JPS5832030A - Electric melting furnace for glass - Google Patents
Electric melting furnace for glassInfo
- Publication number
- JPS5832030A JPS5832030A JP13047981A JP13047981A JPS5832030A JP S5832030 A JPS5832030 A JP S5832030A JP 13047981 A JP13047981 A JP 13047981A JP 13047981 A JP13047981 A JP 13047981A JP S5832030 A JPS5832030 A JP S5832030A
- Authority
- JP
- Japan
- Prior art keywords
- furnace
- electrodes
- glass
- molten glass
- phase
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Classifications
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B5/00—Melting in furnaces; Furnaces so far as specially adapted for glass manufacture
- C03B5/02—Melting in furnaces; Furnaces so far as specially adapted for glass manufacture in electric furnaces, e.g. by dielectric heating
- C03B5/027—Melting in furnaces; Furnaces so far as specially adapted for glass manufacture in electric furnaces, e.g. by dielectric heating by passing an electric current between electrodes immersed in the glass bath, i.e. by direct resistance heating
- C03B5/0275—Shaft furnaces
Landscapes
- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Electrochemistry (AREA)
- Engineering & Computer Science (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Resistance Heating (AREA)
- Glass Melting And Manufacturing (AREA)
- Furnace Details (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は溶融ガラス自体に直接通電し、そのジニール熱
によって原料ガラスバッチを溶融し、そして均質化及び
清澄化する縦型の電気溶融炉、さらに詳しくは方形の横
断面形状とそれに適合した特定の電極配置を持つそのよ
うな電気溶融炉に廚する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vertical electric melting furnace, more specifically a vertical electric melting furnace with a rectangular cross section, in which electricity is applied directly to the molten glass itself, and the raw glass batch is melted, homogenized and clarified by its Genieal heat. Applicable to such an electric melting furnace with a shape and a specific electrode arrangement adapted to it.
ガラス製品、例えばガラス繊維は工業的には一般に粉末
の原料ガラスバッチを耐火材料から構成される溶融平炉
において火炎によシ溶融、清澄化し、その溶融ガラスを
チャンネルを介して耐火材料よ構成るフォーハースに導
びき、コンディショニングを行いつつそのフォーハース
の底部に配設された複数の白金製ブッシングからその構
成白金材料の通電による抵抗発熱によって温度制御しつ
つ紡糸することによって製造される(例えば、特公昭ろ
9−5219号及び同46−64941号公報を参照)
。Glass products, such as glass fibers, are produced industrially by melting and clarifying a powdered raw glass batch by flame in an open hearth melting furnace made of a refractory material, and passing the molten glass through a channel into a melting furnace made of a refractory material. It is manufactured by spinning the platinum material from a plurality of platinum bushings arranged at the bottom of the forehearth while controlling the temperature by heating resistance by energizing the constituent platinum material while conditioning the material. (Refer to Koshoro No. 9-5219 and Koshoro No. 46-64941)
.
このような溶融平炉とフォーハースよ構成る溶融、清澄
、成形糸に対して、近年縦型の電気溶融炉が開発された
。この縦型電気溶融炉は電極を炉の比較的上部に適正に
配置し、炉内溶融ガラスに直接通電するとき、溶融ガラ
スに適当な縦方向の温度分布が生ずるとともに、そのと
き炉内上方の相対的に高温、低密度の溶融ガラスは下方
の相対的に低温、高密度の溶融ガラス領域には重力に逆
ってまでは混入し難いことから同一炉内の相対的に上方
においては溶融ガラスの加熱対流領域が、一方相対的に
下方においては溶融ガラスの層流清澄領域が形成される
という単純な原理に基づくものである。このように、電
気溶融炉はガラスバッチの溶融−攪拌−拡散を同一炉内
で自然に、かつ機能的に達成し、そして炉底近傍におい
て均質、清澄化された溶融ガラスを得るという従来の平
炉系には認められない溶融理論の明解さとプロセス上の
単純さを持ち、かくして装置の小型化と熱効率の向上を
達成している。電気エネルギーの使用はかつてその効率
を考慮に入れても化石燃料に比較して割高であったが、
電気溶融炉におけるプロセスの単純性、高効率性は近年
の化石燃料の高騰とあいまってその有利性を次第に高め
、新しいガラス溶融技術としてその地位を確立しつつあ
る。In recent years, a vertical electric melting furnace has been developed for melting, fining, and forming yarn, which consists of the open hearth and four-hearth melting furnaces. In this vertical electric melting furnace, the electrodes are appropriately placed relatively at the upper part of the furnace, and when electricity is applied directly to the molten glass in the furnace, an appropriate vertical temperature distribution is generated in the molten glass, and at the same time, the electrodes are placed in the upper part of the furnace. The relatively high temperature, low density molten glass is difficult to mix into the relatively low temperature, high density molten glass region below, even against the force of gravity. It is based on the simple principle that a region of heating convection is formed in the molten glass while a region of laminar flow of molten glass is formed relatively below. In this way, the electric melting furnace achieves melting, stirring, and diffusion of a glass batch naturally and functionally in the same furnace, and achieves homogeneous and clarified molten glass near the bottom of the furnace, compared to the conventional open hearth furnace. It has a clarity of melting theory and a simplicity of process that are not found in conventional systems, thus achieving miniaturization of equipment and improvement of thermal efficiency. The use of electrical energy used to be expensive compared to fossil fuels, even when efficiency was taken into account.
The simplicity and high efficiency of the electric melting furnace process, combined with the recent rise in the price of fossil fuels, has gradually increased its advantages, and it is establishing itself as a new glass melting technology.
このような電気溶融炉として、例えば特公昭52−26
884号公報は溶解タンクの上方部分内の少なくとも1
つの溶解帯域で少なくとも2つの複数レベルにおいて溶
融ガラスに通電することによって熱エネルギーを発生さ
せ、それによって前記複数レベルにおいて方向が相反す
る溶融ガラスの循環流を生成、維持する三相交流電極配
置を持つ電気溶融炉及び溶解方法を開示している。As such an electric melting furnace, for example, the
No. 884 discloses that at least one part of the upper part of the dissolution tank is
having a three-phase alternating current electrode arrangement for generating thermal energy by energizing the molten glass in at least two levels in one melting zone, thereby creating and maintaining a circulating flow of molten glass in opposing directions in the levels; An electric melting furnace and melting method are disclosed.
