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Article

Martens Hardness of CAD/CAM Resin-Based Composites

Department of Prosthetic Dentistry, UKR University Hospital Regensburg, 93042 Regensburg, Germany
*
Author to whom correspondence should be addressed.
Appl. Sci. 2022, 12(15), 7698; https://doi.org/10.3390/app12157698
Submission received: 11 July 2022 / Revised: 28 July 2022 / Accepted: 28 July 2022 / Published: 30 July 2022

Abstract

:
(1) Background: The properties of CAD/CAM resin-based composites differ due to differences in their composition. Instrumented indentation testing can help to analyze these differences with respect to hardness, as well as energy-converting capabilities due to viscoelastic behavior. (2) Methods: Eleven materials were investigated using instrumented indentation testing. Indentation depth (hr), Martens hardness (HM), indentation hardness (HIT), indentation modulus (EIT), the elastic part of indentation work (ηIT), and indentation creep (CIT) were investigated, and statistical analysis was performed using one-way ANOVA, Bonferroni post-hoc test, and Pearson correlation (α = 0.05). (3) Results: All of the investigated parameters revealed differences between the analyzed materials. Besides the differences in hardness-associated parameters (hr, HM, and HIT), instrumented indentation testing demonstrated differences in energy-converting properties. The subsequent one-way ANOVA revealed significant differences (p < 0.001). A significant (p < 0.01, Pearson correlation >0.576) correlation between the materials and HM, HIT, or EIT was identified. (4) Conclusions: Due to the differences found in the energy-converting properties of the investigated materials, certain CAD/CAM resin-based composites could show superior stress-breaking capabilities than others. The consequential reduction in stress build-up may prove to beneficial, especially for implant-retained restorations or patients suffering from parafunctions.

1. Introduction

Due to their clearly deviating properties, resin-based CAD/CAM (computer-aided design/computer-aided manufacturing) composites are an interesting clinical alternative to dental ceramics [1]. Similar to direct resin-based composites, resin-based CAD/CAM composites consist of inorganic fillers embedded in an organic polymer matrix, commonly using silanes as coupling agents. Their mechanical properties such as modulus of elasticity or flexural strength are improved due to the standardized polymerization process under industrial conditions compared to chair-side light-curing polymerization [2]. A variation of resin-based composites is the so-called polymer-infiltrated ceramic network (PICN), which comprises a structure-sintered ceramic matrix and a reinforcing polymer network (ceramic content: 86 wt%; polymer content: 14 wt%). Resin-based CAD/CAM composites and resin-infiltrated ceramic networks are used for inlays, onlays, and veneers, as well as tooth- and implant-retained crowns. Some composites are even approved for bridges and for use in patients suffering from bruxism.
One key benefit of these resin-based materials—as advertised by many manufacturers—is the dentine-like modulus of elasticity of approximately 10–30 GPa. Although composites do not reach the high aesthetics of ceramics, they are commonly regarded as less hard and brittle, and they cause less wear and stress in antagonistic teeth [3]. These qualities may be beneficial for the rehabilitation of patients suffering from parafunctions such as bruxism. Energy-dissipation capabilities might also be increased by the utilization of resin-based CAD/CAM composites with a low modulus of elasticity [4,5,6,7]. Implant-supported restorations, with their lower tactility and elasticity of the osseointegrated implants, might benefit from less stress build-up during normal mastication. For example, there is evidence for improved implant osseointegration with low-modulus titanium implants [8,9]. This phenomena is mostly attributed to the so-called stress-shielding effect, which is caused by the differences of the elastic moduli between implant and bone. The mismatch leads to an insufficient transfer of force and therefore inadequate stimulation of bone remodeling [10]. It is suggested that the stimulation of bone growth may be enhanced by reducing or adjusting the elastic modulus of the restorative material.
Yet, with respect to the mechanical properties of CAD/CAM resin-based composites, previous research suggests a fairly inhomogeneous class of materials [11]. This is mostly attributed to different types, sizes, and amounts of inorganic fillers (approximately 60–85 wt%), as well as the organic matrix [12]. The significant differences in CAD/CAM resin materials, e.g., flexural strength (150–330 MPa) and modulus of elasticity (10.3–30.0 GPa), may have impacts under clinical conditions. To properly evaluate the available materials and perhaps even choose certain materials for specific clinical indications, detailed information on their mechanical behavior is essential. One method for evaluating elastic and viscoelastic behavior is indentation hardness testing. Surface hardness is defined as the resistance against plastic and therefore permanent deformation by indentation. Hardness is commonly measured with methods such as Vickers, Rockwell or Brinell hardness testing. However, indentation testing encompasses more than just permanent deformation, as elastic or even viscoelastic components can also be determined by the measurement. These properties can be measured using instrumented indentation testing, also called Martens hardness (HM) testing. HM is derived from the applied force (F) divided by the indentation surface (As), which is a function of the indentation depth (h) (Equation (1)).
H M = F A S ( h )
Furthermore, the constant measurement of force and indentation depth provides a force–indentation depth curve, as well as the fundamentals for additional analysis.
The indentation modulus (EIT), which is determined in the compression mode, is related but not identical to the modulus of elasticity, which is determined in the flexure mode [13]. The elastic part of the indentation (expressed by ηIT) could help in the assessment of the use of resin-based CAD/CAM composites for use as stress-breakers for implant-supported restorations. The time-dependent response to the indentation of a viscoelastic material [14] can be expressed as indentation creep (CIT), expressing the relative increase of strain under constant force application, e.g., due to the rearrangement of polymer chains. As the deformation caused by creep is of plastic character, CIT can help to estimate the long-term dimensional and mechanical stability of a material [15,16,17,18]. Materials that significantly differ in these properties could therefore be used for different applications.
The hypothesis of this study was that different CAD/CAM resin-composite materials show no similarities regarding indentation depth (hr), Martens hardness (HM), indentation hardness (HIT), indentation modulus (EIT), the elastic part of indentation work (ηIT), and indentation creep (CIT). The obtained results can help to estimate the energy-conversion behavior and therefore the clinical performance of the significantly different materials under masticatory loads, as well as their stress-breaking capabilities.

