Jenkins H Donald Brooke, Tudela David, Glasser Leslie
Department of Chemistry, University of Warwick, Coventry, West Midlands, UK.
Inorg Chem. 2002 May 6;41(9):2364-7. doi: 10.1021/ic011216k.
This paper is one of a series exploring simple approaches for the estimation of lattice energy of ionic materials, avoiding elaborate computation. The readily accessible, frequently reported, and easily measurable (requiring only small quantities of inorganic material) property of density, rho(m), is related, as a rectilinear function of the form (rho(m)/M(m))(1/3), to the lattice energy U(POT) of ionic materials, where M(m) is the chemical formula mass. Dependence on the cube root is particularly advantageous because this considerably lowers the effects of any experimental errors in the density measurement used. The relationship that is developed arises from the dependence (previously reported in Jenkins, H. D. B.; Roobottom, H. K.; Passmore, J.; Glasser, L. Inorg. Chem. 1999, 38, 3609) of lattice energy on the inverse cube root of the molar volume. These latest equations have the form U(POT)/kJ mol(-1) = gamma(rho(m)/M(m))(1/3) + delta, where for the simpler salts (i.e., U(POT)/kJ mol(-1) < 5000 kJ mol(-1)), gamma and delta are coefficients dependent upon the stoichiometry of the inorganic material, and for materials for which U(POT)/kJ mol(-1) > 5000, gamma/kJ mol(-1) cm = 10(-7) AI(2IN(A))(1/3) and delta/kJ mol(-1) = 0 where A is the general electrostatic conversion factor (A = 121.4 kJ mol(-1)), I is the ionic strength = 1/2 the sum of n(i)z(i)(2), and N(A) is Avogadro's constant.
本文是探索估算离子材料晶格能的简单方法系列文章之一,避免了复杂的计算。密度ρ(m)这一易于获取、经常报道且易于测量(仅需少量无机材料)的性质,作为形式为(ρ(m)/M(m))(1/3)的线性函数,与离子材料的晶格能U(POT)相关,其中M(m)是化学式质量。依赖于立方根特别有利,因为这大大降低了所用密度测量中任何实验误差的影响。所建立的关系源于晶格能对摩尔体积的立方根倒数的依赖性(先前在Jenkins, H. D. B.; Roobottom, H. K.; Passmore, J.; Glasser, L. Inorg. Chem. 1999, 38, 3609中报道)。这些最新方程的形式为U(POT)/kJ mol⁻¹ = γ(ρ(m)/M(m))(1/3) + δ,对于较简单的盐(即U(POT)/kJ mol⁻¹ < 5000 kJ mol⁻¹),γ和δ是取决于无机材料化学计量比的系数,对于U(POT)/kJ mol⁻¹ > 5000的材料,γ/kJ mol⁻¹ cm = 10⁻⁷ AI(2IN(A))(1/3)且δ/kJ mol⁻¹ = 0,其中A是一般静电转换因子(A = 121.4 kJ mol⁻¹),I是离子强度 = 1/2 n(i)z(i)²的总和,N(A)是阿伏伽德罗常数。