また、特開昭47−13618号公報は炉内複数平面に
電極群を持つガラス電気溶融炉において、1平面の電極
群の内端部をその上方及び下方の平面の電極群の端部間
の間隙に位置せしめ、かくして各下位平面の上昇ガラス
流を上位平面との境界面において各上位平面の下降ガラ
ス流と会合させ、各ガラス流が他方の平面内に浸入する
のを阻止する電気溶融炉と溶融方法を開示している。Japanese Patent Application Laid-open No. 47-13618 discloses that in a glass electric melting furnace having electrode groups on multiple planes in the furnace, the inner end of the electrode group on one plane is connected between the ends of the electrode groups on the upper and lower planes. an electric melting furnace located in the gap, thus causing the ascending glass stream of each lower plane to meet the descending glass stream of each upper plane at the interface with the upper plane, and preventing each glass stream from penetrating into the other plane; and a melting method.
さらに、特公昭56−9455号公報は電気溶融炉にお
いて溶融ガラスの上に堆積する未溶融のガラスバッチあ
るいは不完全溶融バッチが電極付 。Furthermore, Japanese Patent Publication No. 56-9455 discloses that an unmelted glass batch or an incompletely melted glass batch deposited on molten glass in an electric melting furnace is equipped with electrodes.
近の炉壁に向って対流するのを最小限に抑制するために
、溶融ガラスに浸漬されている電極の上方で、かつ溶融
ガラスと接触しない位置において炉壁にバッチ邪摩板手
段を装着した電気溶融炉を開示している。In order to minimize convection toward the nearby furnace wall, a batch warping plate means was attached to the furnace wall above the electrode immersed in the molten glass and at a position where it did not come into contact with the molten glass. Discloses an electric melting furnace.
これらの公報を含めて従来の電気溶融炉はその水平断面
形状としてn = ’1以上の正6n角形、普通は6〜
12角形、典形的には6角形の構造を取る点で共通して
いる。例えば、前記特公昭52−26884号公報は6
角形の上方垂直部とこれに連接する倒立6角錐形の漏斗
形底部から成る炉構造を開示し、また前記特開昭47−
13618号及び特公昭56−9455号公報は共に6
角形の角柱構造を開示している。Conventional electric melting furnaces, including these publications, have a horizontal cross-sectional shape of a regular 6n square with n = '1 or more, usually 6~
They have a common feature in that they have a dodecagonal, typically hexagonal structure. For example, the aforementioned Japanese Patent Publication No. 52-26884 has 6
Discloses a furnace structure consisting of a rectangular upper vertical part and an inverted hexagonal pyramidal funnel-shaped bottom part connected to the upper vertical part, and also discloses the above-mentioned Japanese Patent Application Laid-Open No.
13618 and Japanese Patent Publication No. 56-9455 are both 6
A rectangular prismatic structure is disclosed.
ガラス溶融炉はガラスバッチの溶融に十数百度の温度が
必要とされることから、そのような温度に耐え得る耐火
レンガ等の耐火材料で構成されるが、これらの耐火材料
は周知のように溶融ガラスによる侵蝕を避けられず、そ
の耐用年数は2〜6年程度といわれている。耐用年数経
過後、炉は改修を受け、あるいは新たに建造されるが、
その炉コストはガラス製品の生産コストのかなシ大きな
部分を占める。一方、耐火材料の溶融ガラスによる侵蝕
は操業初期には実際上問題にならないが、操業後期に近
ずくにつれて炉の安全操業にとって大きな問題になる。Glass melting furnaces require a temperature of several hundred degrees to melt a batch of glass, so they are constructed of refractory materials such as refractory bricks that can withstand such temperatures, but as is well known, these refractory materials Corrosion caused by molten glass cannot be avoided, and its service life is said to be about 2 to 6 years. After the end of its useful life, the furnace is refurbished or a new one is built.
The furnace cost accounts for a large portion of the production cost of glass products. On the other hand, corrosion of the refractory material by molten glass does not pose a practical problem in the early stages of operation, but as it approaches the later stages of operation, it becomes a serious problem for the safe operation of the furnace.
従って、炉形態の単純さと炉構造の安定さけ炉建造、あ
るいは炉に対する支持、補強工作の容易さを保証するの
みならず、炉の耐久性を高め、且つ炉の操業安全性を確
保する意味においても重要なファクターである。これら
の観点から従来の電気溶融炉を検討すると、その多角形
態は炉建造の技術的困難さを増し、また外部からの支持
、補強工作を複雑、困難にするとともに、多角形態に基
づく耐火材料相互間の接合目地部の多さは溶融ガラスに
よる侵蝕がよシ激しく進行する侵蝕部位の増大につなが
シ、炉の深さが平炉の数倍に及ぶことと相まって炉の総
合的な構造安定性を阻害する要因となっている。Therefore, the simplicity of the furnace form and the stability of the furnace structure not only guarantee the ease of furnace construction or support and reinforcement work for the furnace, but also increase the durability of the furnace and ensure the operational safety of the furnace. is also an important factor. When considering conventional electric melting furnaces from these viewpoints, the polygonal shape increases the technical difficulty of furnace construction, makes external support and reinforcement work complicated and difficult, and makes it difficult to use refractory materials based on the polygonal shape. The large number of joints between the molten glass leads to an increase in the number of eroded areas where erosion by the molten glass progresses rapidly, and this, coupled with the fact that the depth of the furnace is several times that of an open hearth, impairs the overall structural stability of the furnace. This is a hindering factor.
