Abstract:Asymptotic formulas, as ε → 0 + , are derived for the solutions of the nonlinear differential equation εu +Q(u) = 0 with boundary conditions u(−1) = u(1) = 0 or u (−1) = u (1) = 0. The nonlinear term Q(u) behaves like a cubic; it vanishes at s − , 0, s + and nowhere else in [s − , s + ], where s − < 0 < s + . Furthermore, Q (s ± ) < 0, Q (0) > 0 and the integral of Q on the interval [s − , s + ] is zero. Solutions to these boundary-value problems are shown to exhibit internal shock layers, and the error terms … Show more
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