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Notice TP III
Analyses Thermiques
• Thermogravimétrie (TG) • Analyse thermique différentielle (DTA) • Calorimétrie Différentielle Programmée (DSC)
Définition : Group de techniques pour lesquelles une propriété physique d’un matériau est mesurée en fonction de la température, pendant la mesure le matériau étant soumis à un programme contrôlé en température.
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Assistant S.C. Sandu, 2004 Responsable: R. Sanjinés, 09-2014

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I. Introduction
Les techniques d’analyse thermique sont appliquées dans tous les domaines de la science, de l’archéologie à zoologie et pour tous les types de matériaux.
Tableau 1. Exemple de techniques d’analyse thermique
Technique Paramètre mesuré Instrument utilisé
Thermogravimétrie (TG) Masse Thermo balance
Analyse Thermique Différentielle (DTA)
Différence de températures Appareil DTA
Calorimétrie Différentielle Programmée (DSC)
Différence de flux de chaleur Calorimètre DSC
Analyse Thermomécanique (TMA)
Volume ou longueur Dilatomètre
Thermoluminescence (TL) Emission de la lumière Photo détectrice
Pour d’autres exemples de technique d’analyse thermique consulter la Ref. [1].
Les premières trois méthodes mentionnées auparavant (TG, DSC et DTA) peuvent fournir des informations concernant la stabilité thermique des matériaux et les changements d’enthalpies pendant la décomposition thermique ou pendant les changements de phase. Ces sont ces techniques qu’on va employées au cours de ce TP.
II. Rappels théoriques
2.1. L’analyse thermogravimétrie
C’est une technique dans laquelle la variation de masse d’un échantillon est mesurée en fonction du temps ou de la température lorsque la température de l’échantillon change de façon contrôlée (dite aussi en mode programmée) dans un atmosphère déterminée. Il y a trois modes possibles :
a) mode isotherme: la mesure se fait à température constante

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b) mode quasi-isotherme: l’échantillon est chauffé seulement quand sa masse n’est varie pas. Lorsque la masse change la température est maintenue constante.
c) mode dynamique (le plus utilisé): l’échantillon est chauffé dans un environnement contrôlé (sous vide, gaz neutre, etc.). La montée en température est réglée de sorte à chauffer l’échantillon progressivement, de préférence d’une manière linéaire.
Quelques applications pour la thermogravimétrie :
1. Décomposition thermique des matériaux organiques et inorganiques (polymères, metaux, etc.)
2. Corrosion de métaux dans différentes atmosphères 3. Détermination des températures et des vitesses de sublimation ou
d’évaporation 4. Mesures de désorption, absorption et adsorption 5. Calcination des matériaux
L’appareille de mesure est la thermo balance. L’instrument doit être capable
d’enregistrer les variations de masse avec une précision meilleure de 0.01% est les variations de température avec une précision de 1%. Dans nos expérimentations nous utilisons une microbalance électronique [ref. 1, p 89]. La relation proportionnelle qui lie l’intensité du courant à la force d’équilibrage électromagnétique associe la mesure des variations de courant à la mesure des variations de masse [2].
2.2. L’analyse thermique différentielle (DTA)
C’est une technique dans laquelle la différence de température entre l’échantillon et la référence est mesurée en fonction du temps ou de la température lorsque la température de cet ensemble est programmée dans une atmosphère contrôlée.
2.3. La calorimétrie différentielle programmée (DSC)
C’est une technique dans laquelle le flux de chaleur (puissance thermique) de l’échantillon et la référence est mesuré en fonction du temps ou de la température lorsque la température de cet ensemble est programmée dans une atmosphère contrôlée. En pratique, on mesure la différence de flux de chaleur entre un creuset contenant l’échantillon et un creuset de référence.
2.4 Dispositifs expérimentaux
Les changements de température (en DTA) ou de flux de chaleur (en DSC) sont la conséquence de transitions ou de réactions endothermique (∆Q < 0) ou exothermique (∆Q > 0) [Ref.1, p 214] comme celles déterminées par les changements de phases, fusion, cristallisation, transitions vitreuses, dissociations, oxydations, polymérisation, etc. Ces changements sont détectés par une méthode différentielle (voir figure 1).

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Fig 1. Représentation schématique d’un dispositif expérimental de DTA
Fig.2 Courbe DTA en fonction de la température de chauffage : I – transition de deuxième ordre (ex : transition vitreuse) II et III – pics endothermes (ex : fusion ou décomposition)

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Les courbes DTA ou DSC en fonction de la température de chauffage contiennent des séries de pics orientés négativement (vers le bas) ou positivement (vers le haut) de l’axe de flux de chaleur (Fig. 2). Les positions des pics sur l’axe de température et leur nombre permettent l’identification qualitative du matériau analysé. Quant aux aires des pics, elles permettent les calcules des chaleurs de réaction, transition, fusion, ou cristallisation. Parfois, des informations sur les cinétiques de réactions peuvent être obtenir à partir des courbes DTA/DSC.
La différence de principe entre DTA (b) et DSC (a) est illustrée dans la figure 3.
Fig. 3 Représentation schématique des dispositifs DSC et DTA
2.5 Transition de phase et réactions chimiques
Au sens thermodynamique, la phase caractérise l’état physique d’une substance chimique déterminée ou d’un mélange homogène de telles substances. Un système homogène est un système dont les propriétés restent identiques en tout point. De cette façon on distingue les phases gazeuses, liquides et solides, et dans le cas de la matière condensée, les modifications allotropiques éventuelles concernant la structure cristalline, magnétique, électrique, etc.

