{"data":{"id":"10.6084/m9.figshare.c.3711988","type":"dois","attributes":{"doi":"10.6084/m9.figshare.c.3711988","prefix":"10.6084","suffix":"m9.figshare.c.3711988","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"U. Lācis","affiliation":[],"nameIdentifiers":[]},{"name":"G. A. Zampogna","affiliation":[],"nameIdentifiers":[]},{"name":"S. Bagheri","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Supplementary material from \"A computational continuum model of poroelastic beds\""}],"publisher":"Figshare","container":{},"publicationYear":2017,"subjects":[{"subject":"Mechanical Engineering"},{"subject":"FOS: Mechanical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Computational Physics"},{"subject":"90699 Electrical and Electronic Engineering not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"20302 Electrostatics and Electrodynamics","subjectScheme":"FOR"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2017-03-08","dateType":"Created"},{"date":"2017-03-08","dateType":"Updated"},{"date":"2017","dateType":"Issued"}],"language":null,"types":{"ris":"GEN","bibtex":"misc","citeproc":"article","schemaOrg":"Collection","resourceType":"Collection","resourceTypeGeneral":"Collection"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1098/rspa.20160932","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[{"rights":"CC BY","rightsUri":"https://creativecommons.org/licenses/by/4.0"}],"descriptions":[{"description":"Despite the ubiquity of fluid flows interacting with porous and elastic materials, we lack a validated non-empirical macroscale method for characterizing the flow over and through a poroelastic medium. We propose a computational tool to describe such configurations by deriving and validating a continuum model for the poroelastic bed and its interface with the above free fluid. We show that, using stress continuity condition and slip velocity condition at the interface, the effective model captures the effects of small changes in the microstructure anisotropy correctly and predicts the overall behaviour in a physically consistent and controllable manner. Moreover, we show that the performance of the effective model is accurate by validating with fully microscopic resolved simulations. The proposed computational tool can be used in investigations in a wide range of fields, including mechanical engineering, bio-engineering and geophysics.