2. Materials and Methods

Eleven resin-based CAD/CAM materials (n = 6 per material) were investigated using instrumented indentation testing according to ISO 14577-1 [19]. Table 1 provides an overview over the tested materials, as well as some of their properties (modulus of elasticity E (GPa), filler content wt. (%), and fracture strength FS (MPa)) for the better interpretation of the results of this study. Rectangular specimens (10 × 10 × 2 mm) were produced in CAD/CAM dental milling machine (98 milling blank, Inlab MC X5, Dentsply Sirona, Germany) and polished (1000 grit sandpaper, Tegramin 25, Struers, Germany).
Testing was carried out with a universal hardness-testing machine (ZwickiLine Z2.5, ZwickRoell, Germany; see Figure 1).
The Martens hardness (HM) is the ratio of the maximum force to the associated contact area (N/mm²). Other material parameters, such as indentation modulus, indentation creep, and plastic and elastic work of deformation, can be characterized from a force–indentation depth curve. In this study, force, depth and time during the indentation of the diamond pyramid were continuously recorded. The contact area under load was calculated from the maximum indentation depth. The indentation depth was constantly monitored at a loading speed of 0.5 mm/min to a maximum force of Fmax = 10 N using a Vickers indenter and dwell-time of 10 s. Unloading was performed at 0.1 mm/min. The recorded force–indentation depth curves were used to calculate indentation depth (hr), Martens hardness (HM), indentation hardness (HIT), indentation modulus (EIT), the elastic part of indentation work (ηIT), and indentation creep (CIT) as defined in ISO 14577-1. The Poisson’s ratio of the diamond indenter was set to νi = 0.07, and that of the resin-based composite materials was set to νs = 0.3 [23]. The Young’s modulus of the indenter was Ei = 1140 GPa.
Calculations and statistical analyses were performed using SPSS 25.0 for Windows (IBM, Armonk, NY, USA). The normal distribution of data was controlled using the Shapiro–Wilk test. Means and standard deviations were calculated and analyzed using ANOVA and the Bonferroni test for post-hoc analysis. Pearson correlations were calculated. The level of significance was set to α = 0.05.

