Abstract
4D PC MRI of the aorta has become a routinely available examination, and a multitude of single parameters have been suggested for the quantitative assessment of relevant flow features for clinical studies and diagnosis. However, clinically applicable assessment of complex flow patterns is still challenging. We present a concept for applying radiomics for the quantitative characterization of flow patterns in the aorta. To this end, we derive cross-sectional scalar parameter maps related to parameters suggested in literature such as throughflow, flow direction, vorticity, and normalized helicity. Derived radiomics features are selected with regard to their inter-scanner and inter-observer reproducibility, as well as their performance in the differentiation of sex-, age- and disease-related flow properties. The reproducible features were tested on user-selected examples with respect to their suitability for characterizing flow profile types. In future work, such signatures could be applied for quantitative flow assessment in clinical studies or disease phenotyping.
Keywords: Radiomics, 4D PC-MRI, flow profile, aortic valve stenosis, population, travelling volunteers, reproduciblity
1. Introduction
Four dimensional velocity encoded phase-contrast MRI (4D PC MRI) provides volumetric time-resolved velocity measurements in three spatial directions (1). Clinical interpretation of the highly complex information in the context of aortic diseases has been approached in several studies, which explored the association of flow patterns with pathologies of the aortic valve and vessel wall (2). In many studies, flow patterns were assessed qualitatively based on the inspection of vector visualizations, streamlines, and pathlines (3). Quantitative approaches for the assessment of local hemodynamics are measuring local properties of the velocity vector field in vessel segments or cross-sections (4–6). Helicity- and vorticity-based measures characterize local circulatory flow independent of orientation (7, 8). Other parameters provide information of flow properties with regard to the vascular anatomy. The normalized flow displacement and the angle have been established as measures of flow eccentricity (9–11). Schafstedde et al. (12) have introduced the wall parallelity degree (WPD), defined as the ratio between flow through the vessel cross-section and total flow, to quantify the part of blood flow parallel to the vessel centerline. These measurements use the cross-sectional vessel segmentation to derive the vessel center and the local vessel orientation. The wall shear stress (WSS) has been suggested for the assessment of the impact of flow phenomena on the vessel wall (11, 13). The calculation of this parameter requires the vessel surface points and the local orientation (surface normals) of the vessel wall (14). For the assessment of reflow phenomena, Rodriguez-Palomares et al. further considered the systolic flow reversal ratio (15). The quantitative flow profile analysis using the parameters mentioned above is typically based on aggregating the values per cross-section. We found only one publication which considered flow parameter texture: Garcia et al. reported significant differences in skewness and kurtosis of cross-sectional velocity distributions depending on age, sex and disease (16).
The reproducibility of conventional cross-sectional aortic flow quantification in 4D PC MRI with regard to acquisition, scanner, and observer interaction has been analyzed in previous publications. Morphometric parameters of cross-sections and vessel segments have been analyzed with excellent to good reproducibility for repeated scans, repeated analyses, and different observers in volunteers at a single scanner (17). The reproducibility of wall shear stress and velocity measurements was still moderate to good for systolic phases (18). The recent comparison of flow and wall shear stress measurements between acquisitions with scanners from different manufacturers showed considerable differences (19). The best agreement was found at the sinotubular junction.
Radiomics features have become popular for assessing morphology and tissue properties of anatomical structures (20). Shape characteristics are quantified through features such as area, elongation, and compactness, while co-occurrences and differences in neighboring voxel intensities allow the assessment of intensity patterns. The Image Biomarker Standardization Initiative (ISBI) has defined a set of radiomics features in such a way that implementing software packages now provide reproducible results (21). While radiomics features have been successfully used for phenotyping in oncology, their potential in the area of flow characterization has not yet been explored. As radiomics features depend on the underlying segmentation and the voxel intensity values, they offer a joint assessment of vessel shape and blood flow velocity in the proposed context of 4D PC MRI.
The purpose of this work is to evaluate a radiomics approach for the characterization of flow profiles to enable quantitative phenotyping. To this end, we analyze the reproducibility of radiomics features and study their applicability to the differentiation of normal and pathological flow profiles in the ascending aorta.
