Page 459 - Mechanical Engineers' Handbook (Volume 2)
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450   Closed-Loop Control System Analysis












                                             Figure 6 Plots of ƒ(t) and ƒ(t    )u s (t    ).


                          T4. Multiplication of ƒ(t) by e   t
                                                     L[e   t ƒ(t)]   F(s    )                  (8)
                          T5. Integration Theorem
                                                                      1
                                                              F(s)  ƒ (0)
                                                   L[ ƒ(t) dt]                                 (9)
                                                               s      s
                             where ƒ (0)   ƒ(t) dt evaluated at t   0.
                                    1
                          T6. Final-Value Theorem. If ƒ(t) and dƒ(t)/dt are Laplace transformable, if lim t→  ƒ(t) exists,
                             and if F(s) is analytic in the right-half s-plane including the j  axis, except for a single
                             pole at the origin, then
                                                      lim ƒ(t)   lim sF(s)                    (10)
                                                      t→       s→0
                          T7. Initial-Value Theorem. If ƒ(t) and dƒ(t)/dt are both Laplace transformable, and if
                             lim s→  sF(s) exists, then

                                                       ƒ(0)   lim sF(s)                       (11)
                                                             s→0
                          Example 4 The time function of Example 3 can be written as
                                                 ƒ(t)   tu (t)   (t   T)u (t   T)             (12)
                                                                    s
                                                        s
                          and
                                             L[ƒ(t)]   L[tu (t)]   L[(t   T)u (t   T)]        (13)
                                                         s
                                                                       s
                          But
                                                                  1
                                                        L[tu (t)]                             (14)
                                                            s
                                                                 s  2
                          By using Eqs. (14) and (7) in Eq. (13), we get
                                                      1       1   1
                                               F(s)       e  Ts     (1   e  Ts )
                                                     s  2    s  2  s  2

           2.2  Transforming LTI Ordinary Differential Equations
                          The Laplace transform method yields the complete solution (the particular solution plus the
                          complementary solution) of linear differential equations. Classical methods of finding the
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