A High Gain Input-Parallel Output-Series DC/DC Converter with Dual Coupled Inductors

ABSTRACT

High voltage gain dc–dc converters are required in many industrial applications such as photovoltaic and fuel cell energy systems, high-intensity discharge lamp (HID), dc back-up energy systems, and electric vehicles. This paper presents a novel input-parallel output-series boost converter with dual coupled inductors and a voltage multiplier module. On the one hand, the primary windings of two coupled inductors are connected in parallel to share the input current and reduce the current ripple at the input. On the other hand, the proposed converter inherits the merits of interleaved series-connected output capacitors for high voltage gain, low output voltage ripple, and low switch voltage stress. Moreover, the secondary sides of two coupled inductors are connected in series to a regenerative capacitor by a diode for extending the voltage gain and balancing the primary-parallel currents. In addition, the active switches are turned on at zero current and the reverse recovery problem of diodes is alleviated by reasonable leakage inductances of the coupled inductors. Besides, the energy of leakage inductances can be recycled. A prototype circuit rated 500-W output power is implemented in the laboratory, and the experimental results shows satisfactory agreement with the theoretical analysis.

KEYWORDS

1.      DC–DC converter

2.      Dual coupled inductors

3.      High gain

4.      Input-parallel output-series.

SOFTWARE: MATLAB/SIMULINK

CIRCUIT DIAGRAM:

Fig. 1. Equivalent circuit of the presented converter.

Fig.2 Key theoretical waveforms.

EXPERIMENTAL VERIFICATIONS:

Fig.3 Key experimental current waveforms.

Fig.4 Voltage stress waveforms of power components.

CONCLUSION

For low input-voltage and high step up power conversion, this paper has successfully developed a high-voltage gain dc–dc converter by input-parallel output-series and inductor techniques. The key theoretical waveforms, steady-state operational principle, and the main circuit performance are discussed to explore the advantages of the proposed converter. Some important characteristics of the proposed converter are as follows: 1) it can achieve a much higher voltage gain and avoid operating at extreme duty cycle and numerous turn ratios; 2) the voltage stresses of the main switches are very low, which are one fourth of the output voltage under N = 1; 3) the input current can be automatically shared by each phase and low ripple currents are obtained at input; 4) the main switches can be turned ON at ZCS so that the main switching losses are reduced; and 5) the current falling rates of the diodes are controlled by the leakage inductance so that the diode reverse-recovery problem is alleviated. At the same time, there is a main disadvantage that the duty cycle of each switch shall be not less than 50% under the interleaved control with 180◦ phase shift.

REFERENCES

[1] C.Cecati, F. Ciancetta, and P. Siano, “A multilevel inverter for photovoltaic systems with fuzzy logic control,” IEEE Trans. Ind. Electron., vol. 57, no. 12, pp. 4115–4125, Dec. 2010.

[2] X. H. Yu, C. Cecati, T. Dillon, and M. G. Simoes, “The new frontier of smart grid,” IEEE Trans. Ind. Electron. Mag., vol. 15, no. 3, pp. 49–63, Sep. 2011.

[3] G. Fontes, C. Turpin, S. Astier, and T. A. Meynard, “Interactions between fuel cell and power converters: Influence of current harmonics on a fuel cell stack,” IEEE Trans. Power Electron., vol. 22, no. 2, pp. 670–678, Mar. 2007.

[4] J. Y. Lee and S. N. Hwang, “Non-isolated high-gain boost converter using voltage-stacking cell,” Electron. Lett., vol. 44, no. 10, pp. 644–645, May 2008.

[5] Z. Amjadi and S. S. Williamson, “Power-electronics-based solutions for plug-in hybrid electric vehicle energy storage and management systems,” IEEE Trans. Ind. Electron., vol. 57, no. 2, pp. 608–616, Feb. 2010.

PV-Active Power Filter Combination Supplies Power to Nonlinear Load and Compensates Utility Current

ABSTRACT

The photovoltaic (PV) generation is increasingly popular nowadays, while typical loads require more high-power quality. Basically, one PV generator supplying to nonlinear loads is desired to be integrated with a function as an active power filter (APF). In this paper, a three-phase three-wire system, including a detailed PV generator, dc/dc boost converter to extract maximum radiation power using maximum power point tracking, and dc/ac voltage source converter to act as an APF, is presented. The instantaneous power theory is applied to design the PV-APF controller, which shows reliable performances. The MATLAB/Simpower Systems tool has proved that the combined system can simultaneously inject maximum power from a PV unit and compensate the harmonic current drawn by nonlinear loads.

KEYWORDS

1.      Active power filter (APF)

2.      Instantaneous power theory

3.      Photovoltaic (PV)

4.      Power quality

5.      Renewable energy

SOFTWARE: MATLAB/SIMLINK

 BLOCK DIAGRAM:

Figure 1. proposed design of PV-APF combination.

