Key words:
Abrasion - atomic force microscopy - dental materials - Fourier transform infrared
- surface roughness
Introduction
Wear refers to the progressive loss of material from the surface of teeth or restorative
materials as a result of chemical and mechanical processes such as erosion and abrasion.[1] Within the context of the oral cavity, wear is a complex phenomenon. Wear by toothbrushing
falls into the category of the three-body wear and is most commonly observed on facial
surfaces of teeth and dental restorations.[2] Resistance to abrasive wear is an important property of a dental material. It determines
the longevity of the material in clinical service.[3] Surface roughness has a major influence on the esthetic appearance and discoloration
of restorations. Microorganisms adhere strongly to rough surfaces, thereby promoting
plaque accumulation, caries, and gingival inflammation.[4] Ideal dental restorations should have wear resistance similar to that of tooth.[5] However, till date, wear in composites remains a major concern. The values of average
clinical wear on occlusal surfaces of composite restorations approximates to about
29 μm per year for molars and 15 μm for premolars. Substantially higher values are
reported for proximal wear.[6]
Considerable improvements have been made in terms of mechanical properties of dental
composite resins.[7] Several aspects of the composition and structure of composite resins directly affect
and limit wear resistance.[8] There is a paradigm shift in restorative dentistry with the synthesis of new polymeric
systems and the introduction of the inorganic nanofillers.[9]
[10] Manufacturers usually make unsubstantiated claims about the wear resistance of the
composite resins. To test manufacturer’s claims, an in vitro test method was adopted to evaluate mass loss and surface roughness.[11] In vivo methodologies are generally very time-consuming and hard to accurately reproduce.[12] Therefore, for the present study, an in vitro testing method was employed. The objective of this study was 2-fold, one was to assess
the different types of commercially available composites and compomer materials -
based on surface properties such as structural changes, microhardness, and corresponding
wear resistance. The second was to compare the methodologies used for assessing wear
resistance.
Materials and Methods
In this study, five different types of commercially available materials microhybrid
[FiltekTM Z250 XT, 3M ESPE, Germany], nanocomposites [FiltekTM Z350 XT, 3M ESPE, Germany], packable [QuiXfil, Dentsply, Germany], flowable [Surefull
SDR, Dentsply, Germany], and compomer [Dyract® XP, Dentsply, Germany1 were selected
and their composition is given in [Table 1].
Table 1:
Composition of commercial restorative materials
|
Product name
|
Type
|
Manufacturer
|
Lot
|
Fillers
|
Filler volume (%)
|
Monomers*
|
|
SDR: Smart dentin replacement, Bis-GMA: Bisphenol A glycidylmethacrylate, UDMA: Urethane
dimethacrylate, TEGDMA: Triethylene glycol dimethacrylate, Bis-EMA: Ethoxylated bisphenol-A
dimethacrylate, PEGDMA: Poly (ethylene glycol) dimethacrylate, TCB: Tetracarboxylic
acid-hydroxyethylmethacrylate-ester, TMPTMA: Trimethylolpropane trimethacrylate
|
|
FiltekTM Z250 XT (Z250)
|
Universal microhybrid composite
|
3M ESPE, Germany
|
N703519
|
Zirconia/silica particle size range 0.01-3.5 μm
|
50
|
Bis-GMA, UDMA, Bis-EMA
|
|
FiltekTM Z350 XT (Z350)
|
Nano-composite
|
3M ESPE, Germany
|
N660853
|
Combination of 0.004-0.02 μm nonagglomerated zirconia/silica particles and agglomerated
0.60.1.40 μm clusters
|
57
|
Bi-GMA, UDMA TEGDMA, PEGDMA, Bis-EMA
|
|
QuiXfil (QFL)
|
Fast-setting, packable composite
|
Dentsply, Germany
|
1503000064
|
Strontium glass fractions in two sets ranging from particle size 1.4 μm
|
66
|
Bis-EMA, UDMA, TCB TEGDMA, TMPTMA
|
|
Surefil SDR
|
Low viscosity, flowable composite
|
Dentsply, Germany
|
1503000686
|
Nano-filled Ba/Si alumino fluorosilicate
|
45
|
UDMA, TEGDMA
|
|
Dyract® XP (Dyract)
|
Compomer
|
Dentsply, Germany
|
1502000426
|
Strontium-flouro silicate glass mean filler size 0.8 μm
|
47
|
UDMA, TCB
|
Sample preparation
Samples with 10 mm x 2 mm dimension were prepared in Teflon mold for each material.
