• 제목/요약/키워드: 250 mm Depth

검색결과 65건 처리시간 0.024초

복합 레진으로 수복된 세 가지 첨와형태 와동의 파절 저항성에 관한 연구 (FRACTURE RESISTANCE OF THE THREE TYPES OF UNDERMINED CAVITY FILLED WITH COMPOSITE RESIN)

  • 최훈수;신동훈
    • Restorative Dentistry and Endodontics
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    • 제33권3호
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    • pp.177-183
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    • 2008
  • 심미성 복합레진은 자연 치질을 보존시키며 나아가 잔존 치질의 강도를 강화시켜 준다. 복합레진 수복시 더 많은 치질을 남기기 위해 첨와 (undercut) 형태의 교합면 치질을 남긴 채 복합레진으로 수복하는 경우가 많으나, 어느 정도 강도가 복원되는지에 대해서는 잘 알려져 있지 않다. 이에 본 연구에서는 첨와 형태의 와동을 잔존 치질의 두께 (법랑질 / 법랑질과 상아질)에 따라 형성하고 복합레진으로 충전한 경우, 수복된 치아의 파절 저항성을 손상이 없는 자연치와 비교평가하였다. 상악 대구치 40개의 교합면을 편평하게 삭제한 후 방사선 사진에서 치수각의 위치를 확인하였다. 대상 치아를 각 10개씩 4개군으로 분류하였으며, 1$\sim$3군은 실험군으로 모두 협측에 깊이 7 mm, 근원심 폭경 5 mm의 첨와 형태 와동을 형성하였고, 와동저에서 치수각까지의 거리를 약 0.5 mm로 유지하였으며 교합면쪽의 치질 두께를 달리하였다. 1군은 법랑질과 소량의 상아질로 구성된 치질 두께를 1 mm, 2군은 법랑질과 상아질의 두께를 1.5 mm, 3군은 법랑질과 상아질의 두께를 2 mm가 되도록 하였고, 4군은 건전한 자연치를 와동형성 없이 대조군으로 사용하였다. 두께 측정은 방사선 사진을 스캔한 후 길이 확대 프로그램을 이용하였다. 각 와동을 37% 인산으로 산부식한 다음 단일병 접착제 Single $Bond^{TM}$ (3M/ESPE, USA)를 적용하였고 혼합형 복합레진 Filtek $SZ-250^{TM}$ (3M/ESPE, USA)을 사용하여 적층 충전하였다. 치아를 실온에서 증류수에 24시간 동안 보관한 다음 Sof-Lex system (3M/ESPE, USA)을 사용하여 연마하였다. 이후 자가중합형 레진에 교합면을 기저부에 평행한 상태로 치근부를 매몰한 다음 Universal testing machine (Zwick Z010, Germany)에서 지름 3 mm의 staineless steel rod를 1 mm/min의 cross-head speed로 하중을 가하여 파절 강도를 측정하였다. 통계 분석은 95% 유의 수준의 One-way ANOVA와 Tukey test를 이용하였으며 다음과 같은 결과를 얻었다. 1. 와동 형성 후 복합레진을 수복한 군들은 대조군에 비해 약 75%의 파절 강도를 보였다. 2. 교합면쪽 잔존 치질의 두께에 따른 파절 저항은 유의한 차이를 보이지 않았다 (p > 0.05). 복합레진을 이용하여 첨와 형태의 와동을 수복한 후 파절 강도를 측정한 결과 건전 치아보다는 강도가 낮았지만, 상부의 잔존 치질이 대부분 법랑질로 이루어진 경우에도 복합 레진으로 수복하면 건전 치아 파절 강도의 75%까지 유지할 수 있다는 결론을 얻었다.

부재 두께 변화에 따른 콘크리트의 초기동해 특성 분석 및 깊이진단 (Early Frost Damage and Diagnose of Damage Depth Due to Early Frost Damage of the Concrete According to the Thickness of Members)

