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A predictive model for the evolution of the thermal conductance at the casting-die interfaces in high pressure die casting

Identifieur interne : 003784 ( PascalFrancis/Curation ); précédent : 003783; suivant : 003785

A predictive model for the evolution of the thermal conductance at the casting-die interfaces in high pressure die casting

Auteurs : A. Hamasaiid [France] ; G. Dour [France] ; T. Loulou [France] ; M. S. Dargusch [Australie]

Source :

RBID : Pascal:10-0151730

Descripteurs français

English descriptors

Abstract

An analytical model is proposed to predict the time varying thermal conductance at the casting-die interface during solidification of light alloys during High pressure Die Casting. Details of the topography of the interface between the casting and the die are included in the model through the inclusion of solid surface roughness parameters and the mean trapped air layer at the interface . The transitory phase of the interfacial thermal conductance has been related to the degradation of contact as solidification progresses through the casting thickness. The modelled time varying thermal conductance showed very good agreement with experimentally determined values for different alloy compositions and casting geometries. The analysis shows that the parameters that govern the thermal conductance are different for the first stage of contact compared to the second stage of contact when the alloy begins to solidify.
pA  
A01 01  1    @0 1290-0729
A03   1    @0 Int. j. therm. sci.
A05       @2 49
A06       @2 2
A08 01  1  ENG  @1 A predictive model for the evolution of the thermal conductance at the casting-die interfaces in high pressure die casting
A11 01  1    @1 HAMASAIID (A.)
A11 02  1    @1 DOUR (G.)
A11 03  1    @1 LOULOU (T.)
A11 04  1    @1 DARGUSCH (M. S.)
A14 01      @1 Universite de Toulouse, INSA, UPS, Mines Albi, ISAE, ICA (Institut Clement Ader), CROMeP, Campus Jarlard @2 81013 Albi @3 FRA @Z 1 aut. @Z 2 aut.
A14 02      @1 CAST Cooperative Research Centre, School of Engineering, The University of Queensland @2 St. Lucia, Brisbane QLD 4072 @3 AUS @Z 4 aut.
A14 03      @1 Université de Bretagne-Sud, LIMAT B, rue de Saint-Maudé @2 56321 Lorient @3 FRA @Z 3 aut.
A20       @1 365-372
A21       @1 2010
A23 01      @0 ENG
A43 01      @1 INIST @2 5065 @5 354000189245310160
A44       @0 0000 @1 © 2010 INIST-CNRS. All rights reserved.
A45       @0 26 ref.
A47 01  1    @0 10-0151730
A60       @1 P
A61       @0 A
A64 01  1    @0 International journal of thermal sciences
A66 01      @0 FRA
C01 01    ENG  @0 An analytical model is proposed to predict the time varying thermal conductance at the casting-die interface during solidification of light alloys during High pressure Die Casting. Details of the topography of the interface between the casting and the die are included in the model through the inclusion of solid surface roughness parameters and the mean trapped air layer at the interface . The transitory phase of the interfacial thermal conductance has been related to the degradation of contact as solidification progresses through the casting thickness. The modelled time varying thermal conductance showed very good agreement with experimentally determined values for different alloy compositions and casting geometries. The analysis shows that the parameters that govern the thermal conductance are different for the first stage of contact compared to the second stage of contact when the alloy begins to solidify.
C02 01  X    @0 001D11C01E
C02 02  X    @0 240
C03 01  X  FRE  @0 Conductivité thermique @5 02
C03 01  X  ENG  @0 Thermal conductivity @5 02
C03 01  X  GER  @0 Waermeleitfaehigkeit @5 02
C03 01  X  SPA  @0 Conductividad térmica @5 02
C03 02  X  FRE  @0 Coulée sous pression @5 03
C03 02  X  ENG  @0 Pressure die casting @5 03
C03 02  X  GER  @0 Druckgiessen @5 03
C03 02  X  SPA  @0 Colada bajo presión @5 03
C03 03  X  FRE  @0 Méthode analytique @5 05
C03 03  X  ENG  @0 Analytical method @5 05
C03 03  X  SPA  @0 Método analítico @5 05
C03 04  X  FRE  @0 Solidification @5 06
C03 04  X  ENG  @0 Solidification @5 06
C03 04  X  GER  @0 Erstarren @5 06
C03 04  X  SPA  @0 Solidificación @5 06
C03 05  X  FRE  @0 Transfert chaleur @5 07
C03 05  X  ENG  @0 Heat transfer @5 07
C03 05  X  GER  @0 Waermeuebertragung @5 07
C03 05  X  SPA  @0 Transferencia térmica @5 07
C03 06  X  FRE  @0 Inclusion solide @5 08
C03 06  X  ENG  @0 Solid inclusion @5 08
C03 06  X  GER  @0 Feststoffeinschluss @5 08
C03 06  X  SPA  @0 Inclusión sólida @5 08
C03 07  X  FRE  @0 Condition initiale @5 09
C03 07  X  ENG  @0 Initial condition @5 09
C03 07  X  SPA  @0 Condición inicial @5 09
C03 08  X  FRE  @0 Alliage léger @5 15
C03 08  X  ENG  @0 Light alloy @5 15
C03 08  X  SPA  @0 Aleación ligera @5 15
C03 09  X  FRE  @0 Alliage moulé @5 16
C03 09  X  ENG  @0 Cast alloy @5 16
C03 09  X  GER  @0 Gusslegierung @5 16
C03 09  X  SPA  @0 Aleación moldeada @5 16
C03 10  X  FRE  @0 Interface liquide solide @5 17
C03 10  X  ENG  @0 Liquid solid interface @5 17
C03 10  X  GER  @0 Grenzschicht fluessig fest @5 17
C03 10  X  SPA  @0 Interfase líquido sólido @5 17
C03 11  3  FRE  @0 Alliage base magnésium @2 NK @5 18
C03 11  3  ENG  @0 Magnesium base alloys @2 NK @5 18
C03 12  3  FRE  @0 Alliage base aluminium @2 NK @5 19
C03 12  3  ENG  @0 Aluminium base alloys @2 NK @5 19
C03 13  X  FRE  @0 Coulée sous haute pression @4 CD @5 96
C03 13  X  ENG  @0 High pressure die casting @4 CD @5 96
N21       @1 095

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<s0>An analytical model is proposed to predict the time varying thermal conductance at the casting-die interface during solidification of light alloys during High pressure Die Casting. Details of the topography of the interface between the casting and the die are included in the model through the inclusion of solid surface roughness parameters and the mean trapped air layer at the interface . The transitory phase of the interfacial thermal conductance has been related to the degradation of contact as solidification progresses through the casting thickness. The modelled time varying thermal conductance showed very good agreement with experimentally determined values for different alloy compositions and casting geometries. The analysis shows that the parameters that govern the thermal conductance are different for the first stage of contact compared to the second stage of contact when the alloy begins to solidify.</s0>
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<s5>03</s5>
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<s0>Alliage base aluminium</s0>
<s2>NK</s2>
<s5>19</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Aluminium base alloys</s0>
<s2>NK</s2>
<s5>19</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE">
<s0>Coulée sous haute pression</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG">
<s0>High pressure die casting</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21>
<s1>095</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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