Abstract:X-ray diffraction (XRD) studies on single-walled carbon nanotube (SWNT)
samples prepared by the arc-discharge method were reported. The XRD profile was
basically explained to be a result of triangular packing of SWNTs with a lattice
constant of 17.1 Å and an average nanotube radius of 7.1 Å. We found an
anomalous change in XRD profiles before and after heat-treatment of the SWNT
samples in air at ∼350°C. Combined with gravimetric measurements and resistivity
measurements, a detailed sim… Show more
“…[26][27][28][29][36][37][38] Based on this prior work, it is highly likely that the SWCNTs are completely empty at 324 K, are filled with water between RT and approximately 220 K, and are partially emptied below 220 K due to the WDT. The incomplete emptying of the SWCNTs below 220 K is attributed to the slow dynamics of water at low temperatures (see Fig.…”
Section: Water Encapsulation and Wet-dry Transitionmentioning
confidence: 99%
“…The finite thickness of the bundle is assumed to broaden each Bragg peak, as described by the peak functions. Although this analysis has been widely applied in previous works, [26][27][28]31,[35][36][37][38] it does not provide information regarding all possible water adsorption sites, such as on the bundle surfaces. Therefore, as an alternative approach, we also used the Debye formula below to calculate the XRD patterns, 32,39,40 …”
Section: Xrd Simulations Using the Debye Formulamentioning
confidence: 99%
“…26 The reasons of the reduction in the 10 peak intensity have been investigated by several methods, including neutron diffraction analyses 29 of D 2 O-and H 2 O-SWCNT systems and detailed XRD analyses 37 employing Rietveld and maximum entropy methods. [26][27][28][29]31,[36][37][38] It has been determined that the 10 peak is diminished when water is adsorbed inside the SWCNTs as a result of the subtractive superposition of the X-rays (or neutron beams) diffracted from carbon atoms in the SWCNTs and from water molecules inside the SWCNTs. 36 Conversely, water molecules adsorbed at interstitial channel (IC) sites surrounded by three neighboring SWCNTs tend to increase the 10 intensity, owing to the additive superposition of the diffracted X-rays at the 10 peak position.…”
Section: Water Encapsulation and Wet-dry Transitionmentioning
Diameter-dependent hydrophobicity in carbon nanotubesSingle-wall carbon nanotubes (SWCNTs) are a good model system that provides atomically smooth nanocavities. It has been reported that water-SWCNTs exhibit hydrophobicity depending on the temperature T and the SWCNT diameter D. SWCNTs adsorb water molecules spontaneously in their cylindrical pores around room temperature, whereas they exhibit a hydrophilic-hydrophobic transition or wet-dry transition (WDT) at a critical temperature T wd ≈ 220-230 K and above a critical diameter D c ≈ 1.4-1.6 nm. However, details of the WDT phenomenon and its mechanism remain unknown. Here, we report a systematic experimental study involving X-ray diffraction, optical microscopy, and differential scanning calorimetry. It is found that water molecules inside thick SWCNTs (D > D c ) evaporate and condense into ice Ih outside the SWCNTs at T wd upon cooling, and the ice Ih evaporates and condenses inside the SWCNTs upon heating. On the other hand, residual water trapped inside the SWCNTs below T wd freezes. Molecular dynamics simulations indicate that upon lowering T, the hydrophobicity of thick SWCNTs increases without any structural transition, while the water inside thin SWCNTs (D < D c ) exhibits a structural transition, forming an ordered ice. This ice has a well-developed hydrogen bonding network adapting to the cylindrical pores of the SWCNTs. Thus, the unusual diameter dependence of the WDT is attributed to the adaptability of the structure of water to the pore dimension and shape. Published by AIP Publishing.[http://dx
“…[26][27][28][29][36][37][38] Based on this prior work, it is highly likely that the SWCNTs are completely empty at 324 K, are filled with water between RT and approximately 220 K, and are partially emptied below 220 K due to the WDT. The incomplete emptying of the SWCNTs below 220 K is attributed to the slow dynamics of water at low temperatures (see Fig.…”
Section: Water Encapsulation and Wet-dry Transitionmentioning
confidence: 99%
