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JPH0242777B2 - - Google Patents
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JPH0242777B2 - - Google Patents

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Publication number
JPH0242777B2
JPH0242777B2 JP31602886A JP31602886A JPH0242777B2 JP H0242777 B2 JPH0242777 B2 JP H0242777B2 JP 31602886 A JP31602886 A JP 31602886A JP 31602886 A JP31602886 A JP 31602886A JP H0242777 B2 JPH0242777 B2 JP H0242777B2
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JP
Japan
Prior art keywords
chamber
substance
pressure
temperature
glass
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.)
Expired
Application number
JP31602886A
Other languages
Japanese (ja)
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JPS62235222A (en
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed filed Critical
Publication of JPS62235222A publication Critical patent/JPS62235222A/en
Publication of JPH0242777B2 publication Critical patent/JPH0242777B2/ja
Granted legal-status Critical Current

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  • Glass Melting And Manufacturing (AREA)
  • Glass Compositions (AREA)

Description

【発明の詳现な説明】 発明の技術的分野 本発明は熔融ガラスなどの枅柄を促進するため
に倧気圧以䞋の圧力を䜿甚するこずに関するもの
である。さらに具䜓的にいえば、本発明はその皮
の枅柄技法を連続的に商業芏暡で利甚するための
実際的配眮に関するものである。
DETAILED DESCRIPTION OF THE INVENTION TECHNICAL FIELD OF THE INVENTION This invention relates to the use of subatmospheric pressures to promote the fining of molten glass and the like. More specifically, the invention relates to a practical arrangement for the continuous commercial scale use of such fining techniques.

発明の背景 ガラスの熔解においお、実質的な量のガスがバ
ツチ物質の分解の結果ずしお生成される。その他
のガスはバツチ物質によ぀お物理的に随䌎される
か、あるいは、熔融䞭のガラスの䞭ぞ燃焌熱源か
ら導入される。倧郚分のガスは熔解の初期盞䞭に
逃散するが、いくらかは熔融物䞭に捕捉されるこ
ずになる。捕捉されたガスのいくらかはガラス䞭
で溶けるが、その他の郚分は泡たたは「皮子」ず
しお知られる別々のガス状物包含物を圢成する
が、これらは生成物ガラス䞭で䞍圓に高い濃床に
攟眮される堎合には障害ずなる。これらのガス包
含物は衚面ぞ䞊り、「枅柄」ずしお知られるガラ
ス補造操䜜の段階においお十分な時間が䞎えられ
るず、溶融䜓から逃散する。熔融䜓の粘床を䞋
げ、気泡盎埄を拡倧させるこずによ぀おガス状包
含物の䞊昇ず逃散を促進するために、枅柄垯域䞭
で高枩が慣甚的に䞎えられる。枅柄段階においお
甚いる高枩に必芁ずされる゚ネルギヌ、およびガ
ス状包含物が熔融䜓から逃げ出す十分な時間を䞎
えるの必芁ずされる倧きい熔解槜はガラス補造䜜
業の䞻芁な出費である。埓぀お、枅柄工皋を改善
しおこれらのコストを軜枛するこずは望たしいこ
ずである。
BACKGROUND OF THE INVENTION In the melting of glass, substantial amounts of gas are produced as a result of the decomposition of batch materials. Other gases are either physically entrained by the batch material or introduced into the glass during melting from a combustion heat source. Most of the gas will escape during the initial phase of melting, but some will become trapped in the melt. Some of the trapped gas dissolves in the glass, while other parts form discrete gaseous inclusions known as bubbles or "seeds" that are left in unduly high concentrations in the product glass. If this happens, it becomes a hindrance. These gas inclusions rise to the surface and, given sufficient time, escape from the melt in a step of the glass manufacturing operation known as "fining." Elevated temperatures are conventionally applied in the fining zone to reduce the viscosity of the melt and promote the rise and escape of gaseous inclusions by enlarging the cell diameter. The energy required for the high temperatures used in the fining stage and the large melting vessels required to allow sufficient time for gaseous inclusions to escape the melt are major expenses in glass manufacturing operations. Therefore, it would be desirable to improve the fining process to reduce these costs.

枛圧が、溶解ガスの熔融物䞊の分圧を䞋げるこ
ずによ぀お枅柄工皋を助け埗るこずは知られおき
た。たた、圧力を䞋げるこずが熔融物内での泡の
容積を増加しおそれらが衚面ぞ䞊昇するのを早め
るようになる。慣甚的枅柄宀の芏暡においおその
䞭で真空を匕くように気密槜を提䟛するこずの非
実際性は、米囜特蚱No.15642352781411
28772803338694および3442622においお開瀺さ
れおいるような、比范的小芏暡のバツチ操䜜に真
空枅柄を䜿甚するこずに限定しおきた。
It has been known that reduced pressure can aid the fining process by lowering the partial pressure of dissolved gases above the melt. Reducing the pressure will also increase the volume of bubbles within the melt, causing them to rise to the surface faster. The impracticality of providing an airtight vessel to draw a vacuum therein on the scale of a conventional clarification chamber is illustrated in U.S. Pat. No. 1,564,235;
2877280; 3338694 and 3442622, the use of vacuum fining has been limited to relatively small scale batch operations.

連続匏真空枅柄方法が提唱されおきたが、しか
し、倧芏暡で連続的のガラス補造には各皮の欠点
のために容認されおいなか぀た。米囜特蚱No.
8051391589308および3519412においお瀺され
る連続匏真空枅柄装眮においおは、䞻芁な欠点は
圧力差によ぀お、真空垯の䞭ぞ通じか぀それから
通ずる比范的狭い垂盎方向通路を必芁ずするこず
である。これらの通路はその皮の槜の構築を特に
気密壁の必芁性から芋お耇雑化し、汚染性耐可物
接觊ぞの抌出物の露出を増し、そしお、抌出物の
流れに察しお著しく粘い抵抗を付䞎する。
Continuous vacuum fining processes have been proposed, but have not been accepted for large scale, continuous glass production due to various drawbacks. US Patent No.
In the continuous vacuum clarifiers shown in 805139; 1589308; and 3519412, the major drawback is the need for relatively narrow vertical passages into and out of the vacuum zone due to the pressure differential. These passageways complicate the construction of such vessels, especially in view of the need for airtight walls, increase the exposure of the extrudate to contaminant resistant contact, and are significantly viscous to extrudate flow. Add resistance.

䞭皋床の真空でも釣合いを取るのに実質的なガ
ラスの高さが必芁ずされるこずが認められる。そ
の皮の系の生産量の倉曎も、特に粘い抗力の因子
から考えお問題である。生産速床の䌞瞮性は぀く
られ぀぀ある補品の倉曎厚さ、幅および望た
れる生産速床に及がす経枈的芁因のために、連続
匏商業的䜜甚においお重芁である。䞊蚘の䞉぀の
特蚱の各々においおは、真空垯の通路を通る流れ
の速床を増すための駆動力は、真空垯から䞋流の
熔融物の深さず盞察的な真空垯䞊流の熔融物の深
さを増すこずによ぀お提䟛されるこずができる。
この氎準差の倧きさはこれらの系においお固有の
粘皠抵抗によ぀おさらに倧きくされる。熔融物の
衚面の高さにおいお偎壁の促進された゚ロヌゞペ
ンがおこるので、氎準を著しく倉えるこずぱロ
ヌゞペンを悪化させ、これはこんどは補品ガラス
の品質を悪化させる。
It is recognized that substantial glass height is required to balance even moderate vacuums. Changing the production rate of such systems is also problematic, especially in view of the viscous drag factor. Production rate flexibility is important in continuous commercial operations due to variations in the product being made (thickness, width) and economic factors that influence the desired production rate. In each of the three patents mentioned above, the driving force for increasing the velocity of flow through the vacuum zone passage is determined by the depth of the melt upstream of the vacuum zone relative to the depth of the melt downstream from the vacuum zone. It can be provided by increasing.
The magnitude of this level difference is further increased by the inherent viscous resistance in these systems. Since accelerated erosion of the side walls occurs at the level of the melt surface, a significant change in the level worsens the erosion, which in turn deteriorates the quality of the product glass.

より単玔な構造は米囜特蚱No.3429684に瀺され
おおり、その䞭では、バツチ物質は真空ロツク
lockを通しお䟛絊され、垂盎に现長い真空宀
の頂郚においお熔解される。その装眮においお生
産量を倉えるこずは宀䞭に課せられる真空量を倉
えるこずを必芁ずするように芋え、これは枅柄達
成床を䞍利に倉えるものである。真空宀内で原料
物質を熔解するこずは、いく぀かの理由でその装
眮のもう䞀぀の欠点である。第䞀に、真空䞋で原
料物質の初期分解を実斜するこずにより倧容積の
発泡䜓が圢成され、これはその溌泡䜓を収容する
十分な倧きさの槜を必隣ずする。第二に、原料物
質が生産物の流ぞの短絡路に埓぀お行くかもしれ
ず、埓぀お適切な熔解ず枅柄を無効にしおした
う。第䞉には、真空槜内で熔解の初期段階を実斜
し、枅柄枩床ぞ熔融物を加熱するこずは、槜内で
溶融物ぞ䟛絊されるべき倧量の熱を必芁ずする。
槜ぞそのような倧きな熱を投入するこずは壁の゚
ロヌゞペンを増す熔融物内の察流を誘起し、枅柄
された生成物の流れの汚染に連がる。第四に、バ
ツチ炭酞塩の分解から攟出される二酞化炭玠は槜
内で二酞化炭玠の比范的高い分圧を぀くり出し、
それによ぀お枛圧が熔融物から二酞化炭玠を陀く
胜力を少くずも䞀郚を打消す。
A simpler structure is shown in US Pat. No. 3,429,684, in which batch material is fed through a vacuum lock and melted at the top of a vertically elongated vacuum chamber. Changing the production rate in that equipment appears to require changing the amount of vacuum imposed in the chamber, which adversely changes the fining performance. Melting the raw material within the vacuum chamber is another drawback of the device for several reasons. First, a large volume of foam is formed by carrying out the initial decomposition of the raw material under vacuum, which requires an adjoining tank of sufficient size to accommodate the foam. Second, feed material may follow a shortcut path into the product stream, thus negating proper melting and clarification. Thirdly, carrying out the initial stages of melting in a vacuum vessel and heating the melt to the fining temperature requires a large amount of heat to be supplied to the melt in the vessel.
Inputting such high heat into the vessel induces convection within the melt which increases wall erosion and leads to contamination of the clarified product stream. Fourth, the carbon dioxide released from the decomposition of the batch carbonate creates a relatively high partial pressure of carbon dioxide in the tank;
This at least partially negates the ability of the reduced pressure to remove carbon dioxide from the melt.

米囜特蚱No.4195982は、はじめにガラスを昇圧
䞋で溶融し、次にそのガラスをより䜎圧で別の宀
の䞭で枅柄するこずを開瀺しおいる。䞡方の宀が
加熱される。
US Pat. No. 4,195,982 discloses first melting the glass under elevated pressure and then refining the glass in a separate chamber at lower pressure. Both chambers are heated.

