TW201542480A - Method for manufacturing glass plate, and manufacturing apparatus of glass plate - Google Patents

Abstract

The present invention relates to a glass plate manufacturing method, and a manufacturing apparatus of the glass plate. When using a molded body to form a molten glass, the aforementioned glass plate manufacturing method is provided to ensure no generation of devitrification and heterogeneous molten glass, thereby enabling to produce a high quality glass plate. This invention is a glass plate manufacturing molded which pours molten glass to a molded body for producing a glass plate, comprising: a melting step, which melts glass raw materials to generate molten glass; a supplying step, which supplies the molten glass to the molded body via a transfer pipe; and a forming step, which pours the molten glass to the groove part of the molded body while molding the glass plate from the aforementioned molten glass by the down-draw method. In the supplying step, when the molten glass is supplied from the transfer pipe to the groove part of the molded body, a back pressure gradient section at which the static pressure of downstream is higher than that of the upper stream is specified, and the molten glass is heated in the range from the separation point (i.e., the upstream side of the back pressure gradient section) to the reattachment point (i.e., the downstream side of the back pressure gradient section), so as to control the difference between the static pressure of the separation point and the static pressure of the reattachment point below a reference value.

Description

Method for manufacturing glass plate and manufacturing device for glass plate

The present invention relates to a method for producing a glass sheet and a device for producing a glass sheet.

Previously, in the manufacture of glass sheets, the operation of forming glass sheets using an overflow flow down draw method was performed. In the overflow down-draw method, the glass raw material is melted in a melting tank to prepare molten glass, and the molten glass is subjected to a clarification treatment and a homogenization treatment, and then the molten glass is supplied to the elongated molded body through a transfer pipe. In the elongated molded body, a groove portion extending in the longitudinal direction is provided on the upper portion of the molded body, and molten glass is supplied to one end of the groove portion. The groove portion advances toward the opposite side in the longitudinal direction from the supply side of the molten glass, and the depth of the groove becomes shallower. Therefore, the molten glass overflows from the groove portion of the molded body, and flows downward along the side walls on both sides of the molded body. . The molten glass which flows down the side wall of the both sides of the molded body merges at the lower end of the molded body, and is bonded together to form a glass plate (glass piece).

However, the cross-sectional shape of the flow path of the transfer pipe that supplies the molten glass to the molded body is generally circular, and the cross-sectional shape of the flow path of the groove portion of the molded body is a rectangular shape or a polygonal shape. The cross-sectional shape of the flow path of the transfer pipe is such that the molten pipe is filled with a high-temperature molten glass, and there is no bent portion, and it is preferable to maintain the strength. On the other hand, the cross-sectional shape of the flow path of the molded body groove portion is a rectangular shape or a polygonal shape in order to improve the ease of processing the groove portion. For example, in FIGS. 1 and 3 of Patent Document 1, a molded body having a circular cross-sectional shape of a flow path and a groove having a rectangular cross-sectional shape in a flow path is disclosed. In this case, the molten glass is supplied to the groove of the formed body from the circular shaped conveying pipe. In the case of the glass, the flow path of the molten glass has a step difference and is rapidly expanded.

[Previous Technical Literature] [Patent Literature]

[Patent Document 1] Japanese Patent Laid-Open Publication No. 2008-501609

As described above, in general, the cross-sectional shape of the flow path of the transfer tube that supplies the molten glass to the molded body is a circular shape, and the cross-sectional shape of the flow path of the groove portion of the molded body is a rectangular or polygonal shape, so that it is from the transfer pipe to the molded body. When the molten glass is supplied to the groove portion, the flow path of the molten glass has a stepped portion and is rapidly expanded. Therefore, there is a case where the flow of the molten glass is rapidly increased, and the flow of the molten glass is likely to locally stay (stagnate) in the groove portion of the molded body. The residence of the molten glass flow is liable to cause devitrification of the molten glass. Moreover, the residence of the molten glass flow tends to cause textures of different properties (melting glasses of different properties), and it is also liable to cause streaks. More specifically, after the flow of the molten glass stays, the time of contact with the molded body is longer than that of the molten glass in other portions, so that it is easy to melt the components of the molded body from the surface of the molded body, resulting in molten glass. The composition of the glass changes locally. Further, it is easily affected by the temperature of the molded body, and the viscosity of the molten glass is locally changed. That is, in the molten glass, textures of different properties (melted glass of different properties) are easily generated, and as a result, streaks are easily generated in the glass plate of the final product, and the thickness of the glass plate tends to become uneven.

Further, a glass plate for a flat panel display is formed of a semiconductor element such as a TFT (Thin Film Transistor) on a glass plate. In recent years, in order to achieve further high definition of the display, it is required to replace the previously used α-Si (amorphous silicon). TFT, forming p-Si (low temperature polysilicon) on the glass plate. TFT or oxide semiconductor. At p-Si. In the formation step of the TFT or the oxide semiconductor, there is more α-Si. The step of forming the TFT is a heat treatment step of a higher temperature. Therefore, it is required to form p-Si (low The polystyrene) glass plate of a TFT or an oxide semiconductor has a small heat shrinkage rate. In order to reduce the heat shrinkage rate, it is preferable to increase the strain point of the glass, but the glass having a high strain point tends to have a higher liquidus temperature, and the liquidus viscosity (viscosity in the liquidus temperature) tends to be lower. Therefore, there is also a case where the difference between the viscosity (forming viscosity) of the molten glass required for the formation of the glass plate (glass piece) and the liquid phase viscosity is small, or the forming viscosity is larger than the liquid phase viscosity, and as a result, the glass is easily devitrified. Therefore, when using p-Si (low temperature polysilicon). In the case of forming a glass sheet for forming a TFT or an oxide semiconductor, in particular, a glass having a low liquid phase viscosity, it is necessary to avoid the following situation: the composition of the molded body is melted on the surface of the molded body, and the viscosity of the liquid phase rises (loss occurs) In the groove portion of the molded body which is dangerous, the flow of a part of the molten glass is liable to stay.

Therefore, in order to solve the problems of the prior art, an object of the present invention is to provide a method for producing a glass sheet and a method for producing a glass sheet, which is a method for producing a glass sheet by molding a molten glass using a molded body. The flow of the molten glass is difficult to stay, and the molten glass does not cause devitrification and molten glass of different properties, so that a glass plate of high quality without streaks and uniform thickness can be produced.

An aspect of the present invention is characterized in that it is a glass plate manufacturing method for producing a glass plate by flowing molten glass to a molded body, and includes: a melting step of melting the glass raw material to produce molten glass; and a supply step of passing a conveying pipe that supplies the molten glass to the molded body; and a molding step of forming the glass plate from the molten glass by a down-draw method while flowing the molten glass to the groove portion of the molded body; and in the supplying step, When the molten glass is supplied to the groove portion of the molded body from the transfer pipe, the static pressure downstream is specified to be higher than the upstream reverse pressure gradient interval, and the upstream end from the back pressure gradient interval is the peeling point to the reverse Pressure gradient interval In the range from the downstream end, that is, the reattachment point, the molten glass is heated, and the difference between the static pressure at the peeling point and the static pressure at the reattachment point is controlled to be equal to or less than a reference value.

Preferably, the above reference value is 500 Pa.

Preferably, the viscosity of the molten glass from the peeling point to the reattachment point is 5450 Pa. s below.

Preferably, the distance from the peeling point to the reattachment point is 100 mm or less.