  • 김태우;한민철
    • 한국건축시공학회지
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    • 제19권2호
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    • pp.131-138
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    • 2019
  • 최근에는 열악한 환경에 노출되는 콘크리트 구조물의 품질 확보에 대하여 관심이 증대되고 있다. 그 중에서 낮은 외 기온 조건에서의 초기양생 불량은 콘크리트 구조물의 초기 동해 피해를 일으킬 수 있는 것으로 알려지고 있다. 그러므로 본 연구에서는 겨울철 외기온 조건에서 결합재 종류 및 콘크리트 부재 두께 변화가 콘크리트의 초기동해 깊이에 미치는 영향 분석 및 초기동해 피해를 입은 구조체에 대하여 그 깊이를 명확히 판정하고자 하였다. 실험결과 초기동해피해의 경우 3성분계 혼합시멘트를 사용하고, 부재 두께가 얇을수록 초기동해 깊이가 깊고 코어 공시체의 명도 증가가 지연되었는데, 이는 초기발열량 저하로 콘크리트의 조직 이완이 용이하게 발생하여 흡수율이 증가하기 때문인 것으로 분석된다. 초기동해 깊이 판정은 24시간 침수 후 온도 $20^{\circ}C$, 상대습도 60 %전후인 실내에서 30분 전후로 건조를 시킬 경우 명도값(L) 45 이하의 짙은색과 밝은색으로 구별되는데, 짙은 색부분을 버니어캘리퍼스 등으로 측정하면 손쉽게 판단할 수 있다.

초소수력발전용 좁은 수로 고정형 수직수차 성능실험 (Experiments on Efficiency of Standing Type Waterwheel with Narrow Canal for Micro/Small Scale Hydro Power Plant)

  • 김동진;이경호;안국찬;김봉환;이치우
    • 한국기계가공학회지
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    • 제11권5호
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    • pp.104-108
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    • 2012
  • Recently, small scale hydropower needs to be developed due to its clean, renewable and abundant energy resources. However, suitable draft of hydro-turbine body in combination with differences in wheel blade shapes is not determined yet in the range of small hydropower and it is necessary to study for the effective draft in combination with type. Therefore, watermill shaped of 250mm diameter. hydro-turbine aiming 20 watt class generator is adopted in this study because of its simple structure and high possibility of applying to small hydropower. The result shows that effective draft for the turbine body is variable concerning the size of turbine and flow rate of water. Thus, the difference of water depth between fore and aft turbine body contributes to the increase of torque, angular momentum and power output.

AC8A-T6 알루미늄 합금재의 절삭가공 특성에 관한 연구 (A Study on the Characteristics of Machining for AC8A-T6 Aluminum Alloy)

  • 최현민;김경우;김우순;김용환;김동현;채왕석
    • 한국공작기계학회:학술대회논문집
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    • 한국공작기계학회 2002년도 추계학술대회 논문집
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    • pp.192-197
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    • 2002
  • In this study, examined the cutting characteristics of alumuminum alloy AC8A-T6 that is used to present car piston materials. And in been holding materials machining empirically escape as result that experiment comparison changing the cutting speed and feed on various condition to choose efficient machining condition. The following results can be summarized from this research. 1. As the cutting speed decreased, principal cutting force and thrust cutting force is increased, and reason that cutting force interacts greatly in the low cutting speed is thought by result by BUE's stabilization. 2. The feed speed and cutting speed increase, friction factor is decrescent and the cause appeared the thrust cutting force is fallen than cutting force relatively because chip flow according to increase of the feed rate is constraint. 3. Though specific cutting resistance grows cutting area and the feed rate are few, the cause was expose that shear angle decreases by rake face of tool gets into negative angle remarkably as wear of a cutting tool or defect part of workpiece is cut. 4. Cutting speed do greatly depth of cut is slow, surface roughness examined closely through an experiment that becomes bad, and know that it can get good surface that process cutting speed because do feed rate by 0.1mm/rev low more than 250m/min to get good surface roughness can.

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Soil Carbon Cycling and Soil CO2 Efflux in a Red Pine (Pinus densiflora) Stand

  • Kim, Choon-Sig
    • Journal of Ecology and Environment
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    • 제29권1호
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    • pp.23-27
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    • 2006
  • This study was conducted to evaluate forest carbon cycling and soil $CO_2$ efflux rates in a 42-year-old pine (Pinus densiflora) stand located in Hamyang-gun, Korea. Aboveground and soil organic carbon storage, litterfall, litter decomposition, and soil $CO_2$ efflux rates were measured for one year. Estimated aboveground biomass carbon storage and increment in this stand were $3,250gC/m^2\;and\;156gC\;m^{-2}yr^{-1}$, respectively. Soil organic carbon storage at the depth of 30 cm was $10,260gC/m^2$ Mean organic carbon inputs by needle and total litterfall were $176gC\;m^{-2}yr^{-1}\;and\;235gC\;m^{-2}yr^{-1}$, respectively. Litter decomposition rates were faster in nne roots less than 2 mm diameter size ($<220\;g\;kg^{-1}yr^{-1}$) than in needle litter ($<120\;g\;kg^{-1}yr^{-1}$). Annual mean and total soil respiration rates were $0.37g\;CO_2m^{-2}h^{-1}$ and $2,732g\;CO_2m^{-2}yr^{-1}$ during the study period. A strong positive relationship existed between soil $CO_2$ efflux and soil temperature (r=0.8149), while soil $CO_2$ efflux responded negatively to soil pH (r=-0.3582).

공동주택 현장 측정자료를 활용한 중량충격원의 바닥충격음 차단성능 비교 (Comparison of Impact Sound Insulation Performances of Apartment Floors Against Heavy-weight Impact Sources via Field Measurement Data)

  • 윤창연;연준오;김명준
    • 한국소음진동공학회논문집
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    • 제24권8호
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    • pp.651-658
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    • 2014
  • Notification 2013-611 of MOLIT has come into effect. It relates primarily to new standard impact source. In this study, an in-depth experimental analysis of the difference between a bang machine and an impact ball was performed via field testing of shear wall and flat plate structure at 51 sites. This paper focuses on the difference in single number quantities between a bang machine and an impact ball. At wall thicknesses of 180 and 210 mm in shear wall structure, the single number quantities exhibited differences of 3.1 and 4.5 dB, respectively, and at thicknesses exceeding 250 mm in flat plate structure, the difference was constant at 4.6 dB. With regard to flat plate structures, the single-index difference increased up to 11 dB as the thickness of the floor slab increased. In general, the highest level of contribution for the bang machine was 63 Hz, irrespective of thickness determining bandwidth. The highest level for the impact ball were 63 Hz and 125 Hz. In future research, when reviewing additional field performance measurement data, it will be necessary to consider a detailed examination instead of the current method of uniformly adding 3 dB for all thicknesses and types of structures.

임플랜트 식립부위 형성시 골조직의 온도변화에 관한 연구 (A STUDY ON THE TEMPERATURE CHANGES OF BONE TISSUES DURING IMPLANT SITE PREPARATION)

