synthesis, characterization and infrared emissivity study of polyurethane/tio2 nanocomposites
TRANSCRIPT
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Applied Surface Science 253 (2007) 9154–9158
Synthesis, characterization and infrared emissivity study
of polyurethane/TiO2 nanocomposites
Jing Chen, Yuming Zhou *, Qiuli Nan, Yanqing Sun, Xiaoyun Ye, Zhiqiang Wang
School of Chemistry and Chemical Engineering, Southeast University, Nanjing 211189, China
Received 8 March 2007; received in revised form 21 May 2007; accepted 21 May 2007
Available online 29 May 2007
Abstract
In this study, polyurethane/titania (PU/TiO2) nanocomposites were prepared in ultrasonic process and characterized by fourier transform IR
spectroscopy (FT-IR), powder X-ray diffraction (XRD), thermogravimetric analysis (TGA), differential scanning calorimetry (DSC), transmission
electron microscopy (TEM), scanning electron microscopy (SEM) and infrared emissivity analysis. The TEM and SEM results indicated that the
nanoparticles were dispersed homogeneously in PU matrix on nanoscale. TGA-DSC confirmed that the heat stability of the composite was
improved. Infrared emissivity study showed that the nanocomposite possessed lower emissivity value than those values of pure polymer and
nanoparticles.
# 2007 Elsevier B.V. All rights reserved.
Keywords: Polyurethane; Nano-TiO2; Nanocomposites; Polymers; Emissivity
1. Introduction
Infrared low emissivity coating has found wide application in
civil and military fields such as camouflaging military equipment
or vehicles from infrared detection [1]. As a result of their
excellent physicochemical and optoelectronic properties, nano-
materials have received increasing attention [2] in recent years
and have been studied intensively in low emissivity coating [3].
In practical applications, the coating generally attains the low
emissivity by using nanocomposites based on indium oxide
owing to high emissivity of the coating made of single nanoscale
indium oxide. Few reports, however, have dealt with the coating
made of organic components and inorganic nanoparticles [4,5].
Polyurethanes are widely used in adhesives and coatings of
various materials, e.g., textiles, metals, and plastics [6–8]. In a
recent study, Crawford and Escarsega [9] systematically
reported the dynamic mechanical and durability properties of
novel polyurethane coating for military application. High
emissivity, however, can be found in native polyurethane and
nanooxide that will limit their practical applications. The
nanocomposites combining the merits of polymer and
* Corresponding author. Tel.: +86 25 52090617; fax: +86 25 52090617.
E-mail address: [email protected] (Y. Zhou).
0169-4332/$ – see front matter # 2007 Elsevier B.V. All rights reserved.
doi:10.1016/j.apsusc.2007.05.046
inorganic nanoparticles [10] is recommended to deal with this
problem. Recently, greater attention has been paid to the
preparation of polymer/nanoparticles composites [11–13]. For
instance, Chen et al. [14] reported the preparation of polyester-
based polyurethane/titania hybrid films using a sol–gel process.
Lee and Chen [15] also reported the preparation of PMMA/
titania hybrid films with 3-(trimethoxysilyl)propyl methacry-
late as the coupling agent. However, the use of conventional
synthetic methods results in agglomerating during the reaction
and incompatibility after it [16,17]. Ultrasonic irradiation could
be employed to overcome these disadvantages [18], and Suslick
et al. [19] have explored a variety of applications of ultrasound
to materials chemistry.
In the present paper, the nanocomposite of polyurethane/
TiO2 was synthesized through a simple and convenient
ultrasonic wave dispersion process and infrared emissivity
values at wavelength of 8–14 mm of the composite and its
components were investigated.
2. Experimental
2.1. Materials
Nanoparticles (TiO2) were prepared according to the
literature [20]; toluene 2,4-diisocyanate (TDI) was used with
Fig. 1. FTIR spectra of (a) pure nano-TiO2, (b) pure PU and (c) PU/nano-TiO2.
J. Chen et al. / Applied Surface Science 253 (2007) 9154–9158 9155
low pressure distilled; coupling agent (g-amidopropyl-
triethoxyl silicane) (KH550), o-phenylenediamine, urea, amyl
alcohol, 37% formalin, 4-methylpentanone-2, and dimethyl
formamide were all purchased from Sinopharm Chemical
Reagent Co., Ltd (Shanghai, China). All solvents were
purchased from commercial A.R. grade.
2.2. Characterization
FT-IR spectra were recorded on a Nicolet Magna-IR 750
(USA) spectrometer. First, the samples (PU, TiO2, PU/TiO2
nanocomposites) were dried, and then mulled with KBr pellets.
