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CALCULUS SEM2Q3W7&W8 ISRAEL (KURT) Final-Ver

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Kurt Kareem I. Israel
Teacher Ferdinand Corpuz
Grade 11 – Lorenz
Date Answered: March 25, 2021
Basic Calculus
Semester 2 – Quarter 3 – Weeks 7 - 8
Module 3 – The Derivatives
LESSON 1:
The Chain Rule
Activity 1: What I Know (Page 3)
1. B.
ο‚·
ο‚·
ο‚·
ο‚·
𝑦 = √𝑑 3 + 1 when 𝑑 = 2
1
𝑑
(𝑑 3 + 1)
3
2√𝑑 +1 𝑑π‘₯
𝑑
(𝑑 3 + 1) = 3𝑑 2
𝑑𝑑
1
(3π‘₯ )2
𝑦′ =
2√𝑑 3 +1
𝑦 ′′ =
ο‚·
𝑦 ′′ = √𝑑 3
ο‚·
3𝑑 2
2√𝑑 3 +1
3π‘₯2
2
3
(2√𝑑 +1)(6𝑑)−3𝑑 (
)
2√π‘₯3 +1
2
(2√π‘₯ 3 +1)
ο‚·
ο‚·
=
12𝑑√𝑑 3 +1−
9𝑑4
√𝑑3+1
=
4𝑑 3 +4
=
12𝑑√𝑑 3 +1−9𝑑4
√𝑑 3 +1
12𝑑 4 −12𝑑−9𝑑 4
3𝑑 4 −12𝑑
=
(4𝑑 3 +4)√𝑑 3 +1
+1 (4𝑑 3 +4)
3(2)4−12(2)
72
(4(2)3 +4)√(2)3 +1
2
2
3
= 108
𝑒𝑛𝑖𝑑𝑠/sec
2. cscπ‘œ πœƒ ′ = −4 cot πœƒ csc2 πœƒ
ο‚·
𝑑
π‘‘πœƒ
[csc2 πœƒ + cot 2 πœƒ] =
𝑑
𝑑
π‘‘πœƒ
[csc 2 πœƒ] +
𝑑
𝑑
π‘‘πœƒ
[cot 2 πœƒ]
ο‚·
(2 csc πœƒ )
ο‚·
ο‚·
2 csc πœƒ csc πœƒ (− cot πœƒ)) + 2 cot πœƒ)(− csc2 πœƒ)
cscπ‘œ πœƒ ′ = −4 cot πœƒ csc2 πœƒ
π‘‘πœƒ
[csc πœƒ ] + (2 cot πœƒ )
π‘‘πœƒ
[cot πœƒ]
3. D
3π‘₯
ο‚·
𝑦 = π‘₯2 +1
ο‚·
(3)
ο‚·
ο‚·
𝑑
(
π‘₯
)
𝑑π‘₯ π‘₯ 2 +1
π‘₯(π‘₯ 2 +1)−(π‘₯ 2 +1)π‘₯
𝑦 ′ = (3)
(π‘₯ 2 +1)2
2 +1)
3(−π‘₯
𝑦 ′ = (π‘₯2 +1)2
= (3)
(π‘₯ 2 +1)−2π‘₯π‘₯
(π‘₯ 2 +1)2
=
3(−π‘₯ 2 +1)
(π‘₯ 2 +1)2
4. 𝑓 (π‘₯ )′ = 8π‘₯ 3 + 2π‘₯
ο‚·
ο‚·
ο‚·
π‘†π‘œπ‘™π‘£π‘’: (π‘₯ 2 )(2π‘₯ 2 + 1) = (2π‘₯ )(2π‘₯ 2 + 1) + (4π‘₯)(π‘₯ 2 )
𝑓 (π‘₯ )′ = 4π‘₯ 3 + 2π‘₯ + 4π‘₯ 3
𝑓 (π‘₯ )′ = 8π‘₯ 3 + 2π‘₯
1
(4𝑑 3 +4)
5. A
ο‚·
ο‚·
𝑓 ′(π‘₯ ) = (9 − π‘₯ 2 ) = (9 − 32 ) = 0
𝑓 ′′ (π‘₯ ) = 0 = 0
6. 2π‘₯ sin(π‘₯ ) + π‘₯ 2 cos(π‘₯)
ο‚·
ο‚·
ο‚·
ο‚·
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
′
(π‘₯ 2 ) sin(π‘₯ ) +
𝑑
𝑑π‘₯
(sin(π‘₯ ))π‘₯ 2
(π‘₯ 2 ) = 2π‘₯
(sin(π‘₯ )) = cos(π‘₯ )
𝑦 = 2π‘₯ sin(π‘₯ ) + π‘₯ 2 cos(π‘₯)
7. 2 sec2 (π‘₯ ) tan(π‘₯ ) + 2π‘₯ 𝑠𝑒𝑐 2 (π‘₯ 2 )
ο‚·
ο‚·
ο‚·
ο‚·
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
(sec2 (π‘₯)) +
𝑑
𝑑π‘₯
(tan(π‘₯ 2 ))
(sec2 (π‘₯)) = 2𝑠𝑒𝑐 2 (π‘₯)tan(π‘₯)
(tan(π‘₯ 2 )) = sec2 (π‘₯ 2 )(2π‘₯ )= 2 sec2 (π‘₯ ) tan(π‘₯ ) + sec2 (π‘₯2)(2π‘₯)
2 sec2 (π‘₯ ) tan(π‘₯ ) + 2π‘₯ 𝑠𝑒𝑐 2 (π‘₯ 2 )
8. D
𝑑
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
𝑑 (1+cos(π‘₯))(1−cos(π‘₯))−𝑑π‘₯(1−cos(π‘₯))(1+cos(π‘₯))
(1−cos(π‘₯))2
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
