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Article

An Enhanced Distributed Voltage Regulation Scheme for Radial Feeder in Islanded Microgrid

1
School of Electrical and Information Engineering, Tianjin University, Tianjin 300072, China
2
Department of Electrical and Computer Engineering, COMSATS University Islamabad, Lahore 54000, Pakistan
3
College of Energy and Electrical Engineering, Hohai University, Nanjing 211100, China
4
Department of Electrical Engineering, College of Engineering, Jouf University, Sakaka 72388, Saudi Arabia
5
Engineering and Applied Sciences Research Unit, Jouf University, Sakaka 72388, Saudi Arabia
6
Department of Electrical Engineering, Faculty of Engineering, Aswan University, Aswan 81542, Egypt
*
Authors to whom correspondence should be addressed.
Energies 2021, 14(19), 6092; https://doi.org/10.3390/en14196092
Submission received: 3 August 2021 / Revised: 12 September 2021 / Accepted: 16 September 2021 / Published: 24 September 2021
(This article belongs to the Section A1: Smart Grids and Microgrids)

Abstract

:
Even the simplest version of the distribution networks face challenges such as maintaining load voltage and system frequency stability and at the same time minimizing the circulating reactive power in grid-forming nodes. As the consumers at the far end of the radial distribution network face serious voltage fluctuations and deviations once the load varies. Therefore, this paper presents an enhanced distributed control strategy to restore the load voltage magnitude and to realize power-sharing proportionally in islanded microgrids. This proposed study considers the voltage regulation at the load node as opposed to the inverter terminal. At the same time, a supervisory control layer is put on to observe and correct the load voltage and system frequency deviations. This presented method is aimed at replacing paralleled inverter control methods hitherto used. Stability analysis using system-wide methodical small-signal models, the MATLAB/Simulink, and experimental results obtained with conventional and proposed control schemes verify the effectiveness of the proposed methodology.

1. Introduction

A reliable and stable distribution network represents a crucial aspect to successful power distribution to load demands. Suppling electrical power to loads can be enhanced using a well-organized distribution system [1,2]. Radial distribution networks (RDNs) are considered the most frequently employed distributed network [2,3]. RDNs are chains of conducting lines, which are divided into smaller branches for power delivery to customer’s premises. RDNs are more convenient than other configuration, as it is only fed at one end with low initial network cost. Moreover, it has easy circuit protection schemes to coordinate and design owing to its simplicity in establishing system component rating requirements [4]. As per the power network configuration, RDNs can be divided into three categories, i.e., “AC and DC networks”, “single-phase and three-phase networks”, and “balanced and unbalanced networks” [5]. Most of the developing countries use the AC distribution network as opposed to the DC network. Using DC distribution is a new technology, which requires fewer conductors for power dispersal, which reduces the line losses and cost of the conductors [6]. On the other side, the AC system could be either a single-phase or three-phase system [7]. A three-phase AC network can be further be classified as a balanced or unbalanced system: a balanced network contains the positive phase sequence components with equal magnitude and phase shift, while the unbalanced network has either a positive or negative sequence with irregular magnitude and phase shift. Unequal loading, fault, single-phasing, outrages, etc., are considered as the main causes of disturbances in the distribution system voltages and currents [8,9].
The conventional or renewable source of energy-based distributed generations (DGs) is the low-scale power generation network of wattage between a few kW to MW [10]. Power is provided in the system with respect to the power rating of DG and the identification of critical nodes. Over-voltage and over-current may occur without estimation of location and size of DG. DGs can be classified into four types, i.e., (1) injecting real and reactive power; (2) injecting real power and absorbing reactive power; (3) injecting real power solely; and (4) injecting only reactive power [10,11]. Microgrid (MG) is a cluster of different power sources, e.g., distributed generation units, storage units, microturbines, fuel cells, loads, etc. MG is suitable for the low voltage distribution side [12,13]. The primary task of MG is to deliver quality power without being suffered from voltage fall. The penetration of renewable sources such as fuel cells, PV cells into MG has reduced the fuel cost and CO2 emission [14]. However, proper integration of such sources required the DC to AC inversion, where the setting of power converters and power flow control faces vital challenges. The suitable energy storage system with its control algorithm makes the power flow more efficient [14,15].
Participation of generating units into the grids defines the amount of power to be supplied [2]. The generating unit could also contribute from the distribution side as well. The mode of generation is basically based on the main and subsequent generating units available as a source of power [3,16]. It can be characterized as the centralized generation, where the power generation is controlled by the main power plants and grid. Moreover, depending on the controlling scheme of MG, it can be classified as central controlled MG and local controlled MG, where combination and lone generating units are controlled [11,15]. Depending on the power supply from the substation side, MG operation can be redefined as grid-dependent, where the MG exists in the network even when the main supply is provided from the substation [13]. MG puts its contribution in a grid-dependent radial distribution system when load demand exceeds and power quality goes down. Grid-independent or islanded, where the MG is the only source of power and network is free from the substation that can be occurred during outages. Mainly, MG gives the power during the excess demand in grid-dependent systems, minimizes loss, and maintains power quality [17,18]. It acts as a backup power source during the islanded mode of operation or gird failure situation, controls the loads, converts DC power into AC power, and promises security and protection [19,20].
The study on control of grid-forming units was first carried out in uninterruptible power supply systems with parallel operation [21,22,23]. In islanded MGs, the droop control schemes widely employ to obtain power sharing by using communication channels. Power-sharing control schemes of DG units based on communication are, master/slave [24,25,26], concentrated control [25,27,28] and distributed control [29]. Oppositely the control methodologies without using the communication channel are mainly on the droop idea, which includes four leading categories: (1) virtual framework structure-based scheme [30,31,32,33,34,35]; (2) signal injection strategy [36]; (3) conventional and variants of the droop control [37,38,39,40,41,42,43] and (4) “construct and compensate”-based schemes [37,39,44]. Integrated control schemes refer to hierarchical structures consists of primary, secondary, and tertiary control [45]. The work of primary control layers is to maintain the system voltage and frequency and offer the plug-and-play capability of DGs in MG. The secondary control layers use to correct the voltage and system deviations in order to improve the power quality, while the tertiary control employs to interact with the main grid [46].
In this paper, an effort has been made to enhance voltage regulation in radial feeders, usually employed in an islanded MG distribution network. The electric power generated from various DG units is not used efficiently by the end-users in the world as the consumers at the far end of the distributor face serious voltage fluctuations and deviations once the load varies. In this study, the two DG units are connected to MG through interfacing power inverters. Droop control scheme of parallel-connected inverters is employed at consumers end as opposed to inverter terminal. In islanded mode, the inverter droop control should regulate the user voltage, system frequency, and share-power proportionally. Further, the major contributions of this work are listed below,
  • An enhanced distributed control scheme is presented, which can be used for a limited number of grid-forming nodes;
  • A distributed secondary control layer is employed to restore the load voltage and frequency deviations. Modeling and analysis of an autonomous operation of inverter-based MG being verified through stability analysis using system-wide mathematical small-signal models;
  • MATLAB/Simulink and experimental results are discussed with a comparison of conventional control schemes under load disturbances.
The remainder of this paper is organized as follows. Section 2 presents the operation principle of the system used in this proposed study. Section 3 outlines the derivations of the small-signal model for this MGs system with the employed controls. Section 4 elaborates the stability analysis of the system under the discussed controls. Further, it also presents the simulation and experimental results in detail with a comparison of the conventional and proposed control scheme, and Section 5 concludes the paper.

