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  • 學位論文

電致色變元件之建模與模擬

Modeling and Simulation for Electrochromic Devices

指導教授 : 何國川
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摘要


這篇論文描述作者在博士班研究工作中有關電致色變薄膜和元件的發現,除了第一章的前言與第六章的結論之外,四篇各自獨立的章節構成本篇論文的主體。前三章作者主要針對三種不同類型的電致色變元件,使用一些通用型原理和方程式來建模及模擬。第五章則說明作者如何模擬離子在電致色變薄膜中的輸送過程。因為所有討論的電致色變元件都屬於建模和模擬的工作,所以本篇論文的標題就訂為『電致色變薄膜元件的建模和模擬』,為了清楚說明本篇論文,各章摘要如下所述: 在第二章中,我們提出由紫精 (Heptyl Viologen)(HV(BF4)2) 和TMPD (N,N,N’,N’-tetramethyl-1,4-phenylenediamine) 所組成的溶液型互補式電致色變元件,可用質傳擴散模式來描述,並使用有限元素法來求解。透過此種方式,在著色及去色過程中,給定適當的初始和邊界條件後,擴散物質的暫態濃度分布的數值解可以求得。我們提出極限著色物質是由電極一端較快達到穩態濃度分布的著色物質所決定。於著去色時,模擬出的穩態電流密度與實驗數據相當一致。 在第三章中,利用電腦模擬來探討薄膜型互補式電致色變元件其活性面積對轉換響應的影響。我們使用等效電路模式來模擬薄膜型元件於著去色時其轉換響應曲線。此研究中,使用三氧化鎢 (tungsten oxide, WO3)/普魯士藍 (Prussian blue, PB) 互補式元件當作模擬系統,並且展示元件內電量密度的穩態響應。電腦模擬使用有限元素法軟體COMSOL Multiphysics®。此數值結果可為電致色變元件的發展和應用提供一些有用的資訊。電量密度動態揭示電荷輸送的動力學行為。我們將嵌入及嵌出電量密度值對不同的元件特性長度值作圖,圖中顯示了接近直線正比的關係。我們再將轉換時間對元件特性長度值作圖,圖中再次顯示了接近直線正比的關係。這就是說,愈大的元件面積需要較長的轉換時間。因此,我們可以藉由改變元件面積幾何形狀與電致色變薄膜的熱力學參數,來分析和預測薄膜型元件的轉換響應和光學性能是可行的。 在第四章中,在導電玻璃ITO基材上的普魯士藍薄膜電極,使用碳酸丙烯(propylene carbonate, PC) 作為溶劑,過氯酸鋰 (lithium perchlorate, LiClO4) 作為電解質,用循環伏安分析 (Cyclic Voltammetry, CV) 研究其電化學。提出一個普魯士藍薄膜在ITO電極上的質傳模式用於循環伏安行為,此模式在膜/ITO界面上將併入電子轉移動力學。我們也研究紫精溶液的循環伏安行為,使用Bulter-Volmer方程式來描述紫精溶在ITO電極表面上的循環伏安圖。我們研究此一液一膜型 (PB/HV) 互補式電致色變元件的循環伏安行為,就是將普魯士藍膜的CV和紫精溶液的CV結合在一起。 在第五章中,使用一種新型聚 (胺-醯亞胺,簡稱為Poly(PD-BCD)) 的電致色變薄膜來研究離子輸送,此種薄膜電極利用循環伏安法和電化學微量石英震盪天平(EQCM)來鑑定。藉由EQCM建模及模擬來做實驗數據分析。由於Poly(PD-BCD) 薄膜於氧化時為radical cation以及dication 的狀態,因此,在薄膜氧化過程中陰離子勢必會進入薄膜以平衡電性,而對於陽離子影響的確認方面,本研究利用含有三種不同陽離子基團之過氯酸鹽對薄膜之兩段反應進行分析,分別為LiClO4、NaClO4以及TBACO4,以了解陽離子效應對於薄膜的影響。將質量變化( m)對累積電量(Q)作圖,其電致色變機構就可以求得。從CV-EQCM的測量,在第一次氧化還原階段其 m-Q圖形中的斜率在三種電解質中是不同的,但在第二次氧化還原階段中卻幾乎是相同的。這意義是,在第一次氧化還原階段,陰陽離子都扮演重要角色;然而在第二次氧化還原階段,陽離子的角色較不重要。最後,我們提出Poly(PD-BCD) 有兩個反應機構對此兩個氧化還原階段。

