WO2006111151A1 - Dispositif de rayonnement thermique - Google Patents
Dispositif de rayonnement thermique Download PDFInfo
- Publication number
- WO2006111151A1 WO2006111151A1 PCT/DE2006/000692 DE2006000692W WO2006111151A1 WO 2006111151 A1 WO2006111151 A1 WO 2006111151A1 DE 2006000692 W DE2006000692 W DE 2006000692W WO 2006111151 A1 WO2006111151 A1 WO 2006111151A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- reflector
- radiator
- light source
- housing
- heat radiator
- Prior art date
Links
Classifications
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05B—ELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
- H05B3/00—Ohmic-resistance heating
- H05B3/0033—Heating devices using lamps
- H05B3/009—Heating devices using lamps heating devices not specially adapted for a particular application
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05B—ELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
- H05B2203/00—Aspects relating to Ohmic resistive heating covered by group H05B3/00
- H05B2203/032—Heaters specially adapted for heating by radiation heating
Definitions
- the invention relates to a heat radiator in rod form, consisting of a light source, a housing and a reflector, and a multi-zone radiator.
- Rod-shaped heat radiators are known as so-called round tube or as a double tube with reflector.
- DE 4438870 (Heraeus Noblelight) discloses an infrared radiator with an elongated radiation source in which a quartz glass capillary tube is used which contains a carbon fiber band as the resistance body.
- the quartz glass tube is designed as a double-tube radiator, the rear side being provided with a reflection layer.
- radiators used for heating products with circular or elliptical cross sections emit the radiation in a large emission cone. Only a small part of the technically usable radiation is used to heat the products. The achievable with the known radiators area performance for heating products is therefore not optimal.
- multi-zone radiators which consist of several, arranged in a direction parallel to the heating material heat radiators, it is not yet possible to provide heating energy for heating products within a sharply delimited temperature zone. Also, it is very difficult to comply with the known multi-zone radiators accurate temperature profiles, since the radiation angle of the individual heat radiators are very large and therefore overlaps the radiated heat energy of each heat radiator with the adjacent heat radiator.
- Object of the present invention is to produce a heat radiator of the type mentioned in rod form of vitreous material, which does not have the disadvantages mentioned and allows a small Abstrahlkegel and thus increasing the yield of technically usable radiation.
- the area performance should be precisely adjustable and a variable temperature profile on the surface of the heat-up material should be made possible.
- FIG. 1 An inventively designed heat radiator with a straight front surface is shown in FIG. This already allows a narrow beam angle through the parabolic curved reflection wall.
- FIG. 1 An inventive heat radiator with an integrated, spherically formed or convex lens on the front side is shown in FIG.
- the radiation angle decreases in accordance with the lens curvature, so that a zone with very strong radiation and the focusing of the emitted beams is achieved.
- Fig. 9 emitter according to the prior art
- the radiator is equipped with a light source 2, a housing 3 and a reflector 4 on the back.
- the housing is made of quartz glass, which closes like a shell completely around the light source, wherein a radiation exit surface 5 is located on the front and the reflector surface on the back.
- parabolic-shaped reflector In the case of a parabolic-shaped reflector, the radiation intensities shown in FIG. 1 result, with a higher heat intensity being achieved in the overlapping area of many beams than in the outer area.
- parabolic shape of the reflector prevents radiation in the glass body dead by reflections and thereby accounts in the energy balance as usable radiation.
- FIG. 2 shows an alternative form of the heat radiator with a luminous source 2.1 arranged in the cavity of the housing 3.1 according to the present invention.
- the quartz glass envelope has a reflector 4.1 at the rear and at the front a lenticular thickening 6-1, so that the radiation angle ⁇ is considerably reduced compared to the example of Figure 1.
- the radiation angle ⁇ is in the range of 50 ° to 60 °, wherein the focal length F of the lenticular thickening 6.1 results according to the following equation:
- R 2 inner radius of curvature of the lenticular thickening
- FIG. 3 shows a heat radiator according to the invention with a light source 2.2 arranged in the cavity in the housing 3.2 and with a front and a back lens-shaped thickening 6.2, 7 and a reflector 8 in an application (bonding a spine) represented.
