Transcript Title

The Physics of
Diagnostic Ultrasound
FRCR Physics Lectures
Session 3 & 4
Mark Wilson
Clinical Scientist (Radiotherapy)
[email protected]
Hull and East Yorkshire Hospitals
NHS Trust
Session 3 Overview
Session Aims:
• Recap
• Image Artefacts
• Contrast Agents
• Introduction to Doppler US
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Recap
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Recap
• The term Ultrasound refers to high frequency sound waves.
• Sounds waves are mechanical pressure waves which propagate through a
medium causing the particles of the medium to oscillate backward and forward
• The velocity and attenuation of the ultrasound wave is strongly dependent on
the properties of the medium through which it is travelling
=c/f
c=k/
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Recap
• Diagnostic ultrasound utilises the pulse-echo principle
D
Source of sound
)
)
)
Pulse
Echo
) )
Sound reflected at boundary
Distance = Speed x Time
2D = c x t
• Each pulse-echo sequence produces one line of the image
• Several pulse-echo sequences are needed to compose a full image frame.
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Recap
Ultrasound waves undergo the following interactions:
• Reflection
• Scatter
• Refraction
• Attenuation and Absorption
• Diffraction
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Recap
Reflection
z1
z2
pi , Ii
pt , It
pr , Ir
Intensity Reflection Coefficient (R)
R=
Ir
Ii
=
(
Z2 – Z1
Z1 + Z2
2
)
Acoustic Impedance z =  k
Acoustic Impedance z = c
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Recap
Reflection
• Strength of reflection depends on the difference between the Z values of the
two materials
• Ultrasound only possible when wave propagates through materials with
similar acoustic impedances – only a small amount reflected and the rest
transmitted
• Therefore, ultrasound not possible where air or bone interfaces are present
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Recap
Scatter
• Reflection occurs at large interfaces such
as those between organs where there is a
change in acoustic impedance
• Within most organs there are many small
scale variations in acoustic properties
which constitute small scale reflecting
targets
• Reflection from such small targets does
not follow the laws of reflection for large
interfaces and is termed scattering
• Scattering redirects energy in all
directions, but is a weak interaction
compared to reflection at large interfaces
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Recap
Refraction
When an ultrasound wave crosses a tissue boundary at an angle (non-normal
incidence), where there is a change in the speed of sound c, the path of the
wave is deflected as it crosses the boundary
c1
c2 (>c1)
Snell’s Law
i
t
sin (i)
c1
= c
sin (t)
2
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Recap
Attenuation
• As an ultrasound wave propagates
through a medium, the intensity
reduces with distance travelled
Intensity, I
• Attenuation describes the reduction in
intensity with distance and includes
scattering, diffraction, and absorption
• Attenuation increases linearly with
frequency
Low freq.
High freq.
• Limits frequency used – trade off
between penetration depth and
resolution
I = Ioe- d
Distance, d
Where  is the attenuation coefficient
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Recap
Absorption
• In soft tissue most energy loss (attenuation) is due to absorption
• Absorption is the process by which ultrasound energy is converted to heat in
the medium
• Absorption is responsible for tissue heating
Decibel Notation
Attenuation and absorption is often expressed in terms of decibels
Decibel, dB = 10 log10 (I2 / I1)
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Image Artefacts
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Artefacts
Image Artefacts
When forming a B-mode image, a number of assumptions are made about
ultrasound propagation in tissue. These include:
• Speed of sound is constant
• Attenuation in tissue is constant
• Ultrasound pulse travels only to targets that are on the beam axis and back to
the transducer
Significant variations from these conditions in the target tissues are likely to
give rise to visible image artefacts
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Artefacts
Range Errors
• The distance, d, to the target is derived from the time elapsed between
transmission of the pulse and receipt of the echo from the target, t
• In making this calculation the system assumes that t = 2d / c, where the speed
of sound is constant at 1540 m/s
• If the speed of sound in the medium between the transducer and target is
greater (or less) than 1540 m/s, the echo will arrive back at the transducer
earlier (or later) than expected for a target of that range
Fat c = 1420 m/s
Tissue c = 1540 m/s
Target
Displayed at
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Artefacts
Refraction
Refraction of the ultrasound beam as it
passes between tissues with a different
speed of sound can result in objects
appearing at an incorrect position in
the image
Target
Displayed at
Medium 1
c1
Medium 2
c2 > c1
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Artefacts
Attenuation Artefacts
