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LTC2495 Datasheet(PDF) 23 Page - Linear Technology |
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LTC2495 Datasheet(HTML) 23 Page - Linear Technology |
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23 / 32 page ![]() LTC2495 23 2495f input/reference pins. If the total external RC time constant is less than 580ns the errors introduced by the sampling process are negligible since complete settling occurs. Typically, the reference inputs are driven from a low impedance source. In this case, complete settling occurs even with large external bypass capacitors. The inputs (CH0-CH15, COM), on the other hand, are typically driven from larger source resistances. Source resistances up to 10k may interface directly to the LTC2495 and settle completely; however, the addition of external capacitors at the input terminals in order to filter unwanted noise (antialiasing) results in incomplete settling. The LTC2495 offers two methods of removing these errors. The first is automatic differential input current cancellation (Easy Drive) and the second is the insertion of an external buffer between the MUXOUT and ADCIN pins, thus isolating the input switching from the source resistance. Automatic Differential Input Current Cancellation In applications where the sensor output impedance is low (up to 10k Ω with no external bypass capacitor or up to 500 Ω with 0.001µF bypass), complete settling of the Figure 11. Equivalent Analog Input Circuit input occurs. In this case, no errors are introduced and direct digitization is possible. For many applications, the sensor output impedance combined with external input bypass capacitors produces RC time constants much greater than the 580ns required for 1ppm accuracy. For example, a 10k Ω bridge driving a 0.1µF capacitor has a time constant an order of magnitude greater than the required maximum. The LTC2495 uses a proprietary switching algorithm that forces the average differential input current to zero independent of external settling errors. This allows direct digitization of high impedance sensors without the need for buffers. The switching algorithm forces the average input current on the positive input (IIN +) to be equal to the average input current on the negative input (IIN –). Over the complete conversion cycle, the average differential input current (IIN + – IIN–) is zero. While the differential input current is zero, the common mode input current (IIN + + IIN–)/2 is proportional to the difference between the common mode input voltage (VIN(CM)) and the common mode reference voltage (VREF(CM)). APPLICATIONS INFORMATION IN+ IN– 10k Ω INTERNAL SWITCH NETWORK 10k Ω CEQ 12 µF 10k Ω IIN – REF+ IREF + IIN + IREF – 2495 F11 SWITCHING FREQUENCY fSW = 123kHz INTERNAL OSCILLATOR fSW = 0.4 • fEOSC EXTERNAL OSCILLATOR REF– 10k Ω 100 Ω INPUT MULTIPLEXER EXTERNAL CONNECTION 100 Ω MUXOUTP ADCINP EXTERNAL CONNECTION MUXOUTN ADCINN IIN IIN VV R AVG AVG IN CM REF CM EQ + () = () = − • – () () . 05 IIREF VV V R AVG REF REF CM IN CM + () ≈ + () 15 05 .– .• () () E EQ IN REF EQ REF REF CM V VR where V REF REF V – • : ( 2 =− +− )) – , = ⎛ ⎝ ⎜⎜ ⎞ ⎠ ⎟⎟ =− +− +− + REF REF V IN IN WHERE IN AN IN 2 D D IN ARE THE SELECTED INPUT CHANNELS V IN IN CM − + = () – – . IN R M INTERNAL OSCILLATOR EQ − ⎛ ⎝ ⎜⎜ ⎞ ⎠ ⎟⎟ = 2 271 6 Ω 0 0Hz MODE R 2.98M INTERNAL OSCILLATOR 50Hz/60 EQ =Ω H Hz MODE R 0.833 10 /f EXTERNAL OSCIL EQ 12 EOSC =• () L LATOR |
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