BIOMEDICAL ENGINEERING�BIOMEDICAL TRANSDUCERS (BMF)
PRESSURE MEASUREMENT
Rossana E. Madrid
LAMEIN – DBI – FACET/UNT – INSIBIO/CONICET
Latest update April 2025
Table of contents
Brief history
1628
1727
1929
1956 🡪
PRESSURE UNITS
1 mmHg = 133,32 Pa = 0.1333 kPa
1 cmH2O = 98,0665 Pa
1 atm = 101,325 kPa 1 mbar = 0.1 kPa
PHYSIOLOGICAL PRESSURE RANGES
NORMAL
ANOMALOUS
PRESSURE IN THE CARDIOVASCULAR SYSTEM Characteristics
PARAMETER | PRIMARY SIGNAL CHARACTERISTICS | PRESSURE RANGES |
Blood Pressure (arterial, direct) | Range of f: DC to 200 Hz | 20 a 300 mmHg |
Blood Pressure (arterial, indirect) | Range of f: DC to 5 Hz | 20 a 300 mmHg |
Blood Pressure (venous, direct) | Range of f: DC to 40 Hz | -5 a 20 mmHg |
PRESSURE MEASUREMENT IN THE CARDIOVASCULAR SYSTEM
DIRECT MEASUREMENT
INDIRECT MEASUREMENT
INTRAVASCULAR
SENSOR
EXTRAVASCULAR
SENSOR
AUSCULTATORY METHOD
OSCILOMETRIC
METHOD
DOPPLER ULTRASOUND METHOD
Detection of arterial wall motion
Detection of Doppler blood flow velocity in artery
DIRECT PRESSURE MEASUREMENT
PRESSURE CATETHERS
With a catheter you can...
Indicator Dilution Principle
Método de Fick
Ej: Mikro-Tip® Catheter Pressure Transducer
P = -50 a 300 mmHg fresonance= 35 a 50 kHz
INTRAVASCULAR SENSOR
CATHETER TIP PRESSURE TRANSDUCER
ADVANTAGES
DISADVANTAGES
INTRAVASCULAR SENSOR
CATHETER TIP PRESSURE TRANSDUCER
EXTRAVASCULAR SENSOR � DIAPHRAGM DISPLACEMENT TRANSDUCER
ELASTIC DIAPHRAGM
Strain gauge
Variable Capacitor
Optical Sensor
Inductive Sensor
EXTRAVASCULAR SENSORES
External Transducers
Statham Transducer
Blood Pressure Elastic deflextion Electrical Signal
Standard for Blood Pressure Measurement Hg manometer
DYNAMIC PROPERTIES OF DIRECT PRESSURE MEASURMENT�CATHETER TRANSDUCER SYSTEM
Hydraulic Model of a pressure transducer
P(t) = Applied Pressure
M = Fluid Mass
K = Stiffness
Electrical Model
Dynamic system of a 2nd order system
CTS Distributed parameters System
But... Clinical sets Second order system
Rt << Rc
and
Lt << Lc
Cc << Cd
Bubble
ΔP: P Diff through the segment [Pascal]
F: Flow (m3/seg)
A: Cross section of the catheter [m2]
v: Average flow speed [m/seg]
By applying the Poisseuille Law 🡪
η: Viscosity
dF/dt: Flow Derivative
a: Acceleration [m/s2]
A: Area [m2]
It reduces to:
m: Liquid Mass [Kg]
ρ: Liquid Density [kg/m3]
Ed: Diaphragm Elasticity Module
By Kirchoff Law vi vs vo:
Elasticity Mass Friction
Determine two important parameters
ξ
ω
and
Vd: Displaced Volume in the transducer
CTS Time Response
¿How to measure?
Pressure Step Response:
ξ Influences in the Overshoot and the Rise Time
POSSIBLE RESPONSES
Pressure wave distorsion
MikroTip® vs CTS
Frequency Response
BAND WIDE REQUEREMENTS
SCIENTIFIC
Wide BW in the audiofrequency range
CATHETERSIM
LABORATORY
Accurate reproduction of dP/dt
Higher reuqeriments of BW
Flat response up to 20th armonic
CLINICAL AREA
INTENSIVE CARE
Medium pressure important
instead waveform
CTS Response with and without bubble
CTS Dynamic response (Two techniques):
ωn and ξ
BW Requirements
System fully
characterized
A variable frequency pressure generator is used to analize frequency response
ωn : How fast the system can oscillate
ξ: How quickly the system returns to rest
Why?
1
2
INDIRECT MEASUREMENT
Auscultatory Method with sphygmomanometer
Dimensions of the inflatable cuff
Difficulties:
INDIRECT MEASUREMENT
MEDIUM PRESSURE BY OSCILLOMETRIC METHOD
ADVANTAGES
The maximun oscillation amplitude is easily detectable
Easy to automate
Suitable for continuous monitoring of blood pressure.
DISADVANTAGES
but …
Pd may be obtained from the calculated Ps, Pm and the volume plethysmographic waveform is similar to the waveform of blood pressure
It can be considered that the PV relationship is linear in the range of amplitude of the pressure pulse
ε ≅ 5-7 mmHg
BLOOD PRESSURE MEASUREMENT BY DOPPLER ULTRASOUND
Doppler Ultrasound Ps and Pd
Detecting Arterial Wall Motion
Ordinarily observed at a range of: 200 – 500 Hz
Observed at a range of: 30 – 100 Hz
ADVANTAGES
DISADVANTAGES
To use several different crystals for emitters and receivers
Solution
Detecting arterial blood velocity
THE TRANSDUCER
Difracción patterns
Use: high f and big transducers
Detecting arterial blood velocity
Azhim, A. and Kinouchi, Y. Arterial Blood velocity measurement by portable wireless system for healthcare evaluation: The related effects and significant reference data. Recent Adv. In Biomed. Eng. Ganeish R. Neik, Ed. (2009). ISBN: 978-953-307-004-9. InTech.
Emitter and
receiver
?
1.5 E5 cm/s
Pressure-Velocity Relationship
Bernoulli Equation
INTRA OCULAR PRESSURE (IOP) MEASUREMENT
Goldmann Tonometer
Based ib the Imbert-Fick law: pressure within a sphere (P) is roughly equal to the external force (F) needed to flatten a portion of the sphere divided by the area (A) of the sphere which is flattened:
P = F / A
It applies to surfaces which are perfectly spherical, dry, flexible, elastic and infinitely thin
Goldmann Tonometer
Non-contact applanation Tonometer
Bibliography
Webster JG. 1998. Medical Instrumentation: Application and
Design. New York: John Wiley & Sons Inc.
Biomedical transducers and instruments. Tatsuo Togawa, Toshiyo Tamura and P. Åke Öberg. CRC Press, Boca Raton, New York, 1997.
Sensors and signal conditioning. Ramón Pallá-Areny and John G. Webster. John Wiley & Sons, INC., 1991.