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The shape of the depletion force suggests to fit the numerical data displayed in Fig. 5 with the following empirical function: Ffit (r) =A [1-f (α r)] (rΒ +ar) -bf (α r) e-κr cos [2π δ (r- r0)], with {A,α,Β,a,b,κ,δ, r0 } the set of fitting parameters. Clearly, this equation does not have any ambition to be a proper description of the functional dependence of depletion forces upon distance; it has just been used to smooth the numerical data. In the equation, one can recognize two regimes: The attractive well described by the term rΒ +ar and the subsequent oscillatory damped part described by the exponential-sinusoidal term. The factor f (α r) and its complement to unity have the role of switching continuously from one regime to the other.
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The shape of the depletion force suggests to fit the numerical data displayed in Fig. with the following empirical function: Ffit (r) =A [1-f (α r)] (rΒ +ar) -bf (α r) e-κr cos [2π δ (r- r0)], with {A,α,Β,a,b,κ,δ, r0 } the set of fitting parameters. Clearly, this equation does not have any ambition to be a proper description of the functional dependence of depletion forces upon distance; it has just been used to smooth the numerical data. In the equation, one can recognize two regimes: The attractive well described by the term rΒ +ar and the subsequent oscillatory damped part described by the exponential-sinusoidal term. The factor f (α r) and its complement to unity have the role of switching continuously from one regime to the other. The above functional form has proven to be quite effective for n=6 and not so much for n=12 (see Fig.); actually, for the computation of the potential W (r) by integrating the force, the Akima spline method was used instead.
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