2. Materials and methods
We investigate radiomics shape features as well as texture features of scalar flow quantities, such as the through-plane flow, the angle between flow vector and cross-section normal, and normalized helicity and vorticity. We analyze the reproducibility of these features with respect to acquisition and observer. Furthermore, we use two age-matched cohorts to test whether the reproducible features are suitable for distinguishing different types of flow profiles. A flow chart of the proposed analyses is given in Figure 1
2.1. Data
Our analyses use data sets from three independent studies (Table 1). For the reproducibility assessment of the feature calculation, we consider eight healthy subjects from the travelling volunteer study presented by Demir et al. (19). Each volunteer was scanned on Philips (Ingenia 3T), Siemens (Prisma Fit) and GE (SIGNA Architect 3T) systems with the scan parameters as summarized in Table 1.
Table 1.
Travelling volunteers | Aortic stenosis patients | Population study | |||
---|---|---|---|---|---|
Subjects | 8 | 57 | 132 | ||
Age (years) | |||||
Weight (kg) | |||||
Female | 6 (75%) | 22 (42%) | 68 (52%) | ||
Scanner | Philips Ingenia | Siemens Prisma Fit | GE SIGNA Architect | Philips Achieva | Siemens TrioTim |
Field Strength | 3T | 3T | 3T | 1.5 T | 3T |
Velocity Enc. (cm/s) | 250 | 150 | 150 | 350–600 | 150 |
ECG gating | Retrospective | Prospective | Retrospective | Retrospective | Prospective |
Repetition time (ms) | 3.5 | 5.1 | 4.2 | 3.5 | 5 |
Echo time (ms) | 2.2 | 2.6 | 2.00 | 2.2 | 2.54 |
Flip angle () | 5 | 8 | 8 | 7 | 7 |
Voxel size (mm) | |||||
Timeframes/cycle | 25.00 | 20.00 | 25.00 | ||
Temp. res. (ms) | 28.00 | 40.8 | 66.8 | 38 | 20 |
Heart rate (bpm) |
The applicability of radiomics analysis to characterize flow profiles is tested with data from two additional independent studies. A dataset of patients with aortic stenosis (22) represents a cohort of pathological cases, while a dataset from a population study in the city of Freiburg, Germany (23) serves as control. We were able to include six additional cases in the latter dataset, which could not be analyzed in the initial study. None of the control subjects were diagnosed with valve diseases.
2.2. Image analysis and flow profile assessment
4D flow MR images are analyzed using MEVISFlow. Preprocessing includes background phase offset correction with a polynomial fit and phase unwrapping with the PRELUDE algorithm. The aortic centerline is calculated via skeletonization of the 3D aorta segmentation in the phase contrast magnetic resonance angiography. To achieve comparability, cross-sections are placed according to the definition in Schafstedde et al. (12) (Figure 2). Observers position four cross-sections along the course of the aorta: distal to the coronary ostia (A1.1), proximal to the branch of the brachiocephalic trunc (B1), behind the subclavian artery (B4.1), and next to the pulmonary artery (D1.1). Additional cross-sections are placed automatically with equidistant spacing within the ascending and descending aorta segments. Cross-sectional region of interest (ROI) are segmented manually by the observer. For each cross-section, the ROI is transferred to all time frames of the image sequence by automatic motion tracking using the morphon algorithm (24). The cross-section-based multiplanar reconstructions are resampled to a voxel resolution of 1 mm using trilinear interpolation. For the radiomics analysis, parameter maps are calculated per cross-section and image timepoint (see Figure 2). For the throughflow map, the scalar product of the velocity vector and the normal of cross-sectional plane is calculated for each voxel (Equation 1).
(1) |
For the wall parallelity degree (WPD) map, the throughflow magnitude is divided by the total flow magnitude (Equation 2).
(2) |
The angle is defined as the angular deviation of the velocity vector from the plane normal (Equation 3).
(3) |
Throughflow, wall parallelity degree and angle assess aspects of the flow orientation in relation to the aortic anatomy, which is represented by the orientation and outer contour of the aortic cross-section. The vorticity is defined as the curl of the velocity vector field (equation 4).
(4) |
The absolute local normalized helicity (LNH) is the normalized dot product of the vorticity and the velocity vector .
(5) |
These parameters describe local flow properties derived from the voxel neighborhood without considering the anatomy.
Unsigned parameters are normalized to the interval , signed parameters to . The parameter-specific details are shown in Table 2. For each of the five parameter maps, 79 first- and higher-order radiomics features were extracted using the pyradiomics library.1 We use the standard fixed bin size suggested by pyradiomics for discretization. With additional 2D shape features, a total of 411 features are extracted on each plane for each measured timeframe. The temporal evolution of each feature throughout the cardiac cycle can be visualized as a feature curve (example in Figure 2).
