Abstract
We used dynamic light scattering (DLS) and computer simulations based on the fluctuating lattice Boltzmann equation (LBE) method to study the short-time Brownian dynamics of colloidal particles that interact like hard spheres. The dynamics are characterized by a Q-vector-dependent diffusion coefficient ${\mathit{D}}_{\mathit{S}}$(Q). Using DLS, we have mesaured ${\mathit{D}}_{\mathit{S}}$(Q) in the vicinity of the main (first) peak in the structure factor S(Q) for samples of poly-methylmethacrylate particles at volume fractions \ensuremath{\varphi} ranging from dilute up to the disorder-order transition (i.e., crystallization at \ensuremath{\varphi}=0.494). In addition we have determined the short-time self-diffusion (${\mathit{D}}_{\mathit{S}}^{\mathit{S}}$) and collective-diffusion ${\mathit{D}}_{\mathit{S}}^{\mathit{C}}$ coefficients. We have extracted the same quantities from simulations of equilibrium configurations of hard spheres using a fluctuating lattice Boltzmann equation method for the fluid phase coupled to Newtonian mechanics for the colloidal particles. For all samples studied, close quantitative agreement is found between the results of the DLS experiments and the LBE simulations.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.