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Copper nanoprecipitates in steel studied by atom probe tomography and ab initio based Monte Carlo simulation O. Dmitrieva, P.-P. Choi, T. Hickel, N. Tillack,  D. Ponge, J. Neugebauer, D. Raabe Düsseldorf, Germany WWW.MPIE.DE d.raabe@mpie.de Thanksto:  DFG MRS Fall Conference    30. November 2010     Dierk Raabe
Overview ,[object Object]
Fe-3%Si-1% (2%) Cu model system
Fe-3%Si-Cu engineeringalloy
Simulations (DFT + kMC, model system)
ConclusionsandchallengesRaabe: Adv. Mater. 14 (2002), Roters et al. Acta Mater.58 (2010)
2 Motivation Avoiduseof permanent magnetsanduseinsteadelectricalmagnets in synchronouselectricalengines High strength soft magneticsteels in carenginesreduce CO2emission www.mpie.de
3 Electrical steels for electrical cars
4 Electrical steels Standard soft magnetic steel: based on  Fe3 wt. % Si   ferriticphase, coarse grains  soft-magnetic properties Improvement of the mechanical strength!  precipitation hardening: 1-2 wt. % Cu, aging at 450°C
5 {Jäniche et al., Werkstoffkunde Stahl} 0,1 µm 0,2 µm 0,3 µm 20 nm Nano-precipitates in soft magnetic Fe-3%Si steels magnetic loss (W/kg) 15 nm size Cu precipitates (nm) {JP 2004 339603} nanoparticlestoosmallfor Bloch-wall interaction but  effectiveasdislocationobstacles mechanicallyvery strong soft magnetsformotors Fe-Si steelwithCu nano-precipitates
Overview ,[object Object]
Fe-3%Si-1% (2%) Cu model system
Fe-3%Si-Cu engineeringalloy
Simulations (DFT + kMC, model system)
Conclusionsandchallengeswww.mpie.de
7 Precipitation hardened materials Precipitation hardened electrical steels:  nucleation of copper precipitates in iron-silicon matrix Fe Si 3 wt. % Cu 1 wt. %  Fe Si 3 wt. % Cu 2 wt.% I. II. Cu Cu Cu Fe-3wt% Si ,[object Object]
 water quenching
age hardening at 400-450°C for 10 min - 100 hwww.mpie.de
8 Precipitation hardened electrical steels Atom probe tomography 10 min        120 min                 6000 min      Time, min www.mpie.de
9 58Ni+2 56Fe+2 48Ti+2 55Mn+2 200 nm 60Ni+2 54Fe+2 initiated evaporation by or 24                     26                     28   time of flight  mass / charge state  Time of flight  spatial resolution  layer-by-layer 100 nm –  high  voltage  10 kV + 3D Atom Probe Tomography LEAP (Local Electrode Atom Probe) 3000X HR  3-dimensional  reconstructed  model of specimen (about 100 Millions of atoms)
10 APT results: 3D atomic maps (Laser mode at 60K, 0.4 nJ) Cu 1 wt.%  120 min Fe; Cu nm nm Iso-concentration surfaces at Cu 11 at.% www.mpie.de
11 APT results: 3D atomic maps (Laser mode at 60K, 0.4 nJ) Cu 1 wt.%  Cu 2 wt.%  6000 min 120 min 6000 min 120 min 20 nm 20 nm 20 nm 20 nm 450°C aging Iso-concentration surfaces at Cu 11 at.% Fe-Si-Cu, LEAP 3000X HR www.mpie.de
12 APT results: quantification Cu 1 wt.%  Cu 2 wt.%  6000 min 120 min 6000 min 120 min 3.2 nm ± 0.8 nm 5.0 nm ± 0.8 nm 4.3 nm ± 0.8 nm 6.5 nm ± 1.4 nm Cluster: Fe 71 at% Cu 24 at% Si 5 at% Cluster: Fe 62.9 at% Cu 32.1 at% Si 5.0 at% Cluster: Fe 60.7 at% Cu 35.2 at% Si 4.1 at% Cluster: Fe 51.8 at% Cu 44.6 at% Si 3.6 at% Matrix (without clusters): Cu 0.2 at%                           Cu 0.1 at%                                    Cu 0.2 at%                             Cu 0.1 at% “Enrichment factor”:  content in cluster content in alloy Fe  0.68 Cu  40.1 Si   0.75 Fe  0.65 Cu  44.0 Si   0.68 Fe  0.77 Cu  17 Si   0.78 Fe  0.56 Cu  31.9 Si   0.58 clusters number density, m-3 6.110230.910236.41023	           0.61023 volume fraction of clusters  2%                          2%                                  5%                             3-5% www.mpie.de
13 APT results: Proximity histogram bigger cluster Cu 2 wt.%; 450°C/6000 min smaller cluster 20 nm Cluster size 5 nm 8 nm nm matrix cluster center ,[object Object],  (different stages of particle growth) ,[object Object],residual Fe-content diffuse interface www.mpie.de
Overview ,[object Object]
Fe-3%Si-1% (2%) Cu model system
Fe-3%Si-Cu engineeringalloy
Simulations (DFT + kMC, model system)
Conclusionsandchallengeswww.mpie.de

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