three-dimensional printing of complex-shaped alumina/glass composites

5
DOI: 10.1002/adem.200900213 Three-Dimensional Printing of Complex-Shaped Alumina/ Glass Composites** By Wei Zhang * , Reinhold Melcher, Nahum Travitzky, Rajendra Kumar Bordia and Peter Greil Alumina ceramics are well studied and universally used low cost materials possessing such attractive properties as excellent wear and oxidation resistance, good high tempera- ture strength, etc. [1] In particular, alumina/glass composites are attractive materials for a wide range of engineering applications or biomedical uses such as dental restorations due to their high strength, low thermal conductivity, abrasion resistance, biocompatibility, and esthetics. [2–6] Usually, alu- mina/glass composites are fabricated using an approach where alumina preforms are prepared by traditional pro- cesses such as cold pressing or slip casting, followed by continuous partial sintering at 1100–1400 8C and subsequent glass melt infiltration into the porous structure at 950–1100 8C. [2,4,7,8] Nevertheless, there still remains the challenge of forming complex-shaped alumina/glass compo- sites as the above-mentioned process is limited in respect to the required geometric variety of parts. [2,9] Solid-free form (SFF) or rapid prototyping (RP) techniques, offer completely new paths in order to realize complex-shaped ceramic bodies. Three-dimensional printing (3DP TM ) is an RP process in which powdered material is deposited in layers. [10] A binder solution is locally applied on a powder layer by an ink-jet print head, causing the powder particles to bind to one another and to the printed cross-section one level below. This process is repeated until the entire part is printed. A full dense and complex-shaped composites were fabricated by 3DP process and subsequent pressureless melt infiltration. [11–16] The processing parameters of 3D-printing strongly influ- ence the microstructure and mechanical properties of the COMMUNICATION [*] W. Zhang, Dr. N. Travitzky, Prof. P. Greil Department of Materials Science, Glass and Ceramics Friedrich-Alexander-University Erlangen-Nuremberg Martensstr. 5, 91058 Erlangen, Germany E-mail: [email protected] R. Melcher Robert Bosch GmbH Bamberg Plant, Diesel Systems Postfach 1160, 96045 Bamberg, Germany Prof. R. K. Bordia Department of Materials Science and Engineering, University of Washington Roberts Hall, Box 352120, Seattle, WA 98195, USA Dr. N. Travitzky, Prof. P. Greil Centre for advanced Materials and Processes Friedrich- Alexander-University Erlangen-Nuremberg Dr. -Mack-Strasse 81, 90762 Fuerth, Germany [**] The authors thank the Deutsche Forschungsgemeinschaft (DFG) for financial support and Dr. M. Stephan of Vita Zahnfabrik, Bad Saeckingen, Germany for supply of glass powder and kind advice. R. K. Bordia thanks to the Alexander von Humboldt Foundation for financial support. Alumina/glass composites were fabricated by three-dimensional printing (3DP TM ) and pressureless infiltration of lanthanum-alumino-silicate glass into sintered porous alumina preforms. The preforms were printed using an alumina/dextrin powder blend as a precursor material. They were sintered at 1600 8C for 2 h prior to glass infiltration at 1100 8C for 2 h. The influence of layer thickness and sample orientation within the building chamber of the 3D-printer on microstructure, porosity, and mechanical properties of the preforms and final composites was investigated. The increase of the layer thickness from 90 to 150 mm resulted in an increase of the total porosity from 19 to 39 vol% and thus, in a decrease of the mechanical properties of the sintered preforms. Bending strength and elastic modulus of sintered preforms were found to attain significantly higher values for samples orientated along the Y-axis of the 3D-printer compared to those orientated along the X- or the Z-axis, respectively. Fabricated Al 2 O 3 /glass composites exhibit improved fracture toughness, bending strength, Young’s modulus, and Vickers hardness up to 3.6 MPa m 1/2 , 175 MPa, 228 GPa, and 12 GPa, respectively. Prototypes were fabricated on the basis of computer tomography data and computer aided design data to show geometric capability of the process. ADVANCED ENGINEERING MATERIALS 2009, 11, No. 12 ß 2009 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 1039

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Page 1: Three-Dimensional Printing of Complex-Shaped Alumina/Glass Composites

