 Original research
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Improved voltage tracking of autonomous microgrid technology using a combined resonant controller with leadlag compensator adopting negative imaginary theorem
Protection and Control of Modern Power Systems volume 7, Article number: 10 (2022)
Abstract
Growing application of distributed generation units at remote places has led to the evolution of microgrid (MG) technology. When an MG system functions independently, i.e., in autonomous mode, unpredictable loads and uncertainties emerge throughout the system. To obtain stable and flexible operation of an autonomous MG, a rigid control mechanism is needed. In this paper, a robust highperformance controller is introduced to improve the performance of voltage tracking of an MG system and to eliminate stability problems. A combination of a resonant controller and a leadlag compensator in a positive position feedback path is designed, one which obeys the negative imaginary (NI) theorem, for both singlephase and threephase autonomous MG systems. The controller has excellent tracking performance. This is investigated through considering various uncertainties with different load dynamics. The feasibility and effectiveness of the controller are also determined with a comparative analysis with some wellknown controllers, such as linear quadratic regulator, model predictive and NI approached resonant controllers. This confirms the superiority of the designed controller.
Introduction
Consumption of electrical energy is increasing rapidly, following the rapid growth of the world’s population. To meet the demand, largely fossil fuels have been used. However, fossil fuels pollute the environment. At the same time, they are also depleting dramatically [1, 2]. To overcome this problem, renewable energy is one of the prime solutions, and different renewable energy generating units such as wind turbine, photovoltaic (PV), hydro, biomass, hydrogen fuel cells have been considered as distributed generator (DG) units located at customer sites [3, 4]. These DGs are connected to the utility grid through microgrid (MG) systems. Furthermore, the MG contains various loads including linear and nonlinear, balanced and unbalanced, static and dynamic types, as well as lines and distribution transformers, and energy storage systems (ESS) [5,6,7]. It is also worth noting that DG units cannot provide accurate 50/60 Hz power supply to the MG owing to their characteristics. To interface an MG with DG units, voltage source inverters (VSI) are used, and thus, to obtain the quality voltage and power outputs, VSI control is extremely important [8]. A simple MG structure with some conventional DG units, VSI and loads is depicted in Fig. 1.
An MG must have the ability to accommodate any uncertainty and abnormality, and bring the system back into an equilibrium position within the shortest possible time after a disturbance. The functions of an MG can be segmented into nonisolated (grid connected) mode and isolated (autonomous) mode [9]. In nonisolated mode, the utility grid controls the voltage and frequency of the MG, and the MG is treated as a controllable generator or load. In the case of autonomous mode, the MG itself has to control the different parameters including voltage, frequency, active and reactive power, powerfactor etc. Thus, a robust control system is necessary for satisfactory operation of an autonomous MG.
Research has made significant progress on MG controlling technology for maintaining good performance. The linear quadratic regulator (LQR) [10, 11], integralLQR (ILQR) [12], linear quadratic Gaussian (LQG) [13], and integralLQG (ILQG) [14] are wellknown controllers based on linearization techniques. These have been proposed for the voltage control of an MG. Accurate voltage tracking is the main advantage of these controllers, but the dynamics of these controllers depend on the dynamics of the plant and their performance degrades if the plant changes. Furthermore, according to the order of the plant dynamics, the order of the controller also increases. Proportional integral derivative (PID) [15] and proportional integral (PI) [16] controllers are very common and widely used for voltage and power control of an MG because of their simplicity and easy implementation. However, during disturbances, their performance degrades and steadystate errors occur because of the unbalanced system. In addition, if the operating point changes, the performance of the controllers is also hampered.
Decentralized and distributed control strategies [17,18,19] are two more control systems frequently used in an MG to compensate for deviations in frequency and voltage. These controllers require parameters which are measured by remote sensing blocks and sent back to the controller through low bandwidth communication systems. Thus, the low bandwidth and slow control loop are the principal drawbacks of these controllers.
