SlideShare a Scribd company logo
1 of 24
Improving Non-Invasive Blood
Analysis by Expanding the Medical
         Spectral Window




                Katherine Paseman
Goal: Detect Medical Problems by non-
Invasively measuring Optical
Properties of Blood

Optical Blood   Medical             Example
Property        Diagnostic          Problem
                (Symptom)
Fluorescence    Zinc Protoporphyrin Iron Deficient
                (ZPP) Concentration Anemia, Lead
                                    Poisoning
Absorption      Hemoglobin          Anemia
                Concentration

Scattering      Hematocrit          Low- Blood loss,
                                    High - Dehydration
Beer-Lambert Law
 Optical approaches leverage the Beer-Lambert
  law which uses 3 variables to model light
  entering (Ii) and exiting (Io) a sample.
 Io = Ii 10 –2.303 ε(λ) c t /(64,500 g Hb/mole)
 t – Sample thickness – cm
 c – concentration of absorbent - g/liter (A typical
  value of c for whole blood is 150 g Hb/liter.)
 ε(λ) – extinction coefficient of absorbent, which
  is a function of the light’s wavelength.
    –   Blood’s ε(λ) is very large for λ < 600 nm
    –   This is why a flashlight shone through the hand only
        transmits red light.
Prior Work: Pulse Oximetry

   A Pulse Oximeter non-
    invasively determines Pulse
    and Blood Oxygenation using
    differential light absorption.
   A Photodiode measures light
    intensity of Red (660nm) &
    Infrared (940 nm) LEDs shone
    through Finger during
    systole/diastole.
   Blood Oxygenation is a
    function of the “Ratio of
    Ratios” of Light Intensities at
    these points.
                             Webster, JG. Design of Pulse Oximeters
Prior Work: Masimo pt 1

Most non-invasive blood      λ    Hb02 ε(λ)     Hb ε(λ)
                             nm   cm-1/M        cm-1/M
sensors extend the pulse
oximeter’s differential      610 1506           9443.6
absorption trick. Like the
                             620 942            6509.6
pulse oximeter, they
                             630 610            5148.8
target the finger using
                             660 319.6          3226.56
wavelengths above 600
nm, the so called ”Medical   700 290            1794.28

Spectral Window”, to         730 390            1102.2
collect enough light.        805 844            730.28
                             905 1209.2         769.8

                               Source: Masimo [US7377794]
Prior Work: Masimo pt 2




                          Medical
                          Spectral
                          Window
Prior Work: Samsung pt 1

Samsung’s work [Yoon et. al.        λ     Hb02 ε(λ)   Hb ε(λ)
  2005] states“Three variables            cm-1/M      cm-1/M
  of R569,805, R569,940, and
  R569,975 were used for            569 44496         45072
  calibration and prediction
  models.” producing this
  comment by one author:            660   319.6       3226.56
G Yoon <gyoon@snut.ac.kr> -
  569nm is highly absorbing in      805   844         730.28
  tissue and, at the same time,
  569nm intensity is small          940   1214        693.44
  compared with that at longer
  wavelength. That is why you
  may not get good signal. We       975   1144        389.288
  used a custom-made LED array
  that has several chips of 569nm
  to increase intensity.
Prior Work: Samsung pt 2


                            569 nm lies
                            outside the
                            Medical
                            Spectral
                            Window




                           Medical
                           Spectral
                           Window
Our Research: Target Thumb Webbing
for Absorption instead of Finger

   Our hypothesis: We can
    extend the medical spectral
    window by offsetting the
    increase in extinction
    coefficient at λ< 600 nm with a
    decrease in sample thickness
   [Sabrina Paseman 2008] did
    this by targeting the thumb
    webbing for fluorescence
    measurements.
   We do this for absorption.
   This allows us to get better
    absorption measurements by
    increasing signal and so
    decreasing noise based error.
   It also allows us to detect
    additional sources of error.
The Apparatus
   We created an adjustable width clip
    that fits either the subject’s index
    finger or thumb webbing.
   One end of the clip holds the same
    5-LED package used by Samsung
    and the other holds a fiber optic
    cable which connects to a
    spectrometer.
   This allows us to double check the
    LED’s wavelength, determine LED
    intensity, see if there are any LED
    artifacts, and observe any swamping
    or fluorescing effects.
   The LEDs and spectrometer were
    controlled by an Arduino
    microcontroller.
Experimental Approach 1