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Une transition de phase est donc le passage de la substance d’une phase à une autre qui se traduit par une modification de la structure interne de la substance. Tous les changements de phase s’accompagnent d’une absorption ou d’un dégagement de chaleur. Il faut toujours fournir de la chaleur à un solide pour le fondre ou le sublimer. Inversement, la solidification d’un liquide ou la condensation d’une vapeur dégage de la chaleur.
On appelle chaleur latente de changement de phase d’un corps pur la quantité de chaleur L qu’il faut fournir ou soutirer à un corps d’une certaine masse pour la transformer d’une phase en une autre dans des conditions d’équilibre isotherme/ isobare. Ainsi donc, expérimentalement l’existence d’une chaleur latente facilite la détection d’un changement de phase. Evidemment, la quantité de chaleur présente lors d’un changement de phase dépend non seulement de la chaleur latente mais aussi de la masse total de la substance.
Les réactions chimiques d’oxydation ou de réduction mettent en jeu de l’énergie, le plus souvent sous forme de chaleur. Lorsqu’une réaction thermochimique dégage de l’énergie la réaction est dite exothermique. Au contraire, si la réaction adsorbe de l’énergie, elle est dite endothermique. La détection de ces chaleurs de réaction ou enthalpies de formation permet d’étudier certains mécanismes d’oxydation, de nitruration, d’hydrolyse, etc.
2.6 Transfert de chaleur
Un transfert de chaleur peut s’opérer suivant les trois processus suivants : par conduction, par convection, et par rayonnement thermique. Dans le cas de la conduction thermique, l’énergie thermique s’échange par contact direct de deux corps. C’est ce type de transfert de chaleur qui est utilisé pour la mesure de la température entre l’échantillon et le four. Par contre les processus d’échange de chaleur par convection et par rayonnement thermique sont utilisés pour chauffer l’échantillon. A basses et moyennes températures (4K-600K) le chauffage se fait principalement par convection en utilisant comme gaz d’échange un gaz neutre (He, Ar, N2) ou un gaz réactive (O2, CO, NOx, H2,.. ). A hautes températures ou sous vide, le rayonnement thermique assure un chauffage efficace.
III. Buts de l’expérience
1. Acquérir une connaissance de techniques d’analyses thermiques et de leurs applications.
2. Connaître quels sont les effets physiques et chimiques sur un échantillon soumis à un échauffement prolongé et ou programmé.
3. Investiguer et comparer les propriétés physico-chimiques des matériaux. 4. Calibrer un DSC en utilisant de standards pour la mesure des chaleurs
spécifiques de fusion et de cristallisation des différents matériaux. 5. Etudier la cinétique de la décomposition thermique des composés.

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IV. Exemples d’applications:
1. Transition vitreuse, cristallisation et fusion du PET. 2. Décomposition thermique d’oxalate de calcium hydraté. Calcul des vitesses de
réaction chimique. 3. Cristallisation d’un alliage amorphe Ni-Ti. 4. L’étude des alliages eutectiques (Ex. Sn-Pb). Déterminer la composition
chimique d’un alliage eutectique à partir de données de ATD. 5. Comportement des substances organiques (sucre, pâte de biscuits) lors de leur
cuisson (Attention : adapter la quantité de matière à analyser et le domaine de température !).
6. Décomposition thermique et formation de phases d’une poudre de YBaCuO. 7. Observer le comportement et identifier les changements de phase des
polymères soumis au chauffage contrôlé (lire par ex. ref. 7). 8. Caractérisation de composés ternaires ou quaternaires (poudres) synthétisés par
la méthode SOL-GEL (exemple ref. 8) .
Bibliographie:
1. Thermal Analysis (3rd Edition), W. Wendlandt, John Wiley and Sons (USA), 1986.
2. Notices SETARAM 3. Thermal Analysis, B. Wunderlich, Academic Press (USA),1990. 4. Thermal Characterization of Polymeric Materials, E.A. Turi, Academic Press
(USA), 1981. 5. Thermal Analysis of Foods, V.R. Harwalkar, Elsevier (UK), 1990. 6. Thermal kinetic TG-analysis of metal oxalate complexes, Li Jun &co,
Thermochimica Acta, 406 (2003) 77-87. 7. « Study of the early deactivation in pyrolysis of polymers in the presence of
catalysts », A. Marcilla, A. Gomez-Siurana, D. Berenguer, J. Anal.Appl. Pyrolysis (2007).
8. Synthesis and characterization of Ba1-xSrxTiO3 nanopowders by citric acid gel method », Z. Wang et al, Ceramics International (2006).

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JAAP-2061; No of Pages 7
Study of the early deactivation in pyrolysis of polymers in
the presence of catalysts
A. Marcilla *, A. Gomez-Siurana, D. Berenguer
Dpto. Ingenierıa Quımica, Facultad de Ciencias, Universidad de Alicante, Apartado 99, 03080 Alicante, Spain
Received 20 June 2006; accepted 2 February 2007
Abstract
In this work, the early degradation step of the pyrolysis of some polymers in the presence of certain catalysts has been studied using
thermogravimetric analysis (TGA). Three commercial polymers (PE, PP and EVA) and three catalysts were studied (ZSM-5, MCM-41a, and
MCM-41b), and the MCM-41a catalyst has been selected for the analysis of the earlier steps of the pyrolysis process carried out in the presence of
catalysts. Several cycles of heating–cooling were performed using a thermobalance, in order to analyze the influence of the first stages of
decomposition on the activity of the more accessible active sites involved. In this way, the behaviour of the polymer–catalyst mixtures (20% (w/w)
of catalyst) was studied and compared with that observed in the corresponding thermal degradation as well as in the pyrolysis in the presence of
catalysts, in a single heating cycle.
The results obtained clearly show the existence of an early degradation step. For a polymer–catalyst system with low steric hindrances such as
PE-MCM-41, this early degradation step causes a noticeable decrease of the catalyst activity for the main decomposition step (i.e., cracking of the
chain). The decrease of the catalytic activity is lower for a polymer–catalyst system with higher steric restrictions, as occurs in the EVA-MCM-41
degradation process. However, in this case, the catalyst activity in the first decomposition step (i.e., the loss of the acetoxi groups) is noticeable
decreased after one pyrolysis run, thus reflecting that the active sites involved are mainly the most accessible ones.
# 2007 Elsevier B.V. All rights reserved.
Keywords: Pyrolysis; Catalysts; Deactivation; PP; EVA; HZSM-5; MCM-41
www.elsevier.com/locate/jaap
J. Anal. Appl. Pyrolysis xxx (2007) xxx–xxx
1. Introduction
The rapid growth of the range of applications of plastics:
packaging, agriculture, construction, household, etc., has
turned these materials into a serious environmental problem
since plastics comprise 10 wt% (>30 vol.%) of municipal solid
waste.
Pyrolysis is one of the promising alternatives to dumping or
incineration for the treatment of plastic wastes, where the
polymer sample is heated in an inert atmosphere causing the
cracking of the polymer backbone. The thermal cracking of
polymers produces a very complex mixture of products, which
may be used as fuel but has low value as a source of chemicals.
However, by plastic cracking over different solid catalysts
(pyrolysis in the presence of catalysts) it is possible to obtain
* Corresponding author. Fax: +34 965903826.
E-mail address: [email protected] (A. Marcilla).
0165-2370/$ – see front matter # 2007 Elsevier B.V. All rights reserved.
doi:10.1016/j.jaap.2007.02.002
Please cite this article in press as: A. Marcilla et al., J. Anal. Appl. Py
products with higher commercial value and with a wider
number of applications [1–3].
Modern cracking uses zeolites as catalysts [1–5], which
cause an important reduction in the decomposition temperature
and allow more valuable gaseous products to be obtained.
However, the pore size of the zeolites is limited to a maximum
value of about 1.0 nm, which hinders the access of bulky
molecules to the acid sites located inside the channels. MCM-
41 is a catalyst, member of the relatively new family of
mesoporous materials, first synthesized in 1992 by Beck et al.
[6], which possesses highly regular arrays of uniform size pore
channels ranging from 1.5 to 10 nm and a large surface area,
thus improving the accessibility to the active sites located in the
inner of the mesopores [6].
Coke formation and its retention inside the pores is the main
cause of deactivation of zeolite and aluminosilicates catalysts
in hydrocarbon processing. Deactivation of these catalysts in
the pyrolysis of polymers in the presence of catalysts is mainly
due to active site poisoning and pore blockage by coke
rol. (2007), doi:10.1016/j.jaap.2007.02.002