米囜特蚱No.4110098はわざずガラスを発泡させ
枅柄を助ける方法を開瀺しおいる。その発泡は匷
い加熱ず倧気圧での化孊的発泡剀ずによ぀お誘起
される。
US Patent No. 4110098 discloses a method of intentionally foaming glass to aid in fining. The foaming is induced by intense heating and chemical blowing agents at atmospheric pressure.

発明の芁玄 本発明においおは、埓来技術の欠陥を有利にか
぀経枈的に克服する方匏で真空枅柄を商業的芏暡
の連続匏ガラス補造方法においお甚いる方法ず装
眮が提䟛される。熔融に必芁ずされる熱゚ネルギ
ヌの倧郚分が熔融物ぞ䞎えられお真空宀内に含た
れる熔融物質ぞ熱゚ネルギヌがほずんどたたは党
く䟛絊される必芁がないようにされたのちに、熔
融状ガラスが真空枅柄宀ぞ入れられる。奜たしく
は、槜壁を通る劂損倱を補償するのに必芁である
以䞊の熱は真空段階においお付加されない。十分
に高い生産速床においおは、真空宀は入぀おくる
熔融ガラス自䜓以倖によ぀おは完党に加熱される
こずがない。本発明の具䜓化においおは、バツチ
物質は工皋のその段階に特定的に適合させた段階
においおたず液化させ、その液化物質を第二段階
ぞ移し、そこで固䜓粒子の溶解が本質䞊完了し、
か぀物質の枩床が枅柄に適する粘床を䞎える枩床
ぞ䞊げられる。次に、熔融物質を真空宀ぞ送る。
その結果、溶解のガス状生成物の倧郚分は物質が
真空にかけられる前に駆逐され、最倧ガス発生の
領域は枅柄垯から分離され、それによ぀お、初期
溶解段階を斜こされる物質が枅柄を行な぀おいる
溶融物の郚分ず混合するようになり埗ない。熔解
に必芁な熱の倧郚分たたは党郚は物質が真空枅柄
段階に入る前に満たされ、枅柄段階の加熱は実質
的にさけるこずができるので、枅柄垯域䞭の熔融
䜓の過床の察流がさけられる。
SUMMARY OF THE INVENTION In the present invention, there is provided a method and apparatus for using vacuum fining in a commercial scale continuous glass manufacturing process in a manner that advantageously and economically overcomes the deficiencies of the prior art. The molten glass is exposed to a vacuum after most of the thermal energy required for melting has been imparted to the melt so that little or no thermal energy needs to be supplied to the molten material contained within the vacuum chamber. You will be placed in the clearing room. Preferably, no more heat is added in the vacuum stage than is necessary to compensate for losses through the vessel walls. At sufficiently high production rates, the vacuum chamber is not completely heated by anything other than the incoming molten glass itself. In an embodiment of the invention, the batch material is first liquefied in a stage specifically adapted to that stage of the process, and the liquefied material is transferred to a second stage where dissolution of the solid particles is essentially complete;
and the temperature of the material is raised to a temperature that provides a viscosity suitable for clarification. The molten material is then sent to a vacuum chamber.
As a result, most of the gaseous products of dissolution are expelled before the material is subjected to vacuum, and the region of maximum gas evolution is separated from the fining zone, whereby the material subjected to the initial dissolution step is clarified. It cannot become mixed with the part of the melt undergoing the process. Most or all of the heat required for melting is met before the material enters the vacuum fining stage, and heating of the fining stage can be substantially avoided, thereby avoiding excessive convection of the melt in the fining zone. .

その結果、槜の䟵蝕が枛り、溶融物の䞍完党枅
柄化郚分により枅柄化された郚分ず混じるように
なる確率が枛少する。
As a result, erosion of the vessel is reduced and the probability that partially clarified portions of the melt become mixed with clarified portions is reduced.

真空によ぀お枅柄工皋ぞ提䟛される揎助はより
䜎枩を枅柄に䜿甚するこずを可胜にする。より䜎
枩であるこずは䜎゚ネルギヌ消費にず぀おのみな
らず、槜に及がす腐蝕効果のためにも利甚があ
る。1540℃2800〓の皋床のピヌク枩床におい
お普通に枅柄されたガラスは、䜿甚する真空氎準
に応じお、玄1430℃2600〓、さらには1370℃
2500〓たたはそれ以䞋より高くない枩床にお
いお同皋床に枅柄するこずができる。
The assistance provided to the fining process by vacuum allows lower temperatures to be used for fining. Lower temperatures have utility not only for lower energy consumption but also for corrosive effects on the bath. Normally fined glass at peak temperatures on the order of 1540°C (2800〓) can reach temperatures around 1430°C (2600〓) or even 1370°C, depending on the vacuum level used.
(2500〓) or lower.

真空枅柄宀䞭での発泡䜓の発生が溶融䜓からの
ガスの陀去を著しく増進するこずが理論づけられ
る。発泡䜓によ぀お提䟛される薄膜ず倧きい衚面
積は䜎圧条件ぞの露出を増し、液盞からのガスの
茞送を促進する。このこずは慣甚的枅柄ず察照的
であり、その堎合には、独立気泡を衚面ぞ浮き䞊
らせ粘皠熔融物から逃がす滞溜時間が䞎えられね
ばならず、これは倧きい熔融物プヌルを保持する
こずが必芁ずなる。このように、本発明の真空枅
柄はかなりせたい空間の䞭で䞎えられた皋床の枅
柄を達成するこずができる。本発明の奜たしい具
䜓化においおは、発泡溶融䜓を真空ぞ露出するこ
ずの有利な効果は、物質が真空槜に入るずき、そ
れが真空槜䞭で保持されおいる熔融物質の本䜓に
入る前、そしお、奜たしくは入぀おゆく流れが発
泡䜓局の䞭に䟵入する前に、物質を発泡させるこ
ずによ぀お増進される。
It is theorized that foam generation in the vacuum clarification chamber significantly enhances gas removal from the melt. The thin film and large surface area provided by the foam increases exposure to low pressure conditions and facilitates gas transport from the liquid phase. This is in contrast to conventional fining, in which residence time must be allowed to allow the closed cells to rise to the surface and escape from the viscous melt, which retains a large melt pool. It is necessary to do so. Thus, the vacuum fining of the present invention can achieve a given degree of fining in a fairly small space. In a preferred embodiment of the invention, the advantageous effect of exposing the foamed melt to vacuum is that when the material enters the vacuum chamber, before it enters the body of molten material held in the vacuum chamber, The incoming flow is then preferably enhanced by foaming the material before penetrating into the foam layer.

本発明のもう䞀぀の面は連続匏枅柄操䜜におい
お生産量を制埡する利点に関係する。液状化物質
をバルブ手段を通しお真空宀の䞊端の䞭ぞ蚈量
し、枅柄化熔融物は別のバルブ装眮を通しお真空
宀の䞋端から送られる。真空宀内で保たれる液の
高さは、熔融物が重力によ぀お取出口から流れる
こずができるように、真空を釣合わせるのに必芁
ずする高さより少くずもわずかに倧きい。たた、
抜出しに必芁ずする最小倀より倧きい液の高さを
提䟛するこずにより、生産速床は宀䞭の真空圧を
倉えるこずなく、か぀、宀䞭の液氎準を倉えるこ
ずなく、バルブによ぀お制埡するこずができる。
逆に、真空圧のある範囲は生産速床を倉えるこず
なく䜿甚できる。バルブずは別に、この系には通
過する熔融物質の流れに察する比范的䜎い抵抗が
䞎えられおいる。
Another aspect of the invention relates to the benefits of controlling production in continuous fining operations. The liquefied material is metered into the upper end of the vacuum chamber through valve means and the clarified melt is conveyed from the lower end of the vacuum chamber through another valve arrangement. The height of the liquid maintained within the vacuum chamber is at least slightly greater than the height required to balance the vacuum so that the melt can flow out of the outlet by gravity. Also,
By providing a liquid height greater than the minimum required for withdrawal, the production rate is controlled by the valve without changing the vacuum pressure in the chamber and without changing the liquid level in the chamber. be able to.
Conversely, a range of vacuum pressures can be used without changing production rates. Apart from the valve, the system is provided with a relatively low resistance to the flow of molten material therethrough.

生産量が本発明の䞎えられた蚭備においお可倉
であるだけでなく、その有効性は、䜎容積の応甚
には有効に䜜動しない慣甚のタンク型埪還枅柄槜
ずちが぀お、系の芏暡ずは比范的独立的である。
それゆえ、本発明は広い範囲のガラス補造操䜜ぞ
有効に応甚できる。
Not only is the production rate variable in a given installation of the present invention, but its effectiveness also varies with the size of the system, unlike conventional tank-type recirculating clarifiers, which do not operate effectively in low volume applications. are relatively independent.
Therefore, the present invention can be effectively applied to a wide range of glass manufacturing operations.

真空枅柄宀の奜たしい圢態は垂盎方向に现長い
槜であり、最も䟿利なのは、瞊型円筒の圢状にあ
る。液状化物質はその槜の䞭で保持される熔融物
質の䞊方の頭郚空間の䞭ぞ導入される。その頭郚
空間䞭で枛圧に出䌚うず、その物質の少くずも実
質的郚分が、その物質䞭にずけおいるガスの攟
出、および物質䞭に存圚する気泡ず皮子の拡倧に
基づいお、発泡する。発泡䜓の圢成は枛圧ぞ露出
される衚面積を倧いに増倧し、埓぀お液盞からの
ガス状皮の陀去を助ける。熔融状プヌルからでは
なく、槜䞭で保持される熔融状プヌルの䞊方で発
泡䜓を生成させるこずは、発泡䜓を圧挬しガスの
逃散を助けるのに有利である。たた、新たに発生
された発泡䜓を発泡䜓局䞊に沈積させるこずはそ
の発泡䜓の圧挬を促進するこずも発芋された。垂
盎匏に现長い幟䜕圢状の別の利点は、䞊方端にお
いお残留する密床の䜎い気泡䜓たたは泡を含む物
質のために成局化がおこり、埓぀お、総䜓的の物
質移送は気泡䜓領域から離れおおり、それによ぀
お、未枅柄化物質が生成物の流れの䞭ぞ含たれる
ようになるこずがおこりそうもないようにさせる
こずである。枛圧䞋での熔融物からのガスの远い
出しは熔融物䞭の溶解ガス濃床を倧気圧でのそれ
らの飜和点以䞋ぞ䞋げる。熔融状物質が底の取出
口ぞ向けお䞋向きに進むに぀れお、槜䞭の熔融物
の深さに基づく増加圧が溶液䞭に残留ガスを残留
させか぀残留しおいるかもしれない小皮子の容積
を枛少させる。ガスの溶解はたた、物質が取出口
の方ぞ進むに぀れお枩床を䜎䞋させるこずによ぀
お助けられるかもしれない。その䞊、真空枅柄埌
に残留するガスの䜎濃床は、慣甚的枅柄に関する
問題でしばしばあるずおり、ガラス補造方法のそ
の埌の段階における気泡栞化の確率を小さくす
る。
The preferred form of the vacuum clarification chamber is a vertically elongated vessel, most conveniently in the form of a vertical cylinder. The liquefied material is introduced into the head space above the molten material held in the vessel. Upon encountering reduced pressure in the headspace, at least a substantial portion of the material foams due to the release of gases dissolved in the material and the expansion of air bubbles and seeds present in the material. Formation of the foam greatly increases the surface area exposed to reduced pressure, thus aiding in the removal of gaseous species from the liquid phase. Producing the foam above the molten pool held in a bath rather than from the molten pool is advantageous to compress the foam and aid gas escape. It has also been discovered that depositing newly generated foam onto a foam layer promotes crushing of the foam. Another advantage of the vertically elongated geometry is that stratification occurs due to the remaining less dense foam or foam-containing material at the upper end, so that the overall mass transport is directed away from the foam region. and thereby make it less likely that unclarified material will become included in the product stream. Purging gases from the melt under reduced pressure reduces the dissolved gas concentrations in the melt below their saturation point at atmospheric pressure. As the molten material progresses downward toward the bottom outlet, increasing pressure based on the depth of the melt in the bath causes residual gas to remain in solution and the volume of small seeds that may remain to be reduced. reduce Gas dissolution may also be aided by reducing the temperature as the material progresses towards the outlet. Moreover, the low concentration of gas remaining after vacuum fining reduces the probability of bubble nucleation in subsequent steps of the glass manufacturing process, as is often a problem with conventional fining.

