Digital Signal Processing Reference
In-Depth Information
17.12 Finding Stripline Impedance
The impedance of a stripline trace can be found very accurately even for narrow
traces with (17.24) [11, 12]. It accounts for effects of trace thickness and fringing
and is accurate to better than 2% for wide traces under about 65
Ω
, provided that b
w
bt
is 2.6 mils (66
μ
m) or more. The trace must be wide enough so that
0.35,
and
accuracy improves for larger ratios. This is usually the case for 65
or lower traces
on FR4. Other equations are presented in [3, 11-13] for higher impedance traces.
Equation (17.24) has been recast in a simpler form similar to that presented in
[13]:
Ω
94.15
Z
=
o
C
(17.24)
w K
b
f
ε
9
+
r
8.854
ε
r
The constant K 9 is found with (17.19), and the fringing capacitance C f is found
with (17.25):
(
)
(
)
(
)
2
(17.25)
C
=
5.656
×
ε
×
K
9
×
ln
K
9
+
1
K
9
1 ln
K
9
1
f
r
Although the fringing capacitance is in pF/m, the impedance equation (17.24)
has been scaled so that w , b , and t can be in either mils or centimeters.
For example, for a 5-mil-wide, 0.65-mil-thick stripline on FR4 (
4.0) locat-
ed midway between ground planes spaced 66 mils apart, K 9 is found from (17.19)
to be 1.01. From (17.25) the fringing capacitance, C f is found to be 17.34 pF/meter
( w
ε r
=
=
66).
By using that value for C f in (17.24), Z o is found to be 88
5, t
=
0.65, b
=
Ω
. This is 12% lower
than the actual value of 100
Ω
. This inaccuracy is expected because this trace fails
w
bt
the
test.
0.35
Lowering the impedance by reducing the plane spacing to 12 mils passes the
test and makes K 9
=
1.057 and C f
=
18.85. Using this in (17.24) produces an im-
pedance of 48.8
Ω
, about 1.5% lower than the actual value.
17.13
Finding Exposed Microstrip Impedance
The impedance of a microstrip not covered in solder mask can be found with
(17.26) [11, 12]. It works best for traces under 60
on FR4 that are at least twice
as wide as the distance from the return plane ( h in Figure 17.1). The accuracy is
better than 5% [3] in those cases and improves for wide, lower impedance traces.
Ω
 
 
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