With the increased availability of computational resources, the past decade has seen a rise in the use of computational fluid dynamics (CFD) for medical applications. There has been an increase in the application of CFD to attempt to predict the rupture of intracranial aneurysms, however, while many hemodynamic parameters can be obtained from these computations, to date, no consistent methodology for the prediction of the rupture has been identified. One particular challenge to CFD is that many factors contribute to its accuracy; the mesh resolution and spatial/temporal discretization can alone contribute to a variation in accuracy. This failure to identify the importance of these factors and identify a methodology for the prediction of ruptures has limited the acceptance of CFD among physicians for rupture prediction. The International CFD Rupture Challenge 2013 seeks to comment on the sensitivity of these various CFD assumptions to predict the rupture by undertaking a comparison of the rupture and blood-flow predictions from a wide range of independent participants utilizing a range of CFD approaches. Twenty-six groups from 15 countries took part in the challenge. Participants were provided with surface models of two intracranial aneurysms and asked to carry out the corresponding hemodynamics simulations, free to choose their own mesh, solver, and temporal discretization. They were requested to submit velocity and pressure predictions along the centerline and on specified planes. The first phase of the challenge, described in a separate paper, was aimed at predicting which of the two aneurysms had previously ruptured and where the rupture site was located. The second phase, described in this paper, aims to assess the variability of the solutions and the sensitivity to the modeling assumptions. Participants were free to choose boundary conditions in the first phase, whereas they were prescribed in the second phase but all other CFD modeling parameters were not prescribed. In order to compare the computational results of one representative group with experimental results, steady-flow measurements using particle image velocimetry (PIV) were carried out in a silicone model of one of the provided aneurysms. Approximately 80% of the participating groups generated similar results. Both velocity and pressure computations were in good agreement with each other for cycle-averaged and peak-systolic predictions. Most apparent “outliers” (results that stand out of the collective) were observed to have underestimated velocity levels compared to the majority of solutions, but nevertheless identified comparable flow structures. In only two cases, the results deviate by over 35% from the mean solution of all the participants. Results of steady CFD simulations of the representative group and PIV experiments were in good agreement. The study demonstrated that while a range of numerical schemes, mesh resolution, and solvers was used, similar flow predictions were observed in the majority of cases. To further validate the computational results, it is suggested that time-dependent measurements should be conducted in the future. However, it is recognized that this study does not include the biological aspects of the aneurysm, which needs to be considered to be able to more precisely identify the specific rupture risk of an intracranial aneurysm.
The Computational Fluid Dynamics Rupture Challenge 2013—Phase II: Variability of Hemodynamic Simulations in Two Intracranial Aneurysms
Magdeburg 39106, Germany
Magdeburg 39106, Germany
Magdeburg 39120, Germany
Magdeburg 39106, Germany
Sendai, Miyagi 980-8574,
Japan
Lemesos 3036, Cyprus
