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@ -410,7 +410,7 @@ discussion above. To match the Mindlin solution, one should set
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.. math::
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G_{eff} = \left(\frac{2-\nu_i}{G_i} + \frac{2-\nu_j}{G_j}\right)^{-1}
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where :math:`G` is the shear modulus, related to Young's modulus :math:`E`
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and Poisson's ratio :math:`\nu` by :math:`G = E/(2(1+\nu))`. This can also be
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achieved by specifying *NULL* for :math:`k_t`, in which case a
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@ -476,8 +476,8 @@ created without the rescaling above (:ref:`Walton <WaltonPC>` ).
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force described above. By re-scaling :math:`\xi`, *mindlin_rescale*
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effectively re-scales the tangential force twice, i.e., proportionally to
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:math:`a^2`. This peculiar behavior results from use of the accumulated
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tangential displacement to characterize the contact history. Although
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*mindlin_rescale* remains available for historic reasons and backward
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tangential displacement to characterize the contact history. Although
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*mindlin_rescale* remains available for historic reasons and backward
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compatibility purposes, it should be avoided in favor of *mindlin_rescale/force*.
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The *mindlin_rescale/force* option uses the same form as *mindlin/force*,
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@ -447,7 +447,7 @@ void PairGranular::compute(int eflag, int vflag)
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history[0] -= rsht*nx;
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history[1] -= rsht*ny;
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history[2] -= rsht*nz;
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// also rescale to preserve magnitude
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prjmag = sqrt(history[0]*history[0] + history[1]*history[1] +
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history[2]*history[2]);
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@ -572,7 +572,7 @@ void PairGranular::compute(int eflag, int vflag)
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history[rhist0] *= scalefac;
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history[rhist1] *= scalefac;
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history[rhist2] *= scalefac;
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history[rhist0] += vrl1*dt;
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history[rhist1] += vrl2*dt;
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history[rhist2] += vrl3*dt;
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