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Studies in vitro of the relationship between ultrasound and laser Doppler velocimetry and applicability to the simplified Bernoulli relationship.
Author(s) -
Lilliam M. ValdesCruz,
Ajit P. Yoganathan,
T. Tamura,
Frank M. Tomizuka,
YiRen Woo,
David J. Sahn
Publication year - 1986
Publication title -
circulation
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 7.795
H-Index - 607
eISSN - 1524-4539
pISSN - 0009-7322
DOI - 10.1161/01.cir.73.2.300
Subject(s) - doppler effect , laser doppler velocimetry , velocimetry , pulsatile flow , body orifice , ultrasound , doppler ultrasound , bernoulli's principle , flow measurement , acoustic doppler velocimetry , jet (fluid) , ultrasonic flow meter , flow velocity , medicine , pulse repetition frequency , transducer , flow (mathematics) , optics , biomedical engineering , acoustics , blood flow , mechanics , physics , surgery , radiology , anatomy , telecommunications , astronomy , radar , computer science , cardiology , thermodynamics
While there has been wide general acceptance of Doppler methods that use the simplified Bernoulii relationship to estimate pressure gradients across stenotic orifices, there is still ongoing controversy related to potential sources of error in the method. In this study we tested accuracy o ultrasound Doppler measurements of flow velocity when compared with the gold standard of laser light Doppler anemometry in a pulsatile flow model of pulmonic stenosis in vitro. We tested two commercially available Doppler systems and examined steered and nonsteered, parallel and off-axis and angle-corrected velocity determinations using continuous-wave and high-pulse repetition frequency (HPRF) methods. We also examined the potential range of error in the simplified Bernoulli method. One hundred and twenty individual flow states were examined with three stenotic valve orifices (3.0, 1.0, and 0.5 cm2 flow area) to measure velocities up to 620 cn/sec. A very high correlation coefficient was obtained for the comparison of laser Doppler anemometric and ultrasound velocity recordings by the nonsteered continuous-wave technique (r= .99, SEE = 17.9 cn/sec), but there was a tendency for underestimation of higher velocities when the transducer was positioned at 30 degrees and the ultrasound beam was steered so as to be parallel to the visualized flow jet (r = .98, SEE = 29.6 cn/sec). The HPRF ultrasound Doppler technique was also highly accurate in this optimized setting for measuring velocities (r = .99, SEE = 17 cm/sec), but also slightly underestimated the highest velocities. Our results also verified the accuracy of the simplified Bernoulli equation for converting instantaneous velocity measurements to estimated peak instantaneous gradient (r = .97, SEE = 8.4 mm Hg).

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