このような正多角形の炉構造は給電系の本電源が位相が
互いに1200 ずつずれている三相交流電源であるこ
とに関連している。すなわち、炉の下部における層流清
澄領域のガラスに影響を及はさない適正な対流を生起さ
せるには電極を含む平面内のガラスを電流が均等に流れ
る必要があるが、三相のパワーシステムを用いる場合に
この電流の均等な流れを達成するにはパワーシステムの
3つの相に接続される各電極を同一平面内において正三
角形を形成するように配置するのが最も合理的であって
、前記多角炉構造はこの電極配置に対してn = ’1
以上の、正6n角形の横断面構造が合目的であることに
由来している。This regular polygonal furnace structure is related to the fact that the main power sources of the power supply system are three-phase AC power sources whose phases are shifted by 1200 degrees from each other. That is, the current must flow evenly through the glass in the plane containing the electrodes to create proper convection that does not affect the glass in the laminar fining region at the bottom of the furnace, but in a three-phase power system. In order to achieve an even flow of current when using a power system, it is most rational to arrange the electrodes connected to the three phases of the power system so as to form an equilateral triangle within the same plane. The polygonal furnace structure has n = '1 for this electrode arrangement.
This is because the above-mentioned regular 6n-gonal cross-sectional structure is suitable for the purpose.
しかし、このような三相電極配置によって均等加熱と適
正対流の形成を達成するにはかなシ複雑な通電パターン
、例えば前記特公昭52−26884号公報に典形的に
開示されるように、炉壁に配設された電極を含むレベル
の面内において各電極を頂点とする三角形の辺に最短電
流通路を形成する三角形の通電パターンや、隣シ合う電
極間で炉壁周辺に最短電流通路を形成する炉壁周囲通電
パターン、あるいは複数のレベJしにおいて前記両パタ
ーンを重ね合わせたパターンのような複雑な通電パター
ンを取る必要があυ、これに伴ってその制御技術も複雑
になる。そして、特に電気溶融炉が大型になると、この
ような通電パターンによって広い面積の全面にわたって
均等な、加熱と適正な対流形成及びその制御を達成する
のは非常に困難で、この加熱制御の面からも炉の大きさ
には制限がある。However, in order to achieve uniform heating and formation of proper convection with such a three-phase electrode arrangement, it is difficult to create a furnace with a complicated current pattern, for example, as typically disclosed in Japanese Patent Publication No. 52-26884. A triangular energization pattern that forms the shortest current path on the side of a triangle with each electrode as the apex within the plane of the level that includes the electrodes arranged on the wall, and a triangular current path that forms the shortest current path around the furnace wall between adjacent electrodes. It is necessary to form a complicated energization pattern around the furnace wall, or a pattern in which the two patterns are superimposed on each other at a plurality of levels, and the control technology accordingly becomes complicated. Especially when the electric melting furnace becomes large, it is very difficult to achieve uniform heating and proper convection formation and control over a wide area using such a current pattern, and from the aspect of heating control. However, there are limits to the size of the furnace.
従って、本発明は単純な炉形態を持ち、構造安定性の高
い、そして単純な通電パターンによって均等加熱と適正
対流の形成を可能にし、しかも任意の規模の炉に適用可
能な電極配置を持つ縦型電気溶融炉を提供することを目
的とする。Therefore, the present invention has a simple furnace configuration, has high structural stability, enables uniform heating and formation of proper convection through a simple current flow pattern, and has a vertical electrode arrangement that can be applied to furnaces of any size. The purpose is to provide a type electric melting furnace.
上記目的を達成する本発明によれば、基本的(は、頂部
に原料ガラスバッチの受容開口を有する原料ガラスバッ
チの溶融対流区域と;炉底区域に溶融ガラスの取出開口
を有し、前記溶融対流区域に対して垂直下方に連接する
溶融ガラスの層流清澄区域と;少なくとも前記溶融対流
区域に少なくとも1つの水平レベルにおいて該区域を画
成している周壁に貫通、配設されている電極群とから成
シ;そして前記溶融ガラスの取出開口は任意の流通路を
介してフィーダーに接続されているガラスの電気溶融炉
において:前記炉は方形の横断面形状1組の周壁に1そ
れら周壁に対して実質的に垂直に、かつ等間隔に、そし
て対向関係で、隣シ合う電極間では相互に位相を異にし
、−力対向する電極間では相互に位相を同じくして配置
されていることを特徴とする電気溶融炉が提供される。According to the present invention, which achieves the above objects, the basic structure consists of: a melting convection zone for the raw glass batch having a receiving opening for the raw glass batch at the top; a laminar flow clarification zone of molten glass adjoining vertically downwardly with respect to the convection zone; electrodes disposed through at least said molten convection zone in at least one horizontal level on a peripheral wall defining said zone; and in an electric glass melting furnace, the molten glass take-out opening is connected to a feeder through an arbitrary flow path: the furnace has a set of circumferential walls having a rectangular cross-sectional shape; - arranged substantially perpendicularly, equidistantly, and in opposing relation, with adjacent electrodes being out of phase with each other, and opposing electrodes being in phase with each other; An electric melting furnace is provided.
この本発明によれば、その方形横断面構造は炉の建造と
その支持、補強工作を容易にし、また溶融ガラスによる
′侵蝕がよシ激しく進行する耐火材相間の接合目地部を
減少させ、かくして炉の総合的な構造安定性を著しく向
上させるとともに、周壁に垂直に、かつ等間隔に配列さ
れる電極配置は複雑な加熱制御技術を要することなしに
、そして炉の大/hに係わらず、電極を含む平面内に均
等な通電パターンを形成し、かくして溶融対流区域にバ
ランスのよい熱対流を形成することを可能にする0
以上の本発明を図面を参照してさらに説明すもしかし、
図示電気溶融炉は本発明の好ましい実施態様であって、
本発明がこれらに限定されないことはもちろんである。According to the present invention, the rectangular cross-sectional structure facilitates the construction of the furnace and its supporting and reinforcing work, and also reduces the number of joints between the refractory material phases where erosion by molten glass is more likely to proceed. In addition to significantly improving the overall structural stability of the furnace, the electrode arrangement perpendicular to the peripheral wall and at equal intervals does not require complicated heating control technology, and regardless of the size of the furnace / h. The invention will now be further explained with reference to the drawings, which make it possible to form a uniform current carrying pattern in the plane containing the electrodes, thus creating a balanced thermal convection in the melt convection zone.
