21, rue d’Artois, F-75008 PARIS http : //www.cigre.org B4-204 CIGRE 2012 Requirements of DC-DC Converters to facilitate large DC Grids C.D. BARKER, C.C. DAVIDSON, D.R. TRAINER, R.S. WHITEHOUSE, Alstom Grid UK Ltd United Kingdom SUMMARY Two DC grids may be constructed independently. As these DC grids are independently developed, the operating DC voltage, the operating strategy or even the DC topology may be different and hence, these two DC grids cannot be directly connected. Just as AC systems operating at different voltages require transformers to exchange power, DC grids require DCDC converters to exchange power between networks. A group of offshore windfarms may use a high voltage DC, multi-terminal, bulk power transfer scheme to transfer the power to the onshore AC system. At a future stage a new offshore windfarm may be constructed sufficiently remote from the existing scheme or the mainland to merit a DC transmission connection; but at a lower voltage rating than the existing scheme. An economic method of interconnection may, therefore, be the use of an AC-DC converter at the windfarm and a DC-DC converter local to the existing offshore converter in order to use the existing DC grid to bring the power onshore. Many turbines actually generate an AC output from an AC-DC-AC converter. By removing the DC-AC stage within the wind turbine a medium voltage DC collector bus could be used as a common power interconnection between the DC outputs from multiple wind turbines. A DC-DC converter could then be used to raise the DC voltage to a higher voltage for transmission to an onshore DC to AC converter. For many years the possibility has existed of utilising HVDC to supply multiple small loads dispersed over a large geographical area. As each load may only be at a relatively low power the cost of a 3-phase DC-AC high voltage converter may be prohibitive; but a low cost DC-DC converter could be used to reduce the DC bus voltage at each load centre. There are, today, many existing Line Commutated Converter (LCC) HVDC transmission schemes in operation. By using DC to DC converters it may be possible to interconnect these existing DC schemes with new VSC HVDC converter multi-terminal grids increasing the utilisation of existing grids. KEYWORDS Voltage-Sourced, Converter, HVDC, DC-DC. carl.barker@alstom.com 1. INTRODUCTION The applications for DC-DC converters within HVDC Grids are beginning to emerge as the concept of DC-DC grids gets closer to being a reality with the increased availability of Voltage Source Converters (VSC). The VSC can exchange power between different nodes within a network by reversal of DC current instead of DC voltage, making the power flow between terminals very much more flexible than can be achieved with Line Commutated Converters (LCC). VSC technology also opens up the opportunities for novel circuit topologies and some of these can be applied to converters designed to connect DC systems together. There are many reasons for interconnecting two or more DC circuits and these different reasons result in different requirements. In order to classify the general parameters of a DC-DC converter the following nomenclature has been adopted in this paper: High Power Medium Power Low Power 50 MWdc 0 MWdc ≤ ≤ Vdc HIGH VOLTAGE SIDE Low Ratio Medium Ratio Transferred DC Power ≥ Transferred DC Power ≤ Transferred DC Power ≤ Vdc LOWER VOLTAGE SIDE 1.5 High Ratio ≤ Vdc HIGH VOLTAGE SIDE Vdc LOWER VOLTAGE SIDE Vdc HIGH VOLTAGE SIDE Vdc LOWER VOLTAGE SIDE 500 MWdc 500 MWdc 50 MWdc ≤ 1.5 ≤ 5 ≥ 5 Each of the above categories has their own specific drivers in terms of capital cost, losses, volume etc. Therefore, there is not, necessarily one DC-DC converter topology that is suitable for all applications. Instead, it is envisaged in this paper that there will be many alternative topologies based on common building blocks. 2. LOSSES AND RATINGS If losses are considered, then it can be assumed that for both ‘high power’ and ‘medium power’ loss capitalisation will be a significant factor in the design of the DC-DC conversion process. For ‘low power’ applications however, losses may be less significant since the whole reason for using DC may be that it is the only practical solution to an electrical energy transfer problem and, whilst losses may be higher than with other converter applications, as a percentage, the loss may not be as significant. For high power and medium power converters the component ratings will be significantly affected by the characteristics of the through-put power. Where the power is transferred between DC circuits in a discontinuous manner, for example as pulses of electrical energy transferred between passive components, then the converters must be rated for the maximum instantaneous value of the throughput voltage and current. This can lead to very high component ratings, particularly in terms of valve voltage rating which strongly impacts on the cost of the converter. It is better, therefore, to operate the converter in a manner which provides continuous power flow between the two DC circuits. 