2002
DOI: 10.1016/s1359-4311(02)00022-4
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A simulation of heat transfer during billet transport

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Cited by 27 publications
(21 citation statements)
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“…23 (ii) calculations of the scale conductivity were conducted over a range of void sizes using the thermal conductivity of iron oxides 35 and the formula for heat transfer by radiation over voids, 36 and 2 W m 21 K 21 is adopted (iii) conductance at the interface is uncertain. Jaklič et al 36 assumed that scale detaches from steel, and modelled heat transfer between them as radiation between two infinite parallel planes. The conductance estimated in this way is in hundreds of W m 22 K 21 .…”
Section: Modelling Of Slabsmentioning
confidence: 99%
See 1 more Smart Citation
“…23 (ii) calculations of the scale conductivity were conducted over a range of void sizes using the thermal conductivity of iron oxides 35 and the formula for heat transfer by radiation over voids, 36 and 2 W m 21 K 21 is adopted (iii) conductance at the interface is uncertain. Jaklič et al 36 assumed that scale detaches from steel, and modelled heat transfer between them as radiation between two infinite parallel planes. The conductance estimated in this way is in hundreds of W m 22 K 21 .…”
Section: Modelling Of Slabsmentioning
confidence: 99%
“…The details of the finite difference scheme are as follows: (i) boundary condition at the slab/rider interface depends on whether the beam is walking or stationary, since it determines the time of slab on rider. If the slab is not resting on the rider, the heat is transferred from slab to rider by radiation (equation (35)), otherwise by conductivity (ii) the rider is deeply imbedded into a beam, and heat transfer from gas to its sides is neglected (iii) if the slab is resting on the rider, the effective slab temperature for heat transfer to the rider is a simple contact length based average of slab temperatures at individual nodes (iv) since the rider is composite, the effective physical properties of nodes surrounded by different materials are calculated as in the case of refractory (v) the boundary condition at the slab/rider interface in a particular zone is given by equation (36). The condition depends on the portion of time with slab resting on the rider (vi) the boundary condition at the water/pipe interface is given by equation (37) h r,rad~s e B T 2 Stationary and walking beams obstruct a large portion of radiation from gas to the bottom face of a slab.…”
Section: Heat Transfer To and Through Beamsmentioning
confidence: 99%
“…Temperature is the sensitive factor of mechanical parameters such as rolling force, torque and power, and affects the thickness precision of the product and the surface quality. The temperature is also an important condition for the recrystallization, transformation and precipitation of the hot rolling [1][2][3][4]. The control precision of the rolling temperature determines the structure and properties of the product after rolling.…”
Section: Introductionmentioning
confidence: 99%
“…Algunos trabajos publicados abordan la formación de óxidos dentro de los hornos empujadores de recalentamiento de palanquillas, en el año 2001, Anton Jajlic y sus colaboradores [4] proponen un modelo donde se simula el calentamiento de las palanquillas dentro de un horno de vigas galopantes, el modelo se construyó en tres dimensiones, y evalúa los fenómenos de transporte energético considerando los tres mecanismos de transferencia de calor, la conducción, la convección y la radiación. Los modelos existentes simulan el proceso de calentamiento de las palanquillas durante su desplazamiento.…”
Section: Introductionunclassified