Background: Color M-mode (CMM) has been useful in characterizing left ventricular (LV) relaxation as well as providing information regarding right ventricular (RV) filling dynamics and pressure gradients. The spatiotemporal resolution of CMM offers a unique opportunity to study the effect of chronic pulmonary hypertension (cPH) on biventricular diastolic function.
Methods: Propagation velocities of LV and RV diastolic flows were obtained from 20 individuals with normal pulmonary artery systolic pressures, designated Group I (mean age 50 ± 12 years and 32 ± 6 mmHg) and from 30 patients with cPH, designated Group II (mean age 55 ± 14 years and 81 ± 25 mmHg).
Results: Group II patients not only had a significant difference between RV and LV onset of early (13 ± 55 vs. -223 ± 333 msec; P < 0.003) and late (-494 ± 467 vs. -125 ± 258 msec; P < 0.001) diastolic flows; but also had lower propagation velocities of the main RV (40 ± 10 vs. 28 ± 10 cm/sec; P < 0.0001) and LV (52 ± 11 vs. 37 ± 15 cm/sec; P < 0.0003) diastolic flows than Group I individuals.
Conclusions: It appears that cPH disrupts not only RV and LV diastolic signal distribution but also their temporal occurrence as well as reducing the propagation velocities of the main diastolic signals in both ventricles. These results seem to imply that cPH causes significant interventricular diastolic dyssynchrony and further studies are now needed to correlate these findings with regard to symptoms and patient clinical outcomes.
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http://dx.doi.org/10.1111/j.1540-8175.2011.01660.x | DOI Listing |
PLoS One
January 2025
Department of Mechanical Engineering, Carnegie Mellon University, Pittsburgh, PA, United States of America.
In this work, we propose a non-contact video-based approach that estimates an individual's blood pressure. The estimation of blood pressure is critical for monitoring hypertension and cardiovascular diseases such as coronary artery disease or stroke. Estimation of blood pressure is typically achieved using contact-based devices which apply pressure on the arm through a cuff.
View Article and Find Full Text PDFAbdom Radiol (NY)
January 2025
AGH University of Krakow, Krakow, Poland.
Purpose: Shear wave elastography (SWE) provides a means for adding information about the mechanical properties of tissues to a diagnostic ultrasound examination. It is important to understand the physics and methods by which the measurements are made to aid interpretation of the results as they relate to disease processes.
Methods: The components of how ultrasound is used to generate shear waves and make measurements of the induced motion are reviewed.
Phys Rev Lett
December 2024
University of Connecticut, University of Connecticut, School of Mechanical, Aerospace, and Manufacturing Engineering, Storrs, Connecticut 06269, USA and Institute of Materials Science, Storrs, Connecticut 06269, USA.
Flat lines within a band structure represent constant frequency bands for all momentum values (i.e., they maintain zero group velocity for all wave numbers).
View Article and Find Full Text PDFPhys Rev Lett
December 2024
Institut Langevin, ESPCI Paris, Université PSL, CNRS, 75005 Paris, France.
The interaction between waves and evolving media challenges traditional conservation laws. We experimentally investigate the behavior of elastic wave packets crossing a moving interface that separates two media with distinct propagation properties, observing the noninvariance of wavelength and frequency. Our experimental setup employs an elastic strip whose local stretching can be dynamically altered by pulling one end at a constant velocity.
View Article and Find Full Text PDFRev Sci Instrum
January 2025
Max-Planck-Institut für Plasmaphysik, Garching 85748, Germany.
This article presents an experimental setup capable of providing high spatial and temporal resolution measurements of neutral gas puff injection using a glow discharge to excite the neutral gas and an ultra-high-speed camera to record the emitted light. Using the proposed setup, the shape and propagation velocity of a thermal deuterium gas puff at 1 bar have been measured. The cloud has a conical shape and a propagation velocity of vprop = 1870 ± 270 m/s.
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