Cristian Montalba1, Julio Sotelo1,2, Jesús Urbina1,3, Marcelo Andia1,3, Cristian Tejos1,2, Pablo Irarrázaval1,2, Israel Valverde4,5, and Sergio Uribe1,3
1Biomedical Imaging Center, Pontificia Universidad Católica de Chile, Santiago, Chile, 2Electrical Engineering Department, Pontificia Universidad Católica de Chile, Santiago, Chile, 3Radiology Department, School of Medicine, Pontificia Universidad Católica de Chile, Santiago, Chile, 4Hospital Virgen del Rocio, Universidad de Sevilla, Seville, Spain, 5Institute of Biomedicine of Seville, Universidad de Sevilla, Seville, Spain
Synopsis
The purpose of this work was to study the
accuracy of the estimation of WSS calculated from 4D flow data acquired at
different spatial and temporal resolutions. The data was acquired using a
realistic thoracic aortic phantom in nine different hemodynamic conditions. We conclude that WSS measurements are more sensitive
to changes in spatial resolution than in temporal resolution.
Purpose
To assess the variability of wall shear stress
(WSS) as a function of 4D flow acquisition parameters. This assessment was done
with a realistic phantom because it is difficult to perform on volunteers or
patients. The acquisition of data sets is long (1), ranging from 5 to 30 minutes, so
applying several sequences with different spatial and temporal resolution will
lengthen the scanning time to more than 2 hours. Furthermore, by performing
this study on volunteers it would be difficult to isolate the impact of spatial
and temporal resolutions from other factors such as cardiac cycle variability
and respiratory motion. In this work, we used a realistic thoracic aortic
phantom to study the variability of WSS obtained from 4D flow data when
subjected to changes of spatial and temporal resolutions in nine different
hemodynamic conditions.Methods
The experiments were performed using a Philips MR scanner (Achieva 1.5T, Best, Netherlands) with a 4-element phased-array body coil. The phantom model (T-S-N-005, Elastrat Sarl, Geneva, Switzerland) was equipped with a pulsatile MR-compatible flow pump (Simutec, London, Ontario, Canada), with the same features as explained by Urbina et al (2) (Figure 1). We controlled the pump in terms of flow waveform, heart rate and cardiac output, which allowed us to study nine different hemodynamic conditions: heart rates (HR) of 68, 88 and 115 bpm, and each one with different maximum flow rates (MFR) of 200, 230 and 260 ml /s. For each hemodynamic condition, nine 4D flow sequences were acquired in the entire phantom with different combinations of spatial (from 1.04 to 2.08 mm) and temporal resolutions (from 20 to 60ms cardiac phase). In total, we acquired eighty-one sequences of 4D flow data. All the MR acquisition parameters are summarized in Table 1.
Mean WSS magnitude values were calculated for all 4D flow acquisitions. Since there is not a gold standard measurement for WSS, the 4D flow data with the highest combination of spatial and temporal resolution “HR20ms” (where the nomenclature: HR = highest spatial and 20ms =highest temporal resolution), was used for comparison. More nomenclature is shown in table 2. All 4D flow images were processed with a custom MatLab software toolbox. The quantification process included a semiautomatic segmentation of the aortic phantom and the generation of a tetrahedral finite element mesh, using the same method described previously by Sotelo et al (3). Different tetrahedral meshes were generated for each spatial resolution acquired.
We analyzed the WSS magnitude values in four different sections of the aorta (Figure 2). Bland-Altman plots were created to describe the agreement of WSS values between all 4D flow data and the “gold-standard” HR20ms. Also, Mann-Whitney U test was used to assess statistical differences of WSS magnitude. Differences with P<0.01 were considered significant. The statistical analyses were performed using GraphPad Prism v.6 for Mac (GraphPad Software, La Jolla, CA).
Results
Table 2 shows the
results of WSS magnitude
values for all sections of the aorta. Highest variability was found in
the acquisitions with low spatial resolution. We observed less differences when
the acquisitions were subjected to changes in temporal resolution. In general, the
results showed significant differences when comparing 4D flow data with HR20ms, except for the data
acquired with high spatial and medium temporal resolution HR40ms (where
the nomenclature: HR = highest spatial and 40ms = medium temporal resolution), no significant
differences were observed for this case (p = 0.027). On the other hand, in the
rest of acquisitions (shown in table 2) the results presented significant
differences (p= <0.0001). These findings were corroborated on Bland-Altman
analyses between 4D flow and HR20 (Figure 4). Discussion
In this study we
demonstrated the effect of changes in spatial and temporal resolution on WSS magnitude measurements
obtained from 4D flow acquisitions using a realistic aortic phantom. The WSS magnitude values were highly
sensitive to changes of spatial resolution and less sensitive to changes of
temporal resolution. The great advantage of this study is that we performed
controlled experiments, avoiding any cardiac variability and respiratory
motion. Statistical analysis demonstrated significant differences (p = 0.01)
between HR20ms and in the most of 4D flow acquisitions with different
combinations of spatial and temporal resolutions. Conclusion
Throughout
controlled experiment using an aortic phantom we demonstrated that WSS magnitude values were highly
sensitive to changes of spatial resolution and showed less variability when
data was acquired with different temporal resolution.Acknowledgements
Grant Sponsor:
Anillo ACT1416; Grant Sponsor: Fondo Nacional de Desarrollo Científico y
Tecnológico (FONDECYT), Ministerio de Educación, Chile. Grant Number: FONDECYT
#1141036.References
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