Journal of Modern Power Systems and Clean Energy

ISSN 2196-5625 CN 32-1884/TK

网刊加载中。。。

使用Chrome浏览器效果最佳,继续浏览,你可能不会看到最佳的展示效果,

确定继续浏览么?

复制成功,请在其他浏览器进行阅读

Two-stage Optimization for Active Distribution Systems Based on Operating Ranges of Soft Open Points and Energy Storage System  PDF

  • Can Wang
  • Jianjun Sun
  • Meng Huang
  • Xiaoming Zha
  • Wei Hu
the School of Electrical Engineering and Automation, Wuhan University, Wuhan 430072, China; the State Grid Hubei Electric Power Corporation, Wuhan 430070, China

Updated:2023-01-20

DOI:10.35833/MPCE.2022.000303

  • Full Text
  • Figs & Tabs
  • References
  • Authors
  • About
CITE
OUTLINE

Abstract

Due to the lack of flexible interconnection devices, power imbalances between networks cannot be relieved effectively. Meanwhile, increasing the penetration of distributed generators exacerbates the temporal power imbalances caused by large peak-valley load differences. To improve the operational economy lowered by spatiotemporal power imbalances, this paper proposes a two-stage optimization strategy for active distribution networks (ADNs) interconnected by soft open points (SOPs). The SOPs and energy storage system (ESS) are adopted to transfer power spatially and temporally, respectively. In the day-ahead scheduling stage, massive stochastic scenarios against the uncertainty of wind turbine output are generated first. To improve computational efficiency in massive stochastic scenarios, an equivalent model between networks considering sensitivities of node power to node voltage and branch current is established. The introduction of sensitivities prevents violations of voltage and current. Then, the operating ranges (ORs) of the active power of SOPs and the state of charge (SOC) of ESS are obtained from models between networks and within the networks, respectively. In the intraday corrective control stage, based on day-ahead ORs, a receding-horizon model that minimizes the purchase cost of electricity and voltage deviations is established hour by hour. Case studies on two modified ADNs show that the proposed strategy achieves spatiotemporal power balance with lower cost compared with traditional strategies.

I. Introduction

WITH the higher penetration of wind turbines (WTs) and other distributed generators (DGs) [

1], uncertainties in their outputs exacerbate power imbalances between different networks in the space dimension and expand peak-valley differences in net load within a network in the time dimension [2]. Under this context, soft open points (SOPs) [3], which can transfer active power between networks and compensate reactive power spatially, and energy storage systems (ESSs) [4], which can shift peak power to valley power temporally, have been widely studied. Combined with other regulatory devices, better system operation states can be achieved in active distribution networks (ADNs) [5].

SOPs were originally proposed in [

3] and consist of voltage source converters (VSCs) connected by capacitors. A simulation case composed of three IEEE standard networks was analyzed in [5], where a five-terminal SOP worked as an energy hub that transferred active power between networks. To cope with the complex uncertainties imposed by photovoltaic generations, a real-time scheduling method with SOPs via a multi-timescale framework was proposed in [6], where SOPs were coordinated with on-load tap changer (OLTC), shunt capacitor bank (SCB), and series voltage regulator (SVR). A two-stage robust model was established in [7] to address the uncertainties of photovoltaic outputs, where SOPs were adopted to eliminate voltage violations and reduce the power losses. For a three-phase unbalanced condition in an ADN, an SOP-based operation strategy was proposed in [8], where power losses were reduced and the three-phase unbalance was mitigated. A data-driven operation strategy of SOP was proposed in [9] with inaccurate parameters and frequent changes of operation states, where multiple SOPs were used to connect different areas inside a single ADN. SOPs integrated with ESS were proposed in [10] to improve the flexibility in ADNs, where losses of SOP with energy storage were modeled considering its subsystems. In addition, two IEEE 33-node networks were connected via a SOP with ESS in [10]. Considering the flexible interconnection and multiple application conditions introduced by SOPs, balancing power between different ADNs with the active power transfer of SOPs is another application scope.

To assess the power imbalance condition [

11] and other existing problems in ADNs [5], the coordination of multiple regulatory devices has been studied. To mitigate the imbalance condition of feeder loads, an enhanced SOCP-based method via a multiterminal SOP was proposed in [11]. In addition, SOPs were also applied in the load balance of different feeders in an ADN in [12], which performed better than the network reconfiguration. Aiming at the power flow fluctuation and load imbalance condition caused by the large-scale integration of DGs, a multiterminal SOP was coordinated in [13] with DGs, OLTC, and controllable loads, where the SOP flexibly connected feeders in the distribution network. In sum, SOPs together with other devices are able to balance power spatially and temporally.

Optimization results from the day-ahead stage can provide promising references for the intraday stage with the coordination of the day-ahead stage and the intraday stage. Based on day-ahead load forecast data, the hourly reactive power of DGs was determined in [

12] in coordination with switching operations of OLTC and SCBs. Differences between actual and forecast load data were assumed to be small in [12], the strategy of which lacked reference for the intraday stage. A multi-timescale framework for volt/var optimization was proposed in [13], which coordinated the tap changer on a slow timescale (hourly basis) and the ESS on a fast timescale (15-min basis). The ESS power setpoints obtained in the first stage had no connection to the results in the second stage. The operation curve for the state of charge (SOC) of ESS was predetermined in a day-ahead model in [14], which was unchangeable in the intraday dispatch stage. Since the intraday hourly forecast data may differ greatly from day-ahead data, the intraday rescheduling of an ESS based on day-ahead schemes should be studied. Moreover, in the day-ahead stage, optimization results of SOPs that may provide beneficial references for intraday corrective control are always omitted [14]. An ESS in the intraday stage was dispatched hourly within the optimized SOC limits obtained from the day-ahead stage in [15], where the limits worked as operating ranges (ORs) for the ESS. Therefore, two stages should be coordinated optimally, where the optimal decisions of the intraday stage should be based on the day-ahead schedule.

To cope with the uncertainties of loads and outputs of DGs, robust optimization and stochastic optimization have been widely studied. To ensure the robustness of dispatch decisions under the uncertainties of DGs, a distributionally robust real-time power dispatch model for a coupled transmission grid and ADNs was proposed in [

16]. The proposed stochastic framework in [17] considered the uncertainties of DGs, which were converted to deterministic problems with probabilities. A stochastic model was established to minimize power losses and avoid voltage violations in [18], taking load forecast errors into account. Nevertheless, stochastic programming relies heavily on the accurate formulation of the probability density function, which may be difficult to obtain, while conservativeness can only be reduced but not eliminated in the robust model.

The alternating direction multiplier method (ADMM) is a promising distributed method that can be applied to the optimization of power systems [

19]. For a large-scale ADN with a given division of areas, an ADMM was used to carry out a distributed reactive optimization in [20]. For large numbers of scenarios, it will take the method like the ADMM more time to complete the whole optimization if specific power flow constraints such as DistFlow constraints are included in the model. In this context, a sensitivity-based method can accelerate the computation but with a loss of accuracy. A straightforward analytical derivation of node voltage and line current sensitivities was provided in [21] based on the sparse compound matrix Y. The sensitivities of node voltages with respect to the OLTC were calculated to estimate the voltage in [22]. Similarly, an efficient sensitivity calculation method was used in [23] to update the voltage sensitivities online with respect to the settings of discrete-acting devices. Consequently, to improve the computational efficiency of optimal power flow in massive scenarios, the sensitivity-based optimization method can be adopted.