Table 2.
Throughflow (m/s) | Angle () | Wall parallelity degree | N-Helicity | Vorticity | |
---|---|---|---|---|---|
WPD | LNH | ||||
Input range | |||||
Output range |
For inter-scanner reproducibility assessment, cross-sections from all aortic segments and cardiac phases are considered. To allow comparison at the highest temporal resolution, the feature curves of sequences with lower temporal resolution are upsampled with linear interpolation. For the inter-observer reproducibility assessment, a second observer processed the eight volunteer datasets acquired with scanner one. For the assessment of the inter-observer and inter-scanner agreement, we calculate the intra-class correlation coefficient (ICC). As suggested in (25), is interpreted as poor, ICC 0.5–0.75 as moderate, 0.75–0.9 as good, and an as excellent reproducibility. The features with moderate or better inter-scanner and inter-observer ICC are selected for the application tests.
test the applicability of the suggested flow profile characterization, we compare the feature curves of the first ascending aorta plane (A1.1) obtained in the aortic stenosis patients (cohort 2) to those from subjects of the population study without valve disease (cohort 3). We use the set of features found to be reproducible, which describe the distribution patterns of flow directions, contour shape and mobility, as well as features describing the patterns of vorticity and normalized helicity. Subjects are stratified by sex and age group (Group 1: [20–39] years, Group 2: [40–59] years, Group 3: [60–80] years). As for the reproducibility assessment, the feature curves of the sequences acquired with a lower temporal resolution are upsampled to match the sampling of the sequence with the highest temporal resolution. The suitability for disease classification is tested with a logistic regression model trained with the selected radiomics feature set to distinguish between aortic stenosis and no valve disease. Finally, we explore the systolic radiomics signatures of the different datasets and examine representative flow profiles.
3. Results
All datasets were successfully processed and considered in the radiomics feature evaluation as displayed in Figure 1.
3.1. Reproducibility of radiomics features of flow profiles
3.1.1. Inter-observer reproducibility
The ICC values showed an excellent inter-observer agreement in most features (Excellent: 283, Good: 84, Moderate: 39, Poor: 5, see Table 3), provides an overview of the features for the different parameter maps. Detailed information on the ICC values per feature are given in the supplementary material.
Table 3.
Parameter map | Throughflow | WPD | Angle | N-Helicity | Vorticity | Shape |
---|---|---|---|---|---|---|
Excellent | 53 | 65 | 65 | 42 | 47 | 11 |
Good | 20 | 13 | 12 | 17 | 21 | 1 |
Moderate | 3 | 1 | 2 | 19 | 11 | 3 |
Poor | 3 | 0 | 0 | 1 | 0 | 1 |
Total features | 79 | 79 | 79 | 79 | 79 | 16 |
3.1.2. Inter-scanner reproducibility
The ICC values for the inter-scanner agreement are moderate for 51 features and poor for the other 360 features (Table 4). Table 5 shows the top 5 features with moderate agreement per parameter map. Detailed information on the ICC values are given in the supplement.
Table 4.
Parameter map | Throughflow | WPD | Angle | N-Helicity | Vorticity | Shape |
---|---|---|---|---|---|---|
Excellent | 0 | 0 | 0 | 0 | 0 | 0 |
Good | 0 | 0 | 0 | 0 | 0 | 0 |
Moderate | 1 | 4 | 26 | 4 | 5 | 11 |
Poor | 78 | 75 | 53 | 75 | 74 | 5 |
Total features | 79 | 79 | 79 | 79 | 79 | 16 |
Table 5.
Throughflow | WPD | Angle | N-Helicity | Vorticity | Shape |
---|---|---|---|---|---|
Gray level non-uniformity (GLRLM) | Inverse variance (GLCM) | Zone percentage (GLSZM) | Run length non-uniformity (GLRLM) | Dependence non-uniformity (GLDM) | Perimeter |
Dependence non-uniformity (GLDM) | Inverse difference normalized (GLCM) | Size zone non-uniformity (GLSZM) | Gray level non-uniformity (GLRLM) | Maximum diameter | |
Size zone non-uniformity (GLSZM) | Size-zone non-uniformity (GLSZM) | Dependence non-uniformity (GLDM) | Run entropy (GLRLM) | Major axis length | |
Inverse difference (GLCM) | Dependence non-uniformity (GLDM) | Dependence entropy (GLDM) | Coarseness (NGTDM) | Perimeter to surface ratio | |
IDM (GLCM) | Inverse difference (GLCM) | 90th percentile (first-order) | Area |
For the throughflow parameter maps, only the Gray Level Non-Uniformity derived from the Gray Level Run Length Matrix showed moderate agreement between the different scanners. This feature quantifies the similarity of throughflow values and is thus independent of minor differences in the absolute values. Except for 90th percentile of the vorticity values, only higher-order features showed moderate agreement for the parameter map analysis.
