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MTH240 Lecture 1 Substitution and Integration By Parts

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MTH240 – CALCULUS II
LECTURE 1
Substitution and Integration By Parts
Volume 2 Chapter 3, Section 3.1
Winter 2024
Copyright © (2024) by F. K. Duah
Learning Outcomes
After studying the material covered in this session, you should be
able to :
• Explain the concept of integration by parts.
• Recognize when to use integration by parts.
• Use integration-by-parts formula to solve integration problems.
Copyright © (2024) by F. K. Duah
2
Pre-requisites from Calculus I
It is reasonable to expect the reader to recall the following integrals and their results.
𝑛
1) ‫= π‘₯𝑑 π‘₯ ׬‬
π‘₯ 𝑛+1
𝑛+1
+ 𝑐, 𝑛 ≠ − 1
2) ‫𝑔 )π‘₯(𝑔 𝑓 ׬‬′ π‘₯ 𝑑π‘₯ = 𝐹 𝑔(π‘₯) + 𝑐 where 𝐹(βˆ™) is the antiderivative of 𝑓 ⋅ .
3) ‫π‘₯ 𝑓 ׬‬
4) ‫𝑓 𝑒 ׬‬
5) β€«π‘Ž ׬‬
6)
π‘₯
𝑓 π‘₯
𝑓′ π‘₯
‫π‘₯𝑓׬‬
𝑛 ′
𝑓 π‘₯ 𝑑π‘₯ =
𝑓 ′ π‘₯ 𝑑π‘₯ = 𝑒 𝑓
′
𝑓 π‘₯ 𝑑π‘₯ =
𝑓 π‘₯
𝑛+1
𝑛+1
π‘₯
π‘Žπ‘“ π‘₯
ln π‘Ž
+ 𝑐, 𝑛 ≠ −1
+𝑐
+ 𝑐, π‘Ž > 0, π‘Ž ≠ 1
𝑑π‘₯ = ln 𝑓 π‘₯ + 𝑐
Copyright © (2024) by F. K. Duah
3
Pre-requisites from Calculus I
The following integrals can all easily be evaluated by inspection or by u-substitution even though
they involve the products of two functions in the integrand.
ΰΆ± 18π‘₯ 2
4
6π‘₯ 3 + 13 𝑑π‘₯
ΰΆ± 8π‘₯ − 1 𝑒 4π‘₯
2 −π‘₯
𝑑π‘₯
Copyright © (2024) by F. K. Duah
2π‘₯ 3 + 1
ΰΆ± 4
𝑑π‘₯
π‘₯ + 2π‘₯ 3
ΰΆ± 1−
1
cos π‘₯ − ln π‘₯ 𝑑π‘₯
π‘₯
4
Integration by Parts
When solving an engineering problem that require evaluation of an integral, we may find products of
functions that are difficult to integrate unless they are transformed to integrals that are easier to
integrate than the original integrals. Examples of such integrals are:
ΰΆ± π‘₯𝑒 π‘₯ 𝑑π‘₯
ΰΆ± π‘₯ 2 𝑒 π‘₯ 𝑑π‘₯
ΰΆ± π‘₯ sin π‘₯ 𝑑π‘₯
The technique that transforms such integrals into easier integrals is what is referred to as Integration
by Parts. In the next few slides, we look at the theory behind the technique.
Copyright © (2024) by F. K. Duah
5
Theory of Integration by Parts
Integration by parts is based on the Product Rule of Differentiation.
Suppose 𝑒 and 𝑣 are differentiable functions. The product rule for
differentiation is given by:
𝑑
𝑑𝑒
𝑑𝑣
𝑒𝑣 = 𝑣
+𝑒
.
𝑑π‘₯
𝑑π‘₯
𝑑π‘₯
If we take the antiderivative of both sides of the above equation, we
obtain
𝑑
𝑑𝑒
𝑑𝑣
ΰΆ±
𝑒𝑣 𝑑π‘₯ = ΰΆ± 𝑣
𝑑π‘₯ + ΰΆ± 𝑒
𝑑π‘₯ .
