# A Novel Hysteresis Model of Magnetic Field Strength Determined by Magnetic Induction Intensity for Fe-3% Si Electrical Steel Applied in Cigarette Making Machines

Authors: Hao Wang; Jianbo Zhan; Zhenhua Yu; Ying Zhang; Jiang Yu; Yongfa Gui; Tingting Yu; Jiao Xie; Hongkui Zhang; Yafeng Ji; Na Zan; Rongrong Fu; Deniz Perin
Journal: Journal of Materials
 (2016)

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## Abstract

Hysteresis characteristics of grain-oriented electrical steel were studied through the hysteresis loop. Existing hysteresis fitting simulation methods were summarized, and new Fe-3% Si grain-oriented electrical steel hysteresis loop model was proposed. Undetermined coefficients of the magnetic field intensity and magnetic flux density were determined by both the fixed angle method and the least squares method, and the hysteresis loop model was validated with high fitting degree by experimental data.


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## Body

## 1. Introduction

Fe-3% Si grain-oriented electrical steel is an important soft magnetic material, which is often used for cigarette machine sensor because of its high magnetic flux density and good magnetic performance [1–5]. Therefore, parameters such as iron loss, permeability, shielding efficiency, and Barkhausen noise of Fe-3% Si grain-oriented electrical steel have been studied extensively. When the magnetic flux is alternating, hysteresis and eddy current losses will be generated. Existence of hysteresis and eddy current losses will make the magnetic flux density lag behind the magnetic field intensity; after repeatedly magnetizing multiple cycles, the hysteresis loop forms [6, 7]. Applied sensors in cigarette making machines usually do not consider the complex effects of the hysteresis loop, inevitably leading to errors in the following simulation or performance prediction, which is an important reason why switch protection of cigarette making machine sensor is not accurate enough [8–10].Hysteresis is a quite important magnetic property of Fe-3% Si grain-oriented electrical steel, since its hysteresis loops and magnetization curves reflect the significant characteristics of the material, which is also an important basis for the selection of cigarette machine sensor materials [11, 12]. Study on the material hysteresis loop model is helpful to better understand the hysteresis property of the material, which is significant to the design of materials and related components [13]. With the increasingly higher demand of equipment design accuracy in the actual operation, it is necessary to accurately determine the impact caused by hysteresis [14, 15]. In the characterization analysis of motors, transformers, and other electromagnetic equipment, it is the first step to obtain accurate waveform relationship of B-H loop [16]. When the electromagnetic fields are accurately calculated, there must be a more accurate and rapid method for determining the B-H curve [17].Fe-3% Si grain-oriented electrical steel hysteresis performance can significantly affect its behavior as magnetic sensors [18]. In the characterization analysis of sensors and other detection equipment, the accurate waveforms flux is usually needed, and it is necessary to analyze the electromagnetic fields, and the hysteresis characteristics of grain-oriented electrical steel must be taken into account [1]. To study the hysteresis characteristics, firstly, the hysteresis characteristics of oriented electrical steel should be simulated, namely, the establishing of a mathematical model of hysteresis grain-oriented electrical steel. In this paper, the Fe-3% Si grain-oriented electrical steel hysteresis loop model was studied, and a new model of hysteresis loop was proposed.


## 2. Experimental

Conventional grain-oriented (CGO) electrical steel sheets and high permeability grain-oriented (HGO) electrical steel sheets were the tested materials in this paper. CGO and HGO electrical steel were named CC1 and CH1, respectively, and the chemical composition is shown in Table1.Table 1
Chemical composition of CC1 and CH1 tested materials (mass percent, %).
Sample Si Mn C Cu S P Al Fe CC1 3.05 0.065 0.032 0.028 0.020 0.012 0.008 Balance CH1 3.09 0.072 0.054 0.075 0.018 0.015 0.010 BalanceThe samples were manufactured as standard Epstein samples, and the sample size is 350 mm × 30 mm × 0.3 mm. Initial magnetic properties of CC1 and CH1 at 1.0 T are shown in Table2.Table 2
Initial magnetic properties of CC1 and CH1 steel at 1.0 T.
Sample Iron loss (W/kg) Coercive force (A/m) Relative permeability MBNrms (mV) CC1 0.711 282.9 799.4 0.391 CH1 0.668 287.6 2473.7 0.447A standard Epstein strip for testing is placed between the yokes, and a feedback control system implemented in LabVIEW was used to control the flux density to have repeatable and comparable measurements. The whole measurement was conducted in a magnetic shielding room and the computer was put in another room to avoid interference [2–5].