  • 김평일;김영수;장경수;김창회
    • 대한치과보철학회지
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    • 제40권1호
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    • pp.1-17
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    • 2002
  • The purpose of this study is to examine the possibility of thermal injury to bone tissues during an implant site preparation under the same condition as a typical clinical practice of $Br{\aa}nemark$ implant system. All the burs for $Br{\aa}nemark$ implant system were studied except the round bur The experiments involved 880 drilling cases : 50 cases for each of the 5 steps of NP, 5 steps of RP, and 7 steps of WP, all including srew tap, and 30 cases of 2mm twist drill. For precision drilling, a precision handpiece restraining system was developed (Eungyong Machinery Co., Korea). The system kept the drill parallel to the drilling path and allowed horizontal adjustment of the drill with as little as $1{\mu}m$ increment. The thermocouple insertion hole. that is 0.9mm in diameter and 8mm in depth, was prepared 0.2mm away from the tapping bur the last drilling step. The temperatures due to countersink, pilot drill, and other drills were measured at the surface of the bone, at the depths of 4mm and 8mm respectively. Countersink drilling temperature was measured by attaching the tip of a thermocouple at the rim of the countersink. To assure temperature measurement at the desired depths, 'bent-thermocouples' with their tips of 4 and 8mm bent at $120^{\circ}$ were used. The profiles of temperature variation were recorded continuously at one second interval using a thermometer with memory function (Fluke Co. U.S.A.) and 0.7mm thermocouples (Omega Co., U.S.A.). To simulate typical clinical conditions, 35mm square samples of bovine scapular bone were utilized. The samples were approximately 20mm thick with the cortical thickness on the drilling side ranging from 1 to 2mm. A sample was placed in a container of saline solution so that its lower half is submerged into the solution and the upper half exposed to the room air, which averaged $24.9^{\circ}C$. The temperature of the saline solution was maintained at $36.5^{\circ}C$ using an electric heater (J. O Tech Co., Korea). This experimental condition was similar to that of a patient s opened mouth. The study revealed that a 2mm twist drill required greatest attention. As a guide drill, a twist drill is required to bore through a 'virgin bone,' rather than merely enlarging an already drilled hole as is the case with other drills. This typically generates greater amount of heat. Furthermore, one tends to apply a greater pressure to overcome drilling difficulty, thus producing even greater amount heat. 150 experiments were conducted for 2mm twist drill. For 140 cases, drill pressure of 750g was sufficient, and 10 cases required additional 500 or 100g of drilling pressure. In case of the former. 3 of the 140 cases produced the temperature greater than $47^{\circ}C$, the threshold temperature of degeneration of bone tissue (1983. Eriksson et al.) which is also the reference temperature in this study. In each of the 10 cases requiring extra pressure, the temperature exceeded the reference temperature. More significantly, a surge of heat was observed in each of these cases This observations led to addtional 20 drilling experiments on dense bones. For 10 of these cases, the pressure of 1,250g was applied. For the other 10, 1.750g were applied. In each of these cases, it was also observed that the temperature rose abruptly far above the thresh old temperature of $47^{\circ}C$, sometimes even to 70 or $80^{\circ}C$. It was also observed that the increased drilling pressure influenced the shortening of drilling time more than the rise of drilling temperature. This suggests the desirability of clinically reconsidering application of extra pressures to prevent possible injury to bone tissues. An analysis of these two extra pressure groups of 1,250g and 1,750g revealed that the t-statistics for reduced amount of drilling time due to extra pressure and increased peak temperature due to the same were 10.80 and 2.08 respectively suggesting that drilling time was more influenced than temperature. All the subsequent drillings after the drilling with a 2mm twist drill did not produce excessive heat, i.e. the heat generation is at the same or below the body temperature level. Some of screw tap, pilot, and countersink showed negative correlation coefficients between the generated heat and the drilling time. indicating the more the drilling time, the lower the temperature. The study also revealed that the drilling time was increased as a function of frequency of the use of the drill. Under the drilling pressure of 750g, it was revealed that the drilling time for an old twist drill that has already drilled 40 times was 4.5 times longer than a new drill The measurement was taken for the first 10 drillings of a new drill and 10 drillings of an old drill that has already been used for 40 drillings. 'Test Statistics' of small samples t-test was 3.49, confirming that the used twist drills require longer drilling time than new ones. On the other hand, it was revealed that there was no significant difference in drilling temperature between the new drill and the old twist drill. Finally, the following conclusions were reached from this study : 1 Used drilling bur causes almost no change in drilling temperature but increase in drilling time through 50 drillings under the manufacturer-recommended cooling conditions and the drilling pressure of 750g. 2. The heat that is generated through drilling mattered only in the case of 2mm twist drills, the first drill to be used in bone drilling process for all the other drills there is no significant problem. 3. If the drilling pressure is increased when a 2mm twist drill reaches a dense bone, the temperature rises abruptly even under the manufacturer-recommended cooling conditions. 4. Drilling heat was the highest at the final moment of the drilling process.

복합레진 수복시 와동의 크기 및 수복 방법이 교두 굴곡에 미치는 영향 (INFLUENCE OF CAVITY SIZE AND RESTORATION METHODS ON THE CUSP DEFLECTION IN COMPOSITE RESTORATION)

  • 이미라;이인복;석창인;이상탁;엄정문
    • Restorative Dentistry and Endodontics
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    • 제29권6호
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    • pp.532-540
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    • 2004
  • The aim of this study was to measure the cusp deflection during composite restoration for MOD cavity in premolar and to examine the influence of cavity dimension, C-factor and restoration method on the cusp deflection. Thirty extracted maxillary premolar were prepared to four different sizes of MOD cavity and divided into six groups. The width and depth of the cavity were as follows. Group 1; $1.5{\;}{\times}{\;}1{\;}mm$, Group 2; $1.5{\;}{\times}{\;}2{\;}mm$, Group 3; $3{\;}{\times}{\;}1{\;}mm$, and Group 4-6; $3{\;}{\times}{\;}2{\;}mm$ respectively. Group 1-4 were restored using bulk filling method with Z-250 composite. However, Group 5 was restored incrementally, and Group 6 was restored with an indirect resin inlay. The cusp deflection was recorded at the buccal and lingual cusp tips using LVDT probe for 10,000 seconds. The measured cusp deflections were compared between groups, and the relationship between the cube of the length of cavity wall/the cube of the thickness of cavity wall ($L^3/T^3$). C-factor and cusp deflection or % flexure ($100{\;}{\times}$ cuspal deflection / cavity width) was analyzed. The cusp deflection of Group 1-4 were $12.1{\;}\mu\textrm{m},{\;}17.2{\;}\mu\textrm{m},{\;}16.2{\;}\mu\textrm{m}{\;}and{\;}26.4{\;}\mu\textrm{m}$ respectively. The C-factor was related to the % flexure rather than the cusp deflection. There was a strong positive correlationship between the $L^3/T^3$ and the cusp deflection. The cusp deflection of Group 5 and 6 were $17.4{\;}\mu\textrm{m}{\;}and{\;}17.9{\;}\mu\textrm{m}$ respectively, which are much lower value than that of Group 4.

