Uniaxial and Multiaxial Plastic Deformation of Large Niobium Grains Thomas Gnäupel-Herold1,2, Adam Creuziger, T.Foecke3 of Maryland Center for Neutron Research 3NIST Metallurgy Division 2NIST 1University Formability: strain localization on grain boundaries up to 0.5 mm displacement found between neighboring grains Plastic Properties of Niobium BCC Crystal Structure < 111 > slip direction (close-packed direction) Any plane containing < 111 > is a potential slip plane Experimentally observed in (110), (112) & (123) planes Tensile Tests Orientations Tensile Tests 111 250 S1 S2 S3 S4 S5 S6 S7 S8 S9 S10 S12 S13 S14 S15 S5 S16 S4 S6 true stress [MPa] 200 S3 S2 S1 S9 S14 100 150 S10 S7 S12 S13 S8 S17 110 100 50 0 0 0.2 0.4 0.6 strain 0.8 1 Yield Stress Polycrystal Single crystal YS between 25 MPa and 40 MPa weak anisotropy 25% YS of polycrystal R-Values w R t R-values 1.2 1.0 R 0.8 0.6 0.4 0.2 0.0 g1 g2 g3 g4 g5 g6 g7 g8 g9 g10 g12 g13 g14 g15 P1 P2 P3 Specimen Extreme anisotropy from r=0 (thinning only) to r>1 (no thinning) Polycrystal r=0.1 Large r-values for {210}<-120> Effect of Annealing 250 120 (1),<100>,1000C (3) (2),<111>, 1000C (3),<110>,1000C (2) true stress [MPa] true stress [MPa] 200 (1) (4),<211>, 700C (5),<100>, 700C 150 (2) 100 (4) 50 80 (1) (5) (4) 40 (5) (3) 0 0 0 0.2 0.4 0.6 0.8 1 0 0.01 strain •Yield stress and yield drop increase with annealing temperature 0.02 0.03 strain 0.04 0.05 Sample prep for multiaxial tests Multi-axial Testing A - Uniaxial Test B - Uniaxial Test, 90 deg rotated C - Balanced Biaxial Test D - Plane Strain localization E - Plane Strain, 90 deg. rotated E – Plane Strain EBSD: Misorientations at the tri-junction •Slip lines and smallangle grain boundaries •Diffuse slip, most likely from rapidly changing strain gradients leading to succession of activation/deactivation of localized slip systems Analysis of present data What is known …. What is needed … Slip systems that are Full strain rate locally active at a tensor at every point given point in time on the sample and in time orientations Taylor’s model Imposed strain rate tensor ε11 ε 12 ε 2 ε 13 2 ε 12 2 ε 22 ε 23 2 - ε 11 ε 22 ε 13 2 ε 23 2 Write the strain rate tensor as a γ α α α α α ε m n n m α 2 combination of all the slip systems Conclusions 5 Multi-axial straining tests of tri-crystal plates with identical orientation performed Local strain rate data collected Orientation analysis with EBSD GOAL: determination of locally active slip systems for any given moment