# Low-voltage ride-through capability of a single-stage single-phase photovoltaic system connected to the low-voltage grid.

1. IntroductionMore and more single-phase photovoltaic (PV) systems are connected to the public grid mainly because of the matured PV technology and the declined price of the PV module cell [1]. As it is reported by PHOTON International, there was 27.7 GW of global PV generation systems installed in 2011, nearly 21 GW in Europe, which makes accumulated installed global PV capacity be around 70 GW at the end of 2011. It can be foreseen that the future grid-connected PV systems will play a very important role in the regulation of the conventional power systems.

However, behind the thriving penetration of single-phase grid-connected PV systems, the phenomenon of large-scale Distributed Generation (DG) systems connected to the public grid also raises some concern on the availability, quality, and reliability of the grid. On this basis, many grid requirements are published in recent years by the Transmission System Operators, Distribution System Operators, or international standard committees (e.g., IEC and IEEE) in order to regulate the interaction between DGs and the public grid [2-9]. In spite of this fact, most of these grid requirements are focused on three-phase wind power systems or DGs connected to medium- or high-level grid. There are few grid codes and papers describing the demands for PV systems connected to low-level grid, like single-phase PV systems [6,10-15].

Due to the fast growing installations of grid-connected PV systems, it is expected that the future PV systems will be more active and "smart" with the functionalities of low-voltage ride-through capability and grid support, which are required for three-phase wind power systems. In the future, the grid-connected PV system needs to fulfill the basic grid requirements, like power quality demand, and also provides some ancillary services like-what the conventional power plant does. For instance, the PV inverters should inject some reactive current when the grid presents a voltage sag fault. In that case, the control strategies should be developed in order to help the PV system ride-through during the grid faults.

For single-phase applications, the calculation of active and reactive power is a big challenge, which leads to the difficulty of direct instantaneous power control. Unlike three-phase systems, it is difficult to employ directly a dq-rotating synchronous reference frame in single-phase systems to implement positive sequence control or constant reactive power control [7, 8, 16]. Possible solutions for single-phase applications are based on the single-phase PQ theory, instantaneous power control, or the droop control concept [13,1720]. Moreover, the grid fault detection and synchronization techniques are also challenges for the single-phase system when operating in the grid fault mode.

In this paper, the overall control strategy for single-phase PV systems in the grid faulty mode operation is demonstrated based on the grid requirements defined for three-phase wind power systems as it is expected that they will be the basic requirements for single-phase PV systems. A transport delay grid fault detection method is adopted in this study. A power control method based on the single-phase PQ theory and the Proportional-Resonant (PR) current control scheme is proposed. Finally, the system is tested in simulation and verified by experiments. The results show that the single-phase PV systems are ready for providing ancillary service in the future and the grid detection method has a significant impact on the performance of the single-phase PV systems under grid faults.

2. Grid Requirements

The grid requirements for DGs are updated and revised based on the development and penetration level of DGs and issued in the form of national grid code [2-6], such as E.ON grid code and CEI grid code published by Comitato Elettrotecnico Italiano. In these grid codes, the basic demands are imposed like the power quality (the THD level of the injected current) and the anti-islanding requirement. Considering the penetration level of DGs connected to the grid, combined requirements are expected to be added into the grid codes in the future.

For example, in the German grid code, the DGs should handle ride-through grid fault, known as low-voltage ride-through (LVRT) capability, and support the grid during the voltage recovery. Similar requirements can be found in other countries, like Denmark, Italy, Spain, and USA in which the DGs share a high percentage of power generation. The LVRT capability is defined so that the DG should stay connected to the grid within a short time and inject some reactive power to support the grid when the grid presents a voltage fault. Different LVRT curves with defined stay-connected time are shown in Figure 1.

As it is shown in Figure 1, the DGs should stay connected to the grid when the voltage drops to 0 V in the German grid code in 0.15 seconds. At the same time, the system should inject some reactive current in order to support the grid recovery according to Figure 2.

These grid requirements are set to ensure the safety of utility maintenance personnel and also other devices connected to the public grid and to avoid the grid collapse due to voltage faults. It is expected that these grid requirements will be recommended to be used to regulate single-phase

PV systems, since the impact of large-scale single-phase PV systems on the low-level public grid cannot be ignored. The discussion in this paper is based on these requirements.

