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a Chapter 6 Sonographic Color Flow Mapping: Basic Principles 79<br />

Fig. 6.10. Color Doppler Nyquist effect. The image shows<br />

Doppler color flow mapping of the left ventricular outflow.<br />

Note the change of color from red to yellow and then from<br />

bright blue to dark blue. With the declining velocity, blue<br />

changes first to yellow and then to red. LVOT left ventricular<br />

outflow tract<br />

Fig. 6.11. Doppler color flow depiction of change in the<br />

direction of flow. The image shows Doppler color mapping<br />

of flow through the ascending aorta (AA) and the arch of<br />

the aorta. In the ascending aorta the flow is toward the<br />

transducer and is therefore depicted as red according to<br />

the color bar setting. As the direction of flow changes, the<br />

color becomes blue with a dark line separating the two<br />

hues. LV left ventricle<br />

Fig. 6.9. Color Doppler Nyquist effect. The image shows<br />

Doppler color flow mapping of the left ventricular outflow.<br />

Note the change of color from red to yellow and then from<br />

bright blue to dark blue. With the declining velocity, blue<br />

changes first to yellow and then to red. LVOT left ventricular<br />

outflow tract<br />

is depicted in reversed color surrounded by the nonaliased<br />

flow (Fig. 6.9). This pattern mimics the color<br />

flow appearance of separate streams in differing directions.<br />

The two patterns, howerver, are clearly distinguishable.<br />

In an aliased flow, the higher velocity<br />

generates a higher Doppler shifted frequency, which<br />

is depicted with greater brightness: the higher the<br />

frequency shift, the brighter the color. The brightest<br />

level in the color calibration bar (the uppermost for<br />

the flow toward the transducer and lowermost for the<br />

flow away from the transducer) represents the Nyquist<br />

limit. As the velocity, and therefore the frequency<br />

shift, exceeds this limit, the color wraps<br />

around the calibration bar and appears at the other<br />

end as the most luminous color of the opposite direction<br />

(Fig. 6.10). For example, flow toward the transducer<br />

with an increasing velocity is depicted with an<br />

increasingly bright red color changing to yellow<br />

(Fig. 6.9). As the Nyquist limit is reached, the color<br />

flow shows brightest yellow in the color bar; and as<br />

the limit is exceeded, flow is shown in the brightest<br />

blue. Thus in an aliased flow, the bright or pale color<br />

of one direction is juxtaposed against the bright color<br />

of the opposite direction. In contrast, with genuine<br />

flow separation the distinct flow streams are depicted<br />

in the directionally appropriate colors separated by a<br />

dark margin (Fig. 6.11). Note that the hue that demarcates<br />

an aliased flow depends on the choice of the<br />

color mapping scheme.<br />

When demonstrating aliasing, an apparent contradiction<br />

may be seen between the spectral Doppler<br />

and the Doppler color flow interrogations. Doppler<br />

color flow mapping may show a nonaliased flow pattern<br />

when aliasing is observed with the spectral Doppler<br />

waveform. This phenomenon is explained by the<br />

fact that the mean frequency is less than the peak frequency,<br />

and Doppler color flow depiction is based on<br />

the use of mean frequency, so the Nyquist limit is not<br />

reached as readily as with the peak frequency depiction<br />

by the spectral Doppler method.<br />

Color Doppler aliasing can be eliminated by elevating<br />

the Nyquist limit, which can be achieved by<br />

either increasing the PRF or decreasing the transducer<br />

frequency. However, an increasing PRF may eventually<br />

result in such shortening of the interpulse in-

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