RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (2024)

This paper is a preprint of a paper submitted to the Proceedings of Power Electronics, Machines and Drives 2024 (PEMD 2024) and is subject to Institution of Engineering and Technology Copyright. If accepted, the copy of record will be available at IET Digital Library.

Matthew Deakin\corr   Xu Dengmatthew.deakin@newcastle.ac.ukSchool of Engineering, Newcastle University, Newcastle-upon-Tyne, UK

Abstract

A low-cost reconfiguration stage connected at the output of balanced three-phase, multi-terminal ac/dc/ac converters can increase the feasible set of power injections substantially, increasing converter utilization and therefore achieving a lower system cost. However, the approach has yet to be explored for phase unbalance mitigation in power distribution networks, an important application for future energy systems. This study addresses this by considering power converter reconfiguration’s potential for increasing the feasible set of power transfers of four-wire power converters. Reconfigurable topologies are compared against both conventional four-wire designs and an idealised, fully reconfigurable converter. Results show that conventional converters need up to 75.3% greater capacity to yield a capability chart of equivalent size to an idealised reconfigurable converter. The number and capacity of legs impact the capability chart’s size, as do constraints on dc-side power injections. The proposed approach shows significant promise for maximizing the utilization of power electronics used to mitigate impacts of phase unbalance.

keywords:

MULTIPORT CONVERTER, CONVERTER MULTIPLEXING, POWER DISTRIBUTION, UNBALANCE MITIGATION

1 Introduction

The electrification of demand and uptake of distributed generation in domestic properties will lead to a significant increase in load on low voltage power (LV) distribution networks speakman2022low . In many regions, domestic customers are connected to a single phase supply, or have a three-phase supply feeding single phase loads ma2020review . In the absence of active phase balancing, it can be expected the vast majority of assets that would have to be replaced due to thermal constraints would be under-utilized prior to their replacement. This is because it is the phase with the highest loading, rather than the average loading, which limits operation of the distribution system components such as substation transformers ma2016quantification .

As a result, there has been rapidly growing interest in approaches to increase utilization of congested branches prior to their reinforcement. Proposed approaches include static reallocation of single-phase loads pereira2021phase , dynamic customer phase reallocation via static transfer switch-based ‘phase shifting devices’ shahnia2014voltage ; liu2021load ; cui2023two , the control of single-phase customer generators girigoudar2022integration , or the use of distributed energy resources solutions interfaced through a three-phase four-wire (4W) power converter. The latter approach is shown in Fig.1, with works published considering such an approach including standalone Static Compensator (STATCOM)-based approaches de2016modeling , battery energy storage stecca2022battery , or back-to-back ‘soft open points’ (SOPs) cui2023two . However, the approach is not limited to these and could also include any other dc resource–e.g., an LVDC cable, a three-phase electric vehicle fast charger, or industrial motor drive. These four wire (4W) voltage source converter (VSC)-based systems can support increased utilization by monitoring phase currents at a congested branch (e.g., a substation transformer), then dynamically injecting unbalanced power to reduce loading on heavily loaded phases.

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (1)

If the phase unbalance mitigation provided by a 4W VSC system changes in time, then the loading on the individual legs of the interfacing ac/dc converter will also vary. As a result, a 4W VSC system appears to be an attractive proposition for the use of the multiplexing approach described in deakin2023optimal ; deakin2023multiplexing . In particular, it is proposed that 4W VSC systems are constructed of an arbitrary number of legs, whose current-carrying capacity is not necessarily uniform, and whose output can be connected to any of the four wires of the power distribution system. By allowing the capacity connected to each of the four wires to change dynamically, the feasible set of power transfers can be augmented. The purpose of this work is to explore this feasible set (i.e., the capability chart), and explore how different sizing strategies can increase the size of this set.

There are a few works that have explored the use of power converter reconfiguration for mitigating phase unbalance. In lou2020new , the authors describe a ‘phase changing SOP’, assumed to be constructed using a multi-terminal ‘phase shifting device’ in recent works cui2023two . However, we show in this work that a three-leg, three-phase inverter with equally sized legs cannot benefit from reconfiguration on the output. Alternatively, works on balanced operation of SOPs and their capability charts have been considered in detail in deakin2023multiplexing ; deakin2023optimal . However, to the authors’ knowledge, there are no works that consider capability charts of reconfigurable power converters for arbitrary unbalance mitigation, including the critical effect of neutral currents. This is an important and timely gap, as the proposed reconfiguration approach promising to lower the cost of power electronics by increasing utilization substantially deakin2023multiplexing , and thereby providing a route for network operators to install more cost-effective active solutions to address distribution system congestion.

The major contribution of this work is to address this gap by proposing and calculating capability charts for the proposed four-wire reconfigurable power converters. This includes numerical approaches to determine the size of these capability charts, and corresponding visualizations of these sets. The aim is provide metrics that can demonstrate the improved flexibility of the reconfiguration approach.

This work is structured as follows. In Section2, we describe the proposed topology and define corresponding capability charts, then describe how the area (or volume) of these charts can be calculated numerically to demonstrate performance improvement for a given 4W VSC design. In Section3, a range of case studies are presented to highlight the improvements that can be expected as a result of the proposed reconfiguration. Finally, salient conclusions are drawn in Section4.

2 Methodology

In this work, two basic structures are considered for the 4W VSC system, as shown in Fig.2. A Standalone 4W VSC, as shown in Fig.2a, consists of only a four-wire VSC and dc capacitor, and so the power balance restricts the currents that can be injected (i.e., the sum of active powers injected into the network must have value zero). The standalone device is similar to a STATCOM, which has been used for providing dynamic reactive power compensation in power systems for several decades, and which can transfer power between phases to mitigate high currents. In contrast, the Interconnected 4W VSC systems, as shown in Fig.2b, also has a dc-side component connected to enable a non-zero power injection from the VSC into the ac network.

In this Section, we outline how the capability chart of a both of these classes of 4W VSC systems can be increased by adding the proposed reconfiguration output stage. Firstly, in Section2.1 the mechanism by which this reconfiguration increases the capability chart is revisited, highlighting with a simple example how the proposed approach can be beneficial under unbalanced operation. Subsequently, in Section2.2, capability charts are defined as a set, with it highlighted how the size of these sets change as a function of total VSC capacity. Finally, in Section2.3, numerical routines are described for calculating the size of these sets.

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (2)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (3)

2.1 Proposed Four-Wire Reconfigurable Power Converter

The essence of the proposed approach has been described in detail in deakin2023multiplexing for a balanced, multi-terminal back-to-back VSC system. In a conventional VSC system (Fig.3a), the output of each of the equally-sized half-bridge (HB) legs are hard-wired to the four output wires; the maximum current that can be injected into any one of the phases is static. In contrast, the proposed approach can have any number of legs, m𝑚mitalic_m, whose pu size α𝛼\alphaitalic_α can be varied (at the design stage), and which can be connected to any of the outputs to vary the HB capacity connected to a given phase on-the-fly. It is worth noting that if the mission profile for the 4W VSC does not vary with time, then the proposed approach will not provide a benefit.

There are two major differences between the balanced and unbalanced cases. Firstly, neutral currents can be neglected in the balanced case. In contrast, as we demonstrate in Section3.1, neutral currents are often large and so must be calculated for an accurate determination of the capability chart. Secondly, individual legs of the VSC are considered, rather than three-phase VSC units as in, e.g., deakin2023multiplexing .

