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The Theoretical Basis for Quantitative Ultrasound from Pulse-Echo Data
BRP Support from NIH/NCI RO1CA111289
Timothy J. Hall
Medical Physics Department
University of Wisconsin-Madison
Context for Quantitative Ultrasound
Clinicians use images to describe lesion morphology This lesion is described as “Hypo-echoic” and “Shadowing”
Typical Clinical Breast Ultrasound
Motivation: Quantitative Ultrasound
Mass
Orientation -parallel -not parallel
Shape -round -oval -irregular
Margins -circumscribed -not circumscribed -indistinct -angular -microlobulated -spiculated
Vascularity Special Cases
Calcifications
Posterior acoustic features -none -enhancement -shadowing -combined pattern
Lymph node Intramammary
Boundary -abrupt interface -echogenic halo
ACR BI-RADS®
Ultrasound Lexicon
Clustered microcysts
Foreign body
Mass in skin
Surrounding Tissue -duct changes -Cooper’s ligament changes -edema -architectural distortion -skin thickening -skin retraction/irregularity
Complicated cyst
Lymph node Axillary
-micro-calcification -macro-calcifications -micro-calcification in a mass
-not present (or NA) -present -present adjacent to lesion -diffusely increased surrounding
Echo Pattern -anechoic -hyperechoic -complex -hypoechoic -isoechoic
American College of Radiology Breast Imaging and Reporting Data System
Courtesy of Dr. Elizabeth Burnside, Radiology Dept. UW-Madison
Motivation: Quantitative Ultrasound
American College of Radiology Breast Imaging and Reporting Data System
Mass
Orientation -parallel -not parallel
Shape -round -oval -irregular
Margins -circumscribed -not circumscribed -indistinct -angular -microlobulated -spiculated
Vascularity Special Cases
Calcifications
Posterior acoustic features -none -enhancement -shadowing -combined pattern
Lymph node Intramammary
Boundary -abrupt interface -echogenic halo
ACR BI-RADS®
Ultrasound Lexicon
Clustered microcysts
Foreign body
Mass in skin
Surrounding Tissue -duct changes -Cooper’s ligament changes -edema -architectural distortion -skin thickening -skin retraction/irregularity
Complicated cyst
Lymph node Axillary
-micro-calcification -macro-calcifications -micro-calcification in a mass
-not present (or NA) -present -present adjacent to lesion -diffusely increased surrounding
Echo Pattern -anechoic -hyperechoic -complex -hypoechoic -isoechoic
Motivation: Quantitative Ultrasound
American College of Radiology Breast Imaging and Reporting Data System
80% prevalent 40% malignant Low level echoes
throughout (relative to fat)
12% prevalent 16% malignant
Same echogenicity as
fat
•Anechoic •Hyperechoic •Complex •Hypoechoic •Isoechoic
Hong AS, Rosen EL, Soo MS, Baker JA. BI-RADS for sonography: positive and negative predictive values of sonographic features. AJR Am J Roentgenol 2005; 184:1260-1265.
Figures: Courtesy of Dr. Elizabeth Burnside, Radiology Dept. UW-Madison
• Anechoic • Hyperechoic • Complex • Hypoechoic • Isoechoic
Echo Pattern
Motivation: Quantitative Ultrasound
American College of Radiology Breast Imaging and Reporting Data System
• To be predictive of benign and malignant disease • Help to communicate, facilitate research, and
provide better patients care Many descriptors are subjective and qualitative
Inter-observer disagreement for some descriptors has been shown in the literature1
1Elizabeth Lazarus et al., BI-RADS Lexicon for US and Mammography: Interobserver Variability and Positive Predictive Value, Radiology, 239-2, pp385-391,2006
Goal of QUS
Reduce/remove subjectivity in clinical description of lesions This lesion is described as “Hypo-echoic” and “Shadowing”
Typical Clinical Breast Ultrasound
QUS Theory
Imaging System Properties
Soft Tissue Properties
RF Echo Signal
Ultrasonic (B-mode)
Image
Generalized Image Formation Model
QUS Theory
• We’ve known for many decades about the limiting conditions in acoustic wave propagation – Compare the size of the scattering source (d) with the
acoustic wavelength (λ) • λ << d “specular reflection” (Snell’s law) • λ >> d “Rayleigh scattering” (proportional to f4 d6)
• Physics is more interesting between these limiting
conditions
• Use models for acoustic interactions with tissue to extract physically descriptive parameters – Quantitative ultrasound (QUS)
QUS Theory
• First some definitions – Scattering is an elastic interaction resulting in a change in the
amplitude, frequency, phase or direction of the acoustic wave as a consequence of interacting with a spatial or temporal non-uniformity in the propagation medium
– Absorption is an inelastic process by which some portion of the acoustic wave energy is irreversibly converted into internal energy of the propagating medium structure.
