Misc updates and style fixes
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@ -64,7 +64,7 @@ go to zero, avoiding discontinuities, as bonds approach the critical strain
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.. math::
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w = 1.0 - \left( \frac{r - r_0}{r_0 \epsilon_c} \right^4 .
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w = 1.0 - \left( \frac{r - r_0}{r_0 \epsilon_c} \right)^8 .
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Finally, an additional damping force is applied to the bonded particles.
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This forces is proportional to the difference in the
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@ -38,8 +38,15 @@ normal velocity of particles
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F_D = - \gamma w (\hat{r} \bullet \vec{v})
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where :math:`\gamma` is the damping strength, :math:`\hat{r}` is the
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radial normal vector, and :math:`\vec{v}` is the velocity difference
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between the two particles.
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radial normal vector, :math:`\vec{v}` is the velocity difference
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between the two particles, and :math:`w` is a smoothing factor.
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This smoothing factor is constructed such that damping forces go to zero
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as particles come out of contact to avoid discontinuities. It is
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given by
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.. math::
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w = 1.0 - \left( \frac{r}{r_c} \right)^8 .
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This pair style is designed for use in a spring-based bonded particle model.
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It mirrors the construction of the :doc:`bpm/spring <bond_bpm_spring>` bond style.
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