Motivated by the above facts, to work against spatial power imbalances between networks and temporal power imbalances inside a network and offer a flexible intraday regulation strategy for SOPs and ESSs, this paper focuses on presenting an optimization strategy for flexibly interconnected ADNs under WT uncertainty, including the day-ahead scheduling and intraday corrective control stages. The main contributions of this paper are summarized as follows.

1) To address the limitations of the day-ahead scheduling stage, which provides reference curves for the intraday corrective control stage, ORs of active power of SOPs and the SOC of ESS are constructed from optimization results of large numbers of stochastic scenarios generated by WT uncertainty, of which the total cost is less than that of fixed operation curves in ADNs.

2) To improve the computational efficiency of ORs obtained from the results in large numbers of stochastic scenarios, each network-connected SOP is equivalent to an entity with net loads. Then, current and voltage sensitivities with respect to node power to prevent violations are considered rather than specific power flow constraints, which guarantees the effectiveness of ORs.

The rest of this paper is organized as follows. Section II outlines the framework of spatiotemporal power balance. Sections III and IV formulate the power balancing models in the day-ahead scheduling stage and intraday corrective control stage, respectively. Section V provides the implementation algorithm. Section VI presents the numerical results and an analysis of two modified flexibly interconnected ADNs. Finally, Section VII concludes the paper.

II. Framework of Spatiotemporal Power Balance

A. Flexibly Interconnected ADNs

A flexible network consisting of multiple ADNs interconnected by SOPs has been studied in this paper. An example is shown in Fig. 1, where a two-terminal SOP connects two IEEE 33-node ADNs. ESS is applied to regulate active power while SCBs and static var compensator (SVC) are applied to regulate reactive power within network.

Fig. 1  Two IEEE 33-node ADNs connected by a two-terminal SOP.

B. Coordination of Two Stages

A two-stage optimization strategy for spatiotemporal power balancing in flexibly interconnected ADNs is proposed in this paper. The timescales for the two stages are 24 hours and 1 hour, respectively. The framework of the proposed strategy is shown in Fig. 2, where x1 is the purchase cost of electricity; x2 is the voltage deviation; x3 is the computing time; and x4 is the voltage or current violation.

Fig. 2  Framework of proposed strategy.

Different from continuous-acting devices such as SOPs and ESSs, SCBs are discrete-acting devices. SCB schedules are generated through stochastic optimization.

First, large numbers of stochastic scenarios are generated through the Monte Carlo method according to the day-ahead forecast error of WT power, denoted as Ωsensto. Then, the K-means cluster algorithm is adopted to generate several typical scenarios, denoted as Ωsentyp. Finally, SCB schedules are obtained through stochastic optimization based on typical scenarios. In addition, the SCB schedules will not be changed in the intraday corrective control stage.

In the day-ahead scheduling model between networks, each ADN is equivalent to an entity only with net active and reactive loads to improve computation efficiency in massive scenarios. Meanwhile, sensitivities are introduced to prevent violations of voltage and current in ADNs with the integration of an SOP instead of specific power flow constraints. Since active power can be transferred through the SOP, the SOP is applied to balance power spatially. In the day-ahead scheduling stage, with the objective of minimizing the sum of the purchased active power in 24 hours from all networks, the optimal active power of SOP in each scenario is obtained.

For the generation of OR, the forecast error range is divided equally into several error intervals considering WT uncertainty first. Then, considering Ωsensto, power flow optimization is carried out in each scenario. Based on the optimization results, the upper and lower limits of the active power of SOP and the SOC of ESS are chosen as the OR in each error interval. The whole OR consists of the ORs in all error intervals. To apply ORs in the intraday stage, the error interval in which the forecast error of WT power is located is determined first. Then, the OR in this interval is selected as the OR for the active power of SOP and the SOC of ESS.

In the day-ahead scheduling model within a single network, considering detailed power flow constraints, the power of the ESS and SVC is optimized with the objective of minimizing the weighted sum of peak-valley differences of purchased active power based on the optimal active power of the SOP. Similarly, ORs of the SOC of ESS can be constructed. Because the purchase cost of electricity is the main focus of the power balance and the reactive power has little effect on it, the reactive power of the SVC is omitted in the day-ahead scheduling stage.

In the intraday corrective control stage, the optimization model is established and solved by the ADMM hourly. First, specific ORs of the SOP and ESS should be determined based on hourly forecast errors compared with day-ahead forecast data. Then, with the objective of minimizing the weighted sum of the purchase cost of electricity and voltage deviations, the active power of SOP and the SOC of ESS are optimized in determined ORs, while the reactive power of SOP and SVC is regulated within capacity. Finally, according to the optimization results, the power of the SOP, ESS, and SVC is adjusted hourly by the distribution network operator.

The final optimization results indicate that the proposed strategy using ORs performs better than the traditional strategy. Meanwhile, it takes the equivalent model less time than the detailed model to complete optimization in massive scenarios. In addition, voltage or current violations never occur in the equivalent model when considering sensitivities. By comparison, voltage violations occur in the equivalent model without considering sensitivities.

III. Power Balancing Model in Day-ahead Scheduling Stage

A. Determination of Schedule for Discrete-acting Devices

1) Objective Function

The model to determine the schedule for discrete-acting devices such as SCB minimizes the weighted total purchase cost of electricity from the upstream grid in all typical scenarios Ωsentyp.

(P0)  minfda=pωm=1Nt=1TctpurPm,t,ωup    ωΩsentyp (1)

2) Power Flow Constraints

The DistFlow model is adopted to model the power flow in the ADN. The mathematical formulations can be described as:

ikΦbrPik,t,ω-Pji,t,ω-rjiiji,t,ω=Pi,t,ωikΦbrQik,t,ω-Qji,t,ω-xjiiji,t,ω=Qi,t,ωPi,t,ω=Pi,t,ωWT+Pi,t,ωSOP+Pi,t,ωdis-Pi,t,ωch-Pi,t,ωldQi,t,ω=Qi,tSCB+Qi,t,ωSVC+Qi,t,ωSOP-Qi,t,ωldui,t,ω-uj,t,ω+rij2+xij2iij,t,ω=2rijPij,t,ω+xijQij,t,ωiij,t,ωui,t,ω=Pij,t,ω2+Qij,t,ω2 (2)

3) SOP Constraints

Active power can be transferred between different terminals through the SOP, and reactive power can be compensated by the SOP. The SOP operation constraints can be written as:

Pi,t,ωSOP2+Qi,t,ωSOP2SiSOP2iΨndSOPPi,t,ωSOP+iΨndSOPPi,t,ωSOP,L=0Pi,t,ωSOP,L=AiSOPPi,t,ωSOP2+Qi,t,ωSOP2 (3)

4) ESS Constraints

During one period, active power can only be charged into the ESS or discharged from the ESS. In addition, the SOC of ESS is also constrained.

