CA2238498A1

CA2238498A1 - Apparatus and method for measuring optical characteristics of an object

Info

Publication number: CA2238498A1
Application number: CA002238498A
Authority: CA
Inventors: Wayne D. Jung; Russell W. Jung; Alan R. Loudermilk
Original assignee: Individual
Current assignee: JJL TECHNOLOGIES LLC
Priority date: 1996-01-02
Filing date: 1997-01-02
Publication date: 1997-07-10
Also published as: NO983057D0; AU1571397A; US6040902A; KR19990076942A; JP2000502804A; ATE444478T1; US5745229A; EP0909376A1; EP0909376A4; JP3981154B2; DE69739604D1; AU733060B2; JP2005308764A; KR100432764B1; NO983057L; EP0909376B1; ES2334182T3; WO1997024587A1; US5883708A; JP4243263B2

Abstract

Color/optical characteristics measuring systems and methods are disclosed. Perimeter receiver fiber optics/elements (7) are spaced apart from a central source fiber optic/element (5) and received light reflected from the surface of the object (20) is measured. Light from the perimeter fiber optics (7) pass to a variety of filters. The system utilizes the perimeter receiver fiber optics (7) to determine information regarding the height and angle of the probe (1) with respect to the object (20) being measured. Under processor control (20), the color measurement may be made at a predetermined height and angle. Various color spectral photometer arrangements are disclosed. Translucency, fluorescence, and/or surface texture data also may be obtained. Audio feedback may be provided to guide operator use of the system. The probe (1) may have a removable or shielded tip for contamination prevention.

Description

CA 02238498 1998-0~-2~
WO 97/24587 PCTtUS97/00126 Apparatus and Method for Measuring Optical Characteristics of an Object 5 Field of the Invention The present invention relates to devices and methods for measuring optical Gh~raGteristiGs such as color of ob3ects, and more particularly to devices and methods for measuring the color and other optical characteristics of teeth, fabric or other objects or surfaces with a hand-held probe that presents min;m~l problems with height or angular 1 0 dependencies.
Back~round of the Invention Various color/optical measuring devices such as spectrophotometers and colorimeters are known in the art. To understand the limitations of such conventional devices, it is helpful to understand certain principles relating to color. Without being bound by theory, Applicants 15 provide the following discussion.
The color of an object determines the manner in which light is reflected from the surface of the object. When light is incident upon an object, the reflected light will vary in intensity and wavelength dependent upon the color of the surface of the object. Thus, a red object will reflect red light with a greater intensity than a blue or a green object, and 20 correspondingly a green object will reflect green light with a greater intensity than a red or blue object.
One method of quantifying the color of an object is to ill~lmin~t~ it with broad band spectrum or "white" light, and measure the spectral properties of the reflected light over the entire visible spectrum and compare the reflected spectrum with the incident light spectrum.
25 Such instruments typically require a broad band spectrophotometer, which generally are expensive, bulky and relatively cumbersome to operate, thereby limiting the practical application of such instruments.
For certain applications, the broad band data provided by a spectrophotometer isllnn.ocess~ry. For such applications, devices have been produced or proposed that quantify 30 color in terms of a numerical value or relatively small set of values representative of the color of the object.
It is known that the color of an object can be represented by three values. For example, the color of an object can be represented by red, green and blue values, an intensity CA 02238498 1998-0~-2~

value and color difference values, by a CIE value, or by what are known as "tristimulus values" or numerous other orthogonal combinations. It is important that the three values be orthogonal; i.e., any combination of two elements in the set cannot be included in the third element.
One such method of quantifying the color of an object is to ill~lmin~te an object with broad band "white" light and measure the intensity of the reflected light after it has been passed through narrow band filters. Typically three filters (such as red, green and blue) are used to provide tristimulus light values representative of the color of the surface. Yet another method is to illllmin:~te an object with three monochromatic light sources (such as red, green lo and blue) one at a time and then measure the intensity of the reflected light with a single light sensor. The three measurements are then converted to a tristimulus value representative of the color of the surface. Such color measurement techniques can be utilized to produce equivalent tristimulus values representative of the color of the surface. Generally, it does not matter if a "white" light source is used with a plurality of color sensors (or a continuum in the 15 case of a spectrophotometer), or if a plurality of colored light sources are utilized with a single light sensor.
There are, however, difficulties with the conventional techniques. When light isincident upon a surface and reflected to a light receiver, the height of the light sensor and the angle of the sensor relative to the surface and to the light source also affect the intensity of the 20 received light. Since the color determination is being made by measuring and quantifying the intensity of the received light for different colors, it is important that the height and angular dependency of the light receiver be elimin~t.o.d or accounted for in some manner.
One method for elimin~ting the height and angular dependency of the light source and receiver is to provide a fixed mounting arrangement where the light source and receiver are 25 stationary and the object is always positioned and measured at a preset height and angle. The fixed mounting arrangement greatly limits the applicability of such a method. Another method is to add mounting feet to the light source and receiver probe and to touch the object with the probe to m~int~in a constant height and angle. The feet in such an apparatus must be wide enough apart to insure that a constant angle (usually perpendicular) is m~int~ine.d 30 relative to the object. Such an apparatus tends to be very difficult to utilize on small objects or on objects that are hard to reach, and in general does not work satisfactorily in measuring objects with curved surfaces.

CA 02238498 1998-0~-2~

The use of color measuring devices in the field of dentistry has been proposed. In modern dentistry, the color of teeth typically are quantified by manually comparin~ a patient~s teeth with a set of ~'shade guides." There are numerous shade guides available for dentists in order to properly select the desired color of dental prosthesis. Such shade guides have been 5 utilized for decades and the color determination is made subjectively by the dentist by holding a set of shade guides next to a patient' s teeth and attempting to find the best match.
Unfortunately, however, the best match often is affected by the ambient light color in the dental operatory and the surrounding color of the patient's makeup or clothing and by the fatigue level of the dentist.
Similar subjective color quantification also is made in the paint industry by co~ aling the color of an object with a paint reference guide. There are numerous paint guides available in the industry and the color determination also often is affected by ambient light color, user fatigue and the color sensitivity of the user. Many individuals are color insensitive (color blind) to certain colors, further complicating color determination.
In general, color quantification is needed in many industries. Several, but certainly not all, applications include: dentistry ~color of teeth); dermatology (color of skin lesions);
interior decorating (color of paint, fabrics); the textile industry; automotive repair (m~t~h;n~
paint colors); photography (color of reproductions, color reference of photographs to the object being photographed); printing and lithography; cosmetics (hair and skin color, makeup 20 matching); and other applications in which it useful to measure color in an expedient and reliable manner.
With respect to such applications, however, the limitations of conventional color/optical measuring techniques typically restrict the utility of such techniques. For example, the high cost and bulkiness of typical broad band spectrometers, and the fixed 2~ mounting arrangements or feet required to address the height and angular dependency, often limit the applicability of such conventional techniques.
Moreover, another limitation of such conventional methods and devices are that the resolution of the height and angular dependency problems typically require contact with the object being measured. In certain application5, it may be desirable to measure and quantify 30 the color of an object with a small probe that does not require contact with the surface of the object. In certain applications, for example, hygienic considerations make such contact undesirable. In the other applications such as interior decorating, contact with the object can CA 02238498 1998-0~-2~

mar the surface (such as if the object is coated with wet paint) or otherwise cause undesirable effects.
In summary, there is a need for a low cost, hand-held probe of small size that can reliably measure and quantify the color and other optical characteristics of an object without 5 requiring physical contact with the object, and also a need for methods based on such a device in the field of dentistry and other applications.
~ummary of the Invention In accordance with the present invention, devices and methods are provided ~or measuring the color and other optical characteristics of objects, reliably and with minim~l 10 problems of height and angular dependence. A handheld probe is utilized in the present invention, with the handheld probe cont~ining a number of fiber optics in certain prerellt;d embodiments. Light is directed from one (or more) light source(s) towards the object to be measured, which in certain preferred embodiments is a central light source fiber optic (other }ight sources and light source arrangements also may be utilized). Light reflected from the 1~ object is detected by a number of light receivers. Included in the light receivers (which may be light receiver fiber optics) are a plurality of perimeter receivers (which may be receiver fiber optics, etc.). In certain preferred embodiments, three perimeter fiber optics are utilized in order to take measurements at a desired, and predetermined height and angle, thereby minimi7:ing height and angular dependency problems found in conventional methods. In 20 certain embodiments, the present invention also may measure translucence and fluorescence characteristics of the object being measured, as well as surface texture and/or other optical or surface characteristics.
The present invention may include constituent elements of a broad band spectrophotometer, or, alternatively, may include constituent elements of a tristimulus type 25 colorimeter. The present invention may employ a variety of color measuring devices in order to measure color in a practical, reliable and efficient manner, and in certain preferred embodiments includes a color filter array and a plurality of color sensors. A microprocessor is included for control and calculation purposes. A temperature sensor is included to measure temperature in order to detect abnormal conditions and/or to compensate for temperature 30 ef~ects of the filters or other components of the system. In addition, the present invention may include audio feedback to guide the operator in making color/optical measurements, as well as one or more display devices for displaying control, status or other information.

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With the present invention, color/optical measurements may be made with a handheld probe in a practical and reliable manner, essentially free of height and angular dependency problems, without resorting to fixtures, feet or other undesirable mechanical arrangements for fixing the height and angle of the probe with respect to the object.
Accordingly, it is an object of the present invention to address limitations of ~ conventional color/optical measuring techniques.
It is another object of the present invention to provide a method and device useful in measuring the color or other optical characteristics of teeth, fabric or other objects or surfaces with a hand-held probe of practical size that does not require contact with the object or 1 0 surface.
It is a further object of the present invention to provide a color/optical mea~u,G",ent probe and method that does not require fixed position mechanical mounting, feet or other m~chz~nical impediments.
It is yet another object of the present invention to provide a probe and method useful for measuring color or other optical characteristics that may be utilized with a probe simply placed near the surface to be measured.
It is a still further object of the present invention to provide a probe and method that are capable of determining translucency characteristics of the object being measured.
It is a further object of the present invention to provide a probe and method that are capable of deterrnining surface texture characteristics of the object being measured.
It is a still further object of the present invention to provide a probe and method that are capable of determining fluorescence characteristics of the object being measured.
It is an object of the present invention to provide a probe and method that can measure the area of a small spot singulary, or that also can measure irregular shapes by moving the probe over an area and integrating the color of the entire area.
It also is an object of the present invention to provide probes and methods for measuring optical characteristics with a probe that is held substantially stationary with respect to the object being measured.
Finally, it is an object of the present invention to provide probes and methods for measuring optical characteristics with a probe that may have a removable tip or shield that may be removed for cleaning, disposed after use or the like.

