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ADS5547 Datasheet(PDF) 32 Page - Texas Instruments

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Part # ADS5547
Description  14-BIT, 210 MSPS ADC WITH DDR LVDS/CMOS OUTPUTS
PDF  50 Pages
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Manufacturer  TI [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI - Texas Instruments

ADS5547 Datasheet(HTML) 32 Page - Texas Instruments

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Input Common-Mode
210MSPS
(342 A
m ) xFs
(1)
Reference
VCM
REFM
REFP
INTREF
INTREF
EXTREF
Internal
Reference
ADS5547
Internal Reference
External Reference
ADS5547
SLWS192 – NOVEMBER 2006
APPLICATION INFORMATION (continued)
To ensure a low-noise common-mode reference, the VCM pin is filtered with a 0.1-
µF low-inductance capacitor
connected to ground. The VCM pin is designed to directly drive the ADC inputs. The input stage of the ADC
sinks a common-mode current in the order of 342
µA (at 210 MSPS). Equation 1 describes the dependency of
the common-mode current and the sampling frequency.
This equation helps to design the output capability and impedance of the CM driving circuit accordingly.
ADS5547 has built-in internal references REFP and REFM, requiring no external components. Design schemes
are used to linearize the converter load seen by the references; this and the integration of the requisite
reference capacitors on-chip eliminates the need for external decoupling. The full-scale input range of the
converter can be controlled in the external reference mode as explained below. The internal or external
reference modes can be selected by controlling the MODE pin 23 (see Table 7 for details) or by programming
the serial interface register bit <REF>.
Figure 41. Reference Section
When the device is in internal reference mode, the REFP and REFM voltages are generated internally.
Common-mode voltage (1.5 V nominal) is output on VCM pin, which can be used to externally bias the analog
input pins.
When the device is in external reference mode, the VCM acts as a reference input pin. The voltage forced on
the VCM pin is buffered and gained by 1.33 internally, generating the REFP and REFM voltages. The differential
input voltage corresponding to full-scale is given by Equation 2.
32
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