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Claims  |
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We claim:
1. A blood oxygen saturation monitoring system comprising:
a source of electromagnetic radiation at first, second, third and fourth
wavelengths;
means for positioning said source of electromagnetic radiation to
illuminate a sample of blood;
sensing means for receiving electromagnetic radiation reflected by said
sample of blood and producing an electrical output signal corresponding to
the components of the reflected portions of said electromagnetic radiation
at said first, second, third, and fourth wavelengths;
means for calculating a product of said electrical signals, said product
being in the form of a quadratic equation relating said reflected portions
of said electromagnetic radiation at said first, second, third, and fourth
wavelengths to the oxygen saturation in said blood and for correlating
said product with the oxygen saturation of said blood.
2. The monitoring system according to claim 1, wherein said first, second,
third and fourth sources of electromagnetic radiation comprise first,
second, third and fourth light emitting diodes.
3. The monitoring system according to claim 2, wherein said first and
second light emitting diodes provide electromagnetic radiation having a
wavelength corresponding to red and said third and fourth light emitting
diodes provide electromagnetic radiation having a wavelength corresponding
to infrared.
4. The monitoring system according to claim 3, wherein said first and
second light emitting diodes produce electromagnetic radiation at
approximately 660 and 680 nanometers, respectively and said third and
fourth light emitting diodes produce electromagnetic radiation at 800 and
900 nanometers, respectively.
5. A method for determining the oxygen saturation of arterial blood,
comprising the steps of:
illuminating a sample of said blood with electromagnetic radiation at
first, second, third, and fourth wavelengths;
collecting electromagnetic radiation reflected by said sample of blood and
producing electrical signals corresponding to the reflected components of
said electromagnetic radiation at said first, second, third and fourth
wavelengths;
calculating a product of said electrical signals, said product being in the
form of a quadratic equation relating said reflected portions of said
electromagnetic radiation at said first, second, third, and fourth
wavelengths to the oxygen saturation in said blood and correlating said
product with the oxygen saturation of said blood.
6. The method accroding to claim 5, wherein said first, second, third and
fourth sources of electromagnetic radiation comprise first, second, third
and fourth light emitting diodes.
7. The method according to claim 6, wherein said first and second light
emitting diodes provide electromagnetic radiation having a wavelength
corresponding to red and said third and fourth light emitting diodes
provide electromagnetic radiation having a wavelength corresponding to
infrared.
8. The method according to claim 7, wherein said first and second light
emitting diodes produce electromagnetic radiation at approximately 660 and
680 nanometers, respectively and said third and fourth light emitting
diodes produce electromagnetic radiation at 800 and 900 nanometers,
respectively. |
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Claims  |
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Description  |
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FIELD OF THE INVENTION
The present invention relates generally to an oximeter which can be used to
estimate the degree of oxygen saturation of a patient's blood. More
specifically, the present invention provides a backscatter oximeter which
is capable of providing accurate indications of arterial and venous oxygen
saturations without the need for prior information relating to the oxygen
content of the particular patient's blood.
BACKGROUND
It is well known that hemoglobin and oxyhemoglobin have different optical
absorption spectra and that this difference in absorption spectra can be
used as a basis for an optical oximeter. Most of the currently available
oximeters using optical methods to determine blood oxygen saturation are
based on transmission oximetry. These devices operate by transmitting
light through an appendage such as a finger or an earlobe. By comparing
the characteristics of the light transmitted into one side of the
appendage with that detected on the opposite side, it is possible to
compute oxygen concentrations. The main disadvantage of transmission
oximetry is that it can only be used on portions of the body which are
thin enough to allow passage of light.
Various methods and apparati for utilizing the optical properties of blood
to measure blood oxygen saturation have been shown in the patent
literature. Representative devices for utilizing the transmission method
of oximetry have been disclosed in U.S. Pat. Nos. 4,586,513; 4,446,871;
4,407,290; 4,226,554; 4,167,331; and 3,998,550. Numerous other works have
disclosed theoretical approaches for analyzing the behavior of light in
blood and other materials. The following is a brief list of some of the
most relevant of these references: "New Contributions to the Optics of
Intensely Light-Scattering Materials, Part 1," by Paul Kubelka, Journal of
the Optical Society of America, Volume 38, No. 5, May 1948; "Optical
Transmission and Reflection by Blood," by R. J. Zdrojkowski and N. R.
Pisharoty, IEEE Transactions on Biomedical Engineering, Vol. BME-17, No.
