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Introduction to Nanotechnology

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286 ORGANIC COMPOUNDS AND POLYMERS<br />

1 000<br />

L""'1<br />

300<br />

100<br />

30<br />

10<br />

3<br />

1<br />

.3<br />

.1<br />

1 3 10 30 100 300 1000<br />

Figure 11.2. Dependence of the diameter D of a cylindrical polymer on its diameter : length ratio<br />

D/L for molecular weights from 10 <strong>to</strong> 10' Da, as indicated on the curves. A density p = 1 g/cm3<br />

was assumed in Eq. (11.13) for plotting these curves.<br />

in<strong>to</strong> dispersed clusters that undergo a process of nucleation and growth, until they<br />

finally produce the nanocrystals.<br />

As these crystallites form, they scatter light, and the intensity of the scattered light<br />

Z,(t) relative <strong>to</strong> the incident light intensity I,, after a time t has elapsed, can be used<br />

<strong>to</strong> moni<strong>to</strong>r the rate at which the growth takes place. Figure 1 1.5 plots the normalized<br />

scattered light intensity Is(t)/Io versus the time, and establishes that the growth is<br />

much faster at higher temperatures. This time dependence of Zs(t)/Io follows the<br />

expression [l - exp(a,,,t)]*, where the growth rate constant clap, depends on the<br />

temperature in the manner shown in Fig. 1 1.6. The linearity of this latter plot, which<br />

is called an Arrhenius plot, provides the activation energy for the crystal growth<br />

process, and for perylene nanocrystals this is 68 kJ/mol. The activation energy is the<br />

minimum amount of energy that must be supplied for the nanocrystals <strong>to</strong> form. The<br />

size of the crystallite can be regulated by varying the concentration, temperature, and<br />

mixing procedure, and also by the use of surfactants that modify the surface of the<br />

particles, or reduce the surface tension of the solution. In the particular case of<br />

D/L

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