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412 Chapter 7 Applications of Definite Integrals<br />

7.4<br />

What you’ll learn about<br />

• A Sine Wave<br />

• Length of a Smooth Curve<br />

• Vertical Tangents, Corners, and<br />

Cusps<br />

. . . and why<br />

The length of a smooth curve can<br />

be found using a definite integral.<br />

[0, 2] by [–2, 2]<br />

Figure 7.32 One wave of a sine curve<br />

has to be longer than 2p.<br />

y<br />

x y √<br />

2<br />

k + 2<br />

k<br />

Q<br />

y k<br />

y = sin x<br />

Lengths of Curves<br />

A Sine Wave<br />

How long is a sine wave (Figure 7.32)?<br />

The usual meaning of wavelength refers to the fundamental period, which for y sin x<br />

is 2p. But how long is the curve itself? If you straightened it out like a piece of string<br />

along the positive x-axis with one end at 0, where would the other end be?<br />

EXAMPLE 1<br />

The Length of a Sine Wave<br />

What is the length of the curve y sin x from x 0 to x 2p?<br />

SOLUTION<br />

We answer this question with integration, following our usual plan of breaking the whole<br />

into measurable parts. We partition 0, 2p into intervals so short that the pieces of curve<br />

(call them “arcs”) lying directly above the intervals are nearly straight. That way, each<br />

arc is nearly the same as the line segment joining its two ends and we can take the length<br />

of the segment as an approximation to the length of the arc.<br />

Figure 7.33 shows the segment approximating the arc above the subinterval x k1 , x k .<br />

The length of the segment is Δx 2 k . Δy 2 k The sum<br />

Δx k 2 Δy 2 k<br />

over the entire partition approximates the length of the curve. All we need now is to find<br />

the limit of this sum as the norms of the partitions go to zero. That’s the usual plan, but<br />

this time there is a problem. Do you see it?<br />

The problem is that the sums as written are not Riemann sums. They do not have the<br />

form f c k Δx. We can rewrite them as Riemann sums if we multiply and divide each<br />

square root by Δx k .<br />

O<br />

P<br />

x k–1<br />

x k<br />

Figure 7.33 The line segment approximating<br />

the arc PQ of the sine curve above<br />

the subinterval x k1 , x k . (Example 1)<br />

Group Exploration<br />

Later in this section we will use an integral<br />

to find the length of the sine wave<br />

with great precision. But there are ways<br />

to get good approximations without<br />

integrating. Take five minutes to come<br />

up with a written estimate of the curve’s<br />

length. No fair looking ahead.<br />

x k<br />

x<br />

x k<br />

2 y 2 k x k 2 y k<br />

<br />

2 x<br />

x<br />

k<br />

y<br />

x<br />

1 ( <br />

k<br />

)<br />

2<br />

k<br />

k<br />

This is better, but we still need to write the last square root as a function evaluated at<br />

some c k in the kth subinterval. For this, we call on the Mean Value Theorem for differentiable<br />

functions (Section 4.2), which says that since sin x is continuous on x k1 , x k <br />

and is differentiable on x k1 , x k there is a point c k in x k1 , x k at which Δy k Δx k <br />

sin c k (Figure 7.34). That gives us<br />

1 si nc k <br />

2 Δx k ,<br />

which is a Riemann sum.<br />

Now we take the limit as the norms of the subdivisions go to zero and find that the<br />

length of one wave of the sine function is<br />

2p<br />

1 si nx 2 dx 2p<br />

1 cos 2 x dx 7.64. Using NINT<br />

0<br />

0<br />

How close was your estimate? Now try Exercise 9.<br />

x k

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