(1 + cos(π‘₯ )) = − sin(π‘₯ )
(1 − cos(π‘₯ )) = sin(π‘₯ )
𝑑π‘₯
𝑑 (− sin(π‘₯))(1−cos(π‘₯))−sin(π‘₯)(1+cos(π‘₯))
(
(1−cos(π‘₯))2
𝑑π‘₯
2
sin(π‘₯)
𝑦 ′ = − (1−cos(π‘₯))2
9. B
𝑑
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
3
3
𝑑 (π‘₯ +2)π‘₯−𝑑π‘₯(π‘₯ +2)
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
π‘₯2
3
(π‘₯ + 2) = 3π‘₯ 2
(π‘₯ ) = 1
𝑑π‘₯
𝑑 (3π‘₯ 2 −1)(π‘₯ 3 +2)
𝑑π‘₯
′(
π‘₯2
𝑓 𝑑) =
2π‘₯ 3 −2
π‘₯2
=
=
2π‘₯ 3 −2
π‘₯2
2(−2)3−2
(−2)2
7
= −2
10. C
35 2
𝑑
2
ο‚·
𝑠′ = −
ο‚·
−35(1) + 58 = 23
+ 58𝑑 + 91 = −35𝑑 + 58
11. 2π‘₯𝑒 π‘₯ 2
ο‚·
ο‚·
ο‚·
𝑑
(π‘₯ 2 ) = 2π‘₯
𝑑π‘₯
′(
2
𝑓 𝑑) = 𝑒 π‘₯ (2π‘₯ )
𝑓 ′(𝑑) = 2π‘₯𝑒 π‘₯ 2
2sin(π‘₯)
= − (1−cos(π‘₯))2
12. A
ο‚·
ο‚·
ο‚·
𝑑 1
(sin 2πœƒ)2 (2 cos 2πœƒ)
𝑑π‘₯ 2
2 cos 2πœƒ
2√sin 2 πœƒ
cos 2πœƒ
√sin 2πœƒ
13. A
ο‚·
ο‚·
ο‚·
ο‚·
𝑓 ′(π‘₯ ) = 6π‘₯ 2 − 3
𝑓 ′′ (π‘₯ ) = 12
π‘₯ = 1, π‘‘β„Žπ‘’π‘› 12(1)
12
14. A
ο‚·
𝑑
𝑑π‘₯
(𝑦) = csc(π‘₯ ) − cot(π‘₯)
15. C
ο‚·
ο‚·
𝑑
1
𝑑
(2) 𝑑π‘₯ ((2π‘₯ + 𝑒 2π‘₯ )−1 ) = − (2π‘₯+𝑒2π‘₯ ) 𝑑π‘₯ (2π‘₯ + 𝑒 2π‘₯ )
𝑑
𝑑π‘₯
(2π‘₯ + 𝑒 2π‘₯ ) = (2 + 𝑒 2π‘₯ )(2)
2(2+𝑒 2π‘₯ )
1
ο‚·
2 − (2π‘₯+𝑒2π‘₯ ) (2π‘₯ + 𝑒 2π‘₯ ) = − (2π‘₯+𝑒2π‘₯ )
ο‚·
𝑓 ′(π‘₯ ) = − (2π‘₯+𝑒2π‘₯ )
4(1+𝑒 2π‘₯ )
16. C
ο‚·
ο‚·
ο‚·
1
β„Ž
β„Ž
1
+ 2 = 1(β„Ž)−1 + 2
1
1
1
−1β„Ž−2 + 2 = β„Ž2 + 2
β„Ž2 −2
2β„Ž 2
17. C
ο‚·
ο‚·
6𝑑 − 2 = 6(2) − 2
10π‘š/𝑠𝑒𝑐
18. A
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
(𝑑 2 − 1)3 . 𝐹𝑖𝑛𝑑 π‘‘β„Žπ‘’ π‘ π‘’π‘π‘œπ‘›π‘‘ π‘‘π‘’π‘Ÿπ‘–π‘£π‘Žπ‘‘π‘–π‘£π‘’.
𝑠 ′ = 3(𝑑 2 − 1)2 (2𝑑) = 6𝑑(𝑑 2 − 1)2 = 6𝑑(𝑑 4 − 212 + 1)
𝑠 ′ = 6𝑑 5 − 12𝑑 3 + 6𝑑
𝑑
𝑑
𝑑
(6𝑑 5 ) = 30𝑑 4 , (−12𝑑 3 ) = −36𝑑 2 , & (6𝑑) = 6
𝑑π‘₯
𝑑π‘₯
𝑑π‘₯
𝑠 ′′ = 30𝑑 4 − 36𝑑 2 + 6 = 30(2)4 + 36(2)2 + 6
342 𝑒𝑛𝑖𝑑𝑠/𝑠𝑒𝑐 2
19. A
ο‚·
ο‚·
ο‚·
π·π‘–π‘“π‘“π‘’π‘Ÿπ‘’π‘›π‘‘π‘–π‘Žπ‘‘π‘’: 6πœ‹π‘Ÿ 2
𝑑
(6πœ‹π‘Ÿ 2 ) = 2(6)πœ‹π‘Ÿ 2−1
𝑑π‘₯
𝑦 ′ = 12πœ‹π‘Ÿ
20. 128πœ‹π‘π‘š3 /𝑠𝑒𝑐
4
ο‚·
𝑉 = 3 πœ‹π‘Ÿ 3 & π‘Ÿ = 2𝑑
ο‚·
πΉπ‘–π‘Ÿπ‘ π‘‘ π‘‘π‘’π‘Ÿπ‘–π‘£π‘Žπ‘‘π‘–π‘£π‘’: 𝑉 ′ = 3 πœ‹(2𝑑)2 = 3(2𝑑)2 𝑑𝑑 (2𝑑)
ο‚·
ο‚·
ο‚·
ο‚·
𝑑
𝑑𝑑
4
3
4
𝑑
(2𝑑) = 2
πœ‹(2𝑑)2 (2) = 32πœ‹π‘‘ 2
𝑑
π‘†π‘’π‘π‘œπ‘›π‘‘ π‘‘π‘’π‘Ÿπ‘–π‘£π‘Žπ‘‘π‘–π‘£π‘’: 𝑉 ′′ = 𝑑𝑑 (32πœ‹π‘‘ 2 ) = 64πœ‹π‘‘
64πœ‹(2) = 128πœ‹π‘π‘š3 /𝑠𝑒𝑐
Activity 2: What’s In (Page 5)
1. C. 12
ο‚·
ο‚·
ο‚·
𝑓 (π‘₯ ) = 12π‘₯ + 3
π‘ƒπ‘œπ‘€π‘’π‘Ÿ 𝑅𝑒𝑙𝑒: 𝑓 ′ (π‘₯ ) = (1)121−1 + 0
𝑓 ′(π‘₯ ) = 12
2. A. 0
ο‚·
ο‚·
The derivative of a constant is 0.
