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Title: Dynamic Consolidation of TaC and NanoYSZ Powders


1
Dynamic Consolidation of TaC and Nano-YSZ Powders
SAMPE 2006 Long Beach April 30 May 4, 2006
Presenter Bhaskar Majumdar
  • L. Xu, B.S. Majumdar
  • New Mexico Institute of Mining and Technology,
    Socorro, NM
  • D. Merchant
  • A.F. Research Laboratory, Edwards AFB,CA
  • L. Matson
  • A.F. Research Laboratory, WPAFB, OH

2
Introduction
  • Tantalum carbide (TaC) has the second highest
    melting point (3880C) of known solids, offering
    strong promise in ultra high temperature
    applications. Also, it is electrically
    conductive, and can be electric discharge
    machined (EDM) to complex shapes.
  • However, the high temperatures needed for powder
    consolidation (1900 - 2500C) leads to rapid
    grain growth. This has significant detrimental
    effect on fracture toughness and strength of TaC.
    Therefore, there is a need for an alternate
    processing method for consolidating TaC.
  • Dynamic or shock wave consolidation has the
    advantage that high pressures (5 - 60 GPa) can be
    generated reasonably easily, although for a few
    microseconds. This high pressure, combined with
    temperatures that can reach 1500C (due to
    friction), can be used to consolidate ceramic
    materials.
  • Previous work has shown that the residual strain
    induced during consolidation also has the
    beneficial effect of reducing the temperature
    required for any after-shock sintering treatment,
    aimed at densification and removing
    porosity/defects.

3
Research Objective
  • The objective of this research is to evaluate
    shock wave consolidation as a method to fabricate
    TaC with fine grain size.
  • The high temperature generated during shock wave
    has created strong interparticle bonding so that
    fracture surface is featured with intergranular
    fracture. Therefore, the shock-wave consolidated
    materials may have comparable fracture toughness
    with other structural ceramics, such as SiC and
    Si3N4.
  • Nano-size yttria stabilized zirconia (YSZ) is
    also studied in this investigation, to evaluate
    the potential of shock consolidation to produce
    nano-bulk ceramics. In particular, nano-YSZ
    offers the potential of shaping by plastic
    deformation (like metals) at relatively low
    temperatures.
  • It may also be noted that the consolidation of
    nano-size particles is difficult since they have
    more surface areas and higher friction in
    packing, therefore, unable to reach high green
    density. Shock wave consolidation offers a way
    to obtain high green density for such materials.

4
Determination of the Pressure Need for the
Consolidation
TaC H 15 GPa YSZ H 12 GPa
TaC P 20 GPa YSZ P 18 GPa
1 kg/mm20.01GPa
From Meyers et al., in Shock Waves for Industrial
Applications, Eds Murr et al., (1988)
5
Experimental Materials
  • TaC
  • Micron-size TaC, purity, 99.95, diameter, d
    1 µm. Supplier Inframat Advanced Materials LLC.
    Most of the results in this presentation are for
    this material.
  • YSZ
  • Yttria Stabilized Zirconia (YSZ), d 30 - 60 nm,
    Supplier Inframat

Left image Inframat TaC As-received, SEM image
Right image Inframat TaC After Ball Milling
6
Experimental Setup
  • A double-tube setup was selected for the shock
    consolidation process. This method provides a
    longer duration pulse.
  • A lower pressure reduces the magnitude of
    reflected tensile pulses, thus reducing chances
    of cracking.
  • The cylinders containing the powders were
    evacuated from the bottom, through pre-drilled
    hole, prior to shock consolidation.

7
Experimental Procedures
  • Powders were packed in double-wall steel
    containers, evacuated at room temperature and in
    some case at 250 C, then subjected to explosive
    consolidation.
  • Some samples were heat-treated at 1100 C after
    shock wave consolidation.
  • The microstructure and fracture surfaces of
    samples were examined using FESEM and optical
    microscopy.
  • Vickers hardness measurements were used to assess
    the magnitude of consolidation. A value of 15
    GPa is characteristic of fully dense TaC.
  • Results showed that the extent of consolidation
    depended on axial position along the cylinder.
    Crack free material, combined with fairly high
    density, was observed in the mid-length region of
    the cylinders.