Table 1
Characteristics of the commercial polymers
Material Density
(g/cm3)
Melt index
(g/10 min)a
Vicat
point
(8C)
Tensile
modulus
(MPa)
LDPE 780R 0.923 20 (190/16) 93 115
PP Novolen 1100L 0.910 8 (230/2.2) 70 1500
EVA Escorene UL15028CC 0.950 150 (125/0.3) 64 13
a 8C/kg.
A. Marcilla et al. / J. Anal. Appl. Pyrolysis xxx (2007) xxx–xxx2
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JAAP-2061; No of Pages 7
deposition [7]. Both coking rate and coke composition depend
on a variety of parameters such as the characteristics of
the catalyst pore structure, the characteristics of the acid
sites, the nature of the reactant and the operating conditions
[8,9].
The study of the pyrolysis of polymers in the presence of
catalysts using thermogravimetric analysis (TGA) shows a
early degradation step of the process for some polymer–catalyst
systems. This process causes a widening of the corresponding
peaks in the derivative of TGA curves (DTG curves), and in
some cases, the appearance of a shoulder [10]. This early
degradation step of the decomposition reactions is related to the
acid sites located on the surface of the material [11,12]. In fact,
according to bibliography [13], the influence of the acid sites
located on the external surface and in the pore mouth region of
zeolites cannot be ignored, although the concentration of these
acid sites is assumed to be smaller, generally 3–5% of the total
acid sites.
As an example, previous works on the pyrolysis of EVA in
the presence of catalysts [12,14] showed that, despite the
presence of some catalyst advances noticeably at the beginning
of the pyrolysis of the first step of EVA pyrolysis, the
corresponding temperature of maximum reaction rate – i.e., the
peak temperature in the DTG curves – remains almost
unaltered, thus suggesting a possible simultaneous deactivation
of the active sites involved in the early degradation step, and
consequently the overall process ends at the same temperature
as in the absence of catalyst.
In a previous work [10], a comparative study of the
behaviour of different solid acid catalysts in the pyrolysis of
different polymers was performed. In that work, a possible
influence of some catalysts in the initial degradation steps of
some polymers was observed. A hypothesis was suggested
that the active sites located on the external surface of the
catalyst or, in the case of mesoporous materials, the more
easily accessible active sites, would be involved in these
processes. On the other hand, as previously mentioned, some
studies about the pyrolysis of EVA over different catalysts
[12,14] also suggested that these active sites would undergo
deactivation processes simultaneous with their participation
in the above-mentioned earlier degradation steps. Therefore,
this work is focused on the study of the initial stages of the
pyrolysis in the presence of catalysts of three selected
polymers, with the main objective of validating the
hypothesis previously suggested. In this way, TGA studies
were carried out, and four cycles of heating–cooling were
performed in order to analyze the influence of the first stages
of decomposition on the activity of the active sites involved.
Three polymers (Polyethylene, PE, polypropylene, PP and an
ethylene–vinyl acetate copolymer, EVA) were selected, and
three catalysts were studied (ZSM-5, MCM-41a, and MCM-
41b). Then, MCM-41a was selected to study this phenom-
enon in more detail. The behaviour of polymer-catalyst
mixtures (20% (w/w) of catalyst) was studied and compared
with that observed in the corresponding thermal degradation
as well as in the pyrolysis in the presence of catalysts, in a
single heating cycle.
Please cite this article in press as: A. Marcilla et al., J. Anal. Appl. Py
2. Experimental
2.1. Materials
Table 1 shows the main characteristics of the commercial
polymers (polyethylene, PE, polypropylene, PP, and an
ethylene-vinyl acetate copolymer, EVA) selected in this work.
The nominal vinyl acetate (VA) content of the EVA copolymer
was 27% (w/w). The catalysts used were ZSM-5, MCM-41a
and MCM-41b, prepared in accordance with the method
reported in literature [15,16]. The main characteristics of these
catalysts are summarized in Table 2. As can be seen, in the case
of the MCM-41a, the low value of the Si/Al ratio produces a
material with high acidity. This material also presents a high
pore size and a large surface area, typical of this type of material
[10].
Pure polymer or copolymer samples as well as the
corresponding mixtures with 20% (w/w) catalyst were
pyrolysed under the experimental conditions described in the
next section.
2.2. Equipment and experimental conditions
The pyrolysis experiments were carried out in a Netzsch TG
209 thermobalance controlled by a PC under the Windows
operating system. The atmosphere used was nitrogen with a
flow rate of 45 STPml/min. The balance and the oven
thermocouple of the equipment were calibrated following the
manufacturer’s instructions. Pure polymers as well as mixtures
of powdered polymers and a catalyst of around 4 mg (3.2 mg of
the polymer with 0.8 mg of the catalyst) were pyrolysed.
In the pyrolysis in the absence of catalyst as well as in the
pyrolysis runs in the presence of catalyst in a single heating
cycle, the temperature was raised to 550 8C with a heating rate
of 10 8C/min. On the other hand, for studying the influence of
the initial decomposition steps in the overall process, four
cycles of heating–cooling were applied to the polymer + ca-
talyst system studied. The heating–cooling cycles have been
performed under N2 atmosphere, in the thermobalance
equipment, which is provided with a cooling system, and
involve a heating rate of 10 8C/min and a cooling rate of 50 8C/
min. The initial and final temperatures were 50–300 8C for the
PE mixtures, 50–245 8C for the PP mixtures, and 50–235 8C for
the EVA mixtures, respectively. In each heating run,
temperature was raised to a value below the temperature
corresponding to the apparent beginning of the thermal
decomposition of each polymer. All the heating–cooling runs
rol. (2007), doi:10.1016/j.jaap.2007.02.002