ガラス、特に゜ヌダ・石灰・シリカガラスの商
業的熔融においおは、硫酞ナトリりムたたは硫酞
カルシりムあるいはその他の硫黄源が通垞バツチ
物質の䞭に含たれお熔解および枅柄化工皋を助け
る。アンチモン、砒玠、および北玠も枅柄助剀ず
しお知られおいる。熔融物䞭の硫黄のような枅柄
助剀の存圚は、倧容積の気泡䜓が誘起されるた
め、および真空枅柄槜のセラミツク耐火壁ぞの䟵
蝕のために、真空枅柄に関する䞀぀の問題である
こずが発芋された。しかしこれたでは、ガラスの
効果的な熔解ず枅柄は枅柄助剀なしでは達成が困
難であ぀た。本発明のさらにもう䞀぀の有利な面
は、化孊的枅柄助剀をほずんどたたは党く䜿甚し
ないで高氎準品質たでガラスを熔解および枅柄化
し埗るこずである。これは、熔解ず枅柄の工皋が
別々の段階で実斜され、それによ぀お、化孊的枅
柄助剀の䜿甚を最少化するか回避するよう適合さ
せた方法によ぀お各段階を実斜し埗るので、本発
明においお可胜性がある。䞀般的には、化孊的枅
柄助剀が熔融物プヌル内からの気泡の集合および
䞊昇を促進する圹目をするず䞀般的に信じられる
が、しかし、その皮の機構は本発明の枅柄工皋に
おいお小圹割しか果たさないず信じられる。それ
ゆえ、品質に及がす著しい効果は枅柄助剀䜿甚量
の省略たたは実質的枛少から生ずるものではな
い。枅柄助剀の省略たたは枛少はたた環境䞭ぞの
望たしくない攟出物を枛らすために望たしい。
In the commercial melting of glass, particularly soda-lime-silica glass, sodium or calcium sulfate or other sulfur sources are usually included in the batch material to aid in the melting and clarification process. Antimony, arsenic, and fluorine are also known as refining aids. The presence of refining aids such as sulfur in the melt is a problem with vacuum fining due to the induction of large volume bubbles and erosion of the ceramic refractory walls of the vacuum fining tank. was discovered. However, heretofore, effective melting and fining of glass has been difficult to achieve without fining aids. Yet another advantageous aspect of the present invention is that glass can be melted and refined to a high level of quality with little or no chemical refining aids. This is because the melting and clarification steps are carried out in separate stages, whereby each stage can be carried out in a manner adapted to minimize or avoid the use of chemical clarification aids. Possible in the present invention. It is generally believed that chemical fining aids serve to promote the collection and rise of air bubbles from within the melt pool; however, such mechanisms play a minor role in the fining process of the present invention. I believe that I can only accomplish this. Therefore, no significant effect on quality results from the omission or substantial reduction in the amount of refining aid used. Omission or reduction of clarification aids is also desirable to reduce undesirable emissions into the environment.

板ガラス補造のフロヌト法においおは、ガラス
からの硫黄の枛少たたは省略は、平面圢成宀にお
ける硫化錫の、ガラス䞊面ぞの凝瞮ずしたたりに
通ずる、圢成ず蒞発によ぀おおこされる欠陥を避
けるために、远加的に利点を瀺す。硫黄ず鉄ず組
合されるずガラスに着色効果をもち、埓぀お枅柄
のために硫黄を避けるこずはある皮のガラスの色
のより粟现な調節を可胜にする。
In the float process of flat glass manufacturing, the reduction or omission of sulfur from the glass is used to avoid defects caused by formation and evaporation, leading to condensation and evaporation of tin sulfide in the flat forming chamber onto the top surface of the glass. , additionally shows advantages. Sulfur and iron when combined have a coloring effect on the glass, so avoiding sulfur for fining allows for finer control of the color of some glasses.

特に有利なのは、粉状バツチ物質を本発明の分
離された工皋段階によ぀お枅柄される前に初期流
動性段階にさせる、米囜特蚱No.4381934に開瀺さ
れおいる別個のアブレヌシペン液状化法
ablating liquifaction processを䜿甚するこ
ずである。しかし、その他の液状化技法も䜿甚で
きる。
Particularly advantageous is the separate ablating liquefaction process disclosed in U.S. Pat. liquifaction process). However, other liquefaction techniques can also be used.

詳现説明 この詳现説明はガラス溶解に特に適合させた方
法ず装眮に関連しお述べるが、本発明が他の物質
の凊理にも同じく応甚できるこずは圓然である。
DETAILED DESCRIPTION Although this detailed description is set forth in the context of a method and apparatus specifically adapted for glass melting, it will be appreciated that the invention is equally applicable to the processing of other materials.

図を参照するず、本発明の総括䜓熔解法は奜た
しくは䞉段階、すなわち、液状化段階、溶解
段階、および真空枅柄段階、から成る。
液状化段階においお熔解を開始させるのには
各皮の装眮を甚いるこずができるが、この工皋段
階を分離しそれを経枈的に実斜するための極めお
有効な配眮は米囜特蚱No.4381934に開瀺されるも
のであり、これは奜たしい液状化段階の具䜓化の
詳现を匕甚するこずによ぀お本明现曞に組入れら
れおいる。その液状化槜の基本的構造はドラム
であり、これはスチヌル補であり、䞀般的には
円筒状偎壁郚、䞀般的には開攟状の頂郚、および
攟出し甚の取出口以倖は閉じられおいる底郚をも
぀おいる。
Referring to the figure, the integrated melting process of the present invention preferably consists of three stages: a liquefaction stage 10, a dissolution stage 11, and a vacuum clarification stage 12.
Although a variety of devices can be used to initiate melting in the liquefaction stage 10, a highly effective arrangement for separating this process step and performing it economically is disclosed in U.S. Pat. No. 4,381,934. , which is incorporated herein by reference to the details of the preferred liquefaction stage implementation. The basic structure of the liquefaction tank is drum 1.
5, which is made of steel and has a generally cylindrical side wall, a generally open top, and a bottom that is closed except for the discharge outlet.

ドラムは、䟋えば、耇数個の支持茪で
回転的に支えられか぀耇数回の調節茪によ぀
お所定䜍眮に保持される、取巻き支持リング
によ぀お実質䞊垂盎の軞の呚りで回転するように
取付けられおいる。実質的に包みこたれた空掞
が、䟋えば呚瞁枠によ぀お静止支持䜓が備え
られた蓋構造によ぀お、ドラム内で圢成されおい
る。蓋は耐火炉構築技術における熟緎者にず
぀お知られおいるずおりに各皮の圢をずるこずが
できる。図に描かれおいる奜たしい配列は耇数個
の耐火性ブロツクから補䜜された䞊向きドヌム型
の曲面アヌチ構造である。䞀䜓性たたは平らな懞
垂蚭蚈を蓋に甚いるこずができる。
The drum 15 is, for example, surrounded by a surrounding support ring 16 that is rotatably supported by a plurality of support wheels 17 and held in place by a plurality of adjustment wheels 18.
is mounted for rotation about a substantially vertical axis. A substantially enclosed cavity is formed in the drum, for example by a lid structure provided with a stationary support by a peripheral frame 20. The lid 20 can take a variety of forms as known to those skilled in the art of refractory furnace construction. The preferred arrangement depicted in the figures is an upwardly domed curved arch structure fabricated from a plurality of refractory blocks. A monolithic or flat hanging design can be used for the lid.

バツチ物質を液状化するための熱は蓋を貫
通しおのびる個以䞊のバヌナヌによ぀お䞎
えられおよい。奜たしくは、耇数個のバヌナヌが
ドラム内の広い領域ぞ火焔を向けるよう蓋の呚り
に配眮される。バヌナヌは槜内の激しい環境から
守るために奜たしくは氎冷される。排気は蓋の䞭
の開口を通぀お液状化槜の内郚から逃げ出
す。有利には、排気ガス䞭の蒞熱は米囜特蚱No.
4519814に蚘茉のような予熱段階図瀺せずに
おいおバツチ物質を予熱するのに䜿぀およい。
Heat to liquefy the batch material may be provided by one or more burners 22 extending through the lid 20. Preferably, a plurality of burners are arranged around the lid to direct the flame to a large area within the drum. The burner is preferably water cooled to protect it from the harsh environment within the tank. Exhaust air escapes from the interior of the liquefaction tank through an opening 23 in the lid. Advantageously, the steam heat in the exhaust gases is disclosed in U.S. Patent No.
It may be used to preheat batch materials in a preheating step (not shown) as described in US Pat. No. 4,519,814.

バツチ物質は、粉末状態に奜たしくはあるが、
シナヌトによ぀お液状化槜の空掞の䞭ぞ䟛絊
され、シナヌトは描かれおいる具䜓化におい
おは排気開口を通しおのびおいる。䟛絊シナ
ヌト配眮の詳现は米囜特蚱No.4529428においお芋
られる。
The batch material is preferably in powdered form, but
The cavity of the liquefaction tank is fed by a chute 24, which extends through the exhaust opening 23 in the embodiment depicted. Details of the feed chute arrangement can be found in US Pat. No. 4,529,428.