𝑑π‘₯
𝑑π‘₯
𝑑π‘₯
Copyright © (2024) by F. K. Duah
6
Theory of Integration by Parts
We know from the previous slide that
𝑑
𝑑𝑒
𝑑𝑣
ΰΆ±
𝑒𝑣 𝑑π‘₯ = ΰΆ± 𝑣
𝑑π‘₯ + ΰΆ± 𝑒
𝑑π‘₯.
𝑑π‘₯
𝑑π‘₯
𝑑π‘₯
The antiderivative of the left hand is given by
𝑑𝑒
𝑑𝑣
𝑒𝑣 = ΰΆ± 𝑣
𝑑π‘₯ + ΰΆ± 𝑒
𝑑π‘₯.
𝑑π‘₯
𝑑π‘₯
When we re-arrange the above equation we obtain,
𝑑𝑣
𝑑𝑒
ࢱ𝑒
𝑑π‘₯ = 𝑒𝑣 − ΰΆ± 𝑣
𝑑π‘₯ .
𝑑π‘₯
𝑑π‘₯
The above equation is the integration by parts formula.
Copyright © (2024) by F. K. Duah
7
Integration by Parts
Recall that the integration by parts formula is
𝑑𝑣
𝑑𝑒
ࢱ𝑒
𝑑π‘₯ = 𝑒𝑣 − ΰΆ± 𝑣
𝑑π‘₯.
𝑑π‘₯
𝑑π‘₯
For ease of application, the integration by parts formula is typically rewritten
in terms of differentials as
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒 .
Copyright © (2024) by F. K. Duah
8
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒
Activity 1 Integration By Parts
Evaluate ‫ 𝑒π‘₯ ׬‬−5π‘₯ 𝑑π‘₯.
Solution
Let 𝑒 = π‘₯ and 𝑑𝑣 = 𝑒 −5π‘₯ 𝑑π‘₯
𝑑𝑒 = 𝑑π‘₯ and 𝑣 = ‫׬‬
𝑒 −5π‘₯ 𝑑π‘₯
ΰΆ± π‘₯𝑒 −5π‘₯ 𝑑π‘₯
=
1 −5π‘₯
− 𝑒
5
1 −5π‘₯
1 −5π‘₯
=π‘₯ − 𝑒
−ΰΆ± − 𝑒
𝑑π‘₯
5
5
π‘₯ −5π‘₯
1 5π‘₯
=− 𝑒
−
𝑒 +𝑐
5
25
Copyright © (2024) by F. K. Duah
9
Integration by Parts Choosing u and dv.
Recall the integration by parts formula
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒
There is an order of precedence for the choices of 𝑒 and 𝑑𝑣 and this goes by the acronym LIATE.
L – Logarithm
I – Inverse Trigonometric Functions
A – Algebraic Functions
T – Trigonometric Functions
E – Exponential Functions
Thus, we choose the function which appears first in the list LIATE and let it be 𝑒. We let 𝑑𝑣 be equal to
the other function and 𝑑π‘₯. This is only for guidance and my not always work or without some
preliminary work.
Copyright © (2024) by F. K. Duah
10
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒
Activity 2
Evaluate ‫ π‘₯ ׬‬sin π‘₯ 𝑑π‘₯ .
Solution
Let 𝑒 = π‘₯ and 𝑑𝑣 = sin π‘₯ 𝑑π‘₯
𝑑𝑒 = 𝑑π‘₯ and 𝑣 = ‫ ׬‬sin π‘₯ 𝑑π‘₯ = − cos π‘₯
ΰΆ± π‘₯ sin π‘₯ 𝑑π‘₯ = π‘₯ − cos π‘₯ − ΰΆ± −cos π‘₯ 𝑑π‘₯
= −π‘₯ cos π‘₯ + sin π‘₯ + 𝑐
Copyright © (2024) by F. K. Duah
11
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒
Activity 3
Evaluate ‫ ׬‬5π‘₯ + 1 cos 2π‘₯ 𝑑π‘₯.