Therefore, 𝑓 ′ (π‘₯ ) = 0.
3. A. 4x + 2
ο‚·
ο‚·
ο‚·
ο‚·
π·π‘–π‘“π‘“π‘’π‘Ÿπ‘’π‘›π‘‘π‘–π‘Žπ‘‘π‘’: 𝑓 ′ (π‘₯ ) = 2π‘₯ 2 & 𝑔′(π‘₯ ) = 2π‘₯
𝑑
2(2)π‘₯ 2−1 = 4π‘₯
𝑑π‘₯
𝑑
= 1(2)π‘₯ 1−1 = 2
𝑑π‘₯
′(
𝑓 π‘₯ ) = 4π‘₯ + 2
4. A. 50π‘₯ 4 − 28π‘₯ 3 + 6π‘₯ 2 − 18π‘₯
ο‚·
ο‚·
ο‚·
𝑓 (π‘₯ ) = 10π‘₯ 5 − 7π‘₯ 4 + 2π‘₯ 3 − 9π‘₯ 2 + 192
π‘ƒπ‘œπ‘€π‘’π‘Ÿ 𝑅𝑒𝑙𝑒: 𝑓 ′(π‘₯ ) = 5(10)π‘₯ 5−1 − 4(7)π‘₯ 4−1 + 3(2)π‘₯ 3−1 − 2(9)π‘₯ 2−1 + 0
𝑓 ′(π‘₯) = 50π‘₯ 4 − 28π‘₯ 3 + 6π‘₯ 2 − 18π‘₯
5. B. sec(π‘₯ ) tan(π‘₯)
ο‚·
𝑑
𝑑π‘₯
𝑑
(tan π‘₯) = sec2 π‘₯, 𝑓𝑖𝑛𝑑 𝑑π‘₯ (sec π‘₯)
𝑑
1
ο‚·
𝐹𝑖𝑛𝑑 πΆπ‘œπ‘šπ‘šπ‘œπ‘› π·π‘’π‘Ÿπ‘–π‘£π‘Žπ‘‘π‘–π‘£π‘’: 𝑑π‘₯ [cos(π‘₯)] = −
ο‚·
− cos2(π‘₯) = cos2(π‘₯)
ο‚·
𝑑
𝑠𝑖𝑛(π‘₯)
𝑑π‘₯
sin(π‘₯)
(sec π‘₯) = sec(π‘₯ ) tan(π‘₯)
Activity 3: What’s New (Page 5)
1. 36π‘₯ 2 − 36π‘₯ 2 + 56π‘₯ − 16
ο‚·
ο‚·
𝑓 (π‘₯ ) = (3π‘₯ 2 − 2π‘₯ + 4)2
𝑑
2(3π‘₯ 2 − 2π‘₯ + 4) (3π‘₯ 2 − 2π‘₯ + 4)
ο‚·
𝑑
𝑑π‘₯
𝑑π‘₯
2
(3π‘₯ − 2π‘₯ + 4) = (6π‘₯ − 2)
𝑑
[cos(π‘₯)]
𝑑π‘₯
cos2(π‘₯)
ο‚·
ο‚·
2(3π‘₯ 2 − 2π‘₯ + 4)(6π‘₯ − 2)
36π‘₯ 2 − 36π‘₯ 2 + 56π‘₯ − 16
2. 2cos(2π‘₯)
ο‚·
ο‚·
ο‚·
ο‚·
𝑑
𝑑π‘₯
sin(2π‘₯ )
𝑑
cos(2π‘₯ )
𝑑
𝑑π‘₯
𝑑π‘₯
(2π‘₯ )
(2π‘₯ ) = 2 → cos(2π‘₯ ) (2)
2cos(2π‘₯)
Activity 4: What’s More (Page 8)
Activity 3. Find the derivative, dy/dx of the following using chain rule:
24
a. 𝑓 ′ (π‘₯ ) = − (π‘₯+1)4
3
2
2 𝑑𝑦
ο‚·
𝑑𝑦
2
ο‚·
𝑑𝑦
ο‚·
3 (π‘₯+1) (− (π‘₯+12 ) = − (π‘₯+1)4
ο‚·
𝑓 ′(π‘₯ ) = − (π‘₯+1)4
( ) = 3 (π‘₯+1)
𝑑π‘₯ π‘₯+1
(
2
2
( )
𝑑π‘₯ π‘₯+1
2
) = − (π‘₯+1)2
𝑑π‘₯ π‘₯+1
2 2
2
24
24
972
d. 𝑓 ′(π‘₯ ) = − (3π‘₯+1)3
4
ο‚·
𝑑𝑦
3
ο‚·
4 (3π‘₯+1)
ο‚·
𝑑𝑦
ο‚·
4(
ο‚·
𝑓 ′ (π‘₯ ) = − (3π‘₯+1)3
(
)
𝑑π‘₯ 3π‘₯+1
3 𝑑𝑦
3
(
3
𝑑π‘₯ 3π‘₯+1
)
(
3
3
3π‘₯+1
3
)
𝑑π‘₯ 3π‘₯+1
9
= − (3π‘₯+1)2
3
972
) (− (3π‘₯+1)2 ) = − (3π‘₯+1)3
972
2π‘₯ 2 −2
f. 𝑓 ′ (π‘₯ ) = √π‘₯2
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
𝑑𝑦
𝑑π‘₯
𝑑𝑦
𝑑π‘₯
𝑑𝑦
𝑑π‘₯
−2
π‘₯√π‘₯ 2 − 2
(π‘₯ )√π‘₯ 2 − 2 +
(π‘₯ ) = 1 π‘Žπ‘›π‘‘
𝑑π‘₯
𝑑𝑦
𝑑π‘₯
(1)(√π‘₯ 2 − 2) +
2π‘₯ 2 −2
𝑓 ′(π‘₯ ) = √π‘₯2
𝑑𝑦
(√π‘₯ 2 − 2)(π‘₯ )
(√π‘₯ 2 − 2) =
π‘₯
√π‘₯ 2 −2
π‘₯
√π‘₯ 2 −2
2π‘₯ 2 −2
π‘₯ = √π‘₯2
−2
−2
Activity 5: What I Have Learned (Page 9)
Activity 4.
