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9.6 Newton-Raphson Method for Nonlinear Systems of Equations 379<br />

Hence one step of Newton-Raphson, taking a guess x k into a new guess xk+1,<br />

can be written as<br />

xk+1 = xk −<br />

P (xk)<br />

P ′ (xk) − P (xk) � j<br />

i=1 (xk − xi) −1<br />

(9.5.29)<br />

This equation, if used with i ranging over the roots already polished, will prevent a<br />

tentative root from spuriously hopping to another one’s true root. It is an example<br />

of so-called zero suppression as an alternative to true deflation.<br />

Muller’s method, which was described above, can also be useful at the polishing<br />

stage.<br />

CITED REFERENCES AND FURTHER READING:<br />

Acton, F.S. 1970, <strong>Numerical</strong> Methods That Work; 1990, corrected edition (Washington: Mathematical<br />

Association of America), Chapter 7. [1]<br />

Peters G., and Wilkinson, J.H. 1971, Journal of the Institute of Mathematics and its Applications,<br />

vol. 8, pp. 16–35. [2]<br />

IMSL Math/Library Users Manual (IMSL Inc., 2500 CityWest Boulevard, Houston TX 77042). [3]<br />

Ralston, A., and Rabinowitz, P. 1978, A First Course in <strong>Numerical</strong> Analysis, 2nd ed. (New York:<br />

McGraw-Hill), §8.9–8.13. [4]<br />

Adams, D.A. 1967, Communications of the ACM, vol. 10, pp. 655–658. [5]<br />

Johnson, L.W., and Riess, R.D. 1982, <strong>Numerical</strong> Analysis, 2nd ed. (Reading, MA: Addison-<br />

Wesley), §4.4.3. [6]<br />

Henrici, P. 1974, Applied and Computational Complex Analysis, vol. 1 (New York: Wiley).<br />

Stoer, J., and Bulirsch, R. 1980, Introduction to <strong>Numerical</strong> Analysis (New York: Springer-Verlag),<br />

§§5.5–5.9.<br />

9.6 Newton-Raphson Method for Nonlinear<br />

Systems of Equations<br />

We make an extreme, but wholly defensible, statement: There are no good, general<br />

methods for solving systems of more than one nonlinear equation. Furthermore,<br />

it is not hard to see why (very likely) there never will be any good, general methods:<br />

Consider the case of two dimensions, where we want to solve simultaneously<br />

f(x, y) =0<br />

g(x, y) =0<br />

(9.6.1)<br />

The functions f and g are two arbitrary functions, each of which has zero<br />

contour lines that divide the (x, y) plane into regions where their respective function<br />

is positive or negative. These zero contour boundaries are of interest to us. The<br />

solutions that we seek are those points (if any) that are common to the zero contours<br />

of f and g (see Figure 9.6.1). Unfortunately, the functions f and g have, in general,<br />

no relation to each other at all! There is nothing special about a common point from<br />

either f’s point of view, or from g’s. In order to find all common points, which are<br />

Sample page from NUMERICAL RECIPES IN C: THE ART OF SCIENTIFIC COMPUTING (ISBN 0-521-43108-5)<br />

Copyright (C) 1988-1992 by Cambridge University Press. Programs Copyright (C) 1988-1992 by <strong>Numerical</strong> Recipes Software.<br />

Permission is granted for internet users to make one paper copy for their own personal use. Further reproduction, or any copying of machinereadable<br />

files (including this one) to any server computer, is strictly prohibited. To order <strong>Numerical</strong> Recipes books or CDROMs, visit website<br />

http://www.nr.com or call 1-800-872-7423 (North America only), or send email to directcustserv@cambridge.org (outside North America).

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