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Finite time blow-up of nonradial solutions in an attraction-repulsion chemotaxis system
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This paper considers the attraction–repulsion chemotaxis system: 9cdd5bb6211d51fec1b2435f86ff550" title="Click to view the MathML source">ut=Δu−χ∇⋅(u∇v)+ξ∇⋅(u∇w), b8554605c30e8741b05c3d9628a419" title="Click to view the MathML source">0=Δv+αu−βv, e486e207a" title="Click to view the MathML source">0=Δw+γu−δw, subject to the non-flux boundary condition in a smooth bounded domain Ω⊂R2, with 83b82" title="Click to view the MathML source">χ,ξ≥0, b80617a1cdee8a6f9" title="Click to view the MathML source">α,β,γ,δ>0. We establish the finite time blow-up conditions for nonradial solutions that the finite time blow-up occurs at e889ca1" title="Click to view the MathML source">x0∈Ω whenever Ωu0(x)dx>8π/(χα−ξγ) with b8a99440d3d46a1e7a22a95b5" title="Click to view the MathML source">χα−ξγ>0, under Ωu0(x)|x−x0|2dx sufficiently small. This does agree with the known blow-up conditions for radial solutions of the same model. The previous blow-up conditions for nonradial solutions are more complicated involving a classification to the sign of δ−β.

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