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LTC1290 Datasheet(PDF) 22 Page - Linear Technology

Part # LTC1290
Description  Single Chip 12-Bit Data Acquisition System
Download  28 Pages
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Manufacturer  LINER [Linear Technology]
Direct Link  http://www.linear.com
Logo LINER - Linear Technology

LTC1290 Datasheet(HTML) 22 Page - Linear Technology

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LTC1290
S
APPLICATI
I FOR ATIO
6. Reduced Reference Operation
The effective resolution of the LTC1290 can be increased
by reducing the input span of the converter. The LTC1290
exhibits good linearity and gain over a wide range of
reference voltages (see the typical curves of Linearity and
Gain Error vs Reference Voltage). However, care must be
taken when operating at low values of VREF because of the
reduced LSB step size and the resulting higher accuracy
requirement placed on the converter. The following factors
must be considered when operating at low VREF values:
1. Offset
2. Noise
Offset with Reduced VREF
The offset of the LTC1290 has a larger effect on the output
code when the A/D is operated with reduced reference
voltage. The offset (which is typically a fixed voltage)
becomes a larger fraction of an LSB as the size of the LSB
is reduced. The typical curve of Unadjusted Offset Error vs
Reference Voltage shows how offset in LSBs is related to
reference voltage for a typical value of VOS. For example,
a VOS of 0.1mV which is 0.1LSB with a 5V reference
becomes 0.4LSB with a 1.25V reference. If this offset is
unacceptable, it can be corrected digitally by the receiving
system or by offsetting the “–” input to the LTC1290.
Noise with Reduced VREF
The total input referred noise of the LTC1290 can be
reduced to approximately 200
µV peak-to-peak using a
ground plane, good bypassing, good layout techniques
and minimizing noise on the reference inputs. This noise
is insignificant with a 5V reference but will become a larger
fraction of an LSB as the size of the LSB is reduced. The
typical curve of Noise Error vs Reference Voltage shows
the LSB contribution of this 200
µV of noise.
For operation with a 5V reference, the 200
µV noise is only
0.16LSB peak-to-peak. In this case, the LTC1290 noise
will contribute virtually no uncertainty to the output code.
However, for reduced references, the noise may become
a significant fraction of an LSB and cause undesirable jitter
in the output code. For example, with a 1.25V reference,
this same 200
µV noise is 0.64LSB peak-to-peak. This will
reduce the range of input voltages over which a stable
output code can be achieved by 0.64LSB. In this case
averaging readings may be necessary.
This noise data was taken in a very clean setup. Any setup
induced noise (noise or ripple on VCC, VREF, VIN or V) will
add to the internal noise. The lower the reference voltage
to be used, the more critical it becomes to have a clean,
noise-free setup.
7. LTC1290 AC Characteristics
Two commonly used figures of merit for specifying the
dynamic performance of the A/D’s in digital signal pro-
cessing applications are the Signal-to-Noise Ratio (SNR)
and the “effective number of bits (ENOB).” SNR is defined
as the ratio of the RMS magnitude of the fundamental to
the RMS magnitude of all the nonfundamental signals up
to the Nyquist frequency (half the sampling frequency).
The theoretical maximum SNR for a sine wave input is
given by:
SNR = (6.02N + 1.76dB)
where N is the number of bits. Thus the SNR is a function
of the resolution of the A/D. For an ideal 12-bit A/D the SNR
is equal to 74dB. A Fast Fourier Transform(FFT) plot of the
output spectrum of the LTC1290 is shown in Figures 17a
and 17b. The input (fIN) frequencies are 1kHz and 25kHz
with the sampling frequency (fS) at 50.6kHz. The SNR
obtained from the plot are 73.25dB and 72.54dB.
Rewriting the SNR expression it is possible to obtain the
equivalent resolution based on the SNR measurement.
N = (SNR – 1.76dB)/6.02
This is the so-called effective number of bits (ENOB). For
the example shown in Figures 17a and 17b, N = 11.9 bits
and 11.8 bits, respectively. Figure 18 shows a plot of ENOB
as a function of input frequency. The curve shows the
A/D’s ENOB remain in the range of 11.9 to 11.8 for input
frequencies up to fS/2.
Figure 19 shows an FFT plot of the output spectrum for two
tones applied to the input of the A/D. Nonlinearities in the
A/D will cause distortion products at the sum and differ-
ence frequencies of the fundamentals and products of the


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