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262                   Finite Element Modeling and Simulation with ANSYS Workbench



                                                            f(t)








            FIGURE 8.1
            A dynamic force applied to the structure.


                                          k         f = f(t)
                                                 m          m—mass
                                          c                 k—stiffness
                                                            c—damping
                                                            f(t)—force
                                   FBD:  ku  m     f(t)
                                      cu
                                                     x, u

            FIGURE 8.2
            A single DOF system with damping.


            8.2.1  A Single DOF System
            From the free-body diagram (FBD) and Newton’s law of motion (ma = f), we have:

                                                ft −
                                           mu    = ()  ku −  cu

            that is

                                          mu    +  cu   +  ku =  ft()                   (8.1)

                                           /
                                                                       2
            where u is the displacement,    u =  dudt the velocity, and    u =  d udt  the acceleration.
                                                                   2
                                                                    /
            Free Vibration (no applied force to the mass or f(t) = 0):
              Free vibration occurs when a mass is moved away from its rest position due to initial
            conditions.
              Assuming zero damping (c = 0) in a free vibration, Equation 8.1 becomes:

                                             mu    +  ku = 0                           (8.2)


              The physical meaning of this equation is: inertia force + elastic/stiffness force = 0.
              Although there is no applied force, the mass can have nonzero displacement or experience
            vibrations under the initial conditions. To solve for such nontrivial solutions, we assume:

                                             u(t) = U sin ωt

            where ω is the circular frequency of oscillation and U the amplitude. Substituting this into
            Equation 8.2 yields:
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