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Carbon Nanotube Reinforced Composites: Metal and Ceramic ...

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where p is volume fraction of the filler <strong>and</strong> pc the percolation threshold. The critical<br />

exponents s, s 0 <strong>and</strong> t are assumed to be universal. The conductivity exponent t reflects<br />

the dimensionality of the system with values about 1.3 <strong>and</strong> 2.0 for two <strong>and</strong> three<br />

dimensional r<strong>and</strong>om percolation system, respectively [17]. However, the experimental<br />

conductivity exponent t value can deviate from the universal value as a result of<br />

electron tunneling from conducting fillers above the percolation threshold [18].<br />

According to the literature, the measured percolation threshold in CNT–ceramic<br />

composites is very low, typically in the range of 0.64–4.7 vol%, depending on the type<br />

of ceramic matrix <strong>and</strong> processing technology employed [19, 20].<br />

In terms of a.c. properties, the experimental conductivity <strong>and</strong> dielectric constant<br />

display a pronounced frequency-dependent behavior. The frequency dependence of<br />

effective conductivity <strong>and</strong> dielectric constant of a conductor-insulator composite near<br />

the percolation threshold can be described by the following universal power law<br />

relation [16]:<br />

s / u x<br />

e / u y<br />

6.3 Percolation Concentrationj173<br />

ð6:5Þ<br />

ð6:6Þ<br />

where u is frequency. The critical exponents x <strong>and</strong> y must satisfy the following<br />

relation:<br />

x þ y ¼ 1: ð6:7Þ<br />

Peigney <strong>and</strong> coworkers investigated the percolation behavior of in situ MgAl2O3/<br />

CNT nanocomposites having 0.2–25 vol% CNT [19]. The nanocomposites were<br />

prepared by catalytic chemical vapor deposition followed by hot pressing at 1300 C.<br />

Figure 6.2(a) <strong>and</strong> (b) shows the variation of electrical conductivity with CNT content<br />

for the MgAl2O3/CNTnanocomposites. The inset in Figure 6.2(a) represents a log-log<br />

plot of the conductivity as a function of p-pc. From least-square analysis, a linear fit can<br />

be obtained according to Equation 6.2, yielding an exponent t ¼ 1.73 0.02. <strong>and</strong><br />

percolation threshold p c ¼ 0.64 0.02 vol% (about 0.31 wt%). At the percolation<br />

threshold, the electrical conductivity increases over seven orders of magnitude from<br />

10 8 to 0.4 S m 1 . Comparing with the ultralow value of pc (0.0025 wt%) for MWNT/<br />

epoxy nanocomposites [7], the percolation threshold is two orders of magnitude<br />

higher for the MgAl2O3/CNT nanocomposites. This is attributed to the degradation<br />

of CNTs during hot-pressing at 1300 C.<br />

Very recently, Ahmad et al. studied the electrical conductivity <strong>and</strong> dielectric<br />

behavior of Al2O3/MWNT nanocomposites prepared by SPS at 1350 C [20]. A<br />

percolation threshold of 0.79 vol% was found for such nanocomposites. Further,<br />

the dielectric constant can reach as high as 5000 in the low frequency region by<br />

adding 1.74 vol% MWNT. Shi <strong>and</strong> Liang [21] also investigated the percolation <strong>and</strong><br />

dielectric behavior 3Y-TZP (3 mol% yttria-stabilized tetragonal polycrystalline zirconia)<br />

filled with various MWNT contents. The 3Y-TZP/MWNT nanocomposites were<br />

fabricated by ball milling constituent materials followed by SPS at 1250 C under a<br />

pressure of 60 MPa. Figure 6.3 shows the effective d.c. conductivity vs CNT concentration<br />

for the 3Y-TZP/MWNT nanocomposites. Using the least square fit, the

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