2 Figure 1: A Simple Buck/Boost Converter As an example consider the simple Buck/Boost converter shown in Figure 1 [1]. Assume that Vd1 is larger than Vd2. When switch S1 is closed diode D1 is reverse biased and hence energy is transferred from DC System 1 to the inductor L1 where it is stored as magnetic energy. When switch S1 then opens the diode D1 will be forward biased as energy will transfer from inductor L1 to Capacitor C1 where it will be stored as electrostatic energy. Energy can then be transferred from the capacitor C1 to DC System 2. This operation results in a pulse of energy being drawn from DC System 1 which would require significant DC harmonic filtering to smooth. The load current as seen by the components S1, D1, L1 and C1 will have a greater value than the actual transferred DC current requiring these components to be rated for a higher current than the load current. The voltage rating of the circuit is the difference between +Vd1 and –Vd2 hence the components are rated for a voltage greater than the DC voltage of the system to which they are coupled. In addition the operation of this circuit relies on the electromagnetic and electrostatic storage of energy necessitating large component values. The size of the energy storage component values can, to some extent, be mitigated by increasing the switching frequency of switch S1. However, doing this will increase the converter switching losses. An optimum value for component ratings and losses can be found but the ratings of the individual components within the circuit must always exceed the steadystate load. By using a circuit topology which can transfer energy in a continuous fashion from DC System 1 to DC System 2 and vice versa, the need for rating components for a voltage and current greater than the steady-state load value can be mitigated and hence the rating and losses of the converter can be reduced. The concern with regards to component ratings may not be as significant when considering low power conversion. In this case, as in the case of losses, the cost of the conversion may not be as significant as the requirement to actually deliver the power. As losses can be considered as less of a design factor alternative converter topologies may be more appropriate as they can be provided for a lower capital cost, despite the increase in component ratings. 3. GALVANIC SEPARATION AND FAULT BLOCKING From [2] ‘Galvanic Separation’ is defined as “prevention of electric conduction between two electric circuits intended to exchange power and/or signals”. In the context of DC-DC converters this definition is taken to mean that there is no direct current path between side A and side B of the DC-DC converter. A simple example of such a connection with Galvanic Separation would be the use of a coupling transformer between the two DC circuits, Figure 2(a). Consider the simple DC-DC converter shown in Figure 2(b). A pole-to-ground fault in one symmetrical monopole will result in the voltage on the healthy pole ‘jumping’ up in voltage to a prospective value of 2 pu. With a direct current path connection, this DC voltage shift can be transferred across to the other DC system, that is, a pole-to-ground fault on one DC system can propagate to another DC system via a DC-DC converter. 3 With very fast control response it may be possible to inhibit the DC pole-toground fault transfer between DC systems so long as the power electronic valves associated with the (a) part of the converter connected to the unfaulted system are rated for the maximum voltage difference. This voltage difference may be the determining factor in the rating of the valve as it may be higher than the normal working voltage stress across (b) the converter. Where the converter Figure 2: A Simple DC-DC Converter ratio is ‘low’ the voltage transfer may (a) with Galvanic Separation not be excessive and hence this (b) without Galvanic Separation method may provide an optimum solution. However, with ‘medium’ or ‘high’ voltage ratios the use of Galvanic separation provides the facility of transferring the voltage stress to another component, typically an inter-connection transformer. Fault blocking capability within a DC-DC converter stops a fault on one DC system propagating to the other DC system, that is, it acts as a firewall. Consider Figure 2, a DC-DC short circuit will not cascade through the DC-DC converter if the AC link voltage collapses. 4. HIGH POWER, LOW RATIO CONNECTIONS In AC systems a common means of achieving a voltage change is to use an auto-transformer. The auto-transformer does not offer galvanic separation between the two AC voltage levels and is best suited to low ratio applications; “In most cases an auto-transformer is not a particularly favourable proposition for voltage transformation ratios above 2” [3]. An equivalent in a DC grid would be the interconnection of two DC systems operating at a similar voltage and using the same topology (for example, symmetrical monopole or bipole). +Vd1 +Vd2 -Vd1 -Vd2 Figure 3: A High power, low Ratio DC-DC Converter One possible implementation of the basic converter for this application, based on the “Alternate Arm Converter” [4], [5] is shown in Figure 3 and converts DC-AC-DC. Equally, the now well established Modular Multi-Level Converter topology, such as the ALSTOM Grid MaxSine generation 1, could be 4 used. The two DC-AC converters are 3-phase in order to provide a power through-put capability equivalent to any AC system connection converter that forms part of the DC grid. If higher levels of power transfer were required a multi-phase AC connection between the two systems could be utilised. The form of the AC connection shown in Figure 3 need not be at a frequency such as 50 Hz or 60 Hz. Higher frequencies, such as 500 Hz, are proposed in order to minimise