METHOD AND DEVICE FOR DETECTING UNDESIRED MATTER IN EGGS

Abstract: Described is a method for determining whether a brown egg contains undesired matter such as blood. In two wavelength ranges the transmission of the egg is examined, one of those wavelength ranges corresponding to an absorption peak of blood. The transmission signal of the other wavelength range is corrected with a fixed fraction gamma to correct for the egg being brown.

Description: Title: Method and device for detecting undesired matter in eggs. This invention relates to a method for detecting the presence of undesired matter in an egg as described in the preamble of claim 1. Such a method is generally known in practice and is based on the principle of color spectrum photometry. Although the present invention is generally applicable for detecting undesired matter in general, the present invention is of interest in particular for detecting the presence of blood in eggs, for which reason the present invention will be described hereinbelow for such an exemplary application. In practice, it may happen that an egg intended for consumption, for instance a chicken egg, contains blood. Although the presence of blood is, in principle, harmless, the consumer generally does not find the presence of blood a pleasant sight. For this reason, egg-processing companies generally entertain the desire to supply "pure" eggs only, that is, eggs with as little undesired matter, such as blood, as possible. This implies there is a need for detection equipment to determine whether blood is present in an egg. Such detection equipment is coupled to sorting equipment to remove, during the sorting and packing of eggs, the unsuitable eggs, that is, the eggs that contain undesired matter such as blood. Naturally, such detection equipment should be non-destructive. A well-proven detection method for detecting the presence of blood relies on the fact that an egg is semi-transparent, and is based on the absorption characteristics of eggs and blood. Blood has a strong absorption line at 577 nm; a normal egg has a much lower absorption at this wavelength, and the absorption characteristic of a normal egg is virtually flat in this wavelength range. By directing light at an egg and measuring the amount of transmitted light at 577 nm, the presence of blood can in principle be determined. However, the light, when passing through the egg, will be considerably weakened by the egg itself, and the extent of weakening can vary from one egg to another: it depends inter alia on the thickness of the egg. To correct for the extent of absorption/weakening by the egg itself, the amount of transmitted light is also measured in a narrow wavelength band at some distance from the absorption line referred to; in practice, a wavelength distance of 20 nm is used, and this reference measurement is carried out at approximately 597 nm. The result of the measurement at 577 nm can be corrected for the result of the measurement at 597 nm, to thereby obtain a measuring signal that depends substantially exclusively on the absorption by blood. In practice, this method has proven to yield good results . Even eggs that contain only minute amounts of blood can be detected with a high probability, while the probability that a bloodless egg is falsely rejected is particularly low. The good results referred to, however, have so far applied to white eggs only. In colored eggs, the results are less good, because the coloring of the shell plays a role. In particular, the measuring method referred to has been found to be less reliable in brown eggs. The reason for this reduced reliability has been found to reside in the fact that the shell of brown eggs itself exhibits an absorption in the range of 577 nm. This makes it difficult to discriminate between absorption caused by blood and absorption caused by the brown shell . It is therefore an object of the present invention to make the known blood detection method suitable for examining brown eggs as well. In particular, the object of the present invention is to provide a relatively simple method which enables determining the presence of blood in brown eggs with great accuracy. More particularly, the object of the present invention is to provide a method for processing the measuring signals that are provided by a standard detection device, without requiring modification of such a standard detection device. To that end, the method according to the invention has the features as described in the characterizing clause of claim 1. These and other aspects, features and advantages of the present invention will be clarified by the following description of a preferred embodiment of a method and device according to the invention, with reference to the drawing, in which: Fig. 1 schematically illustrates the principle of blood detection in eggs; Fig. 2 schematically shows a blood detection device; Fig. 3A is a flow diagram illustrating a white-calibration procedure; Fig. 3B is a flow diagram illustrating a brown-calibration procedure; Fig. 4 is a flow diagram illustrating a first example of a measuring procedure according to the present invention; and Fig. 5 is a flow diagram illustrating a second example of a measuring procedure according to the present