2, April 1970; "Optical Diffusion in Blood," by Curtis C. Johnson, IEEE
Transactions on Biomedical Engineering, Vol. BME-17, No. 2, April 1970 and
"Optical Scattering in Blood," by Narayanan R. Pisharoty, (Published
Doctoral Dissertation), No. 7124861, University Microfilms, Ann Arbor,
Mich. (1971).
There has been considerable interest in recent years in the development of
an oximeter which is capable of using reflected light to measure blood
oxygen saturation. A reflectance oximeter would be especially useful for
measuring blood oxygen saturation in portions of the patient's body which
are not well suited to transmission measurements. A theoretical discussion
of a basis for the design of a reflectance oximeter is contained in
"Theory and Development of a Transcutaneous Reflectance Oximeter System
for Noninvasive Measurements of Arterial Oxygen Saturation," by Yitzhak
Mendelson (Published Doctoral Dissertation), No. 8329355, University
Microfilms, Ann Arbor, Mich. (1983). In addition, reflectance oximetry
devices and techniques are shown generally in U.S. Pat. Nos. 4,447,150;
4,086,915; and 3,825,342. Recent work by the present inventor and other
investigators has shown that it is possible to obtain accurate indications
of blood oxygen saturation using reflectance oximetry techniques. One of
the difficulties with previous reflectance oximeters, however, is the need
to have prior information relating to the oxygen content of the patient's
blood in order to construct an oxygen saturation reference curve for that
particular patient. Such information is typically obtained by removing and
analyzing a sample of the patient's blood or by measuring the patient's
oxygen saturation with another monitoring device, such as a transmission
oximeter.
SUMMARY OF THE INVENTION
The present invention overcomes the difficulties of the prior art by
providing a noninvasive backscatter oximeter which is capable of providing
accurate indications of a patient's blood oxygen saturation without the
need for obtaining prior information relating to the oxygen content of the
patient's blood. The oximeter of the present invention determines the
blood oxygen saturation of a patient's blood by a noninvasive optical
technique which takes advantage of differences in the absorption spectra
of hemoglobin and oxyhemoglobin. In the preferred embodiment, the
invention comprises means for illuminating the patient's blood with light
at four different wavelengths, means for measuring the intensity of the
reflected light at each of the four wavelengths after contact with the
blood and means for correlating the intensity of the reflected light with
the oxygen saturation of the patient's blood. The invention oximeter is
calibrated by pressing an optical sensor firmly against the patient's
tissue to remove substantially all of the blood from the tissue. The
tissue is then illuminated with the light at four different wavelengths
and reflected light signals are detected and processed to obtain
information relating to the optical properties of the patient's tissue.
The pressure of the sensor against the tissue is then reduced to allow
blood to return to the tissue and subsequent measurements of light
reflected by the blood are correlated with blood oxygen saturation using
mathematical relationships for arterial and venous oxygen saturation.
BRIEF DESCRIPTION OF THE DRAWING
FIG. 1 is a schematic block diagram of a simplified embodiment of the
backscatter blood oxygen saturation monitoring system of the present
invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
Referring to FIG. 1 the noninvasive monitoring system 10 of the present
invention is shown in its preferred embodiment. A monitoring probe 12 is
positioned over a portion of the patient's tissue 14 such that light
produced by four light emitting diodes (LED) 16, 18, 20 and 22 will be
reflected by blood in the tissue and detected by a photodetector 24. Two
of the LEDs, e.g. 16 and 18, emit light in the red spectrum and the other
two LEDs, e.g. 20 and 22, emit light in the infrared spectrum. In the
preferred embodiment, LEDs 16 and 18 emit light at 660 and 680 nm (red),
respectively, while LEDs 20 and 22 emit light at 800 and 900 nm
(infrared), respectively. However, the invention is not intended to be
limited to the specific wavelength of light produced by the
above-mentioned LEDs. Proper operation of the invention requires only that
two of the light sources have a wavelength for which the absorption
coefficients of hemoglobin and oxyhemoglobin are different.
Operation of the LEDs is controlled by a timing control circuit 26 which
causes the LEDs to emit an ordered sequence of pulses of light at the
above-mentioned wavelengths. These pulses of light are reflected by blood
contained in the patient's tissue and are detected by a photodetector 24.
The reflected light signals detected by detector 24 are converted to a
series of electrical impulses which are demultiplexed by demultiplexer 28
and converted to digital signals by analog-to-digital converter 30. The
resulting sequence of digital signals is then fed into a microprocessor 32
and processed in conjunction with mathematical relationships, described in
greater detail below, to obtain an indication of the patient's arterial
and venous blood oxygen saturations. The resulting values are then
displayed on an appropriate output display 34. The functional features of
the above-described system can be accomplished through the use of
electronic components and techniques which are known in the art.
