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OAK RIDGE NATIONAL LABORATORY U. S. DEPARTMENT OF ENERGY Mo-Si-B Alloy Development J. H. Schneibel Metals and Ceramics Divison, ORNL R. O. Ritchie, J. J. Kruzic Materials Science Division, LBNL 17 th Annual Conference on Fossil Energy Materials Baltimore, MD, April 22-24, 2003.

Mo-Si-B Alloy Development Library/Events/2003/materials... · Mo-Si-B Alloy Development ... •Simple crystal structures ... Determine compressive stress-strain curves at a strain

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OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Mo-Si-B Alloy Development

J. H. SchneibelMetals and Ceramics Divison, ORNL

R. O. Ritchie, J. J. Kruzic Materials Science Division, LBNL

17th Annual Conference on Fossil Energy Materials Baltimore, MD, April 22-24, 2003.

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Why Ultra-High Temperature Materials?Vision 21 is about EFFICIENCY:Service temperature ↑ Efficiency ↑

Nickel-base superalloys: ≤ 1000ºCODS ferritic steels: up to 1400 º C(but low strength and high stress exponent)

Need ultra-high temperature, high strength materialsBest effort, high risk researchLong lead time from research to production (20 years)

Applications: sensor protection, heat exchangers, 1st stage vanes

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Ultra-High Temperature MaterialsBarriers: •Melting point•Oxidation resistance•Fracture toughness•Creep strength

Options:•Simple crystal structures – expensive (Pt, Ir)•Complex crystal structures – brittle

Scientific approach:macro- and microalloying Innovative processing to create optimum microstructure

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Why Mo-Si-B Alloys?

0.0 0.1 0.2 0.3 0.4 0.5

0.5

0.6

0.7

0.8

0.9

1.0 0.0

0.1

0.2

0.3

0.4

0.5

Molybd

enum BoronMo5SiB2

Mo3Si Mo5Si3Mo

•Melting point ≈2000ºC•High strength intermetallics•Equilibrium phases•Oxidation resistance: MoSi2•Toughening: metallic Mo phase

Berczik Akinc

Silicon

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Mo-Si-B alloys are finding interest

Molybdenum-Borosilicide WorkshopOrganized by Airforce, Navy, Pratt&WhitneyAnnapolis, Maryland, March 11 and 12, 2003

TMS Symposium “Beyond Nickel-Base Superalloys”Charlotte, NC, March 14-18, 2004

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Strategy for improving the mechanical properties

of Mo-Si-B Intermetallics

Unlikely that intrinsic brittleness of Mo3Si and Mo5SiB2can be alleviated in the near future

Engineer microstructure to minimize detrimental effect of brittle phases

Focus of this talk on:Microstructure topology and scaleMechanical properties of α-Mo

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

A sucessful microstructure for creep:nickel-base superalloys

CMSX-4

Single crystal superalloy

(Kazim Serin, Post-Doc at ORNL)

Continuous γ solid solution matrixCreep occurs in the γ channels between γ’ (Ni3Al) precipitates

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Optimizing Fracture Toughness

•High α-Mo volume fraction

•Continuous α-Mo

•Coarse α-Mo

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Mo-12Si-8.5B (at. %) cast&annealed (24h/1600ºC)≈40 vol. % discontinuous α-Mo

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Crush cast Mo-Si-B and “coat” powder with Mo

Evaporation of Si and/or: Mo3Si + 1/2O2 SiO↑ + 3 Mo

Mo5SiB2 + 1/2 O2 SiO ↑ + 2 Mo2B + Mo

Mo-20Si-10B powder particle after 16 h at 1600°C in vacuum

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Hot isostatic pressing of Mo-Si-B powderin niobium can (4h/1600°C/30ksi)

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

HIPed Mo-Si-B with continuous α-Mo matrix:nominal composition Mo-15Si-10B; 30 vol.% α-Mo.

