\u201cMagneto-Science\u201d refers to the study of the effects of magnetic fields on physical, chemical and biological processes. This involves exploiting the effects of magnetostatic forces and torques, electro-magnetic couplings and magneto-static energy, from the macroscopic to the atomic scale.<\/p>\n
On the macroscopic scale, magnetostatic forces are exploited to simulate micro-gravity and perform laboratory experiments otherwise carried out in free-fall towers or in space. These same forces can also control convection in fluids, where magnetic properties are temperature-dependent.<\/p>\n On the microscopic scale, magnetic and electromagnetic couplings play an important role in materials development: it is possible to control crystalline texture, modify the shape of crystals and dendrites…<\/p>\n At the atomic scale, in certain systems (e.g. steels), we can observe a significant effect on thermo-dynamic equilibrium temperatures: this provides us with a new lever, in addition to conventional thermal and mechanical treatments, for finding new ways of developing materials.<\/p>\n Some of these effects are already well known, enabling us to invent new experimental conditions, for example in simulated micro-gravity.<\/p>\n Others have yet to be explored, such as the effect on atomic diffusion – an effect observed in several metallurgical systems, with variable results, and for which there is no commonly accepted model.<\/p>\n<\/div>\n [\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=”1″ module_id=”personnel” _builder_version=”4.27.0″ _module_preset=”default” global_colors_info=”{}”][et_pb_row _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_text _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”]<\/p>\n [\/et_pb_text][et_pb_code _builder_version=”4.27.0″ _module_preset=”default” global_colors_info=”{}”] [\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=”1_2,1_2″ _builder_version=”4.25.2″ _module_preset=”default” module_alignment=”center” global_colors_info=”{}”][et_pb_column type=”1_2″ _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_image src=”https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/06\/Magnetic-levitation.jpg” title_text=”Magnetic levitation” _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][\/et_pb_image][\/et_pb_column][et_pb_column type=”1_2″ _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_text _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”]<\/p>\n Magnetic levitation<\/strong><\/p>\n The magnetic levitation is the application of a bulk force that compensates the gravity on every part of a sample. This environment is very similar to free fall such as in drop tube or experiments in orbiting stations.<\/p>\n If the material is diamagnetic, such as water and organic materials, it is even possible to maintain a stable contactless environment for long run experiments (hours) at reduced costs. The magnetic levitation of water was hence demonstrated for the first time in 1991 (E.Beaugnon, R. Tournier, Levitation of organic materials, Nature 349 (6309), 134-136).<\/p>\n An example of such experiments is the recent measurement of free levitating water droplets oscillations (see figure on the left). A droplet is excited by an acoustic wave, resonant modes are explored, and once obtained, the acoustic wave is removed and the droplet freely oscillate. The frequency of the oscillation gives the surface tension, and the decaying of the amplitude gives the viscosity.<\/p>\n [\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=”1_2,1_2″ _builder_version=”4.25.2″ _module_preset=”default” module_alignment=”center” global_colors_info=”{}”][et_pb_column type=”1_2″ _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_text _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”]<\/p>\n Magnetization at high temperature<\/strong><\/p>\n The magnetization M of a sample can be very precisely determined by measuring the magnetic force acting on it. Such measurements are performed during solid state heat treatments and solidification processes of metals at high temperature.<\/p>\n This measurement allows the precise in situ monitoring of phases evolution and transformation. We have studied pure Cobalt, Co-Sn and Co-B near eutectic alloys. In the first case, we have determined that liquid undercooled Cobalt is more magnetic than solid Cobalt at the same temperature, which is contradictory with the liquid expansion and lesser Co to Co magnetic interactions. In the Co-B and Co-Sn ear eutectic alloys, we have observed for the first time a liquid to liquid phase transition at high temperature. On the left picture, an example is given for hypoeutectic CoSn (Jun Wang, Jinshan Li, Rui Hu, Hongchao Kou, Eric Beaugnon, Evidence for the structure transition in a liquid Co\u2013Sn alloy by in-situ magnetization measurement, Materials Letters 145 (2015), 261). The red curve is the heating curve. The linear part corresponds to paramagnetic Curie Weiss law of 1\/M versus T for the first liquid alloy L1 (melting is slightly above 1100 \u00b0C). Above T0<\/sub>, the slope of 1\/M is obviously changed, revealing a new liquid structure L2 that is maintained on cooling (blue curve) until solidification (below 900\u00b0C in an undercooled state).