• 제목/요약/키워드: Curvature of the line

검색결과 260건 처리시간 0.032초

저심도철도용 선형유도전동기의 공극 불균일 과도특성 분석 연구 (A Study on Transient Analysis of Linear Induction Motor with Ununiform Airgap for Shallow-depth Underground Train)

  • 이형우;박찬배;원성홍
    • 전기학회논문지
    • /
    • 제62권5호
    • /
    • pp.723-729
    • /
    • 2013
  • This paper presents an parallel type Linear Induction Motor with ununiform airgap for a shallow-depth underground train with 100‰ grade and 15 m curvature. This parallel type LIM has enough gradability but has inherently ununiform airgap between center and end parts. Consequently, performance when the train passes curved section should be considered with transient analysis. Moreover, general parallel operation, 1C2M which is usually used for train operation, deteriorates LIM performance because of different line velocity between inner and outer LIMs. Transient analysis has many problems such as huge model, lots of meshes, very long calculation time, truncation error and so on. This paper has presented a novel technique using equivalent linear rotating model in order to solve these problems and has analyzed parallel type LIM by using the proposed technique. Finally, LIM performance according to independent operating control has been investigated.

조절력에 따른 Crystalline Lens의 곡률 변화 모델 (Crystalline lens'curvature change model by Accommdation)

  • 박광호;김용근
    • 한국안광학회지
    • /
    • 제7권2호
    • /
    • pp.181-187
    • /
    • 2002
  • 수정체는 조절력의 변화에 의해서 곡률이 변화한다. 조절력은 탄성체인 수정체에 힘을 수직으로 주는 경우 정점 방향으로 길이가 늘어난다. 힘을 받는 수정체는 밀도 분포와 형태가 후면에 치우쳐있어, 후면 방향의 수평 힘 보다 전면 방향의 수평 힘이 더 크다. 그러므로 후면 방향 보다 전면 방향의 두께가 더 많아 늘어난다. 그러나 조절력이 일정 값 보다 커지기 시작하면 전면에서는 팽창률이 한계에 도달하다. 이 때 전면 방향의 수평 힘 보다 후면 방향의 수평 힘이 더 커지게 되어, 전면 방향 보다 후면 방향의 두께가 더 많아 늘어난다. 전면과 후면의 두께변화 차이는 조절력에 대해 2차 곡선(${\Delta}=B_1D+B_2D^2$)을 이룬다. 조절력에 따른 전면과 후면의 두께(${\Delta}t_a$, ${\Delta}t_p$) 차이 변화 곡선은 다음과 같이 표현된다. $${\Delta}t_a=t_a-t_{ao}=t_{max}+t_0{\exp}(-A/B)-t_{ao}$$ $${\Delta}t_p=t_p-t_{po}=t_{min}+t_0{\exp}(A/B)-t_{po}$$ 인간의 수정체에서 구한 각각의 Parameter값은 전면에서 $t_{min}=1.1.06$, $t_0=-0.33$, B=9.32, 후면에서 $t_{max}=1.97$, $t_0=0.10$ B=7.96 등을 얻었다. 조절력에 따른 수정체의 전면과 후면에서 정점 곡률 안정의 변화는 다음과 같다. $$R=R_0+R_1{\exp}(D/k)$$ 수정체에서 구한 각각의 Parameter 값은 전면에서 $R_{min}=5.55$, $R_1=6.87$, k=4.65, 후면에서 $R_{max}=-68.6$, $R_1=76.7$, k=308.5 등을 얻었다.

  • PDF

Turbine Blading Performance Evaluation Using Geometry Scanning and Flowfield Prediction Tools

  • Zachos, Pavlos K.;Pappa, Maria;Kalfas, Anestis I.;Mansour, Gabriel;Tsiafis, Ioannis;Pilidis, Pericles;Ohyama, Hiroharu;Watanabe, Eiichiro
    • 한국추진공학회:학술대회논문집
    • /
    • 한국추진공학회 2008년 영문 학술대회
    • /
    • pp.89-96
    • /
    • 2008
  • This paper investigates the effect of blade deformation, caused by manufacturing inaccuracies, on the performance of a 2-stage axial steam turbine. A high fidelity 3D coordinate Measurement Machine has been employed to obtain the exact geometrical model of the blades. A Streamline Curvature solver was used to predict the overall performance of the turbine. During the manufacturing process of the casts and of the blades themselves, several types of errors can occur which lead to a different geometry from that envisaged by the designer. The main objective of this study is to investigate the effect of those errors on the performance of a 2-stage experimental axial steam turbine. A high fidelity measurement of the actual geometry of both stator and rotor blades has been carried out, using a 3D Coordinate Measurement Machine. The cross sections of the blades obtained by the measurement were compared with those produced by the design process to evaluate the change in blade inlet/exit angles. In addition, the geometrical deviations from the initial design have been subjected to a statistical study in order to locate the nature of the error. The actual(measured) model has been used as input into a Streamline Curvature solver to evaluate its performance. Finally, a comparison with the performance plots of the original geometry has been carried out. A measurable change of efficiency as well as in the total power delivered by the turbine was found. This suggests that the accumulated error caused during the manufacturing procedure plays a significant role in the overall performance of the machine by making it less efficient by more than 1%. Reverse engineering techniques are proposed to predict and alleviate these errors leading thereby to a final design of each stage with improved performance.

