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Article

Frequency and State-of-Charge Restoration Method in a Secondary Control of an Islanded Microgrid without Communication

1
School of Electrical and Computer Engineering, Seoul National University, Seoul 08826, Korea
2
School of Integrated Technology, Gwangju Institute of Science and Technology (GIST), Gwangju 61005, Korea
*
Author to whom correspondence should be addressed.
Appl. Sci. 2020, 10(5), 1558; https://doi.org/10.3390/app10051558
Submission received: 2 January 2020 / Revised: 20 February 2020 / Accepted: 21 February 2020 / Published: 25 February 2020
(This article belongs to the Special Issue Microgrids II)

Abstract

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Featured Application

This work is applicable to a secondary control of distributed energy resources in a microgrid without using communication devices.

Abstract

This paper presents a control method for inverter-interfaced distributed generation (DG) and energy storage systems (ESSs) in an islanded microgrid. The proposed method is focused on secondary control, particularly frequency restoration and maintaining the ESSs’ state of charge (SOC). To recover frequency deviation due to load change, an ESS is used as a droop-controlled grid-forming source. However, the grid-forming ESS cannot manage its own SOC, since it cannot control its own output power; hence, grid-feeding DGs are used to maintain the SOC within a desired range. Management of the SOC, as well as frequency restoration, is conducted by using local controllers without any communication devices, since dependency on communication may deteriorate system reliability in the case of failure. The proposed method for maintaining SOC can be realized by adjusting the system frequency, which is the only value that can be measured locally with almost the same value at every node in a steady state. Frequency restoration can be achieved by a simple ON/OFF scheme of the integral controller with a hysteresis loop to solve problems caused by differences between frequency measurements or set points among DGs.

