4

Click here to load reader

Synthesis and Characterization of Electrospun Mullite Nanofibers

Embed Size (px)

Citation preview

Page 1: Synthesis and Characterization of Electrospun Mullite Nanofibers

CO

DOI: 10.1002/adem.200900222

MM

UNI

Synthesis and Characterization of Electrospun MulliteNanofibers**

CATIO

By Jiang Wu, Hong Lin,* Jianbao Li, Xiaobo Zhan and Junfeng Li

N

In this study, continuous mullite (3Al2O3�2SiO2) nanofibers were fabricated by sol–gel and electro-spinning techniques and calcined at high temperatures to obtain pure ceramic mullite nanofibers.Detail structural characterizations suggested that the productive rate of electrospun mullite nanofiberswere very high and the sintered nanofibers were made of single crystalline grains with size of�100 nm.

[*] Prof. H. Lin, Dr. J. Wu, Prof. J. B. Li, Dr. X. B. Zhan, Dr. J. F. LiState Key Laboratory of New Ceramics and Fine ProcessingDepartment of Materials Science and Engineering TsinghuaUniversity Beijing, 100084, ChinaE-mail: [email protected]

[**] The authors would like to express their gratitude to thesupport provided by the Ministry of Science and Technologyof China (973 Program, 2007CB607504; 863 Program,2007AA03Z524), the National Natural Science Foundationof China (NSFC, 50672041).

ADVANCED ENGINEERING MATERIALS 2010, 12, No. 1--2 � 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 71

Mullite (3Al2O3�2SiO2) is well-known as superior engineer-

ing ceramic materials owing to its relatively high chemical

stability, good refractory properties, high temperature

mechanical strength, and low thermal expansion coeffi-

cient.[1,2] Fabrication of continuous mullite nanofibers is

highly desired because it is an important candidate used as

reinforcement of metals, ceramics, and resins.[3,4] Several

traditional methods such as sol–gel, melt spinning, and

solution spinningmethods have been used to fabricate mullite

fibers.[5–7] Electrospinning is a promising technique that

utilizes electric forces along to drive the spinning process and

to produce fibers. Unlike sol–gel fabricated nanofibers, most

of which contain foreign cations as catalysts and require

further expensive purification, electrospun nanofibers are

more pure, inexpensive, continuous, and relatively easy to

align, assemble, and process into applications.[8–11] Unlike

conventional spinning techniques (e.g., melt spinning and

solution spinning methods) that are capable of producing

fibers with diameters in the micrometer range (�5–15mm),

electrospinning is capable of producing fibers with diameters

in the nanometer range (�50–1000 nm) with less cracks. In the

recent decade, numerous electrospun ceramic nanofibers

including silica, titania, and zirconia, have been fabricated and

studied throughout the world.[12–14] However, very little

literatures have been reported about electrospinning

approach fabricating mullite nanofibers due to its more

complicated stoichiometry/microstructure and relatively

higher synthesis temperature. Recnetly, Dharmaraj et al. have

reported the fabrication of electrospun mullite nanofibers,

which focused on the sintering process, studying the effect of

calcination temperature on the morphology evolution of

mullite nanofibers.[15] However, much less attention has been

paid to the electrospinning process.

In the present work, electrospinning method is introduced

to fabricate mullite nanofibers. Three different solvent

systems including de-ionized water (DI) (solution A), DI/

absolute alcohol (EtOH) (solution B), and DI/N, N-dimethyl-

formamide (DMF) (solution C) were used to prepare precur-

sor spinning solutions. The effect of different solvents on the

micromorphological evolution, crystallization sequence, and

structural properties of both the as-electrospun fibers and the

final sintered mullite nanofibers will be primarily focused and

systematically investigated.

Results and Discussion

The representative morphologies of as-electrospun nano-

fibers prepared from different solutions are presented in

Figure 1(a–f). Although no obvious beads and/or beaded

fibers were identified at low resolution, as shown in

Figure 1(a–c), for the fibers made from solution A, some

small beaded fibers with diameter ranging from 800nm to

2mm were observed with in the scope of this investigation at

high resolution, as shown in Figure 1(d). On the contrary, the

fibers made from solutions B and C had common cylindrical

morphologies with diameters ranging from 300 to 600 nm, as

shown in Figure 1(e) and (f).

