By Serge Lang

ISBN-10: 0387962018

ISBN-13: 9780387962016

This 5th variation of Lang's booklet covers the entire subject matters ordinarily taught within the first-year calculus series. Divided into 5 elements, each one element of a primary path IN CALCULUS comprises examples and functions in terms of the subject coated. moreover, the rear of the publication comprises targeted ideas to a number of the workouts, permitting them to be used as worked-out examples -- one of many major advancements over past variants.

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Example text

9) a Since y takes values in R, it represents a single planar curve connecting the two fixed points (a, y0 ) and (b, y1 ). This is the single-degree-of-freedom case. In the multiple-degrees-of-freedom case, one has y : [a, b] → Rn and accordingly L : R × Rn × Rn → R. This generalization is useful for treating spatial curves (n = 3) or for describing the motion of many particles; the latter setting was originally proposed by Lagrange in his 1788 monograph M´ecanique Analytique. The assumption that y ∈ C 1 is made to ensure that J is well defined (of course we do not need it if y does not appear in L).

30), but also has a very clear mechanical interpretation. 8 Reproduce all the derivations of this subsection (up to this point) for the more general setting of N moving particles. , functions that remain constant along extremals. We now revisit these two conservation laws—as well as another related case—in the context of the principle of least action, which permits us to see their physical meaning. CALCULUS OF VARIATIONS AND OPTIMAL CONTROL 41 Conservation of energy. In a conservative system, the potential is fixed and does not change with time.

It takes the same form in every coordinate system. This allows one to pick convenient coordinates when studying a specific problem. 3. 18) is a second-order differential equation for y(·); indeed, it can be written in more detail as Ly = L y x + L y y y + L y y y . 24) Note that we are being somewhat informal in denoting the third argument of L by y , and also in omitting the x-arguments. 24) can be reduced to a differential equation that is of first order, and therefore more tractable. Special case 1 (“no y”).

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A first course in calculus by Serge Lang


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