CO

DOI: 10.1002/adem.200900213

MM

UNI

Three-Dimensional Printing of Complex-Shaped Alumina/Glass Composites**

CATIO

By Wei Zhang*, Reinhold Melcher, Nahum Travitzky, Rajendra Kumar Bordia and Peter Greil

N

Alumina/glass composites were fabricated by three-dimensional printing (3DPTM) and pressurelessinfiltration of lanthanum-alumino-silicate glass into sintered porous alumina preforms. The preformswere printed using an alumina/dextrin powder blend as a precursor material. They were sintered at1600 8C for 2 h prior to glass infiltration at 1100 8C for 2 h. The influence of layer thickness and sampleorientation within the building chamber of the 3D-printer on microstructure, porosity, and mechanicalproperties of the preforms and final composites was investigated. The increase of the layer thicknessfrom 90 to 150mm resulted in an increase of the total porosity from �19 to �39 vol% and thus, in adecrease of the mechanical properties of the sintered preforms. Bending strength and elastic modulus ofsintered preforms were found to attain significantly higher values for samples orientated along theY-axis of the 3D-printer compared to those orientated along the X- or the Z-axis, respectively.Fabricated Al2O3/glass composites exhibit improved fracture toughness, bending strength, Young’smodulus, and Vickers hardness up to 3.6MPa m1/2, 175MPa, 228GPa, and 12GPa, respectively.Prototypes were fabricated on the basis of computer tomography data and computer aided design data toshow geometric capability of the process.

[*] W. Zhang, Dr. N. Travitzky, Prof. P. GreilDepartment of Materials Science, Glass and CeramicsFriedrich-Alexander-University Erlangen-NurembergMartensstr. 5, 91058 Erlangen, GermanyE-mail: [email protected]

R. MelcherRobert Bosch GmbH Bamberg Plant, Diesel SystemsPostfach 1160, 96045 Bamberg, Germany

Prof. R. K. BordiaDepartment of Materials Science and Engineering, Universityof WashingtonRoberts Hall, Box 352120, Seattle, WA 98195, USA

Dr. N. Travitzky, Prof. P. GreilCentre for advanced Materials and Processes Friedrich-Alexander-University Erlangen-NurembergDr. -Mack-Strasse 81, 90762 Fuerth, Germany

[**] The authors thank the Deutsche Forschungsgemeinschaft(DFG) for financial support and Dr. M. Stephan of VitaZahnfabrik, Bad Saeckingen, Germany for supply of glasspowder and kind advice. R. K. Bordia thanks to the Alexandervon Humboldt Foundation for financial support.

ADVANCED ENGINEERING MATERIALS 2009, 11, No. 12 � 2009 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 1039

Alumina ceramics are well studied and universally used

low cost materials possessing such attractive properties as

excellent wear and oxidation resistance, good high tempera-

ture strength, etc.[1] In particular, alumina/glass composites

are attractive materials for a wide range of engineering

applications or biomedical uses such as dental restorations

due to their high strength, low thermal conductivity, abrasion

resistance, biocompatibility, and esthetics.[2–6] Usually, alu-

mina/glass composites are fabricated using an approach

where alumina preforms are prepared by traditional pro-

cesses such as cold pressing or slip casting, followed by

continuous partial sintering at 1100–1400 8C and subsequent

glass melt infiltration into the porous structure at

950–1100 8C.[2,4,7,8] Nevertheless, there still remains the

challenge of forming complex-shaped alumina/glass compo-

sites as the above-mentioned process is limited in respect to

the required geometric variety of parts.[2,9] Solid-free

form (SFF) or rapid prototyping (RP) techniques, offer

completely new paths in order to realize complex-shaped

ceramic bodies.