The illustrated electric melting furnace is a preferred embodiment of the invention and includes:
Of course, the present invention is not limited to these.
添附図面において、第1図は本発明の方形電気溶融炉の
側断面図を、また第2図は電極配置とこれに対するパワ
ーシステムを示す第1図の■−■面における横断面図を
それぞれ示す。これらの図において、電気溶融炉1は耐
火レンガがら成る周壁2及び炉底壁3によって画成され
、そしてその相対的に上部は溶融ガラスの溶融対流区域
4を構成し、相対的に下部は溶融ガラスの層流清澄区域
5を構成する。In the accompanying drawings, FIG. 1 shows a side sectional view of the rectangular electric melting furnace of the present invention, and FIG. 2 shows a cross-sectional view taken along the plane ■-■ of FIG. 1, showing the electrode arrangement and the power system therefor. . In these figures, an electric melting furnace 1 is defined by a peripheral wall 2 made of refractory bricks and a furnace bottom wall 3, the relative upper part of which constitutes a melting convection area 4 of the molten glass, and the relative lower part of which constitutes a melting convection area 4 for the molten glass. A laminar flow clarification zone 5 of the glass is constituted.
溶融対流区域4の頂部は原料ガラスバッチを受容し、炉
内溶融ガラス6の上にガラスバッチの堆積層7を形成す
るために全面的に解放されている。The top of the melting convection zone 4 is entirely open for receiving the raw glass batch and forming a deposited layer 7 of glass batch on top of the furnace molten glass 6.
この頂部開放口の上方には、図示しないが、原料ガラス
バッチの供給装置が配置され、ガラスバラ1
チがその開放口に連続的に、又は断続的に供給、好まし
くは散布、供給されるようになっている。Although not shown, a feeding device for raw glass batches is disposed above the top opening, so that glass batches are continuously or intermittently fed into the opening, preferably by being scattered. It has become.
この溶融対流区域4においてガラスバッチが溶融され、
熱対流下である程度の清澄、均質化が行われる。The glass batch is melted in this melting convection zone 4,
A certain degree of clarification and homogenization takes place under thermal convection.
一方、層流清澄区域5は前記溶融対流区域4がら垂直下
方に直接連接し、炉底壁3によって閉じられている。こ
の層流清澄区域5において溶融対流区域4から連続供給
される溶融が2スは実質的に完全に均質化及び清澄化さ
れる。均質、清澄化されたガラスは1つの周壁の底端部
に形成される取出開口8から取シ出される。との取出開
口8には、図示されないが、通常はライず−あるいは他
の任意の流通路を介して、成形装置を備えるフィーダー
が接続されている。取出開口8は本図のように1個に限
定されず、複数の周壁に複数個形成することもできる。On the other hand, the laminar flow clarification zone 5 is directly connected vertically downward from the melt convection zone 4 and is closed by the furnace bottom wall 3. In this laminar flow clarification zone 5, the melt continuously supplied from the melt convection zone 4 is substantially completely homogenized and clarified. The homogeneous, clarified glass is removed through a removal opening 8 formed in the bottom end of one of the peripheral walls. Although not shown, a feeder provided with a forming device is usually connected to the take-out opening 8 through a riser or any other flow path. The number of extraction openings 8 is not limited to one as shown in this figure, but a plurality of extraction openings may be formed in a plurality of peripheral walls.
本発明の電気溶融炉1は方形の横断面構造を取る。この
方形炉において、その横断面形状は長方形及び正方形を
取り得る。長方形の横断面形状を2
取る場合、その短辺対長辺の長さの比は大幅に変えるこ
とができ、例えば短辺を長辺のl/3又はそれ以下にす
ることもできる。これは通電される溶融ガラスの電気伝
導度がガラス組成によってかなシ大幅に変わることなど
による。The electric melting furnace 1 of the present invention has a rectangular cross-sectional structure. In this rectangular furnace, its cross-sectional shape can be rectangular or square. In the case of a rectangular cross-sectional shape, the ratio of the length of the short side to the long side can vary considerably, for example the short side can be 1/3 of the long side or less. This is because the electrical conductivity of molten glass to which electricity is applied varies greatly depending on the glass composition.
第1図及び第2図において、数字9は主電極群を表わし
、これら電極を介して炉内溶融ガラスに直接通電し、発
生するジュール熱によって溶融ガラス上のガラスバッチ
層のガラスバッチを溶融ガラスとの接触界面において順
次溶融ガラス化し、かつ溶融ガラスに熱対流を引き起す
。電極群9がこのように機能するために、これら電極−
は典形的には溶融ガラスの液面下10〜601程度の深
さの1つの水平レベルに配置されるが、本発明において
は従来法と同様にこの一次電極群を含めて主電極群を複
数レベルに配設することもできる。In Figures 1 and 2, the number 9 represents a group of main electrodes, and electricity is applied directly to the molten glass in the furnace through these electrodes, and the Joule heat generated transforms the glass batch in the glass batch layer on the molten glass into the molten glass. The glass is sequentially melted and vitrified at the contact interface with the molten glass, and thermal convection is caused in the molten glass. In order for the electrode group 9 to function in this way, these electrodes -
are typically arranged at one horizontal level at a depth of about 10 to 60 cm below the liquid surface of the molten glass, but in the present invention, as in the conventional method, the main electrode group including this primary electrode group is They can also be placed on multiple levels.
本発明において、電極群9は本発明の方形横断面炉の対
向する1組の周壁に、少なくとも1つの水平レベルにお
いて、それら周壁に対して垂直に、かつ実質的に等間隔
に、そして対向関係でそれら周壁に貫通、配設される。In the present invention, the electrode groups 9 are arranged on a pair of opposing circumferential walls of the rectangular cross-section furnace of the present invention, in at least one horizontal level, perpendicular to the circumferential walls and substantially equally spaced, and in opposing relationship. It penetrates and is installed in those surrounding walls.
