ecography at high frequencies and sub-millimeter · pdf filebacking block (absorber) 5 ... is...
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Ecography at high frequencies and sub-millimeter resolution
Elisa Prandini----------------------------
Medical Physics Exam23rd PhD Cycle
10 December 2009
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Ultrasounds● Sound is a pressure
wave that propagates in a medium at a peculiar velocity related to the medium density
● ULTRASOUNDS: acoustic energy with a frequency above human hearing (2Hz-20KHz)
● Medicine uses ultrasounds in diagnostic imaging technique (diagnostic sonography or ultrasonography)
In ultrasonography the wave-properties of sound are the key ingredients of the imaging techniques
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Wave properties of sound● λ=c
sν, where c
s is the sound velocity in the medium
● Reflection (eco)
● Refraction
Acoustic impedance (Z) of a medium
● Scattering● Absorption
(heat)
Attenuation (dB/mm)I=I
0exp[-μx] (intensity att. coefficient)
μ=μa+μ
s with μ
s/μ 0.1-0.3 (liver)
→ conversion into heat dominates→ attenuation is frequency related:
Approx: “n” Mhz – “n” dB/mm
(Reflection fraction)
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The transducer● Electrodes● Piezoelectric crystal
– dimensions → resonance freq.● 1.8 mm: Ʋ=1Mhz● 0.18 mm: Ʋ=10 MHz
● Backing block (absorber)
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Basic Imaging System in modern ecography
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The ecographic image
Image Properties
● Angular resolution
● Axial resolution
● Frame Rate
● Maximum range r: rmax
= vsT/2
● The transducer emits (and receives) short pulses of sonic energy
● The imaging system then waits a time T before sending out another pulse
● During this time T any echoes from obstacles in the path are reflected and received by the transducer
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Angular Resolution IA transducer, or array of transducer, can have circular or rectangular aperture
The angular resolution is the angular beam width. Quantification:
● Study the angular energy distribution and beam pattern obtained by collecting with a receiver at a distance d and angle θ the sound emitted with a frequency f
c by a
transducer of aperture a
Angular distribution of acoustic energy measured by the receiver
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Angular Resolution II● The beam pattern in the
ideal case (and “far field” approx) is a sinc function
● The beam width (i.e. Angular resolution) can be defined as the angular distance between the first zeros of the function
● ΔΘ=2 arcsin(vs/af
c)
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Angular Resolution II
HIGH ANGULAR RESOLUTION REQUIRES
LARGE TRANSDUCER APERTURE AND
FREQUENCE
● The beam pattern in the ideal case (and “far field” approx) is a sinc function
● The beam width (i.e. Angular resolution) can be defined as the angular distance between the first zeros of the function
● ΔΘ=2 arcsin(vs/af
c)
Side lobes effects (image degradation) can be reduced (apodization):
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Angular Resolution of phased arraysPhased array ● Phased arrays are multiple
tranducers whose relative phase is electronically adjusted in order to scan automatically the area of interest
● The bam pattern is not simmetrical anymore, and the beam width is a function of the beam direction
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Axial Resolution I
● We consider a pulse of duration ᐃt and frequence fc
● The axial resolution ᐃr, given by ᐃr = vs x ᐃt, is related
to the bandwidth B of the transducer
● Which frequencies are required to support such a pulse?
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Axial Resolution II● We can study the Fourier Transform of the pulse
● Its FT is the sinc function, with most of the energy contained within the two main lobes centered in ±f
c
● Most of the energy of the pulse can be trasmitted if the transducer has a bandwidth extending to the first zeros of the sinc function (that occurs when ᐃfᐃt=1)
● B = 2ᐃf = 2/ᐃt = 2vs/ ᐃr
FT of the pulse
● High axial resolution ᐃr=B/ 2vs:
increase B → decrease ᐃt
● BUT: at least 1 cycle: ᐃt≥1/fc → B⩽2 f
c
● increase B → decrease ᐃt → incr. fc
● Usually in ultrasonography: B=0.2-0.5 fc
HIGH AXIAL RESOLUTION REQUIRES HIGH FREQUENCIES
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Optimal frequency: a compromise● Both angular and axial resolution increases with increasing
frequencies
● But: better resolution means smaller penetration!
Circular transducer casef-number: ratio of the focal lenght of the transducer to its diameter
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Ultrasonography in practiceIs a very important tool for medical diagnostic used in
many different fields:
– Pregnancy
– Gynaecology
– Neurology (carotid)
– Andrology
– Cardiology (eco doppler)
– Gastroenterology
– Urology
– Cardiovascular system (intravascular ultrasound)
– Oftamology
– DermatologyHigher frequencies allowed!
