A Study of the Normal Turbulence Model in IEC

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WIND ENGINEERING VOLUME 36, NO. 6, 212 PP 759-766 759 A Study of the Normal Turbulence Model in 614-1 Takeshi Ishihara *,1, Atsushi Yamaguchi *,2 and Muhammad Waheed Sarwar *,3 *1 Professor, Department of Civil Engineering,The University of Tokyo, 7-3-1 Hongo Bunkyo Tokyo, 113-8656 Japan Fax:+81-3-5841-1147, E-mail: ishihara@bridge.t.u-tokyo.ac.jp *2 Assistant Professor, Department of Civil Engineering,The University of Tokyo *3 Research Fellow, Department of Civil Engineering,The University of Tokyo Received August 27, 212; Revised November 26, 212; Accepted December 1, 212 ABSTRACT This study examines applicability of Normal Turbulence Model (NTM) in 614-1 for offshore conditions using wind records obtained at an offshore site. The model parameters for estimation of the standard deviation of longitudinal fluctuating velocity, σ 1, in NTM are presented. The identified model parameters for the mean value of σ 1 agree well with those of Normal Turbulence Model, but parameters for the standard deviation of σ 1 are found to be larger than those used in. As a result, the standard deviation of σ 1 obtained by Normal Turbulence Model parameters is underestimated and predicted that by the proposed model parameters shows a good agreement with the observation. Keywords: Normal Turbulence Model, Model parameters, Standard deviation of longitudinal fluctuating velocity 1. INTRODUCTION Wind turbulence significantly influences the fatigue loads acting on the wind turbines and accurate modeling of the standard deviation of fluctuating wind velocity becomes important. In general, a large change in turbulence intensity is observed with a change in wind direction and, rather small turbulence intensities are experienced offshore compared to on-land locations 1). In international standard 614-1 Ed. 3 2) (hereafter called ), Normal Turbulence Model (NTM) is presented to define turbulence under normal operation conditions. The parameters of NTM in the 614-1 were determined by few observation data. Recently, Tanigaki et al. 3) reported a discrepancy between the parameters of NTM proposed by the and those identified by using onshore wind observation data. Especially model parameters concerning the standard deviation of σ 1 (the standard deviation of the longitudinal fluctuating velocity) are significantly underestimated by the NTM of. In this study, the characteristics of the standard deviation of the offshore wind are examined by using observation data measured in Eastern seas of Japan, and the applicability of NTM of for offshore locations is investigated. Model parameters are proposed for offshore wind conditions and accuracy of the proposed NTM is verified by offshore wind observation data. 2. OBSERVATION OF OFFSHORE WIND Offshore wind speed and direction, used in this study, were measured using a propeller-vane anemometer installed at the top of a tower located on a platform for natural gas mining in Iwaki

76 A STUDY OF THE NORMAL TURBULENCE MODEL IN 614-1 gas field, 37 km offshore from the coast of Naraha-machi, Fukushima Prefecture. The platform (Lon. 141 o 27 35 E, Lat. 37 o 18 N) is surrounded by the Pacific Ocean from east to south and by Japanese island from southwest to northwest direction as shown in Figure 1. Figure 2 shows an overview of the offshore wind observation system. Wind speed and direction were measured at 95 m above sea level from the sea surface and 4 lightening rods for safety purposes were placed around the observation system. The diameter of the lightening rods was 61 mm, and the horizontal distance between the lightening rods and the anemometer was kept 3 times the diameter of the rods, i.e., 1832 mm. The effect of the lightening rods presence on wind measurements is ignored since this distance was larger than 8.2 times of the diameter as specified by 14-12-1 4). Table 1 shows the specification of the offshore observation system. A propeller-vane anemometer with optical fiber sensor was adopted, because use of explosion-proof type Iwaki platform for natural gas mining Hirono power plant Fukushima prefecture 37 km Offshore observation site Latitude 37 18' '' north Longitude 141 27' 35'' east The city of lwaki Figure 1: Offshore observation site. Measurement point (a) A drilling derrick (b) Propeller-vane anemometer Figure 2: View of offshore observation system. Table 1: Descriptions of offshore observation system Anemometer Manufacturer Ogasawara Keiki Seisakusho Co., LTD Type Propeller-vane anemometer Detection method 7-optical fibers type Wind direction 16 directions Wind speed ~6m/s Logger Manufacturer NRG System Type SYMPHONIE/2-J Sampling interval 2 seconds Observed data 1-minutes average wind speed and wind direction 1-minutes wind speed standard deviation Observation period Oct. 24~Sept. 26