   Clamp is adjusted to fit the subject’s index finger.
    Subject removes finger so distance between
    spectrometer and LED can be measured with a
    micrometer.
   Thumb webbing is placed over the entire LED
   Spectrometer auto-adjusts the integration time to a
    full scale reading and the data is collected.
   Subject removes thumb webbing and places index
    finger over LED. Data is collected with the same
    integration time and plotted on the same axis for
    comparison
Data: 569 nm Subject 1

                             Thumb webbing
                             Index Finger
       54054.5 counts

                           Integration Time: 404.05 ms


                           Width: 0.7175 cm




           4131.5 counts
Findings

   Transmission increases 13 fold
   Samsung’s LED chip has an artifact at around 875nm
    when the 569nm LED is lit. If Samsung’s device uses
    a photodiode to collect light, especially at low
    intensities, much of the collected light would come
    from the artifact rather than the 569nm absorption
   This method limited the quality of the readings we
    could take from subjects with darker skin
Experimental Approach 2

 Hold  LED underneath the thumb webbing
  and the spectrometer on the other side.
 Let the spectrometer auto-integrate and
  capture the graph.
 For data analysis, find the ratio between the
  ratios of the peak counts at 569nm and the
  integration time               Counts        thumb webbing
                                      Integration timethumb webbing
         Absorption Amplification =
                                      Countsindex finger
                                      Integration timeindex finger
Data: 569 nm Subject 1 Finger

                                Index Finger

                             Integration Time: 3097.90 ms




          13640.500 counts
Data: 569 nm Subject 1 Webbing

                            Thumb Webbing

                         Integration Time: 99.70 ms




      32847.801 counts
Data: 569 nm Subject 2 Finger

                                Index Finger

                             Integration Time: 1736.15 ms




          61598.500 counts
Data: 569 nm Subject 2 Webbing

                              Thumb Webbing

        60849.000 counts   Integration Time: 208.91 ms
Data: 569 nm Subject 3 Finger

                              Index Finger

        60534.000 counts   Integration Time: 3808.11 ms
Data: 569 nm Subject 3 Webbing

                              Thumb Webbing

        55602.750 counts   Integration Time: 114.73 ms
Data: 569 nm


Subject Countstw    Integrationtw Countsif    Integrationif Ampli-
                    (ms)                      (ms)          fication


1       32847.801   99.70         13640.500 3097.90         74.825
2       60849.000   208.91        61598.500   1736.15       8.209
3       55602.750   114.73        60534.000 3808.11         30.488
Conclusions

 Transmission  increases across the board but
  varies from subject to subject
 Our suspicions about the artifact are
  confirmed by our second set up
Further Research
 See  if there is a statistically significant
  difference between the light absorption of
  systolic and diastolic blood at 569, 660, 805,
  940 and 975 nm.
 Correlate more medical problems to
  absorption differentials and fluorescent
  phenomena.
  –   See if there is a statistically significant difference
      between the fluorescence of systolic and diastolic
      blood excited at 425 nm.
 Collect
        data for more subjects with varying
  melanin contents
References
   [Sabrina Paseman 2008] Paseman, Sabrina. The
    Ferrometer: A Device to Detect Iron Deficient Anemia via
    Non-Invasive Optical Measurement of Zinc
    Protoporphyrin. Issue brief no. SO499. Los Angeles:
    University of Southern California, 2008. PDF file.
   [US7377794] "Multiple Wavelength Sensor Interconnect” –
    p57 lists Masimo’s wavelengths
   [Yoon et. Al. 2005] Yoon, Gilwon, Ph.D, et al. "Development
    of a Compact Home Health Monitor for Telemedicine."
    TELEMEDICINE AND e-HEALTH 11.6 (2005): 660-67.
    PDF File.
   “Tabulated Molar Extinction Coefficient for Hemoglobin in
    Water”
    http://omlc.ogi.edu/spectra/hemoglobin/summary.html

More Related Content

What's hot

Sumerschool DPI 2012 Uslar
Sumerschool DPI 2012 UslarSumerschool DPI 2012 Uslar
Sumerschool DPI 2012 UslarDirk Hähnel
 
Optical characterization
Optical characterizationOptical characterization
Optical characterizationAbubakar Yakubu
 
