TW200946265A - Method for detecting breakouts in continuous casting and an apparatus therefor, breakout prevention apparatus, method for estimating solidification shell thickness and an apparatus therefor, and a continuous casting method for steel - Google Patents
Method for detecting breakouts in continuous casting and an apparatus therefor, breakout prevention apparatus, method for estimating solidification shell thickness and an apparatus therefor, and a continuous casting method for steel Download PDFInfo
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- TW200946265A TW200946265A TW98106495A TW98106495A TW200946265A TW 200946265 A TW200946265 A TW 200946265A TW 98106495 A TW98106495 A TW 98106495A TW 98106495 A TW98106495 A TW 98106495A TW 200946265 A TW200946265 A TW 200946265A
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
- B22D11/00—Continuous casting of metals, i.e. casting in indefinite lengths
- B22D11/16—Controlling or regulating processes or operations
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
- B22D11/00—Continuous casting of metals, i.e. casting in indefinite lengths
- B22D11/16—Controlling or regulating processes or operations
- B22D11/18—Controlling or regulating processes or operations for pouring
- B22D11/188—Controlling or regulating processes or operations for pouring responsive to thickness of solidified shell
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
- B22D11/00—Continuous casting of metals, i.e. casting in indefinite lengths
- B22D11/16—Controlling or regulating processes or operations
- B22D11/20—Controlling or regulating processes or operations for removing cast stock
- B22D11/207—Controlling or regulating processes or operations for removing cast stock responsive to thickness of solidified shell
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
- B22D11/00—Continuous casting of metals, i.e. casting in indefinite lengths
- B22D11/16—Controlling or regulating processes or operations
- B22D11/22—Controlling or regulating processes or operations for cooling cast stock or mould
- B22D11/225—Controlling or regulating processes or operations for cooling cast stock or mould for secondary cooling
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Abstract
Description
200946265 六、發明說明: 【發明所屬之技術領域】 本發明係關於一種於熔鋼之連續鑄造中高精度地檢出鑄 片上所產生之鑄漏(breakout),進而防止該鑄漏之方法及裝 置。另外,本發明係關於一種使用上述鑄漏檢出方法之鋼之 連續鑄造方法。 進而本么明亦係關於一種推定炼鋼之連續缚造中之凝固 ❹殼厚度(solldiHcati〇n shell thickness)之方法及裝置。 【先前技術】 於連、β鑄4巾’藉由使注人於矯模巾之熔鋼於铸模内冷卻 而形成凝固殼後,將其自鑄模中抽^然而,若因某種原因 導致凝固殼之形成不充分’而存在凝固殼厚較薄之部位,則 會存在產生簡制之危險,即,#該額殼厚較薄之部位 ❹ 職鑄模出口(鑷模下端)時,凝固殼破裂而導致炼_出。 右產生鑄漏,則必須停止操作,因此必須選擇不會產生禱 漏之操作騎,但料㈣⑽漏㈣分轉低鑄造速度, 則會導致操作效率惡化,故不佳。基於此種背景,期望開發 一種即便進行高輯造亦可準確關斷軸之危險之方 法’目前已提出有各種方法。 例如,於專利文獻1(日本專利特公昭啦39〇3號公報) 中揭示有如下之技術。 該技術係一種連續铸造之縳漏防止方法,其係藉由配置於 098106495 3 200946265 鑄模外表面之薄板型表面熱通量計,f 對與鑄模之排熱量 (heat extraction 〇f mold)相對應之熱通量進行測定, 漏。 止連續鑄造之鎊漏者;其特徵在於:藉由多數個:通二計: 測定鑄模各部分之局部熱通量,當表示該熱通量之時間性變 化的熱通量波形之波高急遽地超過既定值時降低鱗入、 度’進行低速鑄人直至上述波高恢復原狀,藉此防止產2 【發明内容】 (發明所欲解決之問題) ® 專利文獻1中所揭示之技術係使用熱通量計而檢出熱通 量之變化之鑄漏防止方法。鍀模各部分之局部熱通量係表示 來自鎿模之排熱量’排熱量與凝固殼之形成相關。因此,= / 大致合理地預測於熱通量之變化產生異常時,凝固殼厚之形 成會產生異常,而存在產生鑄漏之危險。 然而,若考慮到於鑄模出口處,因凝固殼厚度未達到既定 ❹ 之厚度而產生鑄漏’則僅藉由熱通量之變化,未必可充分地 把握準確之鎮漏之危險性。其原因在於亦存在如下情形:即 便於鑄模内之凝固殼形成過程之初始階段中存在熱通量之 · 異常’只要於凝固毅形成過程之後階段中形成凝固殼,於鑄 _ 模出口處形成既疋厚度之凝固殼’則可判斷無產生鱗漏之危 險。 即,僅藉由先前例中所示之局部熱通量之變化而預測產生 098106495 4 200946265 鑄漏之危險,此難謂足夠準確之指標。 如上所述’鱗漏之產生係與禱模出口處之凝固殼厚度直接 相關’若可高精度地推定凝固殼厚度,則亦可高精度地判斷 產生鑄漏之危險。即,發明者認為重要的是找出與缚模出口 處之凝固殼厚度是否已達到既定厚度之事實密切相關之指 因此’本發明之目的在於提供一種於炫鋼之連續禱造中可 ❹更高精度地檢出鑄片上所產生之铸漏,進而防止該铸漏之方 法及裝置。本發明之另-目的在於提供一種更高精度地推定 鑄模出口處之凝固殼厚度之方法及裝置。 * (解決問題之手段) <現象之調査及解析> 凝固殼厚度與鎊模與鑄片之間之排熱狀態有密切相關。 即’若凝固殼厚度薄,則自則傳遞料模之傳熱量增多, ©導致排熱量增多,相反,若凝固殼厚度厚,則自禱片^遞至 鱗模之傳熱量減少,導致排熱量減少。發明者為了更詳細地 研究該事實,對實際之鑄模内之具體之排熱狀態進行 - 查。 。 ' $ 了檢測排熱狀11,必須求得賴之各部位之熱通量 以如下之方法進行。 圖2係鑄模1之剖視圖,其表示自連接於俊槽4〇之底 且設置於鏵模1内之浸潰嘴嘴(immersi〇n纖ie)3嘴出溶 098106495 200946265 鋼5之(箭頭)狀態。於爐浴面上添加有模製粉7(顯示為 層),該模製粉7流入至鑄模1與熔鋼5之空隙中而發揮潤 滑劑之作用。溶鋼5經由該模製粉7而朝鑄模1排熱,一邊 形成凝固殼9,一邊朝鑄模出口被抽出。 圖3係將形成鑄模1之鑄模銅板11 一部分擴大顯示之剖 視圖。為了求得熱通量,必須檢出鑄模銅板11之溫度梯度, 為了檢出該溫度梯度而使用熱電偶17。如圖3所示,於形 成於鑄模銅板11之外侧面的冷卻水通道13之底部形成孔 15,將上述熱電偶17埋設於該孔15中之在深度方向上相隔 固定距離之兩個部位。可根據該埋設之熱電偶17之輸出而 檢出溫度梯度,並可根據該溫度梯度,藉由計算而求得熱通 量。 將兩根熱電偶17之檢出溫度設為T1(°C)、T2(°C),將埋 設間隔設為d(m),並將鑄模1之熱導率設為;I (J/sw°C), 利用下式而算出局部熱通量ql(J/s · m2)。 ql= λ (Tl-T2)/d 於發明者之調査中,例如於鑄模短邊(於水平剖面成長方 體之鑄模中,較短之邊)之情形時,如圖4之黑色圓點標記 所示,在比通常之爐浴面位置更下方之位置,將由設置於鑄 模厚度方向之兩根熱電偶17所構成的一對熱電偶,每隔40 〜200 mm之高度設置於共計9個部位。根據來自該等熱電 偶17之輸出信號,並藉由上式而求得局部熱通量,對該局 098106495 6 200946265 部熱通量與離爐浴面之位置之關係進行調査。 圖5係表示該調査結果一例之圖表,縱軸表示局部熱通量 • (單位:J/s · m2),橫轴表示離爐浴面之距離(單位:咖)。 再者,於本說明書中,將如下圖表之形狀稱為熱通量分布, 該圖表係將縱軸作為局部熱通量,將橫轴作為離爐浴面之距 離而表示局部熱通量與離爐浴面之距離之關係的圖表。 如圖5之圖表所示,局部熱通量自爐浴面朝鑄模出口方向 _ 減少,於離爐浴面之距離為400 mm附近獲得極小值,其後 顯示出短暫增加之傾向,該增加之傾向於離爐浴面之距離約 為600 mm附近顯示出極大值,其後再次減少。 發明者關注於局部熱通量自朝鑄模出口方向減少之傾向 轉變成短暫上升之傾向,進而反覆進行了研究。 局部熱通量顯示出極小值之位置係離爐浴面之距離^ 400匪附近,該位置係與自浸潰喷嘴3之喷出口所喷出的 e 熔鋼5之喷出流(flow from the spout :箭頭)衝擊缚模短 邊之位置相一致(參照圖2)。此種局部熱通量之變化與炫鋼 喷出流之關係說明以下内容。 • 如圖5所示,局部熱通量隨著自爐浴面朝鱗模出口方向前 • 行而減少’此表示熱阻增加’即’如圖2所示,凝固殼厚度 緩慢地變厚。 然後,可認為於自浸潰喷嘴3所喷出的熔鋼5之喷出流衝 擊凝固殼9之位置處’會引起凝固殼9之再熔解,凝固殼厚 098106495 7 200946265 度減少,由熔鋼流動所產生之熱施加於該變薄之凝固殼9 之凝固界面,而導致局部熱通量上升。 而且,可涊為隨著進一步朝鎊造方向之下游前行,熔鋼流 動之影響會消失,局部熱通量再次減少,因此凝固殼厚變厚。 根據以上之研究,可認為某一瞬間之凝固殼9之形狀係如 圖2所示,自爐浴面至局部熱通量之極小值之位置為止,凝 固殼9之厚度增加’又’自局部熱通量之極小值至極大值為 止’凝固殼9之厚度減少,進而,於局部熱通量之極大值之 後,凝固殼9之厚度再次增加。 於鑄模内,經過凝固殼厚度以上述方式變厚或變薄之過程 而決定鑄模出口處之凝固殼厚度。 可認為於鑄模内,凝固殼厚成長之程度與藉由凝固殼9 再炼解而暫時形成的凝固殼9變薄之程度之關係,係與鑄模 出口處之凝固殼厚度有直接相關。進而,若考慮到鑄漏之產 生與鑄模出口處之凝固殼厚度有相關,則可認為上述兩種程 度之關係與有無產生鑄漏有密切相關。 因此’發明者為了調查上述兩種程度、即凝固殼厚成長之 程度與暫時形成之凝固殼9變薄之程度的關係與產生鏵漏 之關聯’進一步反覆地進行了研究。 <凝固界面熱輸入(solidification interface heat input) 之導入> 假設於鑄模内未產生由熔鋼流引起凝固殼再熔解之現象 098106495 8 200946265 例如於未自浸潰喷嘴噴出熔鋼流而僅抽出鱗模内之溶鋼 時4為凝固殼之厚度會自爐浴面朝鱗模出口緩慢增加。 :::產生如上所述之由熔鋼流所引起之凝固殼之再 之距離=的狀態,並假定與圖5相同將橫轴作為離爐浴面 為局部熱通量之圖表’則預計會形成未於 圖5之情形時所觀察到的中途上升之平穩減少曲線。 Φ =二為於該情形時,凝固殼之鑄模出口處之厚度係與 所獲得之值成比例,,若為此種假定之狀況, 貝=4地將上述圖表之熱通量分布作為產生鏵漏之指標。 、主喑 於現實之鑄模时產生如下絲:因由來自浸 二鐵之喷出流所產生的熔鋼流(以下僅稱為「熔鋼流」) :=而產生凝固殼之再熔解’凝固殼9藉由該再熔解而變 薄,同時,排熱量增大。 pb ’認為於存在熔鋼流之影響的狀態下,_殼厚度之 度不僅與排熱量成比例,亦與自實際狀之排熱量減 ;Ί &之〶響所產生之排熱量所獲得之值成比例。可將 .鋼流之影響所產生之排熱#作為熔鋼流對於凝固界 (以下僅稱為「凝固界面熱輸入」)而進行評價。 •V 4、b此考慮,則於自浸潰噴嘴噴出熔鋼之作業狀態下,可 藉疑固界面熱輸入來評價凝固殼變薄之程度,另〆方面’ 可藉由自可 曰 β由熱電偶測定之局部熱通量減去凝固界面熱輸 入所獲叙值來評價凝赌成長之程度。 098106495 9 200946265 因此,可藉由對該等兩個評價量進行比較研究而設為產生 鑄漏之指標。 然而,若將凝固界面熱輸入設為q2(J/s · m2),將自熔鋼 朝凝固界面之熱傳遞係數設為h(J/s · m2 · °C),將熔鋼之過 熱度設為Δ0 (°C),則可以下式表示該凝固界面熱輸入q2。 q2 = h · Δ ^ .........(1) 其中,h=1.22xl05xV°8 V :熔鋼流速(m/s) ΑΘ =T〇-Ts(°C) τ〇:鑄模内熔鋼溫度(°c)BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method and apparatus for accurately detecting a breakout generated on a cast piece in continuous casting of molten steel, thereby preventing the casting. Further, the present invention relates to a continuous casting method of steel using the above-described casting leakage detecting method. Furthermore, this is also a method and apparatus for estimating the thickness of the solidified clam shell in the continuous restraint of steel making. [Prior Art] Yulian, β-cast 4 towel's, after forming a solidified shell by cooling the molten steel injected into the mold to form a solidified shell, it is drawn from the mold, but if it is solidified for some reason If the formation of the shell is insufficient, and there is a portion where the solidified shell is thin, there is a danger of simplification, that is, when the portion of the front shell is thin, the solid shell is broken when the mold exit (the lower end of the die) And lead to refining _ out. If a casting leak occurs on the right, the operation must be stopped. Therefore, it is necessary to select an operation ride that does not cause a prayer, but the material (4) (10) leakage (four) is converted to a low casting speed, which may result in deterioration of operation efficiency, which is not preferable. Based on this background, it is desired to develop a method of accurately shutting off the shaft even if it is made in a high degree of manufacture. Various methods have been proposed at present. For example, the following technique is disclosed in Patent Document 1 (Japanese Patent Publication No. Sho 39 No. 3). The technique is a method for preventing leakage of continuous casting, which is a sheet-type surface heat flux meter disposed on the outer surface of a mold of 098106495 3 200946265, and f corresponds to a heat extraction 〇f mold of the mold. The heat flux is measured and leaked. The continuous casting of the pound leaker; characterized by: by a majority: pass two: to determine the local heat flux of each part of the mold, when the heat flux waveform indicating the temporal change of the heat flux is irritatingly When the value exceeds a predetermined value, the scale is reduced, and the degree is lowered until the wave height is restored to the original state, thereby preventing the production 2. [Inventive content] (Problems to be solved by the invention) ® The technique disclosed in Patent Document 1 uses a heat pass A method for preventing leakage of the heat flux detected by the meter. The local heat flux of each part of the die means that the heat rejection from the die is related to the formation of the solidified shell. Therefore, = / is roughly reasonably predicted that when the change in the heat flux causes an abnormality, the formation of the solidified shell thickness causes an abnormality, and there is a risk of casting leakage. However, considering the exit of the mold, if the thickness of the solidified shell does not reach the thickness of the predetermined crucible, the casting leakage is caused by the change of the heat flux, and the risk of accurate leakage may not be sufficiently grasped. The reason for this is that there is also a case where there is an abnormality in the heat flux in the initial stage of the solidified shell forming process in the mold, as long as a solidified shell is formed in the stage after the solidification forming process, and both are formed at the exit of the cast mold. The solidified shell of the thickness of the crucible can judge the danger of no scale leakage. That is, it is predicted by the change of the local heat flux shown in the previous example that the risk of casting leakage is 098106495 4 200946265, which is difficult enough to be an accurate indicator. As described above, the generation of the scale leakage is directly related to the thickness of the solidified shell at the exit of the prayer mold. If the thickness of the solidified shell can be accurately estimated, the risk of casting leakage can be judged with high precision. That is, the inventors believe that it is important to find out the fact that the thickness of the solidified shell at the exit of the die has been closely related to the fact that the thickness has reached a predetermined thickness. Therefore, the object of the present invention is to provide a continuous prayer in the steel. A method and apparatus for detecting the casting leakage generated on a cast piece with high precision and preventing the casting leakage. Another object of the present invention is to provide a method and apparatus for estimating the thickness of a solidified shell at the exit of a mold with higher precision. * (Means for Solving Problems) < Investigation and Analysis of Phenomena> The thickness of the solidified shell is closely related to the heat removal state between the pound mold and the cast piece. That is, if the thickness of the solidified shell is thin, the amount of heat transfer from the transfer mold increases, and the amount of heat is increased. On the contrary, if the thickness of the solidified shell is thick, the amount of heat transferred from the prayer sheet to the scale mold is reduced, resulting in heat rejection. cut back. In order to study this fact in more detail, the inventors conducted a check on the specific heat-discharging state in the actual mold. . ' $ For detecting the heat exhaustion 11, the heat flux of each part must be obtained in the following manner. Figure 2 is a cross-sectional view of the mold 1 showing the mouth of the dip nozzle (immersi〇n fiber) which is attached to the bottom of the groove 4 and is placed in the die 1 (the ink nozzle 098106495 200946265 steel 5 (arrow) status. Molded powder 7 (shown as a layer) is added to the surface of the furnace bath, and the molded powder 7 flows into the gap between the mold 1 and the molten steel 5 to function as a lubricant. The molten steel 5 is discharged to the mold 1 via the molded powder 7, and the solidified shell 9 is formed while being drawn toward the exit of the mold. Fig. 3 is a cross-sectional view showing a part of the mold copper plate 11 forming the mold 1 in an enlarged manner. In order to obtain the heat flux, the temperature gradient of the mold copper plate 11 must be detected, and the thermocouple 17 is used to detect the temperature gradient. As shown in Fig. 3, a hole 15 is formed in the bottom of the cooling water passage 13 formed on the outer side of the mold copper plate 11, and the above-mentioned thermocouple 17 is buried in the hole 15 at two locations separated by a fixed distance in the depth direction. The temperature gradient can be detected based on the output of the buried thermocouple 17, and the heat flux can be calculated by calculation based on the temperature gradient. The detection temperatures of the two thermocouples 17 are set to T1 (°C) and T2 (°C), the embedding interval is set to d(m), and the thermal conductivity of the mold 1 is set to; I (J/sw °C), the local heat flux ql (J/s · m2) is calculated by the following equation. Ql= λ (Tl-T2)/d In the investigation of the inventor, for example, in the case of the short side of the mold (in the mold of the horizontal section growth cube, the shorter side), the black dot mark of Fig. 4 It is shown that a pair of thermocouples composed of two thermocouples 17 provided in the thickness direction of the mold are disposed at a total of nine locations at a height of 40 to 200 mm at a position lower than the position of the normal bath surface. Based on the output signals from the thermocouples 17, and the local heat flux was obtained by the above equation, the relationship between the heat flux of the 098106495 6 200946265 portion and the position of the bath surface was investigated. Fig. 5 is a graph showing an example of the results of the investigation, in which the vertical axis represents the local heat flux (unit: J/s · m2), and the horizontal axis represents the distance from the bath surface (unit: coffee). In addition, in the present specification, the shape of the following chart is referred to as a heat flux distribution, and the graph shows the vertical heat flux as a local heat flux and the horizontal axis as a distance from the bath surface to indicate local heat flux and distance. A graph of the relationship between the distances of the bath surfaces. As shown in the graph of Fig. 5, the local heat flux decreases from the furnace bath surface toward the mold exit direction, and a minimum value is obtained at a distance of 400 mm from the bath surface, which then shows a tendency to increase temporarily, which increases. It tends to show a maximum value near the bath surface at a distance of about 600 mm, and then decreases again. The inventors paid attention to the tendency of the local heat flux to decrease from the direction toward the exit of the mold to become a transient rise, and further studied it. The position where the local heat flux shows a minimum value is the distance from the bath surface ^ 400 ,, which is the ejected flow of the e-melting steel 5 ejected from the discharge port of the self-immersion nozzle 3 (flow from the Spout: arrow) The position of the short side of the impact die is the same (refer to Figure 2). The relationship between this change in local heat flux and the discharge of the Hyungang steel illustrates the following. • As shown in Fig. 5, the local heat flux decreases as it goes from the furnace bath surface toward the scale die exit direction. This indicates an increase in thermal resistance. That is, as shown in Fig. 2, the solidified shell thickness gradually increases. Then, it can be considered that the position at which the ejected stream of the molten steel 5 ejected from the dip nozzle 3 impinges on the solidified shell 9 causes re-melting of the solidified shell 9, and the solidified shell thickness is reduced by 098106495 7 200946265 degrees by the molten steel. The heat generated by the flow is applied to the solidification interface of the thinned solidified shell 9, resulting in an increase in local heat flux. Moreover, it can be said that as the further progress toward the direction of the pound, the influence of the flow of the molten steel disappears, and the local heat flux decreases again, so that the solidified shell thickness becomes thicker. According to the above research, it can be considered that the shape of the solidified shell 9 at a certain moment is as shown in Fig. 2, and the thickness of the solidified shell 9 is increased from the position of the furnace bath surface to the minimum value of the local heat flux. The thickness of the solidified shell 9 is reduced from the minimum value of the heat flux to the maximum value, and further, the thickness of the solidified shell 9 increases again after the maximum value of the local heat flux. In the mold, the thickness of the solidified shell at the exit of the mold is determined by the process of thickening or thinning the thickness of the solidified shell in the above manner. It is considered that the relationship between the degree of growth of the solidified shell thickness and the degree of thinning of the solidified shell 9 which is temporarily formed by refining of the solidified shell 9 in the mold is directly related to the thickness of the solidified shell at the exit of the mold. Further, considering that the occurrence of the casting leakage is related to the thickness of the solidified shell at the exit of the mold, it is considered that the relationship between the above two degrees is closely related to the presence or absence of casting leakage. Therefore, the inventors have further studied in order to investigate the relationship between the above two degrees, that is, the degree of growth of the solidified shell thickness and the degree of thinning of the temporarily formed solidified shell 9 and the occurrence of leakage. <Introduction of solidification interface heat input> It is assumed that the solidified shell is not melted by the molten steel flow in the mold. 098106495 8 200946265 For example, the molten steel flow is not ejected from the impregnation nozzle and only extracted. When the molten steel in the scale mold is 4, the thickness of the solidified shell will gradually increase from the furnace bath surface toward the scale die exit. ::: A state in which the distance from the solidified shell caused by the molten steel flow is as described above, and it is assumed that the horizontal axis is the same as the partial heat flux from the furnace surface as shown in Fig. 5 A steady reduction curve of midway rise observed when not in the case of Fig. 5 was formed. Φ = two is the case where the thickness at the exit of the mold of the solidified shell is proportional to the value obtained, and if it is such a hypothetical condition, the heat flux distribution of the above chart is taken as the generation 铧The indicator of leakage. When the main mold is used in reality, the following wire is produced: the molten steel flow (hereinafter referred to as "melted steel flow") generated by the jet flow from the immersed iron: = and the re-melting of the solidified shell is formed. 9 is thinned by the remelting, and at the same time, the amount of heat removal is increased. Pb 'is considered that in the presence of the influence of the molten steel flow, the degree of the thickness of the shell is not only proportional to the amount of heat discharged, but also to the amount of heat exhausted from the actual heat; the heat generated by the sound of the Ί & The value is proportional. The heat rejection # generated by the influence of the steel flow can be evaluated as a molten steel flow for the solidification boundary (hereinafter simply referred to as "solidification interface heat input"). • V 4, b This consideration can be used to evaluate the degree of thinning of the solidified shell by the suspected solid interface heat input in the working state of the molten steel from the impregnation nozzle, and the other aspect can be determined by The local heat flux measured by the thermocouple minus the heat input obtained from the solidification interface is used to evaluate the extent of gambling growth. 098106495 9 200946265 Therefore, it is possible to set an index for casting leakage by performing a comparative study on the two evaluation amounts. However, if the heat input to the solidification interface is set to q2 (J/s · m2), the heat transfer coefficient of the self-melting steel toward the solidification interface is h (J/s · m2 · °C), and the superheat of the molten steel is obtained. When Δ0 (°C) is set, the solidification interface heat input q2 can be expressed by the following formula. Q2 = h · Δ ^ ... (1) where h = 1.22xl05xV°8 V : molten steel flow rate (m/s) ΑΘ = T〇-Ts (°C) τ〇: mold Inner molten steel temperature (°c)