  • PDF

GaAs 기판표면의 Tilt각도가 InGaP 에피막의 탄성특성 및 결정질에 미치는 영향 (Role of Crystallographic Tilt Angle of GaAs Substrate Surface on Elastic Characteristics and Crystal Quality of InGaP Epilayers)

  • 이종원;이철로;김창수;오명석;임성욱
    • 마이크로전자및패키징학회지
    • /
    • 제6권1호
    • /
    • pp.1-10
    • /
    • 1999
  • 본 논문에서는 평탄형 GaAs 기판과 $2^{\circ}$, $6^{\circ}$, $10^{\circ}$경사형 GaAs 기판 등 네 종류의 기판에 유기금속 기강성장장치를 이용하여 InGaP 에피막을 성장시켰고, 기판-에피막간의 격자부정합, 탄성변형, 격자굴곡, 부정합응력 등을 측정하여 기판 경사도, 즉 misorientation이 InGaP 에피막의 탄성특성에 미치는 영향에 대해 최초로 연구하였다. 또한 에피막의 x-선 반치폭과 PL강도 및 PL 반치폭, 발진파장 등을 측정하여 기판의 경사도가 에피막의 결정질에 미치는 영향에 대하여도 연구하였다. 시료 분석은 TXRD(tripple-axis x-ray diffractometer)와 저온 (11K) PL(photoluminescence)를 이용하여 수행했다. 기판 경사도 증가에 따라 Ga 원자의 흡착율이 평탄기판의 경우에 비해 상대적으로 증가하였으며, x-선 반치폭이 감소하였다. 또한 선형 탄성이론에 입각하면 격자 misfit 감소에 따라 부정합응력도 감소해야 하나, 반대로 미세하게 증가하는 현상이 관측되었으며 이는 경사기판을 사용할 때 접계면의 에피막 원자의 탄성효율이 향상되는 것에 기인함을 밝혔다. 그리고 기판의 경사도가 증가함에 따라 PL발진파장이 감소하였고, PL 강도는 증가하였으며, PL 반치폭은 감소하였다. 따라서 본 연구에서는 경사기판을 사용할 때 접계면의 탄성효율이 향상되고, InGaP 에피막의 결정질이 향상됨을 밝혔다.

  • PDF

주곡률 해석 기반의 투영 텍스처를 이용한 스타일 반사 효과 (Stylized Specular Reflections Using Projective Textures based on Principal Curvature Analysis)

  • 이환직;최정주
    • 한국HCI학회논문지
    • /
    • 제1권1호
    • /
    • pp.37-44
    • /
    • 2006
  • 물체의 반사 효과는 물체의 재질, 기하학적 모양 및 조명 환경을 표현하는데 있어 매우 중요한 요소이다. 사진품질을 추구하는 사실적 렌더링에서는 기존의 국소 반사 모델을 사용하여 좋은 결과를 얻을 수 있지만, 사용자의 주관이 중시되는 비사실적 렌더링에서는 사용자가 원하는 반사 효과를 표현할 수 있어야 한다. 텍스처는 사용자가 원하는 반사 효과를 직관적으로 표현할 수 있는 수단이며, 이 텍츠처를 모델에 투영하면 원하는 반사 효과를 얻을 수 있다. 이 때 사용자는 텍스처가 투영될 위치와 크기, 방향을 직접 키프레임으로 정해 줄 수 있다. 그러나 모든 반사 효과를 사용자가 직접 정해준다는 것은 번거로운 일이며, 아울러 실시간 응용분야에는 적용할 수 없는 단점이 있다. 본 논문에서는 국소반사모델과 주곡률 해석을 통해 반사 효과의 위치, 방향 및 크기를 결정하기 위한 텍스처 투영기의 새로운 설정 방법을 제시한다. 광원과 시점 정보로부터 주어진 모델 위에서 최대 명점을 구한 후, 텍스처 투영기를 최대 조명점을 지나는 법선 벡터에 평행한 직선 위에 위치시킨다. 투영기의 방위를 최대 조명점에서의 주방향에 따라서 일치시키고, 투영기의 투영 피라미드의 크기를 주곡률에 따라서 결정한다. 텍스처 투영기의 단순한 이동, 회전 및 주곡률 값의 조절을 통하여 반사 영역의 이동, 회전 및 확대/축소가 가능하다. 본 논문에서 제시한 방법은 DirectX 9.0c와 프로그램이 가능한 셰이더 2.0을 사용하여 GeForce FX 7800 그래픽 카드에 구현되었다. 본 논문의 연구 결과는 만화적 표현을 추구하는 게임 등과 같은 실시간 응용분야에 사용될 수 있으며, 실험 결과에 의하면 수만 개의 다면체 모델에 대한 스타일 반사효과를 실시간에 렌더링할 수 있다.

