P.O. Pro
WIRELESS REFLECTANCE PULSE OXIMETER
Design 1
November 10, 2004
Team # 3
James Hart
Sofia Iddir
Rob Mahar
Naomi Thonakkaraparayil
Table of Contents
Introduction
I Principles of Oximetry
i Figure 1: Absorption Spectra
ii Figure 2: Light Intensity
II Design of Pulse Oximetry Instrumentation
i Figure 3: Overall Block Diagram
ii Figure 4: Swiching of Power Supply
iii Figure 5: LED Circuits
iv Figure 6: Alternative LED Circuits
a) Timing Circuit
v Figure 7: Generating Timing Pulses
b) Pulsing the Light Output
vi Figure 8: Pulsing the LEDs
c) Receiver Circuit
vii Figure 9: Photodiode
d) Sample and Hold Circuit
viii Figure 10: Sample and Hold Circuit
e) Automatic Gain Control Circuit
III Evaluation of Pulse Oximetry Data
a) Accuracy, Bias, Precision, and Confidence Limit
b) What do Pulse Oximeters Really Measure
c) Alarm
ix Figure 11: Schematic of Alarm
IV Wireless Communication
x Figure 12: Block Diagram of Wireless Communication
a) Transmitter/Receiver Communication
xi Figure 13a,b: Block Diagram of Transmitter and Receiver
b) Wi.232
xii Figure 14: Wi.232 Pin Diagram
xiii Figure 15: Wi.232 Mechanical Drawing
V Conclusion
Introduction
Blood oxygen content is now considered the 5th vital sign, joining: temperature, respiratory rate, heart rate and blood pressure [Briggs, 1999; Hill, 2000]. One of the main advantages of pulse oximetry is that measurements are taken non-invasively through optical measurements. The P.O. Pro is a wireless reflectance pulse oximeter device designed to monitor the blood oxygen content and pulse rate of newborn babies and small children. Parents will be able to rest easier knowing that if their child stops breathing or is having trouble breathing at any point, they will be notified by an alarm going off from a portable beeper device.
I Principles of Oximetry
A pulse oximeter measures and displays the pulse rate and the saturation of hemoglobin in arterial blood. This saturation of hemoglobin is a measure of the average amount of oxygen bound to each hemoglobin molecule. The absorption of visible light by a hemoglobin solution varies with oxygenation. The chemical binding of the different types of hemoglobin species changes the physical properties of the hemoglobin as well. The oxygen chemically combined with hemoglobin inside the red blood cells makes up nearly all of the oxygen present in the blood (there is also a very small amount which is dissolved in the plasma).
Oxygen saturation, which is often referred to as SaO2 or SpO2, is defined as the ratio of oxyhemoglobin (HbO2) to the total concentration of hemoglobin present in the blood:
Oxyhemoglobin (HbO2) and hemoglobin (Hb), have significantly different optical
spectra in the wavelength range from 600nm to 1000nm, as shown in Figure 1
Figure 1: Absorption spectra of Hb and HbO2 (the isobestic point is the wavelength at which the absorption by the two forms of the molecule is the same).
The P.O Pro will measure Arterial SaO2 and express it as a percentage. Under normal physiological conditions arterial blood is 97% saturated, while venous blood is 75% saturated. The difference in absorption spectra of HbO2 and Hb is used for the measurement of arterial oxygen saturation because the wavelength range between 600 nm and 1000nm is also the range for which there is least attenuation of light by body tissues (tissue and pigmentation absorb blue, green and yellow light and water absorbs the longer infra-red wavelength).
The half power spectral bandwidth of each LED is approximately 20-30nm. The LED’s and photodiode chips are to be mounted on separate ceramic substrates. A small amount of clear epoxy resin will be applied over the LED’s and photodiode for protection. Recessing and optically shielding the LED’s and photodiode inside the sensor will minimize undesired specular light reflection from the surface of the skin and from the direct light path between the LED’s and photodiode.
