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James Stewart-Calculus_ Early Transcendentals-Cengage Learning (2015)

A five star textbook for college calculus

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Section 5.3 The Fundamental Theorem of Calculus 395

Now we let h l 0. Then u l x and v l x, since u and v lie between x and x 1 h.

Therefore

lim f sud − lim f sud − f sxd and lim f svd − lim f svd − f sxd

h l 0 u l x h l 0 v l x

because f is continuous at x. We conclude, from (3) and the Squeeze Theorem, that

4

tsx 1 hd 2 tsxd

t9sxd − lim

− f sxd

h l 0 h

If x − a or b, then Equation 4 can be interpreted as a one-sided limit. Then Theorem

2.8.4 (modified for one-sided limits) shows that t is continuous on fa, bg.

n

Using Leibniz notation for derivatives, we can write FTC1 as

5

d

y x

f std dt − f sxd

dx a

when f is continuous. Roughly speaking, Equation 5 says that if we first integrate f

and then differentiate the result, we get back to the original function f.

y

1

f

0 1

x

FIGURE 7

f sxd − sinsx 2 y2d

Ssxd − y x

sinst 2 y2d dt

0

S

y

0.5

FIGURE 8

The Fresnel function

Ssxd − y x

sinst 2 y2d dt

0

1

x

Example 2 Find the derivative of the function tsxd − y x

0 s1 1 t 2 dt.

SOLUTION Since f std − s1 1 t 2 is continuous, Part 1 of the Fundamental Theorem

of Calculus gives

t9sxd − s1 1 x 2

Example 3 Although a formula of the form tsxd − y x a

f std dt may seem like a strange

way of defining a function, books on physics, chemistry, and statistics are full of such

functions. For instance, the Fresnel function

Ssxd − y x

sinst 2 y2d dt

0

is named after the French physicist Augustin Fresnel (1788 –1827), who is famous for

his works in optics. This function first appeared in Fresnel’s theory of the diffraction of

light waves, but more recently it has been applied to the design of highways.

Part 1 of the Fundamental Theorem tells us how to differentiate the Fresnel function:

S9sxd − sinsx 2 y2d

This means that we can apply all the methods of differential calculus to analyze S (see

Exercise 71).

Figure 7 shows the graphs of f sxd − sinsx 2 y2d and the Fresnel function

Ssxd − y x 0

f std dt. A computer was used to graph S by computing the value of this integral

for many values of x. It does indeed look as if Ssxd is the area under the graph of f

from 0 to x [until x < 1.4 when Ssxd becomes a difference of areas]. Figure 8 shows a

larger part of the graph of S.

If we now start with the graph of S in Figure 7 and think about what its derivative

should look like, it seems reasonable that S9sxd − f sxd. [For instance, S is increasing

when f sxd . 0 and decreasing when f sxd , 0.] So this gives a visual confirmation of

Part 1 of the Fundamental Theorem of Calculus.

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