Variations in weaving patterns result in distinct stress distributions among the three weaves at identical pressures, and these distinctions amplify with increasing pressure. Notably, the plain weave, featuring the highest entanglement density, encounters substantially greater resistance while moving through the strands. Consequently, stress concentrates more prominently at the strands neighboring the impact center. With increasing pressure, the impact-induced chain sliding extended from the impact center to the far-field region of the weave, yet it did not reach the network boundaries. The minimal in-plane mechanical deformation in response to pressure indicates that thread-thread friction relaxation is the primary mechanism for energy dissipation in the plain weave. In contrast, the stress distribution in the basket weave appears to be the most dispersed among all three fabrics. This is due to the highest freedom of the strands, facilitated by the lowest entanglement density in the basket weave. Consequently, the cube can readily displace the strands away from its direction of travel to dissipate impact energy, resulting in considerable structural deformation compared to its initial configuration. The mixed weave, possessing a moderate number of entanglements, exhibits mechanical behavior resembling that of the plain weave at low pressure but akin to the basket weave at high pressure. Both thread-thread friction relaxation and strand slippage play roles in dissipating energy in the mixed weave. The calculation of the crossing displacement (CD) profiles between ES and mechanical state (MS) further supported the observation (Supplementary Information, Figure ). However, accurately quantifying the individual contributions of both pathways to the energy dissipation process remains challenging. Nevertheless, the findings highlight the significance of weaving pattern in determining the mechanical resistance of molecularly woven materials and the mechanism behind energy dissipation.