2. Proposed Control Strategy

This section presents the MG setup used in this proposed study. To adequately describe the proposed control scheme, we systematically go about describing the mathematical model and power flow control along with the necessary mathematical representations.

2.1. Microgrid Power Network Model

A radial distribution network with a three-phase, three-wire configuration is used in this study, as shown in Figure 1. Power converters and RL load are connected through feeder 1 and feeder 2. This network can work autonomously in an “islanded” mode. Table 1 and Table 2 express the rated system parameters for stability analysis, simulation, and experimental prototype. In this study, load voltage magnitude restoration is considered unlikely the voltage regulation at the inverter terminal. By using the reference frame transformation, the load voltage is transformed into d-q axis components. Based on such sensed measurements at ith node of each inverter, the apparent power S is calculated and dispatched to droop controllers of every ith inverter via low-pass filters. Depending on the received information, the droop controllers further send the reference voltage command to inner voltage and current layers. Distributed secondary layer periodically corrects the load voltage and system frequency deviations.

2.2. Mathematical Model

To understand the varying power relationship corresponding to change in amplitude and frequency, the complex power delivered to the ith ac bus is expressed in term of network voltages and admittances. The complex power delivered to the ith bus can be expressed as:
S i = V i I i *
Applying the algebraic multiplication to Equation (A6) shown by Appendix A and then collecting the real part Pi and imaginary part Qi results:
P i = j = 1 N   | V i | | V j | G i j cos ( φ i φ j ) + B i j sin ( φ i φ j )
Q i = j = 1 N   | V i | | V j | G i j sin ( φ i φ j ) B i j cos ( φ i φ j )
Power angle φ in medium-voltage lines are small, assuming sinφ = φ and cosφ =1, the Equations (2) and (3) re-expressed:
P i , R x = 0 V i V j X i [   sin φ i j ]
Q i , R x = 0 V i 2 V i V j cos φ i j X i
where the mathematical expression of term φij and (ViVj) is given in Appendix B. Equations (4) and (5) illustrates a direct relationship among the real power Pi and power angle φ as well as between the reactive power Qi and voltage difference ViVj.

