Download presentation
Presentation is loading. Please wait.
Published byJody Georgia McCoy Modified over 9 years ago
2
George David Associate Professor Ultrasound Physics 03A: Reflections ‘97
3
George David Associate Professor Perpendicular Incidence Sound beam travels perpendicular to boundary between two media 90 o Incident Angle 1 2 Boundary between media
4
George David Associate Professor Oblique Incidence Sound beam travel not perpendicular to boundary Oblique Incident Angle (not equal to 90 o ) 1 2 Boundary between media
5
George David Associate Professor Perpendicular Incidence What happens to sound at boundary? reflected »sound returns toward source transmitted »sound continues in same direction 1 2
6
George David Associate Professor Perpendicular Incidence Fraction of intensity reflected depends on acoustic impedances of two media 1 2 Acoustic Impedance = Density X Speed of Sound
7
George David Associate Professor An Aside about Reflections Echoes occur at interfaces between 2 media of different acoustic impedances speed of sound X density Medium 1 Medium 2
8
Intensity Reflection Coefficient (IRC) & Intensity Transmission Coefficient (ITC) IRC Fraction of sound intensity reflected at interface <1 ITC Fraction of sound intensity transmitted through interface <1 Medium 1 Medium 2 IRC + ITC = 1
9
IRC Equation Z 1 is acoustic impedance of medium #1 Z 2 is acoustic impedance of medium #2 2 reflected intensity z 2 - z 1 IRC = ------------------------ = ---------- incident intensity z 2 + z 1 For perpendicular incidence Medium 1 Medium 2
10
George David Associate Professor Reflections Impedances equal no reflection Impedances similar little reflected Impedances very different virtually all reflected 2 reflected intensity z 2 - z 1 Fraction Reflected = ------------------------ = ---------- incident intensity z 2 + z 1
11
Why Use Gel? Acoustic Impedance of air & soft tissue very different Without gel virtually no sound penetrates skin 2 reflected intensity z 2 - z 1 IRC = ------------------------ = ---------- incident intensity z 2 + z 1 Acoustic Impedance (rayls) Air400 Soft Tissue1,630,000 Fraction Reflected: 0.9995
12
George David Associate Professor Rayleigh Scattering redirection of sound in many directions caused by rough surface with respect to wavelength of sound
13
Diffuse Scattering & Rough Surfaces heterogeneous media cellular tissue particle suspension blood, for example
14
Scattering Occurs if boundary not smooth Roughness related to frequency frequency changes wavelength »higher frequency shortens wavelength »shorter wavelength “roughens” surface
15
George David Associate Professor Specular Reflections Un-scattered sound occurs with smooth boundaries similar to light reflection from mirror opposite of scatter from rough surface wall is example of rough surface
16
George David Associate Professor Backscatter sound scattered back in the direction of source
17
George David Associate Professor Backscatter Comments Caused by rough surfaces heterogeneous media Depends on scatterer’s size roughness shape orientation Depends on sound frequency affects wavelength
18
George David Associate Professor Backscatter Intensity normally << than specular reflections angle dependance specular reflection very angle dependent backscatter not angle dependent »echo reception not dependent on incident angle increasing frequency effectively roughens surface higher frequency results in more backscatter
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.