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Fractional Behavior in Nature 2019

A special issue of Fractal and Fractional (ISSN 2504-3110).

Deadline for manuscript submissions: closed (30 November 2020) | Viewed by 20835

Special Issue Editor


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Guest Editor
Centre of Technology and Systems-UNINOVA, NOVA School of Science and Technology, NOVA University of Lisbon, Quinta da Torre, 2829-516 Caparica, Portugal
Interests: signal processing; fractional signals and systems; EEG and ECG processing
Special Issues, Collections and Topics in MDPI journals

Special Issue Information

Dear Colleagues,

It is already known that the non-integer order systems can describe the dynamical behavior of materials and processes over vast time and frequency scales, with very concise and computable models.

  1. There is evidence that most of the biological signals have spectra that do not increase or decrease by multiples of 20 dB/sec.
  2. The long-range processes (1/f noise sources)—the fractional Brownian motion (fBm) is the most famous—are very common in nature.
  3. The power law behavior can be found in many processes.

On the other hand, and looking from a much deeper perspective, the fractional derivative implies causality. By respecting the proper time order and including the effects of the past on the evolution of systems and processes, we open the door to a more realistic, non-Markovian view of the world, without drastically increasing the complexity of the system descriptions.

Prof. Dr. Manuel Ortigueira
Guest Editor

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Keywords

  • fractional derivative
  • fractional integral
  • long range
  • power law
  • fractional models
  • fractional discrete-time systems
  • fractional continuous-time systems
  • ARFIMA

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Published Papers (8 papers)

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Editorial

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2 pages, 168 KiB  
Editorial
Editorial for Special Issue “Fractional Behavior in Nature 2019”
by Manuel Duarte Ortigueira
Fractal Fract. 2021, 5(4), 186; https://doi.org/10.3390/fractalfract5040186 - 26 Oct 2021
Cited by 1 | Viewed by 1197
Abstract
The presence of fractional behavior in nature is unquestionable [...] Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)

Research

Jump to: Editorial

17 pages, 917 KiB  
Article
Signal Propagation in Electromagnetic Media Modelled by the Two-Sided Fractional Derivative
by Jacek Gulgowski, Dariusz Kwiatkowski and Tomasz P. Stefański
Fractal Fract. 2021, 5(1), 10; https://doi.org/10.3390/fractalfract5010010 - 18 Jan 2021
Cited by 8 | Viewed by 2118
Abstract
In this paper, wave propagation is considered in a medium described by a fractional-order model, which is formulated with the use of the two-sided fractional derivative of Ortigueira and Machado. Although the relation of the derivative to causality is clearly specified in its [...] Read more.
In this paper, wave propagation is considered in a medium described by a fractional-order model, which is formulated with the use of the two-sided fractional derivative of Ortigueira and Machado. Although the relation of the derivative to causality is clearly specified in its definition, there is no obvious relation between causality of the derivative and causality of the transfer function induced by this derivative. Hence, causality of the system is investigated; its output is an electromagnetic signal propagating in media described by the time-domain two-sided fractional derivative. It is demonstrated that, for the derivative order in the range [1,+), the transfer function describing attenuated signal propagation is not causal for any value of the asymmetry parameter of the derivative. On the other hand, it is shown that, for derivative orders in the range (0,1), the transfer function is causal if and only if the asymmetry parameter is equal to certain specific values corresponding to the left-sided Grünwald–Letnikov derivative. The results are illustrated by numerical simulations and analyses. Some comments on the Kramers–Krönig relations for logarithm of the transfer function are presented as well. Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)
Show Figures

