SBASAE3 December 2025 ADS125H18
PRODUCTION DATA
The Open Wire Current Source (OWCS) on the ADS125H18 provides a diagnostic for a floating or “open wire” on the analog inputs. This is not a fully automated check. The user needs to perform several steps to use this feature. The basic idea is to measure resistance with the current sources with two conversions. If the input is floating, the measured resistance is higher than the predicted value. All OWCS tests are done on a single analog input. If measuring a differential signal using two AINn pins, each pin must be open-wire tested separately. The OWCS multiplexer (MUX) connects the current source to the appropriate input pin as selected by the STEPx_AIN[4:0]. Bit settings of 00000b to 01111b are valid for STEPx_AIN[4:0] when using the OWCS, all other settings - i.e. 10000b to 11111b - are ignored. Set the STEPx_OWCS_EN bit on the step configuration page x to enable the open wire current source.
The recommended sequence for performing an open wire check at an input pin AINn is:
| DEVICE VARIANT | THRESHOLD |
|---|---|
| V12 (±12V) | +17.4% |
| V20 (±20V) | +23.8% |
| V40 (±40V) | +24.4% |
The conclusion for a floating input is not definite due to the following assumption: This open-wire test assumes that the input voltage is not changing between the first and second conversion. If this assumption does not hold, a false positive can occur. Also, if the source impedance is not equal to 0 for non-fault and infinite for a fault condition, then the delta between floating and connected state is reduced, making determining if the value is sufficiently above or below the threshold difficult.
The OWCS works with either internal voltage reference value or an external reference between 2V and AVDD. Due to the ratiometric nature of the OWCS measurement, the reference value does not affect the expected delta in readings.
The OWCS decision thresholds are calculated as follows:
The OWCS current magnitude linearly tracks VREF with a nominal value of 2μA/V of VREF for the ±20V version of ADS125H18. The VREF value used by the OWCS is derived from a node after the VREF multiplexer. Thus, whatever reference, internal or external, supplies the modulator also is used by the OWCS. For a 2.5V VREF, OWCS = 2.5μA. For a 4.0V VREF, OWCS = 4.0μA. This relationship with VREF allows the threshold value mentioned previously to be a fixed % of full scale (or code value or “output referred”), that is, the value is independent of VREF. The OWCS also tracks SiCr resistance so variations in the attenuator absolute values of resistance cancels out as well.
To calculate the expected deltas, see the block diagram in Figure 7-28. Note the IR drop across the OWCS Multiplexer (OWmux) switch is not seen by the ADC and also that the input multiplexer (INmux) resistance doesn’t see the OW current. The first conversion (baseline) has the value Vconv1 = Vbaseline. The second conversion results in Vconv2 = Vbaseline + VIRdrop. The delta between the conversions is VIRdrop where the IVIRdrop = I(OWCS) × Rthev.
The OWCS tracks Vref and drops out, resulting in:
delta (%FSR) = (1μA/Ω) × (Rthev)
For non-fault (non-open) sources, assume for now Rsrc = 0. Then:
Rthev = (R1 || (R2/2))
For faulted (opened/floating) sources, assume for now Rsrc = ∞. Then:
Rthev = R2/2
Table 7-30 shows the typical deltas expected between the two ADC conversions on both a “good” or non-fault input pin, and also on a “bad” or faulted (open/floating) input.
| DEVICE VARIANT |
TYPICAL DELTA (%FSR) Rsrc = 0 "non-fault" |
TYPICAL DELTA (%FSR) Rsrc = ∞ "fault" or "open-wire" |
|---|---|---|
| V12 (±12V) | +16.1% | +18.7% |
| V20 (±20V) | +22.5% | +25.0% |
| V40 (±40V) | +23.7% | +25.0% |
To detect an open-wire condition, compare the measured delta against the threshold shown in Table 7-45. For example, if the delta is 22.9% (±20V Variant), there is no indication of an open wire.
Note that the measured delta depends on the source impedance, however Table 7-30 assumes that the source impedance is infinite for the open wire condition. In a real system, if there is a wire break with some residual connectivity, the source impedance can practically be finite, and can be in the order of several hundred kΩ or several MΩ. Figure 7-29 shows the variation of the delta with the source impedance from 10Ω to 10GΩ. Note that the delta is mostly constant from 10Ω up to about 100kΩ, then starts increasing and then approaches the ideal value closely above 10MΩ.
Table 7-31 lists the delta values for a few source impedance values, based on the data from Figure 7-29.
| DEVICE VARIANT |
TYPICAL DELTA (%FSR) Rsrc = 100kΩ |
TYPICAL DELTA (%FSR) Rsrc = 1MΩ |
TYPICAL DELTA (%FSR) Rsrc = 10MΩ |
|---|---|---|---|
| V12 (±12V) | +16.3% | +17.2% | +18.4% |
| V20 (±20V) | +22.7% | +23.6% | +24.7% |
| V40 (±40V) | +23.8% | +24.3% | +24.9% |
The thresholds suggested in Table 7-45 represent a source impedance value of 1.3MΩ (V12) and 1.4MΩ (V20, V40) according to Figure 7-29 and Table 7-31, meaning any source impedance higher than this value is considered an open wire when using the recommended thresholds. If the source impedance in the system is in the order of 100kΩ or larger, a threshold higher than listed in Table 7-45 can be chosen.
Note the settling requirement for the OWCS as follows:
The OWCS turns on and off between steps as defined on two subsequent step configuration pages. Be sure to allow time for settling before beginning a conversion. Capacitance on the sensor output reacts with the ADS125H18 resistor attenuator and slows the settling when turning on or off the OWCS. A simplified analysis below assumes the resistance is R1 and settling to 5 τ or ≅99% of the final value. Verify that there is time to settle between conversions used to calculate the delta. Keeping the source capacitance as low as possible helps to speed up settling.
| Csrc | TIME TO SETTLE TO 5 τ, 99% |
|---|---|
| 1pF | 26μs |
| 10pF | 80μs |
| 100pF | 620μs |
| 1nF | 6ms |
| 10nF | 60ms |
| 100nF | 600ms |
| 1µF | 6s |