number of carbon nanospheres with sizes of 100–210 nm. And
some striped nanostructures could be observed on the surface of an
individual carbon sphere (Fig. 2c). The selected area electron
diffraction of these carbon nanospheres shows dispersed rings,
indicating that the carbon spheres have low crystalline micro-
graphite structures, which could also be revealed by Raman
scattering (in the next paragraph). Nitrogen sorption isothermal
measurement is conducted on a Coulter Omnisorp 100CX specific
surface analyzer. From the sorption data, the BET surface area of
amorphous carbon nanospheres. The whole reaction could be
formulated as eqn. (3).
–(CF2)–n ? n/2 CF2NCF2
CF2NCF2 + 2 Ca(OH)2 ? 2 CaF2 + C + CO2 + 2 H2O
(1)
(2)
2 –(CF2)–n + 2n Ca(OH)2 ? 2n CaF2 + n C + n CO2 + 2n H2O
(3)
In addition, without any water added in the autoclave, the direct
solid reaction between PTFE and Ca(OH)2 was incomplete. At 550
°C, the water in the autoclave can be regarded as being in the
supercritical state, which can eliminate the limit of transport
between different reactants, and then promote the convertion from
PTFE to amorphous carbon.
In summary, in the supercritical water system at 550 °C, bulk
PTFE materials have been successfully converted into amorphous
carbon nanospheres and the by-product of CaF2, which can be
recycled and have potential applications in industry. The possible
reaction mechanism is also discussed. Supercritical water may play
a key role in the degradation of persistent PTFE wastes. This
method provides an efficient way to deal with waste PTFE
materials. In addition, there is promise in applying this method to
deal with and recycle other stable halogenous polymers.
The authors thank Professor Zhixiang Chen (Institute of Solid
State Physics, Chinese Academy of Sciences, Hefei) for his help in
BET surface area measurements. Financial support from the
National Natural Science Funds and the 973 Projects of China is
gratefully acknowledged.
the carbon nanospheres is about 20.0 m2 g21
.
The crystallinity of the prepared carbon is investigated by Raman
spectrometry on a LABRAM-HR Confocal Laser MicroRaman
Spectrometer using an Ar+ laser with 514.5 nm radiation at room
temperature. In Fig. 3(a), the peak at 1585–1600 cm21 (G-band)
corresponds to an E2g mode of graphite and is related to the
vibration of sp2-bonded carbon atoms in a 2-dimensional graphite
layer.20 Compared with the G-band at 1580 cm21 for the graphitic
carbons,21 the G-band of the products shifts towards a higher
wavenumber due to the less orderly arrangement of the carbon
atoms. The D-band at 1331–1339 cm21 (in Fig. 3(a)) is associated
with vibrations of carbon atoms with dangling bonds at the plane
termination of disordered graphite or glassy carbon. With the
treating temperature increasing, the intensity of the D-band (ID)
decreases and the intensity of the G-band (IG) increases. According
to the relationship La
=
4.4(ID/IG)21 (in nm),20 the small
microcrystalline planar size is 1.4–2.0 nm for the produced carbon
nanospheres.
IR spectra of the samples produced at 400 and 550 °C are shown
in Fig. 3(b) and (c). All the absorption peaks (Fig. 3(b): 1225, 1153,
639, 554 and 503 cm21) are assigned to the vibrations of carbon–
fluorine bonds (–CF2–) in PTFE.22 The absorption peaks at 1640
and 3450 cm21 could be ascribed to the d and n vibrations of water
molecules, respectively. IR spectra of the sample prepared at 550
°C (Fig. 3(c)) show that no absorption peaks can be indexed to
–CF2– or fragments such as C2F4 (1342, 913, 407 cm21), C4F8 (960
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cm21 22
or other organic functional groups. This indicates that the
)
degradation of PTFE in the supercritical water could be complete at
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Fig. 3 Raman shifts of amorphous carbon nanospheres (a); IR spectra of the
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C h e m . C o m m u n . , 2 0 0 4 , 3 4 2 – 3 4 3
343