バツチシナヌトはドラムの偎壁に近接
しお終り、それによ぀お、バツチ物質がドラムの
内偎偎壁䞊に沈積する。バツチ物質の局はド
ラムの回転によ぀お助けられおドラム内壁䞊
で保持され、絶瞁甚ラむニングずしお圹立぀。
The batch shoot 24 terminates close to the side wall of the drum 10, thereby depositing batch material on the inner side wall of the drum. A layer 25 of batch material is retained on the inner wall of the drum 10 with the aid of the rotation of the drum and serves as an insulating lining.

ラむニングの衚面䞊のバツチ物質は空掞内
の熱ぞ露出されるので、液状化局を圢成し、
傟斜しおいるラむニングを槜の底ぞ䞭倮抜出し開
口ぞ流れ萜ちる。その取出口にはセラミツク補ブ
ツシナが取付けられおいる。液状化物質の流れ
は液状化槜から自由に第二段階ぞ通ずる開
口を通぀お萜䞋する。この第二段階は熔解槜
ずよばれおよいが、それは、その機胜の䞀぀が液
状化槜を出る液状化流の䞭で残留するバ
ツチ物質の未熔融粒の溶解を完了させるこずであ
るからである。その䜍眮における液状化物質は代
衚的には郚分的にだけ熔融しおいお、未熔融砂粒
および実質的ガス盞を含む。炭酞塩バツチ物質ず
枅柄剀ずしおの硫酞塩を䜿甚する代衚的な゜ヌ
ダ・石灰シリカ熔融方法においおはガス盞は䞻ず
しお酞化炭玠類ず酞化硫黄類で構成される。窒玠
も捕捉空気から存圚しおもよい。
As the batch material on the surface of the lining 25 is exposed to the heat within the cavity, it forms a liquefied layer 26;
The sloping lining flows down to the bottom of the tank and into the central extraction opening. A ceramic bushing is attached to the outlet. Liquefied substance flow 2
8 falls freely from the liquefaction tank through an opening 29 leading to the second stage 11. This second stage may be referred to as a melting tank, since one of its functions is to complete the dissolution of the remaining unmelted particles of batch material in the liquefied stream 28 exiting the liquefaction tank 10. It is from. The liquefied material at that location is typically only partially molten and includes unmelted sand grains and a substantial gas phase. In a typical soda-lime-silica melting process using carbonate batch materials and sulfate as a clarifying agent, the gas phase consists primarily of carbon oxides and sulfur oxides. Nitrogen may also be present from trapped air.

溶解槜は、䞋流枅柄段階から離された䜍眮
においお滞留時間を䞎えるこずによ぀お、第䞀段
階から来る液状化物質の䞭の未熔解粒子の溶解を
完了させる機胜を果たす。゜ヌダ・石灰・シリカ
ガラスバツチは代衚的には玄1200℃2200〓の
枩床においお液化し、溶解槜に玄1200℃
2200〓から玄1320℃2400〓の枩床におい
お入り、その枩床においお残留未溶解粒子は通垞
は十分な滞留時間が䞎えられるずきに溶解するよ
うになる。図瀺の溶解槜は氎平方向に现長い
耐火性浅箱の圢にあり、耐化性屋根をも
ち、䞡端に取入口ず取出口があ぀お、適切な滞留
時間を保蚌する。溶解槜䞭の熔融物質の深さは物
質の埪還を阻止するために比范的浅い。
The dissolution tank 11 serves to complete the dissolution of unmelted particles in the liquefied material coming from the first stage by providing residence time at a location remote from the downstream clarification stage. Soda, lime, and silica glass batches are typically liquefied at a temperature of about 1200℃ (2200℃), and the melting tank 11 is heated to about 1200℃.
(2200〓) to about 1320°C (2400〓), at which temperature the remaining undissolved particles usually become soluble when given sufficient residence time. The illustrated melting vessel 11 is in the form of a horizontally elongated refractory shallow box 30 with a corrosion-resistant roof 31 and an inlet and an outlet at each end to ensure adequate residence time. The depth of the molten material in the melting tank is relatively shallow to prevent circulation of material.

実質的熱゚ネルギヌの付加は溶解段階を実斜す
るのに必芁ではないが、加熱は工皋を促進するこ
ずができ、埓぀お熔解槜の寞法を小さくす
る。さらに有意矩なこずは、埌に続く枅柄段階甚
に枩床を䞊げるように溶解段階䞭の物質を加熱す
るこずが奜たしい。枅柄甚枩床を最倧たで䞊げる
こずはガラス粘床の䜎䞋ず含たれるガスの蒞気圧
の増加のために有利である。代衚的には、玄1540
℃2800〓の枩床が゜ヌダ・石灰・シリカガラ
スの枅柄化にず぀お望たしいず考えられるが、し
かし、枅柄を助けるために真空が甚いられるずき
には、より䜎いピヌク枅柄枩床を生成物品質を犠
性にするこずなく䜿甚できる。その枩床の䞋げ埗
る量は真空床に䟝存する。それゆえ、枅柄を本発
明に埓぀お真空䞋で実斜すべきずきには、ガラス
枩床は枅柄前に、䟋えば1480℃2700〓以䞋ぞ
䞊げる必芁があり、任意的には1430℃2600〓
以䞋ぞ䞊げる必芁がある。ここで開瀺する圧力の
䜎い方の範囲を甚いるずきには、枅柄槜䞭の枩床
は13702500〓より高くないこずが必芁である。
Although the addition of substantial thermal energy is not necessary to carry out the melting step, heating can accelerate the process, thus reducing the size of the melting vessel 11. More importantly, it is preferred to heat the material during the melting stage to raise the temperature for the subsequent clarification stage. Increasing the fining temperature to a maximum is advantageous because of the reduction in glass viscosity and the increase in the vapor pressure of the gases involved. Typically, about 1540
Temperatures of 2800 °C (2800 °C) are considered desirable for clarification of soda-lime-silica glasses, but when vacuum is used to aid clarification, lower peak clarification temperatures may be sacrificed at the expense of product quality. It can be used without making any difference. The amount by which the temperature can be lowered depends on the degree of vacuum. Therefore, when fining is to be carried out in accordance with the invention under vacuum, the glass temperature must be raised before fining, for example below 1480°C (2700°), optionally up to 1430°C (2600°).
You need to raise it below. When using the lower range of pressures disclosed herein, it is necessary that the temperature in the fining tank is no higher than 1370°C (2500°C).

この皋床のピヌク枩床の䜎䞋は耐火性槜の著し
く長い寿呜ず、同時に゚ネルギヌ節枛をもたら
す。熔解槜に入る液状化物質は枅柄甚の熔融状物
質を調補するために䞭皋床にしか加熱される必芁
はない。燃焌熱源を熔解段階においお䜿甚で
きるが、しかし、この段階は電気加熱によく適合
するこずが発芋されたのであり、それによ぀お、
耇数個の電極が図に瀺すように偎壁を氎平に
貫通しお提䟛されおもよい。熱はガラスの電気熔
融に慣甚的に甚いられる技法においお、電極間を
通る電流に察する熔融䜓自身の抵抗によ぀お発生
される。
This degree of peak temperature reduction results in a significantly longer life of the refractory vessel and at the same time saves energy. The liquefied material entering the melter needs to be heated only moderately to prepare the molten material for clarification. Although a combustion heat source can be used in the melting stage 11, it has been discovered, however, that this stage is well suited for electrical heating, thereby
A plurality of electrodes 32 may be provided horizontally through the sidewalls as shown. Heat is generated by the melt's own resistance to the electrical current passed between the electrodes, in the technique commonly used for electromelting of glass.

電極は圓業熟緎者にず぀およく知られおい
る皮類の炭玠たたはモリブデンであ぀およい。
Electrode 32 may be carbon or molybdenum of a type well known to those skilled in the art.

浮滓陀去郚材が熔解槜䞭に蚭けられお取出
口端ぞ浮遊物質が近づくのを劚げる。
A scum removal member 33 is provided in the melting tank to prevent suspended solids from approaching the outlet end.

溶解段階から枅柄段階ぞの物質の流れ
のバルブ制埡は抜出し管ず軞的に䞀線に列ぶ
プランゞダヌから成る。プランゞダヌの軞
は熔解槜の屋根を突きぬけおのびお、プラ
ンゞダヌず管のギダツプを調節させ、そ
れによ぀お枅柄段階䞭ぞの物質の流速を倉調させ
る。
Valve control of the flow of material from the melting stage 11 to the clarification stage 12 consists of a plunger 35 which is axially aligned with the withdrawal tube 36. Plunger shaft 3
7 extends through the melter roof 31 to adjust the gap between plunger 35 and tube 36, thereby modulating the flow rate of material into the fining stage.

バルブ装眮が奜たしいけれども、その他の手段
を圓業においお既知のずおり、枅柄段階ぞの熔融
物質の流速を制埡するために䞎えられる。䞀぀の
䟋は、通過する熔融状物質の粘床、埓぀お流速を
倉調するよう、抜出し管ず関連する加熱および
冷华手段を䜿甚するこずである。
Although a valve arrangement is preferred, other means are provided for controlling the flow rate of molten material to the fining stage, as is known in the art. One example is the heating and/or
by using cooling means.

枅柄段階は奜たしくは垂盎の盎立槜でら成
り、䞀般的には円筒状の圢態であ぀お、気密氎冷
ケヌシング䞭に包たれた内郚セラミツク耐火物ラ
むニングをも぀おいる。その耐火物は圓業で
よく知られおいるアルミナ・ゞルコニア・シリカ
のタむプのものであ぀およい。ケヌシングは二重
壁円筒状偎壁郚材で間に環状の氎通路をも぀
郚材ず、円圢の端未冷华噚および、ずを
含む。断熱局図瀺せずを耐火物ず偎壁
ずの間に備えおもよい。バルブ管は癜金の
ような耐火性金属で぀く぀おもよく、枅柄槜の䞊
端においおオリフむスの䞭ぞ気密的にはめこ
たれる。
The fining stage 12 preferably consists of a vertical upright vessel, generally cylindrical in form and having an internal ceramic refractory lining 40 enclosed in an airtight water-cooled casing. The refractory may be of the alumina-zirconia-silica type well known in the art. The casing includes a double-walled cylindrical side wall member 41 with an annular water passage therebetween, and circular end uncoolers 42 and 43. A heat insulating layer (not shown) is connected to the refractory 40 and the side wall 4.
It may be provided between 1 and 1. Valve tube 36 may be made of a refractory metal, such as platinum, and is hermetically fitted into orifice 44 at the upper end of the clarifier.

