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厚度对两种大块充填和一种传统后牙树脂基复合材料在高辐照度和高时间分辨率下的固化程度的影响。

Effect of thickness on the degree of conversion of two bulk-fill and one conventional posterior resin-based composites at high irradiance and high temporal resolution.

作者信息

Labrie Daniel, Price Richard B, Sullivan Braden, Salazar Austyn M, Gautam Dixa, Stansbury Jeffrey W, Ferracane Jack L

机构信息

Department of Physics and Atmospheric Science, Dalhousie University, Halifax, Nova Scotia, B3H 4R2, Canada.

Department of Dental Clinical Sciences, Dalhousie University, Halifax, Nova Scotia, B3H 4R2, Canada.

出版信息

J Mech Behav Biomed Mater. 2022 Dec;136:105489. doi: 10.1016/j.jmbbm.2022.105489. Epub 2022 Oct 1.

Abstract

OBJECTIVES

This study: 1) measures the effect of sample thickness and high irradiance on the depth-dependent time delay before photopolymerization reaction onset; 2) determines if exposure reciprocity exists; 3) measures the conversion rate at four irradiance levels; 4) determines the time, t, at which the maximum DC rate is reached for two bulk-fill and one conventional posterior resin-based composites (RBCs).

METHODS

Tetric PowerFill IVA shade (Ivoclar Vivadent) and Aura bulk-fill ultra universal restorative (SDI), and one conventional posterior resin-based composite (RBC), Heliomolar A3 (Ivoclar Vivadent), that were either 0.2 mm, 2 mm, or 4 mm thick were photocured using a modified Bluephase G4 (Ivoclar Vivadent) light-curing unit (LCU) that delivered a single emission band (wavelength centered at 449 nm). The same radiant exposure of 24 J/cm was delivered at irradiances ranging from 0.5 to 3 W/cm by adjusting the exposure time. PowerFill was also photocured for 3 s or 6 s using a Bluephase PowerCure LCU (Ivoclar Vivadent) on the 3 s mode setting. The degree of conversion (DC) was measured in real-time at a high temporal resolution at 30 °C using Attenuated Total Reflection (ATR) FTIR spectroscopy with a sampling rate of 13 DC data points per second. The DC data were analyzed using a phenomenological autocatalytic model. The RBC viscosity was measured at 21 °C and 30 °C. Light transmission through the RBC samples at 22 °C was monitored with time to calculate the extinction coefficients of the RBCs.

RESULTS

The time delay before photopolymerization started increased as the RBC thickness increased and the irradiance decreased. An autocatalytic model described the DC data. The time t was less than 77 ms for the 0.2 mm thick samples of PowerFill irradiated using the highest irradiance of 3 W/cm. Among the three RBCs for each sample thickness and irradiance level, the PowerFill had the smallest time t. There was a time delay of 0.59 s and 1.25 s before the DC started to increase at the bottom of 4 mm thick samples for the PowerFill and Aura, respectively, when an irradiance of 1 W/cm was delivered. The time delay increased to 3.65 s for the Aura when an irradiance of 0.5 W/cm was delivered. The extinction coefficients near 449 nm were 0.78 mm, 0.76 mm, and 1.55 mm during the first 2 s after the start of photocuring of PowerFill, Aura, and Heliomolar, respectively. Only PowerFill followed exposure reciprocity. At T = 30 °C, the viscosity was 3400, 17000, and 5200 Paˑs for PowerFill, Aura, and Heliomolar, respectively.

SIGNIFICANCE

The time delay between when photopolymerization starts at the top and bottom of 2- or 4-mm thick RBC restorations may affect the structural integrity of the bond between the tooth and the bottom of the restoration. Only PowerFill followed exposure reciprocity between irradiance levels of 0.5 to 3 W/cm. Exposure reciprocity did not occur for Aura or Heliomolar, neither of which are optimized for short light exposure or high irradiance conditions.

摘要

目的

本研究:1)测量样本厚度和高辐照度对光聚合反应开始前深度相关时间延迟的影响;2)确定曝光互易性是否存在;3)测量四个辐照度水平下的转化率;4)确定两种大块充填和一种传统后牙树脂基复合材料(RBC)达到最大转化率(DC)的时间t。

方法

使用改良的Bluephase G4(义获嘉伟瓦登特公司)光固化机对厚度为0.2mm、2mm或4mm的Tetric PowerFill IVA色号(义获嘉伟瓦登特公司)、Aura大块充填超通用修复材料(SDI公司)以及一种传统后牙树脂基复合材料Heliomolar A3(义获嘉伟瓦登特公司)进行光固化,该光固化机发出单一发射带(波长以449nm为中心)。通过调整曝光时间,在0.5至3W/cm²的辐照度下提供相同的24J/cm²的辐射曝光量。PowerFill还使用Bluephase PowerCure光固化机(义获嘉伟瓦登特公司)在3s模式设置下进行3s或6s的光固化。使用衰减全反射(ATR)傅里叶变换红外光谱法,在30°C下以高时间分辨率实时测量转化率(DC),采样率为每秒13个DC数据点。使用现象学自催化模型分析DC数据。在21°C和30°C下测量RBC的粘度。在22°C下监测RBC样本的光透过率随时间的变化,以计算RBC的消光系数。

结果

光聚合开始前的时间延迟随着RBC厚度增加和辐照度降低而增加。一个自催化模型描述了DC数据。对于使用3W/cm²最高辐照度照射的0.2mm厚的PowerFill样本,时间t小于77ms。在每个样本厚度和辐照度水平的三种RBC中,PowerFill的时间t最小。当提供1W/cm²的辐照度时,在4mm厚样本底部,PowerFill和Aura的DC开始增加之前分别有0.59s和1.25s的时间延迟。当提供0.5W/cm²的辐照度时,Aura的时间延迟增加到3.65s。在PowerFill、Aura和Heliomolar光固化开始后的前2s内,449nm附近的消光系数分别为0.78mm、0.76mm和1.55mm。只有PowerFill遵循曝光互易性。在T = 30°C时,PowerFill、Aura和Heliomolar的粘度分别为3400、17000和5200Pa·s。

意义

2mm或4mm厚的RBC修复体顶部和底部光聚合开始之间的时间延迟可能会影响牙齿与修复体底部之间粘结的结构完整性。只有PowerFill在0.5至3W/cm²的辐照度水平之间遵循曝光互易性。Aura或Heliomolar不存在曝光互易性,这两种材料均未针对短时间光照或高辐照度条件进行优化。

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