3. Single-Phase Grid-Connected Photovoltaic System in the Grid Faulty Mode Operation

3.1. System Configuration. In consideration of the whole conversion efficiency, a single-stage PV system is connected to the grid through a transformer, which is shown in Figure 3. In some cases, a voltage-boost stage can be used between the DC capacitor C and the inverter, depending on the output voltage level of the PV panels. The boost stage makes the system flexible track the Maximum Power Point (MPP) of the PV panel and also makes it possible to handle the power variation across the DC capacitor C at twice the grid fundamental frequency [9].

The control system shown in Figure 3 consists of a voltage sag detection unit, an Orthogonal Signal Generator (OSG) for power calculation, the power profiles including MPPT control in normal operation, active and reactive power controllers for current reference generation, a grid current controller, and a PWM generation block.

As it can also be seen in Figure 3, in order to implement grid fault operation mode for this system, a voltage sag generator is used by switching the series resistor Rs and the load resistance [R.sub.L]. During the LVRT mode operation, the switch [S.sub.1] is open in order to limit the short-circuit effect on the upstream grid and the switch [S.sub.2] is closed, while in normal operation,[S.sub.1] is closed and [S.sub.2] is open.

An LC filter ([LC.sub.f]) is used as the output filter in order to limit the high-order harmonics coming from the inverter switching behavior. Thus, neglecting all the filter losses, the system at the AC side can be described by

[di.sub.g](t)/dt = [v.sub.nv](t) - [C.sub.f] [d.sup.2][v.sub.g](t)/[dt.sup.2] - [v.sub.g](t)/L, (1)

in the time domain and

[I.sub.g](s) = 1/Ls [V.sub.inv](s) - ([C.sub.f][s.sup.2] + 1/Ls) [V.sub.g](s), (2)

in the Laplace domain, where [i.sub.g] is the injected grid current, [v.sub.inv] is the inverter output voltage, and [v.sub.g] is the grid voltage. Hence, the equivalent model of the output filter can be given as it is shown in Figure 4.

3.2. Voltage Sag Detection. Grid condition information is very important for the control system to perform special functionalities. Similarly, as a part of the grid condition detection, the voltage sag detection is the way to identify the voltage fault and it determines the dynamic performance of the voltage sag compensator [21, 22] and the behavior of the whole control system. It is easy to understand that the system should switch from normal operation mode to grid fault operation mode as soon as possible, once the voltage sag is detected. Hence, it is essential to have a precise and fast fault detection unit.

Recently, many voltage sag detection methods have been proposed, such as Root Mean Square (RMS) method, peak value method (OSG based sag detection techniques), the missing voltage technique, and wavelet transform method [10, 21-25]. The RMS method computes the RMS value of the input signal by using a running average window of one cycle. Therefore, theoretically, this method will introduce one cycle delay in order to give the correct value. The wavelet transform based voltage sag detection is becoming of high interest [24], because of its fast detection speed. However, the implementation of this method is unfortunately not easy in real time.

In this paper, the peak value method is used to detect the voltage fault. The implementation of this method is easy, and by means of the OSG system, it is possible and flexible to calculate the average active and reactive power instantaneously. Since the T/4 Delay structure is used to build up the OSG system as it is shown in Figure 5, the system will introduce a quarter period time delay of the input fundamental period. The peak value of the input voltage can be given by

[V.sub.m] = [square root of [v.sup.2.sub.g] + [v'.sup.2.sub.g]] = [square root of [V.sup.2.sub.m][sin.sup.2]([omega]t) + [V.sup.2.sub.m][cos.sup.2]([omega]t)], (3)

where [v'.sub.g] is the orthogonal signal of the input voltage generated by shifting a quarter period of the input signal.

3.3. Power Calculation and Power Profiles. In different operation modes, the power profiles are different. Firstly, the average active power P and reactive power Q of the system are computed using Discrete Fourier Transform (DFT) structure, as it is shown in Figure 6.

