Abstract

m 2 ; RPA = 0.36±0.1N/m 2 ; LPA = 0.28±0.14N/m 2 . Figure 1 shows the average WSS-M calculated along the cardiac cycle for each segment. Figure 2 depicts Bland Altman plots of the mean WSS measured by the two observers, showing a small bias and standard deviations (mean difference of 0.016N/m 2 , 0.008N/m 2 and 0.005N/ m 2 for the WSS-M in the PA, RPA and LPA respectively). Conclusions In this work we proposed a novel and reproducible method to calculate WSS derived from 4D flow data in the main PA, RPA and LPA. In volunteers, we found a greater WSS in the RPA compared with the LPA, which is probably associated with more complex flow patterns (helices) in the RPA (2). Values of WSS obtained in patients showed increasing values of WSS, probably owe to complex and retrograde flow patterns in the pulmonary circulation.

Highlights

  • Quantification of Wall Shear Stress (WSS) from 4D flow data in the aorta has been recently reported (1)

  • Using a in-house code, three slices were reformatted perpendicular to the main PA, right pulmonary artery (RPA) and left pulmonary artery (LPA)

  • We segmented the blood pool, and calculated Magnitude (WSS-M), Axial (WSS-A), and Circumferential (WSS-C) WSS using a Strain Rate Tensor based on cylindrical coordinates

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Summary

Introduction

Quantification of Wall Shear Stress (WSS) from 4D flow data in the aorta has been recently reported (1). Methods 4D flow data of the whole heart (spatial resolution of 2.5m3, temporal resolution of 38ms) was acquired on 17 volunteers and 5 patients (1 repaired transposition of the great arteries, 2 after Glenn procedure and 2 with partial anomalous pulmonary vein return (1 patient with Atrial Septal Defect)).

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