Douglass Eugene F, Driscoll Peter F, Liu Deli, Burnham Nancy A, Lambert Christopher R, McGimpsey W Grant
Department of Chemistry and Biochemistry, Worcester Polytechnic Institute, Worcester, Massachusetts 01609, USA.
Anal Chem. 2008 Oct 15;80(20):7670-7. doi: 10.1021/ac800521z. Epub 2008 Sep 24.
Analytical gold electrodes were polished mechanically and electrochemically and the true area of the electrode surface was measured by quantitative oxidative/reductive cycling of the electrode. A roughness factor for each electrode was determined from the ratio of the true area to the geometric area. The roughness is fully described by a combination of microscopic roughness (up to tens of nanometers) and macroscopic roughness (on the order of hundreds of nanometers) terms. The electrodes were then derivatized with a self-assembled monolayer (SAM) of dodecanethiol or a thioalkane azacrown and characterized by impedance spectroscopy. The behavior of the electrodes was modeled with either a Helmholtz or Randles equivalent circuit (depending on the SAM used) in which the capacitance was replaced with a constant phase element. From the model, an effective capacitance and an alpha factor that quantifies the nonideality of the SAM capacitance was obtained. The effective capacitance divided by the roughness factor yields the capacitance per unit true area, which is only a function of microscopic roughness. The relationship between this capacitance and the alpha factor indicates that microscopic roughness predominantly affects the nonideality of the film while macroscopic roughness predominantly affects the magnitude of the film's capacitance. Understanding the contribution of the electrode topography to the magnitude and ideality of the SAM capacitance is important in the construction of SAM-based capacitive sensors because it predicts the importance of electrode-electrode variations.
分析型金电极先进行机械抛光和电化学抛光,然后通过电极的定量氧化/还原循环测量电极表面的真实面积。根据真实面积与几何面积的比值确定每个电极的粗糙度因子。粗糙度由微观粗糙度(高达几十纳米)和宏观粗糙度(几百纳米量级)共同描述。然后用十二烷硫醇或硫代烷氮杂冠醚的自组装单分子层(SAM)对电极进行衍生化处理,并通过阻抗谱进行表征。电极的行为用亥姆霍兹或兰德尔等效电路(取决于所使用的SAM)进行建模,其中电容用常相位元件代替。从模型中得到有效电容和量化SAM电容非理想性的α因子。有效电容除以粗糙度因子得到单位真实面积的电容,它仅是微观粗糙度的函数。该电容与α因子之间的关系表明,微观粗糙度主要影响膜的非理想性,而宏观粗糙度主要影响膜电容的大小。了解电极形貌对SAM电容大小和理想性的贡献在基于SAM的电容式传感器构建中很重要,因为它预测了电极间变化的重要性。