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ADS1013-Q1 Datasheet(PDF) 11 Page - Texas Instruments

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Part # ADS1013-Q1
Description  Automotive, Low-Power, I2C-Compatible, 3.3-kSPS, 12-Bit ADCs With Internal Reference, Oscillator, and Programmable Comparator
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Manufacturer  TI1 [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI1 - Texas Instruments

ADS1013-Q1 Datasheet(HTML) 11 Page - Texas Instruments

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t
SAMPLE
ON
OFF
S
1
S
2
OFF
ON
Equivalent
Circuit
fMOD = 250 kHz
ZCM
ZDIFF
ZCM
AINN
AINP
0.7 V
0.7 V
S1
S1
CA1
CB
CA2
S2
S2
0.7 V
0.7 V
AINN
AINP
11
ADS1013-Q1, ADS1014-Q1, ADS1015-Q1
www.ti.com
SBAS511B – JULY 2010 – REVISED DECEMBER 2016
Product Folder Links: ADS1013-Q1 ADS1014-Q1 ADS1015-Q1
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Copyright © 2010–2016, Texas Instruments Incorporated
Feature Description (continued)
8.3.2 Analog Inputs
The ADS101x-Q1 use a switched-capacitor input stage where capacitors are continuously charged and then
discharged to measure the voltage between AINP and AINN. The frequency at which the input signal is sampled
is called the sampling frequency or the modulator frequency (fMOD). ADS101x-Q1 has a 1-MHz internal oscillator
that is further divided by a factor of 4 in order to generate fMOD at 250 kHz. The capacitors used in this input
stage are small, and to external circuitry, the average loading appears resistive. This structure is shown in
Figure 11. The resistance is set by the capacitor values and the rate at which they are switched. Figure 12
shows the setting of the switches illustrated in Figure 11. During the sampling phase, switches S1 are closed.
This event charges CA1 to V(AINP), CA2 to V(AINN), and CB to (V(AINP) – V(AINN)). During the discharge phase, S1 is
first opened and then S2 is closed. Both CA1 and CA2 then discharge to approximately 0.7 V and CB discharges to
0 V. This charging draws a very small transient current from the source driving the ADS101x-Q1 analog inputs.
The average value of this current can be used to calculate the effective impedance (Zeff), where Zeff = VIN /
IAVERAGE.
Figure 11. Simplified Analog Input Circuit
Figure 12. S1 and S2 Switch Timing
The common-mode input impedance is measured by applying a common-mode signal to the shorted AINP and
AINN inputs and measuring the average current consumed by each pin. The common-mode input impedance
changes depending on the full-scale range, but is approximately 6 M
Ω for the default full-scale range. In
Figure 11, the common-mode input impedance is ZCM.
The differential input impedance is measured by applying a differential signal to AINP and AINN inputs where one
input is held at 0.7 V. The current that flows through the pin connected to 0.7 V is the differential current and
scales with the full-scale range. In Figure 11, the differential input impedance is ZDIFF.
Make sure to consider the typical value of the input impedance. Unless the input source has a low impedance,
the ADS101x-Q1 input impedance may affect the measurement accuracy. For sources with high-output
impedance, buffering may be necessary. Active buffers introduce noise, and also introduce offset and gain
errors. Consider all of these factors in high-accuracy applications.
The clock oscillator frequency drifts slightly with temperature; therefore, the input impedances also drift. For most
applications, this input impedance drift is negligible, and can be ignored.


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