<p>A phenomenological mathematical model for Alzheimer’s disease is formulated and analyzed as a dynamical system. In the model, the formation of amyloid-beta (A<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\beta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> </InlineEquation>) proteins is aggregated into three compartments consisting of monomeres, proto-oligomeres, and polymeres, and the net-effect of stimulating and inhibiting feedback loops on the production of monomeres through pro- and anti-inflammatory cytokines is considered. The resulting 4-dimensional nonlinear dynamical system exhibits a uniform dynamical structure irrespective of the numerical values of the parameters with a region of attraction of the trivial equilibrium point (corresponding to no disease) and a region of divergence of the trajectories (corresponding to the presence of the disease) separated by a 3-dimensional stable manifold of a positive equilibrium point acting as stability boundary. Existence and location of this stability boundary are determined by a simple mathematical quantity which expresses the difference between stimulating and inhibiting parameters in the feedback loops and allows a direct interpretation in terms of current treatment approaches.</p>

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An aggregated mathematical model for the progression of Alzheimer’s disease with treatment implications

  • Urszula Ledzewicz,
  • Elżbieta Ratajczyk,
  • Heinz Schättler

摘要

A phenomenological mathematical model for Alzheimer’s disease is formulated and analyzed as a dynamical system. In the model, the formation of amyloid-beta (A \(\beta \) β ) proteins is aggregated into three compartments consisting of monomeres, proto-oligomeres, and polymeres, and the net-effect of stimulating and inhibiting feedback loops on the production of monomeres through pro- and anti-inflammatory cytokines is considered. The resulting 4-dimensional nonlinear dynamical system exhibits a uniform dynamical structure irrespective of the numerical values of the parameters with a region of attraction of the trivial equilibrium point (corresponding to no disease) and a region of divergence of the trajectories (corresponding to the presence of the disease) separated by a 3-dimensional stable manifold of a positive equilibrium point acting as stability boundary. Existence and location of this stability boundary are determined by a simple mathematical quantity which expresses the difference between stimulating and inhibiting parameters in the feedback loops and allows a direct interpretation in terms of current treatment approaches.