Pulsed-wave Doppler echocardiography

Pulsed-wave Doppler echocardiography uses timed ultrasound transmissions and returns to measure motion within a selected sampling region of the heart or nearby vessels. An echo's round-trip delay provides depth information, so a time window can select a location. The resulting Doppler spectrum describes a finite sample volume rather than an exact point.^[ref]

For sound speed $c$ and round-trip delay $t$, the ideal depth is $d=ct/2$. Avoiding ambiguity between successive pulses in a simple single-depth system requires waiting at least $2d/c$ before the next pulse. If $f_r$ is the pulse repetition frequency, this givesThe Doppler signal is sampled once per pulse, so unaliased shifts obey $|\Delta f|<f_r/2$. For aligned flow and transmitted frequency $f_0$,This is the pulsed Doppler depth-velocity tradeoff in the stated idealization. With $c=1540m/s$, $f_0=2.5\mathrm{MHz}$ and $d=0.10\mathrm{m}$, the highest ideal pulse rate is $7700\mathrm{Hz}$ and the corresponding speed limit is about $1.19m/s$. Doubling the depth halves both limits. Practical timing margins can reduce them further.

Aliasing is an ambiguity of the sampled signal, not proof that blood reverses direction. For example, sinusoidal Doppler shifts of $5000\mathrm{Hz}$ and $1000\mathrm{Hz}$ have identical complex samples at a $4000\mathrm{Hz}$ pulse rate, because their frequencies differ by exactly one sampling rate. The example concerns the Doppler signal, not direct sampling of the megahertz acoustic carrier.

High-pulse-rate variants can trade unique range localization for a larger velocity range. Continuous-wave Doppler echocardiography instead transmits and receives continuously, accepting depth ambiguity. The choice of acquisition method therefore changes what information the measured spectrum contains.^[ref]

The pulsed Doppler depth-velocity tradeoff is the restriction linking uniquely localized depth and unaliased beam velocity in a simple repeated-pulse Doppler ultrasound acquisition. Deeper echoes take longer to return, leaving fewer distinct pulse observations per second. Fewer observations reduce the unaliased Doppler ultrasound frequency interval.

For maximum depth $d$, speed of sound $c$ and pulse repetition frequency $f_r$, the ideal nonoverlapping timing restriction is $f_r\le c/(2d)$. The Nyquist frequency is $f_r/2$. Combining this with $f_D=2f_{0}v\cos \theta /c$ givesThe strict inequality excludes the ambiguous Nyquist endpoint. For beam-parallel motion, $|\cos \theta |=1$. At a right angle there is no first-order Doppler sensitivity to the motion; the apparent divergence of the formula does not provide unlimited useful velocity measurement.

For an original calculation, let $c=1540$ m/s and $f_0=2.5$ MHz. A 15 cm depth allows at most approximately 5133 pulses/s in this idealization, with axial Nyquist speed about 0.791 m/s. At 30 cm these bounds fall to approximately 2567 pulses/s and 0.395 m/s. Doubling the transmitted frequency to 5 MHz halves the axial velocity limits at either depth.

These are timing and sampling bounds, not a specification for a particular instrument. Pulse duration, scheduling and processing can lower the usable limit. Moving a spectral baseline changes the displayed signed interval but does not increase its total sampled-frequency width. Continuous-wave Doppler echocardiography avoids this pulse-rate restriction while sacrificing unique depth selection; high-pulse-rate acquisition instead accepts Doppler range ambiguity.^[ref] The acquisition choice determines which ambiguity remains.