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7/28/2019 103_1209_v01e_web
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FraunhoFer InstItute For MechanIcs oF MaterIals
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Dr. Dirk Helm
Phone +49 761 5142-158, [email protected]
F r a u n h o F e r I n s t I t u t e F o r
M e c h a n I c s o F M a t e r I a l s I W M
Thermophysical quanTiTies
and Thermomechanical TesT
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Pierre Bienger
Phone +49 761 5142-381
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Andre Koch
Phone+49 761 5142-466
W h Y W o r K W I t h u s ?
W W W . I W M . F r a u n h o F e r . d e
W W W . I W M . F r a u n h o F e r . d e / t h e r M o p h Y s I K
103_1209_v01e
As research partner for industry and public bodies, Fraunhofer IWM
develops solutions that can improve energy and resource efciency
during manufacture and use of materials and components and can
reduce losses involved in the production, conversion and storage of
energy. The solutions lead to greater component durability, longer
service life and improved reliability as well as more cost-efcient
processes.
Woehlerstrasse 11
79108 Freiburg, Germany
Phone +49 761 5142-0
Ff Ii f Mi f Mi IWM
Directors
Prof. Dr. Peter Gumbsch
Prof. Dr. Ralf B. Wehrspohn
The Fraunhofer IWM uses the latest materials science and
technology ndings to increase material and component
performance levels and create innovative functionalities and
to improve manufacturing processes.
The institute uses its understanding of material behavior to assess
materials and components under a wide range of environmental
conditions and loads: this leads to increased durability, reliability
and availability of components, systems and entire plants.
The well-established link between experimentation and simula-
tion at the Fraunhofer IWM provides an excellent basis for solving
materials technology issues, particularly where resource or energy
savings during manufacture and in use are concerned.
For the virtual development and assessment of materials and
components, the institute works with advanced multiscale
simulations on the nano, micro and macro level or develops
the appropriate models.
The development of and changes to material properties along
a chain of different manufacturing stages can be predicted for
entire manufacturing processes.
http://www.iwm.fraunhofer.de/http://www.iwm.fraunhofer.de/thermophysikhttp://www.iwm.fraunhofer.de/thermophysikhttp://www.iwm.fraunhofer.de/ -
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In our thermophysical laboratory we determine thermal
expansion, specic heat capacity, density, and thermal diffusivity.
From these quantities we calculate the thermal conductivity
of materials. There is a great variety of materials which can be
analyzed by us, ranging from metals, plastics, ceramics and
thermoelectric materials to reactive coatings. We test specimens
in the form of pastes, powders, liquids, and solids at temperatures
from ambient to 2 000 C.
tmmi Ff IWM
With our testing equipment of the type Gleeble 3150 we offer
you the thermomechanical characterization of metallic materials.
We heat conductive materials up to melting temperature and
apply mechanical loads under force or deformation control. Thus,
we are able to simulate heat treatment and welding processes,
and we can conduct warm tension or compression tests. Additio-
nally we determine Time-Temperature-Transformation diagrams,
temperature dependent ow stress curves and temperature
cycles with super-imposed tension-compression loads.
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Measuring from room temperature (RT) to 1 600 C
at heating rates from 0.01 to 50 K/min
Determination of transformation temperatures
Quantitative assessment of exothermal and endothermal
reactions
Measuring in different gas atmospheres and in vacuum
Typical specimen dimensions with solid materials
diameter 5 x 1.2 mm
dimi mig f m g xi
Measuring from RT to 1 600 C at heating rates from
0.01 to 50 K/min
Assessing the coefcient of thermal expansion, phase
transformations and transformation temperatures
Measurements in various gas atmospheres and in vacuum
Typical specimen dimensions: diameter 3 to 10 mm with
length of 5 to 25 mm, similar dimensions for sheet
materials
Measurement of the thermal diffusivity in the range of
0.001 to 1.0 mm2 and from RT to 2 000 C at heating ra
between 0.1 and 50 K/min
Measurements in various gas atmospheres and in vacuum
Diameters of 6, 10, and 12.7 mm for cylindrical specime
max 10 x 10 mm2 for rectangular specimens
Specimen thickness depends on the expected thermal
diffusivity
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Heating rates up to 8 000 K/s, cooling rates up to about
2 500 K/s
Mechanical loads under force or displacement control
Measurement possible in various gas atmospheres and in
vacuum
cmmy y
Analyses of microstructure by Light or Scanning Electron
microscopy (EDX and EBSD analyses where applicable)
Distribution of elements with Glow Discharge Optical Em
Spectroscopy(GDOES)
tmyi Ff IWM o vi
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-0.1
0.1
0.2
0.3
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temperature in C200
DSC in mW/mg
400 600 800 1000 1200
cool down
heat-up
912 C580 C
874 C
742 Cexo
Mig f m iviy wi
l F eqim (lFa)