• During imaging the outgoing pulse and returning echoes are attenuated as
they propagate through tissue, so that echoes from deeper targets are weaker
than those from similar superficial targets
• Time Gain Compensation (TGC) is applied to correct for such changes in
echo amplitude with target depth
• Most systems apply a constant rate of compensation designed to correct for
attenuation in typical uniform tissue
• The operator can also make additional adjustments to compensate via slide
controls that adjust the gain applied specific depths in the image
• TGC artefacts may appear in the image when the applied compensation does
not match that actual attenuation rate in the target tissue
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Artefacts
Acoustic Enhancement
• Occurs when ultrasound passes
through a tissue with low attenuation
Image of renal cyst
• Echoes from deeper lying tissues are
enhanced due to the relatively low
attenuation in the overlying tissue
• This occurs because the TGC is set to
compensate for the greater attenuation
in the adjacent tissues
Low attenuation
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Artefacts
Acoustic Shadowing
• Occurs when ultrasound wave
encounter a very echo dense (highly
attenuating) structure
Image of Gallstone
• Nearly all of the sound is reflected,
resulting in an acoustic shadow
• This occurs because the TGC is set to
compensate for the lower attenuation in
the adjacent tissues
High attenuation
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Artefacts
Reverberation Artefact
• Reverberation artefacts arise due to
reflections of pulses and echoes by
strongly reflecting interfaces
• Occur most commonly where there
is a strongly reflecting interface
parallel to the transducer face
• Involves multiple reflections - Initial
echo returns to reflecting interface as
if it is a weak transmission pulse and
returns a second echo (reverberation)
Transducer
Interface
Reverberation
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Artefacts
Attenuation Artefacts
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Artefacts
Attenuation Artefacts
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Contrast Agents
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Contrast Agents
Ultrasound Contrast Agents
• Ultrasound contrast agents are
gas-filled micro-bubbles which are
injected into the blood stream
• Micro-bubbles will give increased
backscatter signal due to the large
acoustic impedance mismatch
between the gas-filled bubble and
surrounding tissue
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Contrast Agents
Ultrasound Contrast Agents
• Micro-bubble suspension is injected intravenously into the systemic
circulation in a small bolus
• The micro-bubbles will remain in the systemic circulation for a certain
period of time
• Ultrasound waves are directed on the area of interest and when the
micro-bubbles in the blood flow past the imaging window they give rise
to increased signal
• Allows detection of blood flow where it would otherwise not be seen
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Contrast Agents
Ultrasound Contrast Agents
Name
Capsule
Gas
Bubble
Size
LEVOVIST
Palmitic acid
Air
3-5 m
SONOVIST
Cyano-acrylate Air
2 m
DEFINITY
Lipid
Perfluoropropane
2 m
OPTISON
Albumin
Octafluoropropane 3.7 m
SONOVUE
Phospholipids
SF6
2-3 m
SONAZOID
Surfactant
Fluorocarbon
3.2 m
ALBUNEX
Albumin
Air
4 m
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Contrast Agents
Targeted Contrast Agents
• Targeted contrast agents are under preclinical development
• They retain the same general features as untargeted micro-bubbles,
but they are outfitted with ligands that bind to specific receptors
expressed by cell types of interest
• Micro-bubbles theoretically travel through the circulatory system,
eventually finding their respective targets and binding specifically
• If a sufficient number of micro-bubbles have bound to the target area,
an increased signal will be seen
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Doppler Ultrasound
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Doppler Ultrasound
The Doppler Effect
• The Doppler effect is observed regularly in our daily lives, e.g. it can
be heard as the changing pitch of an ambulance siren as it passes by
• The Doppler effect is the change in the observed frequency of the
sound wave (fr) compared to the emitted frequency (ft) which occurs
due to the relative motion between the observer and the source
• Consider three situations
- Source and observer stationary
- Source moving towards observer
- Source moving away from observer
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Doppler Ultrasound
Source and observer stationary
Source
)
))))
Observer
fr = ft
The observed sound has the same frequency as the emitted sound
(Note: Frequency is the number of cycles per second)
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Doppler Ultrasound
Source moving towards observer
)
))))
f r > ft
Causes the wavefronts travelling towards the observer to be more
closely packed, so that the observer witnesses a higher frequency
wave than emitted
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Doppler Ultrasound
Source moving towards observer