The techniques used to calculate oxygen saturation in the invention system
can be understood from the following discussion of the relationships
between the reflected light signals detected by the system. The following
equation describes light reflection from a turbid, both absorbing and
scattering, medium:
##EQU1##
where: R.sub.d --reflection of light from a medium.
d--thickness of the medium.
s--scattering coefficient of medium.
k--absorption coefficient of medium.
For a backscatter oximeter, the following assumptions can be used to
simplify the above equations: (1) tissue thickness can be considered to be
very large, and (2) the optical scattering of bloodless tissue is very
close to the optical scattering of the perfused tissue at systole and
diastole. From the assumption regarding the thickness of the tissue, the
following equation can be obtained:
##EQU2##
Information regarding the optical properties of the tissue can be obtained
if a "bloodless" calibration is performed. This is done by attaching the
sensor 12 to the patient and applying sufficient pressure to the sensor to
temporarily remove the blood from the tissue.
Applying the above equation to voltages measured for bloodless tissue and
for perfused tissue at systole and diastole, the following equations can
be formed:
##EQU3##
where: s.sub.t --scattering coefficient of bloodless tissue.
s.sub.d --scattering coefficient of perfused tissue at diastole.
s.sub.s --scattering coefficient of perfused tissue at systole.
s.sub.a --scattering coefficient of arterial blood.
s.sub.v --scattering coefficient of venous blood.
k.sub.t --absorption coefficient of bloodless tissue.
k.sub.d --absorption coefficient of perfused tissue at diastole.
k.sub.s --absorption coefficient of perfused tissue at systole.
k.sub.a --absorption coefficient of arterial blood.
k.sub.v --absorption coefficient of venous blood.
.DELTA..sub.a --fraction of arterial blood in perfused tissue at systole.
.DELTA..sub.v --fraction of venous blood in perfused tissue at diastole.
C.sub.Hb --Concentration of hemoglobin in the blood.
HbO2--Optical absorption coefficient for oxygenated hemoglobin.
Hb--Optical absorption coefficient for reduced hemoglobin.
OS.sub.a --Oxygen saturation of arterial blood.
OS.sub.v --Oxygen saturation of venous blood.
I.sub.0 --input intensity of light source.
V.sub.t --reflectance voltage signal for bloodless tissue.
V.sub.d --reflectance voltage signal for perfused tissue at diastole.
V.sub.s --reflectance voltage signal for perfused tissue at systole.
If it is assumed that the scattering coefficient of bloodless tissue,
perfused tissue at systole and diastole are approximately the same, the
following equations can be formed:
##EQU4##
By using four light sources of differing wavelengths, a solution can be
obtained for OS.sub.a :
let:
##EQU5##
where: i--light source 1, 2, 3, and 4, respectively.
jkl--combination of three light sources 123, 231, 312, 134, 341, 413, 124,
241, 412, 234, 342, and 423, respectively.
mno--combination of three light sources 123, 134, 124, and 234,
respectively.
The above relation is a quadratic form of an equation relating the voltages
for the bloodless tissue and the perfused tissue at diastole and systole
to OS.sub.a. The above equation will produce two solutions. One of the
solutions will be approximately equal to zero. The other solution will be
the correct solution for OS.sub.a. Calculation of OS.sub.a using the
abovedescribed relation can be easily accomplished using computer
programming techniques which are known in the art. An Arterial Blood
Oxygen Saturation Correlation Program for calculating OS.sub.a has been
shown in FIG. 1 as providing an input to the microprocessor 32.
Once the value of OS.sub.a is obtained as shown above, a solution can be
obtained for O.sub.v :
let:
##EQU6##
where: p--light source 1, 2, and 3, respectively.
qr--combination of two light sources 12 and 13, respectively.
##EQU7##
The above equation will produce two solutions. One of the solutions will be
approximately equal to OS.sub.a. The other solution will be the correct
solution for OS.sub.v. Calculation of OS.sub.v using the above-described
relation can be easily accomplished using computer programming techniques
which are known in the art. A Venous Blood Oxygen Saturation Correlation
Program for calculating OS.sub.v has been shown in FIG. 1 as providing an
input to the microprocessor 32.
While the invention method and apparatus for noninvasive monitoring of
arterial blood oxygen saturation has been described in connection with the
preferred embodiment, it is not intended to be limited to the specific
form set forth herein, but on the contrary, it is intended to cover such
alternatives, modifications and equivalents as may be reasonably included
within the spirit and scope of the invention as defined by the appended
claims.
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Description  |
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