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"PD94bWwgdmVyc2lvbj0iMS4wIiBlbmNvZGluZz0iVVRGLTgiPz4KPHJlc291cmNlIHhtbG5zOnhzaT0iaHR0cDovL3d3dy53My5vcmcvMjAwMS9YTUxTY2hlbWEtaW5zdGFuY2UiIHhtbG5zPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCIgeHNpOnNjaGVtYUxvY2F0aW9uPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCBodHRwOi8vc2NoZW1hLmRhdGFjaXRlLm9yZy9tZXRhL2tlcm5lbC00L21ldGFkYXRhLnhzZCI+CiAgPGlkZW50aWZpZXIgaWRlbnRpZmllclR5cGU9IkRPSSI+MTAuNjA4NC9NOS5GSUdTSEFSRS5DLjM3MTE5ODg8L2lkZW50aWZpZXI+CiAgPGNyZWF0b3JzPgogICAgPGNyZWF0b3I+CiAgICAgIDxjcmVhdG9yTmFtZT5VLiBMxIFjaXM8L2NyZWF0b3JOYW1lPgogICAgPC9jcmVhdG9yPgogICAgPGNyZWF0b3I+CiAgICAgIDxjcmVhdG9yTmFtZT5HLiBBLiBaYW1wb2duYTwvY3JlYXRvck5hbWU+CiAgICA8L2NyZWF0b3I+CiAgICA8Y3JlYXRvcj4KICAgICAgPGNyZWF0b3JOYW1lPlMuIEJhZ2hlcmk8L2NyZWF0b3JOYW1lPgogICAgPC9jcmVhdG9yPgogIDwvY3JlYXRvcnM+CiAgPHRpdGxlcz4KICAgIDx0aXRsZT5TdXBwbGVtZW50YXJ5IG1hdGVyaWFsIGZyb20gIkEgY29tcHV0YXRpb25hbCBjb250aW51dW0gbW9kZWwgb2YgcG9yb2VsYXN0aWMgYmVkcyI8L3RpdGxlPgogIDwvdGl0bGVzPgogIDxwdWJsaXNoZXI+Rmlnc2hhcmU8L3B1Ymxpc2hlcj4KICA8cHVibGljYXRpb25ZZWFyPjIwMTc8L3B1YmxpY2F0aW9uWWVhcj4KICA8cmVzb3VyY2VUeXBlIHJlc291cmNlVHlwZUdlbmVyYWw9IkNvbGxlY3Rpb24iPkNvbGxlY3Rpb248L3Jlc291cmNlVHlwZT4KICA8c3ViamVjdHM+CiAgICA8c3ViamVjdD5NZWNoYW5pY2FsIEVuZ2luZWVyaW5nPC9zdWJqZWN0PgogICAgPHN1YmplY3Qgc3ViamVjdFNjaGVtZT0iRmllbGRzIG9mIFNjaWVuY2UgYW5kIFRlY2hub2xvZ3kgKEZPUykiIHNjaGVtZVVSST0iaHR0cDovL3d3dy5vZWNkLm9yZy9zY2llbmNlL2lubm8vMzgyMzUxNDcucGRmIj5GT1M6IE1lY2hhbmljYWwgZW5naW5lZXJpbmc8L3N1YmplY3Q+CiAgICA8c3ViamVjdD5Db21wdXRhdGlvbmFsIFBoeXNpY3M8L3N1YmplY3Q+CiAgICA8c3ViamVjdCBzdWJqZWN0U2NoZW1lPSJGT1IiPjkwNjk5IEVsZWN0cmljYWwgYW5kIEVsZWN0cm9uaWMgRW5naW5lZXJpbmcgbm90IGVsc2V3aGVyZSBjbGFzc2lmaWVkPC9zdWJqZWN0PgogICAgPHN1YmplY3Qgc3ViamVjdFNjaGVtZT0iRmllbGRzIG9mIFNjaWVuY2UgYW5kIFRlY2hub2xvZ3kgKEZPUykiIHNjaGVtZVVSST0iaHR0cDovL3d3dy5vZWNkLm9yZy9zY2llbmNlL2lubm8vMzgyMzUxNDcucGRmIj5GT1M6IEVsZWN0cmljYWwgZW5naW5lZXJpbmcsIGVsZWN0cm9uaWMgZW5naW5lZXJpbmcsIGluZm9ybWF0aW9uIGVuZ2luZWVyaW5nPC9zdWJqZWN0PgogICAgPHN1YmplY3Qgc3ViamVjdFNjaGVtZT0iRk9SIj4yMDMwMiBFbGVjdHJvc3RhdGljcyBhbmQgRWxlY3Ryb2R5bmFtaWNzPC9zdWJqZWN0PgogICAgPHN1YmplY3Qgc3ViamVjdFNjaGVtZT0iRmllbGRzIG9mIFNjaWVuY2UgYW5kIFRlY2hub2xvZ3kgKEZPUykiIHNjaGVtZVVSST0iaHR0cDovL3d3dy5vZWNkLm9yZy9zY2llbmNlL2lubm8vMzgyMzUxNDcucGRmIj5GT1M6IFBoeXNpY2FsIHNjaWVuY2VzPC9zdWJqZWN0PgogIDwvc3ViamVjdHM+CiAgPGRhdGVzPgogICAgPGRhdGUgZGF0ZVR5cGU9IkNyZWF0ZWQiPjIwMTctMDMtMDg8L2RhdGU+CiAgICA8ZGF0ZSBkYXRlVHlwZT0