CONTROL DIAGRAM:

Figure 2. controller topology of dc/ac VSC in the PV-APF combination.

EXPECTED SIMULATION RESULTS:

Figure 3. output power of pv during running time.

Figure 4. duty cycle and vpv changed by mppt. (a) output

voltage of pv unit. (b) duty cycle of mppt.

Figure 5. utility supplied current waveform.

Figure 6. utility supplied current and pcc voltage waveform.

Figure 7. thd in four modes of pv system operation while

utility supplies power. (a) dq-current mode. (b) pv-apf mode.

(c) apf mode. (d) only utility supplies load.

Figure 8. pv supplied current waveform.

Figure 9. real power from the (a) utility, (b) pv unit, and (c)

load, while the utility supplies power.

Figure 10. imaginary power from the (a) utility, (b) pv unit,

and (c) load, while the utility supplies power.

Figure 11. utility received current waveform.

Figure 12. thd in four modes of pv system operation while

utility receives power. (a) dq-current mode. (b) pv-apf mode.

(c) apf mode. (d) only utility supplies load.

Figure 13. real power from the (a) utility, (b) pv unit, and (c)

load, while the utility receives power.

Figure 14. imaginary power from the (a) utility, (b) pv unit,

and (c) load, while the utility receives power.

CONCLUSION:

Regarding the multifunctional DG concept, in this paper, a dynamic grid-connected PV unit is built and the PV-APF combination system with a local controller is proposed. The controller implements two purposes, which are supplying power from the PV unit and filtering the harmonics of the local nonlinear load. The new controller based on instantaneous power balance has been explained accordingly. The MATLAB/Simpower Systems simulation shows good performances of this controller. The positive influence of MPPT on maximizing PV power output is also validated. The switching among three controllers to dc/ac VSC brings different current waveforms. As a result, the conventional dq-current controller should not be applied when PV is connected to a local nonlinear load regarding power-quality viewpoint. Preferably, the PV-APF controller compensates the utility currents successfully. While a PV unit is deactivated, the APF function can still operate. It is, therefore, technically feasible for these power electronics-interfaced DG units to actively regulate the power quality of the distribution system as an ancillary service, which will certainly make those DG units more competitive.

REFERENCES:

[1] L. Hassaine, E. Olias, J. Quintero, and M. Haddadi, ``Digital power factor control and reactive power regulation for grid-connected photovoltaic inverter,'' Renewable Energy, vol. 34, no. 1, pp. 315_321, 2009.

[2] N. Hamrouni, M. Jraidi, and A. Cherif, ``New control strategy for 2-stage grid-connected photovoltaic power system,'' Renewable Energy, vol. 33, no. 10, pp. 2212_2221, 2008.

[3] M. G. Villalva, J. R. Gazoli, and E. R. Filho, ``Comprehensive approach to modeling and simulation of photovoltaic arrays,'' IEEE Trans. Power Electron., vol. 24, no. 5, pp. 1198_1208, May 2009.

[4] N. R. Watson, T. L. Scott, and S. Hirsch, ``Implications for distribution networks of high penetration of compact _uorescent lamps,'' IEEE Trans. Power Del., vol. 24, no. 3, pp. 1521_1528, Jul. 2009.

[5] I. Houssamo, F. Locment, and M. Sechilariu, ``Experimental analysis of impact of MPPT methods on energy ef_ciency for photovoltaic power systems,'' Int. J. Elect. Power Energy Syst., vol. 46, pp. 98_107, Mar. 2013.

Cascaded Two-Level Inverter-Based Multilevel STATCOM for High-Power Applications

ABSTRACT

In this paper, a simple static var compensating scheme using a cascaded two-level inverter-based multilevel inverter is proposed. The topology consists of two standard two-level inverters connected in cascade through open-end windings of a three-phase transformer. The dc link voltages of the inverters are regulated at different levels to obtain four-level operation. The simulation study is carried out in MATLAB/SIMULINK to predict the performance of the proposed scheme under balanced and unbalanced supply-voltage conditions. A laboratory prototype is developed to validate the simulation results. The control scheme is implemented using the TMS320F28335 digital signal processor. Further, stability behavior of the topology is investigated. The dynamic model is developed and transfer functions are derived. The system behavior is analyzed for various operating conditions.

KEYWORDS

1.      DC-link voltage balance

2.      Multilevel inverter

3.      Power quality (PQ)

4.      Static compensator (STATCOM)

SOFTWARE:  MATLAB/SIMULINK

 BLOCK DIAGRAM

Fig. 1. Power system and the STATCOM model.

EXPECTED SIMULATION RESULTS

Fig. 2. Frequency response ∆V_dc1(s) /∆δ₁(s) at  i^’_q0 =1.02 p.u., δ₁=-0.9⁰,δ₂=178.9⁰,R₁=

80 p.u., R₂=60 p.u.

