Influence of cavity dimension and restoration methods on the cusp deflection of premolars in composite restoration
Introduction
Recently, posterior composite restoration has become more common because of patients’ increased demand for esthetic restoration, improvement of adhesive dentistry due to the dentin bonding system, and concern about amalgam toxicity.
However, the major drawback of composite restoration is the high polymerization shrinkage of the composite material. It has been reported that linear shrinkage ranges from 0.2 to 2% [1], [2], [3] and that volumetric shrinkage ranges from 0.9 to 5.7% [3], [4], [5], [6], [7], using in vitro measurements.
Polymerization shrinkage can lead to detachment of the restoration from the tooth surface, or may induce enamel microcracks. As a consequence, secondary caries and postoperative hypersensitivity due to bacterial infiltration via microleakage may occur [8], [9]. In addition, when the bond strength between the adhesive and the tooth is strong enough, the tooth structure may experience shrinkage stress, resulting in a cusp deflection [10], [11], [12], [13], [14], [15], [16], [17].
Cusp deflection is the result of interactions between the polymerization shrinkage stress of the composite and the compliance of the cavity wall, and is a common biomechanical phenomenon observed in teeth restored with composites.
In order to measure cusp deflection, many methods have been developed, involving photography [10], microscopy [11], [12], strain gauge [13], [14], interferometery [15] and linear variable differential transformer (LVDT) [13], [16], [17]. Cusp deflection during composite restoration has been reported to be about 10–45 μm, varying according to the measurement method, tooth type and cavity size.
There are two important categories of biomechanical factors that influence cusp deflection. The first category is composed of geometric and material factors, such as cavity width, cavity depth [10], [13], [16], the thickness of remaining tooth material [15], [18], the polymerization shrinkage of the composite [15], flow [19] and the compliance of cured composite and tooth [11], [15]. The second category is comprised of clinical factors, such as use of liner [11], [20], filling technique (bulk cure versus incremental cure) [10], [14], [21], [22], [23], restoration methods (direct versus indirect) [24] and use of a light curing method, which influences the polymerization rate [25], [26].
Hood [18] reported that the remaining cusp after cavity preparation acts as cantilever beams under occlusal load. The prepared cavity floor serves as a fulcrum for cusp bending; the cantilever length is increased with cavity depth. According to mechanical principles, the cusp deflection is proportional to the cantilever length cubed, and to the inverse of the thickness of the cantilever cusp cubed.
Feilzer et al. [27], [28] and Davidson and Feilzer [29] reported that the extent of polymerization shrinkage stress can be influenced by the cavity configuration (C-factor, bonded surface/unbonded free surface). As the C-factor increases, the compensation for polymerization shrinkage by the flow of composite decreases, and thus, the polymerization stress at the bonded surface increases.
Many researchers have suggested an incremental filling technique for composite restoration to reduce polymerization shrinkage stress and cusp deflection [10], [14], [29]. However, controversy remains over whether incremental filling can reduce cusp flexure as compared to bulk filling. Segura and Donly [10] and McCullock and Smith [14] reported that the cusp deflection of incrementally filled teeth was significantly lower than that of bulk filled teeth. However, Versluis et al. [21] and Abbas et al. [22] reported that an incremental filling technique generated more shrinkage stress. In addition, Rees et al. [23] reported that there was no significant difference in cusp flexure between the bulk and incremental placement.
The use of indirect composite inlay restoration has recently begun to increase. Indirect restoration was expected to improve the physical properties of restoration and to result in less shrinkage stress, because bulk polymerization occurs extraorally and the space for resin cement is very thin [24]. However, polymerization shrinkage stress is affected by the cavity configuration as well as the extent of polymerization shrinkage of the composite itself [28]. When the composite inlay is bonded, the high C-factor with few free surfaces cannot compensate for the polymerization shrinkage stress. As a consequence, the remaining stress causes cusp deflection and microcracks in the tooth [30]. Rees and Jacobsen [24] reported a cusp tip movement of 0.2–7.4 μm using composite inlay restoration. However, most studies mentioned above have only reported the measurement values of cusp deflection, with few biomechanical analyses of the factors affecting the cusp deflection.
The purpose of this study was to measure the cusp deflections of premolars restored with composite by bulk filling for four different dimensions of MOD cavities, and to compare the cusp flexure resulting from the bulk filling with that of the incremental filling and indirect composite inlay. This biomechanical analysis of the results provides a guideline for successful composite restoration in clinic.
Section snippets
Instrumentation for a measurement device
The device used for measuring cuspal deflection consists of two XYZ tables (Micro Motion Technology, Bucheon, Korea) with three attached micrometers (Mitutoyo, Kawasaki, Japan) and two LVDT probes (AX-1, Solartron Metrology, West Sussex, UK) (Fig. 1). The LVDT probes are capable of detecting linear changes in a range of ±1 mm with a resolution less than 0.1 μm. The calibration of the probe was adjusted to 10 V/mm (10 mV/μm) of the output voltage using the micrometer.
Cuspal deflection was detected
Results
The representative curves of cusp deflection as a function of time for bulk filling of groups 1–4 are shown in Fig. 3a. The cusp deflections mainly occurred within the initial 1500 s and reached a plateau after 2000 s.
Mean cusp deflection for group 1 was 12.1 μm at 10,000 s and those of groups 2, 3, and 4 were 17.2, 16.2 and 26.4 μm, respectively (Table 2, Fig. 4). The amount of cusp deflection increased as the L3/T3 increased (p < 0.05), and there was no significant difference between groups 2 and 3 (
Discussion
In this study, the change in cusp deflection according to cavity dimension was investigated by altering the width and depth of prepared cavities. Unterbrink and Liebenberg [20] reported that shrinkage stress increases with increasing C-factor, and that the size of the restored cavity acts as an important factor in bulk filling. Hood [18] proposed that the cusps remaining after cavity preparation behave as cantilever beams under occlusal loads. The ideal deformation of a cantilever beam,
Acknowledgement
This investigation was supported in part by a grant (03-PJ1-PG1-CH09-0001) from the Ministry of Health and Welfare of Korea.
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