{"data":{"id":"10.6084/m9.figshare.3081970","type":"dois","attributes":{"doi":"10.6084/m9.figshare.3081970","prefix":"10.6084","suffix":"m9.figshare.3081970","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Choudhary, Rehan","nameType":"Personal","givenName":"Rehan","familyName":"Choudhary","affiliation":[],"nameIdentifiers":[]},{"name":"Klauda, Jeffery B.","nameType":"Personal","givenName":"Jeffery B.","familyName":"Klauda","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"The simultaneous mass and energy evaporation (SM2E) model"}],"publisher":"Taylor \u0026 Francis","container":{},"publicationYear":2016,"subjects":[{"subject":"Biophysics"},{"subject":"29999 Physical Sciences not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Physical sciences","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Physiology"},{"subject":"FOS: Biological sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Biological sciences","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"39999 Chemical Sciences not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Chemical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Chemical sciences","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Ecology"},{"subject":"Immunology"},{"subject":"FOS: Clinical medicine","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Clinical medicine","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"69999 Biological Sciences not elsewhere classified","subjectScheme":"FOR"},{"subject":"19999 Mathematical Sciences not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Mathematics","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Mathematics","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Inorganic Chemistry"}],"contributors":[],"dates":[{"date":"2016-03-02","dateType":"Created"},{"date":"2016-03-10","dateType":"Updated"},{"date":"2016","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1080/15459624.2015.1101123","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["75510 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":"In this article, the Simultaneous Mass and Energy Evaporation (SM2E) model is presented. The SM2E model is based on theoretical models for mass and energy transfer. The theoretical models systematically under or over predicted at various flow conditions: laminar, transition, and turbulent. These models were harmonized with experimental measurements to eliminate systematic under or over predictions; a total of 113 measured evaporation rates were used. The SM2E model can be used to estimate evaporation rates for pure liquids as well as liquid mixtures at laminar, transition, and turbulent flow conditions. However, due to limited availability of evaporation data, the model has so far only been tested against data for pure liquids and binary mixtures. The model can take evaporative cooling into account and when the temperature of the evaporating liquid or liquid mixture is known (e.g., isothermal evaporation), the SM2E model reduces to a mass transfer-only model.