????? 1

Size: px
Start display at page:

Download "????? 1"

Transcription

1 Application of Plastics CAE: Focusing on Impact Analysis Sumitomo Chemical Co., Ltd. Plastics Technical Center Masaaki TSUTSUBUCHI Tomoo HIROTA Yasuhito NIWA Tai SHIMASAKI To review recent topics on impact analysis in the field of plastics, this report outlines the application trends and analysis techniques followed by an explanation of the characteristic physical properties of resins which may be the key points for their practical application. First we introduce how we predict yield stress under a wide range of temperatures and strain rates. Second, for the elastic-plastic model, we explain that it may be appropriate to consider dependence of yield stress on stress state and volume increase due to craze generation. Finally, we show how fracture behavior depends on temperature and strain rate. CAE Computer Aided Engineering ) 98Dr. Jason R. Lemon CAE 2) CAE CAE CAE CAE 98 CAE 3) 6) 7), 8) 9) Fig. a Fig. b CAE 2 CAO Computer Aided OptimizationCAO CAE 2) CAO CAE ) CAE CAE Fig. 2 2-

2 Fig. (a) Semi-anechoic chamber (b) Impact testing machine Experimental facilities for Plastics CAE Plastics CAE (Product/Material design and product performance evaluation) < CAE for Polymer Design > Structure & Composition of Materials Fig. 2 CAE CAO Physical properties of Materials * CAE : Computer Aided Engineering CAO : Computer Aided Optimization Plastics CAE system < CAE for Product Design > CAE CAO Performance & Processability of Products ) 6) 7) 8), 9) 2) 23) 24), 25) ) 27) 29) 3) 3) 32), 33) 34) LS-DYNA LS-DYNA 976 DYNA3D

3 Courant Courant u Δt C = Δx C CourantuΔ t Δx u ρe u = E/ρ 2 Δt Δx ρ/e () (2) E =.5GPa ρ = 9kg/m 3 Δx =.m Δ t.77 Δt Courant 35) LS-DYNA 2 Δ x Courant 3 Fluid Structure Interaction: FSI Lagrange Lagrange Euler ALE Arbitrary Lagrangian Eulerian ALE 2-

4 Euler ALE Lagrange 3 36) n σ 2 ε. =, σ ε. 2 ε 2 ε. = ε ε. 2 n (3) σ σ 2 ε ε 2 ε ε 2 n Stress (MPa) 5 5 Strain (a) Original data Stress (MPa) (b) Superposed data by the scaling rule Fig Strain.5s.s.2s.5s s 2s 5s s 2s 5s s 2s 5s.5s s 2s 5s s 2s 5s s 2s 5s Tensile testing results: Relationship between nominal stress and nominal strain 3 Fig. 3.5s ) σθεε E w h σ(ε,ε.,θ) = E (ε.,θ) [ e w(ε.,θ)ε ]e h(ε.,θ)ε 2 w(ε.,θ) 4 Fig. 3 Fig. 3 a E w h ) Cowper-Symonds 5 σ y = σ y [ + (ε. /C ) /p ] σ y σ y ε C p (4) (5) 2-

5 Eyring 6 39) Eyring Eyring V p *σ y V p *σ y 6 PC, PMMA, PP R σ y = Σ sinh T p=α,β V ε.* p *,p ε. *,p = ε.,p exp ΔU p RT σ y ε ε,p TRV p * ΔU p ε. (6) 6 Fig. 4 Fig. 4 6 Yield Stress (MPa) C 3 C 2 C C C C 23 C {(σ xx σ yy ) 2 +(σ yy σ zz ) 2 +(σ zz σ xx ) 2 +6(τ 2 xy + τ 2 yz + τ 2 zx)} σ 2 y 2 (7) σ y σ xx σ yy σ zz τ xy τ yz τ zx 4) von Mises 25) : ε L : ε T Fig. 5 d ε T /d ε L, Fig. 5 Digital Image Correlation Method; DICM 4) Fig. 5 42) Fig. 4.. Strain Rate (s ) Plots: Experimental data Curves: Eq.6 Dependence of yield nominal stress on temperature and nominal strain rate von Mises 7 von Mises Transverse true strain Parallel part length of the specimen: 57mm Fig Slope:.42.2mm/s.m/s Longitudinal true strain Relationship between transverse true strain and longitudinal true strain 2-

6 43) ε pt ε pl ε pt /ε pl.5 Fig. 6 F S S S v σ d σ p 8 F = σ d S = σ p (S S v ) d ΔV V 9 44) d = σ d /σ p = (S S v )/S = /( + ΔV/V ) Tensile Direction F = σ d S = σ p (S S v ) S (8) (9) 3 Fig. 7 A D Table Strain at break A B C D Fig. 7 Table Region C D Break under uniform deformation (A) Break immediately after start of necking (B) Break under propagation of necking (C) Break at the shoulder part of the specimen (D) B Break behavior of the specimen at tensile testing Break behavior Break under uniform deformation Break immediately after start of necking Break under propagation of necking Break at the shoulder part of the specimen C... Strain rate (s ) Relationship between nominal strain at break and nominal strain rate Temperature Low High Nominal strain rate High Low A Fig. 8 a T WLF 45) A B A 23 C 3 C S v C log a T = (T T ref ) C2 + (T T ref ) () Fig. 6 Stress of damaged material Cross-section TTref C C 2 2-

7 Strain at break 4 C 3 C 2 C C C C 23 C log at 5 Exp Temperature ( C) 99 Fig. 9.. Strain rate (s ) Plastics part Fig. 8 Results of time-temperature superposition in region A 23.2 Fig. 7 46) 99 CAE Acceleration (m/s 2 ) 2 Fig. 9 Time (s) Free Motion Headform Analysis (CAO) Analysis (Manual) Experiment Example of simulation of impact test for rib box parts CAO Response Surface Method Modified Method of Feasible Directions 47) CAO. 2-

8 48) 2 Fig. Yield Stress (MPa) Strain rate (s ) (a) Dependence of nominal yield stress on nominal strain rate Strain at break C 4 C 45 C 35 C 4 C 45 C.4 Strain rate (s ) Predicted unstable or unmeasurable condition for tensile test (b) Dependence of nominal strain at break on nominal strain rate Fig. Determination of failure characteristics Fig. Example of drop impact analysis for the standing-pouch A Table A 6 Fig. a Fig. b 35 Fig. 2 Blown off door (a) with poor material properties Fig. 2 Properly opened door (b) with good material properties Airbag cover deployment test analysis result 2-

9 3 Fig 3 Model A von Mises.5 Model B Fig. 4 Model B Model A Upper clamp Lower clamp Fig. 3 Force (N) Fig mm 5mm Dart with hemispherical tip weight: 6.5kg Plate specimen 3mm Schematic diagram of CAE analysis model for the falling weight impact test Drop height : 4cm Displacement (mm) Exp. CAE (Model A) CAE (Model B) Comparison of experimental result and CAE predictions for the falling weight impact test 49) 5) Gough-Joule 5) 52), 53) XFEM 54) 55) CAE CAECAE ) J. R. Lemon, S. K. Tolani and A. L. Klosterman, CAD-Fachgespräch, 98, 6 (98). 2),,,, 5 (24). 3),,,,,, 984-@, 7 (984). 4),,,,,, 992-@, 68 (992). 5),,,,,, 995-!, 75 (995). 6),,,, 2-@, 3 (2). 7) M. Tsutsubuchi, T. Kitayama, Y. Togawa, T. Nishio and, H. Kutschera, Intern. Polym. Process., 5(3), 33 (2). 8),,, 98, 998, 39. 9),,,, 29-!, 4 (29). 2-

