Updated determination of the molar gas constant $R$ by acoustic measurements in argon at UVa-CEM

J J Segovia, D Lozano-Martín, M C Martín, C R Chamorro, M A Villamañán, E Pérez, C García Izquierdo, D del Campo
{"title":"Updated determination of the molar gas constant $R$ by acoustic measurements in argon at UVa-CEM","authors":"J J Segovia, D Lozano-Martín, M C Martín, C R Chamorro, M A Villamañán, E Pérez, C García Izquierdo, D del Campo","doi":"arxiv-2409.10140","DOIUrl":null,"url":null,"abstract":"A new determination of the molar gas constant was performed from measurements\nof the speed of sound in argon at the triple point of water and extrapolation\nto zero pressure. A new resonant cavity was used. This is a triaxial ellipsoid\nwhose walls are gold-coated steel and which is divided into two identical\nhalves that are bolted and sealed with an O-ring. Microwave and electroacoustic\ntraducers are located in the northern and southern parts of the cavity,\nrespectively, so that measurements of microwave and acoustic frequencies are\ncarried out in the same experiment. Measurements were taken at pressures from\n600 kPa to 60 kPa and at 273.16 K. The internal equivalent radius of the cavity\nwas accurately determined by microwave measurements and the first four radial\nsymmetric acoustic modes were simultaneously measured and used to calculate the\nspeed of sound. The improvements made using the new cavity have reduced by half\nthe main contributions to the uncertainty due to the radius determination using\nmicrowave measurements which amounts to 4.7 parts in $10^{6}$ and the acoustic\nmeasurements, 4.4 parts in $10^{6}$, where the main contribution (3.7 parts in\n$10^{6}$) is the relative excess half-widths associated with the limit of our\nacoustic model, compared with our previous measurements. As a result of all the\nimprovements with the new cavity and the measurements performed, we determined\nthe molar gas constant $R$ = (8.314 449 $\\pm$ 0.000 056) J/(K mol) which\ncorresponds to a relative standard uncertainty of 6.7 parts in $10^{6}$. The\nvalue reported in this paper lies -1.3 parts in $10^{6}$ below the recommended\nvalue of CODATA 2014, although still within the range consistent with it.","PeriodicalId":501304,"journal":{"name":"arXiv - PHYS - Chemical Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Chemical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.10140","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

A 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 $10^{6}$ and the acoustic measurements, 4.4 parts in $10^{6}$, where the main contribution (3.7 parts in $10^{6}$) 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 $R$ = (8.314 449 $\pm$ 0.000 056) J/(K mol) which corresponds to a relative standard uncertainty of 6.7 parts in $10^{6}$. The value reported in this paper lies -1.3 parts in $10^{6}$ below the recommended value of CODATA 2014, although still within the range consistent with it.
通过 UVa-CEM 在氩气中的声学测量更新确定摩尔气体常数 $R$
通过测量氩气在水的三相点处的声速以及对零压的推断,对摩尔气体常数进行了新的测定。使用了一个新的谐振腔。这是一个三轴椭圆体,其内壁是镀金钢,分为两个相同的空腔,用螺栓连接并用 O 型环密封。微波和电声传感器分别位于腔体的北部和南部,因此可以在同一实验中测量微波和电声频率。测量是在压力为 600 kPa 至 60 kPa 和温度为 273.16 K 的条件下进行的。通过微波测量精确确定了空腔的内部等效半径,同时测量了前四个径向对称声学模式,并利用它们计算了声速。使用新空腔所做的改进将使用微波测量确定半径所产生的不确定性的主要贡献减少了一半,即 10^{6}$ 中的 4.7 份,而声学测量的不确定性为 10^{6}$ 中的 4.4 份,其中主要贡献(10^{6}$ 中的 3.7 份)是与我们以前的测量结果相比,与我们的声学模型极限相关的相对过剩半宽。由于使用了新的腔体并进行了测量,我们确定了摩尔气体常数 $R$ = (8.314 449 $\pm$ 0.000 056) J/(K mol),这相当于 10^{6}$ 中 6.7 份的相对标准不确定性。本文报告的数值比 CODATA 2014 的建议值低 10^{6}$ 中的 -1.3 部分,但仍在与其一致的范围之内。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信