2014
DOI: 10.1016/j.ijadhadh.2013.09.043
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Development of a constitutive hyperelastic material law for numerical simulations of adhesive steel–glass connections using structural silicone

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Cited by 39 publications
(21 citation statements)
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“…The phenomenological hyperelastic model based on strain energy density was used to characterize the deformation behavior of the Sikaflex adhesive that is incompressible and hyperelastic as discussed in Section . The strain energy density W can be written in a polynomial function of the first and second strain invariants I 1 and I 2 ndtrueprefixmaxt1=()h SEI trueprefixmax22κp el ϕϕnormalop[]20.33emκp el 0.33emϕp1[]fnormald1υnormals2ΓnormaldωEnormalSϕɛsnormalo+ɛc¯χ22where C ij are the material constants. The strain invariants I 1 and I 2 can be expressed in terms of the stretch ratios λ 1 , λ 2 , and λ 3 using the following equations I1=λ12+λ22+λ32 I2=λ12λ22+λ22λ32+λ12λ32…”
Section: Modified Constitutive Model For Sikaflex Adhesivesmentioning
confidence: 99%
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“…The phenomenological hyperelastic model based on strain energy density was used to characterize the deformation behavior of the Sikaflex adhesive that is incompressible and hyperelastic as discussed in Section . The strain energy density W can be written in a polynomial function of the first and second strain invariants I 1 and I 2 ndtrueprefixmaxt1=()h SEI trueprefixmax22κp el ϕϕnormalop[]20.33emκp el 0.33emϕp1[]fnormald1υnormals2ΓnormaldωEnormalSϕɛsnormalo+ɛc¯χ22where C ij are the material constants. The strain invariants I 1 and I 2 can be expressed in terms of the stretch ratios λ 1 , λ 2 , and λ 3 using the following equations I1=λ12+λ22+λ32 I2=λ12λ22+λ22λ32+λ12λ32…”
Section: Modified Constitutive Model For Sikaflex Adhesivesmentioning
confidence: 99%
“…Note that the third strain invariant I3=λ12 λ22 λ32 = 1 is constant for incompressible adhesives; thus it is not included in the strain energy density W (Equation ) …”
Section: Modified Constitutive Model For Sikaflex Adhesivesmentioning
confidence: 99%
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