iVXBkYXRlZCI+MjAxNy0wMy0wODwvZGF0ZT4KICAgIDxkYXRlIGRhdGVUeXBlPSJJc3N1ZWQiPjIwMTc8L2RhdGU+CiAgPC9kYXRlcz4KICA8cmVsYXRlZElkZW50aWZpZXJzPgogICAgPHJlbGF0ZWRJZGVudGlmaWVyIHJlbGF0ZWRJZGVudGlmaWVyVHlwZT0iRE9JIiByZWxhdGlvblR5cGU9IklzU3VwcGxlbWVudFRvIj4xMC4xMDk4L3JzcGEuMjAxNjA5MzI8L3JlbGF0ZWRJZGVudGlmaWVyPgogIDwvcmVsYXRlZElkZW50aWZpZXJzPgogIDxzaXplcy8+CiAgPGZvcm1hdHMvPgogIDx2ZXJzaW9uLz4KICA8cmlnaHRzTGlzdD4KICAgIDxyaWdodHMgcmlnaHRzVVJJPSJodHRwczovL2NyZWF0aXZlY29tbW9ucy5vcmcvbGljZW5zZXMvYnkvNC4wIj5DQyBCWTwvcmlnaHRzPgogIDwvcmlnaHRzTGlzdD4KICA8ZGVzY3JpcHRpb25zPgogICAgPGRlc2NyaXB0aW9uIGRlc2NyaXB0aW9uVHlwZT0iQWJzdHJhY3QiPkRlc3BpdGUgdGhlIHViaXF1aXR5IG9mIGZsdWlkIGZsb3dzIGludGVyYWN0aW5nIHdpdGggcG9yb3VzIGFuZCBlbGFzdGljIG1hdGVyaWFscywgd2UgbGFjayBhIHZhbGlkYXRlZCBub24tZW1waXJpY2FsIG1hY3Jvc2NhbGUgbWV0aG9kIGZvciBjaGFyYWN0ZXJpemluZyB0aGUgZmxvdyBvdmVyIGFuZCB0aHJvdWdoIGEgcG9yb2VsYXN0aWMgbWVkaXVtLiBXZSBwcm9wb3NlIGEgY29tcHV0YXRpb25hbCB0b29sIHRvIGRlc2NyaWJlIHN1Y2ggY29uZmlndXJhdGlvbnMgYnkgZGVyaXZpbmcgYW5kIHZhbGlkYXRpbmcgYSBjb250aW51dW0gbW9kZWwgZm9yIHRoZSBwb3JvZWxhc3RpYyBiZWQgYW5kIGl0cyBpbnRlcmZhY2Ugd2l0aCB0aGUgYWJvdmUgZnJlZSBmbHVpZC4gV2Ugc2hvdyB0aGF0LCB1c2luZyBzdHJlc3MgY29udGludWl0eSBjb25kaXRpb24gYW5kIHNsaXAgdmVsb2NpdHkgY29uZGl0aW9uIGF0IHRoZSBpbnRlcmZhY2UsIHRoZSBlZmZlY3RpdmUgbW9kZWwgY2FwdHVyZXMgdGhlIGVmZmVjdHMgb2Ygc21hbGwgY2hhbmdlcyBpbiB0aGUgbWljcm9zdHJ1Y3R1cmUgYW5pc290cm9weSBjb3JyZWN0bHkgYW5kIHByZWRpY3RzIHRoZSBvdmVyYWxsIGJlaGF2aW91ciBpbiBhIHBoeXNpY2FsbHkgY29uc2lzdGVudCBhbmQgY29udHJvbGxhYmxlIG1hbm5lci4gTW9yZW92ZXIsIHdlIHNob3cgdGhhdCB0aGUgcGVyZm9ybWFuY2Ugb2YgdGhlIGVmZmVjdGl2ZSBtb2RlbCBpcyBhY2N1cmF0ZSBieSB2YWxpZGF0aW5nIHdpdGggZnVsbHkgbWljcm9zY29waWMgcmVzb2x2ZWQgc2ltdWxhdGlvbnMuIFRoZSBwcm9wb3NlZCBjb21wdXRhdGlvbmFsIHRvb2wgY2FuIGJlIHVzZWQgaW4gaW52ZXN0aWdhdGlvbnMgaW4gYSB3aWRlIHJhbmdlIG9mIGZpZWxkcywgaW5jbHVkaW5nIG1lY2hhbmljYWwgZW5naW5lZXJpbmcsIGJpby1lbmdpbmVlcmluZyBhbmQgZ2VvcGh5c2ljcy48L2Rlc2NyaXB0aW9uPgogIDwvZGVzY3JpcHRpb25zPgo8L3Jlc291cmNlPgo=","url":"https://figshare.com/collections/Supplementary_material_from_A_computational_continuum_model_of_poroelastic_beds_/3711988","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"api","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":1,"citationCount":0,"citationsOverTime":[],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2017-03-08T15:36:42.000Z","registered":"2017-03-08T15:36:43.000Z","published":"2017",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