An Hinfinity controller [20, 21] has been proposed to acquire good stabilization with guaranteed performance of an MG. However, the order of the system is a big issue for such a controller and advanced digital signal processing (DSP) is required for satisfactory performance. In addition, high mathematical understanding is needed for modeling this controller, while its slow dynamic response restricts its use. The hierarchical control technique [22, 23] which is another wellknown controller, is commonly used in a power system to control voltage and frequency. Three different levels are required, where each level is assigned to perform a distinctive control action. If one of the control levels collapses, the whole control system fails.
Model predictive control (MPC) [24, 25] is an advanced control technique extensively used to control an MG system while satisfying some constraints. Lower switching frequency and accurate voltage control with lower total harmonic distortion (THD) are the main advantages of this controller. However, sensitivity to parameter variations, as well as the need for an advanced DSP system to implement the higher order system are its major limitations. The hysteresis controller, which is another control technique based on the current controlled pulse width modulation (PWM) technique proposed in [26, 27], has fast transient response and low complexity in design. However, the considerable amount of ripple in current and variation of switching frequency limit its use at large scale. The repetitive controller [28, 29] is also a good competitor for voltage control of an MG. It is designed to eliminate periodic disturbance and minimize harmonics in the system. However, it is difficult to stabilize the controller against all unknown load disturbances, and it responds sluggishly while loads fluctuate.
In order to damp out the resonant mode in a power system, different damping controllers have been proposed, such as the proportional resonant (PRC) [30, 31] and proportional integral resonant controllers (PIRC) [32]. These improve the performance of the MG. These controllers are simple in structure, and can efficiently control selective harmonics and show negligible steadystate error. However, they are extremely sensitive to frequency variation and require accurate tuning. Negative imaginary (NI) basedresonant (NIR) [33], proportional resonant [34] and proportional plus lead compensator controllers [35] also promote voltage tracking performance along with damping resonant peak in islanded MG system, and exhibit robust performance against different load dynamics. However, they show poor performance in minimizing transient oscillation in some cases, and also the magnitude and phase errors in voltage tracking degrade their performance.
The above descriptions demonstrate the need for further improvements in voltage control of an MG system for precise reference tracking. Therefore, in this paper, a robust highperformance controller is designed to amend voltage tracking performance against various uncertainties and different loads in autonomous MG technology for both singlephase and threephase systems. The designed controller is modeled with a resonant (R) controller, series connected with a leadlag compensator (LLC), which obeys the NI theorem for guaranteeing system stability, abbreviated to ‘NIRLLC’ controller. The NIRLLC controller rigorously eliminates the drawbacks mentioned above, and has the advantages of both the resonant controller and leadlag compensator. The lead compensator shifts the root locus to the left for achieving good transient stability, while steady state errors in phase and magnitude are minimized through the lag compensator. The pole and zero of the lag compensator are placed near the origin and close to each other to avoid the instability problem. The main focus of the proposed work is to control the output voltage to track the reference to ensure the lowest magnitude and phase errors as well as THD, considering different uncertainties, nonlinearities and unknown dynamics of loads. To prove the superiority of the designed NIRLLC controller, its performance is compared with the wellknown LQR, MPC and NIR controllers. The controller and the system are simulated through MATLAB software.
The rest of the paper is structured as follows. Section 2 describes MG modeling while Sect. 3 presents the design procedure of the NIRLLC controller. Comparison of controllers is discussed in Sect. 4 and the performance of the controller is evaluated in Sect. 5. Section 6 concludes the paper.
Modeling of autonomous MG technology
