Field-induced alignment dynamics in suspensions of polarizable rods
Identificadores
URI: https://hdl.handle.net/10481/112559DOI: 10.1103/6xfz-s9q9
ISSN: 2470-0053
ISSN: 2470-0045
Metadatos
Mostrar el registro completo del ítemAutor
Zerón Jiménez, Iván Michael; Iturbe-Jabaloyes, Álvaro; Escañuela Copado, Adri; Moncho Jordá, Arturo; Patti, AlessandroEditorial
American Physical Society
Materia
Molecular Dynamics Polarizable rods Liquid crystals
Fecha
2026Referencia bibliográfica
Zerón Jiménez, I. M.; Iturbe-Jabaloyes, A.; Escañuela Copado, A. [et al]. (2026). Field-induced alignment dynamics in suspensions of polarizable rods. Phys. Rev. E. DOI: https://doi.org/10.1103/6xfz-s9q9
Patrocinador
Junta de Andalucía (P21_00015); Banco Santander; University of Granada (ACG265/6a); MICIU/AEI/10.13039/501100011033 and ERDF (PID2022-136540NB-I00); U.S. Army Research Office (W911NF-23-1-0099); European Union within - NextGenerationEU; Spanish Ministry of UniversitiesResumen
Fluids composed of polarizable particles exhibit tunable structural and functional properties when subjected to external electric fields, as the particles tend to reorient and align along the field direction. This field-induced anisotropy leads to pronounced changes in macroscopic properties, rendering these systems highly relevant for applications in nanotechnology. Understanding the dynamics of their response to external fields is crucial for designing responsive materials with fast and controllable actuation. In this work, we employ molecular simulation to study the behavior of suspensions of polarizable rod-like particles under the action of a uniform electric field, with particular attention to the transient dynamics associated with the switching on and off of the field. Induced dipoles
are modeled by independently varying charge magnitude and field strength, yielding a variable effective polarizability. The induced dipole moment of each rod is treated as an effective, externally controlled parameter, and collective polarization effects arising from local electric fields generated by neighboring particles are not explicitly included. The system is studied in a dense regime, where
interparticle interactions play a significant role and are implicitly controlled via pressure. We investigate how the characteristic response time depends on the competition between thermal motion and electric forces across a range of temperatures and field strengths. Our results reveal a rich dynamical behavior: at low to moderate field intensities, increasing the temperature significantly
reduces the response time, as thermal agitation facilitates reorientation. However, beyond a criti cal field strength, the response time plateaus, becoming effectively temperature-independent. This saturation indicates a regime where the aligning torque from the field dominates over thermal fluctuations, setting a lower bound for how fast the system can respond. More specifically, we show that
the alignment dynamics cannot be inferred from single-particle behavior alone, but emerge from a nontrivial interplay of field-induced dipolar torques, thermal fluctuations, and steric interactions at finite density, producing strongly temperature-dependent and nonlinear trends in both the nematic order parameter and response times.