Under normal grid conditions, the system is operating in Maximum Power Point Tracking (MPPT) mode in order to deliver as much energy as possible to the grid, and the power factor is normally near to one. According to the grid requirements, in grid faulty mode operation, the single-phase PV inverter should inject some reactive power into the grid to support the grid voltage during recovery. The amount of reactive power should be injected dependent on the voltage sag depth and the inverter rating current. At the same time, the PV panels should switch to non-MPPT operation mode in order to avoid tripping the inverter overcurrent protection [10, 26, 27]. The operation modes are described in Figure 7.

By employing Park transform ([alpha][beta] [right arrow] dq) to the grid voltage and current in the OSG systems, the active power P and reactive power Q delivered to the grid can also be calculated and expressed as

P = 1/2 [v.sub.gd][i.sub.gd], (4) Q = 1/2 [v.sub.gd][i.sub.gq],

where the subscripts "gd" and "gq" denote the "d" and "q" components of the grid voltage/current in a dq-rotating synchronous reference frame.

As it is stated above, in normal MPPT operation mode, the system is operating at unity power factor. Then, neglecting the switching power losses, the active power P and reactive power Q can be obtained:

P = 1/2 [V.sub.m][i.sub.gd] = 1/2[V.sub.m][I.sub.m] [approximately equal to] [P.sub.PV,MPP] (5)

Q = -1/2 [V.sub.m][i.sub.gq] = 0,

in which [V.sub.m] and [I.sub.m] are the amplitude of the grid voltage and current in MPPT operation mode, respectively, [P.sub.PV,MPP] is the tracked maximum output power of the PV panels.

In faulty grid operation mode, according to Figure 2, the required reactive current under voltage sags can be given as

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (6)

in which V, [V.sub.0], and [V.sub.N] are the amplitude values of the grid instantaneous voltage, initial voltage before grid faults, and the nominal grid voltage, [I.sub.N], [I.sub.q0] are the nominal current and the initial reactive current before a grid failure, and k = ([DELTA][I.sub.q]/[I.sub.n])/([DELTA]V/[V.sub.n]) [greater than or equal to] 2 p.u.. By substituting (6) into (4), the required active power P* and reactive power Q* reference in the grid faulty mode operation can be given as

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (7)

where [P.sub.PV] is the output power of the PV panel in the grid faulty mode operation.

Normally, the nominal current is limited by the inverter maximum rating current, [I.sub.N] [less than or equal to] [I.sub.max], where [I.sub.max] is the inverter maximum rating current and the initial reactive current is zero, [I.sub.q0] = 0 A.

According to (7) and Figure 7, the PV panels should "derate" its output power when the grid presents a voltage fault, as it can be illustrated in Figure 8. The derated power level ([P.sub.PV,MPP] [right arrow] P* or [P.sup.PV]) is dependent on the voltage sag depth and the nominal current. If the voltage drop is small, either by decreasing the PV voltage reference or increasing it can limit the PV output power. However, it should be noted that the PV voltage must be in the inverter input voltage range.

3.4. Power Controllers and Current Reference Generation. Similar to the power calculation in the dq-rotating reference frame, the active power P and reactive power Q for a single-phase application can be computed with the help of OSG systems:

P = 1/2 ([v.sub.g[alpha]][i.sub.g[alpha]] + [v.sub.g[beta]][i.sub.g[beta]], Q = 1/2 ([v.sub.g[beta]][i.sub.g[alpha]] - [v.sub.g[alpha]][i.sub.g[beta]] (8)

in which the subscripts "g[alpha]" and "g[beta]" denote the "[alpha]" and "[beta]" components of the grid voltage/current in a [alpha][beta]-stationary reference frame.

In this way, the currents in a [alpha][beta]-stationary reference frame can be expressed as

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (9)

Since the active power and reactive power are DC quantities in steady state, it is possible to use PI controllers for power regulation, and thus the current reference can be given by

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (10)

where "*" denotes the reference signal, [G.sub.p](s) and [G.sub.q](s) are the transfer functions of the PI controllers for active power and reactive power, respectively, and which can be given by

[G.sub.p](s) = [K.sub.pp] + [K.sub.pi] 1/s,

[G.sub.q](s) = [K.sub.qp] + [K.sub.qi] 1/s. (11)

3.5. Current Controller with Harmonic Compensation. The existing current control methods, such as Proportional Resonant (PR) [28, 29], Deadbeat control (DB), Repetitive controller (RC) [30], and PI control which needs a Park transform ([alpha][beta] [right arrow] dq) [29], can be adopted in different operation modes. In this case, the PR controller is used. For the purpose of the suppression of the injected current harmonics, resonant harmonic compensation method is employed, which is shown in Figure 9.