Figure 1

Figure 1
<p>Considered plane wave propagating in medium described by FOM.</p>
Full article ">Figure 2
<p>Waveforms of signals propagating in FOM with <math display="inline"><semantics> <mrow> <mi>v</mi> <mo>=</mo> <mn>0.98</mn> </mrow> </semantics></math>. (<b>a</b>) reference model <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>v</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> in vacuum). (<b>b</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>. (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>0.9</mn> </mrow> </semantics></math>. (<b>d</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> (i.e., Grünwald–Letnikov derivative). (<b>e</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>1.1</mn> </mrow> </semantics></math>. (<b>f</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>1.5</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 3
<p>Waveforms of signals propagating in FOM with <math display="inline"><semantics> <mrow> <mi>v</mi> <mo>=</mo> <mn>1.02</mn> </mrow> </semantics></math>. (<b>a</b>) reference model <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>v</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> in vacuum). (<b>b</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>. (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>0.9</mn> </mrow> </semantics></math>. (<b>d</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> (i.e., Grünwald–Letnikov derivative). (<b>e</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>1.1</mn> </mrow> </semantics></math>. (<b>f</b>) <math display="inline"><semantics> <mrow> <mo>Θ</mo> <mo>=</mo> <mn>1.5</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 4
<p>Values of input parameters <span class="html-italic">v</span> and <span class="html-italic">θ</span> = Θ<span class="html-italic">v</span> for which (<b>a</b>) two-sided derivative is either causal or anti-causal and (<b>b</b>) system response is causal. (<span style="color:#00FF00">—-</span>) Causal. (<span style="color:#FF0000">—-</span>) Anti-causal. Dotted lines (- - -) represent values not considered in the paper (no attenuation of propagated signal). For values of parameters <span class="html-italic">v</span> and q between the lines, it is acausal (derivative) or non-causal (system).</p>
Full article ">
29 pages, 554 KiB  
Article
Biased Continuous-Time Random Walks with Mittag-Leffler Jumps
by Thomas M. Michelitsch, Federico Polito and Alejandro P. Riascos
Fractal Fract. 2020, 4(4), 51; https://doi.org/10.3390/fractalfract4040051 - 31 Oct 2020
Cited by 13 | Viewed by 2458
Abstract
We construct admissible circulant Laplacian matrix functions as generators for strictly increasing random walks on the integer line. These Laplacian matrix functions refer to a certain class of Bernstein functions. The approach has connections with biased walks on digraphs. Within this framework, we [...] Read more.
We construct admissible circulant Laplacian matrix functions as generators for strictly increasing random walks on the integer line. These Laplacian matrix functions refer to a certain class of Bernstein functions. The approach has connections with biased walks on digraphs. Within this framework, we introduce a space-time generalization of the Poisson process as a strictly increasing walk with discrete Mittag-Leffler jumps time-changed with an independent (continuous-time) fractional Poisson process. We call this process ‘space-time Mittag-Leffler process’. We derive explicit formulae for the state probabilities which solve a Cauchy problem with a Kolmogorov-Feller (forward) difference-differential equation of general fractional type. We analyze a “well-scaled” diffusion limit and obtain a Cauchy problem with a space-time convolution equation involving Mittag-Leffler densities. We deduce in this limit the ‘state density kernel’ solving this Cauchy problem. It turns out that the diffusion limit exhibits connections to Prabhakar general fractional calculus. We also analyze in this way a generalization of the space-time Mittag-Leffler process. The approach of constructing good Laplacian generator functions has a large potential in applications of space-time generalizations of the Poisson process and in the field of continuous-time random walks on digraphs. Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)
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Figure 1

Figure 1
<p>State-probabilities <math display="inline"><semantics> <mrow> <msubsup> <mi>p</mi> <mrow> <mi>λ</mi> <mo>,</mo> <mi>ξ</mi> <mo>,</mo> <mi>n</mi> </mrow> <mrow> <mi>α</mi> <mo>,</mo> <mi>β</mi> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> of the space-time Mittag-Leffler process as a function of <span class="html-italic">t</span> for: (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math> and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>. The results are obtained numerically using Equation (<a href="#FD83-fractalfract-04-00051" class="html-disp-formula">83</a>) for the values <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> (in the left panels) and <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>0.75</mn> </mrow> </semantics></math> (presented in the right panels); we maintain constant the parameters <math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ξ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 2
<p>State density kernel <math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="script">P</mi> <mrow> <msub> <mi>λ</mi> <mn>0</mn> </msub> <mo>,</mo> <mi>ξ</mi> </mrow> <mrow> <mi>α</mi> <mo>,</mo> <mi>β</mi> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> as a function of <span class="html-italic">t</span>. The results are obtained numerically from Equation (<a href="#FD96-fractalfract-04-00051" class="html-disp-formula">96</a>) for: (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math> and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.75</mn> </mrow> </semantics></math> maintaining constant <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ξ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. We present the values for <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mn>0.5</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>1.5</mn> <mo>,</mo> <mn>2</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mn>5</mn> </mrow> </semantics></math> with different colors codified in the colorbar.</p>
Full article ">
15 pages, 6290 KiB  
Article
Fractal and Fractional Derivative Modelling of Material Phase Change
by Harry Esmonde
Fractal Fract. 2020, 4(3), 46; https://doi.org/10.3390/fractalfract4030046 - 14 Sep 2020
Cited by 8 | Viewed by 2373
Abstract
An iterative approach is taken to develop a fractal topology that can describe the material structure of phase changing materials. Transfer functions and frequency response functions based on fractional calculus are used to describe this topology and then applied to model phase transformations [...] Read more.
An iterative approach is taken to develop a fractal topology that can describe the material structure of phase changing materials. Transfer functions and frequency response functions based on fractional calculus are used to describe this topology and then applied to model phase transformations in liquid/solid transitions in physical processes. Three types of transformation are tested experimentally, whipping of cream (rheopexy), solidification of gelatine and melting of ethyl vinyl acetate (EVA). A liquid-type model is used throughout the cream whipping process while liquid and solid models are required for gelatine and EVA to capture the yield characteristic of these materials. Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)
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Figure 1