γi,t,ωdis+γi,t,ωch1    γi,t,ωdis,γi,t,ωch{0,1}0Pi,t,ωchPi,maxchγi,t,ωch0Pi,t,ωdisPi,maxdisγi,t,ωdisEi,ini,ω=Ei,T,ωEi,t,ω=Ei,t-1,ω+ηichPi,t,ωchΔtSiESS-Pi,t,ωdisΔtηidisSiESSEminEi,t,ωEmax (4)

5) SVC Constraints

The reactive power of the SVC can be adjusted continuously, and the operation constraint of the SVC is expressed as:

Qi,minSVCQi,t,ωSVCQi,maxSVC (5)

6) SCB Constraints

Different from the SVC, the reactive power of the SCB is adjusted by switching discrete banks on or off.

Qi,tSCB=Ni,tSCBqSCB0Ni,tSCBNmaxSCBt=1TNi,tSCB-Ni,t-1SCBmaxSCB (6)

7) Security Constraints

ui,minui,t,ωui,max0iij,t,ωiij,max (7)

The decision variables of P0 are shown in (8).

xda=Ni,tSCB (8)

Since optimizing SCB schedules is not the main focus of this paper, algorithm details for solving the model will not be included here. If power flow constraints and SOP constraints are transformed into convex constraints, a mixed-integer second-order cone programming (MISOCP) algorithm can be applied here. The transformation of nonconvex power flow constraints can be reviewed in [

16]. Otherwise, a heuristic algorithm such as the particle swarm optimization (PSO) algorithm is another choice.

B. Equivalent Power Balancing Model Between Networks

1) Objective Function

The power balancing model between networks minimizes the total purchased active power from the upstream grid. According to the power flow calculation formulas, the purchased active power equals the sum of net active loads and active power loss in an ADN. Consequently, the objective function in scenario ω from Ωsensto is expressed as:

(P1)  minfωda,o=m=1Nt=1TPm,t,ωnl-Pm,t,ωSOP+ijΦbrmim,ij,t,ωrij,m (9)

2) Sensitivity Constraints

To prevent voltage and current violations, the sensitivities of node power to voltage and current are considered. The computation of sensitivities can be reviewed in [

24].

The power flow calculation formula of the Newton-Raphson method is shown in (10).

ΔPt,ωΔQt,ω=Jt,ωPθJt,ωPUJt,ωQθJt,ωQUΔθt,ωΔUt,ω    ωΩsensto (10)

According to (10), the deviation of node voltage with respect to node power can be written as:

ΔUt,ω=J1,t,ωΔQt,ω-J2,t,ωΔPt,ωJ1,t,ω=Jt,ωQU-Jt,ωQθJt,ωPθ-1Jt,ωPU-1J2,t,ω=Jt,ωQθJt,ωPθ-1 (11)

Therefore, the computation of the updated node voltage can be expressed as:

Ut,ω'=Ut,ω0-ΔUt,ω (12)

For the sensitivity of branch current with respect to node active power, the computation formula of branch current can be expressed as:

Iij,t,ω=Ui,t,ω2+Uj,t,ω2-2Ui,t,ωUj,t,ωcosθij,t,ωrij2+xij2 (13)

According to the full differential formula, the sensitivity of the branch current with respect to the node active power and node reactive power is shown in (14).

Iij,t,ωPk,t,ω=Iij,t,ωUk,t,ωUk,t,ωPk,t,ω+Iij,t,ωθk,t,ωθk,t,ωPk,t,ωIij,t,ωQk,t,ω=Iij,t,ωUk,t,ωUk,t,ωQk,t,ω+Iij,t,ωθk,t,ωθk,t,ωQk,t,ω (14)

Formula (14) can be transformed into matrix form, which is expressed as:

Mt,ωIθMt,ωIU=Jt,ωPθJt,ωPUJt,ωQθJt,ωQUδt,ωIPδt,ωIQ (15)

Therefore, the calculation formula of elements in the sensitivity matrix is shown in (16).

δt,ωIPδt,ωIQ=JT-1Mt,ωIθMt,ωIU (16)

The updated branch current with sensitivity is expressed as:

It,ω'=It,ω0-ΔIt,ωΔIt,ω=δt,ωIPΔPt,ω+δt,ωIQΔQt,ω (17)

Moreover, the node voltage magnitude and branch current must comply with the security constraint (7).

The decision variables of P1 are shown as:

xωda,o=Pi,t,ωSOP,Qi,t,ωSOP (18)

3) ORs of SOP

In the day-ahead scheduling stage, ORs are composed of ORs in each hour. It should be emphasized that the ORs of the active power of SOP are constraints about its active power, designed for intraday hourly optimization. For period t, the whole forecast interval is equally divided into several small intervals. The minimum and maximum values of Pi,t,ωSOP in each small interval are chosen as the bounds for the OR. An example of the ORs of active power of the SOP can be found in Fig. 2. Formulas of the ORs of active power of SOP are shown as:

Pi,t,k,minSOPPi,t,kSOPPi,t,k,maxSOP    εmin+k-1εsεk<εmin+kεsεs=εmax-εminNE1kNEPi,t,k,minSOP=minωΞkεPi,t,ωSOPPi,t,k,maxSOP=maxωΞkεPi,t,ωSOP (19)

C. Power Balancing Model Within Network

1) Objective Function and Constraints

To further obtain the ORs of the SOC of ESS for the subsequent intraday stage, each network has to be optimized separately. For each single network, the power balancing model minimizes the sum of purchased active power and its weighted sum of peak-valley differences, which is shown in (20). The research subject is network m in scenario ω from Ωsensto.

(P2)  minfm,ωda,i=t=1TPm,t,ωup+tc1,tc2Θcupαm,c,ωPm,tc1,ωup-Pm,tc2,ωup (20)

The hourly purchased active power before optimization, denoted as Pm,t,ωup,b, is sorted in ascending order. Then, by pairing the head and tail active power, 12 pairs are formed. Each pair is weighted from high to low to show that reducing the maximum valley-peak difference is the most important step. The formula of weight is shown in (21).

αm,c,ω=Pm,tc1,ωup,b-Pm,tc2,ωup,btc1,tc2ΘcupPm,tc1,ωup,b-Pm,tc2,ωup,b (21)

To transform the objective to the linear form of decision variables, variable substitutions are made, and related constraints are added, as shown in (23).

minfm,ωda,i=t=1TPm,t,ωup+tc1,tc2Θcupαm,c,ωΔPm,ω,tc1,tc2up (22)

s.t.

