Additionally, the free energy profile, as a function of strand displacement during the sliding process along with x (weft) direction, is calculated using the umbrella sampling method to assess the kinetic barriers of various weaving architectures (Fig. ). Notably, negligible energy changes occur when strand displacement is below 1 nm, indicating the strands can move freely in a short interval within the weaving network despite the existence of entanglements. However, a mechanical barrier emerges between 1.5 to 2.5 nm, as evidenced by a sharp increase in free energy across different weaves. Consistent with structural stability trends, the plain weave, with the highest entanglement density and strongest interstrand interactions, exhibits the highest energy barrier (34 kJ/mol) for strand sliding. Conversely, energy requirements for strand sliding decrease to 23 and 12 kJ/mol in mix and basket weaves, respectively. These discoveries emphasize that strands in weaves with lower entanglement density exhibit increased flexibility and reduced strand-strand friction, facilitating easier sliding within the network (Supplementary Information, Figure ). was conducted on the pulling process of the selected polymer chain (y2) along the x direction in 1/1 Plain weave (navy), 2/1 Mix weave (green), and 2/2 Basket weave (pink).