Low temperature properties of acetonitrile confined in MCM-41.

Low temperature properties of acetonitrile confined in MCM-41.
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DOI:
10.1021/jp052476g
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发表时间:
2005-11
期刊:
The journal of physical chemistry. B
影响因子:
--
通讯作者:
S. Kittaka;T. Iwashita;A. Serizawa;Miki Kranishi;S. Takahara;Y. Kuroda;Toshinori Mori;T. Yamaguchi
S. Kittaka;T. Iwashita;A. Serizawa;Miki Kranishi;S. Takahara;Y. Kuroda;Toshinori Mori;T. Yamaguchi
中科院分区:
其他
文献类型:
--
作者:
S. Kittaka;T. Iwashita;A. Serizawa;Miki Kranishi;S. Takahara;Y. Kuroda;Toshinori Mori;T. Yamaguchi

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采用吸附、红外光谱、差示扫描量热法和准弹性中子散射等方法研究了乙腈在介孔MCM-41中的相变和动力学。乙腈分子在一个单层强烈相互作用的表面羟基注册和扰动的三键在C[三键]N组。吸附在单层以上的分子通过圆柱形孔的中心部分是毛细管凝聚分子(α-乙腈),但它们在吸附-脱附等温线中不显示滞后回线,即,二级毛细凝聚FT-IR测量表明,凝聚相是非常相似的本体液体。α-乙腈在取决于MCM-41的孔径的温度下冷冻,低至29.1 A(C14),低于该温度时不冷冻。此外,在熔点以下观察到α型和β型乙腈之间的相变。应用Gibbs-Thomson方程,假设未冻结层厚度为0.7 nm,给出界面之间的界面自由能差,即,对于液体/孔表面(ps)和α-型/ps,Δ γ(1/α)= 22.4mJ m(-2),并且对于α-型/ps和β-型/ps,Δ γ(α/β)= 3.17mJ m(-2)。QENS实验证实了单层乙腈和α-乙腈的不同行为。单层乙腈分子被锚定以不平移。α-乙腈的QENS光谱的两个洛伦兹分析显示平移运动,但明显减慢。然而,在MCM-41(C18)中α-乙腈的活化能为7.0 kJ mol(-1),相比之下,本体值为12.7 kJ mol(-1)。α-乙腈翻滚旋转扩散的弛豫时间与体积值相似。
The effect of confinement on the phase changes and dynamics of acetonitrile in mesoporous MCM-41 was studied by use of adsorption, FT-IR, DSC, and quasi-elastic neutron scattering (QENS) measurements. Acetonitrile molecules in a monolayer interact strongly with surface hydroxyls to be registered and perturb the triple bond in the C[triple bond]N group. Adsorbed molecules above the monolayer through to the central part of the cylindrical pores are capillary condensed molecules (cc-acetonitrile), but they do not show the hysteresis loop in adsorption-desorption isotherms, i.e., second order capillary condensation. FT-IR measurements indicated that the condensed phase is very similar to the bulk liquid. The cc-acetonitrile freezes at temperatures that depend on the pore size of the MCM-41 down to 29.1 A (C14), below which it is not frozen. In addition, phase changes between alpha-type and beta-type acetonitriles were observed below the melting points. Application of the Gibbs-Thomson equation, assuming the unfrozen layer thickness to be 0.7 nm, gave the interface free energy differences between the interfaces, i.e., Deltagamma(l/alpha) = 22.4 mJ m(-2) for the liquid/pore surface (ps) and alpha-type/ps, and Deltagamma(alpha/beta) = 3.17 mJ m(-2) for alpha-type/ps and beta-type/ps, respectively. QENS experiments substantiate the differing behaviors of monolayer acetonitrile and cc-acetonitrile. The monolayer acetonitrile molecules are anchored so as not to translate. The two Lorentzian analysis of QENS spectra for cc-acetonitriles showed translational motion but markedly slowed. However, the activation energy for cc-acetonitrile in MCM-41 (C18) is 7.0 kJ mol(-1) compared to the bulk value of 12.7 kJ mol(-1). The relaxation times for tumbling rotational diffusion of cc-acetonitrile are similar to bulk values.