66 research outputs found

    Organic Lasing: Correlation between Molecular Structure, Optical and Optoelectronic Properties

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ํ™”ํ•™๊ณผ, 2013. 2. Frรฉdรฉric Laquai.In this thesis mainly two alternating indenofluorene-phenanthrene copolymers were investigated with a variety of spectroscopic and optoelectronic experiments. The different experimental techniques allowed to retrieve deeper insights into their unique optical as well as optoelectronic properties. The motivation of the research presented in this work was to correlate their photophysical properties with respect to their application in electrically pumped lasing. This thesis begins with the description of optical properties studied by classical absorption and emission spectroscopy and successively describes an overall picture regarding their excited state dynamics occurring after photoexcitation studied by time-resolved spectroscopy. The different spectroscopic methods do not only allow to elucidate the different optical transitions occurring in this class of materials, but also contribute to a better understanding of exciton dynamics and exciton interaction with respect to the molecular structure as well as aggregation and photooxidation of the polymers. Furthermore, the stimulated emission properties were analyzed by amplified spontaneous emission (ASE) experiments. Especially one of the investigated materials, called BLUE-1, showed outstanding optical properties including a high optical gain, a low threshold for ASE and low optical losses. Apart from the optical experiments, the charge carrier mobility was measured with the time-of-flight technique and a comparably high hole mobility on the order of 1 x 10ยฒ cmยฒ/(Vs) was determined for BLUE-1 which makes this material promising for organic lasing. The impact of the high charge carrier mobility in this material class was further analyzed in different optoelectronic devices such as organic LEDs (OLEDs) and organic solar cells.1 introduction 1 2 theoretical basics 5 2.1 Absorption and Emission of Light 5 2.2 Electronic configuration of carbon atoms in molecules 7 2.3 Optical Properties of Organic Molecules 8 2.3.1 Optical transitions in organic molecules 8 2.3.2 Absorption of light in organic molecules 10 2.3.3 Spectral lineshapes in organic molecules 13 2.3.4 Photoluminescence quantum efficiency 14 2.3.5 Intermolecular interactions of molecules 15 2.4 The Gaussian Disorder Model 17 2.5 Lasing in Organic Semiconductors 21 2.6 Organic light emitting diodes 22 3 optical spectroscopy 25 3.1 The class of poly(indenofluorenes) 25 3.1.1 Introduction 25 3.2 Experimental 26 3.2.1 Sample preparation 26 3.2.2 Steady-state spectroscopy 27 3.2.3 Time-resolved spectroscopy 27 3.2.4 Amplified spontaneous emission and lasing 30 3.3 Absorption and emission spectroscopy 32 3.3.1 Quasi steady-state excited state absorption 33 3.4 Time-resolved fluorescence spectroscopy on BLUE-1 and BLUE-2 34 3.4.1 Fluorescence spectroscopy 34 3.4.2 Defect emission 39 3.4.3 The origin of non-monoexponential dynamics in BLUE-1 42 3.4.4 Delayed fluorescence of BLUE-1 47 3.5 Amplified spontaneous emission and lasing 51 3.5.1 Introduction 51 3.5.2 Results and discussion on PIF, BLUE-1 and BLUE-2 53 3.5.3 Lasing characteristics 60 3.5.4 ASE from a PIF-triphenylamine copolymer 63 3.6 Transient absorption spectroscopy on BLUE-1 72 3.7 Summary and conclusions of chapter 3 76 4 the influence of high mobilities in optoelectronic devices 79 4.1 Introduction 79 4.2 Experimental 80 4.2.1 Time-of-flight technique 80 4.2.2 OLED preparation 80 4.2.3 OLED characterization 81 4.2.4 Organic solar cell preparation and characterization 82 4.3 The time-of-flight technique 82 4.4 OLED characterization of different PIF-based copolymers 86 4.4.1 Introduction 86 4.4.2 OLED characteristics of BLUE-1 87 4.4.3 OLED characteristics of BLUE-2 91 4.4.4 Multilayer OLEDs- the impact of hole injection layers 93 4.5 Consequences of results on BLUE-1 for future lasing diodes 98 4.6 Exciton dissociation in a wide bandgap polymer 100 4.6.1 Introduction 100 4.6.2 Optical properties of BLUE-1 blended with PCBM 101 4.6.3 Solar cell performance of BLUE-1:PCBM blends 105 4.7 Summary and conclusions of chapter 4 107 5 conclusions and outlook 109 a appendix a 113 bibliography 123Docto

