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This Week Sections 2.1-2.3,2.5,2.6 First homework due Tuesday night at 11:30 p.m. Average and instantaneous velocity worksheet Tuesday available at http://www.math.washington.edu/m124/ (under week 2) print it out before coming to class Professor Christopher Hoffman Math 124

This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

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Page 1: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

This Week

Sections 2.1-2.3,2.5,2.6First homework due Tuesday night at 11:30 p.m.Average and instantaneous velocity worksheet Tuesdayavailable at http://www.math.washington.edu/∼m124/(under week 2)print it out before coming to class

Professor Christopher Hoffman Math 124

Page 2: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Velocity

If an arrow is shot upward on the moon with a velocity of 58meters per second. It height in meters is given by

p(t) = 58t − 0.83t2.

1 Find the average velocity over the time intervals

[1,2], [1,1.5], [1,1.1], [1,1.01], and [1,1.001].

2 Find the instantaneous velocity at t = 1.

Professor Christopher Hoffman Math 124

Page 3: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Average Velocity between 1 and t

Average velocity is change in position divided by change intime.

Average velocity between time 1 and t isp(t)− p(1)

t − 1.

t p(t)−h(1)t−1

2 55.511.5 55.9251.1 56.257

1.01 56.33171.001 56.339

Professor Christopher Hoffman Math 124

Page 4: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Instantaneous Velocity

To see what happens as h approaches 0 we do a little algebra.

p(1 + h)− p(1)(1 + h)− 1

=58(1 + h)− 0.83(1 + h)2 − (58− 0.83(1)2)

h

=58 + 58h − 0.83(1 + 2h + h2)− (58− 0.83)

h

=58h − 1.66h − 0.83h2)

h= 56.34− 0.83h

As h approaches 0 the average velocity approaches 56.34.We say the instantaneous velocity at t = 1 is 56.34 and write

Instantaneous velocity = limh→0

p(1 + h)− p(1)h

= 56.34.

Professor Christopher Hoffman Math 124

Page 5: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Geometric Interpretation

p(1+h)−p(1)h is the slope of the secant line between (1,p(1)) and

(1 + h,p(1 + h)).

As h approaches 0 the secant lines approach the tangent lineat (1,p(1)).

The instantaneous velocity of 56.34 is the slope of the tangentline at (1,p(1)).

Professor Christopher Hoffman Math 124

Page 6: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Two Interpretations

All of our work over the next few weeks can be interpreted asfinding methods to determine the instantaneous velocity for anarbitrary position function.

Geometrically, our work can be interpreted as determining theslope of a tangent line for an arbitrary point on the graph of anarbitrary function.

In order to do this we first must discuss what we mean by thelimit of a function as we approach a point.

Professor Christopher Hoffman Math 124

Page 7: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limits

limx→a f (x) = L means that we can make the value of f (x)arbitrarily close to L by taking x sufficiently close to a but notequal to a.

In this picture limx→2 f (x) = 4.

Professor Christopher Hoffman Math 124

Page 8: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

limx→a f (x) does not depend on the value of f (a).In all of these pictures limx→0 f (x) = 1.

For most of the limits limx→a f (x) = L that we take in this coursef (a) will not be defined.

Professor Christopher Hoffman Math 124

Page 9: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Naive Idea

We will plug in small values of x to try to find

limx→0

sin(x)x

.

x sin(x)x

±1 .84147±1/2 .95885±.4 .973545±.3 .985067±.001 .99999

Based on this we might be tempted to say limx→0 sin(x)/x = 1.

Professor Christopher Hoffman Math 124

Page 10: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Graphical Interpretation

Looking at the graph of y = sin x/x we can see that

limx→0

sin(x)/x = 1.

Professor Christopher Hoffman Math 124

Page 11: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Professor Christopher Hoffman Math 124

Page 12: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Precise Definition of a Limit

The precise definition of a limit is contained in Section 2.4. Wewon’t cover this section in class. We will be content to knowlimits when we see them.

Professor Christopher Hoffman Math 124

Page 13: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Problematic Example

Findlimx→0

sin(π/x).

x sin(π)x

±1 0±1/2 0±1/3 0±1/10 0±1/100 0±1/n 0

Based on this we might be tempted to say

limx→0

sin(π/x) = 0.