Ts :熔鋼固相線溫度(°c) 再者,對於鑄模内熔鋼溫度T〇(°C)而言,可實際測定鑄模 内熔鋼溫度,亦可例如根據餵槽(TD)内熔鋼溫度(實測值), 藉由以下之鑄模内熔鋼溫度估計方程式而計算出。 T〇= 705. 156+ 0. 544086 · Ttd-2. 35053 · Vc- 0. 00303 · W + 18. 12663 · (0. 10181nFC- 0. 3362) 其中,Ttd : TD内熔鋼溫度(°C)(實測值)Ts: molten steel solidus temperature (°c) In addition, for the molten steel temperature T〇(°C) in the mold, the molten steel temperature in the mold can be actually measured, for example, according to the feed tank (TD) melting The steel temperature (measured value) was calculated by the following equation for estimating the molten steel temperature in the mold. T〇= 705. 156+ 0. 544086 · Ttd-2. 35053 · Vc- 0. 00303 · W + 18. 12663 · (0. 10181nFC- 0. 3362) where Ttd : TD inner molten steel temperature (°C ) (measured value)
Vc :鑄造速度(m/分) W :鑄造寬度(m)(實測值) FC :施加電流值(A)(實測值) 如上所述,凝固界面熱輸入q2係為與熱傳遞係數h相關 之量,而熱傳遞係數h係為與炼鋼流速V相關之量。因此, 098106495 10 200946265 為了在線測定凝固界面熱輸入q2,則必須在線測定鑄模内 之熔鋼流速V。然而,難以於作業狀態下在線測定熔鋼流速 V 〇 因此,發明者考慮了如下方法:預先對以各種鑄造速度所 鑄造之鑄片進行採樣,根據該鑄片之枝晶傾角(dendrite angle)求得各鑄造速度之熔鋼流速值,而求得基於該熔鋼流 速值之凝固界面熱輸入q2。此處,所謂枝晶傾角,係指相 ❹對於法線方向而自表面朝厚度方向延伸之枝晶之一次枝之 傾角,該法線方向係相對於鑄片表面之法線方向,習知上述 枝晶傾角與熔鋼流速值有相關。 將該預先求得之凝固界面熱輸入q2稱為「穩定狀態之凝 固界面熱輸入q2」,並將其記作穩定凝固界面熱輸入以叫。 再者’使用稱為敎狀態之料之目的在於騎如浸潰喷嘴 中存在堵塞等、及於箱流速中存在偏流之類之異常狀態。 ® 接著’發明者考慮了如下方法:於欲推定矯模出口處之凝 固殼厚度或者欲評價有無產生鑄漏之作餘態下,就自利用 熱電偶所測定之局部熱通量減去穩定凝固界面熱輸入“ .而餅之齡,求得熱通量分布,並根據職通量分布來評 -價鑄模出口處之凝固殼厚或者有無產生禱漏。考慮以上述方 式自實際測定之局部熱通量減去穩定凝固界面熱輸入‘ 之理由如下所述。 田與自作業狀態下所實際測定之局部熱通量減去穩定凝 098106495 11 200946265 固界面熱輸入q2ree而獲得之熱量相關的熱通量分布成為平 穩減少之曲線時’表示該熱通量分布係與上述未自浸潰噴嘴 喷出熔鋼流而僅抽出鑄模内之熔鋼時之熱流速分布相同。此 表示作業狀態下之凝固界面熱輸入q2與穩定凝固界面熱輸 入q2reg相同。即,於該狀態之情形時,使凝固殼變薄之程 度與通常之由來自浸漬喷嘴之熔鋼流所造成之程度相同’即 與穩定狀態相同,若為此種狀況,則只要鑄模之冷卻如通常 般進行’凝固殼如通常般成長’便可評價為未產生鑄漏。又, 若為此種狀況’則可根據與自實際測定之局部熱通量減去穩 定凝固界面熱輸入q2reg而獲得之熱量相關的熱通量分布, 推定鑄模出口處之凝固殼厚度。 再者,作為應注意之點,當凝固界面熱輸入q2與穩定凝 固界面熱輸入q2reg相同時,可謂不會產生如下鑄漏(以下稱 為「再溶解性鱗漏」)之危險’該鑄漏係由於凝固界面熱輸 入q2之增加導致凝固界面再溶解而引起者,但即便於該情 形時,在熔鋼自彎月面移動至鑄模下端出口為止之期間,有 助於凝固殼厚度之成長的排熱量小,當凝固殼於該移動期間 未充分成長而導致其厚度較薄時,亦存在產生由有助於凝固 殼厚之成長的排熱量小所引起鑄漏(以下僅稱為「排熱不足 性禱漏」)之危險。 另一方面,當與自利用熱電偶所測定之局部熱通量減去穩 定凝固界面熱輸入q2reg所獲得之熱量相關的熱通量分本於 098106495 12 200946265 ’Ί面相距某―距離之位置處上升時,即,如熱通量分布 具有極j值並可形成凸起部分時,表示實際之凝固界面熱輪 卩2大於穩定凝111界面熱輸人q2reg,認為於該狀態下,凝 • 口 <之再熔解程度崎穩定狀態。例如為如下情形:於鱗模 内因反潰噴嘴之堵塞等而導致溶鋼流產生偏流,作為測定 對象的鑄模界面之熱輪入比通常增大。 ㈣ItM’㈣凸起部分之大小程度表示比通常之凝固 ❿界面熱輸人q2還大之熱輪人。即,可作出如下評價:該凸 起。P刀之大J、程度係為使因異常之炼鋼流而引起的凝固殼 再熔解而使凝固威厚度變薄之程度,當該程度較大時,即 便以通常方式對鎢模進行冷卻亦存在產生再熔解性轉漏之 危險性。 如此,求付與自實際剛定之局部熱通量減去穩定凝固界面 熱輸入q2reg所獲得之熱量相關的熱通量分布,藉此,可根 ❹據該熱通量分布中有無W部分㈣凸起部分之大小程 度’明確地把握與穩定狀態減’凝固殼之再轉程度為何 種程度,而可推定_模出口處之㈣殼厚度,同時,可根據 -該厚度等來評價產生再炫解性禱漏之危險性。 又藉由求彳于纟二除去凸起部分之排熱熱量,亦可評價產生 排熱不足性鎊漏之危險性。 <總熱通量Ql、Q2之導入> 因此’發明者針對各種鱗造速度之情形,根據枝晶傾角而 098106495 13 200946265 求得熔鋼錢,並崎各靖料求得穩级目界面熱輸入 q—2reg’自於作餘態下利賴電偶所敎之排熱量減去該穩 定凝固界面熱輸入q2reg,隨之求得熱通量分布根據誠 通量分布來推定凝固殼厚度,並進—步對有無產生鎊漏進行 研究。 以下,對該研究内容加以具體說明。 圖6係將熔鋼流速作為縱軸,將離爐浴面之距離作為橫 軸,於鑄造速度Vc=2.54 m/分、鎢造寬度W=1議匪之 情形下’根據鑄片之枝晶傾角*求得熔鋼流速(m/s)與離爐 浴面之距離(mm)之關係的圖表。 由該圖表求得熔鋼流速V(m/s),並根據上述(1)式求得穩 定凝固界面熱輸人q2“g。接著’彻熱電偶對操作狀態下 之局部熱通4祕丨狀’自測紐與辦敎到之作業 狀態相同的鎊造速度下之穩定凝固界面熱輪入仏,求得 減去後所獲得熱量之熱通量分布。 g 圖7之縱軸表示局部熱通量U/s · m2),横轴表示離爐浴 面之距離(_,又,圖表中黑圓圈之值(Dl)表示由孰電偶測 得之測定值’白圆圈之值⑽表示從由熱電偶測得之測定值 減去穩定凝固界面熱輸入q2reg所獲得之值(ql —Vc : casting speed (m/min) W : casting width (m) (measured value) FC : applied current value (A) (measured value) As described above, the solidification interface heat input q2 is related to the heat transfer coefficient h The amount, and the heat transfer coefficient h is the amount related to the steelmaking flow rate V. Therefore, 098106495 10 200946265 In order to measure the solidification interface heat input q2 on-line, the molten steel flow rate V in the mold must be measured online. However, it is difficult to measure the molten steel flow rate V 在线 in the working state. Therefore, the inventors considered a method of sampling a cast piece cast at various casting speeds in advance, and calculating the dendrite angle of the cast piece. The melt flow rate value of each casting speed is obtained, and the solidification interface heat input q2 based on the molten steel flow rate value is obtained. Here, the dendrite angle refers to the inclination of the first branch of the dendrite extending from the surface toward the thickness direction with respect to the normal direction. The normal direction is relative to the normal direction of the surface of the cast piece. The dendrite angle is related to the melt flow rate value. The previously obtained solidification interface heat input q2 is referred to as "stabilized solidification interface heat input q2", and is referred to as a stable solidification interface heat input. Further, the purpose of using a material called a crucible state is to ride an obstacle such as a clogging in a dipping nozzle, and an abnormal state such as a drift in a tank flow rate. ® Then the 'inventor considered the following method: to estimate the local heat flux measured by the thermocouple minus the stable solidification when it is desired to estimate the thickness of the solidified shell at the exit of the mold or to evaluate whether or not there is a casting leak. The interface heat input ". and the age of the cake, the heat flux distribution is obtained, and according to the distribution of the occupational flux, the solidified shell thickness at the exit of the price casting mold or the presence or absence of a pray leak is considered. Consider the local heat measured by the above method. The reason for the flux minus the heat input at the stable solidification interface is as follows: The local heat flux actually measured in the field and the self-operating state minus the heat-related heat flux obtained by the stable interface 098106495 11 200946265 solid interface heat input q2ree When the quantity distribution becomes a curve of steady reduction, it is indicated that the heat flux distribution is the same as the heat flow rate distribution when the molten steel is not discharged from the impregnation nozzle and only the molten steel in the mold is extracted. This indicates solidification in the working state. The interface heat input q2 is the same as the stable solidification interface heat input q2reg. That is, in the case of this state, the degree of solidification of the solidified shell is generally the same as that from the impregnation nozzle. The flow is caused to the same extent 'that is the same as the steady state. If this is the case, as long as the cooling of the mold is carried out as usual, the 'solidified shell grows as usual' can be evaluated as not producing a casting leak. The condition can be based on the heat flux distribution associated with the heat obtained from the actual measured local heat flux minus the steady solidification interface heat input q2reg, and the thickness of the solidified shell at the exit of the mold is estimated. When the solidification interface heat input q2 is the same as the stable solidification interface heat input q2reg, it is said that the following casting leakage (hereinafter referred to as "re-dissolving scale leakage") does not occur. The casting leakage system is due to the solidification interface heat input q2. The increase causes the solidification interface to be re-dissolved, but even in this case, during the period from the molten steel moving from the meniscus to the lower end of the mold, the heat generation which contributes to the growth of the solidified shell thickness is small, when the solidified shell When the thickness is not sufficiently increased during the movement, the amount of heat generated by the growth of the solidified shell thickness is small (hereinafter referred to as " The danger of insufficient heat exhaustion. On the other hand, when the heat flux associated with the local heat flux measured from the use of the thermocouple minus the heat input from the stable solidification interface heat input q2reg is 098106495 12 200946265 'the position of the face is at a distance from the distance When rising, that is, if the heat flux distribution has a pole value of j and can form a convex portion, it means that the actual solidified interface hot rim 2 is larger than the stable condensed 111 interface heat input q2reg, and it is considered that in this state, the condensation port <The remelting degree is stable. For example, in the scale mold, the molten steel flow is biased due to clogging of the reverse nozzle, and the heat wheel ratio of the mold interface to be measured is generally increased. (4) The size of the convex portion of ItM' (4) indicates that the hot wheel person is larger than the normal solidified ❿ interface heat input person q2. That is, the following evaluation can be made: the convexity. The greater the degree of the P-knife is the degree to which the solidified shell is remelted due to the abnormal steelmaking flow, and the thickness of the solidification is reduced. When the degree is large, even if the tungsten mold is cooled in the usual manner, There is a risk of producing remelting slips. In this way, the heat flux distribution associated with the heat obtained from the actual localized heat flux minus the steady solidification interface heat input q2reg is obtained, whereby the W portion (four) convex in the heat flux distribution can be determined. The degree of the size of the part is 'clearly grasped and the steady state minus the degree of re-rotation of the solidified shell, and the thickness of the shell of the (four) exit at the exit of the mold can be estimated, and at the same time, the re-darkness can be evaluated according to the thickness The danger of sexual prayer. Further, by removing the heat of heat removal from the convex portion by the second step, it is also possible to evaluate the risk of generating an exhaustion-deficient pound leak. <Importing of total heat fluxes Q1 and Q2> Therefore, the inventor obtained the molten steel money according to the dip angle of the decidation angle of 098106495 13 200946265 for the various scales, and the stability of the interface was obtained. The heat input q-2reg' is calculated from the heat dissipation of the Lily galvanic couple in the residual state minus the heat input q2reg of the stable solidification interface, and the heat flux distribution is determined according to the distribution of the solid flux to estimate the thickness of the solidified shell. Further progress is made to study whether or not there is a pound leak. The contents of this study will be specifically described below. Figure 6 shows the flow rate of the molten steel as the vertical axis and the distance from the bath surface as the horizontal axis. Under the condition of casting speed Vc=2.54 m/min and tungsten manufacturing width W=1, the dendrites according to the cast piece Inclination* Find a graph of the relationship between the melt flow rate (m/s) and the distance from the bath surface (mm). From the chart, the molten steel flow rate V (m/s) is obtained, and the stable solidification interface heat input q2 "g is obtained according to the above formula (1). Then the 'hot thermocouple pair local heat flux 4 in the operating state is secreted. The shape of the self-test is the same as the steady-state solidification interface under the pound-making speed, and the heat flux distribution obtained after subtraction is obtained. g The vertical axis of Figure 7 indicates local heat. Flux U/s · m2), the horizontal axis represents the distance from the bath surface (_, again, the value of the black circle in the graph (Dl) indicates the measured value measured by the 孰 couple, the value of the white circle (10) indicates The measured value obtained by the thermocouple minus the value obtained by the stable solidification interface heat input q2reg (ql —
圖8係由圖7中之白圓圈所描繪之_矣,B T之圖表’即示意性地表示 (dl-之熱通量分布之圖’其係對由圖表所包圍之面 積、即局部鏡量之累計值(、_通量)之求法―例進行說明 098106495 14 200946265 之說明圖。 以下,根據圖8對總熱通量之求法進行說明。 首先,如圖8所示,將圖表分割成複數個梯形,藉此求得 各梯形之面積(Q1-1〜Q1-7),藉由將該等面積相加而求得整 體之面積Q。 接著,將圖表中之極小點設為A,將極大點設為B,將鑄 模出口之點設為C,並將三角形ABC作為凸起部分,以如下 φ 之方式求得該凸起部分之面積、即三角形ABC之面積Q2(參 照圖9)。 若將對應於點A之橫軸上之點設為A’,將對應於點C之 橫軸上之點設為C’,求得梯形ACC’ A’之面積Q1-8,並將該 Q1-8與Q1-1〜Q1-3相加所得之面積作為Q1,則求得Q2 = Q -Q卜 根據以上述方式求得之Q1與Q2,對在各個鑄造條件下, φ 該等Q1與Q2與有無產生鑄漏之關係進行研究。將其結果示 於表1。關於有無鑄漏,當殼厚度達到臨限值6丽以下時, 判定為「有」產生鑄漏。 098106495 15 200946265 [表1 ] 研究例 Q1 Q2 有無產生鑄漏 (kJ/ra2) (kJ/m2) 1 19000 1200 無 2 17900 1450 無 3 25000 540 無 4 27000 1500 無 5 28000 3500 無 6 31500 5000 無 7 33500 8500 無 8 27500 6850 無 9 26000 10050 無 10 19500 3550 無 11 18900 4090 無 12 17800 3950 無 13 17900 4500 有 14 19000 5700 有 15 19070 5950 16 19450 7500 有 17 20570 8500 有 18 14000 1000 有 19 13300 100 20 12500 1020 Μ 21 11700 1500 有 22 10500 3200 有 23 9750 1500 Μ 24 8050 300 25 7650 450 有 26 6500 270 有 27 5450 55 有 28 4890 150 Μ 29 14500 10800 有 30 13000 9000 Μ 31 12700 9500 有 32 10700 8000 有 33 10200 7500 有 34 9000 6000 有 35 7050 5500 36 8650 8200 有 37 7400 4500 有 38 5100 4700 39 7150 6800 有 40 6950 6500 有 圖10係於將橫軸設為Ql(kJ/m2),將縱軸設為Q2(kJ/m2) 之座標平面内,對表1中所示之數值進行繪圖,進而根據與 有無產生鑄漏之關係而將座標平面分割成5個區域來表 098106495 16 200946265 示。區域之邊界線為 Ql(a 1)=15〇〇〇(kJ/m2),Q1(a2)== 21000(kJ/m2) > Q2(yS ) = 45〇〇(kj/m2) 0 再者,於圖10所示之區域中,區域(1)〜(3)為有產生鎊 漏危險之區域(即’於上述調査中判定為「有」鑄漏之區域), 區域(4)、(5)為無產生鑄漏危險之區域。 首先,對以有產生鑄漏危險而共通之區域(丨)〜(3)進行比 較研究。 ❹ 〈區域(1)> 可將區域(1)(Q1< αΐ且收2召)評價為如下區域:其Q1 較小且Q2較大,存在產生排熱不足性鑄漏之危險與產生再 熔解性鑄漏之危險此兩者。而且,由於區域中實際上有 產生鑄漏,因此可謂該鑄漏係具有排熱不足性鑄漏及再熔解 性鑄漏此兩者之性質者。 再者,若自凝固殼厚度之觀點來考慮區域(1)之狀態,則 ❹認為存在如下部分,而變薄之程度較大,該部分係凝固殼整 體之厚度因Q1較小而變薄’且凝固殼之厚度因q2較大而局 部變薄之部分。 <區域(2)> 可將區域(2)(Q1< α 1且Q2<冷)評價為如下區域:其卯 小,存在產生排熱不足性鑄漏之危險,但由於其收亦小, 因此產生再炼解性鎊漏之危險性小。而且,由於區域(2)中 實際上有產生鑄漏,因此可謂該鑄漏係具有排熱不足性鑄漏 098106495 17 200946265 之性質者。 再者’若自凝固殼厚度之觀點來考慮區域(2)之狀態,則 認為無論是否存在如下部分,變薄之程度均較小,該部分係 凝固设整體之厚度因Q1較小而較薄,但凝固殼之厚度因Q2 較小而局部變薄之部分。 <區域(3 ) > 可將區域(3)(〇:lSQlSa2且卩22召)評價為如下區 域:其Q1比較大而較少有產生排熱不足性鑄漏之危險,但 由於Q2較大,因此有產生再熔解性鑄漏之危險。而且,由 於區域(3)中實際上有產生鑄漏,因此可謂該鑄漏係具有再 熔解性鑄漏之性質者。 再者,若自凝固殼厚度之觀點來考慮區域之狀態,則 認為存在如下部分,且變薄之程度較大,該部分係凝固殼整 體之厚度因Q1較大而比較厚,但凝固殼之厚度因Q2較大而 局部變薄之部分。 其次,對未產生鑄漏之區域(4)、(5)進行比較研究。 <區域(4) > 可將區域(4)(Q1> α2且Q22/3)評價為如下區域:其Q1 較大而較少有產生排熱不足性鑄漏之危險,但由於收亦較 大,因此有產生再熔解性铸漏之危險。然而,由於該區域(4) 中未產生铸漏,因此可認為:因有助於凝固殼厚度成長之排 熱量足夠大,故即便存在凝固殼整體之厚度較厚而局部之凝 098106495 18 200946265 固殼變薄之部位,亦不至於產生鑄漏。 <區域(5)> 可將區域(5)(Q1> α 1且Q2<召)評價為如下區域:其Q1 比較大而較少有產生排熱不足性鑄漏之危險,且由於Q2較 小,因此亦無產生再熔解性鑄漏之危險。而且,由該區域(5) 中未產生鑄漏可認為因有助於凝固殼厚成長之排熱量較Figure 8 is a diagram of _矣, BT of Figure BT, which is schematically represented by a white circle in Figure 7 (a diagram of the heat flux distribution of dl - which is the area enclosed by the graph, that is, the local mirror amount Explanation of the cumulative value (, _ flux) - an example of the description of 098106495 14 200946265. Hereinafter, the method of calculating the total heat flux will be described based on Fig. 8. First, as shown in Fig. 8, the graph is divided into plural numbers. The trapezoidal shape is used to obtain the area of each trapezoid (Q1-1 to Q1-7), and the area Q is obtained by adding the areas. Next, the minimum point in the graph is set to A, The maximum point is set to B, the point of the exit of the mold is set to C, and the triangle ABC is taken as a convex portion, and the area of the convex portion, that is, the area Q2 of the triangle ABC (see Fig. 9) is obtained as follows. If the point on the horizontal axis corresponding to the point A is A', the point on the horizontal axis corresponding to the point C is set to C', and the area Q1-8 of the trapezoidal ACC'A' is obtained, and the Q1 is obtained. -8 and the area obtained by adding Q1-1 to Q1-3 as Q1, then Q2 = Q - Q is obtained according to Q1 and Q2 obtained in the above manner, for each casting Under the conditions, φ The relationship between Q1 and Q2 and the presence or absence of casting leakage is studied. The results are shown in Table 1. Regarding the presence or absence of casting leakage, when the thickness of the shell reaches the threshold of 6 liters or less, it is judged as "Yes". Produce a casting leak. 098106495 15 200946265 [Table 1] Study Example Q1 Q2 Is there a casting leak (kJ/ra2) (kJ/m2) 1 19000 1200 No 2 17900 1450 No 3 25000 540 No 4 27000 1500 No 5 28000 3500 No 6 31500 5000 No 7 33500 8500 No 8 27500 6850 No 9 26000 10050 No 10 19500 3550 No 11 18900 4090 No 12 17800 3950 No 13 17900 4500 There are 14 19000 5700 There are 15 19070 5950 16 19450 7500 There are 17 20570 8500 There are 18 14000 1000 There are 19 13300 100 20 12500 1020 Μ 21 11700 1500 with 22 10500 3200 with 23 9750 1500 Μ 24 8050 300 25 7650 450 with 26 6500 270 with 27 5450 55 with 28 4890 150 Μ 29 14500 10800 with 30 13000 9000 Μ 31 12700 9500 32 10700 8000 with 33 10200 7500 with 34 9000 6000 with 35 7050 5500 36 8650 8200 with 37 7400 4500 with 38 5100 4700 39 7150 6800 with 40 6950 6500 In the coordinate plane where the horizontal axis is Q1 (kJ/m2) and the vertical axis is Q2 (kJ/m2), the values shown in Table 1 are plotted, and the casting leak is generated depending on the presence or absence of The relationship is divided into five areas to the table 098106495 16 200946265. The boundary line of the region is Ql(a 1)=15〇〇〇(kJ/m2), Q1(a2)== 21000(kJ/m2) > Q2(yS ) = 45〇〇(kj/m2) 0 In the area shown in FIG. 10, the areas (1) to (3) are areas where there is a risk of pound leakage (ie, the area determined as "having" in the above investigation), the area (4), (5) It is an area where there is no danger of casting leakage. First, a comparative study was conducted on areas (丨)~(3) common to the risk of casting leakage. 〈 <Area (1)> The area (1) (Q1<αΐ and 2 calls) can be evaluated as the following area: Q1 is small and Q2 is large, and there is a danger of generating heat-exhaust leakage and generating The danger of melt-casting leaks is both. Further, since the casting leakage actually occurs in the region, it can be said that the casting leakage system has the properties of both the heat-dissipating casting leakage and the re-melting casting leakage. Further, if the state of the region (1) is considered from the viewpoint of the thickness of the solidified shell, the following portion is considered to be present, and the degree of thinning is large, and the thickness of the whole solidified shell is thinned due to the small Q1. And the thickness of the solidified shell is partially thinned due to the large q2. <Zone (2)> The area (2) (Q1 < α 1 and Q2 <cold) can be evaluated as the following area: the small area is small, and there is a risk of causing an exhaustion of the exhaust heat, but since it is small Therefore, the risk of re-refining pounds is small. Moreover, since the casting leakage actually occurs in the region (2), it can be said that the casting leakage system has the property of the heat-dissipating casting leakage 098106495 17 200946265. Furthermore, if the state of the region (2) is considered from the viewpoint of the thickness of the solidified shell, it is considered that the degree of thinning is small regardless of whether or not the following portion exists, and the thickness of the solidified portion of the portion is thinner due to the smaller Q1. However, the thickness of the solidified shell is partially thinned due to the small Q2. <Zone (3) > The area (3) (〇: lSQlSa2 and 卩22call) can be evaluated as the following area: Q1 is relatively large and there is less danger of causing insufficient heat-exhaust casting, but since Q2 is more Large, so there is a danger of remelting casting leakage. Further, since the casting leakage is actually generated in the region (3), it can be said that the casting leakage system has the property of remelting casting leakage. Further, if the state of the region is considered from the viewpoint of the thickness of the solidified shell, it is considered that the following portion exists and the degree of thinning is large, and the thickness of the whole solidified shell of the portion is relatively thick due to the large Q1, but the solidified shell is The thickness is partially thinned due to the large Q2. Secondly, a comparative study was conducted on the regions (4) and (5) where no casting leakage occurred. <Zone (4) > The region (4) (Q1 > α2 and Q22/3) can be evaluated as the following region: Q1 is large and there is less danger of causing insufficient heat-extraction casting, but Larger, so there is a danger of remelting casting leakage. However, since no casting leakage occurs in this region (4), it can be considered that the heat generation amount which contributes to the growth of the solidified shell thickness is sufficiently large, so that even if the thickness of the solidified shell as a whole is thick, the partial condensation is 098106495 18 200946265 The thinning of the shell does not cause casting leakage. <Zone (5)> The region (5) (Q1 > α 1 and Q2 < call) can be evaluated as the following region: Q1 is relatively large and there is less risk of causing heat-exhaustion leakage, and due to Q2 It is small, so there is no danger of remelting casting. Moreover, the occurrence of the casting leakage in the region (5) is considered to be due to the amount of heat generated to contribute to the solidification of the shell thickness.
