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A1-104 CIGRE 2012 Calculation of Electromagnetic Force on ...

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Fig.10 The electromagnetic force distributi<strong>on</strong> acting <strong>on</strong> damping windings under negative sequence operati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g>absolute damping systemIV. CONCLUSIONSThe mathematic model <str<strong>on</strong>g>of</str<strong>on</strong>g> electromagnetic force calculati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> damping system is established in this paper, whichcombined large hydro-generator with Lorentz force method. Taking the 1000MW large hydro-generator as an example,the electromagnetic force distributi<strong>on</strong> under rated operati<strong>on</strong> and negative sequence operati<strong>on</strong> c<strong>on</strong>diti<strong>on</strong> wererespectively analyzed. The c<strong>on</strong>clusi<strong>on</strong>s obtained were as follows:1) Al<strong>on</strong>g the rotati<strong>on</strong> directi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the rotor, the electromagnetic force <str<strong>on</strong>g>of</str<strong>on</strong>g> the first damping winding (1 # dampingwinding) was significantly greater than the rest <str<strong>on</strong>g>of</str<strong>on</strong>g> the damping windings in rated operati<strong>on</strong> and the radialelectromagnetic force was greater than the tangential electromagnetic force.2) Al<strong>on</strong>g the rotati<strong>on</strong> directi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the rotor, the electromagnetic force <str<strong>on</strong>g>of</str<strong>on</strong>g> the last damping winding (9 # dampingwinding) was significantly greater than the rest <str<strong>on</strong>g>of</str<strong>on</strong>g> the damping windings under negative sequence operati<strong>on</strong>.Meanwhile, the tangential magnetic force <str<strong>on</strong>g>of</str<strong>on</strong>g> the No.9 damping winding was greater than the radial electromagneticforce <str<strong>on</strong>g>of</str<strong>on</strong>g> the No.9 damping winding.3) When the absolute damping system was adopted, the electromagnetic force <str<strong>on</strong>g>of</str<strong>on</strong>g> the first damping winding (1 #damping winding) was significantly greater than the rest <str<strong>on</strong>g>of</str<strong>on</strong>g> the damping windings al<strong>on</strong>g the rotati<strong>on</strong> directi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> therotor. Meanwhile, the radial magnetic force <str<strong>on</strong>g>of</str<strong>on</strong>g> the No.1 damping winding was greater than the tangentialelectromagnetic force <str<strong>on</strong>g>of</str<strong>on</strong>g> the No.1 damping winding.4) Under the negative sequence operati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the generator, the radial electromagnetic force played more importantrole than the tangential magnetic force. Under the rated load operati<strong>on</strong>, this otherness was inc<strong>on</strong>spicuous.REFERENCES[1] Li Shufang. Yao Ruoping, and Gao Yougang. “A new method to determine the 3-D field andtranspositi<strong>on</strong> way <str<strong>on</strong>g>of</str<strong>on</strong>g> large generator[C],” Power Engineering Society 1999 Winter Meeting, Vol.2 , No.1,pp.9-12, 1999.[2] Johann Hal demand. “Transpositi<strong>on</strong> in stator bars <str<strong>on</strong>g>of</str<strong>on</strong>g> large turbogenerators[J],” IEEE Transacti<strong>on</strong>s<strong>on</strong> <strong>on</strong>energy c<strong>on</strong>versi<strong>on</strong>, Vol.119, No.3, pp.553-560, 2004.[3] Nabeta S.I, Foggia A , Coulomb J-L , and Reyen,G . “A n<strong>on</strong>-linear time-stepped finite-elementsimulati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> a symmetricl short-circuit in a synchr<strong>on</strong>ous machine[J],” IEEE Trans <strong>on</strong> Magnetics,Vol.31, No.3, pp.2040-2043, 1995.[4] Sturgess J P,Zhu M,and Macd<strong>on</strong>ald D Cl.“Finite-element simulati<strong>on</strong><str<strong>on</strong>g>of</str<strong>on</strong>g> a generator <strong>on</strong> load duringand after a three-phase fault[J],” IEEE Trans <strong>on</strong> EC,Vol.7, No.4, pp.787-793, 1992.[5] Sun Yuguang, Wang Xiangheng, Gui Lin, and Wang Weijian. “Transient calculati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> stator’s internalfaults in synchr<strong>on</strong>ous generator using FEM coupled with multi-loop method[J],” Proceedings <str<strong>on</strong>g>of</str<strong>on</strong>g> theCSEE, Vol.24, No.1, pp.136-141, 2004. (in Chinese)[6] He Chenbing, Gu Yuji<strong>on</strong>g, and Xing Cheng. “Coupled flexural and torsi<strong>on</strong>al vibrati<strong>on</strong>s analysis <str<strong>on</strong>g>of</str<strong>on</strong>g>turbine generator shaft systems caused by short circuit fault[J],” Proceedings <str<strong>on</strong>g>of</str<strong>on</strong>g> the CSEE,Vol.30, No.32,pp.84-90, 2010. (in Chinese)[7] Men Liang , Luo Yingli , and Liu Xia<str<strong>on</strong>g>of</str<strong>on</strong>g>ang , Yang Jinfu,Chi Y<strong>on</strong>gbin . “A case study <str<strong>on</strong>g>of</str<strong>on</strong>g>electromagnetic force distributi<strong>on</strong> <strong>on</strong> rotor core surface <str<strong>on</strong>g>of</str<strong>on</strong>g> turbo generator[J],” Proceedings <str<strong>on</strong>g>of</str<strong>on</strong>g> theCSEE,Vol.25, No.1, pp.81-86, 2005 .(in Chinese)[8] Li Zhiqiang,Luo Yingli,and Meng Liang.“The calculati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> local magnetic force in turbogeneratorwith FEM based virtual work principle[J],” Proceedings <str<strong>on</strong>g>of</str<strong>on</strong>g> the CSEE, Vol.27, No.15, pp.47-52, 2006. (in Chinese)

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