Method and apparatus for heatstrengthening glass sheets

Abstract: A glass sheet heated close to a softening temperature is heat strengthened by cooling it at a certain controlled cooling rate. The cooling is effected in a space between cooling panels (9) and the cooling panels are cooled by a gas jet (8) which is applied to the surfaces of cooling panels (9) facing away from the glass sheet. A cooling space temperature measurement can be used for controlling the power of a cooling jet.

Description: The present invention relates to a method for heat-strengthenign glass sheets in which a glass sheet is heated in a furnace section close to a softening temperature and then cooled in a heat strengthening section at a certain controlled cooling rate, the heated glass sheet being carried into a space between upper and lower cooling panels in said heat strengthening section, the cooling panels being cooled by a plurality of upper and lower gas jets applied to the surfaces of the cooling panels facing away from the glass sheet, said controlled cooling being carried out in a space confined by the cooling panels. The invention relates also to an apparatus for heat-strengthening glass sheets, said apparatus comprising a furnace which is provided with heating elements for heating glass sheets close to a softening temperature, heat strengthening station which is provided with nozzles above and below a glass sheet for blowing a cooling gas, a blower or a fan which is connected to said nozzles by way of a manifold a conveyor for carrying glass sheets in horizontal direction through furnace and cooling station, and upper and lower cooling panels fitted between the cooling nozzles and the conveyor, said cooling panels confining therebetween a cooling space with a glass sheet therein delivering heat to cooling panels which, in turn, are cooled by said blasting of a cooling gas. US-A-4,236,909 discloses a method and apparatus for thermal treatment of glass sheets to provide a break pattern that represents an improvment over the typical break patterns that are produced when glass sheets are either tempered or heat-strengthened by conventional techniques of heating to the above strain point of the glass and a temperature sufficient for tempering followed by cooling at a controlled rate of cooling or are heat-treated by heating the glass sheets to a temperature sufficient for tempering followed by natural cooling. Furthermore, US-A-4,400,194 describes heat-strengthening of glass sheets used in large window openings, where it is important that the glass have suitable break patterns that prevent the glass from forming islands within the supported marginal periphery when the window fractures. Heat-strengthened glass is treated to have a break pattern that permits the fractured glass sheet to be retained within an installation frame by moving a glass sheet through a heating area, force cooling the side portions of the moving sheet while cooling the itermediate portions of the sheet at a lesser rate to establish a temperature gradient between the side portions and the intermediate portion and subsequently applying a quenching medium to the entire moving sheet. The temperature gradient in the sheet is achieved by a plurality of baffles, e.g. plate having an imperforate center portion and apertured or slotted end portions and facilities movable relative to quenching nozzles to control the passage of the quenching medium through the slotted end portion of the baffles to control the temperature gradient imparted to the glass sheet. It is, however, not known from these documents to oscillate the glass sheets between the cooling panels. The heat-strengthening of glass differs from tempering in the sense that the cooling occurs at a substantially slower rate, which also substantially reduces the surface tensions of glass. The characteristics of heat-strengthened glass are described, e.g. in published GB Application 2 191 998. In order to produce standardized heat-strengthened glass, it is necessary that the cooling rate be accurately controlled. A particular problem here is that, as the thickness of glass changes, the cooling rate also changes substantially (if cooling conditions remain constant). On the basis of earlier experiences, it seems that e.g. 8 mm glass is heat-strengthened to the Japanese standards by bringing it to room temperature after heating. This situation appears from the set of heat-strengthening curves shown in the accompanying fig. 6. The figure shows that, if 10 mm glass is treated the same way (cooling at a room temperature), it is already subjected to an excessive heat strengthening. Thus, if 10 mm or 12 mm glass is to be heat-strengthened, this must be carried out in an environment hotter than a room temperature. The following estimates deal with the temperatures of a cooling environment required in heat strengthening. If glass is in slow movement in a quiet environment at a room temperature, according to performed measurements, it cools with a heat-transfer coeeficient of 45 W/m 2 K. Thus, the glass delivers heat at a rate of 50 kW/m 2 . Supposing that the delivered heat capacity of 10 mm glass is obtained approximately as inversely proportional from glass thicknesses: 10 mm 8 mm = 50 kW/m 2 P(10 mm) => P(10 mm) = 40 kW/m 2 Thus, the temperature difference between glass and ambient air will be T = P(10 mm) α · 2 · A = 40000 W/m 2 45 · 2 · 1 = 444°C => T air = 610°C - 444°C ≈ 150°C In a corresponding calculation on 12 mm glass, T air will be 250°C. Figs. 7 and 8 illustrate by way of an example the heating and heat-strengthening curves for 10 mm and 12 mm