Wind Power Harmonic Emission versus Active-Power Production
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1 NORDAC 2014 Topic and no NORDAC 2014 http :// 5.2 Wind Power Harmonic Emission versus Active-Power Production Kai Yang, Math Bollen and Mats Wahlberg Electric Power Engineering Group, Luleå University of Technology SUMMARY Modern wind turbines are commonly equipped with power electronics. The application of either a partial scale frequency converter or a full scale power converter will result in harmonic emission which is distinct from conventional harmonic sources: even harmonics and interharmonics appear with similar magnitudes as odd harmonics. Harmonic and interharmonic measurements on a few individual wind turbines at the medium voltage side of the turbine transformers have been performed with standard Dranetz monitors. Measurements have been performed during a few weeks, with recording the aggregated harmonic and interharmonic subgroups over every 10-minute interval. The measurements involve a full range of active-power production through the individual wind turbines. This work will study the harmonic and interharmonic subgroups as a function of the active-power production for different wind turbines. Spectrograms (up to order 40) against the sorted active-power production present various trends of emission with the increasing power production. THDs and TIDs have been shown with the two characteristics: THDs without apparent trend, whereas TIDs with an increasing trend as a function of active-power. Despite various patterns of individual subgroups as a function of active-power, characterizations of a few subgroup types have been observed: characteristic harmonics vary little with the active power; whereas interharmonics with a strong relation with the active-power production. Keywords: Wind Farms, Power Distribution, Wind Power Generation, Power Quality, Electromagnetic Compatibility, Power System Harmonics, Harmonic Distortion. I. Introduction Modern wind turbines are often equipped with power-electronic converters, either as a fullpower converter or as part of a double-fed induction generator. The double-fed induction wind generators equipped with reduced-capacity power converters are defined as Type-III, and wind generators with full-capacity power converters are as Type-IV [1]. The trend of increasing use of sustainable energy relies much on the conversion technology of power-electronics due to the intermittent supply of energy, e.g. the varying wind condition and the changing solar irradiation. The application of power-electronics thus introduces various advantages, for example energy efficiency and flexibility in the power conversion. However the presence of these power-electronic converters explains the interest in the harmonic emission from individual wind turbines and from wind parks [1][3], by introducing waveform distortions simultaneously.
2 There are various power-conversion-system schemes for the wind energy extraction [4][5][6]. The output waveforms are controlled with certain switching schemes to adapt the grid side. Anyhow the harmonic filters are used to smooth the waveform distortions [6][7]. Besides the harmonic measurement requirements stimulated in IEC [8] and IEC [9], IEC [10] recommends measurement and assessment of power quality characteristic of grid-connected wind turbines. IEC recommends that values of the individual current components (harmonics, interharmonics and higher frequency components) and total harmonic current distortion are measured within the active power bins 0, 10%, 20%, 100% of wind turbine rated power. The highest value for each power bin is reported. From a standardization viewpoint there are reasons for selecting one single value, the maximum value in this case. However, to quantify the turbine emission, this is only of use when there are limited variations of the emission within one power bin. Paper [11], which based on IEC , studies current total harmonic distortion that is independent on the output power for certain harmonics orders on five wind turbines. The fifth harmonic has been shown to be independent for all the five wind turbines. However other harmonics and interharmonics have not been included in that study. Paper [12] has tested a number of 600 kw squirrel-cage induction generator wind turbines on MV level. It presents a decreasing current THD (in percent of fundamental current) with output power. The harmonic orders 3, 5 and 7 are found without obvious trend with the output power. The study in this paper aims at verifying the previous studies on the waveform distortions that are impacted by the output power; and the study has been extended to perform the relationship of output power and the other harmonics and interharmonics, for both Type-III and Type-IV wind turbines. Section II introduces the details of measurement method and the harmonic assessment method that has been used in the analysis. Section III presents the harmonic measurement in relation with the output power. The conclusion of the work is presented in Section IV. II. Measurement Set-up Harmonic measurements were performed with three individual modern wind turbines, involving both Type-III and Type-IV. The turbines are with rated power of 2 MW to 2.5 MW. The wind turbine generators outputs a voltage 660/690 V, which is transformed with a step-up wind turbine transformer to the MV level. The measurement details are listed in Table 1. The standard power-quality monitor Dranetz Power Xplorer PX5 was used together with the conventional voltage and current transformers at the measurement points. The instrument transformers are of sufficient accuracy for harmonic measurements up to a few khz, the harmonic measurement accuracy has been tested in [13] and specified in [2][14].