X-ray diffraction measurements of the composite and its
components were recorded using a Rigaku D/MAX-R with a
copper target at 40 kV and 30 mA. The powder samples were
spread on a sample holder and the diffractograms were recorded
in the range 5–808 at the speed of 58/min. Thermal analysis
experiments were performed using a TG/DSC apparatus
operated in the conventional TG/DSC mode (TMDSC, TA
Q-600, TA Instrument) at the heating rate of 10 8C/min to
simultaneously determine the correlation of temperature and
weight loss in a nitrogen atmosphere. The surface morphology
of the samples was monitored with transmission electron
microscopy (TEM) and scanning electron microscopy (SEM).
TEM was performed on a JEM-1230 microscope operating at
an accelerating voltage of 100 kV. SEM was obtained on the
microscope of LEO-1530vp. Infrared emissivity values of the
samples were carried out on an IRE-I Infrared Emissometer of
Shanghai Institute of Technology and Physics, China.
2.3. Apparatus
The reaction was performed on a JY 92-2D ultrasonic cell
crusher purchased from Scientz Biotechnology Co., Ltd
(Ningbo, China). Ultrasound was a wave of frequency
2 � 104 � 109 Hz and power 700 W.
2.4. Polymer synthesis
The poly [l,3-bis(methylene) benzimidazolin-2-one, toluene
2,4-(biscarbamate)] was synthesized by the typical method
[21]. The diol, viz., l,3-bis(hydroxymethyl) benzimidazolin-2-
one (self-prepared, 0.01 mol, 1.94 g) was dissolved in dry DMF
under N2 atmosphere with constant stirring. Then, diisocyanate
(TDI, 0.0 lmol, 1.742 g) taken in dry 4-methylpentanone-2 was
added in this solution over a period of l h. The reaction mixture
was heated for 2.5 h at 115 8C to obtain the solid. The mixture
was stirred continuously for 3 h, cooled, poured into distilled
water, and then filtered, washed with distilled water, and dried
under reduced pressure at 90 8C.
2.5. Preparation of PU/TiO2 nanocomposites
The preparation of PU/TiO2 nanocomposites was carried out
in an ultrasonic process. First, nanoparticles (0.3 g) were added
into acetone (10 mL), and a small amount of KH550 was
dissolved in H2O (10 mL). In a series of controllable
experiments we found that 10% weight percentage of
KH550 was optimized. Then the mixture of nanoparticles
and KH550 was irradiated under ultrasonic radiation for 30 min
at 30 8C, cooled to room temperature, centrifuged and dried.
After that 0.3 g nano-TiO2 and 0.l g PU were dispersed in
20 mL ethanol and the mixture was irradiated with high-
intensity ultrasound radiation for 30 min at 30 8C. After
irradiation, the resulting suspension was cooled to room
temperature and then centrifuged, and the precipitate was
washed twice with absolute ethanol and distilled water,
respectively. The solid was dried in vacuum at room
temperature for 6 h and was kept for further characterization.
3. Results and discussion
3.1. Spectral data
It can be seen, from the IR spectra of the pure TiO2, PU, and
PU/TiO2 shown in Fig. 1, that in pure TiO2, ı̂(OH) stretching
band and bending band are observed at 3423 and 1637 cm�1,
respectively. Following Knozinger [22], the observed broader
bands at 3500 and 3422 cm�1 were attributed to hydroxyl
groups on different sites and some varying interactions between
hydroxyl groups on TiO2, respectively. The bands at 643 and
540 cm�1 are assigned to the anatase nano-TiO2 [23]. However,
the carbonyl group of urethane and benzimidazolin-2-one is
shown in the region 1725 cm�1 [24]. In the case of the spectrum
of PU/TiO2, where the characteristic peaks of pure PU and TiO2
are still maintained, it may be proved that the structure pf PU
was affected by the presence of TiO2 implying that the TiO2 did
not react with the PU molecules.
3.2. Microstructure
Figs. 2–3 shows the transmission electron microscope and the
scanning electron microscopy micrographs of the pure TiO2
nanoparticles and PU/TiO2 nanocomposites. From Fig. 2 (a), it
can be clearly seen that the nanoparticles have some aggregation.
In contrast to this, in Fig. 2(b–d) and Fig. 3(a–d) the
Fig. 2. TEM micrographs of (a) pure nano-TiO2 and (b-d) PU/nano-TiO2.
J. Chen et al. / Applied Surface Science 253 (2007) 9154–91589156
nanocomposites with size of about 30–35 nm consist of the very
uniform particles. We can see clearly that the nanoparticles are
dispersed in PU matrix on nanoscale, which indicates the
formation of a nanocomposite in some way [25–27]. As
expected, through the ultrasonic technique nanoparticles, which
distribute in the polymer are homogeneous.
