• 대한치과교정학회지
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• 제34권3호
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• pp.253-260
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• 2004

치아의 활주 이동시 교정용 브라켓과 호선 사이의 마찰력은 많은 요인들, 예를 들면 브라켓과 호선의 크기, 형태 그리고 재료, 결찰방법 그리고 브라켓-호선간 각도 등과 관련이 있다. 이런 요인들 대부분에 관하여 명확한 결론이 내려져 있지만 브라켓 폭이 마찰력에 미치는 효과에 관해서는 논란이 있다. 이번 연구는 임상에서와 비슷한 모의 치아 이동시 브라켓 폭이 발생되는 마찰력의 양에 미치는 효과를 조사하기 위해 고안되었다. 폭이 다른 세 가지 브라켓 $(0.018{\times}0.025\;standard)$ 즉 좁은 것 (2.40mm), 중간 것 (3.00mm), 그리고 넓은 것(4.25mm) 등을 $0.016{\times}0.022$ 스테인레스 스틸 호선과 함께 사용하였다 세 가지 브라켓-호선 조합들은 분속 0.5mm로 4분 동안 장치 에서 움직이도록 하였고 각각 7회씩 반복 측정하였다. 생물학적인 상태를 재현하기 위해 치 아 치조 모형은 치근막과 유사한 탄성을 갖는 재료를 이용하는 간접법으로 제작되었다. 게다가 결찰력의 효과를 최소화하기 위하여 브라켓에 레진을 덧붙여서 고무로 결찰함으로써 브라켓 폭의 차이를 보상해주었다. 결과는 다음과 같다: 1. 각 브라켓-호선 조합의 최대 마찰력은; 좁은것(2.40mm): $m4.69gmf$ 중간것 (3.00mm): $72.7\pm54.98gmf$ 넓은것(4.25mm): $72.5\pm94.54gmf$ 2. 호선이 브라켓 슬롯을 지나서 나아갈수록 마찰력은 증가하였다. 3. ANOVA 사후검정 결과 임상과 비슷한 모의 실험에서 브라켓 폭은 마찰력에 아무런 영향을 미치지 않았다(p>0.05).

• 한국소성가공학회:학술대회논문집
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• 한국소성가공학회 2008년도 추계학술대회 논문집
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• pp.138-141
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• 2008

The effects of annealing temperature and time on mechanical properties and microstructures were investigated in cold drawn pearlitic steel wires. During annealing, the increment of the tensile strength at low temperatures found to be due to age hardening, while the decrease in the tensile strength at high temperatures was attributed to age softening, involving the spheroidization of lamellar cementite and recovery of lamellar ferrite. Since tensile strength and the occurrence of the delamination would be closely related to the dissolution of cementite, the lower annealing temperature and the increase of drawing strain caused the higher tensile strength and the easier occurrence of the delamination in cold drawn pearlitic steel wires.

• 대한치과보철학회지
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• 제38권1호
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• pp.59-72
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• 2000

This study was performed to investigate the effects of tooth mobility and design of the direct retainer on the stress of supporting tissues in distal extension removable partial denture. Tooth mobility was simulated and four different types of direct retainer such as Alters clasp, I-bar clasp, wrought wire clasp, and Dalbo attachment were designed and stress on the support-ing tissues were measured and analyzed with straingauge method. The following conclusions were drawn from this study. 1. The stress revealed at the lingual side of alveolar bone of the abutment tooth in edentulous area was the largest. 2. The stress at the lingual side of alveolar bone of the abutment tooth in edentulous area was increased according to the increase of tooth mobility in I-bar clasp and Dalbo attachment. 3. The stress at the residual ridge crest was the great in Dalbo attachment on mobility 0, in I-bar clasp on mobility 1, and in wrought wire clasp on mobility 2. 4. There was little changes of stress according to the increase of tooth mobility at buccal and lingual side of the residual ridge crest and around the abutment teeth in dentulous area.

