RESULTS OF ON-GRID OPERATION OF SUPERCONDUCTOR DYNAMIC SYNCHRONOUS CONDENSER

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1 RESULTS OF ON-GRID OPERATION OF SUPERCONDUCTOR DYNAMIC SYNCHRONOUS CONDENSER Dr. Swarn S. Kalsi, David Madura, and Michael Ross American Superconductor Corporation (USA) Abstract: A high-temperature superconductor (HTS) dynamic synchronous condenser, called SuperVAR has been developed for providing peak and dynamic reactive compensation (leading/lagging) to a power system. It has a small footprint, is readily transportable, and is a viable economic option. This system is also inherently stable to close-in faults and can provide up to twice the nominal rating for about one minute (peak rating) during depressed voltage events. The machine also uses less than half of the energy of a conventional synchronous condenser because the HTS field winding has minimal losses. With its HTS field coils operating at a constant cryogenic temperature, this machine is highly reliable. In October 2004, the first HTS synchronous condenser prototype (8 MVAR, 13.8 kv) was installed on the Tennessee Valley Authority (TVA) grid serving an arc furnace, where it is being exposed to a large number of transients that provide an excellent accelerated age test of the device. TVA will release to manufacture five production units previously ordered (each rated 12 MVAR), contingent on acceptance of the prototype. With this commercial order, the HTS condenser will be the first commercialized HTS application for enhancing power system reliability on the electric power grid. This paper discusses the SuperVAR system s key design features, its performance since January 2005, and its application benefits to a wind farm. Keywords: Capacitors, Dynamic Synchronous Condenser, FACTS (flexible AC Transmission System), LVRT (Low Voltage Ride Through), Reactive Power, Reactors (Inductors), STATCOM (Static Shunt Compensator), SuperVAR (Superconducting Dynamic Synchronous Condenser), SVC (Static VAR Compensator) and VAR (volt-ampere-reactive) I. INTRODUCTION The relative low efficiency and the high maintenance cost of conventional synchronous condensers (employing normal copper field winding) have made these devices fall out of favor for the generation of reactive power in electric power grids. They have been replaced by electronic solutions such as static VAR compensators (SVCs), and flexible AC transmission system (FACTS) devices. These reactive compensation devices are suitable for voltage regulation during steady state operation, but during a voltage collapse situation their output is strongly dependent on the system voltage. This operational characteristic makes such devices less effective at the point in time when their functionality is most needed to boost voltage. A new superconducting synchronous condenser has been introduced that uses standard synchronous condenser frames and stator coils mated with new, power-dense rotor coils made from high-temperature superconductor (HTS) wires. This new condenser is more efficient than conventional machines without the typically high rotor maintenance costs and it produces many times more reactive power than a similarly sized commercial machine. The HTS dynamic synchronous condenser machine eliminates many problems associated with conventional condensers and FACTS electronic devices. The HTS dynamic synchronous condenser employs an HTS field winding that always operates at a constant cryogenic temperature and field current excursions are quite small between no-load and full-load conditions. This inherent feature of the dynamic synchronous condenser machine significantly reduces the need for major rewind as compared to a conventional synchronous condenser, which experiences significant thermal cycling within the rotor. Heavy filters are normally used to attenuate undesirable harmonics produced by many FACTS devices. Since the dynamic synchronous condenser

