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PNNL-13501 - Pacific Northwest National Laboratory

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Figure 1. (a) – (c) Successive magnification of carbon nanotubes grown on a stainless steel substrate<br />

porous silica film. Additional studies are under way to<br />

determine conditions required to grow crack-free carbon<br />

nanotube films.<br />

Two types of surface modification activities were<br />

pursued: 1) decoration of carbon nanotubes with noble<br />

metals (such as platinum), and 2) derivatization of carbon<br />

nanotubes with polymers. Shown in Figure 2 is the<br />

secondary electron image from the in-lens detector of a<br />

carbon nanotube sample that has been decorated with<br />

platinum. The platinum was deposited electrochemically<br />

(5-second deposition period) using the electronically<br />

conductive carbon nanotubes as electrodes. Thus, we<br />

successfully demonstrated that carbon nanotube surfaces<br />

can be electrochemically modified with metal<br />

nanoparticles (approximately 10 nm platinum particles).<br />

Figure 2. Secondary electron image from the in-lens<br />

detector for a 5-second deposition time of platinum<br />

Platinum deposits on carbon nanotubes are of interest to a<br />

wide range of applications from catalysis in general to<br />

hydrogen storage. The use of carbon nanotubes for<br />

catalyst support is of interest because of the uniformity of<br />

carbon nanotube surfaces (defect-free carbon nanotubes<br />

are single crystals) and high thermal and electrical<br />

conductivities. The possibility of storing hydrogen in the<br />

hollow centers of carbon nanotubes has sparked interest<br />

worldwide. Because noble metals (such as platinum) are<br />

known to dissociate molecular hydrogen into atomic<br />

304 FY 2000 <strong>Laboratory</strong> Directed Research and Development Annual Report<br />

hydrogen, the kinetics of hydrogen uptake and release<br />

may be improved.<br />

The high surface area of carbon nanotube films makes<br />

them viable support materials for electrodes. Commercial<br />

polyvinylferrocene from Polysciences Inc. was coated on<br />

carbon nanotube films using a solvent casting technique<br />

where the polyvinylferrocene was dissolved in<br />

dichloromethane. The cyclic voltammogram of the<br />

polyvinylferrocene-coated carbon nanotube film was<br />

obtained in a solution of 0.5 M NaNO3. The result was<br />

then compared to the cyclic voltammogram of a<br />

polyvinylferrocene-coated carbon cloth electrode (GC-14<br />

from the Electrosynthesis Co.). The integrated charge<br />

passed as a function of time for both electrodes is shown<br />

in Figure 3a. The polyvinylferrocene-coated carbon<br />

nanotube electrode exhibited a higher surface charge<br />

density. Furthermore, no difference in electrode<br />

accessibility (solution mass transport rates) was observed<br />

between the two electrodes. This was evident from<br />

Figure 3b, where required for passing the same relative<br />

amount of charge. Therefore, carbon nanotube films<br />

provide additional surface area with negligible mass<br />

transfer limitations.<br />

We have verified the feasibility of using a nuclear<br />

reaction analysis to directly measure the amount of H2<br />

absorbed in carbon nanotubes. Briefly, a beam of 19 F<br />

with a specific energy is imparted on carbon nanotube<br />

samples. The nuclear reaction, 19 F + 1 H → 16 O + 4 He + γ,<br />

occurs only when the 19 F has a specific energy (i.e., the<br />

resonant energy). Because the reaction is very specific to<br />

19 F + 1 H, a measure of the γ yield provides a measure of<br />

the concentration of hydrogen. In addition, variation of<br />

the 19 F energy gives us the ability to obtain the<br />

concentration of hydrogen as a function of depth (the 19 F<br />

must expend sufficient energy before the resonant nuclear<br />

reaction will take place). Figure 4 shows the hydrogen<br />

content of a virgin carbon nanotube sample and the same<br />

sample after it has been dosed with hydrogen at<br />

1 atmosphere for 1 hour. The amount of hydrogen is<br />

approximately 0.2 wt%. This is consistent with published

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