2.3. Power Flow Control

DC power source is connected with the ith inverter bridge, and its output voltage and frequency are adjusted by the power controller and inner voltage and current controllers. All the operating DG units within the system are individually formulated in their d-q frame, which is based on their angular frequency ωi and angle φi. Power electronics inverters interfaced among each DG unit and grid are converted to the d-q frame by using transformation equation as follows:
f D f Q = cos ( φ i ) sin ( φ i ) sin ( φ i ) cos ( φ i ) f d f q
The angle of ith DG unit’s d–q fame can be written:
φ i = ( ξ ω i ) d t
Droop control-based power controller block is shown in Figure 2a. Its purpose is to dispatch the voltage reference v∗odi and v∗oqi to inner control layers. Average output powers (Pi, Qi) are obtained from instantaneous power passing low-pass filters, where the instantaneous real P and reactive Q power in the d-q rotating frame can be written as pi = vodi.iodi+ voqi.ioqi and qi = vodi.ioqi+ voqi.iodi. On individual frame d-q, vodi, voqi, iodi and ioqi are the load voltage and line current of an ith inverter. Droop strategy demonstrates the relationship among the active power and system frequency p-ω, and between the reactive power and feeder load node voltage magnitude Q-V, can be illustrated as, ωi = ωref − mPiPi and v*odi = VrefnQiQi, where ωref, Vref, mPi and nQi are nominal frequency, voltage and droop coefficients, respectively, of each ith DG unit. Further, the reference voltage to the inner voltage layer is denoted by v*odi. Q-V droop control strategy by considering the load node voltage magnitude can be written by (8), illustrated in Figure 2a.
v * o d i = V r e f n Q i Q i
where Vref is the nominal voltage of all inverters, while v*odi is responsible for restoring the feeder load node load voltage, which regulates the voltage deviation caused by the droop controllers.

2.4. Distributed Secondary Control Layer: Voltage and Frequency Regulation

Distributed secondary control layers are used to restores the voltage and frequency deviations as the strategy expressed by Equations (9) and (10).
ω a v g ¯ = i = 1 N ω D G i N ω i = ( ω r e f   ω a v g ¯ ) ς ω i = k p f ω i + k i f ω i d t
where the ωref is the reference frequency, ωDGi is the measured system frequency that is being sensed at all the nodes of ith inverters. The frequency correction term ςωi is sent to the frequency reference of each ith inverter shown in Figure 1. Kpf and Kif are the proportional and integral gains for controllers.
Load voltage regulations schemes can be expressed as:
V a v g ¯ = i = 1 N V D G i N V i = ( V r e f   V a v g ¯ ) ς V i = k p f V i + k i f V i d t
where Vref and VDGi are the nominal reference voltage and measured system voltage, respectively, in d-axis, which is sensed at each inverter’s nodes. Kpf and Kif are the proportional and integral gains for controllers. The updated voltage correction ςω term is applied to the voltage reference of each ith inverter.

3. Small-Signal Analysis of the Microgrid System

Intermittent latencies and delay of component communication links may result in power imbalances between generation sources, deviations in node voltages, and system frequency. Therefore, the stability of the system is analyzed by variations in P-f droop gain mP and communication delay Td. The small-signal modeling strategy is based on three important sub-modules, which are the inverter, network, and loads. State equations of the network and the connected loads with any ith DG inverter are presented in the reference frame by using the transformation strategy.

3.1. Primary Controller

From measured output current and voltage, the instantaneous power can be written as p = vodi.iodi + voqi.ioqi and q = vodi.ioqivoqi.iodi. The small signal modeled for active power can be obtained as given in (11) by linearization.
Δ ˙ P i = ω c i . Δ P i + ω c i ( I o d i Δ v o d i + I o q i Δ v o q i + V o d i Δ i o d i + V o q i Δ i o q i )
v o d q i = v o d i v o q i T ,   i o d q i = i o d i i o q i T
Algebraic modeling for the voltage controller and the current controller can be expressed as follows,
i * l d i = F i . v o d i ω b . C f i . Δ v o q i + K P V i ( v * o d i v * o d i ) + K I V i φ d i
i * l q i = F i . v o q i + ω b . C f i . Δ v o q i + K P V i ( v * o q i v * o q i ) + K I V i φ q i
v * i d i = ω b . L f i . i l q i + K P C i ( i * l d i i l d i ) + K I C . γ d i
v * i q i = ω b . L f i + K P C i ( i * l q i i l q i ) + K I C . Δ γ q i
The small-signal state-space modeling for voltage and current loop is given in Appendix D.

3.2. Grid Side Filter Model

The small-signal model of LC output filter and coupling inductance by assuming that voltage provided by the inverter is the same as demand voltage is expressed as in (17)–(19).
d i l d q i d t = R f i L f i . i l d q i + ω i . i l d q i + 1 L f i . v i d q i 1 L f i . v o d q i
d v o d q i d t = ω i . v o q q i + 1 C f i . i l d q i 1 C f i . i o d q i
d i o d q i d t = R c i L c i . i o d q i + ω i . i o d q i + 1 L c i . v o d i q 1 L c i . v o b d q i
The LC filter and coupling inductance, their linearization small-signal equations are represented by Appendix E.