長方形の横断面炉の場合、電極群は長辺をなす周壁に配
設するのが好ましいが、小型炉の場合はその短辺をなす
周壁に配設することができる。In the case of a rectangular cross-section furnace, the electrode group is preferably arranged on the long side of the circumferential wall, but in the case of a small furnace it can be arranged on the short side of the circumferential wall.
上記の電極配置において、電極は隣シ合う電極間におい
ては相互に異なる位相を持つように、−力対向する電極
間においては同じ位相を持つように配置される。電極間
の位相差は90° 又は120゜とするのが最も一般的
である。In the above electrode arrangement, the electrodes are arranged so that adjacent electrodes have mutually different phases, and electrodes facing each other have the same phase. Most commonly, the phase difference between the electrodes is 90° or 120°.
本発明において、電極は棒状電極で構成される。In the present invention, the electrode is a rod-shaped electrode.
これらの棒状電極は加熱を広い領域に及ぼす意味から炉
の中央部附近まで延在、配置するのが好ましい。また、
それぞれの周壁に複数配置されている電極群において、
両端の電極ではさまれる内側の各相の電極は両側に位相
が異なる電極を持つことから電流密度が高くな9.電極
の消耗が大きいことから、これを防ぐために後述する第
3図および第4図の実施例に示す如くそれぞれ2本の電
極で構成するのが好ましい。These rod-shaped electrodes are preferably extended and placed near the center of the furnace in order to heat a wide area. Also,
In a plurality of electrode groups arranged on each peripheral wall,
9. The inner phase electrodes sandwiched between the electrodes at both ends have electrodes with different phases on both sides, so the current density is high.9. Since the consumption of the electrodes is large, in order to prevent this, it is preferable to construct each electrode with two electrodes as shown in the embodiments shown in FIGS. 3 and 4, which will be described later.
本発明において、電極自体は公知の材質よシ成るものが
使用し得、例えばモリブデン電極がちも上記の電極配置
において、電極間の位相差が、例えば90° 又は12
0° である位相関係は公知の二相又は三相のパワーシ
ステムを用いることによって達成することができる。In the present invention, the electrodes themselves may be made of known materials, such as molybdenum electrodes, and in the above electrode arrangement, the phase difference between the electrodes is, for example, 90° or 12°.
A phase relationship of 0° can be achieved using known two-phase or three-phase power systems.
すなわち、第2図は隣シ合う電極間において位相が互い
に90°異なシ、一方対向する電極は同じ位相を持って
いる、二相のパワーシステムによる棒状電極群9の配置
を示し、そのパワーシステムは三相電源に接続されてい
るレギュレーター10とスコツト結線による二相出力の
変圧器11よ構成る。このパワーシステムによる溶融ガ
ラス中の電流密度、従ってガラス温度の制御はレギュレ
ータ−10によって行われる。That is, FIG. 2 shows the arrangement of the rod-shaped electrode group 9 in a two-phase power system in which adjacent electrodes have a phase difference of 90 degrees from each other, while opposing electrodes have the same phase. It consists of a regulator 10 connected to a three-phase power source and a two-phase output transformer 11 with Scott connection. Control of the current density in the molten glass and therefore the glass temperature by this power system is performed by a regulator 10.
第6図は二相電極配置のもう1つの例を示し、第2図と
同様に二相のパワーシステムと電極間の相互位相関係を
持つが、両端の電極を除いて内側の各位相の電極がそれ
ぞれ2本の電極で構成されている。FIG. 6 shows another example of a two-phase electrode arrangement, which has a two-phase power system and a mutual phase relationship between the electrodes as in FIG. are each composed of two electrodes.
また、第4図はレギュレーター10′と三相出力5
の変圧器11′よ)成る三相のパワーシステムによる転
極配置を示し、各電極9′は図示のようにそれぞれ位相
が相互に120°異なっているR、S、Tの相を持って
いる。FIG. 4 shows a polarity reversal arrangement using a three-phase power system consisting of a regulator 10' and a transformer 11' with a three-phase output 5, and each electrode 9' has a phase of 120 degrees with respect to the other as shown in the figure. It has different R, S, and T phases.
以上説明した本発明の縦型方形電気溶融炉によるガラス
の溶融、清澄過程を第1図及び第2図を主に参照して説
明する。The glass melting and fining process using the vertical rectangular electric melting furnace of the present invention described above will be explained with reference mainly to FIGS. 1 and 2.
第1図及び第2図の電気溶融炉1において、原料ガラス
バッチは炉の頂部開放口に散布、供給され、炉内溶融ガ
ラス6の上に堆積してバッチ層7を形成する。このバッ
チ層7は炉内溶融ガラスからの放熱を遮断する。層1の
ガラスバッチは溶融ガラス6との接触界面において溶融
ガラスから熱を受けて徐々に溶融及びガラス化される。In the electric melting furnace 1 shown in FIGS. 1 and 2, a raw glass batch is distributed and supplied to the top opening of the furnace, and is deposited on the molten glass 6 in the furnace to form a batch layer 7. This batch layer 7 blocks heat radiation from the molten glass in the furnace. The glass batch of layer 1 receives heat from the molten glass at the contact interface with the molten glass 6 and is gradually melted and vitrified.
このときガラス化反応によ多発生するガスは大部分バッ
チ層1を抜け、大気中に散逸する。At this time, most of the gas generated by the vitrification reaction passes through the batch layer 1 and is dissipated into the atmosphere.
