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Peridynamics for Isotropic Materials

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Peridynamic Theory and Its Applications

Abstract

The auxiliary parameters, C in Eq. 2.43 and A and B in Eq. 2.48, can be determined by using the relationship between the force density vector and the strain energy density, \( {W_{(k) }} \), at material point \( k \) given by Eq. 2.49 in the form,

$$ {{\mathbf{t}}_{(k)(j) }}\left( {{{\mathbf{u}}_{(j) }}-{{\mathbf{u}}_{(k) }},{{\mathbf{x}}_{(j) }}-{{\mathbf{x}}_{(k) }},t} \right)=\frac{1}{{{V_{(j) }}}}\frac{{\partial {W_{(k) }}}}{{\partial \left( {\left| {{{\mathbf{y}}_{(j) }}-{{\mathbf{y}}_{(k) }}} \right|} \right)}}\frac{{{{\mathbf{y}}_{(j) }}-{{\mathbf{y}}_{(k) }}}}{{\left| {{{\mathbf{y}}_{(j) }}-{{\mathbf{y}}_{(k) }}} \right|}}, $$

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Reference

  • Silling SA, Askari E (2005) A meshfree method based on the peridynamic model of solid mechanics. Comput Struct 83:1526–1535

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Madenci, E., Oterkus, E. (2014). Peridynamics for Isotropic Materials. In: Peridynamic Theory and Its Applications. Springer, New York, NY. https://doi.org/10.1007/978-1-4614-8465-3_4

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  • DOI: https://doi.org/10.1007/978-1-4614-8465-3_4

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  • Publisher Name: Springer, New York, NY

  • Print ISBN: 978-1-4614-8464-6

  • Online ISBN: 978-1-4614-8465-3

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