Hence, the current closed-loop transfer function ([i.sub.g](s)/[i.sup.*.sub.g](s)) can be expressed as

[i.sub.g](s)/[i.sup.*.sub.g](s) = [G.sub.PR+HC](s) x [G.sub.d](s) / Ls + [G.sub.PR+HC](s) x [G.sub.d](s), (12)

in which [G.sub.PR+HC](s) is the transfer function of PR controller with harmonics compensation and [G.sub.d](s) is the processing and PWM delay [28]. [G.sub.PR+HC](s) and [G.sub.d](s) have the following expressions:

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (13)

where [k.sub.p] is the proportional gain, [k.sub.i] and [k.sub.ih] are the resonant and harmonic compensator gains, h is the harmonic order, [[omega].sub.0] is the fundamental frequency, and [T.sub.s] is the sampling period.

Hereafter, according to the above illustration, the whole control diagram can be structured, as it is shown in Figure 10. It can be seen from Figures 9 and 10 that the harmonics in the grid voltage [v.sub.g] will propagate to the grid current reference [i.sup.*.sub.g]. However, the cascaded harmonic compensators will suppress the harmonics if the gains around the resonance frequencies are high enough. The Bode diagram of the PR controller with selective harmonics compensation is shown in Figure 11, which can be used to tune the parameters, [k.sub.p], [k.sub.i], and [k.sub.ih]. It is shown in Figure 11 that the selection of a large [k.sub.ih] leads to a wide frequency band around the resonance point [8].

It is also worth to point out that the voltage variation of the DC capacitor (DC-link voltage) at twice the grid fundamental frequency will introduce even harmonics in the injected current. Moreover, in faulty grid operation mode, this distortion is much more severe. In this case, the harmonic compensation method by cascading several resonant controllers will cause heavy computation burden and become less practical, when the higher order harmonics need to be compensated [30].

4. Simulation and Experimental Results

Referring to Figures 3 and 10, the whole system is simulated in MATLAB in order to verify the performance of the proposed power control method. In this system, the PV panel is modeled by means of a 3D look-up table [31]. The nominal maximum power [P.sub.PV,MPP] is 1030 W, the voltage [V.sub.PV,MPP] and current [I.sub.PV,MPP] at the maximum power point are 400 V and 2.56 A, respectively. The Incremental Conductance (INC) MPPT method is adopted to capture the maximum output power of the PV system. This INC method is modified according to Figures 7 and 8 in order to limit the output power when the grid voltage drops, presenting a grid fault. The other simulation parameters are listed in Table 1. The PI controller parameters for this simulation are [k.sub.pp] = 6.2, [k.sub.pi] = 1.5, [k.sub.qp] = 1, and [k.sub.qi] = 50. Simulation results are provided in Figures 12 and 13.

As it is shown in Figures 12 and 13, the single-stage single-phase PV system is subjected to a grid fault (about 0.35 p.u.) at t = 0.7 s. This voltage sag lasts for about 320 ms. Since the detection unit needs a few milliseconds ([DELTA]t) to give the correct operation condition of the grid, instead of an immediate response, the MPPT and the control units continue to operate as in a normal condition and thus the grid current rises in this time interval. It happens similarly after the fault is cleared.

Once the grid fault is detected, the MPPT unit is disabled and the control system is switched to grid fault operation mode as it is shown in Figure 7. Soon after, the system starts to inject reactive current as required and limit the active power output to prevent the inverter from overcurrent protection. After the fault is cleared (voltage rises to 0.9 p.u.), the system goes back to its normal operation, and again, it is trying to track the maximum output power of the PV panels. However, as it is shown in Figures 12 and 13, it may take some time because of the MPPT perturbing process.

