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This is an open access journal, and articles are distributed under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike 4.0 License, which allows others to remix, tweak, and build upon the work non-commercially, as long as appropriate credit is given and the new creations are licensed under the identical terms.
Light curing of resin composite is associated with a thermal rise that may have harmful effect on the health of the vital pulp. In addition, desirable polymerization is important to achieve mechanical properties and clinical function. The purpose of this in-vitro study was to compare the thermal rise under normal dentin during photopolymerization and degree of conversion (DC) of bulk fill and conventional resin composite using continuous high- and soft-start mode.
In this in-vitro study, Cl I cavities with a dimension of 4 mm × 4 mm × 4 mm and remaining dentin thickness of 1 mm were prepared on 56 extracted human molars. The temperature rise during the light curing of conventional resin composite (Tetric N Ceram, Ivoclar Vivadent) by incremental filling technique and bulk-fill resin composite (Tetric N Ceram Bulk Fill, Ivoclar Vivadent) by bulk-filling technique were measured with a K-type thermocouple wire. DC of both resin composites was measured using Fourier-transform infrared spectroscopy. Data were analyzed using one-way ANOVA, Tamhane and Duncan post hoc, two-way ANOVA at the significance level of α = 0.05.
Photopolymerization temperature rise due to soft start mode and the first layer of conventional composite was higher than continuous high mode and bulk-filling technique, respectively (P < 0.001). DC of conventional resin composite was higher than bulk-fill composite (P < 0.001).
Soft-start mode produced higher thermal rise than continuous high mode and conventional resin composite showed higher DC than bulk-fill composite.
It is necessary to place several resin composite layers and light cure each layer separately (the incremental technique) to restore deep cavities with the use of conventional resin composites. Therefore, the incremental resin composite technique is a time-consuming procedure. To overcome such a problem, a different type of resin composite has been introduced, which is called bulk-fill resin composite. The unique advantages of this type of resin composite are the feasibility of placing it in 4-mm thick pieces and polymerize these pieces in one step. These resin composites are composed of modified monomers and fillers that have a high capability to conduct light.
One rationale for limiting the thickness of the layers to 2 mm in conventional resin composites is to allow adequate light to penetrate into the material for initiation and completion of polymerization, convert maximum amount of monomers to polymer, and increase the degree of conversion (DC), which affects the mechanical and clinical properties of resin composites.
Light curing of resin composites might exert thermal stresses on the tooth pulp.
Given the clear advantage of bulk-fill resin composites in saving time and costs, it appears it is necessary to evaluate thermal changes resulting from photopolymerization and the heat transferred to the pulp and also to determine DC as a parameter affecting the mechanical properties and biocompatibility of these resin composites. Therefore, the aim of the present study was to evaluate thermal changes, due to polymerization, beyond dentin and DC of two types of bulk fill and conventional resin composites using soft start and continuous high light-curing mode.
Specimen preparation
A total of 56 sound human third molar teeth were used for the purpose of this in-vitro study. The teeth were stored in distilled water up to the day before the study. First, the occlusal surfaces of the teeth were made flat with the use of a disc to achieve better adaptation of the light-curing unit. Then, a Class I cavity, measuring 4 mm in mesiodistal and buccolingual dimensions and in depth, was prepared with the use of a cylindrical diamond bur (tizkavan, Iran). Then, the tooth crowns were removed at a distance of 5 mm from the flattered occlusal surface.
The samples were divided into four study groups (n = 14) in terms of the resin composite type and light-curing mode as follows
Schematic of study groups in terms of the resin composite type and light.curing mode
Measurement of temperature rise
First, the temperature rise resulting from the light-curing procedure
In the conventional resin composite group
In the bulk-fill resin composite group
The increases in temperature in all the samples were determined in an environment with identical temperature. The temperature rise was determined every second for 250 s since the initiation of photopolymerization.
Measurement of the degree of conversion
To determine the DC of the samples, Fourier-transform infrared spectroscopy was carried out at a resolution of 4/cm and 25 scans at a range of 400-'4000/cm. After the thermal change tests, the samples were stored at 37°C for 24 h. Then, the light-curing resin composite samples (n = 6) were retrieved from the teeth, milled and powdered with a mortar and pestle.
Statistical analysis
ANOVA was used to compare the study groups in terms of thermal changes, due to the heterogeneity of variances, followed by post-hoc Tamhane tests. To compare DC after making sure of the normal distribution of data, one-way ANOVA was used for the analysis of data, followed by post-hoc Duncan test. Two-way ANOVA was used to evaluate the effect of light-curing mode and resin composite type on DC. Statistical significance was set at P < 0.05.