CA 02238498 1998-0=,-2~
W O 97/24587 PCT~US97/00126 Brief Description of the Drawin~s The present invention may be more fully understood by a description of certain preferred embodiments in conjunction with the attached drawings in which:
FIG. 1 is a diagram illustrating a preferred embodiment of the present invention;
FIG. 2 is a diagram illustrating a cross section of a probe in accordance with apreferred embodiment of the present invention;
FIG. 3 is a diagram illustrating an arrangement of fiber optic receivers and sensors utilized with a preferred embodiment of the present invention;
FIGS. 4A to 4C illustrate certain geometric considerations of fiber optics;
FIGS. SA and 5B illustrate the light amplitude received by fiber optic light receivers as a function of height from an object;
FIG. 6 is a flow chart illustrating a color measuring method in accordance with an embodiment of the present invention;
~;IGS. 7A and 7B illustrate a protective cap that may be used with certain l~ embodiments of the present invention;
FIGS. 8A and 8B illustrate removable probe tips that may be used with certain embodiments of the present invention;
FIG. 9 illustrates a rlber optic bundle in accordance with another preferred embodiment of the present invention;
FIGS. IOA, lOB, lOC and lOD illustrate and describe other fiber optic bundle configurations that may be used in accordance with yet other preferred embodiments of the present invention;
FIG. 11 illustrates a linear optical sensor array that may be used in certain embodiments of the present invention;
2~ FIG. 12 illustrates a matrix optical sensor array that may be used in certain embodiments of the present invention;
~IGS. 13A and 13B illustrate certain optical properties of a filter array that may be used in certain embodiments of the present invention;
FIGS. 14A and 14B illustrate examples of received light intensities of receivers used ~0 in certain embodiments of the present invention;
E;IG. 1~ is a flow chart illustrating audio tones that may be used in certain preferred embodiments of the present invention;

CA 02238498 1998 - 0~ - 2~
WO 97/24587 7 PCT/US97/û0126 FIG. 16 illustrates an embodiment of the present invention, which utilizes a plurality of rings of light receivers that may be utilized to take measurements with the probe held substantially stationary with respect to the object being measured;
FIGS. 17 and 18 illustrate an embodiment of the present invention, which utilizes a 5 mechanical movement and also may be utilized to take measurements with the probe held substantially stationary with respect to the object being measured; and ~ IGS. 19A to l9C illustrate embodiments of the present invention in which coherent light conduits may serve as removable probe tips.
Detailed Description of the Preferred Embodiments The present invention will be described in greater detail with reference to certain preferred embodiments. As described elsewhere herein, various refinements and substitutions of the various embodiments are possible based on the principles and teachings herein.
With reference to FIG. 1, an exemplary preferred embodiment of a color/optical characteristic measuring system and method in accordance with the present invention will be l 5 described.
Probe tip 1 encloses a plurality of fiber optics, each of which may constitute one or more fiber optic fibers. In a preferred embodiment, the fiber optics contained witnin probe tip 1 includes a single light source fiber optic and three light receiver fiber optics. The use of such fiber optics to measure the color or other optical characteristics of an object will be 20 described later herein. Probe tip 1 is attached to probe body 2, on which is fixed switch 17.
Switch 17 communicates with microprocessor 10 through wire 18 and provides, for example, a mf ch~ni~m by which an operator may activate the device in order to make a color/optical measurement. Fiber optics within probe tip 1 terminate at the forward end thereof (i.e., the end away from probe body 2). The forward end of probe tip l is directed towards the surface 2~ of the object to be measured as described more fully below. The fiber optics within probe tip 1 optically extend through probe body 2 and through fiber optic cable 3 to light sensors 8, which are coupled to microprocessor 10.
It should be noted that microprocessor 10 includes conventional associated components, such as memory (programmable memory, such as PROM, EPROM or 30 EEPROM; working memory such as DRAMs or SRAMs; and/or other types of memory such as non-volatile memory, such as FLASH), peripheral circuits, clocks and power supplies, although for clarity such components are not explicitly shown. Other types of co~ uLillg CA 02238498 1998-0~-2~
WO 97/24587 PCT/US97/001;!6 devices ~such as other microprocessor systems, programmable logic arrays or the like) are used in other embodiments of the present invention.
In the embodiment of FIG. 1, the fiber optics from fiber optic cable 3 end at splicing connector 4. From splicing connector 4, each of the three receiver fiber optics used in this 5 embodiment is spliced into at least five smaller fiber optics (generally denoted as fibers 7), which in this embodiment are fibers of equal diameter, but which in other embodiments may be of unequal diameter (such as a larger or smaller "height/angle" or perimeter fiber, as more fully described herein). One of the fibers of each group of five fibers passes to light sensors 8 through a neutral density filter (as more fully described with reference to ~IG. 3), and 10 collectively such neutrally filtered fibers are utilized for purposes of height/angle determination (and also may be utilized to measure surface characteristics, as more fully described herein~. Four of the remaining fibers of each group of fibers passes to light sensors 8 through color filters and are used to make the color/optical measurement. In still other embodiments, splicing connector 4 is not used, and fiber bundles of, for example, five or 15 =more fibers each extend from light sensors 8 to the forward end of probe tip 1. In certain embodiments, unused ~Ibers or other materials may be included as part of a bundle of fibers for purposes of, for example, easing the manufacturing process for the fiber bundle. What should be noted is that, for purposes of the present invention, a plurality of light receiver fiber optics or elements (such as fibers 7) are presented to light sensors 8, with the light from the 20 light receiver fiber optics/elements representing light reflected from object 20. While the various embodiments described herein present tradeoffs and benefits that may not have been apparent prior to the present invention (and thus may be independently novel), what is important for the present discussion is that light from fiber optics/elements at the forward end of probe tip 1 is presented to sensors 8 for color/optical measurements and angle/height 2~ determination, etc.
Light source 11 in the preferred embodiment is a halogen light source (of, for example, 5-100 watts, with the particular wattage chosen for the particular application), which may be under the control of microprocessor 10. The light from light source 1 1 reflects from cold mirror 6 and into source fiber optic 5. Source fiber optic 5 passes through to the 30 forward end of probe tip 1 and provides the light stimulus used for purposes of making the mea~ulGlllents described herein. Cold mirror 6 reflects visible light and passes infra-red light, and is used to reduce the amount of infra-red light produced by light source 11 before the light is introduced into source fiber optic 5. Such infra-red light reduction of the light from a CA 02238498 l998-0~-2~

halogen source such as light source 11 can help prevent saturation of the receiving light sensors, which can reduce overall system sensitivity. Fiber 15 receives light directly from light source 11 and passes through to light sensors 8 (which may be through a neutral density filter). Microprocessor 10 monitors the light output of light source 11 through fiber 15, and 5 thus may monitor and, if necessary compensate for, drift of the output of light source 11. In - certain embodiments. microprocessor 10 also may sound an alarm (such as through speaker 16) or otherwise provide some indication if abnormal or other undesired performance of light source 11 is detected.
The data output from light sensors 8 pass to microprocessor 10. Microprocessor l0 l O processes the data from light sensors 8 to produce a measurement of color and/or other characteristics. Microprocessor 10 also is coupled to key pad switches 12, which serve as an input device. Through key pad switches 12, the operator may input control information or comm~n~lc~ or information relating to the object being measured or the like. In general, key pad switches 12, or other suitable data input devices (such as push button, toggle, membrane l 5 or other switches or the like), serve as a mechanism to input desired information to mic~ ocessor 10.
Microprocessor 10 also communicates with UART 13, which enables microprocessor 10 to be coupled to an external device such as computer 13A. In such embodiments, data provided by microprocessor 10 may be processed as desired for the particular application, such as for averaging, format conversion or for various display or print options, etc. In the preferred embodiment, UART 13 is configured so as to provide what is known as a RS232 interface, such as is commonly found in personal computers.
Microprocessor 10 also communicates with LCD 14 for purposes of displaying status, control or other information as desired for the particular application. ~or example, color bars, charts or other graphic representations of the color or other collected data and/or the measured obJect or tooth may be displayed. In other embodiments, other display devices are used, such as CRTs, matrix-type LEDs, lights or other mechanisms for producing a visible indicia of system status or the like. Upon system initialization, for example, LCD 14 may provide an indication that the system is stable, ready and available for taking color measulclllcllts.
Also coupled to microprocessor 10 is spealcer 16. Speaker 16, in a preferred embodiment as discussed more fully below, serves to provide audio feedback to the operator, which may serve to guide the operator in the use of the device. Speaker 16 also may serve to provide status or other information alerting the operator of the condition of the system, CA 02238498 1998-0~-2~

