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With increasing temperature, heating rate and weight loss, the amount of the graphitic structure was reduced at the expense of disordered structure.Õâ¾ä»°ÊÇÖ¸ÎÂËÞÉý¸ßÌ¿ºÚʯ½á¹¹¼õÉÙ£¬ÎÞ¶¨ÐͽṹÔö¶àÂð£¿ÎҸоõÎÒºýÍ¿ÁË
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6Â¥2015-07-23 14:53:37
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3Â¥2015-07-18 15:47:41
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4Â¥2015-07-18 18:29:43
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Raman spectra (Fig. 4) of studied samples confirm
presence of two bands: (i) G band at 1,590 cm-1 and (ii)
D band at 1,355 cm-1. G band confirms presence of graphitic structure and D band represents disordered structure
which is form due to the breakdown of symmetry for atoms
close to the edge of graphite sheet when formerly forbidden
transitions became possible [6].
Parameters of Raman spectra such as the position m, the
full width at half-maximum FWHM and areas I of the
G and D bands are documented in the Table 3. Raman
spectra of single-crystal graphite samples show band only
at 1,575 cm-1. Increase of temperature and heating rate of
pyrolysis leads to reduction of graphitic structure¡ªposition
of mG shift to higher value and conversely FWHMG shift to
lower value. This phenomenon was also observed andreported by Darmstadt et al. [6] who studied Raman spectra
of CB
p obtained by pyrolysis of STs at the temperature
range 420¨C700 C. Reduction of graphitic structure is also
confirmed by growing ratio ID/IG with increasing
temperature.
On the other hand, higher thermal treatment of CBc
cause increase of intensity of graphitic structure [5] and
position of mG decrease from about 1,600 cm-1 to around
1,575 cm-1 as the temperature increases from 27 to
2,727 C [5].
Compared to CBc Raman spectra of CBp most approaches to CB
c denoted as N375 and N774. Probably these
two carbon blacks were used as a filler during STs
manufacturing.
Linear relation (Fig. 5) was found between the intensities ID and IG and temperature of pyrolysis and weight
losses of pyrolysed sample. With increasing temperature
ration ID/IG increase and this dependence correlate with
weight loss of pyrolysis of STs
5Â¥2015-07-18 20:59:12
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