Research statement
Research statementResearch statement
Research statementcanfang
 
Image Scanning Microscopy
Image Scanning MicroscopyImage Scanning Microscopy
Image Scanning MicroscopyDirk Hähnel
 
Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...
Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...
Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...HORIBA Particle
 
Advantages of the LA-950 Laser Diffraction PSA
Advantages of the LA-950 Laser Diffraction PSAAdvantages of the LA-950 Laser Diffraction PSA
Advantages of the LA-950 Laser Diffraction PSAHORIBA Particle
 
Scale & Measurement Module
Scale & Measurement ModuleScale & Measurement Module
Scale & Measurement ModuleAccessNano
 
Introduction to laser diffraction
Introduction to laser diffractionIntroduction to laser diffraction
Introduction to laser diffractionHORIBA Particle
 
OBT751 Analytical methods Instrumentation materials
OBT751 Analytical methods Instrumentation materialsOBT751 Analytical methods Instrumentation materials
OBT751 Analytical methods Instrumentation materialsMercy Joseph
 
Introduction to laser dermatology 3
Introduction to laser dermatology 3Introduction to laser dermatology 3
Introduction to laser dermatology 3Islam Noaman
 
上海必和 Bio optics-5-09超光谱高光谱多光谱
上海必和 Bio optics-5-09超光谱高光谱多光谱上海必和 Bio optics-5-09超光谱高光谱多光谱
上海必和 Bio optics-5-09超光谱高光谱多光谱algous
 

What's hot (20)

Mr2521772184
Mr2521772184Mr2521772184
Mr2521772184
 
Sumerschool DPI 2012 Uslar
Sumerschool DPI 2012 UslarSumerschool DPI 2012 Uslar
Sumerschool DPI 2012 Uslar
 
micro:bit亮度感測應用
micro:bit亮度感測應用micro:bit亮度感測應用
micro:bit亮度感測應用
 
Optical characterization
Optical characterizationOptical characterization
Optical characterization
 
Research statement
Research statementResearch statement
Research statement
 
Image Scanning Microscopy
Image Scanning MicroscopyImage Scanning Microscopy
Image Scanning Microscopy
 
Gps Navigation System
Gps Navigation SystemGps Navigation System
Gps Navigation System
 
Laser systems
Laser systemsLaser systems
Laser systems
 
Turbidity measurement
Turbidity measurementTurbidity measurement
Turbidity measurement
 
Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...
Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...
Exosomes: Exploiting the Diagnostic and Therapeutic Potential of Nature’s Bio...
 
Remote sensing
Remote sensingRemote sensing
Remote sensing
 
Advantages of the LA-950 Laser Diffraction PSA
Advantages of the LA-950 Laser Diffraction PSAAdvantages of the LA-950 Laser Diffraction PSA
Advantages of the LA-950 Laser Diffraction PSA
 
Scale & Measurement Module
Scale & Measurement ModuleScale & Measurement Module
Scale & Measurement Module
 
Calibrationfinal
CalibrationfinalCalibrationfinal
Calibrationfinal
 
Introduction to laser diffraction
Introduction to laser diffractionIntroduction to laser diffraction
Introduction to laser diffraction
 
OBT751 Analytical methods Instrumentation materials
OBT751 Analytical methods Instrumentation materialsOBT751 Analytical methods Instrumentation materials
OBT751 Analytical methods Instrumentation materials
 
Varsha project
Varsha projectVarsha project
Varsha project
 
Introduction to laser dermatology 3
Introduction to laser dermatology 3Introduction to laser dermatology 3
Introduction to laser dermatology 3
 
Single beam spectrophotometer
Single beam spectrophotometer Single beam spectrophotometer
Single beam spectrophotometer
 
上海必和 Bio optics-5-09超光谱高光谱多光谱
上海必和 Bio optics-5-09超光谱高光谱多光谱上海必和 Bio optics-5-09超光谱高光谱多光谱
上海必和 Bio optics-5-09超光谱高光谱多光谱
 

Similar to Expanding the medical spectral window v5

Expanding the medical spectral window v7
Expanding the medical spectral window v7Expanding the medical spectral window v7
Expanding the medical spectral window v7kpaseman
 
Expanding the medical spectral window v6
Expanding the medical spectral window v6Expanding the medical spectral window v6
Expanding the medical spectral window v6kpaseman
 