Professor Christopher Hoffman Math 124

Page 14: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

But if we would have chosen

x =2

1 + 4n

then we would have seen a different behavior as the pointsapproached 0.For these values

sin(π/x) = sin(π

2+ 2nπ

)= 1.

Also if we would have chosen

x =2

3 + 4n

then we would have sin(π/x) = sin(3π

2 + 2nπ)= −1.

Professor Christopher Hoffman Math 124

Page 15: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

sin(π/x) oscillates between −1 and 1 infinitely often as x → 0.Thus

limx→0

sin(π/x)

does not exist.

Professor Christopher Hoffman Math 124

Page 16: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Check your work

On every limit calculation where you want to find

limx→a

f (x)

you should plug in values of x near a.

If the numbers you get are not close to your answer then youdid something wrong.

Professor Christopher Hoffman Math 124

Page 17: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Calculating limits graphically

Professor Christopher Hoffman Math 124

Page 18: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Calculating limits graphically

For the function h whose graph is given, state the value of eachquantity if it exists, If it does not exist, explain why

1 limx→−3− h(x)2 limx→−3+ h(x)3 limx→−3 h(x)4 h(−3)5 limx→0 h(x)6 h(0)7 limx→2 h(x)8 h(2)9 limx→5+ h(x)

10 limx→5− h(x)

Professor Christopher Hoffman Math 124

Page 19: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Calculating limits graphically

For the function h whose graph is given, state the value of eachquantity if it exists, If it does not exist, explain why

1 limx→−3− h(x) = 42 limx→−3+ h(x) = 43 limx→−3 h(x) = 44 h(−3) does not exist5 limx→0 h(x) does not exist6 h(0) = 17 limx→2 h(x) = 28 h(2) does not exist9 limx→5+ h(x) = 3

10 limx→5− h(x) does not exist.

Professor Christopher Hoffman Math 124

Page 20: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Infinite limits

Look at a graph of the function f (x) = ln(x).

The graph has a vertical asymptote at x = 0.As x → 0+ the function ln(x) gets more and more negative.We say

limx→0+

ln(x) = −∞.

Professor Christopher Hoffman Math 124

Page 21: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

For every n the line x = π/2 + nπ is a vertical asymptote.We can see that the one sided limits are

limx→π/2−

tan(x) =∞ and limx→π/2+

tan(x) = −∞.

Professor Christopher Hoffman Math 124

Page 22: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

The line x = a is a vertical asymptote of y = f (x) if at least oneof the following is true

limx→a f (x) =∞ or −∞limx→a+ f (x) =∞ or −∞limx→a− f (x) =∞ or −∞

Professor Christopher Hoffman Math 124

Page 23: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Calculating limits graphically

For the function R whose graph is given, state the following1 limx→2 R(x)2 limx→5 R(x)3 limx→−3− R(x)4 limx→−3+ R(x)5 The equations of the vertical asymptotes.

Professor Christopher Hoffman Math 124

Page 24: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Calculating limits graphically

1 limx→2 R(x) = −∞2 limx→5 R(x) =∞3 limx→−3 R(x) does not exist because

limx→−3− R(x) = −∞ while limx→−3+ R(x) =∞4 The equations of the vertical asymptotes are x = −3,

x = 2 and x = 5.

Professor Christopher Hoffman Math 124

Page 25: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

A function f is continuous at a if

limx→a

f (x) = f (a).

This definition requires three things to happen.

1 f (a) exists2 limx→a+ f (x) = f (a)3 limx→a− f (x) = f (a)

Professor Christopher Hoffman Math 124

Page 26: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Graphs of Continuous Functions

This function is continuous at every point except x = −2,2,4and 6.