invention. Fig. 1 illustrates the principle of blood detection in eggs, which is known per se. An egg 3 to be examined is subjected to a first light radiation LI having a first predetermined wavelength λl, coming from a light source 1, and the radiation Tl transmitted by the egg 3 at this wavelength is received by a detector 2, which provides a first electrical signal SI which is representative of the intensity of the received first transmission radiation Tl . Similarly, a second electrical signal S2 is provided, which is representative of the received second transmission radiation T2 at a second predetermined wavelength λ2. These two signals SI and S2 are presented to a signal processing device 10, which on the basis of those signals decides whether or not the egg 3 under examination contains blood. In practice, the wavelengths used are approximately 597 nm (λl) and 577 nm (λ2) , but other wavelengths are, in general, also conceivable. In Fig. 1, for the sake of clarity, the light source 1, the egg 3, and the detector 2 are depicted twice. It is indeed possible to use two different light sources, each transmitting only one of the wavelengths mentioned, and to use two different light sources, each providing only one of the electrical signals mentioned. It is also possible, however, that the two electrical signals SI and S2 are provided by one and the same detector 2, which is sensitive to at least both wavelengths λl and λ2. Also, the light LI and the light L2 can originate from one and the same light source 1, which generates light containing at least both wavelengths λl and λ2. To obtain the first electrical signal si, a first filter (not shown for the sake of simplicity) can be placed in the light path, either between the light source 1 and the egg 3, or between the egg 3 and the detector 2, which first filter is designed to transmit substantially exclusively the first wavelength λl . Similarly, the second electrical signal S2 can be obtained by making use of a second filter, which is designed to transmit substantially exclusively the second wavelength λ2. Naturally, other measuring arrangements are also possible, as will be clear to one skilled in the art. In a particular embodiment, light containing both wavelengths λl and λ2 is aimed at the egg 3 and after passing through the egg 3 is received by a detector with two detection channels ■ which are sensitive to the respective wavelengths. Generally, it holds that the combination of the signals SI and S2 is representative of the absorption characteristic of the egg 3 in the range 577-597 nm. If the intensity of the light LI and L2 emitted by the light source is denoted I (LI) and I (L2) , respectively, and the absorption coefficient of an egg at the wavelengths λl and λ2 is denoted αl and α2 , respectively, the magnitude of the electrical detector signals SI and S2 can be written as fl'(l-αl) -I(L1) and f2" (l-α2) 'I (L2) , where fl and f2 are proportionality factors expressing inter alia the sensitivity of the detector to the wavelengths λl and λ2. The above-mentioned combination of the signals SI and S2 can be expressed, for instance, by defining a state parameter M which is a function of a combination of SI and S2 , for instance M = S1/S2 or M = S1-S2. Hereinafter, the invention will be further elaborated under the assumption that the state parameter is defined on the basis of a differential signal between the detector signals; it will be clear to one skilled in the art how the present invention can be implemented on the basis of a coefficient signal. For an egg without blood, the transmission characteristics (and absorption characteristics) at the two wavelengths λl and λ2 are virtually identical to each other, and any differences in those characteristics will be virtually the same for different eggs with respect to each other. Although the values of SI and S2 can vary for individual eggs, for instance depending on the size of the eggs, the foregoing means that the state parameter M = S1-S2 for bloodless white eggs will be substantially equal to zero or will, at most, have a small value which will, in principle, be the same for all bloodless white eggs. This value will be designated hereinafter as reference state value M white>0 . Because blood has a narrow absorption peak at approximately 577 nm, with a peak width of approximately 10 nm, it holds for a white egg containing blood that the second absorption coefficient α2 will be considerably greater than if the egg did not contain any blood, while for the first absorption coefficient αl the presence or absence of blood will make little difference, if any. This means that the absolute value of the state parameter M will then be significantly greater than the above-mentioned "reference state value" M whlte 0 . In white eggs, this is a reliable indication of the presence of blood, and the magnitude of the difference M-M white 0 is a reliable measure of the amount of blood in the egg in question. To determine whether the amount of blood in an egg is acceptable or not, a state threshold ΔM can be defined, and M-M whlte 0 can be compared with this predefined state threshold ΔM; if M-M whlte 0 < ΔM, the amount of blood is acceptable. As for an egg with a brown shell, the matter is more complicated, because