{"data":{"id":"10.6084/m9.figshare.5245078","type":"dois","attributes":{"doi":"10.6084/m9.figshare.5245078","prefix":"10.6084","suffix":"m9.figshare.5245078","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Minghao Yu","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Simulation for the Effects of Well Pressure and Initial Temperature on Methane Hydrate Dissociation"}],"publisher":"figshare","container":{},"publicationYear":2017,"subjects":[{"subject":"91305 Energy Generation, Conversion and Storage Engineering","subjectScheme":"FOR"},{"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":"2017-07-26","dateType":"Created"},{"date":"2017-07-27","dateType":"Updated"},{"date":"2017","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[],"relatedItems":[],"sizes":["134899 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":"\u003cb\u003e1:\u003c/b\u003e The equilibrium pressure corresponding to the current temperature.\u003cb\u003e2:\u003c/b\u003e Model Verfication.\u003cb\u003e300minPw274\u003c/b\u003e/\u003cb\u003e300minPw279\u003c/b\u003e/\u003cb\u003e300minPw284\u003c/b\u003e/\u003cb\u003e3000minPw274\u003c/b\u003e/ \u003cb\u003e3000minPw279\u003c/b\u003e/\u003cb\u003e3000minPw284\u003c/b\u003e/\u003cb\u003e30000minPw274\u003c/b\u003e/ \u003cb\u003e30000minPw279\u003c/b\u003e/\u003cb\u003e30000minPw284: \u003c/b\u003ePressure distribution in reservoir under well pressure of 3MPa and initial temperature of 274K/279K/284K, and exploiting time of 300/3000/30000min.\u003cb\u003e300min5.0Pw\u003c/b\u003e/\u003cb\u003e300min8.0Pw\u003c/b\u003e/3\u003cb\u003e000min5.0Pw\u003c/b\u003e/\u003cb\u003e3000min8.0Pw\u003c/b\u003e/ \u003cb\u003e30000min5.0Pw\u003c/b\u003e/\u003cb\u003e30000min8.0Pw: \u003c/b\u003ePressure distribution in reservoir under well pressure of 5MPa/8MPa and initial temperature of284K, exploiting time of 300/3000/30000min.\u003cb\u003e300min274T\u003c/b\u003e/\u003cb\u003e300min279T\u003c/b\u003e/\u003cb\u003e300min284T\u003c/b\u003e/\u003cb\u003e3000min279T\u003c/b\u003e/\u003cb\u003e3000min284T\u003c/b\u003e/ \u003cb\u003e30000min279T\u003c/b\u003e/\u003cb\u003e30000min284T: \u003c/b\u003eTemperature distribution in reservoir under well pressure of 3MPa and initial temperature of 274K/279K/284K, exploiting time of 300/3000/30000min.\u003cb\u003e300min274K K\u003c/b\u003e/\u003cb\u003e300min279K K\u003c/b\u003e/\u003cb\u003e300min284K K\u003c/b\u003e/\u003cb\u003e3000min274K K\u003c/b\u003e/\u003cb\u003e3000min279K K\u003c/b\u003e/\u003cb\u003e3000min284K K\u003c/b\u003e/ \u003cb\u003e30000min274K K\u003c/b\u003e/\u003cb\u003e\u003c/b\u003e\u003cb\u003e30000min279K K\u003c/b\u003e/\u003cb\u003e30000min284K K: \u003c/b\u003e Permeability in reservoir under well pressure of 3MPa and initial temperature of 274K/279K/284K, exploiting time of 300/3000/30000min.\u003cb\u003eQg300min3.0 274\u003c/b\u003e/\u003cb\u003e \u003c/b\u003e\u003cb\u003eQg300min3.0 279\u003c/b\u003e/\u003cb\u003e \u003c/b\u003e\u003cb\u003eQg300min3.0 284\u003c/b\u003e/\u003cb\u003eQg300min5.0 284\u003c/b\u003e/\u003cb\u003e \u003c/b\u003e\u003cb\u003eQg300min8.0 284\u003c/b\u003e/\u003cb\u003e \u003c/b\u003e\u003cb\u003eQg3000min3.0 274\u003c/b\u003e/\u003cb\u003eQg3000min3.0 279\u003c/b\u003e/\u003cb\u003e \u003c/b\u003e\u003cb\u003eQg3000min3.0 284\u003c/b\u003e/\u003cb\u003e \u003c/b\u003e\u003cb\u003eQg3000min 5.0 284\u003c/b\u003e/\u003cb\u003e Qg3000min 8.0 284: \u003c/b\u003eCmulative gas produced under well pressure of 3MPa/5MPa/8MPa and initial temperature of 274K/279K/284K, exploiting time of 300/3000/30000min.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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