ZHCSBO2H December 2012 – July 2014 AFE4400
PRODUCTION DATA.
The AFE4400 can be used for measuring SPO2 and for monitoring heart rate. The high dynamic range of the device enables measuring SPO2 with a high degree of accuracy even under low-perfusion (ac-to-dc ratio) conditions. An SPO2 measurement system involves two different wavelength LEDs—usually Red and IR. By computing the ratio of the ac to dc at the two different wavelengths, the SPO2 can be calculated. Heart rate monitoring systems can also benefit from the high dynamic range of the device, which enables capturing a high-fidelity pulsating signal even in cases where the signal strength is low.
For more information on application guidelines, refer to the AFE44x0SPO2EVM User's Guide (SLAU480).
Device connections in a typical application are shown in Figure 108. Refer to the AFE44x0SPO2EVM User's Guide (SLAU480) for more details. The schematic in Figure 108 is a part of the AFE44x0SPO2EVM and shows a cabled application in which the LEDs and photodiode are connected to the AFE4400 through a cable. However, in an application without cables, the LEDs and photodiode can be directly connected to the TXP, TXN and INP, INN pins directly, as shown in the Design Requirements section.
An SPO2 application usually involves a Red LED and an IR LED. These LEDs can be connected either in the common anode configuration or H-bridge configuration to the TXP, TXN pins. Figure 109 shows common anode configuration and Figure 110 shows H-bridge configuration.
The photodiode receives the light from both the Red and IR phases and usually has good sensitivities at both these wavelengths.
The photodiode connected in this manner operates in zero bias because of the negative feedback from the transimpedance amplifier. The connections of the photodiode to the AFE inputs are shown in Figure 111.
The signal current generated by the photodiode is converted into a voltage by the transimpedance amplifier, which has a programmable transimpedance gain. The rest of the signal chain then presents a voltage to the ADC. The full-scale output of the transimpedance amplifier is ±1 V and the full-scale input to the ADC is ±1.2 V. An automatic gain control loop can be used to set the target dc voltage at the ADC input to approximately 50% of full scale. This type of AGC loop can control a combination of LED current and TIA gain to achieve this target value; see Figure 112.
The ADC output is a 22-bit code that is obtained by discarding the two MSBs of the 24-bit registers. The data format is binary twos complement format, MSB first. TI recommends that the input to the ADC does not exceed ±1 V (which is approximately 80% full-scale) because the TIA has a full-scale range of ±1 V.
The dc component of the current from the PPG signal is referred to as Pleth (short for photoplethysmography) current. The input-referred noise current (referred differentially to the INP, INN inputs) as a function of the Pleth current is shown in Figure 113 at a PRF of 100 Hz and for various duty cycles of LED pulsing. For example, a duty cycle of 25% refers to a case where the LED is pulsed for 25% of the pulse repetition period and the receiver samples the photodiode current for the same period of time. The noise shown in Figure 113 is the integrated noise over a 5-Hz bandwidth from dc.