- the beam path is shown with a dashed line, it can be seen that a maximum of surface power for heating the product 9 is achieved by the narrow focus.
- a high uniformity of the bond is provided by the zonal limitation of the radiation field.
- the housing may have instead of the thickening 7 on its back an outwardly curved, patch body, on which the reflector rests flush.
- the heat radiator from the prior art according to FIG. 4 records a high heat loss due to the large reflector wrap angle ⁇ of 340 ° to 355 ° and as a result the missing front / rear lenses.
- the reflector 8.1 is pulled around the housing surface of the radiator far, so that only a small opening angle for the exiting heat ray, which is directed to a spine 9.1 remains. The rest of the non-emergent rays is consumed as heat within the radiator, which is why it must be additionally cooled.
- FIG. 5 shows in section A a multi-zone radiator consisting of six individual heat radiators 10 to 15 whose heat outlet surfaces are arranged parallel to the material to be heated 16. A arranged at the upper portion of the Auffilgutes 16 thread 17 is outside the radiation field of the heat radiator 10 to 15.
- a multi-zone radiator according to the prior art with associated overall temperature profile is shown in section A of Figure 6. Since the radiation fields of the heat radiators 20 to 25 strongly overlap, so-called bulkhead plates, which are water-cooled, are needed in order to limit the heat-affected zone. For example, a partition plate 26 for shielding the thread 27 in the upper region of the Auffilgutes 16 is arranged. With this device, a precisely adjustable temperature profile can not be realized, so that a wavy surface as shown in section C of FIG. 6 results after the deformation of the heating material 16. Due to the scale change to 1: 5, the undeformed thread 27 decreases in the representation "C".
- the temperature profiles of the multi-zone radiator according to the invention are compared as a curve 28 with the curve 29 obtained according to the prior art. It turns out that due to the elevated temperature 30 in the areas large deformation and the lower temperatures 31 in the areas of low deformation, the potential of the heat-up can be better utilized by adjusting the favorable for each deformation temperature profile, so that the inventive arrangement is superior to the prior art in the control of the heating process and the deformation process. Very sharp-edged contours can be imaged on the surface of the heat-up material.
- the beam paths of a conventional round tube radiator with reflector 41 and a conventional double-tube radiator with reflector 42, 43 are shown in FIGS. 6 and 7.
- the radiation angle in a conventional round tube emitter is approximately 180 ° with a uniform radiation distribution.
- the conventional double-tube reflector with the reflector of the beam angle is also about 165 °, but it results from reflected radiation, an area with increased radiation power, due to the reflector shape, a portion of the radiation is reflected back and forth in the radiator so long that the radiation energy completely converted into waste heat.
- Another disadvantage is that a large part of the emitted power is scattered over the entire emission angle and therefore can not contribute to increasing the maximum Einstrahl amongsêt.
- Another advantage is that due to the sharp delimitation of the radiation cone, it is possible to specifically heat only certain zones of the product and thus, for example, to produce a temperature profile in the product.
- the lens creates a focal point in which the power density increases extremely. This focusing has advantages for certain applications, for example in the welding wire preheating.
- the focal point extends as a line or rectangle whose width to the radiator diameter is in a ratio of 0.05 to 0.5, for special applications up to 1, 0.
- the housing is thickened like a lens in the area of the exit surface. But it can also be placed patch body on the housing, which is particularly advantageous on the back of the heat radiator according to the invention.
- the reflection layer is integrated with the rear side of the heat radiator. This means that the beam path is not scattered or broken by intermediate layers, for example by air gaps or by other materials, but is held with high power output within the effective reflection range of the heat radiator.
