1978
DOI: 10.1007/bf00247742
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Dynamic stability of one-dimensional nonlinearly viscoelastic bodies

Abstract: is introduced both as a better approximation to reality and to obtain tractable (parabolic rather than hyperbolic) differential equations .Under this assumption , we show that the des irable theorems for the nonlinear equations : existence , uniqueness, and stability , follow from the analogous theorems for the linearized equations .

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Cited by 10 publications
(5 citation statements)
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“…On the other hand, (1.1)-(1.3) is not the only physically realistic dynamical system associated with potential (2.12), and the equivalence of the Liapounov definition and the energy criterion can properly be discussed within other dynamical systems. Indeed, progress has recently been made in a general justification of this equivalence within the context of viscoelasticity, see [6], [1], and [13]. The first two of these papers discuss stability in very general rod models; in particular, their stress-strain laws are not restricted to being linear as is assumed here.…”
Section: Resultsmentioning
confidence: 99%
“…On the other hand, (1.1)-(1.3) is not the only physically realistic dynamical system associated with potential (2.12), and the equivalence of the Liapounov definition and the energy criterion can properly be discussed within other dynamical systems. Indeed, progress has recently been made in a general justification of this equivalence within the context of viscoelasticity, see [6], [1], and [13]. The first two of these papers discuss stability in very general rod models; in particular, their stress-strain laws are not restricted to being linear as is assumed here.…”
Section: Resultsmentioning
confidence: 99%
“…We study the stability of a naturally straight Kirchhoff rod, aligned along the x-axis, subject to clamped boundary conditions, controlled end-rotation and terminal loads. We start with a general rod-energy in (6) and show that the diagonal rod-energy in (15) is the most general rod-energy compatible with any planar equilibrium state. We approach the stability analysis from a variational perspective and study the second variation of the diagonal rod-energy, including three-dimensional effects into the problem formulation.…”
Section: Discussionmentioning
confidence: 99%
“…Comment: We note that for the rod-energy (6) to have any straight equilibrium state characterized by θ(s) = C 1 and φ(s) = C 2 , for constants C 1 and C 2 , we must have M 13 = M 23 = 0.…”
Section: The Euler-lagrange Equationsmentioning
confidence: 99%
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“…Early work in this direction was done by Browne [1978], who considered the problem of existence, uniqueness and stability for the quasilinear partial differential equations governing the motion of nonlinearly viscoelastic onedimensional bodies.…”
Section: Introductionmentioning
confidence: 99%