Dynamic Strengthening of Carbon Nanotube Fibers under Extreme
Mechanical Impulses
Wanting Xie,
†,‡
Runyang Zhang,
§
Robert J. Headrick,
∥,⊥
Lauren W. Taylor,
⊥
Steven Kooi,
#
Matteo Pasquali,
∥,⊥
Sinan Mü ftü ,
§
and Jae-Hwang Lee*
,†
†
Department of Mechanical and Industrial Engineering and
‡
Department of Physics, University of Massachusetts, Amherst,
Massachusetts 01003, United States
§
Department of Mechanical and Industrial Engineering, Northeastern University, Boston, Massachusetts 02139, United States
∥
Department of Chemistry and
⊥
Department of Chemical and Biomolecular Engineering, Rice University, Houston, Texas 77005,
United States
#
Institute for Soldier Nanotechnologies, MIT, Cambridge, Massachusetts 02139, United States
* S Supporting Information
ABSTRACT: A monofilament fiber spun from individual
carbon nanotubes is an arbitrarily long ensemble of weakly
interacting, aligned, discrete nanoparticles. Despite the
structural resemblance of carbon nanotube monofilament
fibers to crystalline polymeric fibers, very little is known about
their dynamic collective mechanics, which arise from van der
Waals interactions among the individual carbon nanotubes.
Using ultrafast stroboscopic microscopy, we study the
collective dynamics of carbon nanotube fibers and compare
them directly with nylon, Kevlar, and aluminum monofilament
fibers under the same supersonic impact conditions. The in
situ dynamics and kinetic parameters of the fibers show that
the kinetic energy absorption characteristics of the carbon
nanotube fibers surpass all other fibers. This study provides insight into the strain-rate-dependent strengthening mechanics of an
ensemble of nanomaterials for the development of high-performance fibers used in body armor and other protective
nanomaterials possessing exceptional stability in various harsh environments.
KEYWORDS: Nanomaterial armor, microballistics, high-strain-rate hardening, collective friction, impact delocalization
N
atural fibers
1−3
are the oldest example of material
technology; over the past century, synthetic fibers
4
have
accounted for most of the development in high-performance
materials (e.g., aramids and carbon fibers), where polymeric
fibers have been implemented in a multitude of applications.
4,5
In the meantime, because of their combination of high
molecular strength, elastic modulus, and low density,
6−8
carbon nanotubes (CNTs) have been considered the most
promising building blocks for the next-generation of high-
performance fibers that could enable applications as extreme as
space elevators.
9
Progress has been made toward translating
CNT properties to the macroscale via several continuous
fabrication methods, including the solution spinning
10
and
direct spinning
11
of continuous CNT fibers (CNTF). CNTF
mechanical properties are currently limited by the length of
their constituent CNTs; when macroscopic fibers fail, it is due
to the applied stress exceeding the frictional coupling of the
individual CNTs rather than the intrinsic breaking strength of
individual CNTs.
12,13
In macroscopic CNTFs, quasi-static
mechanical characterization reveals an elastic modulus (70−
350 GPa) and tensile strength (0.23−9.0 GPa) well below the
modulus (∼1 TPa) and strength (∼50 GPa) of individual
CNTs.
14,15
Strain-rate dependence of mechanical properties of CNTFs
were reported under low-speed tensile loading conditions,
16,17
where the applied loading speeds were negligible to the
mechanical wave propagation speeds of CNTFs. However,
under extremely fast deformation, combined with the radial
collapse of CNTs enhancing interfacial friction
18,19
and the
intertwined morphology of CNT assemblies within CNTF,
interfacial interactions among CNTs can be substantially
amplified. Thus, the ultrahigh-strain-rate (USR) mechanical
performance of CNTFs may be substantially different from the
characteristics predicted by the quasi-static characteristics of
CNTFs. For the real-time USR characterization of CNTF, it
requires microscopic mechanical excitation and precise
quantification of the ultrafast deformation of specimens. As
seen in the limitation of typical USR characterizations,
20−22
the
Received: January 24, 2019
Revised: April 30, 2019
Published: May 14, 2019
Letter
pubs.acs.org/NanoLett
Cite This: Nano Lett. XXXX, XXX, XXX-XXX
© XXXX American Chemical Society A DOI: 10.1021/acs.nanolett.9b00350
Nano Lett. XXXX, XXX, XXX−XXX
Nano Lett.
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