AustralieFrV1, PascalFrancis, Curation, bibRecord, 001344

Mechanistic simulation of thermomechanical behaviour of thermoelastic martensitic transformations in polycrystalline shape memory alloys

Identifieur interne : 001344 ( PascalFrancis/Curation ); précédent : 001343; suivant : 001345

Mechanistic simulation of thermomechanical behaviour of thermoelastic martensitic transformations in polycrystalline shape memory alloys

Auteurs : Y. Liu [Australie] ; D. Favier [France] ; L. Orgeas [France]

Source :

Journal de physique. IV [ 1155-4339 ] ; 2004.

RBID : Pascal:04-0417886

Descripteurs français

Pascal (Inist)
- Transformation martensitique, Thermoélasticité, Approche mécaniste, Propriété thermomécanique, Joint grain, Stabilité phase, Effet contrainte, Ferroélasticité, Superélasticité, Effet mémoire forme, Effet non linéaire, Hystérésis mécanique, Polycristal, Alliage mémoire forme, Titane alliage, Nickel alliage, Alliage binaire, Etude expérimentale, Equation Clausius Clapeyron, 6220D, 8130K.

English descriptors

KwdEn :
- Binary alloys, Experimental study, Ferroelasticity, Grain boundaries, Martensitic transformations, Mechanical hysteresis, Mechanistic approach, Nickel alloys, Non linear effect, Phase stability, Polycrystals, Shape memory alloy, Shape memory effects, Stress effects, Superelasticity, Thermoelasticity, Thermomechanical properties, Titanium alloys.

Abstract

This paper proposes a mechanistic model to simulate the thermal and mechanical behaviour of shape memory alloys. The model is based on the thermodynamic concept of chemical, elastic and frictional energies for thermoelastic martensitic transformations and plasticity concept of grain interior and grain boundary phases. In a thermoelastic martensitic transformation system, a thermally induced transformation and a mechanically induced (stress-induced) transformation require different operating mechanisms from a mechanistic viewpoint. For a thermally induced transformation, the driving force arises from within the matrix and internal stresses are created as a result of frictional movement. For a mechanically induced transformation, the driving force is provided externally and the frictional movement occurs when the stress exceeds a critical value. This paper proposes a unified mechanistic model taking into account this difference. The model is able to describe, in a schematic and qualitative manner, the behaviour of a thermoelastic martensitic transformation system in both thermally induced and mechanically induced processes, including full and partial thermal transformation cycles, stress-induced martensitic transformation, pseudoelastic deformation and ferroelastic deformation via martensite variant reorientation. Such a model allows the discussion of several aspects concerning the thermal and mechanical behaviour of thermoelastic martensitic transformations, such as the non-linear pseudoelasticity, deformation-induced two-way memory effect, strain dependence of mechanical hysteresis and minor loop behaviour of deformation.