) )))
)
f r < ft
The wavefronts travelling towards the observer will be more spread
out, so that the observer witnesses a lower frequency wave than
emitted
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Doppler Ultrasound
The Doppler Effect
• The resulting change in the observed frequency from that transmitted
is known as the Doppler shift
• The magnitude of the Doppler shift frequency is proportional to the
relative velocity between the source and the observer
• It does not matter if it is the source or the observer is moving
• The Doppler effect enables Ultrasound to be used to assess blood
flow by measuring the change in frequency of the ultrasound scattered
from moving blood
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Doppler Ultrasound
Ultrasound measurement of blood flow
• Transducer is held stationary and the blood moves with respect to the
transducer
• The ultrasound waves transmitted by the transducer strike the moving
blood, so the frequency of the ultrasound experienced by the blood is
dependent on whether the blood is stationary, moving towards or away
from the transducer
• The blood then scatters the ultrasound, some of which travels in the
direction of the transducer and is detected
• The scattered ultrasound is Doppler frequency shifted again as a
result of the motion of the blood, which now acts as a moving source
• Therefore, a Doppler shift has occurred twice between the ultrasound
being transmitted and received back at the transducer
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Doppler Ultrasound
Ultrasound measurement of blood flow
2 ft v
cos
c
Doppler frequency shift, fd = fr – ft =
Target direction

fr = received frequency
ft = transmitted frequency
c = speed of sound
v = velocity of blood
 = angle between the path of the ultrasound beam and the direction of the
blood flow (angle of insonation)
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Doppler Ultrasound
Ultrasound measurement of blood
flow
• The detected Doppler shift also
depends on the cosine of the angle 
between the path of the ultrasound
beam and the direction of blood flow
• The operator can alter  by
adjusting the orientation of the
transducer on the skin surface
cos
1

0
90
• Desirable to adjust  to obtain the
highest Doppler frequency shift
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Doppler Ultrasound
Ultrasound measurement of blood flow
If the angle of insonation of the ultrasound beam is known it is possible
to use the Doppler shift frequency to estimate the velocity of the blood
using the Doppler equation
v =
c fd
2 ft cos
In diseased arteries the lumen will narrow and the blood velocity will
increase
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Doppler Ultrasound
Ultrasound measurement of blood flow
Narrowing in artery
A1
V1
A2
V2
The flow (Q) remains constant
Q = A1 V1 = A2 V2
A = Area
V = Velocity
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Break
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Session 4 Overview
Session Aims:
• Continuous Wave Doppler US
• Pulsed Wave Doppler US
• Harmonic Imaging
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Doppler Ultrasound
Continuous Wave and Pulsed Wave Doppler
• Doppler systems can be either continuous wave or pulsed wave
• Continuous wave (CW) systems transmit ultrasound continuously
• Pulsed wave (PW) systems transmit short pulses of ultrasound
• The main advantage of PW Doppler is that Doppler signals can be
acquired from a known depth
• The main disadvantage of PW Doppler is that there is an upper limit to
the Doppler frequency shift which can be detected
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Doppler Ultrasound
Continuous Wave (CW) Doppler
• In a CW Doppler system there
must be separate transmission
and reception of ultrasound –
transducer with two separate
elements
• The region from which Doppler
signals are obtained is determined
by the overlap of the transmit and
receive ultrasound beams
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Doppler Ultrasound
Pulsed Wave (PW) Doppler
• In a PW Doppler system it is
possible to use the same
transducer element for both
transmit and receive
• The region from which Doppler
signals are obtained is
determined by the depth of the
gate and the length of the gate,
which can both be controlled by
the operator
Transducer
Gate depth
Gate length
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Doppler Ultrasound
Ultrasound signal received by transducer
The received ultrasound signal consists of the following four types of
signal:
• echoes from stationary tissue
• echoes from moving tissue
• echoes from stationary blood
• echoes from moving blood
The task for the Doppler system is to isolate and display the Doppler
signals from blood, and remove those from stationary and moving
tissue
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Doppler Ultrasound
Ultrasound signal received by
transducer
• Doppler signals from blood tend
to be low amplitude (small reflected
echo) and high frequency shift
(high velocity)
• Doppler signals from tissue are
high amplitude (large reflected
echo) and low frequency shift (low
velocity)
• These differences provide the
means by which signals from true