Lemesos 3036, Cyprus
Manchester M60 1QD, UK
Manchester M60 1QD, UK
Highfield, Southampton SO17 1BJ, UK
London W6 7NL, UK
Fairfax, VA 22030
Fairfax, VA 22030
Parma 43125, Italy
Beijing 100124, China
Beijing 100124, China
Barcelona 08002, Spain
Kingsville, TX 78363;
Rochester, MN 55905
Kingsville, TX 78363;
Rochester, MN 55905
Fargo, ND 58102
Fargo, ND 58102
Toronto, ON M5S 3G8, Canada
Toronto, ON M5S 3G8, Canada
Wakayama 640-8505, Japan
Mellon University Joint Institute of Engineering,
Pittsburgh, PA 15219
Mellon University Joint Institute of Engineering,
Pittsburgh, PA 15219
Dortmund 44227, Germany
Dortmund 44227, Germany
Paris 92156, France
Paris 92156, France
Berlin 13353, Germany
Berlin 13353, Germany
Tarragona 43007, Spain
Tarragona 43007, Spain
Ames, IA 50011-2161
Sariyer, Istanbul 34450, Turkey
Sariyer, Istanbul 34450, Turkey
Milharado 2665-305, Portugal
Milharado 2665-305, Portugal
Kansas City, MO 64110
Kansas City, MO 64110
Prague 18675, Czech Republic
Prague 18675, Czech Republic
Montevideo 11300, Uruguay
Montevideo 11300, Uruguay
University of New York,
Buffalo, NY 14203
University of New York,
Buffalo, NY 14203
Toronto, ON M5S 3G8, Canada
Magdeburg 39106, Germany
Magdeburg 39106, Germany
Magdeburg 39106, Germany
Magdeburg 39120, Germany
Magdeburg 39106, Germany
Sendai, Miyagi 980-8574,
Japan
Lemesos 3036, Cyprus
Lemesos 3036, Cyprus
Manchester M60 1QD, UK
Manchester M60 1QD, UK
Highfield, Southampton SO17 1BJ, UK
London W6 7NL, UK
Fairfax, VA 22030
Fairfax, VA 22030
Parma 43125, Italy
Beijing 100124, China
Beijing 100124, China
Barcelona 08002, Spain
Kingsville, TX 78363;
Rochester, MN 55905
Kingsville, TX 78363;
Rochester, MN 55905
Fargo, ND 58102
Fargo, ND 58102
Toronto, ON M5S 3G8, Canada
Toronto, ON M5S 3G8, Canada
Wakayama 640-8505, Japan
Mellon University Joint Institute of Engineering,
Pittsburgh, PA 15219
Mellon University Joint Institute of Engineering,
Pittsburgh, PA 15219
Dortmund 44227, Germany
Dortmund 44227, Germany
Paris 92156, France
Paris 92156, France
Berlin 13353, Germany
Berlin 13353, Germany
Tarragona 43007, Spain
Tarragona 43007, Spain
Ames, IA 50011-2161
Sariyer, Istanbul 34450, Turkey
Sariyer, Istanbul 34450, Turkey
Milharado 2665-305, Portugal
Milharado 2665-305, Portugal
Kansas City, MO 64110
Kansas City, MO 64110
Prague 18675, Czech Republic
Prague 18675, Czech Republic
Montevideo 11300, Uruguay
Montevideo 11300, Uruguay
University of New York,
Buffalo, NY 14203
University of New York,
Buffalo, NY 14203
Toronto, ON M5S 3G8, Canada
Magdeburg 39106, Germany
Manuscript received October 30, 2014; final manuscript received September 30, 2015; published online November 5, 2015. Assoc. Editor: Francis Loth.
Berg, P., Roloff, C., Beuing, O., Voss, S., Sugiyama, S., Aristokleous, N., Anayiotos, A. S., Ashton, N., Revell, A., Bressloff, N. W., Brown, A. G., Jae Chung, B., Cebral, J. R., Copelli, G., Fu, W., Qiao, A., Geers, A. J., Hodis, S., Dragomir-Daescu, D., Nordahl, E., Bora Suzen, Y., Owais Khan, M., Valen-Sendstad, K., Kono, K., Menon, P. G., Albal, P. G., Mierka, O., Münster, R., Morales, H. G., Bonnefous, O., Osman, J., Goubergrits, L., Pallares, J., Cito, S., Passalacqua, A., Piskin, S., Pekkan, K., Ramalho, S., Marques, N., Sanchi, S., Schumacher, K. R., Sturgeon, J., Švihlová, H., Hron, J., Usera, G., Mendina, M., Xiang, J., Meng, H., Steinman, D. A., and Janiga, G. (November 5, 2015). "The Computational Fluid Dynamics Rupture Challenge 2013—Phase II: Variability of Hemodynamic Simulations in Two Intracranial Aneurysms." ASME. J Biomech Eng. December 2015; 137(12): 121008. https://doi.org/10.1115/1.4031794
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