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@ -39,9 +39,10 @@ cutoff.
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</P>
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<P>In contrast to <A HREF = "pair_yukawa.html">pair_style yukawa</A>, this functional
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form arises from the Coulombic interaction between two colloid
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particles, screened due to the presence of an electrolyte.
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<A HREF = "pair_yukawa.html">Pair_style yukawa</A> is a screened Coulombic potential
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between two point-charges and uses no such approximation.
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particles, screened due to the presence of an electrolyte, see the
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book by <A HREF = "#Safran">Safran</A> for a derivation in the context of DVLO
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theory. <A HREF = "pair_yukawa.html">Pair_style yukawa</A> is a screened Coulombic
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potential between two point-charges and uses no such approximation.
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</P>
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<P>This potential applies to nearby particle pairs for which the Derjagin
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approximation holds, meaning h << Ri + Rj, where h is the
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@ -151,4 +152,9 @@ diameter.
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</P>
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<P><B>Default:</B> none
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</P>
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<A NAME = "Safran"></A>
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<P><B>(Safran)</B> Safran, Statistical Thermodynamics of Surfaces, Interfaces,
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And Membranes, Westview Press, ISBN: 978-0813340791 (2003).
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</P>
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</HTML>
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@ -34,9 +34,10 @@ cutoff.
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In contrast to "pair_style yukawa"_pair_yukawa.html, this functional
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form arises from the Coulombic interaction between two colloid
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particles, screened due to the presence of an electrolyte.
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"Pair_style yukawa"_pair_yukawa.html is a screened Coulombic potential
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between two point-charges and uses no such approximation.
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particles, screened due to the presence of an electrolyte, see the
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book by "Safran"_#Safran for a derivation in the context of DVLO
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theory. "Pair_style yukawa"_pair_yukawa.html is a screened Coulombic
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potential between two point-charges and uses no such approximation.
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This potential applies to nearby particle pairs for which the Derjagin
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approximation holds, meaning h << Ri + Rj, where h is the
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@ -145,3 +146,7 @@ diameter.
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"pair_coeff"_pair_coeff.html
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[Default:] none
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:link(Safran)
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[(Safran)] Safran, Statistical Thermodynamics of Surfaces, Interfaces,
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And Membranes, Westview Press, ISBN: 978-0813340791 (2003).
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