    Atomistic origins of mechanical amorphization of SiO2 using solid-state 29Si NMR and local electronic structures for SiO2 high pressure phases using ab initio calculation

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ง€๊ตฌํ™˜๊ฒฝ๊ณผํ•™๋ถ€, 2017. 2. ์ด์„ฑ๊ทผ.Silica (SiO2), the most abundant material on the earth, is a major component of the crust and mantle. Therefore the structure of silica affects the dynamic process of crust or the structural properties of the earth interior. The structure of silica changes not only by pressure-temperature change but also mechanical energy like friction without melting. To understand the properties of interior of rocky planets and the geological process, the detailed understanding of the structure of silica with various conditions is needed. In this study, we performed two major subject related to structure of silica. The first study is about atomistic origin of the mechanical amorphization of silica with an experimental methodology. There have been reported the reduction of fault strength during fault slip, and one of the causes is reported as the formation of the amorphous silica and the silica gel layer on the fault plane. The formation of amorphous silica is due to the frictional energy between the fault surfaces, and the formation of silica gel layer is due to reaction with the water present in the layer or air. In previous, studies on frictional experiments using quartzite rocks, reported the formation of silica and silica gel and also the decrease of friction coefficient, and the observation of the silica gel layer in natural faults has been reported. However, due to the complex structure of amorphous silica and the analytical method limitations, the atomic structure of the amorphized silica and the detailed origin of the mechanical amorphization process have not been clearly identified. In this study, silica was amorphized with mechanical energy by ball mill method, and the resulting amorphous structure was analyzed by high resolution nuclear magnetic resonance (NMR) spectroscopy. The morphology of the amorphized silica and the phases formed by other elements were analyzed using XRD, HR-TEM, and EDS-mapping method. Solid-state nuclear magnetic resonance spectroscopy (NMR) is suitable for the analysis of complex amorphous structures because it yields atomic environments in short range order around specific atoms and provides quantitative information on atomic unit bonding. The 29Si MAS NMR spectra of amorphous silica milled at different rates present that the spectra of samples milled above 600 rpm show a broad amorphous peak over -80 to -120 ppm. These amorphous peaks indicate the presence of Q2 and Q3 structures in the mechanically amorphized silica. The results indicate that the mechanical amorphization of silica occurs only above a certain energy level, and that the amorphization process results in a change in the short range atomic structure and imply the presence of reaction with other elements. This results help to understand the atomic structure of the mechanically amorphized silica and the mechanical amorphization process that occurs without melting in the fault plane. The second study is an electronic structure and detailed origin of spectral feature of O K-edge XRS for crystalline silica using computational computation. Crystalline silica undergoes various phase transition according to pressure-temperature change. Therefore, many studies on the structure of high-pressure phase silica have been reported to understand the internal structure of rocky planets in high temperature and high pressure environment. The most powerful method of in situ high-pressure study for electronic structure is O K-edge x-ray Raman spectroscopy (XRS) using diamond anvil cell and as experimental limitation above ~70 GPa, the computational methods is used to understand the XRS spectrum. However, the detailed relation between spectral feature of O K-edge XRS and structure is still in debate. In this study, we calculated electronic structures and O K-edge XRS spectra for various crystalline silica using ab initio calculation, and proved the origin of O K-edge XRS spectrum. Previous studies have suggested that the origin of the O K-edge XRS spectrum is attributed to the number of Si atoms or the number of O atoms. However, in this study, we have found that the O K-edge XRS spectra of hp-cristobalite with 4-coordination Si, of penta-SiO2 with 5-coordination Si and of stishovite with 6-coordination Si are similar, and O site resolved K-edge XRS spectra the penta-SiO2 revealed that the coordination of atoms does not directly affect the O K-edge XRS spectral feature. These results not only provide an understanding of the electronic structure of high-pressure phase silica, but also provide clear criteria for O K-edge XRS spectral analysis.1. INTRODUCTION 1 2. THEORETICAL BACGROUNDS 3 2.1 NMR TECHNIQUES 3 2.2 BALL MILL METHOD 4 2.3 AB INITIO CALCULATIONS 5 3. ATOMISTIC ORIGINS OF MECHANICAL AMORPHIZATION BY BALL MILL EXPERIMENTS: INSIGHTS FROM SI-29 NUCLEAR MAGNETIC RESONANCE 7 3.1. INTRODUCTION 7 3.2. EXPERIMENTS 9 3.2.1 Sample Preparation and Analysis 9 3.2.2 Planetary Ball Mill 9 3.2.3 NMR Spectroscopy 10 3.2.4 X-ray Diffraction 10 3.3. RESULTS AND DISCUSSION 11 3.3.1. TEM EDS 11 3.3.2. X-ray Diffraction Patterns 11 3.3.3. Si-29 MAS NMR 12 3.4. CONCLUSION 13 REFERENCE 14 4. AB INITIO CALCULATIONS OF LOCAL ELECTRONIC STRUCTURES AND X-RAY RAMAN SCATTERING SPECTRA FOR SIO2 HIGH PRESSURE PHASE 16 4.1 INTRODUCTION 16 4.2 AB INITIO CALCULATIONS 16 4.2.1 Crystal structures 16 4.2.2 Calculation conditions 19 4.2.3 PDOS and O K-edge XRS calculations 20 4.3 RESULTS AND DISCUSSION 21 4.3.1 O K-edge x-ray Raman scattering 21 4.3.2 Correlation between spectrum and crystal structure 22 4.4 CONCLUSION 23 REFERENCE 25 TABLES 29 FIGURE 30 APPENDIX SECTION 42 ABSTRACT IN KOREAN 44Maste

