You've probably held a magnet before. So felt that snap when it grabs a paperclip. The pull that gets stronger the closer you get.
But here's the thing most people never stop to ask: where exactly is that pull the strongest?
Not "at the magnet." That's the lazy answer. The real answer changes depending on what kind of magnet you're talking about, how it's shaped, and whether you're measuring in air or inside the material itself. And if you're designing a motor, building a speaker, or just trying to figure out why your fridge magnet slides down instead of sticking — the details matter.
No fluff here — just what actually works That's the part that actually makes a difference..
Let's break it down But it adds up..
What Is Magnetic Field Strength
Magnetic field strength — usually measured in teslas (T) or gauss (G) — tells you how much force a magnetic field exerts on a moving charge or another magnet. Day to day, it's a vector quantity, meaning it has both magnitude and direction. The field lines visualize it: where they're packed tight, the field is strong. Where they spread out, it's weak That alone is useful..
Simple enough. But the field doesn't just exist "at the magnet." It extends outward, looping from north to south, passing through air, metal, your hand, whatever's in the way. And its intensity drops off fast. Inverse-square-ish fast, though the exact math depends on geometry.
The difference between B and H
You'll see two symbols in textbooks: B (magnetic flux density) and H (magnetic field strength). Consider this: in free space they're proportional — B = μ₀H — but inside a material they diverge. On the flip side, b accounts for the material's own magnetization. H doesn't. For permanent magnets, B is what you usually care about. Still, for electromagnets and coil design, H shows up more. In practice, most of the time when someone asks "where is the field strongest," they mean B. I'll stick with that.
No fluff here — just what actually works.
Why It Matters
If you're an engineer, the answer determines where you put your sensor, your rotor, your read head. Get it wrong by a millimeter and your torque drops, your resolution tanks, your actuator chatters.
If you're a hobbyist, it explains why your DIY magnetic levitation project keeps failing. The sweet spot isn't where you think it is.
And if you're just curious — well, it's one of those questions that seems trivial until you realize the answer shows up in everything from MRI machines to hard drives to the Earth's own field guiding migratory birds And that's really what it comes down to..
Where the Field Is Strongest: The Short Answer
At the poles. Specifically, at the surface of the poles, right where the field lines exit or enter the magnet But it adds up..
For a standard bar magnet, that means the two ends. So naturally, for a horseshoe magnet, it's the tips. But for a disc magnet, it's the flat faces — but only if it's magnetized axially (through the thickness). If it's magnetized diametrically (across the diameter), the strong spots shift to the curved edge Still holds up..
But "at the poles" is only the beginning. The real story is in the details.
Inside vs. outside the magnet
Here's where it gets counterintuitive. The magnetization opposes the applied field inside the material. Even so, inside a permanent magnet, the B field is actually weaker than at the surface. So the peak B sits right at the boundary — the surface — not deep in the bulk.
H, on the other hand, is strongest inside. But H isn't what pulls on your paperclip.
Sharp corners concentrate flux
A rectangular bar magnet has stronger field at its edges and corners than at the center of its pole face. Day to day, the field lines crowd together where the geometry forces them to bend. This is why magnet designers chamfer or round edges when they want uniform fields — and why they don't when they want maximum grab at a point.
Air gaps kill field strength fast
The field drops off dramatically across even a tiny air gap. A 1 mm gap can cut surface field by 30–50% depending on magnet grade and geometry. This is why magnetic circuits use soft iron keepers, yokes, and pole pieces — to shunt flux through high-permeability material instead of air Which is the point..
Most guides skip this. Don't Easy to understand, harder to ignore..
How It Works: Geometry by Geometry
The "where" changes completely with shape. Let's walk through the common ones.
Bar magnet (rectangular)
Strongest at the corners of the end faces. Even so, the center of the pole face is weaker — sometimes 20–30% lower. The field lines bulge outward from the center (fringing) and crowd at the edges. If you're designing a magnetic latch, put your keeper against the whole face, not just the middle Simple, but easy to overlook. Practical, not theoretical..
