2013
DOI: 10.1155/2013/142765
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Transient Simulation of Wind Turbine Towers under Lightning Stroke

Abstract: A simulation algorithm is proposed in this paper for lightning transient analysis of the wind turbine (WT) towers. In the proposed algorithm, the tower body is first subdivided into a discrete multiconductor system. A set of formulas are given to calculate the electrical parameters of the branches in the multiconductor system. By means of the electrical parameters, each branch unit in the multiconductor system is replaced as a coupledπ-type circuit and the multiconductor system is converted into a circuit mode… Show more

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Cited by 3 publications
(5 citation statements)
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“…Since ℎ ≫ 1 and 2 , and 2 is not much larger than 1 , the actual tower body may be simplified as a cylindrical shell, as shown in Figure 1(b). For the purpose of transient calculation, the continuous cylindrical shell can be subdivided into a multiconductor grid constituted by longitudinal and transverse branches [6,7], as shown in Figure 2(a). As the lightning current flowing through the WT tower presents significant harmonic components not exceeding a few MHz, the lightning transient responses should be calculated by the distribution parameter circuit model.…”
Section: Discretization Treatment Of Wt Towermentioning
confidence: 99%
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“…Since ℎ ≫ 1 and 2 , and 2 is not much larger than 1 , the actual tower body may be simplified as a cylindrical shell, as shown in Figure 1(b). For the purpose of transient calculation, the continuous cylindrical shell can be subdivided into a multiconductor grid constituted by longitudinal and transverse branches [6,7], as shown in Figure 2(a). As the lightning current flowing through the WT tower presents significant harmonic components not exceeding a few MHz, the lightning transient responses should be calculated by the distribution parameter circuit model.…”
Section: Discretization Treatment Of Wt Towermentioning
confidence: 99%
“…If the earth is assumed to be perfectly conducting ( = 0), the complex depth is zero according to (2). Substitution of = 0 into (5) or (6) shows that the real part of the impedance is also zero. As a result, the impedance matrix Z is further simplified as…”
Section: Mathematical Problems In Engineeringmentioning
confidence: 99%
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