including an audio tone, beeps or other audible indication (i.e., voice) that the system is initialized and available for taking measurements. Speaker 16 also may present audio information indicative of the measured data, shade guide or reference values corresponding to the rneasured data, or an indication of the status of the color/optical measurements.
Microprocessor 10 also receives an input from temperature sensor 9. Given that many types of filters (and perhaps light sources or other components) may operate reliably only in a given temperature range, temperature sensor 9 serves to provide temperature information to microprocessor 10. In particular, color filters, such as may be included in light sensors 8, may be sensitive to temperature, and may operate reliably only over a certain tt;~ eldt~llG
range. In certain embodiments, if the t~lllpelature is within a usable range, microprocessor 10 may compensate for temperature variations of the color filters. In such embodiments, the color filters are characterized as to filtering characteristics as a function of temperature, either by data provided by the filter manufacturer, or through measurement as a function of temperature. Such filter telll~elaLule compensation data may be stored in the form of a look-l 5 up table in memory, or may be stored as a set of polynomial coef~lcients from which the temperature characteristics of the filters may be computed by microprocessor 10.In general, under control of microprocessor 10, which may be in response to operator activation (through, for example, key pad switches 12 or switch 17), light is directed from light source I 1, and reflected from cold mirror 6 through source fiber optic 5 (and through fiber optic cable 3, probe body 2 and probe tip 1, or through some other suitable light source element) and is directed onto object 20. Light reflected from object 20 passes through the receiver fiber optics/elements in probe tip 1 to light sensors 8 (through probe body 2, fiber optic cable 3 and fibers 7). Based on the information produced by light sensors 8, microprocessor 10 produces a color/optical measurement result or other information to the 2~ = operator. Color measurement or other data produced by microprocessor 10 may be displayed on display 1~, passed through UART 13 to computer 13A, or used to generate audioinformation that is presented to speaker 16. Other operational aspects of the preferred embodiment illustrated in F~G. 1 will be explained hereinafter.
With reference to FIG. 2, a preferred embodiment of a fiber optic arrangement 30 presented at the forward end of probe tip I will now be described. As illustrated in FIG. 2, a cfel~c~d embodiment of the present invention utilizes a single central light source fiber optic, denoted as light source fiber optic S, and a plurality of perimeter light receiver ~Iber optics, denoted as light receivers Rl, R2 and R3. As is illustrated, a preferred embodiment of the ~, CA 02238498 1998-0~-2~
WO 97/24587 1 ~ PCT/US97/00126 present invention utilizes three perimeter fiber optics, although in other embodiments two, four or some other number of receiver fiber optics are utilized. As more fully described herein, the perimeter light receiver fiber optics serve not only to provide reflected light for purposes of making the color/optical measurement, but such perimeter fibers also serve to 5 provide information regarding the angle and height of probe tip I with respect to the surface of the object that is being measured, and also may provide information regarding the surface characteristics of the object that is being measured.
In the illustrated preferred embodiment, receiver fiber optics R1 to R3 are positioned symmetrically around source fiber optic S, with a spacing of about 120 degrees from each 10 other. It should be noted that spacing t is provided between receiver fiber optics Rl to R3 and source fiber optic S. While the precise angular placement of the receiver fiber optics around the perimeter of the fiber bundle in general is not critical, it has been determined that three receiver fiber optics positioned 120 degrees apart generally may give acceptable results. As discussed above, in certain embodiments light receiver fiber optics R1 to R3 each constitute a 15 single fiber, which is divided at splicing connector 4 (refer again to FIG. 1), or, in alternate embodiments, light receiver fiber optics Rl to R3 each constitute a bundle of fibers, numbering, for example, at least five fibers per bundle. It has been determined that, with available fibers of uniform size, a bundle of, for example, seven fibers may be readily produced (although as will be apparent to one of skill in the art, the precise number of fibers 20 may be determined in view of the desired number of receiver fiber optics, manufacturing considerations, etc.~. The use of light receiver fiber optics R1 to R3 to produce color/optical measurements in accordance with the present invention is further described elsewhere herein, although it may be noted here that receiver fiber optics R1 to R3 may serve to detect whether, for example, the angle of probe tip l with respect to the surface of the object being measured 25 is at 90 degrees, or if the surface of the object being measured contains surface texture and/or spectral irregularities. In the case where probe tip l is perpendicular to the surface of the object being measured and the surface of the object being measured is a diffuse reflector (i.e., a matte-type reflector, as compared to a spectral or shiny-type reflector which may have "hot spots"), then the light intensity input into the perimeter fibers should be approximately equal.
30 It also should be noted that spacing t serves to adjust the optimal height at which color/optical measurements should be made (as more fully described below).
In one particular aspect of the present invention, area between the fiber optics on probe tip 1 may be wholly or partially filled with a non-reflective material andlor surface CA 02238498 1998-0~-2~
WO 97n4s87 12 PCT/US97/00126 (which may be a black mat, contoured or other non-reflective surface). Having such exposed area of probe tip I non-reflective helps to reduce undesired reflections, thereby helping to increase the accuracy and reliability of the present invention.
With reference to FIG. 3, a partial arrangement of light receiver fiher optics and 5 sensors used in a pl~r~ ;d embodiment of the present invention will now be described.
Fibers 7 represent light receiving fiber optics, which transmit light reflected from the object being measured to light sensors 8. In a preferred embodiment, sixteen sensors (two sets of eight) are ~l~ili7e-1, although for ease of discussion only 8 are illustrated in FIG. 3 (in this ~IGfell~;d embodiment, the circuitry of FIG. 3 is duplicated, for example, in order to result in l o ~ sixteen sensors). In other embodiments, other numbers of sensors are utilized in accordance with the present invention.
Light from fibers 7 is presented to sensors 8, which in a ~ d embodiment pass through filters 22 to sensing elements 24. In this preferred embodiment, sensing elements 24 include light-to-frequency converters, manufactured by Texas In~ll ull~llts and sold under the 15 part number TSL230. Such converters constitute, in general, photo diode arrays that integrate the light received from fibers 7 and output an AC signal with a frequency proportional to the intensity (not frequency) of the incident light. Without being bound by theory, the basic principle of such devices is that, as the intensity increases, the integrator output voltage rises more quickly, and the shorter the integrator rise time, the greater the output frequency. The 20 outputs of the TSL230 sensors are TTL or CMOS compatible digital signals, which may be coupled to various digital logic devices.
The outputs of sensing elements 24 are, in this embodiment, asynchronous signals of frequencies depending upon the light intensity presented to the particular sensing elements, which are presented to processor 26. In a preferred embodiment, processor 26 is a Microchip 25 : PIC16C55 or PIC16C57 microprocessor, which as described more fully herein implements an algorithm to measure the frequencies of the signals output by sensing elements 24. In other embodiments, a more integrated microprocessor/microcontroller, such as Hitachi's SH
RISC microcontrollers, is utilized to provide further system integration or the like.
As previously described, processor 26 measures the fre~uencies of the signals output 30 from sensing elements 24. In a preferred embodiment, processor 26 implements a software timing loop, and at periodic intervals processor 26 reads the states of the outputs of sensing elements 24. An internal counter is incremented each pass through the software timing loop.
The accuracy of the tin~ing loop generally is determined by the crystal oscillator time base -CA 02238498 1998-0~-2~

(not shown in FIG. 3) coupled to processor 26 (such oscillators typically are quite stable).
After reading the outputs of sensing elements 24, processor 26 performs an exclusive OR
("XOR") operation with the last data read (in a preferred embodiment such data is read in byte length). If any bit has changed, the XOR operation will produce a 1, and, if no bits have changed, the XOR operation will produce a 0. If the result is non-zero, the input byte is saved along with the value of the internal counter (that is incremented each pass through the software timing loop). If the result is zero, the systems waits (e.g., executes no operation instructions) the same amount of time as if the data had to be saved, and the looping operation continues. The process continues until all eight inputs have changed at least twice, which enables measurement of a full 1/2 period of each input. Upon conclusion of the looping process, processor 26 analyzes the stored input bytes and internal counter states. There should be 2 to 16 saved inputs (for the 8 total sensors of FIG. 3) and counter states (if two or more inputs change at the same time, they are saved simultaneously). As will be understood by one of skill in the art, the stored values of the internal counter contains inforrnation l 5 determinative of the period of the signals received from sensing elements 24. By proper subtraction of internal counter values at times when an input bit has changed, the period may be calculated. Such periods calculated for each of the outputs of sensing elements is provided by processor 26 to microprocessor 10 (see, e.g., FIG. 1). From such calculated periods, a measure of the received light intensities may be calcnl~t~(l It should be noted that the sensing circuitry and methodology illustrated in FIG. 3 have been deterrnined to provide a practical and expedient manner in which to measure the light intensities received by sensing elements 24. In other embodiments, other circuits and methodologies are employed (other exemplary sensing schemes are described elsewhere herein).
2~ As fli.ccllc~e.-l above with reference to FIG. 1, one of fibers 7 measures light source 11, which may be through a neutral density filter, which serves to reduce the intensity of the received light in order mzlint:~in the intensity roughly in the range of the other received light intensities. Three of fibers 7 also are from perimeter receiver fiber optics R~ to R3 (see, e.g., FIG. 2) and also may pass through neutral density filters. Such receiving fibers 7 serve to provide data from which angle/height information and/or surface characteristics may be determined.
The rem~ining twelve fibers (of the preferred embodiment's total of 16 fibers) of fibers 7 pass through color filters and are used to produce the color measurement. In a CA 02238498 1998-0~-2~
WO 97/24587 ~ 4 PCTIUS97/0~)126 preferred embodiment, the color filters are Kodak Sharp Cutting Wratten Gelatin Filters, which pass light with wavelengths greater than the cut-off value of the filter (i.e., redish values), and absorb light with wavelengths less than the cut-off value of the filter (i.e., bluish values). "Sharp Cutting" filters are available in a wide variety of cut-off 5 frequencies/wavelengths, and the cut-off values generally may be selected by proper selection of the desired cut-off filter. In a preferred embodiment, the filter cut-off values are chosen to cover the entire visible spectrum and, in general, to have band spacings of approximately the visible band range (or other desired range) divided by the number of receivers/filters. As an example, 700 nanometers minus 400 nanometers, divided by l l bands (produced by twelve 10 color receivers/sensors), is roughly 30 nanometer band spacing.
With an array of cut-off filters as described above, and without being bound by theory or the specific embodiments described herein, the received optical spectrum may be measured/calculated by subtracting the light intensities of "adjacent" color receivers. For example, band I (400 nm to 430 nm) = (intensity of receiver 12) minus (intensity of receiver 15 l l), and so on for the remaining bands. Such an array of cut-off filters, and the intensity values that may result from filtering with such an array, are more fully described in connection with FIGS. 13A to 14B.
It should be noted here that in alternate embodiments other color filter arrangements are uti1i~ 1 For example, "notch" or bandpass filters may be utilized, such as may be 20 developed using Schott glass-type filters (whether constructed from separate longpass/shortpass filters or otherwise).
In a plerel.~d embodiment of the present invention, the specific characteristics of the light source, filters, sensors and fiber optics, etc., are norm~3li7~r~/calibrated by directing the probe towards, and measuring, a known color standard. Such norm~li7~tion/calibration may 25 be performed by placing the probe in a suitable fixture, with the probe directed from a predetermined position (i.e., height and angle) from the known color standard. Such measured norm~li7~tion/calibration data may be stored, for example, in a look-up table, and used by microprocessor lO to normalize or correct measured color or other data. Such procedures may be conducted at start-up, at regular periodic intervals, or by operator 3Q command, etc.
What should be noted from the above description is that the receiving and sensing fiber optics and cil~;uilly illustrated in FIC~. 3 provide a practical and expedient way to CA 02238498 1998 - 0~ - 2~
Wo 97/24587 - 1 5 - PCT/US97/00126 determine the color by measuring the intensity of the light reflected from the surface of the object being measured.
It also should be noted that such a system measures the spectral band of the reflected ~ light from the object, and once measured such spectral data may be utili~ed in a variety of ways. For example, such spectral data may be displayed directly as intensity-wavelength band values. In addition, tristimulus type values may be readily computed (through, for example, conventional matrix math), as may any other desired color values. In one particular embodiment useful in dental applications (such as for dental prostheses), the color data is output in the forrn of a closest match or matches of dental shade guide value(s). In a l O preferred embodiment, various existing shade guides (such as the shade guides produced by Vita Zahnfabrik) are characterized and stored in a look-up table, or in the graphics art industry Pantone color references, and the color measurement data are used to select the closest shade guide value or values, which may be accompanied by a confidence level or other suitable factor indicating the degree of closeness of the match or matches, including, for 1~ example, what are known as ~E values or ranges of AF values, or criteria based on standard deviations, such as standard deviation minimi7:~tion. In still other embodiments, the color measurement data are used (such as with look-up tables) to select materials for the composition of paint or ceramics such as for prosthetic teeth. There are many other uses of such spectral data measured in accordance with the present invention.
It is known that certain objects such as human teeth may fluoresce, and such optical characteristics also may be measured in accordance with the present invention. A light source with an ultraviolet comL)ol~ent may be used to produce more accurate color/optical data with respect to such objects. In certain embo-lim~ntc, a tungsten/halogen source (such as used in a preferred embodiment) may be combined with a UV light source (such as a mercury vapor, xenon or other fluorescent light source, etc.) to produce a light output capable of causing the object to fluoresce. Alternately, a separate UV light source, combined with a visible-light-blocking filter, may be used to illll-nin~te the object. Such a UV light source may be combined with light from a red LED (for example) in order to provide a visual indication of when the UV light is on and also to serve as an aid for the directional positioning of the probe ope~ g with such a light source. A second measurement may be tal~en using the UV light source in a manner analogous to that described earlier, with the band of the red LED or other supplemental light source being ignored. The second measurement may thus be used to produce an indication of the fluorescence of the tooth or other object being measured. With CA 02238498 1998-0~-2~
WO 97/24587 16 PCTtUS97/001~6 such a UV light source, a silica fiber optic (or other suitable material) typically would be required to transmit the light to the object (standard fiber optic materials such as glass and plastic in general do not propagate W light in a desired manner, etc.).
As described earlier, in certain preferred embodiments the present invention utilizes a plurality of perimeter receiver fiber optics spaced apart from and around a central source fiber optic to measure color and determine information regarding the height and angle of the probe with respect to the surface of the object being measured, which may include other surface characteristic information, etc. Without being bound by theory, certain principles underlying this aspect of the present invention will now be described with reference to FIGS. 4A to 4C.
FIG. 4A illustrates a typical step index fiber optic consisting of a core and a cladding.
For this discussion, it is ~sllm~ -cl that the core has an index of refraction of n0 and the cladding has an index of refraction of nn Although the following discussion is directed to "step index" fibers, it will be appreciated by those of skill in the art that such discussion generally is applicable for gradient index fibers as well.
In order to propagate light without loss, the light must be incident within the core of the fiber optic at an angle greater than the critical angle, which may be ~ csGIlted as Sin~
' {nl/n0}, where n0 is the index of refraction of the core and nl is the index of refraction of the cladding. Thus, all light must enter the fiber at an acceptance angle equal to or less than phi, with phi = 2 x Sin~l {l(no2 - n~2)}, or it will not be propagated in a desired manner.
For light entering a fiber optic, it must enter within the acceptance angle phi.Similarly, when the light exits a fiber optic, it will exit the fiber optic within a cone of angle phi as illustrated in FIG. 4A. The value ~(n02 - nl2) is referred to as the apelLulc of the fiber optic. For example, a typical fiber optic may have an ~e.lulc of 0.5, and an acceptance angle of 60~.
Consider using a fiber optic as a light source. One end is illnmin~tt~ by a light source (such as light source 1 1 of FIG. 1), and the other is held near a surface. The fiber optic will emit a cone of light as illustrated in FIG. 4A. If the fiber optic is held perpendicular to a surface it will create a circular light pattern on the surface. As the fiber optic is raised, the radius r of the circle will inerease. As the fiber optic is lowered, the radius of the light pattern 30 will deerease. Thus, the intensity of the light (light energy per unit area) in the illnmin~t~
circular area will increase as the fiber optic is lowered and will decrease as the fiber optic is raised.