Specimens were prepared in a single insertion and compacted using glass slides on
both sides. Samples were thoroughly cured from both sides with 4000 mW/cm2 irradiance for 60s from each side (Flash Max P4 Ortho, Colorado, USA 1503078). The
samples were polished by carefully trimming any excess with a 1200-grit silicon carbide
sheets and using an automatic polishing machine (Metkon GRIPO 2V Grinder Polisher,
Turkey), followed by sonication to remove residue of polishing. Afterward, each specimen
was conditioned in distilled water for 7 days at 37°C, according to the conditioning
described for abrasive wear test IS0/TR 14569. The samples were then air-dried for
an hour. Readings for all tests were recorded before and following the abrasive wear
test.
Fourier-transform infrared spectroscopy
To find the structural changes, spectroscopic analysis of all samples was conducted
before and after treatment. For each sample before and after treatment, 10 spectra
were taken to find out the spectral difference. Thermo Nicolet 6700 (USA) was used
with attenuated total reflectance as accessory. The resolution was 8 cm-1 with 256 scan number. The spectral range was 4000-600 cm-1. OMNIC software (Thermo Fisher Scientific wissenschaftliche Geräte GmbH, Austria)was
used to analyze the spectra.
Principal component and cluster analysis
Chemometric methods were used to quantify the spectral differences of various composite
groups, i.e., untreated Dyract, untreated QFL, untreated SDR (US), untreated Z250
(U2), untreated Z350 (U3), treated Dyract, treated QFL, treated SDR (TS), treated
Z250 (T2), and treated Z350 (T3). These methods were performed using Unscrambler X
10.2 software, purchased from Camo software (Oslo, Norway). Preprocessing comprised
of baseline correction and unit vector normalization. Cluster analysis (CA) was performed
over complete spectral range by Ward’s method using squared Euclidean distance.
Microhardness testing
For a comparison of selected materials before and after simulated toothbrushing, microhardness
was analyzed in terms of Vickers hardness number. Using a 200 g load with 10s dwell
time (Microhardness tester, WOLPERT, 401MVD EQPT 0002, Germany). Six samples from
each group were used and each specimen was indented three times at three different
points, and then the mean reading was recorded.
Weight analysis
Before the abrasive test, samples were weighed using an analytical electronic balance
(Sartorius AG Gottingen BP 110 S, Germany) with accuracy up to 0.1 mg. In this way,
initial mass (M1), for each sample was obtained. Following the abrasive wear test, the samples were
carefully removed, rinsed in tap water, and placed in an ultrasonic water bath (Cole-Parmer,
Vernon Hills, Illinois, USA) for 1 min. The samples were then individually removed,
air-dried, and weighed. In this way, final mass (M2) was obtained for each sample and mass loss (%) was reported for each material post
abrasion using following equation:
Surface roughness analysis
Initial surface roughness was assessed using a noncontact mode 2D Profilometer (PS-50
Nanovea, Russia) and using a 3D-Atomic Force Microscope (AFM SPM-9500J3, Shimadzu
Corp, Japan), operating in tapping mode. Micrographs were obtained at different scan
areas measuring 20 x 20 μm using AFM software (SPM-Offline Shimadzu Corp. Japan).
The roughness average, Ra, is the most widely used one-dimensional (1D) roughness
parameter, and it denotes the arithmetic mean of the absolute values of the collected
roughness data points. Rai (initial values) were taken and means were obtained. Surface roughness (Raf) was measured after the abrasion wear test in the same way as for initial values,
except that the tracing arm of profilometer and tip of AFM were positioned in such
a way that the tracing direction was perpendicular to the direction of tooth brushing
action. 3D images were reported in area selection of 10 μm x 10 μm.