The configuration and modelling of singlephase and threephase autonomous MGs are provided in this section.
Autonomous MG configuration
An MG mainly consists of three essential elements: an input energy source, an energy conversion unit and a filter. A singlephase MG system with these elements is shown in Fig. 2a. For modeling purposes, a DC voltage source is used as the source for generating power, and an IGBTbased full bridge VSI is used to convert the DC voltage into AC. In order to eliminate high frequency harmonic components from the VSI output, a filter consisting of inductor and capacitor is used after the VSI. As the MG system operates at low voltage with short lines, only the series resistance is considered here as line impedance [36]. Figure 2b depicts the threephase MG system, where a threephase VSI and a filter are used to regulate voltage and current. Additionally, the threephase MG has stepup transformer, point of common coupling (PCC) and loads, where loads are connected to the high voltage side of the transformer at PCC [37].
Figure 2a, b also show the closedloop control structures of singlephase and threephase MG systems, respectively. Measured output voltages and reference voltages are injected to the controllers as shown in Fig. 2a, b. Necessary actions are imposed to generate proper control signals which are sent to the PWM blocks to control the IGBT switches.
Mathematical modeling of singlephase MG system
In this subsection, a state space mathematical model is provided for the autonomous MG technology as shown in Fig. 2a. Considering \({\hat{V}}_{L}\) as the voltage across inductor \(L_{s}\), and \({\hat{I}}_{L}\) as inductor current, there is [38, 39]:
Applying KVL yields:
Substituting (1) into (2) yields:
where \({\hat{V}}_{sw}\) and \({\hat{V}}_{G}\) represent input voltage and output voltage, respectively. \({\hat{V}}_{sw} = \tau {\hat{V}}_{DC}\) is the average switching voltage and duty ratio \(\tau \in \{  1,1\}\).
Considering \({\hat{I}}_{C}\) as the current through the capacitor and \({\hat{V}}_{G}\) the capacitor voltage, there is:
Using KCL obtains:
Substituting (4) into (5) yields:
Equations (3) and (6) can be represented in the timedomain as:
Loads in MG are considered as black box as they change randomly and abruptly, and thus, \({\hat{I}}_{G}\) in (7) is treated as disturbance. As the purpose is to follow the reference voltage properly, \({\hat{V}}_{G}\) is considered as output, i.e.:
Considering (7) and (8), the general form of the system in the Laplace domain can be written as [40]:
where \(W_{0} (s) = C_{t} (sI  A_{t} )^{  1} B_{t} + D_{t}\) is the plant transfer function, and \(\Delta_{t} (s) = \left[ {\begin{array}{*{20}c} 0 \\ {  \frac{1}{{C_{s} }}} \\ \end{array} } \right]{\hat{I}}_{G} (s)\) is the output to input uncertainty. Also, the system matrix is \(A_{t} = \left[ {\begin{array}{*{20}c} 0 & {  \frac{1}{{L_{s} }}} \\ {\frac{1}{{C_{s} }}} & 0 \\ \end{array} } \right]\), the input matrix \(B_{t} = \left[ {\begin{array}{*{20}c} {\frac{1}{{L_{s} }}} \\ 0 \\ \end{array} } \right]\); the output matrix \(C_{t} = \left[ {\begin{array}{*{20}c} 0 & 1 \\ \end{array} } \right]\), and the feedthrough matrix \(D_{t} = 0\). The required parameters of the singlephase MG system are listed in Table 1.
Mathematical modeling of threephase MG system
Mathematical analysis of the threephase MG system is constructed with the aid of Fig. 2b. The dynamical equation of the topology in the abcframe can be expressed as [41, 42]:
In (10) and (11), \({\overline{V}}_{t,abc}\), \(\overline{I}_{t,abc}\) and \({\overline{V}}_{abc}\) are \(3 \times 1\) matrices consisting of independent phase quantity in the timedomain. Rearranging (10) and (11) leads to:
Assuming balanced DG units and loads, Eqs. (12) and (13) can be transformed into a rotating dqframe using the Park transformation as:
Equations (14) and (15) consist of components in the d and qaxes, where the d and qaxes represent real and imaginary parts, respectively. Dissociating these two components, Eqs. (14) and (15) are formed as:
The standard state space equations of the MG system can be expressed as:
where, \(A_{m} = \left[ {\begin{array}{*{20}c} 0 & {\omega_{f} } & {\frac{1}{{C_{f} }}} & 0 \\ {  \omega_{f} } & 0 & 0 & {\frac{1}{{C_{f} }}} \\ {  \frac{1}{{L_{f} }}} & 0 & {  \frac{{R_{f} }}{{L_{f} }}} & {\omega_{f} } \\ 0 & {  \frac{1}{{L_{f} }}} & {\omega_{f} } & {  \frac{{R_{f} }}{{L_{f} }}} \\ \end{array} } \right]\), \(B_{m} = \left[ {\begin{array}{*{20}c} 0 & 0 \\ 0 & 0 \\ {\frac{1}{{L_{f} }}} & 0 \\ 0 & {\frac{1}{{L_{f} }}} \\ \end{array} } \right]\), \(C_{m} = \left[ {\begin{array}{*{20}c} 1 & 0 & 0 & 0 \\ 0 & 1 & 0 & 0 \\ \end{array} } \right]\) and \(D_{m} = 0\). Also, the state vectors are \(x(t) = \left[ {\begin{array}{*{20}c} {{\overline{V}}_{d} } & {{\overline{V}}_{q} } & {\overline{I}_{t,d} } & {\overline{I}_{t,q} } \\ \end{array} } \right]^{T}\), the input or control vectors are \(u(t) = \left[ {\begin{array}{*{20}c} {{\overline{V}}_{t,d} } & {{\overline{V}}_{t,q} } \\ \end{array} } \right]^{T}\), and the output vectors are \(y(t) = \left[ {\begin{array}{*{20}c} {{\overline{V}}_{d} } & {{\overline{V}}_{q} } \\ \end{array} } \right]\).
