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[James_H._Harlow]_Electric_Power_Transformer_Engin(BookSee.org)

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From statement 1, the primary energy required to magnetize the core is a product of the flux in the<br />

core and the magnetic reluctance of the core. This energy is called the magnetomotive force, mmf, and<br />

is defined as follows:<br />

S S<br />

mmp<br />

S S<br />

mmp<br />

mmf = ¬= È Î Í ˘ È ˘ È ˘<br />

f k<br />

Z I<br />

Z I<br />

1 ˙ k2Í<br />

˙ = kk<br />

1 2Í<br />

˙<br />

NS f ˚ Î ACmC˚<br />

Î NS f AC mC˚<br />

(2.6.4)<br />

FIGURE 2.6.4 Typical composite core.<br />

TABLE 2.6.1 Core Materials<br />

Material<br />

(0.009–0.014 in.)<br />

Saturation<br />

Density, T<br />

Initial<br />

Permeability,<br />

@ 0.004 T<br />

Maximum<br />

Permeability,<br />

@ T<br />

Trade Names<br />

80% Ni/Fe/Mo 0.760 35,000 150 k @ 0.4 T SuperPerm 80 a<br />

Hymu 80 Mu-Metal b<br />

4–79 Permalloy c<br />

49% Ni/Fe/Mo 1.200 5,000 60 k @ 0.4 T Super Perm 49 a<br />

High Perm 49 c<br />

48-Ni<br />

4750 b<br />

3% Si/Fe – M3 1.900 8,000 51 k @ 1.15 T Microsil a<br />

Silectron d<br />

Oriented T-S e<br />

Hipersil a<br />

3% Si/Fe – M4 1.900 7,200 48 k @ 1.15 T<br />

3% Si/Fe – M6 1.900 6,700 40 k @ 1.15 T<br />

a<br />

Magnetic Metals Co.<br />

b<br />

Allegheny Ludlum Steel.<br />

c<br />

Carpenter Steel.<br />

d<br />

Arnold <strong>Engin</strong>eering.<br />

e<br />

Armco (now AK Steel).<br />

where<br />

f = flux in the core<br />

¬ = magnetic reluctance<br />

k 1 = constant of proportionality<br />

k 2 = constant of proportionality<br />

Z S = secondary impedance<br />

mmp = core mean magnetic path<br />

I S = secondary current<br />

A C = core cross-sectional area<br />

N S = number of secondary turns<br />

m C = permeability of core material<br />

f = frequency, Hz<br />

The magnetic reluctance, in terms of Ohm’s law, is analogous to resistance and is a function of the<br />

core type used. An annular or toroidal core, one that is a continuous tape-wound core, has the least<br />

amount of reluctance. A core with a straight cut through all of its laminations, thereby creating a gap,<br />

exhibits high reluctance. Minimizing gaps in core constructions reduces reluctance. Figure 2.6.5 shows<br />

some of the more common core and winding arrangements. Generally — after the steel material is cut,<br />

stamped, or wound — it undergoes a stress-relief anneal to restore the magnetic properties that may<br />

have been altered during fabrication. After the annealing process, the core is constructed and insulated.<br />

From statement 2, the core permeability, m C , changes with flux density, f/A C . Neglecting leakage flux,<br />

we can now see the error-producing elements. From Equation 2.6.4, an increase in any of the elements<br />

in the denominator will decrease errors, while an increase in Z S and mmf will increase errors.<br />

There are also other contributing factors that, based on the construction of the instrument transformer,<br />

can introduce errors. The resistance of the windings, typically of copper wire and/or foil, introduces<br />

voltage drops (see Figure 2.6.6). Moreover, the physical geometry and arrangement of the windings —<br />

with respect to each other and the core — can introduce inductance and, sometimes, capacitance, which<br />

has an effect on magnetic leakage, reducing the flux linkage from the primary circuit and affecting<br />

performance. A winding utilizing all of its magnetic path will have the lowest reactance. Figure 2.6.5<br />

shows some typical winding arrangements and leakage paths.<br />

Figure 2.6.6 illustrates an equivalent transformer circuit, where<br />

V P = primary-terminal voltage<br />

R ex = wattful magnetizing component<br />

V S = secondary-terminal voltage<br />

Z = secondary burden (load<br />

E P = primary-induced voltage<br />

X ex = wattless magnetizing componen<br />

E S = secondary-induced voltage<br />

I ex = magnetizing current<br />

I P = primary current<br />

I S = secondary current<br />

N P = primary turns<br />

N S = secondary turns<br />

R P = primary-winding resistance<br />

R S = secondary-winding resistance<br />

X P = primary-winding reactance<br />

X S = secondary-winding reactance<br />

© 2004 by CRC Press LLC<br />

© 2004 by CRC Press LLC

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