• 제목/요약/키워드: Static frictional force

검색결과 26건 처리시간 0.019초

자동차용 등속 조인트의 내부 마찰 모델 개발 (Development of Internal Friction Model in Automotive Constant Velocity Joints)

  • 이철희;장민규
    • Tribology and Lubricants
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    • 제24권5호
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    • pp.215-220
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    • 2008
  • An internal friction model was developed to model the frictional behavior of automotive Constant Velocity (CV) joints by using the test data from an instrumented CV joint friction apparatus with actual driveshaft assemblies. Experiments were conduced under different realistic operating conditions of oscillatory speeds, CV joint articulation angles, lubrication, and torque. The experimental data were used to develop a physics-based semi-empirical CV joint internal friction coefficient model as a function of different CV Joint operating parameters. It was found that the proposed friction model captures the experimental results well not only the static behavior of friction coefficient, but also the dynamic friction terms, which is the main source of force that causes vehicle vibration problems.

PRD 강환 말뚝의 연직지지력 특성에 관한 사례 연구 (Case Study on the Characteristics of Vertical Bearing Capacity for Steel Pipe Pile Installed by PRD)

  • 최용규;정창규;정성기;김동철;정태만
    • 한국지반공학회:학술대회논문집
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    • 한국지반공학회 1999년도 봄 학술발표회 논문집
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    • pp.225-232
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    • 1999
  • Construction case of PRD (Percussion Rotary Drill) pipe pile and matters to be attended in construction of PRD pile were reviewed. The compressive and uplifting static pile load tests for PRD piles were performed and, also, analysis by Pile Driving Analyzer was done. Based on these results, bearing components in each resisting part (that is: steel toe, external skin, and internal skin) were measured separately. The measured resisting force was compared to the value calculated by the estimated formula. The pile capacity was mobilized in steel toe area and the external skin friction and the internal friction were not produced. Thus, it could be considered that toe of PRD pile should be supported in hard bearing stratum (for example, the fresh soft rock).

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인공타액하에서 수종 교정선의 마찰력에 관한 실험적 연구 (AN EXPERIMENTAL STUDY ON FRICTIONAL FORCES OF VARIOUS ORTHODONTIC WIRES UNDER ARTIFICIAL SALIVA)

  • 황현식;박영철
    • 대한치과교정학회지
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    • 제19권1호
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    • pp.245-256
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    • 1989
  • Translational movement along an arch wire requires sufficient force to overcome frictional forces between bracket and arch wire. The orthodontist must appreciate the importance of friction in this process, and study out the influencing factors on the level of friction. The purpose of this study was to evaluate the effect of artificial saliva on frictional resistances generated between the bracket and arch wire. Independent variables of this study were arch wire material, angulation and environment. Static frictional forces of cobalt-chromium, heat-treated cobalt-chromium, beta-titanium, stainless steel wires were measured under non-angulated dry, angulated dry, non-angulated saliva, angulated saliva conditions. The results were as follows: 1. Stainless steel wires showed lower friction values in non-angulated dry condition, and heat-treated cobalt-chromium wires showed higher friction values in angulated dry condition. Higher friction values were showed in order of cobalt-chromium. stainless steel, heat-treated cobalt-chromium and beta-titanium wires in non-angulated saliva condition. and were showed in order of stainless steel, cobalt-chromium, heat-treated cobalt-chromium, beta-titanium wires in angulated saliva condition. 2. Angulation increased friction for stainless steel wires under dry condition. 3. Artificial saliva decreased friction for cobalt-chromium wires and increased friction for stainless steel wires under non-angulated condition. 4. Artificial saliva decreased friction for all wires except beta-titanium wires under angulated condition. 5. Regardless of angulation or environment. heat-treated cobalt-chromium and beta-titanium wires showed higher friction values, and stainless steel wires showed lower friction values.

