282 Chapter 11
inductance decreases rapidly as the number of layers is
increased.
11.1.2.4 Winding Capacitances and Faraday Shields
To allow the maximum number of turns in a given
space, the insulation on the wire used to wind trans-
formers is very thin. Called magnet wire, it is most com-
monly insulated by a thin film of polyurethane enamel.
A transformer winding is made, in general, by spinning
the bobbin shown in Fig. 11-10 on a machine similar to
a lathe and guiding the wire to form a layer one wire
thick across the length of the bobbin. The wire is guided
to traverse back and forth across the bobbin to form a
coil of many layers as shown in Fig. 11-15, where the
bobbin cross-section is the solid line on three sides of
the winding. This simple side-to-side, back-and-forth
winding results in considerable layer-to-layer capaci-
tance within a winding or winding section. More com-
plex techniques such as universal winding are
sometimes used to substantially reduce winding capaci-
tances. These capacitances within the windings are rep-
resented by CP and CS in the circuit model of Fig. 11-13.
Additional capacitances will exist between the primary
and secondary windings and are represented by capaci-
tors CW in the model. Sometimes layers of insulating
tape are added to increase the spacing, therefore reduc-
ing capacitance, between primary and secondary wind-
ings. In the bi-filar windings of Fig. 11-14, since the
wires of primary and secondary windings are side by
side throughout, the inter-winding capacitances CW can
be quite high.
In some applications, interwinding capacitances are
very undesirable. They are completely eliminated by the
use of a Faraday shield between the windings. Some-
times called an electrostatic shield, it generally takes the
form of a thin sheet of copper foil placed between the
windings. Obviously, transformers that utilize multiple
layers to reduce leakage inductance will require Faraday
shields between all adjacent layers. In Fig. 11-15 the
dark lines between the winding layers are the Faraday
shields. Normally, all the shields surrounding a winding
are tied together and treated as a single electrical
connection. When connected to circuit ground, as
shown in Fig. 11-16, a Faraday shield intercepts the
capacitive current that would otherwise flow between
transformer windings.
Faraday shields are nearly always used in trans-
formers designed to eliminate ground noise. In these
applications, the transformer is intended to respond only
to the voltage difference or signal across its primary and
have no response to the noise that exists equally (or
common-mode) at the terminals of its primary. A
Faraday shield is used to prevent capacitive coupling,
via CW in Fig. 11-13, of this noise to the secondary. For
any winding connected to a balanced line, the matching
of capacitances to ground is critical to the rejection of
Figure 11-14. Layered windings.
Figure 11-15. Bi-filar windings.
= Primary = Secondary
= Primary = Secondary
Figure 11-16. High frequency equivalent circuit of a
transformer with Faraday shield and driven by a balanced
source.
CC 1
C 1 C 3
RG 1 RP Ideal LLS RS
CS Sec
RL
CL
Faraday
CC 2 Shield
C 2 C 4
RG 2
1 N
Xfmr
Pri CPRP