3 Table 1. Measured objectives details, at the measured points. Turbine No. Generator Type Measurement WT Point Measurement Type Duration Current Voltage Turbine I Asynchronous doublefed Type-III 66 A 22 kv 11 days Turbine II Asynchronous doublefed Type-III 36 A 32 kv 8 days Turbine III SYNC-RT Type-IV 116 A 10 kv 13 days The voltage and current waveforms are continuously acquired on the three phases through PX5 with a sampling frequency of 256 times the power-system frequency (approximately 12.8 khz). The harmonic subgroups are obtained according to IEC every 10 minutes. Next to that a 200-ms waveform of the current was obtained for each of the three phases once every 10 minutes. The total measurement period lasts up to a few weeks at each location. III. Measurement Results A. Evaluation of (inter)harmonic level The spectrum of each 200-ms current waveform from the measurements shows that, frequency components of the spectra vary a lot during the few weeks. The difference between harmonics and interharmonics, between even harmonics and odd harmonics, are not as much pronounced as the conventional generators in one spectrum. The observation of various spectra presents a larger variation of interharmonics than harmonics, especially for certain interharmonic frequencies. Figure 1. The average spectra (5 Hz increment) of the three wind turbines during few weeks. The evaluation of harmonic level has employed average spectrum, to smooth the large variations of (inter)harmonic components. The method quantifies the varying harmonics during a longer time which involves full range of wind power operation states. The results of the three wind turbines have been shown in Figure 1.
4 The emissions of the three wind turbines are different, which are characterized by the average spectra as shown in the figure. The difference is made from the three turbines located in different wind park; and it makes difference from the two Type-III wind turbines (upper and middle sub-figures). The three turbines present a spectrum that is a combination of a broadband spectrum and a number of narrow bands. The narrow bands are mainly low-order integer harmonics up to 1 khz, associated with obvious low-order characteristic harmonics. Turbine I (upper sub-figure) presents a narrow band component centered at 650 Hz and a broadband component covering neighboring frequencies. Except the narrowband emission at integer harmonics (e.g. 150 Hz, 200 Hz), Turbine II (middle sub-figure)) emits obvious narrowband components at 285 Hz and 385 Hz, and a broadband spectrum up to about 400 Hz and between 2000 and 2700 Hz. The spectrum of Turbine III (bottom sub-figure) presents two broadband components around 280 Hz and 380 Hz, next to the narrowband components at harmonics 5 and 7. B. Emission versus active power A study on the emission as a function of active-power is presented. The harmonic and interharmonic subgroups of the three wind turbines, obtained from the 200-ms windows, are shown in Figure 2 as a function of the produced power. The upper figure presents the current emission (in ampere) in logarithm (base 10) with colour. Figure 2. Harmonic (H 2 - H41) and interharmonic (IH IH 41.5) subgroups as a function of active power. Turbine I: Upper left sub-figure; Turbine II: upper right sub-figure; Turbine III: bottom sub-figure. The color scale indicates the magnitude of the harmonic and interharmonic subgroups with red the highest and dark blue the lowest magnitude. The horizontal axis has been obtained by sorting the spectra by the active power, with highest production towards the right. The sorted