glasses. The curves reveal that e.g. 12 mm glass must remain within a 250°C temperature environment for about 250 seconds. On the other hand, a maximum loading delivers heat at a rate of appr. 400 kW. In other words, if heat strengthening is effected in a closed environment, heat must be removed from the environment at a rate of appr. 400 kW in order to maintain the environment at a constant temperature. This corresponds to the supply of 20°C air into the environment at a rate of 2 m 3 /s, since at a rate of 400 kW air can be heated at 2 m 3 /s from 20°C to 250°C. Accordingly, in the case of 10 mm glass, the maximum loading delivers heat at a rate of appr. 450 kW, which corresponds to the raising of the temperature of appr. 3,7 m 3 /s air flow from 20°C to 150°C. As pointed out above, the heat strengthening of e.g. 12 mm glass must be carried out at about 250°C in an environment with no major air movements. If the heat strengthening is carried out in a furnace, the only possible approach is probably to supply into the furnace a sufficient amount of air at a room temperature in order to maintain temperature of the furnace air at equilibrium. On the other hand, this causes a strong movement of air, whereby the coefficient of heat transfer α is considerably increased, approximately doubled. Thus, the cooling rate will be too rapid and the actually required air temperature is in the order of 500°C. In fact, a problem here is to control the air input in a manner that α will remain approximately the same all over the glass and that the air flow coming into contact with glass has reached the same temperature everywhere in itself. Another problem is an increased transfer of heat caused by massive ceramic rolls, the problem being how to obtain the same cooling rate on the top and bottom surfaces of glass. A third problem is a possibility of glass breaking. It is an estimate that, on the average, every 50 th glass is broken. This means that a furnace should be fitted with a scrap conveyor and, furthermore, a furnace must be quickly openable, so that the harmful shattered bits and pieces can be removed from between the rollers or from top of the lower resistances. A fourth problem is the inflexibility of a furnace to varying production: if heat-strengthened glass is produced today, today is no good for any other production since raising the furnace temperature back to the 700°C temperature takes a long time. Furthermore, if one of the chambers of a dual-chamber furnace is used for heat strengthening, it means the heating of glass can only be effected in the other chamber and the lower temperature of the first chamber cannot be exploited. A result of this is then that the heating of large-size glasses becomes essentially more difficult. An object of the invention is to provide a method and an apparatus for heat-strengthening glass sheets without the above problems. A particular object of the invention is to provide a method and an apparatus, whereby the cooling of even rather thick (≧ 10 mm) can be carried out in a controlled fashion, i.e. at a sufficiently slow and uniform rate over the entire surface area of a glass sheet. Another object of the invention is to provide a method and an apparatus capable of producing also tempered glass in addition to heat strengthening. A particular additional object of the invention is to provide a method and an apparatus, capable of flexible production, i.e. also in small series, of both heat-strengthened and tempered glass with a varying glass thickness. These objects are achieved by the method of claim 1 and the apparatus of claim 4. Prefered embodiments are defined in the dependent claims. One embodiment of the invention will now be described in more detail with reference made to accompanying drawings, in which fig. 1 shows an apparatus of the invention in a schematic vertical section. Fig. 2 is a more detailed view in a schematic vertical section showing a heat-strengthening station included in the apparatus. Fig. 3 shows a heat-strengthening station of the invention in a schematic cross-section. Fig. 4 is a schematic side view showing the openability of a heat-strengthening station of the invention and fig. 5 is schematic side view showing an alternative embodiment for the heat-strengthening station. Fig. 6 illustrates heat-strengthening curves for various glass thicknesses. Fig. 7 shows the temperature of 10 mm glass as a function of time at various stages of heat strengthening. In association with the glass temperature curve there is also shown the temperature of each treating station and a coefficient of heat transfer between glass and ambient air. Fig. 8 is a similar to fig. 7 but deals with 12 mm glass whose heat strengthening was carried out by using a test apparatus of the invention. The apparatus shown in fig. 1 includes a first furnace section 1, a second furnace section 2, a heat-strengthening station 3, and a cooling station 4. A conveyor included in furnace 1, 2 comprises horizontal rollers 5 and a conveyor included in stations or sections 3, 4 comprises horizontal rollers 6. Rollers 5 and 6 are used to carry glass sheets from one section to another and, in addition, by rotating the rollers in a reciprocating fashion, the glass sheets are set in an oscillating motion in each section. Heating elements 19 included in furnace sections 1 and 2 can be e.g. resistance elements but it is naturally possible to employ also other types of sources of heat, such as gas burners. Stations 3 and 4 are provided with cooling air nozzles 8 on either side of a top surface level 7 of a conveyor consisting of rollers 6. As shown in more