• 대한소아치과학회지
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• 제23권4호
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• pp.818-839
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• 1996

The strain gage, holographic and photoelastic analysis etc. have been used for stress analysis of prosthesis, orthodontic or orthopedic appliances and filling materials. But these methods has some limitation in analyzing the internal stress. The Finite Element Analysis has been proved to compensate this defect and widely used in this area. The purpose of this study was to compare the stress distributions of the various temporary filling methods being used in pulpotomy procedure. Three different models were designed according to temporary filling material and method: amalgam filling with ZOE base(Model I), amalgam filling with ZPC sub-base and ZOE(Model II), IRM filling only(Model III). The results of the experiment were as follows: 1. In model I under the load case 6 and 1, the significant stress was shown to be concentrated on the buccal portion of crown. 2. Model II showed the similar pattern of stress distribution to Model I. 3. In model III under load case 2, the stress was mainly distributed on the buccal cusp tip and buccal margin of filling material. In same model under the load case 3, the stress was distributed on the lingual cusp tip. 4. Based on the above data, IRM can be assumed to have advantage over the other tested materials in reducing the incidence of crown fracture by localized the stress within the filling materials.

• 대한치과보철학회지
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• 제31권3호
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• pp.303-316
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• 1993

The purpose of this study was to analysis the stress distribution induced by three unit PFM bridges and various cantilever bridges replacing maxillary latersal incisor. The simplified two-dimensional photoelastic models used for this study was contructed in the folio- wing way. CR/R ratio was designed to be 1 : 1, 1 : 1.25 and 1 : 1.5. The pontics of cantilever bridge supported by maxillary canines consisted of wrap-around type, rest-extension type, and simple type. 3-unit PFM bridge was constructed with traditional method. 1kg vertical static load was applied on the center of the incisal edge of the pontic. The stress pattern was examined and recorded by photography. The results obtained were as follows ; 1. The magnitude of stress on the abutment root apex area of a traditional 3-unit bridge was the lowest. 2. The model of cantilevered pontic with a rest showed the relatively well distributed stress around the abutment tooth. The model with simple pontic generated the greatest stress concentration in the supporting structure of the abutment tooth. 3. As the height of bone level reduced, the rotational and vertical force increased around the abutment tooth. 4. The stress concentration of the 3-unit bridges occured on the root apex and stress concentration of the cantilever briage occured on the root apex and cervix area, 5. In the case of the cantilever bridge, stress concentrated distally on the root apex area of the abutment tooth and additional stress was observed mesially on the upper part of the root. Especially in the case of the simple pontic, was phenomenon was more apparent than the others. 6. Force applied to cantilevered pontic was transmitted to the adjacent central incisor through the contact surface. Stress was markedly observed on the mesial cervix area in the case of simple pontic and on the root apex area in the case of wrap-around type and rest-extension type.

• 한국정밀공학회지
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• 제1권3호
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• pp.85-94
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• 1984

The WILDHABER-NOVIKOV gear, one of the circular arc gears, has the large contact area between the convex and concave profiled mating teeth, moves from one end of the tooth to the other axially making a face contact. Hence it provides a large load capacity than the Involute gear and still satisfying the law of gearing. In order to analyze the gear stress, a photoelastic investigation was carried out. Photo elastic model of the WILDHABER-NOVIKOV gears were made of Araldite CT200 in this investigation. For both the many teeth gear and the few teeth gear segments, External gears of all addendum type WILDHABER-NOVIKOV gear and the involute gear were tested. Included were the models with various profile raddi at the same pressure angle 20 .deg. and module 13.5. The flank stresses and fillet stresses of these gears were observed in each case and compared with those of gears. From this investigation, the following results were obtained. A. In the case of having many teeth gear: As the profile radius is increased, the fillet stresses of the WILDHABER-NOVIKOV gear become the same or less than that of the INVOLUTE gea, and the flank stress becomes smaller than that of the INVOLUTE gear. Therefore the better design condition is satisfied with a large profile radius. B. IN the case of having a few teeth gear: As the profile radius is increased the flank stress of WILDHABER-NOVIKOV gear becomes smaller than that of the INVOLUTE gear, but the fillet stresses become larger than that of the INVOLUTE gear. Therefore the larger design condition is satisfied with small profile radius.