CA 02238498 1998-0~-2~

The same principle generally is true for a fiber optic being utilized as a receiver.
Consider mounting a light sensor on one end of a fiber optic and holding the other end near an ilhlmin~ted surface. The fiber optic can only propagate light without loss when the light entering the fiber optic is incident on the end of the fiber optic near the surface if the light 5 enters the fiber optic within its acceptance angle phi. A fiber optic utilized as a light receiver - near a surface will only accept and propagate light from the circular area of radius r on the surface. As the fiber optic is raised from the surface, the area increases. As the fiber optic is lowered to the surface, the area decreases.
Consider two fiber optics parallel to each other as illustrated in FIG. 4B. For lQ simplicity of discussion, the two fiber optics illustrated are identical in size and apellul~. The following discussion, however, generally would be applicable for fiber optics that differ in size and ~ellul~. One fiber optic is a source fiber optic, the other fiber optic is a receiver fiber optic. As the two fiber optics are held perpendicular to a surface, the source fiber optic emits a cone of light that ill--min~tes a circular area of radius r. The receiver fiber optic can only accept light that is within its acceptance angle phi, or only light that is received within a cone of angle phi. If the only light available is that emitted by the source fiber optic, then the only light that can be accepted by the receiver fiber optic is the light that strikes the surface at the intersection of the two circles as illustrated in FIG. 4C. As the two fiber optics are lifted from the surface, the proportion of the intersection of the two circular areas relative to the circular area of the source fiber optic increases. As they near the surface, the proportion of the intersection of the two circular areas to the circular area of the source fiber optic decreases. If the fiber optics are held too close to the surface, the circular areas will no longer intersect and no light emitted from the source fiber optic will be received by the receiver fiber optic.
As discussed earlier, the intensity of the light in the circular area illl-rnin~t~ l by the source fiber increases as the fiber is lowered to the surface. The intersection of the two cones, however, decreases as the fiber optic pair is lowered. Thus, as the fiber optic pair is lowered to a surface, the total intensity of light received by the receiver fiber optic increases to a maximal value, and then decreases sharply as the fiber optic pair is lowered still further to the surface. ~ventually, the intensity will decrease essentially to zero ~assuming the object being measured is not translucent, as described more fully herein), and will remain essentially zero until the fiber optic pair is in contact with the surface. Thus, as a source-receiver pair of fiber optics as described above are positioned near a surface and as their height is varied, the CA 02238498 1998-05-2~

intensity of light received by the receiver fiber optic reaches a maximal value at a peaking or "critical height" hc.
Again without being bound by theory, an interesting property of the critical height hc has been observed. The critical height hc is a function primarily of the geometry of fixed 5 parameters, such as fiber apertures, fiber diameters and fiber spacing. Since the receiver fiber optic in the illustrated arrangement is only detecting a maximum value and not attempting to quantify the value, its maximum in general is independent of the surface characteristics. It is only necessary that the surface reflect sufficient light from the intersecting area of the source and receiver fiber optics to be within the detection range of the receiver fiber optic light 10 ~sensor. Thus, in general red or green or blue or any color surface will all exhibit a maximum at the same critical height hc. Similarly, smooth reflecting surfaces and rough surfaces also will have varying intensity values at the maximal value, but generally speaking all such surfaces will exhibit a maximum at the same critical height hc. The actual value of the light intensity will be a function of the color of the surface and of the surface characteristics, but 15 the height where the maximum intensity value occurs in general will not. This is particularly true with respect to similar types or categories of materials such as teeth, industrial objects, etc.
Although the above discussion has focused on two fiber optics perpendicular to asurface, similar analysis is applicable for fiber optic pairs at other angles. When a fiber optic 20 is not perpendicular to a surface, it generally illllminz~tes an elliptica} area. Similarly, the acceptance area of a receiver fiber optic generally becomes elliptical. As the fiber optic pair is moved closer to the surface, the receiver fiber optic also will detect a maximal value at a critical height independent of the surface color or characteristics. The maximal intensity value measured when the fiber optic pair is not perpendicular to the surface, however, will be 25 less than the maximal intensity value measured when the fiber optic pair is perpendicular to the surface.
Referring now to FIGS. 5A and SB, the intensity of light received as a fiber optic source-receiver pair is moved to and from a surface will now be described. FIG. SA
illustrates the intensity of the received light as a function of time. Corresponding FIG. SB
33 illustrates the height of the fiber optic pair from the surface of the object being measured.
FIGS. 5A and 5B illustrate (for ease of discussion) a relatively uniform rate of motion of the fiber optic pair to and from the surface of the object being measured (although similar illustrations/analysis would be applicable for non-uniform rates as well3.

CA 02238498 l998-0~-2~

FIG. 5A illustrates the intensity of received light as the fiber optic pair is moved to and then from a surface. While FIG. SA illustrates the intensity relationship for a single receiver fiber optic, similar intensity relationships would be expected to be observed for other receiver fiber optics, such as, for example, the multiple receiver fiber optics of FIGS. 1 and 2.
5 In general with the preferred embodiment described above, all fifteen fiber optic receivers (of fibers 7) will exhibit curves similar to that illustrated in FIG. 5A.
FIG. SA illustrates five regions. In region 1, the probe is moved towards the surface of the object being measured, which causes the received light intensity to increase. In region 2, the probe is moved past the critical height, and the received light intensity peaks and then 10 falls off sharply. In region 3, the probe essentially is in contact with the surface of the object being measured. As illustrated, the received intensity in region 3 will vary depending upon the translucence of the object being measured. If the object is opaque, the received light intensity will be very low, or almost zero (perhaps out of range of the sensing circuitry). If the object is translucent, however, the light intensity will be quite high, but in general should 15 be less than the peak value. In region 4, the probe is lifted and the light intensity rises sharply to a maximum value. In region S, the probe is lifted further away from the object, and the light intensity decreases again.
As illustrated, two peak intensity values (discussed as Pl and P2 below) should be detected as the fiber optic pair moves to and from the object at the critical height hc. If peaks 20 Pl and P2 produced by a receiver fiber optic are the same value, this generally is an indication that the probe has been moved to and from the surface of the object to be measured in a consistent manner. If peaks P1 and P2 are of different values, then these may be an indication that the probe was not moved to and from the surface of the object in a desired manner, or that the surface is curved or textured, as described more fully herein. In such a 2~ case, the data may be considered suspect and rejected. In addition, peaks Pl and P2 for each of the perimeter fiber optics (see, e.g., FIG. 2) should occur at the same critical height (assuming the geometric attributes of the perimeter fiber optics, such as aperture, diameter and spacing from the source fiber optic, etc.). Thus, the perimeter fiber optics of a probe moved in a consistent, perpendicular manner to and from the surface of the object being 30 measured should have peaks P 1 and P2 that occur at the same critical height. Monitoring receiver fibers from the perimeter receiver fiber optics and looking for simultaneous (or near simlllt~neous, e.g., within a predetermined range) peaks Pl and P2 provides a mechanism for CA 02238498 1998-0~-2~
WO 97124587 2~ PCT/IJS97/(~0126 determining if the probe is held at a desired perpendicular angle with respect to the object being measured.
In addition, the relative intensity level in region 3 serves as an indication of the level of translucency of the object being measured. Again, such principles generally are applicable 5 to the totality of receiver fiber optics in the probe (see, e.g., fibers 7 of EiIGS. 1 and 3). Based on such principles, measurement techniques in accordance with the present invention will now be described.
FIG. 6 is a flow chart illustrating a measuring technique in accordance with thepresent invention. Step 49 indicates the start or beginning of a color/optical mea~u~ lent.
10 During step 49, any equipment initi~ tion, diagnostic or setup procedures may be performed. Audio or visual information or other indicia may be given to the operator to inform the operator that the system is available and ready to take a measurement. Initiation of the color/optical measurement commences by the operator moving the probe towards the object to be measured, and may be accompanied by, for example, activation of switch 17 (see 15 FIG. 1).
In step 50, the system on a continUing basis monitors the intensity levels for the receiver fiber optics (see, e.g., fibers 7 of FIG. 1). If the intensity is rising, step 50 is repeated until a peak is detected. If a peak is detected, the process proceeds to step 52. In step 52, measured peak intensity P1, and the time at which such peak occurred, are stored in memory 20 (such as in memory included as a part of microprocessor 10), and the process proceeds to step 54. In step 54, the system continues to monitor the intensity levels of the receiver fiber optics. If the intensity is falling, step 54 is repeated. If a "valley" or plateau is rl~otectf~-l (i.e., the intensity is no longer falling, which generally indicates contact or near contact with the object), then the process proceeds to step 56. In step 56, the measured surface intensity (IS) is 25 stored in memory, and the process proceeds to step 58. In step 58, the system continues to monitor the intensity levels of the receiver fibers. If the intensity is rising, step 58 is repeated until a peak is detected. If a peak is ~letecte(l, the process proceeds to step 60. In step 60, measured peak intensity P2, and the time at which such peak occurred, are stored in memory, and the process proceeds to step 62. In step 62, the system continues to monitor the intensity 30 levels of the receiver fiber optics. Once the received intensity levels begin to fall from peak P2, the system perceives that region 5 has been entered (see, e.g., FIG. SA), and the process proceeds to step 64.