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Mo-Si-B alloys with continuous α-MoHIPed from Si-evaporated Mo-20Si-10B

545-90 µmMedium_Low4990-180 µmCoarse3445-90 µmMedium

34≤ 45 µmFine

α-Mo volume fraction, %

Powder size prior to Si semoval

Specimen Designation

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Tensile Testing of Buttonhead Specimensat 3.3×10-3 s-1

Room temperature:premature fracture at 140 MPa:Need to eliminate flawsMo matrix needs improvement

1200ºC in vacuum:0.2% yield stress 336 MPamaximum stress 354 MPaductility 1.8%

“Coarse” microstructureContinuous α-Mo matrix

49 vol. %

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Creep strength

Determine compressive stress-strain curves at a strain rate of 10-5 s-1

Define creep strength as flow stress at 2% plastic strain

0

100

200

300

400

500

600

0 2 4 6 8 10 12 14

Stre

ss, M

Pa

Strain, %

Mo-9.5Nb-12Si-8.5B1300C

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Creep Strength at 1300°C(10-5 s-1, 2% plastic strain)

0

100

200

300

400

500

600

Cre

ep S

treng

th, M

Pa

Cast&annealed40 vol. % α-Mo(discontinuous)

Fine34 v/o α-Mo

Medium34 v/o α-Mo

Medium_Low5 v/o α-Mo

Coarse49 v/o α-Mo

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Rigorous Fracture Toughness Testing

•Disc-shaped compact tension specimens

•Fatigue pre-cracking

•Cycling at low stress intensity:

remove bridging in crack wake

•Crack length from elastic compliance

•Determine resistance curve (R-curve)(Crack-growth resistance KR vs. crack extension ∆a

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Room Temperature Fracture Toughness

0

5

10

15

20

25

0 0.5 1 1.5 2 2.5 3

Stre

ss In

tens

ity, M

Pa m

1/2

Crack Extension, mm Mo-12Si-8.5B40 vol% α-Mo

“medium”34 vol% α-Mo

“coarse”49 vol% α-Mo

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

What can we do to improve toughening efficiency of α-Mo?High toughening efficiency

less α-Mo, better oxidation resistance

• α-Mo ligaments < 1 µm

• Microalloying of α-Mo

• Ductilization of α-Mo by spinel particles

(Mike Brady: chromium)

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Fe-40 at. % Al/TiC:FeAl fractures usually by cleavage;Fracture mode of FeAl ligaments depends on thickness

Fracture stress of FeAl ligament: 500 MPa1 dislocation in pile-up: L=Gb/[πτ(1-ν)]=30 nm70 dislocations in pile-up: ideal cleavage stress for L=2 µmExpect ductile fracture for ligaments < 2 µm

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

FeAl ligaments show ductile fracture for thickness less than 2 µm:

Size scale important for fracture toughness

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Additions of Ti and Zr improvethe ductility and strength of Mo ( TZM):Try this approach with Mo-Si-B alloys

Screening tests:

Flexure tests with chevron-notched specimens

G=W/AKq=[(E×G)/(1-ν2)]1/20

0.005

0.01

0.015

0.02

0.025

0.03

0 0.02 0.04 0.06 0.08 0.1

Load

, kN

Displacement, mm

4 mm

3 mm

notch

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Zr additons improve room temperature fracture toughness,

probably by improving properties of α-Mo

0

2

4

6

8

10

12

14

Mo-12Si-8.5B Mo-12Si-8.5B-1.5Ti Mo-12Si-8.5B-1.5Zr

K q, MPa

m1/

2

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Ductilization of Mo by adding spinel particles (MgAl2O4)

M. P. Brady recently revisited the Scruggs mechanism(1965) for the ductilization of Cr by spinel particles

Scruggs showed that mechanism works for Mo as well

Consolidate Mo powder (2-8 µm) and 3.4 wt% MgAl2O4spinel powder (1- 5 µm) in graphite hot-press:4h/1800°C/20MPa/vacuum

Carry out room temperature flexure tests

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Ductilization of molybdenumby spinel particles (MgAl2O4)

Optimum particle size and volume fraction?Collaboration with Bruce Kang, WVU

OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY

Summary and Conclusions

•Processing of Mo-Mo3Si-Mo5SiB2 with continuous α-Mo matrix•Control of microstructural scale and α-Mo volume fraction•Limited tensile ductility at 1200C•Qualitative correlation between microstructure and creep strength•High room temperature fracture toughness & R-curve behavior•Zr microalloying additions improve fracture toughness•Spinel particles improve ductility of Mo

Future work: Continue to focus on the mechanical properties of α-Mo phase