Another aspect of the present invention is characterized in that it is a glass plate manufacturing apparatus for producing a glass plate by flowing molten glass to a molded body, and includes: a melting device that melts the glass raw material to produce molten glass; and a conveying pipe The molten glass is passed through and supplied to the molded body; the heating device heats the transfer pipe to heat the molten glass flowing through the transfer pipe; the measuring device measures the pressure in the transfer pipe; and the molding device Forming the glass sheet from the molten glass by a down-draw method while flowing the molten glass to the groove portion of the molded body; and the measuring device specifies a static pressure downstream of the transfer tube that is higher than an upstream reverse pressure gradient interval. The heating device heats the molten glass in a range from the upstream end of the back pressure gradient section, that is, the peeling point to the downstream end of the back pressure gradient section, that is, the reattachment point, and controls the back pressure gradient below the reference value. .

According to the present invention, when the molten glass is formed by using the molded body, the flow of the molten glass passing through the groove portion of the molded body is hard to stay, and the molten glass does not cause devitrification and molten glass of different properties, thereby making it possible to produce no streaks and uniformity. A high quality glass plate with a thick plate.

100‧‧‧melting device

101‧‧‧melting tank

101d‧‧‧ bucket

102‧‧‧Clarification tank

103‧‧‧Stirring tank

103a‧‧‧Agitator

104, 105, 106‧‧‧ glass supply tube

106a‧‧‧Glass supply pipe body

106b‧‧‧ Tube Expansion Department

107b‧‧‧ bottom

108b‧‧‧ top

200‧‧‧Forming device

210‧‧‧Formed body

210a‧‧‧Slots

210b‧‧‧ sidewall

210c‧‧‧ bottom front

210d‧‧‧ bottom

210e‧‧‧ slot slope

211a‧‧‧Top counterpart

212‧‧‧ heating device

220‧‧‧ streamline

221‧‧ ‧ peeling point

222‧‧‧Reattachment point

300‧‧‧ cutting device

MG‧‧‧ molten glass

SG‧‧ ‧ glass piece

W1‧‧‧Width

W2‧‧‧Width

W3‧‧‧Width

W4‧‧‧Width

Z1‧‧‧Connected area

Fig. 1 is a view showing an example of a procedure of a method for producing a glass sheet of the embodiment.

Fig. 2 is a view schematically showing an example of a device for performing a melting step to a cutting step in the embodiment.

Fig. 3 (a) is an exploded perspective view showing a connecting portion between the molded body and the glass supply pipe in the embodiment, and (b) is a view showing a connection between the connecting portion and the groove portion when the pipe expanding portion of the embodiment is connected to the groove portion. A diagram of the relative position.

FIG. 4 is a view for explaining the flow of the molten glass when the vicinity of the connection position of the glass supply tube and the molded body in the present embodiment is viewed from above.

FIG. 5 is a view for explaining the flow of the molten glass when the vicinity of the connection position of the glass supply tube and the molded body in the present embodiment is viewed from the side.

Fig. 6 is a view schematically showing a flow line of molten glass.

Fig. 7 (a) and (b) are views for explaining the previous connection state between the groove portion of the molded body and the glass supply tube.

Hereinafter, a method of producing a glass sheet of the present embodiment and a manufacturing apparatus for a glass sheet will be described. Fig. 1 is a view showing an example of a procedure of a method for producing a glass sheet of the embodiment.

(Overall summary of the manufacturing method of glass plate)

The manufacturing method of the glass plate mainly has a melting step (ST1), a clarification step (ST2), a homogenization step (ST3), a supply step (ST4), a molding step (ST5), a slow cooling step (ST6), and a cutting step (ST7). ). Further, there are a grinding step, a polishing step, a washing step, an inspection step, a packing step, and the like, and a plurality of laminated glass sheets stacked in the packing step are conveyed to a customer.

The melting step (ST1) is carried out in a melting tank. In the melting tank, the molten glass is produced by charging the glass raw material into the liquid surface of the molten glass stored in the melting tank and heating it. Further, the molten glass is caused to flow from the outlet provided on one of the inner side walls of the inner side wall of the melting tank toward the downstream step.

In addition to the method in which the molten glass of the melting tank is heated by the heat generated by the molten glass itself, the flame of the burner can be additionally supplied to melt the glass raw material. Further, a clarifying agent is added to the glass raw material. As the clarifying agent, SnO ₂ , As ₂ O ₃ , Sb ₂ O ₃ and the like are known, but are not particularly limited. However, SnO ₂ (tin oxide) can be used as a fining agent in terms of reducing environmental load.

The clarification step (ST2) is carried out at least in the clarification tank. In the clarification step, by heating the molten glass in the clarification tank, the bubble containing O ₂ , CO ₂ or SO ₂ contained in the molten glass absorbs O ₂ generated by the reduction reaction of the clarifying agent, and then grows. It is released after reaching the liquid surface of the molten glass. Further, in the clarification step, the reducing substance obtained by the reduction reaction of the clarifying agent is subjected to an oxidation reaction by lowering the temperature of the molten glass. Thereby, the gas component such as O ₂ remaining in the bubble in the molten glass is reabsorbed into the molten glass, and the bubble disappears. The oxidation reaction and the reduction reaction of the clarifying agent are carried out by controlling the temperature of the molten glass. Further, the clarification step may also use a vacuum defoaming method in which a space for creating a reduced pressure atmosphere is created in the clarification tank, and the bubbles present in the molten glass are grown in a reduced pressure atmosphere to be defoamed. Further, in the clarification step, for example, a clarification method using tin oxide as a clarifying agent is used.

In the homogenization step (ST3), the molten glass in the stirring tank supplied through the piping extending from the clarification tank is stirred using a stirrer to homogenize the glass component. Thereby, the composition unevenness of the glass which is a cause of a stripe etc. can be reduced.

In the supply step (ST4), the molten glass is supplied to the molding apparatus through a pipe extending from the stirring tank.

In the molding apparatus, a forming step (ST5) and a slow cooling step (ST6) are performed.

In the molding step (ST5), the molten glass is formed into a glass piece (glass plate) to produce a flow of the glass piece. Forming uses an overflow down-draw method.

In the slow cooling step (ST6), the glass sheet which flows after molding has a desired thickness, and is further cooled so as not to cause warpage so as not to generate internal strain.

In the cutting step (ST7), the glass sheet supplied from the forming device is cut into a specific length by the cutting device to obtain a plate-shaped glass plate. The glass sheet obtained by cutting is further cut into a specific size to produce a glass sheet of a target size. Then, the end surface of the glass plate is ground and polished, and the glass plate is cleaned to further check for the presence or absence of abnormal defects such as bubbles or streaks, and then the glass plate of the inspected product is packaged as a final product.

Fig. 2 is a view schematically showing an example of a manufacturing apparatus of a glass sheet which performs a melting step (ST1) to a cutting step (ST7) in the embodiment. As shown in FIG. 2, the apparatus mainly has a melting device 100, a forming device 200, and a cutting device 300. The melting apparatus 100 has a melting tank 101, a clarification tank 102, a stirring tank 103, and glass supply pipes 104, 105, and 106.

In the melting apparatus 101 shown in FIG. 2, the input of the glass raw material is performed using the bucket 101d. In the clarification tank 102, the temperature of the molten glass MG is adjusted, and the clarification of the molten glass MG is performed by the oxidation-reduction reaction of a clarifier. Further, in the stirring tank 103, the molten glass MG is stirred by the agitator 103a to be homogenized. In the molding apparatus 200, the glass piece SG is formed from the molten glass MG by the overflow down-draw method using the molded object 210.

(connection of glass supply tube and formed body)

Fig. 3(a) is an exploded perspective view showing a portion where the molded body 210 and the glass supply pipe 106 are connected, and Fig. 3(b) is a view showing a connection region Z1 when the open end of the pipe expansion portion 106b is connected to the open end of the groove portion 210a. A map of the relative positions between the groove portions 210a.

