Integral Subtitusi
Integral Subtitusi
66. Critique the following “proof” that an arbitrary constant 72. Recall that
must be zero: d 1
0= x dx − x dx [sec−1 x] = √
dx |x| x 2 − 1
= (x − x) dx = 0 dx = C Use this to verify Formula 14 in Table 5.2.1.
73. The speed of sound in air at 0 ◦ C (or 273 K on the Kelvin
67. (a) Show that
scale) is 1087 ft/s, but the speed v increases as the temper-
F (x) = tan−1 x and G(x) = − tan−1 (1/x) ature T rises. Experimentation has shown that the rate of
differ by a constant on the interval (0, +⬁) by show- change of v with respect to T is
ing that they are antiderivatives of the same func- dv 1087 −1/2
tion. = √ T
dT 2 273
(b) Find the constant C such that F (x) − G(x) = C by
evaluating the functions F (x) and G(x) at a partic- where v is in feet per second and T is in kelvins (K). Find
ular value of x. a formula that expresses v as a function of T .
(c) Check your answer to part (b) by using trigonomet-
74. Suppose that a uniform metal rod 50 cm long is insulated
ric identities.
laterally, and the temperatures at the exposed ends are main-
68. Let F and G be the functions defined by
tained at 25 ◦ C and 85 ◦ C, respectively. Assume that an x-
x 2 + 3x x + 3, x > 0 axis is chosen as in the accompanying figure and that the
F (x) = and G(x) =
x x, x<0 temperature T (x) satisfies the equation
(a) Show that F and G have the same derivative.
(b) Show that G(x) = F (x) + C for any constant C. d 2T
=0
(c) Do parts (a) and (b) contradict Theorem 5.2.2? Ex- dx 2
plain.
Find T (x) for 0 ≤ x ≤ 50.
u-SUBSTITUTION
The method of substitution can be motivated by examining the chain rule from the viewpoint
of antidifferentiation. For this purpose, suppose that F is an antiderivative of f and that
g is a differentiable function. The chain rule implies that the derivative of F (g(x)) can be
expressed as d
[F (g(x))] = F (g(x))g (x)
dx
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or since F is an antiderivative of f ,
f(g(x))g (x) dx = F (g(x)) + C (2)
For our purposes it will be useful to let u = g(x) and to write du/dx = g (x) in the differ-
ential form du = g (x) dx. With this notation (2) can be expressed as
f(u) du = F (u) + C (3)
The process of evaluating an integral of form (2) by converting it into form (3) with the
substitution
u = g(x) and du = g (x) dx
is called the method of u-substitution. Here our emphasis is not on the interpretation of
the expression du = g (x) dx. Rather, the differential notation serves primarily as a useful
“bookkeeping” device for the method of u-substitution. The following example illustrates
how the method works.
Example 1 Evaluate (x 2 + 1)50 · 2x dx.
Solution. If we let u = x 2 + 1, then du/dx = 2x, which implies that du = 2x dx. Thus,
the given integral can be written as
u51 (x 2 + 1)51
(x 2 + 1)50 · 2x dx = u50 du = +C = +C
51 51
It is important to realize that in the method of u-substitution you have control over the
choice of u, but once you make that choice you have no control over the resulting expres-
sion for du. Thus, in the last example we chose u = x 2 + 1 but du = 2x dx was computed.
Fortunately, our choice of u, combined with the computed du, worked out perfectly to pro-
duce an integral involving u that was easy to evaluate. However, in general, the method of
u-substitution will fail if the chosen u and the computed du cannot be used to produce an inte-
grand in which no expressions involving x remain, or if you cannot evaluate the resulting in-
tegral. Thus, for example, the substitution u = x 2 , du = 2x dx will not work for the integral
2x sin x 4 dx
Example 2
sin(x + 9) dx = sin u du = − cos u + C = − cos(x + 9) + C
u=x+9
du = 1 · dx = dx
u24 (x − 8)24
(x − 8) dx =
23
u23 du = +C = +C
24 24
u=x−8
du = 1 · dx = dx
Another easy u-substitution occurs when the integrand is the derivative of a known
function, except for a constant that multiplies or divides the independent variable. The
following example illustrates two ways to evaluate such integrals.
Example 3 Evaluate cos 5x dx.
Solution.
1 1 1 1
cos 5x dx = (cos u) · du = cos u du = sin u + C = sin 5x + C
5 5 5 5
u = 5x
du = 5 dx or dx = 1
5 du
Alternative Solution. There is a variation of the preceding method that some people
prefer. The substitution u = 5x requires du = 5 dx. If there were a factor of 5 in the inte-
grand, then we could group the 5 and dx together to form the du required by the substitution.
