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Simulated Experiments for Teaching CAD Techniques Using Analytic and Finite Element Solutions of Electromagnetic Two-Dimensional Problems with Longitudinal Symmetry

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DOI: 10.4236/jemaa.2019.116006    159 Downloads   271 Views  

ABSTRACT

The paper describes an approach to teaching low-frequency electromagnetic CAD techniques to undergraduate students pursuing a degree course in electrical engineering. The simulated experiments make use of a two-dimensional open-access software based on the finite-element method. At the laboratory meetings, the problems are initially solved analytically. Upon this, students learn how to create the numeric model and how to define the sequence of field problems that lead to the required solution. Simulation tasks based on a force-producing electromagnet are used to introduce numeric techniques to determine magnetic field distribution, evaluation of energy storage and generation of magnetic forces. The nature of the magnetic force generated in the air gaps of the C-core electromagnet is explained in detail. Magnetic forces are calculated by the classical and weighted versions of the method of Maxwell stress tensor. The paper provides all the basic elements required for further exploration of devices with longitudinal symmetry.

1. Introduction

The present work aims to encourage higher education teachers to use finite element programs as a complementary tool in the teaching of electromagnetics. The enhanced capability of the finite element method in the analysis of problems involving non-homogeneous, non-linear and time-dependent problems has been determinant in the choice of this numerical method. The manuscript takes the reader to a step-by-step simulation journey that provides all the basic elements required for the analysis of electromagnetic devices with longitudinal symmetry. It is worth noting that many practical electrical devices like motors, transformers and actuators possess longitudinal symmetry. The work will certainly benefit higher education teachers who intend to create new virtual laboratories or to introduce changes in the existing ones. A similar work for the exploration of axisymmetric problems has been recently published and appears in [1] . Both papers contain a section devoted to the numeric modeling of the test problem that can serve as a template for future simulation practices on new topics.

Following the high impact of the first application of the finite element method in electrical engineering in 1969, industrial researchers and academic groups soon realized the need for training courses offered to designers and postgraduate students in order to overcome the difficulties in using such a versatile tool in industrial design and education.

There have appeared many papers describing experiences on the use of the finite element method in the teaching of electromagnetics. Some papers describe the experience of academic groups in the development of their electromagnetic field simulators, and explain how these programs have been used as teaching tools [2] . Commercial finite element packages have also been successfully used as an aid in teaching electromagnetics around the world. The main disadvantage of commercial packages is the expensive licensing. In their work, Lowther and Freeman describe how laboratory courses on field simulation based on a commercial software have been devised and implemented in three different universities, and discuss the advantages and disadvantages of finite-element CAD tools in the teaching environment [3] .

At the turn of the century, open-access programs based on the finite element method have been released, and many of these programs have been used as teaching tools [4] [5] [6] . As a result, a limited and free of charge students’ version of commercial packages also started to be released. To make their product even more competitive, some companies have also allowed free access to a series of files containing lecture notes, problem workshops and tutorials based on the limited version of their software [7] [8] . In their experience in teaching electromagnetics, Yin et al. have used a combination of two commercial simulation packages and in-house developed software [9] .

To avoid the rigorous mathematical derivations of variational calculus and make the finite element method more attractive to students, J.R. Cardoso and his collaborators have developed a new mathematical approach to finite-element analysis based on the direct integration of Maxwell’s equations [10] [11] . In recent years, general-purpose mathematical software packages like MATLAB have successfully been used in the teaching of electromagnetics [12] [13] . Very often, students of electrical engineering use MATLAB extensively in other subjects, and their familiarity with that mathematical tool has been the principal reason for the creation of MATLAB-based electromagnetic-fields virtual laboratories [14] [15] . The use of finite element methods in the teaching of electromagnetics is a topic of great interest, and new contributions to the art appear very often in specialized magazines [16] , scientific journals [17] [18] and conference proceedings [19] [20] [21] [22] .