    (A)Study on elemental reception and synthesis process in modern architecture of 1920~30 : focused on office buildings and governmental buildings

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ฑด์ถ•ํ•™๊ณผ,2005.Maste

    (A) Study on design changes and planning factors of high-rise office buidings in Korea since 1960's

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ฑด์ถ•ํ•™๊ณผ, 2011.2. ์‹ฌ์šฐ๊ฐ‘.Docto

    ๋ฐ˜์ถ”๋™๋ฌผ์— ์žˆ์–ด์„œ essential oil์˜ ์ฒจ๊ฐ€๊ฐ€ ํ•ญ๊ท ์ž‘์šฉ, ์ƒ๋ฆฌ์ž‘์šฉ ๋ฐ ์„ฑ์žฅ์„ฑ์ ์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ

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    Thesis (master`s)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๋†์ƒ๋ช…๊ณตํ•™๋ถ€,2003.Essential oils are volatile oils obtained from plants by water distillation or steam distillation. Most essential oils consist of mixtures of hydrocarbons (terpenes etc.), oxygenated compounds (terpenoids etc.) and other components. Essential oils have potential against a wild range of microorganisms including bacteria, fungi, viruses, and protozoa. Some of components in essential oils have neurological effect, and structural similarity to gonadal steroid hormones and nature of the PPARฮณ ligands. It is suggested that essential oils may be substitute for antibiotic and potential regulation factors for some hormone secretions to control muscle and adipose development. So this study was conducted to observe these beneficial functions of essential oils in beef cattle.Maste

    ํ•œ๊ตญ ์ž๊ถ๋‚ด๋ง‰์ฆ ํ™˜์ž์—์„œ alpha 2-Heremans-Schmidt glycoprotein (AHSG) ์˜ ์œ ์ „์ž๋‹คํ˜•์„ฑ์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์˜ํ•™๊ณผ ์‚ฐ๋ถ€์ธ๊ณผํ•™์ „๊ณต,2004.Maste

    ๋„์‚ฐ์œ„ํ—˜๊ณผ ๊ธฐ์—…๊ฐ€์น˜ ํ‰๊ฐ€์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ฒฝ์˜ํ•™๊ณผ ๊ฒฝ์˜ํ•™์ „๊ณต,1999.Maste

