Interdiffusivities matrix of CaO-Al2O3-SiO2 melt at 1723 K to 1823 K
Interdiffusivities matrix of CaO-Al2O3-SiO2 melt at 1723 K to 1823 K
复制标题
CaO-Al2O3-SiO2 熔体在 1723 K 至 1823 K 时的互扩散系数矩阵
DOI:
10.1007/bf02658629
复制
发表时间:
1977
期刊:
影响因子:
--
通讯作者:
K. Goto
中科院分区:
文献类型:
--
作者:
H. Sugawara;K. Nagata;K. Goto
AbstractTernary oxide mixtures of lime, alumina, and silica were premelted and quenched to produce glassy cylinders. A diffusion couple was selected from the mixtures of six different compositions in such a way that the average composition could be 40 wt pct CaO-20 wt pct A12O3 = 40 wt pct SiO2. Penetration curves of the components were measured with a X-ray microprobe analyzer.The interdiffusivities matrix defined with the Matano interface has been obtained from 52 successful diffusion runs at 1723 K to 1823 K as follows;1
% MathType!MTEF!2!1!+-% feaafiart1ev1aaatCvAUfKttLearuqr1ngBPrgarmWu51MyVXgatC% vAUfeBSjuyZL2yd9gzLbvyNv2CaeHbd9wDYLwzYbItLDharyavP1wz% ZbItLDhis9wBH5garqqtubsr4rNCHbGeaGqiVy0df9qqqrpepC0xbb% L8F4rqqrFfpeea0xe9Lq-Jc9vqaqpepm0xbba9pwe9Q8fs0-yqaqpe% pae9pg0FirpepeKkFr0xfr-xfr-xb9adbaqaaeGaciGaaiaabeqaam% aaeaqbaaGceaqabeaacuWGebargaacamaaDaaaleaaiqaacaWFXaGa% a8hmaiaa-1cacaWFXaGaa8hmaaqaaiaa-ndacaWFWaaaaOGaeyypa0% Jaa8hoaiaa-5cacaWF5aGaa8hiaiabgEna0kaa-bcacaWFXaGaa8hm% amaaCaaaleqabaGaa8xlaiaa-fdacaWFXaaaaOGagiyzauMaeiiEaG% NaeiiCaaNaeiikaGIaeyOeI0YaaSaaaeaacaWFYaGaa8xnaiaa-nda% caWFSaGaa83naiaa-bdacaWFWaaabaaceiGaa4Nuaiaa+rfaaaGaei% ykaKIaeiikaGIaa8xBamaaCaaaleqabaGaa8Nmaaaakiabc+caViaa% -nhacqGGPaqkaeaacuWGebargaacamaaDaaaleaacaWFXaGaa8hmai% aa-1cacaWFYaGaa8hmaaqaaiaa-ndacaWFWaaaaOGaeyypa0JaeyOe% I0Iaa8Nmaiaa-5cacaWF1aGaa8hiaiabgEna0kaa-bcacaWFXaGaa8% hmamaaCaaaleqabaGaa8xlaiaa-fdacaWFXaaaaOGagiyzauMaeiiE% aGNaeiiCaaNaeiikaGIaeyOeI0YaaSaaaeaacaWFXaGaa8xoaiaa-r% dacaWFSaGaa83maiaa-bdacaWFWaaabaGaa4Nuaiaa+rfaaaGaeiyk% aKIaeiikaGIaa8xBamaaCaaaleqabaGaa8Nmaaaakiabc+caViaa-n% hacqGGPaqkaaaa!818E!
$$\begin{gathered} \tilde D_{10 - 10}^{30} = 8.9 \times 10^{ - 11} \exp ( - \frac{{253,700}}{{RT}})(m^2 /s) \hfill \\ \tilde D_{10 - 20}^{30} = - 2.5 \times 10^{ - 11} \exp ( - \frac{{194,300}}{{RT}})(m^2 /s) \hfill \\ \end{gathered} $$
2
% MathType!MTEF!2!1!+-% feaafiart1ev1aaatCvAUfKttLearuqr1ngBPrgarmWu51MyVXgatC% vAUfeBSjuyZL2yd9gzLbvyNv2CaeHbd9wDYLwzYbItLDharyavP1wz% ZbItLDhis9wBH5garqqtubsr4rNCHbGeaGqiVy0df9qqqrpepC0xbb% L8F4rqqrFfpeea0xe9Lq-Jc9vqaqpepm0xbba9pwe9Q8fs0-yqaqpe% pae9pg0FirpepeKkFr0xfr-xfr-xb9adbaqaaeGaciGaaiaabeqaam% aaeaqbaaGceaqabeaacuWGebargaacamaaDaaaleaaiqaacaWFYaGa% a8hmaiaa-1cacaWFXaGaa8hmaaqaaiaa-ndacaWFWaaaaOGaeyypa0% JaeyOeI0Iaa8hnaiaa-5cacaWFWaGaa8hiaiabgEna0kaa-bcacaWF% XaGaa8hmamaaCaaaleqabaGaa8xlaiaa-fdacaWFXaaaaOGagiyzau% MaeiiEaGNaeiiCaaNaeiikaGIaeyOeI0YaaSaaaeaacaWFXaGaa83n% aiaa-DdacaWFSaGaa8Nnaiaa-bdacaWFWaaabaaceiGaa4Nuaiaa+r% faaaGaeiykaKIaeiikaGIaa8xBamaaCaaaleqabaGaa8Nmaaaakiab% c+caViaa-nhacqGGPaqkaeaacuWGebargaacamaaDaaaleaacaWFYa% Gaa8hmaiaa-1cacaWFYaGaa8hmaaqaaiaa-ndacaWFWaaaaOGaeyyp% a0Jaa8Nnaiaa-5cacaWFXaGaa8Nmaiaa-bcacqGHxdaTcaWFGaGaa8% xmaiaa-bdadaahaaWcbeqaaiaa-1cacaWFXaGaa8xmaaaakiGbcwga% LjabcIha4jabcchaWjabcIcaOiabgkHiTmaalaaabaGaa83maiaa-f% dacaWF4aGaa8hlaiaa-rdacaWFWaGaa8hmaaqaaiaa+jfacaGFubaa% aiabcMcaPiabcIcaOiaa-1gadaahaaWcbeqaaiaa-jdaaaGccqGGVa% WlcaWFZbGaeiykaKcaaaa!8239!
$$\begin{gathered} \tilde D_{20 - 10}^{30} = - 4.0 \times 10^{ - 11} \exp ( - \frac{{177,600}}{{RT}})(m^2 /s) \hfill \\ \tilde D_{20 - 20}^{30} = 6.12 \times 10^{ - 11} \exp ( - \frac{{318,400}}{{RT}})(m^2 /s) \hfill \\ \end{gathered} $$
where symbols, 10, 20, and 30 mean CaO, A12O3, and SiO2, respectively, and the activation energies are in Joules per mole.The diffusion composition paths obtained are discussed in relation to Cooper’s parallelogram. The composition dependency of the above interdiffusivities is estimated from the quasibinary interdiffusivities in all composition ranges of the present oxide system in liquid state.