5 production values are shown in the bottom curve. Note that the active-power scale is not linear. For Turbine I, characteristic harmonics (H 5 and H 13) remain apparent over the whole range of active-power production. The low-order harmonics, obviously for harmonic 5, become stronger with the increasing production. The interesting observation is that, the emission around harmonic 13 gets stronger at the higher power production; and that the strongest emission shifts to a higher order. The obvious changes occur above 0.5 per-unit active-power production (or around data order 850). Another significant observation is that, around 0.26 per unit active-power the emission shows a minimum. For Turbine II, lower-order (below harmonic 10) harmonics increase in magnitude and the maximum emission shifts to higher orders (interharmonics) from around 0.25 per-unit activepower production. The emission from harmonic order 10 to 30 remains present until around 0.5 pu power production. Above around 0.7 pu power, blue colored regions between harmonic orders H15 - H25 and H30 - H40 present low emission. Another observation is that emission at harmonic orders above H35 increases at 0.2 to 0.4 pu power production. The Type-IV turbine (bottom sub-figure) shows another emission pattern, as shown in Figure 7. The main similarity with the previous two turbines is that, low order harmonics, especially interharmonics (e.g. interharmonic 5.5 and 7.5) next to 12 the characteristic harmonics (e.g. harmonic 5 and 7), increase with an increasing power production. The broadband emission from H35 to H40 is stronger around rated production. The emission of these orders is relatively low from 0.2 to 0.5 pu active power. C. THD and TID as a function of active power The total interharmonic distortion (TID) and Total Harmonic Distortion (THD) of the three turbines, as a function of active power production, are presented as in Figure 3. The horizontal axis represents the active power in per-unit. Figure 3. Total Harmonic Distortions (THD, left figure) and Total Interharmonic Distortion (TID, right figure) as a function of active power. The three wind turbines show a different relation between emission and the active power production. Turbine I shows an increase, turbine II a mild decrease and Turbine III remains about the same. Each turbine is different; there is no clear trend for the relation between THD (in ampere) and active-power production.
6 However all three turbines show a clear increase of TID with active power production. The three trends are a combination of almost linear line with fluctuations at certain active power ranges. D. Individual Subgroups of Turbines I and Turbine III The individual subgroups (H: harmonics; IH: interharmonics) as a function of active power production are presented for one Type-III and one Type-IV wind turbine in Figure 4. Figure 4. Individual Subgroups as A Function of Active PowerIndividual Harmonic (H) and interharmonic (IH) subgroups as a function of active power in phase-a. Turbine I: left figure; Turbine III: right figure. For Turbine I the harmonic and interharmonic orders 3, 7, 12, 16 and 19 are presented. The emission at each active power production shows less spread for interharmonic subgroups than for harmonic subgroups. Harmonic subgroup 7, which is similar to orders 5 and 11, shows a large spread for a given active power production. The curve does not show a strong relation between the emission and the active power. The results for Turbine III are presented with specified orders 3, 4, 6, 7 and 22. Same as the other two turbines, the low order harmonic subgroups (example as harmonic 3 and 4 presented in the figure) spread in a larger range if compare to the higher orders from the same turbine. Individual subgroups of the two turbines present different patterns. Some general patterns can however be observed: the emission for characteristic harmonics is independent on active power; interharmonics (especially neighbouring interharmonics of characteristic harmonic orders) are more dependent on the active power. The spread from the average trend is large for harmonics but small for interharmonics. IV. Conclusion Measurements have been performed of the harmonic emission at three individual wind turbines. The current spectra show a combination of narrowband and broadband components.
