14.3 INTERFERENCE AND NOISE 657
1
f
− 5 f 0 − 4 f 0 − 3 f 0 − 2 f 0 −f 0 0 f 0 2 f 0 3 f 0 4 f 0 5 f 0
(a)
1 +
f^2
f 02
|Hp(f)| =
1
1
f
− 5 f 0 − 4 f 0 − 3 f 0 − 2 f 0 −f 0 0 f 0 2 f 0 3 f 0 4 f 0 5 f 0
(b)
1 +
f^2
f 02
|Hd(f)| =
Figure 14.3.10(a)Preemphasis
filter characteristic.(b)Deempha-
sis filter characteristic.
z(t)
x + ε
x − ε
x
t
t 1 t 2 t 3
z(t 1 )
z(t 2 ) z(t^3 )
Figure 14.3.11Constant signalx
with noise fluctuations.
G=
x
√
Pout/Nout
(14.3.11)
By takingMdifferent samples ofz(t), the arithmetic average can be seen to be
zav=
1
M
(z 1 +z 2 +...+zM) (14.3.12)
If the samples are spaced in time by at least 1/Bseconds, then the noise-induced errors tend to
cancel out and the rms error ofzavbecomes
εM=ε/
√
M (14.3.13)
This averaging method amounts to reducing the bandwidth toB/M.
When the signal in question is a sinusoid whose amplitude is to be measured, averaging
techniques can also be used by utilizing a narrow bandpass filter, or a special processor known