the brown shell also has an absorption peak at λ2. Then the mere given that the state parameter M is significantly greater than the above-mentioned reference state value M whlte 0 is not a reliable indication of the presence of blood. The present invention provides a solution to this problem, which will be described in the following. Fig. 2 diagrammatically shows a blood detection device 20. It comprises a conveying device 21 for eggs 3, for instance a conveyor or the like. Arranged along the conveying device 21 is a detection station 22, which comprises, for instance, a light source 1 and a detector 2, as illustrated in more detail in Fig. 1. The blood detection device 20 further comprises a signal processing device 10 which receives the signals SI and S2 from the detector 2. Further, a removal device 23 is provided, which is arranged to remove eggs from the conveying device 21 under the control of the signal processing device 10. In the foregoing, it has been mentioned that the reference state value M whlte 0 is very small. To eliminate any instrumentation differences, it is preferably ensured that M hιte,o is substantially equal to zero. To that end, the blood detection device 20 is adjusted in a white-calibration procedure, such that in bloodless white eggs the two signals SI and S2 are substantially equal to each other; in other words, wh i te . o is roade equal to zero. This can be accomplished in various ways. Firstly, it is possible to set the light strength of the light source 1 for generating LI and/or the light strength of the light source 1 for generating L2 , such that upon detection it is found that S1=S2. Secondly, it is possible, for instance, to multiply in the signal processing device 10 one of the received signals SI, S2 by a first correction factor c, such that c'Sl=S2 and Sl=cS2, respectively. Hereinafter, it will be assumed that in the calibration the signal processing device 10 multiplies the first detector signal SI by the first correction factor c, such that c'Sl=S2. It is noted that this correction can be carried out through hardware, by an amplifier with an adjustable amplification factor, but it is also possible to carry out this correction through software in the signal processing device 10. The above-mentioned white-calibration procedure is illustrated in Fig. 3A. A bloodless white egg is subjected to the radiation LI and L2 , and the signals SI and S2 are measured (step 101) . Then the first correction factor c is determined as c = S2/S1 (step 102) . If desired, the steps 101 and 102 can be repeated for several eggs, and the obtained values of c can be averaged. Fig. 4 illustrates an example of the actual measuring procedure according to the present invention. First, it is determined whether an egg to be examined is a white or a brown egg. This can be accomplished in different ways. Thus, it is possible, for instance, to employ a color-sensitive detector, which is known per se . In a preferred embodiment of the method according to the present invention, however, use is made of the signals SI and S2 provided by the detectors 2, so that utilization of a separate color- sensitive detector is not needed. The fact is that it has been found that in brown eggs the absorption coefficients αl and oc2 are considerably greater than in white eggs, so that the provided signals SI and S2 have a considerably smaller intensity, making it possible to discriminate between brown and white eggs on the basis of those signals SI and S2. According to the present invention, therefore, in a preferred embodiment of the white-calibration procedure, the magnitude of the signal SI as obtained from bloodless white eggs is fixed as a reference SO (step 103, Fig. 3A) , which will hereinafter be referred to by the term "white-reference" . If desired, step 103 can be repeated for multiple eggs, and the obtained values of SO can be averaged . In the actual measuring procedure on an unknown egg (Fig. 4) the signals SI and S2 are measured (step 201) . To determine whether this unknown egg is a white or a brown egg, in a preferred embodiment of the measuring procedure, the measured signal SI is compared with the above-mentioned white-reference SO (step 202) . If SI is smaller than SO to a sufficient extent, for instance SI < 75% of SO, it is decided that the egg under examination is a brown egg; if not, it is decided that the egg under examination is a white egg (step 203) . If it has been decided that the egg under examination is a white egg, the measuring signals SI and S2 are further processed in a conventional manner to detect the presence of blood. In step 204, a corrected state parameter M c is computed as M c = CS1-S2. In step 205 M c is compared with zero. If M c is significantly greater than zero, it is concluded that the egg in question contains blood; if not, it is concluded that the egg in question does not contain any blood (step 206) . On the basis of this outcome, the signal processing device 10 can control the removal device 23 to remove the blood-containing egg. If, however, it is decided that the egg under examination is a brown egg, first a correction is performed on the measuring signals SI and/or S2 to correct for the shell being brown (step 207) . It has been found that