• Journal of Yeungnam Medical Science
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• 제6권2호
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• pp.223-239
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• 1989

요추의 중립위, 굴곡위 및 신전위에서의 응력 분포의 차이와 수핵의 유무에 따른 응력 분포의 변화를 관찰하기 위해 본 연구를 시행하였으며 등색선의 양상을 관찰하고 그 응력을 해석하여 다음과 같은 결론을 얻었다. 1. 기립 중립위에서는 수핵이 있는 경우는 전방 부위보다 후방부위에 고응력이 집중되었으며, 전후방 모두 내측부와 중간부위가 고응력이고 외측부로 이동할수록 저응력이 관찰되었다. 수핵이 없는 경우는 후방보다 전방부에 고응력이 집중되었으며 국소적으로 응력이 집중되는 양상을 보이고 있다. 2. 최대 굴곡위에서는 수핵의 존재에 관계없이, 전방보다 후방부가 고응력이 집중되었으며, 수핵 유무 비교시 수핵이 있는 경우가 없는 경우보다 전방이 저응력, 후방은 거의 동등한 응력 분포를 나타내었다. 응력 분포도의 분석에 의하면 전반적으로 균등한 응력 분포 양상을 나타냈다. 3. 최대 신전위에서는 수핵 유무에 관계없이 전방부에 고응력, 후방부에 저응력, 내측에 고응력, 외측은 저응력을 나타내었으며, 수핵이 있는 경우 없는 경우보다 고응력을 나타냈다. 4. 기립 중립위와 최대 굴곡위의 비교에서는 기립 중립위보다 굴곡시 수핵의 유무에 관계없이 전반적으로 후방부 응력이 2차 정도 현저히 감소하는 양상을 보이면서 비교적 균등한 응력 분포를 나타냈다. 5. 최대 신전위와 최대 굴곡위의 비교에스는 수핵 존재시 최대 신전위보다 최대 굴곡위에서 응력 분포가 전후방 모두 2차 정도 감소되고 수핵이 없는 경우는 최대 신전위가 굴곡위보다 응력이 전후방 0.5차 정도 감소되었다.

• 대한치과보철학회지
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• 제31권2호
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• pp.271-300
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• 1993

The purpose of this study was to analyze the stress distribution at supporting bone according to the types of connection modality between implant and tooth in the superstrcture. This investigation evaluated the stress patterns in a photoelastic model produced by three different types of dental implants such as Branemark, Steri-Oss, IMZ and resin tooth using the techniques of quasi three dimensional photoelasticity. The teeth-supported bridge had a first molar pontic supported by second premolar and second molar as a control group. The implant and toothsupported bridge had a first molar pontic supported by second premolar and implant posterior retainer as an experimental group. Prostheses were mechanically connected to an adjacent second premolar by the rigid of nonrigid connection, Nonrigid connection used an attachment placed between the tooth-supported and fixture-supported component. The female(keyway) of attachment was placed on the distal end of the retainer supported by the tooth ; the male(Key) of attachment connected to the osseointegrated bridge was engaged into the keyway. All prostheses were casted in the same nonprecious alloy and were cemented and screwed on their respective abutments and implants. 16㎏ of vertical loads on central fossae of second premolar, first molar pontic, implant of second molar were applied respectively and 6.5㎏ of inclined load on middle buccal surface of first molar pontic was applied. The results were as follows : 1. Under the vertical load on the central fossa of first mloar pontic, the stress developed at the apex of tooth of implat was more uniformly distributed in the case of nonrigid connection than in the case of rigid connection. 2. Under the vertical load on the central fossa of first molar pontic, the stress developed around the cervical area of tooth of implant was larger in the case of rigid connection than in the case of nonrigid connection because the bending moment was more occured in the case of rigid connection than in the case of nonrigid connection. 3. Stress was more restricted to the loaded side of nonrigid connection than to that of rigid connection 4. Under the inclined load. The set screw loosening of implant was more easily occured in the case of nonrigid connection than in the case of rigid connection due to torque moment. 5. In the case of Branemark implant, the stress concentration in second premolar was larger and the stress developed around the cervical area of implant was lower than any other cases under the vertical load, because Branemark implant with the flexible gold screw was showed in incline toward second premolar by a bending moment. 6. The stress developed around the apex of tooth or implant was more uniformly distributed in the case of Steri-Oss implant with stiff screw than in the case of Branemark implant under the vertical load. But, the stress developed around the cervical area of the Steri-Oss implant was larger than that of any other implants because bending moment was occured by vertical migration of second premolar. 7. The stress distribution in the case of IMZ implant was similar to the case of natural teeth under small vertical load. But, the residual stress around the implant was showed to occurdue to deformation of IMC and sinking of screw under larger vertical load.

