Zed, I'll assume you're talking about the transient that occurs when an energized inductor (such as a relay coil) has just been disconnected from its power source. Let me start with a little theory.

If you understand capacitance, then inductance is simple -- the two are highly symmetrical. In the same way that a capacitor stores energy as an electrostatic field, an inductor stores energy as a magnetic field.

The rate at which the voltage across a capacitor changes is proportional to the

*current* passing through it:

dV/dT = I/C

e.g. a 1 amp current flowing through a 1-farad capacitor will build a voltage across the capacitor linearly at the rate of 1 volt per second. A capacitor is therefore said to resist any change in voltage across it, but the current through it can change rapidly.

In the same way, the rate at which the current in an inductor changes is proportional to the

*voltage* impressed across it:

dI/dT = V/L

e.g. 1 volt impressed across a 1-henry inductor will build a current through the inductor linearly at the rate of 1 ampere per second. An inductor is therefore said to resist any change in current through it, but the voltage across it can change rapidly.

(Note: Electronics guys normally use "E" for voltage, but physics guys use "V" to differentiate it from Energy "E".)

The energy stored in a capacitor is proportional to the square of the voltage across it:

E = (C x V^2) / 2

The energy stored in an inductor is proportional to the square of the current through it:

E = (L x I^2) / 2

Isn't that a nice symmetry?

Now, to get to your questions:

The slow build-up of the field is due to the controlled voltage applied across the inductance. When you energize a relay coil by connecting a DC voltage across it, the current starts building up at a predictable rate (initially dI/dT=V/L). Eventually, the current reaches a steady state determined by the applied voltage and the coil resistance, and the coil is fully "charged" at that current value. The time constant at which this slow buildup occurs is the ratio of the coil inductance and the circuit resistance (t=L/R).

When this charged inductor suddenly finds itself disconnected from the voltage source, it tries hard to do what it's intended to do: Keep the current flowing through itself at a constant rate. Its terminals immediately rise to whatever voltage is necessary to achieve that current.

As an example, suppose a relay coil draws 1 amp while energized. If we disconnect the power source and immediately connect a 100 ohm resistor across the coil, the coil will produce -100 volts across the resistor, and that voltage will decrease exponentially over time as the coil discharges into the total circuit resistance (the coil resistance plus the external resistor).

Notice two things about that description:

1) The voltage across the resistor is negative compared to the energizing voltage because the inductor is discharging instead of charging.

2) I didn't mention what the energizing voltage was because

*it doesn't make any difference!* It could be 6 volts or 240 volts. The only thing that affects the

*discharge* voltage is the current and the resistance.

It's just like a capacitor that's been charged to 100 volts. If you then remove the charging current and connect a 100 ohm resistor across it, it discharges at -1 amp into the resistor, decreasing exponentially to zero. It doesn't matter what the charging current was.

So, what peak voltage do you get when you disconnect the coil and there's no suppressor of any kind? It's infinite! Theoretically.

In practice, assuming there's no arc or insulation breakdown, the inductance resonates with the stray capacitance in the coil, producing a high-voltage oscillation that decays as the energy gets dissipated in the coil resistance and through other losses. Since the voltage is high, the discharge rate is very fast. Also, since the stray capacitance is unspecified, it's impossible to predict the peak voltage.

This is comparable to taking that charged capacitor, placing a dead short across its terminals and measuring the peak current -- Again, it's theoretically infinite, but limited in practice by the stray inductance and circuit resistance.

Was that more than you wanted to know?

(edit: time constant is ratio L/R, not product LxR)

[This message has been edited by John Crighton (edited 07-25-2005).]