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ADPD4100 데이터시트(PDF) 37 Page - Analog Devices

부품명 ADPD4100
상세설명  Multimodal Sensor Front End
PDF  101 Pages
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ADPD4100 데이터시트(HTML) 37 Page - Analog Devices

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Data Sheet
ADPD4100/ADPD4101
Rev. 0 | Page 37 of 101
Self Capacitance-Based Proximity Measurement
Capacitive proximity measurements can be performed by
measuring self capacitance. As in mutual capacitance-based
proximity measurement, the BPF is bypassed by setting
AFE_PATH_CFG_x to 0E6.
Self capacitance based proximity measurement, however,
requires only one electrode connected to one of the inputs of
ADPD4100/ADPD4101. Capacitance measurement in this case
is performed by creating the voltage difference. To create the
voltage difference, pulse TIA_VREF while the input used is
preconditioned to TIA_VREF, and read the change in the ADC
output when ΔC is induced through the change in the
proximity of the human tissue.
This measurement modality makes use of the capacitance of the
human body to the earth, and ΔC formed due to tissue proximity.
The human body capacitance allows the use of TIA_VREF
pulsing at the input as a voltage difference needed to measure
ΔC. Figure 42 shows a representation of this measurement.
Because TIA_VREF is pulsed at the input, all the extra voltage
at pulsing shows up the same way at the TIA output. Therefore,
TIA has only a positive response compared to the mutual
capacitance-based measurement. The integration sequence
must be centered in such a way that all the dc shift is canceled
and remaining small ac charge due to the change in proximity is
integrated. Figure 43 shows integration sequence timing with
respect to the TIA_VREF pulse to cancel dc shift and integrate
ac charge. The constant part in the TIA output represents the dc
charge, and it must be canceled by the integration sequence so
that only the surge charge accumulation at the positive and the
negative edges of the TIA_VREF pulse are integrated.
However, the baseline measurement without tissue in proximity
is needed to determine true ΔC, which is proportionate to the
change in ADC output read at the proximity event.
Calculate ΔC as follows. For example, when TIA_VREF is
pulsed from 0.9 V to 1.14 V by setting VREF_PULSE_VAL_x to
0, AFE_TRIM_VREF_x to 2, and VREF_PULSE_x to 1, ΔC
then becomes
ΔC = (Δ(ADC Output in LSB) × 0.92 fC/LSB ×
(RINT/2RF)/Number of Pulses)/(2 × (1.14 V − 0.9 V))
Table 22 summarizes the relevant registers for this measurement.
Integrator chop mode can be enabled for this measurement.
CINT
CINT
ELECTRODE
C
TIA
RF
RF
TIA_VREF
INx
INT
RINT
RINT
Figure 42. Self Capacitance Measurement
PRECONDITION
SENSOR
PULSE TIA_VREF
+
INTEGRATION
SEQUENCE
START OF TIME SLOT
MOD_OFFSET_x
MOD_WIDTH_x
INTEG_OFFSET_x
INTEG_WIDTH_x
TIA OUTPUT
PERIOD
(AUTOMATICALLY CALCULATED)
+
PRE_WIDTH_x
(DEFAULT 8µs)
Figure 43. Timing Diagram for Self Capacitance-Based Proximity Measurement
Table 22. Relevant Registers for Self Capacitance Based Proximity Measurement
Group
Time Slot A Register Address1
Bit Field Name
Description
Self Capacitance-Based
Proximity Setup
0x0100, Bits[13:12]
SAMPLE_TYPE_x
Leave at the default setting (0) for default
sampling mode.
0x0101, Bits[8:0]
AFE_PATH_CFG_x
Set to 0x0E6 for TIA, integrator, and ADC.
Bypass BPF.
0x0102, Bits[15:0]
INPxx_x
Enable desired inputs.
0x0103, Bits[14:12]
PRECON_x
Set to 0x5 to precondition sensor to TIA_VREF.
0x0104, Bits[5:0]
TIA_GAIN_CHx_x
Select TIA gain.
0x0104, Bits[7:6]
VREF_PULSE_VAL_x
Select 0x0 to pulse TIA_VREF to 1.14 V.
0x0104, Bits[9:8]
AFE_TRIM_VREF_x
Set to 0x2 to set TIA_VREF = 0.9 V.
0x0104, Bits[10]
VREF_PULSE_x
Set to 0x1 to pulse TIA_VREF.



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