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Pulse glucometry: A new approach for noninvasive blood glucose measurement using instantaneous differential near-infrared spectrophotometry

机译:脉冲血糖仪:使用瞬时差分近红外分光光度法进行无创血糖测量的新方法

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摘要

We describe a new optical method for noninvasive blood glucose (BGL) measurement. Optical methods are confounded by basal optical properties of tissues, especially water and other biochemical species, and by the very small glucose signal. We address these problems by using fast spectrophotometric analysis in a finger, deriving 100 transmittance spectra per second, to resolve optical spectra (900 to 1700 nm) of blood volume pulsations throughout the cardiac cycle. Difference spectra are calculated from the pulsatile signals, thereby eliminating the effects of bone, other tissues, and nonpulsatile blood. A partial least squares (PLS) model is used with the measured spectral data to predict BGL levels. Using glucose tolerance tests in 27 healthy volunteers, periodic optical measurements were made simultaneously with collection of blood samples for in vitro glucose analysis. Altogether, 603 paired data sets were obtained in all subjects and two-thirds of the data or of the subjects randomly selected were used for the PLS calibration model and the rest for the prediction. Bland-Altman and error-grid analyses of the predicted and measured BGL levels indicated clinically acceptable accuracy. We conclude that the new method, named pulse glucometry, has adequate performance for safe, noninvasive estimation of BGL. © 2006 Society of Photo-Optical Instrumentation Engineers.
机译:我们描述了一种新的光学方法用于无创血糖(BGL)测量。光学方法因组织(尤其是水和其他生化物种)的基本光学特性以及非常小的葡萄糖信号而混淆。我们通过在手指中使用快速分光光度分析来解决这些问题,每秒获得100个透射光谱,以解决整个心动周期中血容量脉动的光谱(900至1700 nm)。根据脉动信号计算差异光谱,从而消除骨骼,其他组织和非脉动血液的影响。偏最小二乘(PLS)模型与测得的光谱数据一起使用以预测BGL水平。使用27位健康志愿者的葡萄糖耐量测试,在进行血液光学样本采集的同时,进行了定期光学测量,以进行体外葡萄糖分析。总共在所有受试者中获得了603对配对的数据集,将三分之二的数据或随机选择的受试者中的三分之二用于PLS校准模型,其余的用于预测。对预测和测量的BGL水平进行的Bland-Altman和错误网格分析表明,临床上可接受的准确性。我们得出结论,名为脉冲血糖仪的新方法对于安全,无创地估计BGL具有足够的性能。 ©2006光电仪器工程师协会。

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  • 年度 2006
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  • 正文语种 en
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  • 入库时间 2022-08-20 21:04:11

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