A mathematical model for the P.O Pro begins by considering light at two wavelengths, l1 and l2 passing through tissue and being detected at a distant location. At each wavelength the total light attenuation is described by four different component absorbencies: oxyhemoglobin in the blood (concentration C0, molar absorptivity a0, and effective path length L0), "reduced" deoxyhemoglobin in the blood (concentration Cr molar absorptivity ar and effective path length Lr,), specific variable absorbencies that are not from the arterial blood (concentration Cx molar absorptivity ax and effective path length Lx), and all other non-specific sources of optical attenuation, combined as Ay which can include light scattering, geometric factors, and characteristics of the emitter and detector elements. The total absorbance at the two wavelengths can then be written:
The blood volume change due to the arterial pulse results in a modulation of the measured absorbencies. By taking the time rate of change of the absorbencies, the two last terms in each equation are effectively zero, since the concentration and effective path length of absorbing material outside the arterial blood do not change during a pulse:
All the nonspecific effects on light attenuation are also effectively invariant on the time scale of a cardiac cycle:
Since the extinction coefficients are constant, and the blood concentrations are constant on the time scale of a pulse, the time-dependent changes in the absorbencies at the two wavelengths can be assigned entirely to the change in the blood path length (). With the additional assumption that these two blood path length changes are equivalent (or more generally, their ratio is a constant), the ratio R of the time rate of change of the absorbance at wavelength 1 to that at wavelength 2 reduces to the following:
The functional oxygen saturation is given by
S = C0/(C0 + Cr)
and
IS=Cr/(C0+Cr)
The oxygen saturation can then be written in terms of the ratio R as follows:
The above equation provides the desired relationship between the experimentally determined ratio R and the clinically desired oxygen saturation S. LEDs are not monochromatic light sources, typically with bandwidths between 20 and 50 nm, and therefore standard molar absorptivities for hemoglobin cannot be used directly in the above equation. Also, the simple model presented above is only approximately true; for example, the two wavelengths do not necessarily have the exact same path length changes, and second-order scattering effects have been ignored. Consequently the relationship between S and R is instead determined empirically by fitting the clinical data to a generalized function of the form
S = (k1- k2R)/(k3 - k4R)
A typical empirical calibration for R versus S is shown in Figure 2, together with the curve that standard molar absorptivities would predict. In this way, the measurement of the ratio of the fractional change in signal intensity of the two LED’s is used along with the empirically determined calibration equation to obtain a beat-by-beat measurement of the arterial oxygen saturation in a perfused tissue - continuously, noninvasively, and to an accuracy of a few percent.
Figure 2: Relationship between the measured ratio of fractional changes in light intensity at two wavelengths, R, and the oxygen saturation S.
II Design of Pulse Oximetry Instrumentation
A block diagram of the circuit for a P.O Pro is shown in Figure 3. The main sections of this block diagram are described below.
Figure 3: P.O. Pro block diagram circuit.
The basic optical sensor of a noninvasive pulse oximeter consists of both red and infrared LED’s with peak emission wavelengths of 660 nm and 940 nm respectively, and a silicon photodiode. The Photodiode used has a broad range of spectral responses that overlaps the emission spectra of both the red and infrared LED’s. The light intensity detected by the photodetector depends, not only on the intensity of the incident light, but mainly on the opacity of the skin, reflection by bones, tissue scattering, and the amount of blood in the vascular bed. If both light sources are pulsed, a single photodetector can be used in the probe, since silicon devices are responsive to light having visible and IR wavelengths. Timing circuits could be used to supply, approximately 50 s pulses to the red and IR LED drivers at a repetition rate of 1 kHz, as shown in Figure 4 (a frequency of 1 kHz is suitable because such a frequency is well above the maximum frequency present3 in the arterial pulse).
Figure 4: Switching of Power Supply to Light Sources
High-intensity light outputs can be obtained with the IR LED with currents of up to 1A over a low duty cycle.
