN 3 3 3 iC2 C2 iL For Zero Vector V7(111) Cp + Rg + PV Array Uin For Zero Vector V0(000) vCMV vNo VL1 - D1 iL2 + VL2 - + + C1 iC1 iIN R/Y/B for odd & RY/YB/BR for even L2 iD1 _ Rg N BU in BU in BU in BU in 3 L1 P Cp vCMV v No + (T5-Tst/3)/2 (T3-Tst/3)/2 (T1-Tst/3)/2 Tz v v v BU in 0 0 BU in v No RN YN BN 3 3 3 vCMV vNo -V Tst/2 C2 Tst/2 For Odd Vector (V1,V3,V5): e.g. for V1(100) vCMV R V1 V3 V5 Vst Vst V5 V3 V1 (101) (101) (001) (010) (100) Active (100) and(010) Zero(001) State VC1 B*Uin _ _ YB/BR/RY for odd & B/R/Y for even Fig: Equivalent circuits of the q-ZSI during active and zero state vRN vYN vBN 0 0 0 0 3 3 where, B 1 21 Tst Tz 11 Common Mode Voltage Analysis … Common Mode Voltage Analysis during Shoot-through State In the shoot-through mode the upper and lower switch are turned on at the same time to store energy in inductors (L1 and L2) and capacitors (C1 and C2) for voltage boost. (T6-Tst/3)/2 (T2-Tst/3)/2 (T4-Tst/3)/2 Tst/2 Tst/2 (T4-Tst/3)/2 (T2-Tst/3)/2 (T6-Tst/3)/2 Tz is zero. Diode D1 is open circuited in this mode and the DC link voltage - VC2 (Vst ), k {R,Y,B,RY,YB,BR,RYB} + k iL vRN vYN vBN 000 0 3 3 L1 P Cp + Rg + PV Array Uin During Shoot-through: vCMV v No iC2 C2 VL2 L2 - - UD1 + C1 iC1 Cp + R/Y/B VL2 - + _ Rg iL2 VC1 _ iIN N R/Y/B Fig: Equivalent circuits of the q-ZSI during Shoot-through state 12 Vcmv for different space vectors Space Vector Odd (V1,V3,V5) Even (V2,V4,V6) VCMV BU in 3 2 BU in 3 1) VCMV for odd vector is 50 % less than for even vector. 2) VCMV=0 during Tst . 3) No need to have extra circuitry to block/isolate the leakage current during Tst 4) Increase the efficiency and reliability of the Zero (V0) 0 system. 5) Careful selection of the switching pattern Zero (V7) BUin and voltage vector for inverter switching reduce the VCMV and corresponding leakage current. Vst (all) 0 13 Odd SVPWM Modulation Technique Vq Odd Space Vector Pulse Width Modulation technique V3 (010) is used to reduce the leakage current of q-ZSI I A Single leg shoot-through vector (Vst ), k {R,Y,B} Vref α° II k III V1 (100) Vd is adopted here to reduce the number of switching V5 (001) states and corresponding switching loss. Fig: Odd Voltage Space Vector The time duration of each vector (T1,T3,T5) for six switches are calculated in terms of a reference voltage angle (α), switching time period (Tz), input voltage (Uin) and shoot through time period (Tst). T1 TZ TZ Vref 3 U in cos( ) T3 3TZ Vref TZ TZ Vref cos( ) 3 2U in 2U in sin( ) T5 3TZ Vref TZ TZ Vref cos( ) 3 2U in 2U in sin( ) 14 Odd SVPWM Modulation Technique… Shoot-through state is introduced in each sector along with the active vector dwell time for voltage gain at the output. The effective dwell time is then, T Ti eff Ti st , i ∈{1,3,5} 3 [s1] VAref V/_0 Vd VBref V/_120 Sa [s2] Sast [s3] Sb [s4] Sbst [s5] Sc [s6] Vref f(u) S3 S5 R Y B f(u) Alpha Vq VCref V/_240 S1 Cartesian to Polar Odd_SVPWM S2 S4 S6 Vtr Repeating Sequence1 2 B Scst Boost Factor Embedded MATLAB Function Fig. Matlab Simulink model of Odd SVPWM Generation 15 Switching Pattern and Vcmv Shoot-through State RUP RDOWN V1 (100) YUP YDOWN BUP R BDOWN Y B (B/3)Uin Vcmv R R V1 V3 V5 Vst Vst V5 V3 V1 (100) (010) (001) (101) (101) (001) (010) (100) (T1-Tst/3)/2 (T3-Tst/3)/2 (T5-Tst/3)/2 Tst/2 Tst/2 (T5-Tst/3)/2 (T3-Tst/3)/2 (T1-Tst/3)/2 Tz Fig: Sector-I switching pattern and vCMV of q-ZSI for odd SVPWM 16 Results and Discussion 400 Vrms=242V 300 Output Voltage (Vo) [V] 200 100 0 -100 -200 -300 -400 0.8 0.82 0.84 0.86 0.88 0.9 Simulation time [s] 0.92 0.94 0.96 0.98 1 1.5 Irms=0.94A Load Current (Io) [A] 1 0.5 0 -0.5 -1 -1.5 0.8 0.82 0.84 0.86 0.88 0.9 Simulation time [s] 0.92 0.94 0.96 0.98 1 Fig: Output voltage and load current of Transformerless q-ZSI 17 Fundamental = 341.8 Vpeak (241.7 Vrms) Total Harmonic Distortion (THD) = 0.62% Mag (% of Fundamental) Fundamental (60Hz) = 341.8 , THD= 0.62% 0.4 0.3 0.2 0.1 0 0 20 40 60 80 100 Frequency (Hz) 120 140 160 180 200 0.6 0.4 0.2 0 0 20 40 60 80 100 Frequency (Hz) 120 140 0 Hz (DC): 0.06% 60 Hz (Fnd): 100.00% 120 Hz (h2): 0.45% 180 Hz (h3): 0.01% 240 Hz (h4): 0.27% Fundamental = 1.315 Ipeak (0.93 Irms) Total Harmonic Distortion (THD) = 0.67% Fundamental (60Hz) = 1.315 , THD= 0.67% 0.8 Mag (% of Fundamental) Load Current Harmonics Output Voltage Harmonics Results and Discussion… 160 180 200 0 Hz (DC): 0.04% 60 Hz (Fnd): 100.00% 120 Hz (h2): 0.52% 180 Hz (h3): 0.02% 240 Hz (h4): 0.27% Fig: Harmonic analysis of transformerless q-ZSI 18 Results and Discussion… Common Mode Voltage (Vcmv) [V] 400 350 Vcmv, peak = 172V Vcmv, RMS = 64V 300 Common Mode Voltage (Vcmv) [V] 200 Peak Value of Vcmv 180 RMS value of Vcmv 160 140 120 100 80 60 40 20 0 0.998 0.9982 0.9984 0.9986 0.9988 0.999 0.9992 0.9994 0.9996 0.9998 1 Simulation time [s] 250 200 150 100 50 0 0 0.1 0.2 0.3 0.4 0.5 Simulation time [s] 0.6 0.7 0.8 0.9 1 Fig: Common mode voltage of transformerless q-ZSI 19 Results and Discussion… Fig: Leakage current of transformerless q-ZSI 0.1 0.05 0 -0.05 -0.1 0 0.02 0.1 0.2 0.3 Leakage Current (Il) [A] Leakage Current (Il) [A] I leakage, peak = 10mA I leakage, RMS = 5mA 0.01 0.4 0 0.5 0.6 Simulation time [s] 0.7 0.8 0.9 1 -0.01 -0.02 0.999 0.9991 0.9992 0.9993 0.9994 0.9995 0.9996 Simulation time [s] 0.9997 0.9998 0.9999 1 20 Conclusions • Odd Space Vector Pulse Width Modulation Technique is effective in reducing the common mode voltage and leakage current of q-ZSI. • Boost capability of q-ZSI is maintained by applying single leg shoot-through state. • The leakage current is 10mApeak /5mArms , way below the German standard of 300mA. • Transformerless Quasi Z-Source Inverter is safe to connect to the grid. 21 22 Backup Slides • • • Chinese manufactures dominated the global industry in 2010, with close to 11,000 megawatts of PV cell production. This was the seventh consecutive year in which China at least doubled its PV output. Taiwan was a distant second with 3,600 megawatts produced, followed by Japan with 2,200 megawatts, Germany with 2,000 megawatts, and the United States with 1,100. The top five countries thus accounted for 82 percent of total world PV production. Source: http://www.freesolar.com.au/about-us/our-suppliers 23 Backup Slides Grid-connect inverters - testing standards Standards Australia has released three standards which are pertinent to grid connected inverter systems. These are: AS 4777.1 - 2005 Grid connection of energy systems via inverters Part 1: Installation requirements. AS 4777.2 - 2005 Grid connection of energy systems via inverters Part 2: Inverter requirements. AS 4777.3 - 2005 Grid connection of energy systems via inverters Part 1: Grid protection requirements. Inverters must be tested against AS 4777.2 and 3 - 2005 (or equivalent) and AS3100 (or equivalent) by an appropriate testing laboratory. Source: http://www.solaraccreditation.com.au/approvedproducts/inverters.html 24