Cold from Iron: How a Cheap Alloy Replaces Rare-Earth Magnets ✛ ✎

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
An alloy of iron, nickel, and manganese cools almost as well as gadolinium but costs 35 times less.

The temperature in a room drops by a few degrees while the refrigerator runs without a single moving compressor. Inside, there is no Freon, but a piece of metal that is alternately magnetized and demagnetized. This is the principle of magnetic cooling: when a magnetic field is applied, the material heats up, and when it is removed, it cools down. The cycle is repeated thousands of times, and heat is drawn out of the chamber. The idea is not new, but it has always hit a wall: the cost of the working material. Gadolinium, the benchmark material, costs about 300 dollars per kilogram. It is the diamond among metals.

The authors of the new study decided to do without rare-earth "diamonds." They took three of the most common metals, iron, nickel, and manganese, and cast an alloy of Fe47.5Ni37.5Mn15. The Curie temperature (the point where the material loses its magnetization) turned out to be about 300 K, exactly room temperature. The relative cooling capacity (how much heat the material can transfer per cycle) was 297.68 J/kg in a 5 T field. That is less than gadolinium's 410 J/kg, but the price flips the picture: the entire alloy costs about 8.4 dollars per kilogram. The efficiency per dollar is 25.8 times higher.

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

One might think the next step would be to make nanoparticles of the same composition, since superparamagnetism (the behavior of very small magnetic particles) should enhance the effect. But here the researchers got a surprise. The nanoparticles were produced by pulsed laser ablation in ethanol. When the laser heated them to 4000 K, the ethanol decomposed, and carbon penetrated the particles, up to 23.2 at.%, nearly the solubility limit in the crystal lattice. As a result, the Curie temperature shot up to 477 K, far beyond room temperature. Such a material can no longer cool under normal conditions.

Even small amounts of carbon drastically shift the Curie temperature. In the nanoparticles from ethanol, it rose from 300 K to 477 K, as if a refrigerator suddenly only worked at 200 °C.

The nanoparticle story is not a failure but a valuable lesson. It shows how impurities from the solvent can completely change the magnetic response. For anyone synthesizing nanoparticles by laser ablation in organic liquids, this is a signal: check the composition at the atomic level. Atom probe tomography (microscopy with single-atom resolution) made it possible to see the carbon inside the particles. Now it is clear that returning to room temperature requires a different solvent, such as water or liquid nitrogen, or post-processing to remove the carbon.

The bulk alloy can already be considered a cost-effective alternative to gadolinium in prototypes of magnetic refrigerators. Magnetic cooling promises to be quieter and more environmentally friendly than compressor-based cooling, without harmful gases or vibrations. The path to it lies through cheap transition metal alloys. And that path begins with a simple piece of iron, nickel, and manganese, materials humanity has used for hundreds of years. No diamonds needed.

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.
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