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Accuracy and stability of single-step methods                       189



                                θ                              θ


                            2
                    ω    1            staiit      ω                   staiit
                                      ndar                   2       ndar
                        2

                          1    2                         1    2
                                e  ω                           e  ω
                               θ                                θ  1

                                                                   2
                                2
                    ω                             ω



                                                        2
                          1    2                         1    2
                                e  ω                           e  ω

                  Figure 4.11 Magnitude of the growth coefficient vs. real and imaginary parts of the dimensionless
                  time step. The region of absolute stability lies within the contour of 1.

                            eicit er    ∆t  2             eicit er    ∆t  2
                       2
                       1
                    t                           t


                      1
                                                 1
                                 1           2                 1          2
                                   t                            t
                            iicit er    ∆t  2             iicit er    ∆t  2
                       2
                                                    2
                       1
                                                    1
                    t                             t
                                                   1

                      1                            2
                                2                                         1
                                   t                            t
                  Figure 4.12 Numerical trajectories for dx/dt =−x, x(0) = 1 for explicit Euler and implicit Euler
                  at various time steps less than 2 and greater than 2. Upper right shows loss of absolute stability for
                  the explicit method. Time steps below 2 are {0.1, 0.5, 1.0, 1.5, 1.9}. Time steps above 2 are {2.1, 2.5,
                  2.75, 3}.
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