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대구경 말뚝의 정재하시험시 대구경 경사반력말뚝의 인발거동 (The Pullout Behavior of a Large-diameter Batter ]Reaction Piles During Static Pile Load Test for a Large Diameter Socketed Pipe Pile)

  • 김상옥;성인출;박성철;정창규;최용규
    • 한국지반공학회논문집
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    • 제18권1호
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    • pp.5-16
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    • 2002
  • 본 연구에서는 직경 1,000mm의 시험말뚝에 대한 압축정재하시험 수행시 반력말뚝으로 사용된 직경 2,500mm의 대구경 경사반력소켓말뚝의 인발거동을 분석하였다. 경사반력말뚝은 풍화암층과 연암층 10m에 걸쳐서 현장타설말뚝으로 소켓되어졌으며, 강관부는 강관과 속채움콘크리트로, 그리고 소켓부는 콘크리트와 철근으로 구성되었다. 각 구성부재에 작용하는 변형율을 측정하기 위해 센서를 설치하였으며, 반력말뚝두부의 인발량을 측정하기 위하여 LVDT를 설치하였다. 정재하시험중 재하된 최대인발하중은 10MN이었으며 최대인발변위는 7m, 잔류인발변위는 최대 1mm 정도 발생하였다. 인발하중의 83%를 풍화암층에서 그리고 12%를 연암층에서 지지하는 것으로 나타났으며 풍화암에 소켓된 철근콘크리트부와 연암에 소켓된 털근콘크리트부에서 각각 125.3kPa와 61.8kPa의 인발응력이 발생하였다. 따라서, 풍화암층에서도 인발하중을 충분하게 지지하고 있으므로 풍화암층은 마찰력을 크게 발휘하는 지지층으로 사용되었다.

브라켓 각도 변화에 따른 세라믹 브라켓의 마찰력 측정 (Evaluation of friction of ceramic brackets in various bracket-wire combinations)

  • 차정열;김경석;김동춘;황충주
    • 대한치과교정학회지
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    • 제36권2호
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    • pp.125-135
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    • 2006
  • 최근 사용되고 있는 세라믹 브라켓의 마찰력을 측정하고 비교하고자 실험군으로 3종의 세라믹 브라켓(Crystaline $V^{(R)}$, Tomy, Tokyo, Japan; $Clarity^{(R)}$, 3M Unitek, CA; $Inspire^{(R)}$, Ormco, CA)을 사용하였으며 대조군으로 컴퍼짓 레진브라켓($Spirit^{(R)}$, Ormco, CA)과 메탈브라켓($Kosaka^{(R)}$, Tomy, Tokyo, Japan)을 사용하였다. 활주 시 마찰력은 4개의 브라켓-교정선 경사$(0^{\circ},\;5^{\circ},\;10^{\circ},\;15^{\circ})$에서 각각 측정되었으며 두 종의 교정선 [1. 스테인레스 스틸(Stainless Steel, SDS Ormco, Glendora, CA), 2. 베타-타이타늄(TMA, SDS Ormco, Glendora, CA)]이 사용되었다. 22 mil 브라켓을 만능시험기기에 부착한 후 $.021{\times}.025$ 크기의 교정선에 고무결찰한 후 $34^{\circ}C$의 건조상태에서 5 mm/min 속도로 교정 선을 활주시켰다. TMA 교정선은 스테인레스 스틸 교정선보다 높은 마찰력을 발생시켰으며 모든 브라켓 호선과의 조합에서 브라켓-교정선의 각도가 증가함에 따라 정적, 동적 마찰력이 증가하였다. $0^{\circ}{\sim}5^{\circ}$ 구간에서 마찰력의 크기는 스테인레스 스틸 교정선과 레진 브라켓 조합이 가장 낮게 측정되었으며 다음으로 Crystaline V, 금속 브라켓, Clarity, Inspire의 순으로 나타났다. TMA 교정선에서는 Crystaline V와의 조합이 가장 낮은 마찰력을, 다음으로 컴퍼짓 브라켓, Clarity, 금속 브라켓, Inspire 순으로 나타났다. $5^{\circ}$ 이상에서 마찰력이 급격하게 증가하였으며 스테인레스 스틸 교정선에서 레진 브라켓, Clarity, Crystaline V, 금속 브라켓, Inspire순으로 나타났다. TMA 교정선에서는 레진 브라켓, Crystaline V, Clarity, Inspire, 금속 브라켓 순으로 나타났다. 이때 호선 브라켓 조합에 대한 마찰력은 일반적으로 증가하였으나 마찰력 증가율의 차이로 인해 그룹간 마찰력의 순위가 서로 뒤바뀌는 경우가 관찰되었다. 실리카-삽입 세라믹 브라켓은 기존의 세라믹 브라켓보다 낮은 마찰력을 보여줄 뿐 아니라 브라켓-교정선의 경사도의 증가에서도 비교적 낮은 마찰력 증가율을 나타내어 세라믹 브라켓의 높은 마찰력을 감소시키는데 큰 역할을 할 수 있다고 생각된다.