1.
ο‚·
A. 𝑓 ′ (π‘₯ ) = 4π‘₯ 3 − 24π‘₯ 2 + 36π‘₯ − 8 π‘Žπ‘›π‘‘ 𝑓 ′(2) = 0
οƒ˜ 𝑓 (π‘₯ ) = (π‘₯ 2 − 4π‘₯ + 1)2 ; 𝑓′(2)
𝑑
οƒ˜ πΆβ„Žπ‘Žπ‘–π‘› 𝑅𝑒𝑙𝑒: 2(π‘₯ 2 − 4π‘₯ + 1) 𝑑π‘₯ (π‘₯ 2 − 4π‘₯ + 1)
οƒ˜
οƒ˜
οƒ˜
οƒ˜
οƒ˜
𝑑
𝑑π‘₯
(π‘₯ 2 − 4π‘₯ + 1) = 2π‘₯ − 4
2(π‘₯ 2 − 4π‘₯ + 1)(2π‘₯ − 4)
𝑓 ′(π‘₯ ) = 4π‘₯ 3 − 24π‘₯ 2 + 36π‘₯ − 8
𝑓 ′(2) = 4(2)3 − 24(2)2 + 36(2) − 8
𝑓 ′(2) = 0
2.
ο‚·
A. 𝑓 ′′ (π‘₯ ) = −4π‘₯ 2 cos π‘₯ 2 − 2 sin π‘₯ 2
οƒ˜ 𝑦 = cos π‘₯ 2
𝑑
𝑑
οƒ˜ 𝑑π‘₯ (cos(π‘₯ 2 )) = − sin π‘₯ 2 𝑑π‘₯ π‘₯ 2
𝑑
π‘₯ 2 = 2π‘₯
οƒ˜ 𝑓 π‘₯ ) = − sin π‘₯ 2 (2π‘₯ ) = −2π‘₯ sin(π‘₯ 2 )
𝑑
𝑑
οƒ˜ 𝑑π‘₯ (−2π‘₯𝑠𝑖𝑛(π‘₯ 2 )) = −2 𝑑π‘₯ (π‘₯𝑠𝑖𝑛(π‘₯ 2 ))
οƒ˜
𝑑π‘₯
′(
𝑑
𝑑
οƒ˜ −2 (𝑑π‘₯ (π‘₯ ) sin(π‘₯ 2 ) + 𝑑π‘₯ (sin(π‘₯ 2 ))(π‘₯ ))
𝑑
𝑑
(sin(π‘₯ 2 )) = cos π‘₯ 2 (2π‘₯ )
οƒ˜ −2(1 sin π‘₯ 2 + cos π‘₯ 2 (2π‘₯π‘₯ ) = −2(sin(π‘₯ 2 ) + 2π‘₯ 2 cos(π‘₯ 2 ))
οƒ˜ 𝑓 ′ (π‘₯ ) = −4π‘₯ 2 cos π‘₯ 2 − 2 sin π‘₯ 2
οƒ˜
ο‚·
𝑑π‘₯
(π‘₯ ) = 1 &
𝑑π‘₯
B. 𝑓 ′′(π‘₯ ) = −4π‘₯ 2 cos(π‘₯ 2 ) sin(π‘₯ ) − 4π‘₯ cos(π‘₯ ) sin(π‘₯ 2 ) − sin(π‘₯ ) + cos(π‘₯ 2 ) −
2 sin(π‘₯ 2 ) sin(x)
οƒ˜ 𝑦 = sin π‘₯ cos π‘₯ 2
𝑑
𝑑
οƒ˜ 𝑑π‘₯ (sin(π‘₯ ) cos(π‘₯ 2 )) + 𝑑π‘₯ (cos(π‘₯ 2 )) sin(π‘₯ )
οƒ˜
𝑑
𝑑
sin π‘₯ = cos π‘₯ & 𝑑π‘₯ (cos(π‘₯ 2 )) = −sin(π‘₯ 2 )(2π‘₯)
𝑑π‘₯
′(
οƒ˜ 𝑓 π‘₯ ) = cos(π‘₯ ) cos(π‘₯ 2 ) + (− sin(π‘₯ 2 ) (2π‘₯ )) sin(π‘₯ )
οƒ˜ 𝑓 ′ (π‘₯ ) = cos(π‘₯ ) cos(π‘₯ 2 ) − 2π‘₯ sin(π‘₯ 2 ) sin(π‘₯)
𝑑
οƒ˜ 𝑑π‘₯ (cos(π‘₯ ) cos(π‘₯ 2 )) − (2π‘₯ sin(π‘₯ 2 ) sin(π‘₯))
οƒ˜
𝑑
(cos(π‘₯ ) cos(π‘₯ 2 )) = − sin(π‘₯ ) cos(π‘₯ 2 ) − 2π‘₯ sin(π‘₯ 2 ) cos(π‘₯ )
π‘₯
𝑑
(2π‘₯ sin(π‘₯ 2 )sin(π‘₯)) = 2(sin(π‘₯ 2 ) sin(π‘₯ ) + π‘₯(2π‘₯ cos(π‘₯ 2 ) sin(π‘₯ ) + cos(π‘₯ ) sin(π‘₯ 2 )))
οƒ˜ 𝑓 π‘₯ ) = − sin(π‘₯ ) cos(π‘₯ 2 ) − 2π‘₯ sin(π‘₯ 2 ) cos(π‘₯ ) − 2(sin(π‘₯ 2 ) sin(π‘₯ ) +
π‘₯(2π‘₯ cos(π‘₯ 2 ) sin(π‘₯ ) + cos(π‘₯ )sin(π‘₯ 2 ))
οƒ˜ 𝑓 ′′ (π‘₯ ) = − sin(π‘₯ ) cos(π‘₯ 2 ) − 2π‘₯ sin(π‘₯ 2 ) cos(π‘₯ ) − 2(sin(π‘₯ 2 ) sin(π‘₯ ) +
π‘₯(2π‘₯ cos(π‘₯ 2 ) 𝑠𝑖𝑛
οƒ˜ 𝑓 ′′ (π‘₯ ) = −4π‘₯ 2 cos(π‘₯ 2 ) sin(π‘₯ ) − 4π‘₯ cos(π‘₯ ) sin(π‘₯ 2 ) − sin(π‘₯ ) + cos(π‘₯ 2 ) −
2 sin(π‘₯ 2 ) sin(π‘₯)