ΔPm,ω,tc1,tc2upPm,tc1,ωup-Pm,tc2,ωupΔPm,ω,tc1,tc2upPm,tc2,ωup-Pm,tc1,ωup (23)

Constraints of P2 mainly include (3), (4), (5), and (7). The decision variables of P2 are shown as:

xωda,i=Pi,t,ωch,Pi,t,ωdis,Ei,t,ω (24)

2) ORs of ESS

Similar to the above steps, we can obtain the ORs of SOC of ESS as:

Ei,t,k,minEi,t,kEi,t,k,max    εmin+(k-1)εsεk<εmin+kεsεs=εmax-εminNE1kNEEi,t,k,min=minωΞkεEi,t,ωEi,t,k,max=maxωΞkεEi,t,ω (25)

IV. Power Balancing Model in Intraday Corrective Control Stage

The ORs of the active power of SOP and the SOC of ESS are constructed in the day-ahead scheduling stage, which provides operating bounds for the SOP and ESS in the intraday hourly optimization model.

Generally, day-ahead forecast data are not the same as intraday hourly forecast data. Herein, corrective control must be performed on the power of the SOP and ESS hourly based on day-ahead schedules. Since optimization is carried out hourly during the day, a detailed model can be established. Meanwhile, the objective function minimizes the weighted sum of the hourly purchase cost of electricity from the upstream grid and the voltage deviations.

(P3)  minfin=αupm=1Nt=1TctpurPm,tupfmup+αvdm=1NiΨndmt=1Tui,m,t-1fmvd (26)

αup and αvd are obtained by the analytical hierarchy process (AHP) method. Variable substitution is applied to transform the objective function into a linear form.

minfin=αupm=1Nt=1TctpurPm,tupfmup+αvdm=1NiΨndmt=1Tui,m,t'fmvd (27)

s.t.

ui,m,t'ui,m,t-1ui,m,t'1-ui,m,t (28)

For the intraday model, the constraints of the active power of SOP and the SOC of ESS must be extracted from the ORs. First, the intraday forecast error is calculated and compared with the day-ahead forecast data in period t. Then, the small interval that the error locates is determined and denoted as kt. The ranges for Pi,tSOP and Ei,t are the constraints, as shown in (29).

Pi,t,kt,minSOPPi,tSOPPi,t,kt,maxSOPEi,t,kt,minEi,tEi,t,kt,max    1tT (29)

Considering the above, other constraints of power flow and regulatory resources in each network are included, which are described in Section III-A. The decision variables of P3 are shown as:

xin=Pi,t,ωSOP,Qi,t,ωSOP,Pi,t,ωch,Pi,t,ωdis,Ei,t,ω (30)

V. Implementation Algorithm

A. Transformation of Nonconvex Constraints

Conic relaxation is applied to transform the nonconvex constraints of the sixth constraint in (2) and the third constraint in (3). The transformed constraints are shown as:

[2Pij,t,ω2Qij,t,ωiij,t,ω-ui,t,ω]2Tiij,t,ω+ui,t,ω (31)
Pi,t,ωSOP2+Qi,t,ωSOP2Pi,t,ωSOP,LAiSOP2 (32)

B. ADMM for Flexibly Interconnected ADNs

Flexibly interconnected ADNs can be partitioned and bounded by the DC side of the SOP. Each independent ADN with the AC side of the SOP comprises one control area. The ADMM blends the decomposability of dual ascent with the superior convergence properties of the method of multipliers, which is applicable here [

25].

The active power balance constraint of the SOP should be ensured between different areas. As observed from constraint (3), only boundary active power is exchanged between areas. Taking SOP1 in Fig. 1 as an example, the first constraint in (3) can be rewritten as:

Pi,t,ωSOP+Pi,t,ωSOP,L=PlinkPj,t,ωSOP+Pj,t,ωSOP,L=-Plink (33)

For the flexibly interconnected ADN in Fig. 1, the objective function for the spatial power balance in the day-ahead stage can be expressed as:

minfωda,o=f1+f2f1=P1,t,ωnl-P1,t,ωSOP+ijΦbr1i1,ij,t,ωrij,1f2=P2,t,ωnl-P2,t,ωSOP+ijΦbr2i2,ij,t,ωrij,2 (34)

Taking Network 1 in Fig. 1 as an example, let λ denote the Lagrange multiplier for the active power balance constraint between areas and ρ denote the penalty factor. Then, the objective function of Network 1 can be rewritten as:

LNW1ADMM=f1+ρ2Pi,tSOP+Pi,tSOP,L-Plink2+λPi,tSOP+Pi,tSOP,L-Plink (35)

Operation optimization is carried out for each network. The optimization results of the regulatory devices and boundary active power are obtained. The global value of the boundary data between areas should be updated according to (36).

Pl+1link=Pi,t,l+1SOP+Pi,t,l+1SOP,L-Pj,t,l+1SOP+Pj,t,l+1SOP,L2 (36)

After obtaining the global value, the computation formulas of the raw residual and the dual residual can be expressed as:

w1l+1=Pi,t,l+1SOP+Pi,t,l+1SOP,L-Pl+1links1l+1=Pl+1link-Pllink (37)

Then, based on the boundary active power, the Lagrange multiplier should be updated as:

λl+1=λl+ρPl+1link-Pi,t,l+1SOP-Pi,t,l+1SOP,L (38)

The detailed process of the distributed coordination optimization for flexibly interconnected ADNs with SOPs is summarized below.

Step 1:   initialization. The power flow results of the network without regulatory devices are set as initial values. Then, obtain P0link based on the initial values. Set the initial Lagrange multiplier as 0 and l=0.

Step 2:   optimization. Power flow optimization is carried out for each network, and decision variables and interactive variables are obtained.

Step 3:   update. Update the global value according to (36). Then, the corresponding Lagrange multiplier is updated according to (38).

Step 4:   iteration. Obtain the raw residual and the dual residual of each network according to (37). If the infinite norm of the residual is less than the convergence threshold, stop the iteration and output optimal results. Otherwise, let l=l+1 and return to Step 2.

Following the details mentioned above, the implementation process of the proposed two-stage optimization strategy for spatiotemporal power balancing in flexibly interconnected ADNs is summarized in Algorithm 1, where the day-ahead scheduling stage is shown in lines 2-8, the intraday corrective control stage is shown in lines 9-16, and the problem transformations are shown in lines 15-17.

Algorithm 1

1: Input: parameters of networks and devices and forecast data

2: Generate large numbers of stochastic scenarios Ωsensto based on day-ahead forecast data of WT through Monte Carlo method

3: Generate several typical scenarios Ωsentyp through K-means cluster algorithm

4: Formulate the model to determine schedules for SCB as P0 (1) and solve it

5: Formulate the equivalent day-ahead spatial power balancing model between networks and approximate it as P1 (9) via problem transformations (lines 15-17)

6: Obtain the ORs of the active power of SOP with the forecast error in each hour

7: Formulate the day-ahead temporal power balancing model within the network and approximate it as P2 (20) via problem transformations for each network

8: Obtain ORs of the SOC of ESS with the forecast error in each hour

9: for t=1:T do

10: Collect hourly forecast data of WT

11: Extract the ORs of the active power of SOP and the SOC of ESS according to the hourly forecast error of WT

12: Formulate the intraday corrective control model

13: Execute problem transformations for P3 (26)

14: Solve the above problem via ADMM and the power of SOP, ESS, and SVC is finally determined

15: t:=t+1

16: end for

17: Linearize the objective function through variable substitution

18: Transform nonconvex constraints into second-order conic constraints

19: P1 and P3 are reformulated as second-order cone programming (SOCP) problems, while P2 is reformulated as an MISOCP problem

20: Output: hourly scheduling strategies for SOPs, ESSs, SVCs, and SCBs

VI. Case Study

A. Simulation Setups

The case shown in Fig. 1 is denoted as Case 1. The load curves in the two networks are set to be different, while the WT power curves are the same. The normalized load curves and day-ahead and intraday hourly forecast active power of the WT are depicted in Fig. 3. The day-ahead forecast error ε for WT is set to be ±20%. The day-ahead hourly forecast data are considered to conform to a uniform distribution within the error range. The parameters for integrated devices are shown in Table I. The parameter settings are shown in Table II.

