Electrospun Carbon Nanofiber Webs with Controlled Density of States for Sensor Applications

Xianwen Mao, Fritz Simeon, Gregory C. Rutledge and T. Alan Hatton

(1st place in the Student Paper competition at the Fiber Society meeting in Nov, 2012)

Electrospun carbon nanofiber webs with controlled density of states have been synthesized through varying carbonization conditions to manipulate the concentration of nanosized graphite domains. These materials exhibit adjustable electrochemical activity and biosensitivity: both electron transfer kinetics for various redox systems and direct electron transfer efficiencies with enzymes increase with the DOS of the CNF webs. (Advanced Materials, 2012)

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(New) (2013-01) Electrospun Carbon Nanofiber Webs with Controlled Density of States for Sensor Applications
(New) (2012-12) Mechanical and Transport Properties of Layer-by-layer/Electrospun Nanofiber Composite Proton Exchange Membranes for Use in Direct Methanol Fuel Cells
(2012-05) Electrical conductivity of electrospun polyaniline and polyaniline-blend fibers and mats
(2011-12) On the importance of fiber curvature to the elastic moduli of electrospun nonwoven fiber meshes
(2011-04) Mechanical properties of individual electrospun PA 6(3)T fibers and their variation with fiber diameter
(2010-02) On the Measured Current in Electrospinning
(2010-01) Multifunctional Electrospun Fabrics via Layer-by-Layer Electrostatic Assembly for Chemical and Biological Protection
(2009-10) Molecular simulation of crystal nucleation in n-octane melts
(2009-02) Morphology of Porous and Wrinkled Fibers of Polystyrene Electrospun from Dimethylformamide
(2007-08) American Chemical Society 2007 National Meeting Presentation

Mechanical and Transport Properties of Layer-by-layer/Electrospun Nanofiber Composite Proton Exchange Membranes for Use in Direct Methanol Fuel Cells

Matthew Marchand Mannarino, David S. Liu, Paula T. Hammond, and Gregory C. Rutledge

(Oral presentation awarded 2nd place at 2012 MRS Membrane Symposium)

Improvements to the performance of thin solid polymer electrolytes for use as proton exchange membranes (PEMs) are critical for the advancement of the electrochemical energy devices such as direct methanol fuel cells (DMFCs). The essential properties for polyelectrolyte PEM used in DMFCs include: high ionic conductivity, low fuel/charge crossover, and mechanical stability. PEM fabrication by spray-assisted layer-by-layer (LbL) assembly of sulfonated poly(2,6-dimethyl-1,4-phenylene oxide) and poly(diallyl dimethyl ammonium chloride) [sPPO/PDAC] onto an electrospun fiber mat (EFM) scaffold has been shown to provide ionic conductivity comparable to that of the industry standard, Nafion®, while achieving a two order of magnitude reduction in methanol crossover. Electrospinning is used to create porous nanoscale polymer fiber scaffolds to provide mechanical support as well as mimic the percolated, fibrillar structure of water-swollen Nafion®. Poly(trimethyl hexamethylene terephthalamide) [PA 6(3)T], was used as the electrospun nanofiber "endo-skeleton" for the PEM due to its inherently high mechanical strength, tunable fiber diameter, high porosity, and relative ease of fabrication. Coating the PA 6(3)T EFMs by the vacuum-assisted spray-LbL technique produces composite membranes with conformally coated fibers throughout the bulk of the EFM and gives nanometer control of the thickness of the coating. Since the LbL process treats each fiber as an individual growth surface, entire EFMs (thickness ranging from 25 - 80 μm) can be filled up to 70%with less than 1 μm thick LbL coatings, while retaining up to 50% of the pristine LbL conductivity. In the absence of vacuum, the spray-LbL process forms a film covering all the pores of the EFM without penetrating into the fibers, thus creating a coherent methanol-impermeable capping layer. The mechanical properties of these composite LbL/EFM membranes are drastically improved over those of the LbL film alone, exhibiting the stiffness of PDAC/sPPO films when dry and the strength of the underlying EFM when hydrated. Improvements in the mechanical performance of the composite LbL/EFM PEMs are achieved by manipulating the structure of the underlying nanofiber matrix by heat treatment of the EFM post-spinning to increase the number of weld points between fibers and thus create a stronger fiber network. The dimensional stability of the composite PEMs under humidity cycling is superior to most conventional polyelectrolyte membranes, and the mechanical durability of the LbL/EFM PEMs was also found to be comparable to Nafion®. The composite LbL/EFM PEMs have been tested in a DMFC and preliminary results show higher open circuit voltage compared to Nafion®, as the result of reduced methanol permeability and comparable membrane impedance. Further optimization of the membrane electrode assembly and PEM conditioning indicate the potential for improved fuel cell output.(Advanced Functional Materials, 2013)

