簡易檢索 / 詳目顯示

研究生: 鄭斐澤
Cheng, Fei-Tze
論文名稱: 基於數值反演之自修復材料熱膨脹係數識別與驗證模擬
Numerical Calibration of Thermal Expansion in Self-Healing Materials with Thermo-Mechanical Validation
指導教授: 林冠中
Lin, Kuan-Chung
學位類別: 碩士
Master
系所名稱: 工學院 - 土木工程學系
Department of Civil Engineering
論文出版年: 2026
畢業學年度: 114
語文別: 中文
論文頁數: 142
中文關鍵詞: 自修復材料深共熔溶劑熱膨脹係數數值反算再生核質點法
外文關鍵詞: self-healing materials, deep eutectic solvent, coefficient of thermal expansion, inverse identification, reproducing kernel particle method
相關次數: 點閱:13下載:0
分享至:
查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報
  • 熱觸發型自修復高分子材料因具備自我修復裂縫之能力,於生醫領域與結構健康維護上極具潛力,而熱膨脹係數 (coefficient of thermal expansion, CTE) 為驅動高分子流動與裂縫閉合之關鍵參數。然而,本研究探討之深共熔溶劑 (deep eutectic solvent, DES) 離子凝膠於室溫下力學模數偏低,傳統接觸式量測易因接觸導致試體非預期變形,難以取得可靠之 CTE 數據。
    為突破此限制,本研究結合非接觸光學影像與有限元素法 (Finite Element Method, FEM),建構數值反演 (inverse calibration) 框架。研究先建構基於時溫疊加原理之廣義馬克士威黏彈模型,隨後對受限於模具之凝膠試體進行加熱原位觀測,以實驗位移為基準於 Abaqus 中反覆迭代識別 CTE,並於俯視角雙軸拘束與側視角單側膨脹兩組配置下交叉比對。
    結果顯示,兩種觀測配置反演之 CTE 在量級與形式上存在差異:俯視角於雙軸拘束下得乘冪函數 α(T) = 0.0245 × T^(-1.621),將 24 小時預測誤差由 89% 降至 4–12%;側視角於半自由邊界下得等效 CTE 為 9.3 × 10⁻³ °C⁻¹,與實驗吻合度達 99.98%。此數量級差異表明,反演所得之 CTE 並非材料純粹之熱力學常數,而是反映幾何拘束、重力耦合與高溫黏性流動共同作用之表觀等效參數。
    此外,針對修復後重新拉伸之大變形分析需求,並克服 FEM 於參數反演與大變形模擬之限制,本研究開發結合再生核質點法 (Reproducing Kernel Particle Method, RKPM) 與神經網路之混合求解器 (RKPM-NN),於線彈性與線性黏彈性等基準例題中皆達到與傳統方法相近之精度,為後續自修復材料完整熱-力耦合模擬與自動化參數反算奠定方法學基礎。

    Thermally triggered self-healing polymers, capable of autonomously healing cracks, hold substantial promise for biomedical applications and structural health maintenance. The coefficient of thermal expansion (CTE) plays a pivotal role in driving polymer flow and crack closure. However, the deep eutectic solvent (DES) ionogel investigated in this study exhibits a low mechanical modulus at room temperature, rendering conventional contact-based measurements prone to specimen deformation and precluding reliable CTE acquisition.
    To overcome this limitation, this study integrates non-contact optical imaging with the finite element method (FEM) to establish an inverse identification framework. A generalized Maxwell viscoelastic model based on the time-temperature superposition principle was first constructed. In-situ heating observations were then conducted on mold-confined specimens, and the CTE was iteratively identified in Abaqus using experimental displacements as reference, with cross-validation between a top-view biaxially constrained setup and a side-view unilaterally expanding setup.
    The results indicate that the CTE values inverted from the two observation configurations differ in magnitude and form. Under biaxial constraint, the top-view configuration yielded a power-law function α(T) = 0.0245 × T^(-1.621), reducing the 24-hour prediction error from 89% to 4–12%. Under a semi-free boundary, the side-view configuration yielded an equivalent CTE of 9.3 × 10⁻³ °C⁻¹, with 99.98% agreement against the experiment. This order-of-magnitude difference indicates that the identified CTE is not an intrinsic thermodynamic constant of the material, but rather an apparent equivalent parameter reflecting the combined effects of geometric constraints, gravitational coupling, and high-temperature viscous flow.
    Furthermore, to address large-deformation analysis after healing and to circumvent the limitations of FEM in parameter inversion, a hybrid solver (RKPM-NN) combining the reproducing kernel particle method (RKPM) with neural networks was developed. Validated against linear elastic and viscoelastic benchmarks with accuracy comparable to conventional methods, the solver establishes a methodological foundation for fully coupled thermo-mechanical simulation of self-healing materials and automated parameter identification.