The discussion presented in the following is based on the authors’ teaching experience in the context of a thirty-hour course. The activities include 6 hours of lectures and 24 hours of laboratory classes. The object of the introductory lectures is to present basic concepts of the finite element method: domain discretization, use of simple boundary conditions, polynomial trial functions, and formulation of the system of equations. The lectures are followed by a series of laboratory meetings where analytical calculations and field computations are made on simple physical devices. One of these meetings focuses on the creation of the numeric model of a force-producing electromagnet. This numeric model is employed in six simulated experiments chosen to introduce numeric techniques to determine magnetic field distribution, evaluation of magnetic energy storage, generation of magnetic forces and eddy current losses.

2. The Test Problem

To make the matter concrete, the step-by-step description of the numeric model for planar problems is based on the same device that appears in the simulated experiments: the C-core electromagnet shown in Figure 1. The magnetic force generated in this device attracts the movable rectangular armature into the C-core electromagnet.

In the illustration, lg denotes the length of the two small air gap regions that separate the movable armature from the stationary core. The winding has 250 turns and an intrinsic resistance of 7.5 Ω. In the dc operation, it carries a current of 5.33 A. In the ac operation, the peak current is also 5.33 A.

Figure 1. Sketch of the C-core electromagnet.

The electromagnet shown in Figure 1 represents one of the simplest devices that produce electromechanical forces, and has long been used to teach methods of magnetic force calculation. Two of the most popular types of linear actuators have stationary cores in the shape of “C” and “E”, and are commonly referred to as C-core and E-core actuators, respectively. A C-core actuator has been chosen by Kim, Lowther and Sykulski [23] to evaluate the accuracy of force computation algorithms to determine global forces, as well as force distribution over the surfaces of magnetized bodies in contact. Different types of C-core actuators have also been used to demonstrate applications of the single-solution virtual work method [24] .

3. Analytical Methods

Analytical calculations are important because they bring insight into the subject. When applied to devices with simple geometries, they can provide very accurate or even exact estimates of the quantity under investigation. It is the case of the analytic estimates of the magnetic field strength and attractive force of the C-core electromagnet described in Section 2. In problems involving more complicated slotted magnetized structures, all that can be expected from an analytical solution is to establish the order of magnitude of the quantity under investigation. The main disadvantage of analytical calculations is the lack of flexibility in accommodating alterations in the device’s geometry, its sources and design constraints.

Analytical calculation of global parameters like stored energy, inductance and total forces are usually based on equivalent magnetic circuits containing the sources of magnetomotive forces and a number of interconnected reluctors crossed by the “circulating” magnetic fluxes. These circuits are used together with magnetic Ohm’s law and Ampère’s law to determine the approximate magnitude and direction of the magnetic field strength H or magnetic induction B in the regions of interest. In our simplified analytical approach, the iron sections of the device are modelled by assuming a high constant relative permeability, µr, in the x and y directions. As a result, the problems are treated as magnetically linear, and the magnetic energy storage is considered to be entirely confined to the air regions.

3.1. Ampère’s Law

In the analysis of simple devices like the electromagnet shown in Figure 1, the terminal current i and the number of turns N of the exciting winding are usually known, and Ampère’s law provides a method for determining the magnitude of the H-field,

H d l = N i . (1)

Consider the magnetic actuator depicted in Figure 1 and a magnetic flux f circulating in the clockwise direction. To facilitate the “hand” calculations, the integration contour indicated in (1) should be formed by the union of line-segments that cross the magnetized parts and air gaps in a way that the H-field is tangential to each segment or contour section. In the illustration of Figure 2, each part or section of the integration contour is related to a number: section “1” follows the mean path of the stationary C-core; Sections 2 and 4 follow the mean path of the air gaps; and Section 3 follows the mean path of the movable armature.

Along each of the paths that form the integration contour, the magnitude of the H-field is more or less constant, the field direction is almost tangential to the path, and the integration can be approximated by the summation

k = 1 4 H k l k = N i (2)

where k represents the number of the contour section.

Under idealized conditions, the magnitude of the H-field and related magnetomotive force drops Hl along the iron sections 1 and 3 of the integration contour shown in Figure 2 are negligible, so that

H 1 0 l 1 + H 2 l 2 + H 3 0 l 3 + H 4 l 4 = N i . (3)

If the two air gap regions have the same geometric dimensions, H 2 = H 4 = H g . If lg denotes the length of one air gap, the estimate for the uniform magnetic field, Hg, in the air gap regions is computed by

H g = N i 2 l g . (4)

Once computed the magnitude of the magnetic field in the air gaps, the calculation of the attractive force can be easily performed using the method of Maxwell stress tensor.