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Electrical conductivity of electrospun polyaniline and polyaniline-blend fibers and mats

Yuxi Zhang and Gregory C. Rutledge

Submicrometer fibers of polyaniline (PAni) doped with (+)-camphor-10-sulfonic acid (HCSA) and blended with poly(methyl methacrylate) (PMMA) or poly(ethylene oxide) were electrospun over a range of compositions. Continuous, pure PAni fibers doped with HCSA were also produced by coaxial electrospinning and subsequent removal of the PMMA shell polymer. The electrical conductivities of both the fibers and the mats were characterized. The electrical conductivities of the fibers were found to increase exponentially with the weight percent of doped PAni in the fibers, with values as high as 50 ± 30 S/cm for as-electrospun fibers of 100% doped PAni and as high as 130 ± 40 S/cm upon further solid state drawing. These high electrical conductivities are attributed to the enhanced molecular orientation arising from extensional deformation in the electrospinning process and afterward during solid state drawing. A model is proposed that permits the calculation of mat conductivity as a function of fiber conductivity, mat porosity, and fiber orientation distribution; the results agree quantitatively with the independently measured mat conductivities. (Macromolecules, 2012, v45, 4238-4246)

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On the importance of fiber curvature to the elastic moduli of electrospun nonwoven fiber meshes

Chia-Ling Pai, Mary C. Boyce, and Gregory C. Rutledge

Adequate mechanical integrity of nonwoven fabrics is generally a prerequisite for their practical usage. Nonwoven fiber mats of poly(trimethyl hexamethylene terephthalamide) (PA 6(3)T) with average fiber diameters from 0.1 to 3.6 microns were electrospun from solutions in dimethylformamide and formic acid and their in-plane mechanical response characterized. Two quantitative microstructure-based models that relate the Young's moduli of these fabrics to those of the fibers are considered, one assuming straight fibers and the other allowing for curved fibers. It is found that the model allowing for curved fibers provides a quantitative relationship between the Young's moduli of the mats and those of the fibers themselves. The governing factors that affect the mechanical properties of nonwoven mats are the porosity of the mats, the intrinsic fiber modulus, and the average fiber diameter, curvature (or "curl") and distance between fiber-to-fiber junctions. Especially for submicron diameter fibers, both the intrinsic fiber properties and fiber curvature make important contributions to the mechanical behavior of their nonwoven fabrics. (Polymer, 2011, v52, 6126-6133)

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Mechanical properties of individual electrospun PA 6(3)T fibers and their variation with fiber diameter

Chia-Ling Pai, Mary C. Boyce, and Gregory C. Rutledge

Young's modulus and yield strength of individual electrospun fibers of poly(trimethyl hexamethylene terephthalamide) (PA 6(3)T) have been obtained in uniaxial extension. The Young's modulus is found to exhibit values in excess of the isotropic bulk value, and to increase with decreasing fiber diameter for fibers with diameter less than roughly 500 nm. The yield stress is also found to increase with decreasing fiber diameter. These trends are shown to correlate with increasing molecular level orientation within the fibers with decreasing fiber diameter. Using Ward's aggregate model, the correlation between molecular orientation and fiber modulus can be explained, and reasonable determinations of the elastic constants of the molecular unit are obtained. (Polymer, 2011, v52, 2295-2301 )

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On the Measured Current in Electrospinning

P. K. Bhattacharjee, T. M. Schneider, M. P. Brenner, G. H. McKinley, and G. C. Rutledge

In determining the diameter of the fibers obtained in electrospinning, the current, I, carried by the electrified jet plays a fundamental role. When the surface tension force acting on the electrified jet balances the force due to surface charge repulsion, the diameter of the jet (ht) scales as ht ~ &Sigma 2/3 = (I/Q)2/3 where &Sigma is the volume charge density and Q is the flow rate of the fluid (Phys. Rev. Lett., 90, 144502, 2003). It is demonstrated that for linear homopolymers in organic solvents the total current (Itotal) measured in electrospinning follows a scaling law given by Itotal ~ EQ0.5K0.4, where K is the conductivity of the fluid and E is the electric field strength, calculated as a ratio of the imposed potential difference (V) and the distance between the electrodes (dg). It is further demonstrated that a part of the total current may consist of contributions from charged secondary jets that emanate from the surface of the primary jet and discharge at the counter electrode along with the primary jet. In such cases, the measured total current can be written as Itotal = I + Is, where the term Is signifies the contribution from the charged secondary jets. The secondary jetting phenomenon is invoked when the jet bends and the local electric field on the surface of the jet is intensified. Since the magnitude of I cannot be exactly determined in the presence of secondary jetting, &Sigma is typically estimated on the basis of the measured current, Itotal. It follows that, for cases where Is is small, ht ~ &Sigma2/3 = (I/Q)2/3. However for large values of Is the apparent scaling between ht and &Sigma can significantly deviate from theoretical predictions. These results provide valuable insight into the mechanisms that affect fiber formation in electrospinning and provide one explanation for the deviations from theoretical scaling behavior observed in practice. (J. Appl. Phys. 2010, 107, 044306)