Three-dimensional printing (3DPTM) is an RP process in

which powdered material is deposited in layers.[10] A binder

solution is locally applied on a powder layer by an ink-jet print

head, causing the powder particles to bind to one another and

to the printed cross-section one level below. This process is

repeated until the entire part is printed. A full dense and

complex-shaped composites were fabricated by 3DP process

and subsequent pressureless melt infiltration.[11–16]

The processing parameters of 3D-printing strongly influ-

ence the microstructure and mechanical properties of the

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W. Zhang et al./Three-Dimensional Printing of Complex-Shaped Alumina/Glass Composites

Fig. 1. (a) Process diagram for fabrication of alumina/glass composites and (b) sche-matic of building chamber: machine directions and sample orientations.

printed bodies. For instance, a binder saturation determined

the geometry of an elementary building units, resulting from a

single ink drop in the powder bed and their interaction with

the powder bed, through which the surface finish and

microstructure of the preform may be controlled.[11] In addition,

the preforms printed with slower printing speed showed better

surface structure compared to those with faster speeds even

though the binder saturation levels were similar.[13,17] Influence

of the layer thickness and printing direction on microstructures

and mechanical properties of printed bodies, however, has not

been reported up to date in detail.

The purpose of the present work was to study the effect of

layer thickness and printing direction on the microstructure

and mechanical properties of alumina/glass composites

fabricated by 3D-prnting of porous Al2O3 preforms followed

by their sintering and pressureless melt infiltration with

lanthanum-aluminosilicate glass.

Experimental

Powder Processing

Granulate powder for the fabrication of porous ceramic

preforms was prepared as follows: 120 g dextrin powder

(Superior Gelb/mittel-F, Suedstaerke, Schrobenhausen, Ger-

many) as binder and 19 g of dispersant (Dolapix A88,

Zschimmer & Schwarz, Lahnstein/Rhein, Germany) were

dissolved in 1.35 L distilled water. Subsequently, 1786 g

a-Al2O3 powder (CT 3000 SG, Almatis, Ludwigshafen,

Germany) and 94 g g-Al2O3 powder (PG feinst, Almatis) with

average particle sizes of 0.8 and 3.4mm, respectively, were

suspended. The mixture was homogenized by tumbling it in a

2 L polyethylene bottle with alumina grinding balls for 48 h.

The slurry was freeze dried at 50 8C/37 Pa (Delta 2–24, Christ,

Osterode/Harz, Germany). The dry batch was ball-milled in a

jar for 72 h and sieved through 150mm mesh.

3D-Printing

3D-printing was carried out on a Z310 printer

(Z-Corporation, Burlington/MA, USA) using a water-based

printing solution (ZB56, Z-Corpation). Two types of samples

were fabricated. Bar-shaped samples with nominal dimen-

sions of 6� 7� 60 mm3 were printed for the purpose of

mechanical testing of sintered preforms prior to infiltration.

For infiltration with the glass, plate-shaped samples with a

nominal dimension of 5� 72� 80 mm3 were printed. The

printed bodies were oriented in X-, Y-, and Z-orientations, the

layer thickness was adjusted to 90, 100, 120, and 150mm,

respectively, for each orientation. The orientations within the

build piston are defined as follows: X-orientation is the

direction of print head travel, Y-orientation is the direction of

gantry travel, Z-orientation is the direction of piston move-

ment (Fig. 1(b)). The printed samples were dried in the

powder bed at room temperature for at least 24 h.

Sintering and Melt Infiltration

The dried bar and plate-shaped samples were then sintered

in a resistance-heated furnace (HT 08/17, Nabertherm,

1040 http://www.aem-journal.com � 2009 WILEY-VCH Verlag GmbH & C

Lilienthal, Germany) in air according to the following

temperature setup based on dilatometric results: 25–600 8Cat 600 8C h�1, 600–1100 8C at 1200 8C h�1, 1100–1600 8C at

300 8C h�1, holding time 2 h, 1600–25 8C at 600 8C h�1.

For infiltration, the 50 g lanthanum-aluminosilicate glass

powder (InCeram Alumina, VITA Zahnfabrik, Bad Saeckin-

gen, Germany) was mixed with 80 mL distilled water, 20 mL

glycerin, and 2.4 g dextrin to form a thin slurry which was

applied to one side of the porous alumina preform. The

amount of glass required was estimated on the basis of open

porosity determined by Hg-porosimetry. The plates with

coated face upward were dried and then heated to 1100 8C in

air at 1000 8C h�1 resistance-heated furnace, holding time 2 h.

The cooling was accomplished as follows: 1100–650 8C at

450 8C h�1, 650–400 8C at 170 8C h�1, 400–25 8C at 300 8C h�1. A

process overview is given in Figure 1(a).

