## Exciting current inrush

When a transformer is initially energized, there is a phenomenon known as **exciting current inrush**. Although inrush currents are not generally as damaging as fault currents, the duration of exciting current inrush is on the order of seconds (as compared to on the order of cycles with fault currents).

Exciting current inrush conditions **also occur much more frequently than short circuits**, so this phenomenon is worth exploring.

Consider what happens when initially energizing a single phase transformer. Flux in the core is equal to the integral of the excitation voltage.

If the circuit is closed when the voltage is passing through zero and the initial flux is zero, the sinusoidal flux will be fully offset from zero. The full-offset flux has a peak value that is twice the peak value of a symmetrical sinusoidal flux.

In other words,

the peak flux for a fully offset wave can approach two times the normal peak flux, and this is generally sufficient to drive the core into saturation.

At this point, the only thing that limits exciting current is the **air-core impedance of the winding**, which is several orders of magnitude smaller than the normal magnetizing impedance.

Therefore, the exciting current is much greater than the normal exciting current during the half cycle when the core is saturated. During the opposite half cycle, the core is no longer saturated and the exciting current is approximately equal to the normal exciting current.

**This is illustrated in Figure 1.**

The situation is even more extreme when there is residual flux in the core and the direction of the residual flux is in the same direction as the offset in the sinusoidal flux wave. This is illustrated in Figure 2 below.

**on current different scales**, so the peak current plotted in Figure 2 is actually much larger than the peak current plotted in Figure 1.

### Let’s find the peak inrush current

To find the peak inrush current, limited only by the air-core reactance, it is convenient to calculate the inductance of the winding using cgs units:

where:

**N**– number of turns in the coil**A**– area inside the mean diameter of the coil, cm_{mt}^{2}**l**– axial length of the coil, cm**L**– inductance of the coil, μH

The flux generated by the **inductance φL** is equal to the residual flux plus 2 times the normal flux change minus the saturation flux, since the saturation flux is in the iron. But φL is related to the inductance and the current:

Therefore, the peak inrush current is **expressed in the cgs system of units** as follows:

where:

**I**is in amps and_{peak}**φ**– residual flux_{r}**φ**– normal flux change_{n}**φ**– saturation flux_{s}

Without resistance in the circuit, each successive peak would have the same value and the current inrush would go on indefinitely. With resistance in the circuit, however, there is a significant voltage drop across the resistance and the flux does not have to rise quite as high as the previous cycle.

The integral of the voltage drop represents a net decrease in the flux required to support the applied voltage. Since the **i × R voltage drop** is always in the same direction, each cycle decreases the amount of flux required. When the peak value of flux falls below the saturation value of the core, the inrush current disappears. The rate of decay is not exponential although it resembles an exponentially decaying current.

IMPORTANT!For large power transformers, the inrush current can persistfor several seconds before it finally dies off.

The line reactance has the effect of reducing the peak inrush current by simply adding inductance to the air-core inductance of the winding. There is a definite relationship between inrush current and short circuit current because both are related to the air-core inductance of the windings.

Remember that short circuits tend to exclude flux from the core.

**RULE OF THUMB!**Typically, a rule of thumb is

**that peak inrush currents are a little over 90% of peak short circuit currents**. The magnetic forces caused by inrush currents are generally much smaller than short circuit forces, however. Because only one winding per phase is involved, there is no magnetic repulsion between windings.

The whole problem of analyzing exciting current inrush gets much more difficult when 3-phase transformers are involved. This is because the phase angles of the exciting voltages are 120° apart, there are interactions of currents and voltages between phases, and the three poles of the switching device do not close at exactly the same time.

Nevertheless, it is safe to say

that the peak magnitude of inrush current for three-phase transformers approaches the short circuit current levels.

One of the interesting features of exciting current inrush is that since the current is fully offset, there are large percentages of even harmonics present. Even harmonics are otherwise rarely encountered in power circuits.

### Sympathetic inrush

There is also a phenomenon known as sympathetic inrush, where a transformer that is previously energized will exhibit a sudden change in current when a nearby transformer is switched on. Sympathetic inrush is caused by changes in line voltages from the inrush currents of the second transformer.

**Reference //** Power Transformers Principles and Applications by John J. Winders, Jr. (Purchase hardcopy from Amazon)

Hi Edvard,

I’m a bit puzzled by your definition of air-core impedance and magnetising impedance. Does the transformer have two difference impedance values depending whether the transformer is magnetising (inrush) or in normal on-load operation?

Thank you for the information, the subject is exciting, but what is the change in the inrush current if the transformer is on load?

Regards