Figure 1
<p>Rheological models.</p>
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<p>Bode plots of Maxwell and Kelvin Voigt systems.</p>
Full article ">Figure 3
<p>Fractal network and equivalent system.</p>
Full article ">Figure 4
<p>Power of <span class="html-italic">s</span> in fractal evolution.</p>
Full article ">Figure 5
<p>Cure speed of adhesive versus bond gap [<a href="#B13-fractalfract-04-00046" class="html-bibr">13</a>].</p>
Full article ">Figure 6
<p>Power of <span class="html-italic">s</span> in adhesive cure.</p>
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<p>Schematic of squeeze film geometry showing a sample under test (not to scale).</p>
Full article ">Figure 8
<p>Design of top plate (<b>left</b>) and entire test assembly (<b>right</b>).</p>
Full article ">Figure 9
<p>Frequency response for Cream at 10 <span class="html-fig-inline" id="fractalfract-04-00046-i001"> <img alt="Fractalfract 04 00046 i001" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i001.png"/></span>, 20 <span class="html-fig-inline" id="fractalfract-04-00046-i002"> <img alt="Fractalfract 04 00046 i002" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i002.png"/></span> and 30 <span class="html-fig-inline" id="fractalfract-04-00046-i003"> <img alt="Fractalfract 04 00046 i003" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i003.png"/></span> min (experimental), and the modelled impedance <span class="html-fig-inline" id="fractalfract-04-00046-i004"> <img alt="Fractalfract 04 00046 i004" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i004.png"/></span>.</p>
Full article ">Figure 10
<p>Frequency response for gelatine at 0 <span class="html-fig-inline" id="fractalfract-04-00046-i001"> <img alt="Fractalfract 04 00046 i001" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i001.png"/></span>, 4 <span class="html-fig-inline" id="fractalfract-04-00046-i002"> <img alt="Fractalfract 04 00046 i002" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i002.png"/></span> and 9 <span class="html-fig-inline" id="fractalfract-04-00046-i003"> <img alt="Fractalfract 04 00046 i003" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i003.png"/></span> min (experimental), and the modelled impedance <span class="html-fig-inline" id="fractalfract-04-00046-i004"> <img alt="Fractalfract 04 00046 i004" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i004.png"/></span>.</p>
Full article ">Figure 11
<p>Frequency response near the gel point for gelatine at 0 <span class="html-fig-inline" id="fractalfract-04-00046-i001"> <img alt="Fractalfract 04 00046 i001" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i001.png"/></span>, 1 <span class="html-fig-inline" id="fractalfract-04-00046-i002"> <img alt="Fractalfract 04 00046 i002" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i002.png"/></span> and 2 <span class="html-fig-inline" id="fractalfract-04-00046-i003"> <img alt="Fractalfract 04 00046 i003" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i003.png"/></span> min (experimental), and the modelled impedance <span class="html-fig-inline" id="fractalfract-04-00046-i004"> <img alt="Fractalfract 04 00046 i004" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i004.png"/></span>.</p>
Full article ">Figure 12
<p>Frequency response for ethyl vinyl acetate (EVA) at 97 °C <span class="html-fig-inline" id="fractalfract-04-00046-i001"> <img alt="Fractalfract 04 00046 i001" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i001.png"/></span>, 72 °C <span class="html-fig-inline" id="fractalfract-04-00046-i002"> <img alt="Fractalfract 04 00046 i002" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i002.png"/></span> and 36 °C <span class="html-fig-inline" id="fractalfract-04-00046-i003"> <img alt="Fractalfract 04 00046 i003" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i003.png"/></span> (experimental), and the modelled impedance <span class="html-fig-inline" id="fractalfract-04-00046-i004"> <img alt="Fractalfract 04 00046 i004" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i004.png"/></span>.</p>
Full article ">Figure 13
<p>Experimental frequency response for EVA near the melting point, at 79 °C <span class="html-fig-inline" id="fractalfract-04-00046-i001"> <img alt="Fractalfract 04 00046 i001" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i001.png"/></span>, 72 °C <span class="html-fig-inline" id="fractalfract-04-00046-i002"> <img alt="Fractalfract 04 00046 i002" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i002.png"/></span>, 64 °C <span class="html-fig-inline" id="fractalfract-04-00046-i003"> <img alt="Fractalfract 04 00046 i003" src="/fractalfract/fractalfract-04-00046/article_deploy/html/images/fractalfract-04-00046-i003.png"/></span>.</p>
Full article ">Figure 14
<p>Evolution of <math display="inline"><semantics> <mrow> <mi>β</mi> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> for gelatine.</p>
Full article ">Figure 15
<p>Model fits to experimental data at 72 °C.</p>
Full article ">Figure 16
<p>Evolution of <math display="inline"><semantics> <mrow> <mi>β</mi> <mrow> <mo>(</mo> <mi>T</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> for EVA.</p>
Full article ">
18 pages, 554 KiB  
Article
Fractional SIS Epidemic Models
by Caterina Balzotti, Mirko D’Ovidio and Paola Loreti
Fractal Fract. 2020, 4(3), 44; https://doi.org/10.3390/fractalfract4030044 - 31 Aug 2020
Cited by 20 | Viewed by 3608
Abstract
In this paper, we consider the fractional SIS (susceptible-infectious-susceptible) epidemic model (α-SIS model) in the case of constant population size. We provide a representation of the explicit solution to the fractional model and we illustrate the results by numerical schemes. A comparison with [...] Read more.
In this paper, we consider the fractional SIS (susceptible-infectious-susceptible) epidemic model (α-SIS model) in the case of constant population size. We provide a representation of the explicit solution to the fractional model and we illustrate the results by numerical schemes. A comparison with the limit case when the fractional order α converges to 1 (the SIS model) is also given. We analyze the effects of the fractional derivatives by comparing the SIS and the α-SIS models. Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)
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Figure 1