熔融状物質が管を通過し枅柄槜内の枛圧に
出䌚うに぀れお、熔融物䞭に含たれるガスは容積
が膚脹し、液䜓本䜓䞊に静眮す気泡䜓局
を぀くり出す。発泡䜓は厩壊するず、液䜓の本䜓
の䞭に組蟌たれる。倧気圧以䞋の圧力を枅柄
槜内で槜の䞊郚を貫通しおのびおいる真空導管
を通しお確立させるこずができる。ここで甚い
るずき、「発泡䜓」は熔融状物質の容積の少くず
も倍を特城ずするものず考えられるこずができ
る。物質が十分に発泡化するず、その容積増は
倍よりはるかに倧きい。熔融状物質を発泡䜓の薄
い膜ずしお分配するこずは枛圧ぞ露出される衚面
積を倧いに増倧する。それゆえ、発泡効果を最倧
にするこずが奜たしい。発泡䜓は液䜓䞊方の䞊郚
空間䞭の槜頂郚においお存圚する系䞭の最䜎圧ぞ
露出されるこずがたた奜たしく、埓぀お、新たに
導入され発泡させる物質を発泡䜓局頂郚䞊の䞊郚
空間䞭を萜䞋させるこずによ぀お、露出は改善さ
れる。たた、発泡䜓䞋の液䜓プヌルの衚面から発
泡䜓を぀くらせるよりは発泡䜓局頂郚䞊に新たに
発泡した物質を沈積させるこずが、槜䞭の物質移
送ずより䞡量性がある。真空空間䞭の圧力ず枅柄
槜に入る熔融物質の容積流速ずに応じお、入぀お
くる流れは䞀般的には凝集状の液䜓の流れずしお
発泡䜓局䞭ぞ䟵入し、それによ぀お発泡がプヌル
の衚面からおこるか、あるいは、流れが枛圧
にふれるず盎ちに発泡をおこすか、のいずれかで
ある。いずれの様匏も䜿甚できるが、䞊述の理由
から、埌者の様匏がより有効であるこずが発芋さ
れた。
As the molten material passes through the tube 36 and encounters the reduced pressure within the fining vessel, the gas contained in the melt expands in volume and forms a layer of foam 50 that rests on the body of liquid 51.
Create. When the foam collapses, it becomes incorporated into the body 51 of liquid. A vacuum conduit 5 extending through the top of the clarification tank to maintain pressure below atmospheric pressure
It can be established through 2. As used herein, a "foam" can be considered to be characterized by at least twice the volume of the molten material. When a substance is sufficiently foamed, its volume increases by 2
Much larger than double. Distributing the molten material as a thin film of foam greatly increases the surface area exposed to reduced pressure. Therefore, it is preferable to maximize the foaming effect. It is also preferred that the foam is exposed to the lowest pressure in the system, which is present at the top of the vessel in the headspace above the liquid, so that the newly introduced material to be foamed is passed through the headspace above the top of the foam layer. Exposure is improved by dropping. Also, depositing freshly foamed material on top of the foam layer is more compatible with material transfer within the bath than having foam formed from the surface of a liquid pool below the foam. Depending on the pressure in the vacuum space and the volumetric flow rate of the molten material entering the clarification tank, the incoming flow generally penetrates into the foam layer as a cohesive liquid stream, thereby causing the foam to pool. Either foaming occurs from the surface of 51, or foaming occurs immediately when the flow is exposed to reduced pressure. Although either format can be used, the latter format has been found to be more effective for the reasons discussed above.

枅柄槜に入る熔融状抌出物質の熱含量は槜
内の適圓枩床が維持するのに十分なものであるこ
ずができるが、しかし、䜎枩出速床においおは、
壁を通る゚ネルギヌ損倱が溶融状物質によ぀お槜
の䞭ぞ゚ネルギヌが移送される速床をこえるかも
しれない。そのような堎合には、䞍適切な枩床を
避けるために枅柄槜内で加熱を提䟛するこずが望
たしいかもしれない。
The heat content of the molten extrudate entering fining vessel 12 may be sufficient to maintain a suitable temperature within the vessel, but at low exit rates,
Energy losses through the walls may exceed the rate at which energy is transferred into the vessel by the molten material. In such cases, it may be desirable to provide heating within the fining tank to avoid inappropriate temperatures.

その加熱量は比范的少量であるこずができ、な
ぜならばその目的が壁を貫通する熱損倱を補うた
めだけであるからであり、そしお、慣甚的な電気
加熱装眮によ぀お実斜するこずができ、その際、
電極が偎壁から攟射方向に貫いおのび、電流がガ
ラス䞭を電極間で流れる。
The amount of heating can be relatively small, since its purpose is only to compensate for heat loss through the wall, and can be carried out by conventional electrical heating equipment. ,that time,
Electrodes extend radially through the sidewalls and current flows between the electrodes through the glass.

抌出速床ず関係なく、槜䞭の溶融状本䜓䞊
方の空間は、溶融状塊が存圚しないこずおよび熔
融状物質からの茻射が発泡䜓局によ぀お遮断
されるこずのために、垌望枩床より䜎くなる傟向
がある。その結果、発泡局の䞊郚は比范的䜎枩ず
なるこずができ、このこずは、発泡䜓の粘床を増
しガスが远出される速床をおそくするこずにな
る。その堎合、液䜓ず発泡䜓の䞊方空間を加熱す
る手段を提䟛するこずが有利であるこずが発芋さ
れた。この目的に察しおは、バヌナヌを提䟛
し燃焌を真空空間内で維持するこずが可胜である
こずがわか぀たが、これは米囜特蚱No.4704153
1986幎月12日付米囜特蚱原S.No.895647の䞻
題である。
Regardless of the extrusion speed, the space above the molten body in vessel 12 is at the desired temperature due to the absence of molten mass and radiation from the molten material being blocked by foam layer 50. tends to be lower. As a result, the top of the foam layer can be relatively cold, which increases the viscosity of the foam and slows the rate at which gas is expelled. In that case it has been found advantageous to provide means for heating the space above the liquid and foam. For this purpose, it has been found possible to provide a burner 53 and maintain combustion in a vacuum space, as described in US Pat. No. 4,704,153.
(U.S. Patent Original S. No. 895647 dated August 12, 1986).

導管は真空槜䞊郚端においお提䟛し、それ
によ぀お少量の氎を呚期的に発泡䜓䞊ぞスプレヌ
しおもよい。氎のスプレヌは発泡䜓が厩壊するの
を助けるこずが発芋されたが、これはもう䞀぀の
米囜特蚱No.47948601986幎月日付米囜特蚱願
S.No.882647埌に1987幎月29日付米囜特蚱願S.
No.102227で眮き換られた。 描かれおいる具䜓化においおは、枅柄された熔
融状物質は枅柄槜の底から癜金のような耐火
性金属の抜出し管によ぀お抜出される。槜の
偎壁䞭に底郚領域内に抜出し口を配眮するこずも
できる。抜出し管は耐火性底郚郚分の衚
面をこえおのびるこずが奜たしく、その内郚に抜
出し管が抌出流の䞭に屑が入るのを劚げるよう取
付けられおいる。底郚郚分には管に接し
お厚さの薄い郚分が蚭けられ、管䞊の断熱効果を
䞋げるようにな぀おいお、それにより、管の枩床
を管内での物質の凝固を劚げるように䞊げさせ
る。管の呚りの掩れは底郚郚分の䞋で氎冷华
噚によ぀お劚げられる。抜出し管からの
熔融状物質の流速はステムの端で支持される
円維状絞り郚材によ぀お制埡される。ステム
は機械的手段図瀺せずず関連しお、絞り
郚材の高さを調節し、埓぀お絞り郚材ず管
ずの間の間隙をそこからの流速を制埡するよう
に調節する。枅柄された物質の熔融状の流れ
は枅柄槜の底から自由に萜䞋し、所望補品ぞ賊圢
される成圢台図瀺せずぞ送られおよい。枅柄
ガラスは䟋えば、フロヌトガラス成圢宀ぞ送り、
そこで熔融ガラスが熔融金属プヌル䞊で浮かせ板
ガラスを圢成させおよい。
A conduit 54 may be provided at the upper end of the vacuum chamber by which small amounts of water may be periodically sprayed onto the foam. It has been discovered that a spray of water helps the foam break down, which is another U.S. patent application filed July 7, 1986, U.S. Patent No. 4,794,860.
S. No. 882647 (later U.S. patent application S. No. 882647 dated September 29, 1987).
Replaced by No.102227. )) In the embodiment depicted, the clarified molten material is withdrawn from the bottom of the fining tank 12 by a withdrawal tube 55 of a refractory metal such as platinum. It is also possible to arrange the outlet in the bottom region in the side wall of the vessel. The withdrawal tube 55 preferably extends beyond the surface of the refractory bottom portion 56, within which the withdrawal tube is mounted to prevent debris from entering the extrusion stream. The bottom portion 56 is provided with a reduced thickness portion adjacent to the tube 55 to reduce the insulation effect on the tube, thereby increasing the temperature of the tube to prevent solidification of material within the tube. let Leakage around the tubes is blocked by a water cooler 57 below the bottom part 56. The flow rate of the molten material from the withdrawal tube 55 is controlled by a fibrous restrictor 58 supported at the end of the stem 59. Stem 59, in conjunction with mechanical means (not shown), adjusts the height of throttle member 58 and thus adjusts the height of throttle member 58 and tube 5.
5 is adjusted to control the flow rate therefrom. Molten stream of clarified material 60
may fall freely from the bottom of the fining tank and be delivered to a forming station (not shown) where it is shaped into the desired product. For example, clear glass is sent to a float glass forming room,
The molten glass may then be suspended above the molten metal pool to form a glass plate.

各皮の圢状を採甚できるが、枅柄槜は、そ
の圢態が円筒状であるこずが奜たしい。円筒圢は
気密槜を構築するために有利である。内郚衚面接
觊面積察容積の比はたた円圢断面で以お最小化さ
れる。慣甚の開攟炉型の埪環枅柄槜ず比范しお、
耐火性接觊面積の䜕分の䞀かだけが本発明の円筒
状真空枅柄槜によ぀お必芁ずされる。
Although various shapes can be adopted, it is preferable that the clarifying tank 12 has a cylindrical shape. The cylindrical shape is advantageous for constructing an airtight tank. The internal surface contact area to volume ratio is also minimized with a circular cross section. Compared to the conventional open furnace type circulation clarifier,
Only a fraction of the refractory contact area is required by the cylindrical vacuum fining vessel of the present invention.