The molded body 210 is formed as an elongated structure in which one of the groove portions 210a (the X direction in the drawing) extends in the upper portion thereof. The groove portion 210a advances in the X direction and the depth of the groove becomes shallow. Therefore, the molten glass MG supplied to the groove portion 210a overflows from the groove portion 210a, and flows from the side wall 210b provided on both sides of the molded body 210 vertically downward. The molten glass MG which flows down from the side wall 210b of the both sides is merged in the lower front end 210c provided in the vertical direction below the molded object 210, and is bonded together, and becomes a glass piece (glass plate) SG. The molten glass MG is smoothly supplied (the flow of the molten glass MG is hard to stay (stagnate)) to the groove portion 210a of the molded body 210, and this The case is preferably in the absence of devitrification or streaking. In particular, if the liquidus temperature is high, the viscosity of the liquid phase is close to the viscosity of the molten glass at the forming step (forming viscosity), or the glass having a liquid phase viscosity smaller than the forming viscosity is easily devitrified, it is necessary to avoid supplying the glass supply tube 106 to the groove portion 210a. The flow of the molten glass MG stays.

The flow path of the groove portion 210a of the molded body 210 has a rectangular cross section. On the other hand, the glass supply pipe 106 connected to the groove portion 210a of the molded body 210 is a transfer pipe, and includes a glass supply pipe main body 106a having a certain flow path cross section, and a pipe expansion portion 106b including a glass supply pipe. The cross section of the flow path of the main body 106a is gradually expanded to have a tapered shape. One end of the tube expansion portion 106b is connected to the glass supply tube main body 106a, and the other end of the tube expansion portion 106b is connected to the open end of the groove portion 210a. The cross section of the flow path of the glass supply tube main body 106a has a circular shape, and the cross section of the flow path of the tube expansion portion 106b is gradually changed from a circular shape to a rectangular shape. Further, the cross-sectional shape of the flow path of the glass supply pipe main body 106a, that is, the diameter of the circle is smaller than the groove width of the groove portion 210a. When the glass supply pipe main body 106a supplies the molten glass MG to the groove portion 210a of the molded body 210 through the pipe expansion portion 106b, the cross-sectional width and the width (cross-sectional area) of the cross section of the flow path of the molten glass MG flowing through the glass supply pipe 106 are obtained. As the position close to the opening end of the glass supply tube 106 and the opening end of the groove portion 210a of the molded body 210 is gradually expanded, the groove width of the groove portion 210a becomes the connection position. Further, at the connection position, the edge of the open end of the glass supply tube 106 has a shape conforming to the edge shape of at least the bottom surface of the open end of the groove portion 210a (the linear shape in Fig. 3(a)), and the glass supply tube The wall surface of the 106 (tube expansion portion 106b) is connected to the bottom surface of the groove portion 210a without a step. Here, the horizontal width of the cross section of the flow path of the molten glass MG means the width in the groove width direction of the groove portion 210a, and the vertical width of the cross section of the flow path of the molten glass MG means the vertical direction of the molten glass MG overflowing from the groove portion 210a. The width in the direction.

Specifically, the tube expansion portion 106b has a circular cross-sectional shape at the end of the tube expansion portion 106b connected to the glass supply tube main body 106a, and the bottom surface 107b of the tube expansion portion 106b is at the same position as the bottom of the glass supply tube main body 106a. (Same height), the bottoms are connected to each other without a step. The flow path section of the tube expansion portion 106b changes from a circular shape to a rectangular shape, but this The rectangular shape at the time is at the top opposite to the bottom, and the lateral width and the longitudinal width are widened as approaching the groove portion 210a. Therefore, the space of the tube expansion portion 106b including the upper portion of the top portion 108b is widened. In other words, the cross-sectional shape of the tube-expanding portion 106b is changed from the cross-sectional shape of the circular flow path of the glass supply tube main body 106a, and one of the cross-sectional shapes thereof is changed to a shape conforming to the edge shape of the bottom surface of the groove portion 210a. Here, in the example shown in FIG. 3(b), the edge shape of the bottom surface of the groove portion 210a is linear, and the cross-sectional shape of the tube expansion portion 106b is linear at the end portion connected to the groove portion 210a. In addition, the bottom surface of the groove portion 210a includes a portion extending in the depth direction with a certain groove width, in addition to a portion corresponding to the plane of the groove bottom when the cross-sectional shape of the groove portion 210a is a rectangular shape, The groove width is narrowed stepwise or continuously, and the surface of the groove ends.

Further, the cross-sectional shape of the opening end of the tube-expanding portion 106b connected to the groove portion 210a has a shape that coincides with one of the edge shapes (linear shapes) of the side surface (side wall surface) of the opening end of the groove portion 210a.

Further, the change in the width or the cross-sectional area of the cross section of the flow path of the molten glass MG in the glass supply pipe 106 may be continuously or stepwise, but the continuous width or the cross-sectional area is changed so that the flow of the molten glass MG is as large as possible. It is better in terms of not staying.

In addition, the connection between the groove portion 210a of the molded body 210 and the glass supply tube 106 (tube expansion portion 106b) includes, for example, the contents described in Japanese Laid-Open Patent Publication No. 2013-234107, and the contents are incorporated herein by reference.

As described above, when the tube expansion portion 106b is connected to the groove portion 210a, the tube expansion portion 106b has the same width as the groove width of the groove portion 210a and is connected to the groove portion 210a. As shown in Fig. 3 (b), the tube expansion portion 106b is provided so that the edge of the open end of the tube expansion portion 106b coincides with the edge of the groove portion of the groove portion 210a including the bottom surface. As a result, the molten glass MG that has flowed into the groove portion 210a from the tube expansion portion 106b smoothly flows into the groove 210a from the tube expansion portion 106b, so that the flow of the molten glass MG is hard to stay. When there is no tube expansion portion 106b, when the glass supply tube main body 106a enters the groove portion 210a, the flow path cross section is rapidly enlarged, so that there is a flow of the molten glass MG. The situation of staying. In this case, the molten glass MG is particularly liable to stay at the bottom and the top, and is liable to be a cause of devitrification and a texture of a different nature (a molten glass of a different nature). Therefore, the tube expansion portion 106b is provided so that the edge of the opening portion of the glass supply tube 106, that is, the portion of the tube expansion portion 106b that is connected to the groove portion 210a coincides with the shape of the edge of the groove portion 210a including the bottom portion of the groove bottom portion.

Further, as shown in Fig. 3(b), in the groove portion 210a of the molded body 210, the molten glass MG is supplied from the lower portion of the groove including the bottom surface of the groove portion 210a, and the groove portion 210a is located at the lower portion of the groove at the connection position. The upper portion of the groove above is blocked by a plate member as shown in Fig. 3(a). Therefore, the molten glass MG is supplied from the lower portion of the groove of the groove portion 210a, and the molten glass MG flows smoothly without stopping on the bottom surface, so that the molten glass MG smoothly overflows from the groove portion 210a.