CA 02238498 1998-0=.-2=.
W 097124587 21 PCT~US97/00126 In step 64, the system, under control of microprocessor 10, may analyze the collected data taken by the sensing circuitry for the various receiver fiber optics. In step 64, peaks P1 and P2 of one or more of the various fiber optics may be compared. If any of peaks P 1 and P2 for any of the various receiver fiber optics have unequal peak values, then the data may be 5 rejected, and the entire color measuring process repeated. Again, unequal values of peaks P1 and P2 may be indicative, for example, that the probe was moved in a non-perpendicular or otherwise unstable manner (i.e., angular or lateral movement), and, for example, peak Pl may be representative of a first point on the object, while peak P2 may be representative of a second point on the object. As the data is suspect, in a preferred embodiment of the present 10 invention, data taken in such circllmst~nees are rejected in step 64.
If the data are not rejected in step 64, the process proceeds to step 66. In step 66, the system analyzes the data taken from the neutral-density-filtered receivers from each of the perimeter fiber optics (e.g., Rl to R3 of FIG. 2). If the peaks of the perimeter fiber optics did not occur at or about the same point in time, this may be indicative, for example, that the 1~ probe was not held perpendicular to the surface of the object being measured. As non-perpendicular ~lignment of the probe with the surface of the object being measured may cause suspect results, in a preferred embodiment of the present invention, data taken in such cil-;u~ ances are rejected in step 66. In one preferred embodiment, detection ofsimnlt~neous or near simlllt~nt~ous peaking (peaking within a predetermined range of time) 20 serves as an acceptance criterion for the data, as perpendicular alignment generally is indicated by simultaneous or near simultaneous peaking of the perimeter fiber optics. In other embodiments, step 66 includes an analysis of peak values Pl and P2 of the perimeter fiber optics. In such embodiments, the system seeks to determine if the peak values of the perimeter fiber optics (perhaps normalized with any initial calibration data) are equal within a 25 defined range. If the peak values of the perimeter fiber optics are within the defined range, the data may be accepted, and if not, the data may be rejected. In still other embodiments, a combination of simult~neous peaking and equal value detection are used as acceptance/rejection criteria for the data, and/or the operator may have the ability (such as through key pad switches 12~ to control one or more of the acceptance criteria ranges. With 30 such capability, the sensitivity of the system may be controllably altered by the operator depending upon the particular application and operative environment, etc.
If the data are not rejected in step 66, the process proceeds to step 68. In step 68, the data may be processed in a desired manner to produce output color/optical measurement data.

CA 02238498 1998-0~-2~
WO 97/24587 - 22 - PCT/IJS97/0~126 For example, such data may be normalized in some manner, or adjusted based on temperature compensation or other data detected by the system. The data also may be converted to different display or other formats, depending on the intended use of the data. In addition, the data indicative of the translucence of the object also may be quantified and/or displayed in step 68. After step 68, the process may proceed to starting step 49, or the process may be termin~t~-l, etc.
In accordance with the process illustrated in FIG. 6, three light intensity values (Pl, P2 and IS) are stored per receiver fiber optic to make color and translucency, etc., measurements.
If stored peak values Pl and P2 are not equal (for some or all of the receivers), this is an 10 indication that the probe was not held steady over one area, and the data may be rejected (in other embodiments, the data may not be rejected, although the resulting data may be used to produce an average of the measured data). In addition, peak values P1 and P2 for the three neutral density perimeter fiber optics should be equal or approximately equal; if this is not the case, then this is an indication that the probe was not held perpendicular or a curved surface is 15 being measured. In other embodiments, the system atLe~ t~ to compensate for curved surfaces and/or non-perpendicular angles. In any event, if the system cannot make a color/optical measurement, or if the data is rejected because peak values P1 and P2 are unequal to an unacceptable degree, then the operator is notified so that another measurement or other action may be taken (such as adjust the sensitivity).
20 - With a system constructed and operating as described above, color/optical measurements may be taken of an object, with accepted data having height and angular dependencies removed. Data not taken at the critical height, or data not taken with the probe perpendicular to the surface of the object being measured, etc., are rejected in a preferred embodiment of the present invention. In other embodiments, data received from the 25 perimeter fiber optics may be used to calculate the angle of the probe with respect to the surface of the object being measured, and in such embodiments non-perpendicular or curved :surface data may be compensated instead of rejected. It also should be noted that peak values P1 and P2 for the neutral density perimeter fiber optics provide a measure of the lllmin~nee (gray value) of the surface of the object being measured, and also may serve to quantify the 30 color value.
The translucency of the object being measured may be quantified as a ratio or percentage, such as, for example, (IS/PI) X 100~. In other embodiments, other methods of CA 02238498 1998-0~-2~

quantifying translucency data provided in accordance with the present invention are utilized, such as some other arithmetic function utilizing IS and P1 or P2, etc.
In another particular aspect of the present invention, data generated in accordance with the present invention may be used to implement an automated material mixing/generation 5 machine. Certain objects/materials, such as dental prostheses, are made from porcelain or - other powders/materials that may be combined in the correct ratios to form the desired color of the object/prosthesis. Certain powders often contain pigments that generally obey Beer' s law and/or act in accordance with Kubelka-Munk equations and/or Saunderson equations (if needed) when mixed in a recipe. Color and other data taken from a measurement inl O accordance with the present invention may be used to determine or predict desired quantities of pigment or other materials for the recipe. Porcelain powders and other materials are available in different colors, opacities, etc. Certain objects, such as dental prostheses, may be layered to ~im~ te the degree of translucency of the desired object (such as to ~imlll~tP a human tooth). Data generated in accordance with the present invention also may be used to l 5 determine the thickness and position of the porcelain or other material layers to more closely produce the desired color, translucency, surface characteristics, etc. In addition, based on fluorescence data for the desired object, the material recipe may be adjusted to include a desired quantity of fluorescing-type material. In yet other embodiments, surfacecharacteristics (such as texture~ inforrnation (as more fully described herein) may be used to add a texturing material to the recipe, all of which may be carried out in accordance with the present invention.
For more information regarding such pigment-material recipe type technology, reference may be made to: "The Measurement of Appearance," Second Edition, edited by Hunter and Harold, copyright 1987; "Principles of Color Technology," by Billmeyer and Saltzman, copyright 1981; and "Pigment Handbook," edited by Lewis, copyright 1988. All of the foregoing are believed to have been published by John Wiley & Sons, Inc., New York, NY, and all of which are hereby incorporated by reference.
In certain operative environments, such as dental applications, cont:~min~ion of the probe is of concern. In certain embo~lim~.n~ of the present invention, implements to reduce such contz~min~tion are provided.
FIGS.7A and 7B illustrate a protective cap that may be used to fit over the end of probe tip 1. Such a protective cap consists of body 80, the end of which is covered by optical window 82, which in a preferred embodiment consists of a structure having a thin sapphire CA 02238498 1998 - 0~ - 2~

Wo 97/24587 - 24 - PCT/US97/00126 window. In a preferred embodiment, body 80 consists of stainless steel. Body 80 fits over the end of probe tip I and may be held into place by, for example, indentations formed in body 80, which fit with ribs 84 ~which may be a spring clip or other retainer) formed on probe tip 1. In other embodiments, other methods of affixing such a protective cap to probe tip I
s are utili7Pfl The protective cap may be removed from probe tip I and sterilized in a typical autoclave, hot steam, chemiclave or other sterilizing system.
The thickness of the sapphire window should he less than the critical height of the probe in order to preserve the ability to detect peaking in accordance with the present invention, and preferably has a thickness less than the minim~l height at which the source/receiver cones overlap (see FIGS. 4B and 4C). It also is believed that sapphire windows may be manufactured in a reproducible manner, and thus any light attenuation from one cap to another may be reproducible. In addition, any distortion of the color/optical measurements produced by the s~yhhe window may be calibrated out by microprocessor 10.
Similarly, in other embodiments body 80 has a cap with a hole in the center (as ls opposed to a sapphire window), with the hole positioned over the fiber optic source/receivers.
The cap with the hole serves to prevent the probe from coming into contact with the surface, thereby reducing the risk of cont~ n~tion. It should be noted that, with such embo~;mertts, the hole is positioned so that light from/to the light source/receiver elements of the probe tip is not adversely affected by the cap.
FIGS. 8A and 8B illustrate another embodiment of a removable probe tip that may be used to reduce c~ tion in accordance with the present invention. As illustrated in F~G.
8A, probe tip 88 is removable, and includes four (or a different number, depending upon the application) fiber optic connectors 90, which are positioned within optical guard 92 coupled to connector g4. Optical guard 92 serves to prevent "cross talk" between adjacent fiber 2s optics. As illustrated in FIG. 8B, in this embodiment removable tip 88 is secured in probe tip housing 93 by way of spring clip 96 (other removable ret~ining implements are utilized in other embodiments). Probe tip housing 93 may be secured to base conlle~;lol 95 by a screw or other conventional fitting. It should be noted that, with this embodiment, different size tips may be provided for different applications, and that an initial step of the process may be to install the ~ ly-sized (or fitted tip) for the particular application. Removable tip 88 also may be sterilized in a typical autoclave, hot steam, chemiclave or other sterilizing system, or disposed of. In addition, the entire probe tip assembly is constructed so that it may be readily disassembled for cleaning or repair. In certain embodiments the light source/receiver elements of the removable tip are SU~STITUTE S~IEET (RULE 26) CA 02238498 1998-0~-2~
W097/24587 - 25 - rCTlUS97100126 constructed of glass, silica or similar materials, thereby making them particularly suitable for autoclave or similar high temperature/pressure cleaning methods, which in certain other embodiments the light source/receiver elements of the removable tip are constructed of plastic or other similar materials, which may be of lower cost, thereby making them 5 particularly suitable for disposable-type removable tips, etc.
In still other embodiments, a plastic, paper or other type shield (which may be disposable, cleanable/reusable or the like) may be used in order to address any contzlmin~tion concerns that may exist in the particular application- In such embodiments, the methodology may include positioning such a shield over the probe tip prior to taking color/optical l O measurements, and may include removing and disposing/cleaning the shield after taking color/optical measurements, etc.
With reference to FIG. 9, a tristimulus embodiment of the present invention will now be described. In general, the overall system depicted in FIG. 1 and discussed in detail elsewhere herein may be used with this embodiment. FIG. 9 illustrates a cross section of the l 5 probe tip fiber optics used in this embodiment.
Probe tip 100 includes central source fiber optic 106, surrounded by (and spaced apart from) three perimeter receiver fiber optics 104 and three color receiver fiber optics 102.
Three perimeter receiver fiber optics 104 are optically coupled to neutral density filters and serve as height/angle sensors in a manner analogous to the embodiment describe above.
20 Three color receiver fiber optics are optically coupled to suitable tristimulus filters, such as red, green and blue filters. With this embodiment, a measurement may be made of tristimulus color values of the object, and the process described with reference to FIG. 6 generally is applicable to this embodiment. In particular, perimeter fiber optics 104 may be used to detect simultaneous peaking or otherwise whether the probe is perpendicular to the object being 2~ measured. In addition, taking color measurement data at the critical height also may be used with this embodiment.
FIG. lOA illustrates an embodiment of the present invention, similar to the embodiment discussed with reference to FIG. 9. Probe tip 100 includes central source fiber optic 106, surrounded by (and spaced apart from) three perimeter receiver fiber optics 104 30 and a plurality of color receiver fiber optics 102. The number of color receiver fiber optics 102, and the filters associated with such receiver fiber optics 102, may be chosen based upon the particular application. As with the embodiment of FIG. 9, the process described with reference to FIG. 6 generally is applicable to this embodiment.

