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JPS633004B2 - - Google Patents
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JPS633004B2 - - Google Patents

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Publication number
JPS633004B2
JPS633004B2 JP59140340A JP14034084A JPS633004B2 JP S633004 B2 JPS633004 B2 JP S633004B2 JP 59140340 A JP59140340 A JP 59140340A JP 14034084 A JP14034084 A JP 14034084A JP S633004 B2 JPS633004 B2 JP S633004B2
Authority
JP
Japan
Prior art keywords
cooling
gas
cooling pipe
pipe
tube
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
JP59140340A
Other languages
Japanese (ja)
Other versions
JPS6119713A (en
Inventor
Emi Murakawa
Seiji Taguchi
Ryoji Takabe
Yoshiharu Iwashita
Masahiro Ishii
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
JFE Steel Corp
Original Assignee
Kawasaki Steel Corp
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 by Kawasaki Steel Corp filed Critical Kawasaki Steel Corp
Priority to JP59140340A priority Critical patent/JPS6119713A/en
Priority to US06/751,088 priority patent/US4697453A/en
Priority to CA000486328A priority patent/CA1251945A/en
Publication of JPS6119713A publication Critical patent/JPS6119713A/en
Publication of JPS633004B2 publication Critical patent/JPS633004B2/ja
Priority to US07/275,687 priority patent/US4914948A/en
Granted legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21BMANUFACTURE OF IRON OR STEEL
    • C21B7/00Blast furnaces
    • C21B7/24Test rods or other checking devices
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/02Constructional details
    • G01J5/06Arrangements for eliminating effects of disturbing radiation; Arrangements for compensating changes in sensitivity
    • G01J5/061Arrangements for eliminating effects of disturbing radiation; Arrangements for compensating changes in sensitivity by controlling the temperature of the apparatus or parts thereof, e.g. using cooling means or thermostats

