17.02.2014 Views

Mathematical Methods for Physicists: A concise introduction - Site Map

Mathematical Methods for Physicists: A concise introduction - Site Map

Mathematical Methods for Physicists: A concise introduction - Site Map

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

NUMERICAL METHODS<br />

Solution:<br />

Here f …x† ˆx 2 2. Take x 1 ˆ 1and ˆ 0:001, then Eq. (13.13) gives<br />

x 2 ˆ 1:499750125;<br />

x 3 ˆ 1:416680519;<br />

x 4 ˆ 1:414216580;<br />

x 5 ˆ 1:414213563;<br />

)<br />

x 6 ˆ 1:414113562<br />

x 6 ˆ x 7 :<br />

x 7 ˆ 1:414113562<br />

Numerical integration<br />

Very often de®nite integrations cannot be done in closed <strong>for</strong>m. When this happens<br />

we need some simple and useful techniques <strong>for</strong> approximating de®nite integrals.<br />

In this section we discuss three such simple and useful methods.<br />

The rectangular rule<br />

The reader is familiar with the interpretation of the de®nite integral R b<br />

a<br />

f …x†dx as<br />

the area under the curve y ˆ f …x† between the limits x ˆ a and x ˆ b:<br />

Z b<br />

a<br />

f …x†dx ˆ Xn<br />

iˆ1<br />

f … i †…x i x i1 †;<br />

where x i1 i x i ; a ˆ x 0 < x 1 < x 2 < < x n ˆ b: We can obtain a good<br />

approximation to this de®nite integral by simply evaluating such an area under<br />

the curve y ˆ f …x†. We can divide the interval a x b into n subintervals of<br />

length h ˆ…b a†=n, and in each subinterval, the function f … i † is replaced by a<br />

Figure 13.5.<br />

466

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!