10 ),, 22(), 53 (2). ) M. Walter, H. Chladek and A. Huß, 4th European LS-DYNA Users Conference, 23, G--5. 2) I. Lupea, J. Comier and S. Shah, 8th International LS-DYNA Users Conference, 24, ) T. Yeo and J. Park, 23 ABAQUS Users Conference, 23. 4) T. Goel and N. Stander, Comput. Methods Appl. Mech. Engrg., 98, 237 (29). 5) M. Keranen, S. Krishnaraj, K. Kulkarni, L. Lu, R. Thyagarajan and V. Ganesan, SAE Technical Paper, (25). 6) C. J. Ribeiro, J.C. Viana, F.Vilaça and J. Azenha, Plastics, Rubber and Composites, 35, 253 (26). 7) A. Malladi, Saifuddin and G. Gadekar, SAE Technical Paper, (2). 8),,,,,, No.99-98, 9 (998). 9),,, No.3-99, 3 (999). 2),,,,,, 26, 27. 2),, 32, 5 (26). 22) J. M. Lorenzo, SAE Technical Paper, (999). 23) K. Lee, T. Yeo, S. Park, H. A. Gese and H. Dell, SAE Technical Paper, (28). 24) P.A. Du Bois, M. Koesesters, T. Frank and S. Kolling, 3. LS-DYNA Anwenderforum, 24, C-I-. 25) P.A. Du Bois, S. Kolling, M. Koesters and T. Frank, International Journal of Impact Engineering, 32, 725 (26). 26) M. C. H. Lee and G. E. Novak, SAE Technical Paper, (26). 27),,,,,,, 2, ) D. Yu, J. B. Kwak, S. Park and J. Lee, Microelectronics Reliability, 5, 28 (2). 29) K. H. Low, A. Yang, K.H. Hoon, X. Zhang, J. K. T. Lim and K. L. Lim, Advances in Engineering Software, 32, 683 (2). 3) T. Allen, J. Hart, J. Spurr, S. Haake and S. Goodwill, Procedia Engineering, 2, 3275 (2). 3) A. W. Pugh, R. Hamilton, D. H. Nash and S. R. Otto, Procedia Engineering, 2, 323 (2). 32),,, C, 76(772), 3343 (2). 33) W. Petersen and J. McPhee, Sports Eng., 2(2), 77 (2). 34), C, 65(638), 389 (999). 35),,, 25(4), 34 (26). 36),,,, (995), p ) W. Michaeli, M. Glißmann, Polymer Testing, 2(5), ),, 57(3), 29 (28). 39) E.T.J. Klompen, L.E. Govaert, Mech. Time-depend. Mater., 3, 49 (999). 4),, 5(9), 968 (2). 4) F. Grytten, H. Daiyan, M. Polanco-Loria and S. Dumoulin, Polymer Testing, 28(6), 653 (29). 42) V. Delhaye, A. H. Clausen, F. Moussy, R.Othman and O.S.Hopperstad, International Journal of Impact Engineering, 38(4), 28 (2). 43),, 5, 25, ) M. Nutini and M. Vitali, 7. LS-DYNA Anwenderforum, 28, D-I-. 45),,, 5(6), 25 (22). 46),,,, 26, ),,,,, 2, ),,,, 6, 26, ) R. N. Haward, J. Polym. Sci. Part B:Polymer Physics, 45, 9 (27). 5),, 77(), 2 (24). 5),,,, 3, (983), p ) I. Doghri, Mechanics of Deformable Solids, Linear and Nonlinear Analytical and Computational Aspects, Springer (2), p ),,, A, 77(778), 92 (2). 54) N. Moës, J. Dolbow, and T. Belytschko, International Journal for Numerical Methods in Engineering, 46(), 3 (999). 55),, A, 67 (659), 93 (2). 2-

11 PROFILE Masaaki TSUTSUBUCHI Yasuhito NIWA Tomoo HIROTA Tai SHIMASAKI 2-

薄板プレス成形の高精度変形解析手法と割れ予測

薄板プレス成形の高精度変形解析手法と割れ予測 Finite Element Simulation of Deformation and Breakage in Sheet Metal Forming Noritoshi Iwata, Masao Matui 3 4J2G Stören & Rice FEM In the analysis of sheet metal forming, constitutive equations are examined

More information

Fig. 4. Configuration of fatigue test specimen. Table I. Mechanical property of test materials. Table II. Full scale fatigue test conditions and test

Fig. 4. Configuration of fatigue test specimen. Table I. Mechanical property of test materials. Table II. Full scale fatigue test conditions and test (J. Soc. Mat. Sci., Japan), Vol. 52, No. 11, pp. 1351-1356, Nov. 2003 Fatigue Life Prediction of Coiled Tubing by Takanori KATO*, Miyuki YAMAMOTO*, Isao SAWAGUCHI** and Tetsuo YONEZAWA*** Coiled tubings,

More information

電子部品はんだ接合部の熱疲労寿命解析

電子部品はんだ接合部の熱疲労寿命解析 43 Evaluation for Thermal Fatigue Life of Solder Joints in Electronic Components Haruhiko Yamada, Kazuyoshi Ogawa 2 63Sn- 37Pb 95Pb-5Sn Si Cu Si 63Sn-37Pb Since automotive electronic components are used

More information

The Evaluation on Impact Strength of Structural Elements by Means of Drop Weight Test Elastic Response and Elastic Limit by Hiroshi Maenaka, Member Sh

The Evaluation on Impact Strength of Structural Elements by Means of Drop Weight Test Elastic Response and Elastic Limit by Hiroshi Maenaka, Member Sh The Evaluation on Impact Strength of Structural Elements by Means of Drop Weight Test Elastic Response and Elastic Limit by Hiroshi Maenaka, Member Shigeru Kitamura, Member Masaaki Sakuma Genya Aoki, Member

More information

19 σ = P/A o σ B Maximum tensile strength σ % 0.2% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional

19 σ = P/A o σ B Maximum tensile strength σ % 0.2% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional 19 σ = P/A o σ B Maximum tensile strength σ 0. 0.% 0.% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional limit ε p = 0.% ε e = σ 0. /E plastic strain ε = ε e

More information

Study on Application of the cos a Method to Neutron Stress Measurement Toshihiko SASAKI*3 and Yukio HIROSE Department of Materials Science and Enginee

Study on Application of the cos a Method to Neutron Stress Measurement Toshihiko SASAKI*3 and Yukio HIROSE Department of Materials Science and Enginee Study on Application of the cos a Method to Neutron Stress Measurement Toshihiko SASAKI*3 and Yukio HIROSE Department of Materials Science and Engineering, Kanazawa University, Kakuma-machi, Kanazawa-shi,

More information

Study on Throw Accuracy for Baseball Pitching Machine with Roller (Study of Seam of Ball and Roller) Shinobu SAKAI*5, Juhachi ODA, Kengo KAWATA and Yu

Study on Throw Accuracy for Baseball Pitching Machine with Roller (Study of Seam of Ball and Roller) Shinobu SAKAI*5, Juhachi ODA, Kengo KAWATA and Yu Study on Throw Accuracy for Baseball Pitching Machine with Roller (Study of Seam of Ball and Roller) Shinobu SAKAI*5, Juhachi ODA, Kengo KAWATA and Yuichiro KITAGAWA Department of Human and Mechanical

More information

DPA,, ShareLog 3) 4) 2.2 Strino Strino STRain-based user Interface with tacticle of elastic Natural ObjectsStrino 1 Strino ) PC Log-Log (2007 6)

DPA,, ShareLog 3) 4) 2.2 Strino Strino STRain-based user Interface with tacticle of elastic Natural ObjectsStrino 1 Strino ) PC Log-Log (2007 6) 1 2 1 3 Experimental Evaluation of Convenient Strain Measurement Using a Magnet for Digital Public Art Junghyun Kim, 1 Makoto Iida, 2 Takeshi Naemura 1 and Hiroyuki Ota 3 We present a basic technology