    3D ํ”„๋ฆฐํŒ…์„ ์œ„ํ•œ PETG/๋‚˜๋…ธํด๋ ˆ์ด ๋ฐ ๊ด‘๊ฒฝํ™”์ˆ˜์ง€/๋‚˜๋…ธํด๋ ˆ์ด ๋ณตํ•ฉ์žฌ๋ฃŒ ์ œ์กฐ ๋ฐ ํŠน์„ฑ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๋†์—…์ƒ๋ช…๊ณผํ•™๋Œ€ํ•™ ์‚ฐ๋ฆผ๊ณผํ•™๋ถ€(ํ™˜๊ฒฝ์žฌ๋ฃŒ๊ณผํ•™์ „๊ณต), 2021. 2. ๊น€ํ˜„์ค‘.The purpose of this study is to prepare a nanocomposite material by introducing a nanomaterial to a polymeric material, and apply it to 3D printing to a 3D structure having the functionality fabricate, and investigate the correlation between structural change and physical behavior. In this study, sepiolite clay was combined with polyethylene terephthalate glycol in a molten state using a twinextruder, and the resulting polymer nanocomposite was processed into a filament for extrusion molding of molten resin, applied to a 3D printing and traditional injection molding. As the proportion of sepiolite increased, mechanical properties of nanocomposite materials increased. The 3D printed material showed a higher reinforcing effect compared with the material from to injection molding. Through morphology observation using an electron microscopy and small-angle X-ray scattering, it was confirmed that sepiolite was oriented in the same direction as the 3D printing direction, and such orientation led to reinforcement of physical strength. In addition, computer simulation confirmed the orientation of material with the effective tensile strength. Montmorillonite, sepiolite, and halloysite clay were dispersed in a photocurable resin to prepare a photocurable nanoclay composite resin. The rheological, photo-curing behavior, and mechanical properties of the nanoclay-dispersed resin were investigated. Nanoclay affected the photocuring behavior of resin. Montmorillonite and sepiolite were more effective on improvement mechanical properties halloysite. The applicable amount and effective clay of in photocurable resins were established in 3D printing. Sepiolite showed the highest efficiency in mechanical and rheological properties for 3D printing and the nanoclay orientation of photocurable nanocomposite resin was studied. For 3D printing of low-concentration and low-viscosity of ink, the material was printed in a fumed silica/silicone oil slurry as a supporting matrix. The sepiolite compounded with the photocurable 3D printing material passed through the nozzle during direct ink printing. It was exposed to shearing force, and had orientation consistent with the printing direction. In addition, the tensile properties of the oriented sepiolite enhanced the mechanical properties of the printed composites more efficiently compared with the unoriented sepiolite. The composite of nanoclay to PETG and photocurable resin, improved mechanical properties of printed structures. The nano-oriented structure resulted from the rheological behavior of the material during the 3D printing process.