1. Introduction

The growth of distributed generation (DG) systems has provided many solutions to local energy demand and supply problems. The concept of the microgrid was introduced in the early 2000s [1,2]. One important characteristic of the microgrid is that it can be isolated from or connected to the main power grid. During grid-connected mode operation, the microgrid voltage is maintained by the main grid, and in this mode, the main grid manages load changes in the microgrid with little impact on the system frequency, since the main grid has large inertia relative to the microgrid. In contrast, during islanded mode operation, the microgrid has small or zero mass moment of inertia (e.g., a microgrid with only inverter-interfaced units) [3,4,5,6,7]. Due to their weak inertia, islanded microgrids are vulnerable to load changes. Therefore, controllable distributed generators in an islanded microgrid must respond quickly to frequency deviation.
Energy storage systems (ESSs) have been widely used as primary control units for mitigating the effects of load changes, due to their fast-acting capability [8,9,10,11]. Primary control involves grid support and load sharing, which are usually achieved by droop control, and hence can be implemented locally in a decentralized way. The conventional Pf droop control, virtual impedance loop-based control, adaptive droop control, and robust droop control are included in the droop control category as a primary control [12]. At the secondary control level, the state of charge (SOC) of ESSs and the frequency must be managed to operate an islanded microgrid securely. From the perspective of secondary control architecture, two approaches can be distinguished: centralized and decentralized [13]. Fully centralized control relies on a dedicated central controller with data-gathering capacity and extensive communication between the central controller and controlled units [13]. Hence, a fully centralized control method largely depends on a communication infrastructure that transfers all critical data for microgrid operation, and may limit system reliability in the case of communication failure. In particular, communication failures are more serious in islanded microgrids, since they are isolated from the main grid and must supply loads with limited resources. In contrast, in a fully decentralized control method, each unit only receives local data to operate the system and does not require full awareness of system-wide variables [14,15,16].
Most previous studies implemented a decentralized secondary control system using the multi-agent system (MAS) framework [17,18,19,20,21,22]. In reference [17], a secondary control method based on the MAS concept for microgrids is proposed as an alternative for the coordinated operation of microgrids. In reference [18], power flow calculations are performed to validate that the dispatched values from the market comply with the operational constraints. In [19], additional agents assigned to different tasks are shared by the DG units in proportion to their available unused capacity. A special case of MAS, i.e., a gossip-based technique, is proposed in [20]; here, different units exchange information regarding their operation, such as mismatches between programmed and actual power outputs, and marginal costs. In [21], additional agents that enable multi-stage operation scheduling of microgrids are included in a proposed architecture based on a MAS. A similar architecture, which considers demand-side bids and a sequential negotiation process, is proposed in [22]. Although MAS-based control strategies are largely based on agents’ autonomy and performed locally, they are still based on a communication procedure. Technically, therefore, they are not fully decentralized and are still exposed to the risks of communication failure.
In reference [23], a wireless load-sharing controller for islanding parallel inverters in an AC-distributed system is proposed. The resistive output impedance of the parallel-connected inverters in an islanded microgrid is considered in the proposed controller. However, this does not take secondary control into account. In reference [24], a decentralized voltage control algorithm that minimizes power losses in a microgrid is proposed. Although the power losses are reduced using the proposed method, it does not consider SOC control of electric vehicles or the frequency of the microgrid. In reference [25], a control method for DG units to implement active power sharing and frequency recovery in an islanded microgrid is proposed. By using self-frequency recovery control, the frequency can be restored to the nominal value in a decentralized way. However, to offset the power-sharing mismatches among DGs after frequency recovery, communication is applied momentarily.
In reference [26], the distributed controllers for secondary frequency and voltage control in islanded microgrids is proposed. The proposed controller used local information and communication to perform secondary control. The authors mentioned that the communication between DGs has been a core ingredient in achieving the goal of the secondary control, which makes this paper more noticeable since the main contribution of this paper is to get rid of the communication on a secondary control level. In reference [27], the distributed cooperative control in an islanded microgrid secondary control is proposed. The authors used event-triggered strategy to reset the actual values in the feedback control schemes. The proposed method makes a profound contribution in terms of reducing communication dependency among DGs, but it still uses the communication in the secondary control level. In reference [28], the authors proposed the restoration control method of droop-controlled inverter-based microgrids. In reference [29], the authors used a distributed event-triggered secondary control method to deal with the economic dispatch and frequency restoration control for microgrids consisting of droop-controlled DGs. The authors of [30] and [31] also proposed distributed control methods to restore the voltage and frequency deviation. Some distributed control methods are proposed to coordinate the secondary and tertiary control together [32,33,34]. However, all of them could not be performed in a communication-free manner.
In this paper, a fully decentralized control method for inverter-interfaced DGs, and an ESS without communication, are proposed. As reviewed in the previous works, the communication has been the most important but also the cost-inefficient ingredient in secondary control [26,27,28,29]. To the best of our knowledge, no literature has proposed a fully communication-free way in the secondary control of frequency and SOC restoration so far. In this context, this paper makes the major contribution of proposing a fully communication-free way of frequency and SOC restoration in the secondary control of islanded microgrids. Moreover, by introducing the communication-free secondary control for islanded microgrids for the first time, this paper can encourage many other future research projects on the secondary control of islanded microgrids without communication.
The proposed method assumed that all DGs and ESSs in an islanded microgrid have predetermined hourly output power set points, which are determined at the tertiary control level in accordance with the load pattern and economic benefits, so that the proposed method can be adapted more securely. Only the controllable DGs (i.e., diesel generator, fuel cell, biomass, etc.) are considered to adopt the proposed control method in this paper. The uncontrollable DGs such as renewable energy sources cannot or or partially (by using de-loaded control) able to adopt the proposed method. The proposed control method focuses on secondary control of DGs and the ESS. To ensure a rapid response to load changes, ESSs are used as droop-controlled grid-forming sources. When the SOC and/or frequency operating point deviates from the desired range, all grid-forming sources change their output frequencies. Grid-feeding DGs restore the frequency by changing their output power. To this end, we propose for grid-feeding DGs to use an integral control; however, if there are two or more units with integral control for frequency restoration, they conflict since the frequency measurements and/or the set points may differ from each other in the real world [25]. To prevent this problem, which is known as a hunting effect, an On/Off scheme for frequency integral controllers in grid-feeding DGs is also included in the proposed method, which is implemented to use local controllers and local information only without any communication devices to improve system reliability and reduce the installation cost. However, since this paper is focused on proposing the simple concept of the frequency recovery control without communication for the first time, the detailed analysis, such as stability analysis, has not been implemented. Hence, the scope of this paper is limited to the basic concept of the controller.
The rest of this paper is structured as follows. Section 2 briefly reviews conventional Pf droop control and introduces a droop coefficient determination method to synchronize the output powers of grid-forming units (ESSs in this paper), and hence permit other grid-forming units to estimate the SOC of the ESSs. Section 3 describes a method to integrate the SOC information into the frequency. Section 4 shows a controller for frequency restoration, Section 5 illustrates case studies verifying the effectiveness of the proposed methods, and Section 6 outlines the conclusions.

