In this section, theoretical signal-to-noise ratio (SNR) due to quantization noise and aperture
jitter is discussed. Practical specifications for real ADCs are then presented.
2.3.1 Theoretical Signal-to-Noise Ratio Specifications
and the input signal. First, it is assumed that the noise present is due to quantization error only.
The amplitude of this quantization noise is assumed to be a random variable uniformly
11
distributed over one quantization step. Assuming a sinusoidal input with an amplitude equal to
the FSR of the ADC, the maximum possible theoretical SNR is given as
SNR = 6.02B + 1.76 + 10 log
10
f
s
2f
max
(dB)
(1)
where f
s
is the sampling frequency and f
max
is the maximum frequency of the input analog signal
[2],[9]. The commonly stated theoretical SNR of 6B (dB) is an approximation to this equation
when f
s
= 2f
max
and the 1.76 dB is neglected. From this equation, note that as the sampling
frequency is increased beyond 2f
max
, the SNR increases. This occurs because the quantization
noise power, which is a fixed amount and independent of bandwidth (P
qn
= q
2
/12R), is spread out
over an increasingly wider band as the sampling frequency is increased. This lessens the amount
of the quantization noise that falls within the 0 to f
s
/2 band. Figure 4 shows this phenomenon.
Consequently, oversampling increases the maximum possible SNR. Such oversampling is
sometimes used to realize a greater maximum SNR than at first appears possible. An 8-bit ADC,
with a sampling rate of 20 Msamples/s, for example, can provide 68 dB rather than 48 dB of
maximum SNR for 100-kHz signals in the passband if appropriate digital filtering is used to
recover the 100-kHz signal.
Figure 4. Frequency-spreading of quantization noise power due to oversampling.
Besides being limited by the quantization step size (resolution), the SNR of the ADC also is
limited by aperture jitter. Aperture jitter is the variation in time of the exact sampling instant.
Aperture jitter can be caused externally by jitter in the sampling clock, or internally since the
sampling switch does not open at precise times. Aperture jitter causes a phase modulation of the
sampled signal and thus results in an additional noise component in the sampled signal [10]. The
A
A
P
o
w
er
P
o
w
er
f
s
= f
max
P
qn
=
q
1 R
f
s
=f
max
0
f
0
f
f
max
fs
f
s
≫ f
max
P
qn
=
q
1 R
12
maximum analog input frequency of the ADC is limited by this aperture jitter since the SNR due
to aperture jitter (SNR
aj
) degrades as the input frequency increases. The SNR
aj
is given as
SNR
aj
= 20 log
10
1
2π f
max
t
a
where t
a
is the aperture jitter of the ADC [2]. For sampling at f
s
=2f
max
, both the SNR due to
quantization noise and the SNR due to aperture jitter can be combined to give the overall
SNR [11].
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