Page 50 - Engineering Plastics Handbook
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24   Introduction

        Maxwell spring-and-dashpot model
        The Maxwell model integrates the elastic and viscous behavior of a ther-
        moplastic by combining the spring and dashpot, providing a simple model
        for viscoelastic polymers. The spring and dashpot are in series [10].

                              Stress    = σ  = E ε
                                    spring  s
                              Stress     = σ  = η  d ε
                                    dashpot  d
                                                 dt
             where E = Young’s modulus, MPa (psi)
                   η = viscosity of newtonian fluid (oil) in dashpot, Pa⋅s
        Total strain ε= strain in the spring ε + strain in the dashpot ε d
                                          s
          The Maxwell model represents elastic creep, elastic recovery, and per-
        manent set. In general, the Maxwell model provides reasonable expres-
        sions for stress relaxation, and the Voigt-Kelvin model provides reasonable
        expressions for creep behavior. Creep occurs when a constant stress is
        instantly or rapidly applied over a period of time, and a corresponding
        strain increases over that time. The instant or rapid application of stress
        to a Maxwell model causes instantaneous stretching of the spring, which
        reaches an equilibrium strain ε. Under constant stress the dashpot con-
        tinues to extend with time. When the stress is released, the spring imme-
        diately contracts to an amount equal to its extension, which is elastic
        recovery. The dashpot does not recover, leaving a permanent set, which is
        the amount that the dashpot extended during the time the constant stress
        was applied. This model may not be easy to fit to experimental quantita-
        tive data, but it demonstrates some viscoelastic characteristics [11, 12].


        Voigt spring-and-dashpot model
        The Voigt model spring and dashpot are parallel. The model is a con-
        ventional concept for understanding stress and strain relationships
        when load is applied to a viscoelastic material [10].


        Voigt-Kelvin spring-and-dashpot models
        Spring-and-dashpot models are extended by the Voigt-Kelvin (V-K)
        model, which broadens linear viscoelastic concepts. The spring and
        dashpot are always in parallel. The V-K spring-and-dashpot models are
        useful for understanding creep behavior [11].
                                          +σ
                                    σ=σ s    d
        where σ= total stress acting on a V-K spring-and-dashpot model,
                  MPa (psi)
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