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Development of Titanium alloy Development of Titanium alloy with Controlled Elastic Properties with Controlled Elastic Properties Toyota Central R&D Labs., Inc. T. Furuta Toyota Central R&D Labs., Inc. T. Furuta

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Page 1: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Development of Titanium alloy Development of Titanium alloy with Controlled Elastic Properties with Controlled Elastic Properties

Toyota Central R&D Labs., Inc.T. Furuta

Toyota Central R&D Labs., Inc.T. Furuta

Page 2: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Outline

•Fuel-Efficient Technology of Automobile

•Why Elastic Modulus of Metal is Important? And How to Control Elastic Property

• Developed Ti-Alloys

•TiB Reinforced Titanium MMC

•Gum Metal

• Summary

Page 3: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

FFueluel--Efficient Technology ofEfficient Technology of AutomobileAutomobile

Reduction of Friction Coefficient

Improvement of Unit

Efficiency

Direct Injection Engine

Weight Reduction of Moving Parts

Reduction of Running

ResistanceReduction of

Rolling Resistance

Reduction of Air Resistance

Weight Reduction of Vehicle

Improvementof Engine Combustion

Reduction of Friction Loss

Improvement of Transmission

Efficiency

Application of lightweight with High Strength Material

Optimal Design

Minimization

Hybrid Engine

Diesel Engine

CVT (Belt, Toroidal )

Al, Ti, MgAl, Ti, Mg・・・・・・・・

TOYOTA CENTRAL R&D LABS., INC.

Page 4: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Elastic Modulus of Metal in Material Design

・Tensile Strain:ε=σ/E

d:Wire DiameterD:Coil DiameterN:Number of turns

・Constant ofSpring: K= Gd4

8D3N

m:weight of moving parts

・Resonance point ∝m

E・Iz

・Deflection in Bending :δ ∝ M/E・Iz

E:Young’s Modulus, G:Rigidity Modulus

M:Bending MomentIz:Geometrical

Moment of Inertia

Controlling Elastic properties is Key Technology Controlling Elastic properties is Key Technology

StrengthStrengthDesignDesign

Elastic Elastic DesignDesign

Weight ReductionWeight Reduction

TOYOTA CENTRAL R&D LABS., INC.

Page 5: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Elastic Modulus (GPa)

Gum Metal

Elastic Modulus of Materials

Rubber

Polyethylene

Nylon

Wood

Bone Concrete

Stone

Glass

0.001

1

10

100

1000

Met

alSi3N4Al2O3

TiB2

Mg Al Ti Ti Cu Steel TiB Ti-MMC

Control by Control by CompoundingCompounding

Control of Control of Binding EnergyBinding Energy

TOYOTA CENTRAL R&D LABS., INC.

Page 6: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

TiB Reinforced Titanium Matrix Composite

TOYOTA CENTRAL R&D LABS., INC.

Page 7: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Adaptable of the Reinforcement for BE Titanium Alloy

TiBTiCTiNSiCSi3N4TiB2B4CAl2O3

28.024.724.025.014.734.027.522.5

8.67.49.34.33.26.44.58.1

550460250420320529449350

<0.001 1.01.2 15.0

22.0 26.0Unstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloy

ExcellentPassableFailureFailureFailureFailureFailureFailure

ParticleKnoopHardness(GPa)

ElasticModulus(GPa)

CoefficientLinear Expansion(x10-1K-1)

Maximum Solubility[Matrix] [Particle]

(at%)Estimation

Coefficient of Linear Expansion of Ti alloy is around 9x10-6 K-1

TOYOTA CENTRAL R&D LABS., INC.

Page 8: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Manufacturing Process of Developed MMC

Compacting Sintering Hot Working

Developed MMC

1300℃, 4hr10-5 Torr

Ti Powder

TiB2 Powder

Ti+TiB2→2TiB

Master AlloyPowders

Heat Treatment

Matrix Alloy

392MPa

TOYOTA CENTRAL R&D LABS., INC.

Page 9: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

1.1. α+β α+β based MMCbased MMC TiB / Ti-6Al-4V, TiB / Ti-6Al-4V-1Fe-2Mo

Well balanceIn‐Valve, Valve retainer

2. ββ based MMCbased MMCTiB / Ti-4.3Fe-7Mo-1.4Al-1.4V

High-strengthConnecting-Rod

3. Near Near αα based MMCbased MMCTiB / Ti-6Al-4Sn-4Zr-1Mo-1Nb-0.2SiHeat resistance

Ex-Valve

排気バルブ排気バルブ

バルブリフタバルブリフタ

バルブスフ リ゚ン グバルブスフ リ゚ン グ

吸気バルブ吸気バルブ

コンロッドコンロッド

排気バルブ排気バルブ

バルブリフタバルブリフタ

バルブスフ リ゚ン グバルブスフ リ゚ン グ

吸気バルブ吸気バルブ

コンロッドコンロッド

Possible Application to Automotive parts

Valve Spring

Con-Rod

In-Valve

Ex-Valve

Valve Retainer

TOYOTA CENTRAL R&D LABS., INC.

Page 10: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

80

100

0 10 20 30TiB Content / Vol. %

120

140

160

α+β Matrix (973K x 3.6 ks)

β Matrix(1173K x 3.6 ks)

40

180

200E

last

ic M

odul

us /

GP

a

Ti-6Al-4V Alloy level

340 Stainless Steel level

Ti-8Al-1V-1Mobased MMC

α+β Matrix(973K x 3.6 ks)

Ti-4.3Fe-7Mo-1.4Al-1.4V based MMC

Elastic Modulus vs TiB Content

TOYOTA CENTRAL R&D LABS., INC.

Page 11: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

1200

800

400

 0

Ti-6

Al-4

V

開発

βTi

基M

MC

1600

2000

160

140

120

180

200

100

10

20

30

40

020vo

l %Ti

B /T

i-4.3

Fe-7

Mo-

1.4A

l-1.4

V

2200

10vo

l %Ti

B /T

i-6A

l-4V-

1Fe-

2Mo

TensileStress

FatigueStrength

WearLoss

ElasticModulus

Ela

stic

Mod

ulus

/ G

Pa

Tens

ile S

tress

, Fa

tigue

Stre

ngth

/ M

Pa

Wea

r Los

s /

mg/

km

Mechanical Properties of Developed MMC

TOYOTA CENTRAL R&D LABS., INC.