Solution
Let 𝑒 = 5π‘₯ + 1 and 𝑑𝑣 = cos 2π‘₯ 𝑑π‘₯
1
𝑑𝑒 = 5𝑑π‘₯ and 𝑣 = ‫ ׬‬cos 2π‘₯ 𝑑π‘₯ = sin 2π‘₯
2
ΰΆ± 5π‘₯ + 1 cos 2π‘₯ 𝑑π‘₯ = 5π‘₯ + 1
1
1
sin 2π‘₯ − ΰΆ± sin 2π‘₯
2
2
5𝑑π‘₯
1
5
= 5π‘₯ + 1 sin 2π‘₯ + cos 2π‘₯
2
4
Copyright © (2024) by F. K. Duah
12
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒
Activity 4
Evaluate ‫ ׬‬ln π‘₯ 𝑑π‘₯.
Solution
Let 𝑒 = ln π‘₯ and 𝑑𝑣 = 1 𝑑π‘₯
1
𝑑𝑒 = 𝑑π‘₯ and 𝑣 = ‫π‘₯ = π‘₯𝑑 ׬‬
π‘₯
1
ΰΆ± ln π‘₯ 𝑑π‘₯ = ln π‘₯ π‘₯ − ΰΆ± π‘₯ 𝑑π‘₯
π‘₯
= π‘₯ ln π‘₯ − π‘₯ + 𝑐.
Copyright © (2024) by F. K. Duah
13
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒
Activity 5
Evaluate ‫ π‘₯ ׬‬2 𝑒 π‘₯ 𝑑π‘₯.
Solution
Let 𝑒 = π‘₯ 2 and 𝑑𝑣 = 𝑒 π‘₯ , 𝑑𝑒 = 2π‘₯𝑑π‘₯ and 𝑣 = ‫π‘₯ 𝑒 = π‘₯𝑑 π‘₯ 𝑒 ׬‬
ΰΆ± π‘₯ 2 𝑒 π‘₯ 𝑑π‘₯ = π‘₯ 2 𝑒 π‘₯ − ΰΆ± 𝑒 π‘₯ 2π‘₯ 𝑑π‘₯ = π‘₯ 2 𝑒 π‘₯ − 2 ΰΆ± π‘₯𝑒 π‘₯ 𝑑π‘₯
Integrate ‫ π‘₯𝑑 π‘₯ 𝑒π‘₯ ׬‬using integration by parts. Let 𝑒 = π‘₯ and 𝑑𝑣 = 𝑒 π‘₯ , 𝑑𝑒 = 𝑑π‘₯ and 𝑣 = ‫π‘₯ 𝑒 = π‘₯𝑑 π‘₯ 𝑒 ׬‬
ΰΆ± π‘₯𝑒 π‘₯ 𝑑π‘₯ = π‘₯𝑒 π‘₯ − ΰΆ± 𝑒 π‘₯ 𝑑π‘₯ = π‘₯𝑒 π‘₯ − 𝑒 π‘₯
ΰΆ± π‘₯ 2 𝑒 π‘₯ 𝑑π‘₯ = π‘₯ 2 𝑒 π‘₯ − ΰΆ± 𝑒 π‘₯ 2π‘₯ 𝑑π‘₯ = π‘₯ 2 𝑒 π‘₯ − 2 π‘₯𝑒 π‘₯ − 𝑒 π‘₯ + 𝑐 = π‘₯ 2 𝑒 π‘₯ − 2π‘₯𝑒 π‘₯ + 2𝑒 π‘₯ + 𝑐.
This technique will work for any integral of the form ‫ π‘₯𝑑 π‘₯ 𝑒 𝑛 π‘₯ ׬‬, were 𝑛 is a positive integer.
Copyright © (2024) by F. K. Duah
14
ΰΆ± 𝑒 𝑑𝑣 = 𝑒𝑣 − ΰΆ± 𝑣 𝑑𝑒
Activity 6
Evaluate ‫ π‘₯ 𝑒 ׬‬cos π‘₯ 𝑑π‘₯.