炉内溶融ガラス6の加熱は炉の長辺を形成する対向する
周壁のそれぞれに対して垂直に、かつ等間隔に、炉の中
央部附近まで延在、配置された棒状電極群9に対する二
相パワーシステム10゜6
11からの通電によって達成される。電極は隣シ合う電
極間で位相を90°異にし、一方対向する電極間では同
じ位相を持っている。このような配置の電極に通電する
と、平行な隣シ合う電極間に最短電流通路が形成され、
かつ各電極を中心に、隣接電極方向に減少する電流密度
勾配を持ち、その電極に沿って帯状に均一な最高電流密
度領域が形成される。そしてその最高電流密度領域の形
成に伴ってその近傍に同様に帯状の最高温度領域が形成
され、かくして電極間において電極近傍で高く、電極を
離れるにつれて低くなる温度分布が現われる。最高電流
密度、従って最高温度はレギュレーター10によって行
われる。The molten glass 6 in the furnace is heated by a two-phase electrode group 9 extending perpendicularly to the opposing peripheral walls forming the long sides of the furnace and arranged at regular intervals to near the center of the furnace. This is achieved by energizing from the power system 10°611. Adjacent electrodes have a phase difference of 90°, while opposing electrodes have the same phase. When electricity is applied to the electrodes arranged in this way, the shortest current path is formed between adjacent parallel electrodes,
In addition, a current density gradient decreases in the direction of adjacent electrodes around each electrode, and a uniform highest current density region is formed in a band shape along the electrode. Along with the formation of the highest current density region, a band-shaped highest temperature region is similarly formed in the vicinity thereof, and thus a temperature distribution appears between the electrodes, which is high near the electrodes and decreases as the distance from the electrodes increases. The highest current density and therefore the highest temperature is provided by the regulator 10.
このように高温に加熱された溶融ガラスは相対的に高温
、低密度の最高温度領域のガラスが主に大きな上昇流を
形成してバッチ層Tに向い、その熱の一部をガラスバッ
チの溶融、ガラス化反応に供給し、自身は熱を失って冷
え、低温、高密度となる。この低温、高密度のガラスは
ガラスバッチの溶融、ガラス化反応の結果生成した粗溶
融状態のガラスと混じp合い、下降流となって下方に向
い、そして電極近傍に到達すると再び加熱されて上昇す
る。この一連のザイクルが存在することによシミ極近傍
とガラスバッチ層との間に熱対流としての、激しい循環
流Aが形成される。The molten glass heated to a high temperature in this way has a relatively high temperature, and the low-density glass in the highest temperature region mainly forms a large upward flow toward the batch layer T, and a part of the heat is used to melt the glass batch. , supplied to the vitrification reaction, loses heat and cools down, becoming low temperature and high density. This low-temperature, high-density glass mixes with the coarsely molten glass produced as a result of the glass batch melting and vitrification reaction, flows downward, and when it reaches the vicinity of the electrode, it is heated again and rises. do. Due to the existence of this series of cycles, an intense circulating flow A as thermal convection is formed between the vicinity of the stain and the glass batch layer.
この電気溶融炉1は電極群9による加熱だけを熱源とし
ているので、電極群9の近傍を境に下方に向うにつれて
ガラス温度は徐々に低下する。このため前記循環流人は
電極群よシ下方のある一定の位置までしかその影響を及
ぼさない。このガラスの熱対流領域が前記溶融対流区域
4に対応すらこのガラスの熱対流領域の深さはいろいろ
な因子、例えば設定温度によって変わシ、ケースバイケ
ースであるが、通常は炉の深さの1/2〜315程度の
位置となるように設定される。Since this electric melting furnace 1 uses only the heating by the electrode group 9 as its heat source, the glass temperature gradually decreases as it moves downward from the vicinity of the electrode group 9. Therefore, the circulating flow only exerts its influence up to a certain position below the electrode group. Even if the heat convection area of this glass corresponds to the melting convection area 4, the depth of the heat convection area of this glass will vary depending on various factors, such as the set temperature, and will vary from case to case, but will usually depend on the depth of the furnace. It is set to a position of about 1/2 to 315.
前記粗溶融ガラスはこの溶融対流区域4のガラスにおけ
る循環流人にまき込まれ、循環する間にその不均質部分
は引き伸ばされ、物理的攪拌、混合及び拡散を受けて均
質化が進むとともに、バッチ層近傍で脱泡されなかった
残存ガスの大部分がこの循環中に浮上、脱気される。The crude molten glass is drawn into the circulating stream in the glass of the melting convection zone 4, and during the circulation, its heterogeneous portions are stretched and homogenized through physical stirring, mixing and diffusion, and the batch is Most of the remaining gas that was not degassed near the layer floats to the surface during this circulation and is degassed.
上記第1図及び第2図の方形炉と電極配置に対して、第
6図及び第4図の電極配置を持つ方形炉によるときも、
基本的には第1図及び第2図と同じ通電パターンと熱対
流が形成される。In contrast to the rectangular furnace and electrode arrangement shown in Figs. 1 and 2 above, when using a rectangular furnace with the electrode arrangement shown in Figs. 6 and 4,
Basically, the same current pattern and thermal convection as in FIGS. 1 and 2 are formed.
かくして、本発明の方形電気溶融炉によれば、互いに平
行な炉の対向する1組の周壁に垂直に、かつ等間隔に、
そして対向関係で配設された、隣シ合う平行な電極間に
自然で、かつ単純な、各電極間で相互に均等な平面内通
電パターンを形成することができ、従って溶融対流区域
の全域をカバーしてバランスのよい熱対流を形成するこ
とができる。また、この平面内通電パターンは基本的に
は1つの水平レベルにだけ電極を配置することによって
全水平面をカバーして形成することができ、従ってまた
炉の大型化に対しては電極数の増加で対応することがで
きる。Thus, according to the rectangular electric melting furnace of the present invention, vertically and equally spaced from a pair of opposing circumferential walls of the furnace that are parallel to each other,
A natural and simple in-plane energization pattern can be formed between adjacent parallel electrodes disposed in opposing relation, and mutually uniform between each electrode, thus covering the entire area of the melting convection area. It can be covered to create well-balanced heat convection. In addition, this in-plane energization pattern can basically be formed covering the entire horizontal plane by arranging the electrodes at only one horizontal level, and therefore, for larger furnaces, the number of electrodes can be increased. You can respond with
この溶融対流区域4において溶融、混合されたガラスは
かなシの程度まで清澄化されているが、しかしなお若干
の泡、不均一な脈理及び温度むら9
スは次に順次層流清澄区域5に移行し、炉底まで進む間
に完壁な均質、清澄化と温度の均一化が達成される。In this melting convection zone 4, the melted and mixed glass is refined to a slight degree, but there are still some bubbles, non-uniform striae and temperature irregularities. As it progresses to the bottom of the furnace, complete homogeneity, clarification, and temperature uniformity are achieved.