For the purposes of this work, but without loss of generality, we consider the main purpose of such a system is to inject only active power P𝑃Pitalic_P (and not reactive power), for the following reasons. Firstly, analysis of smart meter data suggests that modern domestic customers have very good power factor–for example, it is suggested in vanin2023analysis that a power factor of unity ought to be assumed for simulation tasks. If this is the case, then injecting reactive power will increase (rather than decrease) loading on each phase, and so is not useful for addressing thermal congestion. Secondly, so long as the converter has sufficient capacity, issues with reactive power can be addressed with single phase assets injecting reactive power (where active power phase rebalancing is not possible without changing the load point). Finally, reactive power can be mitigated dynamically by other low-cost means (e.g., switched capacitor banks). Nevertheless: reactive power could be also considered in future applications, considering applications such as voltage unbalance mitigation.

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (4)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (5)

2.1.1 Example Reconfigurable Converter

An example of a reconfigurable converter, constructed of two HB triplet packages of 45A and 15A respectively are shown in Fig.4. Such a converter can be connected in various operating modes.

  • The converter can operate under balanced operation with maximum power output. In this case, 60A is connected to phase 1–3; the neutral has no capacity allocated to it. In this mode, the converter is acting like a conventional three-wire, three-phase converter.

  • The converter could be used to inject 90A of active power into any of one of phases 1–3 to mitigate a temporary overload, with 90 A connected to the neutral (for the return current). In this mode, the converter is acting like a single-phase converter. 50% extra current can be injected into the phase which the HBs are connected to as compared to the balanced converter.

  • The battery is disconnected for maintenance. 45A of capacity is connected to two of phases 1–3; 30A to the other phase; and 60A to the neutral to enable phase rebalance currents (as shown in Section3.1, the neutral current is typically larger than the phase currents). The converter is acting as a four wire standalone VSC system; depending on the optimal operation, the 45A and 30A converters can be reallocated.

In summary, the selector switches can enable a wide range of unbalanced operation, with a higher utilization of the HBs as compared to a static design. In the next Section, we propose the use of capability charts to systematically study the full range of operation (as compared to the specific operating points highlighted in this example).

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (6)

2.2 Defining Capability Charts

A capability chart can be defined as the feasible operating region of a given power converter, i.e., the feasible currents and/or voltages under which it can operate. This has been defined for balanced reconfigurable converters in deakin2023optimal ; deakin2023multiplexing . However, unbalanced current injections by a converter necessitates consideration of neutral currents, and so in this section we revisit capability chart for the four-wire configuration.

For a 4W power converter operating with a fixed output voltage and no dc-side constraints (e.g., assuming a large dc link capacitor) the power converter’s operating range is determined by the current rating of the capacity connected to each wire Iϕmax+4superscriptsubscript𝐼italic-ϕsuperscriptsubscript4I_{\phi}^{\max}\in\mathbb{R}_{+}^{4}italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT start_POSTSUPERSCRIPT roman_max end_POSTSUPERSCRIPT ∈ blackboard_R start_POSTSUBSCRIPT + end_POSTSUBSCRIPT start_POSTSUPERSCRIPT 4 end_POSTSUPERSCRIPT (in Amps or pu). The phasors representing the phase currents in each leg of the converter Iϕ4subscript𝐼italic-ϕsuperscript4I_{\phi}\in\mathbb{C}^{4}italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT ∈ blackboard_C start_POSTSUPERSCRIPT 4 end_POSTSUPERSCRIPT must therefore satisfy

|Iϕ[i]|Iϕmax[i]i{1, 2, 3, 4}.subscript𝐼italic-ϕdelimited-[]𝑖superscriptsubscript𝐼italic-ϕdelimited-[]𝑖for-all𝑖1234|I_{\phi}[i]|\leq I_{\phi}^{\max}[i]\;\forall\;i\in\{1,\,2,\,3,\,4\}\,.| italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT [ italic_i ] | ≤ italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT start_POSTSUPERSCRIPT roman_max end_POSTSUPERSCRIPT [ italic_i ] ∀ italic_i ∈ { 1 , 2 , 3 , 4 } .(1)

For such a system, consider the m𝑚mitalic_m per-unit leg capacities αm𝛼superscript𝑚\alpha\in\mathbb{R}^{m}italic_α ∈ blackboard_R start_POSTSUPERSCRIPT italic_m end_POSTSUPERSCRIPT, such that

i=1mα[i]=1.superscriptsubscript𝑖1𝑚𝛼delimited-[]𝑖1\sum_{i=1}^{m}\alpha[i]=1\,.∑ start_POSTSUBSCRIPT italic_i = 1 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_m end_POSTSUPERSCRIPT italic_α [ italic_i ] = 1 .(2)

A variable binary matrix B{0,1}4×m𝐵superscript014𝑚B\in\{0,1\}^{4\times m}italic_B ∈ { 0 , 1 } start_POSTSUPERSCRIPT 4 × italic_m end_POSTSUPERSCRIPT has m𝑚mitalic_m columns that each represent the state of the m𝑚mitalic_m one-to-four selector switches, with the sum of each column of B𝐵Bitalic_B having value 1 (to ensure each leg is connected to just one output wire). Then, the capacity connected to each output wire Iϕmaxsuperscriptsubscript𝐼italic-ϕI_{\phi}^{\max}italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT start_POSTSUPERSCRIPT roman_max end_POSTSUPERSCRIPT is simply the sum of the capacities of the legs connected to that wire, i.e.,

Iϕmax=IbaseBα,superscriptsubscript𝐼italic-ϕsubscript𝐼base𝐵𝛼I_{\phi}^{\max}=I_{\mathrm{base}}B\alpha\,,italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT start_POSTSUPERSCRIPT roman_max end_POSTSUPERSCRIPT = italic_I start_POSTSUBSCRIPT roman_base end_POSTSUBSCRIPT italic_B italic_α ,(3)

where the current Ibasesubscript𝐼baseI_{\mathrm{base}}italic_I start_POSTSUBSCRIPT roman_base end_POSTSUBSCRIPT has value of the sum of the capacity of all legs (in Amps). Note that, if a converter is not reconfigurable, then B𝐵Bitalic_B is replaced with an identity matrix.

