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In all equations, the attenuation of light exiting though the print-air interface is modeled by the Fresnel diffuse transmittance term (1-r i, When performing measurements, this would imply that an integrated sphere is used to capture all exiting irradiance components. If a measurement instrument is used that captures the exiting radiance perpendicularly (θ, 0°) or at a small angle (θ, 8°, the exit attenuation term (1-ri, 0.386 appearing in Eqs, 2, 3, 5, 8, 23, 28, 31, 33, and (34) should, according to radiometric considerations, be replaced by the attenuation of the radiance across the print-air interface due both to Fresnel transmittivity and to cone spreading (1-rs (θ), n print)2 in the present case (1-0.0438, 1.532, 0.408 see [28, However, since both terms are numerically close one to another and since the print-air interface is not per
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2) = 0.408 (see [28]). However, since both terms are numerically close one to another and since the print-air interface is not perfectly flat, I do not recommend performing these changes. This is consistent with observations by C. Kortüm who did not observe, for diffusely reflecting media, significant reflectance factor differences between collimated 45°/0° and integrated sphere 45°/d or d/0° measurement geometries [29].
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