Lectures On the Calculus of Variations the Weierstrassian Theory

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We have yet to show that the first integral is also positive, if F-C^>o.
After a known theorem in differential equations it is always possible, as soon as the equation dt is integrated through a continuous function u of ^, which within and on the boundaries of the interval / . . . .^ nowhere vanishes, also to integrate the differential equation d_ dt through a continuous function of /, which, if k does not exceed certain limits, deviates indefinitely little throughout its whole trace from u, an
...d may therefore be represented in the form /t l . 77 I / / l"\ Iw ** ( ^ V) tv Jj where (^, k} becomes indefinitely small at the same time as k for all values of / that come into consideration.
The function u will therefore vanish nowhere within the in terval t . . . . /!. In this manner a certain limit has also been estab lished for k, which it cannot exceed ; but if the condition is also CALCULUS OF VARIATIONS.
161 CHAPTER XI.
THE NOTION OP A FIELD ABOUT THE CURVE WHICH OFFERS A MAXIMUM OR A MINIMUM VALUE OF THE INTEGRAL.


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