οƒ˜
𝑑π‘₯
′′ (
LESSON 2:
Implicit Differentiation
Activity 1: What’s New (Page 11)
1. 𝑦 ′ (π‘₯ ) = −2
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
2π‘₯ + 𝑦 = 8
π·π‘–π‘“π‘“π‘’π‘Ÿπ‘’π‘›π‘‘π‘–π‘Žπ‘‘π‘’ π‘π‘œπ‘‘β„Ž 𝑠𝑖𝑑𝑒𝑠: 2π‘₯ + 𝑦 = 8
𝑑
2 + 𝑑π‘₯ (𝑦) = 0
𝑑
(𝑦) = −2
𝑑π‘₯
′(
𝑦 π‘₯ ) = −2
Activity 2: What’s More (Page 16)
𝑑2
a) 𝑑π‘₯2 (𝑦) =
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
2𝑦 2 −π‘₯ 2
4𝑦 3
or
−π‘₯ 2 +2𝑦 2
4𝑦 3
4𝑦 2 + 5 = 2π‘₯ 2
𝑑
8𝑦 𝑑π‘₯ (𝑦) = 4π‘₯
𝑑
(𝑦 ) =
𝑑π‘₯
π‘₯
2𝑦
𝑑2
( )
2 𝑦 =
𝑑π‘₯
𝑑2
𝑑π‘₯ 2
(𝑦 ) =
𝑑
(𝑦)
𝑑π‘₯
2
2𝑦
𝑦−π‘₯
2𝑦 2−π‘₯ 2
4𝑦 3
=
or
2𝑦 2 −π‘₯ 2
4𝑦 3
−π‘₯ 2 +2𝑦 2
4𝑦 3
LESSON 3:
Related Rates
Activity 1: What’s In (Page 19)
cos(π‘₯)𝑦
1. 𝑦 ′ = 4 sin(4𝑦)−sin(π‘₯)
ο‚·
ο‚·
ο‚·
𝑑𝑦
𝐹𝑖𝑛𝑑 𝑑π‘₯ 𝑖𝑓 cos 4𝑦 + 𝑦 sin π‘₯ = 3
𝑑𝑦
𝑑π‘₯
𝑑
𝑑π‘₯
[cos(4𝑦) + sin(π‘₯ ) 𝑦] =
[cos(4𝑦)] +
𝑑
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
[3]
[sin(π‘₯ ) 𝑦] = 0
𝑑
ο‚·
(− sin(4𝑦))
ο‚·
(−4)
ο‚·
ο‚·
−4𝑦 ′ sin(4𝑦) + cos(π‘₯ ) 𝑦 + sin(π‘₯ ) 𝑦 ′ = 0
−4𝑦 ′ sin(4𝑦) + sin(π‘₯ ) 𝑦 ′ + cos(π‘₯ ) 𝑦 = 0
ο‚·
𝑑𝑦
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑π‘₯
[4𝑦] +
𝑑π‘₯
[sin(π‘₯ )]𝑦 + (sin(π‘₯ ))
𝑑
𝑑π‘₯
[𝑦] = 0
(𝑦) sin(4𝑦) + cos(π‘₯ ) 𝑦 + sin(π‘₯ ) 𝑦 ′ = 0
cos(π‘₯)𝑦
𝑦 ′ = 4 sin(4𝑦)−sin(π‘₯)
2. 𝑦 = 0
ο‚·
ο‚·
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
[𝑦 3 + π‘₯ 3 = 𝑑π‘₯ [8]
𝑑
[𝑦 3 ] +
𝑑
𝑑π‘₯
[π‘₯ 3 ] = 0
ο‚·
(3𝑦 2 )
ο‚·
ο‚·
3𝑦 2 𝑦 ′ + 3π‘₯ 2 = 0
3(𝑦 2 𝑦 ′ + π‘₯ 2 ) = 0
ο‚·
𝑦′ = −
ο‚·
𝐴𝑑 π‘‘β„Žπ‘’ π‘π‘œπ‘–π‘›π‘‘ (0, 2): 𝑦 = − 22 = − 4 = 𝟎
𝑑π‘₯
[𝑦] + 3π‘₯ 2 = 0
π‘₯2
𝑦2
02
0
Activity 2: What’s More (Page 22)
Activity 3. Solve the following problems
1
1. 15πœ‹ π‘šπ‘–π‘™π‘’π‘  π‘π‘’π‘Ÿ π‘¦π‘’π‘Žπ‘Ÿ
ο‚·
ο‚·
ο‚·
𝐴 = πœ‹π‘Ÿ 2
where r = 15
2
𝐴(𝑑) = πœ‹π‘Ÿ (𝑑)
𝑑π‘₯ ′
𝐴 (𝑑) = 2πœ‹π‘Ÿ(𝑑)π‘Ÿ ′(𝑑)
ο‚·
ο‚·
π‘Ÿ(𝑑1 ) = 15 π‘šπ‘–π‘™π‘’π‘ 
𝐴′(𝑑1 ) = 2πœ‹π‘Ÿ(𝑑1 )π‘Ÿ ′(𝑑1 )
𝑑𝑦
𝐴′ (𝑑1 )
2πœ‹π‘Ÿ(𝑑1 )
1
2π‘šπ‘–.2
𝑦
ο‚·
π‘Ÿ′(𝑑1 ) =
ο‚·
π‘Ÿ′(𝑑1 ) = 15πœ‹
ο‚·
π‘‡β„Žπ‘’π‘Ÿπ‘’π‘“π‘œπ‘Ÿπ‘’, π‘‘β„Žπ‘’ 𝑐𝑖𝑑𝑦 ′𝑠 π‘Ÿπ‘Žπ‘‘π‘–π‘’π‘  𝑖𝑠 π‘”π‘Ÿπ‘œπ‘€π‘–π‘›π‘” 𝑏𝑦
=
2πœ‹π‘Ÿ(15 π‘šπ‘–.)