• Structural Engineering and Mechanics
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• 제65권3호
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• pp.223-231
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• 2018

A numerical investigation of the impact of steel ductility on the strength and ductility of two-way corner and edge-supported concrete slabs containing low ductility welded wire fabric is presented. A finite element model was developed for the investigation and the results of a series of concurrent laboratory experiments were used to validate the numerical solution. A parametric investigation was conducted using the numerical model to investigate the various factors that influence the structural behavior at the strength limit state. Different values of steel uniform elongation and ultimate to yield strength ratios were considered. The results are presented and evaluated, with emphasis on the strength, ductility, and failure mode of the slabs. It was found that the ductility of the flexural reinforcement has a significant impact on the ultimate load behavior of two-way corner-supported slabs, particularly when the reinforcement was in the form of cold drawn welded wire fabric. However, the impact of the low ductility WWF has showed to be less prominent in structural slabs with higher levels of structural indeterminacy. The load-deflection curves of corner-supported slabs containing low ductility WWF are brittle, and the slabs have little ability to undergo plastic deformation at peak load.

• 한국주조공학회지
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• 제14권5호
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• pp.464-470
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• 1994

The horizontal continuous casting method with the heated mold was applied to study the solidification structures of the pure Al and Al-0.5wt%Si and Al-1.0wt%Si alloy rods. The results could be summarized as follows: 1. The S/L interface structures of pure Al represented the hexagonal cells at the casting speed of 590 and 350mm/min, respectively. However, the hexagonal cells became irregular as the casting speed and(or) Si amount increased. 2. The striation increased as the Si amount and casting speed increased and was found to result from the occurrence of growth twin crystals by XRD analysis. 3. The striation did not affect the mechanical and electrical property of the drawn wire from the casted rod. This means the striation is not a serious defect which has to consider in the production of micro-sized fine wire in the drawing process.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.104-107
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• 2001

In order to investigate the effect of Ge addition to the Cu matrix on the microstructure and the critical current density, four kinds of internal tin processed Nb$_3$Sn strands with pure Cu and Cu 0.2, 0.4, 0.6 wt % Ge alloys were drawn to 0.8 mm diameter. The microstructure and critical current of internal tin processed Nb$_3$Sn wires that were heat treated at temperatures ranging from 68$0^{\circ}C$ to 74$0^{\circ}C$ for 240h were investigated. The Ge addition to the matrix did not make workability worse. A Ge rich layer in the Cu-Ge matrix suppressed the growth of the Nb$_3$Sn layer and promoted grain coarsening. The greater the Ge content in the matrix, the lower the net Jc result after Nb$_3$sn reaction heat treatment. There was no significant variation in Jc observed with heat treatment temperature ranging from 68$0^{\circ}C$ to 74$0^{\circ}C$. The values of AC loss of Ge added wires were decreased to 40 % compare with no addition wire. Low AC loss was due to segregation of Ge rich layer in the Cu-Ge matrix. If Ge added wire with thin Nb filaments were fabricated, slow diffusion rate of Sn would be overcome and decreased AC loss that is weak Point of internal tin method.

• Progress in Superconductivity
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• 제10권2호
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• pp.79-86
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• 2009

We successfully fabricated C-doped ex-situ $MgB_2$ wires using two different methods such as mechanical alloying(MA) and combined process(CP) of in-situ and ex-situ. In the MA, the precursor powder was prepared with a mixture of $MgB_2$ and 1 at% C powders by planetary ball milling for 0-100 h. In the CP, on the other hand, C-doped $MgB_2$ powder was prepared with Mg, B, and C powders by in-situ process via compaction, sintering, and crushing. The powders prepared by two methods were loaded into Fe tube and then the assemblages were drawn by a conventional powder-in-tube technique. The MA treatment of C-added $MgB_2$ decreased the particles/grains size and resulted in C-doping into $MgB_2$ after sintering, improving the critical current density($J_c$) in high external magnetic field. For the C-doped $MgB_2$ wire by MA for 25 h, the $J_c$ was $4.1{\times}10^3A/cm^2$ at 5 K and 6.4 T, which was 5.9 times higher than that of pure and untreated $MgB_2$ wire. The CP also provided C-doping into $MgB_2$ and improved the $J_c$ in high magnetic field; the C-doped $MgB_2$ wire fabricated by CP exhibited a $J_c$ being 2.3 times higher than that of the ex-situ wire used commercial $MgB_2$ powder at 5 K and 6.0 T($2.7{\times}10^3A/cm^2\;vs.\;1.2{\times}10^3A/cm^2$).