すなわち、層流清澄区域5における溶融ガラスには大量
の溶融ガラスに対して十分に少ないガラスの引出量に基
づいて下方に向う極めて緩慢な、層流としての流れBの
みが存在している。溶融対流区域4からの溶融ガラスは
この層流Bに乗って層流清澄区域5に長時間滞在し、下
方に移行する間に拡散及び熱伝導に基づいて不均質部分
と温度むらが解消される。また、溶融対流区域4からの
溶融ガラス中に残存する小泡のうちジンプ(Lamp)
の式
%式%
(式中、■は層流Bの流速であシ、
gは重力加速度であり、
dは泡の径であ)、
ρは溶融ガラスの密度であシ、そして
ηは溶融ガラスの粘度である)
0
で与えられる径よシ大きいものは溶融ガラスが層流清澄
区域を移行する間に上方に浮上、脱泡され一方それ以下
の微小な泡はガラスが下方に進むにつれて増加する圧力
を受けて、気−液平衡の法則に従いその大半がガラス中
に溶は込む。実際、炉底において溶融ガラスには気泡は
実質的に存在しないことが見い出されている。かくして
、炉底近傍には化学組成的に、及び熱的に均一で、且つ
泡のない、実質的に完全に均質、清澄化された加圧状態
の溶融ガラスが存在し、完全に精製されたガラスがガラ
スの取出開口8に供給される。That is, in the molten glass in the laminar flow clarification zone 5, there is only a very slow downward laminar flow B based on the sufficiently small amount of glass drawn out compared to the large amount of molten glass. The molten glass from the molten convection zone 4 rides this laminar flow B and stays in the laminar flow clarification zone 5 for a long time, and while moving downward, the inhomogeneity and temperature unevenness are eliminated based on diffusion and heat conduction. . In addition, among the small bubbles remaining in the molten glass from the molten convection zone 4, lamps
The formula is % (where ■ is the flow velocity of the laminar flow B, g is the gravitational acceleration, and d is the diameter of the bubble), ρ is the density of the molten glass, and η is the molten glass. Bubbles larger than the diameter given by 0 (the viscosity of the glass) float upwards and are defoamed while the molten glass moves through the laminar flow clarification zone, while smaller bubbles increase as the glass moves downward. Under this pressure, most of it melts into the glass according to the law of vapor-liquid equilibrium. In fact, it has been found that there are virtually no air bubbles in the molten glass at the bottom of the furnace. Thus, near the bottom of the furnace there is a molten glass in a pressurized state that is chemically and thermally uniform, bubble-free, substantially completely homogeneous, clarified, and completely purified. Glass is fed into the glass removal opening 8 .
この濁流清澄区域5には炉の始動時における底部区域の
ガラスの加熱及び/又は炉の運転時に取出開口に供給さ
れる精製ガラスの温度補正のために周壁″に補助電極群
12を貫通、配設することができる。この補助電極群1
2による加熱は層流状態にある溶融ガラスに新たな熱対
流を引き起すことのないように制御されなければならな
い。In this turbid stream clarification zone 5, an auxiliary electrode group 12 is provided through the peripheral wall for heating the glass in the bottom zone at the time of starting the furnace and/or for temperature correction of the refined glass supplied to the take-out opening during operation of the furnace. This auxiliary electrode group 1
The heating by 2 must be controlled so as not to cause new thermal convection in the molten glass which is in a laminar state.
第1図は本発明の電気溶融炉の側断面図であり、第2図
は電極配置と電極に対するパワーシステムを示す第1図
の■−■面の横断面図であり、第3図及び第4図は他の
電極配置とそれに対するパワーシステムを示す炉の横断
面図である。
1・・・電気溶融炉、2・・・周壁、3・・・底壁、4
・・・溶融対流区域、5・・・層流清澄区域、6・・・
溶融ガラス、7・・・ガラスバッチ堆積層、8・・・溶
融ガラス取山開口、9.9′・・・主電極群、10 、
10’・・・レギュレーター、11 、11’・・・変
圧器、12・・・補助電極群、A・・・循環流、B・・
・層流。
代理人 浅 村 皓
外4名
オア 図
12園
2−3図
才4図
・ R2R
−1−/FIG. 1 is a side cross-sectional view of the electric melting furnace of the present invention, FIG. 2 is a cross-sectional view taken along the plane ■-■ of FIG. 1 showing the electrode arrangement and the power system for the electrodes, and FIGS. FIG. 4 is a cross-sectional view of the furnace showing an alternative electrode arrangement and its associated power system. 1... Electric melting furnace, 2... Peripheral wall, 3... Bottom wall, 4
... Melt convection zone, 5... Laminar flow clarification zone, 6...
Molten glass, 7... Glass batch deposited layer, 8... Molten glass stack opening, 9.9'... Main electrode group, 10,
10'...Regulator, 11, 11'...Transformer, 12...Auxiliary electrode group, A...Circulating flow, B...