  • PDF

Membrane Topology of Helix 0 of the Epsin N-terminal Homology Domain

  • Kweon, Dae-Hyuk;Shin, Yeon-Kyun;Shin, Jae Yoon;Lee, Jong-Hwa;Lee, Jung-Bok;Seo, Jin-Ho;Kim, Yong Sung
    • Molecules and Cells
    • /
    • 제21권3호
    • /
    • pp.428-435
    • /
    • 2006
  • Specific interaction of the epsin N-terminal homology(ENTH) domain with the plasma membrane appears to bridge other related proteins to the specific regions of the membrane that are invaginated to form endocytic vesicles. An additional $\alpha$-helix, referred to as helix 0 (H0), is formed in the presence of the soluble ligand inositol-1,4,5-trisphosphate [$Ins(1,4,5)P_3$] at the N terminus of the ENTH domain (amino acid residues 3-15). The ENTH domain alone and full-length epsin cause tubulation of liposomes made of brain lipids. Thus, it is believed that H0 is membrane-inserted when it is coordinated with the phospholipid phosphatidylinositol-4,5-bisphosphate [$PtdIns(4,5)P_2$], resulting in membrane deformation as well as recruitment of accessory factors to the membrane. However, formation of H0 in a real biological membrane has not been demonstrated. In the present study, the membrane structure of H0 was determined by measurement of electron paramagnetic resonance (EPR) nitroxide accessibility. H0 was located at the phosphate head-group region of the membrane. Moreover, EPR line-shape analysis indicated that no pre-formed H0-like structure were present on normal acidic membranes. $PtdIns(4,5)P_2$ was necessary and sufficient for interaction of the H0 region with the membrane. H0 was stable only in the membrane. In conclusion, the H0 region of the ENTH domain has an intrinsic ability to form H0 in a $PtdIns(4,5)P_2$-containing membrane, perhaps functioning as a sensor of membrane patches enriched with $PtdIns(4,5)P_2$ that will initiate curvature to form endocytic vesicles.

가중평균 해석법을 이용한 래핑된 베어링강 어닐링재료의 깊이방향에 대한 잔류응력분포 측정 (Measurement of Residual Stress Distribution in the Depth Direction of Annealed Materials of Lapped Bearing Steel Using Weighted Averaging Analysis Method)

  • 한창석;이찬우
    • 한국재료학회지
    • /
    • 제33권5호
    • /
    • pp.205-213
    • /
    • 2023
  • This paper reports the results of an experimental examination using X-rays to test annealing materials for lapped bearing steel (STB2), to confirm the validity of the weighted averaging analysis method. The distribution behavior for the α𝜓-sin2𝜓 diagram and the presence or absence of differences in the peak method, half-value breadth method, and centroid method were investigated. When lapping the annealed bearing steel (STB2) material, a residual stress state with a non-directional steep gradient appeared in the surface layer, and it was found that the weighted averaging analysis method was effective. If there is a steep stress gradient, the sin2𝜓 diagram is curved and the diffraction intensity distribution curve becomes asymmetric, resulting in a difference between the peak method, half-value breadth method, and centroid method. This phenomenon was evident when the stress gradient was more than 2~3 kg/mm2/㎛. In this case, if the position of the diffraction line is determined using the centroid method and the weighted averaging analysis method is applied, the stress value on the surface and the stress gradient under the surface can be obtained more accurately. When the stress gradient becomes a problem, since the curvature of the sin2𝜓 diagram appears clearly in the region of sin2𝜓 > 0.5, it is necessary to increase the inclination angle 𝜓 as much as possible. In the case of a lapping layer, a more accurate value can be obtained by considering 𝜎3 in the weighted averaging analysis method. In an isotropic biaxial residual stress state, the presence or absence of 𝜎3 can be determined as the presence or absence of strain for sin2𝜓≈0.4.