Fig. 3. Root locus of the transfer function  ∆V_dc1(s) /∆δ₁(s) at  i^’_q0 = - 0.75 p.u., δ₁=-0.57⁰,δ₂=179.6⁰,R₁=

80 p.u., R₂=60 p.u.

Fig. 4. Reactive power control. (a) Source voltage and inverter current.

(b) DC-link voltages of two inverters.

Fig. 5. Operation during fault. (a) Grid voltages on the LV side of the transformer. (b) -axis negative-sequence current component i^’_dn. (c) -axis negative- sequence current component i^’_qn.

CONCLUSION

DC-link voltage balance is one of the major issues in cascaded inverter-based STATCOMs. In this paper, a simple var

Fig. 6. Experimental result: Capacitive mode of operation. (a) Source voltage (50 V/div) and STATCOM current (5 A/div). (b) DC-link voltages of inverter-1 and inverter-2 (20 V/div). Time scale: 5 ms/div. (c) Harmonic spectrum of

current.

Fig. 7. Experimental result: Mode change from capacitive to inductive. (a) DC-link voltages of inverter-1 and inverter-2 (20 V/div). Time scale: 100 ms/div. (b) Source voltage (100 V/div) and STATCOM current (5 A/div) in steady state. Time scale: 100 ms/div.

compensating scheme is proposed for a cascaded two-level inverter- based multilevel inverter. The scheme ensures regulation of dc-link voltages of inverters at asymmetrical levels and reactive power compensation. The performance of the scheme is validated by simulation and experimentations under balanced and unbalanced voltage conditions. Further, the cause for instability when there is a change in reference current is investigated. The dynamic model is developed and transfer functions are derived. System behavior is analyzed for various operating conditions. From the analysis, it is inferred that the system is a non minimum phase type, that is, poles of the transfer function always lie on the left half of the -plane. However, zeros shift to the

right half of the -plane for certain operating conditions. For such a system, oscillatory instability for high controller gains exists.

REFERENCES

[1] N. G. Hingorani and L. Gyugyi, Understanding FACTS. Delhi, India: IEEE, 2001, Standard publishers distributors.

[2] B. Singh, R. Saha, A. Chandra, and K. Al-Haddad, “Static synchronous compensators (STATCOM): A review,” IET Power Electron., vol. 2, no. 4, pp. 297–324, 2009.

[3] H. Akagi, H. Fujita, S. Yonetani, and Y. Kondo, “A 6.6-kV transformerless STATCOM based on a five-level diode-clamped PWMconverter: System design and experimentation of a 200-V 10-kVA laboratory model,” IEEE Trans. Ind. Appl., vol. 44, no. 2, pp. 672–680, Mar./Apr. 2008.

[4] A. Shukla, A. Ghosh, and A. Joshi, “Hysteresis current control operation of flying capacitor multilevel inverter and its application in shunt compensation of distribution systems,” IEEE Trans. Power Del., vol. 22, no. 1, pp. 396–405, Jan. 2007.

[5] H. Akagi, S. Inoue, and T. Yoshii, “Control and performance of a transformerless cascaded PWM STATCOM with star configuration,” IEEE Trans. Ind. Appl., vol. 43, no. 4, pp. 1041–1049, Jul./Aug. 2007.

Dynamic Modeling of Electric Springs

ABSTRACT:

The use of ‘Electric Springs’ is a novel way of distributed voltage control while simultaneously achieving effective demand-side management through modulation of non-critical loads in response to the fluctuations in intermittent renewable energy sources (e.g. wind). The proof-of-concept has been successfully demonstrated on a simple 10 kVA test system hardware. However, to show the effectiveness of such electric springs when installed in large numbers across the power system, there is a need to develop simple and yet accurate simulation models for these electric springs which can be incorporated in large-scale power system simulation studies. This paper describes the dynamic simulation approach for electric springs which is appropriate for voltage and frequency control studies at the power system level. The proposed model is validated by comparing the simulation results against the experimental results. Close similarity between the simulation and experimental results gave us the confidence to use this electric spring model for investigating the effectiveness of their collective operation when distributed in large number across a power system. Effectiveness of an electric spring under unity and non-unity load power factors and different proportions of critical and non-critical loads is also demonstrated.

KEYWORDS:

1.      Demand side management

2.      Reactive power control

3.      Electric springs

SOFTWARE: MATLAB/SIMULINK

BLOCK DIAGRAM:

Fig. 1: Block diagram of the test system with Electric Spring

EXPECTED SIMULATION RESULTS:

Fig. 2: Comparison between line voltages with ES operating in voltage support mode. Reactive power consumption of the intermittent source is increased from 467 to 1100 Var at t=2.0 s (a) simulated response and (b) experimental results.