<\/p>\n [\/et_pb_text][\/et_pb_column][et_pb_column type=”1_2″ _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_image src=”https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/06\/Magnetization-at-high-temperature.jpg” title_text=”Magnetization at high temperature” _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][\/et_pb_image][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=”1″ module_id=”techniques” _builder_version=”4.27.0″ _module_preset=”default” locked=”off” global_colors_info=”{}”][et_pb_row _builder_version=”4.26.0″ _module_preset=”default” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.26.0″ _module_preset=”default” global_colors_info=”{}”][et_pb_text module_id=”techniques” _builder_version=”4.27.0″ _module_preset=”default” global_colors_info=”{}”]<\/p>\n [\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=”4.27.2″ _module_preset=”default” locked=”off” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.27.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_toggle title=”High temperature magnetometer” _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”]<\/p>\n High temperature furnaces (up to 1550 \u00b0C) can be inserted inside superconducting magnets and high field resistive magnets at LNCMI. In the case of superconducting magnets, where long term experiments even for several days can be performed, in situ magnetic measurements have been added.<\/p>\n The heating element is a SiC heater, covered by an insulating refractory material. The furnace is cooled by a water jacket. The sample is positioned above the maximum field on the vertical axis of the magnet, where a downward magnetic force exists for ferromagnetic and paramagnetic materials.<\/p>\n The experiments are realized without vacuum or inert gas, but the solid or liquid metal is protected by a flux glass.<\/p>\n The magnetic force is measured by an electronic scale away from the magnetic field of the magnet. Both magnetic force (from which the magnetization M is calculated) and sample and furnace temperatures are continuously recorded.<\/p>\n [\/et_pb_toggle][et_pb_toggle title=”Stable diamagnetic levitation and in situ measurements” _builder_version=”4.27.4″ _module_preset=”default” locked=”off” global_colors_info=”{}”]<\/p>\n Stable diamagnetic levitation can be performed in both a superconducting magnet (32 mm available bore, or 26 mm with controlled temperature) or a resistive high field magnet with a 50 mm bore.<\/p>\n In these devices, diamagnetic liquids such as water can be levitated, without any contact with the magnet bore and without requiring any container.<\/p>\n We have developed several in situ devices to provide in situ, real-time, monitoring of the sample levitation:<\/p>\n [\/et_pb_toggle][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=”1″ admin_label=”Publications” module_id=”publications” _builder_version=”4.27.0″ _module_preset=”default” global_colors_info=”{}”][et_pb_row _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_text _builder_version=”4.25.2″ _module_preset=”default” global_colors_info=”{}”]<\/p>\n [\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=”4.27.2″ _module_preset=”default” locked=”off” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.27.2″ _module_preset=”default” global_colors_info=”{}”][et_pb_toggle title=”Selected publications” _builder_version=”4.27.4″ _module_preset=”default” hover_enabled=”0″ global_colors_info=”{}” sticky_enabled=”0″]<\/p>\n E.Beaugnon, R. Tournier<\/p>\n Levitation of organic materials<\/p>\n Nature 349, 470 (1991)<\/a><\/p>\n <\/p>\n D Braithwaite, E Beaugnon, R Tournier<\/p>\n Magnetically controlled convection in a paramagnetic fluid<\/p>\n Nature 354, 134-136 (1991)<\/a><\/p>\n <\/p>\n Jun Wang, Jinshan Li, Rui Hu, Hongchao Kou, Eric Beaugnon<\/p>\n Evidence for the structure transition in a liquid Co\u2013Sn alloy by in-situ magnetization measurement<\/p>\n Materials Letters 145, 261 (2015)<\/a><\/p>\n <\/p>\n Jun Wang, Jinshan Li, Rui Hu, Hongchao Kou, Eric Beaugnon<\/p>\n Anomalous magnetism and normal field instability in supercooled liquid cobalt<\/p>\n Appl. Phys. Lett. 105, 144101 (2014)<\/a><\/p>\n <\/p>\n G Diguet, E Beaugnon, JY Cavaill\u00e9<\/p>\n Shape effect in the magnetostriction of ferromagnetic composite<\/p>\n![\"\"](\"http:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2019\/02\/Picture-magnetosciences-300x243.jpg\")
<\/p>Research staff<\/h3>\n
![\"BEAUGNON](\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/07\/Beaugnon-480x640-400x486-1.jpg\")
<\/a><\/figure><\/div>BEAUGNON Eric<\/a><\/span><\/h3>
Topics<\/h3>\n
Techniques<\/h2>\n
![\"\"](\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/06\/High-temperature-magnetometer.jpg\")
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![\"\"](\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/06\/Stable-diamagnetic-levitation-and-in-situ-measurements.jpg\")
<\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\nPublications<\/h3>\n