Figure 2. Integration contour for application of Ampère’s law.

3.2. The Maxwell Stress Tensor Method

Figure 3 contains an enlarged view of the actuator’s right-hand side air gap. In smooth magnetized surfaces, like the ones that form the millimetric gaps of this actuator, the H-field practically does not vary in magnitude from point to point, and its direction is perpendicular to each iron surface. For a magnetic flux f crossing the gap in the -y direction, the magnetic field intensity H emerges from the upper iron-air interface and penetrates the lower iron-air interface. To calculate the net force by integration of the Maxwell stress tensor method, it is firstly necessary to compute the distribution of the magnetic field in terms of the H- (or B-field) at all points in the air region surrounding the object on which the force is to be calculated. In the calculation of the total force acting on a rigid body, the integration surface S could be the surface of the body itself. In computational practice, however, the use of a “surface of air” attached to the iron surface overwhelmingly facilitates the calculation. The area S of this surface of air is usually taken as the magnetic section of the magnetic pole, as indicated in the illustration. At any point of a given interface, the angle between the local force density vector dp and the surface vector dS—taken as the outward normal on the surface—is the double of the angle between the local magnetic field strength H and the surface vector dS. In this particular situation, vectors dp and dS are collinear on the two iron-air boundaries facing each other. As a result, the elemental local force density vector dp is directed downwards in the upper iron-air interface and upwards in the lower iron-air interface. In the illustration, the small arrows emerging from the two artificial layers of air represent the uniform distribution of the elemental force density vector dp.

The above discussion helps to explain the nature of the attractive force generated at the air-gap region. The resulting magnetic force always tends to shorten the length of the air-gap and its value is computed by means of the surface integral of the local force density vector dp over one surface of air. According to Newton’s first law, the force acting on the opposite iron-air surface has the same magnitude and opposite direction.

Figure 3. Vectors H, dS and dp in the air-gap region.

In two-dimensional analysis, when magnetic forces are calculated by the method of Maxwell stress tensor, the surface of integration becomes a contour of integration. In this example, the contour of integration should encompass the movable armature, and the choice of this contour affects the accuracy of computed forces. This happens because the computed field distribution, expressed in terms of the H- or B-field, is only an approximation to the true or “perfect” one, i.e., there is an inherent error in the numerical field distribution, and the independence of the values of computed forces relative to the choice of the integration contour disappears. To overcome the difficulties encountered in choosing integration contours to get accurate and consistent force calculations from imperfect numerical field solutions, McFee, Webb and Lowther [25] have proposed the method of weighted Maxwell stress tensor method. Despite the complexity of its mathematical derivation, the weighted approach became an essential simulation tool of modern electromagnetic CAD systems, wherein the contours of integration and weighting functions are calculated in a completely automated process. The post-processing tasks necessary to use this method are presented in Experiment No 4.

4. Finite Element Model

4.1. Advantages and Disadvantages of the Method

The finite element method is a numeric technique based on the theory of interpolations to solve large-scale problems of high complexity employing a data structure that is, at the same time, simple and flexible. As a result, programs developed for a particular discipline can be applied to solve problems in a different field with little or no modification. The main advantage of the method is its enhanced capability to solve problems involving: 1) complex geometries; 2) non-linearities; 3) non-homogeneous media and 4) time-dependent phenomena. The typical unstructured finite-element meshes allow good representation of curved objects, easy insertion of short gaps as well as increased local resolution in regions wherein rapid variations of the solution are expected to occur.

Despite its worldwide popularity, the method of finite elements has disadvantages, and these include its rigorous mathematical derivation as well as the use of a large amount of input and output data. The method does not produce a general closed-form solution, but only an approximate solution to the numeric model. The construction of a finite-element model invariably involves several user-defined parameters and numerous choices that affect the accuracy and consistency of the finite element solutions. In other words, different numeric models for a given problem may lead to different results, so the quality of the finite element simulations rely heavily on the experience of the user in constructing a finite element model “adequate” to the problem. Besides, experience and judgment are needed to extract and examine the results.