3. Results

The Shapiro–Wilk test confirmed the normal distribution of the tested parameters. The one-way ANOVA revealed significant differences (p < 0.001) within the parameters. Table 2 shows mean results and statistical Bonferroni post-hoc comparison. Force–indentation-curves of the investigated materials are shown in Figure 2.
The mean Martens hardness (HM) ranged from 410.8 ± 55.8 N/mm2 (KA) to 1143.4 ± 124.7 N/mm2 (VE). The ANOVA showed significant (p ≤ 0.001) differences between the results (Table 2). The residual indentation depth (hr) was between 13.9 ± 0.7 µm (VE) and 23.0 ± 1.4 µm (KA), with significant differences between the results (ANOVA: p ≤ 0.001). The indentation hardness (HIT) varied between 666.5 ± 88.2 N/mm2 (KA) and 1834.2 ± 198.0 N/mm2 (VE). The ANOVA confirmed significant (p ≤ 0.001) differences between the results. The indentation modulus (EIT) ranged from 8.8 ± 1.4 kN/mm2 (KA) to 25.3 ± 3.0 kN/mm2 (VE), with significant differences between the results (ANOVA: p ≤ 0.001). The mean elastic part of indentation (ηIT) varied between 40.2 ± 0.5% (VO) and 50.4 ± 4.3% (LU) (Figure 3). The ANOVA confirmed significant differences between the mean values (p ≤ 0.001). The indentation creep (CIT) ranged from 3.2 ± 0.1% (VE) to 5.1 ± 0.4% (KC). The ANOVA showed significant (p ≤ 0.001) differences between the values.
A highly significant (p < 0.01, Pearson correlation >0.576) correlation between the materials and HM, HIT or EIT was identified. Negative correlations were established for hr (−0.623), and CIT (−0.584). No correlation could be determined for ηIT (−0.151, p = 0.227). A significant (p < 0.001) impact of the material was found on HM2 = 0.914), HIT2 = 0.867), EIT2 = 0.910), CIT2 = 0.771), ηIT2 = 0.544), and hr2 = 0.814).

