Audio Transformers 281
turns of heavier wire is needed for the secondary.
Compare this to the total of 240 turns of heavier wire
required in the transformer.
A step-down auto-transformer is shown in the
bottom diagram of Fig. 11-12. Operation is similar
except that the secondary is connected so that its instan-
taneous polarity subtracts from or bucks the input
voltage. For example, we could step down U.S. 120 Vac
power to Japanese 100 Vac power by configuring a
100 V to 20 V step-down transformer as an auto-trans-
former. Thus, a 100 W load can be driven using only a
20 W rated transformer.
The windings of low level audio transformers may
consist of hundreds or even many thousands of turns of
wire, sometimes as small as #46 gauge, whose 0.0015
inch diameter is comparable to a human hair. As a
result, each winding may have a dc resistance as high as
several thousand ohms. Transformer primary and
secondary winding resistances are represented by RP
and RS, respectively, in Fig. 11-8.
11.1.2.3 Leakage Inductance and Winding Techniques
In an ideal transformer, since all flux generated by the
primary is linked to the secondary, a short circuit on the
secondary would be reflected to the primary as a short
circuit. However, in real transformers, the unlinked flux
causes a residual or leakage inductance that can be mea-
sured at either winding. Therefore, the secondary would
appear to have residual inductance if the primary were
shorted and vice-versa. The leakage inductance is
shown as LL in the model of Fig. 11-13. Note that leak-
age inductance is reflected from one winding to another
as the square of turns ratio, just as other impedances are.
The degree of flux coupling between primary and
secondary windings depends on the physical spacing
between them and how they are placed with respect to
each other. The lowest leakage inductance is achieved
by winding the coils on a common axis and as close as
possible to each other. The ultimate form of this tech-
nique is called multi-filar winding where multiple wires
are wound simultaneously as if they were a single
strand. For example, if two windings—i.e. primary and
secondary—are wound as one, the transformer is said to
be bi-filar wound. Note in the cross-section view of Fig.
11-14 how the primary and secondary windings are
side-by-side throughout the entire winding. Another
technique to reduce leakage inductance is to use
layering, a technique in which portions or sections of the
primary and/or secondary are wound in sequence over
each other to interleave them. For example, Fig. 11-15
shows the cross-section of a three-layer transformer
where half the primary is wound, then the secondary,
followed by the other half of the primary. This results in
considerably less leakage inductance than just a
secondary over primary two-layer design. Leakage
Figure 11-12. Auto-transformers employ a buck/boost
principle.
EP
EP
EP
IP
IP IS RL
IP
IS
IS
RL
RL
Figure 11-13. Transformer high frequency parasitic
elements.
CW
RG RP IDEAL LL RS
CS SEC
RL
CL
CW
XFMR
RC
PRI CP^1 N