To design an MIMO control system for a threephase MG in the sdomain, illustrated in Fig. 3a, the nominal plant transfer function is obtained from (20), thus:
Table 2 lists the necessary parameters required for the threephase MG system.
Controller design for singlephase and threephase autonomous MG systems
Controller design for singlephase MG system
Figure 3a shows the block diagram of the closedloop control structure for an autonomous MG system. Here, the reference signal is defined as \(R(s)\) and the output signal is \(Y(s)\). For a singlephase system, \(W(s)\) represents the nominal plant transfer function between input voltage \({\hat{V}}_{sw}\) and output voltage \({\hat{V}}_{G}\), \(H(s)\) is the resonant controller and \(C(s)\) is the leadlag compensator. For robust performance, the feedback compensator \(C(s)\) is connected in series with the resonant controller \(H(s)\). The transfer function of the resonant controller \(H(s)\) for a simple single input single output (SISO) system can be expressed as [33, 43, 44]:
where \(k_{s}\) is the resonant gain of the controller, \(\xi_{s}\) is the damping coefficient, and \(\omega_{s}\) is the resonant frequency. For proper stabilization of this controller, all its parameters are higher than zero. The optimized value of \(\xi_{s}\) is taken, as a large value leads to low damping while a small value provides unwanted phase shift. The closedloop transfer function of the system \(W(s)\) associating with the resonant controller \(H(s)\) can be expressed as:
This resonant controller H(s) is designed by the NI theorem (NIR) [33], which is a simple second order controller. However, this controller has steadystate phase and amplitude errors, and also shows poor performance in transient condition with considerable oscillations.
To alleviate these drawbacks, a leadlag compensator \(C(s)\) is cascaded in series with the resonant controller \(H(s)\), i.e., RLLC controller, for better and robust performance. The RLLC controller is designed to satisfy the NI theorem, and is thus called NIRLLC. According to the NI theorem [43, 45], the positive feedback interconnection of two NI systems will be stable if one of the systems is strictly negative imaginary (SNI) and the DC loop gain remains less than unity. From Fig. 3b, it is clear that the phase of the plant transfer function \(W(s)\) lies within − 180° and 0°, which implies that the system is an NI system. The transfer function of the leadlag compensator \(C(s)\) with a gain \(k_{c}\) can be written as [46, 47]:
The zero and pole of the lead compensator are denoted by \(z_{s1}\) and \(p_{s1}\), respectively, and \(\left {p_{s1} } \right > \left {z_{s1} } \right\). For the lag compensator, \(z_{s2}\) and \(p_{s2}\) are the zero and pole, respectively, and \(\left {z_{s2} } \right > \left {p_{s2} } \right\). The values of the parameters are chosen as \(k_{c} = 3.5\), \(z_{s1} = 4100\), \(p_{s1} = 9600\), \(z_{s2} = 4\) and \(p_{s2} = 3\). The overall closedloop transfer function with the designed NIRLLC controller can be written as:
where \(F(s) = H(s)*C(s)\).
Figure 3b shows that the loop gain \(W(s)*F(s)\) is still less than unity at low frequency which stabilizes the designed controller. Nyquist and rootlocus plots are depicted in Fig. 4a, b, respectively. It can be seen that the stability criterion of the designed NIRLLC controller is guaranteed, as no root is located in the righthalf plane. The performance of the designed NIRLLC controller is examined through imposing different uncertainties and various load dynamics. Different parameters of the SISO NIRLLC controller are listed in Table 3.
Controller design for threephase MG system
Designing a multiple input multiple output (MIMO) controller is much more challenging as multiple subsystems may consist of a number of power sources in each subsystem, while the numbers of control inputs and outputs increase. The closedloop control technique for threephase MG technology is shown in Figs. 2b and 3a, where \({\overline{V}}_{t,d}\) and \({\overline{V}}_{t,q}\) are the two control inputs, and \({\overline{V}}_{d}\), \({\overline{V}}_{q}\) are the two output signals to be controlled. The transfer function matrix of the MIMO closedloop system for plant \(W_{m} (s)\) and controller \(F_{m} (s)\) can be formed as:
where \(F_{m} (s) = H_{m} (s)*C_{m} (s)\).