대형 광학계 연마 장비에 의한 대구경 반사경의 최적 근사 구면 제조 방법에 관한 연구 (An Optical Surfacing Technique of the Best-fitted Spherical Surface of the Large Optics Mirror with Ultra Precision Polishing Machine)

  • 송창규;김경호;황주호;김병섭;박천홍;이호철
    • 한국정밀공학회지
    • /
    • 제30권3호
    • /
    • pp.324-330
    • /
    • 2013
  • This paper describes a novel method to surface large optics mirror with an extremely high hardness, which could replace the high cost of the repetitive off-line measurement steps and the large ultra-precision grinding machine with ultra-positioning control of 10 nm resolution. A lot of diamond pellet to be attached on the convex aluminum base consists of a grinding tool for the concave large mirror, and the tool was pressured down on the large mirror blank. The tool motion at an interval on the spiral path was controlled with each feed rate as the dwell time in the conventional computer-controlled polishing. The shape to be surfaced was measured directly by a touch probe on the machine without any separation of the mirror blank. Total 40 iterative steps of the surfacing and measurement could demonstrate the form error of RMS $7.8{\mu}m$, surface roughness of Ra $0.2{\mu}m$ for the mirror blank with diameter of 1 m and spherical radius of curvature of 5400 mm.

WELDING-INDUCED BUCKLING INSTABILITIES IN THIN PLATES

  • Han, Myoung-Soo;Tsai, Chon-Liang
    • 대한용접접합학회:학술대회논문집
    • /
    • 대한용접접합학회 2002년도 Proceedings of the International Welding/Joining Conference-Korea
    • /
    • pp.661-667
    • /
    • 2002
  • Welding-induced buckling distortion is one of the most problematic concerns in both design and fabrication of welded thin-plate structures. This paper deals with experimental and numerical results of the welding-induced longitudinal and/or buckling distortion occurring in welding of 6mm-thick AH36 high strength steel plates. Effects of the heat input and the plate size on the distortion were experimentally evaluated for square plates. Bead-on-plate welding was performed with the submerged arc welding process along the middle line of plate specimens. Experimental results showed that the longitudinal distortion made a single curvature in the plate, and the distortion magnitude along the weld centerline was proportional to the heat input and the plate size. The experimental results were used to examine the validity of the numerical simulation procedure for welding-induced distortion where the longitudinal distortion mode and magnitude were numerically quantified. Three-dimensional, large deformation, welding simulations were performed for selected weld models. Numerical results of the distortion mode and magnitude were in a good agreement with experimental ones. Depending on the presence of halting the distortion growth during the cooling cycle of welding, the condition discriminating buckling distortion from longitudinal distortion was established. Eigenvalue analyses were performed to check the buckling instability of tested plates with different sizes subjected to different heat inputs. The perturbation load pattern for the analysis was extracted from longitudinal inherent strain distributions. Critical buckling curve from the eigenvalue analyses revealed that the buckling instability is manifested when plate size or heat input increases.

  • PDF

MAGNETIC PROPERTIES OF INNER MAGNETOSPHERE DURING GEOMAGNETIC STORMS INFERRED FROM A TSYGANENKO MAGNETIC FIELD MODEL

  • Lee, D.Y.;Kim, K.C.;Choi, C.R.;Kim, H.J.
    • Journal of Astronomy and Space Sciences
    • /
    • 제21권4호
    • /
    • pp.303-314
    • /
    • 2004
  • In this paper we report some properties of inner magnetospheric structure inferred from the T01_s code, one of the latest magnetospheric models by Tsyganenko. We have constructed three average storms representing moderate, strong, and severe intensity storms using 95 actual storms. The three storms are then modelled by the T01_s code to examine differences in magnetic structure among them. We find that the magnetic structure of intense storms is strikingly different from the normal structure. First, when the storm intensity is large, the field lines anchored at dayside longitudinal sectors become warped tailward to align to the solar wind direction. This is particularly so for the field lines anchored at the longitudinal sectors from postnoon through dusk. Also while for the moderate storm the equatorial magnetic field near geosynchronous altitude is found to be weakest near midnight sector, this depression region expands into even late afternoon sector during the severe storm. Accordingly the field line curvature radius at the equator in the premidnight geosynchronous region becomes unusually small, reaching down to a value less than 500 km. We attribute this strong depression and the dawn-dusk asymmetry to the combined effect from the enhanced tail current and the westward expansion/rotation of the partial ring current.