期刊
ACS NANO
卷 11, 期 12, 页码 12805-12816出版社
AMER CHEMICAL SOC
DOI: 10.1021/acsnano.7b07684
关键词
carbon nanotubes; polyacrylonitrile; poly(methyl methacrylate); molecular dynamics; self-assembly; dispersion; solubility parameters
类别
资金
- Air Force Office of Scientific Research AFOSR [FA9550-14-1-0194]
- National Science Foundation [DMREF 1623947, CNS-0821794]
- University of Colorado at Boulder
- Office of Science of the U.S. Department of Energy [DE-AC05-000R22725]
- DOE Office of Science User Facility [DE-AC02-06CH11357]
- Office of Advanced Cyberinfrastructure (OAC)
- Direct For Computer & Info Scie & Enginr [1532236] Funding Source: National Science Foundation
Debundling and dispersion of carbon nanotubes (CNTs) in polymer solutions play a major role in the preparation of carbon nanofibers,due to early effects on interfacial ordering and mechanical properties. A roadblock toward ultrastrong fibers is the difficulty to achieve homogeneous dispersions of CNTs in polyacrylonitrile (PAN) and poly(methyl methacrylate) (PMMA) precursor solutions in solvents such as dimethyl sulfoxide (DMSO), N,N-dimethylacetamide (DMAc), and N,N-dimethylformamide (DMF). In this contribution, molecular dynamics simulations with accurate interatomic potentials for graphitic materials that include virtual pi electrons are reported to analyze the interaction of pristine single wall CNTs with the solvents and polymer solutions at 25 degrees C. The results explain the barriers toward dispersion of SWCNTs and quantify CNT-solvent, polymer-solvent, as well as CNT-polymer interactions in atomic detail. Debundling of CNTs is overall endothermic and unfavorable with dispersion energies of +20 to +30 mJ/m(2) in the pure solvents, + 20 to +40 mJ/m(2) in PAN solutions, and +20 to +60 mJ/m(2) in PMMA solutions. Differences arise due to molecular geometry, polar, van der Waals, and CH-pi interactions. Among the pure solvents, DMF restricts CNT dispersion less due to the planar geometry and stronger van der Waals interactions. PAN and PMMA interact favorably with the pure solvents with dissolution energies of 0.7 to 1.1 kcal per mole monomer and 1.5 to 2.2 kcal per mole monomer, respectively. Adsorption of PMMA onto CNTs is stronger than that of PAN in all solvents as the molecular geometry enables more van der Waals contacts between alkyl groups and the CNT surface. Polar side groups in both polymers prefer interactions with the polar solvents. Higher polymer concentrations in solution lead to polymer aggregation via alkyl groups and reduce adsorption onto CNTs. PAN and PMMA solutions in DMSO and dilute solutions in DMF support CNT dispersion more than other combinations whereby the polymers significantly adsorb onto CNTs in DMSO solution. The observations by molecular simulations are consistent with available experimental data and solubility parameters and aid in the design of carbon nanofibers. The methods can be applied to other multiphase graphitic materials.
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