Fig. 3  Normalized load curves and day-ahead and intraday hourly forecast active power of WT.

Table I  Parameters for Integrated Devices
DeviceLocationParameter
WT Nodes 10 and 25 in Network 1 and Node 15 in Network 2 SWT=500 kW
ESS Node 15 in Network 1 and Node 33 in Network 2 SESS=800 kWh, PmaxESS,C=PmaxESS,D=200 kW/h, ηC=ηD=0.9, Emin=0.2, Emax=0.9
SVC Node 33 in Network 1 and Node 9 in Network 2 SSVC=500 kvar
SOP Node 30 in Network 1 and Node 18 in Network 2 SSOP=2 MVA, ASOP=0.02
SCB Node 8 in Network 1 and Node 29 in Network 2 qSCB=100 kvar, NmaxSCB=10, ΔmaxSCB=3
Table II  Parameter Settings
ParameterValue
ctpur 01:00-07:00: 61 $/MWh; 08:00-10:00, 16:00-18:00, 22:00-23:00: 138 $/MWh; 09:00-15:00, 19:00-21:00: 220 $/MWh
Umin, Umax 0.93 p.u., 1.07 p.u.

In Table I, S denotes the capacity of each device. The proposed model was implemented in MATLAB R2017b scripts and solved with CPLEX 12.8. The numerical experiments were performed on a PC with an Intel CPU i5-8300h and 16 GB of RAM.

B. Result Analysis for Day-ahead Equivalent Model Considering Sensitivity

1) Error Analysis for Equivalent Model Considering Sensitivity

To analyze the errors of optimization results such as node voltage and branch current, power flow calculation is carried out after the optimization based on the active power of SOP obtained from the equivalent model. Consequently, the average errors and maximum errors of the node voltage and branch current are shown in Table III.

Table III  Errors of Node Voltage and Branch Current
ParameterAverage errorMaximum error
Network 1Network 2Network 1Network 2
Node voltage 0.000600 0.009000 0.01196 0.01966
Branch current 0.003582 0.006195 0.04219 0.09042

In Table III, we can observe that the maximum errors are less than 0.1, respectively, which is acceptable. In addition, the average errors of node voltage and branch current are at the 10-4 and 10-3 levels, which indicates that the proposed equivalent model is highly accurate. It is also verified that none of the scenarios violate the voltage or current limit, which proves that the equivalent model is sufficiently reliable.

2) Analysis of Security Constraint Violations

To verify the superiority of the adoption of sensitivities, an equivalent model without sensitivity-based security constraints is considered as a comparison. Two models with and without consideration of sensitivity are denoted as Model A and Model N, respectively. The results of the violation percent of different scenarios are shown in Table IV. It shows that although branch current violations do not occur in Model N, node voltages in all scenarios exceed the limits. The results indicate that the adoption of sensitivity-constrained node voltage and branch current in the equivalent model is necessary.

Table IV  Violation Percent of Different Scenarios
ParameterViolation percent of model A (%)Violation percent of model N (%)
Network 1Network 2Network 1Network 2
Node voltage 0 0 0 100
Branch current 0 0 0 0

3) Comparison with Detailed Model

In this part, another day-ahead scheduling model between networks is established considering detailed power flow constraints (denoted as detailed model). The ADMM is used to solve the detailed model. The results show that the average computation time in 1000 scenarios using the equivalent model is 1.24 s, while the average computation time in 100 scenarios using the detailed model is 14 s. More than 24 hours are consumed if 1000 scenarios are optimized using the detailed model, which is unacceptable even in the day-ahead scheduling stage. Combined with the analysis of errors, it can be concluded that the equivalent model considering sensitivities computes faster with acceptable accuracy.

C. Result Analysis of ORs

1) Intraday Optimization Results Under Different Conditions

Different conditions are set to compare the optimization results and ORs in different scenarios and error intervals. Six numbers are set for NS, which are 200, 500, 1000, 1500, 2000, and 3000, while four numbers are set for NE, which are NS/2, NS/20, NS/50, and NS/100. In sum, 24 conditions are composed from all combinations. The contours of total costs and voltage deviations in the intraday stage under 24 conditions are shown in Figs. 4 and 5, respectively.

Fig. 4  Contours of total cost under 24 conditions.

Fig. 5  Contours of voltage deviations under 24 conditions.

In Fig. 4, we can observe that all results are close to each other. There are two valleys, where one valley is for NS=2000 and NE=NS/2 and the other is composed of data for NS=200, NE=NS/20, NE=NS/50 and NS=1000, NE=NS/20. Figure 4 indicates that cost will not decrease with more NS and more NE. In Fig. 5, we can also observe that all results are similar. With a smaller NS and a smaller NE, the voltage deviations are smaller.

2) ORs Under Different Conditions

The OR of the active power of SOP in period 19 when NS=1500 and NE=NS/2 is shown in Fig. 6. Taking ESS1 as an example, the OR of the SOC of ESS1 in period 15 when NS=1500 and NE=NS/2 is shown in Fig. 7. The orange parts in the two figures are the final ORs in this period according to the intraday hourly forecast error. Combined with ORs in other periods, the final intraday ORs in the time series are obtained, of which examples are shown in Figs. 8 and 9.

Fig. 6  OR of active power of SOP during period 19 when NS=1500 and NE=NS/2.

Fig. 7  OR of SOC of ESS1 during period 15 when NS=1500 and NE=NS/2.

Fig. 8  Lower and upper bounds of ORs of active power of SOP under different NS or NE. (a) Lower bounds of ORs of active power of SOP under different NS with NE=NS/50. (b) Upper bounds of ORs of active power of SOP under different NS with NE=NS/50. (c) Lower bounds of ORs of active power of SOP under different NE with NS=2000. (d) Upper bounds of ORs of active power of SOP under different NE with NS=2000.

Fig. 9  Lower and upper bounds of ORs of SOC of ESS under different NS or NE. (a) Lower bounds of ORs of SOC of ESS under different NS with NE=NS/20. (b) Upper bounds of ORs of SOC of ESS under different NS with NE=NS/20. (c) Lower bounds of ORs of SOC of ESS under different NE with NS=1000. (d) Upper bounds of ORs of SOC of ESS under different NE with NS=1000.