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A03		`1`		`@0 J. phys., IV`
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A08	`01`	`1`	`ENG`	`@1 Mechanistic simulation of thermomechanical behaviour of thermoelastic martensitic transformations in polycrystalline shape memory alloys`
A09	`01`	`1`	`ENG`	`@1 7th European Mechanics of Materials Conference : Adaptive Systems and Materials: Constitutive Materials and Hybrid Structures`
A11	`01`	`1`		`@1 LIU (Y.)`
A11	`02`	`1`		`@1 FAVIER (D.)`
A11	`03`	`1`		`@1 ORGEAS (L.)`
A12	`01`	`1`		`@1 LEXCELLENT (Christian) @9 ed.`
A12	`02`	`1`		`@1 PATOOR (Etienne) @9 ed.`
A14	`01`			`@1 School of Mechanical Engineering, University of Western Australia @2 Crawley WA 6009 @3 AUS @Z 1 aut.`
A14	`02`			`@1 Laboratoire Sols-Solides-Structures, UMR CNRS 5521, UJF-INPG, BP. 53 @2 38041 Grenoble @3 FRA @Z 2 aut. @Z 3 aut.`
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C01	`01`		`ENG`	@0 This paper proposes a mechanistic model to simulate the thermal and mechanical behaviour of shape memory alloys. The model is based on the thermodynamic concept of chemical, elastic and frictional energies for thermoelastic martensitic transformations and plasticity concept of grain interior and grain boundary phases. In a thermoelastic martensitic transformation system, a thermally induced transformation and a mechanically induced (stress-induced) transformation require different operating mechanisms from a mechanistic viewpoint. For a thermally induced transformation, the driving force arises from within the matrix and internal stresses are created as a result of frictional movement. For a mechanically induced transformation, the driving force is provided externally and the frictional movement occurs when the stress exceeds a critical value. This paper proposes a unified mechanistic model taking into account this difference. The model is able to describe, in a schematic and qualitative manner, the behaviour of a thermoelastic martensitic transformation system in both thermally induced and mechanically induced processes, including full and partial thermal transformation cycles, stress-induced martensitic transformation, pseudoelastic deformation and ferroelastic deformation via martensite variant reorientation. Such a model allows the discussion of several aspects concerning the thermal and mechanical behaviour of thermoelastic martensitic transformations, such as the non-linear pseudoelasticity, deformation-induced two-way memory effect, strain dependence of mechanical hysteresis and minor loop behaviour of deformation.
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C03	`02`	`3`	`FRE`	`@0 Thermoélasticité @5 03`
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C03	`03`	`X`	`ENG`	`@0 Mechanistic approach @5 04`
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C03	`06`	`3`	`FRE`	`@0 Stabilité phase @5 07`
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C03	`07`	`3`	`ENG`	`@0 Stress effects @5 08`
C03	`08`	`3`	`FRE`	`@0 Ferroélasticité @5 09`
C03	`08`	`3`	`ENG`	`@0 Ferroelasticity @5 09`
C03	`09`	`3`	`FRE`	`@0 Superélasticité @5 10`
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C03	`11`	`X`	`FRE`	`@0 Effet non linéaire @5 12`
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C03	`12`	`X`	`SPA`	`@0 Histéresis mecánica @5 13`
C03	`13`	`3`	`FRE`	`@0 Polycristal @5 15`
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C03	`14`	`X`	`FRE`	`@0 Alliage mémoire forme @5 16`
C03	`14`	`X`	`ENG`	`@0 Shape memory alloy @5 16`
C03	`14`	`X`	`SPA`	`@0 Aleación memoria forma @5 16`
C03	`15`	`3`	`FRE`	`@0 Titane alliage @5 17`
C03	`15`	`3`	`ENG`	`@0 Titanium alloys @5 17`
C03	`16`	`3`	`FRE`	`@0 Nickel alliage @5 18`
C03	`16`	`3`	`ENG`	`@0 Nickel alloys @5 18`
C03	`17`	`3`	`FRE`	`@0 Alliage binaire @5 19`
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C03	`20`	`3`	`FRE`	`@0 6220D @4 INC @5 56`
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C07	`01`	`3`	`FRE`	`@0 Métal transition alliage @5 48`
C07	`01`	`3`	`ENG`	`@0 Transition element alloys @5 48`
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A30	`01`	`1`	`ENG`	`@1 EUROMECH-MECAMAT'2003 @2 7 @3 Fréjus FRA @4 2003-05-18`