“…The finite thickness of the bundle is assumed to broaden each Bragg peak, as described by the peak functions. Although this analysis has been widely applied in previous works, [26][27][28]31,[35][36][37][38] it does not provide information regarding all possible water adsorption sites, such as on the bundle surfaces. Therefore, as an alternative approach, we also used the Debye formula below to calculate the XRD patterns, 32,39,40 …”
Section: Xrd Simulations Using the Debye Formulamentioning
confidence: 99%
“…26 The reasons of the reduction in the 10 peak intensity have been investigated by several methods, including neutron diffraction analyses 29 of D 2 O-and H 2 O-SWCNT systems and detailed XRD analyses 37 employing Rietveld and maximum entropy methods. [26][27][28][29]31,[36][37][38] It has been determined that the 10 peak is diminished when water is adsorbed inside the SWCNTs as a result of the subtractive superposition of the X-rays (or neutron beams) diffracted from carbon atoms in the SWCNTs and from water molecules inside the SWCNTs. 36 Conversely, water molecules adsorbed at interstitial channel (IC) sites surrounded by three neighboring SWCNTs tend to increase the 10 intensity, owing to the additive superposition of the diffracted X-rays at the 10 peak position.…”
Section: Water Encapsulation and Wet-dry Transitionmentioning
Diameter-dependent hydrophobicity in carbon nanotubesSingle-wall carbon nanotubes (SWCNTs) are a good model system that provides atomically smooth nanocavities. It has been reported that water-SWCNTs exhibit hydrophobicity depending on the temperature T and the SWCNT diameter D. SWCNTs adsorb water molecules spontaneously in their cylindrical pores around room temperature, whereas they exhibit a hydrophilic-hydrophobic transition or wet-dry transition (WDT) at a critical temperature T wd ≈ 220-230 K and above a critical diameter D c ≈ 1.4-1.6 nm. However, details of the WDT phenomenon and its mechanism remain unknown. Here, we report a systematic experimental study involving X-ray diffraction, optical microscopy, and differential scanning calorimetry. It is found that water molecules inside thick SWCNTs (D > D c ) evaporate and condense into ice Ih outside the SWCNTs at T wd upon cooling, and the ice Ih evaporates and condenses inside the SWCNTs upon heating. On the other hand, residual water trapped inside the SWCNTs below T wd freezes. Molecular dynamics simulations indicate that upon lowering T, the hydrophobicity of thick SWCNTs increases without any structural transition, while the water inside thin SWCNTs (D < D c ) exhibits a structural transition, forming an ordered ice. This ice has a well-developed hydrogen bonding network adapting to the cylindrical pores of the SWCNTs. Thus, the unusual diameter dependence of the WDT is attributed to the adaptability of the structure of water to the pore dimension and shape. Published by AIP Publishing.[http://dx
“…(A.11), (A.12), and (A.13)], and φ(Q − |G K |) is the normalized profile function, which is further modified to an asymmetric form. 16,20 The use the wave vector Q = |Q| instead of scattering angle 2θ is the previous convention, 5,7,8 where the Lorentz factor becomes L(Q) = 1/ sin 2 θ or ∝ 1/Q 2 . By further taking the average of Eq.…”
The structure of bundles of single-walled carbon nanotubes (SWNT) has been refined by Rietveld analysis using neutron and X-ray powder diffraction data. Based on previous simulation studies of powder diffraction data of SWNT and standard Rietveld analyses, we have developed a pattern fit technique for SWNT which provides precise structure parameters. We also show that the present technique can be used with the maximum entropy method (MEM), which is complementary to the Rietveld analysis. Using the neutron diffraction data of pristine SWNT, we have successfully reconstructed the density of carbon nuclei and zero density in the inner cavity of SWNT by MEM.
“…Water encapsulated within hydrophobic SWCNTs, commonly known as ice nanotubes (INT), provide important clues to the functionality of biological nanopores (Sansom and Biggin 2001). Moreover, INTs have been found to exhibit novel properties such as proton conduction, hydrogen-bond network, phase transitions, etc (Maniwa, Kumazawa et al 1999;Hummer, Rasaiah et al 2001;Koga, Gao et al 2001;Martí and Gordillo 2001;Noon, Ausman et al 2002;Mann and Halls 2003;Martí and Gordillo 2003;Mashl, Joseph et al 2003;Wang, Zhu et al 2004). Through a systematic investigation, we have revealed the geometrical structure adopted by INTs within SW-CNT and the signatures in its vibrational spectra (Feng, Zhang et al 2007).…”
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