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Part 1 3.4: The Derivative as a Rate of Change Part 1: Motion Along a Line MATH 165: Calculus I Department of Mathematics Iowa State University Paul J. Barloon MATH 165 Section 3.4

3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

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Page 1: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1

3.4: The Derivative as a Rate of Change

Part 1: Motion Along a Line

MATH 165: Calculus I

Department of Mathematics

Iowa State University

Paul J. Barloon

MATH 165 Section 3.4

Page 2: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Classic Example (Yet Again)

Let’s look once again atthe stoplight problem.

The graph actually showsthe car’s positionaccording to the positionfunction s(t) = 2t2.

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 3: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Classic Example (Yet Again)

Let’s look once again atthe stoplight problem.

The graph actually showsthe car’s positionaccording to the positionfunction s(t) = 2t2.

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 4: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Displacement

We found the averagevelocity over the first 30seconds by first finding thedisplacement of the carover that period:

1800 = s(0 + 30)� s(0)

In general, displacementover a time period �t isgiven by:

�s = s(t +�t)� s(t)

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 5: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Displacement

We found the averagevelocity over the first 30seconds by first finding thedisplacement of the carover that period:

1800 = s(0 + 30)� s(0)

In general, displacementover a time period �t isgiven by:

�s = s(t +�t)� s(t)

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 6: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Displacement

We found the averagevelocity over the first 30seconds by first finding thedisplacement of the carover that period:

1800 = s(0 + 30)� s(0)

In general, displacementover a time period �t isgiven by:

�s = s(t +�t)� s(t)

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 7: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Average Velocity

Then, the average velocitywas:

1800

30=

s(0 + 30)� s(0)

30� 0

In general,average velocity over aperiod �t is given by:

�s

�t=

s(t +�t)� s(t)

�t

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 8: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Average Velocity

Then, the average velocitywas:

1800

30=

s(0 + 30)� s(0)

30� 0

In general,average velocity over aperiod �t is given by:

�s

�t=

s(t +�t)� s(t)

�t

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 9: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Average Velocity

Then, the average velocitywas:

1800

30=

s(0 + 30)� s(0)

30� 0

In general,average velocity over aperiod �t is given by:

�s

�t=

s(t +�t)� s(t)

�t

5 10 15 20 25 30

300

600

900

1,200

1,500

1,800 (30,1800)

(10,200)

(0,0)

time(sec)

distance(feet)

MATH 165 Section 3.4

Page 10: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Velocity

We then let �t “get small” to find the velocity function for thecar.

Definition

If a body’s position at time t is given by s = f (t), then the body’svelocity (or instantaneous velocity) at time t is:

v(t) =ds

dt= lim

�t!0

f (t +�t)� f (t)

�t

MATH 165 Section 3.4

Page 11: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

EXAMPLE 1a: Suppose that a body’s position along a straightline is given by the function s(t) = t2 � 3t + 2 for 0 t 2.

What is the body’s displacement over the given interval?

MATH 165 Section 3.4

Page 12: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph
Page 13: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

EXAMPLE 1b: Suppose that a body’s position along a straightline is given by the function s(t) = t2 � 3t + 2 for 0 t 2.

What is the body’s average velocity over the given interval?

MATH 165 Section 3.4

Page 14: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

EXAMPLE 1c: Suppose that a body’s position along a straightline is given by the function s(t) = t2 � 3t + 2 for 0 t 2.

What is the body’s instantaneous velocity at t = 1 second?

MATH 165 Section 3.4

Page 15: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

EXAMPLE 1d: Suppose that a body’s position along a straightline is given by the function s(t) = t2 � 3t + 2 for 0 t 2.

At what time does the body change direction?

MATH 165 Section 3.4

Page 16: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Speed

As we just saw, the sign of a velocity value is meaningful.Sometimes, though, we are interested in the unsigned rate atwhich position is changing.

Definition

Speed is the absolute value of velocity.

Speed = |v(t)| =����ds

dt

����

MATH 165 Section 3.4

Page 17: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

EXAMPLE 1e: Suppose that a body’s position along a straightline is given by the function s(t) = t2 � 3t + 2 for 0 t 2.

What is the body’s speed at t = 1 second?

MATH 165 Section 3.4

Page 18: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Acceleration

The (instantaneous) rate at which velocity changes is a body’sacceleration.

Definition

If a body’s position at time t is given by s = f (t), then the body’sacceleration at time t is:

a(t) =dv

dt=

d2s

dt2

ora(t) = v 0(t) = s 00(t)

MATH 165 Section 3.4

Page 19: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

EXAMPLE 1f: Suppose that a body’s position along a straightline is given by the function s(t) = t2 � 3t + 2 for 0 t 2.

What is the body’s acceleration at t = 1 second?