4. Discussion

The hypothesis that different CAD/CAM resin-composite materials show no similarities regarding indentation depth (hr), Martens hardness (HM), indentation hardness (HIT), indentation modulus (EIT), the elastic part of indentation work (ηIT), and indentation creep (CIT) could be partly confirmed. The novelty of this study is that the data were used not only to evaluate the material hardness but also to differentiate the elastic and viscoelastic surface parameters. In addition, possible clinical consequences of the results and applications were discussed.
Figure 4 shows the force–indentation depth curves, which highlight individual parameters investigated in this study. In comparison to research on the Martens hardness of CAD/CAM resin-based materials, the published HM values for the PICN material (VE) are distinctly higher (1524–1555 N/mm2) compared to the results of this investigation (1143 N/mm2) [24,25]. Differences here were due to the transverse contraction number required for the calculations. With respect to the resin-composite materials with a filler content of more than 70%, the HM values found in the literature (667–1089 N/mm2) are in line or above the results of this study (588–771 N/mm2) [24,25,26,27]. The HM values reported in the literature for composites with a filler content below 70% are distinctly below (BC*: 151 N/mm2) [24] or in line (477–573 N/mm2) [25,27] with the values obtained in this investigation (411–603 N/mm2). The EIT values found in the literature (2.5–30 kN/mm2) are lower or in line with the results of this study (9–25 kN/mm2) [24]. The CIT values obtained in this study (3.2–5.1%) were slightly higher compared to those of the literature (2.6–3.4%) [26,27].
Creep and therefore CIT values are characterized by the short horizontal parts of a depth curve at peak force. EIT values are determined by the slope of the ascending part of the curve. The curve of VE indicates low CIT and high EIT values, which indicates a low susceptibility to creep and high resistance against elastic deformation. The curve of KA in comparison shows a longer horizontal movement at peak force and a less steep slope of the ascending curve, indicating higher CIT and lower EIT values. In this study, the HM values started at about 400 N/mm2 for the composite with the lowest filler content and were almost twice as high for the composite with the highest filler content. Three times higher values were even identified for PICN, although the inorganic weight content was slightly comparable to that of the highly filled composite. These results confirm previous research that indicated at a positive correlation between inorganic filler content and surface hardness for resin-based composites [28,29,30]. However, our results also confirm the special position of PICN [24,31]. As expected, a comparable behavior was also observed for results of hr, with an approximately 25% lower indentation depth for the highly filled composite or even 40% for the PICN. However, there were also exceptions in the resin-based composite group, since, e.g., materials with the same filler content (BC and ES; approximately 72%) showed differences of up to 25%. Filler type and size, as well as polymer composition or the chemical bonding of the fillers, may also affect materials’ surface properties and explain the differences in materials with similar filler contents [12,32,33,34]. A correlation between surface hardness and inorganic filler content [11] could also be observed for the materials investigated in this study. The relative differences in standard deviations can be attributed to the uneven filler distribution and the resulting different filler content on the material surface. Since the composition and topography of a material’s surface have decisive influence on hardness measurements, results may vary accordingly. In addition, a different polymerization of the matrix due to a distinct manufacturing process can influence results [27]. Resin-composite materials are considered to be less hard and brittle and to cause less stress build-up in antagonistic teeth compared to ceramics. The present material’s properties were within the range of data of human dentine from literature (indentation hardness of 0.4–1.1 GPa and indentation modulus of 12.2–22.9 GPa) [35,36,37]. As the elastic modulus also resembles that of dentin (approximately 15 GPa) [38], CAD/CAM composites could be considered when looking for a biomimetic approach for a dentine replacement [39].
With mean indentation creep CIT values between 3.2% and 5.1%, the analyzed resin composite materials were more resistant to creep compared to human dentine at 8.6 to 10.7% [37]. However, CIT is difficult to interpret in the context of dental materials and their clinical application, as the duration of teeth contact in a physiological masticatory cycle is only about 0.1 to 0.2 s [40], whereas the application time is 10 s during instrumented indentation testing. Assuming only intermittent tooth contact, e.g., while chewing or swallowing, as well as the natural energy-dissipation capabilities of hard dental tissues and the periodontal ligament, the differences in CIT seem to be negligible. However, clenching or bruxism, perhaps even in combination with reduced resiliency in implants or ankylosed teeth, could increase the significance of creep behavior because the magnitude and, especially, the duration of stress application may increase. In these cases, creep will be more relevant for the long-term stability and integrity of the restoration, as stress will also be induced at the intaglio surface [41,42]. This phenomena could lead to debonding, permanent deformation, and perhaps ultimately to an insufficient fit of the restoration. At the tooth–restoration interface, creep could lead to over-contouring or the formation of gaps, which could significantly reduce clinical performance. The energy-dissipating capabilities (“damping effects”) are associated with the conversion of energy (storage and energy dissipation). The obtained ηIT values indicate the work that is converted into potentially stored elastic energy (welastic), whereas the other part of indentation work is mostly dissipated throughout plastic deformation or heat (wplastic).
Based on the current data, an indication-driven selection of the investigated materials could improve clinical performance. For example, the reduced resiliency and tactility of implants could be compensated for by a material that causes less stress build while being creep resistant. Such a material must therefore have low EIT and CIT values. The finite element analysis of inlay or partial crowns with higher elastic moduli points to higher stress build-up within the restoration while simultaneously causing less stress build-up in the cement layer and hard dental tissue [43,44,45]. Materials with high EIT and fracture strength values yet low CIT values could therefore show superior clinical performance when used for partial or inlay crowns. Materials with high CIT values should be considered with caution for permanent restorations. However, the ability to gradually deform under constant stress could be useful in cases where a certain self-balancing effect is desired. These materials could therefore be considered for long-term temporary crowns during pre-prosthodontic treatment, as the viscoelastic behavior could help to self-equilibrate the occlusion. The parameters presented in this study can be regarded as a relevant contribution to established parameters such as flexural strength, wear, and filler content.

5. Conclusions

The authors of this study investigated the mechanical properties (indentation depth (hr), Martens hardness (HM), indentation hardness (HIT), indentation modulus (EIT), elastic part of indentation work (ηIT), and indentation creep (CIT)) of CAD/CAM resin-based composites with instrumented indentation testing. The Martens hardness and energy-conversion capabilities of eleven different CAD/CAM composites were investigated with a reference to clinical application. Within the limitations of this study, the following conclusions can be drawn:
  • The clinical behavior of dental restorations can be influenced by selecting materials based on different elastic and viscoelastic surface parameters.
  • Hardness, indentation modulus, and creep vary significantly between different CAD/CAM resin-based composites.
  • Individual CAD/CAM resin-composites show different stress-breaking capacities for implant-retained crowns. The reduced resiliency and tactility of implants might be compensated for by a material with low EIT and CIT values.
  • Materials with high EIT and low CIT values might be beneficial for partial or inlay crown applications.

