Studies in active matter systems and in the collective motility of organisms
utilize a range of analytical approaches to formulate continuous kinetic models
of collective dynamics from the rules or equations describing agent
interactions. However, the derivation of these models often relies on
Boltzmann's hypothesis of "molecular chaos", often simply called statistical
independence. While it is often the simplest way to derive tractable models it
is not clear whether the statistical independence assumption is valid in
practice. In this work, we develop a Boltzmann-type kinetic model for the
nematic alignment of self-propelled rods where rod reorientation occurs upon
binary collisions. We identify relevant parameters and derive kinetic equations
for the corresponding asymptotic regime. By comparing numerical solutions of
the kinetic equations to an agent-based model that implements our microscopic
alignment rules, we examine the accuracy of the continuous model. The results
indicate that our kinetic model fails to replicate the underlying dynamics due
to the formation of clusters that violate statistical independence.
Additionally, we show that a mechanism limiting cluster formation helps to
improve the agreement between the analytical model and agent simulations. These
results highlight the need to improve modeling approaches for active matter
systems