Crystalline Order and Mechanical Properties of As-Electrospun and Post-treated Bundles of Uniaxially Aligned Polyacrylonitrile Nanofiber Dorna Esrafilzadeh, 2 Rouhollah Jalili, 1 Mohammad Morshed 2 1 ITA-Co Engineering, Unit 7, No. 63, Sheikh e Bahaii Sq, Tehran, 19949–13434 2 Textile Engineering Department, University of Technology, Isfahan, Iran 84154 Received 21 February 2007; accepted 11 October 2007 DOI 10.1002/app.27593 Published online 8 September 2008 in Wiley InterScience (www.interscience.wiley.com). ABSTRACT: This study investigates the crystalline order and mechanical properties of as-electrospun and posttreated polyacrylonitrile nanofibers. To keep the nanofibers under tension during the posttreatment, a modified method of pre- paring bundles such as multifilament yarn was used in which the alignment of the nanofibers and linear density of the bun- dles were controlled successfully. An increase in the nanofib- ers’ diameter from 240 to 500 nm led to the E modulus, ulti- mate strength, and elongation at break of the bundles rising from 836 MPa, 45 MPa, and 38% to 1915 MPa, 98 MPa, and 120%, respectively. The crystallinity index (%) and coherence length of the nanofiber bundles were evaluated through wide-angle X-ray diffraction. The mechanical properties and crystalline order of the nanofiber bundles were both increased as a result of the posttreatment. Wide-angle X-ray diffraction patterns of annealed bundles showed equatorial diffraction from the (10 10) reflection at 5.1 A ˚ and from the (11 20) reflection at 3A ˚ . The values of the coherence length, crys- tallinity index (%), ultimate strength, and E modulus of the bundles prepared from 240-nm nanofibers increased from negligible, 2%, 1109 MPa, and 48 MPa to 54 A ˚ , 35%, 2235 MPa, and 95 MPa after annealing at 858C in a mixture of water (95 wt %) and N,N-dimethylformamide (5 wt %), respectively. Ó 2008 Wiley Periodicals, Inc. J Appl Polym Sci 110: 3014–3022, 2008 Key words: fibers; nanotechnology; X-ray; electrospinning; PAN INTRODUCTION Many applications in textiles and as carbon fiber pre- cursors have been found for polyacrylonitrile (PAN). PAN homopolymer fibers are only rarely used for fiber spinning, and virtually all commercial acrylic fibers are spun from acrylonitrile polymers containing 1–15 wt % comonomers. 1 There are strong intrachain and interchain interactions through secondary bonding because of the large magnitude of the dipole moment of the nitrile groups in PAN fibers. Therefore, upon heating, PAN undergoes a degradation reaction before melting at 320–3308C. 2,3 The spinning processes most commonly used for acrylic fibers involve highly polar solvents, such as N,N-dimethylformamide (DMF), dimethylacetamide, and dimethyl sulfoxide. 4 Recently, PAN nanofibers have been produced by electrospin- ning. The electrospinning technique has been recog- nized as an efficient processing method for manufac- turing nanoscale fibrous structures, which are used in many applications such as filtration, reinforcements in composites, and carbon nanofiber precursors. 5 The majority of textile fibers have a morphology that can be described by the classical two-phase model. In this model, discrete crystalline domains of the order of several hundred angstroms are mixed with amorphous domains of similar or smaller size. A high degree of crystallinity and high orientation of the crystalline molecular segments impart high ten- sile strength and modulus to the fibers. The amor- phous phase gives rise to flexibility and dyeability. 6,7 Whether PAN can be described by the classical model is debatable. In the ordered phase, irregularly twisted yet extended atactic polymer chains are packed hexagonally. 7 Because of the strong inter- chain interactions noted previously, this hexagonal columnar phase behaves as a solid, and it is often referred to as a (two-dimensional) crystal. Wide-angle X-ray scattering of drawn PAN fibers has been shown to have two strong equatorial reflec- tions (Bragg spacings of d 3.0 A ˚ and d 5.3 A ˚ ), indicating an order perpendicular to the fiber axis. This result has frequently been interpreted in terms of hexagonal packing of molecular rods comprising distorted helices or kinked planar zigzags. Some have assumed a single, laterally ordered or paracrys- talline phase, whereas others have proposed a two- phase structure with regions of ordered rods and regions of amorphous material or disordered rods. 7 In the case of nanofibers, their crystalline order may also be of primary importance when these materials are considered for commercial applica- tions. 8 One characteristic feature of the electrospin- Correspondence to: R. Jalili (jaliliar@yahoo.com). Journal of Applied Polymer Science, Vol. 110, 3014–3022 (2008) V V C 2008 Wiley Periodicals, Inc.