More information

JFE.dvi

JFE.dvi ,, Department of Civil Engineering, Chuo University Kasuga 1-13-27, Bunkyo-ku, Tokyo 112 8551, JAPAN E-mail : atsu1005@kc.chuo-u.ac.jp E-mail : kawa@civil.chuo-u.ac.jp SATO KOGYO CO., LTD. 12-20, Nihonbashi-Honcho

More information

untitled

untitled 3 4 4 2.1 4 2.2 5 2.3 6 6 7 4.1 RC 7 4.2 RC 8 4.3 9 10 5.1 10 5.2 10 11 12 13-1 - Bond Behavior Between Corroded Rebar and Concrete Ema KATO* Mitsuyasu IWANAMI** Hiroshi YOKOTA*** Hajime ITO**** Fuminori

More information

Computer Simulation in Thermoplastic Injection Molding Takaaki Matsuoka Toyota Central Research and Development Laboratories, Inc. 41-1, Yokomichi, Na

Computer Simulation in Thermoplastic Injection Molding Takaaki Matsuoka Toyota Central Research and Development Laboratories, Inc. 41-1, Yokomichi, Na Computer Simulation in Thermoplastic Injection Molding Takaaki Matsuoka Toyota Central Research and Development Laboratories, Inc. 41-1, Yokomichi, Nagakute, Aichi 480-11, Japan A package of computer programs

More information

J. Jpn. Inst. Light Met. 65(6): 224-228 (2015)

J. Jpn. Inst. Light Met. 65(6): 224-228 (2015) 65 62015 224 228 ** Journal of The Japan Institute of Light Metals, Vol. 65, No. 6 (2015), 224 228 2015 The Japan Institute of Light Metals Investigation of heat flow behavior on die-casting core pin with

More information

6) , 3) L60m h=4m 4m φ19 SS400 σ y = kn/mm 2 E = 205.8kN/mm 2 Table1 4) 7 Fig.1 5 7) S S 2 5 (Fig.2 ) ( No.1, No.2, No.3, No.4)

6) , 3) L60m h=4m 4m φ19 SS400 σ y = kn/mm 2 E = 205.8kN/mm 2 Table1 4) 7 Fig.1 5 7) S S 2 5 (Fig.2 ) ( No.1, No.2, No.3, No.4) Damages and Earthquake Resistant Performance of Steel Frame Structures with Self Strain Stress (Faculty of Architecture and Structural Engineering) Yutaka NIHO, Masaru TERAOKA (Professor Emeritus of KNCT)

More information

第62巻 第1号 平成24年4月/石こうを用いた木材ペレット

第62巻 第1号 平成24年4月/石こうを用いた木材ペレット Bulletin of Japan Association for Fire Science and Engineering Vol. 62. No. 1 (2012) Development of Two-Dimensional Simple Simulation Model and Evaluation of Discharge Ability for Water Discharge of Firefighting

More information

untitled

untitled - 37 - - 3 - (a) (b) 1) 15-1 1) LIQCAOka 199Oka 1999 ),3) ) -1-39 - 1) a) b) i) 1) 1 FEM Zhang ) 1 1) - 35 - FEM 9 1 3 ii) () 1 Dr=9% Dr=35% Tatsuoka 19Fukushima and Tatsuoka19 5),) Dr=35% Dr=35% Dr=3%1kPa

More information

n-jas09.dvi

n-jas09.dvi Vol. 9 (2009 12 ), No. 03-091211 JASCOME CREEP ANALYSIS DISCONTINUOUS ROCK MASS AROUND UNDERGROUND CAVERN 1) 2) 3) Takakuni TATSUMI, Hidenori YOSHIDA and Masumi FUJIWARA 1) ( 761-0396 2217-20, E-mail:

More information

A Study on Throw Simulation for Baseball Pitching Machine with Rollers and Its Optimization Shinobu SAKAI*5, Yuichiro KITAGAWA, Ryo KANAI and Juhachi

A Study on Throw Simulation for Baseball Pitching Machine with Rollers and Its Optimization Shinobu SAKAI*5, Yuichiro KITAGAWA, Ryo KANAI and Juhachi A Study on Throw Simulation for Baseball Pitching Machine with Rollers and Its Optimization Shinobu SAKAI*5, Yuichiro KITAGAWA, Ryo KANAI and Juhachi ODA Department of Human and Mechanical Systems Engineering,

More information

75 unit: mm Fig. Structure of model three-phase stacked transformer cores (a) Alternate-lap joint (b) Step-lap joint 3 4)

75 unit: mm Fig. Structure of model three-phase stacked transformer cores (a) Alternate-lap joint (b) Step-lap joint 3 4) 3 * 35 (3), 7 Analysis of Local Magnetic Properties and Acoustic Noise in Three-Phase Stacked Transformer Core Model Masayoshi Ishida Kenichi Sadahiro Seiji Okabe 3.7 T 5 Hz..4 3 Synopsis: Methods of local

More information

LNG Tank-Its Structure, the Materials and Welding Techniques Yasunosuke OGAWA, Mitsuhiro SAKAMOTO, Kiyoaki TOYOMASU, Mitsuo OHYAMA, Munemitsu FUKAGAWA, and Yoshinori SAIGA Table 2. Material list for various

More information

Key Words: average behavior, upper and lower bounds, Mori-Tanaka theory, composites, polycrystals

Key Words: average behavior, upper and lower bounds, Mori-Tanaka theory, composites, polycrystals Key Words: average behavior, upper and lower bounds, Mori-Tanaka theory, composites, polycrystals (Q)1=C1(E)1, (0)2=C2(E)2 (4) QQQ= fi(o)1+f2(2+(1-fi-f2)(o)m E=flIE1+12(6)2+(1-fl-f2)(E)D (5a) (5b) (E)i=1E/D+-y,

More information

7章 構造物の応答値の算定

7章 構造物の応答値の算定 (1) 2 (2) 5.4 5.8.4 2 5.2 (3) 1.8 1) 36 2) PS 3) N N PS 37 10 20m N G hg h PS N (1) G h G/G 0 h 3 1) G 0 PS PS 38 N V s G 0 40% Gh 1 S 0.11% G/G 0 h G/G 0 h H-D 2),3) R-O 4) 5),6),7) τ G 0 γ = 0 r 1 (

More information

Developement of Plastic Collocation Method Extension of Plastic Node Method by Yukio Ueda, Member Masahiko Fujikubo, Member Masahiro Miura, Member Sum

Developement of Plastic Collocation Method Extension of Plastic Node Method by Yukio Ueda, Member Masahiko Fujikubo, Member Masahiro Miura, Member Sum Developement of Plastic Collocation Method Extension of Plastic Node Method by Yukio Ueda, Member Masahiko Fujikubo, Member Masahiro Miura, Member Summary Previously, the authors developed the plastic

More information

LOL ONNRION RRISIS OF RQUK RSPONS OF KO ROUN akashi kiyoshi, ept. o ivil ngrg., Kumamoto Univ., Kunihiko Fuchida, ept.

