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Why Radial Magnets →Enter any disc, block or ring geometry, pick a grade, and set an air gap. The calculator returns the estimated on-axis flux density at that gap — what a sensor or gaussmeter sees — and the estimated pull force against a thick mild-steel plate, in pounds, kilograms and newtons.
Two textbook results are combined, with no fudge factors:
| 1 — field at distance | The on-axis flux density of a uniformly magnetized cylinder or block has an exact closed-form solution (shown under formulas). Rings are computed as an outer cylinder minus an inner cylinder — superposition. |
| 2 — force from field | Contact with thick steel is modeled by the image method: the plate behaves like a mirror-image magnet, doubling the normal field at the interface. Maxwell stress then gives F = B²·A / 2µ₀ integrated over the pole face. |
| magnet-to-magnet | By the same image argument, the attraction between two identical magnets in contact approximately equals the single-magnet-to-steel value shown. |
| condition | typical effect on holding force |
|---|---|
| steel thinner than ~1/8″ under a strong magnet | plate saturates — force can drop 30–70% vs. thick plate |
| paint, powder coat or plating (each ~0.05–0.15 mm) | acts as an air gap — expect 5–30% loss per coated surface |
| rough or curved mating surface | effective gap at the interface — often 20–50% loss |
| shear (sliding) loading instead of direct pull | usable force ≈ pull × friction coefficient — often only 15–25% of rated pull |
| elevated temperature | force scales with B², so a 5% Br derate ≈ 10% force loss — see the temperature derating calculator |
| cylinder, on axis | Bz(z) = (Br/2) · [ (z+L)/√((z+L)² + R²) − z/√(z² + R²) ]z = gap from pole face, L = thickness, R = radius |
| rectangular block, on axis | Bz(z) = (Br/π) · [ tan−1( ab / (2z·√(4z² + a² + b²)) ) − tan−1( ab / (2(z+L)·√(4(z+L)² + a² + b²)) ) ]a, b = face dimensions, L = thickness |
| ring, on axis | Bz(z) = Bz,cyl(OD) − Bz,cyl(ID) |
| pull to thick steel | F = (2·Bz(g))² · A / (2µ₀) — image method + Maxwell stress over pole area A at gap g |