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    Crack Control and Performance Improvement for Pile to Concrete Pile-cap Connections of Integral Abutment Bridges

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    ์ตœ๊ทผ ๋Š˜์–ด๋‚˜๋Š” ๊ตํ†ต๋Ÿ‰๊ณผ ๋…ธํ›„ํ™”๋กœ ์ธํ•œ ๋งŽ์€ ๋ฌธ์ œ๋ฅผ ๋ฐœ์ƒ์‹œํ‚ค๊ณ  ์žˆ๋Š” ์กฐ์ธํŠธ ๊ต๋Ÿ‰์— ๋น„ํ•ด, ์œ ์ง€๊ด€๋ฆฌ ๋น„์šฉ์ด ์ €๋ ดํ•˜๊ณ  ์‹œ๊ณต์ด ๊ฐ„ํŽธํ•œ ์ผ์ฒดํ˜•๊ต๋Œ€๊ต๋Ÿ‰์˜ ์‹œ๊ณต ์‚ฌ๋ก€๊ฐ€ ๋Š˜์–ด๋‚˜๊ณ  ์žˆ๋‹ค. ๋ถ๋ฏธ์™€ ์œ ๋Ÿฝ์—์„œ๋Š” 10,000๊ฐœ ์ด์ƒ์˜ ์ผ์ฒดํ˜• ๊ต๋Œ€๊ต๋Ÿ‰์ด ์‚ฌ์šฉ์ค‘์— ์žˆ์œผ๋‚˜(Arockiasamy et al. 2004) ๊ตญ๋‚ด์—์„œ๋Š” ์‹œ๊ณต ์‚ฌ๋ก€๊ฐ€ ์ ์„ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ, ์ด์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋„ ๋ฏธ๋ฏธํ•œ ์‹ค์ •์ด๋‹ค. ์ผ์ฒดํ˜• ๊ต๋Œ€ ๊ต๋Ÿ‰์€ ์กฐ์ธํŠธ๋ฅผ ์ œ์™ธํ•˜๊ณ  ๊ต๋Œ€์™€ ์ƒ๋ถ€๊ตฌ์กฐ๋ฌผ์„ ์ผ์ฒดํ˜•์œผ๋กœ ์‹œ๊ณตํ•œ ๊ต๋Ÿ‰์„ ๋งํ•œ๋‹ค. ๊ธฐ์กด์˜ ์กฐ์ธํŠธ ๊ต๋Ÿ‰์€ ์‹ ์ถ•์ด์Œ์žฅ์น˜์˜ ์ฐจ๋Ÿ‰ ์ถฉ๊ฒฉ์— ์˜ํ•œ ํŒŒ์†๊ณผ ์ด๋ฅผ ํ†ตํ•œ ๋ˆ„์ˆ˜ ๋ฐ ์ œ์„ค์ œ์˜ ์นจํˆฌ๋กœ ๊ต์ขŒ์žฅ์น˜์˜ ์ž‘๋™ ๋ถˆ๋Šฅ, ์žฆ์€ ํŒŒ์†์œผ๋กœ ์ธํ•œ ๊ตํ†ต ์žฅ์• ์™€ ๋ณด์ˆ˜๋น„์šฉ์˜ ์ฆ๊ฐ€, ์‹ ์ถ•์ด์Œ์žฅ์น˜ ๋ฐ ๊ต์ขŒ์žฅ์น˜์˜ ์„ค๊ณ„/์‹œ๊ณต์œผ๋กœ ์ธํ•œ ์‹œ์„ค๋น„์šฉ์˜ ์ฆ๊ฐ€, ์ƒ๋ถ€๊ตฌ์กฐ์™€ ํ•˜๋ถ€๊ตฌ์กฐ์˜ ์—ฐ๊ฒฐ๋ถ€์—์„œ ์ง€์ง„ํ•˜์ค‘, ํ’ํ•˜์ค‘์— ๋Œ€ํ•œ ํšก๋ฐฉํ–ฅ ์ €ํ•ญ์„ฑ ์ทจ์•ฝ ๋“ฑ์˜ ๋ฌธ์ œ์ ์„ ๋…ธ์ถœ์‹œ์ผœ ์™”๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์ผ์ฒดํ˜• ๊ต๋Œ€๊ต๋Ÿ‰์€ ์‹ ์ถ•์ด์Œ์žฅ์น˜์˜ ์ œ๊ฑฐ๋ฅผ ํ†ตํ•ด ์ด๋Ÿฌํ•œ ๋ฌธ์ œ์ ์„ ๊ฐœ์„ ํ•  ์ˆ˜ ์žˆ๋‹ค. ํ•˜์ง€๋งŒ ์ด๋Ÿฌํ•œ ์ผ์ฒดํ˜• ๊ต๋Œ€ ๊ต๋Ÿ‰์€ ๋ฐ˜๋ณต์ ์ธ ์˜จ๋„ํ•˜์ค‘์— ๋”ฐ๋ฅธ ํ† ์งˆ๊ณผ ํŒŒ์ผ์˜ ์ƒํ˜ธ์ž‘์šฉ์— ์˜ํ•ด ํŒŒ์ผ-๊ต๋Œ€ ์—ฐ๊ฒฐ๋ถ€์— ๋ฐœ์ƒํ•˜๋Š” ๊ท ์—ด์ด ๋ฌธ์ œ์ ์œผ๋กœ ์ง€์ ๋˜์–ด ์™”๋‹ค. ๋ฏธ๊ตญ๊ณผ ์œ ๋Ÿฝ์—์„œ๋Š” ๋งŽ์€ ์—ฐ๊ตฌ๊ฐ€ ์ง„ํ–‰๋˜์–ด ์ผ์ฒด์‹ ๊ต๋Œ€ ๊ต๋Ÿ‰์˜ ๊ฑฐ๋™ ๋ฐ ์„ค๊ณ„ํŠน์„ฑ์„ ํŒŒ์•…ํ•˜๊ณ  ์ด๋ฅผ ํ™œ์šฉํ•˜์—ฌ ์„ค๊ณ„๋ฅผ ์‹œ๋„ํ•˜๊ณ  ์žˆ์œผ๋‚˜ ๊ตญ๋‚ด์˜ ๋„๋กœ๊ต์„ค๊ณ„๊ธฐ์ค€ (2012)์—์„œ๋Š” ์•„์ง ์ผ์ฒด์‹ ๊ต๋Œ€ ๊ต๋Ÿ‰์˜ ์„ค๊ณ„ ์ง€์นจ์— ๊ด€ํ•œ ์–ธ๊ธ‰์ด ์ „๋ฌดํ•œ ์‹ค์ •์ด๋ฉฐ 1980๋…„์— ๋ฐœ๊ฐ„๋œ ๋ฏธ๊ตญ FHWA Technical Advisory T 5140.13 (1980)์˜ ์ถ”์ฒœ์‚ฌํ•ญ์— ๋Œ€ํ•œ ์–ธ๊ธ‰๋งŒ ๋˜์–ด์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ผ์ฒดํ˜• ๊ต๋Œ€๊ต๋Ÿ‰์˜ ์„ค๊ณ„์™€ ์—ฐ๊ตฌ์˜ ์ง„ํ–‰์— ๋„์›€์ด ๋˜๊ณ ์ž, ์ผ์ฒดํ˜• ๊ต๋Œ€ ๊ต๋Ÿ‰์—์„œ ๋ฐœ์ƒ ๊ฐ€๋Šฅํ•œ ๊ท ์—ด์˜ ํ˜•์ƒ์„ ์˜ˆ์ธกํ•˜๊ณ  ๊ท ์—ด ๋ฐœ์ƒ์„ ์ €๊ฐํ•˜๊ธฐ ์œ„ํ•œ ์ฒ ๊ทผ ์ƒ์„ธ ๋˜๋Š” ์—ฐ๊ฒฐ๋ถ€ ์ƒ์„ธ๋ฅผ ์ œ์•ˆํ•˜์˜€๋‹ค. ๋˜ํ•œ, ๊ต๋Œ€-ํŒŒ์ผ ์—ฐ๊ฒฐ๋ถ€ ๋ณด๊ฐ•์— ํšจ๊ณผ์ ์ธ ๊ฒƒ์œผ๋กœ ํ™•์ธ๋œ ๋‚˜์„  ์ฒ ๊ทผ ํ˜•์ƒ์˜ ๋ณ€์ˆ˜์—ฐ๊ตฌ๋ฅผ ํ†ตํ•ด ์ฃผ์š” ๋ณ€์ˆ˜๋ฅผ ํ™•์ธํ•˜์˜€๋‹ค. ์ œ์•ˆ๋œ ์—ฐ๊ฒฐ๋ถ€๋Š” ํฌ๊ฒŒ ๊ต๋Œ€ ์ž์ฒด์˜ ๊ฐ•์„ฑ์„ ๋†’์ด๋Š” ๋ฐฉ๋ฒ•๊ณผ ๊ฐ•์„ฑ์„ ์ค„์ด๊ณ  ์ผ์ •๋Ÿ‰์˜ ๋ณ€์œ„๋ฅผ ํ—ˆ์šฉํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์‚ฌ์šฉํ•˜์˜€์œผ๋ฉฐ ๊ฐ•์„ฑ์„ ๋†’์ด๋Š” ๋ฐฉ๋ฒ•์—๋Š” ์—ฐ๊ฒฐ๋ถ€์— ๋‚˜์„  ์ฒ ๊ทผ์„ ์‚ฝ์ž…ํ•˜๋Š” ๊ฒƒ์ด ํšจ๊ณผ์ ์œผ๋กœ ํ™•์ธ๋˜์—ˆ์œผ๋ฉฐ ๊ฐ•์„ฑ์„ ์ค„์ด๊ณ  ์ผ์ •๋Ÿ‰์˜ ๋ณ€์œ„๋ฅผ ํ—ˆ์šฉํ•˜๋Š” ๋ฐฉ๋ฒ•์—๋Š” ์ง€์ค‘์— ์‚ฝ์ž…๋˜๋Š” H ํŒŒ์ผ์˜ ํ”Œ๋žœ์ง€๋ฅผ ๊ฐ์†Œ์‹œํ‚ค๋Š” ๋ฐฉ๋ฒ•๊ณผ, ๋ณ€์œ„๋ฅผ ํ—ˆ์šฉํ•˜๋Š” ์—ฐ๊ฒฐ๋ถ€๊ฐ€ ์ผ์ฒด์‹ ๊ต๋Œ€๊ต๋Ÿ‰์˜ ๊ท ์—ด๋ฐฉ์ง€์— ํšจ๊ณผ์ ์ธ ๊ฒƒ์œผ๋กœ ๋‚˜ํƒ€๋‚ฌ๋‹ค. ๋˜ํ•œ ์ œ์•ˆ๋œ ์—ฐ๊ฒฐ๋ถ€๋Š” ๊ต๋Œ€๋กœ๋ถ€ํ„ฐ ์ „๋‹ฌ๋˜๋Š” ์ƒ๋ถ€๊ตฌ์กฐ๋ฌผ์˜ ๋ฐ˜๋ ฅ์„ ๊ฐ์†Œ์‹œ์ผœ ์ƒ๋ถ€๊ตฌ์กฐ์˜ ๋‚ด๊ตฌ์„ฑ ๋ฐ ๊ตฌ์กฐ๊ฑด์ „์„ฑ๋„ ํ•จ๊ป˜ ํ–ฅ์ƒ์‹œํ‚ค๋Š” ๊ฒƒ์œผ๋กœ ํ™•์ธ๋˜์—ˆ๋‹ค.TABLES OF CONTENTS List of Tables List of Figures Abstract Chapter 1 Introduction 1.1 Problem Statement 1.2 Objectives 1.3 Research Significance 1.4 Research Methodology Chapter 2 Literature Review 2.1 Research about IA bridges 2.1.1 Research about Structural Performance of Integral Abutment Bridges 2.1.2 Research about Thermal Loads in Integral Abutment Bridges 2.2 Numerical Model 2.3 Summary of Literature Review Chapter 3 Theoretical Background 3.1 Material Model for Concrete 3.2 Material Model for Steel Rebar and H-pile 3.3 Contact Chapter 4 Numerical Analysis 4.1 Numerical Model Development 4.1.1 Description of Numerical Model 4.1.2 Numerical Model Setup 4.1.3 Verification of Numerical Model 4.2 Performance of Various Boundary Conditions 4.2.1 Structural Performance depending on Embedded Length 4.2.2 Behavior of IA Bridges according to Various Boundary Conditions 4.3 Proposed Pile-to-pilecap Connection 4.3.1 Proposed Pile-to-pilecap Increased Stiffness Connection Type 4.3.2 Proposed Pile-to-pilecap Flexible Connection Types 4.3.3 Obtained Results of Increased Stiffness Connection Types 4.3.4 Obtained Results of Flexible Connection Types 4.3.5 Comparison of Load-displacement Curves 4.4 Parametric Study 4.4.1 Parameter of Parametric Study 4.4.2 Results of Parametric Study 4.5 Superstructure Model 4.5.1 Development of Superstructure Model 4.5.2 The Results of Increased Stiffness Superstructure Model 4.5.3 The Results of Flexible Superstructure Model 5. Conclusions and Recommendations 5.1 Conclusions from Proposed Connections 5.2 Conclusions from Parametric Study 5.3 Conclusions from Superstructure Model 5.4 Recommendations for Further Study Acknowledgement Bibliograph