Solution
Let 𝑒 = cos π‘₯ and 𝑑𝑣 = 𝑒 π‘₯ , 𝑑𝑒 = −sin π‘₯ 𝑑π‘₯ and 𝑣 = ‫π‘₯ 𝑒 = π‘₯𝑑 π‘₯ 𝑒 ׬‬
ΰΆ± 𝑒 π‘₯ cos π‘₯ 𝑑π‘₯ = cos π‘₯ 𝑒 π‘₯ − ΰΆ± 𝑒 π‘₯ −sin π‘₯ 𝑑π‘₯ = 𝑒 π‘₯ cos π‘₯ − ΰΆ± 𝑒 π‘₯ −sin π‘₯ 𝑑π‘₯ = 𝑒 π‘₯ cos π‘₯ + ΰΆ± 𝑒 π‘₯ sin π‘₯ 𝑑π‘₯
Integrate ‫ π‘₯ 𝑒 ׬‬sin π‘₯ 𝑑π‘₯ using integration by parts. Let 𝑒 = sin π‘₯ and 𝑑𝑣 = 𝑒 π‘₯ , 𝑑𝑒 = cos π‘₯ 𝑑π‘₯ and 𝑣 = ‫π‘₯ 𝑒 = π‘₯𝑑 π‘₯ 𝑒 ׬‬
ΰΆ± 𝑒 π‘₯ sin π‘₯ 𝑑π‘₯ = sin π‘₯ 𝑒 π‘₯ − ΰΆ± 𝑒 π‘₯ cos π‘₯ 𝑑π‘₯ = 𝑒 π‘₯ sin π‘₯ − ΰΆ± 𝑒 π‘₯ cos π‘₯ 𝑑π‘₯
ΰΆ± 𝑒 π‘₯ cos π‘₯ 𝑑π‘₯ = 𝑒 π‘₯ cos π‘₯ + 𝑒 π‘₯ sin π‘₯ − ΰΆ± 𝑒 π‘₯ cos π‘₯ 𝑑π‘₯
𝑒 π‘₯ cos π‘₯ + 𝑒 π‘₯ sin π‘₯
ΰΆ± 𝑒 cos π‘₯ 𝑑π‘₯ =
+𝑐
2
π‘₯
Copyright © (2024) by F. K. Duah
15
Further Review of Calculus I
Activities 7 to 20 are problems aimed at helping you consolidate your knowledge of the techniques of
integration learned in MTH140 of Calculus I.
The activities require knowledge of :
• The Power Rule
• Substitution
• Chain Rule
You are advised to ensure that you are proficient in evaluating integrals of the kind presented in
Activities 7 to 20. But before we look at these, a quick recap of some calculus facts.
Copyright © (2024) by F. K. Duah
16
Review of Calculus I - Derivatives
To progress smoothly through Calculus II, you should be able to recall and evaluate derivatives of the
following forms:
π’…π’š
π’š=𝒇 𝒙
= 𝒇′ 𝒙
𝒅𝒙
𝑦 = π‘˜, where π‘˜ is constant. 𝑑𝑦
=0
𝑦 = 𝑐, where 𝑐 is constant 𝑑π‘₯
𝑑𝑦
𝑦 = π‘₯𝑛
= 𝑛π‘₯ 𝑛−1
𝑑π‘₯
𝑑𝑦
𝑦 = 𝑒π‘₯
= 𝑒π‘₯
𝑑π‘₯
𝑑𝑦 1
𝑦 = ln π‘₯
=
𝑑π‘₯ π‘₯
𝑑𝑦
𝑦 = sin π‘₯
= cos π‘₯
𝑑π‘₯
𝑑𝑦
𝑦 = cos π‘₯
= − sin π‘₯
𝑑π‘₯
Copyright © (2024) by F. K. Duah
17
Review of Calculus I - Derivatives
To progress smoothly through Calculus II, you should be able to recall and evaluate derivatives of the
following forms:
π’š=𝒇 𝒙
𝑦 = tan π‘₯
𝑦 = cot π‘₯
𝑦 = sec π‘₯
𝑦 = csc π‘₯
Copyright © (2024) by F. K. Duah
π’…π’š
= 𝒇′ 𝒙
𝒅𝒙
𝑑𝑦
= sec 2 π‘₯
𝑑π‘₯
𝑑𝑦