2. Sharing State-of-Charge (SOC) Information among Grid-Forming Units without Communication

To respond quickly to load changes, an ESS is proposed to be used as a grid-forming unit. Many studies have used ESSs as grid-feeding units for primary control [8,9,10,11], but a grid-forming unit reacts much faster than a grid-feeding unit and is able to share transient load changes, since a grid-forming unit is controlled as a voltage source [35]. By referring to [35], grid-forming control acts as a fixed-voltage source, and grid-feeding acts as a fixed-current source. For sharing a load change, conventional Pf droop control is used, and the relationship between the output active power and frequency of the grid-forming unit can be expressed as:
f o = f n o m m ( P o P r e f )
where fnom and Pref correspond to the nominal and reference values for frequency and output active power, respectively, and fo and Po correspond to the measured output frequency and active power, respectively. The coefficient m denotes the droop coefficient and is usually determined as [36]:
m = f n o m f m i n P m a x P m i n
where fmin is the allowable minimum value of the system frequency, and Pmax and Pmin are the maximum and minimum output power of a DG, respectively. fmin should be the same for all grid-forming units and Pmax and Pmin can be distinguished based on their power ratings and generation costs, etc. By adjusting the droop coefficients among grid-forming units, the proportion of load sharing can be determined as desired at the primary control level.
The main reason that ESSs have not been used as grid-forming units is that they cannot manage their own SOC, since a grid-forming type unit cannot control its own output power. To solve this problem, the output frequencies of all grid-forming units are adjusted to reflect the rough information of the SOC—i.e., whether the ESS should be charged or discharged—with respect to the frequency. To change the output frequencies of the grid-forming DGs almost simultaneously, other types of grid-forming DGs should know the SOC level of the grid-forming ESS. To achieve this without any communication devices at the secondary control level, it is assumed that all the hourly output power set points are predetermined, and the output power set point and droop coefficient of the ESS are given for every grid-forming DG. With those values known, other grid-forming DGs can estimate the output power of an ESS according to the following equations:
f o , E S S = f n o m m E S S ( P o , E S S P r e f , E S S )
f o , D G = f n o m m D G ( P o , D G P r e f , D G )
where the subscripts ESS and DG denote grid-forming ESS and another type of grid-forming DG, respectively. From the perspective of the ESS, mDG and Pref,DG are given. Since fo,DG is identical to fo,ESS, Equations (3) and (4) can be combined as:
m E S S ( P o , E S S P r e f , E S S ) = m D G ( P o , D G P r e f , D G )
Equation (5) can be rearranged in terms of Po,ESS as:
P o , E S S = m D G m E S S ( P o , D G P r e f , D G ) + P r e f , E S S
From the perspective of grid-forming DG, all variables on the right-hand side of Equation (6) are known, so the output power of the grid-forming ESS can be calculated by Equation (6). The SOC of the grid-forming ESS can be expressed as [37]:
S O C E S S = S O C E S S , i n i t P o , E S S C A P E S S d t
where SOCESS is the SOC of grid-forming ESS, SOCESS,init is the initial value of SOCESS, and CAPESS is the capacity of the grid-forming ESS. Assuming that SOCESS,init and CAPESS are known for every grid-forming DG, grid-forming DGs can estimate the SOC of the grid-forming ESS by using local parameters Equations (6) and (7), without any communication infrastructure.
In this way, all grid-forming units can share the SOC of the grid-forming ESS. It is important to share the SOC information among grid-forming units because this information is incorporated into the system frequency in the proposed method, and the system frequency can be adjusted only by grid-forming units. By measuring the system frequency locally, grid-feeding DGs can adjust their output power to charge or discharge the ESS and hence maintain the SOC within a desired range. The details are discussed in the next section.