3.3. Complete Model of an ith Inverter

The output variables need to the converter in a common reference frame to connect at ith inverter with the rest of the system. In our case, the output currents are the output variables of ith inverters, which can be expressed in vector form ∆iodqi. ∆ioDQi, which is a small-signal output current, can be expressed by Appendix E.1. The bus voltage on the common reference frame is the input signal to the ith inverter model. Therefore, by using reverse transformation, the bus voltage can be converted into an ith individual inverter reference frame.
[ Δ u b d q ] = [ T γ 1 ] . [ Δ u b D Q ] + [ T σ 1 ] [ Δ δ ] ,   where ,   T σ 1 = U b D sin ( δ ) + U b Q cos ( δ ) U b D cos ( δ ) U b Q sin ( δ )
By combining the aforementioned state-space models for three controllers of an ith inverter, which are power controller, voltage controller and current controller, and output grid side LCL filter, the complete small-signal model can be obtained.
[ Δ x ˙ i n v i ] = A i n v i . [ Δ x i n v i ] + B i n v i . [ Δ u b D Q i ] + B i ω c o m . [ Δ ω c o m ]
Δ ω i Δ i o D Q = C i n v ω i C i n v c i . [ Δ x i n v i ]
where
[ Δ x i n v ] = Δ δ i Δ P i Δ Q i Δ φ d i Δ φ q i Δ γ d i Δ γ q i Δ i l d i Δ i l q i Δ v o d i Δ v o q i Δ i o d i Δ i o q i T
The matrices Ainvi, Binvi, Biwcom, Cinvwi, and Cinvci are the system matrices described by Appendix C.

3.4. Combined Model of N Inverters

In MG, the N number of DG inverters may be operating as a source at variable distances among each other. In this section, our approach is to discuss the possible sub-model form of all individual ith to kth DG inverters and combine them with the existing corresponding network. The combined small-signal model of the “N” number of DG inverters is expressed by:
[ Δ x i n v . ] = A i n v . [ Δ x i n v ] + B i n v . [ Δ v b D Q ]
[ Δ i o D Q ] = C i n v c . [ Δ x i n v ]
where the system matrices are given by Appendix F.

3.5. Network and Load Model

If an ith feeder line is connected between node j and k, mathematical modeling can be presented as follows.
d i lineDi d t = R l i n e i L l i n e i i l i n e D i + ω i l i n e Q i + 1 L l i n e i v b D j 1 L l i n e i v b D k
d i lineQi d t = R l i n e i L l i n e i i l i n e Q i ω i l i n e D i + 1 L l i n e i v b Q j 1 L l i n e i v b Q k
[ Δ i l i n e D Q . ] = A L I N E . [ Δ i l i n e D Q ] + B 1 L I N E . [ Δ u b D Q i ] + B 2 L I N E . Δ ω
where
[ Δ i l i n e D Q . ] = [ Δ i l i n e D Q 1   Δ i l i n e D Q 2 Δ i l i n e D Q n ] T , [ Δ u b D Q i ] = [ Δ i b D Q 1   Δ i b D Q 2 Δ i b D Q m ] T , Δ ω = Δ ω c o m
The matrices ALINE, B1LINE, B2LINE, ALINEi, B2LINEi, and B1LINEi are the system matrices given in Appendix F.1. If there are p load points available in a particular network, then the small-signal model can be presented as,
[ Δ i l o a d D Q . ] = A L O A D . [ Δ i l o a d D Q ] + B 1 L L O A D . [ Δ u b D Q i ] + B 2 L O A D . Δ ω i
[ Δ i l o a d D Q ] = [ Δ i l o a d D Q 1   Δ i l o a d D Q 2 Δ i l o a d D Q   p ] T
where ALOAD, B1LOAD, B2LOAD, ALOADi, and B1LOADi are the system matrices described in Appendix G.

3.6. Complete Microgrid Model

It can have observed that the node voltages are used as inputs to every subsystem. In the assurance of well-defined node voltage, a virtual resistor rN is supposed among all m nodes and grounds, which symbolic form can be defined as
[ Δ v b D Q ] = R N ( M I N V [ Δ i o D Q + M l o a d [ Δ i l o a d D Q ] + M N E T [ Δ i l i n e D Q ] )
The diagonal elements of matrix RN is equal to rN, which has a size of 2 m * 2 m matrix. The mapping matrix MINV and Mload are the size of 2 m * 2 m and 2 m * 2 p, respectively. M NET matrix maps the connecting transmission lines onto the network nodes having a size of 2 m * 2 n. Finally, the complete MG small-signal model is given by Equation (30).
Δ x i n v . Δ i l i n e D Q Δ i l o a d D Q = A M G Δ x i n v Δ i l i n e D Q Δ i l o a d D Q
where AMG is the state matrix and given as
A M G = A i n v + B i n v R N M i n v C i n v c B i n v R N M N E T B i n v R N M l o a d B 1 N E T R N M i n v C i n v c + B 2 L I N E C i n v ω A L I N E + B 1 L I N E R N M N E T B 1 L I N e R N M l o a d B 1 L O A D R N M i n v C i n v c + B 2 L O A D C i n v ω B 1 L O A D R N M N E T A l o a d + B 1 L O A D R N M l o a d