Cylindrical / disc magnet (axial magnetization)
Strongest at the outer edge of the flat faces. The center is a local minimum. This surprises people who assume the center is the "bullseye.Practically speaking, the field lines exit the perimeter first, then fan out. " It's not.
Cylindrical / disc magnet (diametral magnetization)
Strongest along the curved sidewall, at the "equator" — the midpoint between the flat faces. The flat faces are weak zones. These magnets act like a bar magnet bent into a circle. Use them when you need radial field, not axial.
Ring magnet (axial)
Strongest at the inner and outer edges of the flat faces. The hole in the middle creates two perimeters. Both concentrate flux. The inner edge often runs hotter (higher B) because the flux path is shorter.
Horseshoe / U-magnet
Strongest at the tips of the poles, especially if they're brought close together with a keeper. The field in the gap between the poles can exceed the surface field of either pole alone — that's the whole point of the shape. It creates a concentrated, uniform field in a defined working volume.
Electromagnets (solenoids)
Strongest inside the coil, at the geometric center. The field lines run parallel through the bore, packed tight. At the ends they flare out and weaken. Not at the ends. Add an iron core and the peak shifts to the core's pole faces — just like a permanent magnet, but switchable Easy to understand, harder to ignore..
Halbach arrays
Basically a special case. A Halbach array rotates magnetization direction across segments to push the field to one side and cancel it on the other. The strongest field sits at the enhanced face, right at the surface. On top of that, the back side? Near zero. These show up in maglev, particle accelerators, and high-efficiency motors.
Common Mistakes / What Most People Get Wrong
Assuming the center is strongest.
It's not. For almost every permanent magnet shape, the peak B is at an edge, corner, or perimeter. The center is a local minimum. This bites people designing magnetic sensors, holders, and couplings Practical, not theoretical..
Thinking "bigger magnet = stronger field everywhere."
A larger magnet produces more total flux, but surface field (B at the pole) saturates around 1.4–1.5 T for the best NdFeB grades. You can't just scale up and expect higher surface field. You get more area at that field, not higher peak.
Ignoring the air gap.
People spec a magnet by its "surface field" from the datasheet, then put a 2 mm plastic cover over it and wonder why the hold force dropped by half. The field in the gap is what matters. Always calculate or measure at your actual working distance.
Confusing pull force with field strength.
Pull force depends on field gradient (how fast
the field decays with distance). You can have a magnet with a higher surface field but a gentler gradient, resulting in lower pull force at practical distances.
Overlooking temperature effects.
The intrinsic coercivity (Hci) and remanence (Br) of NdFeB drop FAST above 80°C. A magnet that tests at 1.4 T at room temperature might fall to 1.1 T at 150°C. If your application runs hot, derate accordingly or choose SmCo.
Expecting perfect models.
Finite element analysis helps, but real-world geometry, magnet quality, and assembly tolerances shift peaks by 10–20%. Build in margin, or prototype and measure It's one of those things that adds up..
Quick Reference Summary
| Magnet Type | Peak Field Location |
|---|---|
| Block/Cylinder (axial) | Flat face center |
| Block/Cylinder (radial) | Curved sidewall (equator) |
| Ring (axial) | Inner + outer edge of flat faces |
| Horseshoe | Pole tips (gap if close) |
| Electromagnet | Coil center; with core, at core face |
| Halbach Array | Enhanced face only |
Conclusion
Magnetic field strength isn't a single number—it's a map. Where you measure it changes everything. A magnet that looks weak at its center might be blazing at its edge. Ignore this, and you'll underspec your sensor gap, miscalculate your holding force, or wonder why your motor isn't delivering expected torque.
The fix is simple: know your geometry, know your field direction, and measure where it matters. Once you do, you're not fighting magnets anymore—you're directing them Small thing, real impact..