• 대한치과교정학회지
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• 제31권3호
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• pp.325-333
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• 2001

바람직한 교정치료는 최적의 교정력을 치아에 가하여 정확하게 치아이동을 조절하고 예측함에 따라 가능해진다. 치관에 힘과 모멘트가 동시에 적용될 때 그 비율(M/F ratio)에 따라 치주인대에 나타나는 응력 분포가 변화하게 되고 이에 따른 회전중심의 위치가 변하게 되는데 이런 양상을 파악함으로써 정확한 치아이동을 조절하고 예측할 수 있다. 본 연구에서는 교정력에 따른 치주인대 및 치조골 부위에서의 응력 분포를 알아보기 위하여 상악 중절치 치근 8부위에 스트레인 게이지를 부착한 인공 치아를 광탄성 레진에 매식한 4mm 정중이개 증례의 상악 전치부 실험모형을 제작하여 응력 분포를 조사하였다. 폐쇄 방법으로 다음과 같은 3가지 방법을 적용하였다. 1. 금속 호선의 삽입 없이 100g의 힘을 발휘하는 elastomeric chain만 사용한 경우, 2. .016" 금속호선을 삽입하고 elastomeric chain을 사용한 경우, 3. .016“x.022” 금속호선을 삽입하고 elastomeric chain을 사용한 경우. 각각의 경우에서 치근의 근심면, 원심면 및 순면, 설면에 나타나는 응력을 계측하여 비교 분석한 결과 다음과 같은 결론을 얻었다. 1. 치근 부착 스트레인 게이지를 이용한 응력 분포 조사 방법으로 치아이동시 치근의 근 원심면 및 순 설면에서의 응력 분포를 파악할 수 있었으며 이에 따른 모멘트 팔의 형성을 추정함으로써 치아의 회전양상을 알 수 있었다. 2. 호선없이 교정력을 적용한 경우 정출 및 경사이동이 컸으며 호선 적용에 따라 압하 및 치체이동 양상을 보이는 것을 응력 분포 파악을 통해 확인할 수 있었다.

• 예술인문사회 융합 멀티미디어 논문지
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• 제7권2호
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• pp.437-444
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• 2017

기계구조물 부재의 단면에 구멍이나 또는 단면이 급격히 변화할 경우, 불연속 부분 주위에서 응력집중이 일어나며 파손이 발생하는 주요 원인이 된다. 그 이유는 부재에 작용하는 평균 응력보다 응력집중 부분에서 훨씬 큰 응력이 작용하기 때문이다. 본 논문에서는 시편의 부분 관통 구멍 주위에서 응력해석을 수행하여 구멍을 통과하는 선상의 주응력 차 값을 구하였다. 광탄성에서 최대주응력과 최소주응력의 차이는 등색프린지 차수와 재료의 프린지 상수를 곱한 값을 빛이 통과한 거리 즉, 시편의 두께로 나눈 값과 같다. 즉, 주응력의 차이는 광탄성 프린지 차수와 비례관계가 있으므로 유한요소해석에 의한 주응력 차이의 분포를 광탄성 실험결과에 비교할 수 있다. 유한요소 범용 소프트웨어인 ANSYS Workbench를 이용하였으며 유한요소법으로 해석된 값을 광탄성 실험으로부터 측정된 값과 비교한 결과 유사한 결과를 얻었다. 이로서 유한요소해석 결과는 실험결과와의 비교를 통해 타당성이 입증될 수 있었다. 또한 구멍깊이 변화에 따라 나타나는 응력분포를 사용하여 응력집중계수를 구하였다. 구멍깊이가 증가할수록 응력집중계수는 증가함을 나타냈다.