# Morphology and Kinetics of Random Sequential Adsorption of Superballs: From Hexapods to Cubes

Source: [Morphology and Kinetics of Random Sequential Adsorption of Superballs: From Hexapods to Cubes](<https://www.sota2.com/research/paper/68fa3a851e209131ce8cb5ec>)

Collection index: [llms.txt](<https://www.sota2.com/research/llms.txt>)

Data updated: 2025-10-25T00:06:40.080Z

Authors: Pooria Yousefi, Hessam Malmir, Muhammad Sahimi

Published: 2019-05-30T16:14:43.000Z

## Abstract

Superballs represent a class of particles whose shapes are defined by ${\|x\|}^{2p}+{\|y\|}^{2p}+{\|z\|}^{2p} \\le R^{2p}$, with $p\\in(0,\\infty)$ being the "deformation parameter". $0\<p\<0.5$ represents a family of hexapodlike (concave octahedrallike) particles, while for $0.5\\leq p\<1$ and $p\>1$ one has, respectively, families of convex octahedrallike and cubelike particles, with $p=1,\\;0.5$ and $\\infty$ representing spheres, octahedra, and cubes. Colloidal zeolite suspensions, catalysis, and adsorption, as well as biomedical magnetic nanoparticles are but a few of the applications of packing of superballs. We introduce a universal method for simulating random sequential adsorption of superballs, which we refer to as "low-entropy" algorithm, in contrast with the conventional algorithm that represents a "high-entropy" method. The two algorithms yield, respectively, precise estimates of the jamming fraction $\\phi\_\\infty(p)$ and $\\nu(p)$, the exponent that characterizes the kinetics of adsorption at long times $t$, $\\phi(\\infty)-\\phi(t)\\sim t^{-\\nu(p)}$. Precise estimates of $\\phi\_\\infty(p)$ and $\\nu(p)$ are obtained and shown to be in agreement, in some special limits, with the existing analytical and numerical results.

## Recorded benchmark results

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## Original sources and implementation

[Original paper](<https://arxiv.org/abs/1905.13151>)

[PDF](<https://arxiv.org/pdf/1905.13151.pdf>)
