Analytic shock-fronted solutions to a reaction–diffusion equation with negative diffusivity

IF 4.6 Q2 MATERIALS SCIENCE, BIOMATERIALS ACS Applied Bio Materials Pub Date : 2024-03-21 DOI:10.1111/sapm.12685
Thomas Miller, Alexander K. Y. Tam, Robert Marangell, Martin Wechselberger, Bronwyn H. Bradshaw-Hajek
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Abstract

Reaction–diffusion equations (RDEs) model the spatiotemporal evolution of a density field u ( x , t ) $u({x},t)$ according to diffusion and net local changes. Usually, the diffusivity is positive for all values of u $u$ , which causes the density to disperse. However, RDEs with partially negative diffusivity can model aggregation, which is the preferred behavior in some circumstances. In this paper, we consider a nonlinear RDE with quadratic diffusivity D ( u ) = ( u a ) ( u b ) $D(u) = (u - a)(u - b)$ that is negative for u ( a , b ) $u\in (a,b)$ . We use a nonclassical symmetry to construct analytic receding time-dependent, colliding wave, and receding traveling wave solutions. These solutions are multivalued, and we convert them to single-valued solutions by inserting a shock. We examine properties of these analytic solutions including their Stefan-like boundary condition, and perform a phase plane analysis. We also investigate the spectral stability of the u = 0 $u = 0$ and u = 1 $u = 1$ constant solutions, and prove for certain a $a$ and b $b$ that receding traveling waves are spectrally stable. In addition, we introduce a new shock condition where the diffusivity and flux are continuous across the shock. For diffusivity symmetric about the midpoint of its zeros, this condition recovers the well-known equal-area rule, but for nonsymmetric diffusivity it results in a different shock position.

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具有负扩散性的反应-扩散方程的冲击前解析解
反应-扩散方程(RDE)根据扩散和局部净变化来模拟密度场的时空演变。通常情况下,扩散率在所有Ⅴ值下都为正值,这会导致密度分散。然而,部分扩散率为负的 RDE 可以模拟聚集,这在某些情况下是首选行为。在本文中,我们考虑了一种具有二次扩散性的非线性 RDE,该扩散性在......时为负。我们利用非经典对称性来构建解析的后退时变、碰撞波和后退行波解。这些解都是多值解,我们通过插入冲击波将它们转换为单值解。我们研究了这些解析解的特性,包括它们的类斯蒂芬边界条件,并进行了相平面分析。我们还研究了恒定解的频谱稳定性,并证明了后退行波具有一定的频谱稳定性。此外,我们还引入了一种新的冲击条件,即扩散率和通量在冲击两侧是连续的。对于围绕其零点中点对称的扩散性,该条件恢复了著名的等面积规则,但对于非对称扩散性,它导致了不同的冲击位置。
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来源期刊
ACS Applied Bio Materials
ACS Applied Bio Materials Chemistry-Chemistry (all)
CiteScore
9.40
自引率
2.10%
发文量
464
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