    中文摘要 I Abstract II 誌謝 VII 目錄 VIII 表目錄 XII 圖目錄 XIII 符號說明 XVII 縮寫對照表 XXIII 第一章 緒論 1 1-1. 研究動機 1 1-2. 文獻回顧 2 1-2.1 熱修復材料 2 1-2.2 數值方法 4 1-2.3 結合類神經網路之數值求解 5 1-3. 本文結構 6 第二章 實驗結果 7 2-1. 自修復材料組成與試體製備 7 2-2. 軸拉伸試驗 10 2-2.1 彈性模數 10 2-2.2 波松比計算 13 2-3. 密度試驗 16 2-4. 熱物理參數識別 17 2-4.1 量測方法之適用性 17 2-4.2 數據穩定性與精確度分析 18 2-5. 流變試驗 19 2-5.1 動態頻率掃描與WLF分析 21 2-5.2 應力鬆弛試驗與Arrhenius分析 26 2-5.3 離子凝膠之多重鬆弛機制探討 29 2-5.4 廣義馬克士威模型擬合 30 第三章 有限元素法介紹 33 3-1. 數學模型與弱形式推導 34 3-1.1 強形式 34 3-1.2 弱形式推導 35 3-1.3 雙線性形式與迦遼金離散化 35 3-2. 有限元素法 37 3-2.1 形狀函數與等參數單元 38 3-2.2 數值積分與單元選擇 39 第四章 自修復材料 42 4-1. 雙視角自修復觀測與數值反演策略 42 4-2. 俯視角:雙軸拘束條件下之自修復變形觀測與係數識別 44 4-2.1 自修復實驗配置與顯微觀測流程 44 4-2.2 影像特徵擷取與變形量計算 46 4-2.3 數值模型建構與邊界設定 48 4-2.4 熱膨脹係數反演結果與對比驗證 50 4-3. 側視角多維熱變形分析與等效係數識別 58 4-3.1 單側膨脹實驗配置與影像擷取 58 4-3.2 影像特徵萃取與真實輪廓面積分析 60 4-3.3 數值模型建構與多物理場邊界設定 63 4-3.4 等向性熱膨脹係數面積反演結果 64 4-4. 雙視角反演識別之綜合討論與本章小結 68 4-4.1 綜合討論:表觀熱膨脹係數與力學環境之依賴特性 68 4-4.2 本章小結 69 第五章 無網格神經網路法介紹 70 5-1. 無網格法 70 5-1.1 Reproducing kernel particle method, RKPM 71 5-1.2 BSKM 73 5-1.3 積分方法 75 5-2. RKPM-NN 78 5-2.1 全連接前饋神經網路 78 5-2.2 RKPM-NN 數值求解策略與損失函數 80 5-3. 基準例題驗證 84 5-3.1 靜態問題 85 5-3.2 動態問題 89 5-3.3 準靜態問題 (黏彈性) 99 第六章 建議與未來展望 108 6-1. 結論 108 6-2. 未來展望 109 參考文獻 111