such a correction, if desired, can be carried out in the same manner for all brown eggs, regardless of the degree of brownness, shell thickness, etc. The magnitude of the correction has likewise been priorly determined, viz. in a calibration procedure which will be designated as "brown-calibration procedure", utilizing bloodless brown eggs . The brown-calibration procedure is illustrated in Fig. 3B. A bloodless brown egg is subjected to the radiation LI and L2 , and the signals SI and S2 are measured (step 111) . Then the signal SI is corrected with the first correction factor c to provide a corrected signal SI ' according to the formula SI 1 = c'Sl (step 112) . As mentioned before, brown eggs exhibit an absorption at 577 nm, so that for brown eggs SI' will be greater than S2. The differential signal ΔS is determined according to the formula ΔS = Sl'-S2 (step 113). Then this differential signal ΔS is expressed as a fraction of the corrected signal SI', according to the formula ΔS = γ ' Sl', that is, the fraction γ is computed according to the formula γ = ΔS/S1 ' (step 114) . Alternatively, the steps 112-114 can be combined into a single step in which the fraction γ is determined according to the formula γ = (cSl-S2) /c'Sl . If desired, the steps 111- 114 can be repeated for multiple eggs, and the obtained values of γ can be averaged. In the eventual measuring procedure, if in step 203 it has been decided that the egg under examination is a brown egg, the corrected state parameter M c is computed as M c = (1- γ) 'CS1-S2 (step 207) . Then, in a comparable manner to that described in respect of white eggs, M c is compared with zero, that is, the measuring procedure proceeds, after step 207, with step 205 already mentioned. Accordingly, it holds that further the following method step is carried out: (f) only for brown eggs, the first and second measuring signal are corrected relative to each other with a fraction γ. This can be carried out by a correction of the first signal SI relative to the second signal, a correction of the second signal relative to the first signal, or a correction of the first and second signal whereby the signals are corrected relative to each other. In this example, it holds in particular that an (SI) of the measuring signals is corrected with the fraction γ. Because according to the invention, the measuring signals SI and S2 must be corrected relative to each other with a fraction γ, it is, of course, also possible to define M c in step 207 as M c = (1-γ) cESl- ES2 , where E is a number not equal to zero. E can be chosen, for instance, to be equal to (1-γ) "1 . In that case, only the signal S2 needs to be corrected with the fraction γ. In that case, it holds that M c = cSl-(l-γ)S2 and therefore only the second measuring signal is corrected. E can also be selected to be equal to (l-γ) ~1/2 , so that M c = (1-γ) +1/2 'cS- (1-γ) "1/2' S2. Both are then subjected to a mutually different correction and are then corrected relative to each other. With the above-described measuring procedure it has been found possible to reliably detect even minute blood spots in brown eggs. Surprisingly, it has been found that the fraction γ can be a substantially constant value which had good utility in brown eggs, regardless of their diameter, the thickness of the shell or the darkness of the shell, and that in all of these cases the above-defined corrected state parameter M c is a reliable indicator of the presence of blood. It will be clear to one skilled in the art that the scope of protection of the present invention as defined by the claims is not limited to the embodiments represented in the drawings and discussed, but that it is possible to alter or modify the represented embodiments of the method according to the invention within the scope of the inventive concept. Thus it is possible, for instance, to skip step 207 and, instead of step 205, to compare the corrected measuring signal (1-γ) c SI with S2. Also, as stated, it is possible to compare a corrected signal S2 with SI. Moreover, a fraction γ 1 can be defined as γ 1 = 1-γ. In the description given hereinabove and in the drawing, γ can then be replaced throughout with 1-γ' . The fraction γ' can then be determined in a brown-calibration according to the formula 1-γ' = ΔS/S' (step 114). If the steps 112-114 are combined into a single step, γ' can be determined in a brown-calibration according to the formula 1-γ' = (c S1-S2) /cSl. It follows that γ' = S2/cSl m the brown-calibration. If γ' has thus been determined, the signals SI and S2 can be corrected relative to each other with the fraction γ' . This can be carried out, for instance, by multiplying the signal SI by the fraction γ' . It is also possible to multiply the signal S2 by the fraction (γ 1 ) 1 . Naturally, it is also possible to multiply the signal SI by E and the fraction γ' and to multiply the signal S2 by E, with E being a random number not equal to zero. In each of these cases, it holds that the signals SI and S2 are corrected relative to each other with the fraction γ' . In step 207, M c can then be defined as M c = cγ' S1-S2, M c = c Sl-γ' S2 or M c = cγ' ES1-ES2, respectively. In the latter case, M c can optionally be defined in step 204 as M c = c E Sl- E S2. In