By Robert F. Brown

Here is a booklet that would be a pleasure to the mathematician or graduate scholar of arithmetic – or perhaps the well-prepared undergraduate – who would favor, with at least heritage and practise, to appreciate the various attractive effects on the center of nonlinear research. in line with carefully-expounded rules from numerous branches of topology, and illustrated through a wealth of figures that attest to the geometric nature of the exposition, the publication might be of titanic assist in supplying its readers with an figuring out of the math of the nonlinear phenomena that signify our actual world.

This booklet is perfect for self-study for mathematicians and scholars drawn to such parts of geometric and algebraic topology, sensible research, differential equations, and utilized arithmetic. it's a sharply concentrated and hugely readable view of nonlinear research through a working towards topologist who has noticeable a transparent route to understanding.

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**Additional info for A Topological Introduction to Nonlinear Analysis**

**Example text**

We are assuming that the wire has so little mass compared to that of the ball attached to it that we can ignore the weight of the wire itself. One of the fundamental ideas in physics is called the principle ofconservation of energy which states that T+V=E where T stands for kinetic energy, V for potential energy and E, the total energy, is a constant. In the case of the pendulum, the kinetic energy depends on the mass of the ball and on how rapidly the arc length of the path of the ball, called s in the figure, is changing.

Rf fl. [-f, fl [-f,fl f f [-f,f], f f) f v" + a sin y = e, T y(O) = y ( "2 ) =0 32 Part I. Fixed Point Existence Theory t) where e: [0, ~ R is a given map and a is a nonzero constant. The boundary condition is a standard one in the theory of differential equations known as the Dirichlet boundary condition. Notice that the differential equation is nonlinear because sin y is a nonlinear function of the solution y. Thus our problem is a second-order nonlinear Dirichlet boundary value problem and that is the kind of problem that we will be concerned with throughout the rest of Part I.

We have already required a function v in the domain of L to be defined on the interval [0, 1), but notice also that it doesn't make any sense to write Lv = v" unless v has a second derivative. And that isn't sufficient since the differential equation can now be written as Ly = f(t, y, y'), and we are told that the function f is continuous , so we must also require that Ly be continuous. Thus , with regard to the domain of the function L, we are only interested in functions v whose second derivative not only exist but are continuous .