The lower and upper bounds of ORs of the active power of SOP in different numbers of scenarios when NE=NS/50 are shown in Fig. 8(a) and (b), respectively. The lower and upper bounds of ORs of the active power of SOP under different numbers of error intervals when NS=2000 are shown in Fig. 8(c) and (d), respectively. Similar to Fig. 8, the lower and upper bounds of ORs of the SOC of ESS under different numbers of scenarios when NE=NS/20 are shown in Fig. 9(a) and (b), respectively. The lower and upper bounds of ORs of the SOC of ESS under different numbers of error intervals when NS=1000 are shown in Fig. 9(c) and (d), respectively.

In Fig. 8(a) and (b), we can observe that when NS/NE is constant, in more scenarios, the lower bound of the OR increases while the upper bound decreases. This is because the scale of the optimization results becomes larger with more scenarios. Then, with higher data density, it is more likely that smaller or larger values are included and bounds become narrower. Conditions and explanations are also applied to Fig. 9(a) and (b). With more scenarios, the gaps between ORs in different scenarios are smaller.

However, the computation time for the generation of ORs remarkably increases with an increasing number of scenarios. In the day-ahead scheduling stage, the computation time for six scenarios is 2008 s, 7051 s, 11345 s, 15688 s, 20035 s, and 28723 s, respectively.

Figure 8(c) and (d) shows that when NS is constant, the lower bounds gradually decrease and the upper bounds increase with smaller NE, which also applies to Fig. 9(c) and (d).

Considering the above analysis, it would be suitable to set NS=1500 and NE=NS/2.

3) Comparison of Different Schemes

The ORs of the active power of SOP and the SOC of ESS compose a whole, which means that comparisons cannot be implemented on only one aspect. Consequently, four different schemes for the day-ahead scheduling stage are set to demonstrate the advantages of the ORs. The intraday models for each scheme are the same.

Scheme 1: deterministic day-ahead scheduling model without considering the uncertainty of WT power.

Scheme 2: stochastic day-ahead scheduling model considering the uncertainty of WT power.

Scheme 3: robust day-ahead scheduling model considering the uncertainty of WT power.

Scheme 4: the proposed day-ahead planning model considering sensitivities and the uncertainty of WT power.

In Scheme 4, NS=1500 and NE=NS/2. Additionally, regulation strategies for the SCB and ESS are planned day-ahead and irrevocable during the day in Schemes 1, 2, and 3. Comparison of intraday optimization results under different schemes is shown in Table V. The SOP applied in Case 1 consists of two VSCs. For simplicity, the active power of only one terminal, i.e., 1-30, under four schemes is shown in Fig. 10. Taking ESS1 as an example, the corresponding SOCs under four schemes are shown in Fig. 11.

Table V  Comparison of Intraday Optimization Results
SchemePurchase cost of electricity ($)Voltage deviation
Network 1Network 2SumNetwork 1Network 2Sum
Before optimization 8637 4625 13262 52.816 24.099 76.915
1 12308 2567 14875 51.312 11.287 62.599
2 12410 2706 15116 50.900 12.595 63.495
3 12410 2723 15133 52.609 11.766 64.375
4 8212 5019 13231 25.005 13.668 38.673

Fig. 10  Active power of SOP under four schemes.

Fig. 11  SOC of ESS1 under four schemes.

Table V shows that the purchase cost of electricity from the upstream grid only decreases under Scheme 4. Combined with the active power of SOP in Fig. 10, different from the other three schemes, active power is transferred from Network 1 to Network 2 due to the limitations of ORs, which indicates that intraday operation economy can be improved by day-ahead power balancing. The cost of Scheme 1 is the lowest of Schemes 1-3. However, the application of Scheme 1 is limited because forecast error is not considered. The cost of Scheme 3 is the highest due to the inclusion of the worst scenario in the robust optimization. Furthermore, we can observe that the voltage deviation of Scheme 4 is far smaller than that of the other schemes in Table V, indicating the superiority of the ORs.

As observed in Fig. 10, curves of the active power of SOP are similar in Schemes 1-3, and more active power is transferred than that in Scheme 4.

Figure 11 shows that the overall trends of the four schemes are similar. Specifically, the rising stages of Schemes 1-3 are similar, while the descending stages of Schemes 1 and 2 are similar. As ESS1 is installed in Network 1, combined with Fig. 3, it can be inferred that ESS1 is charged during the valley-load periods while discharged during the peak-load periods. In addition, considering the unit purchase cost of electricity in Table II, when the unit purchase cost of electricity is low, active power is charged into ESS, and when the unit purchase cost of electricity is high, active power is discharged from ESS, which decreases the total intraday operation cost.

D. Algorithm Evaluation

1) Test on a Large System

Case 2 is based on a demonstration project of SOP in Hangzhou, China. A three-terminal SOP connects three networks, which comprise the 105-node system shown in Fig. 12. The ESS capacity is 1 MWh, and the maximum charging/discharging power is 300 kW. Other ESS parameters and other devices are the same as those in Case 1, as shown in Tables I and II. The day-ahead and intraday hourly forecast active power of the WT and the active loads of the three networks are shown in Fig. 13.

Fig. 12  105-node system composed of three networks.

Fig. 13  Day-ahead and intraday hourly forecast active power of WT and active loads of three networks. (a) Day-ahead and intraday hourly forecast power of WT. (b) Active loads of three networks.

In the day-ahead scheduling stage, the maximum voltage and current errors of the equivalent model considering sensitivities are shown in Fig. 14. We can observe that the voltage error during each period is very small, while the current error seems larger but still less than 0.1. Furthermore, voltage or current violations never occur in all stochastic scenarios.

Fig. 14  Maximum voltage and current errors of equivalent model considering sensitivities in day-ahead scheduling stage. (a) Maximum voltage errors. (b) Maximum current errors.

The purchase costs of electricity from the upstream grid and the voltage deviations of the three networks are depicted in Figs. 15 and 16, respectively. In Fig. 15 and Fig. 16, we can observe that the Scheme 4 performs better than the other three schemes. From the above test results and analysis, we can conclude that the proposed optimization strategy for spatiotemporal power balancing considering ORs of the active power of SOPs and the SOC of ESSs exhibits a good scalability performance in applications on larger systems.

Fig. 15  Purchase cost of electricity from upstream grid of three networks.

Fig. 16  Voltage deviations of three networks.

2) Computation Efficiency

The complexities and computation time of three models, i.e., day-ahead model between networks (P1), day-ahead model within a single network (P2), and intraday corrective control model (P3), are summarized in Table VI to demonstrate the computation performance of the proposed strategy.

Table VI  Complexities and Computation Time of Three Models
CaseModel complexityComputation time (s)
Number of constraintsNumber of variables
P1P2P3P1P2P3P1P2P3
1 9792 31774 1481 3600 15864 744 1.24 9.89 5.42
2 15840 51924 2396 5784 25926 1060 2.35 12.52 10.38

Specifically, the number of constraints and variables in the day-ahead scheduling stage corresponds to each stochastic scenario, while that in the intraday corrective control stage corresponds to each hour. Additionally, the computation time for day-ahead models is the average value in 1000 scenarios, while the computation time for the intraday model is the average value in 24 hours.