Abrasive wear test
For the abrasive wear test, a custom-made toothbrush simulator was constructed in
accordance with IS011609: 2010, equipped with six stations of replaceable brush heads
(Oral B Flat end). Tooth brushing load of 1.5 N was set. To mimic the original condition
of toothpaste (Colgate-Palmolive, Dublin, Ireland), slurry was made with distilled
water in the proportion 1:2. Resin-based samples were mounted in impression compound
and placed in metallic stations. Toothbrushing was accomplished with horizontal movements
of toothbrush and travelled a course of 4.2 cm. Time duration was kept 100 min amounting
to about 12,250 strokes was set. Toothbrushing time of 1.3 years was simulated. With
these parameters, a minimum weight loss of 2 mg by reference material, as described
in IS0/TR 14569, was achieved. The slurry and brush heads were replaced for each sample.
Data analysis
The data were submitted to the analysis of variance (ANOVA) and post hoc Tuckey’s Test, using IBM SPSS statistics version 21, Boston, Massachusetts, USA.
The Pearson’s test was used to verify the correlation between Roughness averages reported
by AFM and Profilometer. In addition, the correlation of roughness alteration with
filler volume and microhardness was also determined.
Results
Fourier-transform infrared spectroscopy
Fourier-transform infrared (FTIR) spectra of samples (Z250, Z350, QFL, SDR, and Dyract)
were collected before and after treatment as shown in [Figure 1a-e].
Figure 1:Comparative Fourier-transform infrared spectra of treated and untreated restorative
materials; (a) Z250, (b) Z350, (c) QFL, (d) SDR, and (e) Dyract
The spectra of untreated samples showed C = O stretching vibration peaks at 1710-1715
cm-1, peak at 1653 cm-1 and 1633 cm-1 attributed to C-C symmetric stretching appeared in all samples except SDR as aromatic
group is not present in this composite. Peak at 1510 cm-1 corresponded to N-H bending vibrations of urethane-based resins. C-H bend was observed
at 1462 cm-1. The overlapping peaks at around 1250-900 cm-1 were due to asymmetric stretching vibration of C-O-C of monomer structure. Another
sharp peak at 771 cm-1 was due to C-H vibrations. After treatment, changes in peak intensities were observed
for all samples specifically at C = O and N-H groups.
Principal component analysis
Principal component analysis (PCA) was performed and a comparison (spectral range;
700-3100 cm-1) was conducted between various treated and untreated dental composites as shown in
[Figure 2]. Different comparative spectral ranges, 1660-1760 cm-1, 1590-1650 cm-1, 1420-1470 cm-1, and 820-1220 cm-1 are given in [Figure 3a-d], respectively. Complete spectral range displayed favorable separation of treated
and untreated dental composites; PC1 separated all composites from TS with 97% variance,
whereas the remaining 2% was observed in PC2 and 1% in PC3 (figure not shown). All
samples have shown distinct cluster formations to be recognizable as one group; however,
US and T3 have demonstrated scattered formations hence suggesting inner group variability
[Figure 2].
Figure 2:Principal component analysis of all treated and untreated composites over the complete
spectral range
Figure 3:Principal component analysis of all treated and untreated composites over (a) 1660–1760
cm-1, (b) 1590–1650 cm-1, (c) 1420–1470 cm-1, and (d) 820–1220 cm-1 region
Similar trends were observed at 1660-1760 cm-1 region; however, the variance observed by PC1 was improved to 98% and the remaining
2% was detected by PC2. Within the treated and untreated composites, the sample groups
can be well discriminated using PCA, whereas US and T3 showed variations within their
respective groups [Figure 3].