Fig. 3: Comparison between voltages injected by the ES. Reactive power consumption of the intermittent source is increased from 467 to 1100 Var at t=2.0 s (a) simulated response and (b) experimental results

Fig. 4: Comparison between voltages across the non-critical load. Reactive power consumption of the intermittent source is increased from 467 to 1100 Var at t=2.0 s (a) simulated response and (b) experimental results

Fig. 5: Comparison between line voltages with ES operating in voltage suppression mode. Reactive power consumption of the intermittent source is reduced from 467 to 110 Var at t=2.0 s (a) simulated response and (b) experimental results

Fig. 6: Comparison between voltages injected by the ES. Reactive power consumption of the intermittent source is reduced from 467 to 110 Var at t=2.0 s (a) simulated response and (b) experimental results

Fig. 7: Comparison between voltages across the non-critical load. Reactive power consumption of the intermittent source is reduced from 467 to 110 Var at t=2.0 s (a) simulated response and (b) experimental results

Fig. 8: Variation of active power consumeb by the non-critical and critical loads under voltage support (subplot a) and suppression (subplot b) modes

Fig. 9: Simulated response following random variations in active power generation and reactive power consumption of the intermittent source. ES is activated at t = 720 s

Fig. 10: Experimental results following random variations in active power generation and reactive power consumption of the intermittent source. ES is activated at t = 720 s

Fig. 11: Simulated response for RL load (both critical load and non-critical load) with a power factor of 0.95 lagging following random variations in active power generation and reactive power consumption of the intermittent source. ES is activated at t = 720 s

Fig. 12: System response for different distribution of non-critical and critical loads (NC:C). Disturbance is increase in reactive power consumption of the intermittent source from 467 to 1100 VAr at t=1.0 s

CONCLUSION:

The electric spring is a new technology that has attractive features including dynamic voltage regulation, balancing power supply and demand [8,9], power quality improvement [14], distributed power compensation [15] and reducing energy storage requreiments for future smart grid [16]. In order to fully explore their full potentials in large-scale power system simulation, an averaged simulation model for the electric spring is proposed here for the smart grid research community. The simulation model is simple for inclusion into large-scale system simulation platforms and yet accurate enough to capture the dynamic behavior of interest in terms of studying voltage and frequency stability. The case studies reported in the previous section exhibited close match between simulation and experimental results confirming the accuracy. The discrepancies, wherever applicable have been accounted for. These are due to the fact that the DC link voltage control loop has been neglected. This results in attaining a different operation point in terms of ES voltage in order to obtain the same line voltage which is possible as suggested by the phasor diagrams in Fig. 3. It is possible, of course, to include the DC link voltage control loop in the model to eliminate these little discrepancies but only at the expense of significant increase in simulation time for large systems. The addition of DC link voltage control loop (with large number of ES distributed across the system) makes the simulation much more complex with little improvement in terms of accuracy.The use of ‘Electric Springs’ is a novel way of distributed voltage control while simultaneously achieving effective demand-side management through modulation of non-critical loads in response to the fluctuations in intermittent renewable energy sources (e.g. wind). This paper describes the simulation approach for electric springs which is appropriate for voltage and frequency control studies at the power system level. Close similarity between the simulation and experimental results gave us the confidence to use this electric spring model for investigating the effectiveness of their collective operation when distributed in large number across a power system. The proposed dynamic model is generic enough to study the performance of ESs under different load power factors and proportion of critical and non-critical loads. The effectiveness of an ES improves with the proportion of non-critical load.

REFERENCES:

[1] P. Palensky and D. Dietrich, "Demand Side Management: Demand Response, Intelligent Energy Systems, and Smart Loads," IEEE Transactions on Industrial Informatics, vol. 7, pp. 381-388, 2011.

[2] A. Brooks, E. Lu, D. Reicher, C. Spirakis, and B. Weihl, "Demand Dispatch," IEEE Power and Energy Magazine,, vol. 8, pp. 20-29, 2010.

[3] D. Westermann and A. John, "Demand Matching Wind Power Generation With Wide-Area Measurement and Demand-Side Management," IEEE Transactions on Energy Conversion, vol. 22, pp. 145-149, 2007.

[4] A. Mohsenian-Rad, "Autonomous Demand-Side Management Based on Game-Theoretic Energy Consumption Scheduling for the Future Smart Grid," IEEE Transactions on Smart Grid, vol. 1, pp. 320-331, 2010.

[5] S. C. Lee, "Demand Side Management With Air Conditioner Loads Based on the Queuing System Model," IEEE Transactions on Power Systems, vol. 26, pp. 661-668, 2011.

[6] M. Parvania and M. Fotuhi-Firuzabad, "Demand Response Scheduling by Stochastic SCUC," IEEE Transactions on Smart Grid, vol. 1, pp. 89-98, 2010.