    ํ˜ˆ๊ด€์ข… ํ‡ด์ถ• ๊ณผ์ •์—์„œ pigment epithelium-derived factor์˜ ์—ญํ• ์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์˜๊ณผํ•™๊ณผ, 2014. 8. ์กฐ์ •ํ˜„.์„œ๋ก : ํ˜ˆ๊ด€์ข…์€ ์–‘์„ฑ์ข…์–‘์œผ๋กœ์„œ ํ˜ˆ๊ด€์˜ ๋น„์ •์ƒ์ ์ธ ์„ฑ์žฅ์œผ๋กœ ์ธํ•ด ์ƒ๊ฒจ๋‚œ๋‹ค. ๊ฐ€์žฅ ๋Œ€ํ‘œ์ ์ธ ํ˜ˆ๊ด€์ข…์€ ์œ ์•„ ํ˜ˆ๊ด€์ข…์ด๋ฉฐ ์ฃผ๋กœ ํƒœ์–ด๋‚œ ํ›„์— ๋ฐœ์ƒํ•˜๊ณ  ๋ฐœ๋ณ‘ ์›์ธ์€ ์•„์ง ์•Œ๋ ค์ ธ ์žˆ์ง€ ์•Š๋‹ค. ๋‹ค๋ฅธ ์ข…์–‘๊ณผ ๋‹ฌ๋ฆฌ ํ˜ˆ๊ด€์ข…์€ ์ดˆ๊ธฐ ๋‹จ๊ณ„์— ์ฆ์‹์„ ํ•˜๊ณ  ํ›„์—๋Š” ํ‡ด์ถ•๊ธฐ๋ฅผ ๊ฑฐ์น˜๋ฉด์„œ ์„œ์„œํžˆ ์‚ฌ๋ผ์ง€๊ฒŒ ๋œ๋‹ค. ์ด๋Ÿฌํ•œ ํ˜ˆ๊ด€์ข… ํ‡ด์ถ• ๊ณผ์ •์€ ์ž˜ ์•Œ๋ ค์ ธ ์žˆ์ง€ ์•Š์€ ์ƒํƒœ์ด๋ฉฐ ์—ฐ๊ตฌ๊ฐ€ ์ง„ํ–‰์ด ๋˜๊ณ  ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์˜ ๊ฐ€์„ค์€ ํ˜ˆ๊ด€์ข… ํ‡ด์ถ•๊ธฐ์˜ ์›์ธ์œผ๋กœ์„œ ํŠน์ • ์š”์†Œ๊ฐ€ ํ˜ˆ๊ด€๋‚ดํ”ผ์„ธํฌ์— ์ž‘์šฉํ•  ๊ฒƒ์œผ๋กœ ์˜ˆ์ƒ๋œ๋‹ค. ์—ฐ๊ตฌ ๋ชฉ์ ์€ ํ‡ด์ถ•๊ธฐ์˜ ์ž‘์šฉํ•˜๋Š” ๊ทธ ํŠน์ • ์š”์†Œ๋ฅผ ํ™•์ธํ•˜๊ณ  ํ˜ˆ๊ด€์ข… ๋‚ดํ”ผ์„ธํฌ์˜ ์–ด๋– ํ•œ ์ž‘์šฉ์„ ์ผ์œผํ‚ค๋Š”์ง€ ๊ด€์ธกํ•˜๋Š” ๊ฒƒ์ด๋‹ค. ๋ฐฉ๋ฒ•: ํ˜ˆ๊ด€์ข… ํ™˜์ž๋กœ๋ถ€ํ„ฐ ํ˜ˆ๊ด€์ข… ์ƒ˜ํ”Œ์„ ์–ป๊ณ  ํ˜ˆ๊ด€๋‚ดํ”ผ์„ธํฌ๋ฅผ ์ถ”์ถœ์„ ํ•œ ํ›„, ์ฆ์‹๊ธฐ ๋ฐ ํ‡ด์ถ•๊ธฐ ๊ฐ„์˜ ์„ธํฌ ์ฆ์‹๋ฅ ๊ณผ PCR ๋ฐ ๋‹จ๋ฐฑ์งˆ array๋ฅผ ํ†ตํ•ด ๊ฐ์ข… ํ˜ˆ๊ด€์ƒ์„ฑ ๋ฐ ํ˜ˆ๊ด€์ƒ์„ฑ์–ต์ œ ์š”์†Œ๋“ค์˜ ๋ฐœํ˜„๋Ÿ‰์˜ ์ฐจ์ด๋ฅผ ๊ด€์ธกํ•˜์˜€๋‹ค. ์ถ”๊ฐ€๋กœ ํ˜ˆ๊ด€์ข… ์กฐ์ง์œผ๋กœ๋ถ€ํ„ฐ ๋ฉด์—ญ์กฐ์งํ™”ํ•™์—ผ์ƒ‰์„ ํ•˜์˜€๋‹ค. ๊ฒฐ๊ณผ: ํ˜ˆ๊ด€์ข… ๋‚ดํ”ผ์„ธํฌ์—์„œ ์ž์‹ ์˜ ์ฆ์‹์„ ์–ต์ œํ•˜๋Š” ์ž๊ฐ€๋ถ„๋น„ ์š”์†Œ๋ฅผ ๋ฐœ๊ฒฌํ•˜์˜€๋‹ค. ์—ฌ๋Ÿฌ ํ˜ˆ๊ด€์ƒ์„ฑ ๋ฐ ํ˜ˆ๊ด€์ƒ์„ฑ์–ต์ œ ์š”์†Œ๋“ค ์ค‘์—์„œ pigment epithelium-derived factor (PEDF)๋ผ๋Š” ์š”์†Œ๊ฐ€ ํ˜ˆ๊ด€์ข… ํ‡ด์ถ•๊ธฐ์—์„œ ์ƒ๋Œ€์ ์œผ๋กœ ๋งŽ์€ ๋ฐœํ˜„๋Ÿ‰์„ ๊ด€์ธกํ•˜์˜€๋‹ค. ์ด PEDF๋Š” ํ˜ˆ๊ด€์ข… ๋‚ดํ”ผ์„ธํฌ์˜ ์ฆ์‹์„ ์–ต์ œํ•˜๋Š” ํšจ๊ณผ๋ฅผ ๋ณด์˜€๊ณ  PEDF์˜ knockdown์„ ํ†ตํ•ด ์–ต์ œ๋˜์—ˆ๋˜ ์„ธํฌ ์ฆ์‹์ด ๋‹ค์‹œ ํšŒ๋ณตํ•˜๋Š” ํ˜„์ƒ์„ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ๋˜ํ•œ ํ˜ˆ๊ด€์ข… ์กฐ์ง์—ผ์ƒ‰์„ ํ†ตํ•ด PEDF๊ฐ€ ํ‡ด์ถ•๊ธฐ์—์„œ ์ƒ๋Œ€์ ์œผ๋กœ ๋งŽ์ด ๋ฐœํ˜„ํ•˜๋Š” ๊ฒƒ์„ ์žฌ์ฐจ ํ™•์ธ ํ•˜์˜€๋‹ค. ๊ฒฐ๋ก : PEDF๋Š” ํ˜ˆ๊ด€์ข… ํ‡ด์ถ•๊ธฐ์— ๋งŽ์€ ๋ฐœํ˜„๋Ÿ‰์„ ๋ณด์ด๋ฉฐ ํ˜ˆ๊ด€์ƒ์„ฑ์–ต์ œ ์š”์†Œ๋กœ์„œ ํ˜ˆ๊ด€๋‚ดํ”ผ์„ธํฌ์˜ ์ฆ์‹์„ ์–ต์ œํ•œ๋‹ค. ๋”ฐ๋ผ์„œ PEDF๋Š” ํ˜ˆ๊ด€์ข… ํ‡ด์ถ• ๊ณผ์ •์—์„œ ์ค‘์š”ํ•œ ์—ญํ• ์„ ๋งก๊ณ  ์žˆ์œผ๋ฉฐ ์ถ”ํ›„ ํ˜ˆ๊ด€์ข…์˜ ์›์ธ ๋˜๋Š” ์น˜๋ฃŒ์ œ ์—ฐ๊ตฌ์— ์ ํ•ฉํ•œ ์—ฐ๊ตฌ๋Œ€์ƒ์ด๋ผ๊ณ  ์ƒ๊ฐ๋œ๋‹ค.Introduction: Hemangioma is a type of vascular tumor resulting from abnormal growth of blood vessels which the cause is unknown. Compared to other vascular tumors, this benign tumor is commonly found in infancy. Hemangioma is distinctive because of its proliferation during the early stage, however, followed by involution where the tumor undergoes regression. The critical onset which proceeds to involution is not well understood and only minor research are evident regarding the involution process. Therefore, this study is centered on the mechanism of the involution of hemangioma. Through this study, I have identified an anti-angiogenic factor called pigment epithelium-derived factor (PEDF) which was found to be highly expressed during the involution phase. Methods: Endothelial cells were extracted from tissues of hemangioma patients and sorted using CD31 antibodies. Then, I observed the cellular growth rate of the hemangioma-derived endothelial cells (HemECs), and screened for pro- and anti-angiogenic factors using an angiogenesis array. Furthermore, I used hemangioma tissue samples for immunochemical staining. Results: I have identified pigment epithelium-derived factor, (PEDF) an anti-angiogenic factor, to be associated with the growth inhibition of hemangioma-derived endothelial cells (HemECs). Also, I have examined that suppression of PEDF restored cell growth in the involuting phase of HemECs. Furthermore, I have confirmed in vivo by immunochemical staining that PEDF was highly expressed, mainly in the involuting phase of hemangioma tissues. Conclusions: These results suggest that PEDF plays a role in the involution of hemangioma by inhibiting the proliferation of HemEC. The regulatory mechanism of PEDF expression as an anti-angiogenic factor could be a potential therapeutic target to treat hemangiomas.Abstract i Contents iii List of tables and figures iv List of abbreviations v Introduction 1 Material and Methods 4 Results 8 Discussion 23 References 28 Abstract in Korean 32Maste

