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Introduction to Nanotechnology

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5.4. CARBON NANOTUBES 123<br />

stretch consists of out-of-phase stretches of the C=O bond length, where one bond<br />

length increases while the other decreases. Similarly carbon nanotubes also have<br />

normal modes of vibration. Figure 5.19 illustrates two of the normal modes of<br />

nanotubes. One mode, labeled AI,, involves an “in and out” oscillation of the<br />

diameter of the tube. Another mode, the E2, mode, involves a squashing of the tube<br />

where it squeezes down in one direction and expands in the perpendicular direction<br />

essentially oscillating between a sphere and an ellipse. The frequencies of these two<br />

modes are Raman-active and depend on the radius of the tube. Figure 5.20 is a plot<br />

of the frequency of the Al, mode as a function of this radius. The dependence of this<br />

frequency on the radius is now routinely used <strong>to</strong> measure the radius of nanotubes.<br />

5.4.5. Mechanical Properties<br />

Carbon nanotubes are very strong. If a weight W is attached <strong>to</strong> the end of a thin wire<br />

nailed <strong>to</strong> the roof of a room, the wire will stretch. The stress S on the wire is defined<br />

as the load, or the weight per unit cross-sectional area A of the wire:<br />

1 350<br />

f 3001<br />

v E,<br />

W<br />

S=-<br />

A<br />

(5.3)<br />

Figure 5.20. Plot of the frequency of the Raman A,, vibrational normal mode versus the radius<br />

of the nanotube. (lOA= 1 nm). (Adapted from R. Sai<strong>to</strong>, G. Dresselhaus, and M. S. Dresselhaus,<br />

Physical Properties of Nanotubes, Imperial College Press, 1998.)

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