2020
DOI: 10.1007/s42102-020-00042-x
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Homogenization of the 1D Peri-static/dynamic Bar with Triangular Micromodulus

Abstract: In peridynamics, boundary effects generally appear due to nonlocality of interparticle forces; in particular, end effects are found in 1D bars. In a previous work by Eriksson and Stenström (J Peridyn Nonlocal Model 2(2):205–228, 2020), a simple method to remove end effects in certain types of 1D bars, or to homogenize such bars, was presented for bars with constant micromodulus. In this work, which is a continuation of Eriksson and Stenström (J Peridyn Nonlocal Model 2(2):205–228, 2020), the homogenizing proce… Show more

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Cited by 3 publications
(3 citation statements)
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“…respectively, where V ( H x ) is the indicator function of H x . The peridynamic solution of equation (6) with C described by equation (12) is investigated in detail by both numerical and analytical methods in 1D case [10,28,31,35] and 2D case [37]. If we assume a linear microelastic material, then in general, the stiffness tensor for the linear microelastic materials can be shown to read as [7,33]…”
Section: Preliminariesmentioning
confidence: 99%
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“…respectively, where V ( H x ) is the indicator function of H x . The peridynamic solution of equation (6) with C described by equation (12) is investigated in detail by both numerical and analytical methods in 1D case [10,28,31,35] and 2D case [37]. If we assume a linear microelastic material, then in general, the stiffness tensor for the linear microelastic materials can be shown to read as [7,33]…”
Section: Preliminariesmentioning
confidence: 99%
“…It is assumed that f ^ ( x ^ , x ) is Riemann-integrable; that does not imply the bounding of f ^ ( x ^ , x ) as | x ^ x | 0 . In particular, for 1D case, the “peridynamic stress” σ ( x ) [29,31] is defined as…”
Section: Preliminariesmentioning
confidence: 99%
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