Page 12: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

The First Family Automobile in the world Installed Titanium In and Ex Valves.

TOYOTA CENTRAL R&D LABS., INC.

Page 13: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Die close Die open

Row Powders + Blending Compaction

Extruding

Sintered Billet

Forging

Sintering

Injection Heating

In Ex ・Annealing・Machining・Surface

Oxidizing

Manufacturing Process of Ti-MMC Valve

5vol%TiB / Ti5vol%TiB / Ti--6Al6Al--4.5Sn4.5Sn--4.5Zr4.5Zr--1Mo1Mo--1Nb1Nb--0.2Si0.2Si--0.3O0.3O

TOYOTA CENTRAL R&D LABS., INC.

Page 14: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Benefits of Developed Engine Valve

Spring

CurrentWeight

TitaniumWeight

WeightRedaction

44.6gIN-Valve

EX-Valve

27g

24g40g

43g 36g

40%

40%

16%

Engine Noise : 30% ReductionMaximum Revolution : 700 r.p.m. Improve

TOYOTA CENTRAL R&D LABS., INC.

Page 15: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

1. Multifunctional Ti Alloy (Gum Metal)low modulus, high strength, …

2. Alloy Designing ab initio calculations in binary alloys, experimental study on alloying element3. ApplicationSpectral Frame, Screws, Bolt,…

Gum MetalGum Metal

T. Saito, et al., T. Saito, et al., ScienceScience, 300 (2003), 464. Multifunctional , 300 (2003), 464. Multifunctional Alloys Obtained via a DislocationAlloys Obtained via a Dislocation--Free Free Plastic Deformation MechanismPlastic Deformation Mechanism

TOYOTA CENTRAL R&D LABS., INC.

Page 16: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

TiTi 25 50 75 1000

50

100

150

200

Elas

tic M

odul

us /G

Pa

Ta

Va Elements Content / mol%

Theoretical PredictionTheoretical Prediction

Elastic Modulus of Ti-X Binary Alloy System

Calculation of a parameter; C11-C12, which is related to elastic modulus of bcc structure and bcc phase stability

ExperimentalExperimental

TiTi 25 50 75 100

Ta

V

Nb

0

50

100

150

200

Elas

tic M

odul

us /G

Pa

0

50

100

150

C11

-C12

(Ti

-Nb)

/GPa

CC1111--CC1212

TOYOTA CENTRAL R&D LABS., INC.

V

Nb

Page 17: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

-100

0

100

200

300

400

3 3.5 4 4.5 5 5.5 6

c 11-

c 12

/ GPa

Relationship between C11-C12 and e/aTiTi--X binary alloy (Nb,Ta,V,MoX binary alloy (Nb,Ta,V,Mo・・・・・・・・))

1211

12111211001

))(2(CC

CCCCE

+−+

=

bcc unstablebcc unstable

Valence Electron Number, e/a

TiTi--25mol% Va25mol% Va

TOYOTA CENTRAL R&D LABS., INC.

Page 18: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

392MPa

1573K×16hr10-3Pa

1073K~1273K

Ti Powder

Compacting

VacuumSintering

Mixing

Nb,Ta,V,Zr,Hf Powder

Hot Working

Cold Working

Manufacturing Process of Gum Metal

Alloy design of Gum MetalAlloy design of Gum Metal

Over a hundred of Ti-Nb-Ta-V-Zr-O (O: 1at%)alloys were prepared.

Relations between Young’s Modulus and alloy compositionwere studied experimentally.

Ultrasonic Measurement of Young’s Modulus

TOYOTA CENTRAL R&D LABS., INC.

Page 19: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

TiTi--24mol%(Ta+Nb+V24mol%(Ta+Nb+V))--((Zr, HfZr, Hf))【【 e/ae/a≒≒4.244.24,,MdMd≒≒2.452.45,,BoBo≒≒2.87 2.87 】】

a) Low Modulus (40GPa) with High Strength (1100MPa)

b) Ultrahigh elastic deformability (2.5%)c) Nonlinear elasticity without any hysteresis d) Super ductility without work hardening e) Invar and Elinvar properties

Cold WorkingCold Working

-- OO

Characteristic of Gum Metal Characteristic of Gum Metal

TOYOTA CENTRAL R&D LABS., INC.

Page 20: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Strain / %

600

1000

1400St

ress

/ M

Pa

1200

800

400

200

00 1 2 3 4 5

1600

As AnnealedNon

linea

r Elas

ticity

Nonlin

ear E

lastic

ity

Elastic Limit

Ti-23Nb-0.7Ta-2.0Zr-1.2O (at %)

90% Cold Worked

Elastic StrainElastic Strain

Change in Stress-strain Curve with Cold working

TOYOTA CENTRAL R&D LABS., INC.

Page 21: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

0

20

40

60

80

100

120

140

0 20 40 60 80 100

1.0

0.5

0

1.5

2.0

2.5

3.0

Reduction in Area / %

Ela

stic

Mod

ulus

/ M

Pa

Atta

inab

le E

last

ic S

train

/ %

Ti-23Nb-0.7Ta-2.0Zr-1.2O (at%)

Elastic Strain

Elastic Modulus

Effect of Cold working

TOYOTA CENTRAL R&D LABS., INC.

Page 22: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Conventional β-Titanium Alloy(TI-15V-3Al-3Cr-3Sn wt%)

Cold Working Ratio / %

Reduction in Area

Har

dnes

s /

Hv 300

200

100

00 20 40 60 80 100

400

20

40

60

80

0

Red

uctio

n in

Are

a /

Ti-23Nb-0.7Ta-2.0Zr-1.2O (at%)

Hardness

Reduction in Area

Hardness, Reduction in Area vs Cold working

Conventional β-Ti Alloy

TOYOTA CENTRAL R&D LABS., INC.

