📝 SummarXiv

Abstract

The role of active stress on the conformational dynamics of a polymer has drawn significant interest due to its potential applications in understanding the energy landscape of protein structures, buckling of biopolymers, genomic spatial organization, and their large scale coherent dynamics. We present a model of bidirectional active force that acts along the polymer's tangent, with its direction stochastically reversing between head to tail and tail to head orientations. The active polymer shows a structural transition from a random coil like state to a compressed state with variations in the active force, directional (polarity) reversal rate, and their fraction. Furthermore, the polymer re-swells and stretches more than its passive limit for a large active force. The polymer's radius of gyration follows the ideal chain-like scaling relation in both the compressed and swelled states. The bidirectional active force also drives dynamical transitions, where the effective diffusivity abruptly shifts from a linear to quadratic increase. Similarly, in the regime of large activity, the linear decrease of the longest relaxation time of the polymer changes to a power law behavior. We have shown that the active polymer's conformational, relaxation, and diffusive behaviors display a transition from an active polar linear polymer model (APLP) to an active Brownian particle (ABP) polymer model with the increase in the fraction of the opposite polarity and their reconfiguration time.