Physica A 388 (2009) 4586–4592
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Physica A
journal homepage: www.elsevier.com/locate/physa
Variable-order fractional differential operators in anomalous
diffusion modeling
HongGuang Sun
a,b,∗
, Wen Chen
a
, YangQuan Chen
b
a
Institute of Soft Matter Mechanics, Department of Engineering Mechanics, Hohai University, No.1 XiKang Road, Nanjing, Jiangsu 210098, China
b
Center for Self-Organizing and Intelligent Systems (CSOIS), Department of Electrical and Computer Engineering, Utah State University, 4160 Old Main Hill,
Logan, UT 84322-4160, USA
article info
Article history:
Received 14 May 2009
Received in revised form 15 June 2009
Available online 21 July 2009
PACS:
66.10.C-
05.10.Gg
02.60.Cb
Keywords:
Anomalous diffusion
Variable-order fractional differential
operator
Probability density function
Complex medium
abstract
The purpose of this paper is to offer a unified discussion of variable-order differential oper-
ators in anomalous diffusion modeling. The characteristics of the new models, in contrast to
constant-order fractional diffusion models, change with time, space, concentration or other
independent quantities. We introduced a classification of variable-order fractional diffu-
sion models based on the possible physical origins which prompt the variable-order. Some
potential applications of the variable-order fractional diffusion models are also discussed.
© 2009 Elsevier B.V. All rights reserved.
1. Introduction
Anomalous diffusion phenomena are observed in various physical, chemical and biological situations, which have
motivated the development of new mathematical and physical models [1]. It has been widely studied both by statistical
methods and differential equation models [2,3]. Fractional diffusion equations account for typical ‘‘anomalous’’ features
which are observed in many systems, e.g. in the cases of dispersive transports in amorphous semiconductors, porous
medium, colloid, proteins, biosystems or even in ecosystems [4,5]. In this study, we focus on the differential equation models
of anomalous diffusion which govern many physical phenomena such as heat, mass or electron transfer; pollutants or liquid
transport through porous media.
Up until now, the constant-order (CO) fractional kinetic equations have been considered in most cases and received
tremendous success in anomalous diffusion modeling and other fields [1,6–8]. However, it has become clear that further
theoretical and numerical investigations are required in order to incorporate adequate tools for the description of more
complicated (or more realistic) stochastic diffusion processes [9]. There are a large class of physical, biological and
physiological diffusion phenomena that the CO fractional diffusion equation with constant coefficients is not equipped to
characterize. The typical features of these phenomena are that they are complex to analysis and the diffusion behaviors
∗
Corresponding author at: Institute of Soft Matter Mechanics, Department of Engineering Mechanics, Hohai University, No.1 XiKang Road, Nanjing,
Jiangsu 210098, China. Tel.: +86 13621586259.
E-mail address: sunhongguang08@gmail.com (H. Sun).
0378-4371/$ – see front matter © 2009 Elsevier B.V. All rights reserved.
doi:10.1016/j.physa.2009.07.024