4.7 Convergence of the Fourier Series 269
nExample 4.10
Consider the mean-square error optimization to obtain an approximation of the periodic sig-
nalx(t)shown in Figure 4.4 from Example 4.5. We wish to obtain an approximatex 2 (t)=
α+ 2 βcos( 0 t), given that it is clear thatx(t)has an average, and that once we subtract it from the
signal the resulting signal is approximated by a cosine function. Minimize the mean-square error
E 2 =
1
T 0
∫
T 0
|x(t)−x 2 (t)|^2 dt
with respect toαandβto find these values.
Solution
To minimizeE 2 we set to zero its derivatives with respect toαandβto get
dE 2
dα
=−
1
T 0
∫
T 0
2[x(t)−α− 2 βcos( 0 t)]dt=−
1
T 0
∫
T 0
2[x(t)−α]dt= 0
dE 2
dβ
=−
1
T 0
∫
T 0
2[x(t)−α− 2 βcos( 0 t)] cos( 0 t)dt= 0
which, after getting rid ofT^20 of both sides of the above equations and applying the orthogonality
of the Fourier basis, gives
α=
1
T 0
∫
T 0
x(t)dt
β=
1
T 0
∫
T 0
x(t)cos( 0 t)dt
For the signal in Figure 4.4 we obtain
α= 1
β=
2
π
giving as approximation the signal
x 2 (t)= 1 +
4
π
cos( 2 πt)
which att=0 gives x 2 ( 0 )=2.27 instead of the expected 2;x 2 (0.25)=1 (because of the
discontinuity at this point, this value is the average of 2 and 0, the values, respectively, before
and after the discontinuity) instead of 2 andx 2 (0.5)=−0.27 instead of the expected 0. n