3. Reflection of SOC into the System Frequency

For the grid-feeding DG units to know the SOC of the ESSs based on the system frequency, the grid-forming units must change their output frequency with respect to the SOC. For grid-forming units to change their output frequency appropriately and allow grid-feeding units to support SOC and frequency management, all possible cases where the SOC needs to be supported must be investigated. The SOC has to be supported when it deviates from the allowable operation range, which is determined by the system operator; this situation is closely related to the output power of the ESS and the system load change, as shown in Table 1, where PESS,ref and PESS are the reference power and output power of the ESS, respectively.
The sign of the ESS output power can be positive (discharging) or negative (charging). The case of zero output power is ignored because it does not cause any change in the SOC. It is assumed that, before the load change, the system is in a steady state and PESS is equal to PESS,ref. Hence, from Equation (1), the system frequency has a nominal value before the load change. In Table 1, Cases 1 and 10 never occur because the output power of the grid-forming ESS will not be increased/decreased after the load is decreased/increased. Similarly, Cases 5 and 12 occur neither since the sign of the output power will change without a load change.
In Cases 3 and 8, the status of the ESS is changed from charging/discharging to discharging/charging. In these cases, the discharging/charging status of the ESS causes a low/high SOC problem. A simple solution is to restore PESS to its reference value, so that the status of ESS can be changed again from discharging/charging to charging/discharging. This can be done by controlling grid-feeding units to recover the frequency to the nominal value (the details will be discussed in the next section).
However, there could be cases in which the frequency falls in the dead band range of the frequency support control of the grid-feeding units. Moreover, in the rest of the cases (Cases 2, 4, 6, 7, 9, and 11), frequency recovery cannot solve the low/high SOC problem since the sign of PESS is still the same as before the load change. In such cases, the output frequency of grid-forming DG must be changed by triggering the low/high SOC signal and hence allowing the grid-feeding DG units to measure the frequency deviation. By measuring the frequency deviation, grid-feeding DG units can adjust their power to restore the frequency and hence maintain the SOC (the details will be discussed in the next section). To this end, a frequency reference controller for grid-forming DG is proposed as shown in Figure 1, where SOCmin and SOCmax are the allowable minimum and maximum of the SOC operation range determined by the operator, Pres is the active power reference during SOC restoration, Psched is the hourly scheduled active power with respect to the system’s load pattern, and mPF is Pf droop coefficient.
As shown in Figure 1, the SOC signal enters into the comparators, which check whether the SOC drops below SOCmin or exceeds SOCmax. If one of those events occurs, the output of the comparator triggers the pulse and generates ‘1’ as the duration, which can be adjusted by the operator. Here, the duration is set as 1 h since the tertiary control time interval of Psched is also considered as 1 h. This time interval can be adjusted by the operator. If Psched is changed, the pulse (low/high SOC signal) is designed to be turned off so that the microgrid can be operated as scheduled data. Note that the output of the add/subtract component, ‘−1’ (low SOC signal) or ‘+1’ (high SOC signal) or ‘0’, will be multiplied by Pres. Since the low/high SOC signal is a step signal, Pres multiplied by the low/high SOC signal enters into the low-pass filter (LPF) to alleviate any step change. Otherwise, a large step change of fref occurs and may result in instability of the system. The switch shown in Figure 1 chooses node ‘a’ or ‘b’ to provide an active power reference as low-pass filtered Pres or Psched, respectively. The selection of the node is determined by the ‘charging/discharging signal’ shown at the bottom of Figure 1. Hence, Pref can be expressed as:
P r e f = { P s c h e d ,   if   Charge / Discharge   signal   is   0 P r e s , L P F ,   if   High   SOC   signal   is   1 P r e s , L P F ,   if   Low   SOC   signal   is   1
where Pres,LPF is the low-pass filtered Pres. The reason for predetermining Pref as a specific constant value while the low/high SOC signal is turned on is that Pref cannot be determined by some criterion considering the whole system. For instance, if communication is used, the charging/discharging active power reference can be determined by a central controller with consideration of the whole system. However, without communication, Pref cannot be determined in a centralized way and hence should be determined locally. By only using local measurements and a local controller, it is impossible to calculate an optimal Pref. Thus, for the sake of convenience, when the low/high SOC signal is turned on, Pref is predetermined as a specific value. The rest of the control scheme is the same as with conventional Pf droop control [35,36]. The parameters used in Figure 1 are shown in Table 2.

