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ISSN (Print) 1013-9052
EISSN 1658-3558

The Saudi Dental Journal,
P.O. Box 52500,
Riyadh 11563,
Kingdom of Saudi Arabia
Tel.
966-1-467-7328
Fax.
933-1-467-7308 /
966-1-467-7534
Email
saudidj@ksu.edu.sa

Relative fracture toughness and hardness of dental ceramics

 

Sharifa Al-Shehri, BDS, MS
Department of Prosthetic Dental Sciences, College of Dentistry, King Saud University, Riyadh, KSA.


Abstract 

 

The resistance of material to crack propagation is defined as fracture toughness (KIC) and is one measure of the strain energy absorbing ability of brittle materials.  An identation technique was used to compare the apparent fracture toughness (KIC) and hardness of six dental ceramic materials to a control soda-lime-silica glass.  The materials studied included Vita VMK 68 body porcelain, Optec HSP body porcelain, Dicor, IPS- Empress castable ceramics, Vitadur N core porcelain and In-Ceram core porcelain.  Alumina reinforced materials (In-Ceram core) resulted in the highest fracture toughness values followed by Vitadur N core porcelain.  IPS-Empress and Optec HSP materials showed moderate but statistically significant (P < 0.0001) greater values compared to conventional feldspathic porcelain Vita VMK68 and a control soda-lime-silica glass.  These differences in KIC were attributed to differences in the nature of crack microstructure interaction.  The hardness of Dicor castable ceramic was significantly lower than all materials tested including soda-lime-silica glass suggesting a lack of direct correlation between those two properties.

 

Introduction

 

Dental ceramics, like all brittle materials, suffer from an inability to absorb appreciable quantities of plastic strain energy prior to fracture.  This liability is manifested in such behavior as flaw sensitivity, low tensile strength, and catastrophic failure.1 One measure of the strain energy absorbing ability of a brittle material is the critical stress intensity factor "fracture toughness" or KIC.  The fracture toughness of a material is related to the level of tensile stress which must be attained in the vicinity of a crack tip before a catastrophic fracture process is initiated.1 Mechanical properties as diverse as strength, thermal shock resistance, and susceptibility to erosive wear are all controlled by this parameter.  Unlike fracture strength, KIC is intrinsic to the material and is less sensitive to such variables of specimen preparation as the size and density of surface flaws.2

Because of the importance of fracture toughness in determining all aspects of brittle material mechanical behavior, knowledge of KIC for dental ceramics is an essential starting point if the resistance to fracture of ceramic base dental prostheses is to be improved. KIC for dental materials is usually determined through the use of an indentation technique.3,4 This method is particularly suited to relatively expensive materials like dental ceramics since small samples are required.  The basis of this technique is the series of cracks that form around a Vickers hardness indentation in a brittle material. (Fig.1) These cracks, which are termed radial cracks, appear to emanate when viewed from above, from each of the corners of the indentation.  The size of these cracks, expressed by the surface dimension c (measured from the center of the indentation), increases with increasing indentation load and is an inverse function of fracture toughness.  The technique has been used to obtain KIC values for a variety of dental materials, including dental amalgam,5,6 commercial dental porcelains,2,7 and composite resins,8 and for indirectly measuring stresses on the interface of metal ceramic restorations.9 The rapid introduction of new dental restorative ceramic materials makes the selection of the appropriate material difficult.  This investigation selected the indentation technique to determine the relative fracture toughness and hardness of several recently introduced dental ceramic materials and compared the results with a traditional feldspathic porcelain and soda-lime-silica glass.

 

Materials and Methods

 

The ceramic materials used in this study are listed in Table 1.

            Ceramic specimens for fracture toughness determination were circular discs 10.0 ± 0.6 mm in diameter and 1.5 ± 0.4 mm in thickness.  The conventional powder systems VMK68, Optec HSP, and Vitadur N core were formed into discs by vibrating and condensing porcelain slurry into a brass mold.  Excess moisture was eliminated from the porcelains by blotting with absorbent tissues.  After dynamic under ambient conditions for a minimum of 4 hours, the discs were fired according to the manufacturer's recommended firing schedule using a commercial porcelain furnace (Vicumat200, Vita Zahnfabrik).

Discs of Dicor (DI) and IPS-Empress (EMP) were prepared with the lost wax technique and were cast or hot pressed, respectively.  The In-Ceram core porcelain discs were made by pouring the slip material into a special silicone mold over a uniform thickness (approximately 0.5 mm gypsum material supplied by the manufacturer.  After setting, the discs were sintered and glass infiltrated according to the manufacturer's instruction. Each disc specimen was mounted in acrylic resin and the exposed surface was ground flat with 150 grit aluminum oxide and polished with a sequence of steps that ranged from 180 to 600 grit.  Final polish was done using 1 µm diamond paste.