FIG. 4 is a view for explaining the flow of the molten glass MG when the glass supply tube main body 106a, the tube expansion portion 106b, and the connection position of the molded body 210 are observed from above. As shown in FIG. 4, when the molten glass MG is supplied from the glass supply pipe 106 to the molded body 210, the width of the cross section of the flow path of the molten glass MG flowing through the glass supply pipe 106 expands as it approaches the molded body 210. The width of the flow path cross section of the tube expansion portion 106b gradually expands from the width W1 of the flow path cross section of the glass supply tube main body 106a to the width W2 of the flow path cross section of the groove portion 210a of the molded body 210. Here, the portion where the lateral width and the vertical width of the cross section of the flow path of the tube expansion portion 106b are connected to the glass supply tube main body 106a and the groove portion 210a, that is, the top portion 108b of the glass supply tube main body 106a and the tube expansion portion 106b The flow of the molten glass MG is likely to stay on the joint portion of the joint portion, the tube expansion portion 106b, and the top corresponding portion 211a (see FIG. 5) of the groove portion 210a corresponding to the height of the top portion 108. The flow rate of the molten glass MG is the fastest in the vicinity of the center of the glass supply pipe 106 in the diameter direction, and is slowed near the outer periphery of the glass supply pipe 106, for example, near the top and near the bottom. When the cross section of the flow path of the glass supply pipe 106 is rapidly expanded, the flow velocity of the molten glass MG flowing after the cross section of the flow path is rapidly expanded is compared with that before the expansion, and the flow rate is lowered rapidly. If the width of the flow path section (pipeline, cross-sectional area) is rapidly enlarged, the influence of the inertia of the fluid is more strongly affected than the viscosity of the fluid, and the flow velocity is fast on the upstream extension line, but after moving away from the above, the flow rate Slower, it is easy to produce a flow stop. Here, the inertia of a fluid refers to the property of maintaining the velocity (speed, flow direction) of the previous flow, and the viscosity of the fluid refers to the property that the above property is caused by the pressure loss of the viscous stress, and the fluid is required The pressure loss is reduced, the velocity gradient is reduced, and as a result the flow expands into a cross section that fills the pipeline. If the pipe is slowly expanded, the viscosity of the fluid is greater than the inertia of the fluid, and the flow is expanded to fill the cross section of the pipe, which is less likely to cause fouling. In particular, in the supply step (ST4) of lowering the temperature of the molten glass MG, if the flow rate of the molten glass MG is slow, the sensible heat of the molten glass MG from the upstream in the above portion is lowered, and the temperature is lowered. After the temperature is lowered, the viscosity of the molten glass MG rises, so that the flow rate is further lowered. In order to prevent this vicious cycle, it is important to pay attention to the piping design and not to form a silt point with a slow flow rate. When a flow rate or a fouling occurs in the vicinity of the flow rate of the molten glass MG, deformation, thickness variation, streaks, and the like are caused in the glass piece (glass plate) formed by the molded body 210. For example, SiO _{2 is} light and easily stays on the upper portion of the glass supply tube 106, while ZrO _{2 is} heavy and easily stays at the lower portion (bottom portion) of the glass supply tube 106. In the glass supply tube 106, unevenness of such components is generated in the molten glass MG, which becomes a cause of streaks. In order to prevent a sudden change in the cross section of the flow path in the glass supply pipe 106, for example, the width ratio W2/W1, W4/W3 is preferably 1.1 to 2, more preferably 1.2 to 1.8. Thereby, the retention of the molten glass MG is suppressed, and it flows smoothly to the groove part 210a of the molded object 210. Further, the length of the tube expansion portion 106b can be arbitrarily changed according to the ratio of the width, and is, for example, preferably 0.1 m to 2 m, and more preferably 0.1 m to 1 m.

FIG. 5 is a view for explaining the flow of the molten glass MG when the glass supply tube main body 106a, the tube expansion portion 106b, and the connection position of the molded body 210 are viewed from the side. As shown in Fig. 5, the glass supply tube main body 106a, the tube expansion portion 106b, and the bottom surface of the molded body 210 are at the same position (same height), and the bottom surfaces are connected without a step difference, so that it is difficult to cause the stay of the molten glass MG. On the other hand, in the glass supply tube main body 106a and the tube expansion portion 106b At the joint portion of the top portion 108b, the longitudinal width of the cross section of the flow path is expanded, so that the flow of the molten glass MG is likely to stay. Therefore, at the joint portion of the top portion 108b, it is necessary to prevent the staying even when the longitudinal width of the cross section of the flow path is expanded. In the present embodiment, the longitudinal width of the cross section of the flow path of the tube expansion portion 106b is gradually expanded from the width W3 to the width W4. Further, in the present embodiment, the heating device 212 is provided between the peeling point and the reattachment point. The peeling point and the reattachment point are described below. The heating device 212 includes, for example, a sheath heater, a cylindrical heater, and a ceramic heater that generate heat by resistance heating, dielectric heating, and microwave heating, and suppresses the stay of the molten glass MG by heating the molten glass MG. The installation position of the heating device 212 can be any position as long as it can heat the molten glass MG flowing through the peeling point and the reattachment point. Further, the molten glass MG flowing through the peeling point and the reattaching point may be heated by electric heating.

(heating of molten glass)

The stay of the flow of the molten glass MG is caused by the expansion of the cross section of the flow path, but the temperature of the molten glass MG near the periphery (for example, the top and the bottom) in the diameter direction of the glass supply tube 106 which is likely to stay is higher than that of the glass supply. When the temperature of the molten glass MG near the center of the pipe 106 in the diameter direction is lower than a certain level (the temperature difference is constant or more), the stay is likely to occur. The temperature of the molten glass MG is related to the viscosity of the molten glass MG. When the temperature difference of the molten glass MG is constant or more, that is, when the pressure difference of the molten glass MG is constant or more, the stay may occur. In the case where the pressure gradient is lowered from the upstream to the downstream in the glass supply pipe 106, no stay occurs, and when the pressure gradient is increased from the upstream to the downstream, a stop may occur. The position at which the molten glass MG is the back pressure gradient, that is, the position at which the stay may occur can be judged based on the flow line of the molten glass MG. Fig. 6 is a view schematically showing a flow line 220 of the molten glass MG. In the vicinity of the joint portion between the glass supply pipe main body 106a in which the flow path is enlarged and the top portion 108b of the pipe expansion portion 106b, and the vicinity of the joint portion between the pipe expansion portion 106b and the top corresponding portion 211a of the groove portion 210a, the staying of the molten glass MG and the fouling are likely to occur. Especially as As shown in FIG. 6, there is a high possibility that it is generated between the vicinity of the peeling point 221 (near) and the vicinity of the reattachment point 222 (near side). Here, the separation point refers to a point at which the flow line 220 of the molten glass MG is away from the surface of the object (the glass supply tube main body 106a and the tube expansion portion 106b), and means that the static pressure downstream is higher than the upstream side of the upstream reverse pressure gradient section. End point. In addition, the point of re-adhesion refers to the point along the surface of the object (the glass supply tube main body 106a and the tube expansion part 106b) after the separation point (downstream), and the flow line 220 of the molten glass MG is again referred to as the back pressure gradient section. The downstream side endpoint. Further, the static pressure refers to the pressure of the fluid that is stationary with respect to the pressure of the dynamic pressure formed by the flow of the fluid. In addition, the flow line 220 of the molten glass MG is a curve (group) in which the velocity vector of the molten glass MG is tangent, and shows the flow of the molten glass MG. Further, the vicinity (near side) means a range of 30 cm from the position of the object (peeling point 221 and reattachment point 222). In the vicinity of the peeling point 221, the molten glass MG flows in a direction away from the inner wall surface of the glass supply tube 106 (the glass supply tube main body 106a and the tube expansion portion 106b). Therefore, in the vicinity of the peeling point 221, the pressure is lower than the other portions (for example, the center portion of the glass supply tube 106 in the diameter direction, the bottom surface 107 of the glass supply tube 106, and the like), and is in a negative pressure state. On the other hand, in the vicinity of the reattachment point 222, the pressure is higher than the other portions and is in a positive pressure state. Here, according to the molecular motion theory, the viscosity (viscosity) is related to the pressure. When the pressure is high (positive pressure state), the viscosity becomes high, and in a state where the pressure is low (negative pressure state), the viscosity becomes low. In the portion where such a pressure difference exists, in other words, the portion where the viscosity is poor, and in other words, the portion where the temperature difference occurs, the stay of the molten glass MG and the fouling are likely to occur. Therefore, in the present embodiment, the molten glass MG is heated by the heating device 212 in the range from the vicinity of the peeling point 221 to the vicinity of the reattachment point 222, thereby reducing the vicinity of the peeling point 221 to the vicinity of the reattachment point 222. The temperature difference of the molten glass MG. By lowering the temperature difference, the difference in viscosity and the pressure difference (reverse pressure gradient) are also eliminated, thereby suppressing the occurrence of sticking and fouling of the molten glass MG.