= −csc 2 π‘₯
𝑑π‘₯
𝑑𝑦
= sec π‘₯ tan π‘₯
𝑑π‘₯
𝑑𝑦
= − csc π‘₯ cot π‘₯
𝑑π‘₯
18
Review of Calculus I - Derivatives
To progress smoothly through Calculus II, you should be able to recall and evaluate derivatives of the
following forms:
π’š=𝒇 𝒙
𝑦 = sin−1 π‘₯
𝑦 = cos−1 π‘₯
𝑦 = tan−1 π‘₯
Copyright © (2024) by F. K. Duah
π’…π’š
= 𝒇′ 𝒙
𝒅𝒙
1
𝑑𝑦
=
𝑑π‘₯
1 − π‘₯2
𝑑𝑦
1
=−
𝑑π‘₯
1 − π‘₯2
𝑑𝑦
1
=
𝑑π‘₯ 1 + π‘₯ 2
19
Review of Calculus I - Integrals
To progress smoothly through Calculus II, you should be able to recall and evaluate integrals of the
following forms:
1) ‫ π‘₯ = π‘₯𝑑 ׬‬+ 𝑐
2) ‫׬‬
π‘₯ 𝑛 𝑑π‘₯
3) ‫π‘₯ 𝑓 ׬‬
=
π‘₯ 𝑛+1
𝑛+1
𝑛 ′
𝑓
+ 𝑐, 𝑛 ≠ − 1
π‘₯ 𝑑π‘₯ =
4) ‫𝑓 𝑒 ׬‬
π‘₯
𝑓 ′ π‘₯ 𝑑π‘₯ = 𝑒 𝑓
5) ‫𝑓 π‘Ž ׬‬
π‘₯
𝑓 ′ π‘₯ 𝑑π‘₯ =
6)
𝑓′ π‘₯
‫π‘₯𝑓׬‬
𝑓 π‘₯
𝑛+1
𝑛+1
π‘₯
π‘Žπ‘“ π‘₯
ln π‘Ž
+ 𝑐, 𝑛 ≠ −1
+𝑐
+ 𝑐, π‘Ž > 0, π‘Ž ≠ 1
𝑑π‘₯ = ln 𝑓 π‘₯ + 𝑐
Copyright © (2024) by F. K. Duah
20
Review of Calculus I - Integrals
To be progress smoothly through Calculus II, you should be able to recall and apply the follow
integrals. Some examples are given where appropriate.
7) ‫ ׬‬sin 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = −cos 𝑓 π‘₯
8)‫ ׬‬cos 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = sin 𝑓 π‘₯
+𝑐
+𝑐
9) ‫ ׬‬sec 2 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = tan 𝑓 π‘₯
+𝑐
10) ‫ ׬‬csc 2 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = −cot 𝑓 π‘₯
+𝑐
11)‫ ׬‬sec 𝑓 π‘₯ tan 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = sec 𝑓 π‘₯
12)‫ ׬‬csc 𝑓 π‘₯ cot 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = −csc 𝑓 π‘₯
13)‫ ׬‬tan 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = ln sec 𝑓 π‘₯
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+𝑐
+𝑐
+𝑐
21
Review of Calculus I - Integrals
To be progress smoothly through Calculus II, you should be able to recall and apply the follow
integrals. Some examples are given where appropriate.