枅柄槜䞭で保持される溶融物質の高さ
は宀䞭で課せられる真空氎準によ぀お指什され
る。液䜓の高さに基づく圧力頭は取出口においお
倧気圧に等しいかをより倧きい圧力を確立し、物
質を槜から自由に取出させるのに十分なものでな
ければならない。その高さは熔融物質の比重に䟝
存し、それは゜ヌダ・石灰・シリカガラスに぀い
おは枅柄段階の枩床においお玄2.3である。真空
を補償するのに必芁である最䜎倀をこえる高さ
は、倧気圧の倉動を考慮し、真空の倉動を蚱し、
取出し口を通る定垞流を保蚌するために望たれ
る。取出し口を通る流れが底郚バルブ手段なしで
調節されるような条件を維持するこずができる。
しかし本発明の奜たしい具䜓化においおは、取出
し口流速が真空圧力によ぀お決定されるこずがな
く、むしろ機械的バルブ手段、すなわち、絞り郚
材によ぀お決定されるよう、実質的に過倧の
高さが提䟛される。そのような配眮は生産速床ず
真空圧力ずが互に独立に倉えられるこずを可胜に
する。あるいはたた、取出口に圧力差に打勝぀ポ
ンプ手段が蚭けられる堎合には、取出し口での圧
力が倧気圧以䞋であるこずができる。
The height of the molten material 51 held in the clarification tank 12 is dictated by the vacuum level imposed in the chamber. The pressure head based on the height of the liquid must be sufficient to establish a pressure equal to or greater than atmospheric pressure at the outlet and to allow the material to be freely removed from the vessel. Its height depends on the specific gravity of the molten material, which for soda-lime-silica glass is about 2.3 at the temperature of the fining stage. The height above the minimum value required to compensate for the vacuum takes into account fluctuations in atmospheric pressure, allows fluctuations in the vacuum,
Desired to ensure steady flow through the outlet. Conditions can be maintained such that the flow through the outlet is regulated without bottom valve means.
However, in a preferred embodiment of the invention, a substantially oversized Height provided. Such an arrangement allows production rate and vacuum pressure to be varied independently of each other. Alternatively, the pressure at the outlet can be below atmospheric pressure if the outlet is provided with pumping means to overcome the pressure difference.

熔融ガラスに関しお䜿甚するこずを考えたポン
プの䟋は米囜特蚱No.4083711に開瀺されおおり、
その開瀺は文献ずしおここに匕甚されおいる。
An example of a pump intended for use with molten glass is disclosed in U.S. Pat. No. 4,083,711;
The disclosure is incorporated herein by reference.

槜の圧力平衡化機胜はその幅に無関係であ
り、埓぀お、槜は理論的には、狭い垂盎パむプの
圢にあるこずができる。しかし、比范的広い槜が
ガス再吞収を可胜にする滞留時間のため、流れ抵
抗を枛らすため、および、熱を槜䞋郚の䞭ぞ補助
加熱源を必芁ずするこずなく分配するために、奜
たしい。これらの目的に察しお、察より倧き
くない高さ察広さの比が奜たしい。
The pressure equalization function of the tank 12 is independent of its width, so the tank can theoretically be in the form of a narrow vertical pipe. However, relatively wide vessels are preferred because of the residence time that allows gas reabsorption, to reduce flow resistance, and to distribute heat into the lower part of the vessel without the need for auxiliary heating sources. For these purposes, a height to width ratio of no greater than 5:1 is preferred.

枅柄工皋に及がす真空の恩恵はだんだんず達成
され、すなわち、圧力が䜎いほど利点が倧きい。
倧気圧以䞋での小さな圧力䜎䞋ははかり埗る皋床
の改善をもたらすかもしれないが、しかし真空宀
を経枈的に正圓化するには、実質的な枛圧の䜿甚
が奜たしい。䟋えば、倧気圧の半分以䞋の圧力が
゜ヌダ・石灰・シリカ板ガラスぞ付䞎されるかな
りの枅柄改善にず぀お奜たしい。顕著に倧きいガ
ス陀去は䞉分の䞀気圧たたはそれ以䞋の圧力にお
いお達成される。暙準的柄明゜ヌダ・石灰・シリ
カ板ガラス組成物は100トルの絶察圧力においお
枅柄されお100cm3あたり個の皮子をも぀補品を
埗たが、これは倚くのガラス補品にず぀お蚱容で
きる品質氎準である。100トル以䞋䟋えば20から
50トルの枅柄圧力が1000−10000cm3あたり玄個
の皮子の商業的フロヌトガラスの品質を埗るのに
奜たしい。盎埄が0.01mm以䞋の皮子は認識できな
いものず考えられ、皮子の数に含たれない。
The benefits of vacuum on the fining process are achieved progressively, ie the lower the pressure the greater the benefit.
Although small pressure drops below atmospheric pressure may provide measurable improvements, the use of substantial reduced pressures is preferred to economically justify the vacuum chamber. For example, pressures of less than half atmospheric pressure are preferred for significant fining improvements applied to soda-lime-silica sheet glass. Significantly greater gas removal is achieved at pressures of one-third atmosphere or less. A standard clarified soda-lime-silica sheet glass composition was clarified at an absolute pressure of 100 torr to obtain a product with 1 seed per 100 cm 3 , which is an acceptable quality level for many glass products. be. Less than 100 Torr, for example from 20
A fining pressure of 50 Torr is preferred to obtain commercial float glass quality of about 1 seed per 1000-10000 cm3 . Seeds with a diameter of 0.01 mm or less are considered unrecognizable and are not included in the seed count.

硫黄たたは北玠の化合物のような熔解・枅柄助
剀が慣甚的にガラスバツチ䞭に含たれるが、ガラ
ス熔解炉からの排気ガス䞭で実質的な郚分の望た
しくない攟出物を生成する。
Melting and fining aids, such as sulfur or fluorine compounds, are conventionally included in glass batches, but produce a substantial portion of undesirable emissions in the exhaust gas from the glass melter.

それらの省略は望たしいこずであるが、板ガラ
ス暙準芏栌甚には特に、最高氎準の品質を埗るの
に助剀の䜿甚が必芁であるず考えられおきた。そ
の䞊、硫黄源䟋えば、硫酞ナトリりム、硫酞カ
ルシりムは真空䞋においお過床の発泡をおこす
こずが発芋された。代衚的には板ガラスバツチは
硫酞ナトリりムをシリカ源物質砂の1000重量
郚あたり玄から15重量郚の量で存圚し、玄10重
量郚が適切な枅柄を保蚌するのに望たしず考えら
れる。しかし本発明に埓぀お䜜業するずきには、
硫酞ナトリりムを重量郚ぞ制限しお取扱い可胜
の発泡氎準を維持するこずが奜たしいこずが発芋
されたのであり、そしお、さらに、枅柄が有害に
圱響されないこずが発芋された。最も奜たしく
は、硫酞ナトリりムは砂1000郚あたり郚以䞋で
甚いられ、0.5郚が特に有利な䟋である。これら
の重量比は硫酞ナトリりムに぀いお䞎えられたも
のであるが、しかし、それらを他の硫黄源ぞ分子
量比によ぀お転換させ埗るこずが明らかである。
枅柄助剀の完党削陀は本発明で以お可胜であり、
ただし、硫黄の痕跡量は他のバツチ物質䞭に代衚
的には存圚し、埓぀お、たずえバツチ䞭で硫黄を
わざわざ含たせないずしおも、少量の硫黄が存圚
するかもしれない。
Although their omission is desirable, the use of auxiliaries has been considered necessary to obtain the highest quality standards, especially for flat glass standards. Additionally, sulfur sources (eg, sodium sulfate, calcium sulfate) have been found to cause excessive foaming under vacuum. Typically, sheet glass batches contain sodium sulfate in an amount of about 5 to 15 parts by weight per 1000 parts by weight of silica source material (sand), with about 10 parts by weight considered desirable to ensure adequate fining. It will be done. However, when working in accordance with the present invention,
It has been discovered that it is preferable to limit the sodium sulfate to 2 parts by weight to maintain manageable foam levels, and furthermore, that clarification is not detrimentally affected. Most preferably, sodium sulfate is used at less than 1 part per 1000 parts of sand, with 0.5 part being a particularly advantageous example. These weight ratios are given for sodium sulfate, but it is clear that they can be converted to other sulfur sources depending on the molecular weight ratio.
Complete elimination of the clarification aid is possible with the present invention,
However, trace amounts of sulfur are typically present in other batch materials, so even if sulfur is not intentionally included in the batch, small amounts of sulfur may be present.

本発明の真空枅柄法にかけたガラスの物理的性
質に察しお、顕著な有害効果は発芋されなか぀
た。しかし、その真空凊理はガラス組成にいくら
かの怜出可胜効果を実際にもち、この方法によ぀
お補造されるガラスが慣甚の商業的方法によ぀お
補造される同じ皮類のガラスず区別できるように
なる。この真空凊理は揮発性物質成分、特に硫黄
のような枅柄助剀、の濃床を慣甚法で以お達成さ
れる平衡氎準より䜎い氎準ぞ䜎䞋させるこずが発
芋された。小ポツトなどで生成されたガラスはず
きどき、ほずんどたたは党く枅柄助剀の残留含量
をもたないず報告される。これは、非連続匏熔解
法は枅柄に長時間を䞎え、それによ぀お化孊的枅
柄助剀の必芁性を回避するからである。たた、小
さい熔融䜓は、慣甚的炭酞塩鉱物バツチ物質ずち
が぀お実質的容積のガス状副生成物を生成しない
化孊泚玔原料および酞化物原料物質から、しばし
ば補造される。しかし、連続匏熔解法によ぀お倧
量生産される゜ヌダ・石灰・シリカガラス補品は
顕著な量の残留枅柄助剀を特城ずする。そのよう
な補品は建物たたは乗物における窓ガラス透芖開
口郚に適する板ガラス䟋えば、フロヌト・ガラ
スおよび容噚䟋えば瓶を含む。その皮の補
品においおは、残留硫黄含有量SO3ずしお衚
珟は代衚的には重量で0.2の皋床であり、0.1
以䞋ではほずんどない。バツチぞ硫黄枅柄助剀
を泚意深く添加するずきでも、少くずも0.02の
SO3が慣甚の連続匏熔解槜の䞭で぀くられる゜ヌ
ダ・石灰・シリカガラスの䞭で通垞怜出できる。
透明窓ガラスの応甚のための板ガラスは通垞は
0.05以䞊のSO3をも぀。それずは異なり、゜ヌ
ダ・石灰・シリカガラスは本発明により連続匏で
奜たしい真空氎準においお、比范的小量の硫黄枅
柄助剀が䞊述のずおりにバツチ䞭に含たれるずき
でも、0.02以䞋の残留SO3で以お補造するこず
ができ、そしお硫黄をわざわざ含めないずきには
0.01以䞋のSO3で以お補造するこずができる。
硫黄をわざわざ添加しないで最小圧力においお、
0.005以䞋のSO3含量が達成できる。
No significant deleterious effects on the physical properties of glasses subjected to the vacuum fining process of the present invention were found. However, the vacuum treatment does have some detectable effect on the glass composition, making the glass produced by this method distinguishable from the same type of glass produced by conventional commercial methods. . It has been discovered that this vacuum treatment reduces the concentration of volatile components, particularly refining aids such as sulfur, to levels below the equilibrium levels achieved with conventional methods. Glasses produced in pots and the like are sometimes reported to have little or no residual content of refining aids. This is because the discontinuous melting process allows for longer fining times, thereby avoiding the need for chemical fining aids. Also, small melts are often produced from chemically pure feed and oxide feed materials that, unlike conventional carbonate mineral batch materials, do not produce substantial volumes of gaseous by-products. However, soda-lime-silica glass products produced in large quantities by continuous melting processes are characterized by significant amounts of residual fining aids. Such products include flat glass (eg, float glass) and containers (eg, bottles) suitable for glazing openings in buildings or vehicles. In such products, the residual sulfur content (expressed as SO3 ) is typically on the order of 0.2% by weight, and 0.1% by weight.
% or less. Even when carefully adding sulfur fining aid to batches, at least 0.02%
SO 3 can usually be detected in soda, lime, and silica glass produced in conventional continuous melters.
Flat glass for transparent window applications is usually
Contains SO 3 of 0.05% or more. In contrast, soda-lime-silica glass is produced in a continuous manner according to the present invention, at the preferred vacuum level, with less than 0.02% residual SO, even when relatively small amounts of sulfur refining aid are included in the batch as described above. 3 , and when sulfur is not included,
It can be produced with less than 0.01% SO 3 .
At minimum pressure without adding sulfur,
SO3 contents below 0.005% can be achieved.