Characterization

Particle size distribution of the granulate powder was

measured in an air stream by laser granulometry (Mastersizer

2000, Malvern Instruments, Malvern, Great Britain). The

porosity and pore size distribution of sintered alumina

preforms was measured by Hg-porosimetry (Pascal 140,

Thermo Electron, Rodano/Milan, Italy). Scanning electron

microscopy (SEM, Quanta 200, FEI, Prague, Czech Republic)

was applied for microstructural and fractographical analysis.

The samples for SEM analysis were ground and polished to a

6mm diamond finish and sputtered with gold. The phase

analysis of the infiltrated alumina samples was conducted by

X-ray powder diffraction (XRD) using monochromatic Cu Ka

radiation at a scanning rate of 0.75 min�1 over a 2u range of

10–708 (D500, Siemens, Karlsruhe, Germany).

Bending strength and fracture toughness of sintered and

infiltrated samples with dimensions of 3� 4� 50 mm3 were

measured by four-point bending method using a universal

testing machine (Instron 4204, Instron Corporation, Canton/

MA, USA) with a crosshead speed of 0.5 mm min�1. The

average values of flexural strength were determined from

measurements conducted on at least 10 testing bars. The bars

were loaded with spans of 20 and 40 mm at room temperature.

The tensile surfaces of the samples were polished to a 6mm

o. KGaA, Weinheim ADVANCED ENGINEERING MATERIALS 2009, 11, No. 12

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Fig. 3. Linear shrinkage in three dimensions of preforms after sintering in dependenceon layer thickness.

diamond finish prior to bending. Fracture toughness of

infiltrated samples was evaluated using the single-

edge-v-notched-beam (SEVNB) method. A saw cut was

tapered using a razor blade with 3mm diamond paste. The

overall depth of the notch, which was determined by light

microscopy (Leica M 420, Leica, Heerbrugg, Switzerland), was

�0.4mm. Young’s modulus of preforms and infiltrated samples

were calculated from the longitudinal sound propagation

velocity measurements using the impulse excitation technique

(Buzz-o-sonic, BuzzMac Software, Glendale, USA) [18]. The

Vickers hardness was conducted on the polished surfaces of

infiltrated specimens at a load of 49N with a duration of 15 s

using a diamond indenter (Zwick 3231, Zwick, Ulm, Germany).

The average hardness value was determined from 10 indentation

measurements.

Results and Discussion

Particle size distribution of (aþ g)-alumina/dextrin pow-

der is presented in Figure 2(a). This powder exhibits a

multimodal particle size distribution with particle size

ranging from 0.1 to 300mm. Representative pore size

distributions are shown for green and corresponding sintered

samples printed with layer thickness of 100mm in Figure 2(b).

The pore size distribution of printed green samples exhibits a

bimodal distribution, showing maxima at 0.3 and 45mm

diameter. The fine pores were eliminated or closed during

Fig. 2. (a) Particle size distribution of (aþ g)-alumina/dextrin powder blend and (b)pore size distribution in green and sintered preform (layer thickness 100mm).

ADVANCED ENGINEERING MATERIALS 2009, 11, No. 12 � 2009 WILEY-VCH Verl

sintering. Therefore, only pores in the range of 40mm were

obtained in the preform after sintering.

Figure 3 shows linear shrinkages in three dimensions of

preforms after sintering in dependence on layer thickness.

No orientational or layer thickness dependences could be

observed considering the standard deviation. The linear

shrinkage of 18.7� 0.3% was measured for all orientations

and layer thicknesses.

An increase of volume fraction of porosity in the sintered

Al2O3 preform was obtained with the increase of the layer

thickness. A minimum porosity of 19� 0.5 vol% was mea-

sured at a layer thickness of 90mm and a maximum of

39� 2.1 vol% at a layer thickness of 150mm (Fig. 4).

Consequently, porosity, and thus layer thickness, has an

effect on the mechanical properties of the sintered preforms.

For example, bending strength increases from 29� 11 to

98� 6 MPa and Young’s modulus increases from 55� 24

to 178� 23 GPa as the layer thickness decreases from 150 to

90mm (Fig. 4). Increasing of the mechanical properties may

be explained by decreasing of porosity in layers with low

thicknesses (Fig. 4).