Table 2
Characteristics of the three catalysts used
Property HZSM-5 MCM-41a MCM-41b
Pore size (nm)a 0.51 � 0.55 1.7 2.4
BET area (m2/g)b 334 956 1136
External surface area (m2/g)c 67 126 383
Pore volume (cm3/g)d 0.27 1.00 1.34
Si/Al ratioe 24 7 47
Acidity (mmol/g)f 1.36 2.08 0.60
Acidity weak acid sites f 0.82 1.39 0.60
Acidity strong acid sitef 0.54 0.69 –
Tdesorption NH3 (8C)f weak
acid sites
165 155 138
Tdesorption NH3 (8C)f strong
acid sites
385 550 –
Aloct/Altetrag 0.12 0.70 0.37
a BJH.b N2 adsorption isotherms; BET method.c N2 adsorption isotherms; t method.d N2 adsorption isotherms; measured at P/P0 = 0.995.e XRF.f TPD of NH3.g NMR.
Fig. 2. DTG and TGA curves from NH3 TPD of the three catalysts studied by
[10].
Fig. 1. TGA and DTG curves obtained in the pyrolysis of PP in the absence of
catalyst and in the pyrolysis in the presence of the different catalysts [10].
A. Marcilla et al. / J. Anal. Appl. Pyrolysis xxx (2007) xxx–xxx 3
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JAAP-2061; No of Pages 7
have been performed under the same experimental conditions
above described.
In order to evaluate the influence of the heating–cooling
cycles on the activity of the catalyst, an experiment was
performed, where the pyrolysis run was stopped when the
fourth cycle was ended and more fresh polymer was added in
order to once more achieve a 20% (w/w) catalyst mixture; then
the pyrolysis in the presence of catalysts was carried out in the
thermobalance, from 50 to 550 8C at 10 8C/min.
3. Results and discussion
According to bibliography [17,18], the first step in the
pyrolysis of a polymer in the presence of catalysts consists in
the cracking of the polymeric chains over the catalyst surface,
leading to oligomers, with higher possibilities for access to the
active sites located in the inner part of the catalyst pores, where
the complete degradation of the oligomers occurs. However,
most articles – referring to [17,19] or not referring to [18,20,21]
this initial step – do not report any noticeable loss of weight
associated to the oligomer formation, and the references are few
where a two-step process is considered [22]. In fact, according
to the results obtained in the present work, the existence of an
initial step involving the formation of volatile compounds
seems to be very dependent on the chemical and structural
characteristics of the polymer and the catalyst.
Fig. 1 shows the TGA and DTG curves obtained for the
pyrolysis of PP in the presence of the two different MCM-41
samples as well all in the presence of HZSM-5 zeolite. The
behaviour of these systems was discussed and compared
elsewhere [10], and here only the relative importance of the
initial decomposition step is emphasised. According to Table 2,
the main differences between the two MCM-41 samples
(MCM-41a and MCM-41b) are related to the respective BET
area and pore size (BET area 956 and 1136 m2/g and pore size
Please cite this article in press as: A. Marcilla et al., J. Anal. Appl. Py
of 1.7 and 2.4 nm, respectively) and the acidity (2.08 and
0.60 mmol/g, respectively). The main characteristics of the
HZSM-5 sample were BET area of 334 m2/g, pore size of
0.51 nm � 0.55 nm and acidity of 1.36 mmol/g [10]. Accord-
ing to these values, the higher specific surface and pore size of
MCM-41b favours the increase of the activity of this sample,
but the higher acidity of MCM-41a results in a higher activity,
as can be seen in Fig. 1, and as discussed elsewhere [10]. On the
other hand, the lower specific surface of HZSM-5 leads as a
consequence to the lower activity of this material in comparison
with the two MCM-41 samples.
According to the results of Fig. 1, the tail appearing at
temperatures below the peak temperature would suggest, for the
three catalysts, the existence of an initial step, and this is
specially marked in the presence of MCM-41a. This behaviour
reflects a clear influence of the catalyst characteristics, and
suggests that this can be only clearly observed if the catalyst
possesses a certain combination of pore size, specific surface
and acidity which lead to the existence of a high enough number
of very accessible active sites with also high enough acidity.
Fig. 2 shows the TGA and DTG curves obtained in programmed
thermal desorption of NH3, in the conditions described
elsewhere [10] for the catalysts reported in Fig. 1. The first
peak – i.e., the peak at lower temperatures – corresponds to the
NH3 desorption from the weak acid sites, whereas the second
rol. (2007), doi:10.1016/j.jaap.2007.02.002