Fig. 5, a second example of a measuring method according to the invention is shown, which comprises a further refinement with respect to the method discussed with reference to Fig. 4. According to the method to be described with reference to Fig. 5, an egg with blood can be distinguished from an egg without blood with a further increased chance of success. The method also works well m, on the one hand, thick-shelled white versus thin-shelled brown eggs and, on the other hand, in light brown eggs and dark brown eggs. Again, in step 301 the first signal SI and the second signal S2 are determined. Also, in a step 302 it is determined according to a predetermined criterion whether the egg under examination is a white egg, a light brown egg or a dark brown egg. In this example, the light brown eggs are separated from the dark brown eggs using a color camera, such as, for instance, two semiconductor diodes that are sensitive to green and red light, respectively. In this example, moreover, using the same camera, it is determined whether the egg is a white egg. Accordingly, in this example, using the camera, it is determined whether the egg is a white, a light brown or a dark brown egg. If the egg is a white egg, a step 303 is carried out which is entirely analogous to the step 204. If the egg is a light brown egg, a step 304 is carried out which corresponds to step 207. The fraction γl , however, is a fraction which has been determined in a light brown-calibration procedure for light brown eggs. All this is entirely analogous to the manner discussed for brown eggs with reference to Fig. 4. If the egg is a dark brown egg, a step 305 is carried out which is again equal to the step 207 discussed with reference to Fig. 4. In this case, however, a fraction γ2 is used for dark brown eggs, which has been obtained entirely analogously in a dark brown-calibration procedure for dark brown eggs, as has been discussed for brown eggs with reference to Fig. 4. Accordingly, the first and second measuring signal for light brown eggs are corrected relative to each other with a first fraction γl for light brown eggs, and the first and second measuring signal for dark brown eggs are corrected relative to each other with a second fraction γ2 for dark brown eggs. Accordingly, the fraction γl has been determined for light brown eggs in a light brown- calibration procedure on the basis of at least one bloodless light brown egg. Further, the fraction γ2 for dark brown eggs has been determined in a dark brown-calibration procedure on the basis of at least one bloodless dark brown egg. In addition, the first and second measuring signal for all eggs are corrected relative to each other with the first correction factor c, which has been determined in the white- calibration procedure on the basis of at least one bloodless white egg. Also, in step 304 for light brown eggs the second measuring signal S2 is compared with the first measuring signal corrected relative to the second measuring signal, (l-γl) c'Sl, where c is the first correction factor satisfying c = S2/S1 in the case of a bloodless white egg. Here, the fraction γl for light brown eggs satisfies γl = (CS1-S2) /c'Sl in the case of a bloodless light brown egg. For dark brown eggs, it holds that the second measuring signal S2 is compared with the first measuring signal corrected relative to the second measuring signal, (1- γ2)'c'Sl, where c is the above-mentioned first correction factor and where said fraction γ2 for dark brown eggs satisfies γ2 = (CS1-S2) /c " Sl in the case of a bloodless dark brown egg. Again, in the white-calibration procedure a bloodless white egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the first correction factor c is defined as c = S2/S1. Further, in the light brown-calibration procedure, a bloodless light brown egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the fraction γl is determined according to the formula γl = (c " Sl-S2) /cSl , and in the dark brown- calibration procedure a bloodless dark brown egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the fraction γ2 is determined according to the formula γ2 = (CS1-S2) /cSl . When the value of M c in step 303, 304, or 305 has been determined, it is compared with 0. All this is carried out entirely analogously to the manner discussed for Fig. 4 with reference to step 205. Again, next, in step 307, entirely analogously to step 206 according to Fig. 4, it is determined whether the value of M c is significantly greater than 0. If this is the case, it is concluded that blood is present in the egg. If this is not the case, it is concluded that no blood is present in the egg. It will be clear that steps 301 and 302 can be carried out in a random order. Further, it is possible to skip steps 303, 304 and 305 and instead, in step 306, to compare the corrected measuring signal cSl, cSl(l-γl) or cSl(l-γ2) with S2. Also, again a fraction γl ' can be defined as γl ' = 1-γl and a fraction γ2 ' can be defined as γ2 ' = l-γ2, all entirely analogously to the manner as discussed with reference to Fig. 4. Also, the signal SI and the fractions γl ' and γ2 ' can then be multiplied again by the factor E mentioned earlier. Such variants are each understood to fall within the scope of the invention.