Expanding the medical spectral window v6
Expanding the medical spectral window v6Expanding the medical spectral window v6
Expanding the medical spectral window v6kpaseman
 
Expanding the medical spectral window v8
Expanding the medical spectral window v8Expanding the medical spectral window v8
Expanding the medical spectral window v8kpaseman
 
Expanding the medical spectral window v8
Expanding the medical spectral window v8Expanding the medical spectral window v8
Expanding the medical spectral window v8kpaseman
 
Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...
Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...
Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...IJECEIAES
 
Guillet mottin 2005 spie_ 5964
Guillet mottin 2005 spie_ 5964Guillet mottin 2005 spie_ 5964
Guillet mottin 2005 spie_ 5964Stéphane MOTTIN
 
Litesizer 500 - Brochure
Litesizer 500 - BrochureLitesizer 500 - Brochure
Litesizer 500 - BrochureStephen Hussey
 
Analysis of LED
Analysis of LEDAnalysis of LED
Analysis of LEDrpiitcbme
 
A biologically inspired cmos image sensor
A biologically inspired cmos image sensorA biologically inspired cmos image sensor
A biologically inspired cmos image sensorSpringer
 
A biologically inspired cmos image sensor
A biologically inspired cmos image sensorA biologically inspired cmos image sensor
A biologically inspired cmos image sensorSpringer
 
In-Depth Understanding of Fiber Optic Sensing Network
In-Depth Understanding of Fiber Optic Sensing NetworkIn-Depth Understanding of Fiber Optic Sensing Network
In-Depth Understanding of Fiber Optic Sensing NetworkSun Telecom
 
Fourier Transform Infrared Spectrometry (FTIR) and Textile
Fourier Transform Infrared Spectrometry (FTIR) and TextileFourier Transform Infrared Spectrometry (FTIR) and Textile
Fourier Transform Infrared Spectrometry (FTIR) and TextileAzmir Latif Beg
 
project proposal final
project proposal finalproject proposal final
project proposal finalChintan Patel
 
S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...
S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...
S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...sipij
 
Structural Health Monitoring Aluminum Honeycomb Sandwich Composite Panel
Structural Health Monitoring Aluminum Honeycomb Sandwich Composite PanelStructural Health Monitoring Aluminum Honeycomb Sandwich Composite Panel
Structural Health Monitoring Aluminum Honeycomb Sandwich Composite PanelDawid Yhisreal
 

Similar to Expanding the medical spectral window v5 (20)

Expanding the medical spectral window v7
Expanding the medical spectral window v7Expanding the medical spectral window v7
Expanding the medical spectral window v7
 
Expanding the medical spectral window v6
Expanding the medical spectral window v6Expanding the medical spectral window v6
Expanding the medical spectral window v6
 
Expanding the medical spectral window v6
Expanding the medical spectral window v6Expanding the medical spectral window v6
Expanding the medical spectral window v6
 
Expanding the medical spectral window v8
Expanding the medical spectral window v8Expanding the medical spectral window v8
Expanding the medical spectral window v8
 
Expanding the medical spectral window v8
Expanding the medical spectral window v8Expanding the medical spectral window v8
Expanding the medical spectral window v8
 
11
1111
11
 
Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...
Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...
Design and Development of a Shortwave near Infrared Spectroscopy using NIR LE...
 
Guillet mottin 2005 spie_ 5964
Guillet mottin 2005 spie_ 5964Guillet mottin 2005 spie_ 5964
Guillet mottin 2005 spie_ 5964
 
OCT Machines
OCT Machines OCT Machines
OCT Machines
 
Litesizer 500 - Brochure
Litesizer 500 - BrochureLitesizer 500 - Brochure
Litesizer 500 - Brochure
 
Analysis of LED
Analysis of LEDAnalysis of LED
Analysis of LED
 
A biologically inspired cmos image sensor
A biologically inspired cmos image sensorA biologically inspired cmos image sensor
A biologically inspired cmos image sensor
 
A biologically inspired cmos image sensor
A biologically inspired cmos image sensorA biologically inspired cmos image sensor
A biologically inspired cmos image sensor
 
In-Depth Understanding of Fiber Optic Sensing Network
In-Depth Understanding of Fiber Optic Sensing NetworkIn-Depth Understanding of Fiber Optic Sensing Network
In-Depth Understanding of Fiber Optic Sensing Network
 
Fourier Transform Infrared Spectrometry (FTIR) and Textile
Fourier Transform Infrared Spectrometry (FTIR) and TextileFourier Transform Infrared Spectrometry (FTIR) and Textile
Fourier Transform Infrared Spectrometry (FTIR) and Textile
 
Linkedin
LinkedinLinkedin
Linkedin
 
project proposal final
project proposal finalproject proposal final
project proposal final
 
S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...
S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...
S IGNAL A ND I MAGE P ROCESSING OF O PTICAL C OHERENCE T OMOGRAPHY AT 1310 NM...
 