Fig. 3. TGA and DTG curves obtained for the pyrolysis in the absence of
catalyst and in the presence of MCM-41a catalytic pyrolysis at 10 8C/min of (a)
PE, (b) PP and (c) EVA.
Table 3
Temperature of maximum decomposition rate for the main decomposition steps
of the different systems studied
Sample Experiment T (8C)
PE Thermal 473
PE-MCM-41 Conventional pyrolysis 358
PE-MCM-41 Pyrolysis after 4 cycles-polymer addition 386
PP Thermal 462
PP + MCM-41 Conventional pyrolysis 340
PP + MCM-41 Pyrolysis after four cycles-polymer addition 356
EVA Thermal 353–468
EVA + MCM-41 Conventional pyrolysis 353–406
EVA + MCM-41 Pyrolysis after 4 cycles-polymer addition 353–405
A. Marcilla et al. / J. Anal. Appl. Pyrolysis xxx (2007) xxx–xxx4
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JAAP-2061; No of Pages 7
peak corresponds to NH3 desorption from stronger acid sites.
The respective peak temperatures indicate the relative strength
of the acid sites. As can be seen, the strength of the weak acid
sites is similar for the three catalysts; but MCM-41b does not
possess strong acid sites, and the strength of the strong acid sites
of MCM-41a is noticeably higher for MCM-41a than for
HZSM-5. Table 2 shows the acidity associated to each type of
acid sites for each material. As can be seen MCM-41a possesses
the higher acidity. Therefore, the two main characteristics of
this material – i.e. high acidity and high accessibility – support
its role in the earlier stage of the pyrolysis in the presence of
catalysts. The behaviour observed for MCM-41b shows that the
only presence of accessibility is not enough for enhancing the
early step of the pyrolysis process. On the other hand, neither
high acidity nor strong acid sites are enough, as the behaviour of
HZSM-5 shows, and the simultaneous presence of high
accessibility properties is also needed.
Therefore, according to the previous comments, MCM-41a
has been selected for the detailed study of the early degradation
step of the pyrolysis in the presence of catalysts process. As
shown in Table 2, this material has high acidity and very
accessible active sites. Fig. 3 shows the TGA and DTG curves
corresponding to decomposition in the absence of catalyst and
the MCM-41a-pyrolysis of PE, PP and EVA. As can be seen, the
DTG curves corresponding to the pyrolysis of PE and PP in the
presence of catalysts (Fig. 3a and b) exhibit a shoulder at
temperatures below the temperature of maximum reaction rate
– i.e., the peak temperature – indicating the existence of an
initial reaction step with some weight loss, i.e. involving the
generation of volatile compounds, which is different to the
main reaction step, despite the fact that both are clearly
overlapped. This shoulder does not appear in the curves
corresponding to the thermal processes curves and, therefore, it
can be concluded that the catalyst must be involved in the
reactions generating the shoulder. As the comparison between
the curves corresponding to the pyrolysis in the absence and in
the presence of catalysts of each polymer shows (Fig. 3a and b),
and in good agreement with bibliography [23–25], the presence
of the catalyst causes a noticeable decrease in the temperature
of maximum reaction rate for the main decomposition step (see
Table 3). Therefore, despite the clear appearance of an early
degradation step, no conclusion can be extracted in relation to
the above-mentioned eventual deactivation processes from the
curves shown in Fig. 3a and b and only the role of the catalyst in
the early beginning of the decomposition can be emphasised.
Fig. 3c shows the TGA and DTG curves corresponding to
the decomposition of EVA in the absence and in the presence of
catalysts. As in the previous case, a shoulder appears in the
DTG peak, corresponding to the first decomposition step and
associated to the participation of the catalyst in the early
degradation step of the process. However, some differences
with respect to the PE and PP cases can be observed. It is well
known that whereas the decomposition of PE and PP in the
absence and in the presence of catalysts show a single main
decomposition step [26], the decomposition of EVA proceeds
through two main decomposition steps [12,27–29], which
involve, respectively, the vinyl acetate groups (VA groups) loss
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A. Marcilla et al. / J. Anal. Appl. Pyrolysis xxx (2007) xxx–xxx 5
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and the cracking of the polymeric chain resulting from the
previous step. These two steps are reflected in the weight loss of
the TGA curves and in the peaks of the corresponding DTG
curves of Fig. 3c. According to bibliography [12], a shift of the
second decomposition step towards lower temperatures appears
as a consequence of the presence of the catalyst, whereas no shift
in the temperature peak of the first decomposition step can be
observed (see Table 3). As in the cases of PE and PP, the early
beginning also appears in the degradation of EVA in the presence
of catalysts. However, in this case, the reaction step affected by
the early beginning is not the cracking of the chain, but the loss of
VA groups. Therefore, it can be concluded that the catalyst also
acts in the first step of EVA degradation, provoking a widening of
the corresponding interval of reaction temperature. Moreover,
the temperature of maximum rate for the first step results almost
unchanged, thus suggesting that the active sites involved in the
process undergo some deactivation process. Nevertheless,
despite this eventual deactivation, related to the participation
of the catalyst in the VA groups loss, the catalyst maintains
enough activity to reduce the temperature of the second
decomposition step, where the polymeric chain is cracked
(see Table 3). Considering the voluminous nature of the VA
groups, the hypothesis that the active sites involved are the more
accessible ones can be suggested.
Therefore, there are two aspects to be studied and assessed:
(a) the influence of the external active sites in the early
beginning of the decomposition process and (b) the eventual
deactivation of these active sites. The first question will be
clarified through the comparison among the behaviours of
different polymer + catalyst systems, and applying the meth-
odology described in the previous section for performing
several consecutive heating–cooling cycles. The second
question will be solved considering the behaviour during these
cycles together with the study of the case where fresh polymer
was added, and then the pyrolysis is continued until 500 8C, in
comparison with the pyrolysis runs in the presence of catalyst,
in a single heating cycle.
3.1. Influence of the external active sites in the early
beginning of the decomposition process
The comparison between Fig. 3a and b shows that the initial
degradation step in the pyrolysis in the presence of catalysts is
more pronounced for the PP decomposition than in the case of
PE. This fact could be related to the high number of tertiary
carbon atoms in the PP chains, which results in a more reactive
polymer [10,30]. However, the case of the pyrolysis of EVA in
the presence of catalysts, also with high number of tertiary
carbons, deserves a separate discussion. Unlike PE and PP,
whose degradation occurs in a main single step, as mentioned
above, the EVA pyrolysis involves two steps. Moreover,
according to bibliography [12], the peak temperature of the first
step is almost not affected by the presence of the acid solid.
Therefore, there are two possibilities:
(a) The chemical processes involved in the early degradation
step of EVA pyrolysis are similar to those occurring in the
Please cite this article in press as: A. Marcilla et al., J. Anal. Appl. Py
cases of PE and PP. In other words, the weight loss observed
before the DTG peak related to the first step of EVA
decomposition is a result of the same chemical reactions in
both cases. However, this hypothesis does not seem very
feasible, because it implies that the catalytic cracking of the
chain could start before the VA groups loss, and this is not
supported by experience [14,27,29].
(b) The active sites of the catalyst are also involved in the step
of VA groups loss. Therefore, the catalytic phenomenon
observed in this case is somewhat different than those
involved in the cases of PE and PP, not corresponding to the
cracking reactions of the main chain, but also involving the
availability of very accessible active sites with enough
acidity. According to the bibliography, this seems to be the
more probable hypothesis, as shown by the composition of
the gas evolved during the first step of EVA pyrolysis (i.e.,
mainly acetic acid). Therefore, the results obtained show
that the process of loss of the VA group’s loss also
undergoes the early degradation step.
3.2. Eventual deactivation of the active sites in the early
beginning of the pyrolysis process in the presence of
catalysts
Fig. 4 shows the TGA curves obtained in the heating–
cooling cycles performed for each polymer + catalyst system.
For each polymer, the final temperature of the heating cycles is
different (300 8C for the PE mixture, 245 8C for the PP mixture,
and 235 8C for the EVA mixture), and has been selected below
the temperature where the pyrolysis in the absence of catalyst
starts, in order to ensure that the weight loss observed could
only be attributed to the catalyst presence. As can be seen, for
the three polymers, the weight loss obtained in the first heating
cycle is higher than that obtained in the next cycles. This fact
can be explained considering that the active sites involved in
this process deactivate quickly, resulting in a material with less
capacity for its catalytic role in the following cycles. In other
words, considering that the existence of deactivation simulta-
neous to the initial step occurs.
The analysis of the different heating–cooling cycles shown
in Fig. 4 indicates that the weight loss associated to the initial
step starts at lower temperatures in the first cycle than in those
following. Table 4 shows the temperatures of the starting point
of the weight loss associated to the first and to the following
heating cycles. Despite the fact that the low temperature
observed for the first cycle could be related to the elimination
of some adsorbed water on the catalyst, a clear decrease of the
starting temperature for the degradation process can be
observed, thus suggesting that deactivation readily occurs.
Moreover, the weight loss observed in each cycle is noticeably
lower in the case of EVA than in the cases of PE and PP. This
behaviour is in good agreement with the fact that the
degradation step affected by the early degradation step
involves lower weight loss in the case of EVA, where only
the 27% corresponding to the VA groups is pyrolysed, in
contrast to the case of PE and PP, where 100% of polymer may
react.
rol. (2007), doi:10.1016/j.jaap.2007.02.002

