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a Chapter 2 Physical Principles of Doppler Ultrasonography 11<br />

T<br />

Amplitude<br />

Time<br />

Fig. 2.4. Period of sound. The duration of one wavelength<br />

of sound is its period. Horizontal axis represents the time<br />

and the vertical axis the magnitude of pressure wave deflections<br />

around the baseline<br />

±<br />

Fig. 2.7. Pressure amplitude of a sound wave. Horizontal<br />

axis depicts distance or time. Vertical axis represents variations<br />

in the acoustic pressure. The plus and minus signs indicate<br />

the positive and negative fluctuations of the pressure,<br />

respectively. P, the amplitude that is the maximum<br />

change in the pressure above or below the baseline value<br />

represented by the horizontal line<br />

Fig. 2.5. Concept of pulse repetition frequency (PRF). The<br />

illustration shows a PRF of 1 KHz (1,000 pulses per second)<br />

sound wave at a location is the rate of flow of energy<br />

per unit of cross-sectional area of the beam at that<br />

location. It is therefore power divided by beam crosssectional<br />

area. Pressure amplitude is measured using<br />

a device called a hydrophone. Intensity (I) is derived<br />

from the pressure amplitude (p) as they are directly<br />

related:<br />

I ˆ p 2 =c<br />

Fig. 2.6. Pulse length, which is the distance in space occupied<br />

by one ultrasound pulse. Horizontal axis represents<br />

the distance and the vertical axis the pressure amplitude<br />

For pulsed Doppler applications, the PFR limits the<br />

highest velocity that can be measured without creating<br />

the artifact known as aliasing. This subject is<br />

further discussed in Chap. 3.<br />

Amplitude, Power, Intensity<br />

The maximum variation in pressure generated in a<br />

medium by a propagating sound wave is called pressure<br />

amplitude (Fig. 2.7). Pressure amplitude is directly<br />

related to the amount of sound energy emanating<br />

from a vibratory source. It is therefore a measure<br />

of the strength of sound radiation. The rate of flow of<br />

ultrasonic energy through the cross-sectional area of<br />

the beam is expressed as its power. The intensity of a<br />

Intensity is expressed by several descriptor parameters<br />

based on its peak and average values.<br />

For continuous-wave Doppler ultrasound, intensity<br />

is measured as the spatial peak value (I sp ) and the<br />

spatial average value (I sa ). The former is measured<br />

usually at the focal point of the beam, the latter at<br />

the cross-sectional location of the beam. For pulsed<br />

Doppler ultrasound it is necessary to consider both<br />

the spatial and the temporal intensity values. Both<br />

peak and average values are measured in various<br />

combinations, as follows: spatial peak temporal peak<br />

(I sptp ), spatial peak temporal average (I spta ), spatial<br />

average temporal peak (I satp ), and spatial average<br />

temporal average (I sata ). Additional descriptors of<br />

pulsed ultrasound intensity include the spatial peak<br />

pulse average intensity (I sppa ), which is the intensity<br />

at the spatial peak averaged over the pulse length.<br />

These measures of sound energy of a transmitted<br />

Doppler ultrasound beam are important for biosafety<br />

considerations and are discussed in Chap. 6.<br />

Ultrasound and Piezoelectric Effect<br />

Audible sound frequency ranges from approximately<br />

10 Hz to 20 KHz. Sound with a frequency of more<br />

than 20 KHz is inaudible to the human ear and is

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