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Finite Strain Shape Memory Alloys Modeling - Scuola di Dottorato in ...

Finite Strain Shape Memory Alloys Modeling - Scuola di Dottorato in ...

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or, <strong>in</strong> components:⎡⎢∂σ⎣∂σab abab= + vc(3.80)⎢ ∂t∂x⎥cσ⎤⎥⎦Next, assume that σ transforms objectively, that is:Tσ = Q() t σQ () t(3.81)From equations (3.79) and (3.81), it follows that:σ T T T= Q () t σQ () t + ⎡ () t () t ⎤ − ⎡ () t () t ⎤⎢⎣ Q Q ⎥⎦ σ σ ⎢⎣ Q Q ⎥(3.82)⎦that is the material time derivative of the Cauchy stress tensor is not objective.Objective rates are essentially mo<strong>di</strong>fied time derivatives of the Cauchy stress tensorconstructed <strong>in</strong> order to preserve objectivity.It is possible to show that any possible objective stress rate is a particular case offundamental geometric object known as Lie derivative (Simo and Marsden, 1984).• The Lie derivative of the Kirchhoff stress tensor or Trusdell stress rate isdef<strong>in</strong>ed as:⎧∂⎫Lvτ = ⎨⎪F ⎡ ( φ)⎤ ⎪ φt⎢⎣F τ F ⎥⎦F ⎬⎪⎩∂⎪⎭⎧⎪ ∂ST⎫⎪ −1= ⎨FF ⎬φ⎪⎩∂t⎪⎭−1 −TT −1(3.83)Us<strong>in</strong>g the expression for the derivative of the <strong>in</strong>verse:50

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