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Double-beam sphere measurement

In a double-beam sphere, the substitution error is eliminated by having both sample and reference on the sphere concurrently and by alternating the measurements between sample and reference, as shown in Fig. 10. [Pg.207]

Measured extinction spectra for aqueous suspensions of polystyrene spheres—the light scatterer s old friend—are shown in Fig. 11.19. Water is transparent only between about 0.2 and 1.3 jam, which limits measurements to this interval. These curves were obtained with a Cary 14R spectrophotometer, a commonly available double-beam instrument which automatically adjusts for changing light intensity during a wavelength scan and plots a continuous, high-resolution curve of optical density. To reproduce the fine structure faithfully, the curves were traced exactly as they were plotted by the instru-... [Pg.317]

Reference and sample measurements are performed consecutively, and the resultant (sample) spectrum is obtained as the ratio of the two photon fluxes onto the detector. In a single-beam spectrometer, there are no other options in a double-beam spectrometer, the photon fluxes of the sample and reference beam path are compared. When an integrating sphere is used with two ports and a white standard in the reference position, the photon fluxes are comparable to each other, and no problems occur. Note that the ports are part of the sphere and that any material change in the reference or sample position will change the average sphere reflectance pave. The reference measurement should be conducted with exactly the same components (windows) as the sample measurement otherwise, "substitution errors" may occur. [Pg.169]


See other pages where Double-beam sphere measurement is mentioned: [Pg.208]    [Pg.208]    [Pg.158]    [Pg.475]    [Pg.384]    [Pg.200]    [Pg.209]    [Pg.72]    [Pg.211]    [Pg.327]    [Pg.56]    [Pg.32]   
See also in sourсe #XX -- [ Pg.208 ]




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