6 research outputs found

    ์ž„์˜์„ฑ์ด ์žˆ๋Š” ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜•์— ๋Œ€ํ•œ ์ •๋Ÿ‰์  ํ•ด์„์— ๊ด€ํ•˜์—ฌ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ์ˆ˜๋ฆฌ๊ณผํ•™๋ถ€,2020. 2. ํ•˜์Šน์—ด.In this thesis, we introduce random elements into the Cucker-Smale(C-S) model and provide quantitative analyses for those uncertainties. In real applications of the Cucker-Smale dynamics, we can expect that the C-S model contains some intrinsic uncertainties in itself and misses some extrinsic factors that might affect the dynamics of particles. Thus, to provide a better description for the dynamics of a C-S ensemble, one needs to incorporate such uncertain factors to the model and evaluate their effects on the dynamics or stability of the C-S system. To fulfill this, we first consider the macroscopic version of the Cucker-Smale model. Namely, we introduce random inputs from communication weights and initial data into the hydrodynamic Cucker-Smale (HCS) model to yield the random HCS model. Furthermore, we address extrinsic uncertainties in the microscopic and mesoscopic level, respectively. For a microscopic model, we introduce a randomly switching network structure to the Cucker-Smale model and investigate sufficient conditions for the emergence of flocking. As a mesoscopic model, we consider the kinetic Cucker-Smale equation perturbed by multiplicative white noise and study the well-posedness and asymptotic dynamics of solutions.๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ์—์„œ๋Š”, ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜•์— ์ž„์˜์  ์š”์†Œ๋ฅผ ๋„์ž…ํ•˜์—ฌ ๊ทธ๋Ÿฌํ•œ ๋ถˆํ™•์‹ค์„ฑ์— ๋Œ€ํ•œ ์ •๋Ÿ‰์  ํ•ด์„์„ ์ œ์‹œํ•œ๋‹ค. ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜•์˜ ๋‹ค์ด๋‚˜๋ฏน์Šค๋ฅผ ์‹ค์ œ๋กœ ์‘์šฉํ•จ์— ์žˆ์–ด ์šฐ๋ฆฌ๋Š” ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜• ์ž์ฒด๊ฐ€ ๋ช‡๋ช‡ ๋‚ด์  ๋ถˆํ™•์‹ค์„ฑ์„ ํฌํ•จํ•˜๊ณ  ์žˆ์œผ๋ฉฐ ์ž…์ž๋“ค์˜ ๋‹ค์ด๋‚˜๋ฏน์Šค์— ์˜ํ•ญ์„ ์ค„ ์ˆ˜ ์žˆ๋Š” ๋ช‡ ๊ฐ€์ง€ ์™ธ๋ถ€์  ์š”์ธ์„ ๋†“์น˜๊ณ  ์žˆ์Œ์„ ์˜ˆ์ƒํ•  ์ˆ˜ ์žˆ๋‹ค. ๊ทธ๋Ÿฌ๋ฏ€๋กœ ์ฟ ์ปค-์Šค๋ฉ”์ผ ์ด์ฒด์˜ ๋‹ค์ด๋‚˜๋ฏน์Šค๋ฅผ ๋” ์ž˜ ์„œ์ˆ ํ•˜๊ธฐ ์œ„ํ•ด, ์ด๋Ÿฌํ•œ ๋ถˆํ™•์‹ค์„ฑ์ด ์žˆ๋Š” ์š”์†Œ๋ฅผ ๋ชจํ˜•์— ๋„์ž…ํ•˜์—ฌ ๊ทธ๊ฒƒ๋“ค์ด ์ฟ ์ปค-์Šค๋ฉ”์ผ ๊ณ„์˜ ๋‹ค์ด๋‚˜๋ฏน์Šค๋‚˜ ์•ˆ์ •์„ฑ์— ์ฃผ๋Š” ์˜ํ–ฅ์„ ํ‰๊ฐ€ํ•  ํ•„์š”๊ฐ€ ์žˆ๋‹ค. ์ด๋ฅผ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•ด, ์šฐ๋ฆฌ๋Š” ์šฐ์„  ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜•์˜ ๊ฑฐ์‹œ์ ์ธ ํ˜•ํƒœ๋ฅผ ๊ณ ๋ คํ•œ๋‹ค. ์ฆ‰, ์šฐ๋ฆฌ๋Š” ํ†ต์‹  ๊ฐ€์ค‘์น˜ ํ•จ์ˆ˜์™€ ์ดˆ๊ธฐ๊ฐ’์—์„œ ์˜ค๋Š” ์ž„์˜์  ์ž…๋ ฅ์น˜๋ฅผ ์œ ์ฒด์—ญํ•™ ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜•์— ํฌํ•จ์‹œ์ผœ ์ž„์˜์  ์œ ์ฒด์—ญํ•™ ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜•์„ ์œ ๋„ํ•œ๋‹ค. ๋” ๋‚˜์•„๊ฐ€ ๋ฏธ์‹œ์  ๊ทธ๋ฆฌ๊ณ  ์ค‘๊ฐ„๋ณด๊ธฐ์  ๋‹จ๊ณ„์—์„œ ์™ธ์  ๋ถˆํ™•์‹ค์„ฑ์— ๋Œ€ํ•ด ๋‹ค๋ฃฌ๋‹ค. ๋ฏธ์‹œ์  ๋ชจํ˜•์— ๋Œ€ํ•ด์„œ, ์ฟ ์ปค-์Šค๋ฉ”์ผ ๋ชจํ˜•์— ์ž„์˜๋กœ ๋ณ€ํ•˜๋Š” ๋„คํŠธ์›Œํฌ ๊ตฌ์กฐ๋ฅผ ๋„์ž…ํ•˜์—ฌ ํ”Œ๋กœํ‚น์˜ ์ฐฝ๋ฐœ์— ๋Œ€ํ•œ ์ถฉ๋ถ„์กฐ๊ฑด์„ ์•Œ์•„๋ณธ๋‹ค. ์ค‘๊ฐ„๋ณด๊ธฐ์  ๋‹จ๊ณ„์˜ ๋ชจํ˜•์œผ๋กœ์„œ, ์šฐ๋ฆฌ๋Š” ๊ณฑ์…ˆ ๋ฐฑ์ƒ‰ ์†Œ์Œ์œผ๋กœ ๋™์š”๋œ ์ฟ ์ปค-์Šค๋ฉ”์ผ ์šด๋™๋ฐฉ์ •์‹์„ ๊ณ ๋ คํ•˜๊ณ  ํ•ด์˜ ์กด์žฌ์„ฑ ๋ฐ ์œ ์ผ์„ฑ๊ณผ ์ ๊ทผ์  ๋‹ค์ด๋‚˜๋ฏน์Šค๋ฅผ ๊ณต๋ถ€ํ•œ๋‹ค.1 Introduction 1 2 Preliminaries 