The ‘‘bending instability’’ is a widely acceptable explana-

tion for electrospinning process.[8,9,16] During electrospinning,

when the electrostatic field reaches a critical value and the

electric force overcomes the surface tension and viscoelastic

force, a jet ejects and starts to bend, forming long fibers. The

properties of the solutions, such as dielectric constant,

viscosity, and volatility, have great influence on the micro-

morphology of as-electrospun fibers.[16] In the present work,

Page 2: Synthesis and Characterization of Electrospun Mullite Nanofibers

COM

MUNIC

ATIO

N

Wu et al./Synthesis and Characterization of Electrospun . . .

Fig. 1. Representative morphologies of as-electrospun nanofibers from (a, d) solution A; (b, e) solution B; and (c, f) solution C.

all the solution systems are conductive due to the addition of

aluminum salt, the micromorphology of as-electrospun fibers

are mainly dependent on the viscosity and the solvent

evaporation. For solution A, the concentration of polyvi-

nylprrolidone (PVP) is as low as 4.4wt%, surface tension is

still the dominant factor and small beaded fibers are formed

during the electrospinning process.[8,9,12] Due to the less

volatilization of de-ionized water, the diameters of obtained

as-electrospun fibers are in the range of 1–2mm, which are

much larger than those of the other two fibers. On the

contrary, for solutions B and C, the concentration of PVP are 6

and 8wt%, respectively. The viscosity of solutions are high

enough to form continuous fibrous structure. The

as-electrospun fibers are thinner and have regular circular

cross-section, which are created by quick evaporation of the

Fig. 2. TG/DSC curves of all three as-electrospun fibers obtained from (a) solution A,(b) solution B, and (c) solution C.

72 http://www.aem-journal.com � 2010 WILEY-VCH Verlag GmbH & Co.

solvents through the drying surface of the jet.[9,16] Although

the small beaded fibers derived from solution A can be

avoided if the PVP consent exceeds 4.4wt%, the diameters of

the final sintered fibers are observed in the range of

micrometers, which will not be discussed in this paper.

Figure 2 shows the thermogravimetry differential scanning

calorimetry (TG/DSC) analysis of all as-electrospun nano-

fibers prepared from three different solutions. TG curves

suggested that themass losses of all three as-electrospun fibers

were finished before 800 8C, indicating the complete volati-

lization and decomposition of solvents and PVP. The

small endothermic peaks occurred at 120 8C were considered

as the dehydration of absorbed water. The broad exothermic

peaks from 300 to 600 8Cwere attributed to the decomposition

and volatilization of PVP. It is noticed that there were

two distinct exothermic peaks at 973 and 1113 8C for the

as-electrospun fibers prepared from solution A, which were

attributed to the formation of g-Al2O3 and mullite. While

only one obvious exothermic peak was observed for the

as-electrospun fibersmade from the other two solutions, at 985

and 983 8C, respectively, indicating the direct formation of

mullite.

It has been reported by Schneider et al. that the crystal-

lization sequence of mullite gel is related to the degree of

mixing of the constituents.[17] If the mixing scale is at atomic

level, the gel is single phase and mullitization can be achieved

directly at 980 8C. If themixing scale is higher than that, the gel

is diphsic and transforms into Al2O3 before the crystallization

of mullite. Typically, ‘‘bending instability’’ causes the length

of an electrospinning jet to elongate up to 50 000 times in a very

short time period.[12] For solutions B and C, such a huge draw

rate and the associated extremely intensive stretching and/or

KGaA, Weinheim ADVANCED ENGINEERING MATERIALS 2010, 12, No. 1--2

Page 3: Synthesis and Characterization of Electrospun Mullite Nanofibers

COM

MUNIC

ATIO

N

Wu et al./Synthesis and Characterization of Electrospun . . .

Fig. 3. Representative morphologies of all sintered mullite nanofibers obtained from (a) solution A, (b) solution B, and (c) solution C.

