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Momentum transfer in suspensions is mediated through the suspending fluid. However, equilibrium properties of a suspension of hard spheres in an inert incompressible medium are equivalent to those of a fluid of hard spheres undergoing Newtonian dynamics in empty space. Therefore, in equilibrium considerations we can entirely neglect the effect of the suspending fluid.
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In our previous paper (Ref.), we plotted the modified film tension rather than Eq.. However, since the quantities γc and γ c differ only by the normal pressure multiplied by a constant factor [cf. Eq.], the equilibrium conditions γc =const and pc⊥ =const imply that the modified film tension γ c is also constant in the film.
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