2 machine produces essentially no harmonics, large filtering equipment is avoided. The HTS dynamic synchronous condenser current output is independent of system voltage but at the same time the output current can be increased several times its continuous rating using a fast exciter [1]-[4]. This over-load current can be maintained for a significant time duration constrained by the stator s I 2 t limit of 60 seconds. II. HTS DYNAMIC SYNCHRONOUS CONDENSER FEATURES While conventional synchronous condensers have been widely used in the power grid, their relatively low efficiency has limited their applications, and their useful lifetime has been limited by field winding insulation degradation caused by field current heating during cyclic operation [5]. The V-curves for typical superconductor and conventional machines are compared in Figure 1. 1 VARS (PU) Absorbing VARS Generating VARS SuperVAR Machine 1 2 3 Field Current (Per Unit) Conventional Synchronous Machine Figure 1: V-curves for Conventional Synchronous and HTS Synchronous Condenser Machines In this example, the field current in a conventional machine must be increased by the factor three from no-load to full-load, which increases the field winding s resistive losses by the factor nine, causing heating of the field coils. Because of temperature rise, the field winding coils expand and contract as the load is varied. This expansion in turn causes fatigue of the insulation that can lead to premature failure of the field winding. Furthermore, under certain circumstances this mechanism can result in thermally sensitive rotors, especially for large synchronous generators. An unbalanced expansion or contraction of the field coils can cause unacceptable vibration excursions, which may seriously limit the operating capabilities of the machine. In contrast, for superconductor synchronous machines, the field current change between no-load and full-load conditions is quite small. Since the resistive losses are negligible under normal operating conditions and the superconductor field winding always operates at a nearly constant cryogenic temperature no expansion or contraction of the winding occurs under normal operation. Consequently, there are no undue thermal stresses on the superconductor field winding, which in turn leads to a longer life. Because the superconductor wire has dramatically reduced losses, the HTS dynamic synchronous condenser is 98.8% efficient, typically 1% more efficient than copper-based conventional units this about double the efficiency of a conventional condenser. The HTS dynamic synchronous condenser machine retains its high efficiency down to partial loads of 25%, whereas the efficiency of conventional machines drops more rapidly due to its field winding losses, which are caused by the high field current. The efficiency of HTS synchronous condensers is comparable to that of SVC and FACTS devices. Thus, the net impact of HTS dynamic synchronous condensers on system losses and operating costs is very favorable. Because of its compact size and low-cost design, the new HTS dynamic synchronous condenser will also be a very economic option for providing peak and dynamic reactive compensation to a power system. It has a small footprint and is readily transportable for easy placement in distribution substations. It has been shown to be inherently stable to transient faults, and can provide up to twice its nominal current for about one minute (peak rating) during depressed voltage events. To demonstrate these features of the HTS dynamic synchronous condenser, the first prototype unit has been put into operation in the TVA grid near an arc furnace [6]. At this site, the testing is intended to show not only that the HTS dynamic synchronous condenser machine is a new, preferred option for handling arc furnace flicker, but that it can also handle hundreds of thousands of transients in less than a year. The as-delivered ± 8 MVAR HTS dynamic synchronous condenser machine (trailerized), with key components highlighted, is shown in Figure 2. The specifications for the prototype and planned production versions of the HTS dynamic synchronous condenser machine are provided in Table I. This HTS dynamic synchronous condenser machine can be built for any voltage between 4.16 kv and 20 kv. Total losses (including refrigeration system) are ~1.2% of the rating. These losses are in the same range as losses in an electronics FACTS device.