By comparison, differences within the treated and untreated groups appeared to be
much greater in the 1590-1650 cm-1 region, and the scores plot for this region showed good separation between all groups,
i.e., 99% for PC1. While the clusters were more widely spread, loading plots for PC1
and PC2 (data not shown) suggested the contrast in the peaks at this region to be
a major influence. Within the treated and untreated samples at 1420-1470 cm-1 region, the sample groups can be well discriminated using PCA. PC1 and PC2, accounting
for 100% of the variance, discriminated all samples on the basis of their chemical
content. The distribution of individual composite type in relation to the variance
explained by PC1 produced clear and separated clusters for each of these samples.
PCA between treated and untreated samples at 820-1220 cm-1 region showed that the variance explained by PC2 separated T2, U2, T3, and U3 from
all other composite types, whereas PC1 distributed TS away from the others. Every
composite type formed a separate cluster with the exception of US and T3 where PC1
demonstrated 98% variance and PC2 2% variance.
Cluster analysis
CA was performed over the complete spectral range (700-3100 cm-1). [Figure 4a] showed the dendrogram of classification results for a dataset comprising of spectra
collected from all untreated dental composites. Two distinct branches are formed where
Z250 and Z350 were grouped together, whereas SDR, QFL, and Dyract have clustered separately.
Altogether, each of the different composites formed well-defined clusters; however,
SDR represented maximum relative distance hence suggesting most inner group variability.
[Figure 4b] showed the dendrogram of classification results for a dataset comprising of spectra
collected from all treated dental composites.
Figure 4:Component analysis of all (a) untreated and (b) treated samples over the complete
spectral range
Two distinct branches are formed where SDR was clearly separated from the remaining
treated composites. All sub-branches purely contained specific composite types with
no one mixing with the other hence complementing the sensitivity of the technique.
Dyract and Z350 demonstrated inner group variability of treated composites on the
basis of maximum relative distance as compared to the rest.
Hardness testing
Comparison of microhardness among treated and untreated composite materials is tabulated
in [Table 2]. Dyract and QFL showed highest and lowest change, respectively, in microhardness
compared to all the composite materials tested. A statistically significant change
in microhardness was found between the groups after simulated toothbrushing (P > 0.05) by one-way ANOVA. Post hoc Tukey’s test showed a significant difference between change in hardness of Dyract
and QFL as well as Z350. There was also a significant difference between the results
of QFL and SDR (P > 0.05). In the context of wear, all tested materials suffered significant mass loss
(P < 0.05). Percentage mass loss of each material is graphically depicted in [Figure 5]. The maximum mass loss was observed in Z250 while Dyract showed the lowest mass
loss. The mass loss observed in the case of SDR was significantly higher than the
other tested composite materials (P < 0.01).
Table 2:
Comparison of microhardness among the tested materials
|
Material
|
Mean microhardness (VHN)
|
|
VHN: Vickers hardness number, SDR: Smart dentin replacement
|
|
Dyract XP
|
103.1±17.04
|
|
FiltekTM Z250
|
92.93±11.21
|
|
FiltekTM Z350
|
109.06±22.86
|
|
QuiXfil
|
100.3±13.73
|
|
Surefil (SDR)
|
84.46±7.75
|
Figure 5:Average weight loss percentages of samples after treatment
Surface roughness
Initially, all tested materials presented relatively low values of surface roughness,
as polishing of all samples was performed before the abrasion test. However, as expected
toothbrush abrasion caused visible nanoscale alterations on the surface of all samples,
varying in extent, according to material as illustrated by 3D pre- and postabrasion
test images obtained with the help of AFM [Figure 6a-e], One-way ANOVA indicated that there was significant difference in the Ra values between the groups (P < 0.05) using both AFM and optical profilometer.
Figure 6:Three-dimensional atomic force microscopy images of restorative materials; (a) Z250,
(b) Z350, (c) QFL, (d) SDR, and (e) Dyract, before (left) and after (right) treatment
The initial and final surface roughness values obtained with AFM and profilometer
are illustrated graphically in [Figure 7a and b], respectively. Following toothbrush abrasion, all tested materials presented a statistically
significant increase in roughness values (P < 0.05). Z25O presented with the highest Raf value after abrasion test and also depicted the highest roughness alteration [Figure 7a and b].
