Worked Example 11.8-1


© 2001 by Karl Hahn
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1) The example is to integrate

   
  ______
 √1 - x2
         dx                                                   eq. 11.8-27
     x
Simple substitution of  u = 1 - x2  won't work on this one because there's nothing you can do about the dx. Trig substitution of  sin(u) = x  does work, but it is just one of several successful attacks you can make on this one. The other kind of attack is to manipulate it into algebraic equivalents of the integrand that we do know how to integrate using simple substitution. Two possible manipulations pop into my head whenever I see a quotient like this. One is to multiply the numerator and denominator by the numerator. The other is to multiply the numerator and denominator by the denominator. Either one of these attacks leads to a solution. So I will show you both because on an exam you would have flipped a coin in your head to choose one, and then followed the one you chose to its conclusion. There's no real way to tell up front which is the shorter road. Here is the longer road first:

Multiply numerator and denominator by the numerator. This gives

   

   1 - x2
    ______ dx                                                 eq. 11.8-28a
 x √1 - x2
Now you can break it up into two pieces

   

   1 - x2
    ______ dx  =
 x √1 - x2

  

     dx
    ______  -
 x √1 - x2

  

   x dx
  ______                  eq. 11.8-28b
 √1 - x2
The right-hand piece succumbs easily to simple substitution. The left-hand piece needs more manipulation. To get the x by itself in the numerator of that piece, we multiply its numerator and denominator by x.

   

   1 - x2
    ______ dx  =
 x √1 - x2

  

    x dx
     ______  -
 x2 √1 - x2

  

   x dx
  ______                 eq. 11.8-28c
 √1 - x2
Now we can substitute

   u  =  1 - x2
hence

1 - u  =  x2
and

  1
-   du  =  x dx      eq. 11.8-28d
  2
We get

   

   1 - x2
    ______ dx  =
 x √1 - x2

    1
  −  
    2

 

     du
         _
 (1 - u)√u

     1
  +   
     2

 

 du
  _                 eq. 11.8-28e
 √u
We could go and integrate the right-hand piece at this point. But we still have another step to go before we integrate the left-hand piece. So I'm going to wait. To integrate the left-hand piece we employ the trick we discussed earlier about substituting for square
roots.

   v2  =  u
and

2v dv  =  du                                  eq. 11.8-29a
Just for thrills, I'm going to apply this substitution to both the right-hand and left-hand
pieces.

     1
   -  
     2

 

     du
         _
 (1 - u)√u

     1
  +   
     2

 

 du
  _  =  -
 √u

 

   dv
         +
 1 - v2

  


 dv            eq. 11.8-29b

I'm going to stop here and do the second approach until it leads to the identical situation as we have above:

Multiply numerator and denominator by the denominator. This gives

   
    ______
 x √1 - x2
           dx                                                eq. 11.8-30a
     x2
This setup immediately lets us substitute

   u  =  1 - x2
hence

1 - u  =  x2
and

  1
-   du  =  x dx      eq. 11.8-28d
  2
to get

   
    ______
 x √1 - x2
           dx  =
     x2

    1
  −  
    2

 
  _
 √u du
                                       eq. 11.8-30b
 1 - u
Now apply the substitution

   v2  =  u
and

2v dv  =  du                                  eq. 11.8-29a
and you get

     1
   −  
     2

 
  _
 √u du
        =  -
 1 - u

 

  v2 dv
                                            eq. 11.8-30c
 1 - v2
I'll leave it to you to apply
polynomial long division to this and apply the remainder rule to the result to get back equation 11.8-29b

Or we could have used trig substitution. The substitution is

   sin(u)  =  x
and
               ___________
cos(u) du  =  √1 - sin2(u) du  =  dx      eq. 11.8-31a
Pursuing this line of attack, we find

   

 1 - sin2(u)
             du  =
    sin(u)

  

 cos2(u) sin(u)
                du  =                    eq. 11.8-31b
     sin2(u)
                                      
 cos2(u) sin(u)
                du
   1 - cos2(u)
Now substitute

   v  =  cos(u)
and

dv  =  -sin(u) du                         eq. 11.8-31c
and we find ourselves right back at right-hand side of equation 11.8-30c, which, in turn, leads back to equation 11.8-29b. The point is that even with integrals that appear hard at first, there is often more than one way that you can arrive at useful results.

To finish this one, we observe that the right-hand side of equation 11.8-29b consists of an integral that we have done several times before by partial fractions plus a second integral that is trivial. The result of all this is


   -


 

   dv
         +
 1 - v2

  


 dv  =


    1
  -   ln
    2



1 + v
     
1 - v




  +  v  +  C             eq. 11.8-32a

Now substitute back using equation 11.8-29a.

     1
   -   ln
     2



1 + v
     
1 - v



                   1
  +  v  +  C  =  -   ln
                   2


     _
1 + √u
     _
1 - √u



      _
  +  √u  +  C      eq. 11.8-32b

Now substitute back again using equation 11.8-28d

     1
   -   ln
     2


     _
1 + √u
     _
1 - √u



      _
  +  √u  +  C  =                                 eq. 11.8-32c


                         1
                       -   ln
                         2


     ______
1 + √1 - x2
     ______
1 - √1 - x2



      ______
  +  √1 - x2  +  C

We can simplify the stuff inside the log by multiplying both its numerator and denominator by its numerator. We end up with perfect squares on both top and bottom, so we can use log identities to carry the one-half into the log and to flip the result to get rid of the minus sign to boot (be sure to do all these steps yourself on paper). We end up with

   
  ______
 √1 - x2
         dx  =
     x


   ln




     x
     ______
1 + √1 - x2



      ______
  +  √1 - x2  +  C            eq. 11.8-32d

Taking the derivative of this result is an interesting adventure, and you should try it. It's easier if you break the log expression up into the log of the numerator minus the log of the denominator. There are lots of cancellations and simplifying to be done as you go, and with no mistakes you will end up with the original integrand.


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