• 대한치과교정학회지
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• 제31권3호
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• pp.335-346
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• 2001

본 연구의 목적은 교정치료의 마무리 단계에서 비람직하지 못한 순설측 경사를 가진 한 개 치아의 이동을 원할 때 브라켓 슬롯의 크기와 각형선재의 종류, 크기에 따라 부여하여야 할 적절한 임상적 torque (SWA의 각형선재에서 나머지 편평한 부분과 이동을 위해 변형시킨 부분의 단면이 이루는 각도만큼의 torque)의 양을 구하고자 하는 것이다. 임상적 torque는 play와 active torque(브라켓에 모멘트를 전달할 수 있는 torque)의 합으로 구성되는데, play는 수학적 공식을 이용하여 계산하였고 active torque는 컴퓨터를 이용한 삼차원 유한요소법으로 구하였다. 유한요소모델은 일렬로 배열된 세 개의 브라켓과 여기에 삽입된 stainless steel, TMA , NiTi 이렇게 3가지 종류의 교정용 각형선재로 구성된 다. 양쪽의 브라켓을 일정한 각도로 비틀어서 가운데 브라켓에 발생하는 모멘트를 계산하였다. 선재의 크기는 많이 사용되는 각형선재인 .016"X.022", .017"X.022", .017"X.025", .018"X.025", .019"X.025", .020"X.025". .021"X.025"의 7개로 디자인하였다. .018" 브라켓에는 .016"X.022", .017"X.022", .017"X.025" 선재를 삽입하여 실험하였고, .022" 브라켓에는 .016"X.022" 선재를 제외한 나미지 선재를 삽입하여 실험하였다. 실험으로 다음과 같은 결과를 얻었다. 1. 삽입된 브라켓 슬롯의 크기에 상관없이 같은 크기와 재질의 교정용 각형선재에 같은 active torque를 가하면 동일한 모멘트가 발생하였다. 2. 선재의 크기가 증가될 수록 동일한 active torque에 의해 발생되는 모멘트의 양은 증가하였다. 실험에 사용한 가장 굵은 선재인 .021"X.033" 선재는 동일한 재질의 가장 가는 .015"X.022" 선재에 비해 약 1.75배 더 큰 torsional stiffness를 가졌다. 3. 선재의 재질에 따라서는 stainless steel, TMA, NiTi순으로 torsional stiffness가 감소하였는데 stainless steel에 비해 TMA는 0.35배, NiTi는 0.16배였다. 4. 브라켓간 거리의 증가와 발생되는 torsional .stiffness는 반비례하였다. 브라켓간 거리의 증가에 의해 감소되는 torsional stiffness의 비율은 선재의 재질과 상관이 있었고 크기에 따라서는 큰 차이가 없었다. 5. 교정치료의 마무리 단계에서 이상적인 순설측 경사이동을 일으키는 임상적 torque의 공식과 값을 구하였다.

• 한국소성가공학회:학술대회논문집
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• 한국소성가공학회 2003년도 춘계학술대회논문집
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• pp.307-310
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• 2003

Non-heat treated steels are attractive in the steel-wire industry since the spheroidization and quenching-tempering treatment are not involved during the processing. In this study, three different steels such as dual phase steel, low-Si steel, and ultra low carbon bainitic steel were used to investigate their deformation resistance and forming limit. Deformation resistance was estimated by calculating the deformation energy and the forming limit was evaluated by measuring the critical strain revealing crack initiation at the notch tip of the specimens. The results showed that deformation resistance was the lowest in the low-Si steel, and the forming limit strain was the highest in the ultra low carbon bainitic steel.

• 수산해양기술연구
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• 제28권2호
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• pp.157-163
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• 1992

In this paper, the relationship between static pressure recovery and turbulent energy was presented in case of swirling flows into a conical diffuser. The distributions of turbulent energy in a diffuser sectional area were measured by a hot wire anemometer. The following conclusion can be drawn from the experiment. Diffuser loss is constituted by a dynamic pressure loss and total pressure loss. The static pressure recovery depends strongly on the total pressure loss. The static pressure recovery depends strongly on the total pressure loss, and the turbulent energy varies inversely as the static pressure recovery coefficient.