Boundary Value Problems in Linear Viscoelasticity by Dr. John M. Golden, Professor Dr. George A. C. Graham

By Dr. John M. Golden, Professor Dr. George A. C. Graham (auth.)

The classical theories of Linear Elasticity and Newtonian Fluids, although trium­ phantly based as mathematical constructions, don't properly describe the defor­ mation and movement of such a lot genuine fabrics. makes an attempt to symbolize the behaviour of actual fabrics less than the motion of exterior forces gave upward thrust to the technological know-how of Rheology. Early rheological experiences remoted the phenomena now labelled as viscoelastic. Weber (1835, 1841), discovering the behaviour of silk threats less than load, famous an immediate extension, via yet another extension over a protracted time period. On elimination of the burden, the unique size was once finally recovered. He additionally deduced that the phenomena of rigidity leisure and damping of vibrations should still take place. Later investigators confirmed that comparable results might be saw in different fabrics. The German institution mentioned those as "Elastische Nachwirkung" or "the elastic aftereffect" whereas the British institution, together with Lord Kelvin, spoke ofthe "viscosityofsolids". The common adoption of the time period "Viscoelasticity", meant to exhibit behaviour combining right­ ties either one of a viscous liquid and an elastic sturdy, is of modern starting place, now not getting used for instance via Love (1934), even though Alfrey (1948) makes use of it within the context of polymers. The earliest makes an attempt at mathematically modelling viscoelastic behaviour have been these of Maxwell (1867) (actually within the context of his paintings on gases; he used this version for calculating the viscosity of a gasoline) and Meyer (1874).

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Example text

The fact that 1(0) is zero, or G(O) is infinite, in this model means that there is no instantaneous response to a suddenly applied stress. Furthermore, stress relaxation under an applied strain is instantaneous since r is zero. 6). We remark that the Maxwell and Voigt models are equivalent to simple differential constitutive relations [for example, Christensen (1982)]. The standard linear solid is a convenient non-trivial but simple model, frequently used in theoretical analysis for purposes of illustrating techniques .

F. Williams (1975) discusses and uses these approaches. The dependence on temperature of the viscoelastic functions is clearly nonlinear, though the mechanical constitutive relation, discussed in Sect. 2, is linear. If the temperature variation is small, the theory may be completely linearized. 9) T= To+ 8 (t ) where 8(t) is a small quantity and To is the average background temperature. 11) where Go(t- to) is the limit of G(t, to) as L1 (I) vanishes, namely, the isothermal relaxation function .

10-12). 24) is given by G(t) = Go + ce I da G, (a)e - a t o Go 2: 0 , , G 1 (a) 2: 0 . 36) If G 1 (a) is a series of delta functions, one recovers the discrete spectrum. 37) ce go = Go+ I daGt(a) , o so that g(a) = - aGt(a) , ~ f g(a) J1(W) = go+ J da - - . 39) a- z for general complex values of z, off the positi ve real axis. Note that j1(i z) has a discontinuity or cut from z = ao to infinity where ao is the lowest value of a such that g(a) is non -zero , so that ao is in general a branch point.

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