Landscapes

  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Materials Engineering (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Manufacturing & Machinery (AREA)
  • General Physics & Mathematics (AREA)
  • Physics & Mathematics (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Radiation Pyrometers (AREA)
  • Blast Furnaces (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 本発明は、高炉炉内等の高温雰囲気内を観測す
る装置に関し、特にその冷却構造に関するもので
ある。 〔従来の技術〕 高炉内における装入物粒度の半径方向分布は、
炉内ガス流れおよび炉内温度分布に強く影響する
因子として重要な高炉操業指数である。 この粒度分布を稼動中の高炉において検出する
装置の一つとして光フアイバを使用する装置があ
る。 例えば、第3図のように高炉1の炉頂空間にお
いて、高炉半径方向に可動な炉頂水平ゾンデ5よ
り下方装入物2の表面に向けて可撓部を具えた光
フアイバ検出器3を降下させ、光源9からの光を
ライトガイド8で導き、光フアイバ10を通して
装入物2表面をテレビカメラ11で画像としてと
らえ、ビデオデツキ12を介してモニタテレビ1
3に入力することにより、炉頂での装入物粒度を
検出することができる。 なお、第3図で6は耐圧シール、7は仕切弁を
示している。炉頂でのガス温度は数百度にまで上
昇することがあり、かつ装入物表面からは多量の
輻射熱が放散されているので、冷却器制御系14
を備えて光フアイバを冷却する必要がある。以下
本発明において光フアイバからなる検出器または
この検出器を内蔵する管状体を検出体と呼ぶ。 このような検出体の冷却装置としては、雰囲気
温度がそれほど高くなく、かつ輻射熱が小さい場
合気体冷却装置が使用できる。その構造について
は、第4図に示すような先端で気体を気体流出口
19から外部雰囲気に開放する気体冷却装置が用
いられ、このような装置では気体復路用の管が不
必要なので、構造が簡単でコンパクトにできる。
しかしこの装置では、雰囲気温度が高い場合、高
温に曝される部分が長い場合または輻射熱が大き
い場合は十分な冷却効果が得られない。 このような苛酷な条件下で使用するものとし
て、特開昭58−6913に見られるような水冷却装置
が採用されてきた。水冷却では第5図に示すよう
に、光フアイバおよびライトガイドを内蔵した管
から成る検出体15を冷却水の往路31と復路3
2を備えた2重冷却管23が包む。この水冷却法
は、冷却効果が大きいが、2重冷却管23の外径
が太くなりコンパクトにできない。また第3図に
示すように検出体は可撓部4を具えている必要が
あるが、2重冷却管23では可撓性が小さい。2
重冷却管23として耐水性フレキシブルチユーブ
を用いても、フレキシブルチユーブ自身かなり大
きな剛性を有するので、最低3重にフレキシブル
チユーブを重ねた第5図の冷却管では、十分に曲
らず検出部20が下方の装入物表面に向かない恐
れがある。さらに2重冷却管内には多量の水が入
るので装置の重量が大きくなり、第3図に示した
可撓部4の根元から折れる恐れがある。 〔発明が解決しようとする問題点〕 本発明は、上記従来の欠点を解消し、検出体の
先端部のみを液状冷媒冷却とし、より根元側の検
出体部分ではある程度の液状冷媒冷却と気体冷却
の複合冷却を採用し、液状冷媒冷却と気体冷却の
それぞれの欠点を解消し、両者の長所を生かした
高温雰囲気内観測装置を提供することを目的とす
る。 〔問題点を解決するための手段〕 本発明の装置の基本的構成を第1図に示す。輻
射熱が大きく温度が最も上昇する恐れのある検出
体先端の検出部20の周囲には液状冷媒冷却管2
8を配設している。この液状冷媒冷却管28は、
剛直で可撓性はない。第1図の実施例では、冷却
管28は一重管で1本の液状冷媒の往路用のチユ
ーブ24を冷却管28の先端まで伸ばし、復路用
のチユーブ25は冷却管28の根元側に取付けて
いるが、冷却管28を2重冷却管構造にしてもよ
い。いずれにしても先端部の冷却管28は剛直で
比較的短いのでコンパクトにできる。もちろん往
路用と復路用の冷却チユーブ24,25は各々2
本以上であつてもよい。 他方、第3図に斜線を施して示した可撓部4に
ついては、先端の冷却管28(第1図)まで冷媒
を輸送するチユーブ24および25が検出体15
の回りに螺旋状に巻き付けられる。このチユーブ
24,25の螺旋の巻回ピツチの粗密具合によつ
て可撓部4の可撓性を調整することができる。す
なわち第3図で下方へ垂れ下つている部分の長さ
lが大きい程、可撓部4を曲げようとする力が大
きくなるが、可撓部4の先端に近い部分(lが小
さい部分)ではチユーブ24,25の螺旋ピツチ
を粗に巻き、根元に行く(lが大になる)に従つ
て密に巻くことによつて、長さlの如何に拘ら
ず、常に同程度の曲率で曲げることができる。 螺旋状チユーブ24および25の中には液状冷
媒が流れているので、この冷却管による検出体1
5のある程度の冷却効果が期待できるが、より大
きな冷却効果を得るために検出体15の周囲16
をチユーブ29で被覆して気体冷却室を設ける。
この時冷却気体19は螺旋状に巻かれたチユーブ
24および25と接触するので、単純な気体冷却
の場合よりも冷却気体の温度の上昇が小さくな
り、それだけ気体冷却効果が上昇する。冷却気体
は可撓部先端で外部雰囲気に開放される他、先端
検出部20の部分でパージガス流通溝22を通る
パージ用気体としても使用される。 螺旋状に巻かれたチユーブ24および25につ
いては、10mmφ程度もしくはそれ以下の耐水性フ
レキシブルチユーブを使用することができる。従
つて2重冷却管構造に比べて本発明の装置は外径
dを小さくすることができる。 また気体冷却室を形成する最外殻チユーブ29
は耐水性である必要がなく、それだけそのチユー
ブ29の材質および構造についての選択範囲が広
くなる。 さらに螺旋状チユーブ24および25内に収納
される液状冷媒は、従来の2重冷却管を用いた場
合よりも少量ですみ、装置の重要がそれだけ小さ
くなる。またそれによつて下方へ垂れ下つている
部分の長さl(第3図)が可撓部4の曲げ半径に
およぼす影響が小さくなる。すなわち装置の重量
が小さい場合、lの大小にかかわらず、可撓部4
の曲り部を同程度の曲率で曲げることができる。 以上述べたように、本発明の高温雰囲気内観測
装置は冷却効果、可撓性、軽量化およびコンパク
ト化に対して大きな改善効果が期待できる。 なお、本発明の冷却装置の構成は可撓性のない
観測装置にも応用することが可能であり、可撓部
4を直線状としたり剛直とすることもできる。 例えば第2図a,bに非直線状で剛直な検出体
の場合の冷却装置の一例を示す。aは検出体の横
断面図、bは側面図である。螺旋状に巻かれた冷
却チユーブ24および25は、この場合、なまし
銅を用いており、検出器を内蔵する検出体15に
ハンダ30付けされており、検出体15の冷却効
果を高めている。 また本発明の冷却装置の構成は、検出器が光フ
アイバである場合だけでなく、その他の温度、圧
力あるいは物質の成分組成等を検出する装置に対
しても用いることができる。特に検出部のみが耐
熱上最も問題となる場合については最も有効であ
る。 〔実施例〕 高温雰囲気内観測装置の光フアイバの代りに熱
電対をパイプの内に挿入して、空冷、水冷および
本発明装置をそれぞれ800℃の高温炉の内へ4m
入れた場合の各部の冷却効果を調べた。冷却条件
を第1表に、また冷却効果を第6図に示す。ただ
し、本発明装置で水冷している水冷却管は先端50
cmである。 第6図から明らかなように単純な空冷に比較し
て、本発明の装置は冷却効果が大きく改善されて
いる。特に先端部については水冷装置と同程度の
冷却効果が得られた。 また、各々の装置について、最外殻パイプの外
径を第2表に示した。冷却2重管構造の場合は
100mmφ程度になるに比べ本発明装置では60mmφ
程度もしくはそれ以下に納めることができた。
[Industrial Application Field] The present invention relates to an apparatus for observing a high-temperature atmosphere such as a blast furnace, and particularly relates to a cooling structure thereof. [Prior art] The radial distribution of the grain size of the charge in the blast furnace is