Dependence Non-Uniformity derived from the Gray Level Dependency Matrix (GLDM) showed moderate agreement for all maps except for throughflow. The Gray Level Dependence Matrix counts the number of occurrences of homogeneous regions with certain sizes. The Dependence Non-Uniformity measures the similarity of dependence, and a low value means fewer zones, indicating larger homogeneous regions. The last row in Figure 6 shows example vorticity maps and corresponding feature maps for three different cases in a systolic timeframe. Vorticity differences result in higher values while the values are low in homogeneous regions. Features such as the Inverse Variance and the Inverse Difference describe the local homogeneity of the parameter values based on the co-occurrence of neighboring parameter values (GLCM). The second row in Figure 6 shows the Inverse Variance feature for WPD maps. The examples show that the feature values are high where the change in the wall parallelity degree is low. If the Inverse Variance and Inverse Difference values of the throughflow-related parameter values (WPD, Angle) are high, the flow profile is smooth with continuous changes in all neighborhoods. The Gray Level Size Zone Matrix (GLSZM) contains the numbers of connected regions with homogeneous values. The Size Zone-Non-Uniformity measures the variability of size zone volumes and is low in the case of homogeneity. The Zone Percentage measures the coarseness and as displayed in row 3 of Figure 6, a high value indicates many regional changes. If the Zone Percentage is high for the throughflow-related parameters, the flow profile is rough or bumpy. For the vorticity map, parameters describing the heterogeneity of the texture patterns (Run Entropy) via the Gray Level Run Length Matrix (GLRLM) and the Coarseness defined via the parameter deviation from a neighbourhood average (derived from the Neighbouring Gray Tone Difference Matrix (NGTDM)) also show moderate agreement. The Gray Level Run Length Matrices contain the numbers of voxels with similar parameter values per direction. These matrices are then combined. The derived Non-Uniformity features show high values for irregular patterns. For the helicity and vorticity maps this could indicate turbulent flow or noise-affected vector fields. The Neighbouring Gray Tone Difference Matrix quantifies the difference between a value and the average value of its neighbours within a certain distance. A high Coarseness value derived from the NGTDM indicates strong value differences in the defined neighborhood. High values of this feature for the normalized helicity or vorticity indicate small turbulences or noise-affected vector fields.
3.2. Application to different age, sex and disease groups
We selected the features with at least moderate reproducibility with regard to ICC values to test whether they can be used to characterize flow profile differences between age groups and between normal and pathological cases. For an age-matched comparison, the second and third cohorts were separated into three groups (Group 1: [20–39], Group 2: [40–59], Group 3: [60–80]) as defined in (26). and age group feature curves for cohort 3, as well as the age group feature curves for cohort 2 are displayed in Figure 3. On average, the observed cross-sectional area was smaller in women, and there are observable differences in the normalized helicity and vorticity patterns. Age-related trends can be observed in cohort 3 with no valve disease. Age-related differences are less pronounced in aortic stenosis patients. Figure 4 shows the average, minimum and maximum values of features related to the flow direction, shape and motion, as well as vorticity and normalized helicity for the datasets of age groups 2 and 3 in cohorts 2 and 3. The curves of the different cohorts differ in value ranges and curve shapes for both age groups. Shape and motion-related features vary more in age group 2.
The logistic regression model trained on the 51 selected features extracted on the systolic feature maps on plane A1.1 achieves an accuracy and F1-value of 1.0 in the differentiation of cases with aortic stenosis and no valve disease. The confusion matrix and the feature importance analysis are displayed in Figure 5. The features found most important for the classification describe the texture patterns of flow angle, normalized helicity and wall parallelity degree.
To test if radiomics signatures can be used to quantitatively describe flow profiles, we examine three cases, which are visually different to a human observer. Figure 6 shows three cases with different flow profiles caused by aortic stenosis (cohort 2) in comparison to a normal subject from cohort 3. The observable differences in the 3D vector visualization of the systolic cross-sectional flow result in clearly distinguishable feature distributions.
