Digital Signal Processing Reference
In-Depth Information
The surface impedance can be defined as the ratio of the electric field at the
surface and the total current density:
E
0
J
T
Z
s
=
(5-27)
Substituting (5-26) into (5-27) and expressing the current density in terms of the
conductivity and the electric field (
J
0
=
σ E
0
) yields
E
0
1
σδ
Z
s
=
1
)
=
(
1
+
j)
ohms
/
square
(5-28)
2
σ E
0
δ(j
−
1
−
The surface impedance is expressed in terms of an area of unit width and unit
length, so the term
ohms/square
is used. Note the similarity of the real part of
(5-28) to equation (5-12), which was the series resistance caused by the skin effect
of a transmission line. For the case where
l
=
w
, the real part of equations (5-28)
and (5-12) are identical. If the real part of (5-28) is resistance, the imaginary part
must therefore be reactance (the impedance of inductance). Since the impedance
of inductance is
jωL
, (5-28) can be expressed in terms of a series resistance
(due to the skin effect) and a series inductance (the internal inductance):
Z
s
=
R
ac
+
jωL
internal
(5-29)
Therefore,
the internal inductance can be calculated directly from the ac resis-
tance
:
R
ac
ω
L
internal
=
(5-30)
Equation (5-30) highlights an important relationship between the skin effect resis-
tance (ac resistance) and the internal inductance. As the skin effect forces the
current to the periphery of the conductor, the resistance increases; however,
since current ceases to flow in the interior of the conductor, the inductance must
decrease. Figure 5-11 plots both the internal inductance and the ac resistance.
Note that when the ac resistance becomes significant, the internal inductance is
almost negligible.
Example 5-2
Calculate the total inductance and the resistance at 2 GHz of a
microstrip transmission line constructed with copper of conductivity
σ
=
5
.
8
×
10
7
(
·
m
)
−
1
, a dielectric constant of
ε
r
=
4
.
0 and the following cross-sectional
dimensions:
t
=
0
.
5 mil,
h
=
2 mils,
w
=
3 mils.
SOLUTION
Step 1:
Determine if the ac or dc resistance should be used. The methodology
presented in Example 5-1 could be used, however, it is easier simply to calculate
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