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Multifunctional Electrospun Fabrics via Layer-by-Layer Electrostatic Assembly for Chemical and Biological Protection

Liang Chen, Lev Bromberg, Jung Ah Lee, Huan Zhang, Heidi Schreuder-Gibson, Phillip Gibson, John Walker, Paula T. Hammond, T. Alan Hatton and Gregory C. Rutledge

Breathable, chemical and biological detoxifying protective fabrics are obtained via functionalization of electrospun fiber mats using a layer-by-layer electrostatic assembly technique. Chemically reactive polyanion, poly(N-hydroxyacrylamide) or poly(hydroxamic acid) (PHA), and bactericidal polycation, poly (N-vinylguanidine) (PVG), were synthesized and electrostatically assembled to generate multifunctional coatings on prefabricated polyacrylonitrile (PAN) fiber mats. Reactivity of PHA in the hydrolysis of diisopropyl fluorophosphate (DFP), a close analog of the chemical warfare agent sarin, was demonstrated. The DFP degradation rate with PHA is comparable to that with compounds such as isonicotinhydroxamic acid methiodide, an efficient catalyst of organophosphate ester hydrolysis. Protective fabrics functionalized with PVG/PHA layers are able to degrade DFP mists, with DFP hydrolysis rates 60-fold higher than those with unmodified fabrics under identical conditions. Fabrics modified with PVG/PHA layers are bactericidal against E. coli and S. epidermidis. Breathability and barrier performance of functionalized fiber mats as protective fabrics were evaluated versus standard reference fabrics (Chemistry of Materials 2010, 22(4), 1429-1436).

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Molecular simulation of crystal nucleation in n-octane melts

Peng Yi, Gregory C. Rutledge

Homogeneous nucleation of the crystal phase in n-octane melts was studied by molecular simulation with a realistic, united-atom model for n-octane. The structure of the crystal phase and the melting point of n-octane were determined through molecular dynamics simulation and found to agree with experimental results. Molecular dynamics simulations were performed to observe the nucleation events at constant pressure and constant temperature corresponding to about 20% supercooling. Umbrella sampling Monte Carlo simulations were used to calculate the nucleation free energy for three temperatures, ranging from 8% to 20% supercooling, and to reveal details of the critical nucleus for the first time. The cylindrical nucleus model was found to provide a better quantitative description of the critical nucleus than the spherical nucleus model. The interfacial free energies of the cylinder model were calculated from the simulation data. As the temperature increased, the interfacial free energy of the side surface remained relatively unchanged, at 7 to 8 mJ/m2, whereas the interfacial free energy of the end surface decreased significantly from 5.4 mJ/m2 to about 3 mJ/m2. These results, and the methods employed, provide valuable and quantitative information regarding the rate limiting step during the solidification of chain molecules, with ramifications for both short alkanes and polymers (J. Chem. Phys., 2009, 131, 134902).

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Morphology of Porous and Wrinkled Fibers of Polystyrene Electrospun from Dimethylformamide

Chia-Ling Pai *, Mary C. Boyce, and Gregory C. Rutledge

( * Finalist, 2009 AkzoNobel Student Award in Applied Polymer Science, Division of Polymer Materials Science and Engineering (PMSE), American Chemical Society)


Submicron diameter fibers of polystyrene (PS) are electrospun from solutions in dimethylformamide (DMF). It is found that the smooth fibers with highly porous interior formed in a humid environment, and wrinkled fibers with consolidated structures formed in a low humidity environment. The resulting interior and exterior structures are found to depend on a competition among the phase separation, solvent drying, and the buckling instability, which have important consequences for the properties of the fibers (Macromolecules, 2009, 42 (6), pp 21022114).

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American Chemical Society 2007 National Meeting Presentation (August 2007)

Structure and Properties of Polyethylene Nanofibers from Molecular Dynamics Simulations (Macromolecules 2007, 40, 8483-8489)

Sezen Curgul, and Gregory C. Rutledge

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updated: Apr-13-2012
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