1
1
14) β€«π‘Ž ׬‬2+π‘₯2 𝑑π‘₯ = π‘Ž tan−1
15) ‫׬‬
16) ‫׬‬
1
π‘Ž2 −π‘₯
𝑑π‘₯ = sin−1
2
1
π‘₯ π‘Ž2 −π‘₯
1
π‘₯
π‘Ž
π‘₯
π‘Ž
𝑑π‘₯ = π‘Ž sec −1
2
Copyright © (2024) by F. K. Duah
+ 𝑐, π‘Ž > 0
+ 𝑐, −π‘Ž ≤ π‘₯ ≤ π‘Ž
π‘₯
π‘Ž
+ 𝑐, π‘Ž > 0
22
𝑛+1
ΰΆ± 𝑓 π‘₯
Activity 7
𝑓 π‘₯
𝑓 π‘₯ 𝑑π‘₯ =
𝑛+1
𝑛 ′
+ 𝑐 , 𝑛 ≠ −1
Evaluate ‫ ׬‬2π‘₯ π‘₯ 2 + 1 5 𝑑π‘₯.
Solution
ΰΆ± 2π‘₯ π‘₯ 2 + 1 5 𝑑π‘₯ = ΰΆ± π‘₯ 2 + 1
π‘₯2 + 1
=
6
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5
2π‘₯ 𝑑π‘₯
6
+ 𝑐.
23
𝑛+1
ΰΆ± 𝑓 π‘₯
Activity 8
𝑓 π‘₯
𝑓 π‘₯ 𝑑π‘₯ =
𝑛+1
𝑛 ′
+ 𝑐 , 𝑛 ≠ −1
Evaluate ‫ π‘₯ ׬‬3π‘₯ 2 + 1 5 𝑑π‘₯.
Solution
ΰΆ± 2π‘₯ π‘₯ 2 + 1 5 𝑑π‘₯ = ΰΆ± π‘₯ 2 + 1
π‘₯2 + 1
=
6
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5
2π‘₯ 𝑑π‘₯
6
+ 𝑐.
24
𝑛+1
𝑓 π‘₯
𝑛 ′
ΰΆ± 𝑓 π‘₯ 𝑓 π‘₯ 𝑑π‘₯ =
𝑛+1
Activity 9
+ 𝑐 , 𝑛 ≠ −1
Evaluate ‫ ׬‬sin3 π‘₯ cos π‘₯ 𝑑π‘₯.
Solution
‫׬‬
sin3 π‘₯
cos 𝑑π‘₯ = ‫ ׬‬sin π‘₯
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3 cos
π‘₯ 𝑑π‘₯ =
sin4π‘₯
4
+ 𝑐.
25
𝑓(π‘₯)
π‘Ž
ΰΆ± π‘Ž 𝑓(π‘₯) 𝑓 ′ π‘₯ 𝑑π‘₯ =
+𝑐
ln π‘Ž
Activity 10
Evaluate‫׬‬
π‘₯3
4
π‘₯
5
𝑑π‘₯ .
Solution
ΰΆ± π‘₯3
4
π‘₯
5
1 π‘₯4
𝑑π‘₯ = ΰΆ± 5
4
=
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4
π‘₯
15
4 ln5
4π‘₯ 3 𝑑π‘₯
+ 𝑐.
26
𝑛+1
Activity 11
ΰΆ± 𝑓 π‘₯
𝑓 π‘₯
𝑓 π‘₯ 𝑑π‘₯ =
𝑛+1
𝑛 ′
+ 𝑐 , 𝑛 ≠ −1
Evaluate ‫ ׬‬cos3 π‘₯ sin π‘₯ 𝑑π‘₯.
Solution
ΰΆ± cos3 π‘₯ sin π‘₯ 𝑑π‘₯ = ΰΆ± − cos π‘₯
3
− sin π‘₯ 𝑑π‘₯
1
= − cos4 π‘₯ + 𝑐.
4
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27
𝑓′ π‘₯
ΰΆ±
𝑑π‘₯ = ln 𝑓 π‘₯ + 𝑐
𝑓 π‘₯
Activity 12
Evaluate ‫ ׬‬cot π‘₯ 𝑑π‘₯.
Solution
cos π‘₯
ΰΆ± cot π‘₯ 𝑑π‘₯ = ΰΆ±
𝑑π‘₯
sin π‘₯
= ln sin π‘₯ + 𝑐
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28
ΰΆ± sin 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = −cos 𝑓 π‘₯
+𝑐
Activity 13
Evaluate‫ ׬‬sin sec π‘₯ sec π‘₯ tan π‘₯ 𝑑π‘₯.
