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Solutions for Calculus Early Transcendentals, Metric Edition, 9th Edition by Stewart | All 16 Chapters Covered

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Solutions for Calculus Early Transcendentals, Metric Edition, 9th Edition by Stewart | All 16 Chapters Covered Unlock your understanding of advanced mathematics with the *Solutions Manual to Calculus: Early Transcendentals, Metric Edition, 9th Edition* by Stewart. This comprehensive solutions guide provides detailed, step-by-step answers to all exercises found in Stewart’s renowned calculus textbook, tailored specifically for the metric edition. Perfect for students and educators seeking clear explanations of calculus concepts such as limits, derivatives, integrals, and transcendental functions, this solutions manual enhances learning and supports exam preparation. With a focus on clarity and academic rigor, it is an essential resource for mastering single and multivariable calculus, preparing for university math courses, or excelling in STEM fields. *Ideal for calculus students, teachers, tutors, and anyone using Stewart’s Calculus 9th Edition, Metric Variant.* Solutions Manual, Calculus Early Transcendentals, Stewart 9th Edition, Metric Edition, Calculus Solutions, Calculus Textbook Answers, Step-by-Step Calculus, Math Study Guide, University Calculus, Advanced Mathematics, Single Variable Calculus, Multivariable Calculus, Calculus Exercises, Mathematics Solutions, Stewart Calculus Answers, Calculus Problem Solving #Calculus #StewartCalculus #EarlyTranscendentals #MetricEdition #CalculusSolutions #MathHelp #STEMEducation #StudyGuide #UniversityMath #Calculus9thEdition

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Calculus: Early Transcendentals 9/e
Metric Version [Stewart], Chapter 1-16




SOLUTIONS

,TABLE OF CONTENTS
1. FUNCTIONS AND MODELS.
2. LIMITS AND DERIVATIVES.
3. DIFFERENTIATION RULES.
4. APPLICATIONS OF DIFFERENTIATION.
5. INTEGRALS.
6. APPLICATIONS OF INTEGRATION.
7. TECHNIQUES OF INTEGRATION.
8. FURTHER APPLICATIONS OF INTEGRATION.
9. DIFFERENTIAL EQUATIONS.
10. PARAMETRIC EQUATIONS AND POLAR COORDINATES.
11. SEQUENCES, SERIES, AND POWER SERIES.
12. VECTORS AND THE GEOMETRY OF SPACE.
13. VECTOR FUNCTIONS.
14. PARTIAL DERIVATIVES.
15. MULTIPLE INTEGRALS.
16. VECTOR CALCULUS.

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1 FUNCTIONS AND MODELS
1.1 Four Ways to Represent a Function

√ √
1. The functions  () =  + 2 −  and () =  + 2 −  give exactly the same output values for every input value, so 
and  are equal.

2 −  ( − 1)
2.  () = = =  for  − 1 6= 0, so  and  [where () = ] are not equal because  (1) is undefined and
−1 −1
(1) = 1.

3. (a) The point (−2 2) lies on the graph of , so (−2) = 2. Similarly,  (0) = −2,  (2) = 1, and  (3)  25.

(b) Only the point (−4 3) on the graph has a ­value of 3, so the only value of  for which () = 3 is −4.

(c) The function outputs () are never greater than 3, so () ≤ 3 for the entire domain of the function. Thus, () ≤ 3 for
−4 ≤  ≤ 4 (or, equivalently, on the interval [−4 4]).

(d) The domain consists of all ­values on the graph of : { | −4 ≤  ≤ 4} = [−4 4]. The range of  consists of all the
­values on the graph of : { | −2 ≤  ≤ 3} = [−2 3].

(e) For any 1  2 in the interval [0 2], we have (1 )  (2 ). [The graph rises from (0 −2) to (2 1).] Thus, () is
increasing on [0 2].

4. (a) From the graph, we have  (−4) = −2 and (3) = 4.

(b) Since  (−3) = −1 and (−3) = 2, or by observing that the graph of  is above the graph of  at  = −3, (−3) is larger
than  (−3).

(c) The graphs of  and  intersect at  = −2 and  = 2, so  () = () at these two values of .

(d) The graph of  lies below or on the graph of  for −4 ≤  ≤ −2 and for 2 ≤  ≤ 3. Thus, the intervals on which
 () ≤ () are [−4 −2] and [2 3].

(e)  () = −1 is equivalent to  = −1, and the points on the graph of  with ­values of −1 are (−3 −1) and (4 −1), so
the solution of the equation  () = −1 is  = −3 or  = 4.

(f) For any 1  2 in the interval [−4 0], we have (1 )  (2 ). Thus, () is decreasing on [−4 0].

(g) The domain of  is { | −4 ≤  ≤ 4} = [−4 4]. The range of  is { | −2 ≤  ≤ 3} = [−2 3].

(h) The domain of  is { | −4 ≤  ≤ 3} = [−4 3]. Estimating the lowest point of the graph of  as having coordinates
(0 05), the range of  is approximately { | 05 ≤  ≤ 4} = [05 4].

5. From Figure 1 in the text, the lowest point occurs at about ( ) = (12 −85). The highest point occurs at about (17 115).

Thus, the range of the vertical ground acceleration is −85 ≤  ≤ 115. Written in interval notation, the range is [−85 115].


°
c 2021 Cengage Learning. All Rights Reserved. May not be scanned, copied, or duplicated, or posted to a publicly accessible website, in whole or in part. 9




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10 ¤ CHAPTER 1 FUNCTIONS AND MODELS

6. Example 1: A car is driven at 60 mih for 2 hours. The distance 
traveled by the car is a function of the time . The domain of the
function is { | 0 ≤  ≤ 2}, where  is measured in hours. The range
of the function is { | 0 ≤  ≤ 120}, where  is measured in miles.


Example 2: At a certain university, the number of students  on
campus at any time on a particular day is a function of the time  after
midnight. The domain of the function is { | 0 ≤  ≤ 24}, where  is
measured in hours. The range of the function is { | 0 ≤  ≤ },
where  is an integer and  is the largest number of students on
campus at once.

Example 3: A certain employee is paid $800 per hour and works a pay

maximum of 30 hours per week. The number of hours worked is 240
238
rounded down to the nearest quarter of an hour. This employee’s 236

gross weekly pay  is a function of the number of hours worked .
4
The domain of the function is [0 30] and the range of the function is 2
{0 200 400     23800 24000}. 0 0.25 0.50 0.75 29.50 29.75 30 hours


7. We solve 3 − 5 = 7 for : 3 − 5 = 7 ⇔ −5 = −3 + 7 ⇔  = 35  − 75 . Since the equation determines exactly

one value of  for each value of , the equation defines  as a function of .

8. We solve 32 − 2 = 5 for : 32 − 2 = 5 ⇔ −2 = −32 + 5 ⇔  = 32 2 − 52 . Since the equation determines

exactly one value of  for each value of , the equation defines  as a function of .

9. We solve 2 + ( − 3)2 = 5 for : 2 + ( − 3)2 = 5 ⇔ ( − 3)2 = 5 − 2 ⇔ ⇔  − 3 = ± 5 − 2

 = 3 ± 5 − 2 . Some input values  correspond to more than one output . (For instance,  = 1 corresponds to  = 1 and
to  = 5.) Thus, the equation does not define  as a function of .

10. We solve 2 + 5 2 = 4 for : 2 + 5 2 = 4 ⇔ 5 2 + (2)  − 4 = 0 ⇔

√ √
−2 ± (2)2 − 4(5)(−4) −2 ± 42 + 80 − ± 2 + 20
= = = (using the quadratic formula). Some input
2(5) 10 5

values  correspond to more than one output . (For instance,  = 4 corresponds to  = −2 and to  = 25.) Thus, the

equation does not define  as a function of .

11. We solve ( + 3)3 + 1 = 2 for : ( + 3)3 + 1 = 2 ⇔ ( + 3)3 = 2 − 1 ⇔  + 3 = 3
2 − 1 ⇔

3
 = −3 + 2 − 1. Since the equation determines exactly one value of  for each value of , the equation defines  as a
function of .



°
c 2021 Cengage Learning. All Rights Reserved. May not be scanned, copied, or duplicated, or posted to a publicly accessible website, in whole or in part.




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