4. Frequency and SOC Restoration Control

As discussed in the previous section, if the SOC deviates from the allowable range, the system frequency is changed by adjusting Pref of grid-forming DGs (see Figure 1), to restore the SOC within the allowable range. grid-feeding DGs adjust their output power by sensing the frequency deviation; thus, both the frequency and the SOC can be maintained within the desired range.
For a single grid-feeding DG, it may be too great a burden to undertake all frequency and SOC restorations. Hence, two or more grid-feeding DGs are proposed to support the frequency only with local measurements. To recover the frequency to the nominal value using only local measurements, integral control of frequency error must be applied. However, in the real world, local measurements and settings can differ slightly from each other, which may cause a problem while recovering the frequency [38]. For instance, two different frequency controllers will conflict with each other when recovering the frequency to the nominal value when their frequency measurements differ. To address this problem, communication is used for secondary control in the real world. To eliminate the dependency on communication, an active power controller for a grid-feeding DG is proposed, as shown in Figure 2, where ∆fint is a binary signal, ‘1’ or ‘0’, to control the “PI On/Off switch”. If ∆fint is ‘1’, the switch is connected to node ‘a’ and the error between fnom and fo enters into the PI controller. If ∆fint is ‘0’, the switch is connected to node ‘b’ and the zero input enters into the PI controller. In other words, the PI controller acts as to eliminate the frequency deviation and yields a value to adjust the active power reference. Before adding this value to the active power reference, it passes the low-pass filter to prevent this value being changed in a step-wise way, and is added to Psched to yield Pref.
The core part of the grid-feeding DG’s active power controller is the process of generating the ∆fint signal, which is shown in Figure 3: the frequency deviation signal goes into the integrator through the dead band block, which prevents too-frequent activation of the ∆fint signal; hence, it tolerates a small deviation in the frequency. The absolute value of the integral of frequency deviation is compared to a certain constant value, Kint, to determine whether or not to restore the frequency. Note that the integrator is used to reflect not only the time, but also the magnitude of the frequency deviation. Kint can be adjusted by the system operator. By decreasing Kint, the frequency can be strictly adjusted to the nominal value but the output of the grid-feeding DG unit will be changed too frequently. The output of the comparator is multiplied by the output of the hysteresis loop, which yields ‘1’ or ‘0’. Hence, ∆fint will be set to ‘1’ to turn on the “PI On/Off switch” in Figure 2, only if both the comparator and the hysteresis loop outputs are ‘1’ will the “PI on/off switch” be on; otherwise, it will be turned off. The hysteresis loop plays a key role in turning off the switch. It outputs ‘1’ when the absolute value of the difference between fnom and fo exceeds a certain value, and outputs ‘0’ if the frequency difference is restored back to a certain other value. For instance, if the former and the latter values are 0.1 and 0.01, respectively, the hysteresis loop outputs ‘1’ if the absolute frequency difference exceeds 0.1 Hz, and outputs ‘0’ if the absolute frequency difference is restored back to 0.01 Hz. Once the hysteresis loop outputs ‘0’, ∆fint becomes ‘0’ and the integrator is reset. Without the proposed hysteresis loop control, secondary control without communication cannot be implemented. The parameters used in Figure 2 and Figure 3 are shown in Table 3.
In summary, the conventional droop control, which is one of the most widely used control methods, is used for the primary control in the proposed method. The proposed method is focused on the secondary control of restoring the frequency and the SOC. The methodology for this proposed control is just adding the active power reference changer for grid-forming unit as shown in Figure 1 and grid-feeding unit as shown in Figure 2 on to the conventional DG control schemes. The rate of active power reference change by the proposed part of the controller is small since we have added LPFs on them. Note that the change rate of the active power reference in the tertiary control is usually larger than that of the secondary control. However, it does not mean that the proposed method can perfectly guarantee the stability of the system. For precise analysis, the small-signal and large-signal stability have to be analyzed and all the parameters in Table 2 and Table 3 should be reconsidered according to the stability analysis. Since the scope of this paper is limited to the basic concept of the controller, the stability analysis and mathematical proof remain as future works.
Consequently, the proposed part of the controller acts as a small-signal change in the conventional droop-based DGs. So, if the conventional droop-based control scheme is stable against a small signal, the proposed methodology can be regarded as stable system. The small-signal stability of microgrids with droop-based DGs has been researched in many other works in the literature and can be referred to [39,40,41].

