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

A five star textbook for college calculus

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224 Chapter 3 Differentiation Rules

We know that if y − f sxd, then the derivative dyydx can be interpreted as the rate of

change of y with respect to x. In this section we examine some of the applications of this

idea to physics, chemistry, biology, economics, and other sciences.

Let’s recall from Section 2.7 the basic idea behind rates of change. If x changes from

x 1 to x 2 , then the change in x is

and the corresponding change in y is

Dx − x 2 2 x 1

Dy − f sx 2 d 2 f sx 1 d

The difference quotient

Dy

Dx − f sx 2d 2 f sx 1 d

x 2 2 x 1

y

P{⁄, fl}

Q{¤, ‡}

Îx

Îy

0 ⁄ ¤

x

m PQ average rate of change

m=fª(⁄)=instantaneous rate

of change

FIGURE 1

is the average rate of change of y with respect to x over the interval fx 1 , x 2 g and can

be interpreted as the slope of the secant line PQ in Figure 1. Its limit as Dx l 0 is the

derivative f 9sx 1 d, which can therefore be interpreted as the instantaneous rate of change

of y with respect to x or the slope of the tangent line at Psx 1 , f sx 1 dd. Using Leibniz notation,

we write the process in the form

dy

dx − lim Dy

Dx l 0 Dx

Whenever the function y − f sxd has a specific interpretation in one of the sciences, its

derivative will have a specific interpretation as a rate of change. (As we discussed in Section

2.7, the units for dyydx are the units for y divided by the units for x.) We now look

at some of these interpretations in the natural and social sciences.

Physics

If s − f std is the position function of a particle that is moving in a straight line, then DsyDt

represents the average velocity over a time period Dt, and v − dsydt represents the instantaneous

velocity (the rate of change of displacement with respect to time). The instantaneous

rate of change of velocity with respect to time is acceleration: astd − v9std − s99std.

This was discussed in Sections 2.7 and 2.8, but now that we know the differentiation

formulas, we are able to solve problems involving the motion of objects more easily.

ExamplE 1 The position of a particle is given by the equation

s − f std − t 3 2 6t 2 1 9t

where t is measured in seconds and s in meters.

(a) Find the velocity at time t.

(b) What is the velocity after 2 s? After 4 s?

(c) When is the particle at rest?

(d) When is the particle moving forward (that is, in the positive direction)?

(e) Draw a diagram to represent the motion of the particle.

(f) Find the total distance traveled by the particle during the first five seconds.

(g) Find the acceleration at time t and after 4 s.

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