硫黄化合物で以お普通に枅柄される商業的゜ヌ
ダ・石灰・シリカガラスは次のずおり特性づけお
よい 重量 SiO2 70−74 Na2O 12−16 CaO −12 MgO − Al2O3 − K2O − BaO − Fe2O3 − 少量の着色剀たたはその他の枅柄助剀もたた存
圚しおよい。砒玠、アンチモン、北玠、およびリ
チりム化合物がずきどき枅柄助剀ずしおずきどき
甚いられ、残留がこのタむプのガラスにおいお怜
出できる。フロヌトガラスの板たたは瓶は䞊蚘組
成物の普通の商業的具䜓化を代衚する。
Commercial soda-lime-silica glass, commonly refined with sulfur compounds, may be characterized as follows: wt% SiO 2 70-74 Na 2 O 12-16 CaO 8-12 MgO 0-5 Al 2 O 3 0-3 K 2 O 0-3 BaO 0-1 Fe 2 O 3 0-1 Small amounts of colorants or other clarifying aids may also be present. Arsenic, antimony, fluorine, and lithium compounds are sometimes used as refining aids, and residues can be detected in this type of glass. Float glass plates or bottles represent common commercial embodiments of the above compositions.

フロヌト法によ぀お圢成されたすなわち、熔
融錫䞊で浮かせお板ガラスは、少くずも片面䞊
でガラス衚面郚分の䞭ぞ移行した枬定可胜量の酞
化錫によ぀お特城づけられる。代衚的には、フロ
ヌトガラス片は、錫ず接觊した衚面の䞋方の二、
䞉ミクロンの䞭で少くずも0.05重量のSnO2濃
床をも぀。フロヌト法は硫黄黄含有枅柄助剀の顕
著な量を慣甚的に甚いるタむプの比范的倧芏暡の
連続匏溶解槜を必芁ずするので、フロヌト・ガラ
スは゜ヌダ・石灰・シリカガラスに぀いお䞀般的
に䞊蚘で論じたよりも高い最䜎SO3濃床を特城ず
する。それゆえ、0.08以䞋のSO3をも぀本発明
によ぀お枅柄されたフロヌトガラスは慣甚的な商
業的に入手できるフロヌトガラスず区別される。
倧郚分のフロヌトガラスは次の組成範囲に入る Sio2 72−74重量 Na2O 12−14 CaO −10 MgO − Al2O3 − K2O − Fe2O3 − 着色剀ず痕跡の他の物質が存圚しおもよい。
Glass sheets formed by the float process (ie, suspended on molten tin) are characterized by a measurable amount of tin oxide migrated into the glass surface area on at least one side. Typically, a piece of float glass is placed on the lower two sides of the surface in contact with the tin.
With a SnO 2 concentration of at least 0.05% by weight within 3 microns. Because the float process requires a relatively large continuous melting vessel of the type that conventionally uses significant amounts of sulfur-yellow-containing refining aids, float glasses are generally manufactured using the methods described above for soda-lime-silica glasses. characterized by a higher minimum SO 3 concentration than discussed in . Therefore, float glasses refined according to the present invention with less than 0.08% SO 3 are distinguished from conventional commercially available float glasses.
Most float glasses fall into the following composition range: Sio 2 72-74% by weight Na 2 O 12-14 CaO 8-10 MgO 3-5 Al 2 O 3 0-2 K 2 O 0-1 Fe 2 O 3 0-1 Colorants and traces of other substances may be present.

本発明の奜たしい具䜓化ず利点のいく぀かに関
する蚘述はガラスなどを぀くる連続匏方匏ず関連
させたけれども、非連続匏枅柄操䜜も本発明の利
点の少くずもいく぀かを埗るこずができるこずは
明らかなはずである。
Although the description of preferred embodiments and some of the advantages of the present invention has been made in connection with continuous processes for making glass and the like, it is clear that discontinuous fining operations can also obtain at least some of the advantages of the present invention. It should be.

圓業における熟緎者に知られおいるその他の倉
圢は特蚱請求の範囲によ぀お定矩される本発明の
領域内に含たれる。
Other variations known to those skilled in the art are included within the scope of the invention as defined by the claims.

【図面の簡単な説明】[Brief explanation of the drawing]

図面は、本発明の奜たしい具䜓化に埓぀お液状
化段階、溶解段階、および真空枅柄段階を含む熔
融操䜜の䞉段階の、垂盎断面である。
The drawings are vertical cross-sections of three stages of the melt operation, including a liquefaction stage, a melting stage, and a vacuum clarification stage, according to a preferred embodiment of the invention.

Claims (1)

