20 research outputs found

    Improved Meshless Method in Point Cloud with High Aspect Ratio and Curvature

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ•ญ๊ณต์šฐ์ฃผ๊ณตํ•™๊ณผ, 2022.2. ๊น€๊ทœํ™.๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ธฐ์กด ๋ฌด๊ฒฉ์ž ๊ณต๊ฐ„ ์ฐจ๋ถ„ ํ•ด์„ ๊ธฐ๋ฒ•์ด ํฐ ์ข…ํšก๋น„ ๋ฐ ๊ณก๋ฅ ์„ ๊ฐ€์ง€๋Š” ์งˆ์  ๋ถ„ํฌ์—์„œ์˜ ์œ ๋™ ํ•ด์„์—์„œ ๊ณก๋ฅ  ๋ฐฉํ–ฅ ์œ ๋™ ๊ฐ€์† ๋“ฑ์˜ ํ˜•ํƒœ๋กœ ๋‚˜ํƒ€๋‚˜๋Š” ๋น„๋ฌผ๋ฆฌ์ ์ด๊ณ  ๋ถ€์ •ํ™•ํ•œ ๊ฒฐ๊ณผ๋ฅผ ๋ณด์ด๋Š” ๋ฌธ์ œ์ ์„ ํ•ด๊ฒฐํ•˜๊ธฐ ์œ„ํ•ด ์›์ธ ๋ถ„์„ ๋ฐ ๊ฐœ์„  ๊ธฐ๋ฒ• ๊ฐœ๋ฐœ์„ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ๊ธฐ์กด ๊ธฐํ•˜ํ•™์  ๋ณด์กด ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•(GC-LSM)๊ณผ ๋น„์ •๋ ฌ ์œ ํ•œ ์ฒด์ ๋ฒ•์ด ๊ณต์œ ํ•˜๋Š” ํŠน์„ฑ์œผ๋กœ๋ถ€ํ„ฐ ์ฐฉ์•ˆํ•˜์—ฌ ๋ผ๊ทธ๋ž‘์ฃผ ์Šน์ˆ˜๋ฒ•์„ ์ด์šฉํ•ด ์ตœ์†Œ์ œ๊ณฑ ๊ณผ์ •์—์„œ ๋ฌธ์ œ๊ฐ€ ๋ฐœ์ƒํ•˜๋Š” ์งˆ์  ์—ฐ๊ฒฐ์„ฑ์— ๋Œ€ํ•œ ๋ฐฉํ–ฅ ์ œ์•ฝ์กฐ๊ฑด์„ ๊ฐ€ํ•˜๋Š” ์ •๋ ฌ ๊ธฐํ•˜ํ•™์  ๋ณด์กด ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•(AGC-LSM)์„ ๊ฐœ๋ฐœํ•˜์˜€์œผ๋ฉฐ ์ œ์•ˆ ๊ธฐ๋ฒ•์€ ๋‹ค์ฐจ์› ์ž„์˜์˜ ์งˆ์  ๋ถ„ํฌ ๋ฐ ์—ฐ๊ฒฐ์„ฑ ๊ตฌ์กฐ์— ํšจ๊ณผ์ ์œผ๋กœ ์ ์šฉ๋  ์ˆ˜ ์žˆ๋‹ค. ํ•ด๋‹น ๊ตฌ์กฐ๋ฅผ ๊ฐ€์ง€๋Š” ๊ฒฉ์ž ๋ฐ ์งˆ์ ์—์„œ ์ œ์•ˆ ๊ธฐ๋ฒ•๊ณผ ๊ธฐ์กด ๊ธฐ๋ฒ•, ๊ทธ๋ฆฌ๊ณ  ๋น„์ •๋ ฌ ์œ ํ•œ์ฒด์ ๋ฒ•(Unstructured FVM)์˜ ์ˆ˜์น˜ ๊ฒฐ๊ณผ ๋น„๊ต ๊ฒ€์ฆ์„ ์ˆ˜ํ–‰ํ•˜์˜€๊ณ  ์ œ์•ˆ ๊ธฐ๋ฒ•์˜ ์ •ํ™•๋„๊ฐ€ ๊ธฐ์กด ๊ธฐ๋ฒ• ๋Œ€๋น„ ํฌ๊ฒŒ ํ–ฅ์ƒ๋˜์—ˆ์œผ๋ฉฐ ๋น„์ •๋ ฌ ์œ ํ•œ์ฒด์ ๋ฒ• ๊ฒฐ๊ณผ๋ฅผ ์ถฉ๋ถ„ํžˆ ๋™์ผํ•˜๊ฒŒ ๋ชจ์‚ฌํ•˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ํฐ ์ข…ํšก๋น„ ๋ฐ ๊ณก๋ฅ  ์งˆ์  ๋ถ„ํฌ๊ฐ€ ํ•„์—ฐ์ ์œผ๋กœ ๋ฐœ์ƒํ•˜๋Š” ์ผ๋ฐ˜์ ์ธ ์ •์ƒ์ƒํƒœ ๋‚œ๋ฅ˜ ์œ ๋™ ํ•ด์„์—์„œ ๋ณธ ์ œ์•ˆ ๊ธฐ๋ฒ•์„ ์ ์šฉํ•˜์—ฌ ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•์˜ ์ •ํ™•ํ•œ ๋‚œ๋ฅ˜ ๊ฒฝ๊ณ„์ธต ํ•ด์„ ๋Šฅ๋ ฅ์„ ํ™•๋ณดํ•˜์˜€๋‹ค.In this study, cause analysis and improved meshless method were developed to