The present disclosure relates to illuminating apparatus used to illuminate hard-copy documents for digital recording, such as in digital scanners, facsimile machines and digital copiers.
In office equipment such as digital copiers and facsimile machines, original hard-copy documents are recorded as digital data using what can be generally called a “scanner.” In a typical scanner, a document sheet is illuminated and the light reflected from the document sheet is recorded by a photosensitive device such as a CCD or CMOS array, to be converted to digital image data. In one embodiment, a narrow strip of the document sheet is illuminated as the sheet is moved through a document handler, or the photosensitive device is moved relative to a platen on which the document sheet is placed.
Designing an illuminator for a scanner presents challenges in providing, among other aspects, an even illumination along the narrow strip of the document, as well as providing a suitable illumination profile across the narrow strip. Irregularities in the illumination level in the illuminated area will result in defects in the image data. An overview of the art of designing illuminators for scanners is given in U.S. Pat. No. 6,236,470.
One type of illuminator useful in document scanning includes a light-transmissive element that exploits internal reflections to direct light from one or more point sources to emerge in substantially parallel rays from an exit surface of the element toward a document. One known type of optical element, used in various contexts, includes a light-transmissive element that exploits internal reflections to direct light from one or more small sources to emerge in substantially parallel rays from an exit surface of the element. Specifically, one known shape for this purpose is a compound parabolic concentrator, or CPC; uses of the CPC are shown in U.S. Pat. No. 5,255,171 and US Patent Application Publication 2004/0131157.
According to one aspect, there is provided an apparatus for illuminating a portion of a document to be recorded. An optical element comprises a light-transmissive material of a predetermined refractory index and defines a curved entry surface, and an exit surface opposite the entry surface. A first substantially parabolic surface is defined between a first edge of the entry surface and a first edge of the exit surface, and a second substantially parabolic surface is defined between a second edge of the entry surface and a second edge of the exit surface.
According to another aspect, here is provided an apparatus for illuminating a portion of a document to be recorded. An optical element comprises a light-transmissive material of a predetermined refractory index and defines an entry surface, and a curved exit surface opposite the entry surface. A first substantially parabolic surface is defined between a first edge of the entry surface and a first edge of the exit surface, and a second substantially parabolic surface is defined between a second edge of the entry surface and a second edge of the exit surface.
According to another aspect, here is provided an apparatus for illuminating a portion of a document to be recorded. An optical element comprises a light-transmissive material of a predetermined refractory index and defines an entry surface, and an exit surface opposite the entry surface. A first substantially parabolic surface is defined between a first edge of the entry surface and a first edge of the exit surface, and a second substantially parabolic surface is defined between a second edge of the entry surface and a second edge of the exit surface, the parabolic surfaces substantially defining a CPC, wherein the CPC defines a theoretical full length relating to the curvatures of the first substantially parabolic surface and the second substantially parabolic surface. The CPC has an actual length of about 0.5 to about 0.9 of the theoretical full length.
According to another aspect, here is provided an apparatus for illuminating a portion of a document to be recorded. An optical element comprises a light-transmissive material of a predetermined refractory index and defines an entry surface, and a curved exit surface opposite the entry surface. A first substantially parabolic surface is defined between a first edge of the entry surface and a first edge of the exit surface, and a second substantially parabolic surface is defined between a second edge of the entry surface and a second edge of the exit surface. The optical element defines a tilt angle in the exit surface thereof, the tilt angle being between five and fifteen degrees from perpendicular to the length of the optical element.
The optical element 10 defines an entry surface 12; an exit surface 14; and a first parabolic surface 16 and second parabolic surface 18. In each case the more curved portion of each parabolic surface 16, 18 is disposed near the entry surface 12, as shown. The exit surface 14 is the surface through which light is directed toward a document, such as shown in
The parabolic surfaces 16, 18 need be only generally parabolic in shape. In one practical embodiment, each parabolic surface 16, 18 can closely follow the shape of half a true parabola. This profile generally forms what is known as a compound parabolic contractor, or CPC. When the CPC is formed from a solid, light-transmissive member exploiting light refraction and total internal reflection, the CPC is typically known as a “dielectric compound parabolic contractor,” or DCPC, but it is conceivable that the optical effect of the CPC can alternatively be obtained with reflective surfaces.
In order to calculate the theoretical length L of a DCPC, as well as determine the characteristics of the parabolic surfaces 16, 18, the following equations can be used:
let a=exit surface ½ width;
a′=entrance surface ½ width;
n=refractive index of DCPC.
θi′=sin−1(a′/a)
theoretical “full” length L=(a+a′)/tanθi′.
(The parabolic surfaces of such a DCPC are defined as follows:
f=a′*(1+sinθi′)
R=2f
Δy=±(a′−f*sinθi′)
Δz=f*cosθi′.)
Once the theoretical full length L of a DCPC is determined, a portion of the theoretical full DCPC can be used. In one practical embodiment, the actual length L′, such as shown in
The
The
In practical implementations of any of the above-described embodiments, other considerations affecting desirable designs include a distance of the CPC to a target; a gap length between the light sources and the CPC; as well as specific characteristics of the LED's or other light sources, such as the angles of emission thereof.
Although the
The claims, as originally presented and as they may be amended, encompass variations, alternatives, modifications, improvements, equivalents, and substantial equivalents of the embodiments and teachings disclosed herein, including those that are presently unforeseen or unappreciated, and that, for example, may arise from applicants/patentees and others.