Figure 7:Surface roughness values of restorative materials using (a) atomic force microscopy
and (b) optical profilometer
Dyract suffered highest mass loss the smoothest surface and the lowest Raf value. Two-tailed Pearson’s correlation was used to verify the correlation between
AFM and optical profilometer, and it was found to be highly significant (P < 0.01). In addition, the correlation of roughness alteration (rate of wear) and
microhardness was found to be significant with filler volume (P < 0.05). The correlation between change in microhardness and surface roughness alterations
of the tested materials with both methodologies, however, was not significant (P > 0.01).
Discussion
In recent years, considerable improvements in the properties of dental composites
have been made; however, wear of composite still remains a concern.[6] In this aspect, the surface properties of restorative material play a major role
in the long clinical life of restoration. In the oral cavity, wear is reflected by
tearing away of organic matrix, exposure of inorganic content, and loss of smaller
filler particles due to chewing and due to toothbrushing in our daily life.[13] This surface roughness results in the loss of esthetics and also leads to an increase
in accumulation of dental plaque and lodging of food particles, which coupled with
bacterial adhesion, subsequently results in the destruction of restoration.[14]
In this study, along with the comparison of the wear of latest available materials,
different available methodologies were used to analyze wear and correlation among
these methodologies was found. For composite restorative materials, composition and
filler morphology play a major role in its resistance against wear.[15] The various materials selected for this study varied with respect to aforementioned
variables.
Chemometric aids have demonstrated excellent sensitivity and specificity over the
past two decades in various research areas from biological tissues to synthetic materials.
These algorithms eliminate the chances of interobserver variability and provide true
reflection of the data provided. PCA was chosen as a tool to investigate the spread
of both treated and untreated dental composite groups and inner-group variation with
various spectral regions selected based on the initial differences observed in the
data. Although visual evaluation of the spectra showed similar peaks, each model presented
as a separate cluster in PCA and CA. The clear separation between and within different
dental composites suggested the substantial differences in the biochemical composition.
Distinct characteristics were observed for SDR samples both in terms of inner-group
variability as well as between groups. These results were consistent with the findings
of FTIR data where the absence of C-C symmetric stretching was observed due to lack
of aromatic groups. CA formed on the basis of molecular differences between the dataset
showed separate branches in the dendrogram for each composite type. Both the treated
and untreated revealed further discrete subsets representing each of the five composite
types, and this discrimination suggested a high sensitivity of the technique. CA also
supported the findings related to the absence of aromatic groups by classifying SDR
in a separate branch of the dendrogram both in treated and untreated states.
The general concept is that, by measuring microhardness of material, a better understanding
of the resistance of material against wear can be obtained. The measurement of microhardness
theoretically implies that a hard surface will suffer less abrasive wear than a soft
surface if other factors remain constant. However, previous studies showed controversial
results, where it was reported that no significant interactions between hardness and
wear.[4]
[16]
[17] On the other hand, a significant relationship between hardness and wear has also
been reported by Wang et al.
[18]
Before toothbrushing simulation, SDR showed minimum microhardness values which were
due to low filler content as compared to other composite materials. The results were
in agreement with previous studies.[16]
[17] Z350 (nanocomposite) showed high hardness value compared to Z250 (microhybrid composite)
which might be due to higher filler loading and higher surface area of filler particles,
which have tendency to improve the interfacial linkage between resin-fillers. Postabrasion,
Dyract and SDR presented with the greatest reduction in surface hardness which can
be attributed to lower filler content compared to other materials.[17] For Dyract, this might be due to the surface dissolution on contact with water,
whereas Z350 and QFL presented with an increase in surface hardness after toothbrushing.
This might be attributed to the surface deposition of dentifrice slurry on the surface
of these materials. No change was observed in the surface hardness of Z250. However,
the overall results of the present study did not find any significant correlation
between changes in microhardness and wear resistance (P > 0.05).