    [1] A. P. Abbott, G. Capper, D. L. Davies, R. K. Rasheed, and V. Tambyrajah. Novel solvent properties of choline chloride/urea mixtures. Chemical Communications, pages 70–71, 2003.
    [2] T. Alfrey and P. Doty. The methods of specifying the properties of viscoelastic materials. Journal of Applied Physics, 16(11):700–713, 1945.
    [3] J. Bai, Y. Zhou, Y. Ma, H. Jeong, H. Zhan, C. Rathnayaka, E. Sauret, and Y. Gu. A general neural particle method for hydrodynamics modeling. Computer Methods in Applied Mechanics and Engineering, 393:114740, 2022.
    [4] M. Baumgaertel and H. H. Winter. Determination of discrete relaxation and retardation time spectra from dynamic mechanical data. Rheologica Acta, 28(6):511–519, 1989.
    [5] T. Belytschko, W. K. Liu, B. Moran, and K. Elkhodary. Nonlinear Finite Elements for Continua and Structures. John Wiley & Sons, 2014.
    [6] G. Chen. Recurrent neural networks (RNNs) learn the constitutive law of viscoelasticity. Computational Mechanics, 67(3):1009–1019, 2021.
    [7] J.-S. Chen and H.-P. Wang. New boundary condition treatments in meshfree computation of contact problems. Computer methods in applied mechanics and engineering, 187(3-4):441–468, 2000.
    [8] J.-S. Chen, H.-P. Wang, S. Yoon, and Y. You. Some recent improvements in meshfree methods for incompressible finite elasticity boundary value problems with contact. Computational Mechanics, 25(2):137–156, 2000.
    [9] H. Eyring. Viscosity, plasticity, and diffusion as examples of absolute reaction rates. The Journal of Chemical Physics, 4(4):283–291, 1936.
    [10] J. D. Ferry. Viscoelastic Properties of Polymers. John Wiley & Sons, 1980.
    [11] J. D. Ferry and H. S. Myers. Viscoelastic properties of polymers. Journal of The Electrochemical Society, 108(7):142C–143C, 1961.
    [12] Z. Gu and J. F. Brennecke. Volume expansivities and isothermal compressibilities of imidazolium and pyridinium-based ionic liquids. Journal of Chemical & Engineering Data, 47(2):339–345, 2002.
    [13] M. Hillman and J.-S. Chen. An accelerated, convergent, and stable nodal integration in Galerkin meshfree methods for linear and nonlinear mechanics. International Journal for Numerical Methods in Engineering, 107(7):603–630, 2016.
    [14] K. Hornik, M. Stinchcombe, and H. White. Multilayer feedforward networks are universal approximators. Neural Networks, 2(5):359–366, 1989.
    [15] C.-W. Huang, S.-C. Wen, C.-H. Hsiao, C.-Z. Zhang, K.-C. Lin, and S.-S. Yu. Digital light processing of soft robotic gripper with high toughness and self-healing capability achieved by deep eutectic solvents. Advanced Functional Materials, 34(24):2314101, 2024.
    [16] D. P. Kingma and J. Ba. Adam: A method for stochastic optimization. arXiv preprint arXiv:1412.6980, 2014.
    [17] P. Lancaster and K. Salkauskas. Surfaces generated by moving least squares methods. Mathematics of computation, 37(155):141–158, 1981.
    [18] T. Le-Duc, H. Nguyen-Xuan, and J. Lee. A finite-element-informed neural network for parametric simulation in structural mechanics. Finite Elements in Analysis and Design, 217:103904, 2023.
    [19] Y. LeCun, Y. Bengio, and G. E. Hinton. Deep learning. Nature, 521(7553):436–444, 2015.
    [20] R. Li, T. Fan, G. Chen, K. Zhang, B. Su, J. Tian, and M. He. Autonomous self-healing, antifreezing, and transparent conductive elastomers. Chemistry of Materials, 32(2):874–881, 2020.
    [21] K.-C. Lin, Y.-C. Tai, P.-H. Lee, H.-K. Wong, Y. Wang, Y.-S. Lu, and J.-S. Chen. An accelerated meshfree computational framework with machine learning classification for multi-phase modeling of landslide. Computers and Geotechnics, 190:107756, 2026.
    [22] D. C. Liu and J. Nocedal. On the limited memory BFGS method for large scale optimization. Mathematical Programming, 45(1):503–528, 1989.
    [23] W. K. Liu, S. Jun, and Y. F. Zhang. Reproducing kernel particle methods. International Journal for Numerical Methods in Fluids, 20(8-9):1081–1106, 1995.
    [24] L. B. Lucy. A numerical approach to the testing of the fission hypothesis. Astronomical Journal, 82:1013–1024, 1977.
    [25] C. Mukesh, K. K. Upadhyay, R. V. Devkar, N. A. Chudasama, G. G. Raol, and K. Prasad. Preparation of a noncytotoxic hemocompatible ion gel by self-polymerization of HEMA in a green deep eutectic solvent. Macromolecular Chemistry and Physics, 217(17):1899–1906, 2016.
    [26] J. G. Oldroyd. On the formulation of rheological equations of state. Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 200(1063):523–541, 1950.
    [27] S. W. Park and R. A. Schapery. Methods of interconversion between linear viscoelastic material functions. Part I—a numerical method based on Prony series. International Journal of Solids and Structures, 36(11):1653–1675, 1999.
    [28] M. Raissi, A. Yazdani, and G. E. Karniadakis. Hidden fluid mechanics: Learning velocity and pressure fields from flow visualizations. Science, 367(6481):1026–1030, 2020.
    [29] C. Rao, H. Sun, and Y. Liu. Physics-informed deep learning for computational elastodynamics without labeled data. Journal of Engineering Mechanics, 147(8):04021043, 2021.
    [30] D. E. Rumelhart, G. E. Hinton, and R. J. Williams. Learning representations by back-propagating errors. Nature, 323(6088):533–536, 1986.
    [31] SIMULIA. Abaqus Analysis User's Guide, 2016.
    [32] A. M. Smith, D. G. Inocencio, B. M. Pardi, A. Gopinath, and R. C. Andresen Eguiluz. Facile determination of the Poisson's ratio and Young's modulus of polyacrylamide gels and polydimethylsiloxane. ACS Applied Polymer Materials, 6(4):2405–2416, 2024.
    [33] TA Instruments. Application of time-temperature superposition principles to DMA. Thermal Analysis Application Brief, 2022.
    [34] R. Tamate, K. Hashimoto, T. Horii, M. Hirasawa, X. Li, M. Shibayama, and M. Watanabe. Self-healing micellar ion gels based on multiple hydrogen bonding. Advanced Materials, 30(36):1802792, 2018.
    [35] H. Wessels, C. Weißenfels, and P. Wriggers. The neural particle method—an updated Lagrangian physics informed neural network for computational fluid dynamics. Computer Methods in Applied Mechanics and Engineering, 368:113127, 2020.
    [36] M. L. Williams, R. F. Landel, and J. D. Ferry. The temperature dependence of relaxation mechanisms in amorphous polymers and other glass-forming liquids. Journal of the American Chemical Society, 77(14):3701–3707, 1955.
    [37] C. Zener. Theory of the elasticity of polycrystals with viscous grain boundaries. Physical Review, 60(12):906, 1941.
    [38] O. C. Zienkiewicz, R. L. Taylor, P. Nithiarasu, and J. Z. Zhu. The Finite Element Method, volume 3. Elsevier, 1977.

    下載圖示
    校外:立即公開
    QR CODE