## 3. Formula Derivation and Modeling

Since the hysteresis loop is nearly symmetrical concerning the loop curve origin point, according to the Fourier series, the magnetic induction intensity and magnetic field strength could be expanded, respectively. Symmetry of the origin makes Fourier series contain only odd entries, and the expanded equations are as shown in(1)H=H1sin⁡ωt+φ1+H3sin⁡ωt+φ3+H5sin⁡ωt+φ5+⋯B=B1sin⁡ωt+ψ1+B3sin⁡ωt+ψ3+B5sin⁡ωt+ψ5+⋯.To simplify the calculation, magnetic induction intensity is taken as the first term, and the magnetic field strength is viewed as a function of magnetic induction intensity, and magnetic field strength should contain unlimited expansion terms. In the derivation and calculation of the model, only the first two terms were used, and the basic model of the hysteresis loop could be obtained. Hence,(2)B=B1sin⁡ωt,(3)H=B11μ1sin⁡ωt+φ1+1μ3sin⁡3ωt+φ3.Equation (3) reflects the nonlinear relationship between the magnetic field strength and magnetic induction intensity, in which φ represents the impact hysteresis. Values of φ1,φ3,μ1, and μ3 are influenced by magnetic field strength, which are determined by hysteresis loop. Once values of φ1,φ3,μ1, and μ3 are determined, ideal hysteresis loop could be simulated. If the hysteresis loop is smooth, the fitting degree will be high.Undetermined parameters could be determined by the fixed angle method. In (2) and (3), H1 represents magnetic field strength H amplitude in the hysteresis loop. Making ωt take different angles, respectively, in this paper, we chose 0, π/3, π/2, and 2π/3; the corresponding H1,H2,H3, and H4 could be found; taking H4 back to the equation of magnetic field strength, the following equations could be obtained: (4)H1=B11μ1sin⁡φ1+1μ3sin⁡φ3,H2=B11μ1sin⁡π3+φ1+1μ3sin⁡π+φ3=B112μ1sin⁡φ1+32μ1cos⁡φ1-1μ3cos⁡φ3,H3=B11μ1sin⁡π2+φ1+1μ3sin⁡3π2+φ3=B11μ1cos⁡φ1-1μ3cos⁡φ3,H4=B11μ1sin2π3+φ1+1μ3sin2π+φ3=B132μ1cos⁡φ1-12μ1sin⁡φ1+1μ3sin⁡φ3.AddingH2 and H4, the following calculation could be obtained:(5)H2+H4=B13μ1cos⁡φ1.After transformation,φ3 could be deleted; hence,(6)H1+H2=B132μ1sin⁡φ1+32μ1cos⁡φ1.To deleteμ1, sine expression concerning φ1 could be obtained through calculation; hence,(7)2H1+H2-H4=B13μ1sin⁡φ1.Deleteμ1, and the expression concerning φ1 could be obtained as(8)2H1+H2-H4H2+H4=3tan⁡φ1,φ1=arctan⁡2H1+H2-H43H2+H4.Value ofμ1 could be calculated as(9)μ1=3B12H1+H2-H4sin⁡φ1or(10)μ1=3B1H2+H4cos⁡φ1.Through a similar method, sine and cosine expression concerningφ3 could be calculated as(11)H1-H2+H4=3B1μ3sin⁡φ3,H2+H4-3H3=3B1μ3cos⁡φ3.To calculateφ3, it is necessary to delete μ3 first, and the following transformation could be made:(12)tan⁡φ3=H1-H2+H43H2+H4-3H3.The value of φ3 could be calculated as(13)φ3=arctan⁡H1-H2+H43H2+H4-3H3.μ 3 could be calculated when taking it back; hence,(14)μ3=3B1sin⁡φ3H1-H2+H4or(15)μ3=3B1cos⁡φ33H2+H4-3H3.After the hysteresis loop was obtained after experiment, other hysteresis loop parameters could be determined by linear interpolation.For givenBk(Bj<Bk<Bj+1), linear interpolation could be applied to calculate model parameters φ1,φ3,μ1, and μ3.Ifφj, φj+1, Bj, Bk, and Bj+1 are given, calculations could be made as follows:(16)φk=φj+φj+1-φjBj+1-BjBk-Bj.When k=1,3, φ1 and φ3 could be calculated, respectively, as (17)B=B1sin⁡ωt+φ1+B3sin⁡ωt+φ3=H1μ1sin⁡ωt+φ1+μ3sin⁡3ωt+φ3.