Magnetic Cooling Without Rare Earths: The FeNiMn Alloy for Room-Temperature Refrigeration ✛ ✎

Original: "Magnetocaloric effect of Fe47.5Ni37.5Mn15 bulk and nanoparticles: A cost-efficient alloy for room temperature magnetic refrigeration"
arXiv:2410.15776 · 2024-10-21 · arXiv non-exclusive · independent analysis · 3 min
A cheap iron-nickel-manganese alloy cools almost as well as gadolinium but costs 35 times less.

Context

Magnetic cooling promises to replace compressor refrigerators but is held back by material costs: gadolinium costs about 300 dollars per kilogram. Neighboring papers on the archive follow the same path, looking for cheap alloys and tuning magnetic properties through grain size, thin films, or heating. This article fits into that line but focuses on a simple ternary alloy of common metals and tests it in two forms: bulk and nanoscale.

Methods

The bulk alloy was melted in an argon arc from pure metals, homogenized for 120 hours at 1050°C, and quenched in water. Nanoparticles were produced by pulsed laser ablation in ethanol. Magnetic properties were measured with a vibrating sample magnetometer, and structure was characterized by X-ray diffraction, electron microscopy, and atom probe tomography. Composition and element distribution were checked down to individual atoms.

Results

The bulk alloy showed a Curie temperature around 300 K and a relative cooling capacity of 297.68 J/kg in a 5 T field. This is lower than gadolinium's 410 J/kg, but given the component prices (iron 0.31, nickel 22, manganese 0.25 dollars per kg), the efficiency per dollar is 25.8 times higher. The nanoparticles were expected to enhance the effect through superparamagnetism, but their Curie temperature jumped to 477 K. The cause is carbon: up to 23.2 at.% inside the particles, near the solubility limit in the FCC lattice. The carbon came from ethanol, which decomposed under laser heating to 4000 K.

Implications

This work follows the general search for inexpensive magnetocaloric materials but stands out by directly comparing bulk and nanoscale forms of the same composition. Neighbors study the effect of grain size or thin films, whereas here a pitfall of miniaturization is shown: impurities from the solvent can completely change the magnetic response. This is the first test for this ternary alloy, and it outlines the limits of laser ablation in ethanol.

Future development

The topic could evolve toward choosing a solvent that does not introduce carbon impurities, such as water or liquid nitrogen. Another path is post-processing the nanoparticles to remove carbon or controlled doping to bring the Curie point back to room temperature. Searching for compositions less sensitive to impurities is also possible.

Impact

The results will influence the development of magnetic refrigerators and air conditioners, where material cost matters. They are also useful for anyone synthesizing nanoparticles by laser ablation in organic liquids.

Next steps

Synthesize nanoparticles of the same alloy in a carbon-free environment and compare the magnetocaloric response. Check whether annealing the already obtained particles can remove carbon without sintering.

Key open problems

For the materials science of magnetocaloric alloys, an open question remains: how to maintain high cooling capacity when going to the nanoscale, where surface effects and impurities start to dominate. This work shows that even small amounts of carbon drastically shift the Curie temperature, limiting the use of cheap synthesis methods.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

The authors fabricated a bulk Fe47.5Ni37.5Mn15 alloy by arc melting followed by homogenization and quenching, as well as nanoparticles of the same composition via pulsed laser ablation in ethanol. Magnetic measurements revealed a Curie temperature of about 300 K and a relative cooling power of 297.68 J/kg in a 5 T field for the bulk sample. The nanoparticles had a Curie temperature of 477 K due to carbon contamination from ethanol, as confirmed by atom probe tomography.

Where its strength is

This work demonstrates the potential of an inexpensive ternary alloy based on transition metals for magnetic cooling and clearly highlights the critical role of impurities when transitioning to the nanoscale form.

Where it could go next

  • Nearby in the archive there is a study where magnetic properties are improved through grain size in bulk material; for this alloy, it might be worth examining how properties change with grain refinement without altering composition.based on: Tiny Magnets with a Fiery Core arXiv:2602.01300
  • Our archive contains research on thin films that enhance magnetic response; it might be interesting to consider producing FeNiMn films and studying the influence of interfaces and strain on the magnetocaloric effect.based on: Thin Films Give Magnets a Stronger Twist arXiv:2601.12581
  • Another neighboring work shows how aluminum doping changes magnetic properties; for FeNiMn, one could test how small additions of aluminum affect the Curie temperature and cooling capacity.based on: Aluminum Makes Magnets Stronger arXiv:2604.04152

Worth trying

  • Try synthesizing FeNiMn nanoparticles in an inert liquid (e.g., hexane) instead of ethanol to avoid carbon contamination.
  • Perform annealing of the nanoparticles in a reducing atmosphere to remove carbon and check whether the Curie temperature returns to 300 K.
  • Measure the magnetocaloric effect of the bulk alloy in fields below 2 T to assess practical applicability in household refrigerators.

Why this may matter

If the magnetocaloric properties of the bulk alloy can be preserved in the nanoscale form or improved through microstructural control, it would pave the way for cheap magnetic coolers based on abundant metals, reducing dependence on rare-earth elements.

Gadolinium, the benchmark magnetocaloric material, costs about 300 dollars per kilogram, while the entire Fe47.5Ni37.5Mn15 alloy costs roughly 8.4 dollars per kilogram, making it 35.7 times cheaper.

\Delta S_M(T,B) = \int_{B_1}^{B_2} \left( \frac{\partial M(T,B)}{\partial T} \right)_B dB
Allows calculating the magnetocaloric effect from magnetization measurements at different temperatures and fields.
D = \frac{K \lambda}{\beta \cos \theta}
Relates the width of an X-ray peak to the average crystallite size; used to check nanoparticle size.

Key numbers

  • relative cooling capacity: 297.68 J/kg in a 5 T field
  • Curie temperature of bulk alloy: about 300 K
  • Curie temperature of nanoparticles: about 477 K
  • carbon content in nanoparticles: up to 23.2 at.%
  • cost advantage over gadolinium: 35.7 times
Scientists
Fred HoyleMargaret BurbidgeJohannes RydbergSatyendra Nath BoseDaniel BernoulliLev Landau
Concepts
magnetic refrigeration magnetic transition Curie temperature aluminum nitride Curie's law room temperature superconductivity nanomaterial manganese cryostat kondo effect dysprosium carbon material catalysis niobium nitride nickel thermal hall effect magnetoresistance molybdenum millikelvin magnetocaloric effect Meissner effect