Title: Chapter 10 Sound Beams
1Chapter 10Sound Beams
2Sound Beams
- Shape
- Regions
- Crystal characteristic vs. depth of focus
- Crystal characteristics which determine the
degree of beam spread (divergence)
3Shape of a Sound Beam
- At the starting point the beam diameter is equal
to the transducers diameter - The beam narrows until it reaches its smallest
diameter - The Focus
- The beam then progressively expands or diverges
4Anatomy of a Sound Beam
- Focus
- Near zone
- Focal length
- Far zone
- Focal zone
5Focus
- The location where the beam diameter is the
narrowest - For a disc-shaped crystal the beam diameter at
the focus ½ the width of the beam as it leaves
the transducer
6Near Zone
- Aka, near field or Fresnel zone
- The region from the transducer to the focus
- The ultrasound beam gradually narrows within the
near zone - The focus is located at the end of the near zone
7Focal Length
- The distance from the transducer to the focus
- Aka, focal depth or near zone length (NZL)
8Far Zone
- The region starting at the focus and extending
deeper - Aka, far field or Fraunhofer zone
- The sound beam diverges within the far zone
- At the beginning of the far zone, the focus, the
beam is ½ as wide as at the transducer - At two near zone lengths from the transducer the
beam width is the same as the active element - At depths greater than two near zone lengths, the
beam is wider than the diameter of the active
element
9Focal Zone
- The region around the focus where the beam is
relatively narrow - Half of the focal zone is located within the near
field and half is located within the far field - Reflections arising within the focal zone create
images that are more accurate than those from
other depths
10Focal Depth Determination
- Fixed focus transducer focal depth is
determined by two characteristics of
the active element - Transducer diameter
- Frequency of the sound
(X) mm
(X) MHz
11Crystal Diameter vs. Focal Depth
- Focal depth is directly related to diameter2
- Larger diameter active element ? deeper focal
depth - Smaller diameter active element ? shallower focal
depth
12Transducer Frequency vs. Focal Depth
- Directly related
- Higher frequency transducer ? deeper focal depth
- Lower frequency transducer ? shallower focal depth
13Focal Depth (NZL) - Calculation
Multiply each side by 10-3
Round 6.16 ? 6.0
14NZL - Calculation
Calculate the NZL given an element diameter of 1
cm frequency of 5 MHz
Unmodified Equation
Modified Equation
15The Problem
- Given the physics, i.e., high frequency ? deep
focal depth - High frequency transducers are utilized to image
superficial structures - Therefore, high frequency transducers are
manufactured with very small diameter crystals to
shorten the focal depth
16Sound Beam Divergence
- Facts
- Sound beam diameter is smallest at the end of the
near zone - The sound beam diverges at depths greater than
the focus - Two transducer characteristics determine the
spread of the beam in the far field - Transducer diameter
- Frequency of the sound
17Transducer Diameter vs. Sound
Beam Divergence
- Crystal diameter beam divergence in the far
field - Inversely related
- Smaller crystals
- Greater beam divergence in the far field
- Larger crystals
- Less beam divergence in the far field
- Larger diameter crystals improve lateral
resolution in the far field due to less beam
divergence
Larger diameter crystals create less beam
divergence in the far field
18Frequency vs. Sound Beam Divergence
- Frequency beam divergence in the far field
- Inversely related
- Higher frequency
- Less beam divergence in the far field
- Higher frequencies have better lateral resolution
in the far field due to less beam divergence - Lower frequency
- Greater beam divergence in the far field
Higher frequency transducer creates less beam
divergence in the far field
19Whats Important
Factors affecting beam divergence in the far field
20Huygens Principle
- Large active elements may be thought of
as millions of tiny, distinct sound sources - Each of these sound sources creates a Huygens
wavelet with a V-shape - V-shaped waves are known as
- Spherical waves
- Diffraction patterns
- Huygens wavelets
21Spherical Waves
- Sound waves produced by very small sources
diverge in the shape of a V - The V-shaped wave is created when the source is
about the size of the sounds wavelength
22Huygens Principle Beam Shape
- Huygens wavelets interfere constructively
destructively - Explains beam shape based upon in-phase
out-of-phase wavelets interfering with each other - Constructive interference leads to hourglass
shaped main sound beam - Destructive interference occurs in areas where
the sound beam is absent
23Lateral Resolution
- The ability to identify two structures as two
distinct structures, which are close together
side-by-side, or perpendicular to the sound
beams main axis - In other words, what is the minimum distance that
two structures (reflectors) , positioned
side-by-side, can be apart and still produce two
distinct echoes on the image
24Lateral Resolution
- Units of distance
- mm, cm
- Smaller numbers are preferable, indicating more
accurate images - Determined by width of the sound beam
- Lateral resolution (mm) Beam diameter (mm)
- Narrower beams have better lateral resolution
- Beam diameter varies with depth, therefore,
lateral resolution changes with depth - Synonyms/Mnemonic LATA
- Lateral
- Angular
- Transverse
- Azimuthal
25Lateral Resolution vs. Focus
- Lateral resolution is best at the focus (end of
near zone) - Lateral resolution is good within the focal
zone
26Lateral Resolution vs. Beam Diameter
- Lateral resolution is best at the narrowest part
of the beam - When two structures are closer together than the
width of the beams diameter, only one reflection
will be seen on the image (suboptimal lateral
resolution at red arrows)
Seen on image
27Lateral vs. Axial Resolution
- In clinical imaging
- Axial resolution is superior to lateral
resolution due to pulses being shorter than
they are wide - Numerical value is less for axial resolution than
it is for lateral resolution - Higher frequencies improve both axial lateral
resolution - Improved axial resolution because of shorter
pulses - Improved lateral resolution because of less beam
divergence in the far field
28Focusing
- Improves lateral resolution by concentrating
sound energy into a narrower beam - Three methods
- External focusing with a lens
- Utilized with single element transducers
- Internal focusing with a curved active element
- Utilized with single element transducers
- Phased array focusing with the electronics of
the ultrasound system - Utilized with array, multiple element, transducers
29Focusing
- Fixed, internal external, focusing techniques
are also known as conventional or mechanical
focusing - With fixed focusing techniques, focusing cannot
be changed - Electronic focusing is adjustable
30External Focusing
- Fixed focusing technique
- Lens is placed in front of the piezoelectric
material - Increased prominence in the arc of the lens
increases the degree of focusing, narrowing the
beam in the focal zone
Active Element
Lens
31Internal Focusing
- Most common form of fixed focusing
- Curved piezoelectric crystal concentrates sound
energy into a narrower beam - As curvature becomes more pronounced, the degree
of focusing increases
Curved PZT crystal
32Phased (Electronic) Focusing
- Phased array means adjustable, or multiple
focusing - More versatile than fixed focusing techniques
- Electronics of the US system focus the sound beam
- Sonographer can alter the focusing
characteristics of the beam - Utilized only with multi-element transducers
33Effects of Focusing
- Four distinct alterations occur to the sound beam
- Beam diameter narrows in the near field and in
the focal zone - Focus is moved closer to the transducer, i.e.,
near field length (focal depth) is reduced - Beam diameter beyond the focal zone widens
- Improved lateral resolution in near focal zones
- Degraded lateral resolution beyond the focal zone
- Size of the focal zone is reduced
- Since the near field length is reduced, the focal
zone will also be reduced
34Summary of Beam Features