The corresponding quantitative values of the radiomics features can be found in the supplementary material. A parallel coordinate plot visualization is shown in Figure 7. To provide an intuitive overview, we kept only at least moderately reproducible features, with visually different values for the selected patients. The patients are represented by lines in the plot. Cohort 2 (aortic valve stenosis) is represented by orange lines, blue lines represent cohort 3 (no valve disease). The colored lines display the selected cases with distinctly different flow profiles. The visualization reveals several features with no or little overlap between cohort 2 and 3 based on the distribution of the parameters wall parallelity degree (WPD), the flow angle, and the normalized helicity. The different flow profiles show individual feature combinations represented by different line patterns in the parallel coordinate plot.
4. Discussion
While the inter-observer agreement of radiomics features was excellent for 283 features, the inter-scanner agreement was only moderate in the best cases. Amongst these, only one feature was derived from the throughflow velocity map. This is in line with the findings by Demir et al., who found considerable differences in the velocity magnitudes measured with the different scanners (19). For wall parallelity degree, normalized helicity, and vorticity only higher-order features showed moderate agreement. For the direction-based angle map, which is independent of the velocity magnitude, the number of moderately reproducible features was considerably higher. Previous studies showed that spatial resolution and signal-to-noise ratio, slice thickness and field strength (27–30) have an impact on radiomics parameters. Especially in the context of 4D PC MRI, the selection of the velocity encoding can have an influence on the radiomics features. One example of a case in a healthy female volunteer scanned with different velocity encodings and thus in velocity-to-noise ratio is presented in the Figure S13 in the supplement.
In accordance with previous studies, we found sex and age-related differences in the aortic cross-sections (16, 31), which were also reflected in the radiomics features. These were accompanied by age-related differences in the patterns of flow directions, normalized helicity and vorticity, which were observed in patients with aortic valve stenoses as well. As shown in Figure 4, the average values of all features differed between subjects with and without aortic stenosis. This is in accordance with previous studies using parameters such as angle and normalized velocity to identify pathological flow patterns in patients with bicuspid aortic valves (32).
The classification test using the features with moderate reproducibility to distinguish between normal valves and aortic valve stenosis based on the systolic parameter maps of cross-section A1.1 in the ascending aorta (see Figure 6) show perfect results as shown in Figure 5. From the 51 features considered for the training of the classifier, the ones which describe homogeneity, and properties of homogeneous regions in the parameter maps of angle, normalized helicity and WPD were considered most important. Shape features had no significant influence. The underlying parameters have been suggested in previous publications (5, 16, 32). The standardized analysis of their distribution patterns however enable a more robust consideration of disease recognition.
In the assessment of different types of systolic flow profiles in the ascending aorta, the radiomics signatures showed different value ranges than the cohort without valve disease. Furthermore, there were clear differences in the wall parallelity degree features and angle patterns. It might therefore be possible to use radiomics signatures of flow for 4D PC MRI-based phenotyping in future studies. The explainability of the origin of the radiomics features allows for an advanced exploration of properties of detected phenotypes. Figure 6 links the radiomics signatures from the parallel coordinate plot in Figure 7 to the underlying feature and parameter maps as well as to the 3D position and flow visualization. The differences in the Gray Level Non Uniformity of the throughflow and the WPD maps clearly differentiate the compact jets from the other flow patterns. The Inverse Variance of the WPD map and the Zone Percentage of the Angle map order the flow profiles according to the amount of local differences in flow direction. The Non Uniformity features of N-Helicity maps separate the types of jets. Figure 6 shows the systolic N-Helicity maps for normal flow and two different jets. The maps differ in size of homogeneous regions, and the map with the smaller connected regions, which corresponds to a coarser flow profile, has a higher Non Uniformity feature value. The vorticity maps in Figure 6 display distribution patterns, which are relatively similar to those of the H-Helicity map, but the GLDM-based Dependence Non-Uniformity results provides a different order of jet types. The Coarseness feature based on the NGTDM separates the angulated and vortex flow from directed flow.
With recent developments in deep learning-based segmentation, the presented processing pipeline could be integrated into automatized and standardized analysis workflows to further seamlessly support image-based diagnostics and decision-making in clinical applications.