LOL ONNRION RRISIS OF RQUK RSPONS OF KO ROUN akashi kiyoshi, ept. o ivil ngrg., Kumamoto Univ., Kunihiko Fuchida, ept. , akiyoshi@kumamoto-u.ac.jp uchida@as.yatsushiro-nc.ac.jp matsu@kumamoto-u.ac.jp 9t1533@eng1.stud.kumamoto-u.ac.jp F NUW Fig.1 - - N 5 3m 1995 L-3mNSU max.1,, 5., 1m/s - - - max=.1m/s JR Fig. Fig.1 (Fig.1/Fig.)Fig.3

More information

X X 1. 1 X 2 X 195 3, 4 Ungár modified Williamson-Hall/Warren-Averbach 5-7 modified modified Rietveld Convolutional Multiple Whole Profile CMWP 8 CMWP

X X 1. 1 X 2 X 195 3, 4 Ungár modified Williamson-Hall/Warren-Averbach 5-7 modified modified Rietveld Convolutional Multiple Whole Profile CMWP 8 CMWP X X a a b b c Characterization of dislocation evolution during work hardening of stainless steels by using XRD line-profile analysis Tomoaki KATO a, Shigeo SATO a, Yoichi SAITO b, Hidekazu TODOROKI b and

More information

Tetsu-to-Hagane Vol. 87 (2001) No. 5 Table 1. Physical properties of particles. (a) side view (b) front view Fig. 1. Experimental apparatus with semic

Tetsu-to-Hagane Vol. 87 (2001) No. 5 Table 1. Physical properties of particles. (a) side view (b) front view Fig. 1. Experimental apparatus with semic Tetsu-to-Hagane Vol. 87 (2001) No. 5 Deadman.Renewal Motion in a Cold Model of Blast Furnace Hiroshi TAKAHASHI and Hideki KAWAI Synopsis : Permeability in coke bed in the lower part of blast furnace is

More information

Fig. 1. Relation between fatigue crack propagation rate and stress intensity factor range. Fig. 2. Effect of stress ratio on fatigue crack opening rat

Fig. 1. Relation between fatigue crack propagation rate and stress intensity factor range. Fig. 2. Effect of stress ratio on fatigue crack opening rat Fatigue Crack Propagation and Fracture Surface in Polyvinyl Chloride by Tetsuro SHIRAISHI The fatigue crack propagation behavior and the fracture surface appearance under several load conditions in polyvinyl

More information

7 OpenFOAM 6) OpenFOAM (Fujitsu PRIMERGY BX9, TFLOPS) Fluent 8) ( ) 9, 1) 11 13) OpenFOAM - realizable k-ε 1) Launder-Gibson 15) OpenFOAM 1.6 CFD ( )

7 OpenFOAM 6) OpenFOAM (Fujitsu PRIMERGY BX9, TFLOPS) Fluent 8) ( ) 9, 1) 11 13) OpenFOAM - realizable k-ε 1) Launder-Gibson 15) OpenFOAM 1.6 CFD ( ) 71 特集 オープンソースの大きな流れ Nonlinear Sloshing Analysis in a Three-dimensional Rectangular Pool Ken UZAWA, The Center for Computational Sciences and E-systems, Japan Atomic Energy Agency 1 1.1 ( ) (RIST) (ORNL/RSICC)

More information

The Effect of the Circumferential Temperature Change on the Change in the Strain Energy of Carbon Steel during the Rotatory Bending Fatigue Test by Ch

The Effect of the Circumferential Temperature Change on the Change in the Strain Energy of Carbon Steel during the Rotatory Bending Fatigue Test by Ch The Effect of the Circumferential Temperature Change on the Change in the Strain Energy of Carbon Steel during the Rotatory Bending Fatigue Test by Chikara MINAMISAWA, Nozomu AOKI (Department of Mechanical

More information

R927清水信彦様.indd

R927清水信彦様.indd Special Issue CFRP 455-8502 9 1 Development Status of Carbon Fiber Reinforced Plastics Nobuhiko SHIMIZU Automotive Center, Toray Industries, Inc., 9-1 Oe-cho, Minato-ku, Nagoya, Aichi 455-8502 Received

More information

Fig. 3 Coordinate system and notation Fig. 1 The hydrodynamic force and wave measured system Fig. 2 Apparatus of model testing

Fig. 3 Coordinate system and notation Fig. 1 The hydrodynamic force and wave measured system Fig. 2 Apparatus of model testing The Hydrodynamic Force Acting on the Ship in a Following Sea (1 St Report) Summary by Yutaka Terao, Member Broaching phenomena are most likely to occur in a following sea to relative small and fast craft

More information

Table 1 Experimental conditions Fig. 1 Belt sanded surface model Table 2 Factor loadings of final varimax criterion 5 6

Table 1 Experimental conditions Fig. 1 Belt sanded surface model Table 2 Factor loadings of final varimax criterion 5 6 JSPE-54-04 Factor Analysis of Relationhsip between One's Visual Estimation and Three Dimensional Surface Roughness Properties on Belt Sanded Surface Motoyoshi HASEGAWA and Masatoshi SHIRAYAMA This paper

More information

untitled

untitled CFD JAXA CFD CFD Navier-Stokes -1- -2-1 CFD CFD Navier-Stokes 1. 2. 2,500,000 CFD Copyright Boeing CFD Boeing B777 HP -3- -4-2 CFD European Transonic Wind tunnel (-163 ) JAXA 2mx2m CFD (Computational Fluid

More information

The Evaluation of LBB Behavior and Crack Opening Displacement on Statically Indeterminate Piping System Subjected to Monotonic Load The plastic collap

The Evaluation of LBB Behavior and Crack Opening Displacement on Statically Indeterminate Piping System Subjected to Monotonic Load The plastic collap The Evaluation of LBB Behavior and Crack Opening Displacement on Statically Indeterminate Piping System Subjected to Monotonic Load The plastic collapse and LBB behavior of statically indeterminate piping

More information

特-7.indd

特-7.indd Mechanical Properties and Weldability of Turbine Impeller Materials for High Temperature Exhaust Gas Turbocharger 1 000 1 050 246 IN100 The increase in environmental awareness in recent years has led to

More information

技術研究報告第26号

技術研究報告第26号 1) 2) 3) 250Hz 500Hz RESEARCH ON THE PHYSICAL VOLUME OF THE DYNAMIC VIBRATION RESPONSE AND THE REDUCTION OF THE FLOOR IMPACT SOUND LEVEL IN FLOORS OF RESIDENTIAL HOUSING Hideo WATANABE *1 This study was

More information

untitled

untitled Application of image correlation technique to determination of in-plane deformation distribution of paper Toshiharu Enomae Graduate School of Agricultural and Life Sciences The University of Tokyo 1 Peters

More information

Fig. 2 Signal plane divided into cell of DWT Fig. 1 Schematic diagram for the monitoring system

Fig. 2 Signal plane divided into cell of DWT Fig. 1 Schematic diagram for the monitoring system Study of Health Monitoring of Vehicle Structure by Using Feature Extraction based on Discrete Wavelet Transform Akihisa TABATA *4, Yoshio AOKI, Kazutaka ANDO and Masataka KATO Department of Precision Machinery

More information

Mikio Yamamoto: Dynamical Measurement of the E-effect in Iron-Cobalt Alloys. The AE-effect (change in Young's modulus of elasticity with magnetization

Mikio Yamamoto: Dynamical Measurement of the E-effect in Iron-Cobalt Alloys. The AE-effect (change in Young's modulus of elasticity with magnetization Mikio Yamamoto: Dynamical Measurement of the E-effect in Iron-Cobalt Alloys. The AE-effect (change in Young's modulus of elasticity with magnetization) in the annealed state of iron-cobalt alloys has been

More information

Plasticity-Induced Martensitic Transformation in Austenitic Stainless Steels SUS 304 and SUS 316 L at Room and Liquid Nitrogen Temperatures (Quantitat

Plasticity-Induced Martensitic Transformation in Austenitic Stainless Steels SUS 304 and SUS 316 L at Room and Liquid Nitrogen Temperatures (Quantitat Plasticity-Induced Martensitic Transformation in Austenitic Stainless Steels SUS 304 and SUS 316 L at Room and Liquid Nitrogen Temperatures (Quantitative Measurement using X-ray Diffraction Method) Yoshifumi

More information

A2, Vol. 69, No. 2 Vol. 16, I_237-I_246, Analytical Investigation of Shear Force Distribution of Perfobond Strip with Plural Perforations * ** *

A2, Vol. 69, No. 2 Vol. 16, I_237-I_246, Analytical Investigation of Shear Force Distribution of Perfobond Strip with Plural Perforations * ** * A2, Vol. 69, No. 2 Vol. 16, I_237-I_246, 213. Analytical Investigation of Shear Force Distribution of Perfobond Strip with Plural Perforations * ** *** **** ***** Noriyuki KUBO, Takeshi SAKAI, Shinji OHGUCHI,