    Strategic Pricing Behavior of Channel Members Before and After the Horizontal Merger Between Manufacturers

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ฒฝ์˜ํ•™๊ณผ, 2012. 8. ์†ก์ธ์„ฑ.In this research, I study the interactions between several manufacturers and one common retailer, focusing on their pricing behavior. Particularly, I try to uncover the nature of the retailer-manufacturer interaction before and after a horizontal merger between two manufacturers in the toilet tissue market. I take a new empirical industrial organization approach, specifying consumer and firm behaviors and using the notion of equilibrium. For the demand side, I apply the random coefficient logit model. The estimation strategy uses simulation and contraction mapping suggested by Berry, Levinsohn, and Pakes (1995). While they estimated demand and cost equations simultaneously, I follow a two-step approach suggested by Chintagunta, Bonfrer, and Song (2002). For the supply side, using the estimate results obtained from the demand equation, I recover price-cost margins and estimate cost parameters under three different gamesโ€•vertical Nash, manufacturer Stackelberg, and retailer Stackelbergโ€•to determine which game fits the data best. Additionally, I introduce a conduct parameter in the model in case the three discrete games are not sufficient to capture a wide enough range of possible interactions. As a result of the nonnested hypothesis test, the conduct parameter model fits the data best. By examining the change in the value of conduct parameters, I find that the merging firm became tougher in its pricing. This implies that the manufacturer priced more competitively trying to increase its price-cost margin. Conversely, the manufacturer whose market share was the lowest behaved in a more accommodating manner toward the retailer resulting in the manufacturer's lower price-cost margin than before the merger. The results suggest that the retailer-manufacturer interaction is heterogeneous across manufacturers. This research shows that channel members are interacting with one another and they devise different strategies depending on the market structure they are confronting.1. introduction 2. Literature Review 3. The Model 4. Estimation Procedure 5. Data 6. Results 7. ConclusionsMaste