In order to validate the effectiveness of the proposed control method, the system is also tested experimentally. Instead of some real PV panels, two DC sources are used as the input power. The whole system consists mainly of

(i) two Delta Elektronika SM 300-5 DC power supply, the nominal DC voltage, [V.sub.DC] = 400 V,

(ii) two DC capacitors connected in parallel, the equivalent capacitance, C = 1100 [mu]F,

(iii) a Danfoss VLT FC302 3-phase inverter which is configured as a single-phase inverter,

(iv) a sag generator as shown in Figure 3, [R.sub.s] = 19.2 [OMEGA] and [R.sub.L] = 20 [OMEGA],

(v) a 5 kVA 3-phase transformer with leakage inductance [L.sub.g] = 2 mH and resistance [R.sub.g] = 0.01[OMEGA] per phase,

(vi) a DS 1103 dSPACE control system.

The PI controller parameters for active power regulation are [k.sub.pp] = 1.2 and [k.sub.pi] = 50, while the parameters for reactive power control are [k.sub.qp] = 1 and [k.sub.qi] = 50. The other parameters of the single-phase system are shown in Table 1. A voltage drop is generated by switching the manual switches [S.sub.1] and [S.sub.2], which are shown in Figure 14. The experimental results are given in Figure 15.

As it is shown in the experimental results, when the grid is subjected to a voltage sag (0.45 p.u.), the detection and control units of the single-phase system cannot react to this sudden change immediately, and thus the grid current is going to enter into a zone where the current reference is not appropriate until the detection unit outputs the sag signal. During the LVRT operation mode, the system is injecting some reactive power into the power grid and at the same time the active power is limited in consideration of the current limitation of the PV inverter, which is shown in Figure 15(b). When the voltage sag is cleared (the voltage amplitude goes to 90% of the nominal value), the system returns to its normal operation mode and is injecting current at unity power factor.

It is also shown in Figure 15 that both the start of the voltage sag and the end of that present a transient time delay ([DELTA][t.sub.1] and [DELTA][t.sub.2]) which is approximately 5 ms (T/4). Firstly, it is because of the fault detection time delay (T/4 Delay sag detection method) as illustrated in the previous paragraph. The power profile might be another reason since it is a step change when the voltage goes back to 90% of the nominal value. The response of the current controller may deteriorate the dynamics as well. Therefore, fast and accurate grid detection and reasonable power profile are necessary for a single-phase system in the grid fault mode operation.

However, the simulation and experimental results demonstrate the flexibility of a single-phase system to provide grid support functionality. The power control method in the test is effective to do so and it can do it fast.

5. Conclusion

Based on the existing grid requirements, this paper discussed the potential of a single-stage single-phase system operating in grid fault condition. The power control method proposed in this paper is effective when the system is switched to grid fault operation mode. It can be concluded that the future single-phase grid-connected PV systems are ready to be more active and more "smart" in the regulation of power grid. Like the conventional generation systems, the single-phase PV systems can also offer some ancillary service in the presence of an abnormal grid condition. However, the performance is dependent on the grid detection and control methods.

http://dx.doi.org/10.1155/2013/257487

Acknowledgment

The authors would like to thank China Scholarship Council (CSC) for supporting this Ph.D. project in the Department of Energy Technology at Aalborg University, Denmark.

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Yongheng Yang and Frede Blaabjerg

Department of Energy Technology, Aalborg University, Pontoppidanstraede 101, 9220 Aalborg, Denmark

Correspondence should be addressed to Yongheng Yang; yoy@et.aau.dk

Received 11 September 2012; Accepted 17 December 2012

Academic Editor: Sih-Li Chen

Table 1: Simulation and experimental parameters. Grid voltage amplitude [V.sub.N] = 325 V Grid frequency [[omega].sub.0] = 2[pi] x 50 rad/s LC filter L = 3.6 mH, [C.sub.f] = 2.35 [micro]F Transformer leakage [L.sub.g] = 4 mH, [R.sub.g] = 0.02 [OMEGA] inductance and resistance Sampling and switching [f.sub.s] = [f.sub.sw] = 10 kHz frequency

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Title Annotation: | Research Article |
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Author: | Yang, Yongheng; Blaabjerg, Frede |

Publication: | International Journal of Photoenergy |

Article Type: | Report |

Geographic Code: | 4EUDE |

Date: | Jan 1, 2013 |

Words: | 5021 |

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