Solution
ΰΆ± sin sec π‘₯ sec π‘₯ tan π‘₯ 𝑑π‘₯ = −cos sec π‘₯ + 𝑐.
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29
ΰΆ± cos 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = sin 𝑓 π‘₯
+𝑐
Activity 14
Evaluate ‫ ׬‬cos 3π‘₯ 3π‘₯ ln 3 𝑑π‘₯.
Solution
ΰΆ± cos 3π‘₯ 3π‘₯ ln 3 𝑑π‘₯ = sin 3π‘₯ + 𝑐.
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30
ΰΆ± sec 2 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = tan 𝑓 π‘₯
+𝑐
Activity 15
Evaluate‫ ׬‬sec2 𝑒 π‘₯ 𝑒 π‘₯ 𝑑π‘₯.
Solution
ΰΆ± sec2 𝑒 π‘₯ 𝑒 π‘₯ 𝑑π‘₯ = tan 𝑒 π‘₯ + 𝑐 .
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31
ΰΆ± csc 2 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = −cot 𝑓 π‘₯
Activity 16
+𝑐
Evaluate ‫ π‘₯ ׬‬2 csc2 π‘₯ 3 − 5 𝑑π‘₯.
Solution
ΰΆ± π‘₯ 2 csc2
π‘₯3
1
− 5 𝑑π‘₯ = ΰΆ± csc2 π‘₯ 3 − 5 3π‘₯ 2 𝑑π‘₯
3
1
= − cot π‘₯ 3 − 5 + 𝑐.
3
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32
ΰΆ± sec 𝑓 π‘₯ tan 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = sec 𝑓 π‘₯
Activity 17
Evaluate‫ ׬‬sec lnπ‘₯ tan lnπ‘₯
+𝑐
1
𝑑π‘₯.
π‘₯
Solution
1
ΰΆ± sec lnπ‘₯ tan lnπ‘₯ 𝑑π‘₯ = sec lnπ‘₯ + 𝑐.
π‘₯
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33
ΰΆ± csc 𝑓 π‘₯ cot 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = −csc 𝑓 π‘₯
Activity 18
Evaluate‫ ׬‬csc
π‘₯ cot
π‘₯
1
2 π‘₯
+𝑐
𝑑π‘₯ .
Solution
ΰΆ± csc
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π‘₯ cot
π‘₯
1
2 π‘₯
𝑑π‘₯ = −csc
π‘₯ + 𝑐.
34
ΰΆ± tan 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = ln sec 𝑓 π‘₯
Activity 19
+𝑐
Evaluate‫ π‘₯ ׬‬5 tan π‘₯ 6 𝑑π‘₯ .
Solution
ΰΆ± π‘₯ 5 tan
π‘₯6
1
𝑑π‘₯ = ΰΆ± tan π‘₯ 6 6π‘₯ 5 𝑑π‘₯
6
1
= ln sec π‘₯ 6 + 𝑐.
6
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35
ΰΆ± tan 𝑓 π‘₯ 𝑓 ′ π‘₯ 𝑑π‘₯ = ln sec 𝑓 π‘₯
Activity 20
+𝑐
Evaluate‫ ׬‬8π‘₯ 2 tan π‘₯ 3 𝑑π‘₯.
Solution
ΰΆ± 8π‘₯ 2 tan
π‘₯3
8
𝑑π‘₯ = ΰΆ± tan π‘₯ 3 3π‘₯ 2 𝑑π‘₯
3
8
= ln sec π‘₯ 3 + 𝑐.
3
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36
Recap
In this session, we have
• introduced and discussed the theory of integration by parts, and looked
at some examples of integration by parts,
• reviewed some common integrals, and
• reviewed how to integrate some functions mentally by inspection.
Next lecture we will develop our understanding of integration by parts and
the application of the reduction formula to solve some problems.
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37
The End
Thank You
For
Coming
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38
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