The position of the peeling point 221 and the reattachment point 222 includes a plurality of thermometers, a liquid level meter, a flow rate meter, and a pressure gauge in the glass supply tube 106 (the glass supply tube main body 106a and the tube expansion unit 106b) (not shown). ) can be specified. For example, the temperature of the molten glass MG and the liquid level are measured, and the measured temperature and liquid level data are used to simulate the specific pressure gradient interval. In this simulation, the shape of the flow path of the molten glass MG is modeled on a computer (specific device), and the fluid region is divided into a plurality of (for example, about 1 million) lattices. Physical property values and boundary conditions are set for simulation. Here, in order to calculate the pressure loss, the density (kg/m ³ ) and the viscosity (Pa.s) of the molten glass MG are set as physical property values. Further, as a boundary condition, an inlet, a wall, and an outlet are set. The inlet is, for example, upstream of the tube expansion 106b, setting the inlet boundary. Then, the mass flow rate (kg/s) of the molten glass MG or the inlet flow rate (m/s) of the molten glass MG is given. Since the wall which becomes the interface between the molten glass MG and the wall surface of the groove part 210a of the molded object 210 is a fixed wall, it is set as the adhesive condition (The boundary flow velocity is zero), and becomes the space surface of the molten glass MG and the groove part 210a of the molded object 210. The wall of the interface (the void surface) is a free liquid surface, so it is set as a sliding condition (the shear stress parallel to the wall is zero). The outlet is at an appropriate position after the molten glass MG overflows (overflows) from the groove portion 210a, and the outlet boundary is set to be an isostatic surface condition. Then, each grid is given an initial value with respect to the flow rate, and the update of the flow rate value is repeated by a repeated calculation (for example, a simple algorithm), thereby obtaining an approximate solution close to the exact solution.

Further, the top portion 108b of the tube expansion portion 106b includes a plurality of thermometers and a flow rate meter from upstream to downstream, and the flow velocity distribution is obtained from the actually measured temperature and flow rate, whereby the top portion 108b of the tube expansion portion 106b can also be obtained. Pressure and pressure gradient on the inner wall surface. Thereby, the specific downstream static pressure is higher than the upstream reverse pressure gradient interval. The peeling point 221 is a position on the upstream side of the back pressure gradient section, and is a position where the pressure in the back pressure gradient section is relatively low. The reattachment point 222 is a position on the downstream side of the back pressure gradient section, and is a position where the pressure is relatively high in the back pressure gradient section. Further, as described above, since the pressure in the glass supply pipe 106, the viscosity of the molten glass MG, and the temperature of the molten glass MG are correlated, it is also possible to measure the viscosity of the molten glass MG or the temperature of the molten glass MG. The position of the peeling point 221 and the reattachment point 222 is obtained.

The heating device 212 controls the difference between the static pressure in the vicinity of the peeling point 221 and the static pressure in the vicinity of the reattachment point 222 (reverse pressure gradient) to be equal to or lower than the reference value. Here, the reference value is, for example, 500 Pa, and even if it is a back pressure gradient, it is a value which does not block the molten glass MG. It is no accident that the back pressure gradient of more than 500 Pa exceeds the calculated degree of error. By the non-accidental back pressure gradient, the molten glass MG is caused to flow twice from the reattachment point 222 toward the peeling point 221. Therefore, the molten glass MG which has not flowed smoothly due to a slight fluctuation in the flow rate or the like circulates in the fouling region due to the secondary flow, and it is difficult to escape from the fouling region. Therefore, major quality defects such as devitrification may occur. In order to control the back pressure gradient, the amount of heat applied by the heating device 212 varies depending on the thermal conductivity of the glass supply pipe 106, the amount of the molten glass MG, the composition of the molten glass MG, the distance from the heating device 212 to the molten glass MG, and the like. Therefore, the heating device 212 measures the measurement result obtained based on a viscometer (not shown), appropriately heats the molten glass MG, and controls the back pressure gradient to be equal to or lower than the reference value. By reducing the back pressure gradient (pressure difference) from the vicinity of the peeling point 221 to the vicinity of the reattachment point 222, the occurrence of sticking and fouling of the molten glass MG can be suppressed.

The temperature of the molten glass MG is gradually lowered toward the downstream in order to approach the temperature suitable for forming in the formed body 210. In the stage before the molten glass MG overflows from the groove portion 210a of the molded body 210, the liquid surface (surface) temperature of the molten glass MG in the groove portion 210a is the lowest. That is, in the flow path cross section of the inlet of the groove portion 210a of the molded body 210 shown in Fig. 5, the temperature of the molten glass MG in the vicinity of the joint portion between the tube expansion portion 106b and the top corresponding portion 211a of the groove portion 210a is the lowest. Therefore, it is necessary to prevent the temperature at the liquid surface (surface) of the molten glass MG in the groove portion 210a from being lowered in the vicinity of the joint portion of the top corresponding portion 211a, and it is necessary to suppress the sticking and the fouling. In the present embodiment, the heating device 212 is provided in the vicinity of the upper portion of the groove portion 210a, in the vicinity of the upper portion (upper surface) of the molded body 210, and particularly in the vicinity of the joint portion between the tube expansion portion 106b and the top corresponding portion 211a of the groove portion 210a. The temperature of the liquid surface of the molten glass MG in the groove portion 210a (the lowest temperature in the cross section of the flow path of the inlet portion of the groove portion 210a of the molded body 210) is suppressed, and the vicinity of the self-peeling point 221 to the vicinity of the reattachment point 222 is suppressed. Back pressure gradient control Made below the reference value. By heating the position where the temperature of the molten glass MG is lowered, that is, from the vicinity of the peeling point 221 to the vicinity of the reattachment point 222, it is possible to suppress the staying and fouling of the molten glass MG supplied to the groove portion 210a.

The heating amount and the set temperature of the molten glass MG which can suppress the stay of the molten glass MG and the fouling can be obtained by the following means. First, in the design stage of determining the structure of the glass supply pipe 106 (the glass supply pipe main body 106a and the pipe expansion part 106b), a fluid analysis simulation is performed, and the structure of the glass supply pipe 106 is designed such that the back pressure gradient is as small as possible. The structure of the area changes). In the fluid analysis simulation, for example, the pressure of the flow path is predicted (calculated) using the expected temperature of the molten glass MG. It is expected that the temperature is obtained by simultaneously desorbing the heat conduction and the flow of the molten glass. In order to simultaneously calculate the flow of the heat guide and the molten glass, glass, platinum, furnace air, and each refractory are used as analysis regions. Physical property values, generation conditions, and boundary conditions are set in order to perform analytical simulation. Here, as the physical property value, the density of the glass [kg/m ³ ], viscosity [Pa. s], specific heat [J/kg. K], thermal conductivity [W/m. K] and platinum, heating device 212 (heater), density of each refractory [kg / m ³ ], specific heat [J / kg. K], thermal conductivity [W/m. K]. Further, as a generation condition, the heat generation density [W/m ³ ] was set in the heat generating portion of the platinum or the heating device 212 (heater). Further, an inlet, a wall, and an outlet are set, and boundary conditions are given to the portion. The inlet is, for example, set the inlet boundary upstream of the tube expansion portion 106b. The inlet is, for example, set the inlet boundary upstream of the tube expansion portion 106b. Then, the mass flow rate (kg/s) of the molten glass MG or the inlet flow rate (m/s) of the molten glass MG and the inflow temperature (° C.) are given. Since the wall which becomes the interface between the molten glass MG and the wall surface of the groove part 210a of the molded object 210 is a fixed wall, it is set as the adhesive condition (The boundary flow velocity is zero), and becomes the space surface of the molten glass MG and the groove part 210a of the molded object 210. The wall of the interface (the void surface) is a free liquid surface, so it is set as a sliding condition (the shear stress parallel to the wall is zero). The outer wall of the refractory is set to have a heat dissipation condition such that the temperature becomes about 30 °C. Set the radiation boundary on the side of the glass or refractory that is in contact with air. The outlet is at an appropriate position after the molten glass MG overflows (overflows) from the groove portion 210a, and the outlet boundary is set to be an isostatic surface condition. The analytical pressure is calculated by setting these conditions, and the predicted pressure of the molten glass in the glass supply pipe 106 is calculated. However, since the back pressure gradient in the glass supply pipe 106, the peeling point caused by the back pressure gradient, and the pressure at the reattachment point depend on the temperature of the molten glass MG, the pressure of the actual glass sheet during molding (during operation) It may be deviated from the predicted pressure obtained by using fluid analysis simulation prediction. Therefore, the temperature of the molten glass MG obtained by the measurement of the actual glass sheet is measured, and the fluid analysis simulation is performed again to obtain the pressure difference in the counter pressure gradient section. Then, the target temperature and the amount of heating of the molten glass MG are determined by the temperature of the molten glass MG having a pressure difference of the obtained back pressure gradient section of the obtained back pressure gradient section of 500 Pa or less. In the heating device 212, the molten glass MG is heated so that the molten glass MG becomes a target temperature, whereby the staying and fouling of the molten glass MG can be suppressed.