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Le document en format XML

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<front><div type="abstract" xml:lang="en">This paper proposes a mechanistic model to simulate the thermal and mechanical behaviour of shape memory alloys. The model is based on the thermodynamic concept of chemical, elastic and frictional energies for thermoelastic martensitic transformations and plasticity concept of grain interior and grain boundary phases. In a thermoelastic martensitic transformation system, a thermally induced transformation and a mechanically induced (stress-induced) transformation require different operating mechanisms from a mechanistic viewpoint. For a thermally induced transformation, the driving force arises from within the matrix and internal stresses are created as a result of frictional movement. For a mechanically induced transformation, the driving force is provided externally and the frictional movement occurs when the stress exceeds a critical value. This paper proposes a unified mechanistic model taking into account this difference. The model is able to describe, in a schematic and qualitative manner, the behaviour of a thermoelastic martensitic transformation system in both thermally induced and mechanically induced processes, including full and partial thermal transformation cycles, stress-induced martensitic transformation, pseudoelastic deformation and ferroelastic deformation via martensite variant reorientation. Such a model allows the discussion of several aspects concerning the thermal and mechanical behaviour of thermoelastic martensitic transformations, such as the non-linear pseudoelasticity, deformation-induced two-way memory effect, strain dependence of mechanical hysteresis and minor loop behaviour of deformation.</div>
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<fC01 i1="01" l="ENG"><s0>This paper proposes a mechanistic model to simulate the thermal and mechanical behaviour of shape memory alloys. The model is based on the thermodynamic concept of chemical, elastic and frictional energies for thermoelastic martensitic transformations and plasticity concept of grain interior and grain boundary phases. In a thermoelastic martensitic transformation system, a thermally induced transformation and a mechanically induced (stress-induced) transformation require different operating mechanisms from a mechanistic viewpoint. For a thermally induced transformation, the driving force arises from within the matrix and internal stresses are created as a result of frictional movement. For a mechanically induced transformation, the driving force is provided externally and the frictional movement occurs when the stress exceeds a critical value. This paper proposes a unified mechanistic model taking into account this difference. The model is able to describe, in a schematic and qualitative manner, the behaviour of a thermoelastic martensitic transformation system in both thermally induced and mechanically induced processes, including full and partial thermal transformation cycles, stress-induced martensitic transformation, pseudoelastic deformation and ferroelastic deformation via martensite variant reorientation. Such a model allows the discussion of several aspects concerning the thermal and mechanical behaviour of thermoelastic martensitic transformations, such as the non-linear pseudoelasticity, deformation-induced two-way memory effect, strain dependence of mechanical hysteresis and minor loop behaviour of deformation.</s0>
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</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Shape memory effects</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE"><s0>Effet non linéaire</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Non linear effect</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA"><s0>Efecto no lineal</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Hystérésis mécanique</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>Mechanical hysteresis</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Histéresis mecánica</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Polycristal</s0>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Polycrystals</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE"><s0>Alliage mémoire forme</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG"><s0>Shape memory alloy</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA"><s0>Aleación memoria forma</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Titane alliage</s0>
<s5>17</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Titanium alloys</s0>
<s5>17</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Nickel alliage</s0>
<s5>18</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Nickel alloys</s0>
<s5>18</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Alliage binaire</s0>
<s5>19</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Binary alloys</s0>
<s5>19</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>20</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>20</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>Equation Clausius Clapeyron</s0>
<s4>INC</s4>
<s5>53</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>6220D</s0>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>8130K</s0>
<s4>INC</s4>
<s5>57</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Métal transition alliage</s0>
<s5>48</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Transition element alloys</s0>
<s5>48</s5>
</fC07>
<fN21><s1>236</s1>
</fN21>
<fN44 i1="01"><s1>PSI</s1>
</fN44>
<fN82><s1>PSI</s1>
</fN82>
</pA>
<pR><fA30 i1="01" i2="1" l="ENG"><s1>EUROMECH-MECAMAT'2003</s1>
<s2>7</s2>
<s3>Fréjus FRA</s3>
<s4>2003-05-18</s4>
</fA30>
</pR>
</standard>
</inist>
</record>

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Mechanistic simulation of thermomechanical behaviour of thermoelastic martensitic transformations in polycrystalline shape memory alloys

Mechanistic simulation of thermomechanical behaviour of thermoelastic martensitic transformations in polycrystalline shape memory alloys

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