3.3. X-ray diffraction data
X-ray diffraction curves of the polymer, nanoparticle and
composite are shown in Fig. 4. PU (Fig. 4(a)) is amorphous
and does not exhibit any anisotropic behaviors [28]. From
Fig. 4(c), we can see that most of the characteristic peaks at
2u values of anatase TiO2 are kept intact. The average size
of the nanocomposites is calculated to be 30–35 nm
according to the Debye-Scherrer formula. However, the
intensities of anatase peaks become weaker in the presence
of PU and the peaks are widened. The findings indicate
that ultrasonic irradiation reduces the crystallite size of
anatase due to the generation of many localized hot spots in
the solution by the ultrasound irradiation, which further
gives rise to the homogeneous formation of a large number of
seed nuclei, leading to a smaller particle size [29–33]. This
feature also agrees with the previous TEM and SEM
measurements.
3.4. Thermal properties
A thermogravimetry-differential scanning calorimetry
(TGA-DSC) study of the obtained nanocomposite is shown
in Fig. 5. The TGA curve of PU/TiO2 composite shows a two-
step weight loss. The weight loss at about 100 8C in the first step
is attributed to the loss of residual water and organic solvent.
The second step, which starts at around 262 8C, corresponds to
polymer degradation. The second peak is much higher than that
of pure PU [28]. Meanwhile, it is obvious that at this
temperature, the total weight loss of the PU/TiO2 is 20%. As
can be seen, until 600 8C the total weight loss of the composite
is much lower than that of pure PU, suggesting that thermal
stability of the composite is improved considerably. The
possible reason for this behavior may be the reduced mobility
of urethane chains in the nanocomposite, which inhibits the
Fig. 3. SEM micrographs of PU/nano-TiO2 (�50000).
J. Chen et al. / Applied Surface Science 253 (2007) 9154–9158 9157
chain transfer reaction, thus slowing the degradation process
[34].
The DSC curve shows that the temperature of endothermic
peak at about 100 8C is attributed to the volatilization of
residual water and organic solvent. The exothermic peak
observed at 262 8C is related to the decomposition of the
polymer. In contrast to this, the decomposition of this kind of
pure PU is only 202 8C [28]. Meanwhile, some small
exothermic peaks observed from 359 to 518 8C are due to
the heat effect of the oxidation combustion of organic
substances [24]. Obviously, this result indicates a strong and
uniform interaction between PU and nanoparticles.
Fig. 4. X-ray diffraction patterns of (a) pure PU, (b) pure nano-TiO2 and (c) PU/
nano-TiO2.
3.5. Infrared emissivity
The infrared emissivity values at wavelength of 8–14 mm of
all the samples are tested (Table 1). It is clear that pure polymer
and TiO2 possess high emissivity values of 0.945 and 0.925,
respectively. Polyurethane has a high infrared emissivity value,
because this kind of polymer has strong absorbability at infrared
wave band [28], and commonly an increase in the absorbability
results in an increase in the emissivity [35]. TiO2 has a high
infrared emissivity value due to the high refractive index
(commonly larger than 0.8) [36]. Conversely, PU/TiO2
composite has the lower infrared emissivity value (0.538) than
Fig. 5. TGA-DSC curves of PU/nano-TiO2.
Table 1
Infrared emissivity values of samples
Samples Infrared emissivity
(eTIR at 8–14 mm)
PU 0.945
TiO2 0.925
PU/TiO2 0.538
J. Chen et al. / Applied Surface Science 253 (2007) 9154–91589158
both of its components. According to X-ray diffraction analysis,
there is no apparent difference in phase structure before and after
the measurement. Therefore, the decrease in infrared emissivity
may be owing to interfacial synergism forces such as hydrogen
bonds or electrostatic interactions between the organic and
inorganic components [37]. These interactions can alter the
original vibration mode of molecules, atoms or pendant groups
on interface between organic and inorganic components [38],
which have some effects on emissivity. Therefore, the decrease of
infrared emissivity of the nanocomposite is most likely to be a
direct consequence of the interfacial interactions.
4. Conclusions
A sonochemical method employed here may be a simple and
inexpensive route to synthesize the PU/nano-TiO2. Infrared
emissivity study at wavelength of 8–14 mn of nanocomposite
and its components showed that the composite possessed lower
emissivity value than those of pure PU and TiO2, and interfacial
interactions had great effect on emissivity of nanocomposites.
Thereby, the nanocomposites can be extended in application as
a novel low infrared emissivity material.
Acknowledgements
The authors are grateful to ‘‘Six Talents Pinnacle Program’’
of Jiangsu Province of China (06-A-033) and ‘‘the New
Century Talents Program’’ of ministry of education of China
(NCET-04-0482) for financial supports.
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