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[James_H._Harlow]_Electric_Power_Transformer_Engin(BookSee.org)

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S1<br />

S2<br />

S3<br />

L1<br />

L2<br />

L3<br />

Series Unit Main Unit<br />

FIGURE 2.3.12 Two-core PST.<br />

FIGURE 2.3.14 Quadrature booster set (300 MVA, 50 Hz, 40012*1.25%/11512*1.45˚ kV).<br />

L<br />

,<br />

,<br />

L<br />

a) b)<br />

S<br />

c)<br />

FIGURE 2.3.15 Winding arrangements.<br />

, L<br />

Y Y<br />

FIGURE 2.3.13 Quadrature booster — simplified connection diagram.<br />

2.3.6 Details of <strong>Transformer</strong> Design<br />

In general, the design characteristics of PSTs do not differ from ordinary power transformers. In the<br />

symmetrical case, however, the phase-angle difference of the currents flowing through the two parts of<br />

the series winding has to be recognized. The additional magnetic field excited by the self-compensating<br />

components in the series winding influences mechanical forces, additional losses, and the short-circuit<br />

impedance. Figure 2.3.15 shows schematically variations of the physical winding arrangements in PSTs.<br />

In Figure 2.3.15a, a double concentric design of a single-phase PST is shown. This arrangement does<br />

not offer any problems with respect to the phase lag between currents and is a standard winding<br />

arrangement in shell-type transformers. In core types, the arrangement of the connecting leads from the<br />

innermost regulating winding need some attention, but this does not present a real obstacle to the use<br />

© 2004 by CRC Press LLC<br />

© 2004 by CRC Press LLC

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