๋ณธ ์—ฐ๊ตฌ์˜ ๋ชฉ์ ์€ ๊ณ ๋ถ„์ž 3D ํ”„๋ฆฐํŒ… ์žฌ๋ฃŒ์— ๋‚˜๋…ธ ์žฌ๋ฃŒ๋ฅผ ์ ์šฉํ•˜์—ฌ ๋‚˜๋…ธ ๋ณตํ•ฉ์žฌ๋ฃŒ๋ฅผ ํ˜•์„ฑํ•˜๊ณ , ๋‚˜๋…ธ๋ณตํ•ฉ์žฌ๋ฃŒ๋ฅผ 3D ํ”„๋ฆฐํŒ…์— ์ ์šฉํ•˜์—ฌ ๋‚˜๋…ธ๋ณตํ•ฉ์žฌ๋ฃŒ์˜ ๊ธฐ๋Šฅ์„ฑ์„ ๊ฐ€์ง€๋Š” 3D ํ”„๋ฆฐํŒ… ๋ฌผ์งˆ์„ ์ œ์กฐํ•˜๊ณ  3D ํ”„๋ฆฐํŒ… ๊ณผ์ • ์ค‘ ์žฌ๋ฃŒ์˜ ๊ตฌ์กฐ ๋ณ€ํ™”์™€ ๋ฌผ๋ฆฌ์  ๊ฑฐ๋™์˜ ์ƒ๊ด€ ๊ด€๊ณ„๋ฅผ ๊ทœ๋ช…ํ•˜๋Š”๋ฐ ์žˆ๋‹ค. ํด๋ฆฌ์—ํ‹ธ๋ Œ ํ…Œ๋ ˆํ”„ํƒˆ๋ ˆ์ดํŠธ ๊ธ€๋ฆฌ์ฝœ์— ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ ํด๋ ˆ์ด๋ฅผ ํŠธ์œˆ์ต์ŠคํŠธ๋ฃจ๋”๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ์šฉ์œต์ƒํƒœ์—์„œ ๋ณตํ•ฉํ™” ํ•˜์˜€์œผ๋ฉฐ ์ƒ์„ฑ๋œ ๊ณ ๋ถ„์ž ๋‚˜๋…ธ๋ณตํ•ฉ์žฌ๋ฃŒ๋ฅผ ์ด์šฉํ•˜์—ฌ ์šฉ์œต์ˆ˜์ง€ ์••์ถœ ์กฐํ˜•์šฉ ํ•„๋ผ๋ฉ˜ํŠธ๋กœ ๊ฐ€๊ณตํ•˜์—ฌ 3D ํ”„๋ฆฐํ„ฐ์— ์ ์šฉํ•˜์˜€์œผ๋ฉฐ ๋น„๊ต๋ฅผ ์œ„ํ•˜์—ฌ ์ „ํ†ต์ ์ธ ์‚ฌ์ถœ์„ฑํ˜•์— ๋˜ํ•œ ์ ์šฉํ•˜์˜€๋‹ค. ๊ณ ๋ถ„์ž ๋‚˜๋…ธ๋ณตํ•ฉ์žฌ๋ฃŒ๋ฅผ ๊ฐ๊ฐ 3D ํ”„๋ฆฐํŒ… ๊ณผ ์‚ฌ์ถœ์„ฑํ˜•์œผ๋กœ ์ธ์žฅ๊ฐ•๋„ ์‹œํŽธ์„ ๋งŒ๋“ค์–ด ๋น„๊ต ๊ธฐ๊ณ„์  ์ธ์žฅ๊ฐ•๋„๋ฅผ ๋น„๊ตํ•˜์˜€๋‹ค. ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ์˜ ๋น„์œจ์ด ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ ๊ธฐ๊ณ„์  ๋ฌผ์„ฑ์ด ์ฆ๊ฐ€ํ•˜์˜€๋‹ค. 3D ํ”„๋ฆฐํŒ… ๋œ ์žฌ๋ฃŒ์˜ ์ธ์žฅ๊ฐ•๋„ ์ฆ๊ฐ€๊ฐ€ ์‚ฌ์ถœ์„ฑํ˜•๊ณผ ๋น„๊ตํ•˜์—ฌ ํ•จ๋Ÿ‰๋Œ€๋น„ ๋†’์€ ๋ณด๊ฐ•ํšจ๊ณผ๋ฅผ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ์ „์žํ˜„๋ฏธ๊ฒฝ์„ ์ด์šฉํ•œ ๋ชจํด๋กœ์ง€ ๊ด€์ฐฐ ๋ฐ ์†Œ๊ฐ์—‘์Šค์„ ์‚ฐ๋ž€๋ฒ•์„ ํ†ตํ•˜์—ฌ ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ๊ฐ€ 3D ํ”„๋ฆฐํŒ… ์ถœ๋ ฅ๋ฐฉํ–ฅ๊ณผ ๋™์ผํ•œ ๋ฐฉํ–ฅ์œผ๋กœ ๋ฐฐํ–ฅ๋˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€์œผ๋ฉฐ ์ด๋Ÿฌํ•œ ๋ฐฐํ–ฅ์„ฑ์˜ ๋ฐœํ˜„์ด ํšจ๊ณผ์ ์ธ ๋ฌผ๋ฆฌ์  ๊ฐ•๋„ ๋ณด๊ฐ• ํšจ๊ณผ๋ฅผ ์ด๋Œ์–ด ๋‚ด๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋˜ํ•œ ์ปดํ“จํ„ฐ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ํ†ตํ•˜์—ฌ ๋ฐฐํ–ฅ๋œ ์žฌ๋ฃŒ๊ฐ€ ํšจ์œจ์ ์ธ ์ธ์žฅ๊ฐ•๋„ ํ–ฅ์ƒ๊ณผ ๊ด€๊ณ„๊ฐ€ ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋ชฌ๋ชจ๋ฆด๋กœ๋‚˜์ดํŠธ, ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ, ํ• ๋กœ์ด์‚ฌ์ดํŠธ ํด๋ ˆ์ด๋ฅผ ๊ด‘๊ฒฝํ™” ์ˆ˜์ง€์— ๋ถ„์‚ฐํ•˜์—ฌ ๊ด‘๊ฒฝํ™” ๋‚˜๋…ธํด๋ ˆ์ด ๋ณตํ•ฉ์ˆ˜์ง€๋ฅผ ์ œ์กฐํ•˜์˜€๋‹ค. ๋‚˜๋…ธํด๋ ˆ์ด๊ฐ€ ๋ถ„์‚ฐ๋œ ๋ ˆ์ง„์˜ ์œ ๋ณ€ํ•™์ , ๊ด‘๊ฒฝํ™” ๊ฑฐ๋™ ๋ฐ ๊ธฐ๊ณ„์  ๋ฌผ์„ฑ ๋ณ€ํ™”์— ๋Œ€ํ•˜์—ฌ ๊ณ ์ฐฐํ•˜์˜€๋‹ค. ๋‚˜๋…ธํด๋ ˆ์ด๋Š” ๋ ˆ์ง„์˜ ๊ด‘๊ฒฝํ™” ๊ฑฐ๋™์— ์˜ํ–ฅ์„ ๋ฏธ์น˜๋ฉฐ ๋ชฌ๋ชจ๋ฆด๋กœ๋‚˜์ดํŠธ์™€ ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ๊ฐ€ ํ• ๋กœ์ด์‚ฌ์ดํŠธ์— ๋น„ํ•˜์—ฌ ๊ธฐ๊ณ„์  ๋ฌผ์„ฑํ–ฅ์ƒ์— ํšจ๊ณผ์ ์ธ ๊ฒƒ์œผ๋กœ ํ™•์ธ ๋˜์—ˆ๋‹ค. ๋‚˜๋…ธํด๋ ˆ์ด๋ฅผ ๊ด‘๊ฒฝํ™” ๋ ˆ์ง„์— ์ฒจ๊ฐ€ํ•˜์˜€์„ ๊ฒฝ์šฐ UV๋ฅผ ์‚ฌ์šฉํ•˜๋Š” 3D ํ”„๋ฆฐํŒ…์— ์ ์šฉ์ด ๊ฐ€๋Šฅํ•œ ๋ฒ”์œ„์™€ ์œ ํšจํ•œ ํด๋ ˆ์ด์— ๋Œ€ํ•˜์—ฌ ์ •๋ฆฝํ•˜์˜€๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ฐ€์žฅ ๋†’์€ ํšจ์œจ์„ ๋ณด์—ฌ์ค€ ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ๋ฅผ ๊ด‘๊ฒฝํ™”ํ˜• 3D ํ”„๋ฆฐํŒ…์— ์ ์šฉํ•จ๊ณผ ๋™์‹œ์— ๊ด‘๊ฒฝํ™” ๋‚˜๋…ธ๋ณตํ•ฉ์ˆ˜์ง€์˜ ๋‚˜๋…ธํด๋ ˆ์ด ๋ฐฐํ–ฅ์„ฑ์— ๋Œ€ํ•˜์—ฌ ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ์˜ ๊ด‘๊ฒฝํ™” ์ˆ˜์ง€์™€์˜ ๋ณตํ•ฉํ™” ์—ฐ๊ตฌ์—์„œ ์–ป์–ด์ง„ ๊ฒฐ๊ณผ๋ฅผ ํ† ๋Œ€๋กœ 3D ํ”„๋ฆฐํŒ… ์ž‰ํฌ์˜ ์ง์ ‘ ์ž‰ํฌ ์ธ์‡„๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ๊ธฐ์กด ์—ฐ๊ตฌ์—์„œ ๊ตฌํ˜„ํ•  ์ˆ˜ ์—†๋˜ ์ €๋†๋„, ์ €์ ๋„์˜ ์ž‰ํฌ์˜ 3D ํ”„๋ฆฐํŒ…์„ ํ„๋“œ ์‹ค๋ฆฌ์นด/์‹ค๋ฆฌ์ฝ˜ ์˜ค์ผ ์Šฌ๋Ÿฌ๋ฆฌ๋ฅผ ์ง€์ง€์ฒด๋กœ ์‚ฌ์šฉํ•˜์—ฌ ์žฌ๋ฃŒ๋ฅผ ์ถœ๋ ฅํ•˜์˜€๋‹ค. ๊ด‘๊ฒฝํ™” 3D ํ”„๋ฆฐํŒ… ์žฌ๋ฃŒ์™€ ๋ณตํ•ฉํ™” ๋œ ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ๋Š” ์ง์ ‘ ์ž‰ํฌ ์ธ์‡„ ์ค‘ ๋…ธ์ฆ์„ ํ†ต๊ณผํ•˜๋ฉฐ ์ „๋‹จ๋ ฅ์— ๋…ธ์ถœ๋˜๊ณ  ํ”„๋ฆฐํŒ… ๋ฐฉํ–ฅ๊ณผ ์ผ์น˜ํ•˜๋Š” ๋ฐฐํ–ฅ์„ฑ์„ ๊ฐ€์ง€๊ฒŒ ๋˜๋Š” ๊ฒƒ์„ ์žฌ๋ฃŒ์˜ ์ธ์žฅ ํŒŒ๋‹จ๋ฉด์˜ ๋ฏธ์„ธ๊ด€์ฐฐ์„ ํ†ตํ•˜์—ฌ ํ™•์ธํ•˜์˜€๋‹ค. ๋˜ํ•œ ๋ฐฐํ–ฅ๋œ ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ๋Š” ์žฌ๋ฃŒ์˜ ๊ธฐ๊ณ„์  ์ธ์žฅํŠน์„ฑ ๋ณด๊ฐ•ํšจ๊ณผ๋Š” ๋ฐฐํ–ฅ๋˜์ง€ ์•Š์€ ์„ธํ”ผ์˜ฌ๋ผ์ดํŠธ์˜ ์ธ์žฅํŠน์„ฑ ๋ณด๊ฐ•ํšจ๊ณผ์™€ ๋น„๊ตํ•˜์—ฌ ๋”์šฑ ํšจ์œจ์ ์œผ๋กœ ๊ฐ•ํ™”๋˜๋Š” ๊ฒƒ์„ ํ™•์ธ ํ•˜์˜€๋‹ค. ๋‚˜๋…ธํด๋ ˆ์ด๋ฅผ PETG์™€ ๊ด‘๊ฒฝํ™” ์ˆ˜์ง€์— ์ ์šฉํ•˜์—ฌ 3D ํ”„๋ฆฐํŒ…์„ ์ง„ํ–‰ํ•˜์˜€์œผ๋ฉฐ ๊ธฐ๊ณ„์  ํŠน์„ฑ์ด ํ–ฅ์ƒ๋œ ๊ณ ๋ถ„์ž ๋‚˜๋…ธ๋ณตํ•ฉ์žฌ๋ฃŒ๋ฅผ ์ถœ๋ ฅํ•˜์˜€์œผ๋ฉฐ, 3D ํ”„๋ฆฐํŒ… ๊ณผ์ • ์ค‘ ์žฌ๋ฃŒ์˜ ์œ ๋ณ€ํ•™์  ๊ฑฐ๋™์— ์˜ํ•œ ๋‚˜๋…ธ๋ฐฐํ–ฅ ๊ตฌ์กฐ๋ฅผ ํ™•์ธํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ด๋ฅผ ํ†ตํ•˜์—ฌ ๊ธฐ๋Šฅ์„ฑ์ด ๋ถ€์—ฌ๋œ3D ํ”„๋ฆฐํŒ… ์žฌ๋ฃŒ๋ฅผ ์žฌ์กฐํ•˜๋ฉฐ ์‚ฐ์—…์  ์‘์šฉ ๋ฒ”์œ„๋ฅผ ํ™•๋Œ€ํ•ด ๋‚˜๊ฐˆ ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ์˜ˆ์ƒํ•œ๋‹ค.Chapter 1 Introduction 1 1. Literature review 7 1.1 3D printing 7 1.2 Fused deposition modelling (FDM) 12 1.3 UV-assisted 3D printing 16 1.4 Direct Ink Write (DIW) 20 1.5 Matrix-assisted 3D printing (MAP) 22 1.6 3D printing materials 24 1.7 FDM 3D printing with polymer composite material 26 1.8 Effects of fillers constituting polymer and photo-curable resin composites on rheological properties 28 1.9 Nano orientation of 3D printed materials 29 3. Objectives 31 3.1. 