4. Results and Discussion

In this section, the stability analysis, simulation, and experimental results for power sharing, voltage, and frequency regulation, are discussed. The simulations on MATLAB/Simulink are conducted on circuit configuration given in Figure 1 for three-phase 50 Hz islanded MG wherein the two paralleled connected DG1 and DG2 are connected to the RL load via feeder impedance X1–R1 and X2–R2. Moreover, the photo of the lab-scaled experiment hardware is illustrated in Figure 3. System and controller parameters that have been used in conventional and proposed control schemes are shown in Table 1 and Table 2.

4.1. Modeling Results

The complete model of the test system under the proposed control scheme is achieved and used to analyze the stability of the system under varying communication latencies and control gains. MATLAB/Simulink and linear analysis tools have been used to obtain modeling results by analyzing this complex system through perturbing dynamical equations. Figure 4a,b shows the stability plot for the proposed control framework by varying real power droop gain mP to trace the network trajectory. The control values of the droop gain mP where system poles appear to be in the vicinity of the unit origin are maximum allowable limits. Therefore, using the poles zero evolutions, the control gain sensitivity and system stability are predicted. The maximum and minimum mP gain values used for the proposed control scheme are 1 × 9.5−9 and 1 × 9.5−5, respectively.
Figure 4c demonstrates the pole and zero traces resulting from the behavior of the MG system by varying the time delays with the proposed control scheme. Movement of system poles is captured by starting with time delay td = 0 and increasing it step by step to a maximum time delay of td = 3 s. Poles are observed in the stable region for the time delay values 0 > td < 1 s and outside the unit circle for the td > 1 s, which makes the MG system divergent and unstable.

4.2. Simulation Results

In this section, the MATLAB/Simulink-based results obtained with conventional and proposed control strategies are discussed. The simulation verifications are composed of two cases. Case 1 outlines the results obtained with a conventional control scheme, while case 2 validates the effectiveness of the proposed control strategy. The initial conditions and control parameters as shown by Table 1 and Table 2 are the same for both cases.

4.2.1. Case 1: MATLAB/Simulink Results with Conventional Control Strategy

Figure 5 shows the results obtained with a conventional control scheme. The objective of this scheme is to hold the load voltage at its original state, i.e., Vref = 300 V, in the presence of load disturbance. To examine the methodology, the disturbance load (Ld1 = 10 mH, Rd1 = 20 Ω) is exerted at time t1, and later the conventional control scheme is activated at the time t2. Figure 5a illustrates the load voltage deviation of 2 V even the load disturbance is not yet exerted. This load voltage further deviates and is set at 393.5 V once the disturbance load is added at time t1, as shown by Figure 5b. The load voltage drop of 4.5 V is removed once the conventional control strategy is activated at t2. Although the conventional scheme is activated, still 2.3 V load voltage deviation is observed, as shown by Figure 5c. Real and reactive power sharing is illustrated by Figure 5d, while Figure 5e,f show the magnified results of real and reactive power, respectively.

4.2.2. Case 2: MATLAB/Simulink Results with Proposed Control Strategy

Figure 6 shows the results obtained with the proposed control scheme. As opposed to the conventional scheme, the initial load voltage is observed at the desired value, i.e., Vref = 300 V, as shown by Figure 6a. Once the disturbance load jXd1/Rd1 is exerted at t1, an obvious 3 V load voltage drop is depicted, as illustrated by Figure 6b. The proposed control scheme is activated at t2, as shown in Figure 6c, where load voltage has resorted to nearly its original state. Figure 6d,g show the real and reactive power-sharing results, respectively, while Figure 7 demonstrates the frequency restoration result using the proposed methodology.

4.3. Experimental Results

An accompanying experiment is carried out to investigate the proposed control scheme. The experiment is conducted for a three-phase, 50-Hz scaled islanded MG prototype, as depicted in Figure 3. The system consists of two identical paralleled DG units with a maximum rating of 3 A, 30 V, connected with RL load via feeder 1 and feeder 2. Ethernet module USR TCP 232 is used for serial communication transmission of data among the data terminal equipment (DTE) and data communication equipment (DCE). The whole platform of islanded MGs is controlled by the desktop control system, wherein LabVIEW has been used to control the DG units.
Figure 8a shows the behavior of load voltage in the presence of disturbance load under a conventional control scheme. Load disturbance of value Ld1 = 1 mH, Rd1 = 5 Ω is added at t1 as shown in Figure 8b (magnified). From the same figure, 1v load voltage deviation is observed once the disturbance load is added. This deviation is removed when the conventional control strategy is activated at t2. However, under the conventional control scheme, still, 2.5 V load voltage deviation is observed, as compared to its original state (Vref = 30 V) as shown in Figure 8c. Figure 8d shows the DGs and load voltage response in the presence of the disturbance load jXd1/Rd1 under the proposed control scheme. About 0.5 V load voltage deviation is noticed once the disturbance load is exerted at t1, as shown in Figure 8e (magnified result). This load voltage deviation is removed, and load voltage is restored to its original state (Vref = 30 V), as shown in Figure 8f (magnified result). System frequency error measured at inverter terminal is regulated within an acceptable range once the proposed control scheme is activated at t2, as in Figure 8g.