blood flow may be separated from
those produced by surrounding
tissue
Amplitude
Tissue
Blood
Frequency
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Doppler Ultrasound
Doppler signal processing
Transducer
Demodulation
Separation of the Doppler
frequencies from the underlying
transmitted signal
Demodulator
Signal
processor
High-pass filtering
Removal of the tissue signal
High-pass filter
Frequency estimator
Frequency estimation
Calculation of Doppler frequency
and amplitudes
Display
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Doppler Ultrasound
Demodulation
• The Doppler frequencies produced by moving blood are a tiny fraction
of the transmitted ultrasound frequency
• E.g. If transmitted frequency is 4 MHz, a motion of 1 m/s will produce a
Doppler shift of 5.2 kHz, which is less the 0.1% of the transmitted
frequency
• The extraction of the Doppler frequency information from the
ultrasound signal received from tissue and blood is called demodulation
• In PW Doppler, need the PRF to be at least twice the maximum
Doppler shift frequency in order to avoid ‘aliasing’ (not a problem in CW)
• Aliasing is an artefact introduced by under-sampling in which high
frequency components take the alias of a low frequency component
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Doppler Ultrasound
High-pass Filtering
Amplitude
Amplitude
Tissue
High-pass
Filtering
Blood
Blood
Frequency
Frequency
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Doppler Ultrasound
Frequency Estimation
• A spectrum analyser calculates the amplitude of all the frequencies
present within the Doppler signal
• In the spectral display the brightness is related to the amplitude of the
Doppler signal component at that particular frequency
Frequency
shift
Time
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Doppler Ultrasound
Aliasing
Original signal
Aliased signal
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Doppler Ultrasound
Aliasing
Aliased signal
Increased PRF
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Doppler Ultrasound
Duplex Imaging
• Duplex imaging combines Doppler information with a real-time B-mode
image
• This produces a 2D representation of the direction and velocity of the
blood flow on a grey-scale image
• In a typical display blood flowing towards the transducer is coded as
red and blood flow away from the transducer is coded blue
Red – towards transducer
Blue – away from transducer
Green - Variance
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Doppler Ultrasound
Doppler Displays – Spectral Doppler
• Available in CW and PW Doppler
• Detailed analysis of distribution of flow
• Examine change in flow with time
Frequency shift
or
Velocity
Time
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Doppler Ultrasound
Doppler Displays – Colour Doppler
• Available in PW Doppler only
• Superimposed Doppler information on underlying B-mode image
• Overall view of flow in region
• The sign (direction), mean Doppler shift (mean velocity) and variance
(turbulence) of Doppler spectrum are usually colour-coded and
displayed
Red – towards transducer
Blue – away from transducer
Green - Variance
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Doppler Ultrasound
Doppler of Common Carotid Artery
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Doppler Ultrasound
Blockage in Carotid Artery
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Doppler Ultrasound
Renal Colour Doppler
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Doppler Ultrasound
Doppler Displays – Power Doppler
• In a Colour Doppler image the magnitude of the frequency shift colour
encodes the pixel value and assigns a colour depending on blood flow
direction
• This Doppler signal processing places a restriction on the motion
sensitivity since the signals received must be extracted to determine the
velocity (magnitude of Doppler shift) and direction (phase shift)
• Power Doppler encodes the strength of the Doppler shifts (amplitude,
intensity, power) with colours and ignores directional (phase) information
• In Power Doppler the magnitude of the Doppler signal is displayed
rather than the Doppler frequency shift (e.g. the density of the red blood
cells is depicted rather than their velocity)
• Power Doppler therefore exhibits increased sensitivity to slow flow
rates at the expense of directional and quantitative flow information
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Doppler Ultrasound
Suspicious dark lesion
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Doppler Ultrasound
Power Doppler – Circle of Willis
Suspicious dark lesion
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Doppler Ultrasound
Prostate Cancer
Suspicious dark lesion
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Harmonic Imaging
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Harmonic Imaging
Introduction
• Harmonic imaging of tissue is useful in suppressing weak echoes
caused by artefact (acoustic noise) which cloud the image and make it
difficult to identify anatomical features.
• These echoes (often called clutter) are particularly noticeable in fluid
filled areas (e.g. heart or cyst) and are a common problem when imaging
large patients.