5. Simulation Results and Discussion

5.1. Simulation Environment

The proposed method was tested by simulation to prove its effectiveness. The microgrid studied in [25], [42,43,44] was modeled with a slight modification and is shown in Figure 4. The power rating of all DGs (DG1 and DG3 are grid-forming units and DG2 and DG4 are grid-feeding units) in the microgrid is 2 MVA and the line parameters are shown in Figure 4. DG1 and DG3 are ESSs and both have a capacity of 4 MWh. Since it takes too long to see the change in SOC in the simulation, the capacity of ESS is scaled down to 1/3600 of 4 MWh. This means that the change in SOC in 1 h can be seen in 1 second (1/3600 h) of simulation time. The Pf droop coefficient for both DG1 and DG3 is 0.01, and the Psched for all units is 0.4 MW.

5.2. Case 1—Frequency Restoration

In Case 1, two different control methods for frequency restoration are compared. They adopt an integral controller and the proposed controller, respectively, for grid-feeding units for frequency restoration. The purpose of this case is to test whether the grid-feeding units restore the frequency without causing any problems, such as the hunting effect, while frequency measurement error among grid-feeding units is simulated. To simulate this measurement error, 0.001 Hz is added to the frequency measured by DG4. The load is changed after 0.8 s of the simulation to cause a frequency deviation. Figure 5 shows the simulation results achieved using an integral controller.
As shown in Figure 5, the frequency drops at 0.8 s due to the load increment. Focusing closely on the zoom in part of the frequency, a measured frequency error among DGs can be observed. The active power of the grid-forming units immediately follows the load change at 0.8 s and hence changes their output frequency. Since grid-feeding units adopt an integral controller to restore the frequency, their active power increases after frequency deviation. However, even after the frequency is restored back to nearly 60 Hz, the active power of DG2 and DG4 does not remain as the steady-state value, but is instead increased and decreased, respectively. This is due to the measurement error, which exists in the real world. Since DG2 and DG4 measure smaller and larger values than 60 Hz, respectively, they keep increasing and decreasing the active power, respectively. Eventually, the system will collapse. Furthermore, if there are set point errors in frequency reference and/or controller gain, the system frequency will not be maintained at a steady-state value.
To overcome this real world problem, new controllers are proposed and the simulation results obtained using the proposed controller are shown in Figure 6. After the frequency deviation, grid-feeding units wait for the ∆fint signal to restore the frequency. Slightly after 1.2 s of simulation time, the ∆fint of DG2 activates earlier than that of DG4, since DG2 measures a smaller frequency value than DG4. At 1.5 s, the ∆fint of DG4 is turned off earlier than that of DG2, since DG4 measures a larger frequency value than DG2. By using this control scheme, the active powers of DG2 and DG4 can reach the steady-state value (see the zoom in part of the active power in Figure 6), even if there is a frequency measurement error (see the zoom in part of the frequency in Figure 6).

5.3. Case 2—SOC Restoration

This case shows that the proposed controller can be used to restore both the frequency and SOC without using communication. In this case, it is assumed that the SOCs of all grid-forming units are exactly the same.
As shown in Figure 7, the SOC drops below SOCmin (set as 20%) at 0.8 s. Subsequently, the low SOC signal (see Figure 1) is turned on and the grid-forming units change their Pref to Pres (see Figure 1). Note that the active power of grid-forming units in Figure 7 did not change at 0.8 s. This means that there is no load change and the frequency is changed only to notify other grid-feeding units of the SOC shortage. After less than 0.2 s, the ∆fint of the grid-feeding units is turned on and the grid-feeding units start to restore the frequency by increasing their output. Simultaneously, by increasing the output of the grid-feeding units, the output of the grid-forming units becomes Pres (set as –0.5 MW) and the SOC is restored back to above SOCmin.

