Separate the energy stored in an ideal coil from resistive power dissipated while it is energized.
Keep joules and watts distinct
For a constant-inductance model, stored magnetic energy is ½LI². Steady resistive dissipation belongs to a separate resistance term. Primary reference: inductor energy.
Stored energy describes a state at a stated current. Power describes a rate of energy transfer. A coil wattage alone therefore does not tell the reviewer how much energy its selected inductance model contains when switching opens.
A fictional coil calculation
Assume an idealized inductance of 0.20 H carrying 0.50 A. Its stored energy is 0.5×0.20×0.50² = 0.025 J. At 1.0 A with the same inductance, that energy becomes 0.10 J. Doubling current quadruples this modeled energy.
If a separate winding resistance is 10 Ω, resistive dissipation at 0.50 A is 2.5 W. Multiplying that power by a 10 s hold gives 25 J of resistive energy over the interval. It is not the 0.025 J magnetic energy snapshot. These invented values describe no installed HM coil.
Ask where the energy goes
List inductance condition, current history, winding resistance and the event of interest. A changing armature position or magnetic saturation can invalidate a constant-L approximation.
A switch-off assessment also needs the actual recirculation or clamp path and device limits. Record that as a separate review item instead of selecting suppression from this energy figure alone. The useful outcome is a budget that distinguishes stored energy, ongoing heating and subsequent energy transfer.
Customer Questions
Is coil power the stored energy?
Watts and joules describe different quantities.
Does doubling current double magnetic energy?
The stated constant-L model gives four times the energy.
Does energy alone set release time?
Current decay also needs the actual voltage path.
Primary References
These references support the technical principles discussed in this guide. The worked examples and review questions are educational.
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