In addition, bending strength as well as Young’s modulus

of sintered samples is affected by their orientation within the

building chamber. In general, samples orientated in the Y-axis

exhibit significantly higher mechanical properties than

samples printed in the X- or Z-orientation (Fig. 4). This effect

is all the more pronounced for increasing layer thickness.

Average values measured for Z-orientation tend to exhibit

significantly higher deviations than those of X- and

Y-orientations, respectively. This behavior might be explained

by the formation of continuous strips along the Y-axis during

printing. In comparison, layers along the X-axis are composed

of those strips being joined to each other. Along the Z-axis,

single layers are laminated, exhibiting interfaces and alter-

nating porosity.

In the case of glass infiltrated samples, no distinct

correlation could be observed as differences between average

values of bending strength and Young’s modulus are smaller

and values of standard deviation tend to sample out higher:

ag GmbH & Co. KGaA, Weinheim http://www.aem-journal.com 1041

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Fig. 4. (a) Effect of layer thickness on the porosity and bending strength of sintered andinfiltrated alumina preforms in dependence on sample orientation and (b) effect of layerthickness on Young’s modulus of sintered and infiltrated alumina preforms in depen-dence on sample orientation.

Fig. 6. Fracture toughness of sintered and infiltrated samples depending on layerthickness.

bending strength increases from 139� 17 to 175� 13 MPa as

the layer thickness decreases from 150 to 90mm; Young’s

modulus is �228� 15 GPa. The same effect is observed

considering hardness of sintered and infiltrated samples:

Vickers hardness of sintered preforms increases from 0.5� 0.2

to 3.2� 1.1 GPa as the layer thickness decreases from 150 to

90mm. In the case of infiltrated samples, Vickers hardness of

11.6� 3 GPa was measured (Fig. 5).

Fig. 5. Hardness HV-5 of sintered and infiltrated samples depending on layer thicknessand tested plane.

1042 http://www.aem-journal.com � 2009 WILEY-VCH Verlag GmbH & C

Fracture toughness of sintered samples is also affected by

their orientation within the building chamber (Fig. 6). Sintered

samples orientated in the Y-axis exhibit significantly

higher fracture toughness than those printed in the X- or

Z-orientation; infiltrated samples orientated in the Y- and

X-axis exhibit significantly higher fracture toughness

(�3.6� 0.2 MPa m1/2) than samples printed in the

Z-orientation (�3� 0.2 MPa m1/2).

SEM examination of the alumina/glass composites

revealed that the glass phase wets the alumina preform well.

The glass melt infiltration into Al2O3 preforms resulted in a

nearly dense composite with homogeneous structure

(Fig. 7(a)). Some closed porosity remained within the struts

and cannot be filled with glass melt. Phase composition

examined by XRD reveals a-Al2O3 to be the only crystalline

phase.

The SEM micrograph of a fracture surface of the alumina/

glass composite shows that a large variety of fracture

mechanisms is present (Fig. 7(b)): a transgranular fracture

path running through the alumina grains (marked by

arrow 1); an intergranular fracture path surrounding the

grains along grain boundaries and along the glass/alumina

interface (marked by arrow 2); a fracture path through the

glass (marked by arrow 3), and crack bridging including

grain-pull-out. Due to residual, internal stress fields in the

Fig. 7. (a) SEM micrograph of alumina/glass composite (layer thickness 120mm) and(b) fracture surface: transgranular fracture path (arrow 1), intergranular fracturepath along the glass/alumina interface (arrow 2), and fracture path through the glass(arrow 3) in the alumina/glass composite.

o. KGaA, Weinheim ADVANCED ENGINEERING MATERIALS 2009, 11, No. 12

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Fig. 8. Parts fabricated using the three-stage process: (a) sintered and infiltratedhalf-skull and (b) sintered and infiltrated turbine wheel.

glass phase, which interact with the stress field of the

propagating crack, the crack is partially forced to propagate

through the alumina grains instead of along the grain

boundaries or alumina/glass interfaces. Crack deflection on

the alumina grains is indicated by a non-planar crack along

grain boundaries and interfaces. Every change in direction

contributes to the crack deflection and increases the fracture

resistance.[19]

The geometric capability of the process can be displayed by

means of prototypes from the engineering biomedical fields

fabricated by the 3D-printing, sintering, and glass infiltration

process (Fig. 8). Parts with complex geometries on the base of

computer tomography (CT) data such as a half skull (Fig. 8(a))

and computer aided design (CAD) data such as a turbine

wheel (Fig. 8(b)) were fabricated. All the geometric details of

the data models were exactly reproduced in the final parts.