4.2. Problem Definition and Geometry

All numeric simulations are carried out using a two-dimensional open-access simulation software based on the finite element method [4] . The work involves one numeric model and a set of problems defined on that model. The study involves a set of problems of magnetism, so it is necessary to select the solver for magnetics problems and, implicitly define the primary quantity of calculation, that is the magnetic vector potential A. In the two-dimensional analysis of problems with translational symmetry, the magnetic vector potential A possesses only a single component in the longitudinal or z-direction, and may be treated as a scalar quantity A.

The selection of the type of symmetry to be exploited—longitudinal in the case of planar problems—is followed by the identification of the length unit associated with the dimensions prescribed in the model’s geometry. In problems with longitudinal symmetry, care must be taken to specify the “depth” parameter. The value prescribed to this parameter—in the same length unit selected for the model’s geometry—represents the length of the device in the “into the page” direction.

An outline of the numerical model with geometrical dimensions in centimeter is shown in Figure 4. The external rectangular region that appears in the illustration is an artificial boundary used to close the domain of analysis. The boundary conditions applied to this rectangular boundary are truncation of the outer boundaries. This technique assumes that no magnetic flux f crosses the boundary in the normal direction. The usual way of applying this mathematical condition is by prescribing A = 0 at this boundary. The main features of the numeric model are summarized in Table 1.

Figure 4. Regions of the numerical model. Geometric dimensions in cm.

Table 1. Features of the finite-element model.

4.3. Problem Assembly

The subdivision of the geometric domain into regions or “blocks” must consider the need of extra degree of mesh fineness in small air-gap regions and pole tips, as well as the need of separately quantifying the energy storage in some regions or areas of the device. In this particular actuator, one single region could be used to model all regions filled by air. However, this would not allow computing the amount of energy storage restricted to each small air-gap region, as required by some force calculation methods.

The proposed finite-element model contains eight regions, and these regions must be correlated to different material media. Initially, a label must be placed in each region, and this label will identify all triangular elements belonging to that region or “block”. The disposition of region labels in the geometric domain is illustrated in Figure 5(a). Labels “X1”, “X2”, “X3” and “X4” are placed in the regions that model the two air gaps, the stator window, and the external area of empty space, respectively. In the same manner, labels “Y1” and “Y2” are placed in the two non contiguous regions that represent the winding, and labels “Z1” and “Z2” are placed in the regions that model the stator and movable armature, respectively. Up to this point, the region labels are abstract entities, not yet defined. To carry on the problem assembly, it is necessary to associate material properties with region labels.

Since one kind of material may be used in different models, electromagnetic field simulators have a built-in library to facilitate the access to materials data files. The library for problems of magnetism contains several material property files of materials commonly used in the industry of electric equipment separated in file directories for conductors, permanent magnets and soft magnetic materials. Very often, the creation of new numeric models requires exchange of data files between the current numeric model and the materials library. For this model, it is necessary to “bring” to the directory entitled “Model Materials” data files that store the physical properties related to the air, copper, as well as data files containing the physical properties of the soft magnetic materials that will be used in the test problems. The correlation between region labels and materials data files is illustrated in Figure 5(b).

Figure 5. (a) Disposition of region labels; (b) Correlation between region labels and materials data files.

It is worth noting that files of material properties may contain a large amount of information. Whereas the data file related to free space or “air” only provides the value of relative magnetic permeability of the material medium ( μ r , x = μ r , y = 1 ), the data file of a soft magnetic material may contain all necessary information to fully characterize the ferromagnetic core of a power transformer, i.e., 1st quadrant B-H curve, loss curves, maximum relative permeability, electric conductivity, lamination thickness and lamination fill factor. Certainly, some familiarity with soft magnetic materials used in industry is important to future engineers. Experiment N˚ 6 takes this fact into account.

