Trill Henning, Eckert Hellmut, Srdanov Vojislav I
Institut für Physikalische Chemie, Westfälische Wilhelms Universität Münster, Schlossplatz 7, 48149 Münster, Germany.
J Am Chem Soc. 2002 Jul 17;124(28):8361-70. doi: 10.1021/ja012765s.
A series of mixed sodalite samples, Na(8)[Al(6)Si(6)O(24)]Br(x).(H(3)O(2))(2-x), with the unit cell stoichiometries varying in the 0 < x <2 region, was made by hydrothermal synthesis and subsequently transformed into Na(6+x)[Al(6)Si(6)O(24)]Br(x).(4H(2)O)(2-x) and Na(6+x)[Al(6)Si(6)O(24)]Br(x).circle(2-x) sodalites. Here, circle refers to an empty sodalite cage. The three series, referred hereafter to as the Br/basic, Br/hydro, and Br/dry series, were characterized by powder diffraction X-ray and by (23)Na, (27)Al, and (81)Br magic angle spinning (MAS) NMR and high-resolution triple quantum (TQ) MAS NMR spectroscopy. We determined that incorporation of Br(-) anions is 130 times more preferred than incorporation of H(3)O(2)(-) anions during the formation of sodalite cages, which permitted precise control of the halide content in the solid. Monotonic trends in chemical shifts were observed as a function of cage occupancy, reflecting continuous changes in structural parameters. A linear correlation between (81)Br chemical shift and lattice constant with a slope of -86 ppm/A was observed for all three series. Likewise, (23)Na chemical shifts for Na(+) cations in salt-bearing sodalite cages correlate linearly with the lattice constant. Both results indicate a universal dependence of the (23)Na and (81)Br chemical shifts on the Na-Br distance. The (27)Al chemical shifts of Br/basic and Br/hydro sodalites obey an established relation between delta(cs) and the average T-O-T bond angle of 0.72 ppm/degrees. Br/dry sodalites show two aluminum resonances, characterized by significantly different chemical shifts and quadrupolar interaction parameters. In that series, local symmetry distortions are evident from strong quadrupolar perturbations in the NMR spectra. P(Q) values for (27)Al vary between 0.8 MHz in Br/basic sodalites and 4.4 MHz in the Br/dry series caused by deviations from the tetrahedral symmetry of the salt-free sodalite cages. For (23)Na, P(Q) values of 0.8, 0.8, 2.0, and 5.7 MHz were found for sodium in bromo, basic, hydro, and dry cages, respectively. In addition, both (23)Na and (81)Br spectra offer some evidence that the Br(-) anions in the Br/dry sodalite are displaced from the center of the expanded sodalite cage. For all three series, the spectral deconvolution of the (23)Na NMR line shapes permits an accurate determination of the mixed sodalite stoichiometry.
通过水热合成制备了一系列混合方钠石样品,化学式为Na(8)[Al(6)Si(6)O(24)]Br(x)·(H(3)O(2))(2 - x),其晶胞化学计量比在0 < x < 2范围内变化,随后转变为Na(6 + x)[Al(6)Si(6)O(24)]Br(x)·(4H(2)O)(2 - x)和Na(6 + x)[Al(6)Si(6)O(24)]Br(x)·circle(2 - x)方钠石。此处,circle表示空的方钠石笼。这三个系列,以下分别称为Br/碱系列、Br/水系列和Br/干系列,通过粉末X射线衍射以及(23)Na、(27)Al和(81)Br魔角旋转(MAS)核磁共振和高分辨率三量子(TQ)MAS核磁共振光谱进行表征。我们确定在方钠石笼形成过程中,Br(-)阴离子的掺入比H(3)O(2)(-)阴离子的掺入优先130倍,这使得能够精确控制固体中的卤化物含量。观察到化学位移随笼占有率的单调趋势,反映了结构参数的连续变化。对于所有三个系列,观察到(81)Br化学位移与晶格常数之间的线性相关性,斜率为 - 86 ppm/A。同样,含盐方钠石笼中Na(+)阳离子的(23)Na化学位移与晶格常数呈线性相关。这两个结果都表明(23)Na和(81)Br化学位移普遍依赖于Na - Br距离。Br/碱和Br/水方钠石的(27)Al化学位移符合δ(cs)与平均T - O - T键角之间已确立的关系,即0.72 ppm/度。Br/干方钠石显示出两个铝共振峰,其化学位移和四极相互作用参数明显不同。在该系列中,核磁共振谱中的强四极扰动表明存在局部对称性畸变。由于偏离无盐方钠石笼的四面体对称性,(27)Al的P(Q)值在Br/碱方钠石中为0.8 MHz,在Br/干系列中为4.4 MHz。对于(23)Na,在溴代、碱、水和干笼中的钠的P(Q)值分别为0.8、0.8、2.0和5.7 MHz。此外,(23)Na和(81)Br光谱都提供了一些证据,表明Br/干方钠石中的Br(-)阴离子从膨胀的方钠石笼中心发生了位移。对于所有三个系列,(23)Na核磁共振线形的光谱去卷积允许准确测定混合方钠石的化学计量比。