Fig. 4. Representative TEM and high-resolution images of all the sintered mullite nanofibers obtained from (a) solution A, (b) solution B, and (c) solution C.

Fig. 5. XRD patterns of sintered nanofibers obtained from (a) solution A, (b) solution B,and (c) solution C.

shearing could result in the meta-stable and almost

atom-uniform mixing of resource components, leading to

the direct formation of mullite.[12] While for solution A, the

high water content induced the fast hydrolyzation and

condensation reactions of aluminum isopropoxide (AIP)

and tetraethylor orthosilicate (TEOS), resulting in less

homogeneity of the as-electrospun fibers and later the

formation of Al2O3 as the secondary phase.

In order to obtain pure mullite nanofibers, all the

as-electrospun fibers were sintered at 1200 8C for 2 h according

to DSC results. The representative morphologies of sintered

nanofibers are shown in Figure 3(a–c). All the sintered

nanofibers were thinner than the as-electrospun ones. The

diameters were 800–1000 nm for the ones made from solution

A, and the sizes/widths were 100–200 nm for the ones made

from solutions B and C. The contraction in fiber diameter/size

was due to the removal and decomposition of PVP.

Additionally, the degree of surface roughness for the sintered

nanofibers was significantly higher than that for the

as-electrospun nanofibers, which was due to the nucleation

and growth of mullite grains during sintering process.

Figure 4(a–c) show the representative transmission elec-

tron microscopy (TEM) and high-resolution images of all the

sinteredmullite nanofibers. The particular nanofiber as shown

in Figure 4(a) had diameters of�500 nm, which was relatively

thin among the nanofibers made from solution A. Even

though, it was still very hard to observe the detailed surface

condition of the fiber clearly due to its large thickness. While

the high-resolution observation was very easy for the

ADVANCED ENGINEERING MATERIALS 2010, 12, No. 1--2 � 2010 WILEY-VCH Ve

particular nanofibers obtained from solutions B and C due

to their ralative thin size. Results indicated that both of the

sintered nanofibers consisted of single crystalline grains with

size of �100 nm.

Figure 5 shows the X-ray diffractometer (XRD) patterns of

all the sintered mullite nanofibers. It is clear that mullite is the

primary phase with Al2O3 as secondary phase. For nanofibers

derived from solution A, the amount of Al2O3 phase was

much higher, which was attributed to the less homogeneity of

its precursor and the different crystallization sequence. While

rlag GmbH & Co. KGaA, Weinheim http://www.aem-journal.com 73

Page 4: Synthesis and Characterization of Electrospun Mullite Nanofibers

COM

MUNIC

ATIO

N

Wu et al./Synthesis and Characterization of Electrospun . . .

for the other two sintered nanofibers, the track amount of

Al2O3 is likely introduced from theAl2O3 crucible used during

the sintering process. It is noted worthy that the XRD result is

obtained from large amount of nanofibers mat, confirming a

high productive rate of electrospun mullite nanofibers.

Conclusions

In summary, nano-scale mullite nanofibers could be easily

synthesized by electrospinning method followed by sintering

process at 1200 8C for 2 h. Results indicated that the properties

of solvents had great influence on the microphology

development and crystallization sequence of as-electrospun

fibers. Due to the less PVP content and low volatilization of

de-ionized water, the diameters of the sintered nanofibers

derived from solution A are in the range of 800–1000 nm. Plus

with the less homogeneity of constituents, large amount of

Al2O3 was formed as secondary phase. While for the sintered

nanofibers made from solutions B and C, the diameters were

in the range of 100–200 nm. XRD and TEM results indicated

that the productive rate of electrospun mullite nanofibers

were very high and the sintered nanofibers were made of

single crystalline grains with size of �100 nm. Due to their

dramatic good performance of mechanical property and

stability, plus with the nano-scale diameters and relatively

high surface area to volume ratio, electrospun mullite

nanofibers are highly expected to be used as structural

materials, such as filtrating membrane and aircraft space

accessories, especially in high temperature oxygen environ-

ment.