This is an important blast furnace operation index as a factor that strongly influences gas flow and temperature distribution in the furnace. One of the devices for detecting this particle size distribution in an operating blast furnace is a device using an optical fiber. For example, as shown in FIG. 3, in the top space of the blast furnace 1, an optical fiber detector 3 equipped with a flexible portion is installed toward the surface of the charge 2 below the top horizontal sonde 5, which is movable in the radial direction of the blast furnace. The light from the light source 9 is guided by the light guide 8, the surface of the charge 2 is captured as an image by the TV camera 11 through the optical fiber 10, and the image is displayed on the monitor TV 1 via the video deck 12.
3, the charge particle size at the top of the furnace can be detected. In addition, in FIG. 3, 6 indicates a pressure seal, and 7 indicates a gate valve. The gas temperature at the top of the furnace can rise to several hundred degrees, and a large amount of radiant heat is dissipated from the surface of the charge, so the cooler control system 14
It is necessary to cool the optical fiber. Hereinafter, in the present invention, a detector made of an optical fiber or a tubular body containing this detector will be referred to as a detection body. As a cooling device for such a detection object, a gas cooling device can be used when the ambient temperature is not so high and the radiant heat is small. Regarding its structure, a gas cooling device is used that releases the gas from the gas outlet port 19 to the outside atmosphere at the tip as shown in Fig. 4, and since such a device does not require a gas return pipe, the structure is simple. Easy and compact.
However, with this device, a sufficient cooling effect cannot be obtained when the ambient temperature is high, when the portion exposed to high temperature is long, or when radiant heat is large. For use under such severe conditions, a water cooling system such as that seen in Japanese Patent Application Laid-Open No. 58-6913 has been adopted. In water cooling, as shown in FIG.
A double cooling pipe 23 with 2 is encased. Although this water cooling method has a large cooling effect, the outer diameter of the double cooling pipe 23 becomes large and cannot be made compact. Further, as shown in FIG. 3, the detection object must include a flexible portion 4, but the double cooling pipe 23 has little flexibility. 2
Even if a water-resistant flexible tube is used as the heavy cooling tube 23, the flexible tube itself has considerable rigidity, so the cooling tube shown in FIG. There is a possibility that it will not be directed towards the surface of the charge below. Furthermore, since a large amount of water enters the double cooling pipe, the weight of the device increases, and there is a risk that the flexible portion 4 shown in FIG. 3 may break at the base. [Problems to be Solved by the Invention] The present invention solves the above-mentioned conventional drawbacks, and cools only the tip of the detection body with liquid refrigerant, and cools the part of the detection body closer to the base with a certain degree of liquid refrigerant cooling and gas cooling. The purpose of the present invention is to provide a high-temperature atmosphere observation device that utilizes the combined cooling of liquid refrigerant and gas cooling, eliminating the drawbacks of both, and taking advantage of the strengths of both. [Means for Solving the Problems] The basic configuration of the apparatus of the present invention is shown in FIG. A liquid refrigerant cooling pipe 2 is installed around the detection section 20 at the tip of the detection object, where the radiant heat is large and the temperature is most likely to rise.
8 are installed. This liquid refrigerant cooling pipe 28 is
Rigid and not flexible. In the embodiment shown in FIG. 1, the cooling pipe 28 is a single-layered pipe, and the tube 24 for the outward path of the liquid refrigerant extends to the tip of the cooling pipe 28, and the tube 25 for the return path is attached to the root side of the cooling pipe 28. However, the cooling pipe 28 may have a double cooling pipe structure. In any case, the cooling pipe 28 at the tip is rigid and relatively short, so it can be made compact. Of course, there are 2 cooling tubes 24 and 25 for the outbound and return trips, respectively.
It can be more than a book. On the other hand, regarding the flexible portion 4 shown with diagonal lines in FIG.