Page 23: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

100100µµmm

100100µµmm

Fractal like microstructure induced by cold working

Cold Workingβ(bcc)

TOYOTA CENTRAL R&D LABS., INC.

0.50.5µµmm

20nm20nm

2nm2nm

転位が見えない?

転位が転位が見えない?見えない?

Elastic Strain Elastic Strain FieldsFields

Page 24: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Cold Drawing

t = 30mm → t = 0.03mm φ = 13mm→ 3mm→ 0.3mm

Cold Worked SamplesCold Worked Samples

Cold Rolling

99% workable without annealing at R .T.       ⇒ SSuper ductility without uper ductility without              work hardeningwork hardening

TOYOTA CENTRAL R&D LABS., INC.

Page 25: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

 

多機能多機能

超弾性

超低弾性率

超強力

超塑性

エリンバー機能

インバー機能

自動車部品

精密機械部品

医療機器

人工骨

装飾品

眼鏡フレーム

航空・宇宙機器

ロボット部品

スポーツ用品

レジャー用品

Automotive Parts

Medical Equipment

Artificial Bone

Aerial & OuterInstrument

Sections of Robot

Sporting Goods

TOYOTA CENTRAL R&D LABS., INC.

Possible ApplicationsPossible Applications

Ornaments

Spectacle Frame

Precision Machinery Parts

Leisure Goods

SuperSuperMultifunctionMultifunction

Super elasticityUltralow modulusUltrahigh strength

Super plasticityElinvar propertyInvar property

Page 26: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Elastic Modulus / GPa

Tens

ile S

treng

th /

MP

a

Mg

1000

0

500

1500

0 50 100 150 200 250

2000

Gum M

etal

Alloys

AlAlloys

TiAlloys

Steels

TOYOTA CENTRAL R&D LABS., INC.

SummarySummary

TiB MMC

Page 27: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

Thank you for your Attention!Thank you for your Attention!

Page 28: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

TITANIUM 2005 21st Annual ITA Conference & Exhibition Scottsdale, Arizona

Development of Titanium Alloys with Controlled Elastic Properties

T. Furuta Toyota Central Research and Development Laboratories Inc., Nagakute, Aichi, Japan

Abstract

In this paper, the work of Toyota Central R & D Labs., Inc. regarding titanium alloys with controlled elastic properties is introduced. These alloys are (1) a TiB reinforced titanium metal matrix composite obtained via a cost-effective powder metallurgy process for automotive engine parts. We found that the TiB particle is the only ideal reinforcement which has a high rigidly, strength and thermodynamic stability in titanium alloy, and (2) Gum Metal, a new multifunctional β titanium alloy, Ti-24at%(Ta+Nb+V)-(Zr +Hf)-O, which exhibits a low elastic modulus, high strength, high elastic deformability, superior cold formability without work hardening, and both Invar and Elinvar properties over a wide temperature range. The multifunctional properties of Gum Metal must offer a wide range of applications in the emerging markets.

1 Introduction

It is well known that titanium alloys are extremely attractive materials for aeronautical, aerospace, automobile and marine applications, because they have excellent properties such as specific strength and corrosion resistance. Nowadays, applications include not only transport components but also a wide range of uses in artificial bone, implants, medical equipment, sporting goods and so on. Therefore, the development of titanium alloy with new functionality has been conducted. In particular, control of the elastic modulus is required for developing new functional and designed components. However, it is very difficult to control the elastic modulus of metals. This is because the elastic modulus of metals is related to the binding energy, and conventional metallurgical processes have no significant effects on the physical properties of metals. The reason for this is that changes that can be effected by plastic working and heat treatment occur at the microstructural level and do not extend to inter-atomic bonds or electronic states. However, we have recently discovered new titanium alloys

Page 29: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

exhibiting multiple “super properties”, by using a blended elemental (BE) method. The BE process is potentially the lowest cost titanium components manufacturing process, and furthermore it enables the production of complex materials that are difficult to make via ingot metallurgy. Metal matrix composites (MMC) and high-alloyed materials containing elements which easily segregate are typical examples.

In this article, the newly developed titanium alloys from Toyota Central R & D Labs are introduced These are (1) a TiB reinforced titanium metal matrix composite obtained via a cost-effective powder metallurgy process for automotive engine parts.[1-9] We found that the TiB particle is the only ideal reinforcement which has a high rigidly, strength and thermodynamic stability in titanium alloy.[2] The developed Ti-MMC has potential that has not been considered in conventional titanium alloys, and (2) Gum Metal, a new multifunctional β titanium alloy group, Ti-24at%(Ta+Nb+V)-(Zr+Hf)-O, which exhibits significant changes in physical and mechanical properties after cold working.[10-12] The developed β titanium alloys simultaneously show a low elastic modulus, high strength, high elastic deformability, superior cold formability without work hardening, and both Invar and Elinvar properties over a wide temperature range.[11]

2 Titanium Metal Matrix Composite (Ti-MMC)

2.1 Selection of an ideal reinforcement for Ti-MMC

While the specific strength of titanium alloy exceeds that of maraging steel, the elastic modulus of titanium alloy is approximately half that of steel. Therefore, weight savings from the use of titanium parts are not as great as expected from the difference in specific gravities between titanium alloy and steel. Additionally, further reductions in the size and weight of automotive components require elastic designing as well as conventional strength designing. In order to overcome this essential problem of titanium alloys, we attempted the development of a totally new type of high performance Ti-MMC. The first major decision for the alloy design was to select an ideal reinforcement. To use the BE method, the requirements for ideal reinforcing compounds are; (1) thermodynamic stability in titanium alloy from approximately 1600 K to room temperature, (2) high rigidity and strength, hardness and heat resistance, (3) mutual insolubility, and (4) minimal difference in thermal expansion between the matrix and reinforcing compounds. We finally decided on titanium monoboride (TiB) as the ideal reinforcement for titanium alloy. This is because TiB has a thermodynamic stability superior to that of current reinforcing compounds such as TiC, SiC, TiN, Si3N4 and TiB2. Table 1 compares the properties of reinforcing compounds for titanium alloys. TiB has outstanding mechanical properties which are desirable for an ideal reinforcement, and the linear

Page 30: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

coefficient of thermal expansion of TiB is nearly equal to that of titanium. Therefore, we selected TiB as the reinforcing compound for the titanium matrix composite.