❹ 大,故凝固殼整體之厚度較厚,且局部無凝固殼變薄之部 位,即便有凝固殻變薄之部位,變薄之程度亦較小。 由上述區域(4)、(5)之研究可知:若對區域(4)之狀態與 區域(5)之狀態進行比較’則更佳為區域(5)之狀態。因此, 當將有產生鑄漏的區域(1)〜(3)之狀態轉變成無產生鎊漏 之狀態時,轉變成區域(4)之狀態亦達有效,但更佳為對操 作條件進行控制,以進一步轉變成區域(5)之狀態。 具體而言,當為區域(1)之狀態時,只要以增大卯而轉變 成區域(4)之狀態,或者進而減小Q2而轉變成區域(5)之狀 態之方式,對操作條件進行控制即可。又,當處於區域 之狀態時,只要以增大讥而轉變成區域(5)之狀態之方式, 對操作條件進行#制即可。&而,當處於區域⑶之狀態時, 只要以減小Q2而轉變成區域⑸之狀態,或者增大qi而轉 變成區域⑷之狀態之方式’對操作條件進行控制即可。 作為增大Q1之操作條件之控制,可列舉降低缚造速度及/ 或加強鑄模冷卻。又,作為減小Q2之操作條件之控制,可 098106495 19 200946265 列舉將電磁制動裝置例如配置於鑄模中之浸漬嘴嘴喷出孔 之上部、下部,藉由施加直流磁場而減慢熔鋼流速。 再者,以上所說明之方法之基本點在於:求得熔鋼自爐浴 面到達鑄模出口為止之期間内朝凝固界面熱輸入之熱通量 Ql與穩定凝固界面熱輸入q2reg,並根據(ql —q2reg)之熱通 量分布而判斷是否會產生鑄漏。除此以外之說明為例示並 不受限於上述内容。 例如亦可根據鑄模冷卻水之入口侧、出口侧之溫度而求得 熱通量ql。又,亦可根據例如藉由鑄模内數值模擬而獲得 之熔鋼流速之推定值之結果,求得穩定凝固界面熱輸入 Q2reg。 (Ql —q2res)之熱通量分布之解析方法最佳為於計算出上 述Q1及Q2後進行,但並不受限於此。例如亦可單純地將上 述凸起部分之高度及位置作為鑄漏產生風險之判定基準(例 如一般認為於衝擊凝固界面之熔鋼流較強且變動較激烈之 設備之情形時較為有效)。 、 者w使用Q1及Q2進行解析時,於熱通量分布中未產 生極小值及凸起部分之情形時,設為= 圖8)、Q2 = 0 即可。於難以日日 確(ql — q2reg)之極小值(例如該極小值不明 :圖了現兩處以上之極小值)之情形時,只要以儘可能接近 所不之圖案之方式描繪近似曲線,求得自(ql —q2reg) 降曲線(對應於圖9之Ql之曲線,即’越接近爐浴面, 098106495 200946265 局部熱通量之降低量 可0 越大之曲線)脱離而成為極小之點艮 又,較佳為考慮Q1 定殼厚度或列定鑄漏。 面,且Q2之變動較小4 推定精度與到定精度 與Q2此兩者,但亦可僅使用Q1來推 。例如於期待溶鋼流不易到達凝固界 <情形時,即便不考慮Q2,亦可期待 當要求得Ql、Q2時, <下降較少。 ❹ 形法)以外之積分手段。 邊界線AC無須為直線, 當然亦可使用以上所說明之方法(才弟 。又,於圖9之解析中,Q1與Q2之 ,例如亦可考慮自爐浴面至A為止之 曲線4而求得為近似曲線。 即便當使用Q1及q2進行具體之鑄漏判定時,亦不受限於 上述說明之方法,只要適當地將Q1用作由凝固引起之排熱 量之指標(即,藉由數值之增大而降低鑄漏之風險之因數), 將Q2用作超過穩定的凝固界面熱輸入之指標(即,藉由數值 ❹ 之增大而增大鑄漏之風險之因數)即可。 然而,由於存在較多之對應於凝固殼厚之成長與收無關 而不充分之情形(上述區域(1)及區域(2))之Ql< α 1、及對 • 應於凝固殼厚之成長與Q2無關而充分避免鑄漏之情形(上 , 述區域(5)之Ql> α2之部分及區域(4))之Qi> α2,因此 較佳為預先設定各個邊界地αΐ及。 於該情形時’ α 1 SQl S α 2之區域成為受到收大小之影 響之區域,因此根據卯之值而判定為有鑄漏之危險即可。 098106495 21 200946265 即’於該情形時’較佳為#達到預先設定之臨限值以上時, 判定為有_之危險。則2之臨限值較佳係根據W而決 定’但最終’亦可於al“Ua2之整個範财設為固定 值。上述表1例之々相當於該固定值。 - 作為其他方法’可考慮進一步細化α^ ^ ,於每個 - 區域中設定臨限值。例如設定《3蝴α1<α3<α4< α 2) ’於化Q1 < α 3之情形時,將❽点}設為對應於產 生鎊漏之條件,於α3_< α4之情形時,將料 對應於產生鑄漏之條件,於α4_$α2之情形時,將q =石3认為對應於產生鑷漏之條件。再者,於該情形時通常 β\< β2<β3〇 另外’於alSQig α2之區域中,亦可將Q2^f(⑴(f 為函數)作為對應於產生鑄漏之條件。例如於表1中,於α 1(15000 kJ/m2)〜α2(21_ kJ/in2)之區域(研究例卜2、 10 17)中,亦可使用Q22 a Ql( α =〇· 25)之判定基準。再 ❹ 者’根據設備之不同’可考慮如下情形(由操作條件所引起 Q1之變動車乂小之情开〉等):不藉由αΐ、“2而設置上述邊 界’而僅需單純地藉* __(α :例如為〇 25)來判定 缚漏即可。 再者’對於Q1及Q2並未特別設置上限,其原因在於:對 應於設備,Q1及Q2之可取用值本身有上限。 再者,於熔鋼為極低碳鋼(extra-l0w carb〇n steel)之情 098106495 22 200946265 形時,以上所例示之“卜 所謂熔鋼為極低碳鋼於常-致。此處, 〇._之鋼。於上述轉漏心1所鑄&之_之階段中α 之基本部分不依賴於疋,中’凝固殼形成現象之解析 行校正,藉此亦可二因:,視需要對係數或臨限值進 ]續地應用於其他鋼種。 密=述’發明者發現:qi、q2之各值與鱗漏之產生有 ❹ 而且各個值與不同之鑄漏產生原因有相關,因 由將Q1 Q2之值作為有無產生铸漏之指標,可高精 度地檢出鳞漏之產生’進而可根據產生鑄漏之原因而適當地 進行用以避免產生鑄漏之危險之控制。 <凝固殼厚之推定> 然而以上述方式所求得之總熱通# Q1可評價為熔鋼凝 固所’肖耗之熱量’又’總熱通量Q2可評價為溶鋼流衝擊凝 固设而使凝固殼再溶解之熱量(即炼鋼流衝擊顯熱)。亦即, ©若根據總熱通量Q1來推定鑄模出σ處之㈣殼厚度,則可 高精度地推定凝固殼厚度。 因此,亦對根據Q1而求得凝固殼厚,並根據凝固殼厚來 董化地評價鎢漏之危險性的可能性進行了研究。以下,對利 • 用總熱通量Q1來推定鑄模出口處之凝固殼厚度之方法進行 說明。 首先’若考慮鎊模内炫鋼凝固之物理過程,則自浸潰喷嘴 注入至鑄模内之熔鋼具有包含顯熱與凝固潛熱之焓:仏(含 098106495 23 200946265 熱量)。而且’該具有焓:Ho之熔鋼因自爐浴面放熱而失去 放熱部分之焓:AHsur,又,於自爐浴面到達鑄模出口之期間, 對鎮模進行冷卻而排熱,藉此失去相當於排熱量部分之始: ΔΗ(焓降:enthalpy drop),最終於鑄模出口處,自鑄模中 抽出具有焓:乩之凝固殼。若以公式來表示該自浸潰喷嘴注 入至鑄模内之熔鋼自爐浴面到達鑄模出口為止之焓之關 係’則如下式(4)所示。 H〇 = Hi + AH + AHsur .........(4) 其中’ H〇 :鑄模内熔鋼之焓(J/kg)❹ is large, so the thickness of the solidified shell as a whole is thick, and there is no partial thinning of the solidified shell. Even if the solidified shell is thinned, the degree of thinning is small. From the above studies of the regions (4) and (5), it is understood that the state of the region (5) is more preferable if the state of the region (4) is compared with the state of the region (5). Therefore, when the state of the regions (1) to (3) where the casting leakage occurs is converted into a state in which no pound leakage occurs, the state of transitioning to the region (4) is also effective, but it is more preferable to control the operating conditions. To further transform into the state of the region (5). Specifically, when it is in the state of the region (1), the operating condition is performed as long as the state of the region (4) is changed by increasing the enthalpy, or the state of the region (5) is further decreased by Q2. Control can be. Further, when it is in the state of the region, the operation condition may be made as long as it is changed to the state of the region (5) by increasing the enthalpy. & However, when in the state of the region (3), it is only necessary to control the operating conditions by changing the state of the region (5) by decreasing Q2 or changing the state of the region (4) by increasing qi. As a control for increasing the operating conditions of Q1, it is exemplified to reduce the speed of the assembly and/or to enhance the cooling of the mold. Further, as a control for reducing the operating condition of Q2, 098106495 19 200946265 exemplifies that the electromagnetic brake device is disposed, for example, in the upper and lower portions of the nozzle opening of the dip nozzle in the mold, and the flow rate of the molten steel is slowed by application of a DC magnetic field. Furthermore, the basic point of the method described above is to obtain the heat flux Q1 and the stable solidification interface heat input q2reg entering the solidification interface during the period from the furnace bath surface to the mold exit, and according to (ql) -q2reg) The heat flux distribution determines whether a casting leak will occur. Descriptions other than the above are exemplified and are not limited to the above. For example, the heat flux ql can be obtained from the temperature on the inlet side and the outlet side of the mold cooling water. Further, the stable solidification interface heat input Q2reg can be obtained from the result of the estimated value of the molten steel flow rate obtained by numerical simulation in the mold, for example. The analysis method of the heat flux distribution of (Ql - q2res) is preferably performed after calculating the above Q1 and Q2, but is not limited thereto. For example, the height and position of the raised portion may be simply used as a criterion for determining the risk of casting leakage (e.g., it is generally considered to be effective when the molten steel flow at the impact solidification interface is strong and the equipment is highly volatile). When using w1 and Q2 for analysis, if the minimum value and the convex portion are not generated in the heat flux distribution, it is sufficient to set == 8) and Q2 = 0. In the case where it is difficult to determine the minimum value of ql — q2reg (for example, the minimum value is unknown: the minimum value of two or more figures is present), as long as the approximate curve is drawn as close as possible to the pattern, From (ql - q2reg) drop curve (corresponding to the curve of Q1 in Figure 9, that is, the closer to the surface of the bath, 098106495 200946265, the curve of the local heat flux can be reduced by 0) becomes a minimum point Further, it is preferable to consider the thickness of the Q1 shell or to specify the casting leak. Face, and the change of Q2 is small. 4 Predictive accuracy and the accuracy of Q2 are both, but only Q1 can be used. For example, when it is expected that the molten steel flow does not easily reach the solidification boundary, even if Q2 is not considered, it is expected that when Q1 and Q2 are required, < Integral means other than ❹ 法). The boundary line AC does not need to be a straight line. Of course, the method described above can also be used. (In addition, in the analysis of Fig. 9, Q1 and Q2, for example, the curve 4 from the bath surface to the A can also be considered. It is an approximation curve. Even when specific casting leak determination is performed using Q1 and q2, it is not limited to the above-described method, as long as Q1 is appropriately used as an index of heat generation caused by solidification (that is, by numerical value The factor of increasing the risk of casting leakage is to use Q2 as an indicator of the heat input exceeding the stable solidification interface (ie, the factor of increasing the risk of casting leakage by increasing the value ❹). Because there are many cases where the growth and solidification of the solidified shell thickness are not sufficient (Q1 < α 1 of the above-mentioned area (1) and area (2)), and the growth of the solidified shell thickness Q2 is irrelevant and the case of casting leakage is sufficiently avoided (Q1 of the region (5) and the portion of the region (4) and the region (4)). Therefore, it is preferable to set the boundary of each boundary αΐ in advance. 'α 1 SQl S α 2 area becomes the shadow of the size In the area, it is determined that there is a risk of casting leakage based on the value of 卯. 098106495 21 200946265 That is, in the case of 'in this case', it is preferable that # is a predetermined threshold or more, and it is judged that there is a danger of _. Then, the threshold value of 2 is preferably determined according to W, but 'the final' can also be set to a fixed value for the whole of Ua2. The above table 1 is equivalent to the fixed value. - As another method' Consider further refining α^^ and setting the threshold in each-area. For example, when "3 butterfly α1<α3<α4<α 2) 'in the case of Q1 < α 3 is set, the point is set In order to correspond to the condition for generating the pound leak, in the case of α3_<α4, the material corresponds to the condition for generating the casting leak, and in the case of α4_$α2, q = stone 3 is considered to correspond to the condition for generating the leak. Furthermore, in this case, usually β\<β2<β3〇in another 'in the region of alSQig α2, Q2^f((1)(f is a function) may also be used as a condition corresponding to the generation of the casting leak. For example, in the table In the case of 1 (15000 kJ/m2) to α2 (21_ kJ/in2) (Research Example 2, 10 17), Q22 can also be used. a Ql (α = 〇 · 25) criterion. In addition, 'depending on the equipment' can consider the following situation (the change of Q1 caused by the operating conditions, the car is small), etc.): not by αΐ, "2 and set the above boundary" and simply borrow * __ (α: for example, 〇 25) to determine the leak. Further, 'the upper limit is not set for Q1 and Q2 because the device corresponds to the device. The available values of Q1 and Q2 have their own upper limit. Furthermore, when the molten steel is ultra-low carbon steel (extra-l0w carb〇n steel) 098106495 22 200946265, the above-mentioned exemplified "the so-called molten steel is very low carbon steel." 〇._之钢. The basic part of α in the stage of the above-mentioned leakage core 1 is not dependent on 疋, and the analytical analysis of the formation phenomenon of the solidified shell is also possible. It is necessary to apply the coefficient or the threshold value to other steel grades. The inventor found that the values of qi and q2 are related to the occurrence of scale leakage and that each value is related to the cause of different casting leakage. By using the value of Q1 Q2 as an indicator of the occurrence of casting leakage, it is possible to detect the occurrence of scale leakage with high precision', and it is possible to appropriately control the risk of casting leakage according to the cause of casting leakage. Presumption of solidified shell thickness> However, the total heat flux #Q1 obtained in the above manner can be evaluated as the heat of the molten steel solidification and the total heat flux Q2 can be evaluated as the molten steel flow impact solidification. The heat of re-dissolving of the solidified shell (ie, the steelmaking stream impacts sensible heat). That is, © if The total heat flux Q1 is used to estimate the thickness of the (four) shell at the σ of the mold, so that the thickness of the solidified shell can be estimated with high precision. Therefore, the solidified shell thickness is also determined according to Q1, and the tungsten is evaluated based on the solidified shell thickness. The possibility of the danger of leakage has been studied. The following is a description of the method for estimating the thickness of the solidified shell at the exit of the mold using the total heat flux Q1. First, if considering the physical process of solidification of the steel in the pound mold, The molten steel injected into the mold from the impregnation nozzle has the enthalpy of sensible heat and solidification: 仏 (including 098106495 23 200946265 heat). And 'the 熔:Ho molten steel loses heat due to heat release from the bath surface Part of the 焓: AHsur, again, during the period from the bath surface to the exit of the mold, cooling the town mold to remove heat, thereby losing the beginning of the equivalent of heat removal: ΔΗ (焓: enthalpy drop), finally At the exit of the mold, a solidified shell having 焓:乩 is extracted from the mold. If the relationship between the molten steel injected into the mold from the surface of the furnace to the exit of the mold is expressed by the formula, the following formula is used ( 4) Shows H〇 = Hi + AH + AHsur ......... (4) wherein 'H〇: enthalpy of molten steel within the mold (J / kg)
Hl :鑄模出口處之凝固殼之焓(j/kg) ΔΗ :鑄模出口處之凝固殼之每單位重量之焓降(J/kg) AHsur:來自爐浴面之放熱部分(J/kg) 此處,、ΔΗμ、H〇分別可以如下之方式求得。 <Hl之求法> 鱗模出口處之凝固殼之焓:IL可由以下之式(5)求得。Hl : 凝固 (j/kg) of the solidified shell at the exit of the mold ΔΗ : the drop per unit weight of the solidified shell at the exit of the mold (J/kg) AHsur: the heat release from the bath surface (J/kg) Where, ΔΗμ, H〇 can be obtained in the following manner. <Method for finding Hl> 凝固: The solidified shell at the exit of the scale mold: IL can be obtained by the following formula (5).
Hi = 67〇. 27 Tiave+ 11958 .........(5) 式(5)係以溫度對固相之鋼之比熱進行積分而求出焓,並 將其作為溫度之函數而表示成式者。式(5)中之Tuve係表示 禱模出口處之凝固殼平均溫度(。〇,該?1咖可由以下所示之 式(6)求得。Hi = 67〇. 27 Tiave+ 11958 (5) Equation (5) is obtained by integrating the specific heat of the steel of the solid phase with temperature and expressing it as a function of temperature. Into the formula. The Tuve in the formula (5) indicates the average temperature of the solidified shell at the exit of the prayer mold ((〇), which can be obtained by the following formula (6).