Professor Christopher Hoffman Math 124

Page 27: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Continuous Functions

Any function defined by the following functions is continuous atevery point in its domain.

polynomialsroot functionstrigonometric functionsinverse trigonometric functionsexponential functions andlogarithmic functions

Professor Christopher Hoffman Math 124

Page 28: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Examples of Continuous Functions

All of the following functions are continuous wherever they aredefined.

f (x) = sin(

3+xx2+1

)g(t) = e3t/4+ln(2t)

r(x) =√

x3+12x−5

m(t) =√

3t + π tan−1(4 cos(t − π))

Professor Christopher Hoffman Math 124

Page 29: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Where are the following functions continuous1 x2 sin(x)

(x−3)(x+4) is continuous except when x = 3 and x = −4

2 ln(x2 − 1) is continuous except when −1 ≤ x ≤ 13 ex/(x−1) is continuous except when x = 1.

Professor Christopher Hoffman Math 124

Page 30: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Evaluating Limits of Continuous Functions

This is the easiest thing we will do all class all quarter.

If f (x) is continuous at a then

limx→a

f (x) = f (a).

Professor Christopher Hoffman Math 124

Page 31: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Evaluating Limits of Continuous Functions

Find the following limits.1 limx→3

√3πx+1x2−6 =

√9π+1

3

2 limy→−2sin√

3y+105y2−3 = sin(2)

17

3 limx→−2

√3cx+127cx+1 =

√12−6cx1−14c for any c < 2 and c 6= 1/14.

When evaluating limits in this course evaluating the function atthe point should always be your first approach.

If this fails then try pugging in numbers close to a. After youmake a guess you must justify your answer.

Professor Christopher Hoffman Math 124

Page 32: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Find

limh→0

(2 + h)3 − 8h

.

Plugging in h = 0 we get 00 .

limh→0

(2 + h)3 − 8h

= limh→0

(2 + h)3 − 8h

= limh→0

8 + 12h + 6h2 + h3 − 8h

= limh→0

12h + 6h2 + h3

h= lim

h→012 + 6h + h2

= 12.

If two functions agree everywhere except at one point a thenthe limits approaching a are the same.

Professor Christopher Hoffman Math 124

Page 33: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Findlimt→0

1/(7 + 3t)− 1/7t

.

Plugging in t = 0 we get 00 .

limt→0

1/(7 + 3t)− 1/7t

= limt→0

7− (7 + 3t)t(7 + 3t)(7)

= limt→0

−3tt(7 + 3t)7

= limt→0

−3(7 + 3t)7

= − 349.

Professor Christopher Hoffman Math 124

Page 34: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Rationalize the denominator

Findlim

t→16

16− t4−√

t.

Plugging in t = 16 we get 00 .

limt→16

16− t4−√

t= lim

t→16

(16− t)(4 +√

t)(4−

√t)(4 +

√t)

= limt→16

(16− t)(4 +√

t)(16− t)

= limt→16

4 +√

t

= 8

Professor Christopher Hoffman Math 124

Page 35: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Find

limx→0

(3x− 3

x3 + x

).

Plugging in x = 0 we get∞−∞.

limx→0

(3x− 3

x3 + x

)= lim

x→0

3(x2 + 1)− 3x3 + x

= limx→0

3x2

x3 + x

= limx→0

3xx2 + 1

=3 · 0

02 + 1= 0.

Professor Christopher Hoffman Math 124

Page 36: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Find

limx→3

x3 − 27x − 3

Plugging in x = 3 we get 00 .

limx→3

x3 − 27x − 3

= limx→0

(x − 3)(x2 + 3x + 9)x − 3

= limx→0

x2 + 3x + 9

= 27.

Professor Christopher Hoffman Math 124

Page 37: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limit Laws

Suppose c is a constant and the limits

limx→a

f (x) and limx→a

g(x)

exist. Then1 limx→a

[f (x) + g(x)

]= limx→a f (x) + limx→a g(x)

2 limx→a[f (x)− g(x)

]= limx→a f (x)− limx→a g(x)

3 limx→a[cf (x)

]= c limx→a f (x)

4 limx→a[f (x) · g(x)

]= limx→a f (x) · limx→a g(x)

5

limx→a

f (x)g(x)

=limx→a f (x)limx→a g(x)

if limx→a g(x) 6= 0

Professor Christopher Hoffman Math 124

Page 38: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Find

limt→−1

(cos(

3πt + 1

)− 3)(3(t + 1)2

√−4t).