WIND ENGINEERING VOLUME 36, NO. 6, 212 PP 759-766 761 equipment was obligated on the natural gas mining facilities. The measurement data was first recorded in the local data logger, and data statistics were transmitted to onshore facility everyday. In this study, the measurement was carried out for two years from October 24 to September 26. The measurement data include 1 minutes mean wind speed, wind direction and standard deviation of wind speed, and are used to estimate model parameters of NTM. Figure 3 shows the wind rose and the frequency distribution of the wind speed at the site. 98.4% of the measurement data is found suitable for this investigation. The prevailing wind direction at the site is northwesterly during winter season, while southerly and northerly wind prevails during spring and autumn seasons. According to the frequency distribution of the wind speed, an occurrence frequency of 32% is observed for wind speeds exceeding 1 m/s that results in a higher mean wind speed, comparing with that of the onshore site. Figure 4 shows the variation of turbulence intensity with increase in wind speed. 9% quantile of measured turbulence intensity is calculated and shown in black circles. The expected value of the turbulence intensity at 15 m/s, called I ref, is also calculated. 1 Frequency (%) (%) 1 8 NW 6 4 2 N NE E Frequency (%) 8 6 4 2 SW S SE 5 1 15 2 25 3 (a) Wind rose (b) Frequency distribution of wind speed Figure 3: Characteristics of offshore wind conditions..6 Obs. I 9 (Obs.) Turbulence intensity.4.2 5 1 15 2 25 3 Figure 4: Variation of turbulence intensity with wind speed.

762 A STUDY OF THE NORMAL TURBULENCE MODEL IN 614-1 3. MODEL PARAMETERS FOR NTM In this study, applicability of the NTM of to the offshore wind is investigated and model parameters of NTM are proposed for offshore conditions. The mean value (σ ave ) and the standard deviation (σ σ ) of σ 1 are calculated for each wind speed bins between cut-in and cutout wind speed, i.e., 3 to 25 m/s. The bin with 1. m/s interval is adopted and the wind speed bins with larger than 2 data are used for the analysis. In accordance with Tanigaki et al. 3), the mean value and the standard deviation of σ 1 can be expressed as below. σ ave = I ref (au + b) (1) σ σ = I ref (αu + β) (2) Here σ ave is the mean value of σ 1, σ σ is the standard deviation of σ 1, U is 1 minutes mean wind speed, I ref is the expected value of turbulence intensity at 15 m/s and the parameters a, b and α, β are the model parameters to estimate the mean value and the standard deviation of σ 1. In 614-1, the model parameters a, b, α, and β are defined as.75, 3.8,, and 1.4 respectively, as shown in Table 2. The representative value of the turbulence standard deviation (σ 9 ) given by 9% quantile of σ 1 is approximated as follows: σ 9 = σ ave + 1.28 σ σ (3) 9% quantile value of turbulence intensity (I 9 ) is obtained by substituting eqns (1 2) in eqn (3). I 9 = σ 9 /U = I ref (a + 1.28α + (b + 1.28β)/U) (4) Figure 5 shows the variation of σ ave /I ref with wind speed for the observations. It tends to increase linearly with increase in the wind speed, and model parameters could successfully represent observation data with reasonable accuracy. Values of the model parameters a and b, defined in NTM of are considered suitable for estimation of σ ave under offshore conditions. The mean values of the standard deviation are calculated from eqn. (1) for NTM parameters of. The Root Mean Square Error (RMSE) is relatively smaller value of 6.5%. This indicates that the model parameters of for estimation of σ ave is suitable for the offshore conditions. Figure 6 shows the variation of σ σ /I ref with wind speed. It also tends to increase linearly with increase in the wind speed. However, NTM of fails to capture this tendency of offshore wind. The similar discrepancy in σ σ /I ref is also reported for the onshore wind observations by Tanigaki et al. 3). It is clear from Fig. 6 that observed σ σ /I ref are considerably larger than NTM Table 2: Proposed and model parameters Present study a.75.75 b 3.8 3.8 α.27 β 2.7 1.4

