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Introduction to the Modeling and Analysis of Complex Systems

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274 CHAPTER 14. CONTINUOUS FIELD MODELS II: ANALYSISWith <strong>the</strong>se replacements, <strong>the</strong> model equation can be rewritten as follows:( )∂(αr ′ )∂∂(γt ′ ) = a(αr′ ) − b(αr ′ )(βf ′ 2 (αr ′ )) + D r∂(δx ′ ) + ∂2 (αr ′ )2 ∂(δy ′ ) 2( )∂(βf ′ )∂∂(γt ′ ) = −c(βf ′ ) + d(αr ′ )(βf ′ 2 (βf ′ )) + D f∂(δx ′ ) + ∂2 (βf ′ )2 ∂(δy ′ ) 2We can collect parameters <strong>and</strong> rescaling fac<strong>to</strong>rs <strong>to</strong>ge<strong>the</strong>r, as follows:∂r ′= aγr ′ − bβγr ′ f ′ + D ( )rγ ∂ 2 r ′∂t ′ δ 2 ∂x + ∂2 r ′′2 ∂y ′2∂f ′∂t ′= −cγf ′ + dαγr ′ f ′ + D ( )fγ ∂ 2 f ′δ 2 ∂x + ∂2 f ′′2 ∂y ′2Then we can apply, e.g., <strong>the</strong> following rescaling choices(a(α, β, γ, δ) =d , a b , 1 √ )a , Dra(14.26)(14.27)(14.28)(14.29)(14.30)<strong>to</strong> simplify <strong>the</strong> model equations in<strong>to</strong>∂r ′= r ′ − r ′ f ′ + ∇ 2 r ′ ,∂t ′ (14.31)∂f ′= −eγf ′ + r ′ f ′ + D∂t ′ ratio ∇ 2 f ′ , (14.32)with e = c/a <strong>and</strong> D ratio = D f /D r . The original model had six parameters (a, b, c, d, D r ,<strong>and</strong> D f ), but we were able <strong>to</strong> reduce <strong>the</strong>m in<strong>to</strong> just two parameters (e <strong>and</strong> D ratio ) witha little additional help from spatial rescaling fac<strong>to</strong>r δ. This rescaling result also tells ussome important information about what matters in this system: It is <strong>the</strong> ratio between <strong>the</strong>growth rate <strong>of</strong> <strong>the</strong> prey (a) <strong>and</strong> <strong>the</strong> decay rate <strong>of</strong> <strong>the</strong> preda<strong>to</strong>rs (c) (i.e., e = c/a), as well as<strong>the</strong> ratio between <strong>the</strong>ir diffusion speeds (D ratio = D f /D r ), which essentially determines<strong>the</strong> dynamics <strong>of</strong> this system. Both <strong>of</strong> <strong>the</strong>se new parameters make a lot <strong>of</strong> sense from anecological viewpoint <strong>to</strong>o.Exercise 14.4Simplify <strong>the</strong> following Keller-Segel model by variable rescaling:∂a∂t = µ∇2 a − χ∇ · (a∇c) (14.33)∂c∂t = D∇2 c + fa − kc (14.34)

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