Tlave^28. 75 Vc+ 1234. 275 .........(6) 其中’ Vc :鑄造速度(m/分) 098106495 24 200946265 式(6)係以 Vc = 1. 4 m/分、1. 8 m/分、2. 2 m/分、2. 6 m/ 分來進行鑄模内之傳熱凝固計算,並將所求得之鑄模出口殼 平均溫度作為Vc之1次式來表示者。將用於式(6)之導出之 圖以圖11表示。圖11之縱軸表示鑄模出口殼厚度方向平均 溫度(°C),橫軸表示鑄造速度(m/分)。 < Msur之求法〉 相當於來自爐浴面之放熱部分之焓:AHsur可由以下之式 ❹ (7)求得。 AHsur= (10000/7100) · (60/Vc) .........(7) 其中,Vc :鑄造速度(m/分) 式(7)係計算出來自爐浴面之放熱部分者,即計算出每單 位體積之熔鋼釋放出多少焓者。若將每單位面積之爐浴面所 釋放出之焓設為ΔΗμ’(單位為W/m2),則每單位體積之熔鋼 之焓釋放量AHsurCJ/kg)只要用AHsur’除以由單位時間之鑄造 ❹ 速度所決定之炼鋼重量即可,因此AHsur^ AHsur’ /(密度7100 xVc/60xl( =單位面積))。而且,將AHsur’設為 10000 W/m2 者為式(7)。 • < Η〇之求法> 鑄模内熔鋼之焓:H。可根據式(8)求得,該式(8)係以溫度 對液相之鋼之比熱進行積分而求出焓,並將其作為溫度之函 數而表示成式者。 H〇= (1x10 10χΤ〇4- 4χ10"7χΤ〇3 + 0. 0005xT〇2- 0. 0098χΤ〇 + 098106495 25 200946265 4.5508)x4. 19x1000 .........(8) 其中,T。:铸模内熔鋼溫度(°c) 再者,對於式(8)中之鑄模内熔鋼溫度T。而言,可於現有 之設備中,利用熱電偶而實際測定鑄模内之熔鋼溫度,並根 據此時之操作條件中作為複迴歸方程式之下述之式(9)而求 得。 T〇 = 705. 156 + 0. 544086 Ttd- 2. 35053 Vc- 0.00303 W + 18. 12663(0. 10181 · ln(FC)-〇. 3362) .........(9) 其中,Ttd :假槽(T/D : tundish)内熔鋼溫度(°c )Tlave^28. 75 Vc+ 1234. 275 .........(6) where 'Vc: casting speed (m/min) 098106495 24 200946265 Equation (6) is Vc = 1. 4 m/min, 1. 8 m/min, 2.2 m/min, and 2. 6 m/min to calculate the heat transfer and solidification in the mold, and the average temperature of the obtained shell of the mold is expressed as the first order of Vc. . The map for the derivation of the equation (6) is shown in Fig. 11. The vertical axis of Fig. 11 indicates the average temperature (°C) in the thickness direction of the exit hole of the mold, and the horizontal axis indicates the casting speed (m/min). <Method of Msur> Equivalent to the heat release from the surface of the hearth: AHsur can be obtained by the following formula 7 (7). AHsur= (10000/7100) · (60/Vc) ... (7) where Vc: casting speed (m/min) Equation (7) calculates the heat release from the bath surface That is, calculate how many defects are released per unit volume of molten steel. If the enthalpy released by the bath surface per unit area is set to ΔΗμ' (unit: W/m2), the AHsurCJ/kg of molten steel per unit volume is simply divided by AHsur' by unit time. The casting speed is determined by the speed of the steelmaking, so AHsur^ AHsur' / (density 7100 x Vc / 60xl (= unit area)). Further, the case where AHsur' is set to 10000 W/m2 is Equation (7). • <求之法> 熔 熔 in the mold: H. The equation (8) can be obtained by integrating the specific heat of the steel in the liquid phase at a temperature to obtain enthalpy, and expressing it as a function of temperature. H〇= (1x10 10χΤ〇4- 4χ10"7χΤ〇3 + 0. 0005xT〇2- 0. 0098χΤ〇 + 098106495 25 200946265 4.5508)x4. 19x1000 (8) where T. : molten steel temperature in the mold (°c). Further, for the molten steel temperature T in the mold of the formula (8). In the conventional apparatus, the temperature of the molten steel in the mold can be actually measured by a thermocouple, and can be obtained as the following equation (9) of the complex regression equation according to the operating conditions at this time. T〇= 705. 156 + 0. 544086 Ttd- 2. 35053 Vc- 0.00303 W + 18. 12663 (0. 10181 · ln(FC)-〇. 3362) .........(9) where , Ttd: false tank (T/D: tundish) inside molten steel temperature (°c)
Vc :鑄造速度(m/分) W :鑄造(M/D : mold)寬度(m) FC.流量控制(FC,flow control)電流(A) 如上所述,由於可求得ΗρΔΗ^'Η。,因此可根據將式(4) 變形而成之下述之式(10)而求得ΑΗ。 ΔΗ= H〇— (Hi + AHsur) .........(10) △H係相當於藉由自爐浴面到達铸模出口為止之期間進行 鑄模冷卻而排熱所產生之排熱量部分之焓,因此鑄模出〇處 之凝固殼厚度D可利用總熱通量Q1由下式(2)表示。 D = Q1/(AH · p ) .........(2) 其中,P :鑄模出口處之凝固殼之密度(kg/m3) 再者,對於p而言,其可以於5處求得汕〜^卯它為止 之固體鐵密度’並使該等成為溫度之函數之方式,由作為姆 098106495 26 200946265 歸方程式(regression equation)之下式(ιι)而求得。 P =(-1. 686x10- W+ 2.7069xi〇-7 Τ^- 5. 2909xl〇-TiaVe+ 7. 9106)xl000 .........(ii) 再者,IL·、ΔΗμ、Hg、p之求法並不受限於上述方法,可 以各種方法求得。 再者,於上述之研究中,總熱通量Q2作為熔鋼流衝擊凝 固殼而使凝固殼再熔解之熔鋼流碰撞顯熱,將其從用以推定 〇 凝固殼厚度之總熱通量中排除。 然而’可認為當於鱗造中,自浸潰噴嘴喷出之熔鋼喷出流 暫時增大時,即存在總熱通量Q2時,藉由熔鋼流而使凝固 殼再溶解’而產生凝固延遲。因此,亦可認為凝固殼厚度變 得比僅排除總熱通量Q2所求得之凝固殼厚度更薄。 因此,以下對考慮了由再熔解所引起之凝固延遲的凝固殼 厚度之精度更高之推定方法進行說明。 # 發明者考慮即便產生由總熱通量Q2所引起之再熔解,亦 不使全部總熱通量Q2用於再熔解凝固殼’而使某一比例之 總熱通量Q2用於再熔解。若如此考慮’且若考慮將根據總 • 熱通量Q1所推定之凝固殼厚度設為D,將考慮由總熱通量 ' Q2所引起之再熔解的凝固殼厚度設為D1,且Q2之X%用於 再溶解’則下述之比例關係成立。 Q1 : D=(Q1—X · Q2) : D1 若關於D1而對上述之比例式進行整理,則= —X · 098106495 27 200946265 Q2/Q1) 〇 因此,只要可求得X,則可求得D1。 因此,若關於X而對上述之比例式進行整理,則X=(D_ Dl)/D · Q1/Q2。該式中所出現之(D_D1)/D之值係作為凝固 延遲度 RSCRetardation of Solidification:凝固延遲 度),於習知文獻之「熔鋼流動、熔鋼過熱度對凝固延遲造 成之影響」((獨)日本學術振興會(japan Society For the Promotion of Science)製鋼第19委員會凝固製程研究會 提出資料:p. 8〜9)中’揭示有該凝固延遲度防可由下述之 式(3)求得。 RS= 0χ(ν°.8.Δ0 ) .........(3) 冷:凝固延遲常數(無單位) V :熔鋼流速(m/s) △ 0 :熔鋼過熱度(°C) RS :凝固延遲度(無單位) 如上所述,熔鋼過熱度Δ0可求得為Δ<9 =T。—TS(T。:鑄模 内熔鋼温度(°C ),Ts :熔鋼固相線溫度(。〇)),因此只要求 得溶鋼流速V,則可求得RS。 而且,熔鋼流速V(m/s)係可利用總熱通量q2並由式(13) 而求得。 V=(Q2/U · t · ΔΘ ))125 .........(13) α :熔鋼流速常數(無單位) 28 098106495 200946265 t:凝固殼經由分布中之極小點後到達鑄模出口為止 之時間⑻ ‘’、、% 若將X=(D —D1)/D.Q1/Q2之式中之(D—Dl)/D替換成 RS,則X = RS · Q1/Q2。若將該X之值代入至上述D1 = D(1 ' —X · Q2/Q1)中,則D1 = D(1 —RS),而可求得考慮了凝固延 遲之凝固殼厚度D1。 如上所述’可求得上述式(3)中所示之凝固延遲度RS,因 ❹ 此可根據D1 = D(1 —RS)而求得考慮了由總熱通量Q2所引起 之凝固延遲的凝固殼厚度D1。 為了驗證以上研究之妥當性,於若干操作條件下求得D 及D1,並將該D及D1與藉由其他方法所獲得之值進行比較。 作為比較法,計算出下述D’及D1,。 D’ =僅利用ql之熱通量分布,且僅由排熱量而計算出之 殼厚度。即,使用ql代替ql —q2reg,計算出相當於總熱通 ❹ 量Q之值(作為Q’),並根據上述式(2)由D,/(ΔΗ · ρ ) 所求得之值。 D1’ =於D’中考慮了凝固延遲之殼厚度。即,根據rS而 . 藉由Dl’ =D’(1 —RS)所求得之值。Vc: casting speed (m/min) W: casting (M/D: mold) width (m) FC. flow control (FC) flow current (A) As described above, ΗρΔΗ^'Η can be obtained. Therefore, it is possible to obtain ΑΗ according to the following formula (10) obtained by deforming the formula (4). ΔΗ= H〇—(Hi + AHsur) (10) ΔH corresponds to the amount of heat generated by heat removal during mold cooling from the furnace bath surface to the exit of the mold. In part, the thickness D of the solidified shell at the exit of the mold can be expressed by the following formula (2) using the total heat flux Q1. D = Q1/(AH · p ) (2) where P: the density of the solidified shell at the exit of the mold (kg/m3). Further, for p, it can be 5 The method of obtaining the solid iron density 'to the extent of the temperature' and making it a function of temperature is obtained by the formula (ιι) of the regression equation as 098106495 26 200946265. P = (-1. 686x10- W+ 2.7069xi〇-7 Τ^- 5. 2909xl〇-TiaVe+ 7. 9106)xl000 ......... (ii) Furthermore, IL·, ΔΗμ, Hg, The method of p is not limited to the above method and can be obtained by various methods. Furthermore, in the above study, the total heat flux Q2 acts as a molten steel stream impinging on the solidified shell, causing the molten steel stream, which is remelted by the solidified shell, to collide with sensible heat, from the total heat flux used to estimate the thickness of the solidified shell. Excluded. However, it can be considered that when the molten steel ejected from the impregnation nozzle is temporarily increased in the scale formation, that is, when the total heat flux Q2 exists, the solidified shell is re-dissolved by the molten steel flow. Delayed solidification. Therefore, it is also considered that the thickness of the solidified shell becomes thinner than the thickness of the solidified shell obtained by excluding only the total heat flux Q2. Therefore, the following is a description of a method for estimating the accuracy of the solidified shell thickness in consideration of the solidification delay caused by remelting. # The inventors considered that even if the remelting caused by the total heat flux Q2 occurs, the total heat flux Q2 is not used to re-melt the solidified shell, and a certain proportion of the total heat flux Q2 is used for remelting. If this is considered, and if the thickness of the solidified shell estimated from the total heat flux Q1 is taken as D, the thickness of the solidified shell which is considered to be remelted by the total heat flux 'Q2' will be set to D1, and Q2 X% is used for redissolution 'The following ratio relationship holds. Q1 : D=(Q1—X · Q2) : D1 If the above formula is sorted for D1, then =—X · 098106495 27 200946265 Q2/Q1) 〇 Therefore, as long as X can be obtained, it can be obtained. D1. Therefore, if the above-described proportional expression is collated with respect to X, X = (D_Dl) / D · Q1/Q2. The value of (D_D1)/D appearing in this formula is used as the retardation degree of solidification (RSCRetardation of Solidification). In the conventional literature, "the influence of molten steel flow and molten steel superheat on solidification delay" (( The Japanese Society for the Promotion of Science (Japan Society for the Promotion of Science), the 19th Committee of the Solidification Process Research Society, presents the data: p. 8~9), which reveals that the solidification delay can be prevented by the following formula (3). Got it. RS = 0χ(ν°.8.Δ0 ) (3) Cold: solidification delay constant (no unit) V: molten steel flow rate (m/s) △ 0 : molten steel superheat ( °C) RS : Solidification delay (no unit) As described above, the molten steel superheat degree Δ0 can be found as Δ < 9 = T. —TS(T.: molten steel temperature (°C) in the mold, Ts: molten steel solidus temperature (.〇)), so only the molten steel flow rate V is required, and the RS can be obtained. Further, the molten steel flow rate V (m/s) can be obtained by the formula (13) using the total heat flux q2. V=(Q2/U · t · ΔΘ )) 125 .........(13) α : molten steel flow rate constant (no unit) 28 098106495 200946265 t: solidified shell arrives after a very small point in the distribution Time until the mold exit (8) '', % If (D - Dl) / D in the formula X = (D - D1) / D. Q1/Q2 is replaced by RS, then X = RS · Q1/Q2. If the value of X is substituted into the above D1 = D(1 ' - X · Q2 / Q1), then D1 = D(1 - RS), and the solidified shell thickness D1 considering the solidification delay can be obtained. As described above, the solidification delay degree RS shown in the above formula (3) can be obtained, because the solidification delay caused by the total heat flux Q2 can be obtained from D1 = D(1 - RS). The solidified shell thickness D1. In order to verify the validity of the above studies, D and D1 were obtained under several operating conditions, and the D and D1 were compared with the values obtained by other methods. As a comparison method, the following D' and D1 were calculated. D' = only the heat flux distribution of ql is used, and the shell thickness is calculated only by the heat rejection. That is, ql is used instead of ql - q2reg, and a value corresponding to the total heat flux amount Q (as Q') is calculated, and the value obtained by D, /(ΔΗ · ρ ) according to the above formula (2) is calculated. D1' = shell thickness in which the solidification delay is considered in D'. That is, the value obtained by Dl' = D' (1 - RS) according to rS.
Dreal=根據鑄片之内部裂痕位置所推定之殼厚度 098106495 29 200946265 [表2]Dreal = shell thickness estimated from the position of the internal crack of the cast piece 098106495 29 200946265 [Table 2]
Vc W Ttd Αθ FC D, Q' Dl' D Q RS Dl Dreal m/分 m ec °C A mm kJ/m2 mm oun kJ/m2 % _ mm 條件1 2.3 1.4 1560 19 359 15.3 31780 14.5 13.2 27420 5.6 12.5 12.0 條件2 2.5 1.1 1551 16 334 13.9 28060 13.0 11.0 22200 6.8 10.3 10.7 條件3 2.0 1.7 1560 12 215 17.1 36280 16.6 15.5 32885 3.2 15.0 16.0 條件4 1.7 1.8 1553 15 133 19.0 40650 18.5 17.5 37324 2.7 17.0 16.2Vc W Ttd Αθ FC D, Q' Dl' DQ RS Dl Dreal m/min m ec °CA mm kJ/m2 mm oun kJ/m2 % _ mm Condition 1 2.3 1.4 1560 19 359 15.3 31780 14.5 13.2 27420 5.6 12.5 12.0 Conditions 2 2.5 1.1 1551 16 334 13.9 28060 13.0 11.0 22200 6.8 10.3 10.7 Condition 3 2.0 1.7 1560 12 215 17.1 36280 16.6 15.5 32885 3.2 15.0 16.0 Condition 4 1.7 1.8 1553 15 133 19.0 40650 18.5 17.5 37324 2.7 17.0 16.2
Vc :鑄造速度 W:鑄造寬度 Τπ> : TD内熔鋼溫度 ΑΘ :熔鋼過熱度 ◎ FC :上極FC直流電流 RS :凝固延遲 由以上之結果可知’ D及D1取穩定地接近於實測值之值, 而且尤其D1係為更進一步改善之值。 如此,可利用總熱通量Q1而求得鑄模出口處之凝固殼厚 度D,進而可求得考慮了凝固延遲之凝固殼厚度μ。 而且’右可求得凝固殼厚度,則可藉由預先求得凝固殼厚 ❹ 度與有無產生鑄漏之關係’而作為有無產生鑄漏之指標。例 如當預測厚度D達到臨限值以下時,可判定為祕產生轉漏 之條件下,或者當_厚度D1 _臨限值以下時,可狀 . 為處於產生鑄漏之條件下。可對應於_、設備、操作條件,- 預先根據先例而設定臨限值,或者藉由理論計算而求得臨限 值0 098106495 30 200946265 而且,該有無產生鑄漏之指標係基於鑄模出口處之凝固殼 厚度者,與上述僅基於熱通量之變化者相比較,其為更直接 之指標,因此可謂其精度較高。 又,對於如上述圖10所例示之基於Q1或者基於Q1及Q2 之鑄漏產生檢出法而言,雖然看上去省略了實際計算凝固殼 厚度之過程,但由於其係根據Ql、Q2對於凝固殼厚之影響 來預測有無產生鑄漏,因此亦可同樣獲得較高之精度。 ❹ 本發明係根據以上之見解而成者,具體而言包含以下之構 成。 (1) 一種連續鑄造之鑄漏檢出方法,其特徵在於,其包括 如下步驟:測定連續鑄造中之鑄模内熔鋼自爐浴面到達鑄模 出口為止之期間朝凝固界面熱輪入之熱通量ql之步驟·根 據下式(1)求得穩定狀態下之鑄模内熔鋼流動所弓丨起之穩定 凝固界面熱輸入q2reg之步驟;針對該等熱通量w與穩定凝 參固界面熱輸入^reg之差(ql ~~ q2reg),求得熔麵自鱗洛:到達 鑄模出口為止之熱通量分布之步驟;及根據讀熱通量分布而 判定有無產生銹漏之危險之步驟。 . q2reg=h.A0 .........(1) . 其中,h :熔鋼與凝固殼之間之熱傳遞係數 A0 :熔鋼之過熱度。 (2) 如上述(1)之連續鑄造之鑄漏檢出方法,其中, 根據針對上述(ql—q2reg)所求得之上述該熱通量分布來 098106495 31 200946265 判定有無產生鑄漏之危險之步驟包括有: 根據上述熱通量分布,藉由 肖由以下方法而求得總熱通量Q1 及Q2之步驟’即’⑴於上述該埶 值之極小點之情形時,當利用量77布巾存在表承極小 】用直線連結該極小點與鑄模出口 處之局部熱通量值時,將與該直線更上方之部分之面積相當 ,總熱通量=Q2,將與如下面積 設為 Q1,該面積係自與由自爐浴面位置至鱗模出口間二量 ❹ =:包的總_減去_ =二:通量分布中不存在表示極小值 之極小點之情形時,將與由自遗 舳旦太敫 面位置至鑄模出口間之該 …、通f刀布之整個曲線所包圍 m脸八 之、、息面積相當的總熱通量設 為總熱通量Q1,將q2設為零之步驟.及 ^據上述總熱通量Q1,或者根據如及收來判 生鑄漏之危險之步驟。 …、座 再者,所謂總熱通量,根據上 ❹ 部熱通量進行料顺狀值。揭^村知其係指對局 ⑶如上述⑵之連續鑄造之碡騎出方法射於 =定有無產生鑄漏之危險之步驟中,將Qi作為由凝固㈣Vc : casting speed W: casting width Τ π > : TD inner molten steel temperature ΑΘ : molten steel superheat ◎ FC : upper pole FC direct current RS : solidification delay From the above results, it can be seen that 'D and D1 are steadily close to the measured value The value, and especially D1, is a further improvement. Thus, the solidified shell thickness D at the exit of the mold can be obtained by using the total heat flux Q1, and the solidified shell thickness μ in consideration of the solidification delay can be obtained. Further, the thickness of the solidified shell can be determined by the right, and the relationship between the thickness of the solidified shell and the presence or absence of the casting leakage can be obtained in advance as an indicator of whether or not the casting leak occurs. For example, when the predicted thickness D reaches the threshold value, it can be judged to be under the condition that the leak occurs, or when the thickness is below the thickness D1 _ threshold, it can be in the condition of generating the casting leakage. Corresponding to _, equipment, operating conditions, - set the threshold according to the precedent in advance, or obtain the threshold by theoretical calculation. 0 098106495 30 200946265 Moreover, the indicator of whether or not the casting leak occurs is based on the exit of the mold. The thickness of the solidified shell is a more direct indicator than the above-mentioned change based only on the heat flux, so it can be said that the precision is high. Further, for the detection method based on Q1 or the Q1 and Q2 based on the above-described FIG. 10, although the process of actually calculating the thickness of the solidified shell is omitted, it is solidified according to Q1 and Q2. The effect of the shell thickness is used to predict the presence or absence of a casting leak, so that higher precision is also obtained. The present invention has been made based on the above findings, and specifically includes the following constitution. (1) A continuous casting casting leak detection method, comprising the steps of: measuring a heat flux of a molten steel in a continuous casting mold to a solidification interface during a period from a furnace bath surface to a mold exit; Step of the amount ql · According to the following formula (1), the step of stabilizing the solidification interface heat input q2reg from the flow of the molten steel in the mold under steady state is obtained; for the heat flux w and the stable condensation solid interface heat Enter the difference of ^reg (ql ~~ q2reg), and find the step of melting the surface from the scale: the heat flux distribution until the exit of the mold; and the step of determining the risk of rust leakage based on the read heat flux distribution. Q2reg=h.A0 ... (1) where h is the heat transfer coefficient between the molten steel and the solidified shell A0: the superheat of the molten steel. (2) The method for detecting a casting leak in the continuous casting according to the above (1), wherein the risk of casting leakage is determined based on the heat flux distribution obtained by the above (ql-q2reg) 098106495 31 200946265 The steps include: according to the heat flux distribution, the step of obtaining the total heat fluxes Q1 and Q2 by the following method is '1' (1) when the minimum value of the enthalpy is above, when the utilization amount is 77 The surface is extremely small. When the local minimum heat flux value at the exit of the mold is connected by a straight line, it will be equivalent to the area above the straight line. The total heat flux = Q2 will be set to Q1 with the following area. The area is from the total amount _ from the position of the bath surface to the exit of the scale die = the total _ of the package minus _ = two: when there is no minimum point indicating the minimum value in the flux distribution, From the position of the 敫 敫 敫 至 至 至 至 至 至 至 、 , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , The step of zero. and ^ according to the above total heat flux Q1, or according to The step of judging the danger of casting a leak. ..., seat Again, the so-called total heat flux, according to the heat flux of the upper part of the feed rate.揭^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
起讀熱量之指標,將Q2作為超過穩定之㈣界面熱I 之才曰標’根據Q1或者根據以及收而判定有無產生禱漏之 危險。 又 ,本發明係如上述(2)之連續鑄造之鑄漏檢出 方法,其 098106495 32 200946265 中’於上述判定有無產生鑄漏之危險之步驟中,亦可將Q1 作為藉由數值之增大來降低鑄漏之風險之因數而處理,將 Q2作為藉由數值之增大來增大鑄漏之風險之因數而處理, 並根據Q1或者根據Q1及Q2來判定有無產生鑄漏之危險。 (4)如上述(2)或(3)之連續鑄造之鑄漏檢出方法,其中, 於根據上述總熱通量Q1來判定有無產生鑄漏之危險之步驟 中’關於針對Q1所預先設定之臨限值α卜α 2(α 1< α 2), 參()田Q1 < α 1日寺’判定為有鑄漏之危險,(ii)當α 1 SQ1 $ α 2時’根據Q2之值而判定為有鑄漏之危險。 β此處較佳為當Q2達到根據Q1而預先設定之臨限值(亦 可為al_Ql$a2之整個範圍中之固定值)以上時,判定為 有禱漏之危險。 ) 述至中任一項之連續铸造之鑄漏檢出方 ❹ , ' ;十_上述(ql —q2reg)所求得之上述熱通量分布 中存在表示極小偵 先設定之臨限值 之情形時,相對於針對Q1所預 之臨限抑,^⑴a2Ul<a2)及針對Q2所預先設定 _,或4 1且似,或者⑽心1且 漏之危險。α1·。2且Q2以時’判定為有鑄 Ρ本發月之連續鑄造之鱗漏方法 續鑄造中之_ 顿在於·測疋連 間朝凝固界面埶::自達鱗模出口為止之期 098106495 、,、之熱通量ql;根據下式⑴求得穩定狀 33 200946265 態下之鑄模内熔鋼流動所引起的穩定凝固界面熱輸入 q2reg;針對該等熱通量“與穩定凝固界面熱輸入以叫之差 (ql —q2reg)’求得熔鋼自爐浴面到達鑄祺出口為止之熱通量 分布;及於上述該熱通量分布中存在表示極小值之極小點之 情形時,當利用直線連結該極小點與鑄模出口處之局部熱通 量值時,將與該直線更上方部分之面積相當的總熱通量設為 Q2 ’將與如下面積相當之總熱通量設為Q1,該面積係自與 由自爐浴面位置至鑄模出口間之該熱通量分布之整個曲線 所包圍的總面積相當之總熱通量減去Q2所獲得之面積,且 相對於針對Q1所預先設定之臨限值、α2(αΐ< α2)及 針對Q2所預先設定之臨限值石’當Ql<al且Q2 2/3,或 者Ql<al且Q2</3,或者且Q22沒時,判 定為有鎊漏之危險。 (6) 如上述(5)之連續鑄造之鑄漏檢出方法,其中,溶鋼為 極低碳鋼,α 1 為 15000(kJ/m2),α 2 為 2l〇〇〇(kJ/m2),々 為 4500(kJ/m2)。 (7) 如上述(2)或(3)之連續鑄造之鑄漏檢出方法,其中, 根據上述總熱通量Q1來判定有無產生鑄漏之危險之步驟包 括有:使用上述總熱通量Q1,根據下式(2)來推定鑄模出口 處之凝固殼厚度D之步驟;及根據上述所推定之凝固殼厚度 D及預先以與產生鑄漏之危險性的關係所求得之臨限值,判 定有無產生鱗漏之危險之步驟。 098106495 34 200946265 D== Q1/(AH · p ) .........(2) 其中,D :鑄模出口處之凝固殼厚度 Q1 :總熱通量(j/y) AH :鑄模出口處之凝固殼之每單位重量之焓降(j/kg) P :鑄模出口之凝固殼密度(kg/m3) 又’將上述ql之單位設為J/s.m2,於上述式⑴中將q2reg 之單位設為J/s · m2 ’將h之單位設為J/s · m2 ·。〇,將A0 ❹ 之單位設為。C。 (8)如上述(2)或(3)之連續铸造之鑄漏檢出方法,其中, 於針對上述(ql —q2reg)所求得之上述熱通量分布中存在表 示極小值之極小點之情形時,根據上述總熱通量Q1及Q2 來判定有無產生鑄漏之危險之步驟包括有:使用上述總熱通 量Q1,根據下式(2)而推定鑄模出口處之凝固殼厚度D之步 驟;使用根據下述式(3)所求得之凝固延遲度RS ,藉由D1 ❷ =D(1 —RS)之關係來推定考慮了凝固延遲之凝固殼厚度D1 之步驟,該凝固延遲係因由總熱通量Q2所引起之再熔解而 產生者;及根據上述所推定之凝固殼厚度D1及預先以與產 • 生鑄漏之危險性的關係所求得之臨限值,判定有無產生鎊漏 - 之危險之步驟。 D = Q1/(AH · p ) (2) 其中,D :鑄模出口處之凝固殼厚度(m) Q1 :總熱通量(J/m2) 098106495 35 200946265 △Η :鑄模出口處之凝固殼之每單位重量之捨降(J/kg) p :鑄模出口之凝固殼密度(kW) RS= y(9x(V0'8*A6> ) .........(3) 其中,RS :凝固延遲度(無單位) y?:凝固延遲常數(無單位) V :熔鋼流速(m/s) Δ0 :嫁鋼過熱度(°C)The indicator of heat reading, Q2 is used as a criterion for exceeding the stability of the (4) interface heat I. According to Q1 or according to the collection and acceptance, it is determined whether there is a risk of praying. Further, the present invention is the method for detecting a casting leak in the continuous casting according to the above (2), and in the step of determining whether or not there is a risk of casting leakage in the above-mentioned step 098106495 32 200946265, Q1 can also be used as an increase in value. To deal with the factor of reducing the risk of casting leakage, Q2 is treated as a factor that increases the risk of casting leakage by increasing the value, and the risk of casting leakage is determined according to Q1 or according to Q1 and Q2. (4) The method for detecting a casting leak in continuous casting according to (2) or (3) above, wherein the step of determining whether or not there is a risk of casting leakage based on the total heat flux Q1 is 'pre-set for Q1 The threshold value α b α 2 (α 1 < α 2), 参() 田 Q1 < α 1日寺' is judged to be a risk of casting leakage, (ii) when α 1 SQ1 $ α 2 'according to Q2 The value is determined to be a risk of casting leakage. Here, it is preferable that when Q2 reaches a threshold value (which may be a fixed value in the entire range of aal_Ql$a2) set in advance according to Q1, it is judged that there is a risk of a prayer leak. The casting leak detection method of continuous casting described in any one of the above, ';10_the above (ql - q2reg) obtained in the above heat flux distribution, there is a case indicating the threshold of the minimum detection setting At the time, relative to the threshold for Q1, ^(1)a2Ul<a2) and _, or 4 1 for Q2, or (10) heart 1 and the risk of leakage. 11·. 