For the MIMO system, \(H_{m} (s)\) and \(C_{m} (s)\) can be provided in the following way:
\(\beta_{m \times m}\) and \(\eta_{m \times m}\) are square matrices of order 2 × 2 for a twostate MG system. The compensator gains are chosen as: \(k_{p} = 2\), \(z_{m1} = 3800\), \(p_{m1} = 8600\), \(z_{m2} = 4\) and \(p_{m2} = 3\). The values of various parameters are listed in Table 4. For better perception of the control mechanism, a flowchart is given in Fig. 5 for the MIMO NIRLLC controller. In the case of the SISO system, \(\beta_{m \times m}\) and \(\eta_{m \times m}\) are 1 × 1 matrices, and there is no need to dissociate the input voltage. However, the rest of the procedure is identical for the two systems. Since the objective is to control the voltage of the autonomous MG system, the corresponding load voltages of the SISO and MIMO systems are considered as inputs, and the outputs of the control systems are the regulated PWM signals for the inverter IGBTs.
Comparative study of controllers
To evaluate the superior performance of the designed NIRLLC controller, timedomain and frequencydomain comparisons are displayed in Figs. 6 and 7, respectively, for singlephase and threephase systems. Commonly used controllers, including LQR and MPC together with NIR controller are considered for comparison. The design procedure of LQR, MPC, and NIR is adopted from [33, 48, 49], respectively. For fair comparison, the resonant controller parameters of the NIR controller and the designed NIRLLC controller are kept the same as shown in Tables 3 and 4, respectively. The required parameters of the LQR controller are chosen as follows:
For the SISO MPC controller, the prediction horizon and control horizon are selected as 10 and 1, respectively, and the weights are chosen as 0.1 and 11. Prediction and control horizons are kept unchanged whereas weights are selected as {0.1, 0.1} and {13, 200} for MIMO MPC.
Numerical values of different terms for different controllers which represent the step responses for singlephase and threephase systems are listed in Tables 5 and 6, respectively. It is clear from the tables that the designed NIRLLC controller for both SISO and MIMO systems achieves outstanding performance. The step response of the closedloop system using the designed SISO NIRLLC controller approaches steadystate with null offset, nearly 76.39%, 86.92% and 77.63% faster than the NIR controller, LQR and MPC, respectively. Incorporating rapid rise time and peak time, the designed NIRLLC controller reduces the overshoot by around 54.35%, 67.31% and 59.41% with respect to the NIR controller, LQR and MPC, respectively. It is also notable that better performance is obtained for the threephase system, with lower percentage of overshoot, faster rise time and peak time, as well as lower settling time with zero steadystate error. Obviously, these relative analyses prove that the designed NIRLLC controller is more reliable than the other controllers in all aspects for voltage tracking of an autonomous MG system.
Performance evaluation for singlephase autonomous MG system
Performance over different uncertainties
Uncertainties in a system arise on account of unknown load parameters, unmodeled load dynamics, load variation etc. In order to achieve robust performance, a controller must perform sensitively under various uncertainties. For robust analysis of the designed NIRLLC controller, multiplicative input uncertainty, inverse additive uncertainty and inverse multiplicative input uncertainty are imposed on the plant, whose block diagrams are depicted in Fig. 8a–c, respectively, where \(W_{0} (s)\), \(E_{0}\) and \(\Delta_{t} (s)\) represent plant transfer function, scalar weights and plant variation, respectively. The values of \(E_{0}\) and \(\Delta_{t} (s)\) are selected by considering 25% of reference amplitudes as plant variation. Effectiveness of the controller against all the uncertainties is shown in Fig. 8d–f. It is clear that the openloop responses become severely distorted because of plant variation, whereas the NIR controller and the designed NIRLLC controller show good performance, while the designed controller attains relatively higher damping than the NIR controller. It is worth mentioning that the literature and previous discussions indicate that the NIR has better responses than both MPC and LQR. Thus, it validates the claim of superior performance of the designed NIRLLC controller over other controller designs.
Performance over changing reference value
As the prime objective of this paper is to design a controller for tracking reference voltage rigorously, the performance of this controller is verified with varying reference value. The following conditions are considered for changing reference grid voltage, \(V_{G}^{ * }\):

