Alvaro Meseguer - Fundamentals of Numerical Mathematics for Physicists and Engineers

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Introduces the fundamentals of numerical mathematics and illustrates its applications to a wide variety of disciplines in physics and engineering Applying numerical mathematics to solve scientific problems, this book helps readers understand the mathematical and algorithmic elements that lie beneath numerical and computational methodologies in order to determine the suitability of certain techniques for solving a given problem. It also contains examples related to problems arising in classical mechanics, thermodynamics, electricity, and quantum physics.
Fundamentals of Numerical Mathematics for Physicists and
Engineers
Provides a modern perspective of numerical mathematics by introducing top-notch techniques currently used by numerical analysts Contains two parts, each of which has been designed as a one-semester course Includes computational practicals in Matlab (with solutions) at the end of each section for the instructor to monitor the student's progress through potential exams or short projects Contains problem and exercise sets (also with solutions) at the end of each section  is an excellent book for advanced undergraduate or graduate students in physics, mathematics, or engineering. It will also benefit students in other scientific fields in which numerical methods may be required such as chemistry or biology.

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In numerical mathematics, a problem is said to be well conditioned when small changes in the input data always lead to small changes in the output solution. By contrast, a problem is said to be ill conditioned when even very small changes in the input data may lead to very large variations in the outcome. In practice it is very important to quantify this sensitivity of the solution to small changes in the input data. Let us quantify this in the case of root‐finding.

Imagine we are asked to find the abscissa картинка 401at which the graph картинка 402intercepts the ordinate картинка 403; see Figure 1.3a. Mathematically, the sought abscissa Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 404is the root Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 405of the equation Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 406, where картинка 407plays the role of a parameter. If картинка 408is slightly changed to Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 409(with Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 410small), the new root will accordingly move to a new value Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 411. If the conditions of the inverse function theorem are satisfied in a neighborhood of Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 412, the equation Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 413defines картинка 414as a function картинка 415with картинка 416, where картинка 417is the inverse function of картинка 418. Accordingly, the derivatives of картинка 419at картинка 420and of at satisfy the relation 121 or - фото 421at Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 422satisfy the relation

(1.21) Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 423

or Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 424for short, where the prime symbols acting on картинка 425and картинка 426must be understood as derivatives with respect to картинка 427and картинка 428, respectively. We can now estimate the location of the new root. Since is small Since the new root is precisely located at - фото 429is small,

Since the new root is precisely located at Finally sinc - фото 430

Since the new root is precisely located at Finally since we conclude from the last equation that - фото 431,

Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 432

Finally, since Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 433, we conclude from the last equation that Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 434. Taking the absolute value and recalling that Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 435,

(1.22) This last expression predicts how far the new root will move in terms of how - фото 436

This last expression predicts how far the new root will move in terms of how much we have perturbed картинка 437. From ( 1.22), we see that no matter how tiny картинка 438may be, картинка 439can potentially be very large if is very small As an example take the equation For the previous equation - фото 440is very small. As an example, take the equation For the previous equation has a simple root at and a double root at - фото 441. For картинка 442, the previous equation has a simple root at картинка 443and a double root at картинка 444(see Figure 1.3b, black curve). For картинка 445and Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 446, the simple root Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 447exhibits a slight displacement to Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 448and Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 449, respectively (see dashed and solid gray curves in Figure 1.3b, respectively). However, for the same values of картинка 450, the double root does experience remarkable changes. In particular, for Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 451, the double root disappears, leading to two simple roots located at Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 452and Fundamentals of Numerical Mathematics for Physicists and Engineers - изображение 453. For картинка 454the effects are even more drastic since the function has no longer any root near Figure 13a Graph intercepting ordinates - фото 455.

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