Next, the stickiness of the molten glass MG without sticking and fouling will be described. As described above, in the flow path cross section of the inlet of the groove portion 210a of the molded body 210, the temperature of the molten glass MG is highest in the vicinity of the center of the tube expansion portion 106b in the diameter direction, and corresponds to the top of the groove portion 210a (the tube expansion portion 106b). The temperature of the molten glass MG near the connection portion of the portion 211a is the lowest. The temperature of the molten glass MG is related to the viscosity of the molten glass MG. In the cross section of the flow path at the inlet of the groove portion 210a of the molded body 210, the molten glass MG has the lowest viscosity near the highest temperature of the molten glass MG, and is melted. The glass MG becomes the lowest temperature and the viscosity of the molten glass MG is the highest. In the vicinity of the maximum viscosity of the molten glass MG, there is a risk of sticking or silting of the molten glass MG. Therefore, by controlling the maximum viscosity of the molten glass MG below the viscosity reference value, it is possible to suppress the stay or the like. In this embodiment, it is preferable to control the viscosity of the molten glass at the open end of the groove portion 210a of the molded body to 3300 Pa. s to 5450Pa. Within the scope of s. That is, it is preferable that the heating device 212 controls the maximum viscosity of the molten glass MG to a viscosity reference value of 5,450 Pa. Preferably, the heating device 212 controls the minimum viscosity of the molten glass MG to 3300 Pa. s above. Further, it is preferable to reduce the viscosity of the molten glass MG by heating the molten glass MG, thereby increasing the flow rate and the static pressure, and controlling the distance from the peeling point 221 to the reattachment point 222 to 100 mm or less. Heating device 212 The heat is changed in accordance with the thermal conductivity of the glass supply pipe 106, the amount of the molten glass MG, the distance from the heating device 212 to the molten glass MG, and the like. Therefore, the heating device 212 measures the measurement result obtained based on a viscometer (not shown) to control the maximum viscosity of the molten glass MG below the viscosity reference value. The heating device 212 can achieve the viscosity of the molten glass MG by appropriately heating the molten glass MG.

FIGS. 7(a) and 7(b) are views for explaining the previous connection state between the groove portion 210a of the molded body 210 and the glass supply tube 106. As shown in Figs. 7(a) and 7(b), the cross section of the flow path at the connection position of the glass supply pipe 106 is smaller than the cross section of the flow path of the groove portion 210a, so that the cross section of the flow path of the molten glass MG is rapidly expanded at the connection position. Therefore, as shown in FIG. 7(b), the flow of the molten glass MG having the velocity component is generated in the direction inclined with respect to the extending direction (X direction) of the groove portion 210a, and the molten glass MG is caused to be in the groove portion 210a. Does not flow smoothly in the X direction. In particular, since the bottom surface of the groove portion 210a is in step contact with the wall surface of the glass supply pipe 106, the flow of the molten glass MG flowing near the bottom surface is largely maintained.

As described above, in the present embodiment, the glass supply tube 106 includes the tube expansion portion 106b at its end portion. At this time, the width of the cross section of the flow path of the molten glass MG flowing through the glass supply pipe 106 gradually expands as it approaches the connection position between the open end of the glass supply pipe 106 and the open end of the groove portion 210a of the molded body 210. The position is the groove width of the groove portion 210a. Further, at the connection position, the edge of the open end of the glass supply tube 106 (tube expansion portion 106b) has a shape conforming to the shape of the edge of at least the bottom surface of the open end of the groove portion 210a of the molded body 210, and the glass supply tube 106 The wall surface is connected to the bottom surface of the groove portion 210a without a step. Further, at the connection position, more specifically, the heating device 212 is provided at a position facing the vicinity of the peeling point 221 from which the molten glass MG may stay to the vicinity of the reattachment point 222. Therefore, in the present embodiment, the molten glass MG can smoothly flow from the glass supply tube 106 to the groove portion 210a of the molded body 210, and the residence time of the molten glass MG in the groove portion 210a can be made relatively constant, and the molten glass can be melted. The glass MG overflows from the groove portion 210a. Therefore, it is difficult to produce a glass that is devitrified or has different properties, and can be made without streaks. A high quality glass plate with a uniform thickness.

In the present embodiment, as shown in FIGS. 3 to 6, the tube expansion portion 106b is used to supply the molten glass MG to the groove portion 210a of the molded body 210, but even FIG. 7(a) and FIG. In the previous connection state shown, the staying and fouling of the molten glass MG can be suppressed by providing the heating device 212 in the reverse pressure gradient interval. The previous connection state is more likely to stay in the molten glass MG than in the connection state using the pipe expansion portion 106b. Therefore, in the previous connection state, the back pressure gradient section, that is, the peeling point 221 and the reattachment point 222 are specified by providing a plurality of pressure gauges, and the molten glass MG is heated by the heating means 212 provided in the section, The staying and fouling of the molten glass MG can be effectively suppressed.

Here, a method of keeping the flow rate of the molten glass MG supplied to the groove portion 210a of the molded body 210 constant will be described. The previous connection state between the groove portion 210a of the molded body 210 shown in Figs. 7(a) and 7(b) and the glass supply pipe 106, and the use pipe expansion portion 106b shown in Figs. 3(a) and 3(b) In the state in which the groove portion 210a of the molded body 210 and the glass supply pipe 106 are connected to each other in the present embodiment, the flow rate of the molten glass MG at the time of reaching the groove portion 210a of the molded body 210 is compared. The pressure loss of the molten glass MG passing through the glass supply pipe main body 106a and the pipe expansion portion 106b is substituted into the Hagen-Pool Xiaoye formula by the flow rate of the molten glass, the viscosity coefficient of the molten glass, the tube radius of the glass supply pipe, and the like. Seek. Here, the pressure loss refers to an energy loss per unit time flow rate when a fluid passes through a pipe or the like, and if the pressure loss increases, the flow rate decreases, and if the pressure loss decreases, the flow rate increases. In the connected state in the present embodiment, since the pipe expansion portion 106b whose pipe diameter is gradually enlarged is used, the pressure loss is reduced as compared with the previous connection state. Since the pressure loss is reduced, the flow rate of the molten glass MG in the present embodiment is increased as compared with the prior art. In order to make the flow rate of the molten glass MG in the present embodiment the same as the flow rate of the molten glass MG (in order to keep it constant), it is necessary to increase the glass supply pipe 106 (the glass supply pipe main body 106a and the pipe expansion part in this embodiment). Pressure loss in 106b). As a method of increasing the pressure loss, for example, there is a method of increasing the flow rate of the molten glass MG, and a method of increasing the viscosity of the molten glass MG. Therefore, in the present embodiment, in order to increase the flow velocity of the molten glass MG flowing through the glass supply tube main body 106a of the molten glass MG to the tube expansion portion 106b, the diameter of the glass supply tube main body 106a is smaller than before, for example, 50~150mm. In addition, the temperature of the molten glass MG flowing through the tube expansion portion 106b from the glass supply tube main body 106a is lower than the previous one, and is lowered to, for example, 1150 ° C to 1300 ° C to increase the viscosity of the molten glass MG. By doing so, the pressure loss in the glass supply tube 106 (the glass supply tube main body 106a and the tube expansion portion 106b) can be increased, and the flow rate of the molten glass MG supplied to the groove portion 210a of the molded body 210 can be kept constant. In addition, the tube diameter of the glass supply tube main body 106a and the temperature of the molten glass MG flowing through the tube expansion portion 106b may be any value depending on the composition of the molten glass MG, the shape, length and width of the tube expansion portion 106b.

