10 research outputs found

    A Study on the Equilibrium State of Nano-Scale System with Molecular Dynamics

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    Recently, we noticed the studies on the temperature boundary layer at a liquid-vapor interface, which reported that there exists the temperature difference over a liquid-vapor interface even though the system is at equilibrium state when the size of a system reduces to a micro-scale. The conclusion of those studies leaves a highly attractive question on whether the definition of equilibrium state should be changed in the case that the size of a system reduces to a nano-scale dimension. From the viewpoint of classical thermo -dynamics, if a system is at equilibrium state, the properties of interest should be measured as the same value within an instrument error. As example, the temperatures of a liquid and a vapor region are actually measured to be identical if they are in a saturated state. Although there are many molecular dynamics (MD) studies to survey the features of a liquid-vapor interface, a solid-liquid interface, or a solid-solid interface, there is no reported study that ascertains the temperature difference over a liquid-vapor interface at equilibrium state. In regard with the temperature discontinuity over an interface, which is the main focus of the present study, Maruyama et al. firstly observed the temperature jump at the solid-liquid interface that is called Kapitza resistance through the MD simulation when evaporation and condensation occur. In their study, they estimated the quantitative temperature jump at solid-liquid interface and calculated the equivalent liquid heat conduction thickness corresponding to an interface thermal resistance. Therefore, it is needed to confirm the temperature discontinuity over a liquid-vapor interface in an equilibrium two phase