\(V_{G}^{ * }\) = 200 V; 0 s < t < 0.035 s;

\(V_{G}^{ * }\) = 250 V; 0.035 s < t < 0.065 s;

\(V_{G}^{ * }\) = 150 V; 0.065 s < t < 0.1 s;
Figure 9 verifies the robust reference tracking performance of the designed NIRLLC controller, despite changing the reference value randomly. The NIR controller exhibits a greater magnitude error than the designed NIRLLC controller, and the NIR controller shows higher oscillations during an abrupt change of reference.
Performance over some conventional loads
Commonly, an MG system deals with ranges of known and unknown loads, and their characteristics may disturb normal operation. With the aid of the designed controller, these problems can be easily addressed. To verify the effectiveness of the designed NIRLLC controller, some common loads are modeled in Fig. 10, and a brief description of these loads is given in Table 11 in the “Appendix”.
Consumer load
This type of load is modeled in Fig. 10a, and improved voltage tracking of the designed NIRLLC controller for such load is demonstrated in Fig. 11a, f. Apart from having the lowest amplitude error, a higher amount of active power is evolved using NIRLLC controller as shown in Fig. l1k.
Harmonic load
Harmonics originate because of different nonlinear loads such as semiconductor devices, switching elements etc. These loads are the prime reason of overheating of motors, cables, and capacitors etc. In order to simulate the effects of harmonic loads, they are modeled as shown in Fig. 10b. The openloop and NIR controller in Fig. 11b, g show more transient oscillations, but the designed NIRLLC controller mitigates the oscillations and tracks the voltage waveform more accurately with fewer harmonics. It is apparent from Fig. 11l that the openloop can extract a very low amount of power, while NIR improves this problem significantly, but the designed NIRLLC has the highest power extraction capability.
Unknown load
Modeling of an unknown load is shown in Fig. 10c, while openloop, NIR and NIRLLC controller responses for this type of load are reported in Fig. 11c, h. It is seen that the designed NIRLLC controller tracks the voltage most effectively with least tracking error despite changing load dynamics. In correspondence to least magnitude error, a comparatively higher amount of power is derived for the NIRLLC controller as shown in Fig. 11m.
Nonlinear load
Often an MG system faces nonlinear loads, e.g., rectifiers, semiconductor devices, computers, printers, electronic lighting ballasts etc. For simulation purposes and simple representation, this type of load is configured as shown in Fig. 10d. Figure 11d, i show that the NIR controller performs better than the openloop system but exhibits some phase shift in voltage tracking. However, the designed NIRLLC controller diminishes the harmonics to a greater extent and has better voltage tracking capability than the others. In terms of power extraction, the designed NIRLLC controller also indicates the best performance as can be seen from Fig. 11n.
Dynamic load
Dynamic loads as configured in Fig. 10e have considerable effects on an MG system. Large transient oscillations in voltage waveform are noted for the openloop and NIR controller, while the designed NIRLLC controller effectively mitigates these oscillations and tracks the reference voltage with near zero tracking error, as shown in Fig. 11e, j. Moreover, relatively higher active power is also obtained for the designed NIRLLC controller as shown in Fig. 11o.
Quantitative analysis of simulation performances
Quantitative analysis for the openloop system, NIR and NIRLLC controllers is carried out with different loads. The THD analysis, and errors of RMS voltage and active power are investigated based on Fig. 11, and are presented in Tables 7, 8 and 9, respectively. Table 7 indicates that the lowest THD are obtained for all kinds of loads with the designed NIRLLC controller. This is followed by the NIR controller. In the case of RMS voltage error, the designed NIRLLC controller minimizes the error noticeably for all loads. Taking the average RMS voltage error, a maximum error of 17.5 V is found for the open loop system, followed by 0.52 V for NIR controller and 0.30 V for the NIRLLC controller. It is clear from Table 9 that the highest active power is extracted by the NIRLLC controller under all types of loads. On average, 1242.84 W active power is extracted with the designed NIRLLC controller. This is 5.06 W and 230.82 W higher than the NIR controller and the openloop system, respectively. These results demonstrate that the NIRLLC controller has better performance under various load conditions than the others.
Performance evaluation for threephase MG system
Simulation performance of the designed MIMO NIRLLC controller is examined by imposing various types of threephase loads, whose details are noted in Table 12 in the “Appendix”. Among different types of loads, consumer load is the most common form of load as depicted in Fig. 12a. The closedloop with the NIRLLC controller and openloop system responses are presented in Fig. 12e, i, respectively. These indicate that the closedloop system performs much better than the openloop system by keeping the load voltage within the desired 1 pu value, while the openloop system has a voltage profile of around 2 pu.
After connecting the nonlinear load as shown in Fig. 12b to the MG system, the NIRLLC controller keeps the load voltage stable and helps it return to its normal state (1 pu) within a minimum time period as shown in Fig. 12f. On the other hand, the output voltage moves from the desirable load level because of the insertion of nonlinear load as shown in Fig. 12j.
The unknown load for a threephase system is modeled in Fig. 12c, and the consequence of such load is shown in Fig. 12g, k for closedloop and openloop systems, respectively. The NIRLLC controller shows a desirable response against this changing load dynamics by maintaining the load voltage to the level of 1 pu, but the openloop system cannot meet the requirement at all.
In order to investigate the performance of the NIRLLC controller during unbalanced condition, an unbalanced load is modeled as shown in Fig. 12d. Because of the control action of the NIRLLC controller, imbalance among phases is controlled rigidly, while the open loop system fails to minimize the effects of unbalanced load as is clearly visible in Fig. 12h, l. Therefore, the desired level of load voltage is obtained for closedloop, but the openloop system completely loses its control after connecting the unbalanced load.
Power quality constraint measurement
Some power quality constraints, such as THD, voltage deviation and voltage imbalance ratio are considered in order to justify the use of the MIMO NIRLLC controller. For the steadystate condition, numerical values are measured for various loads and listed in Table 10. It is clear that all the measured values satisfy the standard IEEE Std1547 [50]. This affirms the robust performance of this NIRLLC controller for threephase MG technology.
Conclusion
This paper presents a leadlag compensator conjugated resonant controller, designed by following the negative imaginary theorem, abbreviated as NIRLLC controller for both singlephase and threephase autonomous MG systems. The efficacy of the proposed controller is proven by comparing its performance with LQR, MPC and NIR controllers and openloop response. From the simulation results and numerical analysis, the following can be stated:

