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                    FIGURE 3-9  Dissipated pseudo-strain energy in a beam fatigue test.
                       If the material is viscoelastic instead of being elastic as in the previous examples, a
                    certain amount of the energy that is expended with each load cycle is used up in
                    overcoming the viscous resistance of the material and not in contributing to the damage
                    of the material. In order to have the correct relation between the apparent and real
                    relaxation moduli of the material, it is necessary to correct for the amount of dissipated
                    energy that is not used directly in damaging the material. In order to make this correction,
                    the concept of pseudostrain energy has been introduced. Although the pseudostrain
                    concept will be presented in detail in Chap. 7, it is repeated here to compliment slight
                    differences in its application to the work presented in this chapter. Pseudostrain energy
                    is the amount of dissipated energy that is available to damage the material. A typical
                    fatigue test on a beam fatigue sample is illustrated in Fig. 3-9.
                       As the load is applied and then reduced it is necessary to apply compressive force in
                    the opposite direction in order to return the beam to its original unstrained location. The
                    graph of applied load versus deflection must be corrected to subtract the amount of
                    energy that has been used to overcome the viscous resistance of the beam to upward and
                    downward movement. This can be done by first finding out what the relaxation modulus
                    of the beam material is by running a relaxation test on the material at a low stress level.
                    Then the beam strain rate history is combined with the convolution integral to predict
                    the linear viscoelastic stress history of the beam s  (t). If this calculated linear viscoelastic
                                                            LVE
                    stress is plotted against the measured stress and a straight line such as shown in Fig. 3-10


                                                                  Linear
                                            Measured stress s  x  x  x  Nonlinear
                                                           x




                                               x
                                             Calculated viscoelastic stress s  LVE


                    FIGURE 3-10  Measured viscoelastic stress versus calculated linear viscoelastic stress.
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