For a four-wire converter injecting in-phase currents (i.e., active powers) into a stiff positive sequence voltage with fixed phase voltage magnitudes |V0|subscript𝑉0|V_{0}|| italic_V start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT |, the per-phase powers P3𝑃superscript3P\in\mathbb{R}^{3}italic_P ∈ blackboard_R start_POSTSUPERSCRIPT 3 end_POSTSUPERSCRIPT are linked to those phase currents Iϕsubscript𝐼italic-ϕI_{\phi}italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT according to the linear relation

Iϕ(P)[i]subscript𝐼italic-ϕ𝑃delimited-[]𝑖\displaystyle I_{\phi}(P)[i]italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT ( italic_P ) [ italic_i ]=P[i]|V0|a(1i),i{1, 2, 3},formulae-sequenceabsent𝑃delimited-[]𝑖subscript𝑉0superscript𝑎1𝑖𝑖123\displaystyle=\dfrac{P[i]}{|V_{0}|a^{(1-i)}}\,,\quad i\in\{1,\,2,\,3\}\,,= divide start_ARG italic_P [ italic_i ] end_ARG start_ARG | italic_V start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT | italic_a start_POSTSUPERSCRIPT ( 1 - italic_i ) end_POSTSUPERSCRIPT end_ARG , italic_i ∈ { 1 , 2 , 3 } ,(4a)
Iϕ(P)[4]subscript𝐼italic-ϕ𝑃delimited-[]4\displaystyle I_{\phi}(P)[4]italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT ( italic_P ) [ 4 ]=i=13Iϕ(P)[i].absentsuperscriptsubscript𝑖13subscript𝐼italic-ϕ𝑃delimited-[]𝑖\displaystyle=-\sum_{i=1}^{3}I_{\phi}(P)[i]\,.= - ∑ start_POSTSUBSCRIPT italic_i = 1 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT 3 end_POSTSUPERSCRIPT italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT ( italic_P ) [ italic_i ] .(4b)

where a=e2πȷ/3𝑎superscript𝑒2𝜋italic-ȷ3a=e^{2\pi\jmath/3}italic_a = italic_e start_POSTSUPERSCRIPT 2 italic_π italic_ȷ / 3 end_POSTSUPERSCRIPT is the phase rotation operator. Note that the neutral current INtrl.subscript𝐼NtrlI_{\mathrm{Ntrl.}}italic_I start_POSTSUBSCRIPT roman_Ntrl . end_POSTSUBSCRIPT flows through the fourth wire in (4),

INtrl.=Iϕ[4],subscript𝐼Ntrlsubscript𝐼italic-ϕdelimited-[]4I_{\mathrm{Ntrl.}}=I_{\phi}[4]\,,italic_I start_POSTSUBSCRIPT roman_Ntrl . end_POSTSUBSCRIPT = italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT [ 4 ] ,(5)

and that the neutral is at the reference voltage at 0V. As a result, the neutral cannot inject either active or reactive power (which is why there are only three components in the powers P𝑃Pitalic_P).

The capability chart can therefore defined as the feasible set of power injections P𝑃Pitalic_P that satisfy the power converter operating constraints, i.e.,

C={P:(1),(3),(4)}.𝐶conditional-set𝑃italic-(1italic-)italic-(3italic-)italic-(4italic-)C=\{P:\eqref{e:i_constraint},\,\eqref{e:max_current},\,\eqref{e:p2i}\}\,.italic_C = { italic_P : italic_( italic_) , italic_( italic_) , italic_( italic_) } .(6)

The advantage of the capability chart in terms of active powers P𝑃Pitalic_P (instead of current phasors Iϕsubscript𝐼italic-ϕI_{\phi}italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT) is that, in the general case of arbitrary P𝑃Pitalic_P (i.e., an Interconnected 4W VSC), the dimension of the set (dim(C)=3dim𝐶3\mathrm{dim}(C)=3roman_dim ( italic_C ) = 3) is the same as the number of variables in P𝑃Pitalic_P.

The total power injected into the ac grid, PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT, is

PTtl.=P[1]+P[2]+P[3].subscript𝑃Ttl𝑃delimited-[]1𝑃delimited-[]2𝑃delimited-[]3P_{\mathrm{Ttl.}}=P[1]+P[2]+P[3]\,.italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT = italic_P [ 1 ] + italic_P [ 2 ] + italic_P [ 3 ] .(7)

For the case of a Standalone 4W VSC (Fig.2a), ac-side powers must balance, i.e., PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT must have value of zero; for an Interconnected 4W VSC, PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT can have a non-zero value.

Given the definition of a capability chart as a set, it is natural to consider the size of the set as a property of interest when comparing converters with different α𝛼\alphaitalic_α. The capability chart volume (CCV) or capability chart area (CCA) are

CCV=C𝑑V,CCA=C𝑑A,formulae-sequenceCCVsubscript𝐶differential-d𝑉CCAsubscript𝐶differential-d𝐴\mathrm{CCV}=\int_{C}dV\,,\qquad\mathrm{CCA}=\int_{C}dA\,,roman_CCV = ∫ start_POSTSUBSCRIPT italic_C end_POSTSUBSCRIPT italic_d italic_V , roman_CCA = ∫ start_POSTSUBSCRIPT italic_C end_POSTSUBSCRIPT italic_d italic_A ,(8)

with the former used for an Interconnected 4W VSC, and the latter a Standalone 4W VSC (whose capability chart C𝐶Citalic_C is two-dimensional, as the three powers P𝑃Pitalic_P are constrained to lie in the plane P[i]=0𝑃delimited-[]𝑖0\sum P[i]=0∑ italic_P [ italic_i ] = 0).

It is worth noting that the CCV and CCA scale with the cube and square of the converter power rating, respectively (as can be observed by considering the units of the integrals). For a given converter, the scaling factors ηV,ηAsubscript𝜂Vsubscript𝜂A\eta_{\mathrm{V}},\,\eta_{\mathrm{A}}italic_η start_POSTSUBSCRIPT roman_V end_POSTSUBSCRIPT , italic_η start_POSTSUBSCRIPT roman_A end_POSTSUBSCRIPT that yield the same volume or area, respectively, for given CCA or CCVs are deakin2023multiplexing

ηV=CCV2CCV13,ηA=CCA2CCA1.formulae-sequencesubscript𝜂V3subscriptCCV2subscriptCCV1subscript𝜂AsubscriptCCA2subscriptCCA1\qquad\eta_{\mathrm{V}}=\sqrt[3]{\dfrac{\mathrm{CCV}_{2}}{\mathrm{CCV}_{1}}}\,%,\eta_{\mathrm{A}}=\sqrt{\dfrac{\mathrm{CCA}_{2}}{\mathrm{CCA}_{1}}}\,.italic_η start_POSTSUBSCRIPT roman_V end_POSTSUBSCRIPT = nth-root start_ARG 3 end_ARG start_ARG divide start_ARG roman_CCV start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_ARG start_ARG roman_CCV start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_ARG end_ARG , italic_η start_POSTSUBSCRIPT roman_A end_POSTSUBSCRIPT = square-root start_ARG divide start_ARG roman_CCA start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_ARG start_ARG roman_CCA start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_ARG end_ARG .(9)

For example, if the value of the CCA of a second converter is double that of a first, then the first converter would need to be a factor of ηA=2subscript𝜂A2\eta_{\mathrm{A}}=\sqrt{2}italic_η start_POSTSUBSCRIPT roman_A end_POSTSUBSCRIPT = square-root start_ARG 2 end_ARG larger to have the same CCA.

2.2.1 HB Sizing Case Studies

To explore potential benefits of the proposed approach for 4W current unbalance mitigation, we consider four sizing and reconfiguration approaches.

  • An m𝑚mitalic_m-leg reconfigurable converter, each with uniform leg sizes of capacity 1/m1𝑚1/m1 / italic_mpu, denoted 𝒰(m)𝒰𝑚\mathcal{U}(m)caligraphic_U ( italic_m ).