There were no significant differences in the DC of the conventional and bulk-fill resin composites between the two light-curing modes. However, DC was significantly different between the two resin composite types
Two-way ANOVA showed that when DC was compared, the cumulative effect of light-curing mode and resin composite type was not significant. The effect of light-curing mode on DC was not statistically significant (P = 0.144); however, the effect of the resin composite type was statistically significant (P < 0.001).
Since the temperature increases after the imitation of photopolymerization of resin composite, resulting in injuries to the dental tissues, the present study was conducted to provide laboratory data on thermal changes within resin composite and the pulp chamber during photopolymerization. In addition, the effect of composite placement technique (the incremental technique vs. bulk-fill technique) on the temperature rise was evaluated with the use of soft start and continuous high light-curing mode.
This explorative, experimental, in-vitro study was done at room temperature (25°C ± 2°C). Jafarzadeh-Kashi mentioned that the bonding agents might be cured more efficiently at human body temperature than at room temperature, although the Scotchbond MP was not significantly affected by the temperature.
Based on the results of the present study, soft-start light-curing mode resulted in a greater temperature rise, which might be due to the greater energy of this mode compared to the continuous high mode. Based on the results of studies by Looney and Price, the differences in the energy produced by light-cured devices are an important factor for differences in temperature increase with the use of different light-curing modes. Lower energies delivered by light-curing modes will result in less temperature rise.
In the present study, the mean ΔT
dwas significantly higher than the mean ΔT
twith the use of both light-curing modes. In a study by Aguiar et al., too, the mean temperature rise in all the groups without resin composites was higher than that in resin composite groups with all the three thicknesses of dentin, consistent with the results of the present study.
While Lloyd and Hansen and Asmussen reported that the curing process of resin composite creates heat and
A comparison of ΔT tvalues showed that the ΔT tvalue of the first layer of conventional resin composite was higher than that of bulk-fill resin composite. Higher ΔT tvalue might be attributed to the thickness of conventional resin composite (2 mm) compared to that of bulk-fill resin composite (4 mm).
Garoushi et al. showed that an increase in the thickness of bulk-fill resin composite from 1 mm to 4 mm resulted in a significant decrease in the penetration of light.
In contrast to the results of the present study, in a study by Kim et al., the temperature rise resulting from a 20-s irradiation of bulk-fill resin composite was higher than that of the first layer of conventional resin composite,
In the present study, in order to simulate the clinical situation, the second layer of conventional resin composite was placed immediately after light curing of the first layer before the temperature returned to normal after light curing the first layer. However, the temperature rise resulting from photopolymerization of the second layer with the use of both light-curing modes was not higher than that of the first layer and the temperature during photopolymerization of the second layer occurred more slowly, and the peak of thermal changes was less than that of the first layer, consistent with the results of a study by Kim et al.
In addition, in the present study, the resin composite placement technique (incremental or layering technique vs. bulkfill) affected DC, but light-curing mode did not show such an effect.
In the incremental technique, resin composite receives higher total energy. Each 2-mm thick layer receives 12 j/cm
2and 13.5 j/cm
2energy with the continuous high- and soft-start light-curing modes, respectively, while with the bulk-fill technique, this amount of energy should cure the whole mass of resin composite with 4-mm thickness. Therefore, the amount of light penetrating the 4-mm thickness decreases, resulting in a decrease in DC. The results of the present study were consistent with those of a study by Chang et al.
Although DC of bulk-fill resin composite was less than that of conventional resin composite, it was at the accep[table 55]% level,
The bulk-fill resin composite used in the present study had hybrid particles. In this context, an increase in filler size results in a decrease in the specific surface area between the filler and the organic matrix, decreasing light scattering and increasing the curing depth.
The temperature rise resulting from the irradiation of the remaining dentin was higher than the final heat of polymerization with the use of both Tetric N-Ceram bulk fill and Tetric N-Ceram conventional resin composites The temperature rise with the use of soft-start light-curing mode was higher than that of continuous high light-curing mode The temperature rise resulting from light curing of the first layer of Tetric N-Ceram resin composite was higher than that of Tetric N-Ceramic bulk-fill resin composite The DC of Tetric N-Ceram resin composite was significantly higher than that of Tetric N-Ceram bulk-fill resin composite The temperature rise and DC are directly correlated with the energy density of the light-curing unit.
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Conflicts of interest
The authors of this manuscript declare that they have no conflicts of interest, real or perceived, financial or non-financial in this article.