{"title":"Pd40Cu30Ni10P20合金在不同状态下的热膨胀和比容","authors":"N. Nishiyama, M. Horino, A. Inoue","doi":"10.2320/MATERTRANS1989.41.1432","DOIUrl":null,"url":null,"abstract":"We measured the thermal expansion and specific volume of the Pd 40 Cu 30 Ni 10 P 20 alloy by thermomechanical analyzer (TMA), fluid (H 2 O) displacement and volume dilatometric methods. At room temperature (293 K), the specific volumes of the Pd 40 Cu 30 Ni 10 P 20 alloy in the relaxed glassy and crystalline states are 0.1070 and 0.1065 m 3 /Mg, respectively. The average linear coefficients of thermal expansion are 17.0 x 10 -6 K -1 at 323 to 523 K in the relaxed glassy state (α relax ), 14.2 x 10 -6 K -1 at 323-673 K in the crystalline state (α cry ) and 39.9 x 10 -6 K -1 at 873-1223 K in the liquid (α liq ). Based on these results, the specific volume of the Pd 40 Cu 30 Ni 10 P 20 alloy as a function of temperature, V(T), is estimated. The extrapolation line of the specific volume for the equilibrium liquid is smoothly connected to the specific volume for the supercooled liquid. On the other hand, the intersection point of the specific volume between the extrapolation of equilibrium liquid and crystal is evaluated at 527 K. In the assumption that the temperature of the intersection point corresponds to the entropic stability limit for the undercooled liquid, it is much lower than that of previous thermodynamic study.","PeriodicalId":18264,"journal":{"name":"Materials Transactions Jim","volume":"21 1","pages":"1432-1434"},"PeriodicalIF":0.0000,"publicationDate":"2000-11-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"30","resultStr":"{\"title\":\"Thermal expansion and specific volume of Pd40Cu30Ni10P20 alloy in various states\",\"authors\":\"N. Nishiyama, M. Horino, A. Inoue\",\"doi\":\"10.2320/MATERTRANS1989.41.1432\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We measured the thermal expansion and specific volume of the Pd 40 Cu 30 Ni 10 P 20 alloy by thermomechanical analyzer (TMA), fluid (H 2 O) displacement and volume dilatometric methods. At room temperature (293 K), the specific volumes of the Pd 40 Cu 30 Ni 10 P 20 alloy in the relaxed glassy and crystalline states are 0.1070 and 0.1065 m 3 /Mg, respectively. The average linear coefficients of thermal expansion are 17.0 x 10 -6 K -1 at 323 to 523 K in the relaxed glassy state (α relax ), 14.2 x 10 -6 K -1 at 323-673 K in the crystalline state (α cry ) and 39.9 x 10 -6 K -1 at 873-1223 K in the liquid (α liq ). Based on these results, the specific volume of the Pd 40 Cu 30 Ni 10 P 20 alloy as a function of temperature, V(T), is estimated. The extrapolation line of the specific volume for the equilibrium liquid is smoothly connected to the specific volume for the supercooled liquid. On the other hand, the intersection point of the specific volume between the extrapolation of equilibrium liquid and crystal is evaluated at 527 K. In the assumption that the temperature of the intersection point corresponds to the entropic stability limit for the undercooled liquid, it is much lower than that of previous thermodynamic study.\",\"PeriodicalId\":18264,\"journal\":{\"name\":\"Materials Transactions Jim\",\"volume\":\"21 1\",\"pages\":\"1432-1434\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2000-11-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"30\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Materials Transactions Jim\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.2320/MATERTRANS1989.41.1432\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Materials Transactions Jim","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2320/MATERTRANS1989.41.1432","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 30
摘要
采用热分析仪(TMA)、流体(h2o)位移法和体积膨胀法测量了Pd - 40cu - 30ni10p20合金的热膨胀率和比容。在室温(293 K)下,Pd 40 Cu 30 Ni 10 p20合金的松弛玻璃态和晶态比容分别为0.1070和0.1065 m3 /Mg。在弛豫玻璃态(α弛豫)下,323 ~ 523 K下的热膨胀平均线性系数为17.0 × 10 -6 K -1,在结晶态(α cry)下,323 ~ 673 K下的热膨胀平均线性系数为14.2 × 10 -6 K -1,在液体(α liq)下,873 ~ 1223 K下的热膨胀平均线性系数为39.9 × 10 -6 K -1。在此基础上,估计了Pd - 40cu - 30ni - 10p20合金的比容随温度V(T)的变化规律。平衡液体比容的外推线与过冷液体比容平滑连接。另一方面,在527 K时计算了外推平衡液与晶体的比容交点。假设交点温度对应过冷液体的熵稳定极限,这比以往的热力学研究要低得多。
Thermal expansion and specific volume of Pd40Cu30Ni10P20 alloy in various states
We measured the thermal expansion and specific volume of the Pd 40 Cu 30 Ni 10 P 20 alloy by thermomechanical analyzer (TMA), fluid (H 2 O) displacement and volume dilatometric methods. At room temperature (293 K), the specific volumes of the Pd 40 Cu 30 Ni 10 P 20 alloy in the relaxed glassy and crystalline states are 0.1070 and 0.1065 m 3 /Mg, respectively. The average linear coefficients of thermal expansion are 17.0 x 10 -6 K -1 at 323 to 523 K in the relaxed glassy state (α relax ), 14.2 x 10 -6 K -1 at 323-673 K in the crystalline state (α cry ) and 39.9 x 10 -6 K -1 at 873-1223 K in the liquid (α liq ). Based on these results, the specific volume of the Pd 40 Cu 30 Ni 10 P 20 alloy as a function of temperature, V(T), is estimated. The extrapolation line of the specific volume for the equilibrium liquid is smoothly connected to the specific volume for the supercooled liquid. On the other hand, the intersection point of the specific volume between the extrapolation of equilibrium liquid and crystal is evaluated at 527 K. In the assumption that the temperature of the intersection point corresponds to the entropic stability limit for the undercooled liquid, it is much lower than that of previous thermodynamic study.