2 and Q2 is judged as the method of continuous casting of the castings in this month. Continued casting _ ton □ 疋 疋 朝 朝 朝 朝 凝固 埶 埶 埶 : : : : 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 098 , the heat flux ql; according to the following formula (1) to obtain a stable shape 33 200946265 state of the molten steel flow in the mold caused by the steady solidification interface heat input q2reg; for the heat flux "with stable solidification interface heat input called The difference (ql - q2reg) 'determines the heat flux distribution of the molten steel from the furnace bath surface to the casting exit; and when there is a minimum point indicating the minimum value in the heat flux distribution, when using the straight line When the local heat flux value at the exit point of the mold is connected, the total heat flux corresponding to the area of the upper portion of the straight line is set to Q2', and the total heat flux corresponding to the following area is set to Q1. The area is the total heat flux from the total area enclosed by the entire curve of the heat flux distribution from the position of the bath surface to the exit of the mold minus the area obtained by Q2, and is preset relative to Q1 Proximity limit, α2 (αΐ< α2) and needle Q2 preset threshold stone 'when Ql<al and Q2 2/3, or Ql<al and Q2</3, or Q22 is absent, it is judged that there is a danger of pound leakage. (6) As above ( 5) The method for detecting the casting leakage of continuous casting, wherein the molten steel is extremely low carbon steel, α 1 is 15000 (kJ/m 2 ), α 2 is 2 l 〇〇〇 (kJ/m 2 ), and 々 is 4500 (kJ / M2) (7) The method for detecting a casting leak in continuous casting according to (2) or (3) above, wherein the step of determining whether or not there is a risk of casting leakage based on the total heat flux Q1 includes: using the total The heat flux Q1, the step of estimating the solidified shell thickness D at the exit of the mold according to the following formula (2); and the thickness D of the solidified shell estimated according to the above and the relationship between the pre-existing and the risk of casting leakage The threshold value is used to determine whether there is a risk of causing scale leakage. 098106495 34 200946265 D== Q1/(AH · p ) (2) where D: the thickness of the solidified shell at the exit of the mold Q1: total heat flux (j/y) AH: enthalpy drop per unit weight of the solidified shell at the exit of the mold (j/kg) P: solidified shell density at the exit of the mold (kg/m3) and 'the above ql Unit set to J/s.m2, in the above formula (1), the unit of q2reg is J/s · m2 ', the unit of h is J/s · m2 ·. 〇, the unit of A0 设为 is set to .C. (8 A casting leak detecting method of continuous casting according to (2) or (3) above, wherein when there is a minimum point indicating a minimum value in the heat flux distribution obtained for the above (ql - q2reg) The step of determining whether or not there is a risk of casting leakage based on the total heat fluxes Q1 and Q2 includes the step of estimating the solidified shell thickness D at the exit of the mold according to the following formula (2) using the above total heat flux Q1; Using the relationship of D1 ❷ = D (1 - RS), the solidification delay thickness RS determined by the following formula (3) is used to estimate the solidified shell thickness D1 in consideration of the solidification delay, which is caused by the total The remelting caused by the heat flux Q2 is generated; and based on the above-mentioned estimated solidified shell thickness D1 and the threshold value obtained in advance in relation to the risk of production and production of the casting leakage, the presence or absence of a pound leak is determined. - The dangerous step. D = Q1/(AH · p ) (2) where D is the thickness of the solidified shell at the exit of the mold (m) Q1 : total heat flux (J/m2) 098106495 35 200946265 △Η : the solidified shell at the exit of the mold Drop per unit weight (J/kg) p : solidified shell density (kW) at the exit of the mold RS = y (9x(V0'8*A6> ) ... (3) where RS : Solidification delay (no unit) y?: Solidification delay constant (no unit) V: Melt flow rate (m/s) Δ0 : Glazing steel superheat (°C)
此處,V=(Q2/(a · t · ΑΘ ))125 Q2 :總熱通量(J/m2) α :熔鋼流速常數(無單位) t:凝固殼經由熱通量分布中之極小點後到達鑄模出口為 止所需之時間(S)Here, V = (Q2 / (a · t · ΑΘ )) 125 Q2 : total heat flux (J / m2) α : molten steel flow rate constant (no unit) t: solidified shell through the heat flux distribution is very small Time required to reach the exit of the mold after the point (S)
又’將上述ql之單位設為j/s · m2,於上述式(1)中,將 q2reg之單位設為J/s · m2 ’將h之單位設為j/s · m2 ·乞,將 △ 0之單位設為。C。 再者,較佳為於針對上述(ql—q2reg)所求得之上述熱通^ 分布中不存在表示極小值之極小點之情形時,以上 方法來推定鑄模出口處之凝固殼厚度,於針對上=(7)$ q2reg)所求得之上述該熱通量分布中存在表叫小Further, 'the unit of ql is set to j/s · m2, and in the above formula (1), the unit of q2reg is J/s · m2 ', and the unit of h is set to j/s · m2 ·乞, The unit of △ 0 is set. C. Furthermore, it is preferable that the above method estimates the thickness of the solidified shell at the exit of the mold when there is no minimum point indicating the minimum value in the heat flux distribution obtained for the above (ql - q2reg), Above = (7) $ q2reg), the above-mentioned heat flux distribution obtained by the above is called small
點之情形時,以上述(8)之方法來推定鑄模出口處之之極’J 厚度’並根據該推定值與上_限值來狀有 _固★ 危險。 .、、、屐生鑄& 098106495 36 200946265 (9)如上述(1)至(6)中任—項之連續鑄造之鑄漏檢出方 法其中&通量ql係於鱗模之鑄造方向設置複數個成一 對之熱電偶根據上述-對熱電偶之輸出而由下式⑷求得 .之局部熱通量’上述一斜熱電偶係埋入至鑄模内於鎊模厚度 方向上之埋入深度不同的兩點間者。 ql= λ(Τ1—T2)/d .........⑷ 其中,λ :鑄模之熱導率 ⑩ ΤΙ、Τ2 :熱電偶之檢出溫度 d:熱電偶之埋設間隔 (10)如上述(7)或(8)之連續鑄造之鑄漏檢出方法,其中, 熱通量ql係於鑄模之厚度方向設置複數個成一對之熱電 偶’根據上述一對熱電偶之輸出而由下式(4)求得之乃部熱 通量’上述一對熱電偶係埋入至鑄模内於鑄模之厚声方白上 之埋入深度不同的兩點間者 (4) q1 ~ λ (ΤΙ — Τ2)/d 其中,λ :鑄模之熱導率(J/s · m · °C) ΤΙ、T2 :熱電偶之檢出溫度(°C) d :熱電偶之埋設間隔(m) (11)一種連續鑄造之鑄漏檢出裝置,其包括有:熱電偶 群,於鑄模之鑄造方向設置複數個成一對之熱電偶而形成, 該一對熱電偶係埋入至於鑄模厚度方向上之深度不同之兩 點者; 098106495 37 200946265 局部熱通量運算手段,輸入來自該熱電偶群之溫度資訊而 求得各熱電偶設置部位之局部熱通量ql ;穩定凝固界面熱 輸入記憶手段,記憶根據下式(1)所求得之穩定狀態下鑄模 内之熔鋼流動所引起的穩定凝固界面熱輸入q2reg之資料; 分布運算手段,針對該等熱通量ql與穩定凝固界面熱輸入 q2reg之差(ql — q2reg),求得熔鋼自爐浴面到達鑄模出口為止 之熱通量分布;及鑄漏判定手段,根據所求得之熱通量分布 來判定有無產生鑄漏之危險。 q2reg= h · Δ θ .........(1) 其中,h:熔鋼與凝固殼之間之熱傳遞係數 ΑΘ :熔鋼之過熱度。 (12)如上述(11)之連續鑄造之鑄漏檢出裝置,其中上述鑄 漏判定手段係如下者: 根據上述熱通量分布,由以下方法求得總熱通量Q1及 Q2 :即,(i)於上述該熱通量分布中存在表示極小值之極小 點之情形時,當利用直線連結該極小點與鑄模出口處之局部 熱通量值時,將與該直線更上方部分之面積相當的總熱通量 設為Q2,將與如下面積相當之總熱通量設為Q1,該面積係 自與由自爐浴面位置至鑄模出口間之該熱通量分布之整個 曲線所包圍的總面積相當之總熱通量減去Q2所獲得之面 積,(ii)於上述該熱通量分布中不存在表示極小值之極小點 之情形時,將與由自爐浴面位置至鑄模出口間之該熱通量分 098106495 38 200946265 布之整個曲線所包gj的總面積相#之總熱通量設為總熱通 量Q1,將Q2設為零, 根據上述總熱通量Q1,或者根據Q1及Q2來判定有無產 生鑄漏之危險。 (13)如上述(12)之連續鑄造之鑄漏檢出裝置,其中,上述 禱漏判定手段係如下者:將上述總熱通量Q1作為由凝固所 引起之排熱量之指標,並視需要將q2作為超過穩定的凝固 ❹界面熱輸入之指標,根據Q1或者根據Q1及Q2來判定有無 產生鑄漏之危險。 再者,如上述(12)之連續鑄造之鑄漏檢出裝置,其中,上 述鑄漏判定手段係如下者:將Q1作為藉由數值之增大來降 低鑄漏之風險之因數而處理,將Q2作為藉由數值之增大來 增大鱗漏之風險之因數而處理’並根據Q1或者根據Q1及 Q2來判定有無產生鎊漏之危險。 © (14)如上述(12)或(13)之連續鑄造之鑄漏檢出裝置,其 中’上述鑄漏判定手段係如下者:相對於針對上述總熱通量 Q1所預先設定之臨限值α 1、α 2( α 1 < α 2),(丨)當Q1 < α .1時,判定為有鑄漏之危險,⑻當田時,根據 • Q2之值而判定為有鑄漏之危險。 此處,較佳為當Q2達到根據Q1而預先設定之臨限值(亦 可為心抑^2之整個範圍中_定值)以上時,判定為 有禱漏之危險。 098106495 39 200946265 (15)如上述(12)或(13)之連續鑄造之鑄漏檢出裝置,其 中,上述鑄漏判定手段係如下者:於針對上述(ql —q2reg) 所求得之上述熱通量分布中存在表示極小值之極小點之情 形時,相對於針對Q1所預先設定之臨限值αΐ、1< α 2)及針對Q2所預先設定之臨限值万,當(i)Ql< α 1且Q2 2/5,或者(ii)Ql< α 1 且 Q2< 召,或者(iii)a 1SQ1S α 2 且Q2 2 /3時,判定為有鑄漏之危險。 即,本發明之連續鑄造之鑄漏檢出裝置特徵在於包括有: 熱電偶群,於鑄模鑄造方向設置複數個成一對之熱電偶而形 成,該一對熱電偶係埋入至於鑄模厚度方向之埋入深度不同 之兩點間者;局部熱通量運算手段,輸入來自該熱電偶群之 溫度資訊而求得各熱電偶設置部位之局部熱通量ql ;穩定 凝固界面熱輸入記憶手段,記憶根據下式(1)所求得之穩定 狀態下之鑄模内熔鋼流動所引起的穩定凝固界面熱輸入 q2reg之資料;分布運算手段,針對該等熱通量ql與穩定凝 固界面熱輸入q2reg之差(ql —q2reg),求得熔鋼自爐浴面到達 鑄模出口為止之熱通量分布;及鑄漏判定手段,於由該分布 運算手段所求得之熱通量分布中存在表示極小值之極小點 之情形時,當利用直線連結該極小點與鑄模出口處之局部熱 通量值時,將與該直線更上方部分之面積相當的總熱通量設 為Q2,將與如下面積相當之總熱通量設為Q1,該面積係自 與由自爐浴面位置至鑄模出口間之該熱通量分布之整個曲 098106495 40 200946265 線所包圍的總面積相當之總熱通量減去Q2所獲得之面積, 且對於針對Q1所預先設定之臨限值α 1、α2(α 1< α2)及 針對Q2所預先設定之臨限值石,當Ql< α 1且Q2 2 yS,或 者Ql< α 1且Q2< /3,或者a 1SQ1S α 2且Q22 /3時判定 為有鑄漏之危險。 (16) 如上述(15)之連續鑄造之鑄漏檢出裝置,其中,於熔 鋼為極低碳鋼之情形時,將α 1設定為15000(kJ/m2),將α ❹ 2 設定為 21000(kJ/m2),將/3 設定為 4500(kJ/m2)。 (17) 如上述(12)或(13)之連續鑄造之鑄漏檢出裝置’其 中’上述鑄漏判定手段包括有:凝固殼厚度運算手段,使用 總熱通量Q1 ’根據下式(2)而對鑄模出口處之凝固殻厚度D 進行運算;及鑄漏判定手段本體,輸入上述凝固殼厚度運算 手段之運算值,根據該運算值D及預先以與產生鑄漏之危險 性的關係所求得之臨限值而判定有無產生鑄漏之危險。 〇 D = Q1/(AH · p ) .........(2) 其中’ D :鑄模出口處之凝固殼厚度(m) Q1 :總熱通量(J/m2) . ΔΗ :鑄模出口處之凝固殼之每單位重量之焓降(j/kg) . P :鑄模出口之凝固殼密度(kg/m3) 又’將上述ql之單位設為J/s · m2,於上述式(1)中,將 q2reg之單位設為J/s · m2 ’將h之單位設為j/s · m2 · °C,將 Δ6»之單位設為。C。 098106495 41 200946265 (18^-hi4(12)^(13)^ 中,上述鑄漏判定手段U· 裝置其 熱通量Q1,根據下式(2、斟锆松, 丹卞仅使用總 運算,進岐㈣據下料 糾度D進仃 ,ni_nn_nCN 所衣侍之凝固延遲度RS,藉 由Μ = Ι)( -RS)之關係而對經考慮凝 Μ進行·該凝固延遲係因由總熱通量Q2::t 解而產生者;及鑄漏判定手段 :、二起之再炫 算手段之運算值,根據”· m輸人上錢固殼厚度運 ㈣運算值D1及縣 危險性的_財得之臨紐_定有減㈣漏之危險 D —Q1/(ΔΗ · p ) .........(2) 其中,D :鑄模出口處之凝固殼厚度(m) Q1 :總熱通量(J/m2) △Η ··鑄模出口處之凝固殼之每單位重量之焓降(J/kg) .缚模出口之凝固殼密度(kg/m3) RS= /3x(V° 8·Δ6» ) .........(3) 其中’ RS :凝固延遲度(無單位) 万:凝固延遲常數(無單位) v :熔鋼流速(m/s) △Θ :熔鋼過熱度(°c) 此處,V = (Q2/( α · t · A 0 ))125 Q2 :總熱通量(J/m2) α :熔鋼流速常數(無單位) 098106495 42 200946265 t:凝固殼㈣熱通量分布中之極小點後到達鱗模出口為 止所需之時間(s) 、 又將上述ql之單位設為J/s.m2,於上述式⑴中將_ •之單位設為J/S · m2,將h之單位設為J/s · β t,將“ 之單位設為。C。 再者,上述凝固殼運算手段較佳為如下者:當⑻一―) 之熱通里刀布中不存在表不極小值之極小點時,以上述(⑺ ❹之方法來對鑄模出口處之凝固殼厚度進行運算,當熱通量分 布中存在表示極小值之極小點時,以上述(⑻之方法來對籍 模出口處之凝固殼厚度進行運算。 (19) 一種連續鑄造之鑄漏防止裝置,其係使用有上述(11) 至(18)中任一項之鑄漏檢出裝置者;其特徵在於:其包括有 控制手段,該控制手段輸入鑄漏判定手段之信號,於鑄漏判 疋手段判定為有鑄漏之危險之情形時,以降低鑄造速度之方 ❿式控制操作條件,或者除該控制以外,進行使鑄模内之熔鋼 流速下降之控制。 (20) —種連續鑄造之鑄漏防止裝置,其係使用有如上述 (11)至(18)中任一項之鑄漏檢出裝置者;其特徵在於:其包 - 括有控制手段,該控制手段輸入鑄漏判定手段之倌號,當鑄 漏判定手段判定為有鑄漏之危險時,以減慢鑄造速度之方式 進行控制。 (21) —種連續鑄造之鑄漏防止裝置, 其係使$有如上述 098106495 43 200946265 (15)或(16)之鑄漏檢出裝置者;其特徵在於: 其包括有控制手段,該控制手段輸入鱗漏判定手段之信 號,於鑄關定手段判定為錢漏之危險之情形下,⑴當 該有危險之判定為基於Q1< α丨A Q2^之危險判定時, (a)以降低铸造速度及/或增_模冷卻之方式控制操作條 件’或者⑹除該控制以外,進行使鑄模内之炫鋼流速下降 之控制;(Π)當為基於Q1< α 1且之危險判定時,以 降低鑄造速度及/或增強鑄模冷卻之方式控制操作條件;㈤ 當為基於且Q2“之危險判定時,進行(A) 使鑄模内之熔鋼流速下降’或者進而⑻降低鑄造速度及/ 或增強鑄模冷卻之控制。 ⑽-種鋼之連_造枝,錢使时上述⑷ 漏檢出方法者;其特徵在於,以如下方式控制操作條件,即 ⑴使Q1 > α 2、或者(jj)铺]<m 判定為有•漏之危險之以2且使Q2成為未被 ⑽-種鋼之連續轉造方法,其係使时上述⑸或⑹ 之鑄漏檢出方法者;其特徵在於,以成為Ql> W且_ 沒’或者Qlg α 1且q2< 0之方式控制操作條件。 (24)如上述(23)之鋼之連續鑄造方法,其中,於操作中, ⑴當Ql< α 1且時’⑷以降低鎊造速度及/或增強 鑷模冷卻之以_操作條件,或者除該控制料,⑻以 使鑄模内之雜流迷下降之方式控制操作條件,當Q1< 098106495 200946265 αΐ且Q2<万時,以降低鏵造速度及/或增強鱗模冷卻之方 式控制操作條件,(iii)tal_^2且收以時,以如 下方式控制操作條件,(A)使鱗模内之溶鋼流迷下降,或者 進而⑻降料造速度及/或増_模冷卻。 (25) 如上述(22)至(24)中任-項之鋼之連續鎊造方法,其 中’熱通量dl係於鑄模之铸造方向設置複數個成一對之熱 電偶’根據上述-賴電偶讀㈣由下式⑷求得之局部 © 熱通量,上述-對熱電偶係埋入至鑷模内於鑄模厚度方向上 之埋入深度不同之兩點間者。 ql= λ (Tl-T2)/d .........⑷ 其中’ λ :鑄模之熱導率 T1 ' :熱電偶之檢出溫度 d :熱電偶之埋設間隔 (26) —種鋼之連續鑄造方法,其係使用有上述(7)之鑄漏 ❹檢出方法者;以使所推定之凝固殼厚度D大於預先以與產生 鎿漏之危險性的關係所求得之臨限值之方式,控制操作條 件。 ♦ (27)一種鋼之連續鑄造方法,其係使用有如上述(8)之鑄 - 漏檢出方法者;以使所推定之凝固殼厚度D1小於預先以與 產生鑄漏之危險性的關係所求得之臨限值之方式,控制操作 條件。 再者,較佳為當(q1 — d2reg)之熱通量分布中不存在極小點 098106495 45 200946265 時,利用上述(26)之方法進行連續鑄造,當存在極小點時, 利用上述(27)之方法進行連續鑄造。 (28)—種連續鑄造之凝固殼厚度推定方法,其特徵在於, 其包括有:測定連續鑄造中鑄模内之熔鋼自爐浴面到達鑄模 出口為止之期間朝凝固界面熱輸入之熱通量ql之步驟;根 據下式(1)而求得穩定狀態下之鑄模内熔鋼流動所引起之穩 定凝固界面熱輸入q2reg之步驟;就該等熱通量ql(J/s · m2) 與穩定減固界面熱輸入Q2reg之差(Ql — Q2reg) ’求付溶鋼自爐 浴面到達鑄模出口為止之熱通量分布之步驟;及(i )於上述 該熱通量分布中存在表示極小值之極小點之情形時,當利用 直線連結該極小點與鑄模出口處之局部熱通量值時,將與該 直線更上方部分之面積相當的總熱通量設為Q2,將與如下 面積相當之總熱通量設為Q1,該面積係自與由自爐浴面位 置至鑄模出口間之該熱通量分布之整個曲線所包圍的總面 積相當之總熱通量減去Q2所獲得之面積,(ii)於上述熱通 量分布中不存在表示極小值之極小點之情形時,將與由自爐 浴面位置至鑄模出口間之該熱通量分布之整個曲線所包圍 的總面積相當的總熱通量設為總熱通量Q1, 使用該等總熱通量Q1,根據下式(2)來推定鑄模出口處之 凝固殼厚度D之步驟。 q2reg = h · ΑΘ .........(1) 其中,q2reg :穩定凝固界面熱輸入(J/s · m2) 098106495 46 200946265 h :熔鋼與凝固殼之間之熱傳遞係數(J/s · m2 · °C ) A0 :熔鋼之過熱度(°C) D = Ql/(AH.p) .........(2) 其中,D :鑄模出口處之凝固殼厚度(m) Q1 :總熱通量(J/m2) AH :鑄模出口處之凝固殼之每單位重量之焓降(J/kg) p :鑄模出口之凝固殼密度(kg/m3)。 φ (29)—種連續鑄造之凝固殼厚度推定方法,其係於熱通量 分布中存在表示極小值之極小點之情形時,推定經考慮凝固 延遲之凝固殼厚度D1者,該凝固延遲係因由總熱通量Q2 所引起之再熔解而產生者;其特徵在於,若將由上述(28) 所求得之凝固殼厚度作為D,則D1 = D(1 —RS)。 其中,RS= /3χ(ν°.8·Δ0 ) .........(3) RS :凝固延遲度(無單位) φ yS :凝固延遲常數(無單位) V :熔鋼流速(m/s) Α6» :熔鋼過熱度(°C) ^ 此處,V=(Q2/(a · t · Δ0 ))125 Q2 :總熱通量(J/m2) α :熔鋼流速常數(無單位) t:凝固殼經由熱通量分布中之極小點後到達鑄模出口為 止所需之時間(S) 098106495 47 200946265 再者’較佳為當(ql-q2reg)之熱通耋分布中不存在極小點 時,利用上述(28)之方法來推測凝固殻厚度(D),當存在極 小點時利用上述(29)之方法來推測凝固殼厚度(D1),藉此分 別推定凝固殼厚度。 (30)如上述(28)或(29)之連續鑄造之凝固殼厚度推定方 法,其中’熱通量ql係於鑄模之鑄造方向設置複數個成一 對之熱電偶,根據上述一對熱電偶之輸出而由下式(4)求得 之局部熱通量,上述一對熱電偶係埋入至鑄模内於鎊模厚度 方向之埋入深度不同之兩點間者。 ql= λ (Tl-T2)/d .........(4) 其中’ Ql :熱通量(J/s · m2) 入:鑄模之熱導率(J/s.m· °C) ΤΙ、T2 :熱電偶之檢出溫度CC) d :熱電偶之埋設間隔(m) (3υ —種連續鑄造之凝固殼厚度推定裝置,其特徵在方 熱電偶群,於鑄模之鑄造方向上設置複數個成 、之…〆*㈣成,該—對熱電偶係埋人至 之深度不同之兩點者;局部 電偶群之溫度㈣而求 以 置部位之局部熱通 熱輪入記憶手段,記憶根據下式⑴所 模内溶鋼流動所叫的穩定凝固界面 輸入‘之m布運算手段,針_ 098106495In the case of a point, the pole 'J thickness' at the exit of the mold is estimated by the method of the above (8), and it is dangerous according to the estimated value and the upper limit value. .,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, A plurality of thermocouples are provided in accordance with the above-mentioned - for the output of the thermocouple, the local heat flux obtained by the following formula (4). The above-mentioned oblique thermocouple is buried in the mold in the thickness direction of the pound mold. Two points with different depths. Ql= λ(Τ1—T2)/d (4) where λ : thermal conductivity of the mold 10 ΤΙ, Τ 2 : detection temperature of the thermocouple d: embedding interval of the thermocouple (10) A casting and leak detecting method for continuous casting according to (7) or (8) above, wherein the heat flux q1 is a plurality of pairs of thermocouples in the thickness direction of the mold, based on the output of the pair of thermocouples The heat flux of the above formula (4) is obtained by embedding the pair of thermocouples into the mold at two points of different depths of the thick sound of the mold (4) q1 ~ λ ( ΤΙ — Τ2)/d where λ : thermal conductivity of the mold (J/s · m · °C) ΤΙ, T2 : temperature of the thermocouple (°C) d : buried interval of the thermocouple (m) ( 11) A continuous casting casting leakage detecting device comprising: a thermocouple group formed by providing a plurality of thermocouples in a casting direction of the casting mold, the pair of thermocouples being embedded in a depth in a thickness direction of the casting mold Two different points; 098106495 37 200946265 Local heat flux calculation method, input the temperature information from the thermocouple group and find the location of each thermocouple setting part Partial heat flux ql; stable solidification interface heat input memory means, memory according to the following formula (1) obtained in the steady state of the molten steel flow in the mold caused by the steady solidification interface heat input q2reg data; distribution operation means, For the difference between the heat flux ql and the stable solidification interface heat input q2reg (ql - q2reg), the heat flux distribution of the molten steel from the furnace bath surface to the mold exit is obtained; and the casting leakage determination means is obtained according to the obtained The heat flux distribution determines the risk of casting leakage. Q2reg= h · Δ θ (1) where h: the heat transfer coefficient between the molten steel and the solidified shell ΑΘ : the superheat of the molten steel. (12) The casting and leak detecting device for continuous casting according to (11) above, wherein the casting leakage determining means is as follows: based on the heat flux distribution, the total heat fluxes Q1 and Q2 are obtained by the following method: (i) in the case where there is a minimum point indicating the minimum value in the heat flux distribution, when the minimum heat flux value at the exit of the mold is connected by a straight line, the area above the straight line is The equivalent total heat flux is set to Q2, and the total heat flux corresponding to the area is set to Q1, which is surrounded by the entire curve from the heat flux distribution from the bath surface position to the mold exit. The total area is equivalent to the total heat flux minus the area obtained by Q2, and (ii) when there is no minimum point indicating the minimum value in the heat flux distribution, the position from the bath surface to the mold The heat flux between the outlets is 098106495 38 200946265 The total heat flux of the total area of the gj package is set to the total heat flux Q1, and Q2 is set to zero, according to the above total heat flux Q1, Or determine the risk of casting leakage based on Q1 and Q2. (13) The casting and leak detecting device for continuous casting according to the above (12), wherein the above-mentioned prayer leakage determining means is such that the total heat flux Q1 is used as an index of heat generation caused by solidification, and if necessary Use q2 as an indicator of the heat input exceeding the stable solidification enthalpy interface, and determine whether there is a risk of casting leakage according to Q1 or according to Q1 and Q2. Further, the casting and leak detecting device of the continuous casting according to the above (12), wherein the casting leakage determining means is as follows: Q1 is treated as a factor that reduces the risk of casting leakage by increasing the numerical value, and Q2 is treated as a factor that increases the risk of scale leakage by increasing the value and determines whether there is a risk of pound leakage based on Q1 or according to Q1 and Q2. (14) The casting and leak detecting device for continuous casting according to (12) or (13) above, wherein the above-mentioned casting leakage determining means is as follows: a predetermined threshold value with respect to the total heat flux Q1 described above α 1 , α 2 ( α 1 < α 2), (丨) When Q1 < α .1, it is judged that there is a risk of casting leakage, and (8) when it is in the field, it is judged to have a casting leak according to the value of • Q2 The danger. Here, it is preferable that when Q2 reaches a threshold value (which may be a predetermined value in the entire range of the heartbeat) which is set in advance according to Q1, it is preferable to have a risk of praying. The casting leakage detecting device of the continuous casting according to the above (12) or (13), wherein the casting leakage determining means is as follows: the heat obtained by the above (ql - q2reg) When there is a case where the minimum value indicating the minimum value exists in the flux distribution, the threshold value α ΐ, 1 < α 2) preset for Q1 and the threshold value set in advance for Q2, when (i) Ql < When α 1 and Q2 2/5, or (ii) Ql < α 1 and Q2 < 召, or (iii) a 1SQ1S α 2 and Q2 2 /3, it is judged that there is a risk of casting leakage. That is, the continuous casting casting leak detecting device of the present invention is characterized by comprising: a thermocouple group formed by providing a plurality of thermocouples in a casting direction, and the pair of thermocouples are buried in the thickness direction of the mold. Into the two points with different depths; local heat flux calculation means, input the temperature information from the thermocouple group to obtain the local heat flux ql of each thermocouple setting part; stable solidification interface heat input memory means, memory basis The data of the stable solidification interface heat input q2reg caused by the flow of the molten steel in the mold under the steady state (1) obtained by the following formula (1); the distribution calculation means, the difference between the heat flux ql and the stable solidification interface heat input q2reg (ql - q2reg), the heat flux distribution of the molten steel from the furnace bath surface to the exit of the mold is obtained; and the casting leakage determining means has a minimum value in the heat flux distribution obtained by the distributed computing means In the case of a very small point, when a local heat flux value at the exit point of the mold is connected by a straight line, the total heat flux corresponding to the area of the upper portion of the straight line is used. For Q2, the total heat flux equivalent to the following area is set to Q1, which is the total area enclosed by the line 098106495 40 200946265 from the heat flux distribution from the bath surface position to the mold exit. The equivalent total heat flux minus the area obtained by Q2, and for the threshold values α 1 , α 2 ( α 1 < α 2 ) preset for Q1 and the threshold stone preset for Q2, when Ql < α 1 and Q2 2 yS, or Ql < α 1 and Q2 < /3, or a 1SQ1S α 2 and Q22 /3 are judged to be a risk of casting leakage. (16) The casting and leak detecting device for continuous casting according to the above (15), wherein, in the case where the molten steel is extremely low carbon steel, α 1 is set to 15000 (kJ/m 2 ), and α ❹ 2 is set to 21000 (kJ/m2), set /3 to 4500 (kJ/m2). (17) The casting and leak detecting device of the continuous casting of the above (12) or (13) wherein the above casting leakage determining means includes: a solidified shell thickness calculating means, using the total heat flux Q1' according to the following formula (2) And calculating the thickness D of the solidified shell at the exit of the mold; and the main body of the casting leakage determining means, inputting the calculated value of the solidified shell thickness calculating means, based on the calculated value D and the relationship with the risk of casting leakage in advance The limit value is obtained to determine whether there is a risk of casting leakage. 