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4.5 The Substitution Rule
The Substitution Rule
Because of the Fundamental Theorem, it’s important to be able to find antiderivatives.
But our antidifferentiation formulas don’t tell us how to evaluate integrals such as
To find this integral we use the problem-solving strategy of introducing something extra. Here the “something extra” is a new variable; we change from the variable x to a new variable u.
The Substitution Rule
Suppose that we let u be the quantity under the root sign in (1), u = 1 + x2. Then the differential of u is du = 2xdx.
Notice that if the dx in the notation for an integral were to be interpreted as a differential, then the differential 2xdx would occur in (1) and so, formally, without justifying our calculation, we could write
The Substitution Rule
But now we can check that we have the correct answer by using the Chain Rule to differentiate the final function of Equation 2:
In general, this method works whenever we have an integral that we can write in the form
∫
f(g(x))g′(x) dx.The Substitution Rule
Observe that if F′ = f, then
∫
F′(g(x)) g′(x) dx = F(g(x)) + C because, by the Chain Rule,[F(g(x))] = F′(g(x))g′(x)
If we make the “change of variable” or “substitution”
u = g(x), then from Equation 3 we have
∫
F′(g(x))g′(x) dx = F(g(x)) + C = F(u) + C =∫
F′(u) duor, writing F′ = f, we get
∫
f(g(x))g′(x) dx =∫
f(u) duThe Substitution Rule
Thus we have proved the following rule.
Notice that the Substitution Rule for integration was proved using the Chain Rule for differentiation.
Notice also that if u = g(x), then du = g′(x) dx, so a way to
remember the Substitution Rule is to think of dx and du in (4) as differentials.
The Substitution Rule
Thus the Substitution Rule says: It is permissible to operate with dx and du after integral signs as if they were differentials.
Example 1
Find
∫
x3 cos(x4 + 2) dx.Solution:
We make the substitution u = x4 + 2 because its differential is du = 4x3 dx, which, apart from the constant factor 4,
occurs in the integral.
Thus, using x3 dx = du and the Substitution Rule, we have
∫
x3 cos(x4 + 2) dx =∫
cos u du=
∫
cos u duExample 1 – Solution
= sin u + C
= sin(x4 + 2) + C
Notice that at the final stage we had to return to the original variable x.
cont’d
Definite Integrals
Definite Integrals
When evaluating a definite integral by substitution, two methods are possible. One method is to evaluate the indefinite integral first and then use the Fundamental Theorem.
For example,
Definite Integrals
Another method, which is usually preferable, is to change the limits of integration when the variable is changed.
Example 6
Evaluate using (5).
Solution:
Let u = 2x + 1 and dx = du.
To find the new limits of integration we note that when x = 0, u = 2(0) + 1 = 1
and
when x = 4, u = 2(4) + 1 = 9
Example 6 – Solution
Therefore
Observe that when using (5) we do not return to the variable x after integrating. We simply evaluate the expression in u between the appropriate values of u.
cont’d
Symmetry
Symmetry
The following theorem uses the Substitution Rule for
Definite Integrals (5) to simplify the calculation of integrals of functions that possess symmetry properties.
Symmetry
Theorem 6 is illustrated by Figure 2.
For the case where f is positive and even, part (a) says that the area under y = f(x) from –a to a is twice the area from 0 to a because of symmetry.
Figure 2
Symmetry
We know that an integral can be expressed as the area above the x-axis and below y = f(x) minus the area
below the axis and above the curve.
Thus part (b) says the integral is 0 because the areas cancel.
Example 8
Since f(x) = x6 + 1 satisfies f(–x) = f(x), it is even and so
Example 9
Since f(x) = (tan x)/(1 + x2 + x4) satisfies f(–x) = –f(x), it is odd and so