Fig. 4. TGA curves corresponding to the heating–cooling cycles of (a)
PE + MCM-41, (b) PP + MCM-41 and (c) EVA + MCM-41.
Table 4
Temperatures corresponding to the starting point of the weight loss in the first
and in the following heating cycles for the different polymers studied
Polymer T (8C)
Cycle 1 Cycle 2 Cycle 3 Cycle 4
PE 89 208 217 225
PP 90 174 176 181
EVA 70 162 167 175
Fig. 5. TGA and DTG curves corresponding to the pyrolysis in the absence and
in the presence of catalyst experiments performed in different conditions for (a)
PE, (b) PP and (c) EVA.
A. Marcilla et al. / J. Anal. Appl. Pyrolysis xxx (2007) xxx–xxx6
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Please cite this article in press as: A. Marcilla et al., J. Anal. Appl. Py
Fig. 5 shows the DTG curves corresponding to the following
pyrolysis runs: (i) pyrolysis in the presence of catalysts, in a
single heating cycle, (ii) pyrolysis in the presence of catalysts
after the four heating–cooling cycles, with addition of fresh
polymer, and (iii) pyrolysis in the absence of catalyst, performed
as described in Section 2. As can be seen, for the three polymers,
the shoulder appearing before the peak of the DTG curves (the
only peak in the cases of PE and PP and the first peak in the case of
EVA), which has been related to the early degradation step, is
clearly diminished after the heating cycles. This behaviour again
indicates that simultaneous deactivation processes occur,
provoking a noticeably loss of the activity of the catalyst after
rol. (2007), doi:10.1016/j.jaap.2007.02.002

A. Marcilla et al. / J. Anal. Appl. Pyrolysis xxx (2007) xxx–xxx 7
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JAAP-2061; No of Pages 7
the heating–cooling cycles, when the fresh polymer is added and
the pyrolysis process is completed.
In the cases of PE and PP, when the pyrolysis in the presence
of catalysts is completed until the complete degradation of the
polymer, the catalyst losses part of its activity after the heating–
cooling cycles, as compared with the pyrolysis in a single
heating cycle (see the corresponding peak temperatures in
Table 3), thus corroborating the previous comments. However,
in the case of EVA, the capacity of the catalyst to decrease the
temperature of the second decomposition step results almost
unmodified by the successive heating–cooling cycles. PE and
PP could access the most of the active sites, i.e. those located on
the external surface, as well as those located at the opening of
the pores or mesopores and in the inner parts of the catalyst.
However, before the VA group loss, the EVA chains can only
access the more accessible active sites (simplifying, the
‘‘external’’ active sites), but leaving unaltered the less
accessible active sites, which therefore remain untouched for
the main decomposition step.
In good agreement with the previous comments, the
decrease of the activity, or in other words, the importance of
the deactivation process, is noticeably higher for PE than for PP.
As has been previously suggested, this behaviour can be
explained considering that the lower steric hindrances
associated to the PE chains could favour the access to the
polymer chains to less accessible active sites, perhaps some
located in the inner part of pores, thus resulting in an increase of
the deactivation of these acid sites. On the other hand, in the
case of EVA the higher steric hindrances associated to the VA
groups make access to the ‘‘less exposed’’ of the more
accessible active sites more difficult, resulting in a lower loss of
activity. For the second decomposition step, (which according
to bibliography [12,14], and in agreement with Figs. 3c and 5c
and Table 3, proceeds through a catalytic mechanism), these
steric effects would be enhanced by the crosslinking
phenomena, suggested by some authors [31], occurring before
the second step of EVA decomposition.
4. Conclusions
The pyrolysis of polymers in the presence of catalysts could
involve the existence of an initial degradation step, depending
on the chemical and structural characteristics of the polymer
and the catalyst. The behaviour observed suggests that this step
can only be clearly observed if the catalysts possesses a certain
combination of pore size, specific surface and acidity which
leads to the existence of a high enough number of very
accessible active sites and with a high enough acidity. On the
other hand, the relative importance of the early beginning of the
process seems to be increased as the reactivity of the polymer
chains increase: i.e., when the number of tertiary carbon atoms
increases. In the case of the pyrolysis of EVA in the presence of
catalysts, the active sites of the catalyst seem to be also involved
in the VA groups loss process.
The results obtained suggest that deactivation processes
occur simultaneously to the initial step. The more accessible
active sites, involved in such processes, are quickly deactivated,
Please cite this article in press as: A. Marcilla et al., J. Anal. Appl. Py
resulting in a noticeable effect in the activity of the catalyst
versus the main decomposition step. On the other hand, the role
of these active sites, as well as the corresponding deactivation
process seems to be increased as the steric hindrances
associated to the polymer structure decreases.
Acknowledgements
Financial support for this investigation has been provided by
the Spanish ‘‘Comision de Investigacion Cientıfica y Tecno-
logica’’ de la Secretarıa de Estado de Educacion, Universi-
dades, Investigacion y Desarrollo and the European
Community (FEDER refunds) (CICYT CTQ2004-02187),
and by the Generalitat Valenciana (project ACOMP06/162).
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Synthesis and characterization of Ba1�xSrxTiO3
nanopowders by citric acid gel method
Zheng Wang a, Shenglin Jiang b, Guangxing Li a, Mingpeng Xi b, Tao Li a,*a Department of Chemistry, Huazhong University of Science and Technology, Wuhan 430074, China
b Department of Electronic Science and Technology, Huazhong University of Science and Technology, Wuhan 430074, China
Received 2 February 2006; received in revised form 20 February 2006; accepted 20 March 2006
Abstract
Stoichiometric and monophasic Ba1�xSrxTiO3 (x = 0.3) nanopowders were successfully prepared by the citric acid gel method using barium
nitrate, strontium nitrate and tetra-n-butyl titanate as Ba, Sr, Ti sources and citric acid as complexing reagent. Thermogravimetric analysis (TGA),
differential scanning calorimetry (DSC), infrared (IR) spectroscopy, X-ray diffraction (XRD) and scanning electron microscopy (SEM) were used
to characterize the thermal decomposition behavior, the crystallization process and the particle size and morphology of the calcined powders. The
results indicated that single-phase and well-crystallized Ba1�xSrxTiO3 (x = 0.3) nanopowders with particle size around 80 nm could be obtained
after calcining the dried gel at 950 8C for 2 h.
# 2006 Elsevier Ltd and Techna Group S.r.l. All rights reserved.
Keywords: Ba1�xSrxTiO3; Sol–gel synthesis; Nanopowders
www.elsevier.com/locate/ceramint
Ceramics International xxx (2006) xxx–xxx
1. Introduction
Ba1�xSrxTiO3 (BST) ceramics, one of the most interesting
materials due to its pyroelectric, ferroelectric and piezoelectric
characteristics, has been widely used in the preparation of high
dielectric capacitors, PTC resistors, transducers and ferro-
electric memories [1–4]. BST powders are usually prepared by
solid-state reaction [5,6] with calcination temperatures in the
range of 1300–1450 8C. Other preparation routes, including the
hydrothermal method [7], the precipitation method [8], the
metalorganic solution deposition (MOSD) technique [9] and
the sol–gel method [10,11], have been reported. It is widely
recognized that chemical synthesis methods are able to provide
high chemical purity, precise composition, uniform micro-
structure and a lower formation temperature of the perovskite
phase based on molecular scale mixing in the preparation of the
precursor [12]. The sol–gel route is proved to be a very
commonly applied chemical method for fabricating uniform
large area thin films and synthesizing powders of micrometer,
sub-micrometer, or nanometer size with high purity and
* Corresponding author. Tel.: +86 27 87544432; fax: +86 27 87544532.
E-mail address: [email protected] (T. Li).
0272-8842/$32.00 # 2006 Elsevier Ltd and Techna Group S.r.l. All rights reserve
doi:10.1016/j.ceramint.2006.03.015
Please cite this article in press as: Z. Wang et al., Synthesis and charac
Ceram. Int. (2006), doi:10.1016/j.ceramint.2006.03.015
homogeneity [13]. However, the sol–gel process based on
hydrolysis of metal alkoxides needs long refluxing time.
Furthermore, the expensive and unstable metal alkoxides or
mixtures of metal salts and metal alkoxides must be dissolved
in large quantities of organic solvents, implying a high cost. As
an alternative to methods reported previously, Liu and co-
workers [14] synthesized BST powder using a citrate gel
method firstly. The process has the advantages of simplicity and
no use of any contaminative and expensive reagents.
Furthermore, the morphology of the particles could be easily
controlled by changing the synthesis parameters.
In this paper, we focus on a novel sol–gel synthesis method
of BST nanopowders involving a new stable aqueous precursor
based on a metal–citrate complex system reported recently. Our
method herein offers an easy route to shorten the procedures,
save energy, easily control the final stoichiometry of BST
composition and lead to uniform, fine powders.
2. Experimental details
Ba1�xSrxTiO3 (x = 0.3) powders were synthesized by a
complex precursor route as summarized in Fig. 1. Citric acid
(99.5+%), tetra-n-butyl titanate, Ti(n-OC4H9)4 (98+%), H2O2
d.
terization of Ba1�xSrxTiO3 nanopowders by citric acid gel method,

