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File: Derivatives Calculus Pdf 173242 | Section6 8
section 6 8 3 20 08 integration by substitution overview with the fundamental theorem of calculus every dierentiation formula translates into integration formula in this section we discuss the technique ...

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               Section 6.8                                                                            (3/20/08)
               Integration by substitution
               Overview: With the Fundamental Theorem of Calculus every differentiation formula translates into
               integration formula. In this section we discuss the technique of integration by substitution which
               comes from the Chain Rule for derivatives. Then we use it with integration formulas from earlier sections.
               Weendthe section with a discussion of some of the highlights in the history of the integral.
               Topics:
                   • Integration by substitution
                   • Substitution in definite integrals
                   • Special linear substitutions
                   • Integrals of tangents, cotangents, secants, and cosecants
                   • History of the integral
               Integration by substitution
               Webegin with the following result.
               Theorem 1 (Integration by substitution in indefinite integrals)   If y = g(u) is continuous on an
               open interval and u = u(x) is a differentiable function whose values are in the interval, then
                                                 Z g(u) du dx = Z g(u) du:                                (1)
                                                        dx
                     Equation (1) states that an x-antiderivative of g(u) du is a u-antiderivative of g(u). Formula (1) is
                                                                   dx
               called integration by substitution because the variable x in the integral on the left of (1) is replaced
               by the substitute variable u in the integral on the right.
                                                                                        †         ′
               Proof of Theorem 1: Suppose that y = G(u) is a u-antiderivative of y = g(u) , so that G (u) = g(u)
               and
                                                   Z g(u) du = G(u)+C:                                    (2)
               The Chain Rule gives, with u = u(x),
                                                d           ′   du       du
                                               dx[G(u)] = G (u) dx = g(u) dx:
                     The last equation shows that y = G(u) is an x-antiderivative of g(u) du, so that
                                                                                   dx
                                                  Z g(u) du dx = G(u)+C:                                  (3)
                                                         dx
               Equations (2) and (3) give (1). There is no constant C of integration in equation (1) because there are
               indefinite integrals on both sides. QED
                     †Part II of the Fundamental Theorem in Section 6.4 implies that every continuous function has antiderivatives.
                                                            254
               Section 6.8, Integration by substitution                                   p. 255 (3/20/08)
                   Weuse Leibniz notation for the derivative du=dx in the integrals on the left of (1) so that we can
              use the formula
                                                    du = du dx
                                                         dx
              in our calculations. Here du=dx denotes the derivative of the function u = u(x); dx is the symbol that is
              used in integrals with x as variable; and du is the symbol in integrals with u as variable.
                   When we apply substitution to the integration formulas from earlier sections, we obtain the
              following list.
                                   Z un du dx = Z un du =   1  un+1+C for n6= −1
                                         dx               n+1
                                    Z 1 du dx=Z 1 du=ln|u|+C
                                       u dx        u
                                    Z u du      Z u       u
                                      e  dx dx =  e du=e +C
                                    Z u du      Z u        1   u
                                      b  dx dx =  b du= ln(b) b +C for positive b 6= 1
                                 Z cosu du dx = Z cosu du = sinu+C
                                         dx
                                 Z sinu du dx = Z sinu du = −cosu+C
                                         dx
                                Z sec2u du dx = Z sec2u du = tanu+C
                                         dx
                                Z csc2u du dx = Z csc2u du = −cotu+C
                                         dx
                             Z secutanu du dx=Z secutanudu=secu+C
                                         dx
                             Z cscucotu du dx = Z cscucotu du = −cscu+C
                                         dx
                             Z p 1       du dx = Z p 1      du=sin–1u+C for a>0
                                 a2 −u2 dx           a2 −u2            a
                               Z  2 1  2 du dx = Z  2 1 2 du = 1 tan–1u+C for a>0
                                 a +u dx           a +u        a       a
                                Z coshu du dx = Z coshu du= sinhu+C
                                         dx
                                Z sinhu du dx = Z sinhu du = coshu+C
                                         dx
                   As will be shown in examples, we choose substitutions that put integrals we want to find in the
              forms of the first integrals in the above equations. The second integrals in these equations are then used
              in the actual calculations.
                   In many cases the appropriate substitution for a particular integral is one that simplifies the most
              complicated part of the integrand.
                p. 256 (3/20/08)                                                        Section 6.8, Integration by substitution
                Example 1         Find the antiderivative Z (x2 +1)5(2x) dx.