(Characteristics and application of glass plates)

In the case where the glass plate of the present embodiment is used for a glass plate for a flat panel display, a glass obtained by mixing glass raw materials so as to have the following glass composition is exemplified.

SiO ₂ : 50 to 70% by mass, Al ₂ O ₃ : 0 to 25% by mass, B ₂ O ₃ : 1 to 15% by mass, MgO: 0 to 10% by mass, CaO: 0 to 20% by mass, SrO: 0 to 20% by mass, BaO: 0 to 10% by mass, and RO: 5 to 30% by mass (wherein R is a combination of Mg, Ca, Sr, and Ba), and an alkali-free glass.

Further, in the present embodiment, although it is an alkali-free glass, the glass plate may be a glass containing a trace amount of an alkali metal and containing a small amount of alkali. In the case of containing an alkali metal, it is preferable to contain R0 ₂ O in a total amount of 0.10% by mass or more and 0.5% by mass or less, preferably 0.20% by mass or more and 0.5% by mass or less (wherein R' is At least one selected from the group consisting of Li, Na, and K is a substance contained in a glass plate. Of course, the total of R' ₂ O may also be less than 0.10% by mass.

Further, in the case of applying the method for producing a glass sheet of the present invention, the glass composition contains, in addition to the above respective components, SnO ₂ : 0.01 to 1% by mass (preferably 0.01 to 0.5% by mass), and Fe ₂ O ₃ : 0 to 0.2% by mass (preferably 0.01 to 0.08% by mass), the glass raw material may be prepared in such a manner that substantially no As ₂ O ₃ , Sb ₂ O _{3 or} PbO is contained in consideration of environmental load.

Moreover, in recent years, in order to achieve further high definition of the screen display of a flat panel display, it is required to use p-Si (low temperature polysilicon). TFT or oxide semiconductor display, not using α-Si (amorphous germanium). TFT display. Here, in the formation step of the p-Si (low temperature polysilicon) TFT or the oxide semiconductor, there is a more α-Si. The step of forming the TFT is a heat treatment step of a higher temperature. Therefore, it is required to form p-Si. The glass plate of the TFT or the oxide semiconductor has a small heat shrinkage rate. In order to reduce the heat shrinkage rate, it is preferable to increase the strain point, but the glass having a high strain point tends to have a higher liquidus temperature and a lower liquid phase viscosity as described above. That is, the liquid phase viscosity is close to the proper viscosity of the molten glass in the forming step. Therefore, in order to suppress devitrification, it is more strongly required that the flow of the molten glass MG does not stay in the groove portion 210a of the formed body 210. In the present embodiment, the flow of the molten glass MG is hard to stay. Therefore, the method for producing a glass plate of the present invention can also be applied to, for example, a glass plate using a glass having a strain point of 655 ° C or higher. In particular, the method for producing a glass sheet of the present invention can also be applied to use a suitable p-Si. A glass plate of a glass having a strain point of 655 ° C or higher, a strain point of 680 ° C or higher, and a strain point of 690 ° C or higher is hard to cause devitrification.

Moreover, the method for producing a glass plate of the present invention can also be applied to a liquid phase viscosity of 6000 Pa. The glass below s, and then the liquid viscosity is 5000Pa. The glass below s, especially the liquid viscosity is 4500Pa. The glass plate of the glass below s is difficult to devitrify.

The strain point is above 655 ° C or the liquid viscosity is 4500 Pa. When the glass below s is used for a glass plate, as a glass composition, for example, a glass plate package is expressed by mass%. Contains the composition of the following ingredients.

Preferably, it contains SiO ₂ : 52 to 78% by mass, Al ₂ O ₃ : 3 to 25% by mass, B ₂ O ₃ : 3 to 15% by mass, RO (wherein R is selected from the group consisting of Mg, Ca, Sr, and Ba) And all the components contained in the glass plate, at least one kind) 3 to 20% by mass, and the mass ratio (SiO ₂ +Al ₂ O ₃ )/B ₂ O _{3 is} in the range of 7 to 20, and the alkali-free glass or trace amount Alkali glass.

Further, in order to increase the strain point, the mass ratio (SiO ₂ + Al ₂ O ₃ )/RO is preferably 7.5 or more. Further, in order to increase the strain point, it is preferred to have a β-OH value of 0.1 to 0.3 mm ^-1 . Further, in order to achieve a high strain point and prevent a decrease in liquid phase viscosity, CaO/RO is preferably 0.65 or more. The glass raw material may be prepared in such a manner that it does not substantially contain As ₂ O ₃ , Sb ₂ O _{3 or} PbO in consideration of environmental load.

Further, in addition to the above-described components, the glass used in the glass plate of the present embodiment may contain various other oxides in order to adjust various physical, melting, clarifying, and forming properties of the glass. Examples of such other oxides are not limited to the following, and examples thereof include SnO ₂ , TiO ₂ , MnO, ZnO, Nb ₂ O ₅ , MoO ₃ , Ta ₂ O ₅ , WO ₃ , Y ₂ O ₃ , and La ₂ O ₃ . Here, since the glass plate for a flat panel display such as a liquid crystal display or an organic EL (Electroluminescence) display is particularly strict in terms of bubbles, it is preferable that at least SnO _{2 having a} large clarification effect is contained in the above oxide.

For the supply of the above RO, a nitrate or a carbonate can be used. Further, it is more preferable to use nitrate as a supply source of RO in order to increase the oxidizability of the molten glass at a ratio suitable for the step.

In the above, the method for producing the glass sheet of the present invention has been described in detail. However, the present invention is not limited to the above-described embodiments, and various modifications and changes can be made without departing from the spirit and scope of the invention.

[Examples]

Hereinafter, the present invention will be described in more detail by way of examples. Further, the present invention is not limited to the following embodiments.

(Example 1)

The position of the peeling point 221 and the position of the reattachment point 222 are specified by measuring the pressure in the tube expansion portion 106b. The temperature at which the flow rate of the molten glass MG at the inlet of the molded body 210 is 100 kg/lday, and the temperature of the molten glass MG flowing from the glass supply pipe main body 106a to the pipe expansion portion 106b is set to 1,235 °C. Further, a tube expansion portion 106b having a width ratio W2/W1, W4/W3 of 1.8 and a length of the tube expansion portion 106b of 0.5 m is provided between the glass supply tube main body 106a and the groove portion 210a. The top portion 108b of the tube expansion portion 106b is provided with a plurality of pressure gauges from upstream to downstream, and the pressure of the inner wall surface of the top portion 108b of the tube expansion portion 106b is measured by each pressure gauge. Then, a pressure position lower than the average value of the pressures measured by the respective pressure gauges is referred to as a peeling point 221, and a pressure position higher than the average value is referred to as a reattachment point 222. As a result, the peeling point 221 is a joint portion between the glass supply tube main body 106a and the top portion 108b of the tube expansion portion 106b, and the reattachment point 222 is located downstream from the peeling point 221 by 100 mm to 120 mm.

