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5128_Ch03_pp098-184

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Section 3.6 Chain Rule 149<br />

Composite f ˚ g<br />

Rate of change at<br />

x is f'(g(x)) • g'(x)<br />

Figure 3.42 Rates of change multiply:<br />

the derivative of f g at x is the derivative<br />

of f at the point gx) times the derivative<br />

of g at x.<br />

x<br />

g<br />

Rate of change<br />

at x is g'(x)<br />

u g(x)<br />

f<br />

Rate of change<br />

at g(x) is f'(g(x))<br />

y f(u) f(g(x))<br />

RULE 8<br />

The Chain Rule<br />

If f is differentiable at the point u gx, and g is differentiable at x, then the<br />

composite function f gx f gx is differentiable at x, and<br />

f gx f gx • gx.<br />

In Leibniz notation, if y f u and u gx, then<br />

d y dy<br />

• d u<br />

,<br />

dx<br />

d u dx<br />

where dydu is evaluated at u gx.<br />

It would be tempting to try to prove the Chain Rule by writing<br />

y <br />

<br />

x<br />

y<br />

u<br />

• u<br />

<br />

x<br />

(a true statement about fractions with nonzero denominators) and taking the limit as<br />

x→0. This is essentially what is happening, and it would work as a proof if we knew<br />

that Du, the change in u, was nonzero; but we do not know this. A small change in x could<br />

conceivably produce no change in u. An air-tight proof of the Chain Rule can be constructed<br />

through a different approach, but we will omit it here.<br />

EXAMPLE 3<br />

Applying the Chain Rule<br />

An object moves along the x-axis so that its position at any time t 0 is given by<br />

xt cos t 2 1. Find the velocity of the object as a function of t.<br />

SOLUTION<br />

We know that the velocity is dxdt. In this instance, x is a composite function:<br />

x cos u and u t 2 1. We have<br />

By the Chain Rule,<br />

dx<br />

sin u<br />

d u<br />

x cos (u)<br />

d u<br />

2t.<br />

dt<br />

u t 2 1<br />

d x dx<br />

• d u<br />

<br />

dt<br />

d u dt<br />

sin u • 2t<br />

sin t 2 1 • 2t<br />

2t sin t 2 1. Now try Exercise 9.

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