3D printing of PETG/sepiolite composites with nano orientation 31 3.2. Behavior and properties of UV curable polymer nanocomposites based on inorganic nanofillers for 3D printing 33 3.3. Embedded DIW 3D printing of UV curable resin/sepiolite composites with nano orientation 34 Chapter 2 3D printing of PETG/sepiolite composites with nano orientation 37 1. Introduction 38 2. Experimental 41 2.1. Materials 41 2.2 Preparation of PETG/sepiolite nanocomposite 44 2.3 Preparation of filaments for FDM 3D printing 46 2.4 Preparation of specimens 48 2.5 Characterizations 52 2.5.1. tensile test 52 2.5.2. Small-angle X-ray scattering (SAXS) 52 2.5.3. Transmission electron microscopy (TEM) 54 2.5.4. Scanning electron microscope (SEM) 54 2.5.5. Rheometer 54 2.5.6. Dynamic mechanical analysis (DMA) 55 2.5.7. Computer simulation 55 3. Results and Discussion 56 3.1 Rheological properties of PETG/SEP composite filaments 56 3.1.1. Rheological properties of molten state of PETG-SEP composite 56 3.1.2. Rheological properties of solid state of PETG-SEP composite 61 3.2 Mechanical properties of 3D printed samples 63 3.3 Morphological properties of PETG/SEP composites. 66 3.3.1. Observation of sepiolite by SEM 66 3.3.2. Observation of post-tensile fracture surface of injection-molded PETG composite by SEM 68 3.3.3. Observation of post-tensile fracture surface of horizontal direction 3D printed PETG composite by SEM 72 3.3.4. Observation of post-tensile fracture surface of vertical direction 3D printed PETG composite by SEM 76 3.3.5. Observation of 3D printed PETG composite by TEM 80 3.4 Anisotropic structure of SEP in the PETG 82 3.4.1. Orientation characteristics of SEP in injection molded composites 82 3.4.2. Orientation characteristics of SEP in 3D printed composites 84 3.4.3. Orientation characteristics of SEP in 3D printed composites in case of after tensile deformation 86 3.5 Simulation of the reinforcement effect of SEP in PETG 88 4. Conclusions 92 Chapter 3 UV curable polymer nanocomposites with inorganic nanofillers for 3D printing 94 1. Introduction 95 2. Experimental 98 2.1. Materials 98 2.2. Material mixing method and curing process 101 2.3. Characterizations 105 2.3.1. Rheological properties of surrey state composites 105 2.3.2. Rheological properties change during photocuring behavior 105 2.3.3. Rheological properties of photo cured composite materials 106 2.3.4. Mechanical Properties 106 2.3.5. Morphological properties 106 3. Results and Discussion 107 3.1 Rheological properties 107 3.1.1. Rheological properties of surrey state composites 107 3.1.2. Rheological properties change during photocuring behavior 110 3.1.3. Rheological properties of photo cured composite materials 112 3.2. Mechanical Properties 114 3.2.1. Tensile properties 114 