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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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22Calculus of variationsIn chapters 2 <strong>and</strong> 5 we discussed how to find stationary values of functions of asingle variable f(x), of several variables f(x,y,...) <strong>and</strong> of constrained variables,where x,y,... are subject to the n constraints g i (x,y,...)=0,i =1, 2,...,n.Inallthese cases the <strong>for</strong>ms of the functions f <strong>and</strong> g i were known, <strong>and</strong> the problem wasone of finding the appropriate values of the variables x, y etc.We now turn to a different kind of problem in which we are interested inbringing about a particular condition <strong>for</strong> a given expression (usually maximisingor minimising it) by varying the functions on which the expression depends. Forinstance, we might want to know in what shape a fixed length of rope shouldbe arranged so as to enclose the largest possible area, or in what shape it willhang when suspended under gravity from two fixed points. In each case we areconcerned with a general maximisation or minimisation criterion by which thefunction y(x) that satisfies the given problem may be found.The calculus of variations provides a method <strong>for</strong> finding the function y(x).The problem must first be expressed in a mathematical <strong>for</strong>m, <strong>and</strong> the <strong>for</strong>mmost commonly applicable to such problems is an integral. Ineachoftheabovequestions, the quantity that has to be maximised or minimised by an appropriatechoice of the function y(x) may be expressed as an integral involving y(x) <strong>and</strong>the variables describing the geometry of the situation.In our example of the rope hanging from two fixed points, we need to findthe shape function y(x) that minimises the gravitational potential energy of therope. Each elementary piece of the rope has a gravitational potential energyproportional both to its vertical height above an arbitrary zero level <strong>and</strong> to thelength of the piece. There<strong>for</strong>e the total potential energy is given by an integral<strong>for</strong> the whole rope of such elementary contributions. The particular function y(x)<strong>for</strong> which the value of this integral is a minimum will give the shape assumed bythe hanging rope.775

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