Module 3 : Doppler Principles Flashcards
doppler principle
change in frequency of sound, light, or other waves caused by the motion of the source or the observer
Doppler effect - ultrasound
- change in frequency of sound caused by the motion of red blood cell (relative to transducer)
- difference between transmitted frequency (transducer frequency) and received frequency (reflected or echo frequency)
movement toward transducer
- echo frequency larger than transducer frequency
- ANTEGRADE FLOW
movement away transducer
- echo frequency will be smaller than transducer frequency
- RETROGRADE FLOW
methods used to detect and analyze doppler shifts
- color flow
- spectral waveforms
- audible sounds
doppler shift basic equation
Fd = Fr - Fo
doppler shift dependent factors
- transmitted (sent) frequency
- velocity of the moving blood
- angle between the moving blood and the sound beam
complex doppler shift equation
Fd = 2 x Fo x V x cos0 / c
angle of insonation
- MOST IMPORTANT FACTOR that influences calculation of the DOPPLER SHIFT
- ideal orientation would be at an angle 0 (largest doppler shift) cos 0 = 1 THIS IS VIRTUALLY IMPOSSIBLE TO ATTAIN EXCEPT IN HEART
- when the blood flow is at an angle of 90 (cos 0 = 0) there is NO SHIFT DETECTED so NO MEASURABLE RETURNING FREQUENCY
correct doppler angle
30 - 60 to the blood vessel
- REDUCE MARGIN OF ERROR, REPRODUCIBLE
doppler angle greater than 60
- doppler shifts difficult to quantify due to large margin of error
- lead to errors in estimates of peak frequency
venous flow assessment
- angle is not important
- velocities are not used
- angle correct is set to zero
continuous wave doppler (CW)
- continuously excited
- contains two piezoelectric elements
+ one transmitting, one receiving - no image produced
- impossible to select a specific depth and region to sample
- knowledge of the anatomy
- advantage : sample high velocity with no aliasing
pulsed wave doppler
- sound pulses produced by the transducer at regular intervals
- isolate signals from a desired depth
- PRF limits measurement of high velocities by producing aliasing
- pulsed doppler instruments combined with real time B Mode
- B mode allows visualization of structure
nyquist limit
- doppler shift exceeds 1/2 the PRF
- occurs when insufficient amount of time to collect the returning signal information before next pulse is sent
spectral display
- doppler shift frequencies are separated into individual frequency components using FAST FOURIER TRANSFORM
- displayed as a spectrum or “image” of the doppler frequency
+ time = horizontal axis (x)
+ velocity = vertical axis (y)
+ brightness of pixel - the z axis ( proportional to the # of rbc’s)
Quadrate detection
- processes the signal as a (+) or (-) value depending on direction of flow relative to the doppler beam
peak systole
- peak velocity of the cardiac cycle
dicrotic notch
- early diastole flow reversal signifies closing of the aortic valve
end diastole
- velocity at end diastole just prior to systole
envelope
- white line that outlines the changes in frequencies
- determined by the number of blood cells in a sample
window
- Clear area below the envelope that displays no frequencies
spectral broadening
- ” thickness” of the white line up to “filing in” of window