wrapped in a spiral around the The flexibility of the flexible portion 4 can be adjusted by adjusting the pitch of the spiral windings of the tubes 24 and 25. In other words, the larger the length l of the part that hangs downward in FIG. Now, by winding the helical pitches of tubes 24 and 25 roughly, and winding them more densely toward the base (l increases), the tubes are always bent with the same degree of curvature, regardless of the length l. be able to. Since liquid refrigerant flows in the spiral tubes 24 and 25, the detection object 1 is
5 can be expected to have a certain degree of cooling effect, but in order to obtain a larger cooling effect, the surrounding area 16 of the detection object 15
is covered with a tube 29 to provide a gas cooling chamber.
At this time, the cooling gas 19 comes into contact with the spirally wound tubes 24 and 25, so that the temperature rise of the cooling gas is smaller than in the case of simple gas cooling, and the gas cooling effect is increased accordingly. The cooling gas is not only released to the external atmosphere at the tip of the flexible portion, but also used as a purge gas that passes through the purge gas distribution groove 22 at the tip detection section 20 . As for the spirally wound tubes 24 and 25, water-resistant flexible tubes with a diameter of about 10 mm or less can be used. Therefore, compared to a double cooling pipe structure, the device of the present invention can have a smaller outer diameter d. The outermost shell tube 29 also forms a gas cooling chamber.
The tube 29 does not need to be water resistant, which gives a wider range of choices regarding the material and structure of the tube 29. Additionally, less liquid refrigerant is contained within the helical tubes 24 and 25 than with conventional dual cooling tubes, making the system less critical. This also reduces the influence of the length l (FIG. 3) of the downwardly hanging portion on the bending radius of the flexible portion 4. In other words, if the weight of the device is small, the flexible portion 4
can be bent with the same degree of curvature. As described above, the high-temperature atmosphere observation device of the present invention can be expected to greatly improve the cooling effect, flexibility, weight reduction, and compactness. Note that the configuration of the cooling device of the present invention can also be applied to an observation device without flexibility, and the flexible portion 4 can be made linear or rigid. For example, FIGS. 2a and 2b show an example of a cooling device for a non-linear and rigid detection object. A is a cross-sectional view of the detection object, and b is a side view. The spirally wound cooling tubes 24 and 25 are made of annealed copper in this case, and are soldered 30 to the detection body 15 containing the detector, thereby increasing the cooling effect of the detection body 15. . Furthermore, the configuration of the cooling device of the present invention can be used not only when the detector is an optical fiber, but also for other devices that detect temperature, pressure, or the composition of substances. This is particularly effective when only the detection part poses the greatest problem in terms of heat resistance. [Example] A thermocouple was inserted into the pipe instead of the optical fiber of the high-temperature atmosphere observation device, and the air-cooled, water-cooled, and inventive devices were each placed 4 m into a high-temperature furnace at 800°C.
We investigated the cooling effect of each part when it was inserted. The cooling conditions are shown in Table 1, and the cooling effect is shown in FIG. However, the tip of the water cooling pipe used in the device of the present invention is 50 mm.
cm. As is clear from FIG. 6, the cooling effect of the apparatus of the present invention is greatly improved compared to simple air cooling. Especially for the tip, a cooling effect comparable to that of a water cooling device was obtained. Table 2 also shows the outer diameter of the outermost pipe for each device. In case of double cooling pipe structure
Compared to about 100mmφ, the device of the present invention has a diameter of 60mmφ.
I was able to get it to about that level or less.

