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The model used in this work has been previously validated by comparison with data of absorption performances with regard to mass transfer phenomenon.
Numerous complications may arise because SED is usually calculated with data of absorption obtained from chemical applications on healthy skin.
Vertical cross-sectional plots (raw data and curve-fitted data) of absorption and reduced scattering coefficients along pixel 200 (the white dashed lines), belong to the ROI, are shown in Fig. 13.
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The model is validated with a large volume of experimental data for absorption of CO2 in membrane contactor units.
This absorption-based approach is surely a promising alternative to the fluorescence-based one, since the measurement and data processing of absorption spectra are much easier and more robust than its fluorescence counterpart.
Regression analysis of normalized data of E2 E3 (absorption ratio at 250 nm and 365 nm) and E4 E6 (absorption ratio at 465 nm and 665 nm) with bacterial abundance, measured at t0 (start of the experiments) and tf (end of the experiments, after 48 hours for experiments ES1b and ES1c and 72 hours for experiment ES1a) for control (C) and microplastics (MP) treatments in ES1.
The KLa values were obtained by fitting the model to experimental data of toluene absorption obtained at empty bed residence times (EBRT) from 7 to 50 s.
After development of the mass balances to both contactors the characteristic parameters have been determined from the fitting of the experimental data of the absorption flux to the mathematical models.
There are marked differences between simulation results and actual measured data of the absorption rate in each layer (Ji et al. 2009).
In Fig. 3, we present the experimental data of transient absorption for the pure P3HT polymer when it is excited by ultrashort laser pulses (150 fs) at 400 nm.
Data of the absorption measurements were statistically analysed with the software PASW Statistics version 18.0 (IBM Corporation, Armonk, NY, USA).
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