9 2.1 Notation 9 2.2 Previous results 10 3 A local sensitivity analysis for the hydrodynamic Cucker-Smale model with random inputs 15 3.1 Pathwise well-posedness of z-variations 16 3.1.1 First-order z-variations 18 3.1.2 Higher-order z-variations 26 3.2 The local sensitivity analysis for stability estimates 32 3.2.1 Higher-order L2-stability 32 3.2.2 L2-stability estimates for z-variations 37 3.3 A local sensitivity analysis for flocking estimate 41 4 On the stochastic flocking of the Cucker-Smale flock with randomly switching topologies 48 4.1 Preliminaries 49 4.1.1 Pathwise dissipative structure 49 4.1.2 A directed graph 52 4.1.3 A scrambling matrix 53 4.1.4 A state transition matrix 54 4.1.5 Previous results 55 4.2 A description of main result 57 4.2.1 Standing assumptions 57 4.2.2 Main result 58 4.3 Emergent behavior of the randomly switching system 61 4.3.1 A matrix formulation 61 4.3.2 Pathwise flocking under a priori assumptions 62 4.3.3 Emergence of stochastic flocking 70 5 Collective stochastic dynamics of the Cucker-Smale ensemble under uncertain communication 74 5.1 Preliminaries 75 5.1.1 Derivation of the SPDE 75 5.1.2 Presentation of main results 78 5.1.3 Elementary lemmas 80 5.2 A priori estimates for classical solutions 82 5.2.1 Quantitative estimates for classical solutions 86 5.3 Global well-posedness and asymptotic dynamics of strong solutions 92 5.3.1 Construction of approximate solutions 94 5.3.2 Estimates on approximate solutions 95 5.3.3 Proof of Theorem 5.1.3 103 6 Conclusion and future works 110 Appendix A Detailed proof of Chapter 3 112 A.1 Proof of Lemma 3.1.2 112 A.2 Proof of Lemma 3.1.5 115 A.3 Proof of Lemma 3.2.4 119 A.4 Proof of Theorem 3.3.2 121 Appendix B Detailed proof of Chapter 5 124 B.1 A proof of Theorem 5.2.1 124 B.2 A proof of Proposition 5.3.3 129 Bibliography 133Docto

    Generalized averaged Gaussian quadrature and applications

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    A simple numerical method for constructing the optimal generalized averaged Gaussian quadrature formulas will be presented. These formulas exist in many cases in which real positive GaussKronrod formulas do not exist, and can be used as an adequate alternative in order to estimate the error of a Gaussian rule. We also investigate the conditions under which the optimal averaged Gaussian quadrature formulas and their truncated variants are internal

    MS FT-2-2 7 Orthogonal polynomials and quadrature: Theory, computation, and applications

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    Quadrature rules find many applications in science and engineering. Their analysis is a classical area of applied mathematics and continues to attract considerable attention. This seminar brings together speakers with expertise in a large variety of quadrature rules. It is the aim of the seminar to provide an overview of recent developments in the analysis of quadrature rules. The computation of error estimates and novel applications also are described

    Propagation of regularity and finite-time collisions for the thermomechanical Cucker-Smale model with a singular communication

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