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[1]台灣電力公司/經營績效/統計資料/歷年平均電價,http://www.taipower.com.tw/,2010/8/17. [2]經濟部能源局/國際原油價格查詢/年均價查詢,http://www.moeaboe.gov.tw/oil102,2010/8/17. [3]台灣電力公司/經營績效/統計資料/歷年行業用電,http://www.taipower.com.tw/TaipowerWeb//upload/files/14/main_2_5_2_4.pdf,2010/8/17. [4]郭欣弘,“馬達動力系統節能選用之探討,”機械工業雜誌229期,pp. 109-112,97年2月號. [5]T. L. Mthombeni, P. Pillay, and R. M. W. Strnat, “New Epstein Frame for lamination core loss measurements under high frequencies and high flux densities,” IEEE Trans. Energy Conv., vol. 22, no. 3, pp. 614-620, Sept. 2007. [6]W. Salz, “A two-dimensional measuring equipment for electrical steel,” IEEE Trans. Magn., vol. 30, no. 3, pp. 1253-1257, May 1994. [7]A. J. Moses and B. Thomas, “Measurement of rotating flux in silicon iron laminations,” IEEE Trans. Magn., vol. 9, no. 4, pp. 651-654, Dec. 1973. [8]W. Brix, K. A. Hempel, and F. J. Schulte, “Improved method for the rotational magnetization process in electrical steel sheets,” IEEE Trans. Magn., vol. 20, no. 5, pp.1708-1710, Sept. 1984. [9]T. Nakata, Y. Ishihara, M. Nakaji, and T. Todaka, “Comparison between the H-coil method and the magnetizing current method for the single sheet tester,” J. Magn. and Magn. Mater., vol. 215, pp. 607-610, 2000. [10]A. Besse, G. Boero, M. Demierre, V. Pott, and R. Popovic, “Detection of a single magnetic microbead using a miniaturized silicon Hall sensor,” Appl. Phys. Lett., vol. 80, no. 22, pp. 3-5, June 2002. [11]G. Crevecoeur, L. Dupre, L. Vandenvossche, and R. Van de Walle, “Local identification of magnetic hysteresis properties near cutting edges of electrical steel sheets,” IEEE Trans. Magn., vol. 44, no. 6, pp. 1010-1013, June 2008. [12]M. Brokate, “Some mathematical properties of the Preisach model for hysteresis,” IEEE Trans. Magn., vol. 25, no. 4, pp. 2922-2924, July 1989. [13]D. L. Atherton, J. R. Beattie, “A mean field Stoner-Wohlfarth hys- teresis model,” IEEE Trans. Magn., vol. 26, no. 6, pp. 3059-3063, Nov. 1990. [14]A. J. Bergqvist, “A simple vector generalization of the Jiles-Atherton model of hysteresis,” IEEE Trans. Magn., vol. 32, no. 5, pp. 4213 -4215, Nov. 1996. [15]D. Makaveev, M. D. Wulf, and J. Melkebeek, “Field homogeneity in a two-phase rotational single sheet tester with square samples,” J. Magn. and Magn. Mater., vol. 196, pp. 937-939, 1999. [16]A. Hasenzagl, B. Weiser, and H. Pfützner, “Novel 3-phase excited single sheet tester for rotational magnetization,” J. Magn. and Magn. Mater., vol. 160, pp. 180-182, 1996. [17]M. Jesenik, V. Gorican, M. Trlep, A. Hamler, and B. Stumberger, “Field homogeneity in a two-phase round rotational single sheet tester with one and both side shields,” J. Magn. and Magn. Mater., vol. 254, pp. 247-249, 2003. [18]W. Brix, K. A. Hempel, and W. Schroeder, “Method for the measure- ment of rotational power loss and related properties in electrical steel sheets,” IEEE Trans. Magn., vol. 18, no. 6, pp. 1469-1471, Nov. 1982. [19]J. G. Zhu and V. S. Ramsden, “Two dimensional measurement of magnetic field and core loss using a square specimen tester” IEEE Trans. Magn., vol. 29, no. 6, pp. 2995-2997, Nov. 1993. [20]H. Pfützner, “The needle method for induction tests:sources of error,” IEEE Trans. Magn., vol. 40, no. 3, pp. 1610-1616, May 2004. [21]G. Loisos and A. J. Moses, “Critical evaluation and limitations of localized flux density measurements in electrical steels,” IEEE Trans. Magn., vol. 37, no. 4, pp. 2755-2757, July 2001. [22]D. Miljavec and B. Zidaric, “Introducing a domain flexing function in the Jiles-Atherton hysteresis model,” J. Magn. and Magn. Mater., vol. 320, pp. 763-768, 2008. [23]J. V. Leite, N. Sadowski, P. kuo-Peng, N. J. Batistela, J. P. A. Bastos, and A. A. de Espindola, “Inverse Jiles-Atherton vector hysteresis model,” IEEE Trans. Magn., vol. 40, no. 4, pp. 1769-1775, July 2004. [24]D. C. Jiles, “Theory of ferromagnetic hysteresis,” J. Magn. and Magn. Mater., vol. 61, pp. 48-60, 1986. [25]N. Sadowski, N. J. Batistela, J. P. A. Bastos, and M. Lajoie-Mazenc, “An Inverse Jiles-Atherton Model to take into account hysteresis in time-stepping finite-element calculations,” IEEE Trans. Magn., vol. 38, no. 2, pp. 797-800, Mar. 2002. [26]J. V. Leite, N. Sadowski, P. Kuo-Peng, N. J. Batistela, and J. P. A. Bastos, “The Inverse Jiles-Atherton Model parameters identification,” IEEE Trans. Magn., vol. 39, no. 3, pp. 1397-1400, Mar. 2003. [27]H. Pfützner, “Rotational magnetization and rotational losses of grain oriented silicon steel sheets-fundamental aspects and theory,” IEEE Trans. Magn., vol. 30, no. 5, pp. 2802-2807, Sept. 1994. [28]K. Senda, M. Ishida, K. Sato, M. Komatsubara, and T. Yamaguchi, “Localized magnetic properties in grain-oriented silicon steel measured by stylus probe method,” Electr. Eng. Japan, vol. 117-A, no. 9, pp. 942-949, Sept. 1997. [29]COMSOL AB, COMSOL Multiphysics User’s Guide, Version 3.5a, Stockholm, Sweden, 2008. [30]K. Koibuchi, T. Ohno, and K. Sawa, “A basic study for optimal design of switched reluctance motor by finite element method,” IEEE Trans. Magn., vol. 33, no. 2, pp. 2077-2080, Mar. 1994. [31]P. Zhou, D. Lin, W. N. Fu, B. Ionescu, and Z. J. Cendes, “A general cosimulation approach for coupled field-circuit problems,” IEEE Trans. Magn., vol. 42, no. 4, pp. 1051-1054, Apr. 1994. [32]A. Deihimi, S. Farhangi, and G. Henneberger, “A general nonlinear model of switched reluctance motor with mutual coupling and multiphase excitation,” Electr. Eng., vol. 84, pp. 143-158, 2002.
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