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It is assumed that the sum of absorption, reflection, and transmission is equal to 1.
The extinction cross section is simply defined as the sum of absorption and scattering cross sections of the nanoparticles.
The total attenuation coefficient of the mucosa layer in the pig trachea sample, depicted by the circles in Fig. 11(b), was dependent on the sum of absorption and scattering.
Assuming there are three major optical absorbers in a body (i.e., oxyhemoglobin (HbO2), deoxyhemoglobin (Hb), and nanoparticle (NP)), the absorption coefficient of localized mouse tissue can be defined by the sum of absorption coefficients for HbO2, Hb, and NP in the region.
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The absorption is the sum of the absorption from the tissue chromophores weighted by their concentration, e.g., where C k is the concentration of the kth chromophore, ε k is the specific absorption spectrum of the kth chromophore in natural log units and the sum is over all the chromophores.
Assuming that the absorption of 3OMD-glucose represents the sum of passive+mediated absorption, the ratio of the amounts absorbed L-rhamnose/3OMD-glucose L-rhamnose/3OMD-glucose L-rhamnose/3OMD-glucoserptindicatesoccurs via the proportionthway.
In this study, the absorption coefficient was modeled as a linear sum of the absorption coefficients of the dominant chromophores; the reduced scattering coefficient was modeled as a power law [ 18].
The tissue absorption coefficient μ a tissue is the sum of the absorption coefficients of all the chromophores present in the interrogation volume, which can be written as: (10) μ a tissue = ∑ k c k ɛ k Here c k and ɛ k are the concentration and extinction coefficient, respectively, of absorbing molecules (index k) such as oxyhemoglobin, deoxyhemoglobin, bilirubin, beta-carotene, lipids and water.
It was noticed that the absorption spectra of the obtained complexes correspond to the sum of the absorption spectra of their components, which indicates a lack of interaction in the ground state.
The interaction between the outer CFRP tube and inner aluminum tube in a hybrid configuration was explored by comparing the sum of energy absorption of individual components with the hybrid form.
Based on a theoretically derived approach we show for the first time that the spatial distribution of the β-nucleating agent N,N′-dicyclohexyl-2,6-naphthalenedicarboxamide (NU-100) in random ethylene propylene copolymer (PP-R) can be determined by μFTIR from the sum of the absorption intensities in three directions of inspection.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com