Ten specimens of each material were fabricated.  Polished samples were placed in an oven at 600oC  for 30 minutes to relieve residual stresses that may have developed because of polishing procedures.  Samples were coated with approximately 40 nm of gold using a vacuum vaporization process to allow the cracks to be more clearly seen.  Also included in the study were specimens of soda-lime-silica glass, which is used in fracture studies as a reference standard.  The reference sample was obtained from a glass microscope slide.  It was prepared with the same coating and testing procedure as used on the ceramic samples 

Determination of fracture toughness

Fracture toughness was determined by the indentation technique. Ten to fifteen indentations were made on each sample at widely separated locations with a load of 1 kg ( 9.8N) for 15 seconds in a microhardness tester.  The fracture toughness was calculated with the following formula KIC = 0.016 (E/H)0.5 (P/c1.5), where KIC is fracture toughness, c is the crack length (measured from the center of indentation), P is the applied indenter load, H is the Vickers hardness (0.47 P/a2), a is the half diagonal of the indentation, and E is the elastic modulus.

A total of 50 cracks were measured for each material with crack size data obtained on 10-15 cracks per specimen.  Measurements were made within 2-4h following indentation. The elastic modulus7 for each material was determined using a three-point bend test of five rectangular specimens with the dimensions of 3x2x25mm.

All the specimens were loaded to failure.  Load and displacement were monitored during testing using a precise computer program which also calculated Youngs modulus from the load displacement curves taking into account sample geometry.  The average E value for each material was used in the formula to calculate fracture toughness.  The fracture toughness data were subjected to analysis of variance (ANOVA) and Tukey's multiple comparison tests to determine significant differences among group means.

 

Results

 

Mean elastic modulus (E) and hardness (H) values for each material are reported in Table 2.  The mean values for E were 279 + 6.4 GPa for In-Ceram, 116.8 + 4 GPa for Vitadur N core, and ranged from 70 + 3.5 to 59.2 + 3.3 GPa for the other materials.  Hardness values ranged from 4.5 to 9.5 GPa.  Results of the one-way ANOVA for hardness and fracture toughness KIC data are summarized in Table 4 and indicate that very highly significant differences (P < 0.0001) existed among group means. Table 2 lists materials in order of increasing mean hardness values and vertical lines connect group means that were not significantly different at the 95% level of confidence.  Dicor castable ceramic resulted in the lowest measured hardness values and In-Ceram core ceramic resulted in the greatest hardness.

Means and standard deviations of the measured crack length and calculated fracture toughness values for each of the ceramic materials tested are listed in Table 3.  The KIC value obtained for the soda-lime-silica glass was 0.8 + 0.04 MN/m3/2 which compared favorably with the literature.10  Mean fracture toughness values for tested dental ceramics ranged from 0.95 + 0.09 MN/m3/2 for VMK68 feldspathic porcelain to 4.58 MN/m3/2 for In-Ceram core porcelain.  Results of the ANOVA for the fracture toughness values are summarized in Table 4 and indicate that a very highly  significant difference (P  0.0001) occurred among group means.  The vertical lines in Table 3 connect group means that were not significantly different at the 95% confidence level.  Alumina reinforced ceramic materials, In-Ceram core and Vitadur N core porcelain, resulted in an appreciably greater fracture toughness than the other materials tested. The two castable ceramic materials tested, Dicor and IPS-Empress, and Optec HSP feldspathic porcelain resulted in an appreciably greater fracture toughness than conventional feldspathic porcelain (VMK68) which had a significantly higher KIC than the reference glass.

 

Discussion

 

The indentation derived fracture toughness and hardness values for conventional feldspathic porcelain, alumina reinforced porcelain, fluormica glass ceramic, Lucite reinforced glass ceramic and reference soda-lime-silica glass were in agreement with similar values reported previously.2,7,10-12       

Hardness is a property of restorative materials that is generally considered important to applications involving friction and wear, although a direct correlation between matched hardness to minimize wear cannot be made. Intraoral conditions limit this; and indeed, a hard material will scratch, abrade, and wear away opposing tooth structure.  It is desirable for a restoration to resist abrasion and have a wear rate equal to that of enamel.  Materials with low hardness, like Dicor castable ceramic, will probably not damage the natural antagonists.  However, the rate of tooth substance wear has been found to be a function of roughness.13