CA 02238498 1998-0~-2 W097/24587 - 26 - PCTrUS97/0012 FIG. 10B illustrates an embodiment of the present invention in which there are aplurality of receiver fiber optics that surround central source fiber optic 240. The receiver fiber optics are arranged in rings surrounding the central source fiber optic. FIG. 10B
illustrates three rings of receiver fiber optics (consisting of fiber optics 242, 244 and 246, respectively), in which there are six receiver fiber optics per ring. The rings may be arranged in successive larger circles as illustrated to cover the entire area of the end of the probe, with the distance from each receiver fiber optic within a given ring to the central fiber optic being equal (or approximately so). Central fiber optic 240 is utilized as the light source fiber optic and is connected to the light source in a manner similar to light source fiber optic 5 illustrated 10 in FIG. 1.
The plurality of receiver fiber optics are each coupled to two or more fiber optics in a manner similar to the arrangement illustrated in FIG. 1 for splicing connector 4. One fiber optic from such a splicing connector for each receiver fiber optic passes through a neutral density filter and then to light sensor circuitry similar to the light sensor circuitry illustrated in 15 l~IG. 3. A second fiber optic from the splicing connector per receiver fiber optic passes through a Sharp Cutting Wrattan Gelatin Filter and then to light sensor Cil~;uitly as discussed elsewhere herein. Thus, each of the receiver fiber optics in the probe tip includes both color measuring elements and neutral light measuring or "perimeter" elements.
FIG. 10D illustrates the geometry of probe 260 (such as described above) 20 ilh-min~ting an area on flat diffuse surface 272. Probe 260 creates light pattern 262 that is reflected diffusely from surface 272 in uniform hemispherical pattern 270. With such a reflection pattern, the reflected light that is incident upon the receiving elements in the probe will be equal (or nearly equal3 for all elements if the probe is perpendicular to the surface as described above herein.
2~ ~IG 10C illustrates a probe illllmin~ting rough surface 268 or a suRace that reflects light spectrally. Spectral reflected light will exhibit hot spots or regions where the reflected light intensity is considerably greater than it is on other areas. The reflected light pattern will be uneven when compared to a smooth surface as illustrate in FIG. 10D.
Since a probe as illustrated in FIG. 10B has a plurality of receiver fiber optics 30 arranged over a large surface area, the probe may be utilized to determine the suRace texture of the surface as well as being able to measure the color and translucency, etc., of the surface as described earlier herein. If the light intensity received by the receiver fiber optics is equal for all fiber optics within a given ring of receiver fiber optics, then generally the surface is CA 02238498 1998 - 0~ - 2~
wo 97r24s87 - 27 - PCT/US97/00126 diffuse and smooth. If, however, the light intensity of receiver fibers in a ring varies with respect to each other, then generally the surface is rough or spectral. By comparing the light intensities measured within receiver fiber optics in a given ring and from ring to ring, the texture and other characteristics of the surface may be quantified.
FIG. 11 illustrates an embodiment of the present invention in which linear optical sensors and a color gradient filter are utilized instead of light sensors 8 (and filters 22, etc.).
Receiver fiber optics 7, which may be optically coupled to probe tip 1 as with the embodiment of FIG. 1, are optically coupled to linear optical sensor 112 through color gradient filter 110. In this embodiment, color gradient filter 110 may consist of series of l O narrow strips of cut-off type filters on a transparent or open substrate, which are constructed so as to positionally correspond to the sensor areas of linear optical sensor 1 12. An example of a commercially available linear optical sensor 112is Texas In~ u,lents part number TSL213, which has 61 photo diodes in a linear array. Light receiver fiber optics 7 are arranged correspondingly in a line over linear optical sensor 112. The number of receiver l 5 fiber optics may be chosen for the particular application, so long as enough are included to more or less evenly cover the full length of color gradient filter l lO. With this embodiment, the light is received and output from receiver fiber optics 7, and the light received by linear optical sensor 112 is integrated for a short period of time (determined by the light intensity, filter characteristics and desired accuracy). The output of linear array sensor 112 is digitized by ADC 114 and output to microprocessor 116 (which may the same processor as microprocessor 10 or another processor).
In general, with the embodiment of FIG. 11, perimeter receiver fiber optics may be used as with the embodiment of FIG. 1, and in general the process described with reference to E~IG. 6 is applicable to this embodiment.
FIG. 12 illustrates an embodiment of the present invention in which a matrix optical sensor and a color filter grid are utilized instead of light sensors 8 (and filters 22, etc.).
Receiver hber optics 7, which may be optically coupled to probe tip 1 as with the embodiment of FIG. 1, are optically coupled to matrix optical sensor 122 through filter grid 120. Filter grid 120is a filter array consisting of a number of small colored spot filters that pass narrow bands of visible light. Light from receiver fiber optics 7 pass through corresponding filter spots to corresponding points on matrix optical sensor 122. In this embodiment, matrix optical sensor 122 may be a monochrome optical sensor array, such as CCD-type or other type of light sensor element such as may be used in a video camera. The CA 02238498 l998-0~-2~

output of matrix optical sensor 122 is digitized by ADC 124 and output to microprocessor 126 (which may the same processor as microprocessor 10 or another processor). Under control of microprocessor 126, matrix optical sensor 126 collects data from receiver fiber optics 7 through color filter grid 120.
In general, with the embodiment of FIG. 12, perimeter receiver fiber optics may be used as with the embodiment of FIG. 1, and in general the process described with reference to F~G. 6 also is applicable to this embodiment.
As will be clear from the foregoing description~ with the present invention a variety of types of spectral color/optical photometers (or tristimulus-type colorimeters) may be constructed, with perimeter receiver fiber optics used to collect color/optical data essentially free from height and angular deviations. In addition, in certain embodiments, the present invention enables color/optical measurements to be taken at a critical height from the surface of the object being measured, and thus color/optical data may be taken without physical contact with the object being measured (in such embodiments, the color/optical data is taken only by passing the probe through region 1 and into region 2, but without n~cç~rily going into region 3 of FIGS. 5A and 5B). Such embodiments may be utilized if contact with the surface is undesirable in a particular application. In the embodiments described earlier, however, physical contact (or near physical contact) of the probe with the object may allow all five regions of FIGS. SA and 5B to be utilized, thereby enabling measurements to be taken such that translucency information also may be obtained. Both types of embodiments generally are within the scope of the invention described herein.
Additional description will now be provided with respect to cut-off filters of the type described in connection with the preferred embodiment(s) of FIGS. 1 and 3 (such as filters 22 of FIG. 3). FIG. 13A illustrates the properties of a single Kodak Sharp Cutting Wratten Gelatin Filter discussed in eonnection with FIG. 3. Such a cut-off filter passes light below a cut-off frequency (i.e., above a cut-off wavelength). Such filters may be manufactured to have a wide range of cut-off frequencies/wavelengths. FIG. 1 3B illustrates a number of such filters, twelve in a pl~relled embodiment, with cut-off frequencies/wavelengths ehosen so that essentially the entire visible band is eovered by the eollection of cut-off filters.
FIGS. 14A and 14B illustrate exemplary intensity mea~ulc;lllents using a cut-off filter arrangement such as illustrated in FIG. 13B, first in the case of a white surface being measured (FIG. 14A), and also in the ease of a blue surface being measured (FIG. 14B~. As illustrated in FIG. 14A, in the case of a white surface, the neutrally filtered perimeter fiber CA 02238498 1998-0~-2~

optics, which are used to detect height and angle, etc., generally will produce the highest intensity (although this depends at least in part upon the characteristics of the neutral density filters). As a result of the stepped cut-off filtering provided by filters having the characteristics illustrated in FIG. 13B, the rem~ining intensities will gradually decrease in 5 value as illustrated in FTC~. 14A. In the case of a blue surface, the intensities will decrease in value generally as illustrated in FIG. 14B- Regardless of the surface, however, the intensities out of the filters will always decrease in value as illustrated, with the greatest intensity value being the output of the filter having the lowest wavelength cut-off value (i.e., passes all visible light up to blue), and the lowest intensity value being the output of the filter having the l O highest wavelength cut-off (i.e., passes only red visible light). As will be understood from the foregoing description, any color data detected that does not fit the decreasing intensity profiles of FIGS. 14A and 14B may be cletected as an abnormality, and in certainembodiments detection of such a condition results in data rejection, generation of an error message or initiation of a diagnostic routine, etc.
l 5 Reference should be made to the FIGS. I and 3 and the related description for a detailed discussion of how such a cut-off filter arrangement may be utilized in accordance with the present invention.
FIG. 15 is a flow chart illustrating audio tones that may be used in certain p,efe.lt;d embodiments of the present invention. It has been discovered that audio tones (such as tones, 20 beeps, voice or the like such as will be described) present a particularly useful and instructive means to guide an operator in the proper use of a color measuring system of the type described herein.
The operator may initiate a color/optical measurement by activation of a switch (such as switch 17 of FIG. 1) at step 150. Thereafter, if the system is ready (set-up, initi~li7.o-1, 25 calibrated, etc.), a lower-the-probe tone is emitted (such as through speaker 16 of FIG. 1) at step 152. The system attempts to detect peak intensity P1 at step 154. If a peak is detected, at step 156 a determination is made whether the measured peak P1 meets the applicable criteria (such as discussed above in connection with FIGS. SA, 5B and 6). If the measured peak P1 is accepted, a ~lrst peak acceptance tone is generated at step 160. If the measured peak P1 is not ~ 30 accepted, an unsuccessful tone is generated at step 158, and the system may await the operator to initiate a further color/optical measurement. Assuming that the first peak was accepted, the system attempts to detect pealc intensity P2 at step 162. If a second peak is detected, at step 164 a determination is made whether the measured peak P2 meets the CA 02238498 1998-0~-2~
WO 97/24587 _ 30 rCT/US97/00126 ~pplicable criteria. If the measured peak P2 is accepted the process proceeds to color calculation step 166 (in other embodiments, a second peak acceptance tone also is generated at step 166). If the measured peak P2 is not accepted, an unsuccessful tone is generated at step 158, and the system may await the operator to initiate a further color/optical measurement. Assuming that the second peak was accepted, a colorloptical calculation is made at step 166 (such as, for example, microprocessor 10 of FIG. 1 processing the data output from light sensors 8, etc.). At step 168, a determination is made whether the color calculation meets the applicable criteria. If the color calculation is accepted, a successful tone is generated at step 170. If the color calculation is not accepted, an unsuccessful tone is l O generated at step 158, and the system may await the operator to initiate a further color/optical measurement.
With unique audio tones presented to an operator in accordance with the particular operating state of the system, the operator's use of the system may be greatly facilitated.
Such audio information also tends to increase operator satisfaction and skill level, as, for example, acceptance tones provide positive and encouraging feedback when the system is operated in a desired manner.
Further embodiments of the present invention will now be described with reference to FIGS. 16-18. The previously described embodiments generally rely on movement of the probe with respect to the object being measured. While such embodiments provide great utility in many applications, in certain applications, such as robotics, industrial control, automated manufacturing, etc. (such as positioning the object and/or the probe to be in proximity to each other, detecting color/optical pl-ope. lies of the object, and then directing the ob~ect, e.g., sorting, based on the detected color/optical plopellies, for further industrial processing, p~c~ging, etc.) it may be desired to have the measurement made with the probe held or positioned substantially stationary above the surface of the object to be measured (in such embodiments, the positioned probe may not be handheld as with certain otherembodiments).
FIG. 16 illustrates such a further embodiment. The probe of this embodiment includes a plurality of perimeter sensors and a plurality of color sensors coupled to receivers 312 - 320. The color sensors and related components, etc., may be constructed to operate in a manner analogous to previously described embodiments. For example, fiber optic cables or the like may couple light from source 310 that is received by receivers 312 - 320 to sharp cut-off ~llters, with the received light measured over precisely defined wavelengths (see, e.g., CA 02238498 1998 - 0~ - 2~

