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纳米晶勃姆石干凝胶的表面与孔隙率

Surface and porosity of nanocrystalline boehmite xerogels.

作者信息

Alphonse Pierre, Courty Matthieu

机构信息

CIRIMAT, UMR-CNRS 5085, Université Paul Sabatier, 118 route de Narbonne, 31062 Toulouse Cedex 04, France.

出版信息

J Colloid Interface Sci. 2005 Oct 1;290(1):208-19. doi: 10.1016/j.jcis.2005.04.013.

DOI:10.1016/j.jcis.2005.04.013
PMID:15936767
Abstract

Boehmite xerogels are prepared by hydrolysis of Al(OC4H9)3 followed by peptization with HNO3 (H+/Al = 0, 0.07, 0.2). XRD and TEM show that these gels are made of nanosized crystals (5-9 nm in width and 3 nm thick). According to the amount of acid, no significant differences are found in size and shape, but only in the spatial arrangement of the crystallites. Nitrogen adsorption-desorption isotherms of nonpeptized gels are of type IV, whereas isotherms of peptized gels are of type I. These isotherms are analyzed by the t-plot method. The majority of pore volume results from intercrystalline mesopores, but the peptized gels also contain intercrystalline micropores. The particle packing is very dense for the gel peptized with H+/Al = 0.2 (porosity = 0.26), but it is less dense in non-peptized gel (porosity = 0.44). Heating these gels under vacuum creates, from 250 degrees C onwards, an intracrystalline microporosity resulting from the conversion of boehmite into transition alumina. But heating also causes intercrystalline micropores collapsing. The specific surface area increases up to a limit temperature (300 degrees C for nonpeptized gels and 400 degrees C for peptized) beyond which sintering of the particles begins and the surface decreases. The PSD are calculated assuming a cylindrical pore geometry and using the corrected Kelvin equation proposed by Kruk et al. Peptized xerogels give a monomodal distribution with a maximum near 2 nm and no pores are larger than 6 nm. Nonpeptized gels have a bimodal distribution with a narrow peak near to 2 nm and a broad unsymmetrical peak with a maximum at 4 nm. Heating in air above 400 degrees C has a strong effect on the porosity. As the temperature increases, there is a broadening of the distribution and a marked decrease of small pores (below 3 nm). However, even after treatment at 800 degrees C, micropores are still present.

摘要

通过Al(OC₄H₉)₃水解,随后用HNO₃(H⁺/Al = 0、0.07、0.2)进行胶溶来制备勃姆石干凝胶。X射线衍射(XRD)和透射电子显微镜(TEM)表明,这些凝胶由纳米晶体组成(宽度为5 - 9纳米,厚度为3纳米)。根据酸的用量,在尺寸和形状上未发现显著差异,只是在微晶的空间排列上有所不同。未胶溶凝胶的氮吸附 - 脱附等温线为IV型,而胶溶凝胶的等温线为I型。这些等温线通过t图法进行分析。大部分孔体积来自晶间中孔,但胶溶凝胶也含有晶间微孔。对于用H⁺/Al = 0.2胶溶的凝胶,颗粒堆积非常致密(孔隙率 = 0.26),但在未胶溶凝胶中堆积密度较小(孔隙率 = 0.44)。在真空中加热这些凝胶,从250℃开始,会由于勃姆石转变为过渡氧化铝而产生晶内微孔。但加热也会导致晶间微孔坍塌。比表面积在达到极限温度之前增加(未胶溶凝胶为300℃,胶溶凝胶为400℃),超过该温度后颗粒开始烧结,表面积减小。假定孔几何形状为圆柱形,并使用Kruk等人提出的校正开尔文方程来计算孔径分布(PSD)。胶溶干凝胶给出单峰分布,最大值在2纳米附近,且没有大于6纳米的孔。未胶溶凝胶具有双峰分布,在2纳米附近有一个窄峰,在4纳米处有一个宽的不对称峰且最大值在此处。在空气中400℃以上加热对孔隙率有很大影响。随着温度升高,分布变宽,小孔(低于3纳米)明显减少。然而,即使在800℃处理后,微孔仍然存在。

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