In Table VI, the computation time for the day-ahead model within the network is obviously more than that between networks because the former is a detailed model with power flow constraints. Meanwhile, the computation time for the intraday corrective control model is far less than 1 hour, which means that the obtained intraday strategy can be easily implemented in the hourly regulation.

VII. Conclusion

In this paper, a two-stage optimization strategy for spatiotemporal power balancing in flexibly interconnected ADNs is proposed. In the day-ahead scheduling stage, considering the uncertainty of WT power, stochastic optimization is carried out to obtain schedules for an SCB with typical scenarios. Then, the ORs of the active power of SOP and the SOC of ESS are obtained from the optimization results in large numbers of stochastic scenarios. To improve computation efficiency, an equivalent model between networks is established, which suppresses violations of system security constraints with sensitivities. In the intraday corrective control stage, different from the existing fixed schedule of ESS regulation, the hourly charging/discharging power of the ESS is flexibly regulated with ORs. The test results reveal that the proposed equivalent model considering sensitivities computes faster than the detailed model, and its error is also acceptable. The power flow calculation result considering the active power of SOP after the optimization proves that voltage or current violations indeed never occur. Meanwhile, the intraday model considering ORs performs better than stochastic optimization and robust optimization, which indicates the superiority of the proposed strategy. For further work, uncertainties in photovoltaic power and loads will be considered. In addition, different settings for the location and capacity of the SOP may affect the power balancing, which is another research topic.

Nomenclature

Symbol —— Definition
A. —— Sets
Ωsensto —— Set of stochastic scenarios
Ωsentyp —— Set of typical scenarios
Ψndm —— Set of nodes in network m
ΨndSOP —— Set of nodes that connect to soft open points (SOPs)
Φbr —— Set of branches
Φbrm —— Set of branches in network m
Θcup —— Set of purchased active power pairs
Ξkε —— Set of scenarios whose forecast error belongs to the kth forecast error interval
B. —— Parameters
αup, αvd —— Objective weights of total purchase cost and voltage deviation
ε —— Forecast error
εmin, εmax —— The minimum and maximum forecast errors
εs —— Small interval of forecast error
εk —— Forecast error of the kth forecast error interval
ηich, ηidis —— Charging and discharging efficiencies of energy storage system (ESS) at node i
ΔmaxSCB —— The maximum switch times of shunt capacitor bank (SCB)
ΔPt,ω, ΔQt,ω —— Vectors of difference of node active and reactive power during period t in scenario ω
Δθt,ω, ΔUt,ω —— Vectors of difference of voltage phase and magnitude during period t in scenario ω
δt,ωIP, δt,ωIQ —— Matrices of sensitivity of branch current with respect to node active power and reactive power
AiSOP —— Loss coefficient of SOP at node i
ctpur —— Unit purchase cost of electricity during period t
Ei,ini,ω, Ei,T,ω —— Initial state of charge (SOC) and final SOC of ESS at node i in scenario ω
Emin, Emax —— The minimum and maximum values of SOC
Emini,t,k, Emaxi,t,k —— The minimum and maximum values of SOC of ESS at node i during period t in the kth forecast error interval
fmup, fmvd —— Total purchase cost and voltage deviations before optimization in network m
iij,max —— The maximum square of current of branch ij
It,ω0, It,ω' —— Vectors of branch current before and after optimization during period t in scenario ω
Jt,ωPθ, Jt,ωPU, Jt,ωQθ, Jt,ωQU —— Submatrices of Jacobian matrix during period t in scenario ω
J —— Jacobian matrix
N —— Number of networks
NS —— Number of scenarios
NE —— Number of error intervals
NmaxSCB —— The maximum number of banks switched in once
pω —— Probability of scenario ω from Ωsentyp
Plink —— Global value of active power of SOP
Pl+1link —— Global value after l+1 iterations
Pi,maxch, Pi,maxdis —— The maximum charging and discharging power of ESS at node i
Pi,t,k,minSOP, Pi,t,k,maxSOP —— The minimum and maximum values of active power of SOP at node i during period t in the kth forecast error interval
qSCB —— Unit reactive capacity of SCB
Qi,minSVC, Qi,maxSVC —— The minimum and maximum reactive power of SVC at node i
rij, xij —— Resistance and reactance of branch ij
rij,m —— Resistance of branch ij in network m
SiSOP —— Capacity of SOP at node i
SiESS —— Capacity of ESS at node i
T —— Number of periods
ui,min, ui,max —— The minimum and maximum squares of voltage magnitude at node i
Ut,ω0, Ut,ω' —— Vectors of voltage magnitude before and after optimization during period t in scenario ω
w1l+1, s1l+1 —— Raw residual and dual residual of network 1 after l+1 iterations
C. —— Variables
αm,c,ω —— Weight of the cth pair of purchased active power in scenario ω in network m
γi,t,ωch, γi,t,ωdis —— 0-1 indexes indicating whether ESS at node i charges or discharges during period t in scenario ω
θk,t,ω —— Voltage phase of node k during period t in scenario ω
θij,t,ω —— Voltage phase deviation between node i and node j during period t in scenario ω
ΔPm,ω,tc1,tc2up —— Substituted variable for the absolute value between Pm,tc1,ωup and Pm,tc2,ωup
Ei,t,k —— SOC of ESS at node i during period t in the kth forecast error interval
Ei,t,ω —— SOC of ESS at node i during period t in scenario ω
Ei,t —— SOC of ESS at node i during period t
im,ij,t,ω —— Square of current of branch ij in period t in scenario ω in network m
iij,t,ω —— Square of current of branch ij during period t in scenario ω
Iij,t,ω —— Current of branch ij during period t in scenario ω
Mt,ωIθ, Mt,ωIU —— Matrices consisting of Iij,t,ω/Pk,t,ω and Iij,t,ω/Qk,t,ω
Ni,tSCB —— Number of banks of SCB switched in at node i during period t
Pm,t,ωnl —— Net active load in network m during period t in scenario ω
Pm,t,ωSOP —— Active power of SOP connected to network m during period t in scenario ω
Pi,tSCB —— Reactive power of SCB at node i during period t
Pij,t,ω, Qij,t,ω —— Active and reactive power of branch ij during period t in scenario ω
Pi,t,ω, Qi,t,ω —— Injected active and reactive power of node i during period t in scenario ω
Pi,t,ωSOP, Qi,t,ωSOP —— Active and reactive power of SOP at node i during period t in scenario ω
Pi,t,ωch, Pi,t,ωdis —— Charging and discharging active power of ESS at node i during period t in scenario ω
Pm,t,ωup —— Purchased active power during period t in network m in scenario ω
Pm,tup —— Purchased active power during period t in network m
Pi,t,ωSOP,L —— Active power loss of SOP at node i during period t in scenario ω
Pi,t,ωSVC —— Reactive power of series var compensator (SVC) at node i during period t in scenario ω
Pi,tSOP, Pi,tSOP,L —— Active power and active power losses of SOP at node i during period t
ui,m,t' —— Substituted variable for the absolute value between 1 and the square of voltage magnitude of node i during period in network m
ui,t,ω —— Square of voltage of node i during period t in scenario ω
Ui,t,ω —— Voltage of node i during period t in scenario ω

