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Chapter 2<br />

Physical Principles of Doppler Ultrasonography<br />

Dev Maulik<br />

This chapter presents the basic concepts of sound<br />

and ultrasound propagation and discusses the physical<br />

principles of the Doppler effect and Doppler<br />

sonography, which are essential for understanding<br />

their diagnostic uses. Although this book focuses primarily<br />

on clinical utilization of the diagnostic Doppler<br />

technology, developing an understanding of the<br />

basic principles is imperative for its proficient use.<br />

The following is a brief introduction and is not intended<br />

to be a comprehensive treatise on the subject.<br />

For a more in-depth discussion, there are several excellent<br />

textbooks that comprehensively examine the<br />

physics of Doppler ultrasonography [1±4].<br />

Propagation of Sound<br />

Sound is a form of mechanical energy that travels<br />

through solid or liquid media as pressure waves<br />

(Fig. 2.1). Sound waves are generated when an object<br />

vibrates in a medium. For example, percussion causes<br />

a drum membrane to vibrate and to generate sound<br />

waves in the air. During vibration the forward movement<br />

of the sound source causes a pressure rise in<br />

the adjacent medium, so the molecules of the medium<br />

become crowded. As the source moves backward<br />

there is a pressure drop in the medium, so the molecules<br />

now move apart. This phenomenon of alternating<br />

molecular compression and rarefaction accompanies<br />

the waves of sound energy as they propagate<br />

along the medium (Fig. 2.2). Although the molecules<br />

vibrate, they remain in their original location and are<br />

not displaced. Sound travels faster in solids than in<br />

liquids and faster in liquids than in gases.<br />

Although usually considered in a unidimensional<br />

plane, in reality sound is transmitted in a three-dimensional<br />

space. Sound waves from a vibratory<br />

source or from a reflector are moving surfaces of<br />

high and low pressures. These surfaces are called<br />

waveforms. The shape of a waveform depends on the<br />

shape of the source or the interface. Thus a plane<br />

waveform emanates from a flat source and a spherical<br />

waveform from a spherical source. With Doppler<br />

ultrasonics, the scattered waveform is spherical, as<br />

red blood cells (RBCs) behave as spherical sources<br />

during the scattering of an incident beam.<br />

Fig. 2.1 A, B. Propagation of sound. A Passage<br />

of a sound pulse through point ªAº in<br />

the medium. B Consequent changes in the<br />

pressure at that point

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