First synthesized in significant quantities in the 1990s, carbon nanotubes (CNTs) have extremely desirable electronic, optical, and mechanical properties. [1][2][3] Exploitation of their electronic, optical, and mechanical properties has, therefore, been a focus of research over the past few decades. It has resulted in their use in a wide range of applications, including wearable, transparent and flexible electronics, gas sensing, catalysis, resistive switching, space exploration, and more. [2,[4][5][6][7][8][9][10][11][12][13] In many of these applications, a CNT network is fabricated as a film, synonymously referred to as a fabric. An example of the structure of a disordered film is shown in Figure 2 in the study by Lyons et al. [14] Due to the complexity of the fabric structure, the desirable properties of a single nanotube do not directly translate into the characteristics of the CNT film as a whole. As a result, significant research has been devoted to understanding how the interaction between individual nanotubes affects electrical and mechanical properties of a CNT fabric.Efforts have been made to understand the conductivity of CNT fabrics and they can be divided into two camps, those that parameterize larger-scale empirical models [14][15][16] and those that are based on CNT film structural models. [17][18][19][20] In all these studies, the total resistance of the film is controlled by the relatively high electrical resistance of quantum-mechanical tunneling of electrons from one CNT to another. In contrast (at low voltages), individual CNTs behave as ballistic conductors, demonstrating quantized conductance