Energy stored in an inductor is equal to:(adsbygoogle = window.adsbygoogle || []).push({});

[itex]\frac{1}{2}L\mathbf{I}^2[/itex]

Where [itex]L[/itex] is the inductance in henries and [itex]I[/itex] is the current in amps.

The energy stored in the inductor doesn't depend on how fast the current is attained, just the fact that it has some inductance and some current.

However, how fast the current can be attained can very well depend on what is supplying the inductor with current. The timing of turning on and off of the inductor magnetic field affects how much work could done by it. So what if we take the energy of the inductor and multiply by the frequency of the pulses? This should not exceed overall electrical power [itex]R{I}^2[/itex] if current electromagnetic theory is correct.

Assuming power factor is 1 (or not assuming power factor is one), [itex]\frac{1}{2}Lf[/itex], where [itex]f[/itex] is frequency of on/off periods the inductor handles (to influence a magnetic rotor), cannot be greater than the resistance [itex]R[/itex] of the coil. Do I have this right?

For example it should be impossible that a coil of 1100 henries with 770 Ohms of resistance can switch its whole magnetic field (i.e. with the current throughout the whole length of the coil) on and off 1.4 times every second. Isn't this well understood in engineering literature (I hope it is)? So [itex]\frac{1}{2}Lf \le R[/itex]?

The time constant of any motor is simply inductance divided by resistance. This would mean that the time constant of the circuit times the frequency of the pulses cannot be greater than 2. Right?

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# Work that can be done via induction (on/off) vs. the electrical power used to make it

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