4.1. Limitations
Inter-observer analysis was only performed on a small number of healthy volunteers, and intra-observer and scan-rescan reproducibility was not assessed. However, based on the results of previous publications (17, 19), we assume that the radiomics feature agreement would be better than the inter-scanner results. The influence of different velocity encodings and thereby different VNR values could be further explored in future work. The datasets of cohorts 2 and 3 were acquired with different scanners, protocols and sequences than those represented in the Travelling colunteers study. While the spatial resolution was comparable in cohorts 2 and 3 to the Travelling-Volunteers-study, the temporal resolution was substantially higher in cohort 3. Furthermore, the velocity encoding in aortic stenosis patients with 350–600 cm/s was higher than 150–250 cm/s in the volunteer datasets. Due to the changes in the scan parameters we cannot be certain that the agreement of the derived radiomics features is comparable.
4.2. Conclusions and outlook
We introduced a concept for the calculation of radiomics signatures in order to quantitatively characterize flow profiles in the aorta. Radiomics features were selected based on their inter-scanner and inter-observer reproducibility and tested for the assessment of sex-, age- and disease-specific differences. We applied selected features to user-defined types of aortic flow profiles. The differences in the corresponding radiomics signatures suggest their utility in PC-MRI-based phenotyping and quantification of disease-related changes. With the new concept radiomics features could be used for an automatic assessment and comparable quantitiative description of hemodynamics properties, which mimics human visual analysis. This could enable the application in clinical studies as well as the definition of decision relevant radiomics signature ranges.
Funding Statement
This work was partially funded by the BMBF project “Berlin Institute for the Foundations of Learning and Data” (grant number 01IS18037E) and by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) - SFB-1470 - B06. AH received funding from Berta-Ottenstein-Programme for Advanced Clinician Scientists, Medical Faculty, University of Freiburg, Germany. We acknowledge financial support from the Open Access Publication Fund of Charité – Universitätsmedizin Berlin and the German Research Foundation (DFG).
Footnotes
Data availability statement
The datasets generated and analyzed during the current study are not publicly available but are available from the corresponding author on reasonable request.
Ethics statement
The studies involving human participants were reviewed and approved by Ethikkommission der Charité - Universitätsmedizin Berlin Ethik-Kommission der Albert-Ludwigs-Universität Freiburg. The patients/participants provided their written informed consent to participate in this study.
Author contributions
AHe, MH: conceptualization. AHa, JSM, SK, SN, JH: data collection and curation. LJ, AHe, MH, CM, AL: data processing. MH, AHe, MI, CM: methodology. MH, AHe: writing-original draft. All: writing-review and editing. All authors contributed to the article and approved the submitted version.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Publisher's note
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
Supplementary material
The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/fcvm.2023.1102502/full#supplementary-material.
References
- 1.Markl M, Frydrychowicz A, Kozerke S, Hope M, Wieben O. 4D flow MRI. J Magn Reson Imaging. (2012) 36:1015–36. 10.1002/jmri.23632 [DOI] [PubMed] [Google Scholar]
