1996
DOI: 10.1007/bf00042789
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Void formation and growth in a class of compressible solids

Abstract: A new class of compressible elastic solids, which includes the Blatz-Ko material as a special case, is proposed. A closed-form solution is constructed and studied for a bifurcation problem modeling void formation in this class of compressible elastic solids. The relation between the void-formation condition and the material parameters is obtained analytically. An energy comparison of the void-formation deformation and the homogeneous expansion deformation is carded out.

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Cited by 8 publications
(9 citation statements)
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“…It is easy to obtain the numerical solutions of 2 for different values of the load parameter Q = q/p from (6). For a neo-Hookean cube, Rivlin tn'n3 presented similar formula.…”
Section: Deformation and Stress Of Rectangular Plate Without Voidmentioning
confidence: 90%
“…It is easy to obtain the numerical solutions of 2 for different values of the load parameter Q = q/p from (6). For a neo-Hookean cube, Rivlin tn'n3 presented similar formula.…”
Section: Deformation and Stress Of Rectangular Plate Without Voidmentioning
confidence: 90%
“…Spherically symmetric deformations of hollow and solid spheres in the conventional isotropic compressible theory involving a strain energy density W (I 1 , I 2 , I 3 ) have been the object of much previous study with respect to inflation and cavitation. In addition to the work summarized by Horgan and Polignone [1], later work includes Lei and Chang [14], Murphy and Biwa [15], Shang and Cheng [16], Pericak-Spector et al [17], and Murphy [18]. In general, closed form integration techniques are easily obtained only for special forms of the stored energy density W (I 1 , I 2 , I 3 ).…”
Section: Spherical Geometry Formulationmentioning
confidence: 98%
“…For the prescribed dead load p 0 > 0, if c ≥ 0 is a solution of (24), then τ rr (0+) can be obtained by (23). For any prescribed dead load p 0 > 0, c = 0 is a solution of (24) and τ rr (0+) is given by (23), so r(R) = R and p(R) = −p 0 are the trivial solutions of the spherical symmetric deformation for an incompressible hyper-elastic sphere.…”
Section: Cavitated Bifurcation For Incompressible Hyper-elastic Spherementioning
confidence: 99%
“…Kakavas [21] studied the influence of cavitation on the stress-strain fields of the compressible Blatz-Ko material in the case of finite deformations. Further references are [22][23][24].…”
Section: Introductionmentioning
confidence: 99%