3.2.2. Elastic modulus 115 3.2.3. Elongation at break 116 3.3. Transmission Electron microscopy (TEM) analysis 118 4. Conclusions 120 Chapter 4 Embedded DIW 3D printing of UV curable resin/sepiolite composites with nano orientation 122 1. Introduction 123 2. Experimental 127 2.1. Materials 127 2.2. Preparation of supporting matrix 129 2.3. Preparation of photocurable resin and sepiolite composite resin 129 2.4 Preparation of specimens 132 2.4.1. Digital light processing (DLP) 3D printing 132 2.4.2. Embedded DIW 3D printing (EMB3D) 132 2.4.3. Post curing of 3D printed materials 133 2.5 Characterizations 137 2.5.1. Rheological properties of supporting matrix 137 2.5.2. Rheological properties of photocurable resin 137 2.5.3. Rheological photocuring properties 138 2.5.4. Tensile test 138 2.5.5. Transmission electron microscopy (TEM) 139 2.5.6. Scanning electron microscope (SEM) 139 2.5.7. Dynamic mechanical analysis (DMA) 139 3. Results and Discussion 141 3.1 Rheological properties of matrix 141 3.1.1. Supporting matrix are rheologically considered in EMB3D printing 141 3.1.2. Rheological shear-thinning properties of supporting matrix 144 3.1.3. Yielding property of supporting matrix 147 3.1.4. Recovery property of supporting matrix 149 3.2. Rheological properties of photocurable composite resin 151 3.2.1. Rheological shear-thinning properties of photocurable composite resin 151 3.2.2. Yielding property of photocurable composite resin 155 3.2.3. Recovery property of photocurable composite resin 157 3.2.4. Rheological properties of photocurable composite resin at photocuring 159 3.2. Mechanical properties of 3D printed samples 161 3.2. Dynamic mechanical properties of 3D printed samples 167 3.3 Morphological properties of 3D printed samples. 169 3.3.1. Observation of sepiolite by SEM 169 3.3.2. Observation of post-tensile fracture surface of DLP printed sepiolite composite by SEM 171 3.3.3. Observation of post-tensile fracture surface of EMB3D printed sepiolite composite by SEM 173 3.3.5. Observation of EMB3D printed composite by TEM 175 4. Conclusions 177 Chapter 5 Concluding remarks 179 5.1. 3D printing of PETG/sepiolite composites with nano orientation 180 5.2. Behavior and properties of UV curable polymer nano composites based on inorganic nano fillers for 3D printing 181 5.3. Embedded DIW 3D printing of UV curable resin/sepiolite composites with nano orientation 182 5.4. Concluding 183 References 185 ์ดˆ ๋ก 204Docto

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ฑด์ถ•ํ•™๊ณผ,2004.Maste

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