More information

Optical Lenses CCD Camera Laser Sheet Wind Turbine with med Diffuser Pitot Tube PC Fig.1 Experimental facility. Transparent Diffuser Double Pulsed Nd:

Optical Lenses CCD Camera Laser Sheet Wind Turbine with med Diffuser Pitot Tube PC Fig.1 Experimental facility. Transparent Diffuser Double Pulsed Nd: *1 *2 *3 PIV Measurement of Field of the Wind Turbine with a med Diffuser Kazuhiko TOSHIMITSU *4, Koutarou NISHIKAWA and Yuji OHYA *4 Department of Mechanical Engineering, Matsue National Collage of Technology,

More information

卒業論文

卒業論文 Cu-Ru ...7 1.1....7 1.2....7 1.3....8...9 2.1....9 2.1.1....9 2.1.2....10 2.2.... 11 2.2.1.... 11 2.2.2. ()...12 2.2.3. ()...13 2.2....15...18 3.1. Cu z ...18 3.1.1....18 3.1.2....19 3.1.3....29 3.2.

More information

Journal of Japan Institute of Light Metals, Vol. 58, No. 2 (2008), pp

Journal of Japan Institute of Light Metals, Vol. 58, No. 2 (2008), pp 58 00847 53 * ** ** Journal of Japan Institute of Light Metals, Vol. 58, No. 008, pp. 47 53 Production of aluminum tall container with flange by hydraulic bulging with compression of surrounding material

More information

土木学会構造工学論文集(2011.3)

土木学会構造工学論文集(2011.3) Vol.57A (11 3 ) RC Consecutve falling-weight impact test of large-scale RC girders under specified total input-impact energy * ** *** **** ***** Norimitsu Kishi, Hisashi Konno, Satoru Yamaguchi, Hiroshi

More information

パナソニック技報

パナソニック技報 Smaller, Lighter and Higher-output Lithium Ion Battery System for Series Hybrid Shinji Ota Jun Asakura Shingo Tode 24 ICECU Electronic Control Unit46 16 We have developed a lithium-ion battery system with

More information

untitled

untitled 2M5-24 SM311 SM332 3 4 e30mm 5 e30mm [2M5-24] 0-5 -10-15 -20-150-125-100-75-50 -25 0 25 50 75 100 125 150 0-5 -10-15 -20-150-125-100-75-50 -25 0 25 50 75 100 125 150 0-5 -10-15 -20-150-125-100-75-50 -25

More information

力学的性質

力学的性質 Materials Science And Engineering, An Introduction: by William D. Callister, Jr., John Wiley & Sons, Inc. Mechanical Metallurgy, G.E.Dieter, McGraw Hill, 1987 Fundamentals of Metal Forming, Robert H. Wagoner,

More information

) BPA ECN EPICLON N-600 Fig.2 Fig Fig.4 DCPD EPICLON HP-7200 ECN Fig.5 DCPD ECN DCPD 6-28) Table 1 BPA Fig.4 Chemical str

) BPA ECN EPICLON N-600 Fig.2 Fig Fig.4 DCPD EPICLON HP-7200 ECN Fig.5 DCPD ECN DCPD 6-28) Table 1 BPA Fig.4 Chemical str Relation between Chemical Structures and Characteristics on Epoxy Resins OGURA Ichiro This paper presents the study of the relation between chemical structures and characteristics of epoxy resins with

More information

013858,繊維学会誌ファイバー1月/報文-02-古金谷

013858,繊維学会誌ファイバー1月/報文-02-古金谷 Development of Non-Contact Measuring Method for Final Twist Number of Double Ply Staple Yarn Keizo Koganeya 1, Youichi Yukishita 1, Hirotaka Fujisaki 1, Yasunori Jintoku 2, Hironori Okuno 2, and Motoharu

More information

Study on Fracture Strength Assessment (The 1st Report) Comparison of JWES approach and R6 approach by Susumu Machida, Member Yukito Hagiwara, Member H

Study on Fracture Strength Assessment (The 1st Report) Comparison of JWES approach and R6 approach by Susumu Machida, Member Yukito Hagiwara, Member H Study on Fracture Strength Assessment (The 1st Report) Comparison of JWES approach and R6 approach by Susumu Machida, Member Yukito Hagiwara, Member Hitoshi Yoshinari, Member J. G. Blauel Summary Japan

More information

Instability of Aerostatic Journal Bearings with Porous Floating Bush at High Speeds Masaaki MIYATAKE *4, Shigeka YOSHIMOTO, Tomoaki CHIBA and Akira CH

Instability of Aerostatic Journal Bearings with Porous Floating Bush at High Speeds Masaaki MIYATAKE *4, Shigeka YOSHIMOTO, Tomoaki CHIBA and Akira CH Instability of Aerostatic Journal Bearings with Porous Floating Bush at High Speeds Masaaki MIYATAKE *4, Shigeka YOSHIMOTO, Tomoaki CHIBA and Akira CHIBA Department of Mechanical Engineering, Tokyo University

More information

Fig. 1. Schematic drawing of testing system. 71 ( 1 )

Fig. 1. Schematic drawing of testing system. 71 ( 1 ) 1850 UDC 669.162.283 : 669.162.263.24/. 25 Testing Method of High Temperature Properties of Blast Furnace Burdens Yojiro YAMAOKA, Hirohisa HOTTA, and Shuji KAJIKAWA Synopsis : Regarding the reduction under

More information

S-5.indd

S-5.indd Development and pplication of Ultrasonic Noise B-scan nalysis ( I-CLT ) Creep Damage ssessment for Fossil-Fuel Boiler Piping precise creep damage assessment method has been required for boiler plants using

More information

Influence of Material and Thickness of the Specimen to Stress Separation of an Infrared Stress Image Kenji MACHIDA The thickness dependency of the temperature image obtained by an infrared thermography

More information

T05_Nd-Fe-B磁石.indd

T05_Nd-Fe-B磁石.indd Influence of Intergranular Grain Boundary Phases on Coercivity in Nd-Fe-B-based Magnets Takeshi Nishiuchi Teruo Kohashi Isao Kitagawa Akira Sugawara Hiroyuki Yamamoto To determine how to increase the coercivity

More information

撮 影

撮 影 DC cathode ray tube, 2.2 log log log + log log / / / A method determining tone conversion characteristics of digital still camera from two pictorial images Tone conversion characteristic Luminance

More information

4. C i k = 2 k-means C 1 i, C 2 i 5. C i x i p [ f(θ i ; x) = (2π) p 2 Vi 1 2 exp (x µ ] i) t V 1 i (x µ i ) 2 BIC BIC = 2 log L( ˆθ i ; x i C i ) + q

4. C i k = 2 k-means C 1 i, C 2 i 5. C i x i p [ f(θ i ; x) = (2π) p 2 Vi 1 2 exp (x µ ] i) t V 1 i (x µ i ) 2 BIC BIC = 2 log L( ˆθ i ; x i C i ) + q x-means 1 2 2 x-means, x-means k-means Bayesian Information Criterion BIC Watershed x-means Moving Object Extraction Using the Number of Clusters Determined by X-means Clustering Naoki Kubo, 1 Kousuke

More information

3. ( 1 ) Linear Congruential Generator:LCG 6) (Mersenne Twister:MT ), L 1 ( 2 ) 4 4 G (i,j) < G > < G 2 > < G > 2 g (ij) i= L j= N

3. ( 1 ) Linear Congruential Generator:LCG 6) (Mersenne Twister:MT ), L 1 ( 2 ) 4 4 G (i,j) < G > < G 2 > < G > 2 g (ij) i= L j= N RMT 1 1 1 N L Q=L/N (RMT), RMT,,,., Box-Muller, 3.,. Testing Randomness by Means of RMT Formula Xin Yang, 1 Ryota Itoi 1 and Mieko Tanaka-Yamawaki 1 Random matrix theory derives, at the limit of both dimension