Claims: Claims 1. A method for detecting the presence of undesired matter in an egg (3), comprising the steps of: (a) irradiating the egg to be examined with radiation (LI, L2) which comprises at least two predetermined wavelength ranges (λl, λ2); (b) providing a first measuring signal (SI) representative of the amount of radiation (Tl) in a first (λl) of said two predetermined wavelength ranges transmitted by the egg (3); (c) providing a second measuring signal (S2) representative of the amount of radiation (T2) in a second (λ2) of said two predetermined wavelength ranges transmitted by the egg (3); (d) comparing the first measuring signal (SI) with the second measuring signal (S2) ; (e) determining the presence of undesired matter in the egg to be examined on the basis of the outcome of said comparison; characterized in that: further the following method step is carried out : (f) only for brown eggs, the first and second measuring signals are corrected relative to each other with at least one fraction (γ,-γ') for brown eggs. 2. A method according to claim 1, characterized in that only for brown eggs, one of said two measuring signals is corrected with the at least one fraction (γ,-γ') . 3. A method according to claim 1 or 2 , characterized in that the at least one fraction (γ,-γ') for brown eggs is maintained constant for all brown eggs. 4. A method according to any one of the preceding claims, characterized in that the at least one fraction (γ:γ ' ) has been determined in a brown-calibration procedure based on at least one bloodless brown egg. 5. A method according to any one of the preceding claims, characterized in that the second measuring signal (S2) is obtained in a wavelength range (λ2) where blood has an absorption peak, and wherein the first measuring signal (SI) is obtained at a wavelength (λl) which is located at a short distance next to said absorption peak. 6. A method according to any one of the preceding claims, characterized in that further according to a predetermined criterion light brown eggs are separated from dark brown eggs, while the first and second measuring signal for light brown eggs are corrected relative to each other with a first fraction (γl;γl') for light brown eggs, and the first and second measuring signal for dark brown eggs are corrected relative to each other with a second fraction (γ2;γ2') for dark brown eggs, the first fraction (γl;γl') differing from the second fraction (γ2,-γ2'). 7. A method according to claim 6, characterized in that the light brown eggs are separated from dark brown eggs using a color camera such as, for instance, two semiconductor diodes which are sensitive to green and red light, respectively. 8. A method according to claim 6 or 7, characterized in that the fraction (γl;γl') for light brown eggs has been determined in a light brown-calibration procedure based on at least one bloodless light brown egg and the fraction (γ2,-γ2') for dark brown eggs has been determined in a dark brown-calibration procedure based on at least one bloodless dark brown egg. 9. A method according to any one of the preceding claims, characterized in that prior to the method step (f) , further the following method step is carried out: (h) determining whether an egg to be examined is a white egg or a brown egg. 10. A method according to claims 7 and 9, characterized in that using the camera it is determined whether an egg is a white, light brown or dark brown egg. 11. A method according to claim 9, characterized in that to determine whether an egg to be examined is a white or a brown egg, the first measuring signal (SI) is compared with a white-reference (SO) . 