ΔF ≈ n kB T [1 + 3/2(D/d)]in which D and d are the diameters of the larger and smaller spheres, T is temperature, kB is Boltzmann's constant, and n is the volume fraction of small spheres. Of course, (1-n) is the volume fraction of large spheres, and the spheres are considered to be perfectly elastic. A more cogent summary of this effect, called depletion attraction, can be found in a paper about cellular organization, reference two.[2]
An artful arrangement of spheres in space. (Figure by Jonas De Kooning, from Wikimedia Commons). |