5. Conclusions

In this paper, an enhanced droop control scheme is presented for microgrids working in islanded mode. The control scheme is able to restore the load voltage deviations and fluctuations due to the droop effect and load effect. The proposed study consists of two decoupled methods, the Q-V control layer shares the reactive power proportionally and restores the load voltage magnitudes, while the P-f control layer addresses the active power sharing and frequency stability. Both sets of control layers have been implemented in a distributed manner. At the same time, the distributed secondary layer is used to regulate the system frequency. Mathematical small-signal models were employed to analyze the performance of the presented scheme using pole-zero evolutions with regard to system stability toward variations in control parameters. Various simulations and experimental results, in comparison to the conventional scheme, showed that the proposed methodology is very effective.

Author Contributions

M.Z.K., C.M. and S.H. contributed to the conceptualization behind this work. M.Z.K. has prepared the write-up and manuscript. S.H., W.A. and E.M.A. helped with small-signal modeling and with the write-up, sectionalizing, and appropriate referencing. All authors have read and agreed to the published version of the manuscript.

Funding

The authors extend their appreciation to the Deputyship for Research and Innovation, Ministry of Education in Saudi Arabia, for funding this work through the project number “375213500”. The authors also would like to extend their sincere appreciation to the central laboratory at Jouf University for supporting this study.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Acknowledgments

The authors would like to thank the editor in chief, the associate editors, and the reviewers for their worthy suggestions, time, and effort in improving and finalizing this paper. The authors would further like to thank Asad Khan ([email protected]) for providing the support in software and validation.

Conflicts of Interest

The authors declare no conflict of interest.

Appendix A

The current injection into ith bus written as
I i = j = 1 N Y i j V j
where Yij terms are admittance matrix elements. By substituting Equation (1) into (2), yields:
S i = V i j = 1 N Y i j V j * = V i j = 1 N Y i j * V j *
where Vi is a phasor term, have the magnitude and angle that can be expressed as Vi = |Vi|φi. Yij is the complex-valued admittance matrix element that can be defined Gij and Bij as the real and imaginary parts, i.e., Yi = Gij + jBij; therefore the Equation (A2) can be expressed as
S i = V i j = 1 N Y i j * V j * = | V i | φ i j = 1 N G i j + j B i j * | V j | φ j * = | V i | φ i j = 1 N G i j j B i j | V j | φ j
= j = 1 N   | V i | φ i | V j | φ j G i j j B i j = j = 1 N   | V i | | V j | ( φ i φ j ) ( G i j j B i j )
By converting the phasor expression into complex function of sinusoids, i.e., V = |V|∠φ = |V|(cosφ + jsinφ),
S i = j = 1 N   | V i | | V j | ( φ i φ j ) ( G i j j B i j )
= j = 1 N   | V i | | V j | cos ( φ i φ j ) + j sin ( φ i φ j ) ( G i j j B i j )
= P i + j Q i

Appendix B

φ i j = X P i V i V j V i V j = X Q i V i

Appendix C. System Matrices

A i n v i = A P i 0 0 B P i B v 1 i C P v i 0 0 B v 2 i B G S F i D v 1 i C P v i B c 1 i C v i 0 B c 1 i D v 2 i + B c 2 i B G S F 2 i   [ T v i 1   0   0 ] + B G S F 3 i C p w i B G S F 1 i D c 1 i C v i B G S F 1 i C c i A G S F i + B G S F 1 i ( D c 1 i D v 2 i + D c 2 i ) 13 × 13
B i n v i = 0 0 0 B G S F 2 T S 1 13 × 2 B i w c o m = B p w c o m 0 0 0 13 × 1 ;   C i n v w i = C p w   0   0   0 1 × 13 i = 1 0   0   0   0 1 × 13 i 1
C i n v c i = T C   0   0   0   0   0   0   T s 2 × 13 ;   Δ x i n v . Δ i l i n e D Q Δ i l o a d D Q = A M G Δ x i n v Δ i l i n e D Q Δ i l o a d D Q
where AMG is the state matrix and given as
A M G = A i n v + B i n v R N M i n v C i n v c B i n v R N M N E T B i n v R N M l o a d B 1 N E T R N M i n v C i n v c + B 2 L I N E C i n v ω A L I N E + B 1 L I N E R N M N E T B 1 L I N e R N M l o a d B 1 L O A D R N M i n v C i n v c + B 2 L O A D C i n v ω B 1 L O A D R N M N E T A l o a d + B 1 L O A D R N M l o a d