- 2.Takahashi K, Sekine T, Ando T, Ishii Y, Kumita S. Utility of 4D flow MRI in thoracic aortic diseases: a literature review of clinical applications, current evidence. Magn Reson Med Sci. (2022) 21:327–39. 10.2463/mrms.rev.2021-0046 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 3.Catapano F, Pambianchi G, Cundari G, Rebelo J, Cilia F, Carbone I, et al. 4D flow imaging of the thoracic aorta: is there an added clinical value? Cardiovasc Diagn Ther. (2020) 10:1068–89. 10.21037/cdt-20-452 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 4.von Spiczak J, Crelier G, Giese D, Kozerke S, Maintz D, Bunck AC. Quantitative analysis of vortical blood flow in the thoracic aorta using 4D phase contrast MRI. PLoS ONE. (2015) 10:e0139025. 10.1371/journal.pone.0139025 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 5.Sigovan M, Dyverfeldt P, Wrenn J, Tseng EE, Saloner D, Hope MD. Extended 3D approach for quantification of abnormal ascending aortic flow. Magn Reson Imaging. (2015) 33:695–700. 10.1016/j.mri.2015.02.020 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 6.Ha H, Kim GB, Kweon J, Lee SJ, Kim YH, Kim N, et al. The influence of the aortic valve angle on the hemodynamic features of the thoracic aorta. Sci Rep. (2016) 6:32316. 10.1038/srep32316 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 7.Bissell MM, Hess AT, Biasiolli L, Glaze SJ, Loudon M, Pitcher A, et al. Aortic dilation in bicuspid aortic valve disease: flow pattern is a major contributor, differs with valve fusion type. Circ Cardiovasc Imaging. (2013) 6:499–507. 10.1161/CIRCIMAGING.113.000528 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 8.Trauzeddel RF, Lobe U, Barker AJ, Gelsinger C, Butter C, Markl M, et al. Blood flow characteristics in the ascending aorta after TAVI compared to surgical aortic valve replacement. Int J Cardiovasc Imaging. (2016) 32:461–7. 10.1007/s10554-015-0792-x [DOI] [PMC free article] [PubMed] [Google Scholar]
- 9.Hope MD, Sigovan M, Wrenn SJ, Saloner D, Dyverfeldt P. MRI hemodynamic markers of progressive bicuspid aortic valve-related aortic disease. J Magn Reson Imaging. (2014) 40:140–5. 10.1002/jmri.24362 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 10.Sigovan M, Hope MD, Dyverfeldt P, Saloner D. Comparison of four-dimensional flow parameters for quantification of flow eccentricity in the ascending aorta. J Magn Reson Imaging. (2011) 34:1226–30. 10.1002/jmri.22800 [DOI] [PubMed] [Google Scholar]
- 11.Mahadevia R, Barker AJ, Schnell S, Entezari P, Kansal P, Fedak PW, et al. Bicuspid aortic cusp fusion morphology alters aortic three-dimensional outflow patterns, wall shear stress, and expression of aortopathy. Circulation. (2014) 129:673–82. 10.1161/CIRCULATIONAHA.113.003026 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 12.Schafstedde M, Jarmatz L, Brüning J, Hüllebrandt M, Nordmeyer S, Harloff A, et al. Population-based reference values for 4D flow MRI derived aortic blood flow parameters. Physiol Meas. (2023). [DOI] [PubMed]
- 13.Kauhanen SP, Hedman M, Kariniemi E, Jaakkola P, Vanninen R, Saari P, et al. Aortic dilatation associates with flow displacement and increased circumferential wall shear stress in patients without aortic stenosis: a prospective clinical study. J Magn Reson Imaging. (2019) 50:136–45. 10.1002/jmri.26655 [DOI] [PubMed] [Google Scholar]
- 14.Zimmermann J, Demedts D, Mirzaee H, Ewert P, Stern H, Meierhofer C, et al. Wall shear stress estimation in the aorta: impact of wall motion, spatiotemporal resolution, and phase noise. J Magn Reson Imaging. (2018) 48:718–28. 10.1002/jmri.26007 [DOI] [PubMed] [Google Scholar]
- 15.Rodriguez-Palomares JF, Dux-Santoy L, Guala A, Kale R, Maldonado G, Teixido-Tura G, et al. Aortic flow patterns and wall shear stress maps by 4D-flow cardiovascular magnetic resonance in the assessment of aortic dilatation in bicuspid aortic valve disease. J Cardiovasc Magn Reson. (2018) 20:28. 10.1186/s12968-018-0451-1 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 16.Garcia J, van der Palen RLF, Bollache E, Jarvis K, Rose MJ, Barker AJ, et al. Distribution of blood flow velocity in the normal aorta: effect of age and gender. J Magn Reson Imaging. (2018) 47:487–98. 10.1002/jmri.25773 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 17.Juffermans JF, Westenberg JJM, van den Boogaard PJ, Roest AAW, van Assen HC, van der Palen RLF, et al. Reproducibility of aorta segmentation on 4D flow MRI in healthy volunteers. J Magn Reson Imaging. (2021) 53:1268–79. 10.1002/jmri.27431 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 18.van Ooij P, Powell AL, Potters WV, Carr JC, Markl M, Barker AJ. Reproducibility, interobserver variability of systolic blood flow velocity, 3D wall shear stress derived from 4D flow MRI in the healthy aorta. J Magn Reson Imaging. (2016) 43:236–48. 10.1002/jmri.24959 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 19.Demir A, Wiesemann S, Erley J, Schmitter S, Trauzeddel RF, Pieske B, et al. Traveling volunteers: a multi-vendor, multi-center study on reproducibility and comparability of 4D flow derived aortic hemodynamics in cardiovascular magnetic resonance. J Magn Reson Imaging. (2022) 55:211–22. 10.1002/jmri.27804 [DOI] [PubMed] [Google Scholar]
