Demagnetisation steps and residual field
Ferromagnetic steel keeps some of the field it was given. That remanence is what holds the particles in place during examination, but afterwards it attracts swarf to machined surfaces, deflects instruments, disturbs arc welding, contaminates bearings and can upset later magnetic particle or ultrasonic work. Demagnetisation removes it by walking the material repeatedly around its hysteresis loop with steadily shrinking amplitude, so the loop spirals in towards the origin and the remanence is left close to zero.
Each reversal must both flip the direction and reduce the peak. If the amplitude is cut without reversing, the material simply relaxes back onto the same branch of the loop and the remanence barely moves. The practical arrangement is either a decaying AC field - which reverses at line frequency while the current is ramped down - or a reversing DC supply that steps the current down and flips polarity at every step.
Each step leaves a fraction of the previous residual, so the field decays geometrically: H = H0 x r^n. Solving for the number of steps gives n = ln(H_limit/H0)/ln(r), rounded up. A per-step reduction ratio around 0.7 is typical of a reversing DC set; a smooth AC decay behaves like a very large number of very small steps. The first step must reach at least the peak current used to magnetise the part, otherwise the deepest part of the loop is never reversed.
The catch with AC demagnetisation is its shallow penetration. It works well on thin sections and on surface remanence, but it will not reach the core of a heavy forging - that needs a reversing DC cycle. The result is verified with a calibrated field indicator or Hall-effect gaussmeter, with a residual limit commonly set at 3 G and tightened to 2 G on aerospace work.
H after n steps = H0 x r^n n = ln(H_limit / H0) / ln(r), rounded up Residual field acceptance: 3 G general, 2 G on many aerospace specifications AC pull-through: withdraw the part at least 1 m from the coil before switching the current off
- Each step must reverse polarity as well as reduce amplitude. Reducing current without reversing does not demagnetise.
- The first step must reach at least the peak current used to magnetise the part.
- AC demagnetisation only reaches the surface layer. Heavy sections need a reversing DC cycle.
- With an AC pull-through coil, draw the part at least 1 m clear before switching the current off, or it will be re-magnetised on the way out.
- Verify with a calibrated field indicator or Hall-effect gaussmeter, not by eye or by picking up swarf.
- Demagnetisation is only required where residual magnetism would interfere with machining, welding, instrumentation, bearings or subsequent examination.
- Parts magnetised with a circular technique can hold a field that does not show externally. Check the bore and end faces as well.
Reference: ASME BPVC Section V (2023 Ed.), Article 7 - demagnetisation requirement; ASTM E1444/E1444M-22 and ASTM E709-21, which give a residual field acceptance of 3 G (240 A/m) for general work. The geometric decay relation is the standard hysteresis-loop model, not a code formula.