4.4. Exciting Winding

The winding is modeled by the two non contiguous rectangular regions shown in Figure 5(a). These regions are identified by labels “Y1” and “Y2”. A “circuit property” must be assigned to both conductive regions. For a given circuit property, it is necessary to specify the magnitude of the terminal current and the winding’s number of turns. In addition, both conducting regions must be defined as series-connected.

The terminal current is specified in units of ampere, either in terms of its constant value I in dc analysis or in terms of its peak value Ip in ac analysis. To enforce a magnetic flux f in the clockwise direction, the specified number of turns is +250 for the left-hand side region and −250 for the right-hand side region. The sign on the number of turns indicates the direction of current flow associated with a positive-valued circuit current. According to the convention of this field simulator, a positive-valued circuit current flows in the “out-of-the-page” direction.

4.5. Mesh Refinement

The labels placed in the different regions of the model are also used in the dialog that defines the “grain” of the mesh in one or more selected regions. The method employed to control the level of discretization in each region is based on the specification of a parameter, δ, known as “edge size”. This parameter defines a constraint on the largest possible size of the elements’ edges allowed in that region. Values prescribed to this parameter in the eight regions of the model are indicated in the illustration of Figure 6.

Figure 7(a) contains a view of the right-hand side air gap and adjacent regions. Two enlarged views of the small rectangular region highlighted in the illustration are used to show the effect of mesh refinement. Figure 7(b) shows the coarse mesh created when the mesh generator is free to choose all elements’ size, whilst Figure 7(c) shows the result of the mesh refinement guided by the specified values of the parameter δ.

5. Experiments

5.1. Experiment 1: Magnetic Force at dc Operation

Consider the C-core electromagnet shown in Figure 1. A constant terminal voltage E = 40 V is applied to the exciting winding. Use the analytic formulae presented in Section 3 and determine the attractive magnetic force acting on the movable armature.

Figure 6. Maximum triangles’ edge size in the eight regions of the model; values in centimeter.

Figure 7. (a) Enlarged view of the right-hand side air gap; (b) Coarse mesh; (c) Refined mesh.

5.2. Solution to Experiment 1

In dc operation, the inductive reactance X L = j w L of the electric circuit is null, and the current is only limited by the resistance of the winding. The terminal current I is constant and computed by Ohm’s law,

I = E R = 5.33 A . (5)

Under idealized conditions, Ampère’s law provides an estimate for the stationary and uniformly distributed magnetic field strength Hg in the two air gap regions,

H g N I 2 l g = 250 × 5.33 2 × 10 3 = 666.25 kA / m , (6)

where lg denotes the length of one air gap.

In both air gaps, the force density vector p is uniformly distributed, and its magnitude is computed by

p = μ 0 H g 2 2 N / m 2 . (7)

If S denotes the stator’s magnetic section, the attractive force Fg in one air gap is given by the product pS,

F g = μ 0 H g 2 2 S N . (8)

The total force, F, attracting the movable armature is the double,

F = 2 F g = μ 0 ( N I ) 2 4 l g 2 S . (9)

Substitution of numeric values gives F = 503 N for the idealized force calculation. It is worth noting that the magnetic force varies with the magnetic field intensity squared. Under idealized conditions and for a giving magnetomotive force NI, (4) yields the highest estimate for the air-gap field intensity and (9) produces the highest estimate for the attractive force acting on the movable armature. Computation of the attractive force under non idealized conditions will be subject of analysis on Experiment N˚4.

5.3. Experiment 2: Relative Permeability and Tangential H-Field

One of the most important properties of ferromagnetic materials is their large relative permeability µr. Iron with 0.2% impurities has a relative permeability of about 6000, and some alloys reach a relative permeability of 106. For a given excitation Ni, the idealized analytic calculations assume that the magnetic field intensity, H, is null in the magnetized parts of the electromagnet and, therefore (4) yields the highest estimate for the magnetic field intensity, Hg, in the air gaps. To investigate what happens in computational practice, two similar problems may be defined on the numeric model. The only feature differentiating the two magnetostatic problems is the relative permeability of the soft magnetic material used in the magnetic core: 1018 Steel in the first solution and M-36 Steel in the second one. The corresponding values of the relative permeabilities are: µr = 529 for the 1018 Steel, and µr = 1,616 for the M-36 Steel. In the investigation, the quantity of prime interest is the tangential component, Htan, of the magnetic field intensity.

