August 20, 2013 weblog
Carbyne is stronger than any known material
(Phys.org) —A paper on Arxiv presents a detailed look at the properties of carbyne, stronger than graphene and diamond, a true supermaterial. The paper is titled, "Carbyne from first principles: Chain of C atoms, a nanorod or a nanorope?" Authors are Mingjie Liu, Vasilii I. Artyukhov, Hoonkyung Lee, Fangbo Xu, and Boris I. Yakobson, from Rice University, in Houston, from the departments of mechanical engineering and materials science, chemistry, and the Smalley Institute for Nanoscale Science and Technology. They have calculated the properties of carbyne. Described as a chain of carbon atoms that are linked by alternate triple and single bonds or by consecutive double bonds, carbyne is of special interest, chemists find, because it is stronger, and stiffer than anything that they have seen before. The discovery of carbyne is not entirely new. Explorations of carbyne have their own history.
Indications of naturally-formed carbyne were observed in such environments as shock-compressed graphite, interstellar dust, and meteorites, said the authors. Recently, chains with length of up to 44 atoms have been chemically synthesized in solution.
Elsewhere, a Rice University report on carbyne research in 2011 said that while carbyne is considered an exotic material, recent experiments showed it can be synthesized and stabilized at room temperature, where the storage is mainly of interest.
Of special interest in the new paper on carbyne is that research by the Rice team indicates just how strong and stiff is this supermaterial. They were able to calculate its properties. In presenting a summary and conclusions of their research, the authors said that they were able to create a comprehensive portrait of carbyne. Some key points are as follows. It has an extreme tensile stiffness, stiffer by a factor of two than graphene and carbon nanotubes—and a specific strength surpassing that of any other known material. Its flexibility is between those of typical polymers and double-stranded DNA, they continued, with a persistence length of ~14 nm.
A combination of unusual mechanical and electronic properties, they said, is of great interest for applications in nanomechanical systems, opto-/electromechanical devices, strong and light materials for mechanical applications, or as high–specific-area energy storage matrices.
Their research was supported by the Robert Welch Foundation, a source of funding for chemistry research, and the Department of Energy.
More information: Carbyne from first principles: Chain of C atoms, a nanorod or a nanorope? arXiv:1308.2258 [cond-mat.mtrl-sci] arxiv.org/abs/1308.2258
Abstract
We report an extensive study of the properties of carbyne using first-principles calculations. We investigate carbyne's mechanical response to tension, bending, and torsion deformations. Under tension, carbyne is about twice as stiff as the stiffest known materials and has an unrivaled specific strength of up to 7.5*10^{7} Nm/kg, requiring a force of ~10 nN to break a single atomic chain. Carbyne has a fairly large room-temperature persistence length of about 14 nm. Surprisingly, the torsional stiffness of carbyne can be zero but can be `switched on' by appropriate functional groups at the ends. We reconstruct the equivalent continuum-elasticity representation, providing the full set of elastic moduli for carbyne, showing its extreme mechanical performance (e.g. a Young's modulus of 32.7 TPa with an effective mechanical thickness of 0.772 {AA}). We also find an interesting coupling between strain and band gap of carbyne, which is strongly increased under tension, from 3.2 to 4.4 eV under a 10% strain. Finally, we study the performance of carbyne as a nanoscale electrical cable, and estimate its chemical stability against self-aggregation, finding an activation barrier of 0.6 eV for the carbyne-carbyne cross-linking reaction and an equilibrium cross-link density for two parallel carbyne chains of 1 cross-link per 17 C atoms (2.2 nm).
via Arxiv Blog
Journal information: arXiv
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