【表】【table】

〔発明の効果〕〔Effect of the invention〕

本発明装置は、冷却効果が優れ、軽量で小径化
でき、また可撓性をもつ装置に最も好適に用いら
れ、可撓性の調整も容易にできる。
The device of the present invention has an excellent cooling effect, is lightweight and can be made small in diameter, and is most suitably used for flexible devices, and the flexibility can be easily adjusted.

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

第1図は本発明の観測装置の実施例の要部縦断
面図、第2図は別の実施例のa横断面図、b側面
図、第3図は観測装置の説明図、第4図、第5図
は従来の装置の要部縦断面図、第6図、第7図は
実施例の効果を示すグラフである。 1……高炉、2……高炉内装入物、3……光フ
アイバ式検出器、4……検出器可撓部、5……炉
頂水平ゾンデ、10……光フアイバ、11……テ
レビカメラ、12……ビデオデツキ、13……モ
ニタテレビ、14……冷却器制御系、15……検
出体、18……気体流入口、19……冷却気体、
20……検出部、22……パージガス流通溝、2
4,25……チユーブ、28……冷却管。
Fig. 1 is a longitudinal cross-sectional view of a main part of an embodiment of the observation device of the present invention, Fig. 2 is a transverse cross-sectional view and b side view of another embodiment, Fig. 3 is an explanatory diagram of the observation device, and Fig. 4 , FIG. 5 is a longitudinal cross-sectional view of a main part of a conventional device, and FIGS. 6 and 7 are graphs showing the effects of the embodiment. DESCRIPTION OF SYMBOLS 1... Blast furnace, 2... Blast furnace contents, 3... Optical fiber detector, 4... Detector flexible part, 5... Furnace top horizontal sonde, 10... Optical fiber, 11... Television camera , 12... Video deck, 13... Monitor TV, 14... Cooler control system, 15... Detection object, 18... Gas inlet, 19... Cooling gas,
20...detection section, 22...purge gas distribution groove, 2
4, 25...Tube, 28...Cooling pipe.