This looks like a mess. Let’s look at the graph.

Professor Christopher Hoffman Math 124

Page 39: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Find

limt→−1

(cos(

3πt + 1

)− 3)(3(t + 1)2

√−4t).

This looks like a mess. Let’s look at the graph.

Professor Christopher Hoffman Math 124

Page 40: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Here is the graph of the function

g(t) =(

cos(3π

t + 1)− 3

)(3(t + 1)2

√−4t)

along with

f (t) = −2(3(t + 1)2√−4t) and h(t) = −4(3(t + 1)2

√−4t).

Notice that as t → −1 all three functions are approaching 0.

Professor Christopher Hoffman Math 124

Page 41: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

As these are continuous functions and defined at t = −1 we get

limt→−1

−2(3(t + 1)2√−4t) = −2(3(−1 + 1)

√−4(−1) = 0

and

limt→−1

−4(3(t + 1)2√−4t) = −4(3(−1 + 1)

√−4(−1) = 0.

The function that we are interested in

g(t) =(

cos(3π

t + 1)− 3

)(3(t + 1)2

√−4t)

is sandwiched in between so limt→−1 g(t) must be zero as well.

Professor Christopher Hoffman Math 124

Page 42: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Sandwich Theorem

This theorem makes the previous slide precise.

TheoremIf f (x) ≤ g(x) ≤ h(x) in some interval around a and

limx→a

(f (x)) = limx→a

(h(x)) = L

thenlimx→a

(g(x)) = L

Professor Christopher Hoffman Math 124

Page 43: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Findlim

x→14

x − 14√14 + x

.

First we plug in x = 14 and get

14− 14√14 + 14

=0√28

= 0.

As this is a continuous function defined at 14 we have

limx→14

x − 14√14 + x

= 0.

Professor Christopher Hoffman Math 124

Page 44: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limit Laws and Graphs

Here is the graph of a function f (x)

Find the following limits.

1 limx→2(f (x)2)

2 limx→−2(f (x)f (x + 3))3 limx→5 f (x)(2− f (x − 3))2

Professor Christopher Hoffman Math 124

Page 45: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Let f (x) = x−1(x+2)x2 .

1 Find all vertical asymptotes of f (x).2 Find the one sided limits of f (x) as x approaches the

asymptotes.

The function is a rational function so it is continuous at everypoint where it is defined.

It is defined everywhere the denominator is not zero, which iswhen x = 0 and x = −2.

It is important to keep signs right. We must be careful about theterms close to zero.

Professor Christopher Hoffman Math 124

Page 46: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

As x → 0+, x2 approaches 0 from the right. Also when x → 0−,x2 approaches 0 from the right.

As x → 0 the numerator x − 1 approaches −1 and x + 2approaches 2.

Thus as x → 0 from either side the numerator is negative andthe denominator is small and positive. The fraction is thus largeand negative. Because of this

limx→0

x − 1(x + 2)x2 = −∞.

Professor Christopher Hoffman Math 124

Page 47: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

As x → −2+ the numerator x − 1 approaches −3 and thedenominator approaches 0 from the positive side.

As the numerator is negative and the denominator is small andpositive the fraction is large and negative. Because of this

limx→−2+

x − 1(x + 2)x2 = −∞.

As x → −2− the numerator x − 1 approaches −3 and thedenominator approaches 0 from the negative side.

As the numerator is negative and the denominator is small andnegative the fraction is large and positive. Thus

limx→−2−

x − 1(x + 2)x2 =∞.

As the two one sided limits differ we have that

limx→−2

x − 1(x + 2)x2

does not exist.

Professor Christopher Hoffman Math 124

Page 48: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

When we graph the function we can see that there are verticalasymptotes at x = −2 and x = 0.

Professor Christopher Hoffman Math 124

Page 49: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

1 Find all vertical asymptotes of x−1(x+2)x2 .

2 Find the one sided limits of f (x) as x approaches theasymptotes.

The function is a rational function so it is continuous at everypoint where it is defined.It is defined everywhere the denominator is not zero, which iswhen x = 0 and x = −2.It is important to keep signs right. We must be careful about theterms close to zero.

