Molecular dynamics simulation of the effect of nanoparticle fillers on ion motion in a polymer host

Abstract There is some empirical evidence to show that proton conductivity in a polymer host (typically Nafion©) can be enhanced by the addition of nanoparticle “fillers”. The possible underlying mechanism(s) involved in such an effect is here probed by Molecular Dynamics (MD) simulation not for proton conductivity, but for lithium-ion conductivity in the system LiX.(PEO) n , where “PEO”=amorphous poly(ethylene oxide); X=Cl, Br, I or BF 4 ; and n lies in the range 10–50. The filler used is a ca. 14-A diameter quasi-spherical nanoparticle of Al 2 O 3 ; simulations are made in the range 290–360 K. Possible conductivity enhancement is assessed by comparing with salt- and/or “particle-free” reference calculations. The most general structural effect observed is that the PEO forms an immobilised “coordination sphere” around the particle, and that this has a crucial effect on all parameters monitored. Typically; Li-ion mobility decreases on the addition of the particle, and is consistently least near the particle surface. Importantly, unpaired BF 4 − anions are found attached to the particle within this region of immobilised PEO, leaving free Li-ions in the regions away from the particle. At lower concentration (Li:EO ratio 1:50), Li-ion conductivity is found to increase on the addition of nanoparticles at 330 K, but decreases or remains unchanged at lower temperatures and higher concentrations. Significant LiX pairing/clustering (for X=Cl, Br, I) is also observed away from the particle surface, and is greatest for LiBr and least for LiCl.

[1]  B. Scrosati,et al.  Nanocomposite polymer electrolytes for lithium batteries , 1998, Nature.

[2]  D. Macfarlane,et al.  Conductivity in amorphous polyether nanocomposite materials , 1999 .

[3]  W. Wieczorek,et al.  Ionic Interactions in Polymeric Electrolytes Based on Low Molecular Weight Poly(ethylene glycol)s , 1998 .

[4]  A. Aabloo,et al.  Molecular dynamics simulation of the effect of adding an Al2O3 nanoparticle to PEO–LiCl/LiBr/LiI systems , 2001 .

[5]  Use of polarized optical absorption to obtain structural information for Na+/Nd3+ beta "-alumina. , 1996, Physical review. B, Condensed matter.

[6]  B. Maigret,et al.  Molecular Dynamics Simulation of Li+BF4- in Ethylene Carbonate, Propylene Carbonate, and Dimethyl Carbonate Solvents , 1998 .

[7]  C. Capiglia,et al.  Effects of nanoscale SiO2 on the thermal and transport properties of solvent-free, poly(ethylene oxide) (PEO)-based polymer electrolytes , 1999 .

[8]  John O. Thomas,et al.  MOLECULAR DYNAMICS SIMULATION OF CRYSTALLINE POLY(ETHYLENE OXIDE) , 1994 .

[9]  L. Curtiss,et al.  Lithium perchlorate ion pairing in a model of amorphous polyethylene oxide , 1999 .

[10]  Harry Partridge,et al.  QUANTUM CHEMISTRY STUDY OF THE INTERACTIONS OF LI+, CL-, AND I- IONS WITH MODEL ETHERS , 1997 .

[11]  Nobuyuki Imanishi,et al.  Enhanced Lithium‐Ion Transport in PEO‐Based Composite Polymer Electrolytes with Ferroelectric BaTiO3 , 1999 .

[12]  A. Aabloo,et al.  Molecular dynamics simulation of temperature and concentration dependence of the ‘filler’ effect for the LiCl/PEO/Al2O3-nanoparticle system , 2003 .

[13]  W. Goddard,et al.  UFF, a full periodic table force field for molecular mechanics and molecular dynamics simulations , 1992 .

[14]  W. V. Gunsteren,et al.  Computer simulation of a polymer electrolyte: Lithium iodide in amorphous poly(ethylene oxide) , 1995 .

[15]  E. Peled,et al.  Charge and mass transport properties of LiI-P(EO)n-Al2O3-based composite polymer electrolytes , 1998 .

[16]  R. Vaia,et al.  Polymer nanocomposites: a new strategy for synthesizing solid electrolytes for rechargeable lithium batteries , 1995 .

[17]  A. Aabloo,et al.  Molecular dynamics simulation of the LiBF4–PEO system containing Al2O3 nanoparticles , 2002 .