1
15πœ‹
π‘šπ‘–π‘™π‘’π‘  π‘œπ‘Ÿ π‘Žπ‘π‘π‘Ÿπ‘œπ‘₯π‘–π‘šπ‘Žπ‘‘π‘’π‘™π‘¦ 0.21 π‘šπ‘–π‘™π‘’π‘  π‘Ž π‘¦π‘’π‘Žπ‘Ÿ.
2. π‘Ÿ ′(𝑑) = 40.21 π‘š3 /𝑠
4
ο‚·
𝑦 = 3 πœ‹π‘Ÿ 2
ο‚·
𝑦(𝑑) = 3 πœ‹π‘Ÿ 2 (𝑑)
ο‚·
𝑦 ′(𝑑) = 3 πœ‹(3π‘Ÿ 2 (𝑑)π‘Ÿ ′(𝑑)) = 4πœ‹π‘Ÿ 2 (𝑑)π‘Ÿ ′(𝑑)
ο‚·
ο‚·
ο‚·
ο‚·
4
4
π‘Ÿ(𝑑1 ) = 4π‘š
π‘š
π‘Ÿ ′(𝑑) = 4πœ‹(4π‘š)2 (0.2 𝑠 ) = 12.8πœ‹
′(
π‘š3
𝑠
= 40.21
π‘š3
𝑠
3
π‘Ÿ 𝑑) = 40.21 π‘š /𝑠
π‘‡β„Žπ‘’π‘Ÿπ‘’π‘“π‘œπ‘Ÿπ‘’, π‘‘β„Žπ‘’ π‘ π‘β„Žπ‘’π‘Ÿπ‘’ 𝑖𝑠 π‘”π‘Ÿπ‘œπ‘€π‘–π‘›π‘” 𝑏𝑦 40.21 π‘š3 /𝑠.
5. 1.73 𝑓𝑑/𝑠
𝑑π‘₯
3𝑓𝑑
ο‚·
𝐺𝑖𝑣𝑒𝑛: 𝑑𝑑 = π‘ π‘’π‘π‘œπ‘›π‘‘ π‘Žπ‘›π‘‘ 𝑐 = 20𝑓𝑑
ο‚·
𝐹𝑖𝑛𝑑: 𝑑𝑑 : 𝑦 = 10
ο‚·
ο‚·
𝑑π‘₯
π‘₯ 2 + 𝑦 2 = 202
π‘₯ 2 + 𝑦 2 = 400
𝑑π‘₯
𝑑π‘₯
ο‚·
2π‘₯ ( 𝑑𝑑 ) + 2𝑦 ( 𝑑𝑑 ) = 0
ο‚·
π‘Šβ„Žπ‘’π‘› 𝑦 = 10, π‘₯ = √400 − 102 = √300
ο‚·
√300 (2 𝑑𝑑 ) + (10 𝑑π‘₯) = 0
ο‚·
(12)
ο‚·
𝑑𝑦
ο‚·
π‘‡β„Žπ‘’π‘Ÿπ‘’π‘“π‘œπ‘Ÿπ‘’, π‘‘β„Žπ‘’ π‘π‘œπ‘‘π‘‘π‘œπ‘š π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘Žπ‘‘π‘‘π‘’π‘Ÿ 𝑖𝑠 𝑠𝑙𝑖𝑑𝑖𝑛𝑔 π‘‘π‘œπ‘€π‘› π‘‘β„Žπ‘’
𝑑π‘₯
𝑑𝑑
=
𝑑𝑦
𝑑𝑦
𝑑π‘₯
= (√300) 𝑑𝑑
𝑑𝑑
√300
10
= 1.73 𝑓𝑑/𝑠
𝑏𝑒𝑖𝑙𝑑𝑖𝑛𝑔 π‘Žπ‘‘ π‘Ž π‘Ÿπ‘Žπ‘‘π‘’π‘œπ‘“ 1.73 𝑓𝑑 π‘π‘’π‘Ÿ π‘ π‘’π‘π‘œπ‘›π‘‘.