Step response and bode plots confirm that the designed NIRLLC controller has better responses than the LQR, MPC and NIR controller for both singlephase and threephase MG systems. Furthermore, the Nyquist plot and rootlocus indicate that system stability is guaranteed.

The NIRLLC controller attains 139.64 dB damping which is 11.74 dB higher than its closest competitor, i.e., NIR controller. In addition, 722 rad/s higher bandwidth is obtained for the NIRLLC controller than the NIR controller.

The NIRLLC controller maintains its superiority for different uncertainties and for continuously changing reference value.

For a SISO system, the NIRLLC controller has the best performance in terms of THD and RMS voltage error, while it also has the capability to extract the highest amount of active power for several types of loads. Similarly, for the MIMO system, the NIRLLC controller maintains all power quality constraints within the IEEE Std1547 standard.

For both SISO and MIMO, the proposed NIRLLC controllers have the best voltage tracking capability for different load dynamics.
Availability of data and materials
Please contact author for data material request.
Abbreviations
 MG:

Microgrid
 NI:

Negative imaginary
 PV:

Photovoltaic
 DG:

Distributed generator
 ESS:

Energy storage system
 VSI:

Voltage source inverter
 LQR:

Linear quadratic regulator
 ILQR:

Integral linear quadratic regulator
 LQG:

Linear quadratic Gaussian
 ILQG:

Integral linear quadratic Gaussian
 PID:

Proportional integral derivative
 PI:

Proportional integral
 DSP:

Digital signal processing
 MPC:

Model predictive control
 THD:

Total harmonic distortion
 PWM:

Pulse width modulation
 PRC:

Proportional resonant controller
 PIRC:

Proportional integral resonant controller
 NIR:

Negative imaginary resonant
 LLC:

Leadlag compensator
 NIRLLC:

Negative imaginary resonant leadlag compensator
 PCC:

Point of common coupling
 IGBT:

Insulated gate bipolar transistor
 SISO:

Single input single output
 MIMO:

Multiple input multiple output
 RMS:

Root mean square
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Conceptualization, MYYUH and MRI; methodology, MYYUH and MRI; software, MYYUH; validation, MRI, TA and MRIS; formal analysis, MYYUH and MRI; writing—original draft, MYYUH; writing—review and editing, MRI, TA and MRIS; supervision, TA and MRIS. All the authors read and approved the final manuscript.
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Md. YahYa Ul Haque received his B.Sc. degree in Electrical and Electronic Engineering from Rajshahi University of Engineering & Technology (RUET). Currently, he is working as a Lecturer with the Department of EEE, Varendra University, Rajshahi. His research interests are renewable energy, power electronics, power system protection and control engineering.
Md. Rashidul Islam received the B.Sc. and M.Sc. degrees in electrical and electronic engineering (EEE) from the Rajshahi University of Engineering and Technology (RUET), Rajshahi, Bangladesh, in 2013 and 2017, respectively. He was a Lecturer with the Department of EEE, Varendra University, Rajshahi. He is currently working as an Assistant Professor with the Department of EEE, RUET. His research interests include nonlinear controller design and applications on renewable energy systems, the applications of power electronics in renewable energy, microgrid systems, and fault ride through capability augmentation. He received the University Gold Medal Award from the RUET. He also received the Prime Minister Gold Medal Award.
Tanvir Ahmed received the B.Sc. and M.Sc. degrees in electrical and electronic engineering from the Rajshahi University of Engineering and Technology (RUET), Rajshahi, Bangladesh, in 2009, and 2012, respectively, and the Ph.D. degree in electrical and information engineering from the University of Sydney, Australia, in 2017. Upon completion of the B.Sc. degree, he joined in electrical and electronic engineering department, RUET, where he is currently a Professor. His research interests include nonlinear optics, optical device, and optical communication.
Md. Rafiqul Islam Sheikh was born in Sirajgonj, Bangladesh, in October 1967. He received the B.Sc. (Eng.) and M.Sc. (Eng.) degrees from the Rajshahi University of Engineering & Technology (RUET), Bangladesh, in 1992 and 2003, respectively, and the Ph.D. degree from the Kitami Institute of Technology, Hokkaido, Kitami, Japan, in 2010, all in electrical and electronic engineering (EEE). He joined as a Lecturer with the EEE Department, RUET, in 1994, where he is currently a Professor. He is also working as a Vice Chancellor with RUET. His research interests are, power system stability enhancement by using FACTs devices, renewable energy technologies, smart grid, and load frequency control of multiarea power systems. He has published many technical journal and conference papers, and authored or coauthored three books, and three book chapters. Dr. Sheikh is the Fellow IEB and the member of BCS Bangladesh.
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Haque, M.YY.U., Islam, M.R., Ahmed, T. et al. Improved voltage tracking of autonomous microgrid technology using a combined resonant controller with leadlag compensator adopting negative imaginary theorem. Prot Control Mod Power Syst 7, 10 (2022). https://doi.org/10.1186/s41601022002314
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DOI: https://doi.org/10.1186/s41601022002314
Keywords
 Negative imaginary theorem
 Resonant controller
 Leadlag compensator
 Autonomous microgrid
 Voltage tracking