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Pure vanadium shows the highest density with<jats:inline-formula><jats:alternatives><jats:tex-math>$${\\rho }_{V}\\left(T\\right)=5.55\\pm 0.03{\\mathrm{gcm}}^{-3}-6.01\\pm 0.52 {10}^{-4}{\\mathrm{gcm}}^{-3}{\\mathrm{K}}^{-1}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:msub><mml:mi>\u03c1<\/mml:mi><mml:mi>V<\/mml:mi><\/mml:msub><mml:mfenced><mml:mi>T<\/mml:mi><\/mml:mfenced><mml:mo>=<\/mml:mo><mml:mn>5.55<\/mml:mn><mml:mo>\u00b1<\/mml:mo><mml:mn>0.03<\/mml:mn><mml:msup><mml:mrow><mml:mi>gcm<\/mml:mi><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>3<\/mml:mn><\/mml:mrow><\/mml:msup><mml:mo>-<\/mml:mo><mml:mn>6.01<\/mml:mn><mml:mo>\u00b1<\/mml:mo><mml:mn>0.52<\/mml:mn><mml:msup><mml:mrow><mml:mn>10<\/mml:mn><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>4<\/mml:mn><\/mml:mrow><\/mml:msup><mml:msup><mml:mrow><mml:mi>gcm<\/mml:mi><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>3<\/mml:mn><\/mml:mrow><\/mml:msup><mml:msup><mml:mrow><mml:mi>K<\/mml:mi><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>1<\/mml:mn><\/mml:mrow><\/mml:msup><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>, pure titanium the lowest at<jats:inline-formula><jats:alternatives><jats:tex-math>$${\\rho }_{Ti}\\left(T\\right)=4.21\\pm 0.02{\\mathrm{gcm}}^{-3}-3.46\\pm 0.30 {10}^{-4}{\\mathrm{gcm}}^{-3}{\\mathrm{K}}^{-1}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:msub><mml:mi>\u03c1<\/mml:mi><mml:mrow><mml:mi>Ti<\/mml:mi><\/mml:mrow><\/mml:msub><mml:mfenced><mml:mi>T<\/mml:mi><\/mml:mfenced><mml:mo>=<\/mml:mo><mml:mn>4.21<\/mml:mn><mml:mo>\u00b1<\/mml:mo><mml:mn>0.02<\/mml:mn><mml:msup><mml:mrow><mml:mi>gcm<\/mml:mi><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>3<\/mml:mn><\/mml:mrow><\/mml:msup><mml:mo>-<\/mml:mo><mml:mn>3.46<\/mml:mn><mml:mo>\u00b1<\/mml:mo><mml:mn>0.30<\/mml:mn><mml:msup><mml:mrow><mml:mn>10<\/mml:mn><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>4<\/mml:mn><\/mml:mrow><\/mml:msup><mml:msup><mml:mrow><mml:mi>gcm<\/mml:mi><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>3<\/mml:mn><\/mml:mrow><\/mml:msup><mml:msup><mml:mrow><mml:mi>K<\/mml:mi><\/mml:mrow><mml:mrow><mml:mo>-<\/mml:mo><mml:mn>1<\/mml:mn><\/mml:mrow><\/mml:msup><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>with every measured alloy ranging between these two extrema. The molar volume was utilized in order to interpret the compositional density dependency. No significant excess volume was evident. It was therefore shown that the Ti\u2013V system acts like an ideal solution regarding density, molar volume and temperature coefficient. This result allows to reliably calculate the density for the complete Ti\u2013V system at any given temperature.<\/jats:p>","DOI":"10.1007\/s10853-022-07090-2","type":"journal-article","created":{"date-parts":[[2022,4,20]],"date-time":"2022-04-20T13:03:41Z","timestamp":1650459821000},"page":"7954-7964","update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":13,"title":["Density and excess volume of the liquid Ti\u2013V system measured in electromagnetic levitation"],"prefix":"10.1007","volume":"57","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-4247-9991","authenticated-orcid":false,"given":"Benedikt","family":"Reiplinger","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"J\u00fcrgen","family":"Brillo","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"297","published-online":{"date-parts":[[2022,4,20]]},"reference":[{"key":"7090_CR1","volume-title":"Materials properties handbook: titanium alloys","author":"R Boyer","year":"1994","unstructured":"Boyer R, Welsch G, Collings E (1994) Materials properties handbook: titanium alloys. 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