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通过不同厚度牙釉质片对氚标记水的清除来测量人牙釉质中的水及其扩散交换。

The water in human dental enamel and its diffusional exchange measured by clearance of tritiated water from enamel slabs of varying thickness.

作者信息

Dibdin G H

机构信息

MRC Dental Group, University of Bristol Dental School, UK.

出版信息

Caries Res. 1993;27(2):81-6. doi: 10.1159/000261522.

Abstract

Tracer clearance studies were used to measure the amount and mobility of the water in human dental enamel. Slabs of enamel whose thickness ranged from 0.4 to 0.8 mm were equilibrated with tritiated water in dilute neutral buffer at 35 degrees C for 1 week, rinsed, and allowed to exchange at the same temperature with stirred unlabelled buffer. This was sampled and counted periodically to allow calculation of diffusion coefficients from the clearance rate. Exchangeable water amounted to 2.0 +/- 0.4% w/w (6.0 +/- 1.2% v/v). Some samples were masked on one side to double the diffusion distance. Diffusion calculations assuming homogeneous diffusion gave anomalous coefficients varying with sample thickness, indicating a more complex system was involved. In contrast, analysis assuming a biphasic distribution of diffusion pathways was much more successful. This assumed slow exchange from an inner pore system 'A' (probably associated with the prism cores) followed by much faster diffusion along a minority of larger pores 'B', such as exist at the prism boundaries. The 'B' pore-volumes were based on past studies of porosity in enamel, and the 'A' volumes on this work. Analysis gave an overall effective diffusion coefficient (De) for thick samples of 4.3 x 10(-7) cm2 s-1. The results were consistent with a DB of 0.9 x 10(-5) cm2 s-1 and a rate-constant (kAB) for exchange between the two pore systems which, if operating over a half-prism width (say 2 microns) would correspond to an 'inner' (DAB) diffusion coefficient in the region of 6 x 10(-12) cm2 s-1.

摘要

示踪剂清除研究用于测量人牙釉质中水的含量和流动性。厚度在0.4至0.8毫米之间的牙釉质薄片在35摄氏度的稀中性缓冲液中与氚化水平衡1周,冲洗后,在相同温度下与搅拌的未标记缓冲液进行交换。定期对其进行采样和计数,以便根据清除率计算扩散系数。可交换水含量为2.0±0.4% w/w(6.0±1.2% v/v)。一些样品的一侧进行了遮蔽,以使扩散距离加倍。假设均匀扩散进行的扩散计算得出的异常系数随样品厚度而变化,这表明涉及到一个更复杂的系统。相比之下,假设扩散途径呈双相分布的分析更为成功。这假定从内部孔隙系统“A”(可能与棱柱核心相关)进行缓慢交换,随后沿着少数较大孔隙“B”(如棱柱边界处存在的孔隙)进行快得多的扩散。“B”孔隙体积基于以往对牙釉质孔隙率的研究,“A”体积基于本研究。分析得出厚样品的总体有效扩散系数(De)为4.3×10⁻⁷平方厘米每秒。结果与DB为0.9×10⁻⁵平方厘米每秒以及两个孔隙系统之间交换的速率常数(kAB)一致,如果在半棱柱宽度(例如2微米)上起作用,该速率常数将对应于6×10⁻¹²平方厘米每秒区域内的“内部”(DAB)扩散系数。

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