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"PD94bWwgdmVyc2lvbj0iMS4wIiBlbmNvZGluZz0iVVRGLTgiPz4KPHJlc291cmNlIHhtbG5zPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCIgeG1sbnM6eHNpPSJodHRwOi8vd3d3LnczLm9yZy8yMDAxL1hNTFNjaGVtYS1pbnN0YW5jZSIgeHNpOnNjaGVtYUxvY2F0aW9uPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCBodHRwOi8vc2NoZW1hLmRhdGFjaXRlLm9yZy9tZXRhL2tlcm5lbC00LjEvbWV0YWRhdGEueHNkIj4KICA8aWRlbnRpZmllciBpZGVudGlmaWVyVHlwZT0iRE9JIj4xMC42MDg0L005LkZJR1NIQVJFLjMwODE5NzA8L2lkZW50aWZpZXI+CiAgPGNyZWF0b3JzPgogICAgPGNyZWF0b3I+CiAgICAgIDxjcmVhdG9yTmFtZT5SZWhhbiBDaG91ZGhhcnk8L2NyZWF0b3JOYW1lPgogICAgPC9jcmVhdG9yPgogICAgPGNyZWF0b3I+CiAgICAgIDxjcmVhdG9yTmFtZT5KZWZmZXJ5IEIuIEtsYXVkYTwvY3JlYXRvck5hbWU+CiAgICA8L2NyZWF0b3I+CiAgPC9jcmVhdG9ycz4KICA8dGl0bGVzPgogICAgPHRpdGxlPlRoZSBzaW11bHRhbmVvdXMgbWFzcyBhbmQgZW5lcmd5IGV2YXBvcmF0aW9uIChTTTJFKSBtb2RlbDwvdGl0bGU+CiAgPC90aXRsZXM+CiAgPGRlc2NyaXB0aW9ucz4KICAgIDxkZXNjcmlwdGlvbiBkZXNjcmlwdGlvblR5cGU9IkFic3RyYWN0Ij4mbHQ7cCZndDtJbiB0aGlzIGFydGljbGUsIHRoZSBTaW11bHRhbmVvdXMgTWFzcyBhbmQgRW5lcmd5IEV2YXBvcmF0aW9uIChTTTJFKSBtb2RlbCBpcyBwcmVzZW50ZWQuIFRoZSBTTTJFIG1vZGVsIGlzIGJhc2VkIG9uIHRoZW9yZXRpY2FsIG1vZGVscyBmb3IgbWFzcyBhbmQgZW5lcmd5IHRyYW5zZmVyLiBUaGUgdGhlb3JldGljYWwgbW9kZWxzIHN5c3RlbWF0aWNhbGx5IHVuZGVyIG9yIG92ZXIgcHJlZGljdGVkIGF0IHZhcmlvdXMgZmxvdyBjb25kaXRpb25zOiBsYW1pbmFyLCB0cmFuc2l0aW9uLCBhbmQgdHVyYnVsZW50LiBUaGVzZSBtb2RlbHMgd2VyZSBoYXJtb25pemVkIHdpdGggZXhwZXJpbWVudGFsIG1lYXN1cmVtZW50cyB0byBlbGltaW5hdGUgc3lzdGVtYXRpYyB1bmRlciBvciBvdmVyIHByZWRpY3Rpb25zOyBhIHRvdGFsIG9mIDExMyBtZWFzdXJlZCBldmFwb3JhdGlvbiByYXRlcyB3ZXJlIHVzZWQuIFRoZSBTTTJFIG1vZGVsIGNhbiBiZSB1c2VkIHRvIGVzdGltYXRlIGV2YXBvcmF0aW9uIHJhdGVzIGZvciBwdXJlIGxpcXVpZHMgYXMgd2VsbCBhcyBsaXF1aWQgbWl4dHVyZXMgYXQgbGFtaW5hciwgdHJhbnNpdGlvbiwgYW5kIHR1cmJ1bGVudCBmbG93IGNvbmRpdGlvbnMuIEhvd2V2ZXIsIGR1ZSB0byBsaW1pdGVkIGF2YWlsYWJpbGl0eSBvZiBldmFwb3JhdGlvbiBkYXRhLCB0aGUgbW9kZWwgaGFzIHNvIGZhciBvbmx5IGJlZW4gdGVzdGVkIGFnYWluc3QgZGF0YSBmb3IgcHVyZSBsaXF1aWRzIGFuZCBiaW5hcnkgbWl4dHVyZXMuIFRoZSBtb2RlbCBjYW4gdGFrZSBldmFwb3JhdGl2ZSBjb29saW5nIGludG8gYWNjb3VudCBhbmQgd2hlbiB0aGUgdGVtcGVyYXR1cmUgb2YgdGhlIGV2YXBvcmF0aW5nIGxpcXVpZCBvciBsaXF1aWQgbWl4dHVyZSBpcyBrbm93biAoZS5nLiwgaXNvdGhlcm1hbCBldmFwb3JhdGlvbiksIHRoZSBTTTJFIG1vZGVsIHJlZHVjZXMgdG8gYSBtYXNzIHRyYW5zZmVyLW9ubHkgbW9kZWwuJmx0Oy9wJmd0OzwvZGVzY3JpcHRpb24+CiAgPC9kZXNjcmlwdGlvbnM+CiAgPHN1YmplY3RzPgogICAgPHN1YmplY3Q+QmlvcGh5c2ljczwvc3ViamVjdD4KICAgIDxzdWJqZWN0IHNjaGVtZVVSST0iaHR0cDovL3d3dy5hYnMuZ292LmF1L2F1c3N0YXRzL2Fic0AubnNmLzAvNkJCNDI3QUI5Njk2QzIyNUNBMjU3NDE4MDAwNDQ2M0UiIHN1YmplY3RTY2hlbWU9IkZPUiI+Mjk5OTkgUGh5c2ljYWwgU2NpZW5jZXMgbm90IGVsc2V3aGVyZSBjbGFzc2lmaWVkPC9zdWJqZWN0PgogICAgPHN1YmplY3Q+UGh5c2lvbG9neTwvc3ViamVjdD4KICAgIDxzdWJqZWN0IHNjaGVtZVVSST0iaHR0cDovL3d3dy5hYnMuZ292LmF1L2F1c3N0YXRzL2Fic0AubnNmLzAvNkJCNDI3QUI5Njk2QzIyNUNBMjU3NDE4MDAwNDQ2M0UiIHN1YmplY3RTY2hlbWU9IkZPUiI+Mzk5OTkgQ2hlbWljYWwgU2NpZW5jZXMgbm90IGVsc2V3aGVyZSBjbGFzc2lmaWVkPC9zdWJqZWN0PgogICAgPHN1YmplY3Q+RWNvbG9neTwvc3ViamVjdD4KICAgIDxzdWJqZWN0PkltbXVub2xvZ3k8L3N1YmplY3Q+CiAgICA8c3ViamVjdCBzY2hlbWVVUkk9Imh0dHA6Ly93d3cuYWJzLmdvdi5hdS9hdXNzdGF0cy9hYnNALm5zZi8wLzZCQjQyN0FCOTY5NkMyMjVDQTI1NzQxODAwMDQ0NjNFIiBzdWJqZWN0U2NoZW1lPSJGT1IiPjY5OTk5IEJpb2xvZ2ljYWwgU2NpZW5jZXMgbm90IGVsc2V3aGVyZSBjbGFzc2lmaWVkPC9zdWJqZWN0PgogICAgPHN1YmplY3Qgc2NoZW1lVVJJPSJodHRwOi8vd3d3LmFicy5nb3YuYXUvYXVzc3RhdHMvYWJzQC5uc2YvMC82QkI0MjdBQjk2OTZDMjI1Q0EyNTc0MTgwMDA0NDYzRSIgc3ViamVjdFNjaGVtZT0iRk9SIj4xOTk5OSBNYXRoZW1hdGljYWwgU2NpZW5jZXMgbm90IGVsc2V3aGVyZSBjbGFzc2lmaWVkPC9zdWJqZWN0PgogICAgPHN1YmplY3Q+SW5vcmdhbmljIENoZW1pc3RyeTwvc3ViamVjdD4KICA8L3N1YmplY3RzPgogIDxwdWJsaXNoZXI+VGF5bG9yICZhbXA7IEZyYW5jaXM8L3B1Ymxpc2hlcj4KICA8cHVibGljYXRpb25ZZWFyPjIwMTY8L3B1YmxpY2F0aW9uWWVhcj4KICA8ZGF0ZXM+CiAgICA8ZGF0ZSBkYXRlVHlwZT0iQ3JlYXRlZCI+MjAxNi0wMy0wMjwvZGF0ZT4KICAgIDxkYXRlIGRhdGVUeXBlPSJVcGRhdGVkIj4yMDE2LTAzLTEwPC9kYXRlPgogIDwvZGF0ZXM+CiAgPHJlc291cmNlVHlwZSByZXNvdXJjZVR5cGVHZW5lcmFsPSJEYXRhc2V0Ij5EYXRhc2V0PC9yZXNvdXJjZVR5cGU+CiAgPHNpemVzPgogICAgPHNpemU+NzU1MTAgQnl0ZXM8L3NpemU+CiAgPC9zaXplcz4KICA8cmVsYXRlZElkZW50aWZpZXJzPgogICAgPHJlbGF0ZWRJZGVudGlmaWVyIHJlbGF0ZWRJZGVudGlmaWVyVHlwZT0iRE9JIiByZWxhdGlvblR5cGU9IklzU3VwcGxlbWVudFRvIj4xMC4xMDgwLzE1NDU5NjI0LjIwMTUuMTEwMTEyMzwvcmVsYXRlZElkZW50aWZpZXI+CiAgPC9yZWxhdGVkSWRlbnRpZmllcnM+CiAgPHJpZ2h0c0xpc3Q+CiAgICA8cmlnaHRzIHJpZ2h0c1VSST0iaHR0cHM6Ly9jcmVhdGl2ZWNvbW1vbnMub3JnL2xpY2Vuc2VzL2J5LzQuMC8iPkNDIEJZIDQuMDwvcmlnaHRzPgogIDwvcmlnaHRzTGlzdD4KPC9yZXNvdXJjZT4=","url":"https://tandf.figshare.com/articles/dataset/The_simultaneous_mass_and_energy_evaporation_SM2E_model/3081970/1","contentUrl":null,"metadataVersion":5,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount":2,"viewsOverTime":[{"yearMonth":"2025-10","total":1},{"yearMonth":"2025-12","total":1}],"downloadCount":0,"downloadsOverTime":[{"yearMonth":"2025-10","total":0},{"yearMonth":"2025-12","total":0}],"referenceCount":0,"citationCount":0,"citationsOverTime":[],"partCount":0,"pa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