  • Three-leg and four-leg converters with uniform HB leg capacities and legs hard-wired to phase wires, denoted 𝒰Fix(3),𝒰Fix(4)superscript𝒰Fix3superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(3),\,\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 3 ) , caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ) respectively. Note that 𝒰Fix(3)superscript𝒰Fix3\mathcal{U}^{\mathrm{Fix}}(3)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 3 ) does not have a neutral for return current.

  • Designs with leg capacities chosen to maximise the Standalone system CCA, 𝒮4Opt.subscriptsuperscript𝒮Opt4\mathcal{S}^{\mathrm{Opt.}}_{4}caligraphic_S start_POSTSUPERSCRIPT roman_Opt . end_POSTSUPERSCRIPT start_POSTSUBSCRIPT 4 end_POSTSUBSCRIPT; or the Interconnected system CCV, 4Opt.subscriptsuperscriptOpt4\mathcal{I}^{\mathrm{Opt.}}_{4}caligraphic_I start_POSTSUPERSCRIPT roman_Opt . end_POSTSUPERSCRIPT start_POSTSUBSCRIPT 4 end_POSTSUBSCRIPT. The sizes of each leg was chosen by evaluating the value of α𝛼\alphaitalic_α that maximises the CCA or CCV using a meshgrid of all α𝛼\alphaitalic_α at a resolution of 0.01 pu. CCA and CCV values for each α𝛼\alphaitalic_α are determined using the method of Section2.3.1.

  • An idealised converter, denoted ΩΩ\Omegaroman_Ω–i.e., a design for which leg capacity can be allocated continuously, providing an upper bound on CCA and CCV values deakin2023multiplexing .

The capability chart for the idealised design ΩΩ\Omegaroman_Ω is found by replacing the leg reconfiguration constraint (3) with the continuous constraint

|Iϕ(P)[i]|1.subscript𝐼italic-ϕ𝑃delimited-[]𝑖1|I_{\phi}(P)[i]|\leq 1\,.| italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT ( italic_P ) [ italic_i ] | ≤ 1 .(10)

2.3 Calculating Capability Chart Area or Volumes

Determining the CCA or CCV requires the evaluation of the multi-dimensional integrals (8). In general, such integrals can be computationally challenging deakin2023multiplexing . However, considering uniform converters 𝒰(m)𝒰𝑚\mathcal{U}(m)caligraphic_U ( italic_m ) or converters with four legs, these integrals can be calculated very conveniently as we demonstrate.

2.3.1 Brute Force Grid Methods

In this work, CCA or CCV values are determined by first considering a regular grid of points over a region R𝑅Ritalic_R that is known to completely enclose the capability chart C𝐶Citalic_C. An indicator function F(P,α)𝐹𝑃𝛼F(P,\,\alpha)italic_F ( italic_P , italic_α ) is then defined that returns value 1 if the point lies within the capability chart and zero otherwise. The CCA or CCV is then conveniently found via a normalised sum of the indicator function values at all points across the grid.

If there are four legs of the converter, then the indicator function is

F4(P,α)={1ifα[i]|Iϕ[i]|i{1, 2, 3, 4},0otherwise,subscript𝐹4𝑃𝛼cases1if𝛼delimited-[]𝑖subscript𝐼italic-ϕdelimited-[]𝑖for-all𝑖12340otherwiseF_{4}(P,\alpha)=\begin{cases}1&\mathrm{if}\quad\alpha[i]\leq|I_{\phi}[i]|\;%\forall\;i\in\{1,\,2,\,3,\,4\}\,,\\0&\mathrm{otherwise\,,}\end{cases}italic_F start_POSTSUBSCRIPT 4 end_POSTSUBSCRIPT ( italic_P , italic_α ) = { start_ROW start_CELL 1 end_CELL start_CELL roman_if italic_α [ italic_i ] ≤ | italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT [ italic_i ] | ∀ italic_i ∈ { 1 , 2 , 3 , 4 } , end_CELL end_ROW start_ROW start_CELL 0 end_CELL start_CELL roman_otherwise , end_CELL end_ROW(11)

where P𝑃Pitalic_P is linked to phase currents (4), Iϕsubscript𝐼italic-ϕI_{\phi}italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT has been assumed as in per-unit, and (with slight abuse of notation) α𝛼\alphaitalic_α and |Iϕ|subscript𝐼italic-ϕ|I_{\phi}|| italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT | have been ordered according to their size. For converters with uniform leg sizing 𝒰(m)𝒰𝑚\mathcal{U}(m)caligraphic_U ( italic_m ), the indicator function is

F𝒰(P,α)={1ifi=14ceil(m|Iϕ(P)[i]|)m,0otherwise,subscript𝐹𝒰𝑃𝛼cases1ifsuperscriptsubscript𝑖14ceil𝑚subscript𝐼italic-ϕ𝑃delimited-[]𝑖𝑚0otherwiseF_{\mathcal{U}}(P,\alpha)=\begin{cases}1&\mathrm{if}\quad\sum_{i=1}^{4}\mathrm%{ceil}(m|I_{\phi}(P)[i]|)\leq m\,,\\0&\mathrm{otherwise\,,}\end{cases}italic_F start_POSTSUBSCRIPT caligraphic_U end_POSTSUBSCRIPT ( italic_P , italic_α ) = { start_ROW start_CELL 1 end_CELL start_CELL roman_if ∑ start_POSTSUBSCRIPT italic_i = 1 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT 4 end_POSTSUPERSCRIPT roman_ceil ( italic_m | italic_I start_POSTSUBSCRIPT italic_ϕ end_POSTSUBSCRIPT ( italic_P ) [ italic_i ] | ) ≤ italic_m , end_CELL end_ROW start_ROW start_CELL 0 end_CELL start_CELL roman_otherwise , end_CELL end_ROW(12)

where ceil()ceil\mathrm{ceil}(\cdot)roman_ceil ( ⋅ ) is the ‘ceiling’ function (i.e., non-integer arguments are rounded up to the nearest integer).

2.3.2 Evaluating the Boundary of the Capability Chart

A complementary approach for exploring the capability chart C𝐶Citalic_C is by finding its boundary. This has two potential uses for analysis and visualization. Firstly, it can be used as a method to determine the CCA or CCV. For example, if the radius r𝑟ritalic_r of the boundary of the capability chart C𝐶Citalic_C of a Standalone 4W VSC is known as a function of the angle θ𝜃\thetaitalic_θ in the plane, then

CCA=θ=02πr(θ)𝑑θ.CCAsuperscriptsubscript𝜃02𝜋𝑟𝜃differential-d𝜃\mathrm{CCA}=\int_{\theta=0}^{2\pi}r(\theta)d\theta\,.roman_CCA = ∫ start_POSTSUBSCRIPT italic_θ = 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT 2 italic_π end_POSTSUPERSCRIPT italic_r ( italic_θ ) italic_d italic_θ .(13)

This could be an advantage as it reduces the dimension of the grid of points that must be evaluated over (e.g., from 2 to 1 for CCAs). Secondly, when the total power injection PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT is non-zero, the boundary is not necessarily connected to the interior of the capability chart (as we show in Section3.2). It therefore provides different information than that which is provided by considering the size of the set (i.e., the CCA or CCV) alone.