Claims (1)

【特許請求の範囲】[Claims] 1 高炉炉頂の高温雰囲気を観測する可撓性を有
する高温雰囲気内観測装置において、検出体の先
端部外周に液状冷媒を用いる冷却管を配設し、該
冷却管へ冷媒を輸送するチユーブを前記検出体の
外周に螺旋状に巻回すると共に検出体のまわりに
気体冷却室を設けたことを特徴とする高温雰囲気
内観測装置。
1. In a flexible high-temperature atmosphere observation device for observing the high-temperature atmosphere at the top of a blast furnace, a cooling pipe using a liquid refrigerant is arranged around the tip of the detection object, and a tube for transporting the refrigerant to the cooling pipe is installed. A high-temperature atmosphere observation device characterized in that the gas cooling chamber is spirally wound around the detection body and a gas cooling chamber is provided around the detection body.
JP59140340A 1984-07-05 1984-07-06 Observing device in high-temperature atmosphere Granted JPS6119713A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP59140340A JPS6119713A (en) 1984-07-06 1984-07-06 Observing device in high-temperature atmosphere
US06/751,088 US4697453A (en) 1984-07-05 1985-07-02 Apparatus for monitoring burden distribution in furnace
CA000486328A CA1251945A (en) 1984-07-05 1985-07-04 Apparatus for monitoring burden distribution in furnace
US07/275,687 US4914948A (en) 1984-07-05 1988-11-23 Apparatus for monitoring burden distribution in furnace

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59140340A JPS6119713A (en) 1984-07-06 1984-07-06 Observing device in high-temperature atmosphere

Publications (2)

Publication Number Publication Date
JPS6119713A JPS6119713A (en) 1986-01-28
JPS633004B2 true JPS633004B2 (en) 1988-01-21

Family

ID=15266552

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59140340A Granted JPS6119713A (en) 1984-07-05 1984-07-06 Observing device in high-temperature atmosphere

Country Status (1)

Country Link
JP (1) JPS6119713A (en)

Families Citing this family (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4914948A (en) * 1984-07-05 1990-04-10 Kawasaki Steel Corp. Apparatus for monitoring burden distribution in furnace
US4697453A (en) * 1984-07-05 1987-10-06 Kawasaki Steel Corp. Apparatus for monitoring burden distribution in furnace
JPH0175807U (en) * 1987-11-10 1989-05-23
JPH02307025A (en) * 1989-05-23 1990-12-20 Fujitsu Ltd Thermometer for vacuum device
JPH0618334A (en) * 1992-06-29 1994-01-25 Mikuni Seisakusho:Kk Temperature measuring device for heated matter
US6175676B1 (en) * 1999-02-23 2001-01-16 Bethlehem Steel Corporation Fiber optic sensor and method of use thereof to determine carbon content of molten steel contained in a basic oxygen furnace
JP2010091288A (en) * 2008-10-03 2010-04-22 Nittetsu Hokkaido Control Systems Corp Optical fiber temperature measuring instrument
US8983256B2 (en) 2011-04-28 2015-03-17 Sumitomo Electric Industries, Ltd. Optical fiber cable
JP2014055851A (en) * 2012-09-12 2014-03-27 Babcock-Hitachi Co Ltd Flame detector, and burner ignition torch equipped with the same

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57174406A (en) * 1981-04-18 1982-10-27 Nippon Steel Corp Probe for observation and measuring inside of blast furnace
JPS6039125B2 (en) * 1981-04-18 1985-09-04 新日本製鐵株式会社 Probe for observation and measurement inside blast furnace

Also Published As

Publication number Publication date
JPS6119713A (en) 1986-01-28

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