                Solution          Because the most complicated part of the integrand in this example is (x2+1)5, we try
                                  the substitution u = x2 +1 which would convert (x2 +1)5 into u5. Then we calculate
                                                du = du dx = d (x2 +1) dx = 2x dx:
                                                      dx       dx
                                  With this u and du, the given integral takes the form,
                                                    Z (x2 +1)5(2x) dx = Z u5 du:
                                        The u-integration can be carried out using the formula,
                                                         Z u5 du = 1u6 +C:
                                                                     6
                                  Then we substitute the formula u = x2 +1 for the final answer:
                                    Z (x2 +1)5(2x) dx = Z u5 du = 1u6 +C = 1(x2 +1)6 +C: 
                                                                     6           6
                       As with any indefinite integral, we can check Example 1 by differentiating the result. This requires
                the Chain Rule because the technique of substitution is derived from the Chain Rule. We obtain
                                      d 1(x2 +1)6 = 1[6(x2 +1)5] d (x2 +1) = (x2 +2)5(2x):
                                      dx 6               6            dx
                The formula for the indefinite integral in Example 1 is correct because its derivative is the original
                integrand.
                       Usually when we carry out an integration by substitution, we have to adjust a constant in the
                integrand to construct du. This procedure is illustrated in the next example.
                                                          Z   3√ 4
                Example 2         Perform the integration   x    x +16dx.
                Solution          Because the most complicated part of the integrand is the square root of x4+16 in the
                                  integral, we use the substitution u = x4 + 16, for which du = d (x4 +16) = 4x3 and
                                                                                         dx    dx
                                                         du = dudx = 4x3 dx:
                                                              dx
                                        To make this substitution, we construct du from the dx and other elements of
                                  the integral. First, we move the x3 next to the dx to have
                                              Z x3px4+16dx=Z px4+16(x3dx):
                                                                                              Z √
                                  The integral on the right of the last equation would equal      u du if it contained
                                  4x3dx instead of x3dx. Since the missing factor 4 is a constant, we can insert it if we
                                  compensate by dividing the entire integral by 4. We write
                 Section 6.8, Integration by substitution                                                p. 257 (3/20/08)
                                            Z x3px4+16dx=Z px4+16(x3dx)
                                                                 1Z p 4            3
                                                              = 4      x +16(4x dx)                                (4)
                                                                 1Z √         1Z    1=2
                                                              = 4      udu= 4     u    du
                                  To finish the example, we carry out the u-integration and put the result in terms of
                                  the original variable x by setting u = x4 + 16. We obtain
                              Z x3px4+16dx= 1Z u1=2 du= 1h 1 u3=2i+C
                                                   4              4 3=2
                                                 = 1 2u3=2 +C = 1u3=2 +C = 1(x4 +16)3=2 +C: 
                                                   4  3              6            6
                       Notice the transition from the first integral to the third integral in (4). Most calculations in
                                                                                                 Z   3√ 4
                mathematics involve simplifying expressions. Here, instead, we put the integral    x    x +16 dx in
                                            1Z √ 4           3                                   3
                the more complicated form 4       x +16 (4x dx) in order to construct du = 4x dx from the terms
                x3 dx in the original integral.
                                                          Z cos(√x)
                Example 3         Find the antiderivatives     √     dx.
                                                                 x
                                                                                      √      1=2   1 −1=2      1
                Solution          Thekeyhereis to recognize that the derivative of u =  x = x    is 2x     = √ ,so
                                                                                                             2 x
                                              1
                                  that du = √ dx. To make this substitution, we divide and multiply by 2 and obtain
                                            2 x
                                       Z      √          Z      √                 Z
                                          cos( x)                       1
                                             √     dx = 2    cos( x)    √ dx =2 cosudu
                                              x                        2 x
                                                                          √ 
                                                      =2sinu+C=2sin          x +C:
                Substitution in definite integrals
                Often the easiest way to evaluate a definite integral by substitution is to make the substitution in the
                corresponding indefinite integral.
                Example 4         Figure 1 shows the region between y =    10x    and the x-axis for
                                                                        (x2 +1)2
                                  0 ≤ x ≤ 3. Find its area.
                                                                      y                 y =    10x
                                                                                             (x2 +1)2
                                                                   3
                                                                   2
                                                                   1
                       FIGURE1                                               1        2        3      x
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