l~IGS. 1, 3 and 11-14 and related description). Color/optical characteristics of the object may be determined from the plurality of color sensor measurements, which may include three such sensors in the case of a tristimulus instrument, or 8, 12, 15 or more color sensors for a more full bandwidth system (the precise number may be determined by the desired color resolution, etc.).
With this embodiment, a relatively greater number of perimeter sensors are utilized (as opposed, for example, to the three perimeter sensors used in certain ~ e~ledembodiments of the present invention). As illustrated in FIG. 16, a plurality of triads of receivers 312 - 320 coupled to perimeter sensors are ~l~ili7P~l, where each triad in the preferred l 0 implementation consists of three fiber optics positioned equal distance from light source 310, which in the preferred embodiment is a central light source fiber optic. The triads of perimeter receivers/sensors may be configured as concentric rings of sensors around the central light source fiber optic. In FIG. 16, ten such triad rings are illustrated, although in other embodiments a lesser or greater number of triad rings may be lltili7~1, depending upon l 5 the desired accuracy and range of operation, as well as cost considerations and the like.
The probe illustrated in FIG. 16 may operate within a range of heights (i.e., distances from the object being measured). As with earlier embodiments, such height characteristics are determined primarily by the geometry and constituent materials of the probe, with the spacing of the minim:~l ring of perimeter sensors determining the minim~l height, and the spacing of the maximal ring of perimeter sensors determining the maximum height, etc. It therefore is possible to construct probes of various height ranges and accuracy, etc., by varying the number of perimeter sensor rings and the range of ring distances from the central source fiber optic. It should be noted that such embodiments may be particularly suitable when measuring similar types of materials, etc.
As described earlier, the light receiver elements for the plurality of receivers/perimeter sensors may be individual elements such as Texas Instruments TSL230 light-to-frequency converters, or may be constructed with rectangular array elements or the like such as may be found in a CCD camera. Other broadband-type of light measuring elements are utilized in other embodiments. Given the large number of perimeter sensors used in such embodiments ~ 30 ~such as 30 for the embodiment of FIG. 16), an array such as CCD camera-type sensing elements may be desirable. It should be noted that the absolute intensity levels of light measured by the perimeter sensors is not as critical to such embodiments of the present CA 02238498 1998-0~-2~

invention; in such embodiments differences between the triads of perimeter light sensors are advantageously utilized in order to obtain optical measurements.
Optical measurements may be made with such a probe by holding/positioning the probe near the surface of the object being measured (i.e., within the range of acceptable 5 heights of the particular probe). The light source providing light to light source 310 is turned on and the reflected light received by receivers 312 - 320 (coupled to the perimeter sensors) is measured. The light intensity of the rings of triad sensors is compared. Generally, if the probe is perpendicular to the surface and if the surface is flat, the light intensity of the three sensors of each triad should be approximately will be equal. If the probe is not perpendicular l o to the surface or if the surface is not flat, the light intensity of the three sensors within a triad will not be equal. It is thus possible to determine if the probe is perpendicular to the surface being measured, etc. It also is possible to compensate for non-perpendicular surfaces by mathematically adjusting the light intensity measurements of the color sensors with the variance in measurements of the triads of perimeters sensors.
Since the three sensors forming triads of sensors are at different distances (radii) from central light source 310, it is expected that the light intensities measured by light receivers 312 -320 and the perimeter sensors will vary. ~or any given triad of sensors, as the probe is moved closer to the surface, the received light intensity will increase to a maximum and then sharply decrease as the probe is moved closer to the surface. As with previously-described 20 embodiments, the intensity decreases rapidly as the probe is moved less than the critical height and decreases rapidly to zero or almost zero for opaque objects. The value of the critical height depends principally upon the distance of the particular receiver from light source 31~. Thus, the triads of sensors will peak at different critical heights. By analyzing the variation in light values received by the triads of sensors, the height of the probe can be 25 determined. Again, this is particularly true when measuring similar types of materials.
The system initially is calibrated against a neutral background (e.g., a gray background), and the calibration values are stored in non-volatile memory (see, e.g., processor 10 of ~IG. 1). For any given color or intensity, the intensity for thereceiverslperimeter sensors (independent of distance from the central source fiber optic) in 30 general should vary equally. Hence, a white surface should produce the highest intensities for the perimeter sensors, and a black surface will produce the lowest intensities. ~Ithough the color of the surface will affect the measured light intensities of the perimeter sensors, it should affect them sl~hst~nti~lly equally. The height of the probe from the surface of the =

CA 02238498 1998 - 0~ - 2~
WO 97l24587 PCT/US97/00126 object, however, will affect the triads of sensors differently. At the minim~l height range of the probe, the triad of sensors in the smallest ring (those closest to the source fiber optic) will be at or about their maximal value. The rest of the rings of triads will be measuring light at intensities lower than their maximal values. As the probe is raised/positioned from the 5 minim~l height, the intensity of the smallest ring of sensors will decrease and the intensity of the next ring of sensors will increase to a maximal value and will then decrease in intensity as the probe is raised/positioned still further. Similarly for the third ring, fourth ring and so on.
Thus, the pattern of intensities measured by the rings of triads will be height dependent. In such embodiments, characteristics of this pattern may be measured and stored in non-volatile 10 RAM look-up tables (or the like) for the probe by calibrating it in a fixture using a neutral color surface. Again, the actual intensity of light is not as important in such embodiments, but the degree of variance from one ring of perimeter sensors to another is.
To determine a measure of the height of the probe from the surface being measured, the intensities of the perimeter sensors (coupled to receivers 312 - 320) is measured. The 15 variance in light intensity from the inner ring of perimeter sensors to the next ring and so on is analyzed and c~ alcd to the values in the look-up table to determine the height of the probe. The determined height of the probe with respect to the surface thus may be utilized by the system processor to compensate for the light intensities measured by the color sensors in order to obtain reflectivity readings that are in general independent of height. As with 20 previously described embodiments, the reflectivity measurements may then be used to determine optical characteristics of the object being measured, etc.
It should be noted that audio tones, such as previously described, may be advantageously employed when such an embodiment is used in a handheld configuration.
For example, audio tones of varying pulses, frequencies and/or intensities may be employed 25 to indicate the operational status of the instrument, when the instrument is positioned within an acceptable range for color measurements, when valid or invalid color measurements have been taken, etc. In general, audio tones as previously described may be adapted for advantageous use with such further embodiments.
FIG. 17 illustrates a further such embodiment of the present invention. The preferred 30 implementation of this embodiment consists of a central light source 310 (which in the cfcllcd implementation is a central light source fiber optic), surrounded by a plurality of light receivers 322 (which in the preferred implementation consists of three perimeter light receiver fiber optics). The three perimeter light receiver fiber optics, as with earlier described CA 02238498 1998-0~-2~

embodiments, may be each spliced into additional fiber optics that pass to light intensity receivers/sensors, which may be implemented with Texas Instruments TSL230 light to frec~uency converters as described previously. One fiber of each perimeter receiver is coupled to a sensor and measured full band width (or over substantially the same bandwidth) such as 5 via a neutral density ~llter, and other of the fibers of the perimeter receivers are coupled to sensors so that the light passes through sharp cut off or notch filters to measure the light intensity over distinct frecluency ranges of light (again, as with earlier described embodiments). Thus there are color light sensors and neutral "perimeter" sensors as with previously described embodiments. The color sensors are utilized to determine the color or 10 other optical characteristics of the object, and the perimeter sensors are utilized to determine if the probe is perpendicular to the surface and/or are utilized to compensate for non-perpendicular angles within certain angular ranges.
In the embodiment of FIG. 17, the angle of the perimeter sensor fiber optics is mechanically varied with respect to the central source fiber optic. The angle of the perimeter 15 receivers/sensors with respect to the central source fiber optic is measured and utilized as described hereinafter. An exemplary mechanical mech~ni.cm, the details of which are not critical so long as desired, control movement of the perimeter receivers with respect to the light source is obtained, is described with reference to FIG. 18.
The probe is held within the useful range of the instrument (determined by the 20 particular configuration and construction, etc.), and a color measurement is initiated. The angle of the perimeter receivers/sensors with respect to the central light source is varied from parallel to pointing towards the central source fiber optic. While the angle is being varied, the intensities of the light sensors for the perimeter sensors (e.g., neutral sensors) and the color sensors is measured and saved along with the angle of the sensors at the time of the light 25 mea~u~ t. The light intensities are measured over a range of angles. As the angle is increased the light intensity will increase to a maximum value and will then decrease as the angle is further increased. The angle where the light values is a maximum is utilized to determine the height of the probe from the surface. As will be apparent to those skilled in the art based on the teachings provided herein, with suitable calibration data, simple geometry 30 may be utilized to calculate the height based on the data measured during variation of the angle. The height measurement may then be utilized to compensate for the intensity of the color/optical measurements and/or utilized to normalize color values, etc.

CA 02238498 1998-0~-2~

FIG. 18 illustrates an exemplary embodiment of a mechanical arrangement to adjust and measure the angle of the perimeter sensors. Each perimeter receiver/sensor 322 is mounted with pivot arm 326 on probe frame 328. Pivot arrn 326 engages central ring 332 in a manner to form a cam mech~nicm Central ring 332 includes a groove that holds a portion of pivot arm 326 to form the cam mech~ni~m Central ring 332 may be moved perpendicular with respect to probe frame 328 via linear actuator 324 and threaded spindle 330. The position of central ring 332 with respect to linear actuator 324 determines the angle of perimeter receivers/sensors 322 with respect to light source 310. Such angular position data vis-a-vis the position of linear actuator 324 may be calibrated in advance and stored in non-10 volatile memory, and later used to produce color/optical characteristic measurement data as previously described.
A further embodiment of the present invention utilizing an alternate removable probe tip will now be described with reference to FIGS. l9A - l9C. As illustrated in FIG. l9A, this embodiment utilizes removable, coherent light conduit 340 as a removable tip. Light conduit 15 340 is a short segment of a light conduit that preferably may be a fused bundle of small fiber optics, in which the fibers are held essentially parallel to each other, and the ends of which are highly polished. Cross-section 350 of light conduit 340 is illustrated in FIG. l9B. Light conduits similar to light conduit 340 have been utilized in what are Icnown as borescopes, and also have been utilized in medical applications such as endoscopes.
Light conduit 340 in this embodiment serves to conduct light from the light source to the surface of the object being measured, and also to receive reflected light from the surface and conduct it to light receiver fiber optics 346 in probe handle 344. Light conduit 340 is held in position with respect to fiber optics 346 by way or co~ ssion jaws 342 or other suitable fitting or coupled that reliably positions light conduit 340 so as to couple light 25 effectively to/from fiber optics 346. Fiber optics 346 may be separated into separate fibers/light conduits 348, which may be coupled to a~lul,liate light sensors, etc., as with previously described embodiments.
In general, the aperture of the fiber optics used in light conduit 340 may be chosen to match the aperture of the fiber optics for the light source and the light receivers. Thus, the 30 central part of the light conduit may conduct light from the light source and illnmin~t~ the surface as if it constituted a single fiber within a bundle of fibers. Similarly, the outer portion of the light conduit may receive reflected light and conduct it to light receiver fiber optics as if it conctitl~t.D~I single fibers. Light conduit 340 has ends that preferably are highly polished CA 02238498 1998-0~-2~

