1996
DOI: 10.1002/sapm1996973277
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The Structure of Internal Layers for Unstable Nonlinear Diffusion Equations

Abstract: We study the structure of diffusive layers in solutions of unstable nonlinear diffusion equations. These equations are regularizations of the forward‐backward heat equation and have diffusion coefficients that become negative. Such models include the Cahn‐Hilliard equation and the pseudoparabolic viscous diffusion equation. Using singular perturbation methods we show that the balance between diffusion and higher‐order regularization terms uniquely determines the interface structure in these equations. It is sh… Show more

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Cited by 35 publications
(31 citation statements)
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“…The excess free energy of each phase are due to compositional effects; here we adopt the Wilson model [45]: f l (c) = c log c + β l c) for the liquid, and f g (c) = c log c + β g c) for the gas. The equilibrium concentrations within each phase are then obtained by the common tangent construction of f l and f g [3,46] (Fig. 1, top).…”
Section: Mathematical Modelmentioning
confidence: 99%
“…The excess free energy of each phase are due to compositional effects; here we adopt the Wilson model [45]: f l (c) = c log c + β l c) for the liquid, and f g (c) = c log c + β g c) for the gas. The equilibrium concentrations within each phase are then obtained by the common tangent construction of f l and f g [3,46] (Fig. 1, top).…”
Section: Mathematical Modelmentioning
confidence: 99%
“…Equation (3.9) can be interpreted as an equal-area rule for F(U ; ω) (Rubinstein and Sternberg [1992], Witelski [1996], ), see Figure 6. For n = 1, (3.9) trivially reduces to an equalarea rule for F (U ; ω).…”
Section: Integral Formulation Of the Radial Problemmentioning
confidence: 99%
“…The finite domain version of this problem gives Vi behaviour for the initial stages until the front hits the far boundary, and then the time behaviour switches to a linear behaviour in t [28,29].…”
Section: The Mathematical Modelmentioning
confidence: 99%