Activity 3: Assessment (Posttest) (Page 27)
1. B.
ο‚·
ο‚·
ο‚·
ο‚·
𝑦 = √𝑑 3 + 1 when 𝑑 = 2
1
𝑑
(𝑑 3 + 1)
3
2√𝑑 +1 𝑑π‘₯
𝑑
(𝑑 3 + 1)
𝑑𝑑
1
′
𝑦 =
2√𝑑 3 +1
𝑦 ′′ =
ο‚·
𝑦 ′′ = √𝑑 3
ο‚·
3𝑑 2
(3π‘₯ )2 =
2√𝑑 3 +1
(2√𝑑 3 +1)(6𝑑)−3𝑑2 (
ο‚·
ο‚·
= 3𝑑 2
3π‘₯2
2√π‘₯3 +1
2
(2√π‘₯ 3 +1)
12𝑑√𝑑 3 +1−
)
9𝑑4
√𝑑3+1
=
4𝑑 3 +4
=
12𝑑 4 −12𝑑−9𝑑 4
3𝑑 4 −12𝑑
=
(4𝑑 3 +4)√𝑑 3 +1
+1 (4𝑑 3 +4)
3(2)4−12(2)
72
(4(2)3 +4)√(2)3 +1
2
2
3
= 108
𝑒𝑛𝑖𝑑𝑠/sec
2. cscπ‘œ πœƒ ′ = −4 cot πœƒ csc2 πœƒ
𝑑
𝑑
𝑑
ο‚·
[csc2 πœƒ + cot 2 πœƒ] = π‘‘πœƒ [csc 2 πœƒ] + π‘‘πœƒ [cot 2 πœƒ]
π‘‘πœƒ
ο‚·
(2 csc πœƒ )
ο‚·
ο‚·
2 csc πœƒ csc πœƒ (− cot πœƒ)) + 2 cot πœƒ)(− csc2 πœƒ)
cscπ‘œ πœƒ ′ = −4 cot πœƒ csc2 πœƒ
𝑑
π‘‘πœƒ
[csc πœƒ ] + (2 cot πœƒ )
𝑑
π‘‘πœƒ
[cot πœƒ]
12𝑑√𝑑 3 +1−9𝑑4
√𝑑 3 +1
1
(4𝑑 3 +4)
3. D
3π‘₯
ο‚·
𝑦 = π‘₯2 +1
ο‚·
(3)
ο‚·
𝑦 ′ = (3)
ο‚·
𝑦′ =
𝑑
π‘₯
(
)
𝑑π‘₯ π‘₯ 2 +1
π‘₯(π‘₯ 2 +1)−(π‘₯ 2 +1)π‘₯
(π‘₯ 2 +1)2
= (3)
(π‘₯ 2 +1)−2π‘₯π‘₯
(π‘₯ 2 +1)2
=
3(−π‘₯ 2 +1)
(π‘₯ 2 +1)2
3(−π‘₯ 2 +1)
(π‘₯ 2 +1)2
4. 𝑓 (π‘₯ )′ = 8π‘₯ 3 + 2π‘₯
ο‚·
ο‚·
ο‚·
π‘†π‘œπ‘™π‘£π‘’: (π‘₯ 2 )(2π‘₯ 2 + 1) = (2π‘₯ )(2π‘₯ 2 + 1) + (4π‘₯)(π‘₯ 2 )
𝑓 (π‘₯ )′ = 4π‘₯ 3 + 2π‘₯ + 4π‘₯ 3
𝑓 (π‘₯ )′ = 8π‘₯ 3 + 2π‘₯
5. A
ο‚·
ο‚·
𝑓 ′(π‘₯ ) = (9 − π‘₯ 2 ) = (9 − 32 ) = 0
𝑓 ′′ (π‘₯ ) = 0 = 0
6. 2π‘₯ sin(π‘₯ ) + π‘₯ 2 cos(π‘₯)
ο‚·
ο‚·
ο‚·
ο‚·
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
′
(π‘₯ 2 ) sin(π‘₯ ) +
𝑑
𝑑π‘₯
(sin(π‘₯ ))π‘₯ 2
(π‘₯ 2 ) = 2π‘₯
(sin(π‘₯ )) = cos(π‘₯ )
𝑦 = 2π‘₯ sin(π‘₯ ) + π‘₯ 2 cos(π‘₯)
7. 2 sec2 (π‘₯ ) tan(π‘₯ ) + 2π‘₯ 𝑠𝑒𝑐 2 (π‘₯ 2 )
ο‚·
ο‚·
ο‚·
ο‚·
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
(sec2 (π‘₯)) + 𝑑π‘₯ (tan(π‘₯ 2 ))
(sec2 (π‘₯)) = 2𝑠𝑒𝑐 2 (π‘₯)tan(π‘₯)
(tan(π‘₯ 2 )) = sec2 (π‘₯ 2 )(2π‘₯ )= 2 sec2 (π‘₯ ) tan(π‘₯ ) + sec2 (π‘₯2)(2π‘₯)
2 sec2 (π‘₯ ) tan(π‘₯ ) + 2π‘₯ 𝑠𝑒𝑐 2 (π‘₯ 2 )
8. D
𝑑
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
𝑑 (1+cos(π‘₯))(1−cos(π‘₯))−𝑑π‘₯(1−cos(π‘₯))(1+cos(π‘₯))
(1−cos(π‘₯))2
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
(1 + cos(π‘₯ )) = − sin(π‘₯ )
(1 − cos(π‘₯ )) = sin(π‘₯ )
𝑑π‘₯
𝑑 (− sin(π‘₯))(1−cos(π‘₯))−sin(π‘₯)(1+cos(π‘₯))