Effect of Hydride Reorientation on Delayed Hydride Cracking In Zr-2.5Nb Tubes

  • Yun Yeo Bum;Kim Young Suk;Im Kyung Soo;Cheong Yong Moo;Kim Sung Soo
    • Nuclear Engineering and Technology
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    • 제35권6호
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    • pp.529-536
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    • 2003
  • The objective of this study is to investigate the reorientation of hydrides with applied stress intensity factor, the peak temperature and the time when to apply the stress intensity factor in a Zr-2.5Nb pressure tube during its thermal cycle treatment. Cantilever beam (CB) specimens with a notch of 0.5 mm in depth made from the Zr-2.5Nb tube were subjected to electrolytic hydrogen charging to contain 60 ppm H and then to a thermal cycle involving heating to the peak temperature of either 310 or $380^{\circ}C$, holding there for 50 h and then cooling to the test temperature of $250^{\circ}C$. The stress intensity factor of either 6.13 or $18.4\;MPa\sqrt{m}$ was applied at the beginning of the thermal cycle, at the end of the hold at the peak temperatures and after cooling to the test temperature, respectively. The reorientation of hydrides in the Zr-2.5Nb tube was enhanced with the increased peak temperature and applied stress intensity factor. Furthermore, when the CB specimens were subjected to $18.4\;MPa\sqrt{m}$ from the beginning of the thermal cycle, the reoriented hydrides occurred almost all over the Zr-2.5Nb tube, surprisingly suppressing the growth of a DHC crack. In contrast, when the CB specimens were subjected to the stress intensity factor at the test temperature, little reorientation of hydrides was observed except the notch region, leading the Zr-2.5Nb to grow a large DHC crack. Based on the correlation between the reorientation of hydrides and the DHC crack growth, a governing factor for DHC is discussed along with the feasibility of the Kim's DHC model.

Notched Ring Test 저속균열 시험편의 응력확대계수정식화 (Development of Stress Intensity Factor Equation for the Notched Ring Test (NRT) Specimen)

  • 표수호;최선웅
    • 한국재료학회지
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    • 제24권2호
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    • pp.87-92
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    • 2014
  • The Notched Ring Test(NRT) has proven to be very useful in determining the slow crack growth behavior of polyethylene pressure pipes. In particular, the test is simple and an order of magnitude shorter in experimental times as compared to the currently used Notched Pipe Test(NPT), which makes this method attractive for use as the accelerated slow crack growth test. In addition, since the NRT specimen is taken directly from the pipe, having maintained the cross-section, processing induced artifacts that would affect the slow crack growth behavior are not altered. This makes the direct comparison to the slow crack growth specimen in pipe from more meaningful. In this study, for comparison with other available slow crack growth methods, including the NPT, the stress intensity factor equation for NRT specimen was developed and demonstrated of its accuracy within 3% of that obtained from the finite element analysis. The equation was derived using a flexure formula of curved beam bending along with numerically determined geometric factors. The accuracy of the equation was successfully tested on 63, 110, 140, 160, 250, and 400 mm nominal pipe diameters, with crack depth ranging from 15 % to 45 % of the pipe wall thickness, and for standard dimensional ratio(SDR) of 9, 11, and 13.6. Using this equation the slow crack results from 110SDR11 NRT specimen were compared to that from the NPT specimen, which demonstrated that the NRT specimen was equivalent to the NPT specimen in creating the slow crack, however in much shorter experimental times.