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Advanced soft- and hard-magnetic material models for the numerical simulation of electrical machines.

机译:用于电机数值模拟的先进软磁性材料模型。

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The development of energy-efficient electrical machines requires an accurate knowledge of the soft- and hard-magnetic material behavior already in the design stage. Accurate numerical models are required which offer the ability of better understanding and modelling in an appropriate accuracy. With such model properties on the one hand accurate simulations can be performed and on the other hand the best possible material choice for a particular application, i.e. for an electrical machine, can be done. The soft-magnetic material constitutes the magnetic core of an electrical machine and its properties. On that account, the accurate prediction of iron losses of soft-magnetic materials for various frequencies and magnetic flux densities, i.e., arbitrary magnetic field waveforms, is eminent for the design of electrical machines [1]. For this purpose different phenomenological iron-loss models were proposed, which describe the loss-generating effects, i.e., hysteresis, non-local eddy currents and anomalous eddy currents. Most of these suffer from poor accuracy for not considering the effect of high frequencies and high material utilization as well as the material degradation due to the magneto-elastic coupling [2, 3, 5]. This paper presents a comparison of common iron-loss models. The IEM-formula used, resolves the limitation by introducing a high-order term of the magnetic flux density and considers the alteration of material-dependent loss-parameters due to the magneto-elastic coupling [3]. The knowledge of the magnetic property deterioration due to induced residual stress occurring during the manufacturing or operation of the electrical machine is indispensable for the contemporary design. It has been widely ascertained that processing of electrical steel laminations significantly alters the magnetic properties of the electrical steel [2-6]. Cutting induces plastic deformation and residual stress in the laminations. Due to their strong sensitivity to mechanical stress, the magnetic properties are locally degraded near the cut edge. The extent of the degradation depends substantially on the process characteristics, i.e., the cutting procedure and cutting parameters in combination with material properties, such as mechanical strength and grain size [4-6]. In [7] a continuous material model for an efficient numerical model of the local magnetization was introduced. By replacing numerically expensive sliced models, the continuous model (CM) is independent of the discretization and converges in the case of coarse meshes to the sliced model [7]. Measured single-sheet specimens are used to identify the different model parameters. In Fig. 1 results on hysteresis loss distribution are presented. The vital advantage of the proposed CM is that properties depend only on the distance to the cut edge. For improved estimation of penetration depth and mechanical stress distribution, novel experimental procedures are utilized [8] and mechanical simulations are evaluated [6] to further advance the cut-edge model. Permanent magnets are central to the electromagnetic energy conversion process in permanent-magnet synchronous and flux-switching machines. In order to design the magnetic circuit and a magnetizing circuit for post-assembly magnetization as well as to analyze the resistance to being demagnetized during the simulation of electrical machines, it is indispensable to describe the magnetization behavior of the permanent magnets accurately. However, due to the complex interplay of the non-linear and hysteretic magnetization behavior and the magnetic anisotropy, it is a complex problem. Commonly, simplified models are used, which are based on empirical and phenomenological approaches. These describe the major loop of the permanent magnets only. However, the magnetization state of the permanent magnet depends on the magnetic and thermic history, i.e., it is indispensable to account for minor loops or incompletely magnetized permanent magnets. In
机译:节能电机的开发需要准确了解已经在设计阶段中的软磁性材料行为。准确的数值模型是必需的,提供更好地理解和以适当的准确性建模的能力。通过这种模型属性,可以进行精确的模拟,另一方面可以进行特定应用的最佳材料选择,即对于电机,可以完成。软磁材料构成电机的磁芯及其性能。在该帐户中,对于各种频率和磁通密度的软磁材料的准确预测,即任意磁场波形,是电机设计的卓越[1]。为此,提出了不同现象的铁损模型,描述了损失产生效果,即滞后,非局部涡流和异常涡流。大多数这些患有差的准确性差,以便不考虑高频率和高材料利用的影响以及由于磁弹性耦合引起的材料劣化[2,3,5]。本文提出了普通铁损模型的比较。所用的IEM-式中,通过引入磁通密度的高次项解析的限制,认为材料有关的损耗参数的改变是由于磁致弹性耦合[3]。由于在电机的制造或操作期间发生的诱导残余应力引起的磁性劣化的认识对于现代设计是必不可少的。已广泛确定的是,电钢叠层的加工显着改变了电钢的磁性[2-6]。切割在叠片中引起塑性变形和残余应力。由于它们对机械应力的强烈敏感性,磁性在切割边缘附近局部地劣化。降解的程度基本上取决于工艺特征,即切割程序和切割参数,与材料性质相结合,例如机械强度和晶粒尺寸[4-6]。在[7]中,引入了用于局部磁化的有效数值模型的连续材料模型。通过更换数值昂贵的切片模型,连续型号(cm)与粗网格的离散化和收敛无关[切片模型[7]。测量的单片样本用于识别不同的模型参数。在图1中。在图1中提出了滞后损失分布的结果。所提出的cm的重要优点是特性仅取决于与切割边缘的距离。为了改善渗透深度和机械应力分布的估计,利用新的实验程序[8],并评估机械模拟[6]以进一步提前削减边缘模型。永磁体是永磁同步和通量开关机中的电磁能量转换过程的核心。为了设计磁路和磁化电路,用于组装后磁化以及在电阻分析到电机的模拟期间被消磁,这是不可缺少准确地描述永磁体的磁化行为。然而,由于非线性和滞后磁化行为和磁各向异性的复杂相互作用,这是一个复杂的问题。通常,使用简化的模型,基于经验和现象学方法。这些仅描述了永磁体的主要环。然而,永磁体的磁化状态取决于磁性和热历史,即,考虑到小环或不完全磁化的永磁体是必不可少的。在

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