References

1

P. Li, H. Ji, C. Wang et al., “Coordinated control method of voltage and reactive power for active distribution networks based on soft open point,” IEEE Transactions on Sustainable Energy, vol. 8, no. 4, pp. 1430-1442, Oct. 2017. [Baidu Scholar] 

2

Z. Liu and J. V. Milanović, “Probabilistic estimation of voltage unbalance in MV distribution networks with unbalanced load,” IEEE Transactions on Power Delivery, vol. 30, no. 2, pp. 693-703, Apr. 2015. [Baidu Scholar] 

3

J. M. Bloemink and T. C. Green, “Increasing distributed generation penetration using soft normally-open points,” in Proceedings of IEEE PES General Meeting, Minneapolis, USA, Aug. 2010, pp. 1-8. [Baidu Scholar] 

4

D. Feng, F. Wu, Y. Zhou et al., “Multi-agent-based rolling optimization method for restoration scheduling of distribution systems with distributed generation,” Journal of Modern Power Systems and Clean Energy, vol. 8, no. 4, pp. 737-749, Jul. 2020. [Baidu Scholar] 

5

F. Sun, J. Ma, M. Yu et al., “Optimized two-time scale robust dispatching method for the multi-terminal soft open point in imbalanced active distribution networks,” IEEE Transactions on Sustainable Energy, vol. 12, no. 1, pp. 587-598, Jan. 2021. [Baidu Scholar] 

6

X. Yang, C. Xu, Y. Zhang et al., “Real-time coordinated scheduling for ADNs with soft open points and charging stations,” IEEE Transactions on Power Systems, vol. 36, no. 6, pp. 5486-5499, Nov. 2021. [Baidu Scholar] 

7

H. Ji, C. Wang, P. Li et al., “An enhanced SOCP-based method for feeder load balancing using the multi-terminal soft open point in active distribution networks,” Applied Energy, vol. 208, pp. 986-995, Dec. 2017. [Baidu Scholar] 

8

H. Ji, C. Wang, P. Li et al., “Robust operation of soft open points in active distribution networks with high penetration of photovoltaic integration,” IEEE Transactions on Sustainable Energy, vol. 10, no. 1, pp. 280-289, Jan. 2019. [Baidu Scholar] 

9

J. Wang, N. Zhou, C. Y. Chung et al., “Coordinated planning of converter-based DG units and soft open points incorporating active management in unbalanced distribution networks,” IEEE Transactions on Sustainable Energy, vol. 11, no. 3, pp. 2015-2027, Jul. 2020. [Baidu Scholar] 

10

W. Cao, J. Wu, and N. Jenkins, “Feeder load balancing in MV distribution networks,” in Proceedings of the 2014 IEEE PES Innovative Smart Grid Technologies Europe (ISGT Europe), Istanbul, Turkey, Jan. 2014, pp. 1-6. [Baidu Scholar] 

11

Z. Ziadi, S.Taira, M. Oshiro et al., “Optimal power scheduling for smart grids considering controllable loads and high penetration of photovoltaic generation,” IEEE Transactions on Smart Grid, vol. 5, no. 5, pp. 2350-2359, Sept. 2014. [Baidu Scholar] 

12

Y. J. Kim, J. L. Kirtley, and L. K. Norford, “Reactive power ancillary service of synchronous DGs in coordination with voltage control devices,” IEEE Transactions Smart Grid, vol. 8, no. 2, pp. 515-527, Mar. 2017. [Baidu Scholar] 

13

R. Zafar, J. Ravishankar, J. E. Fletcher et al., “Multi-timescale model predictive control of battery energy storage system using conic relaxation in smart distribution grids,” IEEE Transactions on Power Systems, vol. 33, no. 6, pp. 7152-7161, Nov. 2018. [Baidu Scholar] 

14

F. Sun, M. Yu, Q. Wu et al., “A multi-time scale energy management method for active distribution networks with multiple terminal soft open point,” International Journal of Electrical Power and Energy Systems, vol. 128, p. 106767, Jun. 2021. [Baidu Scholar] 

15

S. Xie, Z. Hu, and J. Wang, “Two-stage robust optimization for expansion planning of active distribution systems coupled with urban transportation networks,” Applied Energy, vol. 261, p. 114412, Mar. 2020. [Baidu Scholar] 

16

P. Li, Q. Wu, M. Yang et al., “Distributed distributionally robust dispatch for integrated transmission-distribution systems,” IEEE Transactions on Power Systems, vol. 36, no. 2, pp. 1193-1205, Mar. 2021. [Baidu Scholar] 

17

S. Talari, M. Yazdaninejad, and M.-R. Haghifam, “Stochastic-based scheduling of the microgrid operation including wind turbines, photovoltaic cells, energy storages and responsive loads,” IET Generation, Transmission & Distribution, vol. 9, no. 12, pp. 1498-1509, Dec. 2015. [Baidu Scholar] 

18

Y. P. Agalgaonkar, B. C. Pal, and R. A. Jabr, “Stochastic distribution system operation considering voltage regulation risks in the presence of PV generation,” IEEE Transactions on Sustainable Energy, vol. 6, no. 4, pp. 1315-1324, Oct. 2015. [Baidu Scholar] 

19

A. X. Sun, D. T. Phan, and S. Ghosh, “Fully decentralized AC optimal power flow algorithms,” in Proceedings of 2013 IEEE PES General Meeting, Vancouver, Canada, Jan. 2013, pp. 1-5. [Baidu Scholar] 

20

W. Zheng, W. Wu, B. Zhang et al., “A fully distributed reactive power optimization and control method for active distribution networks,” IEEE Transactions on Smart Grid, vol. 7, no. 2, pp. 1021-1033, Mar. 2016. [Baidu Scholar] 

21

K. Christakou, J. LeBoudec, M. Paolone et al., “Efficient computation of sensitivity coefficients of node voltages and line currents in unbalanced radial electrical distribution networks,” IEEE Transactions on Smart Grid, vol. 4, no. 2, pp. 741-750, Jun. 2013. [Baidu Scholar] 

22

G. Valverde and T. van Cutsem, “Model predictive control of voltages in active distribution networks,” IEEE Transactions on Smart Grid, vol. 4, no. 4, pp. 2152-2161, Dec. 2013. [Baidu Scholar] 

23

Y. Guo, Q. Wu, H. Gao et al., “Double-time-scale coordinated voltage control in active distribution networks based on MPC,” IEEE Transactions on Sustainable Energy, vol. 11, no. 1, pp. 294-303, Jan. 2020. [Baidu Scholar] 

24

K. Christakou, M. Paolone, and A. Abur, “Voltage control in active distribution networks under uncertainty in the system model: a robust optimization approach,” IEEE Transactions on Smart Grid, vol. 9, no. 6, pp. 5631-5642, Nov. 2018. [Baidu Scholar] 

25

S. Boyd, N. Parikh, E. Chu et al., “Distributed optimization and statistical learning via the alternating direction method of multipliers,” Foundations and Trends in Machine Learning, vol. 3, no. 1, pp. 1-122, Jan. 2011. [Baidu Scholar]