Fig. 1. Flowchart for the preparation of BST powders.
Z. Wang et al. / Ceramics International xxx (2006) xxx–xxx2
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CERI-2415; No of Pages 5
(30 wt.% in H2O), Ba(NO3)2 (99.5+%), Sr(NO3)2 (99.5+%) and
ammonia solution (25–28 wt.% in H2O) were employed as the
starting ingredients.
Ti(n-OC4H9)4 was added to stirred deionized water, the
precipitation and turbidity were observed gradually, then the
precipitate was filtered and washed for several times with
deionized water. Citric acid and H2O2, both in a 2:1 molar ratio
against Ti(n-OC4H9)4, were added. With the addition of these
ingredients, the solution became orange in color and viscous. The
pH value of the solution was adjusted to 6 using ammonia
solution. A water-soluble crimson precursor for Ti(IV) was
prepared with continuous stirring and refluxing at 60 8C. After
stoichiometric amounts of Ba(NO3)2 and Sr(NO3)2 were
dissolved in citric acid solution (5 M) of pH 6 adjusted by
ammonia solution with molar ratio of CA:M=2:1 (CA, citric acid,
M, Ba, Sr), Ba(II) and Sr(II) precursors were mixed with Ti(IV)
precursor. During the process, the cations molar ratio of Ba:Sr:Ti
was 0.7:0.3:1. The whole mixture was refluxed at 60 8C for 1–2 h
with continuous stirring and then a porous yellow resin was
formed after drying in a furnace at 60 8C overnight under flowing
air. This solid resin precursor was pulverized and then calcined at
various temperatures for 2 h to obtain the BST powders.
The FT-IR spectrum was recorded with an EQUINOX55
(BRUKER) spectrometer by using KBr pellet. The XRD
patterns of the powders were recorded on a Model x’Pert PRO
of PANalytical B.V. diffractometer using Cu Ka radiation
(l = 1.5406 A) in the range from 108 to 808 (2u) to examine the
crystallization and structural development of BST powders.
Thermogravimetric analysis (TGA) and differential scanning
calorimetry (DSC) were performed on a TG/DSC apparatus
Please cite this article in press as: Z. Wang et al., Synthesis and charac
Ceram. Int. (2006), doi:10.1016/j.ceramint.2006.03.015
(Model NETZSCH STA 409 PC) with a heating rate of 10 8C/
min under flowing dry air. The particle size and morphology of
the samples were determined with a scanning electron
microscope (SEM, Model FEI Sirion 200).
3. Results and discussion
The synthesis method is an easy way of obtaining an
aqueous water-soluble precursor without large quantities of
organic solvents used in the synthesis process. In general, the
process consists of three major steps [15]: (1) the metal cations
react with carboxylate ligands to form metal carboxylate
complexes; (2) the formation of metal carboxylate gel by cross-
linking metal carboxylate complexes into a three-dimensional
structure; (3) the decomposition of the precursor gel at
moderate temperature. Note that the compositional homo-
geneity of the final BST powders is no longer ensured at
molecular level mixing once insoluble precipitates have formed
during the precursors preparation. Therefore, a key to success in
the preparation is to find out an experimental condition,
wherein the formation of insoluble precipitates does not occur
throughout sol and gel preparation, so that powders with high
chemical purity and precise composition can be synthesized.
The flowchart presented in Fig. 1 is based on the synthesis of
Ba(II) precursor and Sr(II) precursor reported by Liu and co-
workers [14], however, the preparation of Ti(IV) precursor is
modified: an easy way to synthesize clear Ti(IV) precursor by
the addition of H2O2 and ammonia, which can effectively avoid
the separation of an oil-like two-layer liquid to get Ti(IV)–
citrate complex in the works of Xu et al. [16] and Shen et al.
[17]. Moreover, the formation of a porous drying gel at lower
temperature in furnace does not need higher temperature
(120 8C in vacuum [17]), which is significant in potential
industrial application. During the synthesis process, when the
molar ratio of citric acid to the Ba2+, Sr2+ metal cations was less
than 1.5, white precipitates were observed in the sol due to
relatively low solubility of barium nitrate and strontium nitrate
without insufficient complexation with citric acid. Further-
more, the pH value of the precursor solution is also important
to obtain a clear gel without precipitation. Considering
the stability constants for BaH2Cit+ ðlog10KðBaH2CitþÞ=ðmol�1 dm3Þ = 0.6) and BaCit� ðlog10KðBaCit�Þ=ðmol�1 dm3Þ= 2.95) [14], it was appropriate that the optimum pH value
range was 6.0–7.0.
Fig. 2 shows the TGA and DSC curves of the Ba1�xSrxTiO3
(x = 0.3) precursor. The TG curve shows a drastic weight loss at
162–219 8C, followed by two small weight loss at 219–305 8Cand 305–462 8C; there is a big weight loss in the temperature
range 462–491 8C and no further weight loss beyond 619 8C.
The endothermic peak at 187.4 8C is due to the evaporation of
volatile components, corresponding to a weight loss of 27.6%.
Two successive faint exothermic peaks at 252.9 and 292.2 8Care caused by the burnout of organic species, corresponding to a
total weight loss of 16.2%. Most of organic components are
removed below 488 8C. Exothermic peaks at 479.1 8C,
accompanied by a weight loss of 15.7%, might be due to the
thermal decomposition of citrate complex [16].
terization of Ba1�xSrxTiO3 nanopowders by citric acid gel method,