While TiB is stable in titanium alloys, it is unstable by itself and can not be obtained in powder form. We use a boron powder or several boride powders as raw materials for forming TiB particles. During the sintering, the blended boron powder or boride powders react with titanium powder and are completely transformed to thermodynamically stable TiB particles in the titanium matrix. Due to the thermodynamic stability of the TiB, no reaction occurs around a TiB / titanium matrix boundary. A crystallographic relation is verified by electron diffraction analysis to be; (010) TiB // (001) β, <001) TiB // <110> β and the habit planes of the TiB particle are (100), (101) and (010).This result suggests that excellent crystallographic coherency is maintained at the boundary.[3] The matrix alloy can be changed and is carefully selected for the required properties of the component parts as listed in Table 2 with the master alloy powders used.[3]

2.2 Performance of the developed Ti-MMC

The elastic moduli of the developed Ti-MMC can be controlled by changing the TiB content and the matrix alloy, for example α, α+β or β-Ti alloy. Figure 1 shows changes in

TiBTiCTiNSiCSi3N4TiB2B4CAl2O3

28.024.724.025.014.734.027.522.5

8.67.49.34.33.26.44.58.1

550460250420320529449350

<0.001 1.01.2 15.0

22.0 26.0Unstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloy

ExcellentPassableFailureFailureFailureFailureFailureFailure

ParticleKnoopHardness(GPa)

ElasticModulus(GPa)

CoefficientLinear Expansion(x10-1K-1)

Maximum Solubility[Matrix] [Particle]

(at%)Estimation

Coefficient of Linear Expansion of Ti alloy is around 9x10-6 K-1

Table. 1 Adaptable of the reinforcement for BE titanium alloy.

TiBTiCTiNSiCSi3N4TiB2B4CAl2O3

28.024.724.025.014.734.027.522.5

8.67.49.34.33.26.44.58.1

550460250420320529449350

<0.001 1.01.2 15.0

22.0 26.0Unstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloyUnstable in Ti alloy

ExcellentPassableFailureFailureFailureFailureFailureFailure

ParticleKnoopHardness(GPa)

ElasticModulus(GPa)

CoefficientLinear Expansion(x10-1K-1)

Maximum Solubility[Matrix] [Particle]

(at%)Estimation

Coefficient of Linear Expansion of Ti alloy is around 9x10-6 K-1

Table. 1 Adaptable of the reinforcement for BE titanium alloy.

Ti-6Al-4V - - - - - - - - - - - - - - - - - - - - - - Al-40VTi-6Al-4V-1Mo-0.2B - - - - - - - - - - - - - - Al-40V + MoB + pure BTi-8Al-1Mo-1V - - - - - - - - - - - - - - - - - - Al-38Ti +Al-40V + pure MoTi-6Al-2Sn-4Zr-2Mo-0.2Si - - - - - - - - - - Al-14Sn-28Zr-14Mo-1.4SiTi-6.5Al-4.5Sn-4.5Zr-1Nb-1Mo-0.35Si - - - Al-25Sn-25Zr-5.6Nb-5.6Mo-1.9SiTi-5Al-12Cr-3.3V - - - - - - - - - - - - - - - - - Al-40V + pure CrTi-10V-2Fe-3Al - - - - - - - - - - - - - - - - - - Al-40V + Fe-80V (ferro-V) Ti-4.3Fe-7.0Mo-1.4Al-1.4V - - - - - - - - - Al-50V + Fe-62Mo (ferro-Mo)Ti-33.5Al - - - - - - - - - - - - - - - - - - - - - - Al-38Ti

Master Alloy PowdersMatrix Alloy (mass%)

Table. 2 Matrix alloy composition and master-alloy powders.

Ti-6Al-4V - - - - - - - - - - - - - - - - - - - - - - Al-40VTi-6Al-4V - - - - - - - - - - - - - - - - - - - - - - Al-40VTi-6Al-4V-1Mo-0.2B - - - - - - - - - - - - - - Al-40V + MoB + pure BTi-6Al-4V-1Mo-0.2B - - - - - - - - - - - - - - Al-40V + MoB + pure BTi-8Al-1Mo-1V - - - - - - - - - - - - - - - - - - Al-38Ti +Al-40V + pure MoTi-8Al-1Mo-1V - - - - - - - - - - - - - - - - - - Al-38Ti +Al-40V + pure MoTi-6Al-2Sn-4Zr-2Mo-0.2Si - - - - - - - - - - Al-14Sn-28Zr-14Mo-1.4SiTi-6Al-2Sn-4Zr-2Mo-0.2Si - - - - - - - - - - Al-14Sn-28Zr-14Mo-1.4SiTi-6.5Al-4.5Sn-4.5Zr-1Nb-1Mo-0.35Si - - - Al-25Sn-25Zr-5.6Nb-5.6Mo-1.9SiTi-6.5Al-4.5Sn-4.5Zr-1Nb-1Mo-0.35Si - - - Al-25Sn-25Zr-5.6Nb-5.6Mo-1.9SiTi-5Al-12Cr-3.3V - - - - - - - - - - - - - - - - - Al-40V + pure CrTi-5Al-12Cr-3.3V - - - - - - - - - - - - - - - - - Al-40V + pure CrTi-10V-2Fe-3Al - - - - - - - - - - - - - - - - - - Al-40V + Fe-80V (ferro-V) Ti-10V-2Fe-3Al - - - - - - - - - - - - - - - - - - Al-40V + Fe-80V (ferro-V) Ti-4.3Fe-7.0Mo-1.4Al-1.4V - - - - - - - - - Al-50V + Fe-62Mo (ferro-Mo)Ti-4.3Fe-7.0Mo-1.4Al-1.4V - - - - - - - - - Al-50V + Fe-62Mo (ferro-Mo)Ti-33.5Al - - - - - - - - - - - - - - - - - - - - - - Al-38TiTi-33.5Al - - - - - - - - - - - - - - - - - - - - - - Al-38Ti

Master Alloy PowdersMatrix Alloy (mass%)

Table. 2 Matrix alloy composition and master-alloy powders.