〇D = Q1/(AH · p ) (2) where ' D : solidified shell thickness at the exit of the mold (m) Q1 : total heat flux (J/m2) . ΔΗ :焓 每 (j/kg) per unit weight of the solidified shell at the exit of the mold. P : solidified shell density at the exit of the mold (kg/m3) and 'the unit of ql above is set to J/s · m2, in the above formula In (1), the unit of q2reg is set to J/s · m2 'The unit of h is set to j/s · m2 · °C, and the unit of Δ6» is set. C. 098106495 41 200946265 (18^-hi4(12)^(13)^, the above-mentioned casting leakage determination means U· device heat flux Q1, according to the following formula (2, zirconia pine, Danyu only use the total calculation, into岐 (4) According to the material correction D, ni, ni_nn_nCN The solidification delay RS of the clothing, by the relationship of Μ = Ι) (-RS), the coagulation delay is caused by the total heat flux Q2::t solves the generator; and the method of casting and leaking judgment: the calculation value of the re-shock calculation method of the two, according to "· m loses the money, the thickness of the solid shell (4), the calculated value D1, and the county's risk There is a risk of loss (4) leakage D - Q1/(ΔΗ · p ) (2) where D: the thickness of the solidified shell at the exit of the mold (m) Q1 : total Heat flux (J/m2) △Η ··The drop per unit weight of the solidified shell at the exit of the mold (J/kg). The solidified shell density at the exit of the mold (kg/m3) RS= /3x(V° 8·Δ6» ) (3) where 'RS : solidification delay (no unit) 10,000: solidification delay constant (no unit) v : molten steel flow rate (m/s) △Θ : Fused steel superheat (°c) where V = (Q2/( α · t · A 0 )) 125 Q2 : total heat flux (J/m2) α : molten steel flow rate constant (no unit) 098106495 42 200946265 t: time required for the solidified shell (4) to reach the scale exit after the minimum point in the heat flux distribution (4), and the unit of ql above is set to J/ S.m2, in the above formula (1), the unit of _ • is set to J/S · m2, the unit of h is set to J/s · β t, and the unit of " is set to .C. Further, the solidified shell described above Preferably, the calculation means is: when there is no minimum point of the minimum value in the heat-passing knife cloth of (8)--), the thickness of the solidified shell at the exit of the mold is calculated by the above method ((7), When there is a minimum point indicating a minimum value in the heat flux distribution, the thickness of the solidified shell at the exit of the die is calculated by the above method ((8). (19) A continuous casting casting leakage preventing device is used The casting and leak detecting device according to any one of the above (11), wherein the control means inputs a signal of the casting leakage determining means, and the casting leakage determining means determines that In the case of the danger of casting leakage, the control operation is to reduce the casting speed. Or, in addition to the control, control for lowering the flow rate of the molten steel in the mold. (20) A continuous casting casting leakage preventing device using any one of the above (11) to (18). The casting leakage detecting device is characterized in that: the package includes a control means, and the control means inputs the nickname of the casting leakage determining means, and when the casting leakage determining means determines that there is a risk of casting leakage, the casting speed is slowed down The way to control. (21) A continuous casting casting leakage preventing device, which is a casting leak detecting device of the above-mentioned 098106495 43 200946265 (15) or (16); characterized in that it comprises a control means, the control means When the signal of the scale leakage determination means is input, and the risk of money leakage is determined by the casting method, (1) when the risk determination is based on the risk determination of Q1 < α丨A Q2^, (a) to reduce the casting Speed and / or increase mode cooling mode to control operating conditions ' or (6) in addition to the control, to control the flow rate of the red steel in the mold; (Π) when based on Q1 < α 1 and the risk determination, Reduce the casting speed and / or enhance the cooling mode of the mold to control the operating conditions; (5) When based on the Q2 "danger determination, carry out (A) reduce the flow rate of the molten steel in the mold ' or (8) reduce the casting speed and / or enhance Control of mold cooling. (10) - Connection of steel type _ spurting, money making time (4) Leak detection method; characterized by controlling the operating conditions in the following manner, that is, (1) making Q1 > α 2, or (jj) Shop]<m judged to have The risk is 2 and Q2 is a continuous transfer method of the (10)-type steel, which is the method for detecting the casting and leaking of the above (5) or (6); characterized in that it is Q1 > W and _ no Or the operating condition is controlled by the method of Qlg α 1 and q2 < 0. (24) The continuous casting method of steel according to (23) above, wherein, in operation, (1) when Ql < α 1 and then '(4) to lower the speed of the pound And / or enhance the cooling of the mold to the operating conditions, or in addition to the control material, (8) to control the operating conditions in a manner to reduce the flow of the flow of the mold, when Q1 < 098106495 200946265 α ΐ and Q2 &10000; The operating speed is controlled by the speed and/or the way of strengthening the scale mold. (iii) When tal_^2 is received, the operating conditions are controlled as follows: (A) the molten steel flow in the scale mold is lowered, or (8) is lowered. (25) A method of continuous pound making of steel according to any one of the above (22) to (24), wherein 'the heat flux dl is set in a plurality of casting directions of the mold A pair of thermocouples' according to the above-mentioned Lai 读 reading (4) is obtained by the following formula (4). Flux, above - for the thermocouple to be buried between the two points in the die in the thickness direction of the mold, the difference between the two points. ql = λ (Tl-T2) / d ......... (4) where 'λ: thermal conductivity T1 of the mold: detection temperature of the thermocouple d: embedding interval of the thermocouple (26) - continuous casting method of the steel, which uses the casting leakage test of the above (7) The method of controlling the operating conditions is such that the estimated solidified shell thickness D is greater than a threshold value determined in advance in relation to the risk of occurrence of leakage. ♦ (27) A continuous casting method for steel, which uses the casting-drain detecting method as described in the above (8); so that the estimated solidified shell thickness D1 is smaller than the relationship with the risk of casting leakage. The method of obtaining the threshold value and controlling the operating conditions. Furthermore, it is preferred that when there is no minimum point 098106495 45 200946265 in the heat flux distribution of (q1 - d2reg), continuous casting is performed by the method of (26) above, and when there is a minimum point, the above (27) is utilized. The method performs continuous casting. (28) A method for estimating the thickness of a solidified shell for continuous casting, characterized in that it comprises: determining a heat flux of heat input to a solidification interface during a period from a furnace bath surface to a mold exit in a mold in continuous casting Step of ql; determining the steady solidification interface heat input q2reg caused by the flow of the molten steel in the mold under steady state according to the following formula (1); and the heat flux ql (J/s · m2) and the stability The difference between the heat-reducing interface heat input Q2reg (Ql - Q2reg) 'steps to obtain the heat flux distribution of the molten steel from the furnace bath surface to the exit of the mold; and (i) the minimum value of the heat flux distribution In the case of a very small point, when the minimum heat flux value at the exit of the mold is connected by a straight line, the total heat flux corresponding to the area of the upper portion of the straight line is set to Q2, which is equivalent to the following area. The total heat flux is set to Q1, which is the total heat flux from the total area enclosed by the entire curve of the heat flux distribution from the bath surface location to the exit of the mold minus the area obtained by Q2. , (ii) above the heat flux When there is no minimum point indicating the minimum value in the distribution, the total heat flux corresponding to the total area surrounded by the entire curve of the heat flux distribution from the position of the bath surface to the exit of the mold is set as the total heat. The flux Q1, using the total heat flux Q1, estimates the solidified shell thickness D at the exit of the mold according to the following formula (2). Q2reg = h · ΑΘ .........(1) where q2reg : stable solidification interface heat input (J/s · m2) 098106495 46 200946265 h : heat transfer coefficient between molten steel and solidified shell ( J/s · m2 · °C ) A0 : superheat of molten steel (°C) D = Ql/(AH.p) ... (2) where D: solidification at the exit of the mold Shell thickness (m) Q1: Total heat flux (J/m2) AH: enthalpy drop per unit weight of the solidified shell at the exit of the mold (J/kg) p : solidified shell density (kg/m3) at the exit of the mold. Φ (29)—a method for estimating the thickness of a solidified shell of continuous casting, which is based on the case where there is a minimum point indicating a minimum value in the heat flux distribution, and the solidification delay system is estimated by considering the solidification shell thickness D1 considering the solidification delay. Produced by remelting caused by the total heat flux Q2; characterized in that D1 = D(1 - RS) when the solidified shell thickness obtained by the above (28) is taken as D. Where RS = /3χ(ν°.8·Δ0 ) (3) RS : solidification delay (no unit) φ yS : solidification delay constant (no unit) V : molten steel flow rate (m/s) Α6» : Fused steel superheat (°C) ^ Here, V=(Q2/(a · t · Δ0 )) 125 Q2 : Total heat flux (J/m2) α : Melt flow rate Constant (no unit) t: Time required for the solidified shell to reach the exit of the mold via the minimum point in the heat flux distribution (S) 098106495 47 200946265 Furthermore, it is better to be the heat-pass distribution of (ql-q2reg) When there is no minimum point, the solid shell thickness (D) is estimated by the method of (28) above, and when there is a minimum point, the solid shell thickness (D1) is estimated by the method of the above (29), thereby respectively estimating the solidified shell. thickness. (30) The method for estimating the thickness of a solidified shell of continuous casting according to (28) or (29) above, wherein 'the heat flux ql is a plurality of pairs of thermocouples in the casting direction of the mold, according to the pair of thermocouples The local heat flux obtained by the following formula (4) is outputted, and the pair of thermocouples are buried between the two points in the mold in which the depth of embedding in the thickness direction of the pound mold is different. Ql= λ (Tl-T2)/d (4) where 'Ql: heat flux (J/s · m2) into: thermal conductivity of the mold (J/sm· °C ΤΙ, T2: Thermocouple detection temperature CC) d: Thermocouple buried interval (m) (3υ - a continuous casting solid shell thickness estimation device, characterized by a square thermocouple group, in the casting direction of the mold Set a plurality of formations, ... 〆 * (four) into, the - the thermocouple is buried in two different depths; the temperature of the local galvanic group (four) and the local hot-through heat into the memory means According to the following formula (1), the flow of molten steel in the mold is called the stable solidification interface input 'm cloth operation means, needle _ 098106495
48 200946265 定凝固界面熱輸入q2reg之差(ql-q2reg),求得熔鋼自爐浴面 到達鑄模出口為止之熱通量分布;及凝固殼厚度運算手段, (i )於藉由該分布運算手段所求得之熱通量分布中不存 在表示極小值之極小點之情形時,將與由自爐浴面位置至鑄 模出口間之該熱通量分布之整個曲線所包圍的總面積相當 之總熱通量設為總熱通量Ql,(ϋ)於藉由該分布運算手段 所求得之熱通量分布中存在表示極小值之極小點之情形 ❹ 時,當利用直線連結該極小點與鑄模出口處之局部熱通量值 時,將與該直線更上方部分之面積相當的總熱通量設為 Q2,將與如下面積相當之總熱通量設為Q1,該面積係自與 由自爐浴面位置至鑄模出口間之該熱通量分布之整個曲線 所包圍的總面積相當之總熱通量減去Q2所獲得之面積, 使用該等總熱通量Q1,根據下式(2)對鑄模出口處之凝固 殼厚度D進行運算。 ⑩ q2reg = h · Δ0 .........(1) 其中,q2reg :穩定凝固界面熱輸入(J/s · m2) h :熔鋼與凝固殼之間之熱傳遞係數(J/s · m2 · °C) • Δθ :熔鋼之過熱度(°C) - D = Ql/(AH.p) .........(2) 其中,D :鑄模出口處之凝固殼厚度(m) Q1 :總熱通量(J/m2) △Η :鑄模出口處之凝固殼之每單位重量之焓降(J/kg) 098106495 49 200946265 p :鑄模出口之凝固殼密度(kg/m3)。 (32)如上述(31)之凝固殼厚度推定裝置,其中,凝固殼厚 度運算手段將經考慮凝固延遲之凝固殼厚度作為D1,該凝 固延遲係因由總熱通量Q2所引起之再熔解而產生者,使D1 = D(1-RS)。 其中,RS= θχ(ν°·8·Δ(9 ) .........(3) /3 :凝固延遲常數(無單位) V :溶鋼流速(m/s) ΔΘ :熔鋼過熱度(°C) RS :凝固延遲度(無單位) 此處,V=(Q2/(a · t · Δ0 ))125 Q2 :總熱通量(J/m2) α :炼鋼流速常數(無單位) t:凝固殼經由熱通量分布中之極小點後到達鑄模出口為 止所需之時間(S) 再者,較佳為凝固殼厚度推定裝置於(ql — q2reg)之熱通量 分布中不存在極小點時,利用上述(31)之方法來推測凝固殼 厚度(D),於存在極小點時利用如上述(32)之方法來推測凝 固殼厚度(D1),藉此分別推定凝固殼厚度。 【實施方式】 圖1、圖12及圖13係設置有本發明一實施形態之鑄漏檢 測及防止裝置、及凝固殼厚度推定裝置的連續鎊造設備之說 098106495 50 200946265 明圖。對與圖2相同之部分標註相同之符號。 連續鎮.造设備包括. •鑄模1, •浸潰喷嘴3,連接於銀槽40之底部並設置於鱗模1内’ 將來自餵槽40之熔鋼5喷出; •導輥21 ’對出自鑄模1之缚片19進行引導; •夾送輥(pinch rol 1)23,用以抽出鎮片19 ; ❿ •馬達25,用以對夾送輥23進行旋轉驅動;及 •夾送輥控制裝置27,用以控制馬達25。 於此種構成之連續铸造設備中,設置有包括以下之構成之 鑄漏防止裝置(包括鎊漏檢測裝置及凝固殼厚度推定裝置)。 鑄漏防止裝置包括: •熱電偶群,係將複數成一對之熱電偶17設置於鑄模寬 度方向及鑄造方向上而成者,該一對熱電偶17係埋入至形 ❿成有鑄模1的鑄模銅板11 t之不同深度之兩點者; •局部熱通量運算手段29,於龍厚度方向 該熱電偶群Π之溫度資訊而對各熱電偶設 來自 Λ 通量進行運算; 之局部熱 •穩定凝固界面熱輸入記憶手段31, 。U很據下故n 求得穩定狀態下之鑄模内熔鋼流動所引 所 熱輸入q2reg的資料; 穩定凝固界面 •熱通量分布運算手段32,針對熱_ ^置ql與穩定凝 098106495 200946265 固界面熱輸人q2reg之差(ql-q2reg),求得炫鋼自爐浴面到達 鑄模出口為止之熱通量分布; 铸漏判疋手段33,根據所求得之熱通量分布來判定有 無產生鑄漏之危險; •控制手段35,輸入鑄漏判定手段33之信號,當鎮漏判 定手段33判定為有鑄漏之危險時, (i )以減慢鑄造速度之方式進行控制(圖13), U)以減慢鑄造速度之方式進行控制及/或以使鱗模(内 之熔鋼流速下降之方式進行控制(圖12),或者, (iii)以降低鑄造速度及/或增強鑄模冷卻之方式對操作條 件進行控制,或除該控制以外,進行使鑄模内之熔鋼流速下 降之控制(圖1);及 •警報裝置37,當鑄漏判定手段33判定為有矯漏之危險 時發出警報。 q2reg = h · Δ Θ .........(1) 其中,h:熔鋼與凝固殼之間之熱傳遞係數 ΔΘ:溶鋼之過熱度 於圖1之鑄漏防止裝置中,鑄漏判定手段33進而包括: •凝固殼厚度運算手段34,根據由分布運算手段犯所求 得之熱通量分布而計算出總熱通量Q1及Q2,並使用該等總 熱通量Q1,或者使用Q1及Q2,對鑄模出口處之凝固殼9 之厚度(凝固殼厚度)進行運算;及 098106495 52 200946265 •鑄漏判定手段本體33A,輸入凝固殼厚度運算手段34 之運算值’並根據該運算值及以與產生鑄漏之危險性之關係 所求得之臨限值來判定有無產生鑄漏之危險。 以下’更詳細地對各構成進行說明。 <熱電偶> 熱電偶17與圖3、圖4中所示相同,埋入至鑄模銅板u 中。即,於形成於鎢模銅板11外侧面之冷卻水通道13底部48 200946265 The difference between the heat input q2reg of the solidification interface (ql-q2reg), the heat flux distribution of the molten steel from the furnace surface to the exit of the mold; and the calculation method of the solidified shell thickness, (i) by the distribution operation If there is no minimum point indicating the minimum value in the heat flux distribution obtained by the means, it will be equivalent to the total area surrounded by the entire curve of the heat flux distribution from the position of the bath surface to the exit of the mold. The total heat flux is set to the total heat flux Q1, and (ϋ) when there is a minimum point indicating a minimum value in the heat flux distribution obtained by the distribution operation means, when the minimum point is connected by a straight line When the local heat flux value at the exit of the mold is set, the total heat flux corresponding to the area of the upper portion of the straight line is set to Q2, and the total heat flux corresponding to the following area is set to Q1, which is self-contained. The total heat flux corresponding to the total area enclosed by the entire curve of the heat flux distribution from the position of the bath surface to the exit of the mold minus the area obtained by Q2, using the total heat flux Q1, according to the following formula (2) The solidified shell thickness at the exit of the mold D is operated. 10 q2reg = h · Δ0 (1) where q2reg : stable solidification interface heat input (J/s · m2) h : heat transfer coefficient between molten steel and solidified shell (J/ s · m2 · °C) • Δθ: superheat of molten steel (°C) - D = Ql/(AH.p) ... (2) where D: solidification at the exit of the mold Shell thickness (m) Q1 : Total heat flux (J/m2) △Η : 焓 drop per unit weight of solidified shell at the exit of the mold (J/kg) 098106495 49 200946265 p : solidified shell density at the exit of the mold (kg /m3). (32) The solidified shell thickness estimating device according to (31) above, wherein the solidified shell thickness calculating means takes the solidified shell thickness considering the solidification delay as D1, and the solidification delay is caused by remelting caused by the total heat flux Q2. Producer, let D1 = D(1-RS). Where RS = θχ(ν°·8·Δ(9 ) ... (3) /3 : solidification delay constant (no unit) V : molten steel flow rate (m/s) ΔΘ : molten steel Superheat (°C) RS : Solidification delay (no unit) Here, V=(Q2/(a · t · Δ0 )) 125 Q2 : Total heat flux (J/m2) α : Steelmaking flow rate constant ( t unit) t: time required for the solidified shell to reach the exit of the mold through the minimum point in the heat flux distribution (S) Further, it is preferable that the heat flux distribution of the solidified shell thickness estimating device is (ql - q2reg) When there is no minimum point, the method (31) above is used to estimate the solidified shell thickness (D), and when there is a minimum point, the solidified shell thickness (D1) is estimated by the method of (32) above, thereby presuming solidification, respectively. [Embodiment] FIG. 1, FIG. 12 and FIG. 13 are views showing a continuous leak-making apparatus for a casting leak detection and prevention apparatus and a solidified shell thickness estimating apparatus according to an embodiment of the present invention, 098106495 50 200946265. The same parts as those in Fig. 2 are denoted by the same symbols. Continuous town. Equipment includes: • Mold 1, • Dip nozzle 3, connected to the bottom of silver tank 40 Placed in the scale die 1 'spray the molten steel 5 from the feed tank 40; • The guide roller 21' guides the tab 19 from the mold 1; • Pinch rol 1 23 for extracting the town a sheet 19; a motor 25 for rotationally driving the pinch roller 23; and a pinch roller control device 27 for controlling the motor 25. In the continuous casting apparatus of such a configuration, the following composition is provided The casting leakage preventing device (including the pound leak detecting device and the solidified shell thickness estimating device). The casting leakage preventing device includes: • a thermocouple group, wherein a plurality of thermocouples 17 are placed in the width direction of the mold and the casting direction. The pair of thermocouples 17 are embedded in two points of different depths of the mold copper plate 11 t shaped into the mold 1; • a local heat flux calculation means 29, the thermocouple group in the thickness direction of the dragon The temperature information is calculated for each thermocouple from the Λ flux; the local heat·stable solidification interface heat input memory means 31, U is based on the next n to obtain the steady state of the molten steel flow in the mold Enter the data of q2reg; stable solidification The surface/heat flux distribution calculation means 32, for the difference between the heat _ ^ ql and the stable condensation 098106495 200946265 solid interface heat input q2reg (ql-q2reg), obtain the heat flux from the furnace surface to the mold exit The amount distribution; the casting leakage determining means 33 determines whether or not there is a risk of casting leakage based on the obtained heat flux distribution; • the control means 35 inputs the signal of the casting leakage determining means 33, and the sleep leakage determining means 33 determines that When there is a risk of casting leakage, (i) control by slowing down the casting speed (Fig. 13), U) control by slowing down the casting speed and/or to make the scale mold (the flow rate of the molten steel inside is lowered) Controlling the mode (Fig. 12), or (iii) controlling the operating conditions by reducing the casting speed and/or enhancing the cooling of the mold, or in addition to the control, controlling the flow rate of the molten steel in the mold (Fig. 1); and • The alarm device 37 issues an alarm when the casting leakage determining means 33 determines that there is a risk of leakage. Q2reg = h · Δ Θ ... (1) where h: the heat transfer coefficient between the molten steel and the solidified shell ΔΘ: the superheat of the molten steel is in the casting leakage prevention device of Fig. 1, casting The leak determining means 33 further includes: • a solidified shell thickness calculating means 34 for calculating total heat fluxes Q1 and Q2 based on the heat flux distribution obtained by the distributed computing means, and using the total heat flux Q1, Or using Q1 and Q2, calculating the thickness (solidified shell thickness) of the solidified shell 9 at the exit of the mold; and 098106495 52 200946265 • casting leakage determining means body 33A, inputting the calculated value of the solidified shell thickness calculating means 34 and according to The calculated value and the threshold value obtained by the relationship with the risk of casting leakage are used to determine whether or not there is a risk of casting leakage. Hereinafter, each configuration will be described in more detail. <Thermocouple> The thermocouple 17 is buried in the mold copper plate u as shown in Figs. 3 and 4 . That is, at the bottom of the cooling water passage 13 formed on the outer side surface of the tungsten mold copper plate 11.
