Abstract
The classical result of A. Ambrosetti and G. Prodi [1], in the form of M.S. Berger and E. Podolak [4], gives the exact number of solutions for the problem \[ Δu+g(u)= μϕ_1(x)+e(x) \;\; \mbox{in $D$} , \;\; u=0 \;\; \mbox{on $\partial D$} \,, \] depending on the real parameter , for a class of convex , and (where is the principal eigenfunction of the Laplacian on , and is a smooth domain). By considering generalized harmonics, we give a similar result for the problem \[ Δu+g(u)= μf(x) \;\; \mbox{in $D$} , \;\; u=0 \;\; \mbox{on $\partial D$} \,, \] with . Such problems occur, for example, in "fishing" applications that we discuss, and propose a new model. Our approach also produces a very simple proof of the anti-maximum principle of Ph. Clément and L.A. Peletier [5].
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