Appendix D. Inner Zero Control: Voltage and Current Controller Matrices

Small-signal state-space equations for voltage loop and current loop are
Δ i l d q i * = C v Δ φ d q i + D v 1 Δ v * o d q i + D v 2 Δ i l d q i Δ v o d q i Δ i o d q i
Δ v i d q i * = C c Δ γ d q i + D c 1 Δ i * l d q i + D c 2 Δ i l d q i Δ v o d q i Δ i o d q i
where
C c = K I C i 0 0 K I C i , D c 1 = K P C i 0 0 K P C i ;   D c 2 = K P C ω L f i 0 0 0 0 ω L f i K P C 0 0 0 0
Here, both ∆γdi and ∆γqi are perturbations for PI controllers in the auxiliary state. KPCi and KICi are the proportional and integral gains for the voltage controller loop, respectively, while ilqi and ildi are system measurements.

Appendix E. Grid Side Filter Model

LC filter and coupling inductance, their linearization small-signal equations are represented in following equations, where wo, at a given operating point, is the steady-state frequency.
Δ i l d q i . Δ v o d q i Δ i o d q i = A G S F Δ i l d q i Δ v o d q i Δ i o d q i + B G S F 1 [ Δ v i d q i ] + B G S F 2 [ Δ v b d q i ] + B G S F 3 [ Δ ω ]

Appendix E.1. Complete Model of an ith Inverter

[ Δ i o D Q ] = [ T γ ] . [ Δ i o d q ] + [ T ζ ] . [ Δ δ ] = cos ( δ ) sin ( δ ) sin ( δ ) cos ( δ ) . [ Δ i o d q ] + I o d cos ( δ ) I o q sin ( δ ) I o d sin ( δ ) I o q cos ( δ ) . [ Δ δ ]
where the transformation matrix T γ is,
T γ = cos ( δ ) sin ( δ ) sin ( δ ) cos ( δ ) . [ Δ i o d q ]   ;   T ζ = I o d cos ( δ ) I o q sin ( δ ) I o d sin ( δ ) I o q cos ( δ ) . [ Δ δ ]

Appendix F. Combined Model of N Inverters

[ Δ x i n v ] = A i n v . [ Δ x i n v 1 Δ x i n v 2 Δ x i n v N ] T
A i n v = A i n v 1 + B 1 w c o m C i n v w 1 0 0 A i n v 2 + B 2 w c o m C i n v w 1 13 N × 13 s B i n v = B i n v 1 B i n v 2 13 N × 2 m
[ Δ v b D Q ] = [ Δ v b D Q 1 Δ v b D Q 2 Δ v b D Q N ] ;   C i n v c = [ C i n v c 1 ] 0 0 [ C i n v c 2 ] 2 N × 13 N

Appendix F.1. Network and Load Model

A L I N E = A L I N E 1 0 0 A L I N E 2 2 n × 2 n B 1 L I N E = B 1 L I N E 1 B 1 L I N E 2 2 n × 2 m B 2 L I N E = B 2 L I N E 1 B 2 L I N E 2 2 n × 1
A L I N E i = R l i n e i L l i n e i ω i ω i R l i n e i L l i n e i B 2 L I N E i = I l i n e Q i I l i n e D i B 1 L I N E i = 0 1 L l i n e i 0 0 2 × 2 m
The state equations for RL load connected via an ith node can be written as follows
d i loadDi d t = R l o a d i L l o a d i i l o a d i D i + ω i l o a d i Q i + 1 L l o a d i v b D i
d i loadQi d t = R l o a d i L l o a d i i l o a d i Q i ω i l o a d i D i + 1 L l o a d i v b Q i

Appendix G. Network and Load Model

A L O A D = A L O A D 1 0 0 A L O A D 2 2 p × 2 p ,   B 1 L O A D = B 1 L O A D 1 B 1 L O A D 2 2 P × 2 m , B 2 L O A D = B 2 L O A D 1 B 2 L O A D 2 2 n × 1
where
A L O A D i = R l o a d i L l o a d i ω i ω i R l o a d i L l o a d i   B 2 LOAD = I l o a d Q i I l o a d Q i , B 1 L O A D i = 0 1 L l o a d i 0 0 2 × 2 m

