{"data":{"id":"10.6084/m9.figshare.1354056.v2","type":"dois","attributes":{"doi":"10.6084/m9.figshare.1354056.v2","prefix":"10.6084","suffix":"m9.figshare.1354056.v2","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Geers, Arjan J.","nameType":"Personal","givenName":"Arjan J.","familyName":"Geers","affiliation":[],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-7363-1095","nameIdentifierScheme":"ORCID"}]},{"name":"Larrabide, Ignacio","nameType":"Personal","givenName":"Ignacio","familyName":"Larrabide","affiliation":[],"nameIdentifiers":[]},{"name":"Radaelli, Alessandro G.","nameType":"Personal","givenName":"Alessandro G.","familyName":"Radaelli","affiliation":[],"nameIdentifiers":[]},{"name":"Bogunovic, Hrvoje","nameType":"Personal","givenName":"Hrvoje","familyName":"Bogunovic","affiliation":[],"nameIdentifiers":[]},{"name":"Minsuok Kim","affiliation":[],"nameIdentifiers":[]},{"name":"Andel, Hugo A.F. Gratama Van","nameType":"Personal","givenName":"Hugo A.F. Gratama Van","familyName":"Andel","affiliation":[],"nameIdentifiers":[]},{"name":"Majoie, Charles B.","nameType":"Personal","givenName":"Charles B.","familyName":"Majoie","affiliation":[],"nameIdentifiers":[]},{"name":"VanBavel, Ed","nameType":"Personal","givenName":"Ed","familyName":"VanBavel","affiliation":[],"nameIdentifiers":[]},{"name":"Frangi, Alejandro F.","nameType":"Personal","givenName":"Alejandro F.","familyName":"Frangi","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Reproducibility of hemodynamic simulations of cerebral aneurysms across imaging modalities 3DRA and CTA"}],"publisher":"figshare","container":{},"publicationYear":2015,"subjects":[{"subject":"Medicine"},{"subject":"Mechanical Engineering"},{"subject":"FOS: Mechanical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Mechanical engineering","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2015-03-26","dateType":"Created"},{"date":"2016-01-19","dateType":"Updated"},{"date":"2015","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsPreviousVersionOf","relatedIdentifier":"10.6084/m9.figshare.1354056","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["0 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"This dataset was created as part of the following study: Geers AJ, Larrabide I, Radaelli AG, Bogunovic H, Kim M, Gratama van Andel HAF, Majoie CB, VanBavel E, Frangi AF. Patient-specific computational hemodynamics of intracranial aneurysms from 3D rotational angiography and CT angiography: An in vivo reproducibility study. American Journal of Neuroradiology, 32(3):581–586, 2011. The goal of the study was to determine the reproducibility of blood flow simulations of cerebral aneurysms. Patients with a total of 10 cerebral aneurysms were imaged with both 3D rotational angiography (3DRA) and computed tomographic angiography (CTA). Each image independently was segmented to obtain a vascular model, the same boundary conditions were imposed, and a CFD simulation was obtained. The dataset contains values for geometric and hemodynamic variables that were extracted from the CFD simulations. The variables are defined as follows (TA: time-averaged; PS: peak systole; ED: end diastole): * A_N: Aneurysm neck area\u003cbr\u003e* V_A: Aneurysm volume\u003cbr\u003e* Q_P: TA flow rate in the parent vessel just proximal to the aneurysm\u003cbr\u003e* Q_A: TA flow rate into the aneurysm\u003cbr\u003e* NQ_A: Q_A / Q_P\u003cbr\u003e* WSS_P: Average TA WSS on the wall of a parent vessel segment just proximal to the aneurysm\u003cbr\u003e* WSS_A: Average TA WSS on the aneurysm wall\u003cbr\u003e* NWSS_A: WSS_A / WSS_P\u003cbr\u003e* LWSS_A: Portion of the aneurysm wall with WSS \u0026lt; 0.4 Pa at ED\u003cbr\u003e* MWSS_A: Maximum WSS on the aneurysm wall at PS\u003cbr\u003e* 90WSS_A: 90th percentile value of the WSS on the aneurysm wall at PS\u003cbr\u003e* N90WSS_A: 90WSS_A normalized by the average WSS on the aneurysm wall at PS See https://github.com/ajgeers/3dracta for an analysis of the data.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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