70 research outputs found

    The sufficiency of the Matkowsky condition in the problem of resonance

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    We consider the sufficiency of the Matkowsky condition concerning the differential equation ε y + f ( x , ε ) y ′ + g ( x , ε ) y = 0 ( − a ⩽ x ⩽ b ) \varepsilon y + f(x,\varepsilon )y’ + g(x,\varepsilon )y = 0\;( - a \leqslant x \leqslant b) under the assumption that f ( 0 , ε ) = 0 f(0,\varepsilon ) = 0 identically in ε , f x ( 0 , ε ) ≠ 0 \varepsilon ,{f_x}(0,\varepsilon ) \ne 0 with f &gt; 0 f &gt; 0 for x &gt; 0 x &gt; 0 and f &gt; 0 f &gt; 0 for x &gt; 0 x &gt; 0 . Y. Sibuya proved that the Matkowsky condition implies resonance in the sense of N. Kopell if f f and g g are convergent power series for | ε | &gt; ρ ( ρ &gt; 0 ) , f ( x , 0 ) = − 2 x |\varepsilon | &gt; \rho \;(\rho &gt; 0),f(x,0)=-2x and the interval [ − a , b ] [ - a,b] is contained in a disc D D with center at 0 0 . The main problem in this work is to remove from Sibuya’s result the assumption that D D is a disc.</p

    Stability of planar flames as gasdynamic discontinuities

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    The stability of a steadily propagating planar premixed flame has been the subject of numerous studies since Darrieus and Landau showed that in their model flames are unstable to perturbations of any wavelength. Moreover, the instability was shown to persist even for very small wavelengths, i.e. there was no high-wavenumber cutoff of the instability. In addition to the Darrieus-Landau instability, which results from thermal expansion, analysis of the diffusional thermal model indicates that premixed flames may exhibit cellular and pulsating instabilities as a consequence of preferential diffusion. However, no previous theory captured all the instabilities including a high-wavenumber cutoff for each. In Class, Matkowsky & Klimenko (2003) a unified theory is proposed which, in appropriate limits and under appropriate assumptions, recovers all the relevant previous theories. It also includes additional new terms, not present in previous theories. In the present paper we consider the stability of a uniformly propagating planar flame as a solution of the unified model. The results are then compared to those based on the models of Darrieus-Landau, Sivashinsky and Matalon-Matkowsky. In particular, it is shown that the unified model is the only model to capture the Darrieus-Landau, cellular and pulsating instabilities including a high-wavenumber cutoff for each

    Singular perturbations in noisy dynamical systems

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    Consider a deterministic dynamical system in a domain containing a stable equilibrium, e.g., a particle in a potential well. The particle, independent of initial conditions, eventually reaches the bottom of the well. If however, the particle is subjected to white noise, due, e.g., to collisions with a population of smaller, lighter particles comprising the medium through which the particle travels, a dramatic difference in the behaviour of the Brownian particle occurs. The particle will exit the well. The natural questions then are how long will it take for it to exit and from where on the boundary of the domain of attraction of the deterministic equilibrium (the rim of the well) will it exit. We compute the mean first passage time to the boundary and the mean probabilities of the exit positions. When the noise is small each quantity satisfies a singularly perturbed deterministic boundary value problem. We treat the problem by the method of matched asymptotic expansions (MAE) and generalizations thereof. MAE has been used successfully to solve problems in many applications. However, there exist problems for which MAE does not suffice. Among these are problems exhibiting boundary layer resonance, i.e., the problem of ‘spurious solutions’, which led some to conclude that this was ‘the failure of MAE’. We present a physical argument and four mathematical arguments to modify or augment MAE to make it successful. Finally, we discuss applications of the theory.</jats:p
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