MR제어기의 마찰력비에 따른 단자유도 구조물의 응답감소 (Response Reduction of a SDOF Structure based on Friction Force Ratio of MR Controller)

  • 성지영;민경원
    • 한국전산구조공학회논문집
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    • 제23권4호
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    • pp.435-443
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    • 2010
  • 본 연구에서는 MR(Magneto-Reological)제어기가 설치된 단자유도 구조물의 응답을 예측하기 위하여 구조물의 운동방정식을 해석적으로 분석하고 주요변수를 파악하였다. MR제어기의 수치 모델로는 마찰 및 점성감쇠로 단순모델한 Bingham모델을 사용하였다. 자유진동과 조화진동일때의 응답감쇠를 결정짓는 주요변수가 각각 마찰력과 최대정적복원력의 비 $R_f$, 마찰력과 최대조화가진력의 비 $R_h$ 임을 파악하였다. 비선형 미분방정식을 등가의 선형 미분방정식으로 변환하기 위하여 마찰력에 의한 에너지 소산을 등가의 점성에너지로 치환하여 등가점성감쇠와 등가점성감쇠비를 유도하였다. 마지막으로 등가선형화과정을 검증하기 위하여 실제 지진에 대한 구조물의 응답을 비선형 미분방정식의 해와 비교하였다.

Optimal Friction Materials of Tiny Piezoelectric Ultrasonic Linear Motor

  • Lee, Kyong-Jae;Nahm, Sahn;Kang, Jin-Kyu;Ko, Hyun-Phill;Kang, Chong-Yun;Kim, Hyun-Jae;Yoon, Seok-Jin
    • Transactions on Electrical and Electronic Materials
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    • 제6권6호
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    • pp.249-255
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    • 2005
  • In recent years, a novel tiny piezoelectric linear motor converting a radial mode vibration to a longitudinal mode vibration driven by the impact force has been developed for a camera optical module. The tiny piezoelectric motor is consisted of a shaft, mobile element, and piezoelectric transducer. In this work, the frictional coefficient and static friction force of the interface between the shaft and the mobile element have been investigated according to their respective materials. It was found that two combinations, namely Pyrex glass or stainless steel for the shaft and stainless steel (SUS) for the mobile element, exhibited good dynamic behaviors in the tiny ultrasonic linear motor, which was newly developed based on operating concepts based on Newton's law.

CHIP생성 및 절삭열 발생기구 해석을 위한 유한요소법 적용에 관한 연구 (A Study on the Applications of Finite Element Techniques to Chip Formation and Cutting Heat Generation Mechanism of Cutting Process)