關鍵字

電致色變元件 建模 模擬

並列摘要


This dissertation describes the author’s findings concerning the electrochromic (EC) thin films and devices during his PhD work. Besides the introductory (Chapter 1) and concluding (Chapter 6) chapters, four separate chapters (Chapters 2 to 5) are written as the main body of this dissertation. The first three chapters (Chapters 2 to 4) mainly deal with some universal principles and equations, simulated by the author, for three different configurations of electrochromic devices (ECDs). The last chapter (Chapters 5) addresses how the author simulated ion transport in an electrochromic thin-film. Since all of the ECDs discussed belong to the works for modeling and simulation, this dissertation is entitled “Modeling and Simulation for Electrochromic devices.” To present a clear picture of this dissertation, the main contents are summarized as follows. In the chapter 2, the diffusion model describing mass transport in a solution-type complementary electrochromic device containing heptyl viologen and N,N,N’,N’-tetramethyl-1,4-phenylenediamine is proposed and is solved using the finite element method. Using the method, a numerical solution to the transient concentration profile of the diffusing species is obtained for appropriate initial and boundary conditions during the coloring/bleaching process. Limiting coloring species are presented and are determined by the electrode at which the steady-state concentration profile is established faster. The simulated steady-state current density during coloring/bleaching fit well with the experimental data. In the chapter 3, this study uses computer simulations to investigate the effect of the active area of a complementary electrochromic device on switching response. The switching response curves of darkening and bleaching were simulated with an equivalent circuit model of a thin-film-type device. This study uses a tungsten oxide/Prussian blue complementary device as the simulated system, and demonstrates the steady-state response of the charge density within the device. Computer simulations were performed using the finite element method in the COMSOL Multiphysics® program. Numerical results provide some useful information for the development and application of electrochromic devices. Charge density dynamics reveal the kinetic behavior of charge transport. The graph of injected or extracted charge density versus characteristic lengths for various sizes shows an approximately linear relationship. The graph of switching times versus characteristic lengths also shows an approximately linear relationship. A larger active area produces a longer switching time. By changing the geometrical shape of the active area and the thermodynamic parameters of the two electrodes in electrochromic films, it is possible to analyze and predict the switching response and the optical performance of a thin-film type device. In the chapter 4, the electrochemistry of a Prussian blue (PB) thin film on an ITO electrode was studied in propylene carbonate (PC) solution using the Li+ of lithium perchlorate (LiClO4) electrolyte as the counter ion by cyclic voltammetry (CV). A model is proposed for the cyclic voltammetric behavior of a PB film on an ITO electrode surface. The model incorporates electron-transfer kinetics at film/ITO interface and diffusion within the film. The cyclic voltammetry of a heptyl viologen (HV(BF4)2) solution was also studied. The Butler-Volmer equation was used to describe the cyclic voltammogram of a HV solution on an ITO electrode surface. The cyclic voltammetric behavior of a complementary electrochromic device (ECD) based on a Prussian blue (PB) thin film and a heptyl viologen (HV(BF4)2) solution was studied by the combination of the CVs for the PB film and HV in PC containing 1M LiClO4. In the chapter 5, A new aromatic poly(amine-imide) electrochromic thin film synthesized with N,N-bis(4-aminophenyl)-N’,N’-diphenyl-1,4-phenylenediamine and 3,3’,4,4’-benzo-phenonetetra carboxylic dianhydride, abbreviated as poly(PD-BCD), was used for study of ion transport within thin film. The poly(PD-BCD) thin-film electrode has been characterized by cyclic voltammetry (CV) and electrochemical quartz crystal microbalance (EQCM). Experimental data was analyzed by EQCM modeling and simulation. As the polymer chain acquires positive charge during the oxidation of poly(PD-BCD) to its radical cation state or dication state, the anions would insert into the polymer matrix in order to neutralize the charge. However, when the electrodes were cycled in electrolytes containing different cations, including 0.1 M LiClO4/ACN, 0.1 M NaClO4/ACN and 0.1 M TBAClO4/ACN, the experimental results revealed two mechanisms for the redox reaction. A plot of mass change (Δm) vs. accumulated charge (Q) gave a slope, from which the electrochromic mechanism can be extracted. The slopes of Δm-Q obtained from the CV-EQCM measurements in three electrolytes were different for the first redox stage, but the slopes were almost the same for the second redox stage. This means that, in addition to the involvement of anions, cations also play an important role in the first redox stage, however, the role of the cations is less in the second stage. Moreover, two reaction mechanisms for the two reaction stages of poly(PD-BCD) are proposed in this study.

並列關鍵字

Electrochromic Devices Modeling Simulation

參考文獻


Chapter 1
[4] C. G. Granqvist, E. Avendano, and A. Azens, “Electrochromic Coatings and Devices: Survey of Some Recent Advances,” Thin Solid Films, 442, 201 (2003).
[5] C. M. Lampert, “Chromogenic Smart Materials,” Materials Today, 7, 28 (2004).
[6] C. M. Lampert, “Smart Switchable Glazing for Solar Energy and Daylight Control,” Sol. Energy Mater. Sol. Cells, 52, 207 (1998).
[7] D. R. Rosseinsky, and R. J. Mortimer, “Electrochromic Systems and the Prospects for Devices,” Adv. Mater., 13, 783 (2001).

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