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9.4 In this section we shall use results about orthogonal projections in inner
product spaces to solve problems that involve approximating a given
APPROXIMATION function by simpler functions. Such problems arise in a variety of
PROBLEMS; FOURIER engineering and scientific applications.
SERIES
Best Approximations
All of the problems that we will study in this section will be special cases of the following general problem.
Approximation Problem Given a function f that is continuous on an interval , find the “best possible approximation”
to f using only functions from a specified subspace W of .
Here are some examples of such problems:
(a) Find the best possible approximation to over [0, 1] by a polynomial of the form .
(b) Find the best possible approximation to over [−1, 1] by a function of the form .
(c) Find the best possible approximation to x over by a function of the form
.
In the first example W is the subspace of spanned by 1, x, and ; in the second example W is the subspace of
spanned by 1, , , and ; and in the third example W is the subspace of spanned by 1, , ,
, and .
Measurements of Error
To solve approximation problems of the preceding types, we must make the phrase “best approximation over ”
mathematically precise; to do this, we need a precise way of measuring the error that results when one continuous function is
approximated by another over . If we were concerned only with approximating at a single point , then the error
at by an approximation would be simply
sometimes called the deviation between f and g at (Figure 9.4.1). However, we are concerned with approximation over the
entire interval , not at a single point. Consequently, in one part of the interval an approximation to f may have
smaller deviations from f than an approximation to f, and in another part of the interval it might be the other way around.
How do we decide which is the better overall approximation? What we need is some way of measuring the overall error in an
approximation . One possible measure of overall error is obtained by integrating the deviation over the
entire interval ; that is,
(1)