This investigation indicated that substantial improvements were apparent in fracture toughness of several new dental ceramics relative to conventional feldspathic porcelain, but the fracture resistance of these new materials was still far below that of alumina reinforced materials.  Although the optical properties of ceramic materials were not measured in this investigation, optical effects are critical for selection of materials.  Nevertheless, it could be generally stated that materials with intermediate fracture toughness and translucency similar to feldspathic porcelain (i.e. Optec HSP, Dicor,and IPS- Empress) are often preferred over materials with greater fracture resistance and high opacity (namely, Vitadur N core and In-Ceram core) when higher esthetic properties are required as in anterior crowns and veneers.  On the other hand, if resistance to fracture is the primary concern as for posterior crowns and bridges, higher fracture toughness materials should be selected.

Several approaches to strengthening ceramics have been recognized in the past two decades.  The ways leading to increased fracture toughness or specific fracture energy of ceramics generally involve manipulation and tailoring of the microstructure. The microstructure can be improved by optimizing the proportions of the individual phases, including crystalline and glassy phases, by adjusting their shape and size distribution, by optimizing the size and shape of crystalline grains, and by improving their mutual bonds.  If the ceramic body contains a relatively high proportion of glassy phase, the crack will primarily propagate through this phase and the properties of the other phases will have little effect.  VMK68 and Optec HSP are both leucite reinforced porcelains, though Optec HSP showed higher KIC in this study.  This could be the manifestation of improved microstructure by incorporating a higher amount of the crystalline phase for Optec HSP (48% vol) as compared to VMK (19% vol).14 Another possible reason for the increased KIC of Optec as compared to VMK68 is the difference in grain size of raw material (10-15 m for Optec and 15-20 m for VMK).14

A fine homogeneous microstructure with the smallest grain is another requirement for increasing fracture toughness of ceramics.  The probability of defects occurring in the crystal lattice or in the grains decreases with decreasing grain size, as does the energy of microstresses which has accumulated in grains and is available for possible formation of microcracks.  In addition, grain boundaries always represent an obstacle to crack propagation from one grain to another.15  One favorable property of polycrystalline ceramics is that cracks can only propagate over certain lattice planes inside the grains in the case of transgranular fracture and through the narrow space between the grains for intergranular fracture. The crack propagation is therefore spatially restricted with the result of higher forces necessary and of a larger total fracture area and thus a higher overall energy consumed. The inhomogenous stress distribution in front of the crack due to anisotropy of the elastic properties of the individual crystals also plays a role.  If the grain size is too small, these effects cease to influence the process.15  Evidence for this is given by the generally easy crack propagation in glass whose structure is almost ideally disarranged.

A significant part is also played by the sintering process and the presence of pores. For this reason, a special technique for ultrasonic mixing of In-Ceram core porcelain was introduced with the system.  Residual pores are then removed after sintering through glass infusion.  This technique seems to have a positive effect in reducing the amount of total porosity of this material.  As far as pores are concerned, these should not arise at grain boundaries where they increase the stress concentration at points where weakened bonds already occur. In contrast to this, pores of spherical shape arising for example in the glassy phase may even have a favorable effect by blunting the crack front so that greater energy is required for its growth.15

Particle sizes and the amount of crystalline phase are believed to affect the resulting toughness.  In-Ceram core and Vitadur N core are similar materials that differ mainly in crystalline size (1-5 m for In-Ceram and 10-25 m for Vitadur N core)14 and the amount of crystalline phase in the glass matrix (85+% for the In-Ceram core and 30% (vol) for Vitadur N core).  The improved fracture toughness of In-Ceram core supports the concept that increased amounts and finer grains tend to improve toughness.

A glass ceramic is initially a glass in which, at some stage, the formation of nuclei is enhanced either by the addition of nucleating agent of by using special compositions which are self-nucleating.  The resulting material contains very small crystals in a residual glassy phase.  If the crack, whenever nucleated, takes a tortuous path through the glass ceramic, then more energy will be absorbed in surface production, and fracture toughness will be improved.16  The residual glass phase will be of major importance because stresses developed at the interface between crystal and glass will, to a large extent, determine the crack path.  Stresses between the two phases arise from thermal expansion mismatch, and consideration of this leads to expectations for improved toughness.  For this, suitable oxide additions can be made to the original base glasses so that the residual glass will have a lower coefficient of thermal expansion than the crystalline phase. 

