Graphics Reference
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4.5.2. Theorem. Let X Õ R n and let f : X Æ R be a differentiable function. If a point
p in the interior of X is a relative extremum for f, then p is a critical point of f.
Proof. We give a proof for the case where p is a local maximum. In that case, f( q )
£ p for all points q sufficiently close to p . The definition of the directional derivative
implies that D v f( p ) £ 0 for all directions v . In particular, D v f( p ) £ 0 and D - v f( p ) £ 0.
This and Proposition 4.3.18(1) clearly imply that D v f( p ) = 0, so that —f( p ) = 0 .
Let f : [a,b] Æ R be a C 2
4.5.3. Theorem.
function and assume that c in (a,b) is a
critical point of f.
(1) If f≤(c) < 0, then c is a local maximum for f.
(2) If f≤(c) > 0, then c is a local minimum for f.
(3) If f≤(c) = 0, then nothing can be concluded from this test.
Proof. The easiest way to prove (1) and (2) is to use the Taylor expansion for f. See
[Buck78]. The canonical examples for (1) and (2) are the functions -x 2 and x 2 , respec-
tively. Their graphs are shown in Figure 4.12(a). To prove (3), simply consider the
functions x 4 , -x 4 , and x 3 (Figure 4.12(b)). This finishes the proof of Theorem 4.5.3.
The graph of the function x 3 shows another property of graphs.
Definition. A point c is called an inflection point of a function f(x) if there is an
e>0, so that either
¢¢ () <
(
)
¢¢ () >
(
)
f
x
0
for x
Œ
c
-
e
,
c
and
f
x
0
for x
Œ
c c
,
+
e
or
¢¢ () >
(
)
¢¢ () <
(
)
f
x
0
for x
Œ
c
-
e
,
c
and
f
x
0
for x
Œ
c c
,
+
e
.
y
y
y
x
x
x
f(x) = x 2
f(x) = -x 2
f(x) = x 3
(a)
(b)
Figure 4.12.
Some canonical cases of Theorem 4.5.3.
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