Since there is no factor of 5, we will insert one and compensate by putting a factor of 15 in
front of the integral. The computations are as follows:
1 1 1 1
cos 5x dx = cos 5x · 5 dx = cos u du = sin u + C = sin 5x + C
5 5 5 5
u = 5x
du = 5 dx
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More generally, if the integrand is a composition of the form f(ax + b), where f(x) is
an easy to integrate function, then the substitution u = ax + b, du = a dx will work.
Example 4
−4
dx 3 du −5 3 −4 3 1
1 5 = = 3 u du = − u + C = − x − 8 +C
x−8 u5 4 4 3
3
u = 13 x − 8
du = 1
3dx or dx = 3 du
dx
Example 5 Evaluate .
1 + 3x 2
Solution. Substituting √ √
u= 3x, du = 3 dx
yields
√
dx 1 du 1 1
=√ = √ tan−1 u + C = √ tan−1 ( 3x) + C
1 + 3x 2
3 1+u 2
3 3
With the help of Theorem 5.2.3, a complicated integral can sometimes be computed by
expressing it as a sum of simpler integrals.
Example 6
1 dx
+ sec2 πx dx = + sec2 πx dx
x x
= ln |x| + sec2 πx dx
1
= ln |x| + sec2 u du
π u = πx
1
du = π dx or dx = du
π
1 1
= ln |x| + tan u + C = ln |x| + tan πx + C
π π
The next four examples illustrate a substitution u = g(x) where g(x) is a nonlinear
function.
Example 7 Evaluate sin2 x cos x dx.
Solution.
3 1 √ 1
t 4 3 − 5t 5 dt = − 3
u du = − u1/3 du
25 25 u = 3 − 5t 5
du = −25t 4 dt or − 25
1
du = t 4 dt
1 u4/3 3 4/3
=− +C =− 3 − 5t 5 +C
/
25 4 3 100
ex
Example 10 Evaluate √ dx.
1 − e2x
Solution. Substituting
u = ex , du = ex dx
yields
ex du
√ dx = √ = sin−1 u + C = sin−1 (ex ) + C
1− e2x 1 − u2
√
Solution. The composition x − 1 suggests the substitution
u=x−1 so that du = dx (4)
From the first equality in (4)
x 2 = (u + 1)2 = u2 + 2u + 1
so that
√ √
x 2
x − 1 dx = (u + 2u + 1) u du =
2
(u5/2 + 2u3/2 + u1/2 ) du
Solution. The only compositions in the integrand that suggest themselves are
cos3 x = (cos x)3 and cos2 x = (cos x)2
However, neither the substitution u = cos x nor the substitution u = cos2 x work (verify).
In this case, an appropriate substitution is not suggested by the composition contained in
the integrand. On the other hand, note from Equation (2) that the derivative g (x) appears
as a factor in the integrand. This suggests that we write
cos x dx = cos2 x cos x dx
3
and solve the equation du = cos x dx for u = sin x. Since sin2 x + cos2 x = 1, we then
have
cos3 x dx = cos2 x cos x dx = (1 − sin2 x) cos x dx = (1 − u2 ) du
u3 1
=u− + C = sin x − sin3 x + C
3 3
dx
Example 13 Evaluate dx, where a = 0 is a constant.
a2 + x2
Solution. Some simple algebra and an appropriate u-substitution will allow us to use
Formula 12 in Table 5.2.1.
dx a(dx /a) 1 dx /a u = x /a
= =
a2 + x 2 a 2 (1 + (x /a)2 ) a 1 + (x /a)2 du = dx /a
1 du 1 1 x
= = tan−1 u + C = tan−1 + C
a 1 + u2 a a a
The method of Example 13 leads to the following generalizations of Formulas 12, 13,
and 14 in Table 5.2.1 for a > 0:
du 1 u
= tan−1 + C (5)
a 2 + u2 a a
du u
= sin−1 + C (6)
a 2 − u2 a
u
du 1
= sec−1 + C (7)
u u −a 2 2 a a
dx
Example 14 Evaluate .
2 − x2
√
Solution. Applying (6) with u = x and a = 2 yields
dx x
= sin−1 √ + C
2 − x2 2
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1. Indicate the u-substitution. 2. Supply the missing integrand corresponding to the indicated
u-substitution.
(a) 3x (1 + x ) dx = u25 du
2 3 25
if u =
−1/3
(a) 5(5x − 3) dx = du; u = 5x − 3
and du = .
(b) 2x sin x 2 dx = sin u du if u = and (b) (3 − tan x) sec2 x dx = du;
du = . u = 3 − tan x
√
18x
=
1
du if u =
3
8+ x √
(c)
1 + 9x 2
dx
u
and (c) √ dx = du; u = 8 + x
x
du = .
(d) e3x dx = du; u = 3x
3 1
(d) dx = du if u = and
1 + 9x 2 1 + u2
du = .