Digital Signal Processing Reference
In-Depth Information
4-2
For coupled striplines from Problem 4-1, calculate the near- and far-end
noise for the isolated switching case, and compare your results against
simulation with each line terminated at both ends in the characteristic
impedance calculated.
4-3
Use the SLEM method to calculate the effective impedance and propa-
gation velocity for the coupled striplines shown whose capacitance and
inductance matrices are shown below when all three lines switch in the
same direction. Compare the propagation delay for a 0.5-m coupled length
when only the middle line switches.
10
−
7
10
−
8
10
−
8
3
.
480
×
5
.
268
×
1
.
687
×
10
−
8
10
−
7
10
−
8
L
=
5
.
268
×
3
.
461
×
5
.
268
×
H
/
m
10
−
8
10
−
8
10
−
7
1
.
687
×
5
.
268
×
3
.
480
×
10
−
10
10
−
11
10
−
11
1
.
087
×
−
1
.
172
×
−
7
.
918
×
10
−
11
10
−
10
10
−
11
C
=
−
1
.
172
×
1
.
105
×
−
1
.
172
×
F
/
m
10
−
11
10
−
11
10
−
10
−
7
.
918
×
−
1
.
172
×
1
.
087
×
4-4
Estimate crosstalk pulse amplitudes and pulse widths on the middle lines
of the three-line system from Problem 4-3 when the two outer lines are
switching from low to high. Assume that each line is terminated at both
ends in its characteristic impedance. Compare your results against a fully
coupled simulation.
4-5
Sketch the far-end crosstalk pulse for a two-line case with no termination
at the near end, and matched termination at the far end.
4-6
Use the inductance and capacitance matrices below to determine the
switching activity on lines 1 and 2, given the waveform on line 3 in
Figure 4-32.
10
−
7
10
−
8
10
−
9
×
×
×
3
.
544
1
.
914
5
.
161
10
−
8
10
−
7
10
−
8
L
=
1
.
914
×
3
.
826
×
1
.
914
×
H
/
m
10
−
9
10
−
8
10
−
7
5
.
161
×
1
.
914
×
3
.
544
×
10
−
11
10
−
11
10
−
11
8
.
266
×
−
1
.
108
×
−
2
.
354
×
10
−
11
10
−
10
10
−
11
C
=
−
1
.
108
×
1
.
001
×
−
1
.
108
×
F
/
m
10
−
11
10
−
11
10
−
11
−
2
.
354
×
−
1
.
108
×
8
.
266
×
4-7
Use the inductance and capacitance matrices from Problem 4-6 to deter-
mine the switching activity on lines 1 and 3 given the waveform on line
2 in Figure 4-33.
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