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the elastic modulus at room temperature for the developed Ti-MMCs with different types of matrix alloy with the TiB particle content. In each case, the elastic modulus increases linearly with increasing TiB content. It exceeds 180 GPa for 30 vol.% TiB in the β Ti matrix alloy, which is almost the same as that of stainless steel. The result is in excellent agreement with the topological transformation and mean field theory by A.P. Miodownic calculated from the elastic modulus

and Poisson ratio of titanium alloys (115 GPa and 0.27, respectively) and TiB (550 GPa and 0.19, respectively).[13] Figure 2 summarizes the tensile and fatigue strengths and wear resistance of the developed high-strength Ti-MMCs, such as 10 vol.% TiB / Ti-6Al-4V-1Mo-2Fe MMC [8] and 20 vol.% TiB / Ti-4.3Mo-7Fe-1.4Al-1.4Fe ΜΜC [6] under the post-forged-annealing condition, compared with IM β annealed Ti-6Al-4V. All of the properties of the developed Ti-MMC are far superior to those of Ti-6Al-4V alloy. The anomalous strength with the high elastic modulus means that the Ti-MMC has greater potential for weight reduction in

80

100

0 10 20 30TiB Content / vol.%

120

140

160

α+β Matrix (973K x 3.6 ks)

Ti-4.3Fe-7Mo-1.4Al-1.4Vbased MMC

β Matrix(1173K x 3.6 ks)

40

180

200E

last

ic M

odul

us /

GP

a

Ti-6Al-4V Alloy level

340 Stainless Steel level

Ti-8Al-1V-1Mobased MMC

Figure. 1 Change in Elastic modulus for the developedMMCs with TiB content.

1200

800

400

0

Ti-6

Al-4

V

開発

βTi

基M

MC

1600

2000

160

140

120

180

200

100

10

20

30

40

020vo

l%Ti

B /T

i-4.3

Fe-7

Mo-

1.4A

l-1.4

V

2200

10vo

l%Ti

B /T

i-6Al

-4V-

1Fe-

2Mo

Tensile Stress Fatigue Strength Wear Loss Elastic Modulus

Elas

tic M

odul

us /

GPa

Tens

ile S

tress

, Fat

igue

Stre

ngth

/ M

Pa

Wea

r Los

s /

mg/

km

Figure. 2 Comparison of mechanical properties of high strength developed MMCs with wrought Ti-6Al-4V alloy

1200

800

400

0

Ti-6

Al-4

V

開発

βTi

基M

MC

1600

2000

160

140

120

180

200

100

10

20

30

40

020vo

l%Ti

B /T

i-4.3

Fe-7

Mo-

1.4A

l-1.4

V

2200

10vo

l%Ti

B /T

i-6Al

-4V-

1Fe-

2Mo

Tensile Stress Fatigue Strength Wear Loss Elastic Modulus

Elas

tic M

odul

us /

GPa

Tens

ile S

tress

, Fat

igue

Stre

ngth

/ M

Pa

Wea

r Los

s /

mg/

km

Figure. 2 Comparison of mechanical properties of high strength developed MMCs with wrought Ti-6Al-4V alloy

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automotive parts than conventional titanium alloys, and the excellent wear resistance allows elimination of expensive surface treatment. The combustion temperatures of recent mass-produced engines have a tendency to be increasingly higher, due to the required emission reductions, with exhaust gas temperatures reaching 900゚C and exceeding 800゚C for the actuating temperature of exhaust valves. The exhaust valve materials need to have excellent creep resistance, fatigue strength, and oxidation resistance. Generally, Steel 21-4N, which is well known as heat resistant steel, is used for the exhaust valves of automotive engines. This material has excellent balanced characteristics including static strength, fatigue properties, creep resistance and oxidation resistance at room temperature and high temperatures (around 800゚C) in addition to being cost-effective. Figure 3 shows 0.2 proof strengths at 1073 K for the developed Ti-MMCs

reinforced by 10 vol.% TiB and the heat-resistant materials of 21-4N and Ti-1100. It is apparent that the heat resistance of the developed Ti-MMCs is superior to that of the heat-resistant materials. Figure 4 shows changes in the high-cycle fatigue strength at 1123 K for the developed heat-resistant Ti-MMC with the TiB particle content, which is one of the most essential properties for an exhaust valve. The high temperature fatigue strength of the heat-resistant matrix alloy is considerably improved by the dispersion of TiB particles. It is worth noting that even at a compounding of 5 vol.% TiB or so, it exceeds that of 21-4N steel. Figs. 2 and 3 indicate that careful selection of the matrix alloy system and TiB content for the developed Ti-MMC makes it possible to obtain heat resistance that is superior to that of typical heat-resistant steel at high temperatures beyond 1000 K.

3002001000

TiB/Ti-64

開発 β Ti 基MMC

400 500

TiB/Ti-6242S

6000.2% Proof Stress / MPa

TiB/Ti-Al-Sn-Zr-Nb-Mo-Si

TiB2/TiAl

1073K

21-4N Steel

Ti-1100

Figure. 3 Comparison of 0.2 proof high strength at 1073K for the developed MMCs with the commercial heat resistant materials.

Developed MMCs

Wrought Materials

3002001000

TiB/Ti-64

開発 β Ti 基MMC

400 500

TiB/Ti-6242S

6000.2% Proof Stress / MPa

TiB/Ti-Al-Sn-Zr-Nb-Mo-Si

TiB2/TiAl

1073K

21-4N Steel

Ti-1100

Figure. 3 Comparison of 0.2 proof high strength at 1073K for the developed MMCs with the commercial heat resistant materials.