5.4. Case 3—Existence of SOC Difference among Energy Storage Systems (ESSs)

Unlike Case 2, the SOC may not always be identical among ESSs. In Figure 8, simulation results are shown to illustrate the performance of the proposed controller while the SOCs differ among grid-forming units. Here, the SOC of DG3 is 1% larger than that of DG1. At 0.8 s, the SOC of DG1 drops below SOCmin (20%) and the output frequency drops due to the change in Pref. However, the SOC of DG3 is still above SOCmin immediately after 0.8 s, and DG3 does not change its Pref. Therefore, the two grid-forming units instantaneously output different frequencies. Since DG1 outputs a lower frequency than DG3 at 0.8–0.86 s, the output powers of DG1 and DG3 are decreased and increased, respectively. Consequently, the SOC of DG3 drops faster, and finally drops below 20%. At 0.99 s, ∆fint of the grid-feeding units is turned on and the frequency and SOC are restored.
In Figure 9, simulation results of a larger SOC difference between DG1 and DG 3 are shown. Here, the SOC of DG3 is 5% larger than that of DG1 in order to prove the robustness of the proposed control method in for the worse situation. As shown in Figure 9, DG1 and DG3 deviated their output power from the initial value in an opposite direction for a longer period than that of 1% SOC difference case in order to set their difference smaller. At 1.17 s, both SOCs are increased and thereby prove they worked as intended.
To show a more extreme case, even larger SOC difference among DG1 and DG3 is tested. In Figure 10, simulation results of 10% SOC difference among DG1 and DG 3 are shown. As shown in Figure 10, DG1 and DG3 deviated their output power from the initial value in an opposite direction for a longer period than that of the 5% SOC difference case in order to set their difference smaller. The cases of SOC difference of 1%, 5%, and 10% take 0.22 s, 0.37 s, and 0.56 s, respectively, to start to recover their SOCs within the allowable range. Interestingly enough, for all cases including Case 2 (zero SOC difference), the maximum SOC drop (the minimum SOC) is all the same in every case. It is slightly above 18%. From these simulation results, it can be concluded that the system can be stably operated even for a larger SOC difference among DGs.
SOC difference larger than 10% can be regarded as a problem of SOC estimation and/or the tertiary control level and hence should be solved in terms of a different category. Otherwise, utilizing only a single ESS as the grid-forming unit could be one of the solutions for the SOC difference problem.
By conducting various simulations, the proposed controller is proved to be effective in many cases. However, it is worth noting that this paper is focused on the basic concept of the controller and hence the stability of the system should be further analyzed.

6. Conclusions and Future Works

The reliability of a microgrid is degraded by dependency on a communication system; however, due to problems such as the hunting effect, the frequency restoration process during secondary control of an islanded microgrid (or power system) relies on a communication system. To alleviate this dependency and hence enhance system reliability, new controllers are proposed for grid-forming and grid-feeding DGs in an inverter-based islanded microgrid. The performance of the proposed controllers focuses on the restoration of the frequency and the SOC without using communication.
The simulation is conducted by using MATLAB/SimPowerSystems and the results show that the proposed controller restores not only the frequency, but also the SOC by using only local controllers and data. Furthermore, no stability problems were identified, even with a frequency measurement error among DGs and the SOC difference up to 10% among grid-forming ESS units. From simulation results, it can be noted that an even larger SOC difference can be handled.
To achieve whole-system operation without communication, further control strategies must be developed. For instance, load shedding and reconnection schemes without communication are required to enhance system reliability. After developing such control strategies, others could also be developed step by step and a whole-operation procedure without communication could finally be realized. Furthermore, the stability analysis of the system should be studied in a future work to guarantee the reliability of the proposed controller.
To test the validity of the proposed method in a larger-scale microgrid also remains a future work. However, since the microgrid is usually a small-scale system consisting of several DGs, the scalability of the proposed methods is less important.
It is noticeable that the proposed method is focused on the secondary control only. To share the SOC information among grid-forming ESS units, it still needs some information from the tertiary control level where the communication is necessary. However, the tertiary control level needs a much lower frequency of information updates than the secondary control level. Hence, although it cannot abandon the communication infrastructure for the whole system control hierarchy, the dependency on communication is at least able to be alleviated by using the proposed control method.

