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[James_H._Harlow]_Electric_Power_Transformer_Engin(BookSee.org)

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FIGURE 2.6.21 15-kV wound-type CT cast in epoxy resin. (Photo courtesy of Kuhlman <strong>Electric</strong> Corp.)<br />

FIGURE 2.6.24 Linear-coupler equivalent circuit.<br />

fields, large eddy currents flow in the housings, producing high temperatures. The shield can also be<br />

internal as an integral part of the secondary winding. This technique eliminates the eddy-current<br />

problems. Both techniques are effective in protecting the core from stray flux, but neither will make<br />

it immune from it.<br />

FIGURE 2.6.22 High-voltage wound-type CT in combination steel tank, oil, and porcelain construction. (Photo<br />

courtesy of Kuhlman <strong>Electric</strong> Corp.)<br />

FIGURE 2.6.23 00-V, indoor-class auxiliary CT frame shell-type laminated “EI” core. (Photo courtesy of Kuhlman<br />

<strong>Electric</strong> Corp.)<br />

2.6.4.10 Linear Coupler<br />

The linear coupler (LC), or Rogowski coil, is a current transformer that utilizes a nonmagnetic core,<br />

e.g., wood, plastic, or paper, which acts only as a form for the winding. It is typically a window-type<br />

construction. With an air core, the magnetizing components of error have been removed, thus offering<br />

linear response and no possibility of saturation. They do not produce secondary currents that would<br />

be provided by an ideal CT. If the magnetizing impedance approached infinity, the secondary current<br />

would approach the ideal, i S = –i P (N P /N S ), as seen in Figure 2.6.24. The low permeability of the core<br />

prevents a high-magnetizing inductance, thus providing considerable divergence of performance from<br />

that of a conventional CT. Consequently, protective equipment must be designed to present essentially<br />

infinite impedance to the LC and operate as mutual inductors. Closely matching the LC impedance<br />

will provide maximum power transfer to the device. LC outputs are typically defined by V S /I P , e.g., 5<br />

V per 1000 A. Since the load is high impedance, the LC can be safely open-circuited, unlike the<br />

conventional iron-core CT.<br />

Because coupling is important and there is no iron to direct the flux, the window size is made as small<br />

as possible to accommodate the primary conductor. Positioning is critical, and the return conductor and<br />

adjacent phases must be far enough away from the outer diameter of the LC so that stray flux is not<br />

introduced into the winding. <br />

2.6.4.11 Direct-Current <strong>Transformer</strong><br />

The basic direct-current transformer (DCT) utilizes two coils, referred to as elements, that require external<br />

ac (alternating current) excitation (Figure 2.6.25). The elements are window-type CTs that fit over the<br />

dc bus. The elements are connected in opposition such that the instantaneous ac polarity of one is always<br />

in opposition to the other. The ac flux in one element opposes the dc flux in the primary bus and<br />

desaturates the core, while in the other element the ac flux aids the dc flux and further saturates the core.<br />

This cycle is repeated during the other (opposite polarity) half of the ac cycle. The need to rectify is due<br />

to the square-wave output. The direction of current flow in the primary is not important.<br />

Proximity of the return conductor may have an effect on accuracy due to local saturation. For best<br />

results, all external influences should be kept to a minimum.<br />

The output waveform contains a commutation notch at each half-cycle of the applied exciting voltage.<br />

These notches contribute to the errors and can interfere with the operation of fast-acting devices. Ideally,<br />

© 2004 by CRC Press LLC<br />

© 2004 by CRC Press LLC

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