5.4. Solution to Experiment 2

To facilitate the analysis, the magnetic portions of the electromagnet, stator and armature, are treated as non laminated, isotropic and magnetically linear materials. The relative permeability of isotropic materials has the same value in all directions and, in a two-dimensional analysis, μ r x = μ r y . Under the assumption of magnetic linearity, the value of the relative permeability is constant, and does not vary with the magnetic field intensity. In the numeric model, properties of the two selected soft magnetic materials should be associated with labels Z1 and Z2: 1018 Steel in the first problem and M-36 Steel in the second one. Both material data files must be edited to enforce the option “Linear B-H relationship”. By doing this, the value corresponding to the steepest slope of the non linear B-H data set, known as maximum relative permeability, will be attributed to the relative permeabilities µrx and µry in all subsequent calculations.

Mean values of the H-field tangential component along the integration contour shown in Figure 2 are summarized in Table 2. For the first problem, the averaged values of the tangential H-field along the contour are shown in Figure 8. In the mean, the magnitude of the tangential component, Htan, in the two magnetic sections is only 0.2% of the averaged magnitude of the tangential component, Htan, in the two air gaps. A careful observation of the results indicated in Table 2 shows that the contrast between these two magnitudes becomes

Figure 8. Averaged tangential H-field when the core material is 1018 Steel.

Table 2. Mean value of the tangential H-field in units of A/m.

even more pronounced when the core is made of the more “permeable” material M-36 Steel. As the relative permeability increases from 529 to 1,616, the ratio of the tangential H-fields in the two material media decreases from 0.2% to 0.06%. This helps to explain why in many simplified analytic calculations no attempt is made to compute the magnitude of the tangential H-field in the magnetic sections.

5.5. Experiment 3: Energy Storage in Magnetic Materials

Investigate how the relative permeability of the material employed in the ferromagnetic core affects the storage of magnetic energy in the ferromagnetic core and air-gap regions.

5.6. Solution to Experiment 3

In practice, magnetic materials do store a small amount of magnetic energy, and part of this stored energy is lost in the form of heat dissipation in the ferromagnetic core. With the aid of the numeric model, one may define a sequence of similar problems with increasing values of the core’s relative permeability. To facilitate the analysis, the magnetic portions of the electromagnet, stator and armature, are treated as isotropic and magnetically linear materials. In the simulated work, the relative permeability varies from 500 to 20,000, in steps of 500. For this, a series of new material data files have been created, each one containing a filename and values of the relative magnetic permeability in the x- and y-directions. To facilitate the future use of these materials files, the filename suggests the value of the relative permeability. For example, filename Mu_r 500 suggests a materials data file for a soft magnetic material with relative permeability µr = 500 in the x- and y-directions.

When post-processing the finite-element solutions, it is necessary to quantify: 1) the energy stored in the ferromagnetic core; 2) the energy stored in the two air gaps; and 3) the energy stored in the whole geometric domain. The effect of an increasing magnetic relative permeability on the amount of energy stored in the ferromagnetic core and air gaps is presented in the graph of Figure 9. The characteristic plotted using a solid line represents the percent stored energy in the ferromagnetic core, whilst the characteristic with circular marks represents the percent stored energy in the two millimetric gaps. Observation of former characteristic shows a pronounced decay of the energy stored in the ferromagnetic core along the leftmost portion of the curve: as the relative permeability increases from 500 to 4,000, the percent stored energy in the ferromagnetic core drops from 27% to 4.5%. This variation ought to be compared to the simultaneous increase, from 60% to 80%, in the useful, force-producing stored energy in the two air-gap regions.

5.7. Experiment 4: Relative Permeability and Magnetic Force

Investigate how the relative permeability of the material employed in the ferromagnetic core affects the value of the magnetic force acting on the movable armature when the exciting winding is supplied by a dc current of 5.33 A. The magnetically produced forces must be evaluated numerically, using the numeric method of weighted Maxwell stress tensor.