To efficiently determine the radius at the boundary r𝑟ritalic_r, it is proposed to consider the capability charts in αβγ𝛼𝛽𝛾\alpha\beta\gammaitalic_α italic_β italic_γ co-ordinates via the Clarke transformation,

P^=TClarkeP,^𝑃subscript𝑇Clarke𝑃\hat{P}=T_{\mathrm{Clarke}}P\,,over^ start_ARG italic_P end_ARG = italic_T start_POSTSUBSCRIPT roman_Clarke end_POSTSUBSCRIPT italic_P ,(14)

where the Clarke transformation matrix TClarkesubscript𝑇ClarkeT_{\mathrm{Clarke}}italic_T start_POSTSUBSCRIPT roman_Clarke end_POSTSUBSCRIPT is

TClarke=23[11/21/203/23/21/21/21/2].subscript𝑇Clarke23matrix1121203232121212T_{\mathrm{Clarke}}=\sqrt{\dfrac{2}{3}}\begin{bmatrix}1&-1/2&-1/2\\0&\sqrt{3}/2&-\sqrt{3}/2\\1/\sqrt{2}&1/\sqrt{2}&1/\sqrt{2}\\\end{bmatrix}\,.italic_T start_POSTSUBSCRIPT roman_Clarke end_POSTSUBSCRIPT = square-root start_ARG divide start_ARG 2 end_ARG start_ARG 3 end_ARG end_ARG [ start_ARG start_ROW start_CELL 1 end_CELL start_CELL - 1 / 2 end_CELL start_CELL - 1 / 2 end_CELL end_ROW start_ROW start_CELL 0 end_CELL start_CELL square-root start_ARG 3 end_ARG / 2 end_CELL start_CELL - square-root start_ARG 3 end_ARG / 2 end_CELL end_ROW start_ROW start_CELL 1 / square-root start_ARG 2 end_ARG end_CELL start_CELL 1 / square-root start_ARG 2 end_ARG end_CELL start_CELL 1 / square-root start_ARG 2 end_ARG end_CELL end_ROW end_ARG ] .(15)

The transformed powers P^^𝑃\hat{P}over^ start_ARG italic_P end_ARG in αβγ𝛼𝛽𝛾\alpha\beta\gammaitalic_α italic_β italic_γ co-ordinates can be interpreted as follows. The third element, P^[3]^𝑃delimited-[]3\hat{P}[3]over^ start_ARG italic_P end_ARG [ 3 ], is proportional to the total power injected PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT, as

P^[3]=PTtl.3,^𝑃delimited-[]3subscript𝑃Ttl3\hat{P}[3]=\dfrac{P_{\mathrm{Ttl.}}}{\sqrt{3}}\,,over^ start_ARG italic_P end_ARG [ 3 ] = divide start_ARG italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT end_ARG start_ARG square-root start_ARG 3 end_ARG end_ARG ,(16)

as can be seen by considering (7), (15), (18). This means that co-ordinates P^[1],P^[2]^𝑃delimited-[]1^𝑃delimited-[]2\hat{P}[1],\,\hat{P}[2]over^ start_ARG italic_P end_ARG [ 1 ] , over^ start_ARG italic_P end_ARG [ 2 ] lie in the plane of the Standalone VSC system’s capability chart and correspond to unbalanced power injections. Secondly, the radius r𝑟ritalic_r in polar or cylindrical co-ordinates,

r2=P^[1]2+P^[2]2,superscript𝑟2^𝑃superscriptdelimited-[]12^𝑃superscriptdelimited-[]22r^{2}=\hat{P}[1]^{2}+\hat{P}[2]^{2}\,,italic_r start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT = over^ start_ARG italic_P end_ARG [ 1 ] start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT + over^ start_ARG italic_P end_ARG [ 2 ] start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ,(17)

is proportional to magnitude of the neutral current |INtrl.|subscript𝐼Ntrl|I_{\mathrm{Ntrl.}}|| italic_I start_POSTSUBSCRIPT roman_Ntrl . end_POSTSUBSCRIPT |. This can be seen by considering the magnitude of the neutral current (4) mapped through the Clarke transformation (14). From (17), constraints on neutral currents are therefore circles in αβγ𝛼𝛽𝛾\alpha\beta\gammaitalic_α italic_β italic_γ co-ordinates (rather than ellipses in nominal co-ordinates). Therefore, visualizations in αβγ𝛼𝛽𝛾\alpha\beta\gammaitalic_α italic_β italic_γ co-ordinates have additional symmetry and explainability.

For an Interconnected VSC, it is useful to represent powers P^^𝑃\hat{P}over^ start_ARG italic_P end_ARG in spherical co-ordinates,

P^[1]^𝑃delimited-[]1\displaystyle\hat{P}[1]over^ start_ARG italic_P end_ARG [ 1 ]=rSph.sin(θ)cos(ψ)absentsubscript𝑟Sph𝜃𝜓\displaystyle=r_{\mathrm{Sph.}}\sin(\theta)\cos(\psi)= italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT roman_sin ( italic_θ ) roman_cos ( italic_ψ )(18a)
P^[2]^𝑃delimited-[]2\displaystyle\hat{P}[2]over^ start_ARG italic_P end_ARG [ 2 ]=rSph.sin(θ)sin(ψ)absentsubscript𝑟Sph𝜃𝜓\displaystyle=r_{\mathrm{Sph.}}\sin(\theta)\sin(\psi)= italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT roman_sin ( italic_θ ) roman_sin ( italic_ψ )(18b)
P^[3]^𝑃delimited-[]3\displaystyle\hat{P}[3]over^ start_ARG italic_P end_ARG [ 3 ]=rSph.cos(θ),absentsubscript𝑟Sph𝜃\displaystyle=r_{\mathrm{Sph.}}\cos(\theta)\,,= italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT roman_cos ( italic_θ ) ,(18c)

where rSph.subscript𝑟Sphr_{\mathrm{Sph.}}italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT is the spherical radius, ψ𝜓\psiitalic_ψ the azimuth angle, and θ𝜃\thetaitalic_θ the polar angle. In contrast to cylindrical co-ordinates, if a point at rSph.subscript𝑟Sphr_{\mathrm{Sph.}}italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT is feasible for a given ψ,θ𝜓𝜃\psi,\,\thetaitalic_ψ , italic_θ, then all points between the origin and rSph.subscript𝑟Sphr_{\mathrm{Sph.}}italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT will also be feasible.

The radius at the boundary of the capability chart can be found either by defining an appropriate indicator function and then using a root-finding method, or via an optimization to maximise r𝑟ritalic_r or rSph.subscript𝑟Sphr_{\mathrm{Sph.}}italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT. For example, for a fixed ψ𝜓\psiitalic_ψ and θ𝜃\thetaitalic_θ, the radius rSph.subscript𝑟Sphr_{\mathrm{Sph.}}italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT at the boundary of the capability chart can be determined as the solution of a mixed-integer linear program,

max\displaystyle\maxroman_maxrSph.subscript𝑟Sph\displaystyle\;r_{\mathrm{Sph.}}italic_r start_POSTSUBSCRIPT roman_Sph . end_POSTSUBSCRIPT(19a)
s.t.(1),(3),formulae-sequencestitalic-(1italic-)italic-(3italic-)\displaystyle\mathrm{s.t.}\;\eqref{e:i_constraint},\,\eqref{e:max_current},\,roman_s . roman_t . italic_( italic_) , italic_( italic_) ,(4),(14),(18).italic-(4italic-)italic-(14italic-)italic-(18italic-)\displaystyle\eqref{e:p2i},\,\eqref{e:trn_clarke},\,\eqref{e:trn_spherical}\,.italic_( italic_) , italic_( italic_) , italic_( italic_) .(19b)

2.3.3 Capability Chart Discontinuities

If the current injected into one of the wires has value of zero, then no leg capacity needs to be connected to that wire. This means that at there are regions of the capability chart which, according to the CCA and CCV definitions, do not contribute to the size of the set, as these subsets will be of lower dimension. Nevertheless, as we show in Section3, these points are non-trivial, and could be very useful for supporting some mission profiles.

