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In mathematics, a singular perturbation problem is a problem containing a small parameter that cannot be approximated by setting the parameter value to zero. This is in contrast to regular perturbation problems, for which an approximation can be obtained by simply setting the small parameter to zero. More precisely, the solution cannot be uniformly approximated by an asymptotic expansion : as . Here is the small parameter of the problem and are a sequence of functions of of increasing order, such as . This is in contrast to regular perturbation problems, for which a uniform approximation of this form can be obtained. Singularly perturbed problems are generally characterized by dynamics operating on multiple scales. Several classes of singular perturbations are outlined below. ==Methods of analysis== A perturbed problem whose solution can be approximated on the whole problem domain, whether space or time, by a single asymptotic expansion has a regular perturbation. Most often in applications, an acceptable approximation to a regularly perturbed problem is found by simply replacing the small parameter by zero everywhere in the problem statement. This corresponds to taking only the first term of the expansion, yielding an approximation that converges, perhaps slowly, to the true solution as decreases. The solution to a singularly perturbed problem cannot be approximated in this way: As seen in the examples below, a singular perturbation generally occurs when a problem's small parameter multiplies its highest operator. Thus naively taking the parameter to be zero changes the very nature of the problem. In the case of differential equations, boundary conditions cannot be satisfied; in algebraic equations, the possible number of solutions is decreased. Singular perturbation theory is a rich and ongoing area of exploration for mathematicians, physicists, and other researchers. The methods used to tackle problems in this field are many. The more basic of these include the method of matched asymptotic expansions and WKB approximation for spatial problems, and in time, the Poincaré-Lindstedt method, the method of multiple scales and periodic averaging. For books on singular perturbation in ODE and PDE's, see for example Holmes, ''Introduction to Perturbation Methods'',〔Holmes, Mark H. ''Introduction to Perturbation Methods''. Springer, 1995. ISBN 978-0-387-94203-2〕 Hinch, ''Perturbation methods''〔Hinch, E. J. ''Perturbation methods''. Cambridge University Press, 1991. ISBN 978-0-521-37897-0〕 or Bender and Orszag, ''Advanced Mathematical Methods for Scientists and Engineers''.〔Bender, Carl M. and Orszag, Steven A. ''Advanced Mathematical Methods for Scientists and Engineers''. Springer, 1999. ISBN 978-0-387-98931-0〕 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「singular perturbation」の詳細全文を読む スポンサード リンク
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