the component ratings of the individual cells within the converter for example increasing the AC frequency allows the capacitor value (mF) to be reduced whilst maintaining the same power electronics module. In addition the AC connection need not be sinusoidal. Alternative waveshapes such as a square-wave or trapezoidal can be used, along with the converter to optimise both component ratings and converter losses. In Figure 3 each valve in each of the two three phase converter bridges shown consists of a ‘Director Switch’ in series with a series connection of ‘Full-Bridge’ sub-module. The Full-Bridge modules are rated for the DC voltage of the associated DC system whilst the director switch is rated for the DC voltage of the associated DC system plus an additional offset voltage which could result from a poleto-ground fault in the DC system. Hence, in this configuration fault propagation between DC networks can be blocked without having Galvanic separation. Where the two DC schemes are of different topologies, for example one DC system is a ±320 kV symmetrical monopole whilst the other is a +500 kV monopole (possibly part of a bipole scheme) the shift in ground reference would give rise to a circulating DC component of current between the two DC systems via the ‘AC’ connection, making this arrangement unsuitable for such an application. The ‘AC’ system in Figure 3 is common to both DC/AC converters and hence the AC line-to-line voltage and phase current is common. Where both DC System 1 and DC System 2 are of a similar voltage magnitude the AC quantities can be optimised to minimise the converter losses. The losses of this arrangement would be approximately 75% and the cost approximately 80% when compared to a fundamental frequency back-to-back. However, as the DC voltage difference increases the selection of AC quantities will be less optimised for one, or both, of the DC/AC converters. Considering this, plus the need for additional valve rating to avoid transferring earth shifts this circuit is considered best suited to ‘Low’ DC voltage ratio applications. 5. MEDIUM POWER, MEDIUM RATIO CONNECTIONS Power transfer requirements between two DC systems may not always require a multi-phase AC coupling in which case a single phase interconnection can be used. This can be particularly useful where the DC voltage ratio across the converter is ‘medium’ or ‘high’ and an transformer coupling between the AC connections of the DC/AC converters is to be used, see Figure 4. Transformer couplings, as shown in Figure 4, can also be used to provide Galvanic Separation between the two DC systems. In the case shown, if the two DC systems are both symmetrical monopoles the connection transformer will experience the DC voltage stress resulting from a pole-toground fault across the windings, not transferring the DC voltage step across the electromagnetic transformer coupling. Also, where one DC system is a symmetrical monopole whilst the other is a bipole, as in the example discussed in 4 above, the electromagnetic transformer coupling will block any DC current flow across the ‘AC’ connection. In both cases the connection transformer can experience a high level of DC voltage on the windings and hence this connection transformer must take this DC voltage stress into account in the insulation design. As with the direct AC coupled converters discussed in 4, the ‘AC’ connection does not have to be at 50 Hz or 60 Hz nor does it have to be sinusoidal. Various optimisations can be made between the converter and the connection transformer in order to optimise the overall design. In this case however, the advantages of operating at higher frequencies must also consider the impact on the design of the connection transformer. With increasing frequency the transformer core size can be reduced, thereby, reducing cost and volume (which could be a significant factor if the equipment is to be located 5 offshore on a platform). However, without introducing special materials into the transformer core design the reduction in volume is non-linear, having a reducing impact with increasing frequency. The losses of an arrangement such as that shown in Figure 4 using an AC connection frequency of 500Hz would be approximately 105% and the cost approximately 75% when compared to a fundamental frequency back-to-back. Figure 4: A Medium power, medium Ratio DC-DC Converter 6. CONNECTING A VSC AND LCC INTERCONNECTION To date the majority of HVDC in operation is point-to-point interconnection using Line Commutated Converter (LCC) technology. Such DC interconnections have provided and continue to provide the most cost effective means for bulk power transmission. However, with large, bulk power transmission systems there may be applications where there is an advantage in connecting a VSC with an LCC HVDC connection. +Vd2 VSC - DC System 2 LCC - DC System 1 +Vd1 -Vd2 Figure 5: An LCC/VSC DC-DC Converter A major difference between an LCC and a VSC is that in a VSC connection the DC polarity always remains the same, irrespective of power transmission direction whilst an LCC scheme reverses the 6 polarity of the DC voltage to reverse power transmission direction. Any DC-DC converter which interconnects these two systems must, therefore, be able to exchange power between the two DC systems whilst simultaneously maintaining the DC voltage polarity on one side of the converter and allowing the voltage on the other DC terminal to