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Principles of Biomedical Systems

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Flowmeter Probes. Comes in 1 mm increments for. 1 ~ 24 mm diameter blood vessels ... transducers, whether used for flowmeter or other applications, invariably ... – PowerPoint PPT presentation

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Title: Principles of Biomedical Systems


1
Principles of Biomedical Systems Devices
0909.504.04 / 0909.402.02
WEEK 10 Flow Volume of Blood
2
Measurement of Flow Volume of Blood
  • A measurement of paramount importance
    concentration of O2 and other nutrients in cells
    ? Very difficult to measure
  • Second-class measurement blood flow and changes
    in blood volume ? correlate well with
    concentration
  • Third-class measurement blood pressure ?
    correlates well with blood flow
  • Fourth class measurement ECG ? correlates
    adequately with blood pressure
  • How to make blood flow / volume measurements?
    Standard flow meters, such as turbine flow
    meters, obviously cannot be used!
  • Indicator-dilution method cont./rapid injection,
    dye dilution, thermodilution
  • Electromagnetic flowmeters
  • Ultrasonic flowmeters / Doppler flowmeters
  • Plethysmography Chamber / electric impedance /
    photoplethysmography

3
Indicator Dilution with Continuous Injection
  • Measures flow / cardiac output averaged over
    several heart beats
  • Ficks technique the amount of a substance (O2)
    taken up by an organ / whole body per unit time
    is equal to the arterial level of O2 minus the
    venous level of O2 times the blood flow ?

Change in due to continuously added
indicator m to volume V
Consumption of O2 (mL/min)
Blood flow, liters/min(cardiac output)
Arterial and venousconcentration of O2 (mL/L of
blood)
4
Ficks technique
  • How is dm/dt (O2 consumption) measured?
  • Where and how would we measure Ca and Cv?
    (Exercise)

5
Indicator Dilution with Rapid Injection
  • A known amount of a substance, such as a dye or
    radioactive isotope, is injected into the venous
    blood and the arterial concentration of the
    indicator is measured through a serious of
    measurements until the indicator has completely
    passed through given volume.
  • The cardiac output (blood flow) is amount of
    indicator injected, divided by average
    concentration in arterial blood.

6
Indicator Dilution Curve
After the bolus is injected at time A, there is a
transportation delay before the concentration
begins rising at time B. After the peak is
passed, the curve enters an exponential decay
region between C and D, which would continue
decaying alone the dotted curve to t1 if there
were no recirculation. However, recirculation
causes a second peak at E before the indicator
becomes thoroughly mixed in the blood at F. The
dashed curve indicates the rapid recirculation
that occurs when there is a hole between the left
and right sides of the heart.
7
An Example
8
Dye Dilution
  • In dye-dilution, a commonly used dye is
    indocyanine green (cardiogreen), which satisfies
    the following
  • Inert
  • Safe
  • Measurable though spectrometry
  • Economical
  • Absorption peak is 805 nm, a wavelength at which
    absorption of blood is independent of oxygenation
  • 50of the dye is excreted by the kidneys in 10
    minutes, so repeat measurements is possible

9
Thermodilution
  • The indicator is cold saline, injected into the
    right atrium using a catheter
  • Temperature change in the blood is measured in
    the pulmonary artery using a thermistor
  • The temperature change is inversely proportional
    to the amount of blood flowing through the
    pulmonary artery

10
Measuring Cardiac Output
Several methods of measuring cardiac output In
the Fick method, the indicator is O2 consumption
is measured by a spirometer. The arterial-venous
concentration difference is measure by drawing
simples through catheters placed in an artery and
in the pulmonary artery. In the dye-dilution
method, dye is injected into the pulmonary artery
and samples are taken from an artery. In the
thermodilution method, cold saline is injected
into the right atrium and temperature is measured
in the pulmonary artery.
11
Electromagnetic Flowmeters
  • Based on Faradays law of induction that a
    conductor that moves through a uniform magnetic
    field, or a stationary conductor placed in a
    varying magnetic field generates emf on the
    conductor

