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Discover the EACVI Textbook of Echocardiography 2nd edition

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8<br />

Chapter 1 general principles of echocardiography<br />

result is a real-time image with higher spatial resolution due to a<br />

larger field of view, but even lower temporal resolution because of<br />

prolonged image formation time. To overcome this issue, a ‘full<br />

volume’ 3D data set is formed from stitching together subvolumes<br />

acquired over two to seven sequential cardiac cycles (usually<br />

four). This is a ‘near-real-time’ rather than a ‘real-time’ mode, but<br />

it allows higher line density with relatively high frame rate (still<br />

lower than the current 2D frame rate). ‘Full volume’ acquisition in<br />

one cardiac cycle is also available.<br />

Signal processing<br />

The transducer should receive all returning waves from an<br />

ultrasound pulse before generating a new pulse, to avoid range<br />

ambiguity artefact (confining waves returning late from one pulse<br />

in the same location with waves returning early from the next<br />

pulse). Consequently, the number of pulses per second—pulse<br />

repetition frequency (PRF)—depends on the maximum travelling<br />

time which depends on the imaging depth. For every scan line, the<br />

PRF determines the frame rate—the number of images generated<br />

per second and stored in memory. The higher the depth, the lower<br />

the PRF so the lower the frame rate. The higher the number of<br />

scan lines, the lower the frame rate. Higher imaging sector width<br />

needs more scan lines resulting in lower frame rate. The frame rate<br />

determines the temporal resolution.<br />

In current transducers, able to transmit and receive a range of<br />

frequencies, a different PRF corresponds to each frequency:<br />

◆ 5 MHz = >71.8 PRF<br />

◆ 4 MHz = >60.9 PRF<br />

◆ 3.3 MHz = >55.8 PRF.<br />

From the image stored in the memory an image display is created<br />

and presented. The number of images displayed per second<br />

defines the refresh rate which is smaller or equal to the frame rate.<br />

Both high frame rate and high refresh rate are needed for real-time<br />

imaging (rapid display of images during scanning, presenting the<br />

examined structures in motion).<br />

In older echocardiography machines, image display was performed<br />

in a cathode-ray tube and presented on a television screen<br />

or, later, on a computer monitor. The stored digital information<br />

was converted back to analogue voltages which induced a<br />

proportional strength electron beam generating a proportional<br />

brightness spot of light in the fluorescent tube. The spot moved<br />

across the tube creating the image display.<br />

In current echocardiography machines, both image display<br />

and presentation can be performed on a flat-panel consisting of a<br />

matrix of thousands of liquid crystal display (LCD) elements, acting<br />

as electrically activated light valves which can create grey-scale<br />

or colour images.<br />

Harmonic imaging<br />

Harmonic imaging substantially improves the image quality<br />

in 2D and M-mode. In non-harmonic imaging (fundamental<br />

imaging), the transducer receives only ultrasound signals from<br />

cardiac structures of the same frequency as that of the emitted<br />

ultrasound wave (fundamental frequency). In harmonic imaging,<br />

the transducer receives ultrasound signals from cardiac structures<br />

not only of fundamental frequency but also of higher frequency.<br />

The ultrasound wave produces compression and rarefaction of<br />

tissue particles (see % Fig. 1.1) and also oscillation of these particles<br />

both at fundamental frequency and at higher frequency and<br />

lower amplitude. These higher oscillation frequencies (harmonic<br />

frequencies) are exact multiples of the fundamental frequency. The<br />

harmonic amplitude is proportional with the square of the fundamental<br />

amplitude. Harmonic imaging exploits this non-linear<br />

response of tissue particles to the ultrasound beam.<br />

The generation of harmonic frequencies is a cumulative<br />

phenomenon, progressively augmenting with depth of tissue penetration.<br />

However, it results in a reduction of axial resolution of<br />

the ultrasound image.<br />

Harmonics generation increases with administration of contrast<br />

agents consisting of microbubbles with non-linear properties<br />

which suffer volume resonant oscillations with pressure variations<br />

(see % Chapter 8).<br />

Harmonic imaging places great demands on the transducer. It<br />

must be able both to generate low-frequency but high-amplitude<br />

ultrasound waves and to receive high-frequency but low-amplitude<br />

ultrasound waves. Broad bandwidth transducers have enabled the<br />

use of harmonic frequencies (% Fig. 1.8) resulting in significant<br />

image quality improvement (% Fig. 1.9a,b). The use of the second<br />

harmonic (twice the fundamental frequency) minimizes artefact.<br />

10<br />

5<br />

Fig. 1.8 Principle of harmonic imaging. The propagation of ultrasound in<br />

tissues is non-linear, faster during higher pressure because of higher media<br />

particles compression. This results in progressive wave-shape change because<br />

of added frequencies (harmonics) to the transducer-generated frequency<br />

(fundamental). The phenomenon is more accentuated with higher ultrasound<br />

intensity and at higher depth. Harmonic imaging is obtained by filtering<br />

out the returning fundamental frequencies and receiving only the second<br />

harmonic frequency.<br />

V

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