Trigonometric Integrals
Calculus 2 Lia Vas
Trigonometric Integrals
Let us consider the integrals of the form
f (sin x) cos xdx
or
f (cos x) sin xdx
where f (x) is a function with antiderivative F (x). Using the substitution
u = sin x for the first integral and
u = cos x for the second integral
one can reduce the first integral to f (u)du = F (u) + c = F (sin x) + c and the second integral to f (u)(-du) = -F (u) + c = -F (cos x) + c.
This idea can be applied to the integrals of the form
sinn x cosm x dx
if either m or n are odd. We will refer to this situation as the good case. If n is odd rewrite sinn-1 x as a function of cos x using the trigonometric identity sin2 x =
1-cos2 x. Note that then you obtain an integral of the form f (cos x) sin xdx where f is a polynomial function (thus easy to integrate). You can evaluate the integral using the substitution
u = cos x.
If m is odd rewrite cosm-1 x as a function of sin x using the trigonometric identity cos2 x = 1-sin2 x. Note that then you obtain an integral of the form f (sin x) cos xdx where f is a polynomial function. You can evaluate the integral using the substitution
u = sin x.
Let us consider the case when both n or m are even. Let us refer to this as the bad case (although it is not that bad). The idea is to use one or more of the following three trigonometric identities
sin2 x
=
1 (1
-
cos 2x)
2
cos2
x
=
1 (1
+
cos 2x)
and
1 sin x cos x = sin 2x
2
2
to reduce the integral to a sum of integrals in which the powers of cosines and sines are at most 1.
Then you can integrate term by term.
If you encounter a multiple of x in the argument of sin or cos, note that the three identities above
become
sin2 ax
=
1 2
(1
-
cos 2ax),
cos2 ax
=
1 2
(1
+ cos 2ax),
and
sin ax
cos ax
=
1 2
sin 2ax.
Note: If you have to integrate other trigonometric functions, you can convert them to sin and cos
functions using the trigonometric identities.
1
Practice Problems. Evaluate the following integrals:
1. sin10 x cos x dx
2. sin3 x cos2 x dx
3. ecos x sin x dx
cos x 4. 1 + sin2 x dx
5. tan x dx
6. cos2 x tan x dx
7. sin2 x dx
8. sin2 x cos2 x dx
9. sin5 x dx
10. cos4 x dx
11. Finding the center of mass. Let R be the region between the graphs of f and g such that f (x) g(x) on interval [a, b]. The area A of R is A = ab(f (x) - g(x)) dx. Then the center of mass of R is the point (x?, y?) where
1b
x? =
x (f (x) - g(x)) dx
Aa
1 y? =
b 1 ((f (x))2 - (g(x))2) dx
A a2
Find the center of mass of the region bounded by the given curves. (a) y = sin x, y = cos x, x = 0, x = /4. (b) y = sin 2x, y = 0, x = 0, x = /2.
Solutions.
1. This integral is already in the form f (sin x) cos xdx so use the substitution u = sin x. The
integral becomes
u10
cos
x
du cos x
=
u10du
=
1 11
u11
+c
=
1 11
sin11 x
+ c.
2. The sine function has the odd power. So, this is the "good case". Write sin3 x as sin2 x sin x =
(1 - cos2 x) sin x and get cos2 x sin3 x dx = cos2 x (1 - cos2 x) sin x dx = (cos2 x -
cos4 x) sin x dx. This integral is of the form f (cos x) sin x dx that can be evaluated using
u
=
cos x
du
=
- sin xdx
du - sin x
=
dx.
The
integral
reduces
to
(cos2 x-cos4 x) sin x dx =
(u2
-
u4)
sin
x
-
du sin
x
=
-
(u2
- u4)du
=
-1 3
u3
+
1 5
u5
+
c
=
-1 3
cos3
x
+
1 5
cos5 x
+ c.
3. This integral is of the form f (cos x) sin xdx so use the substitution u = cos x. The integral
becomes
eu
sin
x
-
du sin
x
=
-
eudu = -eu + c = -ecos x + c.
4. This integral is of the form f (sin x) cos xdx so use the substitution u = sin x. The integral
becomes
cos 1+u2
du cos x
=
1 1+u2
du
=
tan-1
u
+
c
=
tan-1(sin x) +
c.
5.
Write tan x as
sin x cos x
=
1 cos
x
sin
x
and
treat
this
as
f
(cos
x)
sin
x.
So,
use
the
substitution
u
=
cos
x
to obtain
1 u
sin
x
-
du sin
x
=
-
1 u
du
=
-
ln
|u|
+
c
=
-
ln
|
cos
x|
+
c.
2
6.
cos2 x tan x dx =
cos2
x
sin cos
x x
dx
=
cos x sin x. Note that this is a good case with both
exponents equal (super good case!) so both substitutions u = cos x and u = sin x could work.