– Acoustic attenuation is the sum of scattering and absorptive losses
QUS Theory
• To estimate an absolute parameter that describes acoustic scattering we compare our data to a model – “Inverse Problem” approach – A model for what?
• The differential scattering cross section
- Defined as the acoustic power scattered per solid angle per unit incident intensity
- Units are (length2 steradian-1)
- Generally normalized to the volume contributing to scattering
- (units become length-1 steradian-1)
QUS Theory
• The differential scattering cross section per unit volume
- (Normalize DSC to the volume contributing to scattering with units of length-1 steradian-1)
- An intrinsic material property
• Special Case – Scattering in the 180o direction
(like pulse-echo ultrasound) • Backscatter coefficient • The acoustic power scattered per solid angle per unit
incident intensity per unit volume in the 180o direction
• Now we have a quantity to model: the BSC
QUS Theory
• The Backscatter Coefficient – The acoustic power scattered per solid angle per
unit incident intensity per unit volume in the 180o direction
• What do we need to know to model it? – Incident intensity – Details of the scattering interaction
QUS Theory
• Incident intensity – Closed-form solutions for simple radiating
surfaces (single-element transducers) – Freely available programs for simulation complex
surfaces (array transducers)
• Typical assumption is incident plane waves
QUS Theory
• Model for backscatter – Continuum model
(continuously varying impedance distribution)
– Discrete scatterer model
QUS Theory
Details of the scattering interaction
• Numerous approaches – Random inhomogeneities – Inhomogeneous wave equation
= Spatial variation from local average compressibility
= Spatial variation from local average mass density
QUS Theory
Details of the scattering interaction – Discrete scatterers
• Numerous approaches – Geometry of the scattering source – Boundary conditions
• Closed-form solutions – Infinite and finite cylinders – Spheres – Prolate spheroids
QUS Theory
• Cylinders (infinite, finite, bent, etc.) – Lax and Feshbach, JASA 20(2): 108-124, 1948. – Faran, JASA 23(4): 405-418, 1951. – Su, et al., JASA 68(2): 687-691, 1980. – Flax, et al., JASA 68(6): 1832-1835, 1980. – Stanton, JASA 94(6): 3454-3462, 1993. – Ye, et al. JASA 102(4): 1964-1976, 1997.
• Assume incident plane wave (normal or oblique) • Compute scattered pressure as a function of angle
Closed-form solutions for scattered pressure
The publication list is examples only and is not exhaustive
QUS Theory
• Single Sphere – Faran, JASA 23(4): 405-418, 1951. – Hickling, JASA 34(10): 1582-1592, 1962.
• Spherical shell and oblate spheroid
– Stanton, JASA 88(3): 1619-1633, 1990. – Stanton, JASA 94(6): 3454-3462, 1993.
• Assume incident plane wave (normal or oblique) • Compute scattered pressure as a function of angle
Closed-form solutions for scattered pressure
The publication list is examples only and is not exhaustive
QUS Theory
• Why so much interest in closed-form solutions for scattering functions? – Scattering theory based on first principles – Comparison between experiment and theory
• Many of the publications on scattering from
cylinders included experimental results
• Early work on scattering from spheres contained comparisons with experiments
QUS Theory
• Discrete models for backscatter – Burke, et al., Ultrasonic Imaging 6: 342—247, 1984.
Ability to accurately measure scattering from single spheres
QUS Theory
Narrowband measurements of scattering from a “cloud” of spherical glass beads in agar Davros, et al. JASA 80(1): 229-237, 1986
4MHz 6MHz 7MHz
QUS Theory
• Comparisons between Faran’s theory for backscatter from spheres Hall, et al., UMB 22(8): 987-997, 1996.
3 transducers required to cover this bandwidth
Scattering from a “cloud” of glass spheres
QUS Theory
Summary • There is a need for quantitative estimates of acoustic
scattering – A common clinical task requires subjective description of
relative echogenicity • Scattering theory has been described for simple
structures • Measurements of phantoms agree very well with
predictions from scattering theory • This is a major step toward the goal of quantifying
scattering in unknown media
Thank you This work was funded, in part, by NIH BRP grant R01CA111289