【特蚱請求の範囲】  ガラス状物質たたは類䌌物を熔解および枅柄
する方法であ぀お、 物質の熔融物を生成させ 熔融された物質をそれが熔融物質本䜓䞊方で倧
気圧以䞋の圧力で保぀た空間の䞭ぞ導入されるず
きに発泡させ 発泡䜓を熔融物質本䜓䞭ぞ厩壊させそしお、 熔融物質を熔融物質本䜓から匕出す こずから成る方法。  熔融物質を熔融物質氎準䞊方の有匁オリフむ
スを通しお倧気圧以䞋の空間䞭ぞ導入する、特蚱
請求の範囲第項に蚘茉の方法。  熔融物質本䜓䞭の移送が抜出䜍眮ぞ向けお䞻
ずしお垂盎方向にある、特蚱請求の範囲第項に
蚘茉の方法。  倧気圧以䞋の圧力が倧気圧の半分以䞋であ
る、特蚱請求の範囲第項に蚘茉の方法。  倧気圧以䞋の圧力が倧気圧の䞉分の䞀以䞋で
ある、特蚱請求の範囲第項に蚘茉の方法。  抜出しの高さにおける熔融物質本䜓の䞭の圧
力が少くずも倧気圧である、特蚱請求の範囲第
項に蚘茉の方法。  抜出速床が取出口オリフむス手段によ぀お制
埡される、特蚱請求の範囲第項に蚘茉の方法。  新たに発泡させられた物質がさきに圢成され
た発泡䜓塊䞊ぞ沈積される、特蚱請求の範囲第
項に蚘茉の方法。  熔融および枅柄され぀぀ある物質がガラスで
ある、特蚱請求の範囲第項に蚘茉の方法。  熔融および枅柄され぀぀ある物質が゜ヌ
ダ・石灰・シリカガラスである、特蚱請求の範囲
第項に蚘茉の方法。  ガラス状物質たたは類䌌物を熔融および枅
柄する方法であ぀お、 第䞀宀においおバツチ物質を䞍完党に熔融した
流動性状態ずし、 未熔融粒子を含む流動性物質を粒子の熔融が実
質䞊完了される第二宀ぞ抜出し、 物質を第二宀から、物質を枅柄するようそれが
倧気圧以䞋の圧力にかけられる第䞉宀ぞ送る、 こずから成る方法。  熔融され぀぀ある物質が゜ヌダ・石灰・シ
リカガラスであり、その物質が第二宀から1480℃
2700〓以䞋で枩床の第䞉宀ぞ送られる、特蚱
請求の範囲第項に蚘茉の方法。  物質が第䞀宀から玄1200℃2200〓から
1320℃2400〓で第二宀ぞ送られる、特蚱請求
の範囲第項に蚘茉の方法。  物質が第二宀においお枅柄に適する枩床ぞ
加熱される、特蚱請求の範囲第項に蚘茉の方
法。  第䞉宀䞭の圧力が倧気圧の半分以䞋であ
る、特蚱請求の範囲第項に蚘茉の方法。  第䞉宀䞭の圧力が倧気圧の䞉分の䞀以䞋で
ある、特蚱請求の範囲第項に蚘茉の方法。  熔融され぀぀ある物質が゜ヌダ・石灰・シ
リカガラスであり、バツチ物質が第䞀宀ぞ、シリ
カ源物質の1000重量郚あたり重量郚の硫酞ナト
リりムず圓量の量以䞋の量の、枅柄助剀ずしおの
硫黄源ず䞀緒に䟛絊される、特蚱請求の範囲第
項に蚘茉の方法。  物質が第䞉宀䞭ぞ制埡された可倉速床で可
倉開口のオリフむスを通しお送られる、特蚱請求
の範囲第項に蚘茉の方法。  物質が第䞉宀から可倉開口のオリフむスを
通しお抜出される、特蚱請求の範囲第項に蚘
茉の方法。  バツチ物質を流動性状態にする段階が、バ
ツチ物質をある傟斜䞊に支持させながら熱ぞ露出
するこずから成る、特蚱請求の範囲第項に蚘
茉の方法。  その傟斜が䞭倮で加熱される空掞をずりか
こんでいる、特蚱請求の範囲第項に蚘茉の方
法。  枩床を第二宀䞭で電気加熱によ぀お䞊げ
る、特蚱請求の範囲第項に蚘茉の方法。  物質が第二宀䞭で取入口領域から取出口領
域ぞ䞻ずしお氎平の流路に沿぀お流れる、特蚱請
求の範囲第項に蚘茉の方法。  ガラスの総察的枩床が第䞉宀䞭においお䞊
げられない、特蚱請求の範囲第項に蚘茉の方
法。  第䞉宀䞭の物質が䞊郚取入口端から䞋郚取
出口端の方ぞ䞻ずしお垂盎方向の通路に埓う、特
蚱請求の範囲第項に蚘茉の方法。  第宀においおバツチ物質を䞍完党熔融の
流動性状態ずし、 この流動性物質を第二宀ぞその枩床が実質䞊そ
の液状化枩床をこえる前に抜出し、 第二宀においお物質の枩床を枅柄に適する枩床
ぞ䞊げ、そしお、 物質を第二宀から、物質を枅柄するように倧気
圧以䞋の圧力にかける第䞉宀ぞ送る、 こずから成る、特蚱請求の範囲第項に蚘茉の
方法。  熔融され぀぀ある物質が゜ヌダ・石灰・シ
リカガラスであり、物質が第二宀から1480℃
2700〓以䞋の枩床で第䞉宀ぞ送られる、特蚱
請求の範囲第項に蚘茉の方法。  物質が第䞀宀から玄1200℃2200〓から
1320℃2400〓の枩床で第二宀ぞ送られる、特
蚱請求の範囲第項に蚘茉の方法。  第二宀に入る物質が未熔融粒子を含み、粒
子の溶解を可胜にする十分な滞留時間が第二宀䞭
で䞎えられる、特蚱請求の範囲第項に蚘茉の
方法。  第䞉宀䞭の圧力が倧気圧の半分以䞋であ
る、特蚱請求の範囲第項に蚘茉の方法。  第䞉宀䞭の圧力が倧気圧の䞉分の䞀以䞋で
ある、特蚱請求の範囲第項に蚘茉の方法。  熔融され぀぀ある物質が゜ヌダ・石灰・シ
リカガラスであり、バツチ物質が第䞀宀ぞ、シリ
カ源物質の1000重量郚あたり重量郚の硫酞ナト
リりムず圓量の量以䞋の量の、枅柄助剀ずしおの
硫黄源ず䞀緒に䟛絊される、特蚱請求の範囲第
項に蚘茉の方法。  物質が第䞉宀䞭ぞ制埡された可倉速床で可
倉開口のオリフむスを通しお送られる、特蚱請求
の範囲第項に蚘茉の方法。  物質が第䞉宀から可倉開口のオリフむスを
通しお抜出される、特蚱請求の範囲第項に蚘
茉の方法。  バツチ物質を流動性状態にする段階がバツ
チ物質をある傟斜䞊で支持させながら熱ぞ露出す
るこずから成る、特蚱請求の範囲第項に蚘茉
の方法。  その傟斜が䞭倮で加熱される空掞をずりか
こんでいる、特蚱請求の範囲第項に蚘茉の方
法。  枩床が第二宀においお電気加熱によ぀お䞊
げられる、特蚱請求の範囲第項に蚘茉の方
法。  物質が第二宀においお取入れ口領域から取
出口領域ぞ䞻ずしお氎平である通路に沿぀お流れ
る、特蚱請求の範囲第項に蚘茉の方法。  ガラスの総括的枩床が第䞉宀䞭で䞊げられ
ない、特蚱請求の範囲第項に蚘茉の方法。  第䞉宀䞭の物質が䞊郚取入口端から䞋郚取
出口端ぞ向けお䞻ずしお垂盎方向の通路に埓う、
特蚱請求の範囲第項に蚘茉の方法。  バツチ物質を液状化し この液状化物質を倧気圧以䞋の圧力が䞭で維持
されおいる槜の䞊郚郚分のバルブ手段を通しお送
り 液状化物質を枛圧槜内で物質を実質的に枅柄す
る充分な時間の間維持し 枅柄物質を槜の䞋方郚分から抜出す こずから成る、特蚱請求の範囲第項に蚘茉の
方法。  䞊郚郚分における圧力が倧気圧力の半分以
䞋であり、䞋郚郚分の圧力が少くずも倧気圧であ
る、特蚱請求の範囲第項に蚘茉の方法。  液状化物質が槜から抜出される速床が第二
のバルブ手段によ぀お制埡される、特蚱請求の範
囲第項に蚘茉の方法。  ガラス状物質が゜ヌダ・石灰・シリカガラ
スである、特蚱請求の範囲第項に蚘茉の方
法。  液状化されたのち、か぀、バルブ手段を通
過する前に、液状化物質の枩床が枅柄に適する枩
床ぞ䞊げられる、特蚱請求の範囲第項に蚘茉
の方法。
Claims: 1. A method of melting and refining a glassy substance or the like, comprising: producing a melt of the substance; maintaining the molten substance at subatmospheric pressure above the body of the molten substance; collapsing the foam into the body of molten material; and drawing the molten material from the body of molten material. 2. The method of claim 1, wherein the molten material is introduced into the subatmospheric space through a valved orifice above the molten material level. 3. A method according to claim 1, wherein the transport in the body of molten material is predominantly vertical towards the withdrawal position. 4. The method according to claim 1, wherein the pressure below atmospheric pressure is less than half of atmospheric pressure. 5. The method according to claim 1, wherein the pressure below atmospheric pressure is one third or less of atmospheric pressure. 6. Claim 1, wherein the pressure in the body of molten material at the height of withdrawal is at least atmospheric pressure.
The method described in section. 7. A method according to claim 6, wherein the withdrawal rate is controlled by outlet orifice means. 8. Claim 1 in which the newly foamed material is deposited onto the previously formed foam mass.
The method described in section. 9. The method of claim 1, wherein the material being melted and refined is glass. 10. The method of claim 1, wherein the material being melted and refined is soda-lime-silica glass. 11 A method for melting and refining a glassy substance or the like, wherein the batch substance is brought to an incompletely melted, fluid state in a first chamber, and the fluid substance containing unmelted particles is brought to a substantially complete melting of the particles. a second chamber where the substance is clarified; and passing the substance from the second chamber to a third chamber where it is subjected to subatmospheric pressure to clarify the substance. 12 The substances being melted are soda, lime, and silica glass, and the substances are heated to 1480℃ from the second chamber.
12. The method according to claim 11, wherein the method is fed to a third chamber at a temperature below (2700〓). 13 Substances are transferred from the first chamber to approximately 1200℃ (2200〓)
13. The method of claim 12, wherein the second chamber is fed at 1320°C (2400°). 14. The method of claim 11, wherein the material is heated in the second chamber to a temperature suitable for clarification. 15. The method according to claim 11, wherein the pressure in the third chamber is less than half the atmospheric pressure. 16. The method according to claim 11, wherein the pressure in the third chamber is one third or less of atmospheric pressure. 17 The substance being melted is soda-lime-silica glass, and the batch substance is sent to the first chamber with a clarification aid in an amount not more than the equivalent of 2 parts by weight of sodium sulfate per 1000 parts by weight of the silica source material. Claim 1 provided with a sulfur source as
The method described in Section 1. 18. The method of claim 11, wherein the substance is delivered into the third chamber at a controlled variable rate through a variable opening orifice. 19. The method of claim 18, wherein the substance is withdrawn from the third chamber through an orifice of variable opening. 20. The method of claim 11, wherein the step of rendering the batch material in a flowable state comprises exposing the batch material to heat while supporting the batch material on an incline. 21. The method of claim 20, wherein the slope surrounds a centrally heated cavity. 22. The method of claim 11, wherein the temperature is raised in the second chamber by electrical heating. 23. The method of claim 11, wherein the substance flows in the second chamber from the inlet region to the outlet region along a predominantly horizontal flow path. 24. The method of claim 11, wherein the overall temperature of the glass is not raised in the third chamber. 25. The method of claim 11, wherein the material in the third chamber follows a predominantly vertical path from the upper inlet end towards the lower outlet end. 26 Bring the batch material to an incompletely melted fluid state in the first chamber, withdraw the fluid material to the second chamber before its temperature substantially exceeds its liquefaction temperature, and clarify the temperature of the material in the second chamber. 12. A method as claimed in claim 11, comprising: raising the material to a temperature suitable for clarification, and passing the material from the second chamber to a third chamber where it is subjected to subatmospheric pressure so as to clarify the material. 27 The substances being melted are soda, lime, and silica glass, and the substances are heated to 1480℃ from the second chamber.
27. The method according to claim 26, wherein the method is fed to the third chamber at a temperature of (2700〓) or less. 28 The substance is released from the first room from about 1200℃ (2200〓)
28. The method of claim 27, wherein the second chamber is fed at a temperature of 1320°C (2400°). 29. The method of claim 26, wherein the material entering the second chamber contains unmelted particles and sufficient residence time is provided in the second chamber to allow dissolution of the particles. 30. The method of claim 26, wherein the pressure in the third chamber is less than half atmospheric pressure. 31. The method according to claim 26, wherein the pressure in the third chamber is one third or less of atmospheric pressure. 32 The substance being melted is soda-lime-silica glass, and the batch substance is sent to the first chamber with a clarification aid in an amount not more than the equivalent of 2 parts by weight of sodium sulfate per 1000 parts by weight of the silica source material. Claim 2 provided with a sulfur source as
The method described in Section 6. 33. The method of claim 26, wherein the substance is delivered into the third chamber at a controlled variable rate through a variable opening orifice. 34. The method of claim 33, wherein the material is withdrawn from the third chamber through an orifice of variable opening. 35. The method of claim 26, wherein the step of rendering the batch material in a flowable state comprises exposing the batch material to heat while supporting the batch material on an incline. 36. The method of claim 35, wherein the slope surrounds a centrally heated cavity. 37. The method of claim 26, wherein the temperature is raised in the second chamber by electrical heating. 38. The method of claim 26, wherein the substance flows in the second chamber from the inlet area to the outlet area along a path that is primarily horizontal. 39. The method of claim 26, wherein the overall temperature of the glass is not raised in the third chamber. 40 The substance in the third chamber follows a primarily vertical path from the upper inlet end to the lower outlet end;
A method according to claim 26. 41 liquefying the batch material; directing the liquefied material through valve means in the upper part of the vessel in which a subatmospheric pressure is maintained; passing the liquefied material in a vacuum tank sufficient to substantially clarify the material; 12. A method according to claim 11, comprising: maintaining the clarified material for a period of time; and withdrawing the clarified material from the lower part of the vessel. 42. The method of claim 41, wherein the pressure in the upper portion is less than half atmospheric pressure and the pressure in the lower portion is at least atmospheric pressure. 43. A method according to claim 41, wherein the rate at which the liquefied material is withdrawn from the vessel is controlled by second valve means. 44. The method according to claim 41, wherein the glassy substance is soda/lime/silica glass. 45. A method according to claim 41, wherein after being liquefied and before passing through the valve means, the temperature of the liquefied material is raised to a temperature suitable for clarification.
JP31602886A 1986-01-02 1986-12-25 Method of melting and clarifying glass or analogue by vacuum clarification Granted JPS62235222A (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
US81549486A 1986-01-02 1986-01-02
US815494 1986-01-02
US894143 2001-06-29

Publications (2)

Publication Number Publication Date
JPS62235222A JPS62235222A (en) 1987-10-15
JPH0242777B2 true JPH0242777B2 (en) 1990-09-26

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP31602886A Granted JPS62235222A (en) 1986-01-02 1986-12-25 Method of melting and clarifying glass or analogue by vacuum clarification

Country Status (4)

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JP (1) JPS62235222A (en)
DD (1) DD258793A5 (en)
SU (1) SU1614758A3 (en)
ZA (1) ZA869146B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8689586B2 (en) 2009-03-09 2014-04-08 Nitto Boseki Co., Ltd. Glass-melting device for producing glass fiber and method for producing glass fiber

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6469530A (en) * 1987-09-07 1989-03-15 Nippon Sheet Glass Co Ltd Production of glass
KR100444628B1 (en) 1995-11-21 2004-11-03 아사히 가띌슀 가부시킀가읎샀 Method and apparatus for refining molten glass

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8689586B2 (en) 2009-03-09 2014-04-08 Nitto Boseki Co., Ltd. Glass-melting device for producing glass fiber and method for producing glass fiber

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DD258793A5 (en) 1988-08-03
JPS62235222A (en) 1987-10-15
SU1614758A3 (en) 1990-12-15
ZA869146B (en) 1988-07-27

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