With u = sin x, one obtains
cos
xu
du cos x
=
1 2
u2
+c
=
1 2
sin2 x +
c.
With u = cos x, one obtains
u
sin
x
-
du sin
x
=
-1 2
u2
+
c
=
-1 2
cos2
x + c.
Note
that
this
is
the
same
as
the
previous
answer
since
-1 2
cos2
x+c
=
-1 2
(1
-
sin2
x) + c
=
-1 2
+
1 2
sin2 x + c
=
1 2
sin2 x + c1.
7. This is the bad case.
Use the trigonometric identity sin2 x =
1 2
(1
-
cos 2x)
to
have
1 2
(1
-
cos 2x)dx.
Use
the
substitution
u
=
2x
and
obtain
1 2
x
-
1 4
sin(2x) + c.
8.
This is the bad case as well.
Use both identities sin2 x =
1 2
(1 - cos
2x)
and
cos2
x
=
1 2
(1
+
cos
2x)
to have
sin2 x cos2 xdx =
1 4
(1
-
cos
2x)(1
+
cos
2x)dx
=
1 4
(1
-
cos2
2x)dx.
Then
use
the
trig
identity
cos2 x
=
1 2
(1
+
cos
2x)
with
2x
instead
of
x
to
reduce
cos2 2x
to
linear
terms.
Obtain
1 4
(1
-
1 2
(1
+
cos
4x))dx
=
(
1 4
-
1 8
-
1 8
cos
4x)dx
=
(
1 8
-
1 8
cos 4x)dx
=
1 8
x
-
1 32
sin 4x
+
c.
Alternatively,
you
can
use
sin x cos x
=
1 2
sin 2x
first
and
then
sin2
2x
1 2
(1
-
cos
4x)
after.
In
this
case, you will get (sin x cos x)2dx =
1 4
sin2
2xdx
=
1 8
(1
-
cos 4x)dx
=
1 8
x
-
1 32
sin 4x
+
c.
9. This is the good case. sin5 x = sin4 x sin x = (sin2 x)2 sin x = (1 - cos2 x)2 sin x. Since this
is of the form f (cos x) sin x, you can use the substitution u = cos x. The integral becomes
(1 - u2)2
sin
x
-
du sin
x
=
-(1
-
2u2
+
u4)du
=
-u
+
2 3
u3
-
1 5
u5
=
-
cos
x
+
2 3
cos3
x
-
1 5
cos5
x
+ c.
10.
This is the bad case.
Using
the
trig
identities
cos4 x
=
(cos2 x)2
=
(
1 2
(1
+
cos 2x))2
=
1 4
(1
+
2 cos 2x + cos2
2x)
=
1 4
(1
+
2
cos
2x
+
1 2
(1
+
cos
4x))
=
1 4
+
1 2
cos 2x +
1 8
+
1 8
cos 4x
=
3 8
+
1 2
cos 2x +
1 8
cos 4x.
Integrating
term
by
term
now,
you
obtain
3 8
x
+
1 4
sin 2x +
1 32
sin 4x + c.
11.
(a)
Note
that
on
(0,
4
)
0/4(cos x - sin x)dx =
cos x is larger than sin x. So the
(sin x + cos x)|0/4
=
2-1
area A can be evaluated as .414. The x-coordinate x? is
A x?
= =
1 .414
this
/4 0
x(cos
x-sin
x)
integral.
x? =
1 .414
dx. Use x(sin x
the integration by parts with u = x and dv =
+ cos x)|0/4 - (- cos x + sin x)|0/4 dx
=
1 .414
(cos x-sin
(
4
2 - 1)
x)dx for = .267.
y? =
1 .414
/4 0
1 2
(cos2
x
-
sin2 x)dx.
This
is
the
"bad
case".
Using the trigonometric identities
for
sin2 x
and
cos2 x,
we
obtain
1 .414
1 4
0/4(1 + cos 2x - 1 + cos 2x)dx
=
1 1.656
/4 0
2
cos
2xdx
=
1 1.656
sin
2x|0 /4
=
.6035.
So,
the
center
of
mass
is
(.267,
.6035).
(b) A =
/2 0
sin
2xdx
=
-1 2
cos
2x|0/2
=
-1 2
(-1
-
1)
=
1.
x?
=
/2 0
x
sin
2xdx.
Using
the
integration
by
parts
obtain
that
x?
=
(
-x 2
cos 2x
+
1 4
sin 2x)|0/2
=
4
.
y?
=
/2 0
1 2
sin2
2xdx.
Using
the
trigonometric
identities
for
sin2 x,
we
obtain
1 4
0/2(1 - cos 4x)dx
=
1 4
(x
-
1 4
sin 4x)|0/2
=
8
.
So,
the
center
of
mass
is
(
4
,
8
).
3
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