Calculation method of eddy current loss in magnetic materials based on magnetic-inductance

Patent metadata

Field	Value
Publication number	US-11790132-B2
Application number	US-202117612942-A
Country	US
Kind code	B2
Filing date	Jan 22, 2021
Priority date	Nov 26, 2020
Publication date	Oct 17, 2023
Grant date	Oct 17, 2023

Abstract

The present invention discloses a calculation method of eddy current loss in magnetic materials based on magnetic-inductance. The present invention proposes a vector model of a magnetic circuit, an eddy current reaction is equivalent to a magnetic-inductance component in the magnetic circuit, and the eddy current loss can be fast calculated by the vector model of the magnetic circuit. When the frequency is high, the eddy current loss dominates an iron loss and can be estimated as an entire iron loss. The present invention proposes the vector model of the magnetic circuit based on which the calculation method of eddy current loss in magnetic materials is proposed as well. Through the proposed method the eddy current loss in magnetic materials can be directly calculated by using the magnetic-inductance and the magnetic flux in the magnetic circuit, which can provide guidance for design and performance evaluation of high-frequency electrical equipment from a brand new viewpoint.

First claim

What is claimed is:

1. A calculation method of eddy current loss in magnetic materials, wherein an eddy current reaction is equivalent to a lumped parameter magnetic-inductance L mc , then a vector model {dot over (F)}={dot over (Φ)}·(R mc +jωL mc ) of a magnetic circuit is established, wherein j is an imaginary unit, R mc is a reluctance of the magnetic circuit, ω is an angular frequency of a magnetic flux varied in the magnetic circuit, {dot over (Φ)} is a magnetic flux vector in the magnetic circuit, and {dot over (F)} is a magnetomotive force (MMF) vector in the magnetic circuit; and the calculation method of eddy current loss in magnetic materials comprises the following steps:
S1, an excitation voltage {dot over (U)} E with a frequency of f 1 is applied to an excitation coil, generating an excitation current İ E , an induced voltage {dot over (U)} D is induced on a detection coil, and active power P input to the excitation coil can be observed by a power analyzer;
S2, the magnetic flux vector {dot over (Φ)} and a flux density B can be obtained through a relationship-{dot over (Φ)}={dot over (U)} D /(2πf 1 N 2 ), wherein N 2 is the number of turns of the detection coil;
S3, a magnetic-inductance L mc_1 of the magnetic circuit with the frequency of f 1 can be derived by the input active power observed in S1 and a relationship formula of P=ω 2 L mc ∥{dot over (Φ)}∥ 2 ;
S4, magnetic fluxes corresponding to different excitation voltages can be obtained in S2 by keeping the frequency of the excitation voltage unchanged while changing amplitude of the excitation voltage {dot over (U)} E ; and then the eddy current losses with the different magnetic fluxes can be calculated by the relationship formula of P=ω 2 L mc ∥{dot over (Φ)}∥ 2 ; and
S5, a magnetic-inductance L mc_2 with a frequency f 2 in the magnetic circuit can be obtained according to a formula

L

mc
⁢
_

⁢
1

L

mc
⁢
_

⁢
2

=

f
2

f
1

,

therefore, when the frequency of the excitation voltage is adjusted to f 2 , then the eddy current losses with the different magnetic fluxes can be obtained as well according to the relationship formula of P=Φ 2 L mc ∥{dot over (Φ)}∥ 2 .

2. The calculation method of eddy current loss in magnetic materials according to claim 1 , wherein virtual magnetic power {dot over (S)} mc of the vector model of the magnetic circuit is further derived by multiplying the MMF with the magnetic flux, as follows:
{dot over ( S )} mc ={dot over (Φ)}·{dot over ( F )}*={dot over (Φ)}·[ R mc ·{dot over (Φ)}*− jωL mc {dot over (Φ)}*]=R mc ∥{dot over (Φ)}∥ 2 jωL mc ∥{dot over (Φ)}∥ 2 .

3. The calculation method of eddy current loss in magnetic materials according to claim 2 , wherein the virtual magnetic power {dot over (S)} mc and electric power {dot over (S)} e are connected through a conversion factor jω, satisfying the following relationship:
{dot over (S)} e =jω{dot over (S)} mc ∥{dot over (Φ)}∥ 2 +jωR mc ∥{dot over (∥)}∥ 2 ,

wherein a real part is active power, and an imaginary part is reactive power.

4. The calculation method of eddy current loss in magnetic materials according to claim 1 , wherein the power consumed by magnetic-inductance in the magnetic circuit corresponds to the power of the eddy current loss P eddy , therefore, the eddy current loss P eddy can be directly calculated by the magnetic-inductance and the magnetic flux in the magnetic circuit, as follows:
P eddy =ω 2 L mc ∥{dot over (Φ)}∥ 2 .

Assignees

• Univ Southeast

Inventors

• Cheng Ming
• Wang Zheng
• Qin Wei
• Zhu Xinkai

Classifications

• G06F30/23 Primary

  using finite element methods [FEM] or finite difference methods [FDM] · CPC title

• H01F41/0246

  Manufacturing of magnetic circuits by moulding or by pressing powder (magnetic cores made by moulding or by pressing powder H01F27/255; soft magnetic particles H01F1/20, H01F1/36) · CPC title

• G06F2119/06

  Power analysis or power optimisation · CPC title