state. At present study, I clarified through the molecular dynamics method that the conclusions of the previous studies might be resulted from the misleading method to calculate the temperature profile. Molecular dynamics simulations compute the motions of individual molecules in models of solids, liquids, and gases. The key idea is motion which describes how positions, velocities, and orientations change with time. From this study, I suggest that there is no temperature discontinuity over a liquid-vapor interface independent of a system size if the system is in equilibrium state. Even though this research is contrary to other recent MD studies, the definition of an equilibrium state from classical thermodynamics can be still applicable to a nano-scale system if the approach is adopted.Abstract โ…ฒ ๊ทธ๋ฆผ ๋ชฉ์ฐจ โ…ด ํ‘œ ๋ชฉ์ฐจ โ…ท ์‚ฌ์šฉ๊ธฐํ˜ธ โ…ธ ์ œ1์žฅ ์„œ ๋ก  1 1.1 ์—ฐ๊ตฌ์˜ ๋ฐฐ๊ฒฝ 1 1.2 ์ข…๋ž˜์˜ ๊ด€๋ จ ์—ฐ๊ตฌ 5 1.3 ์—ฐ๊ตฌ์˜ ๋ชฉ์  9 ์ œ2์žฅ ๊ณ„์‚ฐ๋ฐฉ๋ฒ• 12 2.1 ๋ถ„์ž๋™์—ญํ•™๋ฒ• 12 2.2 ์˜จ๋„์˜ ์ •์˜ 27 2.3 ์˜จ๋„์ œ์–ด๋ฒ• 33 2.4 ์••๋ ฅ์˜ ์ •์˜ 36 2.5 ๊ณ„์‚ฐ๊ณ„์˜ ๊ตฌ์„ฑ 49 2.6 ๋„ค์ด๋ฒ„๋ฆฌ์ŠคํŠธ 57 ์ œ3์žฅ ๊ณ„์‚ฐ๊ฒฐ๊ณผ 61 3.1 ๋„ค์ด๋ฒ„๋ฆฌ์ŠคํŠธ์˜ ์˜ํ–ฅ 61 3.2 ๊ธฐ์•ก๊ณ„๋ฉด ๋ถ„์ž์˜ ์šด๋™ํŠน์„ฑ 72 3.3 ์˜จ๋„๊ฒฝ๊ณ„์ธต 86 3.4 ๋ฐ€๋„๊ฒฝ๊ณ„์ธต 103 ์ œ4์žฅ ๊ฒฐ๋ก  108 ์ฐธ๊ณ ๋ฌธํ—Œ 109 ๋ถ€๋ก 11

    ๋‘์œ ๋ฐ• ๋‹จ๋ฐฑ์งˆ ๊ฐ€์ˆ˜๋ถ„ํ•ด๋ฌผ์˜ ์ œ์กฐ์™€ ๊ทธ ํŠน์„ฑ ๊ตฌ๋ช…

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธๅคงๅญธๆ ก ๅคงๅญธ้™ข :้ฃŸๅ“ๅทฅๅญธ็ง‘,1995.Maste

    Design and Control of Three-phase Permanent Magnet Synchronous Machine Drive with Single or Dual Passive Components per Phase

