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1. Ultrasound Physics 04:Scanner
2. Resonant Frequency Frequency of Highest Sustained Intensity
Transducers preferred or resonant frequency
Examples
Guitar String
Bell
3. Pulse Mode Ultrasound transducer driven by short voltage pulses
short sound pulses produced
Like plucking guitar string
Pulse repetition frequency same as frequency of applied voltage pulses
determined by the instrument (scanner)
4. Pulse Duration Review typically 2-3 cycles per pulse
Transducer tends to continue ringing
minimized by dampening transducer element
5. Damping Material Goal:
reduce cycles / pulse
Method:
dampen out vibrations after voltage pulse
Construction
mixture of powder & plastic or epoxy
attached to near face of piezoelectric element (away from patient)
6. Disadvantages of Damping reduces beam intensity
produces less pure frequency (tone)
7. Bandwidth Damping shortens pulses
the shorter the pulse, the higher the range of frequencies
Range of frequencies produced called bandwidth
8. Bandwidth range of frequencies present in an ultrasound pulse
9. Quality Factor (Q) Unitless
Quantitative Measure of Spectral Purity
10. Which has a Higher Quality Factor?
11. Damping More damping results in
shorter pulses
more frequencies
higher bandwidth
lower quality factor
lower intensity
Rule of thumb
for short pulses (2 - 3 cycles)
quality factor ~ number of cycles per pulse
12. An Aside about Reflections Echoes occur at interfaces between 2 media of different acoustic impedances
speed of sound X density
13. 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
14. IRC Equation Z1 is acoustic impedance of medium #1
Z2 is acoustic impedance of medium #2
15. Reflections Impedances equal
no reflection
Impedances similar
little reflected
Impedances very different
virtually all reflected
16. Why Use Gel? Acoustic Impedance of air & soft tissue very different
Without gel virtually no sound penetrates skin
17. Transducer Matching Layer Transducer element has different acoustic impedance than skin
Matching layer reduces reflections at surface of piezoelectric element
Increases sound energy transmitted into body
18. Transducer Matching Layer placed on face of transducer
impedance between that of transducer & tissue
reduces reflections at surface of piezoelectric element
Creates several small transitions in acoustic impedance rather than one large one
19. Transducer Arrays Virtually all commercial transducers are arrays
Multiple small elements in single housing
Allows sound beam to be electronically
Focused
Steered
Shaped
20. Electronic Scanning Transducer Arrays
Multiple small transducers
Activated in groups
21. Electrical Scanning Performed with transducer arrays
multiple elements inside transducer assembly arranged in either
a line (linear array)
concentric circles (annular array)
22. Linear Array Scanning Two techniques for activating groups of linear transducers
Switched Arrays
activate all elements in group at same time
Phased Arrays
Activate group elements at slightly different times
impose timing delays between activations of elements in group
23. Linear Switched Arrays Elements energized as groups
group acts like one large transducer
Groups moved up & down through elements
same effect as manually translating
very fast scanning possible (several times per second)
results in real time image
24. Linear Switched Arrays
25. Linear Phased Array Groups of elements energized
same as with switched arrays
voltage pulse applied to all elements of a groupBUT
elements not all pulsed at same time
26. Linear Phased Array timing variations allow beam to be
shaped
steered
focused
27. Linear Phased Array
28. Linear Phased Array
29. Linear Phased Array
30. Linear Phased Array
31. Listening Mode Listening direction can be steered & focused similarly to beam generation
appropriate timing variations applied to echoes received by various elements of a group
Dynamic Focusing
listening focus depth can be changed electronically between pulses by applying timing variations as above