IEEE TRANSACTIONS ON MAGNETICS, VOL. 48, NO. 2, FEBRUARY 2012 1011
Optimum Equivalent Models of Multi-Source Systems for the Study of
Electromagnetic Signatures and Radiated Emissions From Electric Drives
A. Sarikhani, M. Barzegaran, and O. A. Mohammed, Fellow, IEEE
Energy Systems Research Lab., Electrical and Computer Eng. Dept., Florida International University, Miami, FL 33174 USA
An optimum equivalent electric machine model for 3-D finite element (3DFE) simulation and evaluation of radiated electromagnetic
field emissions in a multi-machine environment is presented. A typical example of such systems includes electric motors and cable runs
electric drives. Initially, the detailed geometrical model of the machine was simulated in a 3DFE quasi-static electromagnetic domain. An
optimum equivalent model was created using an optimization process based upon the difference between the observed electric and mag-
netic far fields from both the detailed geometrical and the equivalent models. The equivalent model was validated in several examples.
The computed electromagnetic signature results from the equivalent model show acceptable accuracy as compared with the detailed
geometrical model of the machine. The equivalent machine model was obtained with significant reduction in computation time needed
for the evaluation of the radiated fields. The proposed model can be used as an effective method for the simulation of signatures and
radiated electromagnetic field emissions from electric drives in computationally intensive environments.
Index Terms—Electromagnetic interference (EMI), multi-source environments, signature analysis, wave propagation.
I. INTRODUCTION
E
VALUATION of electromagnetic signatures and radiated
fields for the computational assessment of electromag-
netic interference (EMI) can be computationally demanding.
During the design stage, this problem can be challenging and
contribute to increasing cost. We are proposing a model that
can contribute to optimally minimizing the product cost, reduce
time-to-market and lessen trial-and error approaches. Such a
model can also be used to develop mitigation strategies to meet
product safety and compliance standards [1]–[3].
Electrical machines are the backbone of many industries. Be-
cause of their complex structure, numerical modeling in an en-
vironment with finite computational boundaries for quasi-static
EMI at relatively far distances represent a challenging computa-
tional problem especially when the number of multi conductor
systems in the environment are increased. In the recent years,
there has been an increased interest in the expansion of multi-
level numerical simulation tools for the investigation of EMC,
EMI, and signature issues in the early design stages of electrical
apparatus and specially their utilization environments. Some
studies evaluating the signature patterns and radiated emissions
from multi-machine environments represent a progress in this
important area of product development [4]–[6]. Physics-based
numerical modeling of multi-source environments, from the de-
vice level to the environment level remains challenging problem
in computational electromagnetics. As the number of the con-
ductive components within the environment is increased, the
number of self and mutual coupling capacitances and induc-
tances are increase. Therefore, without a proper model reduc-
tion, the FE-based simulation of the physical system may be
difficult to achieve. Also, the simplification of each independent
subsystem within the environment is vital for the creation of nu-
merically viable and simpler environment.
Manuscript received July 07, 2011; revised October 02, 2011 and October
16, 2011; accepted October 16, 2011. Date of current version January 25, 2012.
Corresponding author: O. A. Mohammed (e-mail: mohammed@fiu.edu).
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TMAG.2011.2173794
This paper offers an optimal equivalent model for an example
induction machine representing a multi conductor system in
a study environment. The model was created for simulating
quasi-static far electromagnetic fields propagated from a multi
conductor environment with a large number of degrees of
freedom. The proposed model makes it possible to reduce the
mesh size and make the numerical computation possible. With
this model, it is possible to reduce the number the mesh sizes
and the freedom in the finite element domain in a quasi-static
EMI problem with complex geometrical components.
II. CREATION OF OPTIMAL EQUIVALENT MODELS
A. Theoretical Definitions
In a given environment, the far field is defined as the field at
a distance at which the normal magnetic flux density or normal
electric field propagated from the multi-conductor component in
any arbitrary plane parallel to the component has only one local
maximum. The near field defined, vice versa, as when more than
one local maximum appear in any arbitrary plane. Figs. 1 and 2
show examples of the near and far magnetic fields, respectively.
These figures are the stationary solutions of a two-machine en-
vironment simulated by 3-D quasi-static finite element analysis.
It is seen that the far field almost appeared when the distance of
the measurement plane to the largest machine conductive part
become significant enough.
The propagated quasi-static electric and magnetic fields from
the electrical components specifically at a far distance from the
device is the most effective index in investigating EMI issues. In
[7] and [8], the basis of the analytical methods for the far field
solution is presented. Although the analytical solutions offer low
computational complexity, it fails to handle the multipart envi-
ronments.
The role of the numerical simulation tools becomes more im-
portant when material diversities and geometrical complexities
increase from a certain level. However, these methods also have
serious computational capacity limitations.
In the static magnetic field domain, the far field definition de-
fines the fact that the normal magnetic flux density of a magnetic
dipole is always coincident with the definition of the far field
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