solve the problems that existing meshless method show non-physical and inaccurate results under point cloud with large aspect ratio and curvature. Based on the characteristics shared by geometric conservation least squares method(GC-LSM) and unstructured finite volume methods, the Lagrange multiplier was used to develop aligned geometric conservation least squares method(AGC-LSM) that impose direction constraints on problematic connectivity in the least squares process, and the proposed method can be effectively applied to any multidimensional point distribution and connectivity. The comparison and verification of the numerical results of the proposed method, the existing method, and the unstructured FVM were performed under the mesh that have high aspect ratio and curvature, propsed method shows improved result compare to existing method and shows sufficiently comparable results to those of FVM. In general steady-state turbulent flow analysis, where high aspect ratio and curvature point distributions inevitably occur, the proposed method could be applied to obtain the accurate and robust turbulent boundary layer analysis ability of the meshless method.์ œ 1 ์žฅ ์„œ ๋ก  1 ์ œ 1 ์ ˆ ์—ฐ๊ตฌ์˜ ๋ฐฐ๊ฒฝ 1 ์ œ 2 ์ ˆ ์—ฐ๊ตฌ์˜ ํ•„์š”์„ฑ 3 ์ œ 3 ์ ˆ ๊ฐœ์„ ๊ธฐ๋ฒ• ๊ธฐ์ค€ 4 ์ œ 2 ์žฅ ์ˆ˜์น˜๊ธฐ๋ฒ• 5 ์ œ 1 ์ ˆ ์ง€๋ฐฐ๋ฐฉ์ •์‹ 5 ์ œ 2 ์ ˆ ์ตœ์†Œ์ œ๊ณฑ๋ฒ• ๊ธฐ๋ฐ˜ ๋ฌด๊ฒฉ์ž ๊ณต๊ฐ„ ์ฐจ๋ถ„ 6 ์ œ 3 ์ ˆ ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•๊ณผ ์œ ํ•œ์ฒด์ ๋ฒ•์˜ ์ƒ์‚ฌ 12 ์ œ 4 ์ ˆ ์ •๋ ฌ ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ• 14 ์ œ 5 ์ ˆ ๊ทธ ์™ธ ์ˆ˜์น˜๊ธฐ๋ฒ• 25 ์ œ 3 ์žฅ ์ˆ˜์น˜๊ฒฐ๊ณผ 31 ์ œ 1 ์ ˆ ๋น„๊ต๊ตฐ ์ƒ์„ธ 31 ์ œ 2 ์ ˆ 2D Cylinder 31 ์ œ 3 ์ ˆ 2D Shock Tube 37 ์ œ 4 ์ ˆ 2D RAE2822 Airfoil 44 ์ œ 5 ์ ˆ 3D ONERA M6 Wing 50 ์ œ 4 ์žฅ ๊ฒฐ ๋ก  60 ์ฐธ๊ณ  ๋ฌธํ—Œ 61 Abstract 63์„