5.8. Solution to Experiment 4

The first step of the investigation is the definition of a sequence of similar problems with increasing values of the core’s relative permeability. Like in experiment N˚3, value of the relative permeability varies from 500 to 20,000, in steps of 500. Once the sequence of problems has been generated, it is necessary to launch the solver and then inspect the results. The post-processing of each finite-element solution involves three main steps, to know: 1) the block or region that represents the movable armature must be selected; 2) the “surface integral” command must be selected; and 3) the task “force via weighted stress tensor” must be chosen from the drop list.

Computed forces versus relative permeability are presented in the graph of Figure 10. The dashed horizontal line represents the analytic, idealized value of the attractive force, to know, F = 503 N. The solid line characteristic represents the force values computed numerically using the method of weighted Maxwell stress tensor.

Figure 9. Percentage of stored energy: 1) in the ferromagnetic core: solid line; 2) in the air gaps: circular marks.

Figure 10. Computed forces versus relative permeability.

The characteristic that represents the numeric force calculations resembles a B-H curve and, along its excursion, one can identify the three different regions or portions that form a typical B-H characteristic: 1) firstly, the linear or quasi linear region where 500 μ r 2 , 000 ; 2) secondly, a typical “knee” caused by the low to moderate saturation level of the ferromagnetic core; and 3) the saturated region, where force values practically do not increase any more. The characteristic only exhibits a pronounced increase in force values along the initial portion of the plot. In this quasi linear region, the increase in successive pairs of computed forces falls from 36% to 3.7%. As a consequence of magnetic saturation, only a small increase in successive computed forces can be observed along the second region. For relative permeabilities close to 11,000, the ferromagnetic core is already heavily saturated. As a result, the magnetic field strength at the gaps and the resulting attractive force converge to the values computed analytically by (6) and (9), respectively. For relative permeabilities greater than 11,000, the percent error between numeric and analytic force calculations is less than 1%, i.e., numeric and analytic calculations of the attractive force are computationally equivalent.

5.9. Experiment 5: Magnetic Force at ac Operation

Consider the C-core electromagnet shown in Figure 1. The exciting winding is supplied by an ac sinusoidal current at the operating frequency of 60 Hz. The peak value, Ip, of the terminal current is 5.33 A, the same value of the terminal current at the dc operation. Use the analytic approach and determine the attractive magnetic force acting on the movable armature for this operating condition.

5.10. Solution to Experiment 5

When the exciting winding is supplied by an alternating current, the magnetic field strength H alternates and so does the force density vector p. If Ip denotes the peak value of the ac current, the instantaneous current is

i ( t ) = I p cos ( ω t ) , (10)

and the magnitude of the force density vector in the two air-gap regions is computed by

p = μ 0 n 2 i 2 ( t ) 8 l g 2 N / m 2 . (11)

The instantaneous force density vector can be expressed, either in terms of the fundamental angular frequency ω as

p ( t ) = μ 0 n 2 I p 2 8 l g 2 cos 2 ( ω t ) N / m 2 , (12)

or in terms of the double angular frequency 2ω,

p ( t ) = μ 0 n 2 I p 2 8 l g 2 [ 1 2 + 1 2 cos ( 2 ω t ) ] N / m 2 . (13)

The product of the force density times the area S gives the attractive force in one air gap. For two air gaps, the value ought to be doubled. The alternating attractive magnetic force F (t) acting on the movable armature is thus given by

F ( t ) = ( 2 S ) μ 0 n 2 I p 2 8 l g 2 [ 1 2 + 1 2 cos ( 2 ω t ) ] N . (14)

Substitution of numeric values yields the following expression for the double-frequency attractive force:

F ( t ) = 503 2 + 503 2 cos ( 2 ω t ) N . (15)

In the graph of Figure 11, one can identify three important features of the sinusoidal characteristic that represents the double-frequency magnetic force: 1) its peak value is equal to fdc, the value of the stationary dc magnetic force, represented in the graph by the horizontal solid line; 2) its minimum value is zero; 3) its mean value, represented by the horizontal dashed line, is equal to fdc/2, half the value of the dc magnetic force.