Roughness average (Ra) is a well-accepted comparative feature, which quantifies surface
texture by means of randomized readings of amplitude.[19] In most previous studies, Raf was interpreted as the only predictor of roughness and change in surface roughness
which corresponds directly to rate of wear is usually not mentioned. A composite material
with a high Rai will also have a high Raf. The previous studies lacked in reporting the change in surface roughness and compared
the two equipment (profilometer and AFM) on the basis of roughness values (Raf) thus acting as a confounder.
The scale and resolution of the results generated by the profilometer and the AFM
are not comparable. However, the results for each of the five groups being tested
showed a similarity in trends in mutual comparison when it came to increasing Ra for both testing techniques.[4]
[13] The present study showed a significant correlation between the two contrary to a
previous study which showed no correlation between the Ra values obtained using both
techniques.[12]
[16]
Among composite material, QFL showed best results in terms of minimum change in roughness
and final roughness average. Even though QFL showed the smoothest surface, but unlike
compomers, it demonstrated lower mass loss. The mass loss was only more than SDR.
The better wear resistance can be due to the higher filler volume along with better
bonding between the filler and matrix component. The presence of triethylene glycol
dimethacrylate (TEGDMA) can be another reason of better wear resistance as it enhances
the filler-matrix interaction and improves polymerization which reduces the effect
of water sorption.[20]
[21] TEGDMA has a polyether backbone that increase its flexibility,[22] and this may allow better molecular interaction and hence better polymerization.
This results in increased degree of conversion reducing sorption and making the structure
stiffer.
The minimum mass loss was recorded for the SDR, even though it presented with a greater
change in roughness compared to Dyract and QFL. The minimum mass loss might be attributed
to the presence of smaller particles and reduced interparticle spacing resulting in
even distribution that favors the matrix against tearing completely. Greater mass
loss in the case of Dyract and SDR complements the reduction in surface microhardness
of these materials. However, for roughness changes, according to previous studies,
higher filler-loading resulted in greater wear resistance.[23] The presence of lower filler content of flowable composite than packable composites
explained the higher change in roughness. Not only the filler volume but also the
filler-particle size affects the wear resistance.[24] Turssi et al.
[25] suggested that the presence of large particles theoretically cause greater abrasion.
Increase in filler-particle size, causes an increase in the coefficient of friction,
and stress spreads readily from the filler particles to the resin matrix, resulting
in greater wear. In addition, wear affects the surface properties of materials such
as hardness and elastic modulus.[26] This was reflected in the comparison of particle sizes of microhybrid material Z250
and nanocomposites Z350. Due to higher surface area and surface energy, nanosized
particles improve the performance of resin composites.[27]
[28]
On comparing the mass loss of Z350 with Z250, the former showed significantly lower
than latter (P < 0.01). Z350 presented a smoother surface when compared with the Z250.
This was due to the more homogenous distribution and greater volume of filler content
of nanocomposites.[29] Overall, Z250 presented with the greatest mass loss and roughest surface after toothbrush
abrasion test. This was somewhat expected, as when any of the hybrid materials are
subjected to abrasion, the resin between and around the heterogeneous filler-particle
distribution is lost, leading to protruding filler particles. Over time, the entire
filler particles are plucked out creating bumps and craters and a highly roughened
surface.[30] There are a few limitations of this in vitro study; the wear of materials was analyzed in the laboratory set up where oral environment
could not be simulated. This study was limited to abrasive wear. Clinically, toothbrushing
may affect the rate of abrasive wear depending on hardness of bristles and abrasiveness
of dentifrices. The variations and complexity of oral environment may affect the wear
behaviors and clinical performance of restorative materials.
Conclusions
The structure and composition of composites and compomer materials, in particular,
the matrix characteristics, type of filler, and filler-particle size greatly affect
the wear resistance. FTIR along with PCA/CA confirmed structural changes and revealed
information about chemical groups prone to bring change in materials properties. Greatest
mass loss was reported by Z250 while SDR suffered the minimum mass loss. The smoothest
surface was demonstrated by the Dyract while the roughest surface was that of Z250.
AFM and Optical profilometer can be used in tandem for roughness analysis and correlation
between these techniques are highly significant, where AFM offered a higher precision
at a nanoscale level.
Financial support and sponsorship
Nil.