The subspaces of these points in a given co-ordinate system can be found by setting one of the powers P𝑃Pitalic_P to zero (or the neutral current INtrl.subscript𝐼NtrlI_{\mathrm{Ntrl.}}italic_I start_POSTSUBSCRIPT roman_Ntrl . end_POSTSUBSCRIPT), then solving for the parameters that capture that locus. For example, for a fixed azimuth angle ψ𝜓\psiitalic_ψ (in spherical co-ordinates (18)), the powers are a function of polar angle θ𝜃\thetaitalic_θ as

TClarker[cos(ψ)0sin(ψ)001][sin(θ)cos(θ)]=P.superscriptsubscript𝑇Clarke𝑟matrix𝜓0𝜓001matrix𝜃𝜃𝑃T_{\mathrm{Clarke}}^{\intercal}r\begin{bmatrix}\cos(\psi)&0\\\sin(\psi)&0\\0&1\end{bmatrix}\begin{bmatrix}\sin(\theta)\\\cos(\theta)\end{bmatrix}=P\,.italic_T start_POSTSUBSCRIPT roman_Clarke end_POSTSUBSCRIPT start_POSTSUPERSCRIPT ⊺ end_POSTSUPERSCRIPT italic_r [ start_ARG start_ROW start_CELL roman_cos ( italic_ψ ) end_CELL start_CELL 0 end_CELL end_ROW start_ROW start_CELL roman_sin ( italic_ψ ) end_CELL start_CELL 0 end_CELL end_ROW start_ROW start_CELL 0 end_CELL start_CELL 1 end_CELL end_ROW end_ARG ] [ start_ARG start_ROW start_CELL roman_sin ( italic_θ ) end_CELL end_ROW start_ROW start_CELL roman_cos ( italic_θ ) end_CELL end_ROW end_ARG ] = italic_P .(20)

The angle θ𝜃\thetaitalic_θ that will yield the i𝑖iitalic_ith element of P𝑃Pitalic_P to be zero can be found by setting the i𝑖iitalic_ith row of (20) to be zero, then solving for θ𝜃\thetaitalic_θ.

3 Results

In this section, we evaluate the size of the capability charts for the converter sizing approaches given in Table3, considering both Standalone and Interconnected 4W VSC operation. This demonstrates how the proposed approach can improve converter flexibility. Both qualitative and quantitative properties of these capability charts are considered to explore the performance of these designs.

3.1 Capability Chart Areas for Standalone Four-Wire VSCs

In the first instance, we consider the boundary of the capability chart C𝐶Citalic_C for a Standalone VSC for a conventional, fixed design 𝒰Fix(4)superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ) and compare this against the idealised design ΩΩ\Omegaroman_Ω, as shown in Fig.5. The constraints on power injection on the phase legs form a hexagon (in direct analogy to the balanced three-terminal SOP case deakin2023optimal ). In contrast, the constraint on the neutral current forms an ellipse. Interestingly, this ellipse is completely contained within the hexagon. This highlights that a converter with all four legs sized symmetrically highly underutilizes the three phase legs–only the neutral leg is active on the boundary of the capability chart. The idealised capability chart completely encapsulates the 0.25pu hexagon, and so even if the neutral current were not the limiting factor (or an alternative means was provided for the neutral return, such as a split-capacitor), the idealised design ΩΩ\Omegaroman_Ω would still improve performance as compared to a fixed four-leg VSC 𝒰Fix(4)superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ).

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (7)

In Fig.6, the boundary of the capability charts for three designs are illustrated in nominal and αβγ𝛼𝛽𝛾\alpha\beta\gammaitalic_α italic_β italic_γ co-ordinates, with the capability chart of the benchmark cases Ω,𝒰Fix(4)Ωsuperscript𝒰Fix4\Omega,\,\mathcal{U}^{\mathrm{Fix}}(4)roman_Ω , caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ) shown in dashed lines. It can be seen in this figure that the capability chart varies significantly depending on the sizing α𝛼\alphaitalic_α. For the 5-converter uniform design 𝒰(5)𝒰5\mathcal{U}(5)caligraphic_U ( 5 ), 0.4pu is allocated to the neutral and so the capability chart is a hexagon. For a uniform, 8-converter uniform design 𝒰(8)𝒰8\mathcal{U}(8)caligraphic_U ( 8 ), the capability chart is enlarged significantly, although, it can be seen that that design is mostly contained within the optimal 4-converter design 𝒮4Opt.subscriptsuperscript𝒮Opt4\mathcal{S}^{\mathrm{Opt.}}_{4}caligraphic_S start_POSTSUPERSCRIPT roman_Opt . end_POSTSUPERSCRIPT start_POSTSUBSCRIPT 4 end_POSTSUBSCRIPT. Additionally, Fig.6 shows that many of the properties of capability chart areas of reconfigurable balanced VSCs can be observed: non-convexity; existence of capability charts as strict supersets of other capability charts; and, large increases in area compared to a conventional design deakin2023optimal .

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (8)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (9)

The CCA-based converter sizing ratio ηAsubscript𝜂A\eta_{\mathrm{A}}italic_η start_POSTSUBSCRIPT roman_A end_POSTSUBSCRIPT for the leg sizing approaches collected in Table3 are plotted in Fig.7, considering uniform designs with up to 15 legs m𝑚mitalic_m. From this figure, the poor performance of conventional designs 𝒰Fix(3),𝒰Fix(4)superscript𝒰Fix3superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(3),\,\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 3 ) , caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ) can clearly be seen–for the former, there is no neutral return, and so power can only be transferred between two phases at a time (and so the CCA is trivially zero). For the latter, it can be seen that the fixed converter 𝒰Fix(4)superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ) requires 57.8% capacity increase to achieve the same capacity as the optimal design 𝒮4Opt.subscriptsuperscript𝒮Opt4\mathcal{S}^{\mathrm{Opt.}}_{4}caligraphic_S start_POSTSUPERSCRIPT roman_Opt . end_POSTSUPERSCRIPT start_POSTSUBSCRIPT 4 end_POSTSUBSCRIPT, with an upper limit of an increase 75.3% as compared to the idealised converter ΩΩ\Omegaroman_Ω. It is also interesting to see that designs with uniformly-sized converters are relatively inefficient at increasing the capacity of the CCA, with 15 uniformly-sized converters required to achieve a larger CCA than the optimal design 𝒮Opt.(4)superscript𝒮Opt4\mathcal{S}^{\mathrm{Opt.}}(4)caligraphic_S start_POSTSUPERSCRIPT roman_Opt . end_POSTSUPERSCRIPT ( 4 ). This highlights how effective choice of leg sizes α𝛼\alphaitalic_α can yield substantially increased flexibility, echoing previous findings deakin2023optimal ; deakin2023multiplexing .