When blood flows in the vessel with velocity u
and passes through the magnetic field B, the
induced emf e measured at the electrodes is.
For uniform B and uniform velocity profile u, the
induced emf is eBLu. Flow can be obtained by
multiplying the blood velocity u with the vessel
cross section A.
12
ElectromagneticFlowmeter Probes
  • Comes in 1 mm increments for 1 24 mm
    diameter blood vessels
  • Individual probes cost 500 each
  • Made to fit snuggly to the vessel during
    diastole
  • Only used with arteries, not veins, as
    collapsed veins during diastole lose contact
    with the electrodes
  • Needless to say, this is an INVASIVE
    measurement!!!
  • A major advantage is that it can measure
    instantaneous blood flow, not just average
    flow

13
Ultrasonic Flowmeters
  • Based on the principle of measuring the time it
    takes for an acoustic wave launched from a
    transducer to bounce off red blood cells and
    reflect back to the receiver.
  • All UT transducers, whether used for flowmeter or
    other applications, invariably consists of a
    piezoelectric material, which generates an
    acoustic (mechanical) wave when excited by an
    electrical force (the converse is also true)
  • UT transducers are typically used with a gel that
    fills the air gaps between the transducer and the
    object examined

14
Near / Far Fields
  • Due to finite diameters, UT transducers produce
    diffraction patterns, just like an aperture does
    in optics.
  • This creates near and far fields of the UT
    transducer, in which the acoustic wave exhibit
    different properties
  • The near field extends about dnfD2/4?, where D
    is the transducer diameter and ? is the
    wavelength. During this region, the beam is
    mostly cylindrical (with little spreading),
    however with nonuniform intensity.
  • In the far field, the beam diverges with an angle
    sin?1.2 ?/D, but the intensity uniformly
    attenuates proportional to the square of the
    distance from the transducer

Higher frequencies and larger transducers should
be used for nearfield operation. Typical
operating frequency is 2 10 MHz.
15
UT Flowmeters
Zero-crossingdetector / LPF
Determine direction
High acoustic impedance material
16
Transit time flowmeters
Effective velocity of sound in blood velocity of
sound (c) velocity of flow of blood averaged
along the path of the ultrasound (û) û1.33u for
laminar flow, û1.07u for turbulent flowu
velocity of blood averaged over the cross
sectional area, this is differentthan û because
the UT path is along a single line not over an
averaged of cross sectional area Transit time
in up/down stream direction Difference
between upstream and downstream directions
17
Transit Time Flowmeters
The quantity ?T is typically very small and very
difficult to measure, particularly in the
presence of noise. Therefore phase detection
techniques are usually employed rather then
measuring actual timing.
18
Doppler Flowmeters
  • The Doppler effect describes the change in the
    frequency of a received signal , with respect to
    that of the transmitted signal, when it is
    bounced off of a moving object.
  • Doppler frequency shift

Speed of blood flow (150 cm/s)
Source signal frequency
Angle between UT beamand flow of blood
Speed of sound in blood (1500 m/s)
19
Doppler Flowmeters
20
Problems Associated withDoppler Flowmeters
  • There are two major issues with Doppler
    flowmeters
  • Unlike what the equations may suggest, obtaining
    direction information is not easy due to very
    small changes in frequency shift that when not in
    baseband, removing the carrier signal without
    affecting the shift frequency becomes very
    difficult
  • Also unlike what the equation may suggest, the
    Doppler shift is not a single frequency, but
    rather a band of frequencies because
  • Not all cells are moving at the same velocity
    (velocity profile is not uniform)
  • A cell remains within the UT beam for a very
    short period of time the obtained signal needs
    to be gated, creating side lobes in the frequency
    shift
  • Acoustic energy traveling within the beam, but at
    an angle from the bam axis create an effective
    ??, causing variations in Doppler shift
  • Tumbling and collision of cells cause various
    Doppler shifts

21
Directional Doppler
  • Directional Doppler borrows the quadrature phase
    detector technique from radar in determining the
    speed and direction of an aircraft.
  • Two carrier signals at 90º phase shift are used
    instead of a single carrier. The /- phase
    difference between these carriers after the
    signal is bounced off of the blood cells indicate
    the direction, whereas the change in frequency
    indicate the flowrate

22
Directional Doppler
(a) Quadrature-phase detector. Sine and cosine
signals at the carrier frequency are summed with
the RF output before detection. The output C from
the cosine channel then leads (or lags) the
output S from the sine channel if the flow is
away from (or toward) the transducer. (b) Logic
circuits route one-shot pulses through the top
(or bottom) AND gate when the flow is away from
(or toward) the transducer. The differential
amplifier provides bi-directional output pulses
that are then filtered.
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