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Effect of impurities on the metastable zone width of solute-solvent systems

机译:杂质对溶质-溶剂体系亚稳区宽度的影响

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The novel approach to interpret the metastable zone width obtained by the polythermal method using the classical theory of three-dimensional nucleation proposed recently [K. Sangwal, Cryst. Growth Des. 9 (2009) 942] is extended to describe the metastable zone width of solute-solvent systems in the presence of impurities. It is considered that impurity particles present in the solution can change the nucleation rate J by affecting both the kinetic factor A and the term B related with the solute-solvent interfacial energy γ. An expression relating metastable zone width, as defined by the maximum supercooling △T_(max) of a solution saturated at temperature T_0, with cooling rate R is proposed in the form: (T_0/△T_(max))~2 = F(1-ZlnR), where F and Z are constants. The above relation can also be applied to describe the experimental data on maximum supercooling △T_(max) obtained at a given constant R as a function of impurity concentration c_i by the polythermal method and on maximum supersaturation σ_(max) as a function of impurity concentration c_i by the isothermal method. Experimental data on △T_(max) obtained as a function of cooling rate R for solutions containing various concentrations c_i of different impurities and as a function of concentration c_i of impurities at constant R by the polythermal method and on σ_(max) as a function of impurity concentration c_i by the isothermal method are analyzed satisfactorily using the above approach. The experimental data are also analyzed using the expression of the self-consistent Nyvlt-like approach [K. Sangwal, Cryst. Res. Technol. 44 (2009) 231]: In(△T_(max)/T_0) = Φ+β In R, where Φ and β are constants. It was found that the trends of the dependences of Φ and β on impurity concentration c_i are similar to those observed in the trends of the dependences of constants F and Z on c_i predicted by the approach based on the classical nucleation theory.
机译:最近提出的使用三维热成核的经典理论来解释通过多热法获得的亚稳区域宽度的新方法[K.克里斯·桑沃尔增长目标9(2009)942]被扩展以描述在存在杂质的情况下溶质-溶剂系统的亚稳区宽度。认为存在于溶液中的杂质颗粒可通过影响与溶质-溶剂界面能γ相关的动力学因子A和项B两者而改变成核率J。提出了一个由温度T_0饱和的溶液的最大过冷却量△T_(max)定义的,具有冷却速率R的亚稳态区域宽度的表达式,形式为(T_0 /△T_(max))〜2 = F( 1-ZlnR),其中F和Z为常数。上述关系也可以用于描述通过多热法在给定常数R下作为杂质浓度c_i的函数获得的最大过冷却△T_(max)和作为杂质函数的最大过饱和度σ_(max)的实验数据。等温法测定浓度c_i。通过多热法获得的关于不同冷却液浓度C_i的溶液的冷却速度R的函数△T_(max)以及在常数R处常数R的杂质浓度c_i的函数的σT(max)的实验数据使用上述方法可以令人满意地分析等温法测定的杂质浓度c_i。还使用自洽的Nyvlt样方法的表达来分析实验数据[K.克里斯·桑沃尔Res。技术。 [44(2009)231]:In(△T_(max)/ T_0)=Φ+β在R中,其中Φ和β为常数。发现,Φ和β对杂质浓度c_i的依赖性的趋势与基于经典成核理论的方法所预测的常数F和Z对c_i的依赖性的趋势相似。

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