Developed MMCs

Wrought Materials

0

100

200

300

10 10 10 10 104 5 6 7 8

1123K

10TiB5TiB

Matrix Alloy21-4N R=-1

Fatig

ue S

treng

th /

MP

a

Ti-6Al-4Sn-4Zr-1Nb-1Mo -0.2Si-0.3O based MMC

Figure. 4 Comparison of fatigue strength at 1123K for the developed MMCs with the commercial heatresistant materials.

Number of cycles / Nf

0

100

200

300

10 10 10 10 104 5 6 7 8

1123K

10TiB5TiB

Matrix Alloy21-4N R=-1

Fatig

ue S

treng

th /

MP

a

Ti-6Al-4Sn-4Zr-1Nb-1Mo -0.2Si-0.3O based MMC

Figure. 4 Comparison of fatigue strength at 1123K for the developed MMCs with the commercial heatresistant materials.

Number of cycles / Nf

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2.3 Applications of the developed Ti-MMC In October 1998, a new mass-produced public car using titanium engine valves (both intake

and exhaust) was released by TOYOTA Motor Corporation (Fig. 5). Both valves were manufactured via a newly developed cost-effective P/M forging process. Furthermore, the material for the exhaust valve is a high performance Ti-MMC.[9] Synergistic effects of the

heat-resistant matrix alloy and the reinforcement particles (TiB) achieve the excellent mechanical properties of the developed Ti-MMC. The ideal composition of the matrix alloy was determined to be Ti-6Al-4Sn-4Zr-1Nb-1Mo-0.2Si-0.3O, taking into consideration the high temperature creep, fatigue and oxidation resistances. In addition, taking into consideration the ductility, hot formability and machinability, which are essential to the component production in addition to the heat resistance, the ideal amount of TiB particle was determined to be 5 vol.%. A new engine installed with these valves had a valve weight that was 40% less and a valve spring that was 16% less than that for an engine installed with

conventional steel valves. As a result, the maximum revolution increased by 700 rpm and the noise in the high revolution range decreased by 30%. Moreover, the reduction in friction reduced the camshaft driving torque by 20%, and high performance and low fuel consumption were achieved. Last year, in 2004, more than 250000 of the developed Ti-MMC valves were produced as automotive and motorcycle engine valves on the Japanese market (Fig. 6).

Figure 5. The Toyota Alltezza, 1998 Japanese Car of the Year, the first familyautomobile in the world to feature titanium intake and exhaust valves.

Figure 6. The developed BE titanium intake valve (left) and Ti-MMC exhaust valve (right).

Page 34: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

3 Multi Functional Titanium Alloy

3.1 Design of low elastic modulus titanium alloy We have recently developed a multifunctional β titanium alloy, Gum Metal,[10] that exhibits

a low elastic modulus with high strength, by using the BE method and a new alloy design method. From literature and experience, the elastic modulus of titanium alloy takes a minimum value near the composition limit of the bcc phase. It is also well known that several electronic parameters, such as (i) the valence electron number (e/a); (ii) the bond order (Bo value), and (iii) the "d" electron-orbital energy level (Md value), [14] are strongly related to the phase stability. However, there have been few attempts to theoretically compute and predict elastic moduli of titanium-based alloys. We first calculated elastic moduli using the ultra-soft pseudo-potential method within a generalized gradient approximation to the density function theory, and found a new method for theoretical calculation.[15] This new theoretical calculation can accurately predict the elastic modulus by calculating elastic constants (c11, c12, c44) of Ti-X binary alloy systems (X=V, Nb, Ta, Mo and W). From the calculation results, we found that (c11-c12) is correlated with the averaged valence electron number (e/a), and the value (c11-c12) approaches zero when an e/a is close to 4.24. The results also indicate that the polycrystalline elastic modulus of Ti-X binary alloys attains a minimum value with an e/a of around 4.24. So, we are quite sure that an e/a of around 4.24 is one of the most important requirements in the design of a low-elastic modulus titanium alloy. Next, we experimentally investigated the efficient group IVa elements, which improve the strength of the alloy without increasing the elastic modulus, allowing changes in Bo and Md while maintaining an e/a of 4.24. We finally reached an optimum combination of these three electronic numbers; an e/a of around 4.24; a Bo of around 2.87; and an Md of around 2.45. The unique properties such as low elastic modulus, high strength and cold-workability only appear when all three of these magic numbers are satisfied simultaneously, and each alloy system requires significant cold working and the presence of a certain amount of oxygen, at least 0.7 at%. The composition of the developed alloy is fundamentally expressed as Ti-24 at% (Ta+Nb+V)-(Zr, Hf)-O. Various alloy compositions are available, such as Ti-23Nb-0.7Ta-2Zr-O and Ti-12Ta-9Nb-3V-6Zr-O (in at %), wherein each alloy has a simple body-centered-cubic (bcc) crystal structure. 3.2 Mechanical properties of Gum Metal

The unique characteristics of Gum Metal are developing by cold working. Figure 7 shows a change in tensile stress-strain curve at room temperature with cold working for a typical alloy, Ti-23Nb-0.7Ta-2Zr-1.2O. The elastic modulus drops dramatically as a result of the cold working, from 70 GPa to 55 GPa, at near-zero stress, and the yield stress increases after cold working. We can confirm non-linearity in elasticity for the cold-worked specimen, with the

Page 35: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

gradient of the stress-strain curve in the elastic region continuously decreasing with a stress increase. Figure 8 shows changes in elastic properties, such as elastic limit strength, average elastic modulus and attainable elastic strain. Here, the average elastic modulus is the average value of the gradients during non-linear elasticity. The attainable elastic strain of the solution treatment material is about 1% and increases to 2.5% after 90% cold working. The average elastic modulus decreases with increasing cold working ratio, this downward trend is unsurpassed and decreases to below 40 GPa at 90% cold working.