Professor Christopher Hoffman Math 124

Page 50: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

As x → 0+, x2 approaches 0 from the right. Also when x → 0−,x2 approaches 0 from the right.

As x → 0 the numerator x − 1 approaches −1 and x + 2approaches 2.

Thus as x → 0 from either side the numerator is negative andthe denominator is small and positive. The fraction is thus largeand negative. Because of this

limx→0

x − 1(x + 2)x2 = −∞.

Professor Christopher Hoffman Math 124

Page 51: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

As x → −2+ the numerator x − 1 approaches −3 and thedenominator approaches 0 from the positive side.

As the numerator is negative and the denominator is small andpositive the fraction is large and negative. Because of this

limx→−2+

x − 1(x + 2)x2 = −∞.

As x → −2− the numerator x − 1 approaches −3 and thedenominator approaches 0 from the negative side.

As the numerator is negative and the denominator is small andnegative the fraction is large and positive. Thus

limx→−2−

x − 1(x + 2)x2 =∞.

As the two one sided limits differ we have that

limx→−2

x − 1(x + 2)x2

does not exist.

Professor Christopher Hoffman Math 124

Page 52: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limit Laws

Suppose c is a constant and the limits

limx→a

f (x) and limx→a

g(x)

exist. Then1 limx→a

[f (x) + g(x)

]= limx→a f (x) + limx→a g(x)

2 limx→a[f (x)− g(x)

]= limx→a f (x)− limx→a g(x)

3 limx→a[cf (x)

]= c limx→a f (x)

4 limx→a[f (x) · g(x)

]= limx→a f (x) · limx→a g(x)

5 limx→af (x)g(x) =

limx→a f (x)limx→a g(x) if limx→a g(x) 6= 0

Professor Christopher Hoffman Math 124

Page 53: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

To infinity and beyond

Professor Christopher Hoffman Math 124

Page 54: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Definition of Limits at∞

We writelim

x→∞f (x) = L

when the values of f (x) can be made arbitrarily close to L bytaking x sufficiently large. Similarly we write

limx→−∞

f (x) = L

when the values of f (x) can be made arbitrarily close to L bytaking sufficiently large negative values for x .

Professor Christopher Hoffman Math 124

Page 55: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limits at∞ Graphically

Consider the function f (x) = 3− 2e−x

As x gets large f (x) gets closer to 3. The graph of f (x) getscloser to the graph of y = 3 and we write

limx→∞

3− 2e−x = 3.

Professor Christopher Hoffman Math 124

Page 56: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limits at∞ Graphically

As x gets more and more negative 3− 2e−x gets more andmore negative as well. We write

limx→−∞

3− 2e−x = −∞.

Professor Christopher Hoffman Math 124

Page 57: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Horizontal Asymptotes

The line y = L is a horizontal asymptote of the curve y = f (x) ifeither

limx→∞

f (x) = L or limx→−∞

f (x) = L.

Thus y = π/2 and y = −π/2 are horizontal asymptotes and

limx→−∞

tan−1(x) = π/2 and limx→∞

tan−1(x) = −π/2

Professor Christopher Hoffman Math 124

Page 58: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limits of polynomials at∞

If r > 0 then limx→∞ x r =∞If r < 0 then limx→∞ x r = 0If r is even then limx→−∞ x r =∞If r is odd then limx→−∞ x r = −∞

Professor Christopher Hoffman Math 124

Page 59: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Limits Laws at∞

Suppose c is a constant and the limits

limx→∞

f (x) and limx→∞

g(x)

exist. Then

1 limx→∞[f (x) + g(x)

]= limx→∞ f (x) + limx→∞ g(x)

2 limx→∞[f (x)− g(x)

]= limx→∞ f (x)− limx→∞ g(x)

3 limx→∞[cf (x)

]= c limx→∞ f (x)

4 limx→∞[f (x) · g(x)

]= limx→∞ f (x) · limx→∞ g(x)

5 limx→∞f (x)g(x) =

limx→∞ f (x)limx→∞ g(x) if limx→∞ g(x) 6= 0

Professor Christopher Hoffman Math 124

Page 60: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Extended Real Numbers

When working with limits it is useful to use the extended realnumbers.

