Short versionNo curve, no claim. The demagnetization curve is the one document that turns a performance statement into something a stranger can check, and it is cheap to produce if you actually have a magnet.
A permanent magnet's entire performance is one curve. The numbers on a datasheet — remanence, the two coercivities, energy product — are not four separate facts, they are four points on it, and everything an engineer needs to know about whether the magnet survives its application is in the curve's shape rather than in any single number. If that sentence is new, the long version is here.
Measuring it is not exotic. It is a standardized test with a standardized instrument, defined internationally in IEC 60404-5,1 and any company that makes magnets has run it thousands of times, because it is also how they decide what to ship and what to scrap. So when a company does not publish a curve, there are only two explanations. Either they do not have a magnet yet — which is a perfectly respectable place to be, and they should say so — or they have one and do not like how the curve looks.
When a curve IS published, read it for four things:
Both curves, not one. A proper plot shows the normal curve (B against H) and the intrinsic curve (J against H) together. The coercivity that decides whether a magnet survives a motor lives on the intrinsic curve. A plot showing only B is not wrong, but it is the flattering half.
Temperature. A single room-temperature curve is the beginning of a datasheet, not a datasheet. Real producers publish a family of curves at 20, 60, 100, 150 °C and upward, because that is where the knee moves and the knee is what kills parts in service. Room temperature is where every material looks its best, which is presumably why it is often the only temperature offered.
What was measured. A hysteresigraph running the standard test on a real magnet, or a vibrating-sample magnetometer running a few milligrams of aligned powder in epoxy? Both produce a curve that looks like a curve. Only one of them describes something you could bolt into a machine. Powder measurements skip the three things that hurt: alignment loss in a real pressed part, density, and the demagnetizing field of a real shape. If the method and the sample mass are not stated, that omission IS the finding.
Whether the numbers reconcile with each other. This one you can do on your phone.
The best energy product any material can ever reach is set by its remanence alone:
(BH)max ≤ Br² / 4μ₀and you only get there if the intrinsic coercivity, expressed as a field, is at least half the remanence:
μ₀HcJ ≥ Br / 2So a material advertising a remanence of 1.4 T has a theoretical ceiling of about 390 kJ/m³ (49 MGOe) — and needs at least 0.7 T, roughly 7 kOe or 557 kA/m, of intrinsic coercivity to claim it. If the same announcement quotes a coercivity of 2 kOe, the arithmetic caps that material at perhaps 24 MGOe with a perfectly square loop, which nothing has, and much less than that in any machine that gets warm. The headline number and the coercivity number are describing two different materials, and only one of them exists.
In practiceI came at coercivity backwards. My first real work in magnetics was figuring out how to erase things — hard drives and floppy disks — which is the same property viewed from the wrong end, and it taught me early that taking magnetization away is far harder than putting it there. That asymmetry is the whole commercial value of a permanent magnet, and it is precisely the property that new materials are short of. When somebody leads with how much field their material produces, I am already thinking about how easily it gives it back.