By Daniel Fleisch

ISBN-10: 0521193699

ISBN-13: 9780521193696

Vectors and tensors are one of the strongest problem-solving instruments on hand, with purposes starting from mechanics and electromagnetics to basic relativity. figuring out the character and alertness of vectors and tensors is seriously very important to scholars of physics and engineering. Adopting an identical strategy utilized in his hugely renowned A Student's consultant to Maxwell's Equations, Fleisch explains vectors and tensors in simple language. Written for undergraduate and starting graduate scholars, the e-book presents a radical grounding in vectors and vector calculus earlier than transitioning via contra and covariant parts to tensors and their functions. Matrices and their algebra are reviewed at the book's aiding web site, which additionally good points interactive strategies to each challenge within the textual content the place scholars can paintings via a chain of tricks or decide to see the full answer right away. Audio podcasts provide scholars the chance to listen to very important thoughts within the booklet defined by means of the writer.

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Additional info for A Student's Guide to Vectors and Tensors

Sample text

It’s common to call these other variables u and υ and to allow both x and y to depend on one or both of u and υ. You may encounter situations in which you know the variation in u and υ, and you want to know how much your function z will change due to those changes. 26) The chain rule is a concise expression of the fact that z depends on both x and y, and since both x and y may change if u changes, the change in z with respect to u is the sum of two terms. The first term is the change in x due to the change in u times the change in z due to that change in x , and the second term is the change in y due to the change in u change in y times the change in z due to that .

Thus r = (x2+y2+z2)1/2 and Á = k/(x2 + y2 + z2)1/2. You can find the value of the Laplacian for this case using Eq. 45; the first step is to find the partial derivative of Á with respect to x after which you take another partial with respect to x: The same approach for the second-order partials with respect to y and z gives and Now it’s just a matter of adding all three second-order partials: So for a three-dimensional function with 1/r-dependence, the Laplacian of the function is zero everywhere away from the origin.

You can do a rough check on your calculated partial derivative in Eq. 21 by inserting the value of –3 for y to see that the slope of z at this value of y is 12(x)(–3) + 3 + 5(–3) = –36x – 12. Thus as you move in the x-direction at y = –3, the slope should vary from +96 at x = –3, to zero at x = –1/3, and down to –120 at x = +3. 9. Likewise, Eq. 22 tells you that the slope of z in the y-direction at x = –3 is constant and positive, also consistent with the behavior expected from a quick analysis of the shape of the function z.

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A Student's Guide to Vectors and Tensors by Daniel Fleisch

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