blood flow measurement due to doppler effect

17
Blood Flow Measurement Due to Doppler Effect EE01083064 EE01083293

Upload: dewey

Post on 20-Jan-2016

40 views

Category:

Documents


0 download

DESCRIPTION

Blood Flow Measurement Due to Doppler Effect. EE01083064 EE01083293. Introduction. Beam of ultrasound with a transmitted frequency f T is transmitted and reflected back from the red blood cells. f D = f T (2v/c) cos θ f T = Transmitted frequency f d =Doppler shift frequency - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Blood Flow Measurement Due to Doppler Effect

Blood Flow Measurement Due to

Doppler EffectEE01083064EE01083293

Page 2: Blood Flow Measurement Due to Doppler Effect

Introduction

Page 3: Blood Flow Measurement Due to Doppler Effect

Beam of ultrasound with a transmitted frequency fT is transmitted and reflected back from the red blood cells.

fD = fT(2v/c) cosθ

fT= Transmitted frequencyfd=Doppler shift frequency

θ = angle of incidenceC= the velcity of ultrasound

Page 4: Blood Flow Measurement Due to Doppler Effect

Doppler shift frequency normally is in audible range.

Page 5: Blood Flow Measurement Due to Doppler Effect

According to the EquationfD = fT(2v/c) cosθ

The signal reflected back contain the information about the velocity of the blood and direction of

blood flow.

HOW CAN WE EXTRACT THESE INFORMATION FROM THE SIGNAL??????

Page 6: Blood Flow Measurement Due to Doppler Effect

Process to find these terms. This is done by simple possible system

contain oscillator. This drives the trasmitting crystal at its

resonant frequency. Resonant frequency would be 10MHZ for

superficial blood vessel and 5MHZ or less for deeper vessels such as aorta or the aliace arteries.

Mixing

Page 7: Blood Flow Measurement Due to Doppler Effect

The Received crystal converts the reflected ultrasound energy into an electrical signal .

Then it is amplified by RF amplifier.

Then multiplied by transmitted signal.

Further there is a low pass filter to take just Doppler frequency.

Page 8: Blood Flow Measurement Due to Doppler Effect

AT = A cosωT tAR = B cos(ωT+ ωD) tAT Transmitted SignalAR Received Signal

V= AT x AR

V= A cosωT t x B cos(ωT+ ωD) t

V=AB/2 cos(2ωT+ ωD)+ AB/2 cos(ωD t)

Mathematical Calculation

Page 9: Blood Flow Measurement Due to Doppler Effect
Page 10: Blood Flow Measurement Due to Doppler Effect

The Direction of Blood Flow is Lost. Due to these limitations, It is only

used for simple test such as detection of deep vein thrombosis.

Limitations of this Simple System

Page 11: Blood Flow Measurement Due to Doppler Effect

Have two separate demodulator channels, one for forward and other for reverse flow.

Use zero crossing detectors to decide the direction of blood flow.

Solution for this Limitation(Zero crossing Detector)

Page 12: Blood Flow Measurement Due to Doppler Effect
Page 13: Blood Flow Measurement Due to Doppler Effect

Received signal is multiplied by Ecosωt and by a phase shifted version of transmitted signal E cos(ωt+φ)

If received signal is same asAR=Bcos(ωt+ωD)

then VB= BE/2cos(ωDt) ……….(1) so, VA = BE/2cos(ωDt- φ) ……….(2)

So, signal is two channels A & B are identical apart from a phase shift φ

∠ VB - ∠ VA = φ

Page 14: Blood Flow Measurement Due to Doppler Effect

When φ = 90 & ωD > 0 ( forward flow)

Page 15: Blood Flow Measurement Due to Doppler Effect

When φ = 90 & ωD < 0 ( Reverse flow)

Page 16: Blood Flow Measurement Due to Doppler Effect

True Directional Doppler Demodulation System

Preserves all the directional information in the signal

Combination of previous circuit and some new components.

Has limitation that It does not do frequency analysis of the reflected signal.

Page 17: Blood Flow Measurement Due to Doppler Effect