    Game theoretic approach to a mechanism design for transfer pricing by MNC

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธๅคงๅญธๆ ก ๅคงๅญธ้™ข :็ถ“็‡Ÿๅญธ็ง‘ ็ถ“็‡Ÿๅญธๅฐˆๆ”ป,1997.Docto

    Improved Meshless Method in Point Cloud with High Aspect Ratio and Curvature

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    ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ธฐ์กด ๋ฌด๊ฒฉ์ž ๊ณต๊ฐ„ ์ฐจ๋ถ„ ํ•ด์„ ๊ธฐ๋ฒ•์ด ํฐ ์ข…ํšก๋น„ ๋ฐ ๊ณก๋ฅ ์„ ๊ฐ€์ง€๋Š” ์งˆ์  ๋ถ„ํฌ์—์„œ์˜ ์œ ๋™ ํ•ด์„์—์„œ ๊ณก๋ฅ  ๋ฐฉํ–ฅ ์œ ๋™ ๊ฐ€์† ๋“ฑ์˜ ํ˜•ํƒœ๋กœ ๋‚˜ํƒ€๋‚˜๋Š” ๋น„๋ฌผ๋ฆฌ์ ์ด๊ณ  ๋ถ€์ •ํ™•ํ•œ ๊ฒฐ๊ณผ๋ฅผ ๋ณด์ด๋Š” ๋ฌธ์ œ์ ์„ ํ•ด๊ฒฐํ•˜๊ธฐ ์œ„ํ•ด ์›์ธ ๋ถ„์„ ๋ฐ ๊ฐœ์„  ๊ธฐ๋ฒ• ๊ฐœ๋ฐœ์„ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ๊ธฐ์กด ๊ธฐํ•˜ํ•™์  ๋ณด์กด ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•(GC-LSM)๊ณผ ๋น„์ •๋ ฌ ์œ ํ•œ ์ฒด์ ๋ฒ•์ด ๊ณต์œ ํ•˜๋Š” ํŠน์„ฑ์œผ๋กœ๋ถ€ํ„ฐ ์ฐฉ์•ˆํ•˜์—ฌ ๋ผ๊ทธ๋ž‘์ฃผ ์Šน์ˆ˜๋ฒ•์„ ์ด์šฉํ•ด ์ตœ์†Œ์ œ๊ณฑ ๊ณผ์ •์—์„œ ๋ฌธ์ œ๊ฐ€ ๋ฐœ์ƒํ•˜๋Š” ์งˆ์  ์—ฐ๊ฒฐ์„ฑ์— ๋Œ€ํ•œ ๋ฐฉํ–ฅ ์ œ์•ฝ์กฐ๊ฑด์„ ๊ฐ€ํ•˜๋Š” ์ •๋ ฌ ๊ธฐํ•˜ํ•™์  ๋ณด์กด ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•(AGC-LSM)์„ ๊ฐœ๋ฐœํ•˜์˜€์œผ๋ฉฐ ์ œ์•ˆ ๊ธฐ๋ฒ•์€ ๋‹ค์ฐจ์› ์ž„์˜์˜ ์งˆ์  ๋ถ„ํฌ ๋ฐ ์—ฐ๊ฒฐ์„ฑ ๊ตฌ์กฐ์— ํšจ๊ณผ์ ์œผ๋กœ ์ ์šฉ๋  ์ˆ˜ ์žˆ๋‹ค. ํ•ด๋‹น ๊ตฌ์กฐ๋ฅผ ๊ฐ€์ง€๋Š” ๊ฒฉ์ž ๋ฐ ์งˆ์ ์—์„œ ์ œ์•ˆ ๊ธฐ๋ฒ•๊ณผ ๊ธฐ์กด ๊ธฐ๋ฒ•, ๊ทธ๋ฆฌ๊ณ  ๋น„์ •๋ ฌ ์œ ํ•œ์ฒด์ ๋ฒ•(Unstructured FVM)์˜ ์ˆ˜์น˜ ๊ฒฐ๊ณผ ๋น„๊ต ๊ฒ€์ฆ์„ ์ˆ˜ํ–‰ํ•˜์˜€๊ณ  ์ œ์•ˆ ๊ธฐ๋ฒ•์˜ ์ •ํ™•๋„๊ฐ€ ๊ธฐ์กด ๊ธฐ๋ฒ• ๋Œ€๋น„ ํฌ๊ฒŒ ํ–ฅ์ƒ๋˜์—ˆ์œผ๋ฉฐ ๋น„์ •๋ ฌ ์œ ํ•œ์ฒด์ ๋ฒ• ๊ฒฐ๊ณผ๋ฅผ ์ถฉ๋ถ„ํžˆ ๋™์ผํ•˜๊ฒŒ ๋ชจ์‚ฌํ•˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ํฐ ์ข…ํšก๋น„ ๋ฐ ๊ณก๋ฅ  ์งˆ์  ๋ถ„ํฌ๊ฐ€ ํ•„์—ฐ์ ์œผ๋กœ ๋ฐœ์ƒํ•˜๋Š” ์ผ๋ฐ˜์ ์ธ ์ •์ƒ์ƒํƒœ ๋‚œ๋ฅ˜ ์œ ๋™ ํ•ด์„์—์„œ ๋ณธ ์ œ์•ˆ ๊ธฐ๋ฒ•์„ ์ ์šฉํ•˜์—ฌ ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•์˜ ์ •ํ™•ํ•œ ๋‚œ๋ฅ˜ ๊ฒฝ๊ณ„์ธต ํ•ด์„ ๋Šฅ๋ ฅ์„ ํ™•๋ณดํ•˜์˜€๋‹ค.In this study, cause analysis and improved meshless method were developed to solve the problems that existing meshless method show non-physical and inaccurate results under point cloud with large aspect ratio and curvature. Based on the characteristics shared by geometric conservation least squares method(GC-LSM) and