c70富勒烯纯溶胶的合成及其在电解溶液中的稳定性

N. Mchedlov-Petrossyan, Mykyta O Marfunin, V. Klochkov, Petro Radionov
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摘要

本文研究了son/nC70型C70纯溶胶的合成和表征,并研究了氯化钠和十六烷基三甲基溴化铵(CTAB)对C70纯溶胶的混凝作用。在C70浓度为3.3×10-6 M时,电动势ζ= -40±4 mV,粒径以ζ -平均值表示为97±3 nm;在较高的C70浓度1.7×10-5和6.9×10-5 M下,粒径保持不变:99 ~ 100 nm。通过对NaCl浓度的增径速率(DIR)测定了临界混凝浓度(CCC)值。CCCs是浓度依赖性的:在C70浓度3.3×10-6, 1.7×10-5和6.9×10-5 M下分别为250,145和130 mM。CTAB表面活性剂的CCC要低得多,约为5×10-3 mM。然而,在0.02 mM CTAB下,过充电位高达ζ = + 40 mV,胶体颗粒稳定发生。如果只考虑静电斥力和分子引力,用Derjaguin-Landau-Verwey-Overbeek理论解释NaCl对纯sol的凝聚作用,就可以确定真空中C70-C70相互作用的Hamaker常数:AFF≈7×10-20 J.另一方面,如果我们使用之前在有机溶胶研究中得到的值AFF = (16.0-16.6) ×10-20 J,那么水溶胶的数据只能通过引入额外类型的相互作用来解释。根据Churaev和Derjaguin的术语,我们应该考虑结构对相互作用能的贡献,相互作用能稳定纯溶胶。
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HYDROSOL OF C70 FULLERENE: SYNTHESIS AND STABILITY IN ELECTROLYTIC SOLUTIONS
This article is devoted to the synthesis and characterization of the hydrosol of C70 of the son/nC70 type and to its coagulation by sodium chloride and cetyltrimethylammonium bromide (CTAB). At C70 concentration of 3.3×10–6 M, the electrokinetic potential is ζ= –40 ± 4 mV, the particle size expressed as Zeta-average is 97±3 nm; at higher C70 concentrations, 1.7×10–5 and 6.9×10–5 M, the size stays the same: 99 – 100 nm. The critical concentration of coagulation (CCC) values, were determined using the diameter increasing rate (DIR) on NaCl concentration. The CCCs are concentration-dependent: 250, 145, and 130 mM at C70 concentrations 3.3×10–6, 1.7×10–5, and 6.9×10–5 M, respectively. The CCC for the CTAB surfactant is much lower, about 5×10–3 mM. At 0.02 mM CTAB, however, the overcharging up to ζ = + 40 mV and stabilization of the colloidal particles take place. Interpretation of the hydrosol coagulation by NaCl using the Derjaguin–Landau–Verwey–Overbeek theory makes it possible to determine the Hamaker constant of the C70–C70 interaction in vacuum, if only electrostatic repulsion and molecular attraction are taking into account: AFF ≈ 7×10–20 J. On the other hand, if we use the value AFF = (16.0–16.6)×10–20 J, obtained earlier in the study of organosols, then the data for hydrosols can be explained only by the introduction of an additional type of interactions. Following the terms of Churaev and Derjaguin, one should take into account the structural contribution to the interaction energy, which stabilizes the hydrosol.
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