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€,2020. 2. ํ•˜์ •์ต.๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ๋ฅผ ์ด์šฉํ•œ 3์ƒ ์˜๊ตฌ์ž์„ ๋™๊ธฐ ์ „๋™๊ธฐ์˜ ๊ตฌ๋™ ๋ฐฉ๋ฒ•์„ ์ œ์•ˆํ•œ๋‹ค. 3์ƒ ์˜๊ตฌ ์ž์„ ๋™๊ธฐ ์ „๋™๊ธฐ๋Š” ์†Œํ˜• ๊ฐ€์ „๋ถ€ํ„ฐ ์ „๊ธฐ ์ž๋™์ฐจ, ๋ฐœ์ „๊ธฐ ๋“ฑ์˜ ๋Œ€ํ˜• ์ „๋ ฅ ๋ณ€ํ™˜ ์‹œ์Šคํ…œ๊นŒ์ง€ ๋‹ค์–‘ํ•˜๊ฒŒ ์‚ฌ์šฉ๋˜๊ณ  ์žˆ๋‹ค. ์ตœ๊ทผ์—๋Š” ๋‹จ์ผ ์ „๋™๊ธฐ ๊ตฌ๋™์œผ๋กœ ๋‹ค์–‘ํ•œ ์šด์ „ ํŠน์„ฑ์„ ์š”๊ตฌํ•˜๋Š” ์‘์šฉ ๋ถ„์•ผ๊ฐ€ ์ฆ๊ฐ€ํ•˜๊ณ  ์žˆ๋‹ค. ํ•˜์ง€๋งŒ ๊ธฐ์กด์˜ 3์ƒ ์ธ๋ฒ„ํ„ฐ๋งŒ์œผ๋กœ๋Š” ์ „์•• ๋ฐ ์ „๋ฅ˜์˜ ์ œํ•œ์œผ๋กœ ์ธํ•ด ์ตœ๋Œ€ ์šด์ „ ์˜์—ญ์ด ์ œํ•œ๋œ๋‹ค. ์ „๋™๊ธฐ ๋ฐ ์ž…๋ ฅ ์ „์••์›์„ ์žฌ์„ค๊ณ„ํ•จ์œผ๋กœ์จ ์ด๋ฅผ ํ•ด๊ฒฐํ•  ์ˆ˜ ์žˆ์œผ๋‚˜, ๊ฐ€์ „ ์ œํ’ˆ๊ณผ ๊ฐ™์ด ๋Œ€๋Ÿ‰ ์ƒ์‚ฐ๋˜๋Š” ์‘์šฉ ๋ถ„์•ผ์—์„œ๋Š” ์„ค๋น„ ๋น„์šฉ์˜ ์ฆ๊ฐ€๋กœ ์ธํ•ด ์ด๋Ÿฌํ•œ ๋ฐฉ๋ฒ•์„ ์‚ฌ์šฉํ•  ์ˆ˜ ์—†๋‹ค. ์ด์™€ ๊ฐ™์ด ์ „๋™๊ธฐ์˜ ์žฌ์„ค๊ณ„๊ฐ€ ๋ถˆ๊ฐ€๋Šฅํ•  ๊ฒฝ์šฐ์—๋Š” ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๋ณ€๊ฒฝ์„ ํ†ตํ•ด ์šด์ „ ์˜์—ญ์„ ํ™•์žฅํ•ด์•ผ ํ•œ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ๋ฅผ ์ด์šฉํ•œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๋ณ€๊ฒฝ์„ ํ†ตํ•ด ์ „๋™๊ธฐ์˜ ์šด์ „ ์˜์—ญ์„ ํ™•์žฅํ•˜๊ธฐ ์œ„ํ•œ ๋ฐฉ๋ฒ•์„ ์ œ์•ˆํ•œ๋‹ค. ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ๋ฅผ 3์ƒ ์ธ๋ฒ„ํ„ฐ์™€ ์ „๋™๊ธฐ ์‚ฌ์ด์— ์‚ฝ์ž…ํ•จ์œผ๋กœ์จ, ๊ธฐ์กด 3์ƒ ์ธ๋ฒ„ํ„ฐ๋งŒ์œผ๋กœ๋Š” ๊ตฌ๋™์ด ๋ถˆ๊ฐ€๋Šฅํ–ˆ๋˜ ์šด์ „ ์˜์—ญ์—์„œ ์ „๋™๊ธฐ์˜ ์šด์ „์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•œ๋‹ค. ์ฆ‰, ๋Šฅ๋™ ์ „๋ ฅ ๋ณ€ํ™˜ ์žฅ์น˜์ธ ์ธ๋ฒ„ํ„ฐ์™€ ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ์˜ ์กฐํ•ฉ์„ ํ†ตํ•ด ๋‹จ์ผ ์ „๋™๊ธฐ๋กœ๋„ ์‚ฌ์šฉ์ž์— ๋”ฐ๋ผ ๋‹ค์–‘ํ•œ ์šด์ „ ํŠน์„ฑ์„ ๋งŒ์กฑํ•  ์ˆ˜ ์žˆ์œผ๋ฏ€๋กœ, ์ „๋™๊ธฐ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ์„ฑ๋Šฅ์„ ํ™•์žฅํ•  ์ˆ˜ ์žˆ๋‹ค. ๋˜ํ•œ ์ตœ๊ทผ์—๋Š” ๊ณ ์„ฑ๋Šฅ ์ˆ˜๋™ ์†Œ์ž์˜ ์ œ์ž‘ ๊ธฐ์ˆ  ๋ฐœ๋‹ฌ๋กœ ์ธํ•ด ๊ทธ ๊ฐ€๊ฒฉ์ด ํ•˜๋ฝํ•˜๊ณ  ์žˆ์œผ๋ฏ€๋กœ, ๊ฐ€๊นŒ์šด ๋ฏธ๋ž˜์—๋Š” ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ์˜ ์ ์šฉ ์‹œ ๊ทธ ํšจ๊ณผ ๋Œ€๋น„ ๊ฐ€๊ฒฉ์˜ ์ด์ ๋„ ์ƒ๊ธธ ๊ฒƒ์œผ๋กœ ์˜ˆ์ƒ๋œ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ์˜ ์ž„ํ”ผ๋˜์Šค ๋ณ€ํ™˜ ํŠน์„ฑ์„ ์ด์šฉํ•˜์—ฌ ํŠน์ • ์šด์ „์ ์—์„œ ์ „๋™๊ธฐ์˜ ์šด์ „ ํŠน์„ฑ์„ ๊ฐœ์„ ํ•˜๊ฑฐ๋‚˜ ์šด์ „ ์˜์—ญ์„ ํ™•์žฅํ•˜๋Š” ๋ฐฉ๋ฒ•์— ๋Œ€ํ•ด ์•Œ์•„๋ณธ๋‹ค. ์ด ๋•Œ ์„ค๊ณ„ ์ž์œ ๋„์— ๋”ฐ๋ผ ๋‹ค์–‘ํ•œ ์„ค๊ณ„๊ฐ€ ๊ฐ€๋Šฅํ•˜์ง€๋งŒ, ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ƒ๋‹น ์ž„ํ”ผ๋˜์Šค์˜ ๊ฐœ์ˆ˜๊ฐ€ 1๊ฐœ์ธ ๊ฒฝ์šฐ์™€ 2๊ฐœ์ธ ๊ฒฝ์šฐ์— ๋Œ€ํ•ด ๋‹ค๋ฃฌ๋‹ค. ์ด๋ฅผ ํ†ตํ•ด ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ์˜ 2๊ฐ€์ง€ ํ˜•ํƒœ์ธ ์ปคํŒจ์‹œํ„ฐ ๋„คํŠธ์›Œํฌ์™€ ์ธ๋•ํ„ฐ-์ปคํŒจ์‹œํ„ฐ ๋„คํŠธ์›Œํฌ๋ฅผ ์†Œ๊ฐœํ•œ๋‹ค. ๊ฐ๊ฐ์˜ ๋„คํŠธ์›Œํฌ๋ฅผ ์ ์šฉํ•˜์˜€์„ ๋•Œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ํŠน์„ฑ๊ณผ ์ด๋กœ ์ธํ•œ ์šด์ „ ์˜์—ญ ํ™•์žฅ ํšจ๊ณผ์— ๋Œ€ํ•ด ์•Œ์•„๋ณด๊ณ , ์‹œ์Šคํ…œ ๋ถ„์„์„ ํ†ตํ•ด ๋„คํŠธ์›Œํฌ ์ œ์ •์ˆ˜์˜ ์„ค๊ณ„ ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•œ๋‹ค. ๊ทธ ํ›„ ์ œ์•ˆ๋œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ์ œ์ •์ˆ˜ ์˜ค์ฐจ์— ๋Œ€ํ•œ ์˜ํ–ฅ๊ณผ ์†์‹ค ์š”์†Œ ๋“ฑ์„ ๋ถ„์„ํ•จ์œผ๋กœ์จ ์ œ์•ˆํ•˜๋Š” ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ์‹ ๋ขฐ์„ฑ๊ณผ ํšจ์œจ ํŠน์„ฑ์— ๋Œ€ํ•ด ์•Œ์•„๋ณธ๋‹ค. ๋˜ํ•œ ์„ค๊ณ„๋œ ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ๋ฅผ ์ ์šฉํ•œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๋™ํŠน์„ฑ์— ๋Œ€ํ•ด ์•Œ์•„๋ณธ ํ›„ ์ด๋ฅผ ์ด์šฉํ•˜์—ฌ ํ”ผ๋“œ๋ฐฑ ์ „๋ฅ˜ ์ œ์–ด๊ธฐ๋ฅผ ๊ตฌ์„ฑํ•œ๋‹ค. ๊ฐ ์žฅ์˜ ๋งˆ์ง€๋ง‰์—์„œ๋Š” ์‹คํ—˜์„ ํ†ตํ•ด ์ œ์•ˆํ•˜๋Š” ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ๋ฅผ ์ด์šฉํ•œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ์ด๋ก ๊ณผ์˜ ์ •ํ•ฉ์„ฑ์— ๋Œ€ํ•ด ์‚ดํŽด๋ณด๊ณ , ํšจ์œจ ๋˜๋Š” ๋ถ€ํ”ผ์™€ ๊ฐ™์ด ์‹ค์ œ ์‹œ์Šคํ…œ์— ์ ์šฉ ์‹œ ๊ณ ๋ คํ•ด์•ผํ•  ์‚ฌํ•ญ๋“ค์— ๋Œ€ํ•ด ์•Œ์•„๋ณธ๋‹ค. ๋˜ํ•œ ์ƒ์šฉ ์—์–ด์ปจ ์ปดํ”„๋ ˆ์„œ, ๋ฌด์„  ์ง„๊ณต ์ฒญ์†Œ๊ธฐ ๋“ฑ์˜ ์ „๋™๊ธฐ์— ์ œ์•ˆ๋œ ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ๋ฅผ ์ ์šฉํ•จ์œผ๋กœ์จ ์ œ์•ˆํ•˜๋Š” ๋ฐฉ๋ฒ•์ด ์‹ค์ œ ์‘์šฉ ๋ถ„์•ผ์— ์‚ฌ์šฉ ๊ฐ€๋Šฅํ•จ์„ ํ™•์ธํ•œ๋‹ค.This dissertation proposes the methods for driving and controlling three-phase permanent magnet synchronous motors using a passive network. A three-phase