reverse. Such a converter is shown in Figure 5. In Figure 5 the VSC side of the DC-DC converter consists of a three phase converter with each valve in the converter comprising a Full-bridge converter rated at Vd2 voltage in series with a Director switch rated at Vd2. As the Director switches are unidirectional this converter can only withstand one DC voltage polarity. On the LCC connected side of the DC-DC converter each converter valve is composed entirely of Full-bridge sub-modules. As the full bridge sub-module can connect the submodule capacitor in either polarity energy can be transferred from the LCC DC system to the AC connection within the DC-DC converter irrespective of the polarity of the DC. Figure 5 shows the AC connection within the DC-DC converter as a 3-phase connection but, as with the previous cases considered, a multi-phase AC connection can be used for high power connections whilst a single-phase converter can be used for medium power transmission levels. Also, the AC connection may be at a higher frequency than 50/60 Hz and non-sinusoidal. Considering a 500Hz connection the losses and cost would be comparable to a fundamental frequency back-to-back converter connection of the same power rating but the footprint (and hence offshore platform requirements) would be reduced, reducing the overall cost of the scheme. 7. DC CONNECTION OF OFFSHORE WINDFARMS There are many applications being discussed for DC interconnections associated with offshore DC windfarms. The majority of applications presently under review consist of a point-to-point DC connection from onshore to an offshore platform and then to an offshore AC collector grid which connects the individual wind turbines through a distribution system. The wind turbines themselves, based on present technology, will probably consist of an AC generator connected to an AC-DC-AC converter within the wind turbine nacelle. Hence, the conversion process from generation to load is AC-DC-AC-DC-AC. The offshore AC distribution grid which is the middle ‘AC’ within this conversion chain actually consists of many medium voltage three-phase AC cables interconnecting windfarm clusters. Because of the high capacitance within the cables, line-end reactors are normally included on the offshore platforms in order to improve the voltage profile under light load conditions. These line-end reactors take up space on the platform as do the three-phases of equipment associated with each connection. More importantly, each of the DC-AC converters will, to some extent, introduce AC harmonics into the AC systems. With different converters (those associated with wind turbines and those associated with the power transmission) the harmonic profile can be quite complex. Taking this into account along with the large amount of capacitance and inductance in the offshore AC grid and a corresponding lack of damping because of the absence of any significant loads offshore leads to a situation where the offshore AC system is likely to suffer from resonance-associated problems and the risk of overvoltage and consequential tripping. An alternative, which attempts to overcome the difficulty associated with the offshore AC grid is to only utilise DC offshore. Figure 6 shows an example of a possible future windfarm DC connection that does not need an offshore AC grid and thereby eliminates the problems associated with such a system. In Figure 6 the wind turbine generators generate DC at their terminals. These wind turbines are collected into small ‘clusters’ and these clusters are connected to the medium voltage terminals of a DC-DC converter. In order to minimise capital cost and to minimise footprint on an offshore platform, the medium voltage converter consists of a full-bridge phase arm and a capacitor phase arm. Where the medium voltage power is high, exceeding the current rating of the VSC sub-modules it is possible to parallel up the full-bridge arm. This converter is connected to a single-phase step-up transformer to a single-phase thyristor bridge. Thyristors were selected for this stage as they have a significantly higher power density compared to present day VSC technology and the technology is well proven. Whilst on the medium-voltage side the converters can be connected in parallel the higher voltage thyristor converters are series connected. In this way a group of wind farm clusters can be arranged in order to 7 give a high voltage DC connection without any individual DC-DC converter having to produce a very large voltage ratio. Individual series connected thyristor bridges in Figure 6 can be taken out of service by bypassing the converter, thereby reducing the overall DC operating voltage of the interconnection. As the onshore converter is constructed from full-bridge VSC sub-modules the converter can continue to operate with a reduced DC voltage compared to the peak converter AC voltage. The method of bypassing and reconnected series connected thyristor bridges is a well known technique going back to the early mercury-arc converters [6], hence, an out of service thyristor converter can readily be brought back into service following an outage. The land based converter is able to operate with bypassed thyristor bridges and hence lower DC voltages, as it is a full-bridge converter which is able to operate at lower DC voltages. A difficulty when designing DC offshore windfarm connections is that when the wind isn’t blowing it is necessary to supply