Conclusions

Nearly dense parts of alumina/lanthanum-glass composite

with complex geometries were successfully fabricated by

3D-printing, sintering of the printed bodies, and post-

pressureless glass infiltration into sintered porous preforms.

The relationship of layer thickness of the 3D-printing process,

porosity, and mechanical properties of alumina preforms to

those of the corresponding composites was clarified: in

general, the minimization of the layer thickness will reduce

the porosity, and, as a result, bending strength and Young’s

modulus of the alumina preforms increase. Sample orienta-

tion also has a significant influence: mechanical properties of

sintered preforms orientated along the Y-axis of 3D-printer

are higher than those along the X- and Z-axis, respectively.

The mechanical properties of alumina/glass composites were

considerably improved by infiltration with lanthanum-

ADVANCED ENGINEERING MATERIALS 2009, 11, No. 12 � 2009 WILEY-VCH Verl

aluminosilicate glass and tend to no longer depend on the

layer thickness and direction.

Received: July 16, 2009

Final Version: August 10, 2009

Published online: November 27, 2009

[1] S. Taktak, M. S. Baspinar, Mater. Des. 2005, 26, 459.

[2] Q. Zhu, G. de, With, L. J. M. G. Dortmans, F. Feenstra, J.

Eur. Ceram. Soc. 2005, 25, 633.

[3] X. P. Luo, J. M. Tian, Y. L. Zhang, L. Wang, Dent. Mater.

2002, 18, 216.

[4] X. J. Sheng, H. Xu, Z. H. Jin, Y. L. Wang, Mater. Lett. 2004,

58, 1750.

[5] M. Kalin, S. Jahanmir, Wear 2003, 255, 669.

[6] M. Guazzato, M. Albakry, L. Quach, M. V. Swain, Dent.

Mater. 2005, 21, 454.

[7] H. Claus, Quintessenz Zahntech. 1990, 16, 35.

[8] D. Y. Lee, D. J. Kim, B. Y. Kim, Y. S. Song, Mater. Sci. Eng.

A 2003, 341, 98.

[9] P. Greil, Mater. Chem. Phys. 1999, 61, 64.

[10] M. Cima, E. Sachs, T. L. Fan, J. F. Bredt, S. P. Michaels,

S. Khanuja, A. Lauder, S. J. Lee, D. Brancazio, A. Cur-

odeau, H. Tuerck, United States Patent (1995), No.

5387380.

[11] J. Moon, A. C. Caballero, L. Hozer, Y.-M. Chiang,

M. J. Cima, Mater. Sci. Eng. A 2001, 298, 110.

[12] R. Melcher, S. Martins, N. Travitzky, P. Greil, Mater Lett.

2006, 60, 572.

[13] C. R. Rambo, N. Travitzky, K. Zimmermann, P. Greil,

Mater. Lett. 2005, 59, 1028.

[14] X. W. Yin, N. Travitzky, P. Greil, Int. J. Appl. Ceram.

Technol. 2007, 4, 184.

[15] X. W. Yin, N. Travitzky, R. Melcher, P. Greil, Int. J. Mater.

Res. 2006, 97, 492.

[16] N. Travitzky, K. Zimmermann, R. Melcher, P. Greil,

Ceram. Trans. 2006, 175, 37.

[17] W. Sun, D. J. Dcosta, F. Lin, T. El-Raghy, J. Mater. Process.

Technol. 2002, 127, 343.

[18] M. Radovic, E. Lara-Curzio, L. Riester, Mater. Sci. Eng. A

2004, 368, 56.

[19] H. Hornberger, S. Marquis, S. Christiansen, H. P. Strunk,

J. Mater. Res. 1996, 11, 855.

ag GmbH & Co. KGaA, Weinheim http://www.aem-journal.com 1043