章顺虎, 赵德文, 刘南君, 高彩茹. 中厚板轧后冷却正规阶段温度场变分解[J]. 工程力学, 2013, 30(增刊): 363-368. DOI: 10.6052/j.issn.1000-4750.2012.03.S044
引用本文: 章顺虎, 赵德文, 刘南君, 高彩茹. 中厚板轧后冷却正规阶段温度场变分解[J]. 工程力学, 2013, 30(增刊): 363-368. DOI: 10.6052/j.issn.1000-4750.2012.03.S044
ZHANG Shun-hu, ZHAO De-wen, LIU Nan-jun, GAO Cai-ru. VARIATIONAL SOLUTION OF CONTINUOUS COOLING TEMPERATURE FIELD FOR PLATE AFTER ROLLING DURING FULLY DEVELOPED REGIME[J]. Engineering Mechanics, 2013, 30(增刊): 363-368. DOI: 10.6052/j.issn.1000-4750.2012.03.S044
Citation: ZHANG Shun-hu, ZHAO De-wen, LIU Nan-jun, GAO Cai-ru. VARIATIONAL SOLUTION OF CONTINUOUS COOLING TEMPERATURE FIELD FOR PLATE AFTER ROLLING DURING FULLY DEVELOPED REGIME[J]. Engineering Mechanics, 2013, 30(增刊): 363-368. DOI: 10.6052/j.issn.1000-4750.2012.03.S044

中厚板轧后冷却正规阶段温度场变分解

VARIATIONAL SOLUTION OF CONTINUOUS COOLING TEMPERATURE FIELD FOR PLATE AFTER ROLLING DURING FULLY DEVELOPED REGIME

  • 摘要: 该文从导热微分方程和定解条件出发,设定了预先满足边界条件的试函数,并结合拉格朗日乘子法,构建了里兹温度场泛函的广义表达式,经泛函变分,首次获得了中厚板轧后冷却正规阶段温度场的变分解,该解为板厚δ ,换热系数α ,比热cp,冷却时间t ,热传导率λ ,钢板密度ρ ,开冷温度T0,水温Tf的函数。该解与分离变量法获得的解析解比较表明,该解对分离变量法获得的解析解具有较高的逼近程度,两者最大误差不超过7℃。该文导出的平均温度出现在x =0.577δ 的位置上,心表温差随着冷却时间的增加而减少。该文中变分解法未报道。

     

    Abstract: From the heat conduction, differential equations and definite conditions, a trial function which satisfies boundary condition in advance is set. With the Lagrange multiplier method, the generalized expression of Ritz temperature field functional is first established. The variational solution of temperature field for a plate after rolling during fully developed regime is then first obtained by functional variation. It is a function of plate thick δ, heat transfer coefficient α, specific heat cp, cooling time t, thermal conductivity λ, plate density ρ, starting cooling temperature T0, and water temperature Tf. The comparison between the variational results and those analytical results by the separation variable method shows that the present results have high forecast precision and the maximum error between them is no more than 7%. It is also deduced that the average temperature occurs at the location of x=0.577δ, and the temperature difference between plate surface and centre along the thick direction decreases as the cooling time increases. The method in the present paper has not been reported yet.

     

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