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一种用于动力学底物分析标准曲线的新型线性图,其范围扩展至米氏常数以上:应用于甘油的发光分析。

A new linear plot for standard curves in kinetic substrate assays extended above the Michaelis-Menten constant: application to a luminometric assay of glycerol.

作者信息

Lundin A, Arner P, Hellmér J

机构信息

Research Center, Karolinska Institute, Huddinge University Hospital, Sweden.

出版信息

Anal Biochem. 1989 Feb 15;177(1):125-31. doi: 10.1016/0003-2697(89)90026-2.

Abstract

In conventional kinetic substrate assays the standard curve is plotted as observed reaction rate, upsilon obs, versus added substrate concentration, Sadd, and has a linearity limited to Sadd much less than Km. From this plot the blank reaction rate, upsilon bl, is easily estimated but not the contaminating substrate concentration, Scon, present in reagents (unless it is the only blank source). Thus the actual substrate concentration, S = Scon + Sadd, cannot be estimated as required for the various linear plots based on the Michaelis-Menten equation. We have derived an expression, (upsilon obs - upsilon bl)/Vapp = Sadd/(Kmapp + Sadd), containing only those parameters measured for a conventional standard curve (Vapp and Kmapp are obtained from a plot of (upsilon obs - upsilon bl) versus (upsilon obs - upsilon bl)/Sadd). A plot of (upsilon obs - upsilon bl)/Vapp versus Sadd/(Kmapp + Sadd) can be used as a standard curve with the following advantages over the conventional standard curve: (a) For all kinetic substrate assays it is identical and connects the points (0, 0) and (1, 1). Thus deviations from true Michaelis-Menten kinetics or erroneous kinetic constants are easily detected. (b) Since it is linear even above Km, the analytically useful range is considerably extended. (c) For assays with a wide dynamic range it can be used in lin-lin or log-log form. The procedure is illustrated for a kinetic assay of glycerol (Kmapp = 40 mumol/liter). The plot was found to be entirely linear in the range 0.07-100 mumol/liter (glycerol concentration in cuvette).

摘要

在传统的动力学底物分析中,标准曲线是以观察到的反应速率(υobs)对添加的底物浓度(Sadd)绘制的,其线性范围限于Sadd远小于Km。从该图中可以很容易地估计空白反应速率(υbl),但无法估计试剂中存在的污染底物浓度(Scon)(除非它是唯一的空白来源)。因此,实际底物浓度S = Scon + Sadd,无法按照基于米氏方程的各种线性图的要求进行估计。我们推导了一个表达式(υobs - υbl)/Vapp = Sadd/(Kmapp + Sadd),其中只包含为传统标准曲线测量的那些参数(Vapp和Kmapp是从(υobs - υbl)对(υobs - υbl)/Sadd的图中获得的)。(υobs - υbl)/Vapp对Sadd/(Kmapp + Sadd)的图可作为标准曲线,与传统标准曲线相比具有以下优点:(a) 对于所有动力学底物分析,它都是相同的,并且连接点(0, 0)和(1, 1)。因此,很容易检测到与真实米氏动力学的偏差或错误的动力学常数。(b) 由于它在Km以上也是线性的,因此分析上有用的范围大大扩展。(c) 对于具有宽动态范围的分析,它可以以线性-线性或对数-对数形式使用。以甘油的动力学分析(Kmapp = 40 μmol/升)为例说明了该程序。发现该图在0.07 - 100 μmol/升(比色皿中的甘油浓度)范围内完全线性。

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