Author Contributions

Conceptualization and writing—review and editing, M.R.; writing—review and editing, S.H.; investigation and data curation, S.S.-F.; writing—review and editing, T.S.; writing—original draft preparation, A.S. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Data are contained within the article.

Acknowledgments

We thank the manufacturers for providing the investigated materials.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. (a) ZwickiLine Z2.5 and (b) schematic test procedure with maximum indentation depth (hmax) at application of maximum force (Fmax) and residual indentation depth (hmin) after stress relaxation.
Figure 1. (a) ZwickiLine Z2.5 and (b) schematic test procedure with maximum indentation depth (hmax) at application of maximum force (Fmax) and residual indentation depth (hmin) after stress relaxation.
Applsci 12 07698 g001
Figure 2. Force–indentation depth curves of the tested composite materials.
Figure 2. Force–indentation depth curves of the tested composite materials.
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Figure 3. Martens hardness (HM), indentation modulus (EIT), and indentation creep (CIT) scaled to percentage of maximum value. Materials ordered by increasing amount of inorganic filler content.
Figure 3. Martens hardness (HM), indentation modulus (EIT), and indentation creep (CIT) scaled to percentage of maximum value. Materials ordered by increasing amount of inorganic filler content.
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Figure 4. Showcase force–indentation depth curve. Wplastic/elastic = plastic/elastic indentation work; dF/dh = contact stiffness S; Fmax = maximum force; hmax = maximum indentation depth; hr = depth at contact stiffness tangent.
Figure 4. Showcase force–indentation depth curve. Wplastic/elastic = plastic/elastic indentation work; dF/dh = contact stiffness S; Fmax = maximum force; hmax = maximum indentation depth; hr = depth at contact stiffness tangent.
Applsci 12 07698 g004
Table 1. Materials, manufacturers, abbreviations (Abbr.), modulus of elasticity (E), filler content (wt.), fracture strength (FS) according to manufacturer’s specifications or literature: a [20], b [21], c [22], and d [11]). Filler content classification: low-fill ≤ 74% wt. ≤ compact.
Table 1. Materials, manufacturers, abbreviations (Abbr.), modulus of elasticity (E), filler content (wt.), fracture strength (FS) according to manufacturer’s specifications or literature: a [20], b [21], c [22], and d [11]). Filler content classification: low-fill ≤ 74% wt. ≤ compact.
MaterialManufacturerAbbr.E [GPa]wt. [%] dFS [MPa]
CerasmartGC Corp., Tokyo, JPCS12.1 a66.9231
Brilliant CriosColtene Holding AG, Altstätten, CHBC10.372.0198
EsteliteTokuyama Dental, Chiyoda, JPEL13.872.4225
Block HCShofu Dental GmbH, Ratingen, GERBL9.5 b64.1191
Katana AvenciaKuraray Noritake, Tokyo, JPKA12.458.6190
KZR CADYamakin Co. Ltd., Kochi, JPKC10.469.0235
Experimental EX20.078.3200
Lava Ultimate3M Deutschland GmbH, Neuss, GERLU12.775.4204 c
Grandio blocVOCO GmbH, Cuxhaven, GERGB18.084.5330
VOCO ExperimentalVOCO GmbH, Cuxhaven, GERVOn/a79.7n/a
Vita EnamicVITA Zahnfabrik, Bad Säckingen, GERVE30.085.1150–160