12. A method according to any one of the preceding claims, characterized in that the first and second measuring signal for all eggs are corrected relative to each other with a first correction factor (c) which has been determined in a white-calibration procedure based on at least one bloodless white egg. 13. A method according to any one of claims 1-5, characterized in that the second measuring signal (S2) is compared with a first measuring signal corrected relative to the second measuring signal, (l-γl)'c'Sl, where c is a first correction factor which satisfies c = S2/S1 in the case of a bloodless white egg, and said fraction γ for brown eggs satisfies γ = (cSl-S2) /c'Sl in the case of a bloodless brown egg. 14. A method according to claim 6, 7 or 8 , characterized in that for light brown eggs the second measuring signal (S2) is compared with a first measuring signal corrected relative to the second measuring signal, (l-γl) c'Sl, where c is a first correction factor which satisfies c = S2/S1 in the case of a bloodless white egg, and said fraction γl for light brown eggs satisfies γl = (c'Sl-S2) /cSl in the case of a bloodless light brown egg, while for dark brown eggs the second measuring signal (S2) is compared with a first measuring signal corrected relative to the second measuring signal, (l-γ2)'c'Sl, where c is said first correction factor and said fraction γ2 for dark brown eggs satisfies γ2 = (CS1-S2) /c'Sl in the case of a bloodless dark brown egg. 15. A method according to claim 13 or 14, characterized in that in a white-calibration procedure a bloodless white egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the first correction factor c is determined as c = S2/S1. 16. A method according to claim 11, wherein in a white-calibration procedure a bloodless white egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the white-reference (SO) is defined as the value of the first measuring signal (SI) . 17. A method according to claims 4 and 12, wherein in the brown-calibration procedure a bloodless brown egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the fraction γ is determined according to the formula γ = (CS1-S2) /c'Sl . 18. A method according to claims 8 and 14, characterized in that in the light brown-calibration procedure a bloodless light brown egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the fraction γl is determined according to the formula γl = (c Sl-S2)/c SI, and in the dark brown-calibration procedure a bloodless dark brown egg is subjected to the radiation LI and L2 , the signals SI and S2 are measured, and the fraction γ2 is determined according to the formula γ2 = (c S1-S2) /c SI . 19. A method according to any one of the preceding claims, wherein the second wavelength (λ2) is approximately equal to 577 nm and wherein the first wavelength (λl) is approximately equal to 597 nm. 20. A detection device (20) arranged for carrying out the method according to any one of the preceding claims 1-19, comprising : a conveying device (21) for conveying eggs (3) ; a detection station (22) , arranged along the conveying device (21) , comprising at least one light source (1) for emitting said radiation (Tl, T2) and at least one detector (2) , for providing said measuring signals (SI, S2) ; and a signal processing device (10) of which a signal input is coupled for receiving said measuring signals (SI, S2) . 21. A device according to claim 20, arranged for carrying out the method according to any one of claims 4, 12-15, 17 or 18, wherein the signal processing device (10) is arranged to compute in a white-calibration procedure the first correction factor (c) as c = S2/S1. 22. A device according to claim 20 or 21, wherein the signal processing device (10) is arranged to determine in a brown-calibration procedure the fraction γ according to the formula γ = (CS1-S2) /c'Sl . 23. A device according to claim 20 or 21, wherein the signal processing device (10) is arranged to determine in a light brown-calibration procedure the fraction γl according to the formula γl = (cSl-S2) /c'Sl, and to determine in a dark brown-calibration procedure the fraction γ2 according to the formula γ2 = (cSl-S2) /c'Sl . 24. A device according to any one of claims 20, 21, or 23, wherein the signal processing device (10) is arranged to determine in an actual measuring procedure whether an egg to be examined is a white, light brown or dark brown egg, and if the egg to be examined is a light brown egg, to compute the value (l-γl)'c'Sl, and if the egg to be examined is a dark brown egg, to compute the value (l-γ2)cSl.

Inventors: SCHOUENBORG KURT OTTO PETER, SCHOUENBORG, KURT, OTTO, PETER
Applicants: FOOD PROCESSING SYSTEMS, SCHOUENBORG KURT OTTO PETER, FPS FOOD PROCESSING SYSTEMS B.V., SCHOUENBORG, KURT, OTTO, PETER
Application year: 1998
Main classification: G01N33
IPC codes: G01J3, G01N21, G01N33