In the previous section,
we saw some solved examples demonstrating integration by substitution. In
this section, we will see the application of trigonometric identities in the process of integration. We have already seen some examples in the previous section. For example, in the solved example 23.7(ii) of the previous section, we used the identity:
sinA−sinB = 2cos(A+B2)sin(A−B2)
Now we will see some advanced problems
Solved example 23.8
Find the following integrals:
(i) ∫[cos2x]dx
(ii) ∫[sin2xcos3x]dx
(iii) ∫[sin3x]dx
(iv) ∫[sin3xcos4x]dx
Solution:
Part (i):
1. We have the identity: cos2A=2cos2A−1
•
From this, we get: cos2A=1+cos2A2
2. So for our present problem, we can write:
1∫[cos2x]dx = ∫[1+cos2x2]dx 2 = 12∫[1]dx + 12∫[cos2x]dx
3. The R.H.S has two terms. We will consider each term separately.
First term:
•
This term is easy. We can directly write:
12∫[1]dx = x2+C1
Second term:
For this term, we use the method of substitution.
(i)
The derivative of
(2x) is 2.
• So we put u = 2x
⇒ dudx = 2
⇒ 2 dx = du
(ii) So we want:
12∫[2cos2x2]dx = 12∫[cosu2]du
•
This integration gives:
12sinu2+C2 = sin2x4+C2
4. Now, based on step 2, we get:
1∫[cos2x]dx = x2+C1 + sin2x4+C2 2 = x2+sin2x4+C
• Note that, the constants C1, C2 etc., can be combined into a single constant C because, all constants, when differentiated, will give zero only.
Part (ii):
1. We have the identity:
sinA−sinB=2cos(A+B2)sin(A−B2)
•
From this, we get: cos(A+B2)sin(A−B2)=sinA−sinB2
2. So for our present problem, we can write:
1A+B2 = 3x 2A−B2 = 2x
•
Solving the two equations, we get:
A = 5x and B = 1x
•
So the given function can be rearranged as:
1∫[sin2xcos3x]dx = ∫[sin5x−sinx2]dx 2 = 12∫[sin5x]dx − 12∫[sinx]dx
3. The R.H.S has two terms. We will consider each term separately.
First term:
For this term, we use the method of substitution.
(i)
The derivative of
(5x) is 5.
• So we put u = 5x
⇒ dudx = 5
⇒ 5 dx = du
(ii) So we want:
12∫[5sin5x5]dx = 12∫[sinu5]du
•
This integration gives:
12−cosu5+C1 = −cos5x10+C1
Second term:
•
This term is easy. We can directly write:
12∫[sinx]dx = −cosx2+C2
4. Now, based on step 2, we get:
1∫[sin2xcos3x]dx = −cos5x10+C1 − −cosx2+C2 2 = −cos5x10+cosx2+C
• Note that, the constants C1, C2 etc., can be combined into a single constant C because, all constants, when differentiated, will give zero only.
Part (iii):
1.
The given expression can be rearranged as follows:
1sin3x = sinxsin2x 2 = sinx(1−cos2x) 3 = sinx−sinxcos2x
2. So for our present problem, we can write:
1∫[sin3x]dx = ∫[sinx−sinxcos2x]dx 2 = ∫[sinx]dx − ∫[sinxcos2x]dx
3. The R.H.S has two terms. We will consider each term separately.
First term:
•
This term is easy. We can directly write:
∫[sinx]dx = −cosx+C1
Second term:
For this term, we use the method of substitution.
(i)
The derivative of
(cos x) is −sin x.
• So we put u = cos x
⇒ dudx = −sinx
⇒ (−sin x)dx = du
(ii) So we want:
∫[(−1)(−1)sinxcos2x]dx = ∫[(−1)u2]du
•
This integration gives:
(−1)u33+C2 = (−1)cos3x3+C2
4. Now, based on step 2, we get:
1∫[sin3x]dx = −cosx+C1 − (−1)cos3x3+C2 2 = −cosx + cos3x3+C
• Note that, the constants C1, C2 etc., can be combined into a single constant C because, all constants, when differentiated, will give zero only.
Alternate method:
1. We have the identity: sin3A=3sinA−4sin3A
•
From this, we get: sin3A=3sinA−sin3A4
2. So for our present problem, we can write:
1∫[sin3x]dx = ∫[3sinx−sin3x4]dx 2 = 34∫[sinx]dx − 14∫[sin3x]dx
3. The R.H.S has two terms. We will consider each term separately.
First term:
•
This term is easy. We can directly write:
34∫[sinx]dx = −3cosx4+C1
Second term:
For this term, we use the method of substitution.
(i)
The derivative of
(3x) is 3.
• So we put u = 3x
⇒ dudx = 3
⇒ 3 dx = du
(ii) So we want:
14∫[3sin3x3]dx = 14∫[sinu3]du
•
This integration gives:
14−cosu3+C2 = −cos3x12+C2
4. Now, based on step 2, we get:
1∫[sin3x]dx = −3cosx4+C1 − −cos3x12+C2 2 = −3cosx4+cos3x12+C
• Note that, the constants C1, C2 etc., can be combined into a single constant C because, all constants, when differentiated, will give zero only.
We see that, the results obtained by the two methods are different. But their equality can be proved by using trigonometric identities. This is shown below:
1−3cosx4+cos3x12 = −3cosx4+4cos3x−3cosx12 2 = −3cosx4+4cos3x12−3cosx12 3 = −3cosx4+cos3x3−cosx4 4 = −4cosx4+cos3x3 5 = −cosx+cos3x3
Part (iv):
1. We have the identity:
sinA−sinB=2cos(A+B2)sin(A−B2)
•
From this, we get: cos(A+B2)sin(A−B2)=sinA−sinB2
2. So for our present problem, we can write:
1A+B2 = 4x 2A−B2 = 3x
•
Solving the two equations, we get:
A = 7x and B = 1x
•
So the given function can be rearranged as:
1∫[sin3xcos4x]dx = ∫[sin7x−sinx2]dx 2 = 12∫[sin7x]dx − 12∫[sinx]dx
3. The R.H.S has two terms. We will consider each term separately.
First term:
For this term, we use the method of substitution.
(i)
The derivative of
(7x) is 7.
• So we put u = 7x
⇒ dudx = 7
⇒ 7 dx = du
(ii) So we want:
12∫[7sin7x7]dx = 12∫[sinu7]du
•
This integration gives:
12−cosu5+C1 = −cos7x14+C1
Second term:
•
This term is easy. We can directly write:
12∫[sinx]dx = −cosx2+C2
4. Now, based on step 2, we get:
1∫[sin3xcos4x]dx = −cos7x14+C1 − −cosx2+C2 2 = −cos7x14+cosx2+C
•
Note that, the constants C1, C2
etc., can be combined into a single constant C because, all constants,
when differentiated, will give zero only.
In the next section, we will see a few more solved examples.
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