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Methods

schematic picture of the HEMS beamline

The following instruments are available:

• HEMS – High-Energy Materials Science Beamline (P07):

for the study of residual stress, textures, phases and nano-structures

E-mail contact

Contact: Dr. Norbert Schell

• HEMS Grain Mapper:

for studies of the grain structure of materials

E-mail contact

Contact: Dr. Norbert Schell

• High-Energy Materials Science Beamline with white beam (P61A, since 2021):

for spatially resolved studies of, e.g., of near-surface residual stresses and phases

E-mail contact

Contact: Dr. Guilherme Abreu Faria

Contact: Dr. Gleb Dovzhenko

• RÖDI – Lab-X-ray diffractometer:

for the study of residual stress, textures and phases at the surface

E-mail contact

Contact: Dr. Dieter Lott

• NanoStar – Lab-small-angle scattering instrument:

for the study of nano-structures like, e.g., precipitates

E-mail contact

Contact: Dr. Dieter Lott

In the following the most important methods are described.

Note that we are using high photon energies (50 … 150 keV) for penetration deep into material.

• Diffraction – phase analysis

For the quantitative determination of phase contents of a material.

Stacked diffractogram plot

The example is about the development of laser welding as a joining technique for TiAl alloys. The image shows a stacked diffractogram plot during an in-situ laser welding experiment. Melting (stage 2), solidification (stage 4) and phase transformations (stage 5) in a TiAl alloy could be observed with a time resolution of 100 ms.

J. Liu et al., Metall. Mater. Trans. A (2016) DOI: 10.1007/s11661-016-3726-x

• Diffraction – residual stress analysis

For the determination of residual stresses in the interior of materials and components. Conical slits are available for spatial resolution along the beam.

distribution of residual stress in a CT sample with a laser shock peening treatment

The example is about laser shock peening (LSP) of Al alloys. LSP is a surface treatment that can improve fatigue properties. The picture shows the distribution of residual stress in a CT sample with a laser shock peening treatment (area marked with dashed lines).

N. Kashaev et al., Intern. J. Fatigue 98 (2017) 223–233.

• Diffraction – texture analysis

For the determination of the crystallographic textures of the phases present in a material.

Laser beam welded Ti alloy sheets

The crystallographic texture of a material can have a strong influence on the anisotropy of mechanical properties. It also affects residual the stress distribution which in turn influences fatigue properties of welds. This influence was studied in laser beam welded Ti alloy sheets. The picture shows how samples with different orientations of the rolling direction with respect to the welding direction were selected.

E. Maawad et al., Materials & Design 101 (2016) 137–145.

• Diffraction – grain mapping

3DXRD for the determination of position, orientation and internal strains of all grains within a gauge volume.

martensite formation in an austenitic Fe-Cr-Ni alloy during cooling

The example is about martensite formation in an austenitic Fe-Cr-Ni alloy during cooling. The single-grain data indicated that stacking faults appear as precursors to the martensite. The picture shows a diffraction pattern with single diffraction peaks (a) and a peak profile with fit (b).

Y. Tian et al., Scripta Mater. 136 (2017) 124–127.

• Diffraction – energy-dispersive

For the determination of phase content, residual stresses and textures with position and time resolution within a fixed gauge volume. (Since 2021.)

• Small-angle X-ray scattering (SAXS)

For the analysis of nano structures like e.g. precipitates.

SAXS-Signal bei 1300 °C ohne und bei 1100°C mit härtenden Ausscheidungen

Additive manufacturing of Ni-based superalloys opens up new possibilities, but also comes with processing problems that require a deep understanding of the formation and dissolution of g‘ precipitates. SAXS enables the determination of size distributions and volume fractions of precipitates in the size range 1...100 nm with high sensitivity. The picture shows the SAXS signal at 1300°C without, and at 1000 °C with hardening precipitates. The measurement was carried out at P07 with a time resolution of 1 s during an in-situ SLM experiment.

B. Wahlmann et al., Acta Mater. 180 (2021) 84–96.