3 480V to 120V Communication Commands, Data and Excitation and Control Start-up Synchronous Motor Condenser Cryocoolers Cryocooler Compressors Figure 2: +/- 8 MVAR HTS Synchronous Condenser Machine from American Superconductor Rating Voltage Table I: HTS Synchronous Condenser Specifications Parameter Specification Ambient Temperature Losses ± 8 MVAR (prototype unit) ± 12 MVAR (production unit) 4.16 to 20 kv line to line -30 o to +40 o C 1.2% rating at 8 MVA, including 30 kw 480 V auxiliary power The HTS dynamic synchronous condenser support system consisting of the following subsystems: HTS rotor Stator lubrication and cooling system Refrigeration Exciter, control and communication system Auxiliary power system Startup motor and controller A conceptual diagram of the subsystems is shown in Figure 3. TVA will release to manufacture five production units previously ordered (each rated 12 MVAR), contingent on the acceptance of the 8MVAR prototype. With this initial commercial order, the HTS dynamic synchronous condenser will be the first commercialized HTS application for the electric power grid. 480V, 3Phase Auxiliary Power Motor Controller Start-up Motor Water Stator Lube Water Helium Cooling Chiller Skid Compressors Air Fan Air Oil Stator Neon Helium and Exciter HTS Rotor Refrigerator Module Figure 3: HTS Synchronous Condenser Support Systems The open-circuit and short-circuit test measurements are shown in Figure 4. The machine does not exhibit any saturation effect over the operating range (1.3 pu voltage). Parameters measured from these tests are summarized in Table II. These parameters can be utilized for simulation of this machine with commercial codes such as PSS/E, EMTP and PSCAD. PU Terminal Voltage and Stator Current 1.400 1.200 1.000 0.800 0.600 0.400 0.200 O/C Voltage S/C Current 0.000 0 50 100 150 200 Field Current (A) Figure 4: Open-Circuit and Short-circuit (Steady-state) Measurements on the HTS Dynamic Synchronous Condenser III. TEST RESULTS ON GRID After factory testing, the machine was installed at an electric arc furnace and began grid operation on October 10, 2004. It was put into regular operation in early January 2005. Since then the machine has been operating to help reduce flicker caused by the arc furnace. MVARs supplied by the machine during a typical melt cycle are shown in Figure 5. The figure shows MVAR contributions at onesecond intervals, though the peak instantaneous contribution could be significantly higher. The machine has been absorbing transient disturbances with very high negative (>30%) and zero sequence (>15%) current components as shown in Figure. 6 and Figure 7. The rotor with a continuous damper winding, in the form of a copper shell, absorbs

4 heating created by negative and zero sequence currents very effectively with an insignificant temperature rise in cryogenic components. The stator winding has also withstood these currents while staying within the peak allowable temperature. In summary, testing so far has been successful. Table II: Measured Parameters for the 8 MVAR HTS Dynamic Synchronous Condenser Parameters Measure Synchronous reactance (x d ), pu 0.36 Transient reactance (x d ), pu 0.21 Sub-transient reactance (x d ), pu 0.13 Sub-transient reactance (x q ), pu 0.13 Armature short-circuit time constant (τ sc ), s 0.05 D-axis Transient O/C time constant (τ do ), s 860 D-axis Sub-transient O/C time constant (τ do ), s 0.02 Q-axis Sub-transient O/C time constant (τ qo ), s 0.04 Armature resistance (r a ), pu 0.007 Inertia constant, s 1.4 regulation and low voltage ride through (LVRT) capabilities unless additional equipment was installed to mitigate this situation. Approximately 40 MVAR of additional capacitive reactive support was required in order to meet the voltage regulation and power factor requirements. Simulations also showed that the wind farm would not survive a number of three-phase and single-line to ground transmission faults without tripping at least a portion of the wind turbines. Negative Sequence Current (pu) 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 0 500 1000 1500 2000 2500 3000-0.1 Time (sec) Figure 6: Negative Sequence Currents Experienced by HTS Dynamic Synchronous Condenser During an Arc Furnace Burn Cycle 0.3 MVARS 6.0 5.0 4.0 3.0 2.0 1.0 0.0 MVAR 0 500 1000 1500 2000 2500 3000-1.0 Time (sec) Figure 5: MVARs Supplied by HTS Synchronous Condenser During an Arc Furnace Burn Cycle IV. WIND FARM APPLICATION (SIMULATION) Simulations with PSS/E code show that an HTS dynamic synchronous condenser can provide benefit to an existing 78 MW Midwestern (U.S.) wind farm, as shown in Figure 8. Previous studies have shown that this wind farm would have inadequate voltage Zero Sequence Current (pu) 0.2 0.2 0.1 0.1 0.0 0 500 1000 1500 2000 2500 3000-0.1 Time (sec) Figure 7: Zero Sequence Currents Experienced by HTS Dynamic Synchronous Condenser During an Arc Furnace Burn Cycle A simulation study was conducted by the American Superconductor transmission planning team. In order to improve the LVRT capability of the wind farm, the study assumed two 12 MVA HTS dynamic synchronous condenser units in the simulation. The HTS dynamic synchronous condenser units, rated at 13.8 kv, were connected to the 34.5 kv main collector bus (see Figure 9) of the wind farm through two 12 MVA transformers. With the HTS dynamic synchronous condenser units installed, the LVRT capability of the solution was significantly improved. A comparison, with and without