・Laminar flow. Agent Asamura Akira 4 people orer Fig. 12 Garden 2-3 Fig. 4 Fig. R2R -1-/
Claims (5)
ガラスバッチの溶融対流区域と;炉底区域に溶融ガラス
の取出開口を有し、前記溶融対流区域に対して垂直下方
に連接する溶融ガラスの層流清澄区域と;少なくとも前
記溶融対流区域に少なくとも1つの水平レベルにおいて
該区域を画成している周壁に貫通、配設されている電極
群とから成シ;そして前記溶融ガラスの取出開口は任意
の流通路を介してフィーダーに接続されているガラスの
電気溶融炉において:前記炉は方形の横断面形状に形成
され;そして前記電極群は棒状電極で構成され、そして
各電極は前記方形横断面炉の対向する1組の周壁に、そ
れら周壁に対して実質的に垂直に、かつ等間隔に、そし
て対向関係で、隣シ合う電極間では相互に位相を異にし
、一方対向する電極間では相互に位相を同じくして配置
されていることを特徴とするガラスの電気溶融炉。(1) A raw glass batch melting convection area having a receiving opening for the raw glass batch at the top; a molten glass convection area having a molten glass take-out opening at the bottom area and connecting vertically downward to the melting convection area; a laminar flow clarification zone; a set of electrodes extending through and disposed in at least one horizontal level in the circumferential wall defining the zone; and an outlet opening for the molten glass; In a glass electric melting furnace connected to a feeder via an arbitrary flow path: the furnace is formed in the shape of a rectangular cross section; and the electrode group is composed of rod-shaped electrodes, and each electrode A pair of opposing peripheral walls of a surface furnace are provided with electrodes substantially perpendicular to the peripheral walls, equidistantly spaced, and in opposing relation, with adjacent electrodes being out of phase with each other, and electrodes facing each other being An electric glass melting furnace characterized by being arranged in phase with each other.
囲第(1)項に記載の電気溶融炉。(2) The electric melting furnace according to claim (1), wherein the cross-sectional shape of the furnace is rectangular.
記特許請求の範囲第(2)項に記載の電気溶融炉。(3) The electric melting furnace according to claim (2), wherein the electrode group is disposed on a peripheral wall forming a long side of the furnace.
許請求の範囲第(1)項から第(3)項のいずれか1項
に記載の電気溶融炉。(4) The electric melting furnace according to any one of claims (1) to (3), wherein the phase difference between adjacent electrodes is 90°.
特許請求の範囲第(1)項から第(3)項のいずれか1
項に記載の電気溶融炉。 ・ (6)電極が炉の中央部附近まで延在、配置されて
いる前記特許請求の範囲第(3)項から第(5)項のい
ずれか1項に記載の電気溶融炉。 (力 両端の電極ではさまれる内側の各相の電極がそれ
ぞれ2本の電極で構成されている前記特許請求の範囲第
(1)項から第(6)項のいづれか1項に記載の電気溶
融炉。(5) Any one of claims (1) to (3) above, wherein the phase difference between adjacent electrodes is 1200°.
The electric melting furnace described in Section. - (6) The electric melting furnace according to any one of claims (3) to (5), wherein the electrode extends and is arranged near the center of the furnace. (Force) The electric melting system according to any one of Claims (1) to (6), wherein the electrodes of each phase on the inside sandwiched between the electrodes at both ends are each composed of two electrodes. Furnace.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13047981A JPS5832030A (en) | 1981-08-20 | 1981-08-20 | Electric melting furnace for glass |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13047981A JPS5832030A (en) | 1981-08-20 | 1981-08-20 | Electric melting furnace for glass |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS5832030A true JPS5832030A (en) | 1983-02-24 |
Family
ID=15035229
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13047981A Pending JPS5832030A (en) | 1981-08-20 | 1981-08-20 | Electric melting furnace for glass |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5832030A (en) |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63256286A (en) * | 1987-04-14 | 1988-10-24 | Kubota Ltd | Solid phase joining method for metal parts |
| JPH01167237A (en) * | 1987-12-24 | 1989-06-30 | Nippon Sheet Glass Co Ltd | Glass melting furnace |
| US6983006B2 (en) | 2003-04-01 | 2006-01-03 | Motoaki Miyazaki | All-electric glass-melting deep furnace and method of refining and supplying glass |
| WO2012132474A1 (en) * | 2011-03-31 | 2012-10-04 | AvanStrate株式会社 | Glass substrate production method |
| JP5668066B2 (en) * | 2011-03-31 | 2015-02-12 | AvanStrate株式会社 | Manufacturing method of glass substrate |
| RU203377U1 (en) * | 2020-04-03 | 2021-04-01 | Федеральное государственное бюджетное образовательное учреждение высшего образования "Саратовский государственный технический университет имени Гагарина Ю.А." (СГТУ имени Гагарина Ю.А.) | Diffusion welding device |
| JP2021533059A (en) * | 2018-07-27 | 2021-12-02 | コーニング インコーポレイテッド | A method for heating metal containers in the glass manufacturing process |
-
1981
- 1981-08-20 JP JP13047981A patent/JPS5832030A/en active Pending
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63256286A (en) * | 1987-04-14 | 1988-10-24 | Kubota Ltd | Solid phase joining method for metal parts |
| JPH01167237A (en) * | 1987-12-24 | 1989-06-30 | Nippon Sheet Glass Co Ltd | Glass melting furnace |
| US6983006B2 (en) | 2003-04-01 | 2006-01-03 | Motoaki Miyazaki | All-electric glass-melting deep furnace and method of refining and supplying glass |
| WO2012132474A1 (en) * | 2011-03-31 | 2012-10-04 | AvanStrate株式会社 | Glass substrate production method |
| CN103080025A (en) * | 2011-03-31 | 2013-05-01 | 安瀚视特控股株式会社 | Glass substrate production method |
| CN103124700A (en) * | 2011-03-31 | 2013-05-29 | 安瀚视特控股株式会社 | Manufacturing method of glass substrate |
| JP5668066B2 (en) * | 2011-03-31 | 2015-02-12 | AvanStrate株式会社 | Manufacturing method of glass substrate |
| JP2021533059A (en) * | 2018-07-27 | 2021-12-02 | コーニング インコーポレイテッド | A method for heating metal containers in the glass manufacturing process |
| US12043565B2 (en) | 2018-07-27 | 2024-07-23 | Corning Incorporated | Methods for heating a metallic vessel in a glass making process |
| RU203377U1 (en) * | 2020-04-03 | 2021-04-01 | Федеральное государственное бюджетное образовательное учреждение высшего образования "Саратовский государственный технический университет имени Гагарина Ю.А." (СГТУ имени Гагарина Ю.А.) | Diffusion welding device |
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