Residual stress in the interface is tensile, and fracture will always be expected to be intergranular, with longer path length and higher fracture toughness.16  This  is the primary strengthening mechanism in the case of Dicor and IPS Empress glass ceramics.  The leucite reinforced IPS Empress is further strengthened through the residual stresses created by volume reduction associated with the high to low temperature phase transformation of leucite.  This, in addition to the high coefficient of thermal contraction, creates a situation that causes leucite crystals to contract substantially more than the glass matrix that surrounds the particles and are frozen during the cooling phase.  Tensile forces are created in the particles leading to microcracking in the leucite phase.  Branching of a primary crack into a greater number of secondary cracks or simultaneous growth of many cracks leads to an increase in the fracture surface and volume, reducing the stress peaks.17,18

 

Conclusions

 

  1. In-Ceram had substantially greater hardness and fracture toughness than all other materials.
  2. Dicor had a moderate fracture toughness and the lowest hardness, suggesting a weakcorrelation between the two properties.
  3. Alumina was the most effective toughening phase currently used in dental ceramics.
  4. Leucite and fluor mica were both effective atincreasing the toughness of ceramic materials (Optec HSP, IPS-Empress, and Dicor castable ceramics) over that of conventional feldspathic porcelain but the effect was not as pronouncedas with alumina.

 

Acknowledgement

 

This study (NF 1802) is registered with the College of Dentistry, Research Center (CDRC), King Saud University.

Address reprint requests to:

Dr. Sharifa Al-Shehri
P.O. Box 60169
Riyadh 11545  KSA

 

References

 

  1. Kingery WD. Introduction to Ceramics. 2nd ed. London: John Wiley & Sons; 1976.
  2. Morena R, Lockwood PE, Fairhurst CW. Fracture toughness of commercial dental porcelains. Dent Mater 1986;2:58-62.
  3. Lawn BR. The indentation crack as a model surfaceflaw. In; Bradt, R.C., Evans, AG Hasselman, DPH,Lange FF eds.: Fracture Mechanics of Ceramics. Volume 5. New York: Plenum Press, 1983:1-25.
  4. Evans AG. Fracture toughness: The role of indentation techniques. In: Freiman SW ed. Fracture  Mechanics Applied to Brittle Materials. Special  technical publication 678. Philadelphia: AmericanSociety for Testing and Materials 1979;pp.112-135.
  5. Roberts JC, Powers JM, Craig RG.  Fracture toughness  and critical strain energy release rate of dental amalgam.  J Mater Sci 1978;13:965-971.
  6. Lloyd CH, Adamson M. The fracture toughness (KIC) of amalgam.  J Oral Rehabil 1985;12:59-68.
  7. Anusavice KJ, Lee RB. Effect of firing temperatureand water exposure on crack propagation in unglazed porcelain. J Dent Res 1985;64:Abstr.1092.
  8. Yoshimoto S, Nakajima N, Kubota A, Iwamoto F.Fracture toughness of posterior composite resin.  J  Dent Res 1985;64:Abstr. 37.
  9. Rosenstiel SF, Porter SS. Apparent fracture  toughness of dental porcelain with a metal substructure.  Dent Mater 1988;4:187-190.
  10. Wiederhorn SM.  Fracture surface energy of glass.  JAm Ceram Soc 1969;52:99-105.
  11. Jones DW, Rizkalla AS, Sutow EJ, King HW. Indentation fracture toughness and dynamic young's modulus of ceramic biomaterials.  Mat Sci Eng 1988;A105/106:207-13.
  12. Seghi RR, Denry IL, Rosenstiel SF.  Relative fracture toughness and hardness of new dental ceramics.  JProsthet Dent 1995;74:145-150.
  13. Seghi RR, Rosenstiel SF, Bauer P.  Abrasion of human  enamel by different dental ceramics in vitro. J Dent Res 1991;70:221-225.
  14. Denry IL, Rosenstiel SF, Holloway JA.Characterization of crystalline leucite in dental  porcelain [Abstract]. J Dent Res 1994;73:369.
  15. Mencik J. Strength and fracture of glass and ceramics.  Glass Science and Technology Vol. 12.  New York E. Silvier Science Pub. Co. Inc 1992;242-279.
  16. McColm IJ. Ceramic science for materials technologists. New York Leonard Hill 1983;204-  234.
  17. Claussen N, Steeb J. Toughening of ceramic composites by oriented nucleation of microcracks.  J Am Ceram Soc 1976;59:457-456.
  18. Evans AG, Heuer AH, Porter DL. Fracture toughnessof ceramics. In: Fracture 1977  Advances in research  on the strength and fracture of materials. Editor: D.M.R. Taplin. Pergamon Press, New York, 1978. 

 

Tables and Figures

 


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