Figure 1
<p>Comparison between the solutions to the susceptible-infectious-susceptible (SIS) model and the explicit and numerical fractional solutions to (<a href="#FD1-fractalfract-04-00044" class="html-disp-formula">1</a>) with <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.99</mn> </mrow> </semantics></math>. The analysis shows correspondence between SIS model and the case <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> of our model. This result was expected, and it confirms the continuity wit respect to <math display="inline"><semantics> <mi>α</mi> </semantics></math> (see (P4)).</p>
Full article ">Figure 2
<p>Comparison between the explicit and numerical fractional solutions to (<a href="#FD1-fractalfract-04-00044" class="html-disp-formula">1</a>) with <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 3
<p>Comparison between the explicit and numerical fractional solutions to (<a href="#FD1-fractalfract-04-00044" class="html-disp-formula">1</a>) with <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 4
<p>Comparison between the solutions to the SIS model and the fractional solutions to (<a href="#FD1-fractalfract-04-00044" class="html-disp-formula">1</a>) with <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.99</mn> </mrow> </semantics></math> (continuity w.r. to <math display="inline"><semantics> <mi>α</mi> </semantics></math>).</p>
Full article ">Figure 5
<p>Comparison between the fractional solutions to (<a href="#FD1-fractalfract-04-00044" class="html-disp-formula">1</a>) with <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 6
<p>Comparison between the fractional solutions to (<a href="#FD1-fractalfract-04-00044" class="html-disp-formula">1</a>) with <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>.</p>
Full article ">
15 pages, 474 KiB  
Article
Mathematical Description of the Groundwater Flow and that of the Impurity Spread, which Use Temporal Caputo or Riemann–Liouville Fractional Partial Derivatives, Is Non-Objective
by Agneta M. Balint and Stefan Balint
Fractal Fract. 2020, 4(3), 36; https://doi.org/10.3390/fractalfract4030036 - 21 Jul 2020
Cited by 13 | Viewed by 2969
Abstract
In this paper, it is shown that the mathematical description of the bulk fluid flow and that of content impurity spread, which uses temporal Caputo or temporal Riemann–Liouville fractional order partial derivatives, having integral representation on a finite interval, in the case of [...] Read more.
In this paper, it is shown that the mathematical description of the bulk fluid flow and that of content impurity spread, which uses temporal Caputo or temporal Riemann–Liouville fractional order partial derivatives, having integral representation on a finite interval, in the case of a horizontal unconfined aquifer is non-objective. The basic idea is that different observers using this type of description obtain different results which cannot be reconciled, in other words, transformed into each other using only formulas that link the numbers representing a moment in time for two different choices from the origin of time measurement. This is not an academic curiosity; it is rather a problem to find which one of the obtained results is correct. Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)
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<p>Aquifers and wells.</p>
Full article ">
13 pages, 285 KiB  
Article
Fractional Derivatives and Dynamical Systems in Material Instability
by Peter B. Béda
Fractal Fract. 2020, 4(2), 14; https://doi.org/10.3390/fractalfract4020014 - 16 Apr 2020
Cited by 2 | Viewed by 2238
Abstract
Loss of stability is studied extensively in nonlinear investigations, and classified as generic bifurcations. It requires regularity, being connected with non-locality. Such behavior comes from gradient terms in constitutive equations. Most fractional derivatives are non-local, thus by using them in defining strain, a [...] Read more.
Loss of stability is studied extensively in nonlinear investigations, and classified as generic bifurcations. It requires regularity, being connected with non-locality. Such behavior comes from gradient terms in constitutive equations. Most fractional derivatives are non-local, thus by using them in defining strain, a non-local strain appears. In such a way, various versions of non-localities are obtained by using various types of fractional derivatives. The study aims for constitutive modeling via instability phenomena, that is, by observing the way of loss of stability of material, we can be informed about the proper form of its mathematical model. Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)