  • 황준;남궁석
    • 한국정밀공학회지
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    • 제12권9호
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    • pp.148-155
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    • 1995
  • The object of this study is to achieve a gteater understanding of meterial removal process and its mechanism. In this study, some applications of finite element techniques are applied to analyze the chip formation and cutting heat generation mechanism of metal cutting. To know the effect of cutting parameters, simulations employed some independent cutting variables change, such as constitutive deformation laws of workpiece and tool material, frictional coefficients and tool-chip contact interfaces, cutting speed, tool rake angles, depth of cut and this simulations also include large elastic-plastic defor- mation, adiabetic thermal analysis. Under a usual plane strain assumption, quasi-static, thermal-mechanical coupling analysis generate detailed informations about chip formation process and cutting heat generation mechanism Some cutting parameters are affected to cutting force, plastic deformation of chip, shear plane angle, chip thickness and tool-chip contact length and reaction force on tool, cutting temperature and thermal behavior. Several aspects of the metal cutting process predicted by the finite element analysis provide information about tool shape design and optimal cutting conditions.

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초전도 저널베어링 Substator의 특성평가 (Static Properties of Superconductor Journal Bearing Substator for Superconductor Flywheel Energy Storage System)

  • 박병준;정세용;이정필;박병철;정년호;성태현;한영희
    • Progress in Superconductivity
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    • 제10권1호
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    • pp.55-59
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    • 2008
  • A Superconductor Flywheel Energy Storage System(SFES) mainly consists of a pair of non-contacting High Temperature Superconductor(HTS) bearings that provide very low frictional losses, a composite flywheel with high energy storage density. The HTS bearings, which offer dynamic stability without active control, are the key technology that distinguishes the SFES from other flywheel energy storage devices, and great effort is being put into developing this technology. The Superconductor Journal Bearing(SJB) mainly consists of HTS bulks and a stator, which holds the HTS bulks and also acts as a cold head. Static properties of HTS bearings provide data to solve problems which may occur easily in a running system. Since stiffness to counter vibration is the main parameter in designing an HTS bearing system, we investigate SJB magnetic force through static properties between the Permanent Magnet(PM) and HTS. We measure stiffness in static condition and the results are used to determine the optimal number of HTS bulks for a 100kWh SFES.

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충돌 후 지면 조건에 따른 다양한 볼의 속도변화에 관한 연구 (Changes of Various Balls Velocity under the Different Surface Conditions after Impact)

  • 박진
    • 한국운동역학회지
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    • 제17권1호
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    • pp.91-97
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    • 2007
  • The purpose of this study was to investigate the changes of various balls velocity under the different surface conditions after impact. For this study, four different balls were used which are golf ball, tang-tang ball, table tennis ball, and iron ball. And two different types of ground conditions were used which are artificial grass green and glass green. Movements of putter head and ball were recorded with 2 HD video cameras(60 Hz, 1/500s shutter speed). Small size control object($18.5cm{\times}18.5cm{\times}78.5cm$) was used in this study. To transfer the same amount of kinetic energy to the ball, pendulum putting machine was used. Analyzing the process of impact and the ball movement, a putter was digitized the whole movement but the ball was digizited within the 50cm movement. Velocities were calculated by the first central difference method(Hamill & Knutzen, 1995). Putter head velocities were about 112.2cm/s-116.2cm/s at impact. Maximum ball velocities were appeared 0.08s-0.10s after impact no matter what the ground conditions are. Table tennis ball recorded higher ball velocities than the other ball velocities and iron ball recorded the lowest ball velocity in this group. But Table tennis ball was influenced with the frictional force and immediately was decreased at the artificial grass green condition. If an object is received the kinetic energy under the static condition(v=0cm/s), the object recorded the maximum velocity shortly after the impact and then decreased the velocity because of the frictional force. The ball distance from the start position to the peak velocity position is about 6cm-10cm under the 112.2cm/s-116.2cm/s putting velocity with putter. 0.25 seconds later after impact balls were placed 40cm distance from the original position except iron ball. In this study, ball moving distances were too short therefore it was not possible to investigate the reactions after the translational force is disappeared. Rotational force would play a major role at the end of the ball movement. Future study must accept two things. One is long distance movement of ball and the other is balanced ground. Three-piece ball is a good item to investigate the golf ball movement on the different surface conditions.