Spetrophotometer
SpetrophotometerSpetrophotometer
Spetrophotometer
 
Structural Health Monitoring Aluminum Honeycomb Sandwich Composite Panel
Structural Health Monitoring Aluminum Honeycomb Sandwich Composite PanelStructural Health Monitoring Aluminum Honeycomb Sandwich Composite Panel
Structural Health Monitoring Aluminum Honeycomb Sandwich Composite Panel
 

Expanding the medical spectral window v5

  • 1. Improving Non-Invasive Blood Analysis by Expanding the Medical Spectral Window Katherine Paseman
  • 2. Goal: Detect Medical Problems by non- Invasively measuring Optical Properties of Blood Optical Blood Medical Example Property Diagnostic Problem (Symptom) Fluorescence Zinc Protoporphyrin Iron Deficient (ZPP) Concentration Anemia, Lead Poisoning Absorption Hemoglobin Anemia Concentration Scattering Hematocrit Low- Blood loss, High - Dehydration
  • 3. Beer-Lambert Law  Optical approaches leverage the Beer-Lambert law which uses 3 variables to model light entering (Ii) and exiting (Io) a sample.  Io = Ii 10 –2.303 ε(λ) c t /(64,500 g Hb/mole)  t – Sample thickness – cm  c – concentration of absorbent - g/liter (A typical value of c for whole blood is 150 g Hb/liter.)  ε(λ) – extinction coefficient of absorbent, which is a function of the light’s wavelength. – Blood’s ε(λ) is very large for λ < 600 nm – This is why a flashlight shone through the hand only transmits red light.
  • 4. Prior Work: Pulse Oximetry  A Pulse Oximeter non- invasively determines Pulse and Blood Oxygenation using differential light absorption.  A Photodiode measures light intensity of Red (660nm) & Infrared (940 nm) LEDs shone through Finger during systole/diastole.  Blood Oxygenation is a function of the “Ratio of Ratios” of Light Intensities at these points. Webster, JG. Design of Pulse Oximeters
  • 5. Prior Work: Masimo pt 1 Most non-invasive blood λ Hb02 ε(λ) Hb ε(λ) nm cm-1/M cm-1/M sensors extend the pulse oximeter’s differential 610 1506 9443.6 absorption trick. Like the 620 942 6509.6 pulse oximeter, they 630 610 5148.8 target the finger using 660 319.6 3226.56 wavelengths above 600 nm, the so called ”Medical 700 290 1794.28 Spectral Window”, to 730 390 1102.2 collect enough light. 805 844 730.28 905 1209.2 769.8 Source: Masimo [US7377794]
  • 6. Prior Work: Masimo pt 2 Medical Spectral Window
  • 7. Prior Work: Samsung pt 1 Samsung’s work [Yoon et. al. λ Hb02 ε(λ) Hb ε(λ) 2005] states“Three variables cm-1/M cm-1/M of R569,805, R569,940, and R569,975 were used for 569 44496 45072 calibration and prediction models.” producing this comment by one author: 660 319.6 3226.56 G Yoon <gyoon@snut.ac.kr> - 569nm is highly absorbing in 805 844 730.28 tissue and, at the same time, 569nm intensity is small 940 1214 693.44 compared with that at longer wavelength. That is why you may not get good signal. We 975 1144 389.288 used a custom-made LED array that has several chips of 569nm to increase intensity.
  • 8. Prior Work: Samsung pt 2 569 nm lies outside the Medical Spectral Window Medical Spectral Window
  • 9. Our Research: Target Thumb Webbing for Absorption instead of Finger  Our hypothesis: We can extend the medical spectral window by offsetting the increase in extinction coefficient at λ< 600 nm with a decrease in sample thickness  [Sabrina Paseman 2008] did this by targeting the thumb webbing for fluorescence measurements.  We do this for absorption.  This allows us to get better absorption measurements by increasing signal and so decreasing noise based error.  It also allows us to detect additional sources of error.
