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基于动力学模型的确定性预测凝胶基单手性单壁碳纳米管分离。

A kinetic model for the deterministic prediction of gel-based single-chirality single-walled carbon nanotube separation.

机构信息

Departments of Chemical Engineering, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139, USA.

出版信息

ACS Nano. 2013 Feb 26;7(2):1779-89. doi: 10.1021/nn305939k. Epub 2013 Feb 8.

Abstract

We propose a kinetic model that describes the separation of single-chirality semiconducting carbon nanotubes based on the chirality-selective adsorption to specific hydrogels. Experimental elution profiles of the (7,3), (6,4), (6,5), (8,3), (8,6), (7,5), and (7,6) species are well described by an irreversible, first-order site association kinetic model with a single rate constant describing the adsorption of each SWNT to the immobile gel phase. Specifically, we find first-order binding rate constants for seven experimentally separated nanotubes normalized by the binding site molarity (M(θ)): k₇,₃ = 3.5 × 10⁻⁵ M(θ)⁻¹ s⁻¹, k₆,₄ = 7.7 × 10⁻⁸ M(θ)⁻¹ s⁻¹, k₈,₃ = 2.3 × 10⁻⁹ M(θ)⁻¹ s⁻¹, k₆,₅ = 3.8 × 10⁻⁹ M(θ)⁻¹ s⁻¹, k₇,₅ = 1.9 × 10⁻¹¹ M(θ)⁻¹ s⁻¹, k₈,₆ = 7.7 × 10⁻¹² M(θ)⁻¹ s⁻¹, and k₇,₆ = 3.8 × 10⁻¹² M(θ)⁻¹ s⁻¹. These results, as well as additional control experiments, unambiguously identify the separation process as a selective adsorption. Unlike certain chromatographic processes with retention time dependence, this separation procedure can be scaled to arbitrarily large volumes, as we demonstrate. This study provides a foundation for both the mechanistic understanding of gel-based SWNT separation as well as the potential industrial-scale realization of single-chirality production of carbon nanotubes.

摘要

我们提出了一个动力学模型,用于描述基于特定水凝胶对单手性半导体碳纳米管的手性选择性吸附的单手性碳纳米管的分离。(7,3)、(6,4)、(6,5)、(8,3)、(8,6)、(7,5)和(7,6)七种单分散碳纳米管的实验洗脱谱可以很好地用不可逆一级位点缔合动力学模型描述,该模型使用单一速率常数描述每个 SWNT 与固定凝胶相的吸附。具体而言,我们发现七种实验分离的碳纳米管的归一化到结合位摩尔浓度(M(θ))的一级结合速率常数为:k₇,₃ = 3.5 × 10⁻⁵ M(θ)⁻¹ s⁻¹,k₆,₄ = 7.7 × 10⁻⁸ M(θ)⁻¹ s⁻¹,k₈,₃ = 2.3 × 10⁻⁹ M(θ)⁻¹ s⁻¹,k₆,₅ = 3.8 × 10⁻⁹ M(θ)⁻¹ s⁻¹,k₇,₅ = 1.9 × 10⁻¹¹ M(θ)⁻¹ s⁻¹,k₈,₆ = 7.7 × 10⁻¹² M(θ)⁻¹ s⁻¹,和 k₇,₆ = 3.8 × 10⁻¹² M(θ)⁻¹ s⁻¹。这些结果以及其他对照实验明确地将分离过程确定为选择性吸附。与具有保留时间依赖性的某些色谱过程不同,我们证明这种分离程序可以扩展到任意大的体积,这为基于凝胶的 SWNT 分离的机制理解以及单手性碳纳米管的潜在工业规模生产提供了基础。

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