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METHOD OF secondary cooling of the slab in the continuous casting machines under steady-state and transient conditions CASTING

机译:稳态和瞬态条件下连铸机板坯的二次冷却方法

摘要

method u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 secondary cooling in continuous u0441u043bu00a0u0431u0430 car u043bu0438u0442u044cu00a0 blanks for stationary and transitional regimes, including pitch metal crystal u0438u0437u0430u0442u043eu0440 of intermediate bucketu0432u044bu0442u00a0u0433u0438u0432u0430u043du0438u00a0 of billets and its variable speed cooling zones by a u043eu0445u043bu0430u0434u0438u0442u0435u043bu00a0 (water or water - air mixture) on the surface of billets with the large and small radii and the definition of cost u043eu0445u043bu0430u0434u0438u0442u0435u043bu00a0, u043eu0442u043bu0438u0447u0430u044eu0449u0438u0439u0441u00a0, however, that the u043eu0445u043bu0430u0434u0438u0442u0435u043bu00a0 zones u043eu043fu0440u0435u0434u0435u043bu00a0u044eu0442 of u0432u044bu0440u0430u0436u0435u043du0438;where to see the water in the second zone u043eu0445u043bu0430u0436u0434u0435u043du0438u00a0, m3 / h;;(i = 1, 2,..., n is the number of secondary u043eu0445u043bu0430u0436u0434u0435u043du0438u00a0 u043eu043fu0440u0435u0434u0435u043bu00a0u044eu0449u0438u0439 zone;;current u0432u0440u0435u043cu00a0, counted from the beginning of casting, with.;[*] - the dependence of heat transfer coefficient on the surface of the u0441u043bu00a0u0431u0430 (w / m2) from time to time, u043au043eu0442u043eu0440u0430u00a0 u043eu043fu0440u0435u0434u0435u043bu00a0u0435u0442u0441u00a0 depending on the regime u043eu0445u043bu0430u0436u0434u0435u043du0438u00a0 u0434u043bu00a0 brand became a and by calculation with the task of u0437u0430u0442u0432u0435u0440u0434u0435u0432u0430u043du0438u00a0 with a given change in surface temperature u0441u043bu00a0u0431u0430 t = t [*];;* a = * (zi) u0432u0440u0435u043cu00a0 (c), the u043cu043du043bu0437 element u0441u043bu00a0u0431u0430, which in the current time u043du0430u0445u043eu0434u0438u0442u0441u00a0 point zi technology axis, and which u043eu043fu0440u0435u0434u0435u043bu00a0u0435u0442u0441u00a0 numerically from and u043du0442u0435u0433u0440u0430u043bu044cu043du043eu0433u043e u0443u0440u0430u0432u043du0435u043du0438u00a0:;where (') - the change of casting speed in time, m / s;;gi {} - u0444u0443u043du043au0446u0438u00a0, u043eu0431u0440u0430u0442u043du0430u00a0 to dependence (gi), where gi - the u043eu0445u043bu0430u0434u0438u0442u0435u043bu00a0 flow (m3 / u043c2u0447) in the second zone u043eu0445u043bu0430u0436u0434u0435u043du0438u00a0, coefficient of heat transfer on the surface of u0441u043bu00a0u0431u0430 in this zone, the p rich dependence (gi) (i = 1, 2,..., n) can u0440u0430u0437u043bu0438u0447u0430u0442u044cu0441u00a0 u0434u043bu00a0 separate zones;;z = z0i - zi; zi characteristic coordinates zones, m, starting from the she had a meniscus.;z0i coordinates u0441u0435u0440u0435u0434u0438u043d zones, m;;li - length zone, m;;u0432i - u043eu0445u043bu0430u0436u0434u0430u0435u043cu0430u00a0 width u0441u043bu00a0u0431u0430 in the second zone.
