Phase formation rules for high entropy alloys

Содержание

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Acknowledgements Prof. GuoLiang Chen; Prof. Hywel A Davies; Prof. Peter K

Acknowledgements

Prof. GuoLiang Chen;
Prof. Hywel A Davies;
Prof. Peter K Liaw;


Prof. George Smith;
Prof. Zhaoping Lu;
XueFei Wang; YunJun Zhou; FangJun Wang.
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Outlines I. Background & Motivations II. Results & Discussions III. Summaries

Outlines

I. Background & Motivations
II. Results & Discussions
III. Summaries

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(1) Conventional alloys I. Background & Motivations Steel, A=Fe, B=Carbon, δB

(1) Conventional alloys

I. Background & Motivations

Steel, A=Fe,
B=Carbon, δB<2%;
Cast Iron, A=Fe,


B=Carbon, δB<6.5%

1.1 Alloys Design Strategy

Alloy=A+δB+ δC+;
A>50%; …

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(2) High Entropy Alloys HEAs=A+B+C+D+E; 50% 15% AlCoCrFeNi=HEA , Zhou, APL,

(2) High Entropy Alloys
HEAs=A+B+C+D+E; 50%15%

AlCoCrFeNi=HEA ,
Zhou, APL, 2007

CoCrCuFeNi=HEA,
Yeh, MMTA,

2004;

FCC type HEA Solid Solution

BCC type HEA Solid Solution

Al20[TiVMnHEA]80,
Zhou, MSEA, 2007

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Solid solution has higher entropy than the mechanical mixture does. 1.2 Thermodynamically For the regular solution:

Solid solution has higher entropy than the mechanical mixture does.

1.2 Thermodynamically

For

the regular solution:
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Gibbs Free Energy ΔGmix =ΔHmix-TΔSmix

Gibbs Free Energy

ΔGmix =ΔHmix-TΔSmix

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1.3 Properties and Applications High Strength; Zhou, APL, 2007; High wear

1.3 Properties and Applications

High Strength; Zhou, APL, 2007;
High wear resistance; Lin,

Surface Coating technology, 2008.
High corrosion resistance; Lee, Thin Solid Films, 2008;
High thermo-stability; Tsai, APL, 2008.

Properties

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1 Coatings, Barriers, etc. Diffusion barriers for Cu interconnections; Tsai, APL,

1 Coatings, Barriers, etc.
Diffusion barriers for Cu interconnections; Tsai, APL, 2008
2

Structural Materials
3 Energy Storage Materials,
Raju, Journal of power Sources, 2008;
4 Molds

Potential Applications

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To understand what is the dominant factors for the phase formation

To understand what is the dominant factors
for the phase formation

of the HEAs

1 Atomic radius, or atomic volume;

The contents of Al, Ti, Cu, Co in
the HEAs were changed

Kittel, Introduction to Solid State Physics

1.4 Motivations

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2 Enthalpy of Mixing; 3 Entropy of Mixing

2 Enthalpy of Mixing;

3 Entropy of Mixing

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4 Cooling Rate 5 Tensile and compressive properties Critical cooling rate?

4 Cooling Rate

5 Tensile and compressive properties

Critical cooling rate? Like the

BMG?

Tensile elongation=0? Like BMG?

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CoCrFeNiCu1-yAly FCC BCC, High APE to Lower APE, with larger atoms

CoCrFeNiCu1-yAly

FCC BCC, High APE to Lower APE, with larger atoms Al

2.1.

Alloying with different atomic size, Al, Cu, Co, Ti

Ti0.5CoCrFeNiCu1-yAly

(y=0, 0.25, 0.5, 0.75)

II. Results & Discussions

Al=1.438A

3.579A

2.913A,2.872A

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Cu=1.278A CoCrFeNiAlCuy ( y=0, 0.25, 0.5) Ti0.5CoCrFeNiAlCuy No PHASE TRANSITION

Cu=1.278A

CoCrFeNiAlCuy

( y=0, 0.25, 0.5)

Ti0.5CoCrFeNiAlCuy

No PHASE TRANSITION

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Co=1.251A The smaller BCC transit to FCC firstly after adding Co Biger BCC1phase:2.913A; Smaller BCC2phase:2.872A

Co=1.251A

The smaller BCC transit to FCC firstly after adding Co

Biger BCC1phase:2.913A;

Smaller BCC2phase:2.872A
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[Al1Co1Cr1Fe1Ni1]Tix alloys BCC+Ti BCC+BCC Ti=1.448A

[Al1Co1Cr1Fe1Ni1]Tix alloys

BCC+Ti BCC+BCC

Ti=1.448A

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After adding Ti, Laves phase forms

After adding Ti, Laves phase forms

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Zhou, APL, 2008 The transition is mainly lattice distortion induced and APE related

Zhou, APL, 2008

The transition is mainly lattice distortion induced and APE

related
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A schematic showing the additional effects

A schematic showing the additional effects

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Zhang, AEM, 2008 2.2. Considering of the enthalpy of mixing ΔHmix

Zhang, AEM, 2008

2.2. Considering of the enthalpy of mixing ΔHmix

Mg based

BMG

Zr based BMG

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2.3. Considering of the entropy of mixing ΔSmix High Entropy is

2.3. Considering of the entropy of mixing ΔSmix

High Entropy is not

good for the formation of BMG
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2.4 Cooling Rate AlCoCrFeNi

2.4 Cooling Rate

AlCoCrFeNi

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AlCoCrFeNi 2mm 5mm 8mm 10mm

AlCoCrFeNi

2mm

5mm

8mm

10mm

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AlCoCrFeNi

AlCoCrFeNi

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2.5 Tensile and Compressive properties XRD pattern for the CoCrCuFeNiAl0.5 alloy.

2.5 Tensile and Compressive properties

XRD pattern for the CoCrCuFeNiAl0.5 alloy.

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Table Room temperature mechanical test results for the CoCrCuFeNiAl0.5 alloy εP:

Table Room temperature mechanical test results for the CoCrCuFeNiAl0.5 alloy

εP: plastic strain; ε0.2 : yield strength; σmax: compressive/tensile strength

Φ5×10

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III. Summaries 1 Atomic size mismatch is the dominant factor for

III. Summaries

1 Atomic size mismatch is the dominant factor for the

phase formation of the high entropy alloys;
2 The formation of solid solution for the HEAs intends to have enthalpy of mixing close to zero;
3 High entropy of mixing facilitates the formation of the solid solution rather than the BMGs;
4 Cooling rate plays rather important role for the homogeneous microstructure than for the phase formation;
5 HEA can have tensile elongations as high as 19%.