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                                                V shell = V outer  − V inner
                                                         cylinder  cylinder

                                                                  2
                                                          2
                                                     = πr h − πr h
                                                          2
                                                                  1

                                                           2
                                                     = π r − r  1 2  h
                                                           2
                                                     = π(r 2 + r 1 )(r 2 − r 1 )h

                                                            r 2 + r 1
                                                     = 2π           h(r 2 − r 1 )
                                                               2


                                              r 2 + r 1
                                If we let r av =     represent the average radius and
                                                 2
                                 r = r 2 − r 1 represent the shell wall thickness, we may write


                                                      V shell = 2πr av h r



                                As  r → 0, and the number of shells within the solid →∞,
                                the sum of their volumes will approach the volume of the solid
                                of revolution.
                                    As a mnemonic device we may represent the average ra-
                                dius by r, the length of the shell by h, and the (infinitesimal)
                                shell wall thickness by dr. The volume of a typical shell may
                                be thought of as 2πrhdr and the total volume is



                                                                b

                                                      V = 2π      rhdr
                                                               a


                                In a given problem, dr will be replaced by either dx or dy, de-
                                pending upon the axis of rotation (dx if rotated about the
                                y axis and dy if rotated about the x axis). In either case,
                                the height h and the radius r must be expressed in terms of
                                the variable of integration. The limits of integration must cor-
                                respond to the variable of integration as well.

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