and cut perpendicular, particularly the end coupling light to fiber optics 346. Similarly, the end of ~Iber optics 346 abutting light conduit 340 also is highly polished and cut perpendicular to a high degree of accuracy in order to minimi7(. light reflection and cross talk between the light source fiber optic and the light receiver fiber optics and between adJacent receiver fiber optics. Light conduit 340 offers significant advantages including in the manufacture and in~t~ t;on of such a removable tip. For example, the probe tip need not be particularly aligned with the probe tip holder; rather, it only needs to be held against the probe tip holder such as with a compression mechanism (such as with compression jaws 342) so as to couple light effectively to/from fiber optics 346. Thus, such a removable tip mechanism 10 may be implemented without alignment tabs or the like, thereby faci1it~ting easy insta}lation of the removable probe tip. Such an easy in~f~ hle probe tip may thus be removed and cleaned prior to installation, thereby facilitating use of the color/optical measuring apparatus by dentists, medical professions or others working in an environment in which cont~min~tion may be a concern. Light conduit 340 also may be implemented, for example, as a small 15 section of light conduit, which may facilitate easy and low cost mass production and the like.
A further embodiment of such a light conduit probe tip is illustrated as light conduit 352 in FIG. l 9C. Light conduit 352 is a light conduit that is narrower on one end (end 354) than the other end (end 356). Contoured/tapered light conduits such as light conduit 352 may be fabricated by heating and stretching a bundle of small fiber optics as part of the fusing 20 process. Such light conduits have an additional interesting property of mzlgnification or reduction. Such phenomena result because there are the same number of fibers in both ends.
Thus, light entering narrow end 354 is conducted to wider end 356, and since wider end 356 covers a larger area, it has a magnifying affect.
Light conduit 352 of FIG. 19C may be utilized in a manner similar to light conduit 25 = 340 (which in general may be cylindrical) of FIG. l9A. Light conduit 352, however, measures smaller areas because of its reduced size at end 354. Thus, a relatively larger probe body may be manufactured where the source fiber optic is spaced widely from the receiver fiber optics, which may provide an advantage in reduced light reflection and cross talk at the junction, while still m~int~ining a small probe measuring area. Additionally, the relative 30 sizes of narrow end 354 of light conduit 352 may be varied. This enables the operator to select the size/characteristic of the removable probe tip according to the conditions in the particular application. Such ability to select sizes of probe tips provides a further advantage CA 02238498 1998 - 0~ - 2~
WO 97J24~87 PCT/US97l00126 in making optical characteristics measurements in a variety of applications and operative environments.
As should be apparent to those skilled in the art in view of the disclosures herein, light conduits 340 and 356 of FIGS. 19A and l9C need not necessarily be cylindrical/tapered as 5 illustrated, but may be curved such as for specialty applications, in which a curved probe tip ~ may be advantageously employed (such as in a confined or hard-to-reach place). It also should be apparent that light conduit 352 of FIG. l9C may be reversed (with narrow end 354 coupling light into fiber optics 346, etc., and wide end 356 positioned in order to take measurements) in order to cover larger areas.
Additionally, and to emphasize the wide utility and variability of various of the inventive concepts and techniques disclosed herein, it should be apparent to those skilled in the art in view of the disclosures herein that the apparatus and methodology may be utilized to measure the optical properties of obiects using other optical focusing and gathering elements, in addition to the fiber optics employed in preferred embodiments herein. For example, 15 lenses or mirrors or other optical elements may also be utilized to construct both the light source element and the light receiver element. A flashlight or other commonly available light source, as particular examples, may be utilized as the light source element, and a common telescope with a photoreceiver may be utilized as the receiver element in a large scale embodiment of the invention. Such refinements utilizing teachings provided herein are 20 expressly within the scope of the present invention.
As will be a~pa,~nt to those skilled in the art, certain refinements may be made in accordance with the present invention. For example, a central light source fiber optic is utilized in certain preferred embodiments, but other light source arrangements (such as a plurality of light source fibers, etc.). In addition, lookup tables are utilized for various aspects 25 of the present invention, but polynomial type calculations could similarly be employed. Thus, although various preferred embodiments of the present invention have been disclosed for illustrative purposes, those skilled in the art will appreciate that various modifications, additions and~or substitutions are possible without departing from the scope and spirit of the present invention as disclosed in the claims.
Reference is also made to copending international application filed on even dateherewith under the Patent Cooperation Treaty, for "Apparatus and Method for Measuring Optical Characteristics of Teeth," by the inventors hereof, which is hereby incorporated by reference.

Claims

What is claimed is:
1. A method for determining optical characteristics of an object, comprising thesteps of:
measuring the object by moving a probe in proximity to the object, wherein the probe provides light to the surface of the object from one or more light sources, and receives light reflected from the object through a plurality of light receivers;
determining the intensity of reflected light received by more than one of the light receivers with first sensors; and measuring the optical characteristics of the object with second sensors based on light received by one or more of the light receivers in response to the intensity determinations made by the first sensors, wherein the measurement produces data indicative of the optical characteristics of the object.
2. The method of claim 1, wherein the optical characteristics of the object comprise color characteristics.
3. The method of claim 1, wherein the optical characteristics of the object comprise translucence characteristics.
4. The method of claim 1, wherein the optical characteristics of the object comprise fluorescence characteristics.
5. The method of claim 1, wherein the optical characteristics of the object comprise surface texture characteristics.
6. The method of claim 1, wherein the probe comprises one or more light source fiber optics coupled to a light source and a plurality of light receiver fiber optics coupled to the first and second sensors.
7. The method of claim 1, wherein the plurality of light receivers are each spaced a first distance from a first light source on the probe, and wherein the plurality of light receivers are spaced apart from adjacent light receivers on the probe by a second distance.
8. The method of claim 7, wherein the probe comprises three light receivers spaced around the first light source, wherein the light receivers are spaced apart from adjacent light receivers with an angular spacing of about 120 degrees.
9. The method of claim 1, wherein the first sensors comprise light measuring sensors measuring the same bandwidth, and wherein the second sensors comprise a color spectrophotometer.

10. The method of claim 9, wherein the second sensors comprise a plurality of filters optically coupled to a plurality of light measuring devices.
11. The method of claim 10, wherein the filters comprise filters that pass light of predetermined frequencies of received light.
12. The method of claim 1, wherein the first sensors comprise light measuring sensors measuring the same bandwidth, and wherein the second sensors comprise a color tristimulus measuring device.
13. The method of claim 1, further comprising the steps of:
processing the measured data with a computing device; and displaying a representation corresponding to the measured data on a display device.
14. The method of claim 13, wherein the computing device is coupled to a telecommunication device, the method further comprising transmitting data corresponding to the measured data to a remote facility.
15. The method of claim 1, the method further comprising generating audio information, wherein the audio information is indicative of the status of the optical characteristics determination.
16. The method of claim 1, wherein the probe has a removable cover element.
17. The method of claim 16, wherein the removable cover element comprises a shield.
18. The method of claim 16, further comprising positioning the removable cover element on the probe prior to measuring the object.
19. The method of claim 16, further comprising the steps of sterilizing the removable cover element and positioning the cover element on the probe prior to measuring the object.
20. The method of claim 1, wherein the probe has a removable tip.
21. The method of claim 20, further comprising positioning the removable tip on the probe prior to measuring the object.
22. The method of claim 20, further comprising sterilizing the removable tip andpositioning the removable tip on the probe prior to measuring the object.
23. The method of claim 1, wherein the step of determining the intensity of reflected light with the first sensors comprises the steps of:
determining a first peak intensity value with one or more of the first sensors as the probe is moved towards the object; and determining a second peak intensity value with one or more of the first sensors as the probe is moved away from the object.
24. The method of claim 23, wherein the object is measured with the second sensors when the first and second peak intensity values are substantially equal. 25. The method of claim 23, further comprising the steps of:
comparing the first and second peak intensity values;
accepting the data measured by the second sensors if the compared first and second peak intensity values are within a predetermined range; and rejecting the data measured by the second sensors if the compared first and second peak intensity values are outside the predetermined range.
26. The method of claim 25, further comprising the steps of:
generating first audio information if the measured data is accepted; and generating second audio information if the measured data is rejected.
27. The method of claim 25, further comprising the step of modifying the predetermined range.
28. The method of claim 23, further comprising the step of determining an intermediate intensity value with the first sensors at a time intermediate between the time when the first and second peak intensity values are determined, wherein the intermediate intensity value corresponds to the translucence of the object.
29. The method of claim 28, wherein the intermediate intensity value is determined when the probe is in contact or near contact with the object.
30. The method of claim 1, wherein the optical characteristics of the object aremeasured without the probe contacting the object.
31. The method of claim 1, wherein the object is measured at a time when a plurality of the first sensors measure peak intensity values as the probe moves with respect to the object.
32. The method of claim 1, wherein the object is measured when the probe is at apredetermined distance from the object.
33. The method of claim 1, wherein the object is measured when the probe is at apredetermined distance and angle with respect to the object.
34. An apparatus for determining optical characteristics of an object, comprising:

a probe movable to be in proximity to the object, wherein the probe provides light to the surface of the object from one or more light sources, and receives light reflected from the object through a plurality of light receivers;
first sensors for determining the intensity of reflected light received by more than one of the light receivers; and second sensors for measuring the optical characteristics of the object based on light received by one or more of the light receivers in response to the intensity determinations made by the first sensors, wherein the measurement produces data indicative of the optical characteristics of the object.
35. A method comprising the steps of:
measuring a first object by moving a probe in proximity to the first object, wherein the probe provides light to the surface of the first object from one or more light sources, and receives light reflected from the first object through a plurality of light receivers;
determining the intensity of reflected light received by more than one of the light receivers with first sensors;
measuring the optical characteristics of the first object with second sensors based on light received by one or more of the light receivers in response to the intensity determinations made by the first sensors, wherein the measurement produces data indicative of the optical characteristics of the first object;
preparing a second object based on the data indicative of the optical characteristics of the first object, wherein constituent materials of the second object are selected based on said data.
36. The method of claim 35, wherein the constituent materials are selected basedon Kubelka-Munk equations and/or Saunderson equations.
37. A method comprising the steps of:
measuring an object by moving a probe in proximity to the object, wherein the probe provides light to the surface of the object from one or more light sources, and receives light reflected from the object through a plurality of light receivers;
determining the intensity of reflected light received by more than one of the light receivers with first sensors;
measuring the optical characteristics of the object with second sensors based on light received by one or more of the light receivers in response to the intensity determinations made by the first sensors, wherein the measurement produces data indicative of the optical characteristics of the object; and performing an industrial process on the object based on said data.
38. The method of claim 37, wherein the industrial process comprises sorting theobject based on said data.
39. An apparatus for measuring the color of an object with a probe as the probe is moved with respect to the object, comprising:
a probe having a central light source and a plurality of light receivers spaced apart from the central light source, wherein light from the central light source reflects into the plurality of light receivers;
sensors coupled to receive light from the light receivers, wherein at least some of sensors measure the value of the intensity of light in predetermined color bands;
a processor coupled to receive data from the light sensors;
wherein the processor monitors the intensity values for one or more of the lightreceivers and stores data from the sensors at time when the one or more light receivers have a peak intensity value.