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (10)

3.2 Capability Chart Volumes for Interconnected Four-Wire VSCs

The boundary of the capability chart for the conventional, fixed design 𝒰Fix(4)superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ) and the idealised design ΩΩ\Omegaroman_Ω are plotted in Fig.8 and Fig.9, respectively, for a range of values of total power injection PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT. As expected, it can be observed a total power injection PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT with value zero matches the Standalone 4W VSC (Fig.5); but, as the total power injection PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT increases, the shape of the capability chart changes significantly. For example, as PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT increases above 0.5 pu, the set of feasible injections quickly reduces, reaching a single point at 1pu injection. A power injection PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT of 0.5pu leads to the greatest per-phase power injection potential of 0.5pu (by comparison, if the power injection PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT is 1pu, the per-phase power injection is 1/3pu, i.e., 50% lower).

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (11)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (12)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (13)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (14)

For reconfigurable designs, the capability charts of Interconnected 4W VSC systems are more complex than those of Standalone systems. For example, the capability chart for three angles of azimuth ψ𝜓\psiitalic_ψ are plotted in Fig.10 (only the first quadrant is plotted due to symmetry). The filled areas are calculated using Section2.3.1’s brute-force method, with the red outer boundary line calculated by determining the boundary in spherical co-ordinates (Section2.3.2); the black dashed line indicating the boundary of the idealised design. It can be observed that the Interconnected VSC can have isolated points, as described in Section2.3.3. Due to the complex non-convexities in the capability chart, only snapshots at given ψ𝜓\psiitalic_ψ are given (as compared to the full capability charts which can be plotted in Fig.8 and Fig.9 for the conventional and idealised designs, respectively).

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (15)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (16)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (17)

For a fixed value of PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT, the capability charts can have more complexity again. The capability charts for three values of PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT are shown in Fig.11, with solid coloured areas are plotted using Section2.3.1’s brute-force methods (coloured area); red lines calculated using Section2.3.2’s boundary method in cylindrical co-ordinates; and, black dashed lines showing the boundary of the capability chart of the idealised design ΩΩ\Omegaroman_Ω and benchmark 𝒰Fix(4)superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ). There are two main differences between these spherical and cylindrical capability charts representations. Most strikingly, there can be ‘holes’ in the capability charts when plotted for a fixed PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT, as shown in Fig.11b and Fig.11c. For example, close to the origin, it may be the case that even with the smallest leg connected to the neutral, there is not sufficient capacity to inject PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT in an (almost) balanced way; so, there must be a reasonable amount of unbalanced power injected to enable the full value of PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT.

Secondly, it is interesting to note that when there is a fixed PTtl.subscript𝑃TtlP_{\mathrm{Ttl.}}italic_P start_POSTSUBSCRIPT roman_Ttl . end_POSTSUBSCRIPT, there can be isolated points (Fig.11a), isolated lines (Fig.11b), and isolated areas (Fig.11c). This could lead to more complex operation as compared to a conventional power converter–a more complicated procedure would need to be run to determine the connection of the converters as the mission profile changes, for example.

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (18)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (19)
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (20)

Finally, the CCV-based converter size ratios ηVsubscript𝜂V\eta_{\mathrm{V}}italic_η start_POSTSUBSCRIPT roman_V end_POSTSUBSCRIPT for various designs are shown in Fig.12. Compared to the Standalone 4W VSC case, the gap between the size ratio ηVsubscript𝜂V\eta_{\mathrm{V}}italic_η start_POSTSUBSCRIPT roman_V end_POSTSUBSCRIPT of the conventional design 𝒰Fix(4)superscript𝒰Fix4\mathcal{U}^{\mathrm{Fix}}(4)caligraphic_U start_POSTSUPERSCRIPT roman_Fix end_POSTSUPERSCRIPT ( 4 ) and the idealised design ΩΩ\Omegaroman_Ω, the potential for improvement is slightly reduced to 62.7%. Nevertheless, it remains a significant increase, and this ratio is still larger than that of the three-terminal SOP considered in deakin2023optimal (which has a value of ηAsubscript𝜂A\eta_{\mathrm{A}}italic_η start_POSTSUBSCRIPT roman_A end_POSTSUBSCRIPT of 150% for the idealised design). In contrast to the Standalone VSC, uniform sizing is also much more effective at increasing the CCV compared to optimal design 4Opt.subscriptsuperscriptOpt4\mathcal{I}^{\mathrm{Opt.}}_{4}caligraphic_I start_POSTSUPERSCRIPT roman_Opt . end_POSTSUPERSCRIPT start_POSTSUBSCRIPT 4 end_POSTSUBSCRIPT, with the nine-converter design 𝒰(9)𝒰9\mathcal{U}(9)caligraphic_U ( 9 ) surpassing the CCV of the optimal design 4Opt.subscriptsuperscriptOpt4\mathcal{I}^{\mathrm{Opt.}}_{4}caligraphic_I start_POSTSUPERSCRIPT roman_Opt . end_POSTSUPERSCRIPT start_POSTSUBSCRIPT 4 end_POSTSUBSCRIPT.

RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (21)

4 Conclusion

The reconfiguration of power converters using low-cost selector switches in applications with variable mission profiles has previously shown significant promise in balanced distribution systems. In this work, the approach has been shown to be effective as a potential approach for current unbalance mitigation, with a conventional design requiring between 62.7% and 75.3% increased capacity to match an idealised converter. Efficient numerical methods have been given to determine the feasible sets and boundary of the capability charts, with more complex capability charts as compared to previously considered reconfigurable converters, particularly when the VSCs are interconnected to a dc-side power source or load.

It is concluded that power converter reconfiguration can be an effective tool for reallocating capacity of individual legs of power converters in several different applications. Future work could explore hardware approaches to implement the proposed reconfiguration approach to consider more clearly the practical challenges of implementing the selector switches. In addition, other optimal design and operational approaches will be considered to further increase converter flexibility and utilization.

5 Acknowledgements

M. Deakin was supported by the Royal Academy of Engineering under the Research Fellowship programme. X. Deng was supported by Newcastle University Academic Track (NUAcT) Fellowship scheme.

