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Method and apparatus for determining the reflectance of translucent objects

  • US 6,721,054 B1
  • Filed: 10/11/2001
  • Issued: 04/13/2004
  • Est. Priority Date: 04/15/1999
  • Status: Expired due to Fees
First Claim
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1. A method for determining a corrected reflectance value for a translucent object, the method comprising the steps of:

  • a) measuring a relationship between a normalized lateral diffusion error and a spatial distribution value for each of a set of calibration standards, by;

    i) illuminating an illuminated area of a standard and determining a first reflectance for a measured area of the standard, ii) illuminating only the measured area of the standard and determining a second reflectance for the measured area of the standard, iii) calculating the normalized lateral diffusion error for the standard from the first reflectance and the second reflectance, iv) determining the spatial distribution value for at least one of the first reflectance and the second reflectance, v) preparing a calibration curve showing the relationship between the normalized lateral diffusion error and the spatial distribution value for each standard;

    b) determining an uncorrected reflectance for a measured area of the object by;

    i) illuminating an area of the object to produce the measured area of the object, ii) measuring an uncorrected reflectance for the measured area of the object;

    c) determining at least one spatial distribution value for the measured area of the object from the reflectance of at least two concentric areas of the measured area of the object;

    d) determining a normalized lateral diffusion error for the uncorrected reflectance of the measured area of the object from the spatial distribution value for the measured area of the object and the calibration curve; and

    e) calculating the corrected reflectance value from the uncorrected reflectance for the measured area of the object and the normalized lateral diffusion error;

    in which;

    the illuminated area of the standard is larger than the measured area of the standard; and

    the measured area of the standard is far enough away from the edge of the illuminated area of the standard to be essentially free from diffusion effects.

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