Fractional Equations of Curie-von Schweidler and Gauss Laws
arXiv:0907.1837 · doi:10.1088/0953-8984/20/14/145212
Abstract
The dielectric susceptibility of most materials follows a fractional power-law frequency dependence that is called the "universal" response. We prove that in the time domain this dependence gives differential equations with derivatives and integrals of noninteger order. We obtain equations that describe "universal" Curie-von Schweidler and Gauss laws for such dielectric materials. These laws are presented by fractional differential equations such that the electromagnetic fields in the materials demonstrate "universal" fractional damping. The suggested fractional equations are common (universal) to a wide class of materials, regardless of the type of physical structure, chemical composition or of the nature of the polarization.
11 pages, LaTeX
References in corpus (4)
- Physical interpretation of initial conditions for fractional differential equations with Riemann-Liouville fractional derivatives
- Dynamics with Low-Level Fractionality
- Comparison of methods for estimating continuous distributions of relaxation times
- Signs of low frequency dispersions in disordered binary dielectric mixtures (50-50)
Cited by in corpus (9)
- Differential Equations with Fractional Derivative and Universal Map with Memory
- Fractional Dissipative Standard Map
- Universal Fractional Map and Cascade of Bifurcations Type Attractors
- On Fractional Eulerian Numbers and Equivalence of Maps with Long Term Power-Law Memory (Integral Volterra Equations of the Second Kind) to Grnvald-Letnikov Fractional Difference (Differential) Equations
- Fractional Dynamical Systems
- Origin of the Curie-von Schweidler law and the fractional capacitor from time-varying capacitance
- Fractional relaxation and wave equations for dielectrics characterized by the Havriliak-Negami response function
- Tempered relaxation with clustering patterns
- Evolution of Systems with Power-Law Memory: Do We Have to Die?