permanent magnet synchronous motors are used in a variety of applications, from small home appliances to large power systems such as electric vehicles and generators. Recently, there are many applications which demand a variety of operating characteristics for a single motor. However, when a conventional three-phase inverter is used, the maximum operating range of the motor is limited due to the voltage and current limitations. Redesigning a motor and an input voltage source is one solution, but this method is not reasonable in mass production such as home appliances due to increased cost of the production facilities. In this situation where redesigning of a motor is impossible, the operating area can be extended only by modifying the driving circuits. In this paper, passive networks are proposed to extend operating area of three-phase permanent magnet synchronous motors. A passive network is placed between the three-phase inverter and the motor. It makes the motor operate in an operating area where the motor cannot be driven by the three-phase inverter alone. That is, various driving characteristics of the motor are satisfied by the combination of an active devices and a passive network. In this way, the performance of the motor drive system can be extended. In addition, the price of the high-performance passive components has been recently declining due to the development of manufacturing technologies. Therefore, in the near future, it is expected that the passive network will have a price advantage. In this dissertation, the impedance conversion characteristics of the passive network are used to improve the operating characteristics of the motor at specific operating points or to extend the operating region. Many types of the passive network can be designed depending on the degree of design freedom, but this paper only deals with the passive networks which have one or two impedances per phase. So, two types of passive networks are introduced: capacitor networks and inductor-capacitor networks. The effect of the operating area extension is discussed according to the types of the passive networks, and the designing methods for the parameters of the each network are presented. Also, the reliability of the proposed drive system is presented by analyzing the effect from the parameter error. Also, efficiency characteristics of the proposed system are compared to that of the conventional system. In addition, the dynamic performances of the proposed drive systems are obtained by applying the proposed feedback current controllers. At the end of each chapter, the verifications of the proposed methods are presented by the experimental results. Also, it is confirmed that the proposed methods can be used in practical applications by applying them to the commercial applications such as air conditioner compressor or a wireless vacuum cleaner.์ œ 1 ์žฅ ์„œ ๋ก  1 1.1 ์—ฐ๊ตฌ ๋ฐฐ๊ฒฝ 1 1.2 ์—ฐ๊ตฌ ๋ชฉ์  7 1.3 ๋…ผ๋ฌธ์˜ ๊ตฌ์„ฑ 10 ์ œ 2 ์žฅ ์ „์••ํ˜• ์ธ๋ฒ„ํ„ฐ๋ฅผ ์ด์šฉํ•œ 3์ƒ ์˜๊ตฌ ์ž์„ ๋™๊ธฐ ์ „๋™๊ธฐ์˜ ๊ตฌ๋™ ์‹œ์Šคํ…œ 13 2.1 3์ƒ ์ธ๋ฒ„ํ„ฐ์— ์˜ํ•œ 3์ƒ ์˜๊ตฌ ์ž์„ ์ „๋™๊ธฐ ๊ตฌ๋™ 13 2.1.1 3์ƒ ์ „์••ํ˜• ์ธ๋ฒ„ํ„ฐ 13 2.1.2 3์ƒ ์˜๊ตฌ ์ž์„ ๋™๊ธฐ ์ „๋™๊ธฐ 17 2.2 ์ˆ˜๋™ ์†Œ์ž ๋ฐ ๋Šฅ๋™ ์†Œ์ž๋ฅผ ์ด์šฉํ•œ ๊ต๋ฅ˜ ์ „๋™๊ธฐ์˜ ์šด์ „ ํŠน์„ฑ ๊ฐœ์„  ๋ฐฉ์•ˆ 19 2.2.1 ๊ณ ์ • ๊ต๋ฅ˜ ์ „์••์›์— ์ง์ ‘ ์—ฐ๊ฒฐ๋œ ๊ต๋ฅ˜ ์ „๋™๊ธฐ์˜ ๊ตฌ๋™ 20 2.2.2 ์ธ๋ฒ„ํ„ฐ๋ฅผ ์ด์šฉํ•œ ๊ต๋ฅ˜ ์ „๋™๊ธฐ์˜ ๊ตฌ๋™ 26 2.3 ์—ฐ๊ตฌ์˜ ๋ฐฉํ–ฅ์„ฑ 31 ์ œ 3 ์žฅ ๋‹จ์ผ ์ˆ˜๋™ ์†Œ์ž๋ฅผ ์ด์šฉํ•œ 3์ƒ ์˜๊ตฌ์ž์„ ๋™๊ธฐ ์ „๋™๊ธฐ์˜ ๊ตฌ๋™ ์‹œ์Šคํ…œ 35 3.1 ์ œ์•ˆ๋œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๊ตฌ์กฐ 36 3.2 ์ œ์•ˆ๋œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๋™์ž‘ ์›๋ฆฌ ๋ฐ ์„ค๊ณ„ ๋ฐฉ๋ฒ• 40 3.2.1 ์ผ์ • ์ถœ๋ ฅ ์ „๋ ฅ ์†๋„ ์˜์—ญ ํ™•์žฅ์„ ์œ„ํ•œ ์ปคํŒจ์‹œํ„ฐ ๋„คํŠธ์›Œํฌ 40 3.2.2 ์ผ์ • ํ† ํฌ ์†๋„ ์˜์—ญ ํ™•์žฅ์„ ์œ„ํ•œ ์ปคํŒจ์‹œํ„ฐ ๋„คํŠธ์›Œํฌ 53 3.2.3 ์ œ์•ˆ๋œ ์‹œ์Šคํ…œ์˜ ์ œ์ •์ˆ˜ ์˜ค์ฐจ์— ์˜ํ•œ ์˜ํ–ฅ ๋ฐ ์†์‹ค 71 3.3 ์ œ์•ˆ๋œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ์ „๋ฅ˜ ์ œ์–ด๊ธฐ 82 3.3.1 ํ”ผ๋“œ๋ฐฑ ์ œ์–ด๊ธฐ 83 3.3.2 ์ „๋ฅ˜ ์ง€๋ น ์ƒ์„ฑ๊ธฐ 88 3.3.3 ์ปคํŒจ์‹œํ„ฐ ์˜คํ”„์…‹ ์ „์•• ์ œ์–ด๊ธฐ 92 3.3.4 ์ „๋ฅ˜ ์ œ์–ด๊ธฐ์˜ ์ „์ฒด ๊ตฌ์กฐ 98 3.4 ์ œ์•ˆ๋œ ์‹œ์Šคํ…œ์˜ ํ•œ๊ณ„ ๋ฐ ํ•ด๊ฒฐ ๋ฐฉ์•ˆ 100 3.4.1 ์ €์† ํ† ํฌ ํ™•๋ณด ๋ฐฉ์•ˆ 1: ๋น„๋™๊ธฐ ์ €์† ๊ตฌ๋™ 101 3.4.2 ์ €์† ํ† ํฌ ํ™•๋ณด ๋ฐฉ์•ˆ 2: ๋ฆด๋ ˆ์ด์— ์˜ํ•œ ๊ตฌ๋™ ๋ฐฉ๋ฒ• ์ „ํ™˜ 105 3.5 ์‹คํ—˜ ๊ฒฐ๊ณผ 110 3.5.1 ์‹คํ—˜ ์„ธํŠธ ๊ตฌ์„ฑ 110 3.5.2 ์šด์ „ ์˜์—ญ ํ™•์žฅ ์„ฑ๋Šฅ ๊ฒ€์ฆ 114 3.5.3 ์ „๋ฅ˜ ์ œ์–ด๊ธฐ ์„ฑ๋Šฅ ๊ฒ€์ฆ 124 3.5.4 ์ €์† ํ† ํฌ ํ™•๋ณด ๋ฐฉ์•ˆ ๊ฒ€์ฆ 129 ์ œ 4 ์žฅ ์ธ๋•ํ„ฐ-์ปคํŒจ์‹œํ„ฐ ๋„คํŠธ์›Œํฌ๋ฅผ ์ด์šฉํ•œ 3์ƒ ์˜๊ตฌ ์ž์„ ๋™๊ธฐ ์ „๋™๊ธฐ์˜ ๊ตฌ๋™ ์‹œ์Šคํ…œ 132 4.1 ์ œ์•ˆ๋œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๊ตฌ์กฐ 132 4.2 ์ œ์•ˆ๋œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๋™์ž‘ ์›๋ฆฌ ๋ฐ ์„ค๊ณ„ ๋ฐฉ๋ฒ• 136 4.2.1 ์ œ์•ˆ๋œ ๋„คํŠธ์›Œํฌ์˜ ๋™์ž‘ ์›๋ฆฌ 136 4.2.2 ์ œ์•ˆ๋œ ๋„คํŠธ์›Œํฌ์˜ ์„ค๊ณ„ ๋ฐฉ๋ฒ• 139 4.2.3 ์ œ์•ˆ๋œ ๋„คํŠธ์›Œํฌ๋ฅผ ์ด์šฉํ•œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ๋ถ„์„ 153 4.2.4 ์ œ์•ˆ๋œ ์‹œ์Šคํ…œ์˜ ์ œ์ •์ˆ˜ ์˜ค์ฐจ์— ์˜ํ•œ ์˜ํ–ฅ ๋ฐ ์†์‹ค 160 4.3 ์ œ์•ˆ๋œ ๊ตฌ๋™ ์‹œ์Šคํ…œ์˜ ์ „๋ฅ˜ ์ œ์–ด๊ธฐ 168 4.4 ์‹คํ—˜ ๊ฒฐ๊ณผ 178 4.4.1 ์‹คํ—˜ ์„ธํŠธ ๊ตฌ์„ฑ 178 4.4.2 ์šด์ „ ์˜์—ญ ํ™•์žฅ ์„ฑ๋Šฅ ๊ฒ€์ฆ 182 4.4.3 ์ „๋ฅ˜ ์ œ์–ด๊ธฐ ์„ฑ๋Šฅ ๊ฒ€์ฆ 190 ์ œ 5 ์žฅ ๊ฒฐ๋ก  ๋ฐ ํ–ฅํ›„ ๊ณผ์ œ 193 5.1 ๊ฒฐ๋ก  193 5.2 ํ–ฅํ›„ ๊ณผ์ œ 195 ์ฐธ๊ณ  ๋ฌธํ—Œ 198 ๋ถ€ ๋ก 206 A.1 ๋ชจ์˜ ์‹คํ—˜ ๋ฐ ์‹คํ—˜์— ์‚ฌ์šฉ๋œ ์ „๋™๊ธฐ ์ œ์ •์ˆ˜ 206 A.2 ์ปคํŒจ์‹œํ„ฐ์˜ ์ „๋ฅ˜ ์ •๊ฒฉ 208 A.3 LC ๋„คํŠธ์›Œํฌ์˜ ๋น„๋Œ€์นญ ์ œ์ •์ˆ˜ ์˜ค์ฐจ์˜ ์˜ํ–ฅ ๊ณ„์‚ฐ 209 A.4 ์ˆ˜๋™ ๋„คํŠธ์›Œํฌ ์ ์šฉ ์‹œ ๊ณ ๋ ค ์‚ฌํ•ญ 213 A.4.1 ์ „๋™๊ธฐ์˜ ์ „์•• ์ •๊ฒฉ 213 A.4.2 ์ „๋™๊ธฐ์˜ ๋ฐœ์—ด ์ •๊ฒฉ 213 A.4.3 ๊ณ ์žฅ ์ƒํ™ฉ 215 ABSTRACT 220Docto