形成孔15(參照圖3),其中埋入熱電偶17,於鑄模之鑄造 方向上9個部位(共計18根)設置一對熱電偶17,該一對熱 電偶17係埋藏在於深度方向上相隔固定距離之兩個部位。 再者,於本實施形態中,熱電偶17埋入至鑄模之短邊侧 及長邊(於水平剖面成長方體之鑄模中的較長邊)側,對鱗模 之每個邊進行測量,根據每個邊之㈣值來判定有無產生轉 漏。 <局部熱通量運算手段> 2部熱通量運算手段29輸入熱電偶Π之㈣而對局部 通量Qlit行運算。局部熱通料算手段29鋪由中央處 单兀_ ’ Central Pr〇cessingUnit)執行既定之程式而 現,於該程式中,如上所述 將兩根熱電偶17之檢出溫 設為ΤΙ、T2 ’將埋設間隔設為d α,及將鑄模1之熱導率設 λ,寫入計算出局部熱通量之下式(4)。 ql= λ (Tl-T2)/d .........(4) 098106495 200946265 <穩定凝固界面熱輸入記憶手段> 穩定凝固界面熱輸入5己憶手段31記憶如下資料,, 係根據下式(1)所求得之穩定狀態下之__誠 起的穩定凝固界面熱輸入q2reg之資料。 q2reg= h · Δ θ .........(1) 其中,h=l. 22xl05xV°_8 V :溶鋼流速(m/s) ΑΘ =T〇-TsA hole 15 (see FIG. 3) is formed in which a thermocouple 17 is buried, and a pair of thermocouples 17 are provided in nine places (total of 18) in the casting direction of the mold, and the pair of thermocouples 17 are buried in the depth direction. Two parts of a fixed distance. Furthermore, in the present embodiment, the thermocouple 17 is embedded in the short side and the long side of the mold (on the longer side in the mold of the horizontal cross-section growth body), and each side of the scale mold is measured, according to The value of each side (four) is used to determine whether there is a slip. <Local heat flux calculation means> The two-part heat flux calculation means 29 inputs (4) the thermocouple 而 and operates on the local flux Qlit row. The local heat flux calculation means 29 is executed by the central unit _ 'Central Pr〇cessing Unit), and in this program, the temperature of the two thermocouples 17 is set to ΤΙ, T2 as described above. 'Set the embedding interval to d α and set the thermal conductivity of the mold 1 to λ, and write the local heat flux below the formula (4). Ql= λ (Tl-T2)/d .........(4) 098106495 200946265 <Stabilization of solidification interface heat input memory means> Stable solidification interface heat input 5 Memories means 31 memory as follows, According to the following equation (1), the steady-state solidification interface heat input q2reg of the steady state is obtained. Q2reg= h · Δ θ (1) where h=l. 22xl05xV°_8 V : molten steel flow rate (m/s) ΑΘ =T〇-Ts
To :鑄模内熔鋼溫度(°C) Ts :熔鋼固相線溫度(°C) 再者’求得穩定_界面熱輪人I之方 方法··當以既定之鑄造速度進行操作時,根據所鱗造^ 之枝晶傾角而求得_流速,簡軸 述式(1)求得穩定凝固界面熱輸入q2“。 、’’、、土 ,據- <熱通量分布運算手段> 熱通量分布運算手段32自各裝 運算手™· …之穩定凝固界面熱輪入二: 熱等通量差f求糊自⑽物咖仏 熱通量分布運算手段32與 CPU M ^ π I熟通量運算手段 係精由CPU執仃既定之程 見現者’於該程式中寫入有 098106495 200946265 上述熱通量分布進行運算之邏輯。 <凝固殼厚度運算手段> 於圖1之鑄漏防止裝置中所設置的凝固殼厚度運算手段 34係根據由熱通量分布運算手段32所求得之熱通量分布, ' 對鑄模出口處之凝固殼厚度D進行運算。具體之運算方法如 下所述。 於由熱通量分布運算手段32所求得的熱通量分布中不存 φ 在表示極小值之極小點之情形時,將與由自爐浴面位置至鑄 模出口間之該熱通量分布之整個曲線所包圍的總面積相當 之總熱通量設為Q1,使用該總熱通量Q1根據下式(2)而對 鑄模出口處之凝固殼厚度D進行運算。 又,於由熱通量分布運算手段32所求得的熱通量分布中 存在表示極小值之極小點之情形時,當利用直線連結該極小 點與鑄模出口處之局部熱通量值時,將與該直線更上方之部 φ 分面積相當的總熱通量設為Q2,將與如下面積相當之總熱 通量設為Q1,該面積係自與由自爐浴面位置至鑄模出口間 之該熱通量分布之整個曲線所包圍之總面積相當的總熱通 • 量減去Q 2所獲得之面積,使用該總熱通量Q1且根據下式(2 ) 對鑄模出口處之凝固殼厚度D進行運算(參照圖9)。 D-Q1/(AH· p) .........(2) 其中,D :鑄模出口處之凝固殼厚度(m) AH :鑄模出口處之凝固殼之每單位重量之焓降(J/kg) 098106495 55 200946265 p :鑄模出口之凝固殼密度(kg/m3) 再者,作為更進一步提高精度之計算方法,凝固殼厚度運 算手段34亦可使用由下述式(3)所獲得之凝固延遲度RS, 藉由式D1==D(1 —RS)而計算出考慮了凝固延遲之凝固殼厚 度D1,該凝固延遲係因由總熱通量Q2所引起之再熔解而產 生者。當上述熱通量分布中不存在極小點時,無論是求得D 來代替D1之演算法,還是使Q2 = 0來求得D1之演算法,所 獲得之結果均相同,因此可選擇任一者。 RS= βχ(Υ〇κΑΘ) .........(3) /3 :凝固延遲常數(無單位) V :熔鋼流速(m/s) ΑΘ :熔鋼過熱度(°C) RS :凝固延遲度(無單位) 此處,V=(Q2/(a · t · A(9 ))125 Q2 :總熱通量(J/m2) α :炼鋼流速常數(無單位) t:凝固殼經由熱通量分布中之極小點後到達鑄模出口為 止所需之時間(S) <鑄漏判定手段> 於圖1之鑄漏防止裝置中,鑄漏判定手段33具有上述凝 固殼厚度運算手段34與鑄漏判定手段本體33A。於圖12及 圖13之鑄漏防止裝置中,鑄漏判定手段33不經由凝固殼厚 098106495 56 200946265 度運算’而是根據由熱通量分布運算手段32運算出之熱通 量分布,直接地判定有無產生鑄漏之危險。以下,分成各個 情形進行說明。 於圖1之鑄漏防止裝置之情形時,鑄漏判定手段本體33A 輸入凝固殼厚度運算手段34之運算值(凝固殼厚度d或 D1),根據該運算值及預先以與產生鎊漏之危險性之關係所 求得之臨限值而判定有無產生鑄漏之危險。 ❹ 臨限值係針對各種Ql、Q2與相對於該等之凝固殼厚度, 及於該凝固殼厚度下有無產生鑄漏,藉由預先取得模擬實驗 或實際操作中之資料而求得。例如將鑄模出口處之目標凝固 殼厚設為20〜30 mm之範圍内之數值(或者數值範圍),且將 凝固殼厚為5〜7 mm之範圍内之數值作為在其以下時則判定 有鑄漏之危險之臨限值。 Φ 於圖12或圖13之鑄漏防止裝置之情形時,鑄漏判定手段 33根據熱通量分布運算手段32所運算出之熱通量分布,例 如求得上述圖9所示之Q i與q 2之關係,並根據該等之關係 與預先所設定之臨限值而判定有無產生鑄漏之危險。 例如求得上述圖9所示之Q1、q2,根據與針對奶所預先 a2Ul<a2)及針對Q2所預先設定之 設定之臨限值α1 臨限值A之關係,以如圖10 漏之危險。 所示之基準來収有無產生鑄 098106495 57 200946265 Q2〈冷或(ΰ1)α1㈣且㈣万時,判定為有鑄漏 之危險。鑄漏判定手段33於判定為⑽漏之危險時,對控 制手&輸出„亥判定之要點。此時,最好一併輸出禱漏之 危險為基於Q1 < α 1到2以者、或者基於Q1 < α 1且Q2 <冷者、或者基於且Q2g石者。 再者限值α 1、α 2、/3取決於溶鋼之種類,例如於溶 鋼為極低碳鋼之情形時,α 1 = 15〇〇〇(kj/m2),“ 2 = 21000(kJ/m2),石=4500(kJ/m2)。再者,所謂極低碳鋼,係 指碳含量為0· 01 mass%以下者。 亦可使用基於Q1之基準、或者基於卯與Q2之關係之其 他判斷基準。例如於上例中,亦可MalSQ1$a2時或收 為根據Q1而更詳細$又疋之臨限值以上時,判斷是否有鎊漏 之危險。 作為其他方法’例如亦可於收與以之比值Q2/Q1之值為 預先所設定之臨限值以上時,判定有產生鑄漏之危險。該臨 限值取決於義之翻,例如於物為極低碳鋼之情形時為 0· 25 〇 鑄漏判定手段33或者鑄漏判定手段33A亦係藉由⑶以執 行既定之程式而實現者,於該程式中寫入有上述判定之邏 輯。 <控制手段> 控制手段35於鑄漏判定手段33判定有鑄漏之危險時,根 098106495 58 200946265 據該判定結果而對各種裝置進行控制以避免鱗漏。 例如於圖12之鑄漏防止裝置之情形時,具體而言,關於 上述dd及々,控制手段35若自鎢漏判定手段33輪 入存在因Ql< al 似;?所引起之鑄漏之危險之信號, 則對夾送據魏置27輸“示減慢馬達25之_速度之 信號。又,除此以夕卜,亦可對電磁制動裝置41輸出施加如 使鑄模1内之熔鋼流速下降之直流磁場之信號。又,控制手 ❹段35若自鑄漏判定手段33輸入存在因Q1< α i且Q2<冷 所引起之鏞漏之危險之信號,則對夾送輥控制裝置27輸出 指示減慢馬達25之旋轉速度之信號。進而,控制手段犯 若自鑄漏判定手段33輸入存在因石所 引起之鎊漏之危險之信號,則對電磁制動裝置41輸出施加 如使鑄模1内之熔鋼流速下降之直流磁場之信號。 又,於圖1之鑄漏防止裝置之情形時,具體而言,控制手 ®段35若自鱗漏判定手段34輸入存在鱗漏之危險之信號,則 對夾送輥控制裝置27輸出指示減慢馬達25之旋轉速度之信 號。又,除此以外,亦可對電磁制動裝置41輸出施加如使 . 鑄模1内之熔鋼流速下降之直流磁場之信號。 又,於圖13之鑄漏防止裝置之情形時,控制手段35若自 铸漏判疋手段33輸入存在铸漏之危險之信號,則僅以減慢 鑄造速度之方式進行控制,即,藉由對夾送輥控制裝置27 輸出指示減慢馬達25之旋轉速度之信號來因應。 098106495 59 200946265 除此以外,雖然任-圖中均未表示,但亦可進行如下控 制’即,朝_鑄歡冷卻水㈣鑄财卻控制手段發钟 號,強化鑄模冷卻而増加凝固殼厚。該控制可有效地因應^ Q1不足所引起之排熱不足性鑄漏。 " 控制手段35亦係藉由CPU執行既定之 該程式中寫入有輸出上述指令信號之邏輯。 者於 <警報裝置> 警報裝置37若輸入來自禱漏判定手段33之_ 警報。警報之種類並無限制,例如 ㈤务出 該等之組合等。 n'警㈣之點亮、 對以如上之方式構成之本實施形態之 於自浸潰噴嘴3中嘴出熔鋼5後 仃說月 連續鱗造鱗片19之操作中,將來自Γ電由偶71進行冷卻而 局部熱通娜手段29以對局部熱通電至 該運算結果輸入至分布運算手段32中。埶 、,、< 將 段32根據自局部熱通量運算手段扣所^入1運异手 Ql、及纪憶於穩定凝固界面熱輸入記憶手 11 :、量 固界面熱輸人q2w,對ql—必“進行料,/之穩定凝 運算〜果而對熱通量分布進行運算。然後,關於運算所獲得 098106495 200946265 之熱通量分布’求得例如圖9所示之Q1,,將該等運算 值Q1與Q2輪入至鑄漏判定手段犯中。To : The temperature of the molten steel in the mold (°C) Ts : The solidus temperature of the molten steel (°C) In addition, the method of obtaining the stability _ the interface of the hot wheel person I is operated at a predetermined casting speed. According to the dip angle of the scale of the scale, the flow rate is obtained, and the simple axis (1) is used to obtain the stable solidification interface heat input q2 "., '', and soil, according to - <heat flux distribution calculation means> The heat flux distribution calculation means 32 from the stable solidification interface of each of the operation hands TM·...the heat wheel is entered into two: the heat flux difference f is obtained from the paste (10) the material curry heat flux distribution operation means 32 and the CPU M ^ π I The familiar flux calculation method is executed by the CPU. The current process is described in the program. The logic of the above heat flux distribution is calculated in the program. <solidified shell thickness calculation means> The solidified shell thickness calculating means 34 provided in the casting leakage preventing means calculates the solidified shell thickness D at the exit of the mold based on the heat flux distribution obtained by the heat flux distribution calculating means 32. The specific arithmetic method As described below, the heat flux obtained by the heat flux distribution operation means 32 When there is no φ in the distribution, in the case of indicating the minimum point of the minimum value, the total heat flux corresponding to the total area surrounded by the entire curve of the heat flux distribution from the position of the bath surface to the exit of the mold is set to Q1, using the total heat flux Q1, the solidified shell thickness D at the exit of the mold is calculated according to the following formula (2). Further, there is a representation in the heat flux distribution obtained by the heat flux distribution calculating means 32. In the case of a minimum of the minimum value, when the local minimum heat flux value at the exit of the mold is connected by a straight line, the total heat flux corresponding to the area above the straight line of the straight line is set to Q2, The total heat flux corresponding to the area is set to Q1, which is the total heat flux minus the total area enclosed by the entire curve of the heat flux distribution from the bath surface position to the mold exit. To the area obtained by Q 2 , the total heat flux Q1 is used and the solidified shell thickness D at the exit of the mold is calculated according to the following formula (2) (refer to Fig. 9). D-Q1/(AH· p) .. (2) where D: solidified shell thickness at the exit of the mold (m) AH: mold exit The enthalpy drop per unit weight of the solidified shell at the place (J/kg) 098106495 55 200946265 p : solidified shell density at the exit of the mold (kg/m3) Further, as a calculation method for further improving the accuracy, the solidified shell thickness calculation means 34 It is also possible to calculate the solidified shell thickness D1 in consideration of the solidification delay by the solidification delay degree RS obtained by the following formula (3) by the formula D1==D(1 - RS), which is caused by the total heat The remelting caused by the flux Q2 is generated. When there is no minimum point in the heat flux distribution, whether D is used instead of D1 or Q2 = 0, the algorithm of D1 is obtained. The results obtained are all the same, so either one can be selected. RS=βχ(Υ〇κΑΘ) .........(3) /3 : Solidification delay constant (no unit) V : Melt flow rate (m/s) ΑΘ : Fused steel superheat (°C) RS: solidification delay (no unit) Here, V = (Q2 / (a · t · A (9 )) 125 Q2 : total heat flux (J / m2) α : steelmaking flow rate constant (no unit) t : time required for the solidified shell to reach the exit of the mold through the minimum point in the heat flux distribution (S) < casting leakage determining means> In the casting leakage preventing apparatus of Fig. 1, the casting leakage determining means 33 has the above solidification The shell thickness calculating means 34 and the casting leakage determining means main body 33A. In the casting leakage preventing means of Figs. 12 and 13, the casting leakage determining means 33 does not operate via the solidified shell thickness 098106495 56 200946265 degrees, but is based on the heat flux distribution. The heat flux distribution calculated by the calculation means 32 directly determines whether or not there is a risk of casting leakage. Hereinafter, the case will be described in each case. In the case of the casting leakage preventing device of Fig. 1, the casting leakage determining means body 33A is input to the solidified shell. The calculated value of the thickness calculation means 34 (solidified shell thickness d or D1), based on the calculated value and the risk of generating a pound leak in advance The relationship between the thresholds is determined to determine whether there is a risk of casting leakage. 临 The threshold value is for each of Ql, Q2 and the thickness of the solidified shell relative to the solid shell, and whether there is a casting leak under the thickness of the solidified shell. It is obtained by obtaining the data in the simulation experiment or the actual operation in advance. For example, the target solidified shell thickness at the exit of the mold is set to a value (or a numerical range) in the range of 20 to 30 mm, and the solidified shell thickness is 5 The value in the range of ~7 mm is used as the threshold value for determining the risk of casting leakage. Φ In the case of the casting leakage preventing device of Fig. 12 or Fig. 13, the casting leakage determining means 33 is based on the heat flux. The heat flux distribution calculated by the distribution calculation means 32 obtains, for example, the relationship between Q i and q 2 shown in FIG. 9 , and determines whether or not a casting leak occurs based on the relationship and the threshold value set in advance. For example, the relationship between Q1 and q2 shown in Fig. 9 is obtained based on the relationship with the pre-set a1U1 <a2) for milk and the threshold α1 threshold A set in advance for Q2, as shown in Fig. 10. Danger of leakage. The basis shown indicates whether or not there is a casting 098106495 57 200946265 Q2 <cold or (ΰ1) α1 (four) and (four) million, it is judged that there is a danger of casting leakage. When the casting leakage determining means 33 determines that the risk of the leak is (10), the control hand & outputs the key point of the determination. In this case, it is preferable to output the risk of the prayer leak based on Q1 < α 1 to 2, Or based on Q1 < α 1 and Q2 < cold, or based on Q2g stone. Further, the limits α 1 , α 2, / 3 depend on the type of molten steel, for example, when the molten steel is extremely low carbon steel. , α 1 = 15 〇〇〇 (kj/m 2 ), “ 2 = 21000 (kJ/m 2 ), stone = 4500 (kJ/m 2 ). Further, the term "very low carbon steel" means a carbon content of 0.001 mass% or less. Other benchmarks based on the Q1 benchmark or based on the relationship between 卯 and Q2 can also be used. For example, in the above example, it is also possible to determine whether there is a risk of a pound leak when MalSQ1$a2 or when it is received in more detail than the threshold of Q1 according to Q1. As another method, for example, when the ratio of the ratio Q2/Q1 is equal to or greater than the threshold value set in advance, it is determined that there is a risk of casting leakage. The threshold value depends on the flipping of the sense, for example, when the object is extremely low carbon steel, the 0. 25 〇 casting leak determining means 33 or the casting leak determining means 33A is also realized by executing the established program by (3). The logic of the above determination is written in the program. <Control means> When the casting leakage determining means 33 determines that there is a risk of casting leakage, the root device 098106495 58 200946265 controls various devices to prevent scale leakage based on the determination result. For example, in the case of the casting leakage preventing device of Fig. 12, specifically, regarding the above-mentioned dd and 々, the control means 35 is rotated from the tungsten leak determining means 33 by Q1 <al; The signal of the danger of casting leakage caused by the pinch is sent to the signal indicating the speed of the slowing motor 25. In addition, in addition, the output of the electromagnetic brake device 41 can also be applied. a signal of a DC magnetic field in which the flow rate of the molten steel in the mold 1 is decreased. Further, if the control handcuffs section 35 inputs a signal indicating a risk of leakage due to Q1 < α i and Q2 < cold, The pinch roller control device 27 outputs a signal indicating that the rotation speed of the motor 25 is slowed down. Further, the control means commits a signal to the electromagnetic brake device if a signal indicating the risk of a pound leak due to the stone is input from the casting leakage determining means 33. 41 outputs a signal of a DC magnetic field to which the flow rate of the molten steel in the mold 1 is lowered. Further, in the case of the casting leakage preventing device of Fig. 1, specifically, the control hand segment 35 is input from the scale leakage determining means 34. If there is a danger of the risk of scale leakage, the pinch roller control device 27 outputs a signal indicating that the rotation speed of the motor 25 is slowed down. In addition, the output of the electromagnetic brake device 41 may be applied as in the mold 1. Melt flow rate decreases In the case of the casting leakage preventing device of Fig. 13, when the control means 35 inputs a signal indicating the risk of casting leakage from the casting leakage determining means 33, it is controlled only by slowing down the casting speed. That is, the pinch roller control device 27 outputs a signal indicating that the rotation speed of the motor 25 is slowed down. 098106495 59 200946265 Other than that, although not shown in the drawings, the following control can be performed. , _ cast Huan cooling water (four) casting money but control means to send the bell, strengthen the mold cooling and add solidified shell thickness. This control can effectively respond to the lack of heat caused by the lack of Q1 casting. " Control 35 The logic for outputting the command signal is also written in the program by the CPU. The <alarm device> alarm device 37 inputs an _alarm from the prayer leak determining means 33. The type of the alarm is not limited. For example, (5) to deal with such a combination, etc. n's (4) lighting, for the embodiment of the present embodiment, the self-impregnated nozzle 3 in the mouth of the molten steel 5 Exercise of 19 In the process, the local heat is supplied from the capacitor 71 and the local heat flux means 29 is applied to the local heat to the result of the calculation, and is input to the distribution operation means 32. 埶, ,, < The amount of calculation means deducting the key into the 1st hand Ql, and Ji Yi in the stable solidification interface heat input memory hand 11:, the solid-solid interface heat input q2w, the ql- must be "material, / the stable coagulation operation ~ fruit The heat flux distribution is calculated. Then, regarding the heat flux distribution obtained by the calculation 098106495 200946265, Q1 shown in Fig. 9, for example, is obtained, and the arithmetic values Q1 and Q2 are rounded up to the casting leakage determination means.