    Fundamental research for introducing the probabilistic flood forecasting to Korea

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ฑด์„คํ™˜๊ฒฝ๊ณตํ•™๋ถ€, 2011.2. ๊น€์˜์˜ค.Maste

    Real-time control of neoclassical tearing mode in time-dependent simulations on tokamak plasmas

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์—๋„ˆ์ง€์‹œ์Šคํ…œ๊ณตํ•™๋ถ€, 2011.8. ๋‚˜์šฉ์ˆ˜.Maste

    Beliefs about gifted education and classroom practice of the science teachers at science academy in Korea

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ณผํ•™๊ต์œก๊ณผ ์ง€๊ตฌ๊ณผํ•™์ „๊ณต,2005.Docto

    LNG ํ”Œ๋žœํŠธ์˜ Fractionation ๊ณต์ •์˜ ๋ชจ๋ธ๋ง ๋ฐ ์‹œ๋ฎฌ๋ ˆ์ด์…˜

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2011.8. ํ•œ์ข…ํ›ˆ.Maste

    Plasma Current and Pressure Profile Effects on Tearing Mode Onset in Steady-state Hybrid Scenarios on DIII-D Tokamak

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์—๋„ˆ์ง€์‹œ์Šคํ…œ๊ณตํ•™๋ถ€, 2017. 2. ๋‚˜์šฉ์ˆ˜.Tearing mode (TM) instability is a kind of resistive magnetohydrodynamic instability that limits the performance of the tokamak plasma. A correct understanding of this phenomenon is essential for high performance steady-state operation, especially the onset of TMs. Based on the steady-state hybrid experiments performed on the DIII-D device, the occurrence of TM is identified and analyzed, and the effect of the plasma current and the pressure profiles on the tearing stability is investigated in terms of the tearing stability index โˆ†". The characteristics of the mode is mainly investigated using the system of magnetic pick-up Mirnov probes. The FFT analysis and the phase-fitting method are applied to identify the mode onset, the mode amplitude, and the mode number in the experiments. The mode onset was defined for this thesis that the phasefolding disappears in the phase-fitting results of poloidal probe array. Since the tearing stability is sensitive to the equilibrium current and pressure profiles, the more accurate and tightly constrained equilibrium is reconstructed using the well-measured plasma profiles using various diagnostics for the discharges in the database. The characteristics of plasma current and pressure profiles at tearing mode onset in the database of DIII-D steady-state hybrid discharges seems to be more sensitive to the global feature of plasma profile through li and fp, and the effect of plasma resistivity at the mode surface through '( than the local feature of plasma profile through Lq and Lp. From the result of the best fit equation in the dimensionless form using rs and 'TA the global feature of profiles and the current profile can affect more than the local feature of profiles and the pressure profile, respectively. The tearing stability index โˆ†" is calculated with the experimental equilibria in two ways, by MHD codes (PEST-III and resistive DCON) and by MRE. They are verified and validated in reasonable agreement. It is noteworthy that the determined โˆ†โ€ฒ can be positive regardless of the mode onset, so the conventional wisdom of โˆ†" > 0 for tearing destabilization may not be the sufficient condition, rather a positive value greater than a certain threshold could replace this under the toroidal geometry. The analytical formula of the