∞ ·∞ =∞∞+∞ =∞∞+ a =∞a∞ =∞ if a > 0a∞ = −∞ if a < 0∞−∞ =???

Professor Christopher Hoffman Math 124

Page 61: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Rational Functions

Find the following limits.limx→∞(−5x3 + 2(r − 1)x)

limx→∞x3/2+2πx7−2x

1

limx→−∞−5x3+2(r−1)x√

x4+1

Professor Christopher Hoffman Math 124

Page 62: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Polynomials

With polynomials the largest term dominates. To see this wefactor out the largest power of x .

limx→∞

(−5x3 + 2(r − 1)x) = limx→−∞

x3(−5 + 2(r − 1)/x2)

= limx→−∞

x3 limx→−∞

(−5 + 2(r − 1)/x2)

= (−∞)(−5)= ∞

Professor Christopher Hoffman Math 124

Page 63: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Divide by the largest power of the denominator

For functions like this we divide top and bottom by the largestpower of the denominator.

limx→∞

x3/2 + 2πx7 − 2xx2 − 1

= limx→∞

(1/x2)(x3/2 + 2πx7 − 2x)(1/x2)(x2 − 1)

= limx→∞

x−1/2 + 2πx5 − 2/x)1− 1/x2

=limx→∞(x−1/2 + 2πx5 − 2/x)

limx→∞(1− 1/x2)

=0 +∞+ 0

1− 0= ∞

Professor Christopher Hoffman Math 124

Page 64: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Divide by the largest power of the denominator

For this problem we want to divide by x2 =√

x4.

limx→−∞

−5x3 + 2(r − 1)x√x4 + 1

= limx→−∞

(1/x2)(−5x3 + 2(r − 1)x)(1/x2)

√x4 + 1

= limx→−∞

−5x + 2(r − 1)/x√1 + 1/x4

=limx→−∞(−5x + 2(r − 1)/x)

limx→−∞√

1 + 1/x4

=−5(−∞) + 0

1= −∞

Professor Christopher Hoffman Math 124

Page 65: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

limx→∞

(√x2 + 3x + 2− x

)We rationalize the numerator by multiplying the expression by

√x2 + 3x + 2 + x√x2 + 3x + 2 + x

limx→∞

(√x2 + 3x + 2− x

)= lim

x→∞

(√x2 + 3x + 2− x

) √x2 + 3x + 2 + x√x2 + 3x + 2 + x

= limx→∞

x2 + 3x + 2− x2√

x2 + 3x + 2 + x

= limx→∞

3x + 2√x2 + 3x + 2 + x

Professor Christopher Hoffman Math 124

Page 66: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Then we multiply numerator and denominator by 1/x .

limx→∞

(√x2 + 3x + 2− x

)= lim

x→∞

(3x + 2)(1/x)(√

x2 + 3x + 2 + x)(1/x)

= limx→∞

3 + 2/x(√

1 + 3/x + 2/x2 + 1)

=limx→∞(3 + 2/x)

limx→∞(√

1 + 3/x + 2/x2 + 1)

=3

1 + 1

=32

Professor Christopher Hoffman Math 124

Page 67: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

For all real numbers a > 0,b and c find

limx→∞

(√ax2 + bx + c − 5x

)and lim

x→−∞

(√ax2 + bx + c − 5x

)As in the previous problem we will multiply the expression times

√ax2 + bx + c + 5x√ax2 + bx + c + 5x

and then factor out the largest power of the denominator.

Professor Christopher Hoffman Math 124

Page 68: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

limx→∞

(√ax2 + bx + c − 5x

)= lim

x→∞(√

ax2 + bx + c − 5x)√

ax2 + bx + c + 5x√ax2 + bx + c + 5x

= limx→∞

ax2 + bx + c − 25x2√

ax2 + bx + c + 5x

= limx→∞

(a− 25)x2 + bx + c√ax2 + bx + c + 5x

= limx→∞

(1/x)(a− 25)x2 + bx + c)(1/x)(

√ax2 + bx + c + 5x)

= limx→∞

(a− 25)x + b + c/x√a + b/x + c/x2 + 5

=limx→∞((a− 25)x + b + c/x)

limx→∞(√

a + b/x + c/x2 + 5)

=limx→∞((a− 25)x + b + 0)√

aNow we have to break the answer up into cases.

