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代表性层理论在粉末样品近红外反射光谱中的应用。

Application of representative layer theory to near-infrared reflectance spectra of powdered samples.

作者信息

Cairós Carlos, Coello Jordi, Maspoch Santiago

机构信息

Dpto. Química, Facultad de Ciencias, Cn, Universidad Autónoma de Barcelona, 08193 Bellaterra, Spain.

出版信息

Appl Spectrosc. 2008 Dec;62(12):1363-9. doi: 10.1366/000370208786822313.

Abstract

The diffuse reflectance near-infrared (NIR) spectrum of a powdered sample includes the contribution of specular and diffuse reflectance, which is a function of absorbance and scattering. The fraction of light scattered depends in a complex manner on the physical properties of the sample such as particle size, refraction index, etc. Several theories to study the dependence of NIR spectra on the particle size have been proposed. The best known is the Kubelka-Munk model, an approach based on continuous mathematics. Recently Dahm and Dahm put forward an alternative method, the representative layer theory (RLT), which uses discontinuous mathematics as a basis. This approach can be used to identify and disentangle the scattering and absorbance signals as well as their dependence on the particle size. The scattering and absorption coefficient of NaCl (a nonabsorbing material) and of potassium hydrogen phthalate, KHP (a strong absorber), have been estimated through the application of the representative layer theory, working on a particle size range from 63 to 450 microm. In both samples, the absorption coefficient of the sample (K) remains constant and practically independent of the particle size, while the scattering coefficient of the sample (S) decreases when the particle diameter increases, becoming stable around a diameter of 250 microm.

摘要

粉末样品的漫反射近红外(NIR)光谱包含镜面反射和漫反射的贡献,这是吸光度和散射的函数。散射光的比例以复杂的方式取决于样品的物理性质,如粒径、折射率等。已经提出了几种研究近红外光谱与粒径依赖性的理论。最著名的是库贝尔卡-蒙克模型,一种基于连续数学的方法。最近,达姆和达姆提出了另一种方法,即代表性层理论(RLT),它以不连续数学为基础。这种方法可用于识别和分离散射信号与吸光度信号及其对粒径的依赖性。通过应用代表性层理论,在粒径范围为63至450微米的情况下,估算了氯化钠(一种非吸收性材料)和邻苯二甲酸氢钾(KHP,一种强吸收剂)的散射系数和吸收系数。在这两个样品中,样品的吸收系数(K)保持恒定,实际上与粒径无关,而样品的散射系数(S)在粒径增大时减小,在直径约250微米时变得稳定。

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