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dc.contributor.authorSegovia Puras, José Juan 
dc.contributor.authorLozano Martín, Daniel 
dc.contributor.authorMartín González, María del Carmen 
dc.contributor.authorChamorro Camazón, César Rubén 
dc.contributor.authorVillamañán Olfos, Miguel Ángel 
dc.contributor.authorPérez, Eduardo
dc.contributor.authorGarcía Izquierdo, Carmen
dc.contributor.authorCampo, Dolores del
dc.date.accessioned2018-03-15T20:41:22Z
dc.date.available2018-08-10T23:40:29Z
dc.date.issued2017
dc.identifier.citationMetrologia 54 (2017) 663-673es
dc.identifier.issn1681-7575es
dc.identifier.urihttp://uvadoc.uva.es/handle/10324/29085
dc.descriptionProducción Científicaes
dc.description.abstractA new determination of the molar gas constant was performed from measurements of the speed of sound in argon at the triple point of water and extrapolation to zero pressure. A new resonant cavity was used. This is a triaxial ellipsoid whose walls are gold-coated steel and which is divided into two identical halves that are bolted and sealed with an O-ring. Microwave and electroacoustic traducers are located in the northern and southern parts of the cavity, respectively, so that measurements of microwave and acoustic frequencies are carried out in the same experiment. Measurements were taken at pressures from 600 kPa to 60 kPa and at 273.16 K. The internal equivalent radius of the cavity was accurately determined by microwave measurements and the first four radial symmetric acoustic modes were simultaneously measured and used to calculate the speed of sound. The improvements made using the new cavity have reduced by half the main contributions to the uncertainty due to the radius determination using microwave measurements which amounts to 4.7 parts in 106 and the acoustic measurements, 4.4 parts in 106, where the main contribution (3.7 parts in 106) is the relative excess half-widths associated with the limit of our acoustic model, compared with our previous measurements. As a result of all the improvements with the new cavity and the measurements performed, we determined the molar gas constant R = (8.314449  0.000056) J·K-1·mol-1 which corresponds to a relative standard uncertainty of 6.7 parts in 106. The value reported in this paper lies -1.3 parts in 106 below the recommended value of CODATA 2014, although still within the range consistent with it.es
dc.format.mimetypeapplication/pdfes
dc.language.isoenges
dc.publisherIOP PUBLISHINGes
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.subjectTermodinámicaes
dc.subject.classificationMolar gas constantes
dc.subject.classificationTriaxial ellipsoid resonatores
dc.subject.classificationKelvines
dc.subject.classificationMicrowave resonancees
dc.subject.classificationSpeed of soundes
dc.subject.classificationAcoustic resonancees
dc.titleUpdated determination of the molar gas constant R by acoustic measurements in argon at UVa-CEM.es
dc.typeinfo:eu-repo/semantics/articlees
dc.identifier.doi10.1088/1681-7575/aa7c47es
dc.identifier.publicationfirstpage663es
dc.identifier.publicationissue54es
dc.identifier.publicationlastpage673es
dc.identifier.publicationtitleUpdated determination of the molar gas constant R by acoustic measurements in argon at UVa-CEM.es
dc.identifier.publicationvolume54es
dc.peerreviewedSIes
dc.description.embargo2018-08-10es
dc.description.projectMEC ENE2013-47812-Res
dc.description.projectJunta de Castilla y León VA035U16es


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