μ 1 H k and μ3Hk could be calculated by linear interpolation.Ifμ1j,μ1j+1,H1j,H1j+1, and Hk were given, the following calculations could be made:(18)L1x=xk+1-xxk+1-xkyk+x-xkxk+1-xkyk+1,μ1Hk=H1j+1-HkH1j+1-H1j·μ1jH1j+Hk-H1jH1j+1-H1j·μ1j+1H1j+1.The two-point linear interpolation could be expressed as(19)μ1=μ1jH1j+1-H1jH1j+μ1j+1Hk-H1jH1j+1H1j+1-H1jHk.Similarly, ifμ1j,μ1j+1,H1j,H1j+1, and Hk were given, μ3 could be calculated as(20)μ3=μ3jH3j+1-H3jH3j+μ3j+1Hk-H3jH3j+1H3j+1-H3jHk.New models of hysteresis loop were derived above, and the calculation of undetermined coefficient method was given utilizing interpolation step, and the model is simple and convenient.Least squares curve fitting method is a common fitting method. When using such method to make calculation of undetermined coefficients, since the basic relationship equations of the magnetic induction density and magnetic field strength have been given, undetermined parameters of the model can be determined by magnetic field strength and magnetic induction density values of a set of experimental measurements. AssumingH1,B1,H2,B2,H3,B3,… are known and H is the measured magnetic induction intensity and H′ is the calculated magnetic induction intensity, then undetermined coefficients φ1,φ3,μ1,andμ3 could be determined by residual square difference minimization of the measured and calculated values. Hence,(21)Q=∑k=1nek2=∑k=1nBk-fBk,μ1,μ3,ψ1,ψ32.Undetermined coefficients ofB-H loop model can be calculated while Q takes the minimum value in (21). Hence,(22)∂Q∂μ1=0,∂Q∂μ3=0,∂Q∂ψ1=0,∂Q∂ψ3=0.The equations consist of the above four equations; the undetermined coefficients could be obtained, which could be back to the original hysteresis models. The relationship between the magnetic induction intensity and magnetic field strength can be obtained, illustrating the hysteresis loop model.


## 4. Model Application

The proposed model was applied forB-H curve fitting, as shown in Figure 1. The error of the single data point is controlled within 5%, achieving fine fitting effect.Figure 1
Comparison of original and fittingB-H loop graph of (a, b) CC1 and (c, d) CH1 grain-oriented electrical steel.
(a) (b) (c) (d)Figure1 simulation results show fine fitting result, and it is suitable for the working condition of silicon steel applied in the cigarette sensor machines, which is the possible complex magnetization condition in normal working conditions.


## 5. Conclusions

Expansion of the magnetic induction intensity and magnetic field strength was made according to the Fourier series, respectively. The magnetic field strength was determined by the magnetic induction intensity, and the undetermined parameters of angles, magnetic induction intensity, and the magnetic field strength could be determined by fixed angle method and the least squares method. General application steps of the model were given. The proposed model was applied forB-H curve fitting, and the error of the single data point is controlled within 5%, achieving fine fitting effect.



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*Source: 1509498-2016-10-18.xml*