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Theoretical framework

CabanaPD uses the peridynamic formulation1 2. Given a bounded body \(\mathcal{B}\subset \mathbb{R}^3\), the equation of motion for a material point \({\bf x} \in \mathcal{B}\) at time \(t\geqslant 0\) is:

\[ \rho \frac{\partial^2 {\bf u}}{\partial t^2}({\bf x},t) = \int_{\mathcal{H}_{\bf x}} {\bf f}({\bf x}^\prime, {\bf x},t) dV_{\bf x^\prime} + {\bf b}({\bf x},t), \]

where \(\mathbf{x}\) denotes the position in the reference configuration, \(\rho\) is the mass density, \({\bf u}\) is the displacement field, \({\bf f}\) is the bond force function, \({\bf b}\) is a prescribed body force density, and \(\mathcal{H}_{\bf x}\) is the nonlocal neighborhood of \({\bf x}\) defined by $$ \mathcal{H}_{\bf x}:=\lbrace {\bf x}^\prime \in \mathcal{B}: \lVert{\bf x}^\prime -{\bf x}\rVert\leqslant \delta \rbrace, $$ where \(\|\cdot\|\) denotes the Euclidean norm, \(\delta>0\) is the maximum distance over which nonlocal interactions occur (called the horizon), and \({\bf x}^\prime\in\mathcal{H}_{\bf{x}}\) denotes a neighboring material point.

References


  1. S.A. Silling, Reformulation of elasticity theory for discontinuities and long-range forces, Journal of the Mechanics and Physics of Solids 48(1) (2000): 175-209. doi:10.1016/S0022-5096(99)00029-0 

  2. S.A. Silling, M. Epton, O. Weckner, J. Xu, and E. Askari, Peridynamic states and constitutive modeling, Journal of Elasticity 88 (2007): 151–184 (2007). doi:10.1007/s10659-007-9125-1