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Higher Order Delta Functions
vt vt
V
– t + 5
3
2 – t + 6
1
1 0 1 2 3 4 5 6 7
ts
1
2t
2
Figure 3.22. Equations for the linear segments of Figure 3.21
vt = 2tu t + 0 1 – 2tu t – 1 – 2u t – 1 – 2u t – 2 – tu t – 2
0
0
0
0
+ 5u t – 0 2 + tu t – 4 – 5u t – 4 + u t – 4 – u t – 5
0
0
0
0
tu t – – 0 5 + 6u t – 5 + tu t – 7 – 6u t – 7
0
0
0
or
vt = 2tu t + 0 1 + – 2t + 2 u t – 1 + – t + 3 u t – 2
0
0
+ t – 4 u t – 0 4 + – t + 5 u t – 5 + t – 6 u t – 7
0
0
b. The derivative of vt is
dv 2u t + 1 + 2tG t + 1 – 2u t – 1 + – 2t + 2 G t – 1
------ =
dt 0 0
(3.53)
u t – – 0 2 + – t + 3 G t – 2 + u t – 4 + t – 4 G t – 4
0
u t – – 0 5 + – t + 5 G t – 5 + u t – 7 + t – 6 G t – 7
0
From the given waveform, we observe that discontinuities occur only at t = – 1 , t = 2 , and
t = 7 . Therefore, G t – 1 = 0 , G t – 4 = 0 , and G t – 5 = 0 , and the terms that contain these
delta functions vanish. Also, by application of the sampling property,
–
2tG t + 1 = ^ 2t ` G t + 1 = 2G t + 1
t = – 1
– t + 3 G t – 2 = – t + 3 ^ ` G t – 2 = G t – 2
t = 2
t – 6 G t – 7 = t – 6 ^ ` G t – 7 = G t – 7
t = 7
and by substitution into (3.53), we get
Circuit Analysis II with MATLAB Applications 3-17
Orchard Publications