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IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES 1
On the Equivalence Between the Maxwell-Garnett
Mixing Rule and the Debye Relaxation Formula
Bartlomiej Salski, Member, IEEE, and Malgorzata Celuch, Member, IEEE
Abstract—This paper presents a closed-form noniterative
transformation of the Maxwell-Garnett mixing rule for biphased
mixtures to the triple-pole Debye relaxation formula. For the
first time, it is formally proven that such a transformation is
complete for conductive constituent materials. In other words,
the Maxwell-Garnett representation of any biphased mixture of
any conductive materials always has its formal equivalent in the
Debye form with three poles at most. For specific aspect ratios
of ellipsoidal inclusions, the number of poles reduces to one or
two, which is formally proven herein, while in previous studies, a
single-pole Debye model was arbitrarily assumed. The proposed
transformation provides Debye parameters as an explicit function
of a mixture composition, which is competitive to alternative
techniques based on laborious curve-fitting algorithms. The newly
proposed approach is of particular importance to time-domain
modeling of dilute mixtures, where the Maxwell-Garnett mixing
rule is usually approximated with available dispersive models.
Computational examples given in this paper show advantages of
the presented method over previous Maxwell-Garnett to Debye
conversion algorithms, in terms of accuracy, robustness, and
computational cost.
Index Terms—Carbon, composite materials, computational elec-
tromagnetics, dispersion, electromagnetic wave absorption.
I. INTRODUCTION
A
RTIFICIALLY composed inhomogeneous materials
have recently attracted a lot of attention within the
research and industrial communities. One of the main reasons
is that they offer very interesting possibilities of modifying
bulk electromagnetic properties of composite materials with
practically no influence on their mechanical properties. Thus,
classical construction materials used for a variety of applica-
tions may also acquire new functions, such as screening of
electromagnetic waves or their reflectionless absorption. This
concerns, for example, polymer composites doped with carbon
fibers or nanotubes [1]. Due to a complicated microscopic
geometry of such mixtures, a quantitative knowledge about
their electromagnetic properties is not that straightforward so
it has become essential to develop models (either analytical or
numerical) providing macroscopic electromagnetic properties
Manuscript received December 20, 2011; revised April 20, 2012; accepted
April 27, 2012. This work was supported in part by the Polish National Centre
for Research and Development under Contract ERA-NET-MNT/14/2009.
B. Salski is with QWED, Warsaw 02-078, Poland (e-mail: bsalski@qwed.
com.pl).
M. Celuch is with the Institute of Radioelectronics, Warsaw University of
Technology, Warsaw 00-665, Poland (e-mail: mceluch@ire.pw.edu.pl).
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/TMTT.2012.2201743
of such mixtures. Those models must be sufficiently accurate to
allow virtual prototyping with as little as possible of costly and
time-consuming experiments. It is frequently required to pre-
dict electrical properties of a particular mixture, or, reversing
the problem, adjusting the mixture composition providing the
desired material properties. The only practical approach is to
develop models of macroscopic homogeneous equivalents of
microscopically inhomogeneous mixtures. Otherwise, direct
electromagnetic analysis of an inhomogeneous material com-
prising nanoscale insertions would typically lead to prohibitive
requirements for computer resources.
Typically, the models of effective permittivity of mixtures are
specified in a frequency domain [2]. Thus, they are not directly
applicable in time-domain simulations. One of the advantages of
time-domain methods is the possibility of extracting wideband
characteristics from a single simulation. To profit from such a
possibility, one needs to apply a time-domain model, which is
accurate in a wide frequency band. Typically, time-consuming
and often cumbersome procedures for fitting the effective per-
mittivity formula with one of the dispersive models available
in the time-domain are applied. Such an approach is often used
to fit the classical Maxwell-Garnett mixing rule [3], quantifying
effective permittivity of dilute mixtures, with the Debye relax-
ation formula, the implementation of which is known in time-
domain computational routines [4], [5]. There are a few methods
frequently applied to convert one dispersive model to another,
such as genetic algorithms [6] or other large-scale optimization
methods [7]. A common disadvantage of those methods, how-
ever, is that there is no certainty that the convergence between
the two models will be achieved. Moreover, if a curve-fitting
algorithm fails to converge, it is not clear whether it is due to
an erroneously chosen optimization algorithm, a wrong starting
point, or simply because the models are nonequivalent.
Recently, to overcome the aforementioned drawbacks, the
concept of a noniterative transformation of the Maxwell-Gar-
nett mixing rule to the single-pole Debye model has been intro-
duced by the authors of this paper [8], [9]. It has been shown
that, under explicitly specified conditions, the transformation is
accurate and robust. A similar approach has been independently
investigated in [10] and [11], where the authors focused on the
conditional equivalence between the single-pole Debye model
and the Maxwell-Garnett formula for the mixtures with spher-
ical and cylindrical inclusions. The authors of [10] and [11] have
provided a solution for several types of constituent materials,
such as nondispersive, dispersive, and conductive. It can also
be recalled that an alternative method, converting a biphased
Frohlich model to the Lorentz-Debye dispersive model, has also
been recently published [12].
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