Page 272 - Biomedical Engineering and Design Handbook Volume 2, Applications
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250  DIAGNOSTIC EQUIPMENT DESIGN

                       receive processing used to create this beam is referred to as beam formation. Due to its central
                       role in ultrasonic imaging, beam formation will be discussed in detail later on.
                         The strength of the received echoes is usually displayed as increased brightness on the screen (hence
                       the name for the basic ultrasonic imaging mode, B-mode, with B for brightness). A two-dimensional data
                       set is acquired as the transmitted beam is steered or its point of origin is moved to different locations on
                       the transducer face. The data set that is acquired in this manner will have some set of orientations of the
                       acoustic rays. The process of interpolating this data set to form a TV raster image is usually referred to as
                       scan conversion. With Doppler signal processing, mean Doppler shifts (which correspond to velocities of
                       the scatterers such as red blood cells) at each position in the image can be determined from as few as 4 to
                       12 repeated transmissions. The magnitudes of these mean frequencies can be displayed in color superim-
                       posed on the B-mode image and can be used to show areas with significant blood flow.

           9.2.2 Physical Constants and Typical System Operating Parameters
                       It may be useful to consider typical system operating parameters. The following table lists some
                       physical constants that help define the operating parameters of today’s systems:
                         Typical attenuation in tissue  0.5 dB/cm ⋅ MHz for one-way travel
                         Speed of sound in tissue            1540 m/s (or roughly 13 μs/cm for round-trip travel)
                       One of the challenges of ultrasonic imaging relates to that very high attenuation. To put this in numerical
                       terms, a typical 5-MHz transducer is expected to penetrate approximately 10 cm. Thus, the signal leaving
                       the transmitting transducer will undergo attenuation in the order of 25 dB before it reaches a scattering
                       site. At that point, a small fraction of the energy will be reflected, let us say the reflected echo will be
                       another 30 dB down; and the return will bring about another 25 dB of attenuation. Thus, the entire atten-
                       uation has been about 80 dB. A typical ultrasound image will contain some 40 to 50 dB of dynamic range;
                       hence, needless to say, there is a strong need for careful low-noise designs for ultrasound front ends.
                         The following table gives some system design parameters commonly used for B-mode imaging:
                         Transducer frequencies           2–15 MHz
                         Transducer bandwidth            50–90% fractional bandwidth
                         Typical depths of penetration   18 cm (abdominal imaging)
                                                         16 cm (cardiac imaging)
                                                         5 cm (small parts and peripheral vascular imaging)
                         Time to acquire one 20-cm acoustic ray  ~260 μs
                         Pulse repetition frequency (PRF)  4 kHz
                         Typical number of rays in an image  128–400
                         Data acquisition frame rates    10–80 frames/s
                       Due to frequency-dependent attenuation, applications with greater penetration requirements use the
                       lower transducer frequencies. The instrument parameters have been selected or have evolved to their cur-
                       rent values as manufacturers have optimized their instruments to the needs of the various clinical appli-
                       cations. Given compromises that have to be made, resolution of scanners is been limited to roughly 0.4
                       mm with 7- to 12-MHz transducers to approximately 2 to 4 mm with the 2.5- to 3.5-MHz transducers.
                       The penetration at which these resolutions can be achieved is approximately 4 cm for the higher fre-
                       quencies and 15 cm or more for the lower frequencies. Whether or not this performance can be achieved
                       on any given patient is dependent on factors such as uniformity of speed of sound, which is highly patient
                       dependent (O’Donnell, 1988). The degree of and correction for sound speed variations in ultrasound sys-
                       tems continues to receive much attention (Fink, 1992; Flax, 1988; Li, 1995; Nock, 1988; O’Donnell,
                       1988; Trahey, 1988; Zhu, 1993a, 1993b; Krishnan, 1996; Rigby, 2000; Silverstein, 2001).
           9.2.3 Clinical Applications
                       B-mode imaging has found numerous uses in today’s clinic (Goldberg, 1990; Sarti, 1987). Some of
                       these are
                         Abdominal imaging  Identification of tumors, cysts in liver, kidneys
                         Cardiology        Valvular insufficiency (flail leaflet), myocardial dyskinesis,
                                           septal defects, congenital malformations
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