6 References

References

  • [1]A.Speakman, O.Harris, C.Birkinshaw-Doyle, and D.Mills, “Low voltagenetwork capacity study,” UK Department for Business, Energy and IndustrialStrategy (BEIS), Tech. Rep., July 2022,https://www.gov.uk/government/publications/low-voltage-network-capacity-study.
  • [2]K.Ma, L.Fang, and W.Kong, “Review of distribution network phase unbalance:Scale, causes, consequences, solutions, and future research directions,”CSEE Journal of Power and Energy systems, vol.6, no.3, pp. 479–488,2020.
  • [3]K.Ma, R.Li, I.Hernando-Gil, and F.Li, “Quantification of additionalreinforcement cost from severe three-phase imbalance,” IEEETransactions on Power Systems, vol.32, no.5, pp. 4143–4144, 2016.
  • [4]O.Pereira, J.Quirós-Tortós, and G.Valverde, “Phase rebalancing ofdistribution circuits dominated by single-phase loads,” IEEETransactions on Power Systems, vol.36, no.6, pp. 5333–5344, 2021.
  • [5]F.Shahnia, P.J. Wolfs, and A.Ghosh, “Voltage unbalance reduction in lowvoltage feeders by dynamic switching of residential customers among threephases,” IEEE Transactions on Smart Grid, vol.5, no.3, pp.1318–1327, 2014.
  • [6]B.Liu, F.Geth, N.Mahdavi, and J.Zhong, “Load balancing in low-voltagedistribution networks via optimizing residential phase connections,” in2021 IEEE PES Innovative Smart Grid Technologies-Asia (ISGTAsia).IEEE, 2021, pp. 1–5.
  • [7]X.Cui, G.Ruan, F.Vallée, J.-F. Toubeau, and Y.Wang, “A two-levelcoordination strategy for distribution network balancing,” IEEETransactions on Smart Grid, vol.15, no.1, pp. 529–544, 2024.
  • [8]K.Girigoudar, M.Yao, J.L. Mathieu, and L.A. Roald, “Integration ofcentralized and distributed methods to mitigate voltage unbalance using solarinverters,” IEEE Transactions on Smart Grid, vol.14, no.3, pp.2034–2046, 2022.
  • [9]A.S. deMorais, F.L. Tofoli, and I.Barbi, “Modeling, digital control, andimplementation of a three-phase four-wire power converter used as a powerredistribution device,” IEEE Transactions on Industrial Informatics,vol.12, no.3, pp. 1035–1042, 2016.
  • [10]M.Stecca, T.B. Soeiro, A.K. Iyer, P.Bauer, and P.Palensky, “Batterystorage system as power unbalance redistributor in distribution grids basedon three legs four wire voltage source converter,” IEEE Journal ofEmerging and Selected Topics in Power Electronics, vol.10, no.6, pp.7601–7614, 2022.
  • [11]M.Deakin, “Optimal hybrid multiplexed ac/dc/ac power converters,” in19th International Conference on AC and DC Power Transmission (ACDC2023).IET, 2023.
  • [12]——, “Multiplexing power converters for cost-effective and flexible softopen points,” IEEE Transactions on Smart Grid, vol.15, no.1, pp.260–271, 2024.
  • [13]C.Lou, J.Yang, T.Li, and E.Vega-Fuentes, “New phase-changing soft openpoint and impacts on optimising unbalanced power distribution networks,”IET Generation, Transmission & Distribution, vol.14, no.23, pp.5685–5696, 2020.
  • [14]M.Vanin, H.Ergun, R.D’hulst, K.Vanthournout, and D.VanHertem, “Analysisand insights from reactive power measurements of low voltage users,” in27th International Conference on Electricity Distribution (CIRED2023).IET, 2023.
RECONFIGURABLE POWER CONVERTERS WITH INCREASED UTILIZATION FOR UNBALANCED POWER DISTRIBUTION SYSTEM APPLICATIONS (2024)

FAQs

What are the applications of power converters? ›

In electric trains, the power is transferred from the overhead lines to the motors using a power converter like the one shown in the figure. This converter generates the required voltages for controlling the torque and speed of the electric motor.

What are the factors that affect the performance of power electronic converters? ›

For example, high temperatures can reduce the efficiency of the converter by increasing its internal resistance. The operating conditions of the converter can also impact its efficiency. Factors such as the frequency of the input voltage, the output current, and the load can all affect the performance of the device.

What is an example of a power converter? ›

frequency converter (input AC/output AC), also called, cycloconverter or phase converter. A power converter can also be made of the union of two or more basic converters, e.g. power converters in wind turbines normally consist of a rectifier (generator-side converter) and an inverter (grid-side converter).

What are converters used for? ›

A converter is any electronic device capable of changing electric power from one form to another. Since there are two major types of electric power, namely alternating current (AC) and direct current (DC), a converter converts from one form to another. This means you can change AC to DC or DC to AC with a converter.

What are the four types of converters? ›

There are several kings of converters based on the source input voltage and the output voltage and these falls into four categories namely the AC to DC converter known as the rectifier, the AC to AC clycloconverter or frequency changer, the DC to DC voltage or current converter, and the DC to AC inverter.

Why would I need a power converter? ›

While the purpose of an adapter is to simply help the plugs on your electronics fit into (or more aptly, adapt to the shape of) foreign outlets, a converter's job is to change the voltage found in an outlet to match that of your devices.

What are the disadvantages of power converters? ›

Power electronics converters in power system dynamics have limitations such as reduced efficiency, lower noise immunity, and decreased system reliability when operating at elevated temperatures 1 4.

What are the application of power electronics in power system? ›

Power electronics are widely used in motor control systems such as industrial automation, robotics, and power generation systems. They are utilized to regulate the speed and torque of electric motors, resulting in enhanced efficiency and reduced energy consumption.

Why power electronic converters are applied in distribution systems? ›

The power electronic converter is then used to provide the connection/conversion between the generation units and the grid/consumers, to achieve high efficiency and meet the grid requirements, including frequency, voltage, active and reactive power, flickers, harmonics and ride-through capabilities, etc.

What are the basics of power converters? ›

Power converters ensure compatibility between the power source and the electrical devices by converting the power into the appropriate form and level. Energy efficiency: Power converters can significantly improve energy efficiency by adjusting the voltage and current to match the load requirements precisely.

How do you use a power converter? ›

The converter is connected to the input 220V mains power with a national standard power plug cable, which can be directly connected to the domestic household mains. Turn on the switch, and the output end is a universal universal socket, and the electrical appliance can be directly connected to the socket.

What's the difference between a power converter and a power adapter? ›

An adapter changes the plug configuration so your US power plugs fit into the wall socket in the foreign country you are visiting. A converter changes the electricity so you can use your NON-DUAL-VOLTAGE appliances when visiting a foreign country.

How does a power converter work? ›

How does a Power Converter work? Power converters function through the use of semiconductor components that control and modify electrical power. These components include diodes, transistors, and thyristors, among others.

What is the importance of power converter? ›

Power converters used to convert the DC to AC in consumer electronics. Converters used to enhance the efficiency of batteries in consumer electronics, such as laptops and smartphones. Generation systems, such as fuel cells, can provide backup power for consumer electronics, considering power outage conditions.

What is the difference between a power inverter and a converter? ›

Converters convert the voltage of an electric device, usually alternating current (AC) to direct current (DC). On the other hand, inverters convert direct current (DC) to alternating current (AC).

What are the application of power switching devices? ›

A few applications of power semiconductors in switch mode include lamp dimmers, switch mode power supplies, induction cookers, automotive ignition systems, and AC and DC electric motor drives of all sizes.

What are the applications of current to voltage converter? ›

One example of such an application is using the photodiode sensor to measure light intensity. The output of the photodiode sensor is a current which changes proportional to the light intensity. Another advantage of the opamp circuit is that the voltage across the photodiode (current source) is kept constant at 0V.

What is the purpose of the electrical converter? ›

These converters are used to convert AC from the power grid into DC, which is required by most electronic devices. They are commonly found in various power supplies, including chargers for batteries and electronic gadgets. DC-AC converters, also known as inverters.

What are the applications of AC DC converters? ›

There are a lot of real-life applications that are based on this conversion. AC/DC converters are used in industrial process control systems, consumer devices, measurement equipment, semiconductor manufacturing equipment, medical devices, and defense applications.

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