• Harmonic imaging is possible by utilising harmonic frequencies of the
ultrasound pulse.
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Harmonic Imaging
The Ultrasound Pulse
• Ideally the US pulse would rise and fall very quickly and contain only
one frequency (or wavelength)
• In reality the US pulse contains a finite range of frequencies (or
wavelengths)
Actual
Ideal
Frequency
Frequency
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Harmonic Imaging
Spatial Pulse Length (SPL)
The spatial pulse length (in mm) is defined as  n
Where  is the wavelength and n is the number of cycles
A wider range of wavelengths and more cycles produces a longer SPL
Use a higher frequency and shorter US pulse to give smaller SPL and
improved resolution
For Diagnostic US typical SPL values range from 0.3 to 1.0 mm
SPL
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Harmonic Imaging
Bandwidth
Amp
• Bandwidth describes the spread of
US frequencies the transducer can
transmit/receive
• The frequency content may be
specified in terms of the Q factor:
Q factor = F0 / (F2 – F1)
• An increased bandwidth and a
decreased SPL reduces the Q Factor
• High Q = pure ultrasound pulse
Freq
F0 is the centre frequency and the
lower and upper frequencies (F2 and
F1) are at half the peak amplitude
(reduction of 3 dB)
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Harmonic Imaging
Side Lobes
• Ideally US pulse energy appears
as a single front travelling in
forward direction
• Some energy travels off in
different directions called side
lobes
side lobes
Main lobe
• The energy transmitted in side
lobes can reduce image quality
(contrast and resolution)
Transducer
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Harmonic Imaging
Non-linear Propagation
• In the description of propagation of sound waves given in the first session the
wave propagated with a fixed speed determined by the properties of the medium
• This is a good approximation to reality when the amplitude of the wave is
small, but at higher pressure amplitudes the effects on non-linear propagation
become noticeable
• The speed at which each part of the wave travels is related to the properties of
the medium and to the local particle velocity, which enhances or reduces the
speed
• In the high pressure (compression) parts of the wave this results in a slight
increase in speed
• In the low pressure (rarefaction) parts of the wave this results in a slight
decrease in speed
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Harmonic Imaging
Non-linear Propagation
• As the wave propagates into the
medium the compression parts catch
up with the rarefaction parts
• The compression parts become
taller and narrower in amplitude,
while the rarefaction become lower in
amplitude
• The rapid changes in pressure in
the compression parts of the wave
appear in the pulse spectrum as high
frequency components, these are
multiples of the fundamental
frequency F0 known as Harmonics
Fundamental Frequency
F0
Second Harmonic
2F0
Third Harmonic
3F0
Frequency
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Harmonic Imaging
Harmonic Imaging
• In harmonic imaging an US pulse is transmitted with fundamental frequency F0
but due to non-linear propagation the returning echoes also contain energy at
harmonic frequencies 2 F0 and 3 F0.
• The imaging system ignores the fundamental frequency component of the echo
and forms an image using only the 2nd harmonic component.
• The effective ultrasound beam (the harmonic beam) is narrower than the
conventional beam because non-linear propagation occurs most strongly in the
highest amplitude parts of the transmitted beam (i.e. near beam axis).
• Weaker parts of the beam such as side lobes and edges of the main lobe
produce little harmonic energy and are suppressed in relation to the central part
of the beam.
• Harmonic imaging also reduces acoustic noise from weak echoes and
reverberations.
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Harmonic Imaging
Transmit Pulse
Received Echo
Filtered Echo
Transducer
Bandwidth
Transmit
Pulse
F0
Frequency
F0
2F0
2F0
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Harmonic Imaging
Harmonic Imaging
• Harmonic imaging can only be performed with a wide bandwidth
transducer which can respond to both the fundamental frequency and
its 2nd harmonic.
• The received echoes are passed through a filter which removes
frequencies around F0 and only allows through those near to 2F0.
• As ‘acoustic noise’ echoes are mainly at the fundamental frequency,
they are suppressed giving a clearer image.
• To achieve good separation of the received 2nd harmonic frequencies
from the fundamental frequencies, the frequency spectra of the pulse
and received echoes must be made narrower than in normal imaging.
• Reduction of the frequency range results in an increase in pulse
length and a reduction in axial resolution.
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The End
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