It is worth noting that the alternating magnetic field due to the exciting winding generates an alternating attractive force that drops to zero twice each cycle of the driving alternating current. This would cause undesired mechanical vibration of the magnetized parts and metallic contacts attached to the actuator at the “closed” position. In practice, this does not happen. Industrial ac actuators and contactors contain restoring springs and shading rings designed in a way that the net attractive force never drops below the mechanical forces created by the restoring springs. The reduction of the flux due to the exciting winding occurs simultaneously to the increase in the magnetic flux due to the currents induced in the shading rings, so that the circulating magnetic flux never drops to zero. A detailed discussion on the combined effect of the fluxes provided by the ac exciting winding and shading rings may be found in [26] .

5.11. Experiment 6: Eddy Current in Laminated Cores

Most electric power equipment employ cores built up out of thin laminations in the attempt to reduce eddy current effects. To gain some experience on the analysis of electric devices used in real-world engineering, specify the core of the electromagnet as a laminated structure. Use the built-in library to choose the material employed in the laminations. Try to find a soft magnetic material with maximum relative permeability higher than 1,000. The peak value of the 60-Hz exciting terminal current is 5.33 A. The quantity of prime interest in the analysis is the eddy current loss.

5.12. Solution to Experiment 6

Data files for soft magnetic materials are found in separate file directories, to know: 1) Low Carbon Steel; 2) Magnetic Stainless Steel; 3) Silicon Iron; 4) Cobalt Iron; and 5) Nickel Alloys. The first material used in Experiment N˚ 2, the 1018 Steel, belongs to the family of “low carbon steels”, and may be disregarded because its maximum relative permeability is only 528. The second material, the M-36 Steel, belongs to the family of “silicon irons”, and satisfies the problem’s constraint: its maximum relative permeability is µr = 1,616. Other special attributes of the M-36 laminated structure include: the electric conductivity of the lamination σlam = 2.0 MS/m, the thickness of each lamination Tlam = 0.635 mm, and the fill factor of the pack of laminations, FFlam = 0.98 per unit. If only the loss caused by eddy currents in the ferromagnetic core is to be computed, it’s necessary to access the M-36 Steel data file and specify the maximum hysteresis lag angle as zero, i.e., fhmax = 0.

Figure 11. Variation of ac and dc magnetic forces.

When post-processing the field solution, it’s necessary to choose the task “total losses” from the drop list related to the numeric surface integration over the ferromagnetic core. This experiment illustrates an application wherein eddy currents are restricted by lack of space, not by the high resistivity of the core’s material. For this problem, the eddy current loss amount to 1.31 watt, and this represents only 0.6% of the apparent power input. This level of power loss is completely satisfactory for most practical design constraints.

6. Conclusion

The work discusses the use of finite element programs as a complementary tool in the teaching of electromagnetics. All simulations in the virtual laboratory make use of a two-dimensional open-access software. An important aspect of the laboratory of simulations is its library of simulated experiments. Considerable time and effort is necessary to build and maintain a library of simulated experiments. The library must be updated periodically, and new experiments must incorporate the enhancements of the field simulator. To reach efficient and effective training, qualitative and quantitative issues have to be considered when planning the activities in the laboratory of simulations. A small number of assigned experiments may take the students to draw simple conclusions restricted to a particular class of problems. On the other hand, the indiscriminate use of a very large number of experiments may result in an exhaustive activity that adversely interferes with the time students need for exercising their creativity and thinking deeply during the laboratory classes and homework.

Acknowledgements

Thanks are given to David Meeker for the use of the electromagnetic field simulator FEMM (http://www.femm.info/wiki/HomePage). Thanks are also due to the Brazilian Federal Agency for Postgraduate Studies (CAPES), for the sponsored access to several scientific web sites.

Conflicts of Interest

The authors declare no conflicts of interest regarding the publication of this paper.

Cite this paper

Nogueira, A. , Weinert, R. and Maldonado, L. (2019) Simulated Experiments for Teaching CAD Techniques Using Analytic and Finite Element Solutions of Electromagnetic Two-Dimensional Problems with Longitudinal Symmetry. Journal of Electromagnetic Analysis and Applications, 11, 79-99. doi: 10.4236/jemaa.2019.116006.

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