More information

(1.2) T D = 0 T = D = 30 kn 1.2 (1.4) 2F W = 0 F = W/2 = 300 kn/2 = 150 kn 1.3 (1.9) R = W 1 + W 2 = = 1100 N. (1.9) W 2 b W 1 a = 0

(1.2) T D = 0 T = D = 30 kn 1.2 (1.4) 2F W = 0 F = W/2 = 300 kn/2 = 150 kn 1.3 (1.9) R = W 1 + W 2 = = 1100 N. (1.9) W 2 b W 1 a = 0 1 1 1.1 1.) T D = T = D = kn 1. 1.4) F W = F = W/ = kn/ = 15 kn 1. 1.9) R = W 1 + W = 6 + 5 = 11 N. 1.9) W b W 1 a = a = W /W 1 )b = 5/6) = 5 cm 1.4 AB AC P 1, P x, y x, y y x 1.4.) P sin 6 + P 1 sin 45

More information

1 Fig. 1 Extraction of motion,.,,, 4,,, 3., 1, 2. 2.,. CHLAC,. 2.1,. (256 ).,., CHLAC. CHLAC, HLAC. 2.3 (HLAC ) r,.,. HLAC. N. 2 HLAC Fig. 2

1 Fig. 1 Extraction of motion,.,,, 4,,, 3., 1, 2. 2.,. CHLAC,. 2.1,. (256 ).,., CHLAC. CHLAC, HLAC. 2.3 (HLAC ) r,.,. HLAC. N. 2 HLAC Fig. 2 CHLAC 1 2 3 3,. (CHLAC), 1).,.,, CHLAC,.,. Suspicious Behavior Detection based on CHLAC Method Hideaki Imanishi, 1 Toyohiro Hayashi, 2 Shuichi Enokida 3 and Toshiaki Ejima 3 We have proposed a method for

More information

Stress Singularity Analysis at an Interfacial Corner Between Anisotropic Bimaterials Under Thermal Stress Yoshiaki NOMURA, Toru IKEDA*4 and Noriyuki M

Stress Singularity Analysis at an Interfacial Corner Between Anisotropic Bimaterials Under Thermal Stress Yoshiaki NOMURA, Toru IKEDA*4 and Noriyuki M Stress Singularity Analysis at an Interfacial Corner Between Anisotropic Bimaterials Under Thermal Stress Yoshiaki NOMURA, Toru IKEDA*4 and Noriyuki MIYAZAKI Department of Mechanical Engineering and Science,

More information

14 FEM [1] 1992 [3] 1(a)(b) 1(c) [2] 2 ( 財 ) 日本海事協会 36 平成 14 年度 ClassNK 研究発表会

14 FEM [1] 1992 [3] 1(a)(b) 1(c) [2] 2 ( 財 ) 日本海事協会 36 平成 14 年度 ClassNK 研究発表会 1. 1(1) 1(2)[1] 1992 [2] 1992 [3] 100 100 比率 (%) 80 60 40 変形腐食亀裂 相対損傷数 80 60 40 変形腐食亀裂 20 20 0 0 5 10 15 20 25 船齢 ( 年 ) 0 0 5 10 15 20 25 船齢 ( 年 ) (1) Ratio of Each Damage (2) Number of Damage Fig.1 Relation

More information

1 1.1,,,.. (, ),..,. (Fig. 1.1). Macro theory (e.g. Continuum mechanics) Consideration under the simple concept (e.g. ionic radius, bond valence) Stru

1 1.1,,,.. (, ),..,. (Fig. 1.1). Macro theory (e.g. Continuum mechanics) Consideration under the simple concept (e.g. ionic radius, bond valence) Stru 1. 1-1. 1-. 1-3.. MD -1. -. -3. MD 1 1 1.1,,,.. (, ),..,. (Fig. 1.1). Macro theory (e.g. Continuum mechanics) Consideration under the simple concept (e.g. ionic radius, bond valence) Structural relaxation

More information

.I.v e pmd

.I.v e pmd Structural Design for Curved Panels by Laminated Composite Materials (Identification of Lamination Parameters Using Modal Testing Method ) Tetsuya NARISAWA, Shohei IWATA Abstract - Using a modal testing

More information

Estimation of Photovoltaic Module Temperature Rise Motonobu Yukawa, Member, Masahisa Asaoka, Non-member (Mitsubishi Electric Corp.) Keigi Takahara, Me

Estimation of Photovoltaic Module Temperature Rise Motonobu Yukawa, Member, Masahisa Asaoka, Non-member (Mitsubishi Electric Corp.) Keigi Takahara, Me Estimation of Photovoltaic Module Temperature Rise Motonobu Yukawa, Member, Masahisa Asaoka, Non-member (Mitsubishi Electric Corp.) Keigi Takahara, Member (Okinawa Electric Power Co.,Inc.) Toshimitsu Ohshiro,

More information

Continuous Cooling Transformation Diagrams for Welding of Mn-Si Type 2H Steels. Harujiro Sekiguchi and Michio Inagaki Synopsis: The authors performed

Continuous Cooling Transformation Diagrams for Welding of Mn-Si Type 2H Steels. Harujiro Sekiguchi and Michio Inagaki Synopsis: The authors performed Continuous Cooling Transformation Diagrams for Welding of Mn-Si Type 2H Steels. Harujiro Sekiguchi and Michio Inagaki Synopsis: The authors performed a series of researches on continuous cooling transformation

More information

Time and Temperature Dependence of Recovery Behavior of Residual Strains in Largely Deformed Glassy Poly (Methyl Methacrylate) by Shin'ya YOSHIOKA*, Ryoji NAKAGAWA** and Yukuo NANZAI* Time and temperature

More information

Table 1 Properties of Shrink Films on Market Fig. 2 Comparison of Shrinkage curves of PS and PET films. Fig. 3 Schematic diagram of "Variations in bot

Table 1 Properties of Shrink Films on Market Fig. 2 Comparison of Shrinkage curves of PS and PET films. Fig. 3 Schematic diagram of Variations in bot Bowing Reduction in Biaxial Stretching Process of Styrenic Shrink Film and Its Properties YAMADA Hirofumi TAKEI Toshio and MORITA Tsuyoshi Trimming weight of PET bottle is tried from the trends of aseptic

More information

Table 1 Type of polymeric coating materials Fig. 2 Results of suppressive effects of polymeric coating materials on the progress of neutralization of concrete. Table 2 Evaluation of the suppressive effects

More information

206“ƒŁ\”ƒ-fl_“H„¤‰ZŁñ

206“ƒŁ\”ƒ-fl_“H„¤‰ZŁñ 51 206 51 63 2007 GIS 51 1 60 52 2 60 1 52 3 61 2 52 61 3 58 61 4 58 Summary 63 60 20022005 2004 40km 7,10025 2002 2005 19 3 19 GIS 2005GIS 2006 2002 2004 GIS 52 2062007 1 2004 GIS Fig.1 GIS ESRIArcView

More information

: u i = (2) x i Smagorinsky τ ij τ [3] ij u i u j u i u j = 2ν SGS S ij, (3) ν SGS = (C s ) 2 S (4) x i a u i ρ p P T u ν τ ij S c ν SGS S csgs

: u i = (2) x i Smagorinsky τ ij τ [3] ij u i u j u i u j = 2ν SGS S ij, (3) ν SGS = (C s ) 2 S (4) x i a u i ρ p P T u ν τ ij S c ν SGS S csgs 15 C11-4 Numerical analysis of flame propagation in a combustor of an aircraft gas turbine, 4-6-1 E-mail: tominaga@icebeer.iis.u-tokyo.ac.jp, 2-11-16 E-mail: ntani@iis.u-tokyo.ac.jp, 4-6-1 E-mail: itoh@icebeer.iis.u-tokyo.ac.jp,