- 20.van Griethuysen JJM, Fedorov A, Parmar C, Hosny A, Aucoin N, Narayan V, et al. Computational radiomics system to decode the radiographic phenotype. Cancer Res. (2017) 77:e104–7. 10.1158/0008-5472.CAN-17-0339 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 21.Zwanenburg A, Vallieres M, Abdalah MA, Aerts H, Andrearczyk V, Apte A, et al. The image biomarker standardization initiative: Standardized quantitative radiomics for high-throughput image-based phenotyping. Radiology. (2020) 295:328–38. 10.1148/radiol.2020191145 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 22.Nordmeyer S, Hellmeier F, Yevtushenko P, Kelm M, Lee CB, Lehmann D, et al. Abnormal aortic flow profiles persist after aortic valve replacement in the majority of patients with aortic valve disease: how model-based personalized therapy planning could improve results. A pilot study approach. Eur J Cardiothorac Surg. (2020) 57:133–41. 10.1093/ejcts/ezz149 [DOI] [PubMed] [Google Scholar]
- 23.Harloff A, Mirzaee H, Lodemann T, Hagenlocher P, Wehrum T, Stuplich J, et al. Determination of aortic stiffness using 4D flow cardiovascular magnetic resonance—a population-based study. J Cardiovasc Magn Reson. (2018) 20:43. 10.1186/s12968-018-0461-z [DOI] [PMC free article] [PubMed] [Google Scholar]
- 24.Tautz L, Hennemuth A, Peitgen H-O. Motion analysis with quadrature filter based registration of tagged MRI sequences. In: Camara O, Konukoglu E, Pop M, Rhode K, Sermesant M, Young A, editors. Statistical atlases and computational models of the heart. Imaging and modelling challenges. Springer Berlin Heidelberg (2012). p. 78–87.
- 25.Koo TK, Li MY. A guideline of selecting and reporting intraclass correlation coefficients for reliability research. J Chiropr Med. (2016) 15:155–63. 10.1016/j.jcm.2016.02.012 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 26.Harloff A, Hagenlocher P, Lodemann T, Hennemuth A, Weiller C, Hennig J, et al. Retrograde aortic blood flow as a mechanism of stroke: MR evaluation of the prevalence in a population-based study. Eur Radiol. (2019) 29:5172–9. 10.1007/s00330-019-06104-z [DOI] [PubMed] [Google Scholar]
- 27.Mayerhoefer ME, Szomolanyi P, Jirak D, Materka A, Trattnig S. Effects of MRI acquisition parameter variations and protocol heterogeneity on the results of texture analysis and pattern discrimination: an application-oriented study. Med Phys. (2009) 36:1236–43. 10.1118/1.3081408 [DOI] [PubMed] [Google Scholar]
- 28.Jirák D, Dezortová M, Hájek M. Phantoms for texture analysis of MR images. Long-term and multi-center study. Med Phys. (2004) 31:616–22. 10.1118/1.1646231 [DOI] [PubMed] [Google Scholar]
- 29.Waugh SA, Lerski RA, Bidaut L, Thompson AM. The influence of field strength and different clinical breast MRI protocols on the outcome of texture analysis using foam phantoms. Med Phys. (2011) 38:5058–66. 10.1118/1.3622605 [DOI] [PubMed] [Google Scholar]
- 30.Saha A, Yu X, Sahoo D, Mazurowski MA. Effects of MRI scanner parameters on breast cancer radiomics. Expert Syst Appl. (2017) 87:384–91. 10.1016/j.eswa.2017.06.029 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 31.van Ooij P, Garcia J, Potters WV, Malaisrie SC, Collins JD, Carr JC, et al. Age-related changes in aortic 3d blood flow velocities and wall shear stress: implications for the identification of altered hemodynamics in patients with aortic valve disease. J Magn Reson Imaging. (2016) 43:1239–49. 10.1002/jmri.25081 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 32.Garcia J, Barker AJ, Collins JD, Carr JC, Markl M. Volumetric quantification of absolute local normalized helicity in patients with bicuspid aortic valve and aortic dilatation. Magn Reson Med. (2017) 78:689–701. 10.1002/mrm.26387 [DOI] [PMC free article] [PubMed] [Google Scholar]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Data Availability Statement
The datasets generated and analyzed during the current study are not publicly available but are available from the corresponding author on reasonable request.