Week 4 beam geometry
Ultrasound Beam
The ultrasound beam represents the area through which sound energy is emitted from the transducer.
The width of the beam changes with the distance from the transducer.
Intensity is not uniform across the beam.
The beam is three-dimensional and symmetrical around its axis.
Divided into:
Near Field (Fresnel Zone): Cylindrical shape.
Far Field (Fraunhofer Zone): Cone-shaped, diverging.
Factors Affecting Beam Shape
Frequency and Wavelength: Higher frequency leads to longer near field and reduced far field divergence.
Transducer Diameter (Aperture): Narrow crystals create narrower beams but shorter near fields; larger crystals result in wider beams with longer near fields.
Transducer Design: Causes alterations in beam shape; includes phased and linear arrays which enhance the number of focal zones.
Aperture size and beam shape
Aperture is the size of the source of ultrasound, a single crystal or group of crystals
Narrow crystal diameter (smaller aperture) results in a narrower beam in the near field but near field length is shorter and there is more divergence in the far field
Wider crystal diameter (larger aperture) results in a wider beam in the near field but produces a longer near-field length and has less divergence in the far field
Transducer design and beam shape
Phased and Linear arrays transduces can alter the beam shape by increasing the number of focal zones
Lenses focus because the propagation speed is higher than through tissues
Refraction at the surface of the lens forms the beam so that a focal region occurs (transducer B)
Crystal transducer also applies a degree of focusing to the beam (transducer A)
Focusing the Beam
Focusing brings the end of the near zone closer to the transducer face
Focusing can only be achieved in the near zone, where the beam is narrowest
Effects of focusing:
Reduces beam width in the focal zone, improves lateral resolution.
Focal length is the distance from the transducer to the focal center.
Mathematical Relationships
Beam width at the near zone's (focal length) end is approximately half of the transducer aperture
At the far zone, beam width is double the size of the beam in the focal point
The length of the focal zone is:
Inversely proportional to the wavelength
Directly proportional to the diameter of the crystal (D)
Directly proportional to the propagation speed ©
Has a square relationship with the aperture diameter
Formulae:
f = c{D^2}{c ƛ}
where f = focal length, D = transducer diameter, c = propagation speed, and ƛ = wavelength.
Beam Intensity
Intensity is measured as power (watts) per unit area.
Factors affecting intensity uniformity - intensity is not uniform throughout the length or width of the beam
Non-defined edges of the beam - intensity will decrease from the centre outward
Divergence of beam - intensity will be distributed over a larger area in the far field
Interference effects in the near field from the multiple points source of the crystals
Broadband transducer will show fewer interference effects and more uniformity due to its numerous frequency components
Reflection Strength: A small reflector at beam center (max intensity) yields stronger echo at the centre of the beam than on the periphery. This can lead to a false interpretation of the reflective properties of the tissue being examined, as the variability in echo strength may not accurately represent the underlying anatomy.
Further non-uniformity of intensity can be caused when the beam is focused to improve spatial resolution because a narrower beam will be within the focal zone
Intensity is greatest in the focal zone and therefore a stronger echo will be received from a given structure that lies within the focal zone
Side Lobes
Energy from the transducer radiates at various angles (side lobes), which can create artefacts in images.
3D and have the same frequency as the main beam
Any interfaces encountered by any of these side lobes will return echoes which the ultrasound machine assumes to have been received by the main beam
Grating Lobes
Arise from multi-crystal transducers (array transducers), can generate additional beams at various angles.
These lobes may lead to image artefacts and degrade lateral resolution due to the effective widening of the beam
Slice Thickness
Refers to the beam dimension at 90° to the scan plane.
Symmetrical beams have equal beam width and slice thickness at circular apertures.
Differences in rectangular apertures can lead to larger slice thickness than beam width, causing imaging artifacts.
Recap on Transducers
Common types:
Linear array
Convex array
Phased array
Vector array
Key features:
Beam scanning, focusing techniques, dimensions (rectangles, sectors).
Summary
Transducers produce sound beams with distinct near and far zones.
Various factors influence the beam's three-dimensional shape and its intensity uniformity.
Artifacts can arise from inherent beam characteristics such as side lobes, beam width, and slice thickness inconsistencies.
Further Readings
Links to additional resources for in-depth study on ultrasound beam characteristics and artifacts.