2006 AIChE Annual Meeting
(692f) The Viscoelastic Behavior of Perfluoropolyether Lubricant Via Molecular Dynamics
Authors
In this study, we first conducted the equilibrium molecular dynamics simulations to investigate the nanostructure of PFPE lubricant bulk system using a bead-spring model. The clusters of functional chain-ends are observed, which is responsible for the peculiar rheological response measured. By integrating the so-called SOLLD equation of motion and imposing the Lee-Edwards' boundary condition, non-equilibrium molecular dynamics simulations were carried out to examine the viscoelastic properties of PFPE bulk system under oscillatory shear. A sinusoidal form of shear strain was first applied to the PFPE melt, and the resultant shear stress was calculated. Then, in terms of the simulated strain-stress curve, one can calculate the complex modulus G* = G'+iG". Here, G' is the elastic, storage, or in-phase shear modulus related to the elastic energy stored by the PFPE melt, which measures the solid-like behavior of the melt; and G″ is the viscous, loss, or out-of-phase shear modulus related to the energy dissipated by the viscous flow, which measures the liquid-like behavior of the melt. Our study has suggested that the viscoelastic behavior of PFPE lubricants strongly depends on the molecular architecture (e.g., endgroup functionality) and external conditions (e.g., temperature and oscillation frequency). Nonfunctional PFPEs exhibit liquid-like behavior; while pseudo-reptation-like behavior is captured for functional PFPEs, where endgroup couplings are found to be dissociated at high temperature. The dynamic viscosity was further calculated and its comparison with our calculated shear viscosity is also provided to validate the Cox-Merz rule.
Since the confinement of molecules in dimensions comparable to their size gives rise to a unique behavior, we also incorporated the nano/micro-scale confinement effect into the PFPE system. To study this, the nano-mechanics of PFPE films, including compression and tension were examined. In our thought experiment, the PFPE films are coated onto two nanoscale separated solid surfaces facing each other which can be verified by atomic force microscope. As the top surface moves downward, a complete contact of nanofilms occurs. As moving the top surface up afterward at a constant speed, molecules are elongated to form the fluid bridge between the two surfaces. The film normal stress was calculated as a function of wall separation for both nonfunctional and functional PFPEs, where a characteristic hysteresis nature was observed and can be used to illustrate the viscoelastic properties of PFPE films via the N-mode Maxwell model. We have found that functional PFPE exhibits an additional mode with a smaller elastic constant but a much longer relaxation time, due to the strong endgroup coupling.
[Reference]
1. Jhon, M.S., Physicochemical Properties of Nano Structured Perfluoropolyether Films, Advances in Chemical Physics, vol. 129, pp.1-79, 2004.
2. Q. Guo, P. S. Chung, H. G. Chen, and M. S. Jhon, "Molecular rheology of perfluoropolyether lubricant via non-equilibrium molecular dynamics simulation," J. Appl. Phys., vol. 99, pp. 08N105, 2006.