2007
DOI: 10.4064/ba55-1-3
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A Dynamic Frictionless Contact Problem with Adhesion and Damage

Abstract: Summary. We consider a dynamic frictionless contact problem for a viscoelastic material with damage. The contact is modeled with normal compliance condition. The adhesion of the contact surfaces is considered and is modeled with a surface variable, the bonding field, whose evolution is described by a first order differential equation. We establish a variational formulation for the problem and prove the existence and uniqueness of the solution. The proofs are based on the theory of evolution equations with mono… Show more

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Cited by 10 publications
(12 citation statements)
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“…(14) represents the equation of motion where ρ denotes the material mass density, (15) and (16) are the displacement and traction boundary conditions, respectively. Condition (17) represents the normal damped response condition and a local friction law described above. (18) represents a homogeneous Neumann boundary condition where ∂α ∂ν represents the normal derivative of α.…”
Section: Problem Statementmentioning
confidence: 99%
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“…(14) represents the equation of motion where ρ denotes the material mass density, (15) and (16) are the displacement and traction boundary conditions, respectively. Condition (17) represents the normal damped response condition and a local friction law described above. (18) represents a homogeneous Neumann boundary condition where ∂α ∂ν represents the normal derivative of α.…”
Section: Problem Statementmentioning
confidence: 99%
“…Condition (17) represents the normal damped response condition and a local friction law described above. (18) represents a homogeneous Neumann boundary condition where ∂α ∂ν represents the normal derivative of α. In (19), we consider the initial conditions where u 0 is the initial displacement, v 0 the initial velocity and α 0 is the initial damage.…”
Section: Problem Statementmentioning
confidence: 99%
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“…[6,11,12,15,19,20] and the recent references [1,13]. Contact problems for elastic-viscoplastic materials of the form (1.2) are studied in [2,5,18,20]. The damage subject is extremely important in design engineering, since it directly affects the useful life of the designed structure or component.…”
Section: U(t)) + Eε(u(t)) (13)mentioning
confidence: 99%
“…When β = 1 there is no damage in the material, when β = 0 the material is completely damaged, when 0 < β < 1 there is partial damage and the system has a reduced load carrying capacity. Contact problems with damage have been investigated in [10,16,17,18,20]. In this paper the inclusion used for the evolution of the damage field is…”
Section: U(t)) + Eε(u(t)) (13)mentioning
confidence: 99%