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. 2009 Apr 1;114(2):69–81. doi: 10.6028/jres.114.006

Fig. 2.

Fig. 2

A model of the light fluxes exciting the cuvette. The incident flux is attenuated by its passage through the cuvette and exits the back of the cuvette as the transmitted flux Φt. Along the path of the incident flux, a scatter flux arises due to scattering from particles in the analyte. The scattered flux, Φs, exits the cuvette and some of the scattered flux may enter the IS detector. The thick vertical lines represent the cuvette walls each of which transmits a fraction t of the incident flux.