(
(1−cos(π‘₯))2
𝑑π‘₯
2
sin(π‘₯)
𝑦 ′ = − (1−cos(π‘₯))2
9. B
𝑑
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
3
3
𝑑 (π‘₯ +2)π‘₯−𝑑π‘₯(π‘₯ +2)
𝑑π‘₯
𝑑
𝑑π‘₯
𝑑
π‘₯2
3
(π‘₯ + 2) = 3π‘₯ 2
(π‘₯ ) = 1
𝑑π‘₯
𝑑 (3π‘₯ 2 −1)(π‘₯ 3 +2)
𝑑π‘₯
′(
𝑓 𝑑) =
π‘₯2
2π‘₯ 3 −2
π‘₯2
=
=
2π‘₯ 3 −2
π‘₯2
2(−2)3−2
(−2)2
7
= −2
2sin(π‘₯)
= − (1−cos(π‘₯))2
10. C
35 2
𝑑
2
ο‚·
𝑠′ = −
ο‚·
−35(1) + 58 = 23
+ 58𝑑 + 91 = −35𝑑 + 58
11. 2π‘₯𝑒 π‘₯ 2
ο‚·
ο‚·
ο‚·
𝑑
(π‘₯ 2 ) = 2π‘₯
𝑑π‘₯
′(
𝑓 𝑑) = 𝑒 π‘₯ 2 (2π‘₯ )
𝑓 ′(𝑑) = 2π‘₯𝑒 π‘₯ 2
12. A
ο‚·
ο‚·
ο‚·
𝑑 1
(sin 2πœƒ)2 (2 cos 2πœƒ)
𝑑π‘₯ 2
2 cos 2πœƒ
2√sin 2 πœƒ
cos 2πœƒ
√sin 2πœƒ
13. A
ο‚·
ο‚·
ο‚·
ο‚·
𝑓 ′(π‘₯ ) = 6π‘₯ 2 − 3
𝑓 ′′ (π‘₯ ) = 12
π‘₯ = 1, π‘‘β„Žπ‘’π‘› 12(1)
12
14. A
ο‚·
𝑑
𝑑π‘₯
(𝑦) = csc(π‘₯ ) − cot(π‘₯)
15. C
ο‚·
ο‚·
𝑑
1
𝑑
(2) 𝑑π‘₯ ((2π‘₯ + 𝑒 2π‘₯ )−1 ) = − (2π‘₯+𝑒2π‘₯ ) 𝑑π‘₯ (2π‘₯ + 𝑒 2π‘₯ )
𝑑
𝑑π‘₯
(2π‘₯ + 𝑒 2π‘₯ ) = (2 + 𝑒 2π‘₯ )(2)
2(2+𝑒 2π‘₯ )
1
ο‚·
2 − (2π‘₯+𝑒2π‘₯ ) (2π‘₯ + 𝑒 2π‘₯ ) = − (2π‘₯+𝑒2π‘₯ )
ο‚·
𝑓 ′(π‘₯ ) = − (2π‘₯+𝑒2π‘₯ )
4(1+𝑒 2π‘₯ )
16. C
ο‚·
ο‚·
ο‚·
1
β„Ž
β„Ž
+ = 1(β„Ž)−1 +
2
1
1
1
2
1
−1β„Ž−2 + 2 = β„Ž2 + 2
β„Ž2 −2
2β„Ž 2
17. C
ο‚·
ο‚·
ο‚·
π·π‘–π‘“π‘“π‘’π‘Ÿπ‘’π‘›π‘‘π‘–π‘Žπ‘‘π‘’: 3𝑑 2 − 2𝑑 + 5 = 6𝑑 − 2
6𝑑 − 2 = 6(2) − 2
10π‘š/𝑠𝑒𝑐
18. A
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
ο‚·
(𝑑 2 − 1)3 . 𝐹𝑖𝑛𝑑 π‘‘β„Žπ‘’ π‘ π‘’π‘π‘œπ‘›π‘‘ π‘‘π‘’π‘Ÿπ‘–π‘£π‘Žπ‘‘π‘–π‘£π‘’.
𝑠 ′ = 3(𝑑 2 − 1)2 (2𝑑) = 6𝑑(𝑑 2 − 1)2 = 6𝑑(𝑑 4 − 212 + 1)
𝑠 ′ = 6𝑑 5 − 12𝑑 3 + 6𝑑
𝑑
𝑑
𝑑
(6𝑑 5 ) = 30𝑑 4 , (−12𝑑 3 ) = −36𝑑 2 , & (6𝑑) = 6
𝑑π‘₯
𝑑π‘₯
𝑑π‘₯
𝑠 ′′ = 30𝑑 4 − 36𝑑 2 + 6 = 30(2)4 + 36(2)2 + 6
342 𝑒𝑛𝑖𝑑𝑠/𝑠𝑒𝑐 2
19. A
ο‚·
ο‚·
ο‚·
π·π‘–π‘“π‘“π‘’π‘Ÿπ‘’π‘›π‘‘π‘–π‘Žπ‘‘π‘’: 6πœ‹π‘Ÿ 2
𝑑
(6πœ‹π‘Ÿ 2 ) = 2(6)πœ‹π‘Ÿ 2−1
𝑑π‘₯
𝑦 ′ = 12πœ‹π‘Ÿ
20. 128πœ‹π‘π‘š3 /𝑠𝑒𝑐
4
ο‚·
𝑉 = 3 πœ‹π‘Ÿ 3 & π‘Ÿ = 2𝑑
ο‚·
πΉπ‘–π‘Ÿπ‘ π‘‘ π‘‘π‘’π‘Ÿπ‘–π‘£π‘Žπ‘‘π‘–π‘£π‘’: 𝑉 ′ = 3 πœ‹(2𝑑)2 = 3(2𝑑)2 𝑑𝑑 (2𝑑)
ο‚·
ο‚·
ο‚·
ο‚·
𝑑
𝑑𝑑
4
3
4
𝑑
(2𝑑) = 2
πœ‹(2𝑑)2 (2) = 32πœ‹π‘‘ 2
𝑑
π‘†π‘’π‘π‘œπ‘›π‘‘ π‘‘π‘’π‘Ÿπ‘–π‘£π‘Žπ‘‘π‘–π‘£π‘’: 𝑉 ′′ = 𝑑𝑑 (32πœ‹π‘‘ 2 ) = 64πœ‹π‘‘
64πœ‹(2) = 128πœ‹π‘π‘š3 /𝑠𝑒𝑐
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