Professor Christopher Hoffman Math 124

Page 69: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

limx→∞

(√ax2 + bx + c − 5x

)=

limx→∞((a− 25)x + b + 0)√a

If a > 25 then the leading term has a positive coefficient andthe limit approaches∞.

If a < 25 then the leading term has a negative coefficient andthe limit approaches∞.

If a = 25 then the limit becomes b/5.

The limits as x → −∞ are found the the same way.

Professor Christopher Hoffman Math 124

Page 70: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Findlim

x→∞

(√4x4 + 5x3 + 10− (2x2 + x)

).

Again we will multiply by the conjugate and divide by thehighest power of x in the denominator.

limx→∞

(√4x4 + 5x3 + 10− (2x2 + x)

)= lim

x→∞

(√4x4 + 5x3 + 10− (2x2 + x)

) √4x4 + 5x3 + 10 + (2x2 + x)√4x4 + 5x3 + 10 + (2x2 + x)

= limx→∞

(4x4 + 5x3 + 10)− (2x2 + x)2√

4x4 + 5x3 + 10 + (2x2 + x)

= limx→∞

(4x4 + 5x3 + 10)− (4x4 + 4x3 + x2)√4x4 + 5x3 + 10 + (2x2 + x)

= limx→∞

x3 − x2 + 10√4x4 + 5x3 + 10 + (2x2 + x)

Professor Christopher Hoffman Math 124

Page 71: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

= limx→∞

x − 1 + 10/x2

2

√4 + 5/x + 10/x4 + 2 + 1/x2

= ∞

Professor Christopher Hoffman Math 124

Page 72: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

1 Find all vertical asymptotes of x−1(x+2)x2 .

2 Find all horizontal asymptotes of x−1(x+2)x2 .

3 Find the one sided limits of f (x) as x approaches theasymptotes.

The function is a rational function so it is continuous at everypoint where it is defined.It is defined everywhere the denominator is not zero, which iswhen x = 0 and x = −2.It is important to keep signs right. We must be careful about theterms close to zero.

Professor Christopher Hoffman Math 124

Page 73: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

As x → 0+, x2 approaches 0 from the right. Also when x → 0−,x2 approaches 0 from the right.

As x → 0 the numerator x − 1 approaches −1 and x + 2approaches 2.

Thus as x → 0 from either side the numerator is negative andthe denominator is small and positive. The fraction is thus largeand negative. Because of this

limx→0

x − 1(x + 2)x2 = −∞.

Professor Christopher Hoffman Math 124

Page 74: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

As x → −2+ the numerator x − 1 approaches −3 and thedenominator approaches 0 from the positive side.

As the numerator is negative and the denominator is small andpositive the fraction is large and negative. Because of this

limx→−2+

x − 1(x + 2)x2 = −∞.

As x → −2− the numerator x − 1 approaches −3 and thedenominator approaches 0 from the negative side.

As the numerator is negative and the denominator is small andnegative the fraction is large and positive. Thus

limx→−2−

x − 1(x + 2)x2 =∞.

As the two one sided limits differ we have that

limx→−2

x − 1(x + 2)x2

does not exist.

Professor Christopher Hoffman Math 124

Page 75: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Sketch a graph of a function f (x) with the following properties.1 has horizontal asymptotes y = 0 and y = 42 has vertical asymptotes x = −3 and x = 43 limx→4 f (x) =∞4 limx→−3 f (x) does not exist.

Professor Christopher Hoffman Math 124

Page 76: This Week - University of Washingtonhoffman/124/week2...1 limx!3 p 3ˇx+1 x2 6 = p 9ˇ+1 3 2 limy! 2 sin p 3y+10 5y2 3 = sin(2) 17 3 limx! 2 p 3cx+12 7cx+1 = p 12 6cx 1 14c for any

Graphical limitsComposition of functions.Change of variables.

Professor Christopher Hoffman Math 124