Fig. 2. Combined TG-DSC curves of uncalcined BST precursor with x = 0.3.
Fig. 4. FT-IR spectra of the gel (a) and the powders calcined at (b) 600 8C; (c)
800 8C and (d) 950 8C.
Z. Wang et al. / Ceramics International xxx (2006) xxx–xxx 3
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CERI-2415; No of Pages 5
Fig. 3 shows the FT-IR spectra of the Ba1�xSrxTiO3 (x = 0.3)
precursor. For the precursor with CA/M = 1.0 and pH 6.0, two
bands, possibly the asymmetric and symmetric stretching
vibrations of carboxylate [18], are observed at 1581 and
1398 cm�1. For the precursor with CA/M = 2.0 and pH 6.0,
there are two strong absorption peaks at 1574 and 1400 cm�1,
corresponding to the asymmetric stretching mode and the
symmetric stretching mode of COO� for a bridging complex,
respectively [19]. The band at 1078 cm�1 is observed, which is
attributed to the organic network or the COH groups [20]. The
broad absorption band around 3400 cm�1 is due to the O–H
stretching modes for the intermolecular hydrogen bond or
molecular water. The FT-IR spectrum of Ba1�xSrxTiO3
(x = 0.3) precursor with CA/M = 1.5 and pH 6.0 is similar to
that of the precursor with CA/M = 2.0 and pH 6.0. The
characteristic intensity increased for the metal carboxylate
complexes (Fig. 3c) can be ascribed to the enhanced interaction
between metal cations and carboxylate ligands. Fig. 4 is the FT-
IR spectra of Ba1�xSrxTiO3 (x = 0.3) gel powders heat-treated
at various temperatures, showing the evolution of the materials
Fig. 3. FT-IR spectra of (a) CA/M = 1; (b) CA/M = 1.5; (c) CA/M = 2.0 in the
condition of pH 6.0.
Please cite this article in press as: Z. Wang et al., Synthesis and charac
Ceram. Int. (2006), doi:10.1016/j.ceramint.2006.03.015
with the increase in calcinations temperature. For the spectrum
of gel powders, the strong and sharp absorption bands at 1399
and 1572 cm�1 may be ascribed to the nsym(COO�) and
nasym(COO�) of acetyl groups, respectively. Broadened
absorption band at 3440 cm�1 associates with O–H stretch
of intermolecular hydrogen bonds or molecular water. The
HOH bending mode characteristic of water appears at
1630 cm�1. After firing more than 800 8C, the band intensity
of the carbonate group at 1443 cm�1 was reduced significantly,
but a large broad band appeared at 555 cm�1. Music et al. [21]
have assigned that this band is caused by the metal-oxygen
stretching vibration of Ti–O bond. It revealed that the formation
of a large amount of BST.
The phase formation starting from the BST precursor was
studied by means of XRD. Fig. 5 shows the XRD patterns of
the Ba1�xSrxTiO3 precursor with x = 0.3 and powders
calcined at various temperatures. Fig. 5a shows the precursor
to be amorphous. Some small diffraction peaks appeared for
the powders calcined at 500 8C, indicating that incipient
crystallization starts from around 500 8C. The perovskite-like
phase crystallization occurred at 600 8C. However, there was
still an impurity phase of barium carbonate (JCPDS 01-0506)
with the diffraction peaks at 24.08 and 34.28 (2u 8). The
intensity of the diffraction peaks of BaCO3 decreased with the
increase in calcination temperature, which agreed with FT-IR
results (Fig. 4). At 950 8C, the carbonate impurity phase
disappeared and the tetragonal perovskite monophase of
Ba1�xSrxTiO3 (x = 0.3) was obtained (JCPDS 89-0274).
Obviously, this temperature was much lower than for the
solid-state reaction method [22]. The crystallite size of the
particles calcined at various temperatures could be calculated
by the Scherrer’s equation: D = kl/b cos u, where D is the
crystallite size, k is a constant (0.9, spheres), l is the
wavelength of the X-ray radiation, b is the line width obtained
after correction for the instrumental broadening and u is the
angle of diffraction. The crystallite size obtained from XRD
data (950 8C) is 86 nm.
terization of Ba1�xSrxTiO3 nanopowders by citric acid gel method,

Fig. 6. SEM micrograph of BST powders calcined at 950 8C for 2 h.
Fig. 5. Powder X-ray diffraction patterns of Ba1�xSrxTiO3 (x = 0.3) precursor
(a) and powders calcined at (b) 500 8C; (c) 600 8C; (d) 800 8C; (e) 900 8C and
(f) 950 8C.
Z. Wang et al. / Ceramics International xxx (2006) xxx–xxx4
+ Models
CERI-2415; No of Pages 5
From the SEM image (Fig. 6) of the Ba1�xSrxTiO3 (x = 0.3)
sample calcined at 950 8C, the particle size was estimated to be
around 80 nm, a value consistent with the one calculated by the
XRD data.
4. Conclusions
A novel synthesis process was designed and stoichiometric
and monophasic Ba1�xSrxTiO3 (x = 0.3) nanopowders were
Please cite this article in press as: Z. Wang et al., Synthesis and charac
Ceram. Int. (2006), doi:10.1016/j.ceramint.2006.03.015
successfully prepared by the citric acid gel method. The process
is an easy way for obtaining an aqueous water-soluble
precursor. Single-phase and well-crystallized Ba1�xSrxTiO3
(x = 0.3) nanopowders could be synthesized at 950 8C with
particle size of around 80 nm.
Acknowledgements
This work was supported by the National 973 Project of
China (2004CB619300) and the HUST Postgraduate Innova-
tion Foundation (2005).
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