detail in fig. 2, said nozzles 8 are associated with nozzle housings 18, the cooling air being supplied therein by means of blowers or fans 11 and 12. Naturally, it is also possible to employ compressors or combinations of fans and compressors depending on desired blast pressures and the actual size of a jet orifice. In terms of construction, said nozzles 8 can be identical to those typically used in the quenching stations of tempering plants. These have been generally known and used in various configurations for decades and, thus, such construction is not described further in this context. A novel feature in the invention is the fitting of cooling panels 9 between blast nozzles 8 and a glass sheet 15 to be heat-strengthened. The cooling panels 9 are made of a highly heat-conductive material, preferably a metal, and secured to nozzle housings 18. The cooling panels 9 confine therebetween a heat-strengthening chamber 10, whose temperature can be controlled by cooling said upper and lower cooling panels 9 by means of cooling air jets. The power of fans 11 and 12 is controlled by means of temperature sensors 13', connected with thermostats 13 and a regulator 14. Said sensors 13' can be adapted to measure temperature between cooling panels 9 or glass temperature or both. In addition to controlling the power of fans 11 and 12, the temperature of space 10 can be controlled by adjusting the distance of panels 9 from glass sheet 15. The best way of doing this is to move the entire set of nozzle housings 18 together with their panels 9 in vertical direction. Of course, it is also possible to make the distance of panels 9 from nozzles 8 adjustable. The chamber space 10 is designed as a closed environment by having its ends and sides thermally insulated. Thus, heat is transmitted in a controlled fashion over the entire surface area of glass sheet 15 to cooled metal panels 9. The transmission of heat is effected by means of both radiation and convection. A thermal insulation barrier confining space 10 at the ends and sides, and serving also as a flow barrier, can be designed by using fixed or movable walls. Fig. 2 illustrates a vertically movable gate 16 in the end wall. Especially at the ends, the insulation and flow barrier can also comprise an air screen 17 which closes after a glass sheet has arrived in the chamber space. It is also possible that, particularly with small-size glasses, the space confined by said panels has open sides. As can be seen from fig. 3, metal panels 9 are preferably solid continuous plates and the material thereof is e.g. AISI 304 2BA. One or each surface of cooling panels 9 can be provided with heat-exchange ribs 9.2 for intensifying the transmission of heat. This may be necessary as heat must be removed from chamber 10 at a rate of 450 kW (which is roughly equivalent to the cooling capacity of the refrigeration machinery of an indoor ice-hockey rink). As a result of the temperature difference between glass sheets 15 and ambient air there will be undesired flows created also in chamber 10 leading to a non-uniform cooling of glass sheet 15. Primarily, the cooling power increases in the marginal sections of a glass sheet. In order to compensate for this irregular cooling effect, it may be preferable that the surface area of heat-excange ribs 9.2 per unit area of cooling panel 9 be larger in the central area of a cooling panel than in the end and/or side edges. In fact, generally by varying the density and/or height of heat-exchange ribs 9.2 it is possible to eliminate the irregularities detected in cooling. It is also possible to employ local heating resistances e.g. between rollers 6 for controlling the regularity of cooling. When heat-strengthening small individual pieces of glass, such resistances can be used at the same time for preheating the chamber space, if necessary. By arranging the nozzle housings along with panels 9 thereof to be pivotable by the area of one of the side edges thereof or, as shown in fig. 4, by the area of at least one of the ends thereof to lie at a major distance from conveyor 6, the bits of broken glass can be readily removed. Neither need said panels 9 be continuous over the entire surface area of heat-strengthening station 3 but the panels can be made up by smaller panelunits 9.1, as shown in fig. 5. Thus, for example, the material and thickness of various panel units 9.1 can be selected to be different e.g. in the central and marginal areas. Another special feature associated with a heat-strengthening apparatus of the invention is that one and the same apparatus can be readily used also for tempering glasses having varying thicknesses. The glass heat-strengthening process involves the heat-strengthening of glass in station 3 and then rapidly cooling it in station 4 by means of an effective cooling air blast, as shown by the curves of figs. 7 and 8. If, instead of heat strengthening, the glass is to be tempered, it will be driven through heat-strengthening station 3 directly into cooling station 4 for carrying out an effective quenching operation. This can be done on all types of glass having a thickness over 3 mm. However, the apparatus is capable of tempering also 3 mm thick glass by designing cooling panels 9 to be readily removable whereby, with panels 9 removed, the quenching operation can be carried out in station 3. Thus, even thin glass does not have enough time for excessive cooling prior to a tempering blast. The invention is not limited to the above embodiment but a variety of modifications can be to its details and structural design within a scope of protection defined by the annexed claims.