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<p>Dynamic bifurcation of Malvern–Cristescu material: tangent stiffness as function of <math display="inline"><semantics> <mi>κ</mi> </semantics></math> at various orders of derivative <math display="inline"><semantics> <mi>β</mi> </semantics></math>.</p>
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<p>Static bifurcation of Aifantis–Tarasov material: critical tangent stiffness as function of <math display="inline"><semantics> <mi>κ</mi> </semantics></math> at various orders of derivative <math display="inline"><semantics> <mi>β</mi> </semantics></math>.</p>
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<p>Stability chart for <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>−</mo> <mn>0.8</mn> </mrow> </semantics></math>.</p>
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12 pages, 3713 KiB  
Article
Fractional-Order Models for Biochemical Processes
by Eva-H. Dulf, Dan C. Vodnar, Alex Danku, Cristina-I. Muresan and Ovidiu Crisan
Fractal Fract. 2020, 4(2), 12; https://doi.org/10.3390/fractalfract4020012 - 10 Apr 2020
Cited by 12 | Viewed by 2939
Abstract
Biochemical processes present complex mechanisms and can be described by various computational models. Complex systems present a variety of problems, especially the loss of intuitive understanding. The present work uses fractional-order calculus to obtain mathematical models for erythritol and mannitol synthesis. The obtained [...] Read more.
Biochemical processes present complex mechanisms and can be described by various computational models. Complex systems present a variety of problems, especially the loss of intuitive understanding. The present work uses fractional-order calculus to obtain mathematical models for erythritol and mannitol synthesis. The obtained models are useful for both prediction and process optimization. The models present the complex behavior of the process due to the fractional order, without losing the physical meaning of gain and time constants. To validate each obtained model, the simulation results were compared with experimental data. In order to highlight the advantages of fractional-order models, comparisons with the corresponding integer-order models are presented. Full article
(This article belongs to the Special Issue Fractional Behavior in Nature 2019)
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<p>Comparison between simulated and experimental data for experiment 1 using <span class="html-italic">Lactobacillus plantarum</span>.</p>
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<p>Comparison between simulated and experimental data for experiment 2 using <span class="html-italic">L. plantarum</span>.</p>
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<p>Comparison between simulated and experimental data for experiment 3 using <span class="html-italic">L. plantarum</span>.</p>
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<p>Comparison between simulated and experimental data for experiment 1 using <span class="html-italic">Lactobacillus casei</span>.</p>
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<p>Comparison between simulated and experimental data for experiment 2 using <span class="html-italic">L. casei</span>.</p>
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<p>Comparison between simulated and experimental data for experiment 3 using <span class="html-italic">L. casei</span>.</p>
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<p>Comparison between simulated and experimental data for experiment 1 using both types of bacteria.</p>
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<p>Comparison between simulated and experimental data for experiment 2 using both types of bacteria.</p>
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<p>Comparison between simulated and experimental data for experiment 3 using both types of bacteria.</p>
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