Page 52 - Engineering Plastics Handbook
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26   Introduction

          To calculate the shear modulus for the elastic portion (below the elas-
        tic limit), use
                                         ∆τ
                                     G =
                                         ∆γ
        where G is the slope of the curve.

          Formulas for linear viscoelastic models can be applied to tensile defor-
        mation as well as shear deformation by replacing the shear stress τ
        with tensile stress σ, shear strain γ with tensile strain ε, shear modu-
        lus G with Young’s tensile modulus E, and newtonian shear viscosity η
        with Trouton’s tensile viscosity η [11–13].
                                       e
        Shear viscosity and shear modulus
        Shear viscosity with the dashpot depicting a linear newtonian fluid is
        calculated by
                                          τ
                                      η =
                                          γ*
        where η= shear viscosity of a newtonian fluid in dashpot, Pa⋅s (cP)
               τ= shear stress, MPa (psi)
                                   −1
              γ* = shear strain rate, s
            10 P = 1000 centipoise (cP)
          Two conditions are that (1) a constant stress is suddenly applied, and
        (2) strain is assumed to be zero when the stress is applied. Shear mod-
        ulus G from a linear elastic model depicting a hookean solid is deter-
        mined by G =τ/γ [11].


        Poisson’s Ratio
        Poisson’s ratio ν is the ratio of transverse contraction to longitudinal
        extension in the stretching direction. For the purposes of visualization
        only, picture a tough rubbery sheet, push a dull thin rod into the sheet,
        and you have transverse contraction and longitudinal extension. In a
        practical mode, Poisson’s ratio is about 0.33 for many solid plastics and
        just under 0.5 for elastomers.
                                       − ε
                                   ν =   transverse
                                       ε
                                        longitudinal
        The transverse strain −ε transverse  is defined as negative, and the longitudi-
        nal strain ε longitudinal  is defined as positive so that ν has a positive value.
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