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微流控设备中的扩散系数测量

Diffusion coefficient measurements in microfluidic devices.

作者信息

Culbertson Christopher T, Jacobson Stephen C, Michael Ramsey J

机构信息

Oak Ridge National Laboratory, Chemical Sciences Division, P.O. Box 2008, Oak Ridge, TN 37831-6142, USA.

出版信息

Talanta. 2002 Feb 11;56(2):365-73. doi: 10.1016/s0039-9140(01)00602-6.

Abstract

Four methods for measuring diffusion coefficients were compared on a microfabricated fluidic device using rhodamine 6G as the analyte. The measurements were made using a static imaging method and three dynamic methods-stopped flow, varying the applied potential (E-field method), and varying the detection length (length method). Under conditions where analyte-wall interactions (adsorption) are minimized, e.g. in a 50/50 (v/v) methanol/aqueous buffer, the stopped flow (2.71+/-0.09x10(-6) cm(2) s(-1)), E-field (2.684+/-0.005x10(-6) cm(2) s(-1)) and the static imaging (2.69+/-0.02x10(-6) cm(2) s(-1)) measurements were all within experimental error of one another and previously reported values. Under 100% aqueous conditions, however, the diffusion coefficient measured dynamically was 11% larger than that measured statically. Diffusion coefficients for rhodamine B, fluorescein, 2',7'dichloro-fluorescein (DCF), rhodamine 6G, tetramethylrhodamine labeled glutamic acid and isoleucine, and fluorescein conjugated bovine serum albumin and ovalbumin were also measured using the static imaging method.

摘要

在一个使用罗丹明6G作为分析物的微流控装置上,对四种测量扩散系数的方法进行了比较。测量采用静态成像方法和三种动态方法——停流法、改变施加电位(电场法)以及改变检测长度(长度法)。在分析物与壁面相互作用(吸附)最小化的条件下,例如在50/50(v/v)甲醇/水缓冲液中,停流法(2.71±0.09×10⁻⁶ cm² s⁻¹)、电场法(2.684±0.005×10⁻⁶ cm² s⁻¹)和静态成像法(2.69±0.02×10⁻⁶ cm² s⁻¹)的测量结果彼此之间都在实验误差范围内,并且与先前报道的值相符。然而,在100%水溶液条件下,动态测量的扩散系数比静态测量的大11%。还使用静态成像法测量了罗丹明B、荧光素、2',7'-二氯荧光素(DCF)、罗丹明6G、四甲基罗丹明标记的谷氨酸和异亮氨酸,以及荧光素偶联的牛血清白蛋白和卵清蛋白的扩散系数。

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