7 Narrowband components appear especially with characteristic harmonics and mainly for loworder harmonics. The measurements show that the emissions from the turbines are small but that the emissions contain a higher level of interharmonics than that is normal with harmonicemission loads. The measurements showed different relations between THD and active-power production for different turbines. The variation of THD with active power is relatively small. The relation between total interharmonic distortion (TID) and active-power production is similar for the three turbines; an increase in TID with increasing active-power production. Individual harmonic and interharmonic subgroups show different relations between emission and active-power production. Characteristic harmonics are shown to be independent on the active-power. They show large variations even for small variations in active-power. However the neighboring interharmonics present a strong dependency on the active power. A general observation is that the dominant interharmonics increase with active power production, whereas the dominant harmonics remain more constant. V. Acknowledgement The authors would like to thank the financial support from the Vindforsk program and Skellefteå Kraft Elnät AB, throughout the project. Thanks also to the colleagues in the Electric Power Engineering group at Luleå University of Technology for the helpful discussions and ideas! VI. References [1] T. Ackermann, Wind Power in Power systems, Wiley [2] J. Arrillaga, N.R.Watson, Power system harmonics, 2nd Ed., Wiley, [3] M.H.J. Bollen, Irene Y.H. Gu, Signal Processing of Power Quality Disturbances, Wiley Section 2.5. [4] S. Heier, Grid Integration of Wind Energy Conversion Systems, 2nd edition, JohnWiley & Sons, Ltd., Chichester, England, [5] B. Wu, High-Power Converters and AC Drives, 1st edition, Wiley-IEEE Press,Piscataway, NJ, [6] B. Wu, Y. Lang, N. Zargari, S. Kouro, Power Conversion and Control of Wind Energy Systems, IEEE Power Engineering Series, Wiley, Hoboken, NJ, [7] R. Teodorescu, M. Liserre, P. Rodriguez, Grid Converters for Photovoltaic and Wind Power Systems, 1st edition, John Wiley & Sons, Ltd., New York, [8] CENELEC, IEC , Electromagnetic compatibility (EMC) Part 4 7:Testing and measurement techniques general guide on harmonics and inter-harmonics measurements and instrumentation, for power supply systems and equipment connected thereto, IEC , 2002.
8 [9] CENELEC, IEC , Electromagnetic compatibility (EMC) - Part 4-30: Testing and measurement techniques - Power quality measurement methods, IEC , [10] IEC : Wind-turbine Generator Systems, Part 21: Measurements and assessment of power quality characteristics of grid connected wind turbines. [11] S.T. Tentzerakis, S.A. Papathanassiou, An investigation of the harmonic emissions of wind turbines, IEEE Transactions on Energy Conversion 22 (1) (2007) [12] L. Sainz, J. Mesas, R. Teodorescu, P. Rodriguez, Deterministic and stochasticstudy of wind farm harmonic currents, IEEE Transactions on Energy Conversion25 (4) (2010) [13] D. Douglass, Current transformer accuracy with asymmetric and high frequency fault currents, IEEE Transactions on Power Apparatus and Systems, vol. PAS-100, no. 3, pp , March [14] J. Arrillaga, N.R. Watson, S. Chen, Power system quality assessment, Wiley Section 5.2. VII. Biographies Kai Yang received his M.Sc. degree from Blekinge Institute of Technology, Sweden in 2009 and the Licentiate degree from Luleå University of Technology, Sweden in Now he is a PhD student in the Electric Power Engineering Group at Luleå University of Technology, Skellefteå, Sweden. The main research interest is in the field of wind power quality, harmonics and distortion. Math H.J. Bollen (M 93-SM 96-F 05) received the M.Sc. and Ph.D. degrees from Eindhoven University of Technology, Eindhoven, The Netherlands, in 1985 and 1989, respectively. Currently, he is professor in electric power engineering at Luleå University of Technology, Skellefteå, Sweden and R&D Manager Electric Power Systems at STRI AB, Gothenburg, Sweden. He has among others been a lecturer at the University of Manchester Institute of Science and Technology (UMIST), Manchester, U.K., professor in electric power systems at Chalmers University of Technology, Gothenburg, Sweden, and technical expert at the Energy Markets Inspectorate, Eskilstuna, Sweden. He has published a few hundred papers including a number of fundamental papers on voltage dip analysis, two textbooks on power quality, understanding power quality problems and signal processing of power quality disturbances, and two textbooks on the future power system: integration of distributed generation in the power system and the smart grid - adapting the power system to new challenges. Mats Wahlberg is currently working at Skellefteå Kraft Elnät, Skellefteå, Sweden as research engineer. He has been with the company for about 30 years. He has a long experience obtained from involvement in a wide range of tasks. Some examples are calculations of constructions, losses and protection relays. In the last 15 years the main focus of his work has been with power quality issues and different kinds of communications. He is also a member of working group CIGRE C4:33 and CEATI Lightning & Grounding. He is also senior research engineer at Luleå University of Technology, Skellefteå, Sweden.
This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and
This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and education use, including for instruction at the authors institution
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