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Z b
j g.x/ j dx .b a/ max
axb
j g.x/ j :
(1.35)
a
-
Yet Another Integral Inequality. A more general result can also be useful; Let
f D f.x/ and g D g.x/ be bounded functions defined on the interval Œa; b.
Then,
Z b
j g.x/ j Z b
a
j f .x/g.x/ j dx max
axb
j f.x/ j dx:
(1.36)
a
-
The Triangle Inequality. For any real numbers x and y,wehave
j x C y j j x j C j y j :
(1.37)
Generally, for real numbers x 1 ;x 2 ;:::;x n ,wehave
ˇ
ˇ
n X
n X
x i
j x i j :
(1.38)
i D1
i D1
-
The Taylor Series. It is hard to find a more important tool for the development
and analysis of numerical methods than the Taylor series. For future reference,
we shall state it here in several versions. Let g D g.x/ be a function with n C 1
continuous derivatives. Then we have the following expansion 10 :
1
2 ˛ 2 g 00 .x/ C 1
g.x C ˛/ D g.x/ C ˛g 0 .x/ C
˛ n g .n/ .x/ C R nC1 ;
(1.39)
where
R nC1 D 1
.n C 1/Š ˛ nC1 g .nC1/ .x C /;
for some in the interval bounded by x and x C ˛. This can be written more
compactly as (recall that 0Š D 1)
n X
˛ m
g .m/ .x/ C R nC1 :
g.x C ˛/ D
(1.40)
mD0
The Taylor series expansion can also be written as
10 The notation g .n/
may seem a bit unfamiliar, but it simply means
d n g
dx n
i.e., g .n/
is the nth order derivative of the function g with respect to x.
 
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