{"data":{"id":"10.4121/uuid:87829ef5-be45-40e7-a0a7-b4c514633e26","type":"dois","attributes":{"doi":"10.4121/uuid:87829ef5-be45-40e7-a0a7-b4c514633e26","prefix":"10.4121","suffix":"uuid:87829ef5-be45-40e7-a0a7-b4c514633e26","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Hilgersom, Koen","nameType":"Personal","givenName":"Koen","familyName":"Hilgersom","nameIdentifiers":[{"nameIdentifier":"0000-0002-2513-8255","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Suárez, F. (Francisco)","nameType":"Personal","givenName":"F. (Francisco)","familyName":"Suárez","nameIdentifiers":[{"nameIdentifier":"0000-0002-4394-957X","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Zijlema, M. (Marcel)","givenName":"M. (Marcel)","familyName":"Zijlema","affiliation":[],"nameIdentifiers":[]},{"name":"Hausner, M.B. (Mark)","nameType":"Personal","givenName":"M.B. (Mark)","familyName":"Hausner","nameIdentifiers":[{"nameIdentifier":"0000-0001-7941-6970","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Tyler, S.W. (Scott)","nameType":"Personal","givenName":"S.W. (Scott)","familyName":"Tyler","nameIdentifiers":[{"nameIdentifier":"0000-0002-0477-5351","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"van de Giesen, N.C. (Nick)","nameType":"Personal","givenName":"N.C. (Nick)","familyName":"van de Giesen","nameIdentifiers":[{"nameIdentifier":"0000-0002-7200-3353","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]}],"titles":[{"title":"A free-surface solar pond model with a sloping edge: model code and data [version 1]"}],"publisher":"TU Delft","container":{},"publicationYear":2016,"subjects":[{"subject":"Interdisciplinary Engineering","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0915"},{"subject":"FOS: Other engineering and technologies","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"SWASH (Simulating WAves till SHore)"},{"subject":"distributed temperature sensing"},{"subject":"double-diffusion"},{"subject":"double-diffusive convection"},{"subject":"energy storage"},{"subject":"free-surface model"},{"subject":"heat storage"},{"subject":"heat transport"},{"subject":"non-hydrostatic model"},{"subject":"salt transport"},{"subject":"solar energy"},{"subject":"solar pond"},{"subject":"thermohaline stratification"},{"subject":"Time: 2009-03-09/2009-03-16"}],"contributors":[{"name":"TU Delft, Faculty Of Civil Engineering And Geosciences, Department Of Water Management","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]}],"dates":[{"date":"2016-09-27","dateType":"Issued"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[],"relatedItems":[],"sizes":[],"formats":["media types: application/octet-stream, application/pdf, application/zip, text/plain, text/x-shellscript, video/avi"],"version":"1","rightsList":[{"rights":"4TU General Terms of Use","rightsUri":"https://doi.org/10.4121/resource:terms_of_use"}],"descriptions":[{"description":"A non-hydrostatic free-surface model was set up to simulate salt and heat transport in a solar pond in order to: 1) investigate the added value of free-surface models for these types of simulations, and 2) assess the importance of heat transport along a sloping side wall. This data set presents the source code, the raw measurement and model data, and several movies comparing the vertical two-dimensional (2DV) model simulations to the measurements. The presented model code is an extension of the SWASH non-hydrostatic model, which is briefly introduced in this document. A complete discussion of the model results and conclusions are provided in an accompanying article.","descriptionType":"Abstract"}],"geoLocations":[{"geoLocationPlace":"Solar pond in laboratory, University of Nevada, Reno","geoLocationPoint":{"pointLatitude":"39.5414","pointLongitude":"-119.8145"}}],"fundingReferences":[],"xml":"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