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Figure 1. MG power network model and proposed control strategy.
Figure 1. MG power network model and proposed control strategy.
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Figure 2. (a) Power controller of ith inverter (b) inner voltage and current control layer.
Figure 2. (a) Power controller of ith inverter (b) inner voltage and current control layer.
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Figure 3. (a) General procedure of LabVIEW control system. (b) Laboratory experimental prototype.
Figure 3. (a) General procedure of LabVIEW control system. (b) Laboratory experimental prototype.
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Figure 4. Poles zero plots: (a) effect of the mPi variation; (b) effect of the nQi variation; (c) effect of the time delay td on system stability.
Figure 4. Poles zero plots: (a) effect of the mPi variation; (b) effect of the nQi variation; (c) effect of the time delay td on system stability.
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Figure 5. MATLAB/Simulink results with the conventional control scheme. (a) Behavior of load voltage and inverter terminal voltage. (b) Disturbance load jXd1/Rd1 added at t1. (c) Voltage regulation with the conventional control scheme. (d) Real and reactive power sharing. (e) Magnified active power. (f) Magnified reactive power.
Figure 5. MATLAB/Simulink results with the conventional control scheme. (a) Behavior of load voltage and inverter terminal voltage. (b) Disturbance load jXd1/Rd1 added at t1. (c) Voltage regulation with the conventional control scheme. (d) Real and reactive power sharing. (e) Magnified active power. (f) Magnified reactive power.
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Figure 6. MATLAB/SIMULINK results with proposed control scheme. (a) Behavior of load voltage and inverter terminal voltages. (b) Disturbance load jXd1/Rd1 added at t1. (c) Voltage regulation with proposed control scheme. (d) Real power sharing. (e,f) Magnified active power. (g) Reactive power sharing. (h) Magnified reactive power.
Figure 6. MATLAB/SIMULINK results with proposed control scheme. (a) Behavior of load voltage and inverter terminal voltages. (b) Disturbance load jXd1/Rd1 added at t1. (c) Voltage regulation with proposed control scheme. (d) Real power sharing. (e,f) Magnified active power. (g) Reactive power sharing. (h) Magnified reactive power.
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Figure 7. Frequency (angular) regulation.
Figure 7. Frequency (angular) regulation.
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Figure 8. Experimental results. (a) Behavior of load voltage and inverter terminal voltages with conventional control scheme. (b) Disturbance load jXd1/Rd1 added at t1. (c) Voltage regulation with conventional control scheme. (d) Behavior of load and inverter terminal voltages with proposed control scheme. (e) Disturbance load jXd1/Rd1 added at t1. (f) Voltage regulation with proposed control scheme. (g) Frequency regulation, (h) Magnified Frequency Regulation Curve.
Figure 8. Experimental results. (a) Behavior of load voltage and inverter terminal voltages with conventional control scheme. (b) Disturbance load jXd1/Rd1 added at t1. (c) Voltage regulation with conventional control scheme. (d) Behavior of load and inverter terminal voltages with proposed control scheme. (e) Disturbance load jXd1/Rd1 added at t1. (f) Voltage regulation with proposed control scheme. (g) Frequency regulation, (h) Magnified Frequency Regulation Curve.
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Table 1. System parameters for stability analysis and experimental prototype.
Table 1. System parameters for stability analysis and experimental prototype.
Sr. No.Control Parameters for Stability Analysis
1Droop GainsMinMax
mP0.020.32
2Consensus frequency
kpf0.45-
kif4.5 × e−04-
3Consensus voltage
kpV0.32.5
kiV0.080.48
4Time delay
τdelay06 × e−03
Sr. No.Control Parameters for Experimental Prototype
ComponentsUnitsComponentsUnits
1Operating frequency50 HzSampling rate1 ms
2DG units ratings3 A, 30 VjXi1, jXi2200 uH
3jXc1, jXc220 uFjXg1, jXg260 uH
4Lline1/Rline12 mH/0.2 ΩLload/Rload2 mH/10 Ω
5Lline2/Rline22 mH/0.2 ΩLd1/Rd11 mH/5 Ω
Table 2. System parameters for simulations.
Table 2. System parameters for simulations.
Sr.ComponentsUnitsComponentsUnits
1Nominal frequency50 HzLload/Rload80 mH/60 Ω
2Simulations Vref300 VLd1/Rd110 mH/20 Ω
3Lline1/Rline1; Lline2/Rline22 mH/0.2 Ω; 2 mH/0.2 ΩSwitching-Frequency16 kHz
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Khan, M.Z.; Mu, C.; Habib, S.; Alhosaini, W.; Ahmed, E.M. An Enhanced Distributed Voltage Regulation Scheme for Radial Feeder in Islanded Microgrid. Energies 2021, 14, 6092. https://doi.org/10.3390/en14196092

AMA Style

Khan MZ, Mu C, Habib S, Alhosaini W, Ahmed EM. An Enhanced Distributed Voltage Regulation Scheme for Radial Feeder in Islanded Microgrid. Energies. 2021; 14(19):6092. https://doi.org/10.3390/en14196092

Chicago/Turabian Style

Khan, Muhammad Zahid, Chaoxu Mu, Salman Habib, Waleed Alhosaini, and Emad M. Ahmed. 2021. "An Enhanced Distributed Voltage Regulation Scheme for Radial Feeder in Islanded Microgrid" Energies 14, no. 19: 6092. https://doi.org/10.3390/en14196092

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