Claims: A method for heat-strengthening glass sheets in which a glass sheet is heated in a furnace section (1,2) close to a softening temperature and then cooled in a heat strengthening section (3) at a certain controlled cooling rate, the heated glass sheet being carried into a space between upper and lower cooling panels (9) in said heat strengthening section (3), the cooling panels being cooled by a plurality of upper and lower gas jets applied to the surfaces of the cooling panels (9) facing away from the glass sheet, said controlled cooling being carried out in a space (10) confined by the cooling panels (9) characterized by covering said upper and lower gas jets by said cooling panels over the entire area of said heat strengthening section (3) for uniform cooling of said glass sheet (15); reciprocating or oscillating said glass sheet (15) between said cooling panels (9) during the course of said controlled cooling for heat strengthening; measuring the temperature between the cooling panels (9) or the temperature of said glass sheet and; adjusting the power of the gas jets under the control of said temperature measurement (13) for maintaining a desired temperature in the space (10) between the cooling panels. A method as set forth in claim 1, characterized by measuring the temperature of the top and bottom side of the glass sheet (15) oscillated between cooling panels (9) and by separately adjusting the power of the upper and lower gas jets under the control of temperature measurements (13). A method as set forth in claim 1 or 2, characterized in that the distance of cooling panels (9) from glass sheet (15) is adjusted. An apparatus for heat-strengthening glass sheets, said apparatus comprising a furnace (1, 2) which is provided with heating elements (19) for heating glass sheets close to a softening temperature, heat strengthening station (3) which is provided with nozzles (8) above and below a glass sheet for blowing a cooling gas, a blower or a fan (11, 12) which is connected to said nozzles by way of a manifold (20), a conveyor (5, 6) for carrying glass sheets in horizontal direction through furnace (1, 2) and cooling station (3), and upper and lower cooling panels (9) fitted between the cooling nozzles (8) and the conveyor (6), said cooling panels (9) confining therebetween a cooling space (10) with a glass sheet therein delivering heat to cooling panels (9) which, in turn, are cooled by said blasting of a cooling gas, characterized in that said upper and lower nozzles (8) in said heat strengthening station (3) are covered by said cooling panels (9) over the entire area of said heat strengthening station (3) for uniform cooling of the heated glass sheets while oscillating the glass sheets between the cooling panels (9) with said conveyor (6), and said cooling space (10) is provided with temperature measuring elements (13') which are adapted to control the blasting power of said nozzles (8) at least above the glass sheet and/or to adjust the distance of the cooling panels (9) from the level of conveyor (6). An apparatus as set forth in claim 4, characterized in that for adjusting the distance of the cooling panels (9) from the glass sheet (15), said cooling panels (9) are mounted on nozzle housings (18) which can be manipulated to various distances from the glass sheet. An apparatus as set forth in claim 5, characterized in that said nozzle housings (18) along with said cooling panels (19) can be opened over the area of at least one of the side edges or ends thereof to lie at a sufficient distance from the conveyor (6) for facilitating the removal of pieces of broken glass. An apparatus as set forth in claim 4, characterized in that said cooling panels (9) are provided with heat-exchange ribs (9.2) on one or either side of the panel. An apparatus as set forth in claim 7, characterized in that the density and/or height of the heat-exchange ribs (9.2) is different in different parts of the cooling panel. An apparatus as set forth in claim 8, characterized in that the surface area of the heat-exchange ribs (9.2) per unit area of the cooling panel (9) is larger in the central area of the cooling panel than in the end and/or side edges. An apparatus as set forth in claim 4, characterized in that said blasting nozzles (8) are disposed and dimensioned to match the design of a quenching station, whereby the removal of cooling panels (9) transforms said heat-strengthening station (3) into a quenching station. An apparatus as set forth in claim 4, characterized in that the apparatus includes a cooling station (4) after said heat strengthening station (3) which is provided with said cooling panels (9) the cooling station (4) serving as a quenching station. The application of an apparatus as set forth in claim 11, characterized in that said apparatus is applied both as a heat-strengthening and a tempering unit in a manner that glass sheets to be tempered are driven through the heat-strengthening station (3) to a following quenching station (4). The application of an apparatus as set forth in claim 11, characterized in that the glass sheets heat-strengthened in the heat-strengthening station (3) are carried to the following cooling station (4) for rapid cooling when the glass sheet temperature in the heat-strengthening station (3) has dropped to the range of 420 - 470°C. An apparatus as set forth in claim 4, characterized in that said cooling panels consist of separate, jointable and removable elements. An apparatus as set forth in claim 4, characterized in that there are flow barriers (16, 17) at the ends and/or sides of the space (10) between the cooling panels (9).

Inventors: VEHMAS JUKKA HEIKKI, VEHMAS, JUKKA HEIKKI
Applicants: TAMGLASS ENG OY, TAMGLASS ENGINEERING OY
Application year: 1991
Main classification: C03B27
IPC codes: C03B27