the auxiliary loads associated with the wind turbines from the onshore AC system. Typically the load of the wind turbine, which is mostly composed of protection and auxiliary loads, is only a small percentage of the power that the wind turbine is designed to generate. The required power flow is therefore asymmetric. It may be possible to supply this auxiliary load from a separate supply, possibly AC, run in parallel with the high power DC connection. Alternatively, in the arrangement shown in Figure 6 it would be possible to supply a small windfarm load associated with one or more windfarm clusters by reversing the power flow through the DC-DC converters, operating the thyristor bridges as inverters. As losses will be of less significance in this operating mode and considering that the actual power being supplied onshore to offshore is relatively small the thyristor bridge can be operated with a relatively high extinction angle in order to mitigate the risk of commutation failures. AC System The overall losses of a scheme such as that shown in Figure 6 compared to an offshore AC grid with a single point-to-point VSC HVDC connection are expected to reduce by in excess of 10%. However, the greater benefit may come from an improved stability of the offshore grid. Figure 6: An Offshore Windfarm DC Grid with Integrated DC-DC Converters 8 8. REMOTE LOAD INTERCONNECTION VIA MULTI-TERMINAL HVDC There are certain locations in the world where the communities are widely dispersed and each community may only contain a relatively small number of people. From an electrical perspective this means long distance transmission of relatively low power, from a few kW to a few MW. Such power levels are difficult to transmit efficiently over long distances using AC because of the regulation effects on the transmission line. Local generation can, and frequently is, used for such small communities but the cost of the fuel can be very high when both the cost of the fuel and the cost of fuel transport are considered. However, it may be possible to cost effectively transmit this power using DC. Consider a scenario where there are ten communities spread along a several hundred mile corridor. Each communities load may vary from, say, nothing to 2 MW, hence the total power to be transmitted varies from 0 MW to 20 MW. Because of the long distances over which the power is to be transmitted the DC current needs to be kept as low as possible. By using a reasonably high DC voltage the DC current can be kept low, so if we assumed a DC voltage at the sending converter of -100 kVdc the maximum load current would be 200 Adc. The DC transmission could be done as a two wire transmission circuit, with one wire at -100 kVdc and one at nominally 0 kVdc. Alternatively, the connection could be made with a single wire at -100 kVdc and using the earth as a return path. The cost inhibitor for such a long distance, medium power HVDC scheme has, to date, been the cost of each of the receiving converters, as each one, in the scenario outlined above, must be rated for -100 kVdc but only 20 Adc. However, with imaginative use of the now established VSC building blocks, alternative converter arrangements can be envisaged which can overcome the high capital cost obstacle. The power transmitted is ‘Low’ hence, as discussed in 2 above the capitalised cost of losses can be neglected. Figure 7 gives a proposal for a local community DC-DC converter. The idea of using a DC-DC converter is two fold. Firstly, the -100 kVdc stress is taken, in this circuit, by a single converter arm, reducing the DC voltage to a lower level where a DC-AC converter can be connected to supply the local community. Studies have shown that typically the total number of power transistors and capacitors reduce to less than 30% of a full voltage 3-phase DC-AC converter. Figure 7: A Low Power, High Ratio DC-DC Converter The converter shown in Figure 7 is known as a “Cascade Converter”. Each of the resonant circuit blocks are tuned to the same frequency. At each half cycle of this resonant frequency charge is transferred down the stack, from one resonant circuit to the next until, at the bottom 9 stage of the converter where energy can be extracted. The operation is similar to that of the Cockcroft-Walton generator [7], except that, in this instance power flow is generally from highvoltage to low-voltage. 9. CONCLUSION The paper has introduced a number of potential future developments and applications of power electronics to both realise future DC Grids and to facilitate better power transmission. BIBLIOGRAPHY [1] [2] [3] [4] [5] [6] [7] N. Mohan, T.M. Underland, W.P. Robbins, “Power Electronics: Converters, Applications and Design”, John Wiley & Sons, 1989, p81 http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=151-12-26 A.C. Franklin, D.P. Franklin, “J&P Transformer Book, 11th Edition”, Butterworths, 1983, p162. D.R.Trainer, C.C.Davidson, C.D.M.Oates, N.M.MacLeod, R.W.Crookes, D.R.Critchley, “A New Hybrid Voltage-Sourced Converter for HVDC”, CIGRÉ session 2010, paper B4-111. M.M.C.Merlin., T.C.Green., P.D.Mitcheson, D.R. Trainer, D.R.Critchley, R.W.Crookes, “A New hybrid Multi-Level Voltage-Source Converter with DC Fault Blocking Capability”, IET 9th International Conference on AC and DC Power Transmission, London, October 2010. T.C.J. Cogle, “The Nelson River Project”, Electrical Review, 23 November 1973. http://en.wikipedia.org/wiki/Cockcroft_Walton 10