8
Macroscopic View of the Billets
  • The caving in of the double wall region
    corresponds to the densification of the billets
  • The powders were nearly fully dense at the bottom
    of the billets

Consolidation
Densified Region
9
Microstructures of Consolidated TaC
  • The hardness near the bottom of the sample is
    14.5 GPa (fully dense TaC, 15 ? 0.5 GPa).
  • This bottom region also contains cracks.
  • The fracture toughness was measured as 4.8 MPavm
    (structural SiC and Si3N4 have a value between 4
    and 6 MPavm).

10
Middle Part of the Billets
  • The density at half around the consolidated
    billets is 11.6 g/cm3, 83 of theoretical
    density. Hardness test gave a value of 4.8 GPa.
  • The region is fracture free. Three bend bars have
    been machined from the billets of this region.
  • Residual strain has been generated inside powders
    in the billets. The observed XRD line broadening
    has verified this effect. This middle region can
    be sintered or HIPed at much lower temperature.

As received
After shock
11
Calculations related to the residual stain stored
in the TaC powders
  • From GSAS software analysis on XRD data, the
    residual stain stored in the TaC powders can be
    obtained as 2.4 x 10-3.
  • The Faulkners formula gives the energy stored in
    the powders,E, Youngs modulus, ?, Poissons
    ration. e, residual stain. The energy is
    calculated as 320 J/mol.
  • The activation energy of TaC is 380 kJ/mol. Even
    though the strain induced energy is small, the
    diffusion coefficient will increase largely
    because of its exponential form.

12
After Consolidation Heat-treatment
  • Heat-treatment was conducted at 1100 C for the
    middle part of the billets. A thin strip of high
    reflectivity with a golden color could be
    observed around the periphery of the sample.
  • The width of the strip is 50 µm and 130 µm for
    the 6 hr and 24 hr heat-treatment sample,
    respectively. The hardness at the strip of the 24
    hr sample is 11 GPa and interior is 6.4 GPa.
  • The densification at such a low temperature
    indicate that diffusion controlled sintering is
    easier after shock-wave consolidation processing.

Sample
Mount
Layer
100 mm
24 hr sample
13
Characterization of the YSZ billet
  • Microstructure of at the bottom of the YSZ billet
    shows no features and a smooth surface (left
    image).
  • the fracture surface revealed transgranular
    fracture that spanned across many particle sizes.
    The surface exhibits typical cleavage type
    fracture (right image).
  • Hardness of the region is 9.7 GPa, quite
    comparable to the theoretical value, 12 GPa.

14
Summary
  • Dynamic consolidation trials of TaC powders (from
    Inframat) indicate promise, and confirm that the
    double-tube method is a good approach for
    consolidating TaC powders.
  • Cracking has been absent in the mid-length of the
    billets, although the density there is only 83
    of theoretical density. Heat treatments in argon
    at 1100C suggest that sintering may be active at
    this low temperature around the periphery of the
    sample. The hardness there reached approximately
    11 GPa, comparable to a hardness of 15 GPa of
    fully dense TaC.
  • The consolidation trial with YSZ was quite
    successful, in spite of a low tap density. The
    hardness of 9.7 GPa HV in the bottom region was
    comparable to literature values of 12 GPa.
    Fracture surfaces revealed transgranular fracture
    that spanned many individual YSZ particles, and
    confirmed consolidation of the nano YSZ.

15
Acknowledgement
  • This work has been funded by the Air Force
    Research Laboratory at Edwards Air Force Base,
    contract number FA9300-05-M-T013.
  • The shock wave explosive consolidation test was
    accomplished at Energetic Materials Research and
    Testing Center (EMRTC) of New Mexico Institute of
    Mining and Technology. Mr. Tony Zimmerly offered
    generous help for the experimental setup.

16
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