5 the HTS dynamic synchronous condenser machine installation, of the wind farm voltage and real power output in response to a low voltage fault described in the interconnection agreement is shown in Figure 10. 1.00 p.u. 0.90 p.u. 0.80 p.u. With SuperVAR Without SuperVAR Utility Interconnection Point T1 80 MVA 138 kv 34.5 kv 34.5 kv Collector System 0.70 p.u. 80 MW 60 MW 34.5 kv Bus Voltage Wind Farm MW Output With SuperVAR 40 MW Without SuperVAR (Wind Turbines Trip Due to Low Voltage) Figure 8: 78 MW Existing Wind Farm, No Compensation Equipment Without the HTS dynamic synchronous condenser units installed, the fault event causes all the turbines in the wind farm to trip on low voltage, as is demonstrated in Figure 10. With the HTS dynamic synchronous condenser solution installed, the 34.5 kv bus voltage is kept high enough so that no turbines trip and the wind farm successfully rides through the event. Thus, the LVRT issue can be solved by the two HTS dynamic synchronous condenser units. Utility Interconnection Point T1 80 MVA 138 kv 34.5 kv 12 MVA SuperVAR TM 12 MVA SuperVAR TM 12 MVA 34.5 13.8 kv Substation Transformers 1200 Amp Breaker 34.5 kv Collector System Figure 9: Wind Farm with Two HTS Dynamic Synchronous Condenser Units Installed to Improve LVRT 20 MW Figure 10: Wind Farm Bus Voltage and MW Output with and without SuperVAR Dynamic Synchronous Condenser V. CONCLUSIONS A SuperVAR dynamic synchronous condenser machine was installed on the grid in October 2004 and gradually brought to regular operation in early January 2005. The machine is improving power factor and reducing flicker caused by the arc furnace. The HTS dynamic synchronous condenser can solve a variety of utility problems without the operational and performance limitations of conventional machines and electronic FACTS devices. Simulation studies have shown that HTS dynamic synchronous condenser machines installed at the collector bus of a wind farm system will mitigate voltage regulations and LVRT problems. With a combination of steady voltage regulating output and fast reacting transient capability, the HTS dynamic synchronous condenser can address a number of additional problems associated with integration of wind farms with the grid. This machine will provide outstanding value to transmission system operators beginning in 2006. VI. ACKNOWLEDGEMENTS The authors acknowledge support of the Tennessee Valley Authority for the development of the HTS dynamic synchronous condenser. They also acknowledge the support of the American Superconductor engineering and technical staff.

6 VII. REFERENCES [1] S. S. Kalsi, On Grid Performance of a Superconductor Dynamic Synchronous Condenser, Presented at the CIGRE 2005 Symposium on Power Systems with Dispersed Generation, Athens, Greece, 14-17 April 2005 [2] S. S. Kalsi, D. Madura and M. Ingram, Superconductor Synchronous Condenser for Reactive Power Support in an Electric Grid, Presented at the IEEE Applied Superconductivity Conference, Jacksonville, Florida, October 2004 [3] D. Bradshaw, Super Reactive Power for the Power System through SuperVAR High Temperature Superconductor Dynamic Synchronous Condensers, Presented at the IEEE Power Engineering Society Meeting, Denver, CO, June 2004 [4] S. S. Kalsi, et al, Superconducting Dynamic Synchronous Condenser For Improved Grid Voltage Support, Presented at the IEEE T&D Conference, Dallas, Texas, August 2003 [5] S. S. Kalsi, K. Weeber, H. Takesue, C. Lewis, H-W. Neumueller and R. D. Blaugher, Development Status of Rotating Machines Employing Superconducting Field Windings, Proceedings of the IEEE, No. 10, October 2004, pp. 1688-1704 [6] M. Ingram, Customer Side of the Value of SuperVAR, EPRI Power Delivery Applications for Superconductivity Task Force, Nashville, TN, August 10-11, 2004