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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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CALCULUS OF VARIATIONSB(b, y(b))dsdxdyA(a, y(a))Figure 22.2An arbitrary path between two fixed points.◮Show that the shortest curve joining two points is a straight line.Let the two points be labelled A <strong>and</strong> B <strong>and</strong> have coordinates (a, y(a)) <strong>and</strong> (b, y(b))respectively (see figure 22.2). Whatever the shape of the curve joining A to B, the lengthof an element of path ds is given byds = [ (dx) 2 +(dy) 2] 1/2=(1+y ′2 ) 1/2 dx,<strong>and</strong> hence the total path length along the curve is given byL =∫ ba(1 + y ′2 ) 1/2 dx. (22.7)We must now apply the results of the previous section to determine that path which makesL stationary (clearly a minimum in this case). Since the integral does not contain y (orindeed x) explicitly, we may use (22.6) to obtaink = ∂F y ′=∂y ′ (1 + y ′2 ) . 1/2where k is a constant. This is easily rearranged <strong>and</strong> integrated to giveky = x + c,(1 − k 2 )1/2which, as expected, is the equation of a straight line in the <strong>for</strong>m y = mx + c, withm = k/(1 − k 2 ) 1/2 . The value of m (or k) can be found by dem<strong>and</strong>ing that the straight linepasses through the points A <strong>and</strong> B <strong>and</strong> is given by m =[y(b) − y(a)]/(b − a). Substitutingthe equation of the straight line into (22.7) we find that, again as expected, the total pathlength is given byL 2 =[y(b) − y(a)] 2 +(b − a) 2 . ◭778

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