Affi 12 _ 13之鏵漏防止裝置之情形時,鑄漏判定手段 33對於所輪入之Q1或者進而所輸入之Q2,根據預先設定之 規則來判疋有無產生鎊漏之危險。例如以圖12之Q1及Q2 之各值與預先所設定之上述臨限值αΐ、α2、/5之關係來判 疋有無產生轉漏之危險。 ❹ 於圖1之鑄漏防止裝置之情形時,凝固殼厚度運算手段 34首先根據由熱通量分布運算手段32所求得之熱通量分 布,藉由上述方法而求得總熱通量Q1或者進而求得Q2。然 後’凝固设厚度運算手段34㈣根據該總熱通量Q1或者進 而根據Q2,藉由上述方法而對鑄模出口處之凝固殼厚度d 或者Μ進行運算。進而鑄漏判定手段本體,輸入由凝固 殼厚度運算手段34運算出之凝固殼厚度D或者D卜並以該 ❿值與預先設定之臨限值之關係而判定有無產生禱漏之危險。 當判定之結果為無產生鑄漏之危險時,按原樣繼續進行操 作。 • 另一方面,當判定之結果為判定有產生鑄漏之危險時,鑄 漏判定手段33將表示有鑄狀危險之信號輸出至控制手段 35。又,與此同時,將發出警報之指令信號輸出至警報裝置 37 ° 於圖12或圖13之鑄漏防止裝置之情形時,鑄漏判定手段 098106495 61 200946265 33亦可進而對控制手段35輸出鑄漏之危險之種類。例如關 於上述α 1、α 2、0,輸出通知信號,該通知信號係意指處 於排熱不足性鑄漏之危險區域中(Ql< α 1且Q2<召),還是 處於再’熔解性鑄漏之危險區域中且Q2之 召)’或者是處於該兩者之危險區域中(Q1< α 1且冷)。 控制手段35若輸入來自鑄漏判定手段33之信號,則進行 例如用以使鑄造速度下降,同時,使熔鋼流速下降之控制。 作為用以使鑄造速度下降之控制,具體而言,控制手段 35對夾送輥控制裝置27輸出指示減慢馬達25之旋轉速度 之信號。輸入有該信號之夾送輥控制裝置27以降低馬達25 之轉速之方式進行控制。藉由降低馬達25之轉速而使鑄造 速度下降,鑄模1内之凝固殼厚變厚,因此可避免產生鑄漏 之危險。 作為用以使熔鋼流速下降之控制,具體而言控制手段 35對電磁制動裝置41輸出施加如使鑄模1内之溶鋼流速下 降之直机磁場之彳s號。若輪出該信號’則藉由電磁制動裝置 41而對鑄模1施加直流礎場,*使_模丨内之熔鋼流速下 降。流速下降,·_擊凝赌界面之速度下降, 凝固殼之再熔解之程度變小,因此顧殼厚度仍然變厚可 避免產生鑄漏之危險。 於圖12之鑄漏防止敦置之情形時,亦可對應於上述使用 αΐ α2 /3之判定,進行如下#述之更詳細之處理。 098106495 200946265 控制手段35若輸入來自鑄漏判定手段33之信號,則於該 信號為基於Ql< α 1且Q22 β者之情形時,由於該情形係 有產生排熱不足性鑄漏與再熔解性鑄漏此兩者之危險之情 形’因此進行用以使鑄造速度下降並使溶鋼流速下降之控 制。 作為用以使鑄造速度下降之控制,具體而言,控制手段 35對炎送輥控制裝置27輸出指示減慢馬達25之旋轉速度 Ο 之信號。輸入有該信號之夾送輥控制裝置27以降低馬達25 之轉速之方式進行控制。藉由降低馬達25之轉速而使鑄造 速度下降,鑄模1内之凝固殼厚變厚,因此可避免產生排熱 不足性鎊漏之危險。 作為用以使熔鋼流速下降之控制,具體而言,控制手段 35對電磁制動裝置41輸出施加如使鑄模丨内之熔鋼流速下 降之直流磁場之信號,若輸出該信號,則藉由電磁制動裝置 參41而對鑄模1施加直流磁場,使鎊模1内之熔鋼流速下降。 若熔鋼流速下降,則熔鋼衝擊凝固殼界面之速度下降,凝固 殼之再熔解之減變小’因此可避免產生因殼之再溶解 • 所引起之鑄漏之危險。 又於來自鑄漏判定手段33之信號為基於qi〈 α 1且收 〈石者之情形時’由於該情形係有產生排熱不足性鑄漏之危 險之情形’因此控制手段35對夾送輕控制裝置27輸出指示 減慢馬達25之旋轉速度之信號。藉此,鑄造速度下降,鑄 098106495 63 200946265 模1内之凝固殼厚變厚,因此可避免產生排熱不足性鑄漏之 危險。 又’於來自鑄漏判定手段33之信號為基於 且者之情形時,由於該情形係有產生再熔解性鑄漏 之危險之情形’因此控制手段35對電磁制動裝置41輸出施 加如使鎊模1内之熔鋼流速下降之直流磁場之信號,藉此可 如上述般避免產生再熔解性鑄漏。 另外’警報裝置若輸入來自鑄漏判定手段33之信號,則 發出警報。藉此,可對操作員發出產生鑄漏之危險之通知。 再者’當然於圖1、12及13中,由以下部分構成鑄漏檢 出裝置’即由熱電偶17所構成之熱電偶群、局部熱通量運 算手段29、穩定凝固界面熱輸入記憶手段31、熱通量分布 運算手段32及鑄漏判定手段33(或者進而警報裝置37)。 又’於圖1中,由以下部分構成凝固殼厚度推定裝置,即由 熱電偶17所構成之熱電偶群、局部熱通量運算手段29、穩 定凝固界面熱輸入記憶手段31、熱通量分布運算手段32及 凝固殼厚度運算手段34。 例如使用圖12中所揭示之連續鎮造設備,以2· 0 m/分之 鑄造速度對極低碳鋼進行操作之後,Q2<4500 kJ/m2,但Q1 之值為Q1 < 15000 kJ/m2,而出現了排熱不足性鑄漏產生之 危險。因此,使躊造速度下降至〇. 5 m/分為止之後,Q12 15000 kJ/m2,可獲得充分之凝固殼摩度,而可防止鑄漏之 098106495 64 200946265 產生。再者,於使凝固殼厚達足夠厚之後,再次提高鑄造速 度,藉此可進行高速鑄造。 又,使用圖12中所揭示之連續鎊造設備,以2. 5 m/分之 鑄造速度對極低碳鋼進行操作之後,Q1之值為15000 kJ/m2 SQ1S21000 kJ/m2,Q2 之值為 Q224500 kJ/m2,而出現再 熔解性鑄漏產生之危險。因此,可使電磁制動裂置41作動 而使Q2之值下降至小於4500 kJ/m2之值,而可防止產生再 ❹ 熔解性鑄漏。 進而’使用圖13中所揭示之連續鑄造設備,於實際效果 不脫離 15000 kJ/m2SQl$ 21000 kJ/m2之條件下,以 2 0 m/ 分之鎢造速度對極低碳鋼進行操作之後,Q2/Q1之值超過 〇. 25。因此’使鑄造速度下降至〇. 5 m/分為止之後,Q2/Q1 <0. 25 ’可獲得充分之凝固殼厚度,而可防止鱗漏之產生。 再者,於使凝固殼厚達足夠厚之後,再次提高鑄造速度,藉 ❿ 此可進行高速鑄造。 藉由本實施形態,可根據與鑄模出口處之凝固殼厚有直接 相關之熱通量分布來判定有無產生鑄漏之危險,或者可根據 該分布而求得與鑄漏有直接相關之鑄模出口處之凝固私厚 度’並根據該凝固殼厚度來判定有無產生鑄漏,因此,於各 種操作條件下,可高靈敏度地、簡單且確實地預知鳞漏之產 生,而可確實地防止鑄漏。又,關於產生鑄漏之危險,亦可 一併判定該鑄漏是再熔解性鑄漏還是排熱不足性鱗 L-l 匕 098106495 65 200946265 可選擇最佳之防止手段。 再者,於以上所說明之本發明之内容或實施形態中,作為 根據熱通量分布而求得與總熱通量或與凸料分之大小相 當的熱通量之累計值之方法,主要揭示了以幾何學之方式進 行之方法。然而’本發明並不受限於此,例如亦可藉由對圖 表進行積分而求得總熱通量。 (產業上之可利用性) 於本發明中’測定連續鑄造中之鑄模内熔鋼自爐浴面到達 鑄模出口為止之期間朝凝固界面熱輸入之熱通量ql,龙針 對熱通量ql與穩定狀態下之鑄模内熔鋼流動所引起的穩定 凝固界面熱輸入q2reg之差(ql 一 q2reg),求得熔鋼自爐浴面到 達鑄模出口為止之熱通量分布,根據該熱通量分布來判定有 無產生鱗漏之危險,因此於各種操作條件下,可高靈敏度 地、簡單且確實地預知鑄漏之產生,而可確實地防止鑄漏。 又,根據上述熱通量分布而求得總熱通量卯及Q2並進行解 析,藉此可進而判定每個鑄漏之原因,因此可根據原因進行 適當之用以避免鑄漏之因應。 進而,由於使用上述總熱通量Q1、或者進而使用Q2來推 定鑄模出口處之凝固殼厚度,因此可高精度地推定凝固殼厚 度。 如上所述’本發明於連續鑄造之控制領域中發揮各種優異 之效果。 098106495 66 200946265 【圖式簡單說明】 圖1係設置有本發明一實施形態之鑄漏防止裝置的連續 鑄造設備之說明圖。 ,其係表示埋入 ,其係表示熱電 ,其係表示熱電 ,其係表示局部 圖2係說明用以解決問題之手段之說明圖 有熱電偶之連續鑄造用鑄模一例的剖視圖。 圖3係說明用以解決問題之手段之說明圖 偶之埋入方法一例的說明圖。In the case of the leak prevention device of Affi 12 _ 13, the casting leakage determining means 33 judges whether or not there is a risk of a pound leak based on a predetermined rule for the Q1 to be wheeled or the Q2 to be input. For example, the relationship between the values of Q1 and Q2 in Fig. 12 and the aforementioned threshold values αΐ, α2, and /5 are used to determine whether or not there is a risk of slipping. In the case of the casting leakage preventing device of Fig. 1, the solidified shell thickness calculating means 34 first obtains the total heat flux Q1 by the above method based on the heat flux distribution obtained by the heat flux distribution calculating means 32. Or find Q2 in turn. Then, the solidification thickness calculation means 34 (4) calculates the solidified shell thickness d or 处 at the exit of the mold according to the total heat flux Q1 or according to Q2 by the above method. Further, the main body of the casting leakage determining means inputs the solidified shell thickness D or D calculated by the solidified shell thickness calculating means 34, and determines whether or not there is a risk of praying by the relationship between the threshold value and a predetermined threshold value. When the result of the judgment is that there is no danger of casting leakage, continue the operation as it is. • On the other hand, when the result of the determination is that it is determined that there is a risk of casting leakage, the casting leakage determining means 33 outputs a signal indicating that there is a risk of casting to the control means 35. At the same time, when the command signal for issuing an alarm is output to the alarm device 37 ° in the case of the casting leakage preventing device of FIG. 12 or FIG. 13, the casting leakage determining means 098106495 61 200946265 33 can further output the casting to the control means 35. The type of danger that is leaking. For example, regarding the above α 1 , α 2 , 0, the notification signal is output, and the notification signal means that it is in a dangerous area where the exhaust heat is insufficient to cast (Ql < α 1 and Q2 < call), or is in a re-melting casting In the dangerous area of the leak and the call of Q2) or in the dangerous area of the two (Q1 < α 1 and cold). When the control means 35 inputs a signal from the casting leakage determining means 33, for example, control for lowering the casting speed and lowering the flow rate of the molten steel is performed. As the control for lowering the casting speed, specifically, the control means 35 outputs a signal for instructing the pinch roller control means 27 to slow down the rotational speed of the motor 25. The pinch roller control device 27 to which the signal is input is controlled to reduce the number of revolutions of the motor 25. By lowering the rotational speed of the motor 25 and lowering the casting speed, the solidified shell thickness in the mold 1 becomes thicker, so that the risk of casting leakage can be avoided. As a control for lowering the flow rate of the molten steel, specifically, the control means 35 applies a 直s number to the electromagnetic brake device 41 to output a linear magnetic field such as a flow rate of the molten steel in the mold 1. If the signal is rotated, a DC base field is applied to the mold 1 by the electromagnetic brake device 41, and the flow rate of the molten steel in the mold is lowered. When the flow rate is lowered, the speed of the smashing gambling interface is lowered, and the degree of remelting of the solidified shell becomes small, so that the thickness of the shell is still thickened to avoid the risk of casting leakage. In the case where the casting leakage is prevented in the case of Fig. 12, the more detailed processing as described below may be performed in accordance with the above-described determination using αΐ α2 /3. 098106495 200946265 When the control means 35 inputs the signal from the cast-drain determination means 33, when the signal is based on Ql < α 1 and Q22 β, the case is caused by the occurrence of exhaustion-deficient casting leakage and re-melting property. The situation of the danger of casting both of them is therefore controlled so that the casting speed is lowered and the flow rate of the molten steel is lowered. As a control for lowering the casting speed, specifically, the control means 35 outputs a signal indicating that the rotational speed Ο of the motor 25 is slowed down to the inflame-feeding roller control device 27. The pinch roller control device 27 to which the signal is input is controlled to reduce the number of revolutions of the motor 25. By lowering the rotation speed of the motor 25 and lowering the casting speed, the solidified shell thickness in the mold 1 becomes thicker, so that the risk of the exhaustion of the exhaust heat is prevented. As a control for lowering the flow rate of the molten steel, specifically, the control means 35 outputs a signal to the electromagnetic brake device 41 to apply a DC magnetic field such that the flow velocity of the molten steel in the mold is lowered, and if the signal is output, electromagnetic The brake device 41 applies a DC magnetic field to the mold 1 to lower the flow rate of the molten steel in the pound mold 1. If the flow rate of the molten steel is lowered, the speed at which the molten steel impacts the solidified shell interface is lowered, and the reduction of the remelting of the solidified shell is small, so that the risk of casting leakage due to re-dissolution of the shell can be avoided. Further, when the signal from the casting-drain determining means 33 is based on qi < α 1 and the case of receiving the stone, the situation is caused by the risk of causing the exhaustion of the exhausting heat. Therefore, the control means 35 is light on the pinch. The control device 27 outputs a signal indicating that the rotational speed of the motor 25 is slowed down. As a result, the casting speed is lowered, and the solidified shell thickness in the mold 1 is thickened, so that the risk of insufficient heat-extracting casting leakage can be avoided. Further, when the signal from the casting leakage determining means 33 is based on the case, since the situation is in danger of generating remelting casting leakage, the control means 35 applies the output of the electromagnetic braking device 41 such as the pound mode. The signal of the DC magnetic field in which the flow rate of the molten steel in 1 is lowered, whereby the remelting casting leakage can be avoided as described above. Further, when the alarm device inputs a signal from the casting leakage determining means 33, an alarm is issued. In this way, the operator can be notified of the danger of creating a casting leak. Furthermore, of course, in Figs. 1, 12 and 13, the casting leakage detecting device is composed of the following: a thermocouple group composed of the thermocouple 17, a local heat flux calculation means 29, and a stable solidification interface heat input memory means. 31. Heat flux distribution calculation means 32 and casting leak determination means 33 (or further alarm means 37). Further, in Fig. 1, the solidified shell thickness estimating device, that is, the thermocouple group composed of the thermocouple 17, the local heat flux calculating means 29, the stable solidification interface heat input memory means 31, and the heat flux distribution are constituted by the following portions. The calculation means 32 and the solidified shell thickness calculation means 34. For example, using the continuous ballasting apparatus disclosed in Fig. 12, after operating very low carbon steel at a casting speed of 2.0 m/min, Q2 < 4500 kJ/m2, but the value of Q1 is Q1 < 15000 kJ/ M2, and there is a danger of heat-exhaust leakage. Therefore, after the manufacturing speed is reduced to 〇. 5 m/min, Q12 15000 kJ/m2 can obtain sufficient solidified shell friction, and can prevent the casting of 098106495 64 200946265. Further, after the solidified shell thickness is sufficiently thick, the casting speed is increased again, whereby high-speed casting can be performed. Further, after operating the ultra-low carbon steel at a casting speed of 2.5 m/min using the continuous pounding apparatus disclosed in Fig. 12, the value of Q1 is 15000 kJ/m2 SQ1S21000 kJ/m2, and the value of Q2 is Q224500 kJ/m2, and there is a danger of remelting casting leakage. Therefore, the electromagnetic brake rupture 41 can be actuated to lower the value of Q2 to a value of less than 4500 kJ/m2, and the occurrence of re-melting melt-casting can be prevented. Further, using the continuous casting equipment disclosed in FIG. 13, after the actual effect is not deviated from 15000 kJ/m2SQl$21000 kJ/m2, the ultra-low carbon steel is operated at a tungsten production speed of 20 m/min. The value of Q2/Q1 exceeds 〇. 25. Therefore, after the casting speed is lowered to 〇5 m/min, a sufficient solidified shell thickness can be obtained for Q2/Q1 < 0. 25 ', and generation of scale leakage can be prevented. Further, after the solidified shell is thick enough, the casting speed is increased again, whereby high-speed casting can be performed. According to this embodiment, it is possible to determine the presence or absence of a risk of casting leakage based on the heat flux distribution directly related to the solidified shell thickness at the exit of the mold, or to obtain a mold exit directly related to the casting leakage based on the distribution. According to the thickness of the solidified shell, it is determined whether or not a casting leak occurs. Therefore, under various operating conditions, the occurrence of scale leakage can be predicted with high sensitivity, simplicity, and reliability, and the casting leakage can be surely prevented. Further, regarding the risk of casting leakage, it is also possible to determine whether the casting leakage is a remelting casting leak or a heat exhausting insufficient scale. L-l 098 098106495 65 200946265 The best prevention means can be selected. Furthermore, in the content or embodiment of the present invention described above, the method of obtaining the integrated value of the heat flux corresponding to the total heat flux or the size of the convex material according to the heat flux distribution is mainly The method of doing it in a geometric way is revealed. However, the present invention is not limited thereto, and for example, the total heat flux can also be obtained by integrating the map. (Industrial Applicability) In the present invention, 'the heat flux ql to the heat input to the solidification interface during the period from the furnace surface of the molten steel in the continuous casting to the exit of the mold is measured, and the heat is applied to the heat flux ql and The difference between the steady solidification interface heat input q2reg caused by the flow of molten steel in the mold under steady state (ql-q2reg), the heat flux distribution of the molten steel from the furnace bath surface to the exit of the mold is obtained, according to the heat flux distribution In order to determine whether or not there is a risk of occurrence of scale leakage, the occurrence of casting leakage can be predicted with high sensitivity, simplicity, and reliability under various operating conditions, and the casting leakage can be surely prevented. Further, the total heat flux 卯 and Q2 are obtained based on the heat flux distribution and analyzed, whereby the cause of each casting leak can be further determined, so that it can be appropriately used for the purpose of avoiding the occurrence of the casting leakage. Further, since the total heat flux Q1 is used or the thickness of the solidified shell at the exit of the mold is estimated using Q2, the solidified shell thickness can be estimated with high accuracy. As described above, the present invention exerts various excellent effects in the field of control of continuous casting. 098106495 66 200946265 [Brief Description of the Drawings] Fig. 1 is an explanatory view of a continuous casting apparatus provided with a casting leakage preventing device according to an embodiment of the present invention. In the case of embedding, it is a thermoelectric system, which is a thermoelectric system, and is a part of a mold for continuous casting in which a thermocouple is used. Fig. 3 is an explanatory view showing an example of a method of embedding the illustration of the means for solving the problem.
圖4係說明用以解決問題之手段之說明圖 偶之安裝位置一例的說明圖。 圖5係說明用以解決問題之手段之說明圖 熱通量(縱軸:J/s · m2)與離爐浴面之距離(橫轴:mm)之關 係之一例的圖表。 圖6係說明用以解決問題之手段之說明圖,其係表示熔鋼 流速(縱轴:m/s)與離爐浴面之距離(橫軸:mm)之關係之一 _ 例的圖表。 圖7係說明用以解決問題之手段之說明圖,其係表示局部 熱通量ql(黑圓圈)及(ql — q2reg)(白圓圈)(縱軸:J/s · m2) • 與離爐浴面之距離(橫軸:mm)之關係之一例的圖表。 圖8係說明用以解決問題之手段之說明圖,其係表示由表 示局部熱通量與離爐浴面之距離之關係之圖表所表示的熱 通量分布之面積求法之一例的說明圖。 圖9係說明用以解決問題之手段之說明圖,其係表示由表 098106495 67 200946265 示局部熱通量與離爐浴面之距離之關係之圖表所表示的熱 通量分布Q1及Q2之面積求法之一例的說明圖。 圖10係說明用以解決問題之手段一例之說明圖,其係表 示於將橫軸設為Ql(kJ/m2),將縱轴設為Q2(kJ/m2)之座標平 面内,對表1所示之數值進行繪圖,進而以與有無產生鑄漏 之關係將座標平面分割成5個區域的圖。 圖11係說明用以解決問題之手段之說明圖,其係表示鑄 造速度與鑄模出口處之殼厚度方向之平均溫度之關係之一 例的圖表,縱軸表示鑄模出口殼厚度方向平均溫度(°C),橫 軸表示鑄造速度(m/分)。 圖12係設置有本發明另一實施形態之鑄漏防止裝置的連 續鑄造設備之說明圖。 圖13係設置有本發明另一實施形態之鑄漏防止裝置的連 續鑄造設備之說明圖。 【主要元件符號說明】 1 鑄模 3 浸潰喷嘴 5 熔鋼 7 模製粉 9 凝固殼 11 鑄模銅板 13 冷卻水通道 098106495 68 200946265 15 (冷卻水通道底部之)孔 17 熱電偶 19 鑄片 21 導輥 23 夾送輥 25 馬達 27 夾送輥控制裝置 ❹ 29 局部熱通量運算手段 31 穩定凝固界面熱輸入記憶手段 32 熱通量分布運算手段 33 鑄漏判定手段 33A 鑄漏判定手段本體 34 凝固殼厚度運算手段 35 控制裝置 ⑩ 37 警報裝置 40 餵槽 41 電磁制動裝置 098106495 69Fig. 4 is an explanatory view showing an example of the mounting position of the illustration of the means for solving the problem. Fig. 5 is a diagram for explaining an example of a means for solving the problem. An example of the relationship between the heat flux (vertical axis: J/s · m2) and the distance from the bath surface (horizontal axis: mm). Fig. 6 is an explanatory view for explaining a means for solving the problem, which is a graph showing a relationship between a molten steel flow velocity (vertical axis: m/s) and a distance from the furnace surface (horizontal axis: mm). Figure 7 is an explanatory diagram for explaining the means for solving the problem, which shows local heat flux ql (black circles) and (ql - q2reg) (white circles) (vertical axis: J/s · m2) A graph showing an example of the relationship between the distance of the bath surface (horizontal axis: mm). Fig. 8 is an explanatory view for explaining a means for solving the problem, and is an explanatory view showing an example of the area of the heat flux distribution indicated by a graph showing the relationship between the local heat flux and the distance from the bath surface. Figure 9 is an explanatory view for explaining the means for solving the problem, which is an area showing the heat flux distributions Q1 and Q2 represented by a graph showing the relationship between the local heat flux and the distance from the bath surface by the table 098106495 67 200946265. An explanatory diagram of an example of the method. Fig. 10 is an explanatory view showing an example of means for solving the problem, which is shown in a coordinate plane in which the horizontal axis is Q1 (kJ/m2) and the vertical axis is Q2 (kJ/m2). The numerical values shown are plotted, and the coordinate plane is divided into five regions in relation to the presence or absence of a casting leak. Fig. 11 is an explanatory view for explaining a means for solving the problem, which is a graph showing an example of the relationship between the casting speed and the average temperature in the thickness direction of the shell at the exit of the mold, and the vertical axis indicates the average temperature in the thickness direction of the mold outlet shell (°C). ), the horizontal axis represents the casting speed (m/min). Fig. 12 is an explanatory view showing a continuous casting apparatus provided with a casting leakage preventing device according to another embodiment of the present invention. Fig. 13 is an explanatory view showing a continuous casting apparatus provided with a casting leakage preventing device according to another embodiment of the present invention. [Main component symbol description] 1 Mold 3 Impregnation nozzle 5 Melting steel 7 Molding powder 9 Solidified shell 11 Molded copper plate 13 Cooling water passage 098106495 68 200946265 15 (Bottom of cooling water passage) Hole 17 Thermocouple 19 Casting 21 Guide roller 23 Pinch roller 25 Motor 27 Pinch roller control device ❹ 29 Local heat flux calculation means 31 Stable solidification interface Heat input memory means 32 Heat flux distribution calculation means 33 Cast leak determination means 33A Cast leak determination means body 34 Solidified shell thickness calculation Means 35 Control device 10 37 Alarm device 40 Feeding tank 41 Electromagnetic brake device 098106495 69
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