Author Contributions

Investigation and methodology, J.-O.L.; conceptualization, supervision, project administration, and writing, Y.-S.K. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the Ministry of Education, grant number NRF-2018R1D1A1A02085348.

Acknowledgments

This research was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (NRF-2018R1D1A1A02085348).

Conflicts of Interest

The authors declare no conflict of interest.

References

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Figure 1. Proposed frequency reference controller for a droop-controlled grid-forming distributed generation (DG).
Figure 1. Proposed frequency reference controller for a droop-controlled grid-forming distributed generation (DG).
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Figure 2. Proposed active power reference controller for grid-feeding distributed generation (DG).
Figure 2. Proposed active power reference controller for grid-feeding distributed generation (DG).
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Figure 3. Proposed frequency deviation signal generator.
Figure 3. Proposed frequency deviation signal generator.
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Figure 4. One-line diagram of the studied microgrid.
Figure 4. One-line diagram of the studied microgrid.
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Figure 5. Frequency restoration results achieved using the integral controller.
Figure 5. Frequency restoration results achieved using the integral controller.
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Figure 6. Frequency restoration results obtained using the proposed controller.
Figure 6. Frequency restoration results obtained using the proposed controller.
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Figure 7. SOC restoration results when the SOCs are same.
Figure 7. SOC restoration results when the SOCs are same.
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Figure 8. SOC restoration results for SOC difference of 1% between DG1 and DG3.
Figure 8. SOC restoration results for SOC difference of 1% between DG1 and DG3.
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Figure 9. SOC restoration results for SOC difference of 5% between DG1 and DG3.
Figure 9. SOC restoration results for SOC difference of 5% between DG1 and DG3.
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Figure 10. SOC restoration results for SOC difference of 10% between DG1 and DG3.
Figure 10. SOC restoration results for SOC difference of 10% between DG1 and DG3.
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Table 1. All possible cases of state-of-charge (SOC) change.
Table 1. All possible cases of state-of-charge (SOC) change.
Case No.Steady StateTransient StateAfter Load Change
Sign 1 of PESS,ref
(= Sign of PESS)
Load ChangeSign 1 of PESSPossible Risk
1+IncreaseN/A
2+Low SOC
3DecreaseHigh SOC
4+Low SOC
5No changeN/A
6+Low SOC
7IncreaseHigh SOC
8+Low SOC
9DecreaseHigh SOC
10+N/A
11No changeHigh SOC
12+N/A
1 Positive and negative signs for discharge and charge, respectively.
Table 2. Parameters used in Figure 1.
Table 2. Parameters used in Figure 1.
SOCmin (%)SOCmax (%)Time Constant of Low Pass Filter (s)Droop Coefficient, mPF (pu)
20900.00010.01
Table 3. Parameters used in Figure 2 and Figure 3.
Table 3. Parameters used in Figure 2 and Figure 3.
Proportional Gain (pu)Integral Gain (pu)Time Constant of LPF (s)Dead Band Range (Hz)Kint (Hz∙s)Hysteresis Loop ON/OFF Value (Hz)
0.000050.00060.03± 0.1500.1/0.01

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Lee, J.-O.; Kim, Y.-S. Frequency and State-of-Charge Restoration Method in a Secondary Control of an Islanded Microgrid without Communication. Appl. Sci. 2020, 10, 1558. https://doi.org/10.3390/app10051558

AMA Style

Lee J-O, Kim Y-S. Frequency and State-of-Charge Restoration Method in a Secondary Control of an Islanded Microgrid without Communication. Applied Sciences. 2020; 10(5):1558. https://doi.org/10.3390/app10051558

Chicago/Turabian Style

Lee, Jin-Oh, and Yun-Su Kim. 2020. "Frequency and State-of-Charge Restoration Method in a Secondary Control of an Islanded Microgrid without Communication" Applied Sciences 10, no. 5: 1558. https://doi.org/10.3390/app10051558

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