Landscapes
- Control Of Resistance Heating (AREA)
- Non-Portable Lighting Devices Or Systems Thereof (AREA)
Abstract
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP06722810A EP1897410B1 (fr) | 2005-04-20 | 2006-04-20 | Dispositif de rayonnement thermique |
DE112006001693T DE112006001693A5 (de) | 2005-04-20 | 2006-04-20 | Wärmestrahler |
DE502006002083T DE502006002083D1 (de) | 2005-04-20 | 2006-04-20 | Wärmestrahler |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102005018454.5 | 2005-04-20 | ||
DE200510018454 DE102005018454A1 (de) | 2005-04-20 | 2005-04-20 | Wärmestrahler |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2006111151A1 true WO2006111151A1 (fr) | 2006-10-26 |
Family
ID=36644862
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/DE2006/000692 WO2006111151A1 (fr) | 2005-04-20 | 2006-04-20 | Dispositif de rayonnement thermique |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP1897410B1 (fr) |
DE (3) | DE102005018454A1 (fr) |
WO (1) | WO2006111151A1 (fr) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101951705A (zh) * | 2010-08-31 | 2011-01-19 | 广东格兰仕集团有限公司 | 发热管 |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US606792A (en) * | 1898-07-05 | Electric radiator | ||
US4017758A (en) * | 1974-04-16 | 1977-04-12 | U.S. Philips Corporation | Incandescent lamp with infrared filter |
GB2133259A (en) * | 1982-12-31 | 1984-07-18 | Hans Fritz | Electric radiant heater |
US5276763A (en) * | 1990-07-09 | 1994-01-04 | Heraeus Quarzglas Gmbh | Infrared radiator with protected reflective coating and method for manufacturing same |
FR2732181A1 (fr) * | 1995-03-21 | 1996-09-27 | Thermal Quartz Schmelze | Projecteur de rayonnement et panneau radiant |
Family Cites Families (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR777012A (fr) * | 1933-10-31 | 1935-02-09 | Perfectionnements aux lampes électriques d'éclairage | |
FR829585A (fr) * | 1937-11-19 | 1938-06-30 | Appareil d'éclairage | |
DE1817548U (de) * | 1960-06-29 | 1960-09-01 | Accumulatoren Fabrik Ag | Gluehbirne mit eingebautem reflektor. |
DE2413111A1 (de) * | 1974-03-19 | 1975-10-09 | Cima International Distributio | Lampe fuer bildwurfeinrichtungen |
DE4021798A1 (de) * | 1990-07-09 | 1992-02-06 | Heraeus Quarzglas | Infrarotstrahler mit geschuetzter reflexionsschicht und verfahren zu seiner herstellung |
DE4438870B4 (de) * | 1994-11-03 | 2004-11-11 | Heraeus Noblelight Gmbh | Infrarotstrahler mit langgestrecktem Widerstandskörper als Strahlenquelle |
DE10029437B4 (de) * | 2000-06-21 | 2005-11-17 | Heraeus Noblelight Gmbh | Infrarotstrahler und Verfahren zum Betreiben eines solchen Infrarotstrahlers |
-
2005
- 2005-04-20 DE DE200510018454 patent/DE102005018454A1/de not_active Withdrawn
-
2006
- 2006-04-20 DE DE502006002083T patent/DE502006002083D1/de not_active Expired - Fee Related
- 2006-04-20 WO PCT/DE2006/000692 patent/WO2006111151A1/fr active Application Filing
- 2006-04-20 EP EP06722810A patent/EP1897410B1/fr not_active Expired - Fee Related
- 2006-04-20 DE DE112006001693T patent/DE112006001693A5/de not_active Withdrawn
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US606792A (en) * | 1898-07-05 | Electric radiator | ||
US4017758A (en) * | 1974-04-16 | 1977-04-12 | U.S. Philips Corporation | Incandescent lamp with infrared filter |
GB2133259A (en) * | 1982-12-31 | 1984-07-18 | Hans Fritz | Electric radiant heater |
US5276763A (en) * | 1990-07-09 | 1994-01-04 | Heraeus Quarzglas Gmbh | Infrared radiator with protected reflective coating and method for manufacturing same |
FR2732181A1 (fr) * | 1995-03-21 | 1996-09-27 | Thermal Quartz Schmelze | Projecteur de rayonnement et panneau radiant |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101951705A (zh) * | 2010-08-31 | 2011-01-19 | 广东格兰仕集团有限公司 | 发热管 |
Also Published As
Publication number | Publication date |
---|---|
EP1897410A1 (fr) | 2008-03-12 |
DE102005018454A1 (de) | 2006-11-09 |
DE112006001693A5 (de) | 2008-04-03 |
EP1897410B1 (fr) | 2008-11-12 |
DE502006002083D1 (de) | 2008-12-24 |
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