It is well known that the large elastic strain obtained in "super-elastic alloys" originates from a reversible martensitic transformation, such as stress-induced α" transformation, dubbed "pseudo-elastic deformation".[16, 17] Conversely, Gum Metal shows a quite unique elastic behavior with no hysteresis in the stress-strain relation, as seen in Fig. 7, which is inherent in conventional super-elastic alloys. We confirmed by in-situ XRD measurement during tensile loading that all β peaks shift monotonically to higher 2θ angles with increasing tensile strain up to 2.7%. This result suggests that no phase transformation such as stress-induced

α" or rearrangement of variants of α" occurs during tensile deformation, and that the true elastic deformation of β crystal proceeds in Gum Metal.[11]

Oxygen content, as well as cold working, influences the elastic properties of multifunctional alloys. Figure 9 shows effects of oxygen content on the attainable elastic strain and the elastic modulus of the Ti-23Nb-0.7Ta-2Zr-O

Tensile Strain / %

As Annealed

Non-L

inear

Elas

ticity

600

1000

1400

Tens

ile S

tress

/ M

Pa

1200

800

400

200

00 1 2 3 4 5

Elastic Limit90% Cold Worked

1600

Ti-23Nb-0.7Ta-2.0Zr-1.2O

Figure. 7 Change in stress-strain curve of Ti-23Nb-0.7Ta-2.0Zr-1.2O alloy before and after cold working.

Tensile Strain / %

As Annealed

Non-L

inear

Elas

ticity

600

1000

1400

Tens

ile S

tress

/ M

Pa

1200

800

400

200

00 1 2 3 4 5

Elastic Limit90% Cold Worked

1600

Ti-23Nb-0.7Ta-2.0Zr-1.2O

Figure. 7 Change in stress-strain curve of Ti-23Nb-0.7Ta-2.0Zr-1.2O alloy before and after cold working.

Cold Working Ratio / %

60

100

140

Ela

stic

Mod

ulus

/ G

Pa

120

40

20

00 20 40 60 80 100

1.5

2.5

3.0

2.0

1.0

0.5

0

Ela

stic

Lim

it st

reng

th /

MPa

600

1000

1400

1200

800

400

200

0

Atta

inab

le E

last

ic S

train

/ M

Pa

Elastic Limit Strength

Elastic Strain

Average Elastic Modulus

80

Ti-23Nb-0.7Ta-2.0Zr-1.2O

Figure. 8 Change in elastic properties and elastic limit strength with cold working ratio.

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alloy before and after cold working with a 90% reduction in area. The attainable elastic strain increases with increasing oxygen content and is enormously accelerated by the cold working. That of the cold-worked alloy is only 1% at a lower oxygen level (0.3 mol%), but it increases to 2.5% at around 1 mol% oxygen. The elastic modulus gradually increases with increasing oxygen content. That of the cold-worked alloy at 3 mol% oxygen is about 70 GPa, which is still a small value for a titanium alloy. It can be seen from Fig. 9 that both oxygen addition and cold working are

fundamental for achieving a low elastic modulus with high attainable elastic strain. Additionally, the effect of oxygen content on the tensile strength is remarkable; it reaches 1600 MPa at 3 mol% O. The strength increases to approximately 2100 MPa after the aging treatment. The ductility maintains a very high value, exceeding 40% even at 3 mol% O. Furthermore, an important point to emphasize is the fact that the heat-treated alloy maintains a reduction in area of 10 % along with an ultra-high strength of more than 2000 MPa.[11]

3.3 Applications of multifunctional titanium alloy Gum Metal

Cold-workability is an important factor for practical applications. Figure 10 shows the effects of cold working on hardness and reduction in area. The Vickers hardness and the reduction in area of the multifunctional alloy both remain approximately constant regardless of the cold working ratio. On the other hand, the hardness of the conventional β titanium alloy gradually increases with an increasing cold working ratio. This suggests that the multifunctional alloy has super-plastic like deformability at room temperature without any work hardening. Figure 11 shows an example of the cold-worked samples. Since the alloy does not show work hardening after cold working, continuous deformation without annealing is possible to more than 99.9% under any kind of cold working, such as formation of a round bar, wire or thin sheet. Namely, no amount of plastic deformation at room temperature causes work hardening or decreased ductility, which is a nifty property for the practical use of Gum Metal.

Gum Metal, which has various unique characteristics that set it apart from other metals, is a

0

1.0

0 1 2 3Oxygen Content / mol.%

Atta

inab

le E

last

ic S

train

/ %

80

Ela

stic

Mod

ulus

/ G

Pa

604020

2.0

3.0

4.0

0

100

Cold Working

Cold Working

Elastic Strain

Ti-23Nb-0.7Ta-2.0Zr

Elastic Modulus

Figure. 9 Change in elastic properties oxygen content and cold working.

0

1.0

0 1 2 3Oxygen Content / mol.%

Atta

inab

le E

last

ic S

train

/ %

80

Ela

stic

Mod

ulus

/ G

Pa

604020

2.0

3.0

4.0

0

100

Cold Working

Cold Working

Elastic Strain

Ti-23Nb-0.7Ta-2.0Zr

Elastic Modulus

Figure. 9 Change in elastic properties oxygen content and cold working.

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totally new material that has infinite possibilities for practical applications. Figure 12 shows examples of (a) a spectacle frame and (b) precision screws. The spectacle frame made from Gum Metal is very flexible, with supreme die-press formability. The material for precision screws is required to have extreme cold formability with high strength. The properties of Gum Metal are optimal for this use, and furthermore, the elastic property prevents the screws from coming loose. They are already on

the market in Japan. Each function or complex function of Gum Metal will provide a wide range of applications for automotive components, artificial bone, implants, medical equipment, sporting goods, decorative materials and aerial and outer space instruments in the near future (Figure 13).

Conventional β-Titanium Alloy(TI-15V-3Al-3Cr-3Sn wt%)

Cold Working Ratio / %

Reduction in Area

Tens

ile S

tress

/ M

Pa

300

200

100

00 20 40 60 80 100

Hardness

400

Ti-23Nb-0.7Ta-2.0Zr-1.2O 20

40

60

80

0

Red

uctio

n in

Are

a /

%Figure. 10 effect of cold working on hardness and reduction in area.

