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首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Interaction of Magnesium Ions with Pristine Single-Layer and Defected Graphene/Water Interfaces Studied by Second Harmonic Generation
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Interaction of Magnesium Ions with Pristine Single-Layer and Defected Graphene/Water Interfaces Studied by Second Harmonic Generation

机译:二次谐波研究镁离子与原始单层和变形石墨烯/水界面的相互作用

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This work reports thermodynamic and electrostatic parameters for fused silica/water interfaces containing cm~2-sized graphene ranging from a single layer of pristine graphene to defected graphene. Second harmonic generation (SHG) measurements carried out at pH 7 indicate that the surface charge density of the fused silica/water interface containing the defected graphene (—0.009(3) to —0.010(3) C/m~2) is between that of defect-free single layer graphene (-0.0049(8) C/m~2) and bare fused silica (-0.013(6) C/m~2). The interfacial free energy of the fused silica/water interface calculated from the Lippmann equation is reduced by a factor of 7 in the presence of single-layer pristine graphene, while defected graphene reduces it only by a factor of at most 2. Subsequent SHG adsorption isotherm studies probing the Mg~(2+) adsorption at the fused silica/water interface result in fully reversible metal ion interactions and observed binding constants, K_(ads), of 4(1) — 5(1) × 10~3 M~(-1) for pristine graphene and 3(1) — 4(1) × 10~3 M~(-1) for defected graphene, corresponding to adsorption free energies, △G_(ads), referenced to the 55.5 molarity of water, of—30(1) to —31.1(7) kJ/mol for both interfaces, comparable to Mg~(2+) adsorption at the bare fused silica/water interface. Maximum Mg~(2+) ion densities are obtained from Gouy—Chapman model fits to the Langmuir adsorption isotherms and found to range from 1.1(5) — 1.5(4) × 10~(12) ions adsorbed per cm2 for pristine graphene and 2(1) — 3.1(5) × 10~(12) ions adsorbed per cm for defected graphene, slightly smaller than those of for Mg~(2+) adsorption at the bare fused silica/water interface ((2—4) × 10~(12) ions adsorbed per cm~2), assuming the magnesium ions are bound as divalent species. We conclude that the presence of defects in the graphene sheet, which we estimate here to be around 1.3 × 10~(11) cm~2, imparts only subtle changes in the thermodynamic and electrostatic parameters quantified here.
机译:这项工作报告了包含cm〜2尺寸石墨烯的熔融二氧化硅/水界面的热力学和静电参数,范围从单层原始石墨烯到有缺陷的石墨烯。在pH 7下进行的二次谐波生成(SHG)测量表明,含有缺陷石墨烯的熔融石英/水界面的表面电荷密度(-0.009(3)至-0.010(3)C / m〜2)在无缺陷单层石墨烯(-0.0049(8)C / m〜2)和裸露的熔融二氧化硅(-0.013(6)C / m〜2)。在单层原始石墨烯存在下,由Lippmann方程计算得出的熔融二氧化硅/水界面的界面自由能降低了7倍,而有缺陷的石墨烯最多将其降低了2倍。随后的SHG吸附等温线研究Mg〜(2+)在熔融二氧化硅/水界面的吸附,导致金属离子相互作用完全可逆,观察到的结合常数K_(ads)为4(1)— 5(1)×10〜3 M原始石墨烯的〜(-1)和缺陷石墨烯的3(1)-4(1)×10〜3 M〜(-1),对应于吸附自由能△G_(ads),参考摩尔比为55.5对于两个界面,水的浓度都为-30(1)至-31.1(7)kJ / mol,与裸露的熔融二氧化硅/水界面处的Mg〜(2+)吸附相当。从Gouy-Chapman模型获得的最大Mg〜(2+)离子密度与Langmuir吸附等温线拟合,发现原始石墨烯和每cm2吸附的离子范围为1.1(5)-1.5(4)×10〜(12)离子。缺陷石墨烯每厘米吸附的2(1)— 3.1(5)×10〜(12)离子,比在裸露的熔融二氧化硅/水界面吸附的Mg〜(2+)的吸附离子稍小((2-4)假设镁离子以二价键形式结合,则每厘米2吸收10×(12)个离子。我们得出的结论是,石墨烯片中缺陷的存在(据我们估计约为1.3×10〜(11)cm〜2)仅对此处量化的热力学和静电参数产生了细微的变化。

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