  • 10. The Apparatus  We created an adjustable width clip that fits either the subject’s index finger or thumb webbing.  One end of the clip holds the same 5-LED package used by Samsung and the other holds a fiber optic cable which connects to a spectrometer.  This allows us to double check the LED’s wavelength, determine LED intensity, see if there are any LED artifacts, and observe any swamping or fluorescing effects.  The LEDs and spectrometer were controlled by an Arduino microcontroller.
  • 11. Experimental Approach 1  Clamp is adjusted to fit the subject’s index finger. Subject removes finger so distance between spectrometer and LED can be measured with a micrometer.  Thumb webbing is placed over the entire LED  Spectrometer auto-adjusts the integration time to a full scale reading and the data is collected.  Subject removes thumb webbing and places index finger over LED. Data is collected with the same integration time and plotted on the same axis for comparison
  • 12. Data: 569 nm Subject 1 Thumb webbing Index Finger 54054.5 counts Integration Time: 404.05 ms Width: 0.7175 cm 4131.5 counts
  • 13. Findings  Transmission increases 13 fold  Samsung’s LED chip has an artifact at around 875nm when the 569nm LED is lit. If Samsung’s device uses a photodiode to collect light, especially at low intensities, much of the collected light would come from the artifact rather than the 569nm absorption  This method limited the quality of the readings we could take from subjects with darker skin
  • 14. Experimental Approach 2  Hold LED underneath the thumb webbing and the spectrometer on the other side.  Let the spectrometer auto-integrate and capture the graph.  For data analysis, find the ratio between the ratios of the peak counts at 569nm and the integration time Counts thumb webbing Integration timethumb webbing Absorption Amplification = Countsindex finger Integration timeindex finger
  • 15. Data: 569 nm Subject 1 Finger Index Finger Integration Time: 3097.90 ms 13640.500 counts
  • 16. Data: 569 nm Subject 1 Webbing Thumb Webbing Integration Time: 99.70 ms 32847.801 counts
  • 17. Data: 569 nm Subject 2 Finger Index Finger Integration Time: 1736.15 ms 61598.500 counts
  • 18. Data: 569 nm Subject 2 Webbing Thumb Webbing 60849.000 counts Integration Time: 208.91 ms
  • 19. Data: 569 nm Subject 3 Finger Index Finger 60534.000 counts Integration Time: 3808.11 ms
  • 20. Data: 569 nm Subject 3 Webbing Thumb Webbing 55602.750 counts Integration Time: 114.73 ms
  • 21. Data: 569 nm Subject Countstw Integrationtw Countsif Integrationif Ampli- (ms) (ms) fication 1 32847.801 99.70 13640.500 3097.90 74.825 2 60849.000 208.91 61598.500 1736.15 8.209 3 55602.750 114.73 60534.000 3808.11 30.488
  • 22. Conclusions  Transmission increases across the board but varies from subject to subject  Our suspicions about the artifact are confirmed by our second set up
  • 23. Further Research  See if there is a statistically significant difference between the light absorption of systolic and diastolic blood at 569, 660, 805, 940 and 975 nm.  Correlate more medical problems to absorption differentials and fluorescent phenomena. – See if there is a statistically significant difference between the fluorescence of systolic and diastolic blood excited at 425 nm.  Collect data for more subjects with varying melanin contents
  • 24. References  [Sabrina Paseman 2008] Paseman, Sabrina. The Ferrometer: A Device to Detect Iron Deficient Anemia via Non-Invasive Optical Measurement of Zinc Protoporphyrin. Issue brief no. SO499. Los Angeles: University of Southern California, 2008. PDF file.  [US7377794] "Multiple Wavelength Sensor Interconnect” – p57 lists Masimo’s wavelengths  [Yoon et. Al. 2005] Yoon, Gilwon, Ph.D, et al. "Development of a Compact Home Health Monitor for Telemedicine." TELEMEDICINE AND e-HEALTH 11.6 (2005): 660-67. PDF File.  “Tabulated Molar Extinction Coefficient for Hemoglobin in Water” http://omlc.ogi.edu/spectra/hemoglobin/summary.html