The P.O Pro will generate a digital switching pulse to drive the red and infrared LED’s in the sensor alternately at a converter repetition rate of approximately 1KHz. The transmitted light detected by the photodiode is amplified and converted to a voltage using an op-amp configured as a current-to-voltage converter. At this point in the circuit the signal is fed to two identical sections, one for each of the transmitted wavelengths. Since the light is pulsed, we need to use a sample-and-hold circuit to reconstitute the waveforms at each of the two wavelengths. The same timing circuits that were used to control the red and NIR LED drivers are also used to provide the control pulses for the corresponding sample-and-hold circuits. The outputs from these circuits are then filtered with a band-pass filter (with 0.5 Hz and 5 Hz cut-off frequencies) in order to remove primarily the dc component but also high frequency noise. The resulting signals thus represent the cardiac-synchronous information in the waveforms and these are further amplified before they are converted to digital format for subsequent analysis by the microprocessor.
It can be seen from the block diagram in Figure 6 that the output from each sample-and-hold is also passed to a low-pass filter. This is the first stage of an automatic gain control (AGC) circuit that adjusts the light intensity from the corresponding LED so that the dc level always remains at the same value (example 2V) regardless of the thickness or characteristics of the. Reasons for using an AGC circuit include: firstly, the amplitude of the ac signal (which may vary between 0.1% and 2% of the total signal) is also within a pre-defined range and this makes the amplifier that follows the band-pass filter easier to design. Secondly, the dc component of the transmitted red and IR signals can be set at the same value (2 V) in each case. Hence it can be eliminated from the formula used by the microprocessor to calculate the oxygen saturation
Each of the main circuits shown in the block diagram will now be considered. A constant current source drives the LEDs. A simple potential circuit for achieving this is shown in Figure 8a in which an op-amp is combined with a bipolar transistor. In this circuit, the negative feedback forces ve = vin. Thus,
Ie = Vin/R1.
Since the collector current is almost equal to the emitter current (Ic is equal to Ie + Ib), the LED current is therefore also given by:
ILED = Vin/R1.
Figure 5: Two possible circuits for constant current LED driving
However, this current source is slightly imperfect because the small base current, Ib, may vary with Vce. This arises because the op-amp stabilizes the emitter current whereas the load sees the collector current. By using a FET instead of a bipolar transistor, this problem can be avoided as shown in Figure 8b. Since the FET draws no gate current, the output is sampled at the source resistance without error, eliminating the base current error of the bipolar transistor. The load current is limited by the IDS(on) of the MOSFET. If a bipolar power supply is available, the circuits of Figure 5 can be further simplified by omitting Vin and tying the non-inverting input of the op-amp to ground as shown in Figures 6(a) and 6(b) in both of which:
ILED = 12 V/R1.
Figure 6: Alternative circuits for constant current LED driving when a bipolar power supply is available.
a) Timing circuit
The accuracy of the timing is not of much importance; hence the timing circuit can be built around the 555-timer integrated circuit. From the data sheet for this i.c, it can easily be worked out that the circuit given in Figure 7 can be configured, for example by setting C = 22 nF, Ra = 56kand Rb = 3.3k, to give a 50 s pulse approximately every millisecond, as intended
Figure 7: Generating the timing pulses for pulse oximetry.
b) Pulsing the light output from the LEDs
The output from the LED can be pulsed by connecting an n-channel enhancement-mode MOSFET across it as shown in Figure 8. The pulses from the output pin of the 555 timer (pin 3) are taken to the gate of the transistor. The FET needs to be an enhancement-mode MOSFET for it to be turned fully off and on by the gate pulses. The MOSFET chosen for this task should also be capable of handling the maximum current flowing through the LED.
Figure 8: Pulsing the LED.
c) Receiver circuit
The simplest solid-state optical detector is the photodiode. Photodiode detectors normally operate with reverse bias applied to the p-n junction (photoconductive mode). When light falls on the junction region of the photodiode, an electron-hole pair is created; under the influence of the junction (or built-in) field, the hole is swept towards the p-material and the electron towards the n-material. The resulting light current is seen as a large increase in the reverse current. For the purposes of signal amplification, the photocurrent must be transformed into a voltage with moderate output impedance; this is achieved with the circuit shown in Figure 9, the op-amp being configured as a current-to-voltage converter. Because of the high junction resistance of the reverse-biased photodiode, the op-amp should be a FET type with very high input impedance. Since the negative input of the op-amp acts like a virtual ground, the output voltage of the circuit is