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[James_H._Harlow]_Electric_Power_Transformer_Engin(BookSee.org)

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in the 1960s, it was found that a transformer with a delta-connected primary was more prone to<br />

ferroresonance problems because of higher capacitance between buried primary cables and ground. An<br />

acceptable preventive was to go to grounded-wye-grounded-wye transformers on all but the heaviest<br />

industrial applications.<br />

2.2.5 Operational Concerns<br />

Even with the best engineering practices, abnormal situations can arise that may produce damage to<br />

equipment and compromise the continuity of the delivery of quality power from the utility.<br />

2.2.5.1 Ferroresonance<br />

Ferroresonance is an overvoltage phenomenon that occurs when charging current for a long underground<br />

cable or other capacitive reactance saturates the core of a transformer. Such a resonance can result in<br />

voltages as high as five times the rated system voltage, damaging lightning arresters and other equipment<br />

and possibly even the transformer itself. When ferroresonance is occurring, the transformer is likely to<br />

produce loud squeals and groans, and the noise has been likened to the sound of steel roofing being<br />

dragged across a concrete surface. A typical ferroresonance situation is shown in Figure 2.2.10 and consists<br />

of long underground cables feeding a transformer with a delta-connected primary. The transformer is<br />

unloaded or very lightly loaded and switching or fusing for the circuit operates one phase at a time.<br />

Ferroresonance can occur when energizing the transformer as the first switch is closed, or it can occur<br />

if one or more distant fuses open and the load is very light. Ferroresonance is more likely to occur on<br />

systems with higher primary voltage and has been observed even when there is no cable present. All of<br />

the contributing factors — delta or wye connection, cable length, voltage, load, single-phase switching<br />

— must be considered together. Attempts to set precise limits for prevention of the phenomenon have<br />

been frustrating.<br />

2.2.5.2 Tank Heating<br />

Another phenomenon that can occur to three-phase transformers because of the common core structure<br />

between phases is tank heating. Wye–wye-connected transformers that are built on four- or five-legged<br />

cores are likely to saturate the return legs when zero-sequence voltage exceeds about 33% of the normal<br />

line-to-neutral voltage. This can happen, for example, if two phases of an overhead line wrap together<br />

and are energized by a single electrical phase. When the return legs are saturated, magnetic flux is then<br />

forced out of the core and finds a return path through the tank walls. Eddy currents produced by magnetic<br />

flux in the ferromagnetic tank steel will produce tremendous localized heating, occasionally burning the<br />

tank paint and boiling the oil inside. For most utilities, the probability of this happening is so low that<br />

it is not economically feasible to take steps to prevent it, other than keeping trees trimmed. A few, with<br />

a higher level of concern, purchase only triplex transformers, having three separate core-coil assemblies<br />

in one tank.<br />

2.2.5.3 Polarity and Angular Displacement<br />

The phase relationship of single-phase transformer voltages is described as “polarity.” The term for voltage<br />

phasing on three-phase transformers is “angular displacement.”<br />

2.2.5.3.1 Single-Phase Polarity<br />

The polarity of a transformer can either be additive or subtractive. These terms describe the voltage that<br />

may appear on adjacent terminals if the remaining terminals are jumpered together. The origin of the<br />

polarity concept is obscure, but apparently, early transformers having lower primary voltages and smaller<br />

kVA sizes were first built with additive polarity. When the range of kVAs and voltages was extended, a<br />

decision was made to switch to subtractive polarity so that voltages between adjacent bushings could<br />

never be higher than the primary voltage already present. Thus the transformers built to ANSI standards<br />

today are additive if the voltage is 8660 or below and the kVA is 200 or less; otherwise they are subtractive.<br />

This differentiation is strictly a U.S. phenomenon. Distribution transformers built to Canadian standards<br />

are all additive, and those built to Mexican standards are all subtractive. Although the technical definition<br />

of polarity involves the relative position of primary and secondary bushings, the position of primary<br />

bushings is always the same according to standards. Therefore, when facing the secondary bushings of<br />

an additive transformer, the X1 bushing is located to the right (of X3), while for a subtractive transformer,<br />

X1 is farthest to the left. To complicate this definition, a single-phase pad-mounted transformer built to<br />

ANSI standard Type 2 will always have the X2 mid-tap bushing on the lowest right-hand side of the lowvoltage<br />

slant pattern. Polarity has nothing to do with the internal construction of the transformer<br />

windings but only with the routing of leads to the bushings. Polarity only becomes important when<br />

transformers are being paralleled or banked. Single-phase polarity is illustrated in Figure 2.2.11.<br />

2.2.5.3.2 Three-Phase Angular Displacement<br />

The phase relation of voltage between H1 and X1 bushings on a three-phase distribution transformer is<br />

referred to as angular displacement. ANSI standards require that wye–wye and delta–delta transformers<br />

have 0˚ displacement. Wye–delta and delta–wye transformers will have X1 lagging H1 by 30˚. This<br />

difference in angular displacement means that care must be taken when three-phase transformers are<br />

paralleled to serve large loads. Sometimes the phase difference is used to advantage, such as when<br />

supplying power to 12-pulse rectifiers or other specialized loads. European standards permit a wide<br />

variety of displacements, the most common being Dy11. This IEC designation is interpreted as Delta<br />

primary–wye secondary, with X1 lagging H1 by 11 30˚ = 330˚, or leading by 30˚. The angular displacement<br />

of Dy11 differs from the ANSI angular displacement by 60˚. Three-phase angular displacement is<br />

illustrated in Figure 2.2.12.<br />

FIGURE 2.2.10 Typical ferroresonance situation. (From IEEE C57.105-1978, IEEE Guide for Application of <strong>Transformer</strong><br />

Connections in Three-Phase Distribution Systems, copyright 1978 by the Institute of <strong>Electric</strong>al and Electronics<br />

<strong>Engin</strong>eers, Inc. The IEEE disclaims any responsibility or liability resulting from the placement and use in the described<br />

manner. Information is reprinted with the permission of the IEEE.)<br />

FIGURE 2.2.11 Single-phase polarity. (Adapted from IEEE C57.12.90-1999. The IEEE disclaims any responsibility<br />

or liability resulting from the placement and use in the described manner. Information is reprinted with the<br />

permission of the IEEE.)<br />

© 2004 by CRC Press LLC<br />

© 2004 by CRC Press LLC

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