Conventional β-Titanium Alloy(TI-15V-3Al-3Cr-3Sn wt%)

Cold Working Ratio / %

Reduction in Area

Tens

ile S

tress

/ M

Pa

300

200

100

00 20 40 60 80 100

Hardness

400

Ti-23Nb-0.7Ta-2.0Zr-1.2O 20

40

60

80

0

Red

uctio

n in

Are

a /

%Figure. 10 effect of cold working on hardness and reduction in area.

Figure 11. Example of the cold worked samples.

t = 30mm → t = 0.03mm φ= 13mm→ 3mm→ 0.3mm

Figure 11. Example of the cold worked samples.

t = 30mm → t = 0.03mm φ= 13mm→ 3mm→ 0.3mm

Figure 12. Demonstrates example of (a) a spectacle frame and (b) precision screws.

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4 Summary

We have developed high performance TiB reinforced Ti-MMC and a multi functional titanium alloy, Gum Metal, by using the BE method. These materials could not be manufactured via conventional ingot metallurgy.

TiB reinforced Ti-MMC has remarkable properties such as high rigidity, high strength (both tensile and fatigue), and superior heat resistance and wear resistance. All these superior properties are attributed to the characteristics of TiB, such as thermodynamic stability in titanium alloy, and outstanding mechanical and physical properties. We found that the TiB particle is the only compound that satisfied the requirements for ideal reinforcement of titanium matrix alloy. Gum Metal simultaneously possesses multi functions such as a low elastic modulus (40 GPa), high strength (more than 1100 MPa), high elastic deformability (2.5%), super-plastic like deformability at room temperature without work hardening, and Invar and Elinvar properties.

The developed alloys bring many new possibilities to titanium technology. For example, the anomalous strength with high elastic modulus means that Ti-MMC has a greater ability for weight reduction in automotive parts than conventional titanium alloys. The multifunctional properties of Gum Metal will provide a wide range of applications for automotive components, artificial bone, implants, medical equipments, sporting goods, decorative materials and aerial and outer space instruments in the near future.

Sporting Goods

Automotive Parts Spectacle Frame

Medical Equipment

Ornaments

Artificial Bone

Precision Machinery Parts

Aerial & Outer Space Instrument

Sections of Robot

Leisure Goods

SuperSuperMultifunctionMultifunctionSuper elasticity

Ultralow modulusUltrahigh strengthSuper plasticityElinvar propertyInvar property

Figure 13. Possible applications of Gum Metal.

Page 39: Development of Titanium alloy with Controlled Elastic Properties · 2018-04-14 · Development of Titanium Alloys with Controlled Elastic Properties T. Furuta Toyota Central Research

5 References

[1] T. Furuta and T. Saito, Current Advances in Material and Processes, ISIJ, 4 (1991), pp. 1739. [2] T. Saito and T. Furuta and T. Yamaguchi, in: K. Kishi, N. Takeda and Y. Kagawa (Eds.), Proc. Conf. 3rd Japan Int. SAMPE Symposium, SAMPE, Tokyo, 2, 1993, pp. 1810. [3] T. Saito, T. Furuta and T. Yamaguchi, in: F. H. Froes and J. Storer (Eds.), Recent Advances in Titanium Metal Matrix Composites, TMS, Warrendal, 1995, pp. 33. [4] T. Saito, Advance Performance Materials, 2 (1995), pp. 121. [5] T. Saito, H. Takamiya and T. Furuta, in P. A. Blenkinsop, W. J. Evance and H. M. Flower (Eds.), Titanium 95, IoM, 4, London, 1995, pp. 2859. [6] T. Saito, H. Takamiya and T. Furuta, Mater. Sci. and Eng. A, 243 (1998), pp. 273. [7] T. Furuta, T. Saito and H. Takamiya, Current Advances in Material and Processes, ISIJ, 10 (1997), pp. 1337 [8] T. Furuta, T. Yamaguchi, Y. Shibata and T. Saito, in I.V. Gorynin and S.S. Ushkov (Eds.), TITANIUM ’99 Science and Technology, CRISM “PROMETEY”, Russia, 2000, pp.1917. [9] T. Yamaguchi, H. Morishita, S. Iwase, S. Yamada, T. Furuta and T. Saito, SAE Transaction J. of Material and Manufacturing Section 5 vol. 109 (2000), pp 416. [10] T. Saito, T. Furuta, J. H. Hwang, S. Kuramoto, K. Nishino, N. Suzuki, R. Chen, A. Yamada, K. Ito, Y. Seno, T. Nonaka, H. Ikehata, N. Nagasako, C. Iwamoto, Y. Ikuhara and T. Sakuma, Science, 300 (2003), pp. 464. [11] T. Furuta, K. Nishino, J. H. Hwang, A. Yamada, K. Ito, S. Osawa, S. Kuramoto, N. Suzuki, R. Chen and T. Saito, in: G. Lutjering, J. Albrecht (Eds.), Ti-2003 Science and Technology, WILEY-VCH, Weinheim, 2004, pp. 1519. [12] S. Kuramoto, T. Furuta, J. H. Hwang, Y. Seno, T. Nonaka, H. Ikehata, N. Nagasako, K. Nishino, T. Saito, C. Iwamoto, Y. Ikuhara and T. Sakuma, in: G Lutjering, J. Albrecht, (Eds.), Ti-2003 Science and Technology, WILEY-VCH, Weinheim, 2004, pp. 1527. [13] Z. Fan, A.P. Miodownik, L. Chandrasekaran and M. Ward-Close, J. of Materials Science, 29 (1994), pp. 1127. [14] M. Morinaga, N. Yukawa, T. Maya, K. Sone and H. Adachi, in: P. Lacombe, R. Tricot, G. Béranger (Eds.), Sixth World Conference on Titanium 1988, Les Editions de Phisique, Les Ulis Cedex, 1989, pp. 1373. [15] H. Ikehata, N. Nagasako, T. Furuta, A. Fukumoto, K. Miwa and T. Saito, Phys. Rev. B, 70 (2004), pp. 174113-1 [16] C. Baker, Metal. Sci. J., 5 (1971), pp. 92. [17] T. W. Duerig, J. Alberecht, J. Richter and P. Fischer, Acta Metall, 30 (1982), pp. 2161.