unstructured finite volume methods, the Lagrange multiplier was used to develop aligned geometric conservation least squares method(AGC-LSM) that impose direction constraints on problematic connectivity in the least squares process, and the proposed method can be effectively applied to any multidimensional point distribution and connectivity. The comparison and verification of the numerical results of the proposed method, the existing method, and the unstructured FVM were performed under the mesh that have high aspect ratio and curvature, propsed method shows improved result compare to existing method and shows sufficiently comparable results to those of FVM. In general steady-state turbulent flow analysis, where high aspect ratio and curvature point distributions inevitably occur, the proposed method could be applied to obtain the accurate and robust turbulent boundary layer analysis ability of the meshless method.์ œ 1 ์žฅ ์„œ ๋ก  1 ์ œ 1 ์ ˆ ์—ฐ๊ตฌ์˜ ๋ฐฐ๊ฒฝ 1 ์ œ 2 ์ ˆ ์—ฐ๊ตฌ์˜ ํ•„์š”์„ฑ 3 ์ œ 3 ์ ˆ ๊ฐœ์„ ๊ธฐ๋ฒ• ๊ธฐ์ค€ 4 ์ œ 2 ์žฅ ์ˆ˜์น˜๊ธฐ๋ฒ• 5 ์ œ 1 ์ ˆ ์ง€๋ฐฐ๋ฐฉ์ •์‹ 5 ์ œ 2 ์ ˆ ์ตœ์†Œ์ œ๊ณฑ๋ฒ• ๊ธฐ๋ฐ˜ ๋ฌด๊ฒฉ์ž ๊ณต๊ฐ„ ์ฐจ๋ถ„ 6 ์ œ 3 ์ ˆ ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ•๊ณผ ์œ ํ•œ์ฒด์ ๋ฒ•์˜ ์ƒ์‚ฌ 12 ์ œ 4 ์ ˆ ์ •๋ ฌ ๋ฌด๊ฒฉ์ž ๊ธฐ๋ฒ• 14 ์ œ 5 ์ ˆ ๊ทธ ์™ธ ์ˆ˜์น˜๊ธฐ๋ฒ• 25 ์ œ 3 ์žฅ ์ˆ˜์น˜๊ฒฐ๊ณผ 31 ์ œ 1 ์ ˆ ๋น„๊ต๊ตฐ ์ƒ์„ธ 31 ์ œ 2 ์ ˆ 2D Cylinder 31 ์ œ 3 ์ ˆ 2D Shock Tube 37 ์ œ 4 ์ ˆ 2D RAE2822 Airfoil 44 ์ œ 5 ์ ˆ 3D ONERA M6 Wing 50 ์ œ 4 ์žฅ ๊ฒฐ ๋ก  60 ์ฐธ๊ณ  ๋ฌธํ—Œ 61 Abstract 63์„

    Spectrum of the ring of integer-valued polynomials on Z

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    Master์ •์—ญ D๊ฐ€ ์ฃผ์–ด์กŒ์„ ๋•Œ D[X]์™€ K[X]์‚ฌ์ด์˜ ํŠน๋ณ„ํ•œ ์„ฑ์งˆ์„ ๊ฐ–๋Š” ํ™˜ Int(D)๋ฅผ ์ •์˜ํ•˜๊ณ , ๊ทธ ์„ฑ์งˆ๋“ค์„ ์กฐ์‚ฌํ•˜์˜€๋‹ค. ๊ทธ๋ฆฌ๊ณ  Int(Z)์˜ ์†Œ์ด๋ฐ์•Œ๋“ค์„ ์™„๋ฒฝํžˆ ๋ถ„๋ฅ˜ํ•˜๋Š”๋ฐ ์ค‘์ ์„ ๋‘์—ˆ๋‹ค.Let D be a domain with quotient field K. Then we can define the ring of integer-valued polynomials on D, denoted by Int(D), which lies between D[X] and K[X] and we investigated the properties of Int(D). And we completely describe all prime ideals of Int(Z)
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