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Ultrasonography in dermatology● High frequencies can be used in other
medical fields, such as dermatology (since 1979)
● Well established (diagnostic): 7.5, 15, 20 MHz
● Under study 100-150 MHz frequencies: fine structure
20 MHz ultrasonography:
● Axial res. 80 μm
● Lateral res. 200 μm
● Max depth: 1 cm
Typical use in diagnostic:
● Attenuation: in homogeneous structures (cysts) is smaller
● Skin thickness measurements
● Morphological change of limph-nodes
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Ultrasonography in oftamology● 10 - 20 MHz probes for diagnostic
● Deep structure of the eye (posterior segment)
● Important parameter: depth of field (axial range around the focus where the echo amplitude is at least ½ max) → simultaneous imaging of anterior and posterior segment of the eye is not possible with good resolution!
– 10 - 20 MHz → dof 9mm – 5mm
– Suitable for posterior segment
● In oftamology, usually mechanically scanned single element - focused transducer are employed
● The research in this sector now is trying to apply arrays (linear or circular)
20 MHz, dof 5mm, axial res. 0.5 mm
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UBM: Ultrasounds BioMicroscopy● UBM is a technique that uses very high
frequency ultrasounds for the study of the eye at microscopic resolution
● Typical range is 50-100 MHz
● The axial resolution is of the order of hundredth of μm
● The penetration is ∼mm
● Typical diagnostic use:anomalies in the structure of outer parts of the eye (angle-closure glaucoma)
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UBM images● Used to study the outer layers of
the eye (with high resolution)
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What can we “listen” from this image?
- The cornea, lens and irid are well visible
- Some informations are displayed:
● Dimensions: 5x5mm
● T delay: 2.24 mm
● Gain: 73 dB
● Time Gain Compensation (5 dB/mm) → suggests a frequency above 50 MHz
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Some measurementsstep 1: “set scale”
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The vertical profile
0.5 mm0.5 mm
2 mm
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The axial resolution
The resolution is of the order of 0.04 mm
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The “background” is quite flat
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The lens aperture
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An example of LSF
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Last measure: the irido-corneal angle
22.3°
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A new technique... back to light● Comparison between UBM image and AS-OCT (Anterior
Segment Optical Coherence Tomography)
● AS OCT is based on principles of low coherence interferometry
UBM● 50 MHz ● lateral resolution 50 μm ● axial resolution of 25 μm● Tissue penetration 4.0 to 5.0 mm● The scanner produces 5.0 mm x 5.0 mm field ● scan rate 8 frames/s
AS OCT● 13 μm wavelenght● lateral resolution 60 μm ● axial resolution is 18 μm● The scan was 16.0 mm in diameter and 6.0 mm deep (tissue)● Image acquisition rate of 8 frames/s
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Conclusions● Ultrasonography is a very useful diagnostic tool
– In general is non invasive
– No collateral effects● However:
– Skilled operator needed
– The image quality (axial and agular resolution) requires high frequencies, limited by strong attenuation
– High resolution (tens of microns) images can be achieved only in superficial scans
● UBM is a common technique that uses very high frequency ultrasounds for the study of the anterior segment of the eye with ∼50μm resolution
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Bibliography● “Basic physics of Ultrasound Imaging”, J.E.Aldrich, 2007
● “Basic Principles of Ultrasound Imaging System Design”, notes by A.Seagar, 2002
● “Priciples of Medica Imaging”, K.K.Shung, 1992
● “Ultrasound biomicroscopy”, C.Pavlin, 1998
● “Advances in UBM”, F.S.Foster, 2000
● “Improved High-Resolution Ultrasonic Imaging of the Eye”, R.Silverman, 2008
● “A comparison of 10 MHz and 20 MHz ultrasound probes in imaging the eye and orbit”, S.A.Hewick, 2004
● “Ultrasonography in dermatology”, D.Dill-Muller, 2007
● “Comparison of AS-OCT and UBM for assessment of the anterior segment”, T.Dada, 2007
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Backup slides
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Acoustic Impedance of Body Tissues
Medium Z (kg m-2s-1)
Air 4.29 x 102
Blood 1.59 x 106
Water 1.50 x 106
Brain 1.58 x 106
Soft Tissue 1.63 x 106
Bone 7.78 x 106
Muscle 1.70 x 106
Skin 1.70 x 106
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Sound velocity
Medium v (m s-1)
Air 300
Blood 1570
Water 1500
Fat 1450
Soft Tissue 1540
Liver 1560
Bone 3300-4080
Iron 5000
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The Scans
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Scans