tearing stability threshold โˆ†1 " is reviewed for the semi-collisional regime and the collisionless banana regime. By comparing the analytical โˆ†1 " with the โˆ†" calculated from PEST-III code near the TM onset, it is found that the condition of โˆ†" > โˆ†1 " is required for the mode onset in the experiment. A preliminary study on the โˆ†1 " estimation from the normalized mode growth rate is performed by NIMROD code. The โˆ†2 " can be fitted for negative or marginal growth rate using the relation between the normalized mode growth rate 3'- from NIMROD and the โˆ†" from PEST-III. Finally, a stability diagram of n = 1 tearing mode onset is suggested with local and global features of plasma profiles. Onset condition of n = 1 TM is analyzed by the difference between โˆ†" and โˆ†1 " , and its stability diagram is derived in terms of the local (โ–ฝ/II and โ–ฝp) and global (BN) variations for steady-state hybrid scenarios. To calculate โˆ†" โˆ’ โˆ†1 " for the stability diagram, a novel modeling package has been developed by integrating IPS/FASTRAN for equilibrium reconstruction, PEST-III/DCON for linear stability โˆ†" calculation, and the โˆ†1 " solver for analytical โˆ†1 " calculation. The stability boundary at the mode onset, โˆ†" = โˆ†1 " , is mapped on Lp-Lq diagram. Characteristics of this stability boundary show that the TM unstable area expands, then the stability boundary moves as BN increases. This stability diagram can be used to design and control experiments to avoid n = 1 TM.Chapter 1. Research background and objectives 1 1.1. Thermonuclear fusion in tokamak 2 1.2. Advanced operation scenarios for fusion reactor 7 1.3. Tearing instability in the steady-state hybrid scenarios 11 1.4. Physics of tearing mode 14 1.5. Objective and outline of this dissertation 18 Chapter 2. Experimental observations of tearing mode in DIII-D steady-state hybrid discharges 19 2.1. Identification of the tearing mode and its onset 23 2.2. Equilibrium reconstruction with kinetic measurements constraints โ€“ Kinetic EFIT 27 2.3. Characteristics of plasma current and pressure profiles at tearing mode onset 33 Chapter 3. Determination of tearing mode stability in terms of โˆ†โ€ฒ39 3.1. Numerical evaluation of tearing mode stability โˆ†โ€ฒ from the MHD codes 41 3.2. Experimental estimation of tearing mode stability โˆ†โ€ฒ from the modified Rutherford equation 45 3.3. Validation and verification of determined โˆ†โ€ฒ 47 Chapter 4. Determination of the onset condition for tearing mode in terms of โˆ†2" 51 4.1. Analysis of tearing instability threshold โˆ†> " 53 4.2. Comparison of โˆ†โ€ฒ with โˆ†> " for stable and unstable discharges of tearing mode 55 4.3. Estimation of โˆ†> " from the extended MHD simulation 59 Chapter 5. Development of tearing mode onset model 65 5.1. Descriptions of tearing mode onset model 66 5.2. Construction of modeled equilibrium with the parametric variations 68 5.3. Stability boundary for tearing mode onset on Lp-Lq diagram 71 Chapter 6. Conclusions 79 6.1. Summary and concluding remarks 80 6.2. Recommendations for future work 82 Bibliography 84 Abstract in Korean 90Docto

    (An) approach to Extension of Unified Modeling Language for Business Process Modeling

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