MATH 165 Section 3.4

Page 20: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

Quiz Yourself

The graph at the right show abody’s velocity at time t.

What is the body’s accelerationat time t = 2 seconds?

A) 4

B) 2

C) 0

D) �2

E) �4

MATH 165 Section 3.4

Page 21: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 1 Motion Along a Line

The End

MATH 165 Section 3.4

Page 22: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2

3.4: The Derivative as a Rate of Change

Part 2: Related Rates

MATH 165: Calculus I

Department of Mathematics

Iowa State University

Paul J. Barloon

MATH 165 Section 3.4

Page 23: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

Introduction

In our car (and generic “body”) examples, the independentvariable has always been time (t):

Position = s(t)

Velocity = v(t) = s 0(t)

Acceleration = a(t) = v 0(t) = s 00(t)

We now consider situations in which the independent variable issomething else . . .

MATH 165 Section 3.4

Page 24: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

Introduction

In our car (and generic “body”) examples, the independentvariable has always been time (t):

Position = s(t)

Velocity = v(t) = s 0(t)

Acceleration = a(t) = v 0(t) = s 00(t)

We now consider situations in which the independent variable issomething else . . .

MATH 165 Section 3.4

Page 25: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

Introduction

In our car (and generic “body”) examples, the independentvariable has always been time (t):

Position = s(t)

Velocity = v(t) = s 0(t)

Acceleration = a(t) = v 0(t) = s 00(t)

We now consider situations in which the independent variable issomething else . . .

MATH 165 Section 3.4

Page 26: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

Introduction

In our car (and generic “body”) examples, the independentvariable has always been time (t):

Position = s(t)

Velocity = v(t) = s 0(t)

Acceleration = a(t) = v 0(t) = s 00(t)

We now consider situations in which the independent variable issomething else . . .

MATH 165 Section 3.4

Page 27: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

Introduction

In our car (and generic “body”) examples, the independentvariable has always been time (t):

Position = s(t)

Velocity = v(t) = s 0(t)

Acceleration = a(t) = v 0(t) = s 00(t)

We now consider situations in which the independent variable issomething else . . .

MATH 165 Section 3.4

Page 28: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

A Cube

The volume of a cube may beconsidered to be a function ofthe length of the sides l :

V (l) = l3

So, it makes sense to ask aboutthe instantaneous rate of changeof the volume with respect to theside length:

dV

dl=

d

dl[l3] = 3l2

MATH 165 Section 3.4

Page 29: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

A Cube

The volume of a cube may beconsidered to be a function ofthe length of the sides l :

V (l) = l3

So, it makes sense to ask aboutthe instantaneous rate of changeof the volume with respect to theside length:

dV

dl=

d

dl[l3] = 3l2

MATH 165 Section 3.4

Page 30: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

EXAMPLE 1a: At what ratedoes the volume of a cubechange with respect to sidelength when l = 5 ft?

MATH 165 Section 3.4

Page 31: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

EXAMPLE 1b: Byapproximately how much doesthe volume increase when theside length changes from 5 to 5.1feet?

MATH 165 Section 3.4

Page 32: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

Note that this isjust the slope of thetangent at l = 5when volume isgraphed on thevertical axis andside length on thehorizontal:

MATH 165 Section 3.4

Page 33: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

Quiz Yourself

Suppose that a spill is forming a circular oil slick around a leakingtanker. How fast does the area of the slick change with respect toits radius when that radius is 90 feet?

A) 45⇡ ft2/ft

B) 90⇡ ft2/ft

C) 180⇡ ft2/ft

D) 810⇡ ft2/ft

E) 8100⇡ ft2/ft

MATH 165 Section 3.4

Page 34: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph
Page 35: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

Part 2 Related Rates

The End

MATH 165 Section 3.4

Page 36: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

MATH 165 14–19,32–37 Warm-Up Question – Sep. 14, 2018

Suppose that a body’s position along a straight line

is given by the function s(t) = t2 � 3t + 2 for

0 t 2 (t in seconds).

At what time(s) does the body change direction?

A) t = 0 secs

B) t = 1 sec

C) t = 32 secs

D) t = 2 secs

E) t = 1 and t = 2 secs

F) The body does not change direction

Page 37: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph
Page 38: 3.4: The Derivative as a Rate of Change - Part 1: Motion ... · Part 1 Motion Along a Line Classic Example (Yet Again) Let’s look once again at the stoplight problem. The graph

MATH 165 14–19,32–37 Warm-Up Question – Sep. 14, 2018

Suppose that a body’s position along a straight line

is given by the function s(t) = t2 � 3t + 2 for

0 t 2 (t in seconds).

At what time(s) does the body change direction?

A) t = 0 secs

B) t = 1 sec

*C) t = 32 secs

D) t = 2 secs

E) t = 1 and t = 2 secs

F) The body does not change direction