WIND ENGINEERING VOLUME 36, NO. 6, 212 PP 759-766 763 3 Observation 2 σ ave / I ref 1 5 1 15 2 25 Figure 5: Variation of σ ave /I ref with wind speed. 2 15 Observat ion Present study σ σ / I ref 1 5 5 1 15 2 25 Figure 6: Variation of σ σ /I ref with wind speed. of. In order to model the standard deviation of σ 1, parameters α and β shown in eqn. (2) are identified by using the least squares method as.27 and 2.7 respectively, which are larger than and 1.4 defined in NTM of and are close to.15 and 2. proposed by Tanigaki et al. 3) based on onshore wind observations. σ σ is estimated using both proposed and model parameters. It is clear that use of model parameters results in considerable underestimation of σ σ, while the predicted σ σ by the proposed model parameters shows better agreement with the observed ones. The RMSE of σ σ is reduced from 8.2% for NTM of to 4.% for the proposed model. To examine overall performance parameters of the proposed model parameters (a, b, α, and β ), the turbulence intensities I 9 estimated by NTM of and proposed model are presented in Figure 7. Model parameters of NTM of result in significant underestimation of I 9, while I 9 calculated using proposed parameters agrees well with the measurement. This indicates that it is necessary to use proposed values of parameters α and β for accurate estimation of turbulence intensity, I 9. As mentioned above, the parameters for the mean value and the standard deviation of σ 1 in the 614-1 Ed. 3 were determined by few observation data. The accuracy of the mean

764 A STUDY OF THE NORMAL TURBULENCE MODEL IN 614-1.3.2 Observation Present study I 9.1 5 1 15 2 25 Figure 7: Variation of I 9 with wind speed. value of σ 1 is verified by several researches, while the parameters for the standard deviation of σ 1 in the 614-1 are less than those obtained by the recent observations. It implies that the parameters for the standard deviation of σ 1 should be modified in the next edition of the 614-1. 4. CONCLUSION The characteristics of the turbulence standard deviation are investigated using offshore wind observations data and limitations of the Normal Turbulence Model of are clarified. The conclusions from this study are summarized as follows: 1. The model parameters (a, b) identified from the offshore wind observations show close agreement with those defined in NTM of for estimation of the mean value of σ 1, while the identified model parameters (α, β) corresponding to the standard deviation of σ 1 are significantly larger than those defined in NTM of. 2. The model parameters defined in NTM of leads to accurate estimation of mean value of σ 1, but significant underestimation of standard deviation of σ 1 is observed. This results in underestimation of the turbulence intensity I 9. The proposed model parameters in this study improve estimation accuracy of I 9 agreement with the observation. and show good ACKNOWLEDGMENT The offshore wind observation data used in this study was obtained in a joint research between The University of Tokyo, Tokyo Electric Power Company, and Kajima Corporation, and the analysis was conducted as a part of project funded by The New Energy and Industrial Technology Development Organization (NEDO), Japan. The authors wish to express their deepest gratitude to the concerned parties for their assistance during this study. REFERENCES [1] Tsuchiya, M., Ishihara, T., Fukumoto, Y., The wind observation on the pacific ocean for offshore wind farm, Proceedings of EWEC 26, 26. [2] 614-1, Wind turbines Part 1: Design requirements, Ed.3, 25.

WIND ENGINEERING VOLUME 36, NO. 6, 212 PP 759-766 765 [3] Tanigaki, S., Kogaki, T., Matsumiya, H., Imamura, H., Japanese wind turbulence characteristics in relation to turbulence model in 614-1 Ed. 3, Proceedings of EWEC 21, 21. [4] 614-12-1, Wind turbines Part12-1: Power performance measurements of electricity producing wind turbines, 21.