Classifications

• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
  • G01N21/47—Scattering, i.e. diffuse reflection
  • G01N21/4738—Diffuse reflection, e.g. also for testing fluids, fibrous materials

Definitions

• the invention relates to a method and an apparatus for reflection measurement of unburned carbon in fly ash from a heating plant, whereby is used a residue coal or carbon meter with a transparent measuring tube, preferably made of glass, wherein an ash sample taken from the fly ash in the flue duct of the heating plant can be passed through one end of the measuring tube and deposited inside the measuring tube and after completion of the reflection measurement can be blown out of the measuring tube or back to the flue duct.
• a reflection measurement is obtained a reflecting coefficient providing a relative expression for the content of unburned carbon in the fly ash.
• a reflection measurement on a surface area of the ash sample said area abutting the inner surface of the measuring tube, can be made e.g. by means of electromagnetic waves which e.g. may provide a colour measuring.
• the result of a reflection measurement can be shown by an apparatus with digital reading or analog output of residue carbon as percentage.
• the ash might have stratified so as to provide "black carbon stripes” or carbonless “white ash stripes”. If measuring takes place in one of said "stripes", the measuring will erroneously show an excessively high or excessively low residual carbon content, respectively, in the ash.
• An air pocket may occur in the ash, which air poc- ket cannot reflect an electromagnetic wave train, e.g. from infrared light. Thus, a reflection measurement on the air pocket will also erroneously show an excessively high residual carbon content.
• the ash is relatively homogeneous but might from time to time be very inhomogeneous. In the latter case a reflection measurement will show a different residual carbon content depending on the position of the area on the ash surface where the masure ent is made.
• the waves may have hit one of the ment.-oned "stripes", a black particle or an air pocket in an otherwise white ash surface and may thus have provided an erroneous picture of the content of carbon in the ash and thus of the operational status of the heating plant.
• Only one energy content coefficient for each ash sample is obtained. More energy content coefficients are obtained by measuring by means of one and same apparatus on subsequent ash samples or by simultaneous measurings by moans of several apparatuses each measuring its respective ash sample.
• This known method thus demands an extensive number of measurings on different ash samples and subsequent extensive calculations in order to obtain a useful measuring result.
• the object of the present inven- tion for reflection measurement to provide a method and an apparatus being less time consuming, and whereby the mentioned disadvantages have been eliminated, and whereby a high probability of a correct measuring result can be obtained quickly.
• this is achieved by a method of the kind mentioned above, which is characterized in that the reflection measurement is made by directing wave trains of infrared light emitted from sources towards each of at least two different areas on the surface of the ash sample located in the tube and at a certain distance from the sources, that the part of the wave train which thereby is reflected, is returned to respective infrared detecting receivers, and that the proportion between the energy of mutually dependent wave trains respectively emitted towards the ash sample surface and reflected therefrom is measured, so that at least one reflection measurement is made on at least two different areas abutting the inner side of the measuring tube on the outer surface of the ash sample, and that the results of the reflection measurements are compared in the form of reflec- tion coefficients.
• At least two reflection coefficients is obtained which can be immediately compared and on the basis hereof be accepted or rejected, by means of only one measuring operation comprising all measurings of the strength of several emitted and reflected wave trains of infrared light having a wave length from about 7600 A and up to about 1 mm, and which are emitted towards and reflected from only one ash sample.
• the method according to the invention is therefore more simple with respect to measurings, as well as time saving compared to the known methods. If the reflection coefficients measured are practically identical, the measuring operation is accepted.
• the method in an embodiment of the invention be characterized in that measurements are made in ash sample surface areas located at different planes perpen- dicularly to the axis of the measuring tube.
• the me-thod may be characterized in that measurements are made in ash sample surface areas being mutually angularly displaced around the axis of the measuring tube.
• the method may be characterized in that measurements are made in six ash sample surface areas located in two radial planes with three ash sample surface areas in each plane.
• measurements can be made on several areas on the surface of the ash sample, not only in one plane, but also in ash sample surface areas located on vertical lines, inclined lines or on curved lines.
• an average coefficient is calculated based on the reflection co- efficients measured.
• the reflection coefficients differing essentially from said average coefficient will be extracted.
• a new average coefficient is calculated, which can be considered as the valid reflection coefficient, the result of the measuring operation.
• the method according to the invention may also be characterized in that transmission measurements are made regularly through the measuring tube when it has been emptied for ash, for achieving a transmission coefficient for the set point correction or for calibration purposes.
• the transmission coefficient measured by an empty measuring tube can be used as calibration value by subsequently measured reflec- tion coefficients when the measuring tube is filed. If the measuring tube transmits too little light, the measuring tube should be cleaned with respect to adhering soot or should be changed due to wear and tear.