(Example 2)

The heating device 212 is provided in the range from the peeling point 221 specified in the first embodiment to the reattachment point 222, and the deformation, thickness variation, streaks, and the like of the glass sheet formed by the molded body 210 are confirmed. The heating amount of the molten glass MG was set to 3000 W. The other conditions were set in the same manner as in the first embodiment. The results of deformation, thickness deviation, and streaking of the glass sheet formed under these conditions are shown in Table 1.

As shown in Table 1, in the case of the above conditions, deformation, thickness deviation, and streaks which did not satisfy the required specifications were not produced in the formed glass sheet. According to the above results, it is understood that the cross section of the flow path from the glass supply pipe 106 toward the groove portion 210a is gradually expanded, and the molten glass is heated from the connection position of each pipe to the downstream position, whereby the molten glass can be prevented from staying in the glass supply pipe 106, It is fouled to prevent deformation, thickness deviation, and streaks.

(Example 3)

When the glass supply tube main body 106a is connected to the groove portion 210a without using the tube expansion portion 106b, and the heating device 212 is not provided, the deformation, thickness deviation, and streaks of the glass sheet formed by the molded body 210 are confirmed. And so on. Other conditions were set in the same manner as in the second embodiment. The results of deformation, thickness deviation, and streaking of the glass sheet formed under these conditions are shown in Table 2.

As shown in Table 2, in the case of the above conditions, it was confirmed that deformation, thickness deviation, and streaks were generated, and the required specifications were not satisfied. According to the above results, it is understood that when the cross section of the flow path from the glass supply pipe 106 toward the groove portion 210a is not gradually expanded, and the molten glass is not heated from the connection position of each pipe to the downstream position, the molten glass cannot be suppressed. The glass supply tube 106 stays and is fouled, thereby causing deformation, thickness deviation, and streaks.

(Example 4)

Investigation of the pressure, temperature, viscosity of the molten glass MG flowing through the glass supply pipe 106 and the groove portion 210a of the molded body 210, and the correlation with the deformation, thickness variation, and streaks generated in the glass plate formed by the molded body 210 . Under the conditions of Example 2 and the conditions of Example 3, the pressure at the peeling point 221 and the reattachment point 222, and the temperature and viscosity of the molten glass MG were measured. Pressure measurement using a pressure gauge, a temperature gauge, and a viscosity gauge Force, temperature and viscosity of molten glass MG. The measurement results of the pressure are shown in Table 3. Further, the measurement results of the temperature of the molten glass MG are shown in Table 4. Further, the measurement results of the viscosity of the molten glass MG are shown in Table 5.

As shown in Table 3, under the conditions of Example 2, the pressure difference (reverse pressure gradient) between the peeling point 221 and the reattachment point 222 was 450 Pa to 500 Pa, and under the conditions of Example 3, it was 600 Pa to 650 Pa. Since, as described above, in the second embodiment, the glass sheet is not deformed, the thickness deviation, and the stripe (satisfying the required specifications), in the third embodiment, the glass sheet is deformed or the like (not meeting the required specifications), so that it is known that When the pressure difference (reverse pressure gradient) between the peeling point 221 and the reattachment point 222 is 500 Pa or less, deformation or the like does not occur, and when it is at about 600 Pa, deformation or the like occurs.

Further, as shown in Table 4, the distance from the peeling point 221 to the reattachment point 222 was 80 mm to 100 mm under the conditions of Example 2, and was 140 mm to 160 mm under the conditions of Example 3. As described above, in the second embodiment, no deformation, thickness deviation, and streaking were generated, and the implementation was carried out. In Example 3, deformation, thickness deviation, and streaks were generated. Therefore, it is understood that if the distance from the peeling point 221 to the reattachment point 222 is 100 mm or less, the glass sheet does not have a variation in the thickness of the deformed sheet or the streaks. When the molten glass is heated, the viscosity of the molten glass is lowered, the flow rate is increased, and the static pressure at the peeling point and the reattachment point is changed. It is understood that if the pressure difference between the static pressure at the peeling point and the static pressure at the reattachment point becomes small, that is, the distance from the peeling point to the reattachment point is close, and the distance is 100 mm or less, the staying and fouling of the molten glass can be suppressed.

Further, as shown in Table 5, under the conditions of Example 2, the viscosity of the molten glass MG was 3,300 Pa. s~5450Pa. s, under the conditions of Example 3, the viscosity of the molten glass MG is 2750Pa. s~7350Pa. s. As described above, in the second embodiment, deformation, thickness deviation, and streaks were not generated, and in Example 3, deformation, thickness variation, and streaks were generated. Therefore, it is understood that the difference between the viscosity of the molten glass MG at the peeling point 221 and the viscosity of the molten glass MG at the reattachment point 222 is 5,450 Pa. Below s, the glass sheet is not deformed or the like.

According to the above results, it is understood that by controlling the back pressure gradient, distance, and viscosity from the peeling point to the reattachment point, the staying and fouling of the molten glass can be suppressed, thereby preventing deformation, thickness deviation, and streaking.

106a‧‧‧Glass supply pipe body

106b‧‧‧ Tube Expansion Department

108b‧‧‧ top

210‧‧‧Formed body

210a‧‧‧Slots

211a‧‧‧Top counterpart

212‧‧‧ heating device

W3‧‧‧Width

W4‧‧‧Width

Claims (5)

A method for producing a glass sheet, comprising: flowing a molten glass to a molded body to produce a glass sheet, and comprising: a melting step of melting the glass raw material to produce molten glass; and a supplying step of conveying the above by a conveying pipe a molten glass is supplied to the molded body; and a molding step of forming the glass sheet from the molten glass by a down-draw method while flowing the molten glass to a groove portion of the molded body; and in the supplying step, from the transporting When the tube supplies the molten glass to the groove portion of the molded body, the static pressure downstream is specified to be higher than the back pressure gradient portion of the molten glass upstream, and the peeling point from the upstream end of the back pressure gradient interval to the above In the range of the downstream side end of the back pressure gradient section, that is, the reattachment point, the molten glass is heated, and the difference between the static pressure of the peeling point and the static pressure of the reattachment point is controlled to be equal to or less than a reference value. A method of producing a glass sheet according to claim 1, wherein said reference value is 500 Pa. The method for producing a glass plate according to claim 1 or 2, wherein the viscosity of the molten glass from the peeling point to the reattachment point is 5450 Pa. s below. The method for producing a glass sheet according to any one of claims 1 to 3, wherein a distance from the peeling point to the reattachment point is 100 mm or less. A glass plate manufacturing apparatus characterized in that a molten glass is flowed to a molded body to produce a glass plate, and includes: a melting device that melts the glass raw material to produce molten glass; and a conveying pipe that passes the molten glass And supplying to the above shaped body; a heating device that heats the conveying pipe to heat the molten glass flowing through the conveying pipe; a specific device that specifies a pressure in the conveying pipe; and a forming device that flows the molten glass to the formed body on one side Forming the glass plate from the molten glass by a down-draw method on the groove portion; and the specific device is specified such that the static pressure in the downstream of the transfer pipe is higher than the reverse pressure gradient interval of the upstream molten glass, and the heating device is reversed from the above In the range from the upstream end of the pressure gradient section, that is, the peeling point to the downstream end of the back pressure gradient section, that is, the reattachment point, the molten glass is heated to control the back pressure gradient to be equal to or less than the reference value.