2000
DOI: 10.1103/physrevlett.84.5552
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Tensile Loading of Ropes of Single Wall Carbon Nanotubes and their Mechanical Properties

Abstract: The mechanical response of 15 single wall carbon nanotube (SWCNT) ropes under tensile load was measured. For 8 of these ropes strain data were obtained and they broke at strain values of 5.3% or lower. The force-strain data are well fit by a model that assumes the load is carried by the SWCNTs on the perimeter of each rope. This model provides an average breaking strength of SWCNTs on the perimeter of each rope; the 15 values range from 13 to 52 GPa (mean 30 GPa). Based on the same model the 8 average Young's … Show more

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Cited by 2,446 publications
(1,363 citation statements)
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References 22 publications
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“…The prominent first and second subband absorption manifolds of these PNES-SWNT suspensions exhibit marked spectral red shifts, and modest absorption band broadening, relative to the SDS-SWNT benchmark spectrum. Figure 1b displays absorptions assigned previously to (6,5), (8,3), (7,5), and (7,6) nanotubes 1,53 and highlights the extent of the spectral red shifts in PNES-SWNT suspensions for these bands with respect to the corresponding reference transitions in the SDS-SWNT spectrum. Table 1 shows that while the degree of these PNES-SWNT transition red shifts range from 115 to 225 cm -1 , the absolute shift magnitude depends clearly on both tube chirality and solvent [MeOH (ε ) 33; 118-170 cm -1 ) < DMF (ε ) 38; 141-215 cm -1 ) < H 2 O (ε ) 80; 196-215 cm -1 ) ∼DMSO (ε ) 47; 172-224 cm -1 ); these spectral dependences are notably consistent with the theoretical predictions made by Strano and Choi which have heretofore lacked experimental precedent.…”
mentioning
confidence: 82%
“…The prominent first and second subband absorption manifolds of these PNES-SWNT suspensions exhibit marked spectral red shifts, and modest absorption band broadening, relative to the SDS-SWNT benchmark spectrum. Figure 1b displays absorptions assigned previously to (6,5), (8,3), (7,5), and (7,6) nanotubes 1,53 and highlights the extent of the spectral red shifts in PNES-SWNT suspensions for these bands with respect to the corresponding reference transitions in the SDS-SWNT spectrum. Table 1 shows that while the degree of these PNES-SWNT transition red shifts range from 115 to 225 cm -1 , the absolute shift magnitude depends clearly on both tube chirality and solvent [MeOH (ε ) 33; 118-170 cm -1 ) < DMF (ε ) 38; 141-215 cm -1 ) < H 2 O (ε ) 80; 196-215 cm -1 ) ∼DMSO (ε ) 47; 172-224 cm -1 ); these spectral dependences are notably consistent with the theoretical predictions made by Strano and Choi which have heretofore lacked experimental precedent.…”
mentioning
confidence: 82%
“…[1][2][3] CNTs have the potential to revolutionize numerous applications where nano-sized metallic and/or semiconducting components are required along with high strength, [4,5] large flexibility [6] and superb chemical stability. [7,8] In particular, metallic (met-) nanotubes are highly suited for nanoscale circuits, [9] ultrathin, flexible, and transparent conductors, [10] supercapacitors, [11] field emitters, [12] actuators, [13] and nanosized electrochemical probes.…”
Section: Introductionmentioning
confidence: 99%
“…Theoretical and experimental work on the mechanical properties of individual or bundles of CNTs proceeded well at the end of the last century. [1][2][3] It is now widely held that the modulus and strength of a typical single-walled carbon nanotube (SWNT) can reach 640 and 37 GPa, respectively, which surpass those of all existing materials. [4] However, because of weak intertube interactions, it is still a great challenge to acquire such super mechanical properties when CNTs are assembled as macroarchitectures (such as fibers and films).…”
mentioning
confidence: 99%