• the method can be carried out by means of an appa- ratus of the kind mentioned in the introductory clause, which method according to the invention is characterized in that the apparatus has radiation sources for emitting wave trains of infrared light towards each of at least two different areas on the surface of the ash sample, the surface of which abutting the inner surface or side of the measuring tube, receivers for reception of the reflected wave trains from the respective areas, means for measuring the proportion (reflection coefficient) between the energy of interconntected wave trains respectively emitted towards the ash sample surface area and reflected therefrom, means for comparing the reflection coefficients, means for calculation and showing their average value after the most differing reflection coeffici- ent/s has/have been extracted.
• An embodiment of the apparatus is advantageous by the residue carbon meter comprising an element consisting of a section of a hollow cylinder being placed relatively to the measuring tube in such position that the inner wall of the cylinder is located at a distace from and parallel to the outer wall of the measuring tube, and where at least two pairs of channels are provided between the outer wall and the inner wall of the cylinder, said channels being arranged in pairs and so with respect to each other that a wave train of infra- red light can be emitted from an infrared radiation source, such as an infrared diode, through the one channel of a pair and towards an area of the surface of the ash sample, and so that a part of the wave train emitted is reflected from the ash sample surface area and will be returned through the other channel of the pair of channels to a receiver of the infrared light radiation.
• an infrared radiation source such as an infrared diode
• An embodiment of the apparatus is advantageous thereby that the cylinder contains channel pairs being so arranged that measurements may be made in ash sample surface areas located at different planes perpendicularly to the axis of the measuring tube.
• Another embodiment of the apparatus is advanta ⁇ reous thereby that the cylinder contains channel pairs being so arranged that measurements can be made in ash sample surface areas located mutually angularly displaced around the ax:-s of the measuring tube.
• a further embodiment of the apparatus is advantageous thereby that the cylinder contains six channel pairs; being so arranged that measurements are made in six ash sample surface areas located on two radial planes with three areas in each plane.
• the inner wall 14 of the cylinder 13 is adapted for being located at a certain distance from and parallel to the outer wall of the transparent measuring tube of the residue carbon meter.
• the wall of the cylinder 13 has at least two channels or pairs of channels 1 and 2, 3 and 4 extending between the inner wall 13 and the outer wall 15 of the cylinder, and the shown embodiment implies six pairs of channels 1 and 2, 3 and 4 etc.
• the axis of a first channel 1 is directed radially against an area on the inner side of the measuring tube.
• the axis of another channel 2 is arranged at the same axial plane as the first channel 1 , below said channel 1 and at an angle of e.g. 25° with respect thereto and directed against the same area on or a small distance behind the inner side of the measuring tube.
• a subsequent channel pair 3, 4 consisting of a channel 3 arranged at a plane below the first channel 1.
• the axis of said channel 3 is directed radially against another area on or a small distance behind the inner side of the measuring tube.
• the other channel 4 in this pair of channels is arranged at the same axial plane as the channel 3 belonging to the pair, above said channel and at an angle relatively thereto and di- rected against the other area on or a small distance behind the inner side of the measuring tube.
• a wave train of infrared light from e.g. an infrared diode is emitted through e.g. the channels 1, 3, ... arranged radially in the channel pairs towards the surface of the ash for illuminating of areas on the ash surface. From each of these areas is returned a part of the infrared light reflected from the areas through the other channels 2, 4, .. etc of the pairs to infrared receivers or vice versa.
• a reflection coefficient can be measured from each of six measuring areas on the ash sample, and an average coefficient of said reflection coefficients can be calculated after a correction based on at least one calibration value which as mentioned can be measured on an empty measuring tu- be.
• each channel pair can be used a single channel for emission and reflection of wave trains, e.g. through two of the fiber- optical light guides or bunches thereof arranged in the channel.
• a central fiber-optical light guide bunch may advantageously be arrang- ed in each channel, said bunch being totally or partly surrounded by a fiber-optical light guide bunch arranged around the central bunch.
• the electromagnetic wave train is the emitted through one and reflected through the other fiber- optical light guide bunch.
• the value calculated as valid reflection coefficient is an intermediate result used for calculation of the weight percentage of unburned carbon in the fly ash, which is the result to be presented.

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• Physics & Mathematics (AREA)
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• General Health & Medical Sciences (AREA)
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• Investigating Or Analysing Materials By Optical Means (AREA)

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• 1996
  • 1996-07-05 DK DK74796A patent/DK173406B1/da not_active IP Right Cessation
• 1997
  • 1997-07-07 EP EP97928142A patent/EP1009997A1/en not_active Withdrawn
  • 1997-07-07 CN CN97196187A patent/CN1093937C/zh not_active Expired - Fee Related
  • 1997-07-07 WO PCT/DK1997/000300 patent/WO1998002729A1/en not_active Ceased
  • 1997-07-07 AU AU32555/97A patent/AU3255597A/en not_active Abandoned
  • 1997-07-07 RU RU99101936/28A patent/RU2180744C2/ru not_active IP Right Cessation

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