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    ์„ ๋ฐ•, ์ž ์ˆ˜ํ•จ์ด ์ถ”์ง„ํ•˜๋ฉด ์ˆ˜์ค‘๊ตฌ์กฐ๋ฌผ ํ›„๋ฅ˜์— ์™€๋ฅ˜๊ฐ€ ๋ฐœ์ƒํ•˜๊ณ  ์ด์— ๋”ฐ๋ฅธ ์™€๋ฅ˜๊ธฐ์ธ ๊ตฌ์กฐ์ง„๋™์ด ์œ ๋ฐœ๋œ๋‹ค. ์ตœ๊ทผ ์„ ๋ฐ•, ์ž ์ˆ˜ํ•จ์˜ ๊ณ ์†ํ™” ๋ฐ ๋Œ€ํ˜•ํ™” ์ถ”์„ธ์— ๋”ฐ๋ผ ๊ณ ์ฐจ๋ชจ๋“œ์—์„œ ์œ ๋ฐœ๋˜๋Š” ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™ ๋ฐ ํ”ผ๋กœํŒŒ๊ดด์— ๋Œ€ํ•œ ์ค‘์š”์„ฑ์ด ๊ฐ•์กฐ๋˜๊ณ  ์žˆ๋‹ค. ๊ณ ์† ์œ ์†ํ™˜๊ฒฝ์˜ ์™€๋ฅ˜๋Š” ์ €์† ์œ ์†ํ™˜๊ฒฝ ๋Œ€๋น„ ํฐ ์ง„๋™์„ ์œ ๋ฐœํ•˜๋ฏ€๋กœ ์ด์— ๊ด€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ํ•„์š”ํ•˜๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ˆ˜์ค‘๋‚ ๊ฐœ ๊ณ ์ฐจ๋ชจ๋“œ์—์„œ ์œ ๋ฐœ๋˜๋Š” ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์„ ์˜ˆ์ธกํ•˜๊ธฐ ์œ„ํ•œ ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ ํ•ด์„ ๋ฐฉ๋ฒ•๋ก ์„ ์ œ์‹œํ•˜์˜€๋‹ค. ๊ณ ์ฐจ๋ชจ๋“œ๋ฅผ ๊ณ ๋ คํ•œ ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ ํ•ด์„์„ ์ˆ˜ํ–‰ํ•˜์—ฌ ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์„ ๋„์ถœํ•˜๊ณ  ์‹คํ—˜๊ฒฐ๊ณผ์™€ ๋น„๊ตํ•จ์œผ๋กœ์จ ๋ฐฉ๋ฒ•๋ก ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ์ตœ์ข…์ ์œผ๋กœ ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์œผ๋กœ๋ถ€ํ„ฐ ๋„์ถœ๋œ ์ตœ๋Œ€ von Mises ์‘๋ ฅ์„ ๋…ธ๋ฅด์›จ์ด ์„ ๊ธ‰์—์„œ ์ œ์‹œํ•œ S-N ์„ ๋„์— ์ ์šฉํ•จ์œผ๋กœ์จ ๊ณ ์ฐจ๋ชจ๋“œ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ ํ•ด์„์˜ ํšจ์šฉ์„ฑ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๊ณ ์ฐจ๋ชจ๋“œ๋ฅผ ๊ณ ๋ คํ•˜์—ฌ ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์‘๋‹ต์„ ๋„์ถœํ•  ๊ฒฝ์šฐ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ์— ์˜ํ•œ ๋ฝ์ธ(Lock-in) ํŠน์„ฑ์„ ํ™•์ธํ•˜์˜€์œผ๋ฉฐ ๊ณ ๋ คํ•˜์ง€ ์•Š์€ ๊ฒฝ์šฐ ๋Œ€๋น„ ์ง„๋™์‘๋‹ต๊ณผ ์ตœ๋Œ€ von Mises ์‘๋ ฅ์—์„œ 10๋ฐฐ ์ด์ƒ์˜ ์ฐจ์ด๋ฅผ ๋ณด์˜€๋‹ค. ํ–ฅํ›„์—๋Š” ์™ธํŒ”๋ณด ๊ฒฝ๊ณ„์กฐ๊ฑด ๋ฐ ํ˜•์ƒ์— ๋Œ€ํ•œ ํ™•์žฅ์—ฐ๊ตฌ๊ฐ€ ํ•„์š”ํ•˜๋‹ค.N
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