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414 Chapter 7 Applications of Definite Integrals<br />

EXAMPLE 2<br />

Applying the Definition<br />

Find the exact length of the curve<br />

y 4 2<br />

x<br />

3<br />

1 for 0 x 1.<br />

SOLUTION<br />

d y<br />

4 2<br />

• 3 dx<br />

3 2 x12 22 x 12 ,<br />

which is continuous on 0, 1. Therefore,<br />

)<br />

L 1<br />

2<br />

( 1 d y<br />

dx<br />

dx<br />

0<br />

1<br />

( 22x12)<br />

2<br />

1 <br />

0<br />

1<br />

1 8x dx<br />

0<br />

2 1<br />

3 • 1 1 <br />

8<br />

8x32]<br />

0<br />

1 3<br />

.<br />

6<br />

dx<br />

y<br />

(8, 2)<br />

Now try Exercise 11.<br />

We asked for an exact length in Example 2 to take advantage of the rare opportunity it<br />

afforded of taking the antiderivative of an arc length integrand. When you add 1 to the<br />

square of the derivative of an arbitrary smooth function and then take the square root of that<br />

sum, the result is rarely antidifferentiable by reasonable methods. We know a few more<br />

functions that give “nice” integrands, but we are saving those for the exercises.<br />

(–8, –2)<br />

Figure 7.36 The graph of y x 13 has<br />

a vertical tangent line at the origin where<br />

dydx does not exist. (Example 3)<br />

(–2, –8)<br />

(2, 8)<br />

Figure 7.37 The curve in Figure 7.36<br />

plotted with x as a function of y. The<br />

tangent at the origin is now horizontal.<br />

(Example 3)<br />

x<br />

y<br />

x<br />

Vertical Tangents, Corners, and Cusps<br />

Sometimes a curve has a vertical tangent, corner, or cusp where the derivative we need to<br />

work with is undefined. We can sometimes get around such a difficulty in ways illustrated by<br />

the following examples.<br />

EXAMPLE 3<br />

A Vertical Tangent<br />

Find the length of the curve y x 13 between 8, 2 and 8, 2.<br />

SOLUTION<br />

The derivative<br />

d y<br />

1 1<br />

dx<br />

3 x23 <br />

3x<br />

23<br />

is not defined at x 0. Graphically, there is a vertical tangent at x 0 where the derivative<br />

becomes infinite (Figure 7.36). If we change to x as a function of y, the tangent<br />

at the origin will be horizontal (Figure 7.37) and the derivative will be zero instead of<br />

undefined. Solving y x 13 for x gives x y 3 , and we have<br />

L 2<br />

2<br />

x<br />

<br />

y ) dy 2<br />

1 3y 2 <br />

2 dy 17.26. Using NINT<br />

2 1 ( d d<br />

2<br />

Now try Exercise 25.

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