Table 2. Material, abbreviation (Abbr.), mean and standard deviation (in brackets) for indentation depth (hr), Martens hardness (HM), indentation hardness (HIT), indentation modulus (EIT), elastic part of indentation work (ηIT), and indentation creep (CIT). Identical superscript letters indicate column-wise non-significant (Bonferroni post hoc test, p > 0.05) differences between the materials.
Table 2. Material, abbreviation (Abbr.), mean and standard deviation (in brackets) for indentation depth (hr), Martens hardness (HM), indentation hardness (HIT), indentation modulus (EIT), elastic part of indentation work (ηIT), and indentation creep (CIT). Identical superscript letters indicate column-wise non-significant (Bonferroni post hoc test, p > 0.05) differences between the materials.
MaterialAbbr.hr [µm]HM [N/mm2]HIT [N/mm2]EIT [kN/mm2]ηIT [%]CIT [%]
CerasmartCS22.8 a,b,d,f
(1.7)
441.3 a,b,d,f
(60.1)
688.5 a,b,c,d,f,g
(88.8)
10.2 a,b,d,f,g,h
(1.9)
48.3 a,b,c,d,f,g,h,i,j
(7.0)
4.7 a,b,c,d,e,f,g
(0.5)
Brilliant CriosBC22.7 a,b,d,f
(0.5)
438.5 a,b,d,f
(40.4)
689.5 a,b,c,d,f,g
(40.0)
10.0 a,b,d,f,h
(1.6)
44.1 a–k
(2.1)
4.9 a,b,c,d,e,f,g
(0.3)
EsteliteEL19.4 c,d,e,g,h,j,k
(0.7)
602.8 c,e,g,h,k
(47.9)
940.2 a,b,c,d,e,f,g,h,j,k
(66.8)
13.9 c,f,g
(1.5)
45.2 a–k
(1.6)
4.5 a,b,c,d,e,f,g,j
(0.3)
Block HCBL22.1 a,b,c,d,f,g
(0.7)
457.3 a,b,d,f,g,h
(27.4)
724.0 a,b,c,d,f,g
(46.1)
10.2 a,b,d,f,g,h
(0.6)
48.5 a,b,c,d,f,g,h,i,j
(0.7)
4.5 a,b,c,d,e,f,g,h,j
(0.2)
Katana AvenciaKA23.0 a,b,d,f
(1.4)
410.8 a,b,d,f
(55.8)
666.5 a,b,c,d,f,g
(88.2)
8.8 a,b,d,f
(1.4)
50.0 a,b,c,d,f,g,h,i
(2.3)
5.0 a,b,c,d,e,f,g
(0.2)
KZR CADKC19.7 c,d,e,g,j,k
(1.6)
584.0 c,d,e,g,j,k
(45.1)
920.5 a,b,c,d,e,f,g,h,j,k
(141.6)
13.5 a,c,d,g,h
(0.6)
45.6 a–k
(7.4)
5.1 a,b,c,d,e,f,g
(0.4)
ExperimentalEX18.7 c,e,g,h,j,k
(0.1)
694.7 c,e,g,h,j,k
(8.5)
1034.5 c,e,g,h,j,k
(12.3)
17.8 e,j,k
(0.3)
40.5 b,c,e,g,j,k
(0.3)
4.8 a,b,c,d,e,f,g
(0.4)
Lava UltimateLU19.1 c,e,g,h,j,k
(3.3)
588.3 c,d,e,g,h,k
(122.6)
1008.7 c,e,g,h,j,k
(331.2)
12.2 a,b,c,d,g,h
(2.2)
50.4 a,b,c,d,f,g,h,i
(4.3)
3.8 d,h,i,j,k
(0.4)
Grandio blocGB17.4 c,e,g,h,j,k
(0.8)
771.2 e,j,k
(73.7)
1184.8 c,e,g,h,j,k
(107.8)
18.4 e,j,k
(2.0)
42.7 a,b,c,d,e,g,i,j,k
(1.5)
4.0 c,d,h,j,k
(0.2)
VOCO ExperimentalVO18.7 c,e,g,h,j,k
(0.3)
692.0 c,e,g,h,j,k
(212.0)
1036.8 c,e,g,h,j,k
(32.3)
17.5 e,j,k
(0.8)
40.2 b,c,e,g,j,k
(0.5)
3.8 h,i,j,k
(0.2)
Vita EnamicVE13.9
(0.7)
1143.3
(124.7)
1834.2
(198.0)
25.3
(3.0)
49.2 a,b,c,d,f,g,h,i,j
(0.7)
3.2 h,i,k
(0.1)
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Rosentritt, M.; Hahnel, S.; Schneider-Feyrer, S.; Strasser, T.; Schmid, A. Martens Hardness of CAD/CAM Resin-Based Composites. Appl. Sci. 2022, 12, 7698. https://doi.org/10.3390/app12157698

AMA Style

Rosentritt M, Hahnel S, Schneider-Feyrer S, Strasser T, Schmid A. Martens Hardness of CAD/CAM Resin-Based Composites. Applied Sciences. 2022; 12(15):7698. https://doi.org/10.3390/app12157698

Chicago/Turabian Style

Rosentritt, Martin, Sebastian Hahnel, Sibylle Schneider-Feyrer, Thomas Strasser, and Alois Schmid. 2022. "Martens Hardness of CAD/CAM Resin-Based Composites" Applied Sciences 12, no. 15: 7698. https://doi.org/10.3390/app12157698

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