Experimental

Commercially available AIP (C9H21O3Al), hydrous alumi-

num nitrate [AN, Al(NO3)3�9H2O) and PVP (Mw¼ 1 000 000)

were used as the raw materials. Three different spinning

solutions (DI, DI/EtOH, and DI/DMF), were prepared. The

source solutions were mixed and stirred at 80 8C for 0.5 h,

resulting viscous semilucent solutions for electrospinning.

The following three spinning solutions were suggested as the

optimal and representative systems:

Solution A: AIP/AN/TEOS/DI¼ 2:1:1:50 with 4.4wt% PVP

Solution B: AIP/AN/TEOS/DI/EtOH¼ 2:1:1:25:25 with

6wt% PVP

Solution C: AIP/AN/TEOS/DI/DMF¼ 2:1:1:25:25 with

8wt% PVP

The viscous solution was contained in a glass capillary and

ejected with a voltage of 18 kV. A dense web of fibers was

collected on the aluminum foil which was served as the

counter electrode. The obtained web of fibers was calcined at

74 http://www.aem-journal.com � 2010 WILEY-VCH Verlag GmbH & Co.

1200 8C for 2 h with a heating rate of 10 8Cmin�1. The thermal

analysis of the as-electrospun precursor nanofibers was

carried out up to 1200 8C in N2 by TG/DSC (NETZSCH

STA 409PC/PG, Germany). The phase transformation and

microstructure of mullite nanofibers were studied by XRD

(D/max-III, Rigaku, Japan), scanning electron microscopy

(SEM, LEO 1530, Germany) and high resolution TEM (JEOL

JEM-2010F, Japan).

Received: July 28, 2009

Final Version: August 19, 2009

Published online: November 27, 2009

[1] K. N. Lee, Coat. Technol. 2000, 133, 1.

[2] P. A. Lessing, R. S. Gordon, K. S. Mazdiyasni, J. Am.

Ceram. Soc. 1975, 58, 145.

[3] H. Y. Lu, W. L. Wang, W. H. Tuan, M. H. Lin, J. Am.

Ceram. Soc. 2004, 87, 1843.

[4] L. B. Kong, H. Huang, T. S. Ma, F. Boey, R. F. Zhang,

Z. H. Wang, J. Eur. Ceram. Soc. 2003, 23, 2547.

[5] J. Greener, J. R. G. Evans, J. Eur. Ceram. Soc. 1997, 17,

1173.

[6] G. D. Kim, D. A. Lee, H. I. Lee, S. J. Yoon,Mater. Sci. Eng,

A-Struct. 1993, 167, 171.

[7] Y. B. Zhang, Y. P. Ding, J. Q. Gao, J. F. Yang, J. Eur. Ceram.

Soc. 2009, 29, 1101.

[8] Y. Dzenis, Science 2004, 304, 1917.

[9] Y. M. Shin, M. M. Hohman, M. P. Brenner, Appl. Phys.

Lett. 2001, 78, 1149.

[10] T. Han, A. L. Yarin, D. H. Reneker, Ploymer 2008, 49,

2160.

[11] D. Fallahi, M. Rafizadeh, N. Mohammadi, B. Vahidi,

Polym. Int. 2008, 57, 1363.

[12] R. Chandrasekar, L. F. Zhang, J. Y. Howe, N. E. Hedin,

Y. Zhang, H. Fong, J. Mater. Sci. 2009, 44, 1198.

[13] X. H. Yang, C. L. Shao, Y. H. Liu, J. Mater. Sci. 2007, 42,

8470.

[14] S. W. Lee, Y. U. Kim, S. S. Choi, T. Y. Park, Y. L. Joo, S. G.

Lee, Mater. Lett. 2007, 61, 889.

[15] N. Dharmaraj, C. Kim, P. Prabu, B. Ding, H. Kim,

P. Viswanathamurthi, Int. J. Electrospun Nanofibers and

Applications 2007, 1, 63.

[16] Y. You, S. J. Lee, B. M. Min, W. H. Park, J. Appl. Polym.

Sci. 2006, 99, 1214.

[17] H. Schneider, B. Saruhan, D. Voll, I. Merwin, A. Sebald,

J. Eur. Cream. Soc. 1993, 11, 87.

KGaA, Weinheim ADVANCED ENGINEERING MATERIALS 2010, 12, No. 1--2