机译:方法 u0443 u043f u0440 u0430 u0432 u043b u0435 u043d u0438 u00a0在连续 u0441 u043b u00a0 u0431 u0430轿车 u043b u0438 u0442 u044c u0040中的二次冷却过渡方式,包括中间桶的沥青金属晶体 u0438 u0437 u0430 u0442 u043e u0440 u0432 u044b u0442 u00a0 u0433 u0438 u0432 u0430 u043d u0438 u00a0及其变速通过在半径较大和较小的方坯表面上通过 u043e u0445 u043b u0430 u0434 u0438 u0442 u0435 u043b u00a0(水或水-空气混合物)来冷却区域,并定义成本 u0445 u043b u0430 u0434 u0438 u0442 u0435 u043b u00a0, u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0438 u0439 u04439 u0441 u00a0但是 u0445 u043b u0430 u0434 u0438 u0442 u0435 u043b u00a0区域 u043e u043f u0440 u0435 u0434 u0435 u043b u00a0 u044e u0442 u0432 u044b u0440 u0430 u0435 u043d u0438;哪里可以看到第二个区域中的水 u043e u0445 u043b u0430 u0436 u0434 u0435 u043d u0438 u00a0,m3 / h ;;(i = 1,2,...,n是次要 u043e u0445 u043b u0430 u0436 u0434 u0435 u043d u0438 u00a0 u043e u043f u0440 u0435 u0434 u0435 u043b u00a0 u044e u0449 u0438 u0439区域;当前 u0432 u0440 u0435 u043c u00a0,从转换开始算起[*]-时不时地,传热系数对 u0441 u043b u00a0 u0431 u0430(w / m2)的依赖性, u043a u043e u0442 u043e u0440 u0430 u00a0 u043e u043f u0440 u0435 u0434 u0435 u043b u00a0 u0435 u0442 u0441 u00a0取决于系统 u043e u0445 u043b u043b u0430 u0436 u0434 u0435 u043d u043d u00a0 u0434 u043b u00a0品牌成为a,并通过计算 u0437 u0430 u0442 u0432 u0435 u0440 u0434 u0435 u0435 u0432 u0430 u043d u0438 u00a0温度 u0441 u043b u00a0 u0431 u0430 t = t [*] ;; * a = *(zi) u0432 u0440 u0435 u043c u00a0(c), u043c u043d u043b u0437元素 u0441 u043b u00a0 u0431 u0430,在当前时间 u043d u0430 u0445 u043e u0434 u0438 u0442 u0441 u00a0点zi工艺轴,以及哪个 u043e u043f u0440 u0435 u0434 u0435 u043b u043b u00a0 u0435 u0442 u0441 u00a0从 u043d u0442 u0435 u0433 u0440 u0430 u043b u044c u043d u043e u0433 u043e u0443 u0440 u0430 u0432 u0432 u043d u0435 u043d u0438 u00 ;其中(')-时间随时间的变化,m / s ;; gi {}- u0444 u0443 u043d u043a u0446 u0438 u00a0, u043e u0431 u0440 u0430 u0442 u043d u0430 u00a0到依赖项(gi),其中gi-第二个区域中的 u043e u0445 u043b u0430 u0434 u0438 u0442 u0435 u043b u00a0流量(m3 / u043c2 u0447) u043e u0445 u043b u0430 u0436 u0434 u0435 u043d u0438 u00a0,该区域中 u0441 u043b u00a0 u0431 u0430表面的传热系数,p依赖关系(gi)( i = 1,2,...,n)可以 u0440 u0430 u0437 u043b u0438 u0447 u0430 u0442 u044c u0441 u00a0 u0434 u043b u00a0单独的区域; z = z0i-zi ; zi特征坐标区域m,从其弯月面开始。; z0i坐标 u0441 u0435 u0440 u0435 u0434 u0438 u043d区域m,; li-长度区域m ;; u0432i- u043e u0445 u043b u0430 u0436 u0434 u0430 u0435 u043c u0430 u00a0宽度 u0441 u043b u00a0 u0431 u0430在第二个区域中。

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