More information

日立金属技報 Vol.34

日立金属技報 Vol.34 Influence of Misorientation Angle between Adjacent Grains on Magnetization Reversal in Nd-Fe-B Sintered Magnet Tomohito Maki Rintaro Ishii Mitsutoshi Natsumeda Takeshi Nishiuchi Ryo Uchikoshi Masaaki Takezawa

More information

SAXS Table 1 DSC POM SAXSSAXS PF BL-10C BL-15A Fig. 2 LC12 DSC SAXS 138 C T iso T iso SAXS q=1.4 nm -1 q=(4π/λ)sin(θ/2), λ:, θ: Fig. 3 LC12 T iso Figu

SAXS Table 1 DSC POM SAXSSAXS PF BL-10C BL-15A Fig. 2 LC12 DSC SAXS 138 C T iso T iso SAXS q=1.4 nm -1 q=(4π/λ)sin(θ/2), λ:, θ: Fig. 3 LC12 T iso Figu 1 1 1 1,2 1,2 1 2 Correlation between Microphase Separation and Liquid Crystallization in Structure Formation of Liquid Crystalline Block Copolymers Shin-ichi TANIGUCHI 1, Hiroki TAKESHITA 1, Masamitsu

More information

車両開発における構造・機構のCAE

車両開発における構造・機構のCAE Mechanical CAE in Automotive Design Yoshio Kojima The urgent issues for automobile companies today are how to reduce the time and cost required for developing a new car. CAE ( Computer Aided Engineering

More information

note1.dvi

note1.dvi (1) 1996 11 7 1 (1) 1. 1 dx dy d x τ xx x x, stress x + dx x τ xx x+dx dyd x x τ xx x dyd y τ xx x τ xx x+dx d dx y x dy 1. dx dy d x τ xy x τ x ρdxdyd x dx dy d ρdxdyd u x t = τ xx x+dx dyd τ xx x dyd

More information

S-6.indd

S-6.indd Structural Health Monitoring with Fiber Optic Deformation Sensor ( SOFO ) SOFO SOFO ( SOFO V ) ( SOFO Dynamic ) 2 SOFO The fiber optic deformation sensor, SOFO, has excellent characteristics such as ease

More information

perature was about 2.5 Ž higher than that of the control irrespective of wind speed. With increasing wind speeds of more than 1m/s, the leaf temperatu

perature was about 2.5 Ž higher than that of the control irrespective of wind speed. With increasing wind speeds of more than 1m/s, the leaf temperatu Studies on the Row Covering Methods of Vinylon Cheesecloth to Prevent Cold Injury in Cabbage Daizou IGARASHI*, Masumi OKADA** and Keiichl NAKAYAMA*** *Miura Branch, Kanagawa Horticultural Experiment Station,

More information

鉄鋼協会プレゼン

鉄鋼協会プレゼン NN :~:, 8 Nov., Adaptive H Control for Linear Slider with Friction Compensation positioning mechanism moving table stand manipulator Point to Point Control [G] Continuous Path Control ground Fig. Positoining

More information

& Vol.5 No (Oct. 2015) TV 1,2,a) , Augmented TV TV AR Augmented Reality 3DCG TV Estimation of TV Screen Position and Ro

& Vol.5 No (Oct. 2015) TV 1,2,a) , Augmented TV TV AR Augmented Reality 3DCG TV Estimation of TV Screen Position and Ro TV 1,2,a) 1 2 2015 1 26, 2015 5 21 Augmented TV TV AR Augmented Reality 3DCG TV Estimation of TV Screen Position and Rotation Using Mobile Device Hiroyuki Kawakita 1,2,a) Toshio Nakagawa 1 Makoto Sato

More information

空力騒音シミュレータの開発

空力騒音シミュレータの開発 41 COSMOS-V, an Aerodynamic Noise Simulator Nariaki Horinouchi COSMOS-V COSMOS-V COSMOS-V 3 The present and future computational problems of the aerodynamic noise analysis using COSMOS-V, our in-house

More information

29 Short-time prediction of time series data for binary option trade

29 Short-time prediction of time series data for binary option trade 29 Short-time prediction of time series data for binary option trade 1180365 2018 2 28 RSI(Relative Strength Index) 3 USD/JPY 1 2001 1 2 4 10 2017 12 29 17 00 1 high low i Abstract Short-time prediction

More information

JAMSTEC Rep. Res. Dev., Volume 12, March 2011, 27 _ 35 1,2* Pb 210 Pb 214 Pb MCA 210 Pb MCA MCA 210 Pb 214 Pb * 2

JAMSTEC Rep. Res. Dev., Volume 12, March 2011, 27 _ 35 1,2* Pb 210 Pb 214 Pb MCA 210 Pb MCA MCA 210 Pb 214 Pb * 2 JAMSTEC Rep. Res. Dev., Volume 12, March 2011, 27 _ 35 1,2* 1 1 1 1 210 Pb 210 Pb 214 Pb MCA 210 Pb MCA MCA 210 Pb 214 Pb 2010 10 4 2010 12 10 1 2 * 237-0061 2-15 046-867-9794 ogurik@jamstec.go.jp 27 210

More information

2 ( ) i

2 ( ) i 25 Study on Rating System in Multi-player Games with Imperfect Information 1165069 2014 2 28 2 ( ) i ii Abstract Study on Rating System in Multi-player Games with Imperfect Information Shigehiko MORITA

More information

変 位 変位とは 物体中のある点が変形後に 別の点に異動したときの位置の変化で あり ベクトル量である 変位には 物体の変形の他に剛体運動 剛体変位 が含まれている 剛体変位 P(x, y, z) 平行移動と回転 P! (x + u, y + v, z + w) Q(x + d x, y + dy,

変 位 変位とは 物体中のある点が変形後に 別の点に異動したときの位置の変化で あり ベクトル量である 変位には 物体の変形の他に剛体運動 剛体変位 が含まれている 剛体変位 P(x, y, z) 平行移動と回転 P! (x + u, y + v, z + w) Q(x + d x, y + dy, 変 位 変位とは 物体中のある点が変形後に 別の点に異動したときの位置の変化で あり ベクトル量である 変位には 物体の変形の他に剛体運動 剛体変位 が含まれている 剛体変位 P(x, y, z) 平行移動と回転 P! (x + u, y + v, z + w) Q(x + d x, y + dy, z + dz) Q! (x + d x + u + du, y + dy + v + dv, z +

More information

A Feasibility Study of Direct-Mapping-Type Parallel Processing Method to Solve Linear Equations in Load Flow Calculations Hiroaki Inayoshi, Non-member

A Feasibility Study of Direct-Mapping-Type Parallel Processing Method to Solve Linear Equations in Load Flow Calculations Hiroaki Inayoshi, Non-member A Feasibility Study of Direct-Mapping-Type Parallel Processing Method to Solve Linear Equations in Load Flow Calculations Hiroaki Inayoshi, Non-member (University of Tsukuba), Yasuharu Ohsawa, Member (Kobe

More information

, 3, STUDY ON IMPORTANCE OF OPTIMIZED GRID STRUCTURE IN GENERAL COORDINATE SYSTEM 1 2 Hiroyasu YASUDA and Tsuyoshi HOSHINO

, 3, STUDY ON IMPORTANCE OF OPTIMIZED GRID STRUCTURE IN GENERAL COORDINATE SYSTEM 1 2 Hiroyasu YASUDA and Tsuyoshi HOSHINO , 3, 2012 9 STUDY ON IMPORTANCE OF OPTIMIZED GRID STRUCTURE IN GENERAL COORDINATE SYSTEM 1 2 Hiroyasu YASUDA and Tsuyoshi HOSHINO 1 950-2181 2 8050 2 950-2181 2 8050 Numerical computation of river flows

More information

磁性物理学 - 遷移金属化合物磁性のスピンゆらぎ理論

磁性物理学 - 遷移金属化合物磁性のスピンゆらぎ理論 email: takahash@sci.u-hyogo.ac.jp May 14, 2009 Outline 1. 2. 3. 4. 5. 6. 2 / 262 Today s Lecture: Mode-mode Coupling Theory 100 / 262 Part I Effects of Non-linear Mode-Mode Coupling Effects of Non-linear

More information

DEIM Forum 2009 C8-4 QA NTT QA QA QA 2 QA Abstract Questions Recomme

DEIM Forum 2009 C8-4 QA NTT QA QA QA 2 QA Abstract Questions Recomme DEIM Forum 2009 C8-4 QA NTT 239 0847 1 1 E-mail: {kabutoya.yutaka,kawashima.harumi,fujimura.ko}@lab.ntt.co.jp QA QA QA 2 QA Abstract Questions Recommendation Based on Evolution Patterns of a QA Community

More information

MmUm+FopX m Mm+Mop F-Mm(Fop-Mopum)M m+mop MSuS+FX S M S+MOb Fs-Ms(Mobus-Fex)M s+mob Fig. 1 Particle model of single degree of freedom master/ slave sy

MmUm+FopX m Mm+Mop F-Mm(Fop-Mopum)M m+mop MSuS+FX S M S+MOb Fs-Ms(Mobus-Fex)M s+mob Fig. 1 Particle model of single degree of freedom master/ slave sy Analysis and Improvement of Digital Control Stability for Master-Slave Manipulator System Koichi YOSHIDA* and Tetsuro YABUTA* Some bilateral controls of master-slave system have been designed, which can

More information

(1 ) (2 ) Table 1. Details of each bar group sheared simultaneously (major shearing unit). 208

(1 ) (2 ) Table 1. Details of each bar group sheared simultaneously (major shearing unit). 208 2463 UDC 621.771.251.09 : 621.791.94: 669.012.5 Improvement in Cold Shear Yield of Bar Mill by Computer Control System Koji INAZAKI, Takashi WASEDA, Michiaki TAKAHASHI, and Toshihiro OKA Synopsis: The

More information

修士論文

修士論文 2004 Decay of timber and its mechanical characteristic 1075015 1075015 1. 1 1. 2. 3. 4. 5. 4.5. 2. JIS 3. 3.1 3.1.1 ( ) ( ) i 3.1.2 3.1.3 10 3.2 ( 3% ) 4 3% ii Decay of timber and its mechanical characteristic

More information

2003/3 Vol. J86 D II No.3 2.3. 4. 5. 6. 2. 1 1 Fig. 1 An exterior view of eye scanner. CCD [7] 640 480 1 CCD PC USB PC 2 334 PC USB RS-232C PC 3 2.1 2

2003/3 Vol. J86 D II No.3 2.3. 4. 5. 6. 2. 1 1 Fig. 1 An exterior view of eye scanner. CCD [7] 640 480 1 CCD PC USB PC 2 334 PC USB RS-232C PC 3 2.1 2 Curved Document Imaging with Eye Scanner Toshiyuki AMANO, Tsutomu ABE, Osamu NISHIKAWA, Tetsuo IYODA, and Yukio SATO 1. Shape From Shading SFS [1] [2] 3 2 Department of Electrical and Computer Engineering,

More information

.N..

.N.. Examination of the lecture by the questionnaire of class evaluation -Analysis and proposal of result at the first term of fiscal year - Kazuo MORI, Tukasa FUKUSHIMA, Michio TAKEUCHI, Norihiro UMEDA, Katuya

More information

System to Diagnosis Concrete Deterioration with Spectroscopic Analysis IHI IHI IHI The most popular method for inspecting concrete structures for dete

System to Diagnosis Concrete Deterioration with Spectroscopic Analysis IHI IHI IHI The most popular method for inspecting concrete structures for dete System to Diagnosis Concrete Deterioration with Spectroscopic Analysis IHI IHI IHI The most popular method for inspecting concrete structures for deterioration ( for example, due to chloride attack ) is

More information

Fig. 1 Structure of a Sebaceous Follicle (Ref.1).

Fig. 1 Structure of a Sebaceous Follicle (Ref.1). Importance and Countermeasures for Sebum Control in Application of Makeup Cosmetics Koichi NOMURA POLA Chemical Industries, Inc., R&D Planning Department 27-1, Takashimadai, Kanagawa-ku, Yokohama 221-0833,

More information

[ 30 p. 1-8 (2012)] / ** *** Numerical Analysis of Metal Transfer Phenomena - critical condition between globular and spray transfer mode - by KADOTA

[ 30 p. 1-8 (2012)] / ** *** Numerical Analysis of Metal Transfer Phenomena - critical condition between globular and spray transfer mode - by KADOTA [ 30 p. 1-8 (2012)] / ** *** Numerical Analysis of Metal Transfer Phenomena - critical condition between globular and spray transfer mode - by KADOTA Keiji and HIRATA Yoshinori Metal transfer modes in

More information

新しい価値創出に貢献する大規模CAEシミュレーション

新しい価値創出に貢献する大規模CAEシミュレーション CAE Large-scale CAE Simulation Supporting New Value-creation あらまし CAE Computer Aided Engineering LS-DYNA CAE CAE afjrls-dyna CAE Abstract In the manufacturing industry, numerical simulation assisted by

More information

Title 混合体モデルに基づく圧縮性流体と移動する固体の熱連成計算手法 Author(s) 鳥生, 大祐 ; 牛島, 省 Citation 土木学会論文集 A2( 応用力学 ) = Journal of Japan Civil Engineers, Ser. A2 (2017), 73 Issue

Title 混合体モデルに基づく圧縮性流体と移動する固体の熱連成計算手法 Author(s) 鳥生, 大祐 ; 牛島, 省 Citation 土木学会論文集 A2( 応用力学 ) = Journal of Japan Civil Engineers, Ser. A2 (2017), 73 Issue Title 混合体モデルに基づく圧縮性流体と移動する固体の熱連成計算手法 Author(s) 鳥生, 大祐 ; 牛島, 省 Citation 土木学会論文集 A2( 応用力学 ) = Journal of Japan Civil Engineers, Ser. A2 (2017), 73 Issue Date 2017 URL http://hdl.handle.net/2433/229150 Right

More information

Fig.2 Optical-microscope image of the Y face-cross sec- tion of the bulk domain structure of a 0.4-mm-thick MgO-LiNbO3 crystal after chemical etching.

Fig.2 Optical-microscope image of the Y face-cross sec- tion of the bulk domain structure of a 0.4-mm-thick MgO-LiNbO3 crystal after chemical etching. Blue EGreen Solid State Lasers Using MgO-LiNbO3 Periodic Domain Inverted Bulk Crystal and Their Applications Koji KAMIYAMA, Yoji OKAZAKI, and Akinori HARADA Fuji Photo Film. Co., Ltd., Miyanodai Technology

More information

Vol. 21, No. 2 (2014) W 3 mm SUS304 Ni 650 HV 810 HV Ni Ni Table1 Ni Ni μm SUS mm w 50 mm l 3 mm t 2.2 Fig. 1 XY Fig. 3 Sch

Vol. 21, No. 2 (2014) W 3 mm SUS304 Ni 650 HV 810 HV Ni Ni Table1 Ni Ni μm SUS mm w 50 mm l 3 mm t 2.2 Fig. 1 XY Fig. 3 Sch 110 : 565-0871 2-1 567-0871 11-1 660-0811 1-9 - 1 tanigawa@jwri.osaka - u.ac.jp Influence of Laser Beam Profile on Cladding Layer TANIGAWA Daichi, ABE Nobuyuki, TSUKAMOTO Masahiro, HAYASHI Yoshihiko, YAMAZAKI

More information