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Packet #24 The Fundamental Theorem of Calculus

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1 Packet #24 The Fundamental Theorem of Calculus
Math 180 Packet #24 The Fundamental Theorem of Calculus

2 In packet #22, we saw how to visualize an estimation of distance traveled using velocity samples at 5-second intervals.

3 In packet #22, we saw how to visualize an estimation of distance traveled using velocity samples at 5-second intervals.

4 In packet #22, we saw how to visualize an estimation of distance traveled using velocity samples at 5-second intervals.

5 In packet #22, we saw how to visualize an estimation of distance traveled using velocity samples at 5-second intervals.

6 In packet #22, we saw how to visualize an estimation of distance traveled using velocity samples at 5-second intervals.

7 To get a more accurate estimation, we could sample every second.

8 To get a more accurate estimation, we could sample every second.

9 To get a more accurate estimation, we could sample every second.

10 To get a more accurate estimation, we could sample every second.

11 What if we could sample every instant?

12 What if we could sample every instant?

13 What if we could sample every instant?

14 What if we could sample every instant?

15 The Fundamental Theorem of Calculus, Part 2 (also called The Evaluation Theorem) If 𝑓 is continuous on π‘Ž,𝑏 and 𝐹 is any antiderivative of 𝑓 on π‘Ž,𝑏 , then 𝒂 𝒃 𝒇 𝒙 𝒅𝒙=𝑭 𝒃 βˆ’π‘­(𝒂)

16 Ex 1. Evaluate. 0 πœ‹ cos π‘₯ 𝑑π‘₯

17 Notation: 𝐹 π‘₯ π‘Ž 𝑏 = 𝐹 π‘₯ π‘Ž 𝑏 =𝐹 𝑏 βˆ’πΉ π‘Ž

18 Ex 2. Evaluate. βˆ’ πœ‹ 4 0 sec π‘₯ tan π‘₯ 𝑑π‘₯ 1 4 3 2 π‘₯ βˆ’ 4 π‘₯ 2 𝑑π‘₯ βˆ’3 βˆ’2 𝑑π‘₯ π‘₯+1

19 Let’s go back to the velocity function, 𝑣 𝑑
Let’s go back to the velocity function, 𝑣 𝑑 . Consider the area under 𝑣 𝑑 from 𝑑=0 to 𝑑=π‘₯ (where π‘₯ is a variable here). This area represents the change in position over that time interval. Note that the area is a function of π‘₯.

20 The Fundamental Theorem of Calculus, Part 1 If 𝑓 is continuous on π‘Ž,𝑏 , then 𝐹 π‘₯ = π‘Ž π‘₯ 𝑓 𝑑 𝑑𝑑 is continuous on π‘Ž,𝑏 and differentiable on π‘Ž,𝑏 and its derivative is 𝑓 π‘₯ : 𝑭 β€² 𝒙 = 𝒅 𝒅𝒙 𝒂 𝒙 𝒇 𝒕 𝒅𝒕 =𝒇 𝒙

21 Ex 3. Use the Fundamental Theorem to find 𝑑𝑦 𝑑π‘₯
Ex 3. Use the Fundamental Theorem to find 𝑑𝑦 𝑑π‘₯ . 𝑦= π‘Ž π‘₯ 𝑑 3 +1 𝑑𝑑 𝑦= π‘₯ 5 3𝑑 sin 𝑑 𝑑𝑑 𝑦= 1 π‘₯ 2 cos 𝑑 𝑑𝑑 𝑦= 1+3 π‘₯ 𝑒 𝑑 𝑑𝑑

22 By the way, here’s another way to get intuition about the FTOC, Part 1…

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28 What is the rate at which the area is changing. That is, what is 𝐹′(π‘₯)
What is the rate at which the area is changing? That is, what is 𝐹′(π‘₯)? Let’s estimate it:

29 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ actual change in area β‰ˆ 𝑓 π‘₯ β‹…β„Ž estimated change in area 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž β‰ˆπ‘“ π‘₯ lim β„Žβ†’0 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž =𝑓 π‘₯ 𝐹 β€² π‘₯ =𝑓 π‘₯ So, 𝒅 𝒅𝒙 𝒂 𝒙 𝒇 𝒕 𝒅𝒕 =𝒇 𝒙 .

30 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ actual change in area β‰ˆ 𝑓 π‘₯ β‹…β„Ž estimated change in area 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž β‰ˆπ‘“ π‘₯ lim β„Žβ†’0 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž =𝑓 π‘₯ 𝐹 β€² π‘₯ =𝑓 π‘₯ So, 𝒅 𝒅𝒙 𝒂 𝒙 𝒇 𝒕 𝒅𝒕 =𝒇 𝒙 .

31 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ actual change in area β‰ˆ 𝑓 π‘₯ β‹…β„Ž estimated change in area 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž β‰ˆπ‘“ π‘₯ lim β„Žβ†’0 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž =𝑓 π‘₯ 𝐹 β€² π‘₯ =𝑓 π‘₯ So, 𝒅 𝒅𝒙 𝒂 𝒙 𝒇 𝒕 𝒅𝒕 =𝒇 𝒙 .

32 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ actual change in area β‰ˆ 𝑓 π‘₯ β‹…β„Ž estimated change in area 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž β‰ˆπ‘“ π‘₯ lim β„Žβ†’0 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž =𝑓 π‘₯ 𝐹 β€² π‘₯ =𝑓 π‘₯ So, 𝒅 𝒅𝒙 𝒂 𝒙 𝒇 𝒕 𝒅𝒕 =𝒇 𝒙 .

33 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ actual change in area β‰ˆ 𝑓 π‘₯ β‹…β„Ž estimated change in area 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž β‰ˆπ‘“ π‘₯ lim β„Žβ†’0 𝐹 π‘₯+β„Ž βˆ’πΉ π‘₯ β„Ž =𝑓 π‘₯ 𝐹 β€² π‘₯ =𝑓 π‘₯ So, 𝒅 𝒅𝒙 𝒂 𝒙 𝒇 𝒕 𝒅𝒕 =𝒇 𝒙 .

34 𝒅 𝒅𝒙 𝒂 𝒙 𝒇 𝒕 𝒅𝒕 =𝒇 𝒙 In other words, the rate at which the area is changing is equal to the function value of 𝑓 at π‘₯.

35 The Net Change Theorem The net change of 𝐹(π‘₯) over π‘Ž,𝑏 is: 𝐹 𝑏 βˆ’πΉ π‘Ž = π‘Ž 𝑏 𝐹 β€² π‘₯ 𝑑π‘₯ ex: The net change in position (displacement) from 𝑑=2 to 𝑑=3 is 𝑠 3 βˆ’π‘  2 . We could also calculate net change in position using the integral 2 3 𝑣(𝑑) 𝑑𝑑. If you instead wanted total distance traveled from 𝑑=2 to 𝑑=3, you would calculate 2 3 𝑣 𝑑 𝑑𝑑.

36 The Net Change Theorem The net change of 𝐹(π‘₯) over π‘Ž,𝑏 is: 𝐹 𝑏 βˆ’πΉ π‘Ž = π‘Ž 𝑏 𝐹 β€² π‘₯ 𝑑π‘₯ ex: The net change in position (displacement) from 𝑑=2 to 𝑑=3 is 𝑠 3 βˆ’π‘  2 . We could also calculate net change in position using the integral 2 3 𝑣(𝑑) 𝑑𝑑. If you instead wanted total distance traveled from 𝑑=2 to 𝑑=3, you would calculate 2 3 𝑣 𝑑 𝑑𝑑.

37 The Net Change Theorem The net change of 𝐹(π‘₯) over π‘Ž,𝑏 is: 𝐹 𝑏 βˆ’πΉ π‘Ž = π‘Ž 𝑏 𝐹 β€² π‘₯ 𝑑π‘₯ ex: The net change in position (displacement) from 𝑑=2 to 𝑑=3 is 𝑠 3 βˆ’π‘  2 . We could also calculate net change in position using the integral 2 3 𝑣(𝑑) 𝑑𝑑. If you instead wanted total distance traveled from 𝑑=2 to 𝑑=3, you would calculate 2 3 𝑣 𝑑 𝑑𝑑.

38 The Net Change Theorem The net change of 𝐹(π‘₯) over π‘Ž,𝑏 is: 𝐹 𝑏 βˆ’πΉ π‘Ž = π‘Ž 𝑏 𝐹 β€² π‘₯ 𝑑π‘₯ ex: The net change in position (displacement) from 𝑑=2 to 𝑑=3 is 𝑠 3 βˆ’π‘  2 . We could also calculate net change in position using the integral 2 3 𝑣(𝑑) 𝑑𝑑. If you instead wanted total distance traveled from 𝑑=2 to 𝑑=3, you would calculate 2 3 𝑣 𝑑 𝑑𝑑.

39 ex: The net change in the volume 𝑉 𝑑 of water in a tank is 𝑉 𝑑 2 βˆ’π‘‰ 𝑑 1 = 𝑑 1 𝑑 2 𝑉 β€² 𝑑 𝑑𝑑. ex: The net change in population 𝑛 𝑑 is 𝑛 𝑑 2 βˆ’π‘› 𝑑 1 = 𝑑 1 𝑑 2 𝑛 β€